<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xmlns:planet="http://planet.intertwingly.net/" xmlns:indexing="urn:atom-extension:indexing" indexing:index="no">
  <title>Planet Musings</title>
  <updated>2012-02-15T04:46:01Z</updated>
  <generator uri="http://intertwingly.net/code/venus/">Venus</generator>
  <author>
    <name>Jacques Distler</name>
    <email>distler@golem.ph.utexas.edu</email>
  </author>
  <id>http://golem.ph.utexas.edu/~distler/planet/atom.xml</id>
  <link href="http://golem.ph.utexas.edu/~distler/planet/atom.xml" rel="self" type="application/atom+xml"/>
  <link href="http://golem.ph.utexas.edu/~distler/planet/" rel="alternate"/>

  <entry>
    <id>tag:blogger.com,1999:blog-13869903.post-5555606302774605223</id>
    <link href="http://nanoscale.blogspot.com/feeds/5555606302774605223/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=13869903&amp;postID=5555606302774605223" rel="replies" title="0 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/13869903/posts/default/5555606302774605223" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/13869903/posts/default/5555606302774605223" rel="self" type="application/atom+xml"/>
    <link href="http://nanoscale.blogspot.com/2012/02/gaming-system.html" rel="alternate" title="Gaming the system" type="text/html"/>
    <title>Gaming the system</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><div style="font-family: Verdana,sans-serif;"><span style="font-size: 85%;">Two semi-related topics have come to mind lately.  First, <a href="http://science-professor.blogspot.com/2012/02/citation-conspiracy.html" target="_blank">this post</a> by the FSP caught my attention, regarding "citation circles", where a sub-community within a scientific discipline agree to cite each others' work.  I've heard of such things, and there's nothing inherently wrong there as long as the citations are relevant and don't consciously omit other equally relevant papers.  Still, I never considered this practice to have too much impact.  Back when I was in grad school, I'd heard of something that is equally fine ethically, and perhaps more important to progress in the long term:  the timely reviewing circle - a group of scientists who agree to respond promptly to invitations to review one anothers' work.  This is not a matter of conspiring to give positive reviews, but an agreement to get manuscripts through the review process quickly.  Imagine if certain "Letters" journals were actually speedy!</span></div><div style="font-family: Verdana,sans-serif;"><span style="font-size: x-small;"><br/></span></div><span style="font-size: 85%;"><span style="font-family: Verdana,sans-serif;">The second topic is the idea of trying to influence the selection of referees.  Of course, under many circumstances you as an author can suggest possible referees for scientific papers or grant proposals.  Let's call that a first-order influence.  It's a way of making sure that the editors can get the paper out to technically knowledgeable people in a specialty.  (I've been told by multiple editors that authors who try to suggest "friendly" referees often do themselves more harm than good, because those suggested reviewers are often more harsh than randomly selected peers.)  Recently I learned about a "higher-order" approach:  avoiding citing the work of potentially hostile reviewers, under the assumption that the editor/program officer often gets referee ideas from the reference lists.  I am very skeptical that this approach could matter in a statistically significant way.</span></span><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/13869903-5555606302774605223?l=nanoscale.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-15T04:17:35Z</updated>
    <published>2012-02-15T04:17:00Z</published>
    <author>
      <name>Doug Natelson</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/13340091255404229559</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-13869903</id>
      <category term="concepts"/>
      <author>
        <name>Doug Natelson</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/13340091255404229559</uri>
      </author>
      <link href="http://nanoscale.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/13869903/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://nanoscale.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/13869903/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>A blog about condensed matter and nanoscale physics.  Why should high energy and astro folks have all the fun?</subtitle>
      <title>nanoscale views</title>
      <updated>2012-02-15T04:17:35Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://sbseminar.wordpress.com/?p=4498</id>
    <link href="http://sbseminar.wordpress.com/2012/02/14/arxiv-overlays-at-scholastica/" rel="alternate" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/02/14/arxiv-overlays-at-scholastica/#comments" rel="replies" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/02/14/arxiv-overlays-at-scholastica/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">arXiv overlays at Scholastica</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">The guys at Scholastica (some grad students at UChicago) just added arXiv integration to their journal management software. It’s pretty impressive, and it seems they’re very actively working on the software. I’m sure they’d be really excited if one upshot of the current debate about publishing was some journals switching to (or new journals starting [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4498&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>The guys at <a href="http://scholasticahq.com">Scholastica</a> (some grad students at UChicago) just added <a href="http://blog.scholasticahq.com/post/17592143685/arxiv-integration-with-scholastica-scholastica">arXiv integration</a> to their journal management software.</p>
<p>It’s pretty impressive, and it seems they’re very actively working on the software. I’m sure they’d be really excited if one upshot of the current debate about publishing was some journals switching to (or new journals starting on) their software. If journals are going to abandon the big commercial publishers, we need to make sure there are viable alternatives; and part of that is ensuring that the basic software for managing manuscripts and referee reports is up to par. Even if we’re not actually ready to move on any particular journals, it seems like it would be pretty useful to try out things like Scholastica, and their ‘competitors’ <a href="http://pkp.sfu.ca/?q=ojs">OJS</a>, <a href="http://annotum.org/">Annotum</a>, and <a href="http://msp.org/services.html">EditFlow</a>. Explaining which features are needed to the developers, and being able to explain to editorial boards exactly what is available, will be really helpful.</p>
<p>I created a dummy journal on their site, called “<a href="http://scholasticahq.com/journals/experiments-in-mathematical-publishing">Experiments in Mathematical Publishing</a>“. If anyone would like to play around with the interface, try submitting a paper there. (Submit one of your old arXiv papers, for example!) Their interface has a feedback form, and we can discuss things here or, even better, over at the <a href="http://www.math.ntnu.no/~stacey/Mathforge/Math2.0/comments.php?DiscussionID=23">Math2.0 forum</a>. If you submit something, I’ll ‘assign’ something to you to ‘referee’, for the sake of trying out the whole interface. If anyone would like to be an ‘editor’, just let me know. I’ll eventually delete the journal, of course.</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/sbseminar.wordpress.com/4498/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/sbseminar.wordpress.com/4498/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/sbseminar.wordpress.com/4498/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4498&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-14T21:21:38Z</updated>
    <published>2012-02-14T21:20:03Z</published>
    <category scheme="http://sbseminar.wordpress.com" term="journals"/>
    <category scheme="http://sbseminar.wordpress.com" term="publishing"/>
    <author>
      <name>Scott Morrison</name>
      <uri>http://tqft.net/</uri>
    </author>
    <source>
      <id>http://sbseminar.wordpress.com/feed/atom/</id>
      <link href="http://sbseminar.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://sbseminar.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://sbseminar.wordpress.com/osd.xml" rel="search" title="Secret Blogging Seminar" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://sbseminar.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Representation theory, geometry and whatever else we decide is worth writing about today.</subtitle>
      <title xml:lang="en">Secret Blogging Seminar</title>
      <updated>2012-02-14T21:21:39Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>tag:golem.ph.utexas.edu,2012:%2Fcategory%2F3.2497</id>
    <link href="http://golem.ph.utexas.edu/category/2012/02/modern_perspectives_in_homotop.html" rel="alternate" type="application/xhtml+xml"/>
    <title type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><em>Modern Perspectives in Homotopy Theory</em></div>
    </title>
    <summary xml:lang="en">A school on modern developments in homotopy theory.</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img alt="MathML-enabled post (click for more details)." class="mathlogo" src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" title="MathML-enabled post (click for details)."/></a></div>

<p>This April (10th - 13th) takes place the a school titled</p>

<p><em><strong>Modern Perspectives in <a href="http://ncatlab.org/nlab/show/homotopy%20theory">Homotopy Theory</a></strong></em></p>

<p>subtitled</p>

<p><em><a href="http://ncatlab.org/nlab/show/%28infinity,1%29-category">∞-Categories</a>, <a href="http://ncatlab.org/nlab/show/%28infinity,1%29-operad">∞-Operads</a> and <a href="http://ncatlab.org/nlab/show/homotopy%20type%20theory">Homotopy Type Theory</a></em></p>

<p>in Swansea, UK.</p>

<p>See the <a href="http://maths.swan.ac.uk/staff/jhg/minischool2012/index.html">school’s website</a>. </p>

<p>David Gepner will speak about <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mn>∞</mn></math>-categories, Ieke Moerdijk about <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mn>∞</mn></math>-operads (and <a href="http://ncatlab.org/nlab/show/dendroidal%20set">dendroidal sets</a>), and Mike Shulman about <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mn>∞</mn></math>-type theory.</p></div>
    </content>
    <updated>2012-02-14T21:19:22Z</updated>
    <published>2012-02-14T21:07:58Z</published>
    <category term="Conference"/>
    <author>
      <name>urs</name>
      <email>urs.schreiber@math.uni-hamburg.de</email>
      <uri>http://www.math.uni-hamburg.de/home/schreiber</uri>
    </author>
    <source>
      <id>tag:golem.ph.utexas.edu,2006:nCategoryCafe/3</id>
      <icon>http://golem.ph.utexas.edu/category/images/favicon.ico</icon>
      <link href="http://golem.ph.utexas.edu/category/" rel="alternate" type="application/xhtml+xml"/>
      <link href="http://golem.ph.utexas.edu/category/atom10.xml" rel="self" type="application/atom+xml"/>
      <link href="http://golem.ph.utexas.edu/category/comments.atom" rel="replies" type="application/atom+xml"/>
      <rights xml:lang="en">Copyright (c) 2012, The n-Category Collective</rights>
      <subtitle xml:lang="en">A group blog on math, physics and philosophy</subtitle>
      <title xml:lang="en">The n-Category Café</title>
      <updated>2012-02-14T21:19:22Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://asymptotia.com/?p=11218</id>
    <link href="http://asymptotia.com/2012/02/14/entangled-2/" rel="alternate" type="text/html"/>
    <link href="http://asymptotia.com/2012/02/14/entangled-2/#comments" rel="replies" type="text/html"/>
    <link href="http://asymptotia.com/2012/02/14/entangled-2/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Entangled</title>
    <summary xml:lang="en">Gosh, I got a bit swamped there over the last week. Several things took me away from sitting down and doing a blog post, including teaching my class (more on that shortly), working on a film project (more on that longly)  and doing my taxes (late this year - bah!) and the usual raft of committee meetings and so forth. But one of them was locking myself away for two days with my computer and a web connection and writing a paper from start to finish with  Tameem Albash. We'd more or less completed the bulk of the project  over two months ago, with some very interesting results that we'd talk about from time to time to try to understand what was going on, but I held things up, being distracted by several other things (some of which you know about from this blog). We decided two weeks ago that we'd just finish the thing once and for all, and then somehow ten days went by with me not getting to it. Then I decided to close the door and just do it. So from lunchtime on Friday through lunchtime on Sunday I became a recluse (kind of) and I wrote, in turn with Tameem, as we emailed and IMed back and forth, until we had a nice paper entitled "Holographic Studies of Entanglement Entropy in Superconductors". 

It is a project I've been hoping to do for a long time, but not all the pieces were on the market until late last year.  The entanglement entropy has been a quantity of interest among physicists in various fields for years, especially in the condensed matter and quantum information community, and is regarded [...]</summary>
    <updated>2012-02-14T20:53:49Z</updated>
    <published>2012-02-14T19:36:39Z</published>
    <category scheme="http://asymptotia.com" term="Los Angeles"/>
    <category scheme="http://asymptotia.com" term="science"/>
    <category scheme="http://asymptotia.com" term="string theory"/>
    <category scheme="http://asymptotia.com" term="work"/>
    <author>
      <name>Clifford</name>
      <uri>http://asymptotia.com</uri>
    </author>
    <source>
      <id>http://asymptotia.com/feed/atom/</id>
      <link href="http://asymptotia.com" rel="alternate" type="text/html"/>
      <link href="http://asymptotia.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <title xml:lang="en">Asymptotia</title>
      <updated>2012-02-14T20:53:49Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/catdynamics/2012/02/must_read.php</id>
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/_MUlAL2pA2Y/must_read.php" rel="alternate" type="text/html"/>
    <title>Must Read</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
for astronomers:</p>

<p><a href="http://arxiv.org/abs/1202.2738">Discovery and Depth</a></p>

<p>"...the current situation calls for bold leadership and tough decisions and not merely the proverbial rearrangement of the chairs in the dining hall of the Costa Concordia as it approached the Isola del Giglio."<sup>14</sup> Kulkarni (2011)</p> <a href="http://scienceblogs.com/catdynamics/2012/02/must_read.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/_MUlAL2pA2Y" width="1"/></div>
    </summary>
    <updated>2012-02-14T16:55:55Z</updated>
    <category term="astro"/>
    <source>
      <id>http://scienceblogs.com/catdynamics/</id>
      <author>
        <name>Steinn Sigurðsson</name>
      </author>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Speculations on astronomy, astrophysics, news I find interesting, theoretical issues, science and science policy.  
I will digress into computational physics, science fiction and general issues and basically whatever I feel like whenever. 
And, of course, cats.</subtitle>
      <title>Dynamics of Cats</title>
      <updated>2012-02-14T17:08:27Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://quomodocumque.wordpress.com/?p=3311</id>
    <link href="http://quomodocumque.wordpress.com/2012/02/14/bayesian-linference/" rel="alternate" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/14/bayesian-linference/#comments" rel="replies" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/14/bayesian-linference/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Bayesian Linference</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">I hate to go up against Nate Silver on a subject he knows much better than I do, but is he really right that there’s a one-in-four chance that Jeremy Lin is actually a Hall-of-Fame-level superstar, based on his first four starts in the league? Silver observes that only 41 times in the last 25 [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3311&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>I hate to go up against Nate Silver on a subject he knows much better than I do, but is he really right that <a href="http://fivethirtyeight.blogs.nytimes.com/2012/02/11/jeremy-lin-is-no-fluke/">there’s a one-in-four chance that Jeremy Lin is actually a Hall-of-Fame-level superstar</a>, based on his first four starts in the league?</p>
<p>Silver observes that only 41 times in the last 25 years has a player scored 20 points, shot 50% from the field, and recorded 6 assists in four straight games, as Lin did last week.  Most of those players were really, really good — about a quarter are in the hall of fame.  Michael Jordan, LeBron James, Isaiah Thomas — you get the idea.</p>
<p>But there’s something fishy here.  This isn’t a list of “streaks as good as Jeremy Lin’s first four games.”  It’s a list of “streaks which are good as Jeremy Lin’s first four games in the <em>exact same way</em> as Jeremy Lin’s first four games.”  Every Hall of Fame – eligible baseball player with 1600 RBI and 2800 hits is in the Hall, except Harold Baines and Rafael Palmeiro.  But that shouldn’t make you think Baines deserves to be in, because I chose my criteria precisely to match what is impressive about Harold Baines.</p>
<p>Then, too:  Michael Jordan, LeBron James, and Isaiah Thomas were ranked as elite players before they ever set foot on a professional court.  Jeremy Lin had a strong but not dominant college career against Ivy League competition, and has been let go by several NBA teams that have watched him play.  I am as happy as anybody to see a Harvard player succeed in the bigs, but surely it’s reasonable to start with a pretty down-weighted prior.</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/quomodocumque.wordpress.com/3311/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/quomodocumque.wordpress.com/3311/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/quomodocumque.wordpress.com/3311/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3311&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-14T16:44:48Z</updated>
    <published>2012-02-14T15:37:59Z</published>
    <category scheme="http://quomodocumque.wordpress.com" term="math"/>
    <category scheme="http://quomodocumque.wordpress.com" term="news"/>
    <category scheme="http://quomodocumque.wordpress.com" term="basketball"/>
    <category scheme="http://quomodocumque.wordpress.com" term="jeremy lin"/>
    <author>
      <name>JSE</name>
      <uri>http://quomodocumque.wordpress.com</uri>
    </author>
    <source>
      <id>http://quomodocumque.wordpress.com/feed/atom/</id>
      <link href="http://quomodocumque.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://quomodocumque.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://quomodocumque.wordpress.com/osd.xml" rel="search" title="Quomodocumque" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://quomodocumque.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Math, Madison, food, the Orioles, books, my kids.</subtitle>
      <title xml:lang="en">Quomodocumque</title>
      <updated>2012-02-15T00:49:06Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://terrytao.wordpress.com/?p=5748</id>
    <link href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/" rel="alternate" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#comments" rel="replies" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">254B, Notes 6: Non-concentration in subgroups</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">In the last three notes, we discussed the Bourgain-Gamburd expansion machine and two of its three ingredients, namely quasirandomness and product theorems, leaving only the non-concentration ingredient to discuss. We can summarise the results of the last three notes, in the case of fields of prime order, as the following theorem. Theorem 1 (Non-concentration implies [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5748&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>
 In the <a href="http://terrytao.wordpress.com/2011/12/16/254b-notes-3-quasirandom-groups-expansion-and-selbergs-316-theorem/">last</a> <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">three</a> <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/">notes</a>, we discussed the Bourgain-Gamburd expansion machine and two of its three ingredients, namely quasirandomness and product theorems, leaving only the non-concentration ingredient to discuss. We can summarise the results of the last three notes, in the case of fields of prime order, as the following theorem.
</p>
<blockquote><p><b>Theorem 1 (Non-concentration implies expansion in <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/>)</b> <a name="nce"/> Let <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> be a prime, let <img alt="{d \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d \geq 1}"/>, and let <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> be a symmetric set of elements in <img alt="{G := SL_d(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3A%3D+SL_d%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G := SL_d(F_p)}"/> of cardinality <img alt="{|S|=k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CS%7C%3Dk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|S|=k}"/> not containing the identity. Write <img alt="{\mu := \frac{1}{|S|} \sum_{s\in S}\delta_s}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu+%3A%3D+%5Cfrac%7B1%7D%7B%7CS%7C%7D+%5Csum_%7Bs%5Cin+S%7D%5Cdelta_s%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu := \frac{1}{|S|} \sum_{s\in S}\delta_s}"/>, and suppose that one has the non-concentration property <a name="hag">
</a></p><p align="center"><a name="hag"><img alt="\displaystyle  \sup_{H &lt; G}\mu^{(n)}(H) &lt; |G|^{-\kappa} \ \ \ \ \ (1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7BH+%3C+G%7D%5Cmu%5E%7B%28n%29%7D%28H%29+%3C+%7CG%7C%5E%7B-%5Ckappa%7D+%5C+%5C+%5C+%5C+%5C+%281%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{H &lt; G}\mu^{(n)}(H) &lt; |G|^{-\kappa} \ \ \ \ \ (1)"/></a></p><a name="hag">
</a><p><a name="hag"/> for some <img alt="{\kappa&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa&gt;0}"/> and some even integer <img alt="{n \leq \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cleq+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \leq \Lambda \log |G|}"/>. Then <img alt="{Cay(G,S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28G%2CS%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(G,S)}"/> is a two-sided <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for some <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> depending only on <img alt="{k, d, \kappa,\Lambda}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C+d%2C+%5Ckappa%2C%5CLambda%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k, d, \kappa,\Lambda}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  From <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#hag">(1)</a> we see that <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> is not supported in any proper subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, which implies that <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> generates <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. The claim now follows from the Bourgain-Gamburd expansion machine (Theorem 2 of <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">Notes 4</a>), the product theorem (Theorem 1 of <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/">Notes 5</a>), and quasirandomness (Exercise 8 of <a href="http://terrytao.wordpress.com/2011/12/16/254b-notes-3-quasirandom-groups-expansion-and-selbergs-316-theorem/">Notes 3</a>). <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Remark 1</b>  The same argument also works if we replace <img alt="{F_p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_p}"/> by the field <img alt="{F_{p^j}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_%7Bp%5Ej%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_{p^j}}"/> of order <img alt="{p^j}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%5Ej%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p^j}"/> for some bounded <img alt="{j}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bj%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{j}"/>. However, there is a difficulty in the regime when <img alt="{j}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bj%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{j}"/> is unbounded, because the quasirandomness property becomes too weak for the Bourgain-Gamburd expansion machine to be directly applicable. On theother hand, the above type of theorem was generalised to the setting of cyclic groups <img alt="{{\bf Z}/q{\bf Z}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+Z%7D%2Fq%7B%5Cbf+Z%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf Z}/q{\bf Z}}"/> with <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> square-free <a href="http://arxiv.org/abs/1001.3664">by Varju</a>, to arbitrary <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> <a href="http://arxiv.org/abs/1006.3365">by Bourgain and Varju</a>, and to more general algebraic groups than <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/> and square-free <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> <a href="http://arxiv.org/abs/1108.4900">by Salehi Golsefidy and Varju</a>. It may be that some modification of the proof techniques in these papers may also be able to handle the field case <img alt="{F_{p^j}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_%7Bp%5Ej%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_{p^j}}"/> with unbounded <img alt="{j}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bj%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{j}"/>. </p></blockquote>
<p/>
<p>
It thus remains to construct tools that can establish the non-concentration property <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#hag">(1)</a>. The situation is particularly simple in <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>, as we have a good understanding of the subgroups of that group. Indeed, from Theorem 14 from <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/">Notes 5</a>, we obtain the following corollary to Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#nce">1</a>:
</p>
<blockquote><p><b>Corollary 2 (Non-concentration implies expansion in <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>)</b> <a name="nce2"/> Let <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> be a prime, and let <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> be a symmetric set of elements in <img alt="{G := SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3A%3D+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G := SL_2(F_p)}"/> of cardinality <img alt="{|S|=k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CS%7C%3Dk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|S|=k}"/> not containing the identity. Write <img alt="{\mu := \frac{1}{|S|} \sum_{s\in S}\delta_s}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu+%3A%3D+%5Cfrac%7B1%7D%7B%7CS%7C%7D+%5Csum_%7Bs%5Cin+S%7D%5Cdelta_s%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu := \frac{1}{|S|} \sum_{s\in S}\delta_s}"/>, and suppose that one has the non-concentration property <a name="hag-2">
</a></p><p align="center"><a name="hag-2"><img alt="\displaystyle  \sup_{B}\mu^{(n)}(B) &lt; |G|^{-\kappa} \ \ \ \ \ (2)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7BB%7D%5Cmu%5E%7B%28n%29%7D%28B%29+%3C+%7CG%7C%5E%7B-%5Ckappa%7D+%5C+%5C+%5C+%5C+%5C+%282%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{B}\mu^{(n)}(B) &lt; |G|^{-\kappa} \ \ \ \ \ (2)"/></a></p><a name="hag-2">
</a><p><a name="hag-2"/> for some <img alt="{\kappa&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa&gt;0}"/> and some even integer <img alt="{n \leq \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cleq+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \leq \Lambda \log |G|}"/>, where <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> ranges over all Borel subgroups of <img alt="{SL_2(\overline{F})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7BF%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{F})}"/>. Then, if <img alt="{|G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|}"/> is sufficiently large depending on <img alt="{k,\kappa,\Lambda}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C%5Ckappa%2C%5CLambda%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k,\kappa,\Lambda}"/>, <img alt="{Cay(G,S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28G%2CS%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(G,S)}"/> is a two-sided <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for some <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> depending only on <img alt="{k, \kappa,\Lambda}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C+%5Ckappa%2C%5CLambda%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k, \kappa,\Lambda}"/>. </p></blockquote>
<p/>
<p>
It turns out <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#hag-2">(2)</a> can be verified in many cases by exploiting the solvable nature of the Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. We give two examples of this in these notes. The first result, <a href="http://www.ams.org/mathscinet-getitem?mr=2415383">due to Bourgain and Gamburd</a> (with earlier partial results <a href="http://www.ams.org/mathscinet-getitem?mr=1900698">by Gamburd</a> and <a href="http://www.ams.org/mathscinet-getitem?mr=1645694">by Shalom</a>) generalises Selberg’s expander construction to the case when <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> generates a thin subgroup of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>:
</p>
<blockquote><p><b>Theorem 3 (Expansion in thin subgroups)</b> <a name="esp-thm"/> Let <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> be a symmetric subset of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> not containing the identity, and suppose that the group <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/> generated by <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> is not <a href="http://en.wikipedia.org/wiki/Solvable_group#Virtually_solvable_groups">virtually solvable</a>. Then as <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> ranges over all sufficiently large primes, the Cayley graphs <img alt="{Cay(SL_2(F_p), \pi_p(S))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5Cpi_p%28S%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \pi_p(S))}"/> form a two-sided expander family, where <img alt="{\pi_p: SL_2({\bf Z}) \rightarrow SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi_p%3A+SL_2%28%7B%5Cbf+Z%7D%29+%5Crightarrow+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi_p: SL_2({\bf Z}) \rightarrow SL_2(F_p)}"/> is the usual projection. </p></blockquote>
<p/>
<blockquote><p><b>Remark 2</b>  One corollary of Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a> (or of the non-concentration estimate <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#piu">(3)</a> below) is that <img alt="{\pi_p(S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi_p%28S%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi_p(S)}"/> generates <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> for all sufficiently large <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>, if <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/> is not virtually solvable. This is a special case of a much more general result, known as the <a href="http://en.wikipedia.org/wiki/Approximation_in_algebraic_groups">strong approximation theorem</a>, although this is certainly not the most direct way to prove such a theorem. Conversely, the strong approximation property is used in generalisations of this result to higher rank groups than <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 1</b>  In the converse direction, if <img alt="{\langle S\rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S\rangle}"/> is virtually solvable, show that for sufficiently large <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>, <img alt="{\pi_p(S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi_p%28S%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi_p(S)}"/> fails to generate <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>. (<em>Hint:</em> use Theorem 14 from <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/">Notes 5</a> to prevent <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> from having bounded index solvable subgroups.) </p></blockquote>
<p/>
<blockquote><p><b>Exercise 2 (Lubotzsky’s 1-2-3 problem)</b>  Let <img alt="{S := \{ \begin{pmatrix}1 &amp; \pm 3 \\ 0 &amp; 1 \end{pmatrix}, \begin{pmatrix}1 &amp; 0 \\ \pm 3 &amp; 1 \end{pmatrix}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D1+%26+%5Cpm+3+%5C%5C+0+%26+1+%5Cend%7Bpmatrix%7D%2C+%5Cbegin%7Bpmatrix%7D1+%26+0+%5C%5C+%5Cpm+3+%26+1+%5Cend%7Bpmatrix%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S := \{ \begin{pmatrix}1 &amp; \pm 3 \\ 0 &amp; 1 \end{pmatrix}, \begin{pmatrix}1 &amp; 0 \\ \pm 3 &amp; 1 \end{pmatrix}}"/>. </p>
<ul>
<li>(i) Show that <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> generates a free subgroup of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>. (<em>Hint:</em> use a ping-pong argument, as in Exercise 23 of <a href="http://terrytao.wordpress.com/2011/12/06/254b-notes-2-cayley-graphs-and-kazhdans-property-t/">Notes 2</a>.) </li>
<li>(ii) Show that if <img alt="{v, w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bv%2C+w%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{v, w}"/> are two distinct elements of the sector <img alt="{\{ (x,y) \in {\bf R}^2_+: x/2 &lt; y &lt; 2x \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+%28x%2Cy%29+%5Cin+%7B%5Cbf+R%7D%5E2_%2B%3A+x%2F2+%3C+y+%3C+2x+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ (x,y) \in {\bf R}^2_+: x/2 &lt; y &lt; 2x \}}"/>, then there os no element <img alt="{g \in \langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in \langle S \rangle}"/> for which <img alt="{gv = w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bgv+%3D+w%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gv = w}"/>. (<em>Hint:</em> this is another ping-pong argument.) Conclude that <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/> has infinite index in <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>. (Contrast this with the situation in which the <img alt="{3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{3}"/> coefficients in <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> are replaced by <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> or <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>, in which case <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/> is either all of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>, or a finite index subgroup, as demonstrated in Exercise 23 of <a href="http://terrytao.wordpress.com/2011/12/06/254b-notes-2-cayley-graphs-and-kazhdans-property-t/">Notes 2</a>). </li>
<li>(iii) Show that <img alt="{Cay(SL_2(F_p), \pi_p(S))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5Cpi_p%28S%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \pi_p(S))}"/> for sufficiently large primes <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> form a two-sided expander family.
</li>
</ul>
</blockquote>
<p/>
<blockquote><p><b>Remark 3</b>  Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a> has been generalised to arbitrary linear groups, and with <img alt="{F_p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_p}"/> replaced by <img alt="{{\bf Z}/q{\bf Z}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+Z%7D%2Fq%7B%5Cbf+Z%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf Z}/q{\bf Z}}"/> for square-free <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/>; see <a href="http://arxiv.org/abs/1108.4900">this paper of Salehi Golsefidy and Varju</a>. In this more general setting, the condition of virtual solvability must be replaced by the condition that the connected component of the Zariski closure of <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/> is <a href="http://en.wikipedia.org/wiki/Perfect_group">perfect</a>. An effective version of Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a> (with completely explicit constants) was recently obtained <a href="http://arxiv.org/abs/1201.1139">by Kowalski</a>. </p></blockquote>
<p/>
<p>
The second example concerns Cayley graphs constructed using random elements of <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>.
</p>
<blockquote><p><b>Theorem 4 (Random generators expand)</b> <a name="random-thm"/> Let <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> be a prime, and let <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/> be two elements of <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> chosen uniformly at random. Then with probability <img alt="{1-o_{p \rightarrow \infty}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1-o_%7Bp+%5Crightarrow+%5Cinfty%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1-o_{p \rightarrow \infty}(1)}"/>, <img alt="{Cay(SL_2(F_p), \{x,x^{-1},y,y^{-1}\})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5C%7Bx%2Cx%5E%7B-1%7D%2Cy%2Cy%5E%7B-1%7D%5C%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \{x,x^{-1},y,y^{-1}\})}"/> is a two-sided <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for some absolute constant <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Remark 4</b>  As with Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a>, Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#random-thm">4</a> has also been extended to a number of other groups, such as the Suzuki groups (in <a href="http://arxiv.org/abs/1005.0782">this paper of Breuillard, Green, and Tao</a>), and more generally to finite simple groups of Lie type of bounded rank (in forthcoming work of Breuillard, Green, Guralnick, and Tao). There are a number of other constructions of expanding Cayley graphs in such groups (and in other interesting groups, such as the alternating groups) beyond those discussed in these notes; see <a href="http://arxiv.org/abs/1105.2389">this recent survey of Lubotzky</a> for further discussion. It has been conjectured <a href="http://www.ams.org/mathscinet-getitem?mr=1235570">by Lubotzky and Weiss</a> that <em>any</em> pair <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/> of (say) <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> that generates the group, is a two-sided <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for an absolute constant <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>: in the case of <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>, this has been established for a density one set of primes <a href="http://www.ams.org/mathscinet-getitem?mr=2746951">by Breuillard and Gamburd</a>. </p></blockquote>
<p/>
<p align="center"><b> —  1. Expansion in thin subgroups  — </b></p>
<p>
We now prove Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a>. The first observation is that the expansion property is monotone in the group <img alt="{\langle S \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle}"/>:
</p>
<blockquote><p><b>Exercise 3</b>  Let <img alt="{S, S'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%2C+S%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S, S'}"/> be symmetric subsets of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> not containing the identity, such that <img alt="{\langle S \rangle \subset \langle S' \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+S+%5Crangle+%5Csubset+%5Clangle+S%27+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle S \rangle \subset \langle S' \rangle}"/>. Suppose that <img alt="{Cay(SL_2(F_p), \pi_p(S))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5Cpi_p%28S%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \pi_p(S))}"/> is a two-sided expander family for sufficiently large primes <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>. Show that <img alt="{Cay(SL_2(F_p), \pi_p(S'))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5Cpi_p%28S%27%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \pi_p(S'))}"/> is also a two-sided expander family. </p></blockquote>
<p/>
<p>
As a consequence, Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a> follows from the following two statments:
</p>
<blockquote><p><b>Theorem 5 (Tits alternative)</b> <a name="tits"/> Let <img alt="{\Gamma \subset SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma+%5Csubset+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma \subset SL_2({\bf Z})}"/> be a group. Then exactly one of the following statements holds: </p>
<ul>
<li>(i) <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> is virtually solvable. </li>
<li>(ii) <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> contains a copy of the free group <img alt="{F_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_2}"/> of two generators as a subgroup.
</li>
</ul>
</blockquote>
<p/>
<blockquote><p><b>Theorem 6 (Expansion in free groups)</b> <a name="expand"/> Let <img alt="{x,y \in SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy+%5Cin+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y \in SL_2({\bf Z})}"/> be generators of a free subgroup of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>. Then as <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> ranges over all sufficiently large primes, the Cayley graphs <img alt="{Cay(SL_2(F_p), \pi_p(\{x,y,x^{-1},y^{-1}\}))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28SL_2%28F_p%29%2C+%5Cpi_p%28%5C%7Bx%2Cy%2Cx%5E%7B-1%7D%2Cy%5E%7B-1%7D%5C%7D%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(SL_2(F_p), \pi_p(\{x,y,x^{-1},y^{-1}\}))}"/> form a two-sided expander family. </p></blockquote>
<p/>
<p>
Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#tits">5</a> is a special case of the famous <a href="http://en.wikipedia.org/wiki/Tits_alternative">Tits alternative</a>, which among other things allows one to replace <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> by <img alt="{GL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BGL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{GL_d(k)}"/> for any <img alt="{d \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d \geq 1}"/> and any field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> of characteristic zero (and fields of positive characteristic are also allowed, if one adds the requirement that <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> be finitely generated). We will not prove the full Tits alternative here, but instead just give an <em>ad hoc</em> proof of the special case in Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#tits">5</a> in the following exercise.
</p>
<blockquote><p><b>Exercise 4</b>  Given any matrix <img alt="{g \in SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2({\bf Z})}"/>, the singular values are <img alt="{\|g\|_{op}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Cg%5C%7C_%7Bop%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|g\|_{op}}"/> and <img alt="{\|g\|_{op}^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Cg%5C%7C_%7Bop%7D%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|g\|_{op}^{-1}}"/>, and we can apply the singular value decomposition to decompose
</p><p align="center"><img alt="\displaystyle  g = u_1(g) \|g\|_{op} v_1^*(g) + u_2(g) \|g\|_{op}^{-1} v_2(g)^*" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++g+%3D+u_1%28g%29+%5C%7Cg%5C%7C_%7Bop%7D+v_1%5E%2A%28g%29+%2B+u_2%28g%29+%5C%7Cg%5C%7C_%7Bop%7D%5E%7B-1%7D+v_2%28g%29%5E%2A&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  g = u_1(g) \|g\|_{op} v_1^*(g) + u_2(g) \|g\|_{op}^{-1} v_2(g)^*"/></p>
<p> where <img alt="{u_1(g),u_2(g)\in {\bf C}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu_1%28g%29%2Cu_2%28g%29%5Cin+%7B%5Cbf+C%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u_1(g),u_2(g)\in {\bf C}^2}"/> and <img alt="{v_1(g), v_2(g) \in {\bf C}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bv_1%28g%29%2C+v_2%28g%29+%5Cin+%7B%5Cbf+C%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{v_1(g), v_2(g) \in {\bf C}^2}"/> are orthonormal bases. (When <img alt="{\|g\|_{op}&gt;1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Cg%5C%7C_%7Bop%7D%3E1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|g\|_{op}&gt;1}"/>, these bases are uniquely determined up to phase rotation.) We let <img alt="{\tilde u_1(g) \in {\bf CP}^1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+u_1%28g%29+%5Cin+%7B%5Cbf+CP%7D%5E1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde u_1(g) \in {\bf CP}^1}"/> be the projection of <img alt="{u_1(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu_1%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u_1(g)}"/> to the projective complex plane, and similarly define <img alt="{\tilde v_2(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+v_2%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde v_2(g)}"/>.</p>
<p>
Let <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> be a subgroup of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>. Call a pair <img alt="{(u,v) \in {\bf CP}^1 \times {\bf CP}^1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28u%2Cv%29+%5Cin+%7B%5Cbf+CP%7D%5E1+%5Ctimes+%7B%5Cbf+CP%7D%5E1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(u,v) \in {\bf CP}^1 \times {\bf CP}^1}"/> a <em>limit point</em> of <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> if there exists a sequence <img alt="{g_n \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg_n+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g_n \in \Gamma}"/> with <img alt="{\|g_n\|_{op} \rightarrow \infty}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Cg_n%5C%7C_%7Bop%7D+%5Crightarrow+%5Cinfty%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|g_n\|_{op} \rightarrow \infty}"/> and <img alt="{(\tilde u_1(g_n), \tilde v_2(g_n)) \rightarrow (u,v)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Ctilde+u_1%28g_n%29%2C+%5Ctilde+v_2%28g_n%29%29+%5Crightarrow+%28u%2Cv%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\tilde u_1(g_n), \tilde v_2(g_n)) \rightarrow (u,v)}"/>. </p>
<ul>
<li>(i) Show that if <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> is infinite, then there is at least one limit point. </li>
<li>(ii) Show that if <img alt="{(u,v)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28u%2Cv%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(u,v)}"/> is a limit point, then so is <img alt="{(v,u)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28v%2Cu%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(v,u)}"/>. </li>
<li>(iii) Show that if there are two limit points <img alt="{(u,v), (u',v')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28u%2Cv%29%2C+%28u%27%2Cv%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(u,v), (u',v')}"/> with <img alt="{\{u,v\} \cap \{u',v'\} = \emptyset}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Bu%2Cv%5C%7D+%5Ccap+%5C%7Bu%27%2Cv%27%5C%7D+%3D+%5Cemptyset%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{u,v\} \cap \{u',v'\} = \emptyset}"/>, then there exist <img alt="{g,h \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%2Ch+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g,h \in \Gamma}"/> that generate a free group. (<em>Hint:</em> Choose <img alt="{(\tilde u_1(g), \tilde v_2(g))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Ctilde+u_1%28g%29%2C+%5Ctilde+v_2%28g%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\tilde u_1(g), \tilde v_2(g))}"/> close to <img alt="{(u,v)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28u%2Cv%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(u,v)}"/> and <img alt="{(\tilde u_1(h),\tilde v_2(h))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Ctilde+u_1%28h%29%2C%5Ctilde+v_2%28h%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\tilde u_1(h),\tilde v_2(h))}"/> close to <img alt="{(u',v')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28u%27%2Cv%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(u',v')}"/>, and consider the action of <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> and <img alt="{h}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h}"/> on <img alt="{{\bf CP}^1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+CP%7D%5E1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf CP}^1}"/>, and specifically on small neighbourhoods of <img alt="{u,v,u',v'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%2Cv%2Cu%27%2Cv%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u,v,u',v'}"/>, and set up a ping-pong type situation.) </li>
<li>(iv) Show that if <img alt="{g \in SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2({\bf Z})}"/> is hyperbolic (i.e. it has an eigenvalue greater than 1), with eigenvectors <img alt="{u,v}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%2Cv%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u,v}"/>, then the projectivisations <img alt="{(\tilde u,\tilde v)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Ctilde+u%2C%5Ctilde+v%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\tilde u,\tilde v)}"/> of <img alt="{u,v}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%2Cv%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u,v}"/> form a limit point. Similarly, if <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is regular parabolic (i.e. it has an eigenvalue at 1, but is not the identity) with eigenvector <img alt="{u}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u}"/>, show that <img alt="{(\tilde u,\tilde bu)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Ctilde+u%2C%5Ctilde+bu%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\tilde u,\tilde bu)}"/> is a limit point. </li>
<li>(v) Show that if <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> has no free subgroup of two generators, then all hyperbolic and regular parabolic elements of <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> have a common eigenvector. Conclude that all such elements lie in a solvable subgroup of <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/>. </li>
<li>(vi) Show that if an element <img alt="{g \in SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2({\bf Z})}"/> is neither hyperbolic nor regular parabolic, and is not a multiple of the identity, then <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is conjugate to a rotation by <img alt="{\pi/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi/2}"/> (in particular, <img alt="{g^2=-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E2%3D-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^2=-1}"/>). </li>
<li>(vii) Establish Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#tits">5</a>. (<em>Hint:</em> show that two square roots of <img alt="{-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-1}"/> in <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> cannot multiply to another square root of <img alt="{-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-1}"/>.)
</li>
</ul>
</blockquote>
<p/>
<p>
Now we prove Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#expand">6</a>. Let <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> be a free subgroup of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> generated by two generators <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/>. Let <img alt="{\mu := \frac{1}{4} (\delta_x +\delta_{x^{-1}} + \delta_y + \delta_{y^{-1}})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu+%3A%3D+%5Cfrac%7B1%7D%7B4%7D+%28%5Cdelta_x+%2B%5Cdelta_%7Bx%5E%7B-1%7D%7D+%2B+%5Cdelta_y+%2B+%5Cdelta_%7By%5E%7B-1%7D%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu := \frac{1}{4} (\delta_x +\delta_{x^{-1}} + \delta_y + \delta_{y^{-1}})}"/> be the probability measure generating a random walk on <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>, thus <img alt="{(\pi_p)_* \mu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Cpi_p%29_%2A+%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\pi_p)_* \mu}"/> is the corresponding generator on <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>. By Corollary <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#nce2">2</a>, it thus suffices to show that <a name="piu">
</a></p><p align="center"><a name="piu"><img alt="\displaystyle  \sup_{B}((\pi_p)_* \mu)^{(n)}(B) &lt; p^{-\kappa} \ \ \ \ \ (3)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7BB%7D%28%28%5Cpi_p%29_%2A+%5Cmu%29%5E%7B%28n%29%7D%28B%29+%3C+p%5E%7B-%5Ckappa%7D+%5C+%5C+%5C+%5C+%5C+%283%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{B}((\pi_p)_* \mu)^{(n)}(B) &lt; p^{-\kappa} \ \ \ \ \ (3)"/></a></p><a name="piu">
</a><p><a name="piu"/> for all sufficiently large <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>, some absolute constant <img alt="{\kappa&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa&gt;0}"/>, and some even <img alt="{n = O(\log p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+O%28%5Clog+p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = O(\log p)}"/> (depending on <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>, of course), where <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> ranges over Borel subgroups.
</p>
<p>
As <img alt="{\pi_p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi_p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi_p}"/> is a homomorphism, one has <img alt="{((\pi_p)_* \mu)^{(n)}(B) = (\pi_p)_* (\mu^{(n)})(B) = \mu^{(n)}(\pi_p^{-1}(B))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%28%5Cpi_p%29_%2A+%5Cmu%29%5E%7B%28n%29%7D%28B%29+%3D+%28%5Cpi_p%29_%2A+%28%5Cmu%5E%7B%28n%29%7D%29%28B%29+%3D+%5Cmu%5E%7B%28n%29%7D%28%5Cpi_p%5E%7B-1%7D%28B%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{((\pi_p)_* \mu)^{(n)}(B) = (\pi_p)_* (\mu^{(n)})(B) = \mu^{(n)}(\pi_p^{-1}(B))}"/> and so it suffices to show that </p>
<p align="center"><img alt="\displaystyle  \sup_{B} \mu^{(n)}(\pi_p^{-1}(B)) &lt; p^{-\kappa}. " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7BB%7D+%5Cmu%5E%7B%28n%29%7D%28%5Cpi_p%5E%7B-1%7D%28B%29%29+%3C+p%5E%7B-%5Ckappa%7D.+&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{B} \mu^{(n)}(\pi_p^{-1}(B)) &lt; p^{-\kappa}. "/></p>
<p> To deal with the supremum here, we will use an argument <a href="http://www.ams.org/mathscinet-getitem?mr=2415383">of Bourgain and Gamburd</a>, taking advantage of the fact that all Borel groups of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/> obey a common group law, the point being that free groups such as <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> obey such laws only very rarely. More precisely, we use the fact that the Borel groups are solvable of derived length two; in particular we have <a name="abed">
</a></p><p align="center"><a name="abed"><img alt="\displaystyle  [[a,b],[c,d]] = 1 \ \ \ \ \ (4)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5B%5Ba%2Cb%5D%2C%5Bc%2Cd%5D%5D+%3D+1+%5C+%5C+%5C+%5C+%5C+%284%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  [[a,b],[c,d]] = 1 \ \ \ \ \ (4)"/></a></p><a name="abed">
</a><p><a name="abed"/> for all <img alt="{a,b,c,d \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d \in B}"/>. Now, <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> is supported on matrices in <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> whose coefficients have size <img alt="{O(\exp(O(n)))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%5Cexp%28O%28n%29%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(\exp(O(n)))}"/> (where we allow the implied constants to depend on the choice of generators <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/>), and so <img alt="{(\pi_p)_*( \mu^{(n)} )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28%5Cpi_p%29_%2A%28+%5Cmu%5E%7B%28n%29%7D+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(\pi_p)_*( \mu^{(n)} )}"/> is supported on matrices in <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> whose coefficients also have size <img alt="{O(\exp(O(n)))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%5Cexp%28O%28n%29%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(\exp(O(n)))}"/>. If <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> is less than a sufficiently small multiple of <img alt="{\log p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clog+p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\log p}"/>, these coefficients are then less than <img alt="{p^{1/10}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%5E%7B1%2F10%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p^{1/10}}"/> (say). As such, if <img alt="{\tilde a,\tilde b,\tilde c,\tilde d \in SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+a%2C%5Ctilde+b%2C%5Ctilde+c%2C%5Ctilde+d+%5Cin+SL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde a,\tilde b,\tilde c,\tilde d \in SL_2({\bf Z})}"/> lie in the support of <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> and their projections <img alt="{a = \pi_p(\tilde a), \ldots, d = \pi_p(\tilde d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%3D+%5Cpi_p%28%5Ctilde+a%29%2C+%5Cldots%2C+d+%3D+%5Cpi_p%28%5Ctilde+d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a = \pi_p(\tilde a), \ldots, d = \pi_p(\tilde d)}"/> obey the word law <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> in <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>, then the original matrices <img alt="{\tilde a, \tilde b, \tilde c, \tilde d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+a%2C+%5Ctilde+b%2C+%5Ctilde+c%2C+%5Ctilde+d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde a, \tilde b, \tilde c, \tilde d}"/> obey the word law <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> in <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/>. (This lifting of identities from the characteristic <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> setting of <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> to the characteristic <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/> setting of <img alt="{SL_2({\bf Z})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+Z%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf Z})}"/> is a simple example of the “Lefschetz principle”.)</p>
<p>
To summarise, if we let <img alt="{E_{n,p,B}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE_%7Bn%2Cp%2CB%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E_{n,p,B}}"/> be the set of all elements of <img alt="{\pi_p^{-1}(B)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpi_p%5E%7B-1%7D%28B%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pi_p^{-1}(B)}"/> that lie in the support of <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/>, then <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> holds for all <img alt="{a,b,c,d \in E_{n,p,B}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd+%5Cin+E_%7Bn%2Cp%2CB%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d \in E_{n,p,B}}"/>. This severely limits the size of <img alt="{E_{n,p,B}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE_%7Bn%2Cp%2CB%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E_{n,p,B}}"/> to only be of polynomial size, rather than exponential size:
</p>
<blockquote><p><b>Proposition 7</b> <a name="snipe"/> Let <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> be a subset of the support of <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> (thus, <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> consists of words in <img alt="{x,y,x^{-1},y^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%2Cx%5E%7B-1%7D%2Cy%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y,x^{-1},y^{-1}}"/> of length <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>) such that the law <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> holds for all <img alt="{a,b,c,d \in E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd+%5Cin+E%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d \in E}"/>. Then <img alt="{|E| \ll n^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cll+n%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \ll n^2}"/>. </p></blockquote>
<p/>
<p>
The proof of this proposition is laid out in the exercise below.
</p>
<blockquote><p><b>Exercise 5</b>  Let <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> be a free group generated by two generators <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/>. Let <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> be the set of all words of length at most <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> in <img alt="{x,y,x^{-1},y^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%2Cx%5E%7B-1%7D%2Cy%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y,x^{-1},y^{-1}}"/>. </p>
<ul>
<li>(i) Show that if <img alt="{a,b \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b \in \Gamma}"/> commute, then <img alt="{a, b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2C+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a, b}"/> lie in the same cyclic group, thus <img alt="{a = c^i, b = c^j}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%3D+c%5Ei%2C+b+%3D+c%5Ej%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a = c^i, b = c^j}"/> for some <img alt="{c \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c \in \Gamma}"/> and <img alt="{i,j \in {\bf Z}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bi%2Cj+%5Cin+%7B%5Cbf+Z%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{i,j \in {\bf Z}}"/>. </li>
<li>(ii) Show that if <img alt="{a \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in \Gamma}"/>, there are at most <img alt="{O(n)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28n%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(n)}"/> elements of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> that commute with <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/>. </li>
<li>(iii) Show that if <img alt="{a,c \in \Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cc+%5Cin+%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,c \in \Gamma}"/>, there are at most <img alt="{O(n)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28n%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(n)}"/> elements <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> with <img alt="{[a,b] = c}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ba%2Cb%5D+%3D+c%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{[a,b] = c}"/>. </li>
<li>(iv) Prove Proposition <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#snipe">7</a>.
</li>
</ul>
</blockquote>
<p/>
<p>
Now we can conclude the proof of Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a>:
</p>
<blockquote><p><b>Exercise 6</b> <a name="lase"/> Let <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> be a free group generated by two generators <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/>. </p>
<ul>
<li>(i) Show that <img alt="{\| \mu^{(n)} \|_{\ell^\infty(\Gamma)} \ll c^n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E%5Cinfty%28%5CGamma%29%7D+%5Cll+c%5En%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\| \mu^{(n)} \|_{\ell^\infty(\Gamma)} \ll c^n}"/> for some absolute constant <img alt="{0 &lt; c&lt;1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%3C+c%3C1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 &lt; c&lt;1}"/>. (For much more precise information on <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/>, see <a href="http://www.ams.org/mathscinet-getitem?mr=109367">this paper of Kesten</a>.) </li>
<li>(ii) Conclude the proof of Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#esp-thm">3</a>.
</li>
</ul>
</blockquote>
<p/>
<p align="center"><b> —  2. Random generators expand  — </b></p>
<p>
We now prove Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#random-thm">4</a>. Let <img alt="{{\bf F}_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+F%7D_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf F}_2}"/> be the free group on two formal generators <img alt="{a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b}"/>, and let <img alt="{\mu := \frac{1}{4}(\delta_a + \delta_b + \delta_{a^{-1}}+ \delta_{b^{-1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu+%3A%3D+%5Cfrac%7B1%7D%7B4%7D%28%5Cdelta_a+%2B+%5Cdelta_b+%2B+%5Cdelta_%7Ba%5E%7B-1%7D%7D%2B+%5Cdelta_%7Bb%5E%7B-1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu := \frac{1}{4}(\delta_a + \delta_b + \delta_{a^{-1}}+ \delta_{b^{-1}}}"/> be the generator of the random walk. For any word <img alt="{w \in {\bf F}_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw+%5Cin+%7B%5Cbf+F%7D_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w \in {\bf F}_2}"/> and any <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/> in a group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, let <img alt="{w(x,y) \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y) \in G}"/> be the element of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> formed by substituting <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/> for <img alt="{a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b}"/> respectively in the word <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/>; thus <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> can be viewed as a map <img alt="{w: G \times G \rightarrow G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%3A+G+%5Ctimes+G+%5Crightarrow+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w: G \times G \rightarrow G}"/> for any group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. Observe that if <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> is drawn randomly using the distribution <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/>, and <img alt="{x,y \in SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy+%5Cin+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y \in SL_2(F_p)}"/>, then <img alt="{w(x,y)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y)}"/> is distributed according to the law <img alt="{\tilde \mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde \mu^{(n)}}"/>, where <img alt="{\tilde \mu := \frac{1}{4}(\delta_x + \delta_y + \delta_{x^{-1}}+ \delta_{y^{-1}})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctilde+%5Cmu+%3A%3D+%5Cfrac%7B1%7D%7B4%7D%28%5Cdelta_x+%2B+%5Cdelta_y+%2B+%5Cdelta_%7Bx%5E%7B-1%7D%7D%2B+%5Cdelta_%7By%5E%7B-1%7D%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\tilde \mu := \frac{1}{4}(\delta_x + \delta_y + \delta_{x^{-1}}+ \delta_{y^{-1}})}"/>. Applying Corollary <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#nce2">2</a>, it suffices to show that whenever <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> is a large prime and <img alt="{x,y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y}"/> are chosen uniformly and independently at random from <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/>, that with probability <img alt="{1-o_{p \rightarrow \infty}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1-o_%7Bp+%5Crightarrow+%5Cinfty%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1-o_{p \rightarrow \infty}(1)}"/>, one has <a name="www">
</a></p><p align="center"><a name="www"><img alt="\displaystyle  \sup_B {\bf P}_w ( w(x,y) \in B ) \leq p^{-\kappa} \ \ \ \ \ (5)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_B+%7B%5Cbf+P%7D_w+%28+w%28x%2Cy%29+%5Cin+B+%29+%5Cleq+p%5E%7B-%5Ckappa%7D+%5C+%5C+%5C+%5C+%5C+%285%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_B {\bf P}_w ( w(x,y) \in B ) \leq p^{-\kappa} \ \ \ \ \ (5)"/></a></p><a name="www">
</a><p><a name="www"/> for some absolute constant <img alt="{\kappa}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa}"/>, where <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> ranges over all Borel subgroups of <img alt="{SL_2(\overline{F_p})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7BF_p%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{F_p})}"/> and <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> is drawn from the law <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> for some even natural number <img alt="{n = O(\log p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+O%28%5Clog+p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = O(\log p)}"/>.
</p>
<p>
Let <img alt="{B_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B_n}"/> denote the words in <img alt="{{\bf F}_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+F%7D_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf F}_2}"/> of length at most <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>. We may use the law <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> to obtain good bound on the supremum in <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#www">(5)</a> assuming a certain non-degeneracy property of the word evaluations <img alt="{w(x,y)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y)}"/>:
</p>
<blockquote><p><b>Exercise 7</b>  Let <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> be a natural number, and suppose that <img alt="{x,y \in SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy+%5Cin+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y \in SL_2(F_p)}"/> is such that <img alt="{w(x,y) \neq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29+%5Cneq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y) \neq 1}"/> for <img alt="{w \in B_{100n} \backslash \{1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw+%5Cin+B_%7B100n%7D+%5Cbackslash+%5C%7B1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w \in B_{100n} \backslash \{1\}}"/>. Show that
</p><p align="center"><img alt="\displaystyle  \sup_B {\bf P}_w ( w(x,y) \in B ) \ll \exp(-cn)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_B+%7B%5Cbf+P%7D_w+%28+w%28x%2Cy%29+%5Cin+B+%29+%5Cll+%5Cexp%28-cn%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_B {\bf P}_w ( w(x,y) \in B ) \ll \exp(-cn)"/></p>
<p> for some absolute constant <img alt="{c&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c&gt;0}"/>, where <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> is drawn from the law <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/>. (<em>Hint:</em> use <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> and the hypothesis to lift the problem up to <img alt="{{\bf F}_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+F%7D_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf F}_2}"/>, at which point one can use Proposition <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#snipe">7</a> and Exercise <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#lase">6</a>.) </p></blockquote>
<p/>
<p>
In view of this exercise, it suffices to show that with probability <img alt="{1-o_{p \rightarrow\infty}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1-o_%7Bp+%5Crightarrow%5Cinfty%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1-o_{p \rightarrow\infty}(1)}"/>, one has <img alt="{w(x,y) \neq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29+%5Cneq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y) \neq 1}"/> for all <img alt="{w \in B_{100n} \backslash \{1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw+%5Cin+B_%7B100n%7D+%5Cbackslash+%5C%7B1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w \in B_{100n} \backslash \{1\}}"/> for some <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> comparable to a small multiple of <img alt="{\log p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clog+p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\log p}"/>. As <img alt="{B_{100n}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB_%7B100n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B_{100n}}"/> has <img alt="{\exp(O(n))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cexp%28O%28n%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\exp(O(n))}"/> elements, it thus suffices by the union bound to show that <a name="xyp">
</a></p><p align="center"><a name="xyp"><img alt="\displaystyle  {\bf P}_{x,y}(w(x,y)=1) \leq p^{-\gamma} \ \ \ \ \ (6)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7B%5Cbf+P%7D_%7Bx%2Cy%7D%28w%28x%2Cy%29%3D1%29+%5Cleq+p%5E%7B-%5Cgamma%7D+%5C+%5C+%5C+%5C+%5C+%286%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  {\bf P}_{x,y}(w(x,y)=1) \leq p^{-\gamma} \ \ \ \ \ (6)"/></a></p><a name="xyp">
</a><p><a name="xyp"/> for some absolute constant <img alt="{\gamma &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgamma+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gamma &gt; 0}"/>, and any <img alt="{w \in {\bf F}_2 \backslash \{1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw+%5Cin+%7B%5Cbf+F%7D_2+%5Cbackslash+%5C%7B1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w \in {\bf F}_2 \backslash \{1\}}"/> of length less than <img alt="{c\log p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%5Clog+p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c\log p}"/> for some sufficiently small absolute constant <img alt="{c&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c&gt;0}"/>.
</p>
<p>
Let us now fix a non-identity word <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> of length <img alt="{|w|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7Cw%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|w|}"/> less than <img alt="{c\log p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%5Clog+p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c\log p}"/>, and consider <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> as a function from <img alt="{SL_2(k) \times SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29+%5Ctimes+SL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k) \times SL_2(k)}"/> to <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> for an arbitrary field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>. We can identify <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> with the set <img alt="{\{ (a,b,c,d)\in k^4: ad-bc=1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+%28a%2Cb%2Cc%2Cd%29%5Cin+k%5E4%3A+ad-bc%3D1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ (a,b,c,d)\in k^4: ad-bc=1\}}"/>. A routine induction then shows that the expression <img alt="{w((a,b,c,d),(a',b',c',d'))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))}"/> is then a polynomial in the eight variables <img alt="{a,b,c,d,a',b',c',d'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd%2Ca%27%2Cb%27%2Cc%27%2Cd%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d,a',b',c',d'}"/> of degree <img alt="{O(|w|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7Cw%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|w|)}"/> and coefficients which are integers of size <img alt="{O( \exp( O(|w|) ) )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28+%5Cexp%28+O%28%7Cw%7C%29+%29+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O( \exp( O(|w|) ) )}"/>. Let us then make the additional restriction to the case <img alt="{a,a' \neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \neq 0}"/>, in which case we can write <img alt="{d = \frac{bc+1}{a}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%3D+%5Cfrac%7Bbc%2B1%7D%7Ba%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d = \frac{bc+1}{a}}"/> and <img alt="{d' =\frac{b'c'+1}{a'}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%27+%3D%5Cfrac%7Bb%27c%27%2B1%7D%7Ba%27%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d' =\frac{b'c'+1}{a'}}"/>. Then <img alt="{w((a,b,c,d),(a',b',c',d'))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))}"/> is now a rational function of <img alt="{a,b,c,a',b',c'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Ca%27%2Cb%27%2Cc%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,a',b',c'}"/> whose numerator is a polynomial of degree <img alt="{O(|w|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7Cw%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|w|)}"/> and coefficients of size <img alt="{O( \exp( O(|w|) ) )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28+%5Cexp%28+O%28%7Cw%7C%29+%29+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O( \exp( O(|w|) ) )}"/>, and the denominator is a monomial of <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/> of degree <img alt="{O(|w|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7Cw%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|w|)}"/>.
</p>
<p>
We then specialise this rational function to the field <img alt="{k=F_p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%3DF_p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k=F_p}"/>. It is conceivable that when one does so, the rational function collapses to the constant polynomial <img alt="{(1,0,0,1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%281%2C0%2C0%2C1%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(1,0,0,1)}"/>, thus <img alt="{w((a,b,c,d),(a',b',c',d'))=1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%3D1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))=1}"/> for all <img alt="{(a,b,c,d),(a',b',c',d') \in SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29+%5Cin+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b,c,d),(a',b',c',d') \in SL_2(F_p)}"/> with <img alt="{a,a' \neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \neq 0}"/>. (For instance, this would be the case if <img alt="{w(x,y) = x^{|SL_2(F_p)|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28x%2Cy%29+%3D+x%5E%7B%7CSL_2%28F_p%29%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w(x,y) = x^{|SL_2(F_p)|}}"/>, by <a href="http://en.wikipedia.org/wiki/Lagrange%27s_theorem_(group_theory)">Lagrange’s</a> theorem, if it were not for the fact that <img alt="{|w|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7Cw%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|w|}"/> is far too large here.) But suppose that this rational function does not collapse to the constant rational function. Applying the Schwarz-Zippel lemma (Exercise 23 from <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/">Notes 5</a>), we then see that the set of pairs <img alt="{(a,b,c,d),(a',b',c',d') \in SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29+%5Cin+SL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b,c,d),(a',b',c',d') \in SL_2(F_p)}"/> with <img alt="{a,a' \neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \neq 0}"/> and <img alt="{w((a,b,c,d),(a',b',c',d'))=1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%3D1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))=1}"/> is at most <img alt="{O( |w| p^5 )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28+%7Cw%7C+p%5E5+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O( |w| p^5 )}"/>; adding in the <img alt="{a=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a=0}"/> and <img alt="{a'=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'=0}"/> cases, one still obtains a bound of <img alt="{O(|w|p^5)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7Cw%7Cp%5E5%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|w|p^5)}"/>, which is acceptable since <img alt="{|SL_2(F_p)|^2 \sim p^6}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CSL_2%28F_p%29%7C%5E2+%5Csim+p%5E6%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|SL_2(F_p)|^2 \sim p^6}"/> and <img alt="{|w| = O( \log p )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7Cw%7C+%3D+O%28+%5Clog+p+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|w| = O( \log p )}"/>. Thus, the only remaining case to consider is when the rational function <img alt="{w((a,b,c,d),(a',b',c',d'))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))}"/> is identically <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> on <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> with <img alt="{a,a' \neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \neq 0}"/>.
</p>
<p>
Now we perform another “Lefschetz principle” maneuvre to change the underlying field. Recall that the denominator of rational function <img alt="{w((a,b,c,d),(a',b',c',d'))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%28%28a%2Cb%2Cc%2Cd%29%2C%28a%27%2Cb%27%2Cc%27%2Cd%27%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w((a,b,c,d),(a',b',c',d'))}"/> is monomial in <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/>, and the numerator has coefficients of size <img alt="{O(\exp(O(|w|)))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%5Cexp%28O%28%7Cw%7C%29%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(\exp(O(|w|)))}"/>. If <img alt="{|w|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7Cw%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|w|}"/> is less than <img alt="{c\log p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%5Clog+p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c\log p}"/> for a sufficiently small <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>, we conclude in particular (for <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/> large enough) that the coefficients all have magnitude less than <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>. As such, the only way that this function can be identically <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> on <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> is if it is identically <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> on <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> for all <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> with <img alt="{a,a' \neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \neq 0}"/>, and hence for <img alt="{a=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a=0}"/> or <img alt="{a'=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'=0}"/> also by taking Zariski closures.
</p>
<p>
On the other hand, we know that for some choices of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>, e.g. <img alt="{k={\bf R}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%3D%7B%5Cbf+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k={\bf R}}"/>, <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> contains a copy <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> of the free group on two generators (see e.g. Exercise 23 of <a href="http://terrytao.wordpress.com/2011/12/06/254b-notes-2-cayley-graphs-and-kazhdans-property-t/">Notes 2</a>). As such, it is not possible for any non-identity word <img alt="{w}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bw%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{w}"/> to be identically trivial on <img alt="{SL_2(k) \times SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29+%5Ctimes+SL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k) \times SL_2(k)}"/>. Thus this case cannot actually occur, completing the proof of <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#xyp">(6)</a> and hence of Theorem <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#random-thm">4</a>.
</p>
<blockquote><p><b>Remark 5</b>  We see from the above argument that the existence of subgroups <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/> of an algebraic group with good “independence” properties – such as that of generating a free group – can be useful in studying the expansion properties of that algebraic group, even if the field of interest in the latter is distinct from that of the former. For more complicated algebraic groups than <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>, in which laws such as <a href="http://terrytao.wordpress.com/2012/02/13/254b-notes-6-non-concentration-in-subgroups/#abed">(4)</a> are not always available, it turns out to be useful to place further properties on the subgroup <img alt="{\Gamma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5CGamma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\Gamma}"/>, for instance by requiring that all non-abelian subgroups of that group be Zariski dense (a property which has been called <em>strong density</em>), as this turns out to be useful for preventing random walks from concentrating in proper algebraic subgroups. See <a href="http://arxiv.org/abs/1010.4259">this paper of Breuillard, Guralnick, Green and Tao</a> for constructions of strongly dense free subgroups of algebraic groups and further discussion. </p></blockquote><p/>
<br/>Filed under: <a href="http://terrytao.wordpress.com/category/teaching/254b-expansion-in-groups/">254B - expansion in groups</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathgr/">math.GR</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathpr/">math.PR</a> Tagged: <a href="http://terrytao.wordpress.com/tag/non-concentration/">non-concentration</a>, <a href="http://terrytao.wordpress.com/tag/random-walks/">random walks</a> <a href="http://feeds.wordpress.com/1.0/gocomments/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/terrytao.wordpress.com/5748/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/terrytao.wordpress.com/5748/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/terrytao.wordpress.com/5748/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5748&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-14T16:43:11Z</updated>
    <published>2012-02-14T00:51:02Z</published>
    <category scheme="http://terrytao.wordpress.com" term="254B - expansion in groups"/>
    <category scheme="http://terrytao.wordpress.com" term="math.GR"/>
    <category scheme="http://terrytao.wordpress.com" term="math.PR"/>
    <category scheme="http://terrytao.wordpress.com" term="non-concentration"/>
    <category scheme="http://terrytao.wordpress.com" term="random walks"/>
    <author>
      <name>Terence Tao</name>
      <uri>http://www.math.ucla.edu/~tao</uri>
    </author>
    <source>
      <id>http://terrytao.wordpress.com/feed/atom/</id>
      <link href="http://terrytao.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://terrytao.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://terrytao.wordpress.com/osd.xml" rel="search" title="What&amp;#039;s new" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://terrytao.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <title xml:lang="en">What's new</title>
      <updated>2012-02-15T04:28:30Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://blogs.discovermagazine.com/cosmicvariance/?p=7971</id>
    <link href="http://feedproxy.google.com/~r/CosmicVarianceBlog/~3/bxHpFnSEQXY/" rel="alternate" type="text/html"/>
    <title>Darwinism of the Inanimate</title>
    <summary>Via Laura Hollis at the Twitter machine, here’s an interesting paper by chemist Addy Pross. The author tries to extend the idea of Darwinian natural selection to the realm of inanimate objects. Toward a general theory of evolution: Extending Darwinian theory to inanimate matter Addy Pross Though Darwinian theory dramatically revolutionized biological understanding, its strictly [...]</summary>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Via <a href="https://twitter.com/#!/LauraHollister/status/166586920531533824">Laura Hollis</a> at the Twitter machine, here’s <a href="http://www.jsystchem.com/content/2/1/1">an interesting paper</a> by chemist <a href="http://www.bgu.ac.il/~pross/">Addy Pross</a>. The author tries to extend the idea of Darwinian natural selection to the realm of inanimate objects.</p>
<blockquote><p><a href="http://www.jsystchem.com/content/2/1/1"><strong>Toward a general theory of evolution: Extending Darwinian theory to inanimate matter</strong></a><br/>
Addy Pross</p>
<p>Though Darwinian theory dramatically revolutionized biological understanding, its strictly biological focus has resulted in a widening conceptual gulf between the biological and physical sciences. In this paper we strive to extend and reformulate Darwinian theory in physicochemical terms so it can accommodate both animate and inanimate systems, thereby helping to bridge this scientific divide. The extended formulation is based on the recently proposed concept of dynamic kinetic stability and data from the newly emerging area of systems chemistry. The analysis leads us to conclude that abiogenesis and evolution, rather than manifesting two discrete stages in the emergence of complex life, actually constitute one single physicochemical process. Based on that proposed unification, the extended theory offers some additional insights into life’s unique characteristics, as well as added means for addressing the three central questions of biology: what is life, how did it emerge, and how would one make it?</p></blockquote>
<p>It’s a paper by a chemist, published in the <em>Journal of Systems Chemistry</em>, but doesn’t seem to require much in the way of specialized knowledge in order to read it, have a look.  The central idea seems to be something called “dynamic kinetic stability.” A stable system is one that doesn’t change over time; a dynamic-kinetically stable system is one that doesn’t change in some particular features, but only by taking advantage of some other kind of change. <span id="more-7971"/> The water in a river flows, but what we think of as “the river” remains fairly stable over time; an organism metabolizes, but maintains its structure for an extended period; individuals within a population come and go, while the population itself can be stable.</p>
<p>I’m very sympathetic to these kinds of ideas — they are reminiscent of <a href="http://blogs.discovermagazine.com/cosmicvariance/2010/03/09/from-eternity-to-book-club-chapter-nine/">Chapter Nine</a> of <em>From Eternity to Here</em>.  But my first impression is that the synthesis is going in the wrong direction.  Biological organisms are made of the same kind of atoms as everything else, subject to the same kind of rules, so it’s not surprising to think that their evolution should be described by a theory that also applies to inanimate objects.  But (maybe this is my physicist’s bias showing) I would tend to reserve “Darwinism” for actual biology, and instead try to develop a general theory of the evolution of complex structures and information that reduced to biological Darwinism in the appropriate circumstances.  I’m willing to be talked out of it, though.</p>
<p>Thoughts?  Especially from anyone familiar with the relevant chemistry or biology?</p>

<p><a href="http://feedads.g.doubleclick.net/~a/PI7opvZjnae1uBAu4NzH8LvkHQI/0/da"><img border="0" ismap="true" src="http://feedads.g.doubleclick.net/~a/PI7opvZjnae1uBAu4NzH8LvkHQI/0/di"/></a><br/>
<a href="http://feedads.g.doubleclick.net/~a/PI7opvZjnae1uBAu4NzH8LvkHQI/1/da"><img border="0" ismap="true" src="http://feedads.g.doubleclick.net/~a/PI7opvZjnae1uBAu4NzH8LvkHQI/1/di"/></a></p><img height="1" src="http://feeds.feedburner.com/~r/CosmicVarianceBlog/~4/bxHpFnSEQXY" width="1"/></div>
    </content>
    <updated>2012-02-14T16:41:46Z</updated>
    <category term="Science"/>
    <category term="Top Posts"/>
    <author>
      <name>Sean Carroll</name>
    </author>
    <source>
      <id>http://blogs.discovermagazine.com/cosmicvariance</id>
      <link href="http://blogs.discovermagazine.com/cosmicvariance" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/CosmicVarianceBlog" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <subtitle>Random samplings from a universe of ideas.</subtitle>
      <title>Cosmic Variance</title>
      <updated>2012-02-15T02:08:07Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.quantumdiaries.org/?p=18853</id>
    <link href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/" rel="alternate" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/#comments" rel="replies" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Why do we expect a Higgs boson? Part II: Unitarization of Vector Boson Scattering</title>
    <summary xml:lang="en">Hi everyone—it’s time that I wrap up some old posts about the Higgs boson. Last December’s tantalizing results may end up being the first signals of the real deal and the physics community is eagerly awaiting the combined results to be announce at the Rencontres de Moriond conference next month. So now would be a great [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Hi everyone—it’s time that I wrap up some old posts about the Higgs boson. Last December’s tantalizing results may end up being the first signals of the real deal and the physics community is eagerly awaiting the combined results to be announce at the <a href="http://indico.in2p3.fr/conferenceDisplay.py?confId=6001">Rencontres de Moriond</a> conference next month. So now would be a great time to remind ourselves of why we’re making such a big deal out of the Higgs.</p>
<p><span style="font-size: 20px; font-weight: bold;">Review of the story so far </span></p>
<p>Since it’s been a while since I’ve posted (sorry about that!), let’s review the main points that we’ve developed so far. See the linked posts for a reminder of the ideas behind the words and pictures.</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/wp-content/uploads/2011/12/Goldstone-Eaten-four.png"><img alt="" class="aligncenter size-full wp-image-18854" height="221" src="http://www.quantumdiaries.org/wp-content/uploads/2011/12/Goldstone-Eaten-four.png" width="318"/></a></p>
<p>There’s not only one, but <em>four</em> particles associated with the Higgs. Three of these particles <a href="http://www.quantumdiaries.org/2011/10/10/who-ate-the-higgs/">“eaten” by the <em>W</em> and <em>Z</em> bosons to become massive</a>; they form the “longitudinal polarization” of those massive particles. The fourth particle—the one we really mean when we refer to <em>The</em> Higgs boson—is responsible for <a href="http://www.quantumdiaries.org/2011/11/21/why-do-we-expect-a-higgs-boson-part-i-electroweak-symmetry-breaking/">electroweak symmetry breaking</a>. A cartoon picture would look something like this:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/wp-content/uploads/2011/12/HiggsSimplified.png"><img alt="" class="aligncenter size-full wp-image-18859" height="321" src="http://www.quantumdiaries.org/wp-content/uploads/2011/12/HiggsSimplified.png" width="500"/></a></p>
<p>The solid line is a one-dimensional version of the Higgs potential. The <em>x</em>-axis represents the Higgs ”<a href="http://www.quantumdiaries.org/2011/06/03/higgs-and-the-vacuum-viva-la-vev/">vacuum expectation value</a>,” or <em>vev</em>. For any value other than zero, this means that the Higgs field is “on” at every point in spacetime, allowing fermions to bounce off of it and hence <a href="http://www.quantumdiaries.org/2011/06/19/helicity-chirality-mass-and-the-higgs/">become massive</a>. The <em>y</em>-axis is the potential energy cost of the Higgs taking a particular vacuum value—we see that to minimize this energy, the Higgs wants to roll down to a non-zero vev.</p>
<p>Actually, because the Higgs vev can be any <em>complex</em> number, a more realistic picture is to plot the Higgs potential over the complex plane:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/wp-content/uploads/2011/12/Higgs-Potential-lookdown.png"><img alt="" class="size-full wp-image-18856 aligncenter" height="270" src="http://www.quantumdiaries.org/wp-content/uploads/2011/12/Higgs-Potential-lookdown.png" width="426"/></a></p>
<p style="text-align: center;"> </p>
<p style="text-align: left;">Now the minimum of the potential is a circle and the Higgs can pick any value. Higgs <em>particles</em> are quantum excitations—or ripples—of the Higgs field. Quantum excitations which push along this circle are called <strong>Goldstone bosons</strong>, and these represent the parts of the Higgs which are <a href="http://www.quantumdiaries.org/2011/10/10/who-ate-the-higgs/">eaten by the gauge bosons</a>. Here’s an example:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/higgs-potential-goldstone-2/" rel="attachment wp-att-18866"><img alt="" class="aligncenter size-full wp-image-18866" height="232" src="http://www.quantumdiaries.org/wp-content/uploads/2011/12/Higgs-Potential-Goldstone.png" width="365"/></a></p>
<p style="text-align: left;">Of course, in the Standard Model we know there are <em>three</em> Goldstone bosons (one each for the <em>W+</em>, <em>W-</em>, and <em>Z</em>), so there must be three “flat directions” in the Higgs potential. Unfortunately, I cannot fit this many dimensions into a 2D picture. <img alt=":-)" class="wp-smiley" src="http://www.quantumdiaries.org/wp-includes/images/smilies/icon_smile.gif"/>  The remaining Higgs particle is the excitation in the not-flat direction:</p>
<p style="text-align: center;"><img alt="" class="aligncenter" height="243" src="http://www.quantumdiaries.org/wp-content/uploads/2011/11/Higgs-Potential-radial.png" width="383"/></p>
<p style="text-align: left;">Usually all of this is said rather glibly:</p>
<blockquote>
<p style="text-align: left;">The Higgs boson is the particle which is responsible for giving mass.</p>
</blockquote>
<p style="text-align: left;"><span style="font-size: 20px; font-weight: bold;">A better reason for why we need the Higgs</span></p>
<p>The above story is nice, but you would be perfectly justified if you thought it sounded like a bit of overkill. Why do we need all of this fancy machinery with Goldstone bosons and these funny “Mexican hat” potentials? Couldn’t we have just had a theory that <em>started out</em> with massive gauge bosons without needing any of this fancy “<em>electroweak symmetry breaking</em>” footwork?</p>
<p>It turns out that <em>this </em>is the main reason why we need the Higgs-or-something-like it. It turns out that if we tried to build the Standard Model without it, then something very nefarious happens. To see what happens, we’ll appeal to some Feynman diagrams, which you may want to <a href="http://www.quantumdiaries.org/2010/02/14/lets-draw-feynman-diagams/">review</a> if you’re rusty.</p>
<p>Suppose you wanted to study the scattering of two <em>W</em> bosons off of one another. In the Standard Model you would draw the following diagrams:</p>
<p><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/unitarization/" rel="attachment wp-att-18867"><img alt="" class="aligncenter size-medium wp-image-18867" height="76" src="http://www.quantumdiaries.org/wp-content/uploads/2011/12/unitarization-300x76.png" width="300"/></a></p>
<p>There are other diagrams, but these two will be sufficient for our purposes. You can draw the rest of the diagrams for homework, there should be three more that have at most one virtual particle. In the first diagram, the two <em>W</em> bosons annihilate into a virtual <em>Z</em> boson or a photon (γ) which subsequently decay back into two <em>W</em> bosons. In the second diagram it’s the same story, only now the <em>W</em> bosons annihilate into a virtual Higgs particle.</p>
<p>Recall that these diagrams are shorthand for mathematical expressions for the probability that the <em>W</em> bosons to scatter off of one another. If you always include the sum of th<em>e </em>virtual <em>Z</em>/photon diagrams with the virtual Higgs diagram, then everything is well behaved. On the other hand, if you ignored the Higgs and <em>only</em> included the <em>Z</em>/photon diagram, then the mathematical expressions do not behave.</p>
<p>By this I mean that the probability keeps growing and growing with energy like the monsters that fight the Power Rangers. If you smash the two <em>W</em> bosons together at higher and higher energies, the number associated with this diagram gets bigger and bigger. If  these numbers get too big, then it would seem that probability isn’t conserved—we’d get probabilities larger than 100%, a mathematical inconsistency. That’s a problem that not even the Power Rangers could handle.</p>
<p>Mathematics doesn’t actually break down in this scenario—what really happens in our “no Higgs” theory is something more subtle but also disturbing: the theory becomes <strong>non-perturbative</strong> (or “strongly coupled”). In other words, the theory enters a regime where <a href="http://www.quantumdiaries.org/2010/12/11/when-feynman-diagrams-fail/">Feynman diagrams fail</a>. The simple diagram above no longer accurately represents the <em>W</em> scattering process because of large corrections from additional diagrams which are more “quantum,” i.e. they have more unobserved internal virtual particles. For example:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/wwloop/" rel="attachment wp-att-20255"><img alt="" class="aligncenter size-full wp-image-20255" height="104" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/wwloop.png" title="wwloop" width="186"/></a></p>
<p>In addition to this diagram we would also have even more involved diagrams with even more virtual particles which also give big corrections:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/wwloop2/" rel="attachment wp-att-20256"><img alt="" class="aligncenter size-full wp-image-20256" height="103" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/wwloop2.png" title="wwloop2" width="215"/></a></p>
<p>And so forth until you have more diagrams than you can calculate in a lifetime (even with a computer!). Usually these “very quantum” diagrams are negligible compared to the simpler diagrams, but in the non-perturbative regime each successive diagram is almost as important as the previous. Our <a href="http://xkcd.com/55/">usual tools fail us</a>. Our “no Higgs theory” avoids mathematical inconsistency, but at the steep cost of losing predictivity.</p>
<div style="border-style: dashed; border-width: 1px; padding: 5px; margin: 25px 50px 25px 50px;">Now let me be totally clear: there’s nothing “wrong” with this scenario… nature may very well have chosen this path. In fact, we know at least one example where it has: <a href="http://www.quantumdiaries.org/2010/12/11/when-feynman-diagrams-fail/">the theory of quarks and gluons (QCD) at low energies is non-perturbative</a>. But this is just telling us that the “particles” that we see at those energies aren’t quarks and gluons since they’re too tightly bound together: the relevant particles at those energies are mesons and baryons (e.g.pions and protons). Even though QCD—a theory of quarks and gluons—breaks down as a calculational tool, nature allowed us to describe physics in terms of perfectly well behaved (perturbative) “bound state” objects like mesons in an<a href="http://www.quantumdiaries.org/2011/02/17/effective-theories-dancing-with-the-quarks/"><em>effective</em> theory of QCD</a>. The old adage is true: when nature closes a door, it opens a window.</div>
<p>So if we took our “no Higgs” theory seriously, we’d be in an uncomfortable situation. The theory at high energies would become “strongly coupled” and non-perturbative just like QCD at low energies. It turns out that for <em>W</em> boson scattering, this happens at around the TeV scale, which means that we should be seeing hints of the substructure of the Standard Model electroweak gauge bosons—which we do not. (Incidentally, the signatures of such a scenario would likely involve something that behaves somewhat like the Standard Model Higgs.)</p>
<p>On the other hand, if we had the Higgs and we proposed the “electroweak symmetry breaking” story above, then this is never a problem. The probability for <em>W</em> boson scattering doesn’t grow uncontrollably and the theory remains well behaved and perturbative.</p>
<h2>Goldstone Liberation at High Energies</h2>
<p>The way that the Higgs mechanism saves us is somewhat technical and falls under the name of the <strong>Goldstone Boson Equivalence Theorem</strong>. The main point is that our massive gauge bosons—the ones which misbehave if there were no Higgs—are actually a pair of particles: a massless gauge boson and a massless Higgs/Goldstone particle which was “eaten” so that the <a href="http://www.quantumdiaries.org/2011/10/10/who-ate-the-higgs/">combined particle is massive</a>. One cute way of showing this is to show the <em>W</em> boson eating Gold[stone]fish:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/goldstonefish-2/" rel="attachment wp-att-20259"><img alt="" class="aligncenter size-full wp-image-20259" height="161" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/Goldstonefish.png" title="Goldstonefish" width="277"/></a></p>
<p>Indeed, at low energies the combined “massless <em>W</em> plus Goldstone” particle behaves just like a massive <em>W</em>. A good question right now is “low compared to what?” The answer is the Higgs vacuum expectation value (<em>vev</em>), i.e. the energy scale at which electroweak symmetry is broken.</p>
<p>However, at very high energies compared to the Higgs <em>vev</em>, we should expect these two particles to behave independently again. This is a very intuitive statement: it would be very disruptive if your cell phone rang at a “low energy” classical music concert and people would be very affected by this; they would shake their heads at you disapprovingly. However, at a “high energy” heavy metal concert, nobody would even hear your cell phone ring.</p>
<p>Thus at high energies, the “massless <em>W</em> plus Goldstone” system really behaves like two different particles. In a sense, the Goldstone is being liberated from the massive gauge boson:</p>
<p style="text-align: center;"><a href="http://www.quantumdiaries.org/2012/02/14/why-do-we-expect-a-higgs-boson-part-ii-unitarization-of-vector-boson-scattering/goldstonefishout/" rel="attachment wp-att-20260"><img alt="" class="aligncenter size-medium wp-image-20260" height="138" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/Goldstonefishout-300x173.png" title="Goldstonefishout" width="240"/></a></p>
<p>Now it turns out that the massless <em>W</em> is perfectly well behaved so that at high energies. Further, the set of all four Higgses together (the three Goldstones that were eaten and <em>the</em> Higgs) are also perfectly well behaved. However, if you separate the four Higgses, then each individual piece behaves poorly. This is fine, since the the four Higgses come as a package deal when we write our theory.</p>
<p>What electroweak symmetry breaking really does is that it mixes up these Higgses with the massless gauge bosons. Since this is just a reshuffling of the same particles into different combinations, the entire combined theory is still well behaved. This good behavior, though, hinges on the fact that even though we’ve separated the four Higgses, all four of them are still in the theory.</p>
<p><em>This</em> is why the Higgs (the one we’re looking for) is so important: the good behavior of the Standard Model depends on it. In fact, it turns out that any well behaved theory with massive gauge bosons must have come from some kind of Higgs-like mechanism. In jargon, we say that the Higgs <strong>unitarizes</strong> longitudinal gauge boson scattering.</p>
<div style="border-style: dashed; border-width: 1px; padding: 5px; margin: 25px 50px 25px 50px;"><strong>For advanced readers</strong>: What’s happening here is that the theory of a complex scalar Higgs doublet is perfectly well behaved. However, when we write the theory nonlinearly (e.g. chiral perturbation theory, nonlinear sigma model) to incorporate electroweak symmetry breaking, we say something like: <em>H(x) = (v+h(x)) exp (i π(x)/v)</em>. The <em>π’s </em>are the Goldstone bosons. If we ignore the Higgs, <em>h,</em> we’re doing gross violence to the well behaved complex scalar doublet. Further, we’re left with a non-renormalizable theory with dimensionful couplings that have powers of 1/<em>v</em> all over the place. Just by dimensional analysis, you can see that scattering cross sections for these Goldstones (i.e. the longitudinal modes of the gauge bosons) must scale like a positive power of the energy. In this sense, the problem of “unitarizing <em>W</em> boson scattering” is really the same as UV completing a non-renormalizable effective theory. [I thank Javi S. for filling in this gap in my education.]</div>
<h2>Caveat: Higgs versus Higgs-like</h2>
<p>I want to make one important caveat: all that I’ve argued here is that we need something to play the role of <em>the</em> Higgs in order to “restore” the “four well behaved Higgses.” While the Standard Model gives a simple candidate for this, there are other theories beyond the Standard Model that give alternate candidates. For example, the Higgs itself might be a “meson” formed out of some strongly coupled new physics. There are even “Higgsless” theories in which this “unitarization” occurs due to the exchange of new gauge bosons. But the point is that there needs to be <em>something </em>that plays the role of <em>the</em> Higgs in the above story.</p></div>
    </content>
    <updated>2012-02-14T16:23:31Z</updated>
    <published>2012-02-14T16:23:31Z</published>
    <category scheme="http://www.quantumdiaries.org" term="Latest Posts"/>
    <author>
      <name>Flip Tanedo</name>
      <uri>http://www.lepp.cornell.edu/~pt267/</uri>
    </author>
    <source>
      <id>http://www.quantumdiaries.org/feed/atom/</id>
      <link href="http://www.quantumdiaries.org" rel="alternate" type="text/html"/>
      <link href="http://www.quantumdiaries.org/feed/atom/" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">Thoughts on work and life from particle physicists from around the world.</subtitle>
      <title xml:lang="en">Quantum Diaries</title>
      <updated>2012-02-14T16:23:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/principles/2012/02/and_experiment_in_teaching_wri.php</id>
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/qNDZ516A0gE/and_experiment_in_teaching_wri.php" rel="alternate" type="text/html"/>
    <title>An Experiment in Teaching Writing: A Look Inside the Sausage Factory</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>As I've said a bazillion times already this term, I'm teaching a class that is about research and writing, with a big final paper due at the end of the term. Because iterative feedback is key to learning to write, they also have to turn in a complete rough draft, which I will mark up and have them revise.</p>

<p>One of the many, many problems with teaching writing is that too many students regard the writing of drafts as pointless busy-work. Others have no real concept of what a rough draft <em>is</em>-- when I've collected drafts in the past, I often get things that would barely qualify as an outline, let alone a draft. Already this term, I've had to explain severl times that when I ask for a draft of the final paper, I want a draft of the <em>whole thing</em>.</p>

<p>I think this stems partly from a misconception about the nature of expertise when it comes to writing. That is, I think a lot of students believe that once you really know what you're doing, you don't have to write in stages. Expert writers, in this view, just sit down at the computer and crank out flawless articles, fully formed. There's some truth to this at the college level-- God knows I never did more than one draft of anything in college, before my senior honors thesis. But at the professional level, it's nonsense; indeed, between college and now, I've turned into an obsessive reviser. I do multiple drafts of <em>blog posts</em>.</p>

<p>Getting students to believe this is a hard sell, though, and I've struggled to get them to take the process seriously. I'm going to try something different this week, though: giving them a look inside the sausage factory of the writing process. I'm going to let them see my rough drafts.</p>
 <a href="http://scienceblogs.com/principles/2012/02/and_experiment_in_teaching_wri.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/principles/2012/02/and_experiment_in_teaching_wri.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/qNDZ516A0gE" width="1"/></div>
    </summary>
    <updated>2012-02-14T15:21:15Z</updated>
    <category term="Course Reports"/>
    <source>
      <id>http://scienceblogs.com/principles/</id>
      <author>
        <name>Chad Orzel</name>
      </author>
      <link href="http://scienceblogs.com/principles/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Thoughts on physics, politics, and pop culture, by a physics professor at a small liberal arts college, plus occasional conversations with his dog.</subtitle>
      <title>Uncertain Principles</title>
      <updated>2012-02-14T15:45:09Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://profmattstrassler.com/?p=2616</id>
    <link href="http://profmattstrassler.com/2012/02/14/8-tev-over-7-tev/" rel="alternate" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/14/8-tev-over-7-tev/#comments" rel="replies" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/14/8-tev-over-7-tev/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">The Benefits of 8 TeV Collisions Over 7 TeV.</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">Yesterday, a commenter asked me a very good question that I realized I hadn’t yet addressed on this site.  Answering it gives us a chance to look at real data from the Large Hadron Collider [LHC], and to see what differences … <a href="http://profmattstrassler.com/2012/02/14/8-tev-over-7-tev/">Continue reading <span class="meta-nav">→</span></a><img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2616&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Yesterday, a commenter asked me a very good question that I realized I hadn’t yet addressed on this site.  Answering it gives us a chance to look at real data from the <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/introduction-to-the-large-hadron-collider/" target="_blank" title="Introduction to the&#xA0;LHC">Large Hadron Collider</a> [LHC], and to see what differences will arise the machine’s energy is <a href="http://press.web.cern.ch/press/PressReleases/Releases2012/PR01.12E.html" target="_blank">increased from 7 TeV to 8</a>.</p>
<p>The protons that are smashed together at the LHC <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/whats-a-proton-anyway/" target="_blank" title="What&#x2019;s a Proton,&#xA0;Anyway?">are made from many quarks, gluons and antiquarks</a>. The proton-proton collisions take place at a definite energy: 7 <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/some-technical-concepts/a-technical-concept-gev-and-tev/" target="_blank" title="GeV and&#xA0;TeV">TeV</a> = 7000 GeV in 2011, <a href="http://press.web.cern.ch/press/PressReleases/Releases2012/PR01.12E.html" target="_blank">8 TeV = 8000 GeV  in 2012.</a>  But what we’re mainly interested in — what can really create new physical phenomena for us to observe — are the collisions of a quark in one proton with an antiquark in the other proton, or the collision of two gluons, etc. These “mini-collisions” carry only a fraction — typically a very small fraction — of the total proton-proton collision energy. <strong><em>How high a fraction can they carry?  <strong><em>and what are the motivations for increasing the energy from 7 TeV per collision to 8 TeV?</em></strong>  </em></strong><a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/whats-a-proton-anyway/proton-collisions-vs-quarkgluonantiquark-mini-collisions/" title="Proton Collisions Vs. Quark/Gluon/Antiquark&#xA0;Mini-Collisions">Click here for the answer.</a></p>
<br/>Filed under: <a href="http://profmattstrassler.com/category/lhc-background-info/">LHC Background Info</a>, <a href="http://profmattstrassler.com/category/particle-physics/">Particle Physics</a> Tagged: <a href="http://profmattstrassler.com/tag/atlas/">atlas</a>, <a href="http://profmattstrassler.com/tag/cms/">cms</a>, <a href="http://profmattstrassler.com/tag/detectors/">detectors</a>, <a href="http://profmattstrassler.com/tag/gluons/">gluons</a>, <a href="http://profmattstrassler.com/tag/jets/">jets</a>, <a href="http://profmattstrassler.com/tag/particle-physics-2/">particle physics</a>, <a href="http://profmattstrassler.com/tag/quarks/">quarks</a> <a href="http://feeds.wordpress.com/1.0/gocomments/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/profmattstrassler.wordpress.com/2616/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/profmattstrassler.wordpress.com/2616/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/profmattstrassler.wordpress.com/2616/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2616&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-14T14:39:47Z</updated>
    <published>2012-02-14T14:41:47Z</published>
    <category scheme="http://profmattstrassler.com" term="LHC Background Info"/>
    <category scheme="http://profmattstrassler.com" term="Particle Physics"/>
    <category scheme="http://profmattstrassler.com" term="atlas"/>
    <category scheme="http://profmattstrassler.com" term="cms"/>
    <category scheme="http://profmattstrassler.com" term="detectors"/>
    <category scheme="http://profmattstrassler.com" term="gluons"/>
    <category scheme="http://profmattstrassler.com" term="jets"/>
    <category scheme="http://profmattstrassler.com" term="particle physics"/>
    <category scheme="http://profmattstrassler.com" term="quarks"/>
    <author>
      <name>Matt Strassler</name>
      <uri>http://profmattstrassler.wordpress.com</uri>
    </author>
    <source>
      <id>http://profmattstrassler.com/feed/atom/</id>
      <link href="http://profmattstrassler.com" rel="alternate" type="text/html"/>
      <link href="http://profmattstrassler.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://profmattstrassler.com/osd.xml" rel="search" title="Of Particular Significance" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://profmattstrassler.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Conversations About Science with Theoretical Physicist Matt Strassler</subtitle>
      <title xml:lang="en">Of Particular Significance</title>
      <updated>2012-02-14T23:45:40Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://johncarlosbaez.wordpress.com/?p=7944</id>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/quantropy-part-2/" rel="alternate" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/quantropy-part-2/#comments" rel="replies" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/quantropy-part-2/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Quantropy (Part 2)</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">In my first post in this series, we saw that filling in a well-known analogy between statistical mechanics and quantum mechanics requires a new concept: ‘quantropy’. To get some feeling for this concept, we should look at some examples. But to do that, we need to develop some tools to compute quantropy. That’s what we’ll [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7944&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>In my <a href="http://johncarlosbaez.wordpress.com/2011/12/22/quantropy/">first post in this series</a>, we saw that filling in a well-known analogy between statistical mechanics and quantum mechanics requires a new concept: ‘quantropy’.  To get some feeling for this concept, we should look at some examples.  But to do that, we need to develop some tools to compute quantropy.  That’s what we’ll do today.</p>
<p>All these tools will be borrowed from statistical mechanics.  So, let me remind you how to compute the entropy of a system in thermal equilibrium starting if we know the energy of every state.  Then we’ll copy this and get a formula for the quantropy of a system if we know the action of every history.</p>
<h3> Computing entropy </h3>
<p>Everything in this section is bog-standard.  In case you don’t know, that’s British slang for ‘extremely, perhaps even depressingly, familiar’.  Apparently it rains so much in England that bogs are not only standard, they’re the <i>standard</i> of what counts as standard!</p>
<p>Let <img alt="X" class="latex" src="http://s0.wp.com/latex.php?latex=X&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="X"/> be a measure space: physically, the set of states of some system.  In statistical mechanics we suppose the system occupies states with probabilities given by some probability distribution</p>
<p><img alt="p : X \to [0,\infty) " class="latex" src="http://s0.wp.com/latex.php?latex=p+%3A+X+%5Cto+%5B0%2C%5Cinfty%29+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="p : X \to [0,\infty) "/></p>
<p>where of course </p>
<p><img alt="\int_X p(x) \, dx = 1 " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cint_X+p%28x%29+%5C%2C+dx+%3D+1+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\int_X p(x) \, dx = 1 "/></p>
<p>The <b>entropy</b> of this probability distribution is</p>
<p><img alt="S = - \int_X p(x) \ln(p(x)) \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=S+%3D+-+%5Cint_X+p%28x%29+%5Cln%28p%28x%29%29+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="S = - \int_X p(x) \ln(p(x)) \, dx "/></p>
<p>There’s a nice way to compute the entropy when our system is in thermal equilibrium.  This idea makes sense when we have a function </p>
<p><img alt="H : X \to \mathbb{R} " class="latex" src="http://s0.wp.com/latex.php?latex=H+%3A+X+%5Cto+%5Cmathbb%7BR%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="H : X \to \mathbb{R} "/> </p>
<p>saying the <b>energy</b> of each state.  Our system is in <b>thermal equilibrium</b> when <img alt="p" class="latex" src="http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="p"/> maximizes entropy subject to a constraint on the expected value of energy:</p>
<p><img alt="\langle H \rangle = \int_X H(x) p(x) \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+H+%5Crangle+%3D+%5Cint_X+H%28x%29+p%28x%29+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle H \rangle = \int_X H(x) p(x) \, dx "/></p>
<p>A famous calculation shows that thermal equilibrium occurs precisely when <img alt="p" class="latex" src="http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="p"/> is the so-called <b>Gibbs state</b>:</p>
<p><img alt="\displaystyle{ p(x) = \frac{e^{-\beta H(x)}}{Z} } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+p%28x%29+%3D+%5Cfrac%7Be%5E%7B-%5Cbeta+H%28x%29%7D%7D%7BZ%7D+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ p(x) = \frac{e^{-\beta H(x)}}{Z} } "/></p>
<p>for some real number <img alt="\beta" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbeta&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\beta"/>, where <img alt="Z" class="latex" src="http://s0.wp.com/latex.php?latex=Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z"/> is a normalization factor called the <b>partition function</b>:</p>
<p><img alt="Z = \int_X e^{-\beta H(x)} \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=Z+%3D+%5Cint_X+e%5E%7B-%5Cbeta+H%28x%29%7D+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z = \int_X e^{-\beta H(x)} \, dx "/></p>
<p>The number <img alt="\beta" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbeta&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\beta"/> is called the <b>coolness</b>, since physical considerations say that</p>
<p><img alt="\displaystyle{ \beta = \frac{1}{T} } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+%5Cbeta+%3D+%5Cfrac%7B1%7D%7BT%7D+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ \beta = \frac{1}{T} } "/></p>
<p>where <img alt="T" class="latex" src="http://s0.wp.com/latex.php?latex=T&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T"/> is the <b>temperature</b> in units where Boltzmann’s constant is 1.</p>
<p>There’s a famous way to compute the entropy of the Gibbs state; I don’t know who did it first, but it’s both straightforward and tremendously useful.  We take the formula for entropy</p>
<p><img alt="S = - \int_X p(x) \ln(p(x)) \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=S+%3D+-+%5Cint_X+p%28x%29+%5Cln%28p%28x%29%29+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="S = - \int_X p(x) \ln(p(x)) \, dx "/></p>
<p>and substitute the Gibbs state</p>
<p><img alt="\displaystyle{ p(x) = \frac{e^{-\beta H(x)}}{Z} } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+p%28x%29+%3D+%5Cfrac%7Be%5E%7B-%5Cbeta+H%28x%29%7D%7D%7BZ%7D+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ p(x) = \frac{e^{-\beta H(x)}}{Z} } "/></p>
<p>getting</p>
<p><img alt="\begin{array}{ccl} S &amp;=&amp; \int_X p(x) \left( \beta H(x) - \ln Z \right)\, dx \\   \\  &amp;=&amp; \beta \, \langle H \rangle - \ln Z \end{array}  " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbegin%7Barray%7D%7Bccl%7D+S+%26%3D%26+%5Cint_X+p%28x%29+%5Cleft%28+%5Cbeta+H%28x%29+-+%5Cln+Z+%5Cright%29%5C%2C+dx+%5C%5C+++%5C%5C++%26%3D%26+%5Cbeta+%5C%2C+%5Clangle+H+%5Crangle+-+%5Cln+Z+%5Cend%7Barray%7D++&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\begin{array}{ccl} S &amp;=&amp; \int_X p(x) \left( \beta H(x) - \ln Z \right)\, dx \\   \\  &amp;=&amp; \beta \, \langle H \rangle - \ln Z \end{array}  "/></p>
<p>Reshuffling this a little bit, we obtain:</p>
<p><img alt="- T \ln Z = \langle H \rangle - T S" class="latex" src="http://s0.wp.com/latex.php?latex=-+T+%5Cln+Z+%3D+%5Clangle+H+%5Crangle+-+T+S&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="- T \ln Z = \langle H \rangle - T S"/></p>
<p>If we define the <b>free energy</b> by</p>
<p><img alt="F = - T \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+-+T+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = - T \ln Z"/></p>
<p>then we’ve shown that</p>
<p><img alt="F = \langle H \rangle - T S " class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+%5Clangle+H+%5Crangle+-+T+S+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = \langle H \rangle - T S "/></p>
<p>This justifies the term ‘free energy’: it’s the expected energy minus the energy in the form of heat, namely <img alt="T S." class="latex" src="http://s0.wp.com/latex.php?latex=T+S.&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T S."/></p>
<p>It’s nice that we can compute the free energy purely in terms of the partition function and the temperature, or equivalently the coolness <img alt="\beta" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbeta&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\beta"/>:</p>
<p><img alt="\displaystyle{ F = - \frac{1}{\beta} \ln Z }" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+F+%3D+-+%5Cfrac%7B1%7D%7B%5Cbeta%7D+%5Cln+Z+%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ F = - \frac{1}{\beta} \ln Z }"/></p>
<p>Can we also do this for the entropy?  Yes!  First we’ll do it for the expected energy:</p>
<p><img alt="\begin{array}{ccl} \langle H \rangle &amp;=&amp; \displaystyle{ \int_X H(x) p(x) \, dx } \\   \\  &amp;=&amp; \displaystyle{ \frac{1}{Z} \int_X H(x) e^{-\beta H(x)} \, dx } \\   \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{d}{d \beta} \int_X e^{-\beta H(x)} \, dx } \\ \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{dZ}{d \beta} } \\ \\  &amp;=&amp; \displaystyle{ - \frac{d}{d \beta} \ln Z } \end{array} " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbegin%7Barray%7D%7Bccl%7D+%5Clangle+H+%5Crangle+%26%3D%26+%5Cdisplaystyle%7B+%5Cint_X+H%28x%29+p%28x%29+%5C%2C+dx+%7D+%5C%5C+++%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+%5Cfrac%7B1%7D%7BZ%7D+%5Cint_X+H%28x%29+e%5E%7B-%5Cbeta+H%28x%29%7D+%5C%2C+dx+%7D+%5C%5C+++%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-%5Cfrac%7B1%7D%7BZ%7D+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cint_X+e%5E%7B-%5Cbeta+H%28x%29%7D+%5C%2C+dx+%7D+%5C%5C+%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-%5Cfrac%7B1%7D%7BZ%7D+%5Cfrac%7BdZ%7D%7Bd+%5Cbeta%7D+%7D+%5C%5C+%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cln+Z+%7D+%5Cend%7Barray%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\begin{array}{ccl} \langle H \rangle &amp;=&amp; \displaystyle{ \int_X H(x) p(x) \, dx } \\   \\  &amp;=&amp; \displaystyle{ \frac{1}{Z} \int_X H(x) e^{-\beta H(x)} \, dx } \\   \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{d}{d \beta} \int_X e^{-\beta H(x)} \, dx } \\ \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{dZ}{d \beta} } \\ \\  &amp;=&amp; \displaystyle{ - \frac{d}{d \beta} \ln Z } \end{array} "/></p>
<p>This gives</p>
<p><img alt="\begin{array}{ccl} S &amp;=&amp; \beta \, \langle H \rangle - \ln Z \\ \\ &amp;=&amp; \displaystyle{ - \beta \, \frac{d \ln Z}{d \beta} - \ln Z }\end{array} " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbegin%7Barray%7D%7Bccl%7D+S+%26%3D%26+%5Cbeta+%5C%2C+%5Clangle+H+%5Crangle+-+%5Cln+Z+%5C%5C+%5C%5C+%26%3D%26+%5Cdisplaystyle%7B+-+%5Cbeta+%5C%2C+%5Cfrac%7Bd+%5Cln+Z%7D%7Bd+%5Cbeta%7D+-+%5Cln+Z+%7D%5Cend%7Barray%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\begin{array}{ccl} S &amp;=&amp; \beta \, \langle H \rangle - \ln Z \\ \\ &amp;=&amp; \displaystyle{ - \beta \, \frac{d \ln Z}{d \beta} - \ln Z }\end{array} "/></p>
<p>So, if we know the partition function of a system in thermal equilibrium as a function of the temperature, we can work out its entropy, expected energy and free energy.  </p>
<h3> Computing quantropy </h3>
<p>Now we’ll repeat everything for quantropy!  The idea is simply to replace the energy by action and the temperature <img alt="T" class="latex" src="http://s0.wp.com/latex.php?latex=T&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T"/> by <img alt="i \hbar" class="latex" src="http://s0.wp.com/latex.php?latex=i+%5Chbar&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="i \hbar"/> where <img alt="\hbar" class="latex" src="http://s0.wp.com/latex.php?latex=%5Chbar&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\hbar"/> is Planck’s constant.  It’s harder to get the integrals to converge in interesting examples.  But we’ll worry about that next time, that when we actually do an example!  </p>
<p>It’s annoying that in physics <img alt="S" class="latex" src="http://s0.wp.com/latex.php?latex=S&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="S"/> stands for both entropy and action, since in this article we need to think about both.  People also use <img alt="H" class="latex" src="http://s0.wp.com/latex.php?latex=H&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="H"/> to stand for entropy, but that’s no better, since that letter also stands for ‘Hamiltonian’!  To avoid this let’s use <img alt="A" class="latex" src="http://s0.wp.com/latex.php?latex=A&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="A"/> to stand for action.  This letter is also used to mean ‘Helmholtz free energy’, but we’ll just have to live with that.  It would be real bummer if we failed to unify physics just because we ran out of letters.</p>
<p>Let <img alt="X" class="latex" src="http://s0.wp.com/latex.php?latex=X&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="X"/> be a measure space: physically, the set of histories of some system.  In quantum mechanics we suppose the system carries out histories with amplitudes given by some function</p>
<p><img alt="a : X \to \mathbb{C} " class="latex" src="http://s0.wp.com/latex.php?latex=a+%3A+X+%5Cto+%5Cmathbb%7BC%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a : X \to \mathbb{C} "/></p>
<p>where perhaps surprisingly</p>
<p><img alt="\int_X a(x) \, dx = 1 " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cint_X+a%28x%29+%5C%2C+dx+%3D+1+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\int_X a(x) \, dx = 1 "/></p>
<p>The <b>quantropy</b> of this function is</p>
<p><img alt="Q = - \int_X a(x) \ln(a(x)) \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=Q+%3D+-+%5Cint_X+a%28x%29+%5Cln%28a%28x%29%29+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Q = - \int_X a(x) \ln(a(x)) \, dx "/></p>
<p>There’s a nice way to compute the entropy in Feynman’s path integral formalism.  This formalism makes sense when we have a function </p>
<p><img alt="A : X \to \mathbb{R} " class="latex" src="http://s0.wp.com/latex.php?latex=A+%3A+X+%5Cto+%5Cmathbb%7BR%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="A : X \to \mathbb{R} "/> </p>
<p>saying the <b>action</b> of each history.  Feynman proclaimed that in this case we have</p>
<p><img alt="\displaystyle{ a(x) = \frac{e^{i A(x)/\hbar}}{Z} } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+a%28x%29+%3D+%5Cfrac%7Be%5E%7Bi+A%28x%29%2F%5Chbar%7D%7D%7BZ%7D+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ a(x) = \frac{e^{i A(x)/\hbar}}{Z} } "/></p>
<p>where <img alt="\hbar" class="latex" src="http://s0.wp.com/latex.php?latex=%5Chbar&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\hbar"/> is Planck’s constant and <img alt="Z" class="latex" src="http://s0.wp.com/latex.php?latex=Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z"/> is a normalization factor called the <b>partition function</b>:</p>
<p><img alt="Z = \int_X e^{i A(x)/\hbar} \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=Z+%3D+%5Cint_X+e%5E%7Bi+A%28x%29%2F%5Chbar%7D+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z = \int_X e^{i A(x)/\hbar} \, dx "/></p>
<p>Last time I showed that we obtain Feynman’s prescription for <img alt="a" class="latex" src="http://s0.wp.com/latex.php?latex=a&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a"/> by demanding that it’s a stationary point for the <b>quantropy</b> </p>
<p><img alt="Q = - \int_X a(x) \, \ln (a(x)) \, dx" class="latex" src="http://s0.wp.com/latex.php?latex=Q+%3D+-+%5Cint_X+a%28x%29+%5C%2C+%5Cln+%28a%28x%29%29+%5C%2C+dx&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Q = - \int_X a(x) \, \ln (a(x)) \, dx"/></p>
<p>subject to a constraint on the <b>expected action</b>:</p>
<p><img alt="\langle A \rangle = \int_X A(x) a(x) \, dx " class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+A+%5Crangle+%3D+%5Cint_X+A%28x%29+a%28x%29+%5C%2C+dx+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle A \rangle = \int_X A(x) a(x) \, dx "/></p>
<p>As I mentioned <a href="http://johncarlosbaez.wordpress.com/2012/02/10/quantropy-part-2/">last time</a>, the formula for quantropy is dangerous, since we’re taking the logarithm of a complex-valued function.  There’s not really a ‘best’ logarithm for a complex number: if we have one choice we can add any multiple of <img alt="2 \pi i" class="latex" src="http://s0.wp.com/latex.php?latex=2+%5Cpi+i&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="2 \pi i"/> and get another.  So in general, to define quantropy we need to pick a choice of <img alt="\ln (a(x))" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cln+%28a%28x%29%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\ln (a(x))"/> for each point <img alt="x \in X." class="latex" src="http://s0.wp.com/latex.php?latex=x+%5Cin+X.&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="x \in X."/>  That’s a lot of ambiguity! </p>
<p>Luckily, the ambiguity is much less when we use Feynman’s prescription for <img alt="a." class="latex" src="http://s0.wp.com/latex.php?latex=a.&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a."/>  Why?  Because then <img alt="a(x)" class="latex" src="http://s0.wp.com/latex.php?latex=a%28x%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a(x)"/> is defined in terms of an exponential, and it’s easy to take the logarithm of an exponential!  So, we can declare that</p>
<p><img alt="\ln (a(x)) = \displaystyle{ \ln \left( \frac{e^{iA(x)/\hbar}}{Z}\right) } = \frac{i}{\hbar} A(x) - \ln Z  " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cln+%28a%28x%29%29+%3D+%5Cdisplaystyle%7B+%5Cln+%5Cleft%28+%5Cfrac%7Be%5E%7BiA%28x%29%2F%5Chbar%7D%7D%7BZ%7D%5Cright%29+%7D+%3D+%5Cfrac%7Bi%7D%7B%5Chbar%7D+A%28x%29+-+%5Cln+Z++&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\ln (a(x)) = \displaystyle{ \ln \left( \frac{e^{iA(x)/\hbar}}{Z}\right) } = \frac{i}{\hbar} A(x) - \ln Z  "/></p>
<p>Once we choose a logarithm for <img alt="Z" class="latex" src="http://s0.wp.com/latex.php?latex=Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z"/>, this formula will let us define <img alt="\ln (a(x))" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cln+%28a%28x%29%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\ln (a(x))"/> and thus the quantropy.</p>
<p>So let’s do this, and say the quantropy is</p>
<p><img alt="\displaystyle{ Q = \int_X a(x) \left( \frac{i}{\hbar} A(x) - \ln Z \right)\, dx } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+Q+%3D+%5Cint_X+a%28x%29+%5Cleft%28+%5Cfrac%7Bi%7D%7B%5Chbar%7D+A%28x%29+-+%5Cln+Z+%5Cright%29%5C%2C+dx+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ Q = \int_X a(x) \left( \frac{i}{\hbar} A(x) - \ln Z \right)\, dx } "/></p>
<p>We can simplify this a bit, since the integral of <img alt="a" class="latex" src="http://s0.wp.com/latex.php?latex=a&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a"/> is 1:</p>
<p><img alt="\displaystyle{ Q = \frac{i}{\hbar} \langle A \rangle - \ln Z }  " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+Q+%3D+%5Cfrac%7Bi%7D%7B%5Chbar%7D+%5Clangle+A+%5Crangle+-+%5Cln+Z+%7D++&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ Q = \frac{i}{\hbar} \langle A \rangle - \ln Z }  "/></p>
<p>Reshuffling this a little bit, we obtain:</p>
<p><img alt="- i \hbar \ln Z = \langle A \rangle - i \hbar Q" class="latex" src="http://s0.wp.com/latex.php?latex=-+i+%5Chbar+%5Cln+Z+%3D+%5Clangle+A+%5Crangle+-+i+%5Chbar+Q&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="- i \hbar \ln Z = \langle A \rangle - i \hbar Q"/></p>
<p>By analogy to free energy in statistical mechanics, let’s define the <b>free action</b> by</p>
<p><img alt="F = - i \hbar \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+-+i+%5Chbar+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = - i \hbar \ln Z"/></p>
<p>I’m using the same letter for free energy and free action, but they play exactly analogous roles, so it’s not so bad.  Indeed we now have</p>
<p><img alt="F = \langle A \rangle - i \hbar Q " class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+%5Clangle+A+%5Crangle+-+i+%5Chbar+Q+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = \langle A \rangle - i \hbar Q "/></p>
<p>which is the analogue of a formula we saw for free energy in thermodynamics.  </p>
<p>It’s nice that we can compute the free action purely in terms of the partition function and Planck’s constant. Can we also do this for the quantropy?  Yes!  </p>
<p>It’ll be convenient to introduce a parameter</p>
<p><img alt="\displaystyle{ \beta = \frac{1}{i \hbar} }" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+%5Cbeta+%3D+%5Cfrac%7B1%7D%7Bi+%5Chbar%7D+%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ \beta = \frac{1}{i \hbar} }"/></p>
<p>which is analogous to ‘coolness’.  We could call it ‘quantum coolness’, but a better name might be <b>classicality</b>, since it’s big when our system is close to classical.  Whatever we call it, the main thing is that unlike ordinary coolness, it’s imaginary!    </p>
<p>In terms of classicality, we have</p>
<p><img alt="\displaystyle{ a(x) = \frac{e^{- \beta A(x)}}{Z} } " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+a%28x%29+%3D+%5Cfrac%7Be%5E%7B-+%5Cbeta+A%28x%29%7D%7D%7BZ%7D+%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\displaystyle{ a(x) = \frac{e^{- \beta A(x)}}{Z} } "/></p>
<p>Now we can compute the expected action just as we computed the expected energy in thermodynamics:</p>
<p><img alt="\begin{array}{ccl} \langle A \rangle &amp;=&amp; \displaystyle{ \int_X A(x) a(x) \, dx } \\ \\  &amp;=&amp; \displaystyle{ \frac{1}{Z} \int_X A(x) e^{-\beta A(x)} \, dx } \\   \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{d}{d \beta} \int_X e^{-\beta A(x)} \, dx } \\ \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{dZ}{d \beta} } \\ \\  &amp;=&amp; \displaystyle{ - \frac{d}{d \beta} \ln Z } \end{array}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbegin%7Barray%7D%7Bccl%7D+%5Clangle+A+%5Crangle+%26%3D%26+%5Cdisplaystyle%7B+%5Cint_X+A%28x%29+a%28x%29+%5C%2C+dx+%7D+%5C%5C+%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+%5Cfrac%7B1%7D%7BZ%7D+%5Cint_X+A%28x%29+e%5E%7B-%5Cbeta+A%28x%29%7D+%5C%2C+dx+%7D+%5C%5C+++%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-%5Cfrac%7B1%7D%7BZ%7D+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cint_X+e%5E%7B-%5Cbeta+A%28x%29%7D+%5C%2C+dx+%7D+%5C%5C+%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-%5Cfrac%7B1%7D%7BZ%7D+%5Cfrac%7BdZ%7D%7Bd+%5Cbeta%7D+%7D+%5C%5C+%5C%5C++%26%3D%26+%5Cdisplaystyle%7B+-+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cln+Z+%7D+%5Cend%7Barray%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\begin{array}{ccl} \langle A \rangle &amp;=&amp; \displaystyle{ \int_X A(x) a(x) \, dx } \\ \\  &amp;=&amp; \displaystyle{ \frac{1}{Z} \int_X A(x) e^{-\beta A(x)} \, dx } \\   \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{d}{d \beta} \int_X e^{-\beta A(x)} \, dx } \\ \\  &amp;=&amp; \displaystyle{ -\frac{1}{Z} \frac{dZ}{d \beta} } \\ \\  &amp;=&amp; \displaystyle{ - \frac{d}{d \beta} \ln Z } \end{array}"/></p>
<p>This gives:</p>
<p><img alt="\begin{array}{ccl} Q &amp;=&amp; \beta \,\langle A \rangle - \ln Z \\ \\ &amp;=&amp; \displaystyle{ - \beta \,\frac{d \ln Z}{d \beta} - \ln Z } \end{array} " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbegin%7Barray%7D%7Bccl%7D+Q+%26%3D%26+%5Cbeta+%5C%2C%5Clangle+A+%5Crangle+-+%5Cln+Z+%5C%5C+%5C%5C+%26%3D%26+%5Cdisplaystyle%7B+-+%5Cbeta+%5C%2C%5Cfrac%7Bd+%5Cln+Z%7D%7Bd+%5Cbeta%7D+-+%5Cln+Z+%7D+%5Cend%7Barray%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\begin{array}{ccl} Q &amp;=&amp; \beta \,\langle A \rangle - \ln Z \\ \\ &amp;=&amp; \displaystyle{ - \beta \,\frac{d \ln Z}{d \beta} - \ln Z } \end{array} "/></p>
<p>So, if we can compute the partition function in the path integral approach to quantum mechanics, we can also work out the quantropy, expected action and free action!   </p>
<p>Next time I’ll use these formulas to compute quantropy in an example: the free particle.  We’ll see some strange and interesting things.</p>
<p><a name="summary"/></p><a name="summary">
<h3> Summary </h3>
</a><p><a name="summary"/></p>
<p>Here’s where our analogy stands now:</p>
<table border="1">
<tbody><tr>
<td><b>Statistical Mechanics</b></td>
<td><b>Quantum Mechanics</b></td>
</tr>
<tr>
<td>states: <img alt="x \in X" class="latex" src="http://s0.wp.com/latex.php?latex=x+%5Cin+X&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="x \in X"/></td>
<td>histories: <img alt="x \in X" class="latex" src="http://s0.wp.com/latex.php?latex=x+%5Cin+X&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="x \in X"/></td>
</tr>
<tr>
<td>probabilities: <img alt="p: X \to [0,\infty)" class="latex" src="http://s0.wp.com/latex.php?latex=p%3A+X+%5Cto+%5B0%2C%5Cinfty%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="p: X \to [0,\infty)"/></td>
<td>amplitudes: <img alt="a: X \to \mathbb{C} " class="latex" src="http://s0.wp.com/latex.php?latex=a%3A+X+%5Cto+%5Cmathbb%7BC%7D+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a: X \to \mathbb{C} "/></td>
</tr>
<tr>
<td>energy: <img alt="H: X \to \mathbb{R}" class="latex" src="http://s0.wp.com/latex.php?latex=H%3A+X+%5Cto+%5Cmathbb%7BR%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="H: X \to \mathbb{R}"/></td>
<td>action: <img alt="A: X \to \mathbb{R}" class="latex" src="http://s0.wp.com/latex.php?latex=A%3A+X+%5Cto+%5Cmathbb%7BR%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="A: X \to \mathbb{R}"/> </td>
</tr>
<tr>
<td>temperature: <img alt="T" class="latex" src="http://s0.wp.com/latex.php?latex=T&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T"/></td>
<td>Planck’s constant times <i>i</i>: <img alt="i \hbar" class="latex" src="http://s0.wp.com/latex.php?latex=i+%5Chbar&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="i \hbar"/></td>
</tr>
<tr>
<td>coolness: <img alt="\beta = 1/T" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbeta+%3D+1%2FT&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\beta = 1/T"/></td>
<td>classicality: <img alt="\beta = 1/i \hbar" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cbeta+%3D+1%2Fi+%5Chbar&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\beta = 1/i \hbar"/></td>
</tr>
<tr>
<td>partition function: <img alt="Z = \sum_{x \in X} e^{-\beta H(x)}" class="latex" src="http://s0.wp.com/latex.php?latex=Z+%3D+%5Csum_%7Bx+%5Cin+X%7D+e%5E%7B-%5Cbeta+H%28x%29%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z = \sum_{x \in X} e^{-\beta H(x)}"/></td>
<td>partition function: <img alt="Z = \sum_{x \in X} e^{-\beta A(x)}" class="latex" src="http://s0.wp.com/latex.php?latex=Z+%3D+%5Csum_%7Bx+%5Cin+X%7D+e%5E%7B-%5Cbeta+A%28x%29%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Z = \sum_{x \in X} e^{-\beta A(x)}"/></td>
</tr>
<tr>
<td>Boltzmann distribution: <img alt="p(x) = e^{-\beta H(x)}/Z" class="latex" src="http://s0.wp.com/latex.php?latex=p%28x%29+%3D+e%5E%7B-%5Cbeta+H%28x%29%7D%2FZ&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="p(x) = e^{-\beta H(x)}/Z"/></td>
<td>Feynman sum over histories: <img alt="a(x) = e^{-\beta A(x)}/Z" class="latex" src="http://s0.wp.com/latex.php?latex=a%28x%29+%3D+e%5E%7B-%5Cbeta+A%28x%29%7D%2FZ&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="a(x) = e^{-\beta A(x)}/Z"/></td>
</tr>
<tr>
<td>entropy: <img alt="S = - \sum_{x \in X} p(x) \ln(p(x))" class="latex" src="http://s0.wp.com/latex.php?latex=S+%3D+-+%5Csum_%7Bx+%5Cin+X%7D+p%28x%29+%5Cln%28p%28x%29%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="S = - \sum_{x \in X} p(x) \ln(p(x))"/></td>
<td>quantropy: <img alt="Q = - \sum_{x \in X} a(x) \ln(a(x))" class="latex" src="http://s0.wp.com/latex.php?latex=Q+%3D+-+%5Csum_%7Bx+%5Cin+X%7D+a%28x%29+%5Cln%28a%28x%29%29&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Q = - \sum_{x \in X} a(x) \ln(a(x))"/></td>
</tr>
<tr>
<td>expected energy: <img alt="\langle H \rangle = \sum_{x \in X} p(x) H(x) " class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+H+%5Crangle+%3D+%5Csum_%7Bx+%5Cin+X%7D+p%28x%29+H%28x%29+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle H \rangle = \sum_{x \in X} p(x) H(x) "/></td>
<td>expected action: <img alt="\langle A \rangle = \sum_{x \in X} a(x) A(x) " class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+A+%5Crangle+%3D+%5Csum_%7Bx+%5Cin+X%7D+a%28x%29+A%28x%29+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle A \rangle = \sum_{x \in X} a(x) A(x) "/></td>
</tr>
<tr>
<td>free energy: <img alt="F = \langle H \rangle - TS" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+%5Clangle+H+%5Crangle+-+TS&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = \langle H \rangle - TS"/></td>
<td>free action: <img alt="F = \langle A \rangle - i \hbar Q" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+%5Clangle+A+%5Crangle+-+i+%5Chbar+Q&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = \langle A \rangle - i \hbar Q"/></td>
</tr>
<tr>
<td>  <img alt="\langle H \rangle = - \frac{d}{d \beta} \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+H+%5Crangle+%3D+-+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle H \rangle = - \frac{d}{d \beta} \ln Z"/>  </td>
<td> <img alt="\langle A \rangle = - \frac{d}{d \beta} \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=%5Clangle+A+%5Crangle+%3D+-+%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="\langle A \rangle = - \frac{d}{d \beta} \ln Z"/></td>
</tr>
<tr>
<td> <img alt="F = -\frac{1}{\beta} \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+-%5Cfrac%7B1%7D%7B%5Cbeta%7D+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = -\frac{1}{\beta} \ln Z"/> </td>
<td> <img alt="F = -\frac{1}{\beta} \ln Z" class="latex" src="http://s0.wp.com/latex.php?latex=F+%3D+-%5Cfrac%7B1%7D%7B%5Cbeta%7D+%5Cln+Z&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="F = -\frac{1}{\beta} \ln Z"/>    </td>
</tr>
<tr>
<td>  <img alt="S = - \ln Z - \beta \,\frac{d}{d \beta}\ln Z " class="latex" src="http://s0.wp.com/latex.php?latex=S+%3D+-+%5Cln+Z+-+%5Cbeta+%5C%2C%5Cfrac%7Bd%7D%7Bd+%5Cbeta%7D%5Cln+Z+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="S = - \ln Z - \beta \,\frac{d}{d \beta}\ln Z "/> </td>
<td> <img alt="Q = - \ln Z - \beta \,\frac{d }{d \beta}\ln Z " class="latex" src="http://s0.wp.com/latex.php?latex=Q+%3D+-+%5Cln+Z+-+%5Cbeta+%5C%2C%5Cfrac%7Bd+%7D%7Bd+%5Cbeta%7D%5Cln+Z+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="Q = - \ln Z - \beta \,\frac{d }{d \beta}\ln Z "/>
</td>
</tr>
</tbody></table>
<p>I should also say a word about units and dimensional analysis.  There’s enormous flexibility in how we do dimensional analysis.  Amateurs often don’t realize this, because they’ve just learned one system, but experts take full advantage of this flexibility to pick a setup that’s convenient for what they’re doing.  The fewer independent units you use, the fewer dimensionful constants like the speed of light, Planck’s constant and Boltzmann’s constant you see in your formulas.  That’s often good.  But here I don’t want to set Planck’s constant equal to 1 because I’m treating it as analogous to temperature—so it’s important, and I want to <i>see</i> it.  I’m also finding dimensional analysis useful to check my formulas. </p>
<p>So, I’m using units where mass, length and time count as independent dimensions in the sense of dimensional analysis.  On the other hand, I’m not treating temperature as an independent dimension: instead, I’m setting Boltzmann’s constant to 1 and using that to translate from temperature into energy.   This is fairly common in some circles. And for me, treating temperature as an independent dimension would be analogous to treating Planck’s constant as having its own independent dimension!  I don’t feel like doing that.</p>
<p>So, here’s how the dimensional analysis works in my setup:</p>
<table border="1">
<tbody><tr>
<td><b>Statistical Mechanics</b></td>
<td><b>Quantum Mechanics</b></td>
</tr>
<tr>
<td>probabilities: dimensionless</td>
<td>amplitudes: dimensionless </td>
</tr>
<tr>
<td>energy: <img alt="ML/T^2" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T^2"/> </td>
<td>action: <img alt="ML/T" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T"/> </td>
</tr>
<tr>
<td>temperature: <img alt="ML/T^2" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T^2"/></td>
<td>Planck’s constant: <img alt="ML/T" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T"/></td>
</tr>
<tr>
<td>coolness: <img alt="T^2/ML" class="latex" src="http://s0.wp.com/latex.php?latex=T%5E2%2FML&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T^2/ML"/></td>
<td>classicality: <img alt="T/ML " class="latex" src="http://s0.wp.com/latex.php?latex=T%2FML+&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="T/ML "/></td>
</tr>
<tr>
<td>partition function: dimensionless </td>
<td>partition function: dimensionless </td>
</tr>
<tr><td>entropy: dimensionless </td>
<td>quantropy: dimensionless </td>
</tr><tr>
<td>expected energy: <img alt="ML/T^2" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T^2"/></td>
<td>expected action: <img alt="ML/T" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T"/></td>
</tr>
<tr>
<td>free energy: <img alt="ML/T^2" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T^2"/></td>
<td>free action: <img alt="ML/T" class="latex" src="http://s0.wp.com/latex.php?latex=ML%2FT&amp;bg=ffffff&amp;fg=333333&amp;s=0" title="ML/T"/></td>
</tr>
</tbody></table>
<p>I like this setup because I often think of entropy as closely allied to information, measured in bits or nats depending on whether I’m using base 2 or base <i>e</i>.  From this viewpoint, it should be dimensionless.  </p>
<p>Of course, in thermodynamics it’s common to put a factor of Boltzmann’s constant in front of the formula for entropy.  Then entropy has units of energy/temperature.  But I’m using units where Boltzmann’s constant is 1 and temperature has the same units as energy!  So for me, entropy is dimensionless.</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/johncarlosbaez.wordpress.com/7944/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/johncarlosbaez.wordpress.com/7944/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/johncarlosbaez.wordpress.com/7944/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7944&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-14T12:46:24Z</updated>
    <published>2012-02-10T15:15:32Z</published>
    <category scheme="http://johncarlosbaez.wordpress.com" term="information and entropy"/>
    <category scheme="http://johncarlosbaez.wordpress.com" term="physics"/>
    <author>
      <name>John Baez</name>
      <uri>http://math.ucr.edu/home/baez/</uri>
    </author>
    <source>
      <id>http://johncarlosbaez.wordpress.com/feed/atom/</id>
      <link href="http://johncarlosbaez.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://johncarlosbaez.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/osd.xml" rel="search" title="Azimuth" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <title xml:lang="en">Azimuth</title>
      <updated>2012-02-14T12:46:26Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://michaelnielsen.org/blog/?p=1052</id>
    <link href="http://feedproxy.google.com/~r/michaelnielsen/wmna/~3/UuriktzEedc/" rel="alternate" type="text/html"/>
    <title>How you can help the Federal Research Public Access Act (FRPAA) become law</title>
    <summary>As many of you no doubt know, the Federal Research Public Access Act; (FRPAA, pronounced fur-pa) was introduced into the US Congress a few days past.  It’s a terrific bill, which, if it passes, will have the effect of making all US Government-funded scientific research accessible to the public within 6 months of publication. Open access legislation like FRPAA [...]</summary>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>As many of you no doubt know, the <a href="http://cyber.law.harvard.edu/hoap/Notes_on_the_Federal_Research_Public_Access_Act">Federal Research Public Access Act</a>; (FRPAA, pronounced fur-pa) was introduced into the US Congress a few days past.  It’s a terrific bill, which, if it passes, will have the effect of making all US Government-funded scientific research accessible to the public within 6 months of publication.</p>
<p>Open access legislation like FRPAA doesn’t just happen in a vacuum.  The <a href="http://www.taxpayeraccess.org/">Alliance for Taxpayer Access</a> (ATA) is a Washington D.C.-based advocacy group that works to promote open access policies within the US Government.  The ATA worked with Congress (and many other organizations) to help pass the <a href="http://publicaccess.nih.gov/">NIH public access policy</a> in 2008, and have been working for the past several years with members of Congress on FRPAA.</p>
<p>In this post, I interview <a href="http://www.arl.org/sparc/about/staff/joseph.shtml">Heather Joseph</a>, the Executive Director of the <a href="http://www.arl.org/sparc/">Scholarly Publishing and Academic Resources Coalition (SPARC)</a>, which convenes the ATA, and ask her about the bill, about next steps, and about how people can help.</p>
<p><strong>Q:</strong> <em>Heather, thanks for agreeing to be interviewed! What is FRPAA, and what’s it trying to accomplish?</em></p>
<p>Thank you, Michael – I’m happy to talk about this bill!</p>
<p>In a nutshell, FRPAA is designed to make sure that the results of scientific research paid for by the public can be accessed by the public. Most people are surprised to learn that this isn’t automatically the case; they assume that if their tax dollars pay for a research study, they should be entitled to read the results.  But the reality is quite different.  Right now, if you want to access articles that report on publicly funded science, you have pay to do so, either through a subscription to a scientific journal (which can cost thousands of dollars a year), or though pay-per-view, which can easily cost upwards of $30 per article. This presents an often-unsurmountable obstacle for exactly those people who most want (or need) access – scientists, students, teachers, physicians, entrepreneurs – who too often find themselves unable to afford such fees, and end up locked out of the game.</p>
<p>Out of eleven federal agencies that fund science here in the United States, only one – the National Institutes of Health – actually has a policy that ensures that the public can freely access the results of their funded research online. FRPAA is designed to tackle this issue head on, and to make sure that the science stemming from all U.S. agencies is made freely available to anyone who wants to use. it.</p>
<p>FRPAA is a very straightforward bill – it simply says that if you receive money from a U.S. Agency to do scientific research, you agree (upfront) to make any articles reporting on the results available to the public in a freely accessible online database, no later than six months after publication in a peer-reviewed journal.</p>
<p><strong>Q:</strong> <em>What is the Alliance for Taxpayer Access (ATA)? What role did the ATA play in advocating for FRPAA?</em></p>
<p>The ATA is a coalition of groups who are working together to try and craft a positive solution to this problem.  In 2004, the library community (led by my home organization, SPARC) decided that there must be other groups who shared our frustration over the current access situation. We reached out to research organizations, patient advocacy groups, consumer organizations, publishers, student groups – anyone we could think of who shared the goal of unlocking access to taxpayer funded research.  We quickly attracted more than 80 organizations, representing millions of individuals. This created a whole new opportunity to advocate for national access policies from a much stronger position… there really <em>is</em> strength in numbers!</p>
<p>The ATA has evolved into the leading advocacy organization for taxpayer access to the results of taxpayer funded research. We knock on Congressional doors, talking with policymakers about  the current barriers  to access, and about new opportunities for scientific progress once those barriers are brought down. We are all about leveraging the public’s investment in science by making sure that anyone who is interested can easily access and build on this research. That’s how science advances, after all.</p>
<p><strong>Q:</strong> <em>In 2008, the Congress passed the NIH public access policy.  Can you tell us about that, and the ATA’s role?</em></p>
<p>Absolutely!  As I mentioned, the NIH is currently the only U.S. agency that has a policy guaranteeing the public access to the results of its funded research. The idea for the policy surfaced in 2003, when Congress expressed concern that results of the public’s nearly $30 billion annual investment in NIH research were not being made as widely accessible as they should be.  They asked the NIH Director to create a policy to address the problem, setting in motion what would become 4 long years of intense debate in the scientific community. </p>
<p>Not surprisingly, some journal publishers expressed immediate concern that any policy that provided access to research results through any other channels other than subscription-based journals would irreparably damage their businesses. Because journal publishing is big business (nearly $9 billion in annual revenues) publishers were able to use their long-established trade associations to aggressively lobby the NIH and Congress against the establishment of such a policy.</p>
<p>The scientists, librarians, patients, and others who favored the policy found themselves at a disadvantage, advocating as individual organizations without a coordinated voice. This was the main reason the ATA was established, and we quickly found ourselves at the center of the debate, helping to ensure that all stakeholders who favored the establishment of a public access policy had a way to present a united message to policymakers. Ultimately, Congress passed a landmark policy fully supported by the ATA that was enacted in 2008. </p>
<p><strong>Q:</strong> <em>Who works at the ATA?</em></p>
<p>The ATA is essentially a virtual coalition. While we’ve grown to represent over 100 organizations, the organization’s advocacy is carried out by a pretty small core group of staff (all of whom have other full time jobs!)  Besides myself, the wonderful <a href="https://twitter.com/#!/nshockey">Nick Shockey</a> and Andrea Higginbotham are responsible for the coalition’s online presence – keeping our <a href="http://www.taxpayeraccess.org/">website</a> up to date, maintaining our <a href="http://www.taxpayeraccess.org/action/FRPAA2012.shtml">Congressional Action Center</a>, and keeping our members looped in on various email lists.  We also rely on our incredibly active members to help us continually refine our messages, and look for opportunities to spread the word about our work.  People like <a href="http://www.geneticalliance.org/bio.terry">Sharon Terry</a> at the <a href="http://www.geneticalliance.org">Genetic Alliance</a>, <a href="http://www.arl.org/arl/staff/adler.shtml">Prue Adler</a> at the <a href="http://www.arl.org">Association of Research Libraries</a>, and <a href="http://community.parentprojectmd.org/profile/PatFurlong">Pat Furlong</a> at <a href="http://www.parentprojectmd.org/site/PageServer?pagename=nws_index">Parent Project Muscular Dystrophy</a> are prime examples of some of the people who keep the ATA active on the front lines. Also: there is no cost to join the ATA (SPARC picks up the relatively low tab to keep it humming!); and the door is open for any organization to <a href="http://www.taxpayeraccess.org/membership/join/index.shtml">sign on as a member through our website</a>. If you’re interested, please let us know!</p>
<p><strong>Q:</strong> <em>What happens next, with FRPAA?  How does it (hopefully) become law? What could derail it?</em></p>
<p>The next steps for FRPAA will be for us (and our advocates) to encourage other members of Congress to sign onto the bill as co-sponsors. Generating a nice, robust list of supporting members of Congress is key in helping to keep the profile of the bill high.  Procedurally, the bill will be referred to Committee for further consideration; in the Senate, it will go to the Homeland Security and Government Affairs Committee, and in the House, the Committee on Oversight and Government Reform will receive the bill.  As with any legislation, FRPAA faces an uphill battle in an election year, but given the growing attention this issue has received in the past year (from the White House Office of Science and Technology Policy, to the America COMPETES Act, to the recent Research Works Act), we’re hopeful that the bill can continue to advance.</p>
<p>I think the biggest threat is inaction, so vocal support from stakeholders will be crucial!</p>
<p><strong>Q:</strong> <em>What can people do to help FRPAA become law?</em></p>
<p>The most important thing that people – especially active scientists – can do help advance this bill is to speak out in support of this bill.  And we need folks to speak out in two ways:</p>
<p>First, speak out to your members of Congress. The ATA has an <a href="http://www.taxpayeraccess.org/action/action_frpaa/FRPAA2012.shtml">Action Center</a> set up so that you can simply log on, pick your Senators and Representatives, and automatically generate a letter asking them to support FRPAA.  The Action Center has all kinds of information about the bill, including Talking Points, FAQ’a and even template letters, to help make the process as easy as possible. <a href="http://www.taxpayeraccess.org/action/action_frpaa/FRPAA2012.shtml">Check it out!</a></p>
<p>Second, speak out to your colleagues and your community.  Blog about the bill, or spread the word on Twitter.  Consider writing an OpEd for your local newspaper, or writing an article for your organization’s newsletter. The more people become aware of this issue, the more they support it. Help us spread the word!</p>
<p><strong>Q:</strong> <em>Finally, how can people follow what the ATA is doing, and keep up with your calls for action?</em></p>
<p>You can sign onto the Alliance for Taxpayer Access by going to <a href="http://www.taxpayeraccess.org/membership/join/index.shtml">our website</a>. There’s no charge.</p>
<p>If you simply want to be added to our email list for alerts and updates, contact either or myself (heather@arl.org)  or Andrea Higginbotham (andrea@arl.org), or follow us on Twitter at <a href="https://twitter.com/#!/sparc_na">@SPARC_NA</a>.</p>
<img height="1" src="http://feeds.feedburner.com/~r/michaelnielsen/wmna/~4/UuriktzEedc" width="1"/></div>
    </content>
    <updated>2012-02-14T12:38:43Z</updated>
    <category term="Uncategorized"/>
    <author>
      <name>admin</name>
    </author>
    <source>
      <id>http://michaelnielsen.org/blog</id>
      <link href="http://michaelnielsen.org/blog" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/michaelnielsen/wmna" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <title>Michael Nielsen</title>
      <updated>2012-02-14T13:08:20Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-2846514233477399562.post-4781151250494856618</id>
    <link href="http://resonaances.blogspot.com/feeds/4781151250494856618/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=2846514233477399562&amp;postID=4781151250494856618" rel="replies" title="6 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default/4781151250494856618" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default/4781151250494856618" rel="self" type="application/atom+xml"/>
    <link href="http://resonaances.blogspot.com/2012/02/how-to-find-stop.html" rel="alternate" title="How to find a stop" type="text/html"/>
    <title>How to find a stop</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Lately there's been a surge of interest in hypothetical scalar partners of the top quark, the <span style="font-style: italic;">stops</span> in short.  So it may be a good moment to sell a few technical details to a larger audience. For theorists, a stop is easy to distinguish experimentally: it looks like a top but with a twiddle on top. However experimentalists are not as smart, and they have to invest much more time and effort in order to identify stops at the LHC.<br/><br/><a href="http://4.bp.blogspot.com/-IbTsUFJsWZs/TzklSOsAN9I/AAAAAAAAAl0/mFr1wwVNdqI/s1600/Josh_StopDecay.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708634997779347410" src="http://4.bp.blogspot.com/-IbTsUFJsWZs/TzklSOsAN9I/AAAAAAAAAl0/mFr1wwVNdqI/s320/Josh_StopDecay.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 191px; height: 164px;"/></a>What it looks like depends first of all on <span style="font-weight: bold;">how it decays</span>.  Even the minimal SUSY model offers countless possibilities.  Leaving out the case of stable stops,  in the MSSM stops ultimately decays to a number of known particles from the Standard Model  plus the lightest supersymmetric partner (LSP) who is assumed to be a very weakly interacting particle showing up as missing momentum in a detector.  Some possible decay chains are:<br/>Stop → top + LSP,   Stop → W + sbottom  → W + b + LSP,  Stop → bottom + chargino  → bottom + W + LSP, etc.<br/>The bottom line is that the MSSM stop should manifest itself at the LHC as an excess of events with:<br/><ul><li> top and/or bottom quarks,<br/></li><li>significant missing energy due to the LSP. </li></ul><a href="http://4.bp.blogspot.com/-_UQX9z7kjoE/TzkuzNucXbI/AAAAAAAAAmw/w74DEZw47L4/s1600/SUSYxsections_Prospino.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708645460061478322" src="http://4.bp.blogspot.com/-_UQX9z7kjoE/TzkuzNucXbI/AAAAAAAAAmw/w74DEZw47L4/s320/SUSYxsections_Prospino.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 278px; height: 215px;"/></a>Now, <span style="font-weight: bold;">how to produce</span> it.  Being top partners, stops carry a color charge, hence they can be produced in gluon collisions which are easy to come by at the LHC. However, on the plot you see that  production  of stop pairs is far less frequent than that of  gluinos and 1st generation squarks of similar mass.  In physics jargon, s-channel production of scalar particles is velocity suppressed as a consequence of  angular momentum conservation. This is the main reason why, as you'll see below, the LHC limits on stop pair production are so much weaker than those on gluinos. However, there is a trick to boost the stop production rate by producing them indirectly in gluino decays: gluino → stop + top, as long as the gluino is  not much heavier <a href="http://3.bp.blogspot.com/-bf-79RC7klk/Tzo1CWxBHgI/AAAAAAAAAng/Lr_h5Fta318/s1600/SUSY_stopProduction.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708933792232709634" src="http://3.bp.blogspot.com/-bf-79RC7klk/Tzo1CWxBHgI/AAAAAAAAAng/Lr_h5Fta318/s320/SUSY_stopProduction.png" style="float: left; margin: 0pt 10px 10px 0pt; cursor: pointer; width: 102px; height: 146px;"/></a>than the stops.  As a bonus, this production mode generates more junk in the detector that could be helpful in discriminating signal from background. For example, one can imagine the sequence:<br/>pp → 2 gluinos → 2 stops + 2 tops  →  4 tops + 2 LSPs<br/>which leaves us with 4 top quarks in the final state. The 4-top production rate in the  Standard Model is very small, therefore observation of such a final state at this point would be a clear sign of new physics. Another place where this sort of  cascades could show up are the searches for same-sign top quarks.<br/><br/><a href="http://1.bp.blogspot.com/-ts0aI1W5gvY/Tzkm21Rea5I/AAAAAAAAAmk/Y63ggjqOddY/s1600/ATLAS_stoplimits1fb"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708636726123981714" src="http://1.bp.blogspot.com/-ts0aI1W5gvY/Tzkm21Rea5I/AAAAAAAAAmk/Y63ggjqOddY/s320/ATLAS_stoplimits1fb" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 218px; height: 147px;"/></a>What is the <span style="font-weight: bold;">experimental situation so far</span>?   As far as I know, the LHC collaborations have not yet published any limits on <span style="font-style: italic;">direct</span> stop production.  On the other hand, <span style="font-style: italic;">gluino mediated</span> stop production was targeted in <a href="https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-130/">this note</a> based on 1 fb-1 of ATLAS data. The plot shows that gluinos  decaying in the sequence:<br/>gluino → top + stop   → 2 tops + bottom + chargino→ 2 tops + bottom + W + LSP<br/>cannot be lighter than 500 GeV. During the next 30 days leading to the Moriond conference many more searches based on larger data samples will be released, starting with the Valentine Day ATLAS <a href="http://indico.cern.ch/conferenceDisplay.py?confId=175617">talk</a>.<br/><a href="http://3.bp.blogspot.com/-ZjqQTlpZJyQ/Tzkle6bU8NI/AAAAAAAAAmA/MmXFw9_D0Jo/s1600/Josh_DirectStops.png"/><br/><a href="http://4.bp.blogspot.com/-neshacc_g3w/Tzk3xvUWLmI/AAAAAAAAAnI/DzntQToZl94/s1600/stopVhiggsino.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708655330323738210" src="http://4.bp.blogspot.com/-neshacc_g3w/Tzk3xvUWLmI/AAAAAAAAAnI/DzntQToZl94/s320/stopVhiggsino.png" style="float: right; margin: 0 0 10px 10px; cursor: pointer; cursor: hand; width: 320px; height: 160px;"/></a>For today, we can get some idea of the current LHC  sensitivity from <a href="http://arxiv.org/abs/1110.6926">this paper</a>,  which compiles a large number of SUSY searches and recasts the results in terms of limits on stops.  The LHC reach for direct stop production (right plots) is poor, corresponding to stop mass of only 200-300 GeV.  For gluino mediated stop production (plots below) the limits are much better and  extend to approximately 700 GeV gluino masses (though the precise limits  may depend on details of the SUSY spectrum; it is probably possible to design spectra for which these limits are somewhat weaker).  Amusingly, the dedicated ATLAS search does not seem to be the most sensitive probe of gluino mediated stop production. Instead, more stringent limits come from vanilla SUSY searches (decaying top quarks produce jets, b-jets,   and/or leptons that can be picked up by these searches). We'll see very soon whether the coming experimental analyses will significantly improve these limits.<br/><div style="text-align: left;"><a href="http://2.bp.blogspot.com/-pttM6mAkVR0/Tzk34ulAlOI/AAAAAAAAAnU/eLs3cVLJllA/s1600/StopGluino.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708655450384274658" src="http://2.bp.blogspot.com/-pttM6mAkVR0/Tzk34ulAlOI/AAAAAAAAAnU/eLs3cVLJllA/s320/StopGluino.png" style="display: block; margin: 0px auto 10px; text-align: center; cursor: pointer; width: 355px; height: 177px;"/></a></div>Update: see the <a href="http://indico.cern.ch/getFile.py/access?resId=0&amp;materialId=slides&amp;confId=175617">slides</a> of the Feb 14 ATLAS talk for more limits on stops.<div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/2846514233477399562-4781151250494856618?l=resonaances.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-14T10:29:26Z</updated>
    <published>2012-02-13T14:12:00Z</published>
    <author>
      <name>Jester</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/08947218566941608850</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-2846514233477399562</id>
      <category term="Distraction"/>
      <category term="April Fools"/>
      <category term="Report"/>
      <category term="Jest"/>
      <category term="News"/>
      <category term="Musing"/>
      <category term="Review"/>
      <author>
        <name>Jester</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/16844247827820646813</uri>
      </author>
      <link href="http://resonaances.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://resonaances.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>Particle Physics Blog</subtitle>
      <title>RÉSONAANCES</title>
      <updated>2012-02-15T00:42:02Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-22973357.post-8937828373640211404</id>
    <link href="http://backreaction.blogspot.com/feeds/8937828373640211404/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=22973357&amp;postID=8937828373640211404" rel="replies" title="11 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/8937828373640211404" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/8937828373640211404" rel="self" type="application/atom+xml"/>
    <link href="http://backreaction.blogspot.com/2012/02/updated-science-symbol.html" rel="alternate" title="Updated science symbol" type="text/html"/>
    <title>Updated science symbol</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Following some suggestions in the comments, I have made an updated version of the science symbol. I've added a hint of arrows to the circle and a touch of color. I think it looks much better now, more dynamic.<br/><a href="http://1.bp.blogspot.com/--8xqpKUPUIc/Tzoc1AjUnPI/AAAAAAAABJ8/JbfozSnVmRU/s1600/science.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708907174652321010" src="http://1.bp.blogspot.com/--8xqpKUPUIc/Tzoc1AjUnPI/AAAAAAAABJ8/JbfozSnVmRU/s400/science.jpg" style="display: block; margin: 0px auto 10px; text-align: center; cursor: pointer; cursor: hand; width: 370px; height: 400px;"/></a><br/>You can also have that carved in stone...<br/><br/><a href="http://1.bp.blogspot.com/-36uB6XFkifM/Tzon2YmDB7I/AAAAAAAABLc/2S63sYrytk8/s1600/science_3d.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708919292913977266" src="http://1.bp.blogspot.com/-36uB6XFkifM/Tzon2YmDB7I/AAAAAAAABLc/2S63sYrytk8/s400/science_3d.jpg" style="display: block; margin: 0px auto 10px; text-align: center; cursor: pointer; cursor: hand; width: 370px; height: 400px;"/></a><br/>Pendolski suggested to add something in the middle to represent knowledge. I was thinking that in the middle you can add a symbol to your specific profession. You might for example want to point out that you're not just a scientist, but a rocket scientist.  <br/><br/><br/><br/><br/><table border="0" width="450"><tbody><tr><td><a href="http://3.bp.blogspot.com/-HxVMTrN9dUo/Tzof4OpSvsI/AAAAAAAABKU/clGHGabyz1g/s1600/science_rocket.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708910528509951682" src="http://3.bp.blogspot.com/-HxVMTrN9dUo/Tzof4OpSvsI/AAAAAAAABKU/clGHGabyz1g/s400/science_rocket.jpg" style="float: center; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a> <a href="http://2.bp.blogspot.com/-jR_njx1EKDU/Tzofy0cqvzI/AAAAAAAABKI/yxfi9IW1XaU/s1600/science_apple.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708910435578330930" src="http://2.bp.blogspot.com/-jR_njx1EKDU/Tzofy0cqvzI/AAAAAAAABKI/yxfi9IW1XaU/s400/science_apple.jpg" style="float: left; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a></td><td><a href="http://1.bp.blogspot.com/-Kv_medI5psk/TzogV4fxaGI/AAAAAAAABLE/MwqYQP_PgPo/s1600/science_hbar.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708911037960513634" src="http://1.bp.blogspot.com/-Kv_medI5psk/TzogV4fxaGI/AAAAAAAABLE/MwqYQP_PgPo/s400/science_hbar.jpg" style="float: left; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a><a href="http://4.bp.blogspot.com/-n5kw5zuzxGs/TzogVu4BUuI/AAAAAAAABK4/Qosmxfs89T4/s1600/science_blogger.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708911035377865442" src="http://4.bp.blogspot.com/-n5kw5zuzxGs/TzogVu4BUuI/AAAAAAAABK4/Qosmxfs89T4/s400/science_blogger.jpg" style="float: left; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a></td><td><a href="http://1.bp.blogspot.com/-A5OQl60c83c/TzogVXy7Z3I/AAAAAAAABKs/dT9rAxm-6F0/s1600/science_dna.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708911029182490482" src="http://1.bp.blogspot.com/-A5OQl60c83c/TzogVXy7Z3I/AAAAAAAABKs/dT9rAxm-6F0/s400/science_dna.jpg" style="float: left; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a><a href="http://1.bp.blogspot.com/-DVEga9G2qlc/TzogHEXMUzI/AAAAAAAABKg/iD2_5nb5ihc/s1600/science_e.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5708910783447716658" src="http://1.bp.blogspot.com/-DVEga9G2qlc/TzogHEXMUzI/AAAAAAAABKg/iD2_5nb5ihc/s400/science_e.jpg" style="float: left; margin: 0 10px 10px 0; cursor: pointer; cursor: hand; width: 160px; height: 173px;"/></a></td></tr></tbody></table><br/>If you like the symbol, feel free to use it. I'm using Corel Draw, <a href="http://prime-spot.de/Bilder/science.cdr">you can download the source file here</a>. You will probably need the fonts Life BT and Book Antiqua.<div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/22973357-8937828373640211404?l=backreaction.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-14T09:36:33Z</updated>
    <published>2012-02-14T09:20:00Z</published>
    <author>
      <name>Bee</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/06151209308084588985</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-22973357</id>
      <category term="Sociology of Science"/>
      <category term="This and That"/>
      <category term="Particle Physics"/>
      <category term="Physics"/>
      <category term="Useless Knowledge"/>
      <category term="Philosophy"/>
      <category term="Photo"/>
      <category term="Distraction"/>
      <category term="Art"/>
      <category term="Quantum Gravity"/>
      <category term="Academia"/>
      <category term="Comic"/>
      <category term="Science"/>
      <category term="Peer Review"/>
      <category term="Poll"/>
      <category term="Papers"/>
      <category term="Psychology"/>
      <category term="Politics"/>
      <category term="Germany"/>
      <category term="Baby"/>
      <category term="History of Science"/>
      <category term="Travel"/>
      <category term="Infotainment"/>
      <category term="Biology"/>
      <category term="Science and Society"/>
      <category term="Interna"/>
      <category term="Physicists"/>
      <category term="Random Thoughts"/>
      <category term="Canada"/>
      <category term="Humor"/>
      <category term="Astrophysics"/>
      <category term="Video"/>
      <category term="Blog"/>
      <category term="Books"/>
      <author>
        <name>Bee</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/06151209308084588985</uri>
      </author>
      <link href="http://backreaction.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://backreaction.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <title>Backreaction</title>
      <updated>2012-02-14T21:31:23Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-10448119.post-7196289084176992414</id>
    <link href="http://hoggresearch.blogspot.com/feeds/7196289084176992414/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/gravitational-lens-modeling.html#comment-form" rel="replies" title="0 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/7196289084176992414" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/7196289084176992414" rel="self" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/gravitational-lens-modeling.html" rel="alternate" title="gravitational lens modeling" type="text/html"/>
    <title>gravitational lens modeling</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Despite all my intentions to stop working on strong gravitational lensing, I keep getting accidentally pulled back, with interesting projects from Marshall and new discoveries from Tsalmantza.  Today I pitched some strong lensing modeling projects to NYU graduate student Cato Sandford.  The idea is to simultaneously model multi-epoch multi-band imaging (with variable PSF) with a time-varying multiply imaged quasar and the galaxy that is lensing it.  That conversation is about the only real research I can report on today.</p><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/10448119-7196289084176992414?l=hoggresearch.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-14T02:23:15Z</updated>
    <published>2012-02-14T02:23:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="not research"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="talking"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="model"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="imaging"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="gravitational lensing"/>
    <author>
      <name>Hogg</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/18398397408280534592</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-10448119</id>
      <category term="Willman 1"/>
      <category term="clustering"/>
      <category term="merging"/>
      <category term="galaxy"/>
      <category term="PHAT"/>
      <category term="HMF"/>
      <category term="proper motion"/>
      <category term="amateur"/>
      <category term="sdss"/>
      <category term="LSST"/>
      <category term="virtual observatory"/>
      <category term="tractor"/>
      <category term="robot"/>
      <category term="funding"/>
      <category term="telescope"/>
      <category term="digital camera"/>
      <category term="meta data"/>
      <category term="proposal"/>
      <category term="disk"/>
      <category term="fundamental astronomy"/>
      <category term="roweis"/>
      <category term="classification"/>
      <category term="practice"/>
      <category term="decision"/>
      <category term="travel"/>
      <category term="linear algebra"/>
      <category term="interstellar medium"/>
      <category term="web 2.0"/>
      <category term="email"/>
      <category term="bayes"/>
      <category term="scattering"/>
      <category term="atlas"/>
      <category term="quasar"/>
      <category term="confusion"/>
      <category term="minor planet"/>
      <category term="anthropology"/>
      <category term="gravitational lensing"/>
      <category term="reading"/>
      <category term="black hole"/>
      <category term="visualization"/>
      <category term="halo"/>
      <category term="cosmology"/>
      <category term="seminar"/>
      <category term="information"/>
      <category term="2mass"/>
      <category term="chemistry"/>
      <category term="HST"/>
      <category term="gravity"/>
      <category term="panstarrs"/>
      <category term="philosophy"/>
      <category term="experiment"/>
      <category term="WMAP"/>
      <category term="sample"/>
      <category term="baryon acoustic feature"/>
      <category term="radial velocity"/>
      <category term="ukidss"/>
      <category term="dark sector"/>
      <category term="parallax"/>
      <category term="spectroscopy"/>
      <category term="brown dwarf"/>
      <category term="LTFDFCF"/>
      <category term="kinematics"/>
      <category term="cosmography"/>
      <category term="transparency"/>
      <category term="flickr"/>
      <category term="calibration"/>
      <category term="optimization"/>
      <category term="editing"/>
      <category term="star formation"/>
      <category term="ultraviolet"/>
      <category term="statistics"/>
      <category term="testing"/>
      <category term="correlation"/>
      <category term="galex"/>
      <category term="intergalactic medium"/>
      <category term="noise"/>
      <category term="computing"/>
      <category term="dissertation"/>
      <category term="citizen science"/>
      <category term="nasa"/>
      <category term="planet"/>
      <category term="wise"/>
      <category term="talking"/>
      <category term="spitzer"/>
      <category term="cluster"/>
      <category term="CDM"/>
      <category term="astrometry"/>
      <category term="environment"/>
      <category term="imaging"/>
      <category term="press"/>
      <category term="MCMC"/>
      <category term="gaia"/>
      <category term="evolution"/>
      <category term="primus"/>
      <category term="compression"/>
      <category term="phase space"/>
      <category term="relativity"/>
      <category term="weapons"/>
      <category term="archive"/>
      <category term="Solar System"/>
      <category term="Milky Way"/>
      <category term="code"/>
      <category term="observing"/>
      <category term="learning"/>
      <category term="point-spread function"/>
      <category term="Euclid"/>
      <category term="hardware"/>
      <category term="catalog"/>
      <category term="science"/>
      <category term="database"/>
      <category term="thinking"/>
      <category term="gamma-ray burst"/>
      <category term="exoplanet"/>
      <category term="white dwarf"/>
      <category term="theory"/>
      <category term="hipparcos"/>
      <category term="radio"/>
      <category term="law"/>
      <category term="pulsar"/>
      <category term="Gaussian process"/>
      <category term="osss"/>
      <category term="politics"/>
      <category term="meeting"/>
      <category term="photometry"/>
      <category term="star"/>
      <category term="not research"/>
      <category term="API"/>
      <category term="cosmic ray"/>
      <category term="substructure"/>
      <category term="post-starburst"/>
      <category term="archetype"/>
      <category term="life"/>
      <category term="time"/>
      <category term="literature"/>
      <category term="dynamics"/>
      <category term="comet"/>
      <category term="anthropic"/>
      <category term="supernova"/>
      <category term="Earth"/>
      <category term="PTF"/>
      <category term="Fermi"/>
      <category term="search"/>
      <category term="usno-b"/>
      <category term="mathematics"/>
      <category term="dust"/>
      <category term="coffee"/>
      <category term="project management"/>
      <category term="model"/>
      <category term="data"/>
      <category term="writing"/>
      <author>
        <name>Hogg</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/18398397408280534592</uri>
      </author>
      <link href="http://hoggresearch.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://hoggresearch.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>galaxies, stellar dynamics, exoplanets, and fundamental astronomy</subtitle>
      <title>Hogg's Research</title>
      <updated>2012-02-14T20:52:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://dabacon.org/pontiff/?p=6038</id>
    <link href="http://dabacon.org/pontiff/?p=6038" rel="alternate" type="text/html"/>
    <link href="http://dabacon.org/pontiff/?p=6038#comments" rel="replies" type="text/html"/>
    <link href="http://dabacon.org/pontiff/?feed=atom&amp;p=6038" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Randomized Governance</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">What if instead of electing our representatives in government, we simply chose them at random? A new Rasmussen poll asked 1,000 likely voters exactly this question. Turns out, 43% thought that a random choice of people from the phonebook would … <a href="http://dabacon.org/pontiff/?p=6038">Continue reading <span class="meta-nav">→</span></a></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>What if instead of electing our representatives in government, we simply chose them at random?</p>
<p>A <a href="http://www.rasmussenreports.com/public_content/politics/general_politics/february_2012/43_say_random_choices_from_phone_book_better_than_current_congress">new Rasmussen poll</a> asked 1,000 likely voters exactly this question. Turns out, 43% thought that a random choice of people from the phonebook would do a better job than the current legislators, a plurality. Of course, these people were themselves chosen randomly from a phonebook, so I’m not sure they are entirely unbiased. <img alt=":)" class="wp-smiley" src="http://dabacon.org/pontiff/wp-includes/images/smilies/icon_smile.gif"/> </p>
<p>But why stop at the legislators? Why not just write random legislation using <a href="http://en.wikipedia.org/wiki/Context-free_grammar">context-free grammars</a>? We already have software that can <a href="http://pdos.csail.mit.edu/scigen/">automatically write scientific papers</a>, so it doesn’t seem like a stretch. I guess that a lot of this random legislation would be <a href="http://dabacon.org/pontiff/?p=5948">better than SOPA</a>.</p></div>
    </content>
    <updated>2012-02-13T23:02:04Z</updated>
    <published>2012-02-13T02:02:05Z</published>
    <category scheme="http://dabacon.org/pontiff" term="Funny Ha Ha"/>
    <category scheme="http://dabacon.org/pontiff" term="Politics"/>
    <author>
      <name>sflammia</name>
    </author>
    <source>
      <id>http://dabacon.org/pontiff/?feed=atom</id>
      <link href="http://dabacon.org/pontiff" rel="alternate" type="text/html"/>
      <link href="http://dabacon.org/pontiff/?feed=atom" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">A College of Quantum Cardinals</subtitle>
      <title xml:lang="en">The Quantum Pontiff</title>
      <updated>2012-02-13T23:02:04Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/principles/2012/02/how_to_teach_relativity_to_you_2.php</id>
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/oktiaYpMXLY/how_to_teach_relativity_to_you_2.php" rel="alternate" type="text/html"/>
    <title>How to Teach Relativity to Your Dog Photoshop Contest Results</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>So, the big <a href="http://dogphysics.com/relativity_info.html"><cite>How to Teach Physics to Your Dog</cite></a> Photoshop contest concluded on Friday. We got five really good entries, and the judges (me and Kate) had a hard time reaching a decision. After long deliberation, though, we've come up with a solution. </p>

<p>But first, the entries:</p>

 <a href="http://scienceblogs.com/principles/2012/02/how_to_teach_relativity_to_you_2.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/principles/2012/02/how_to_teach_relativity_to_you_2.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/oktiaYpMXLY" width="1"/></div>
    </summary>
    <updated>2012-02-13T19:21:24Z</updated>
    <category term="Book Writing"/>
    <source>
      <id>http://scienceblogs.com/principles/</id>
      <author>
        <name>Chad Orzel</name>
      </author>
      <link href="http://scienceblogs.com/principles/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Thoughts on physics, politics, and pop culture, by a physics professor at a small liberal arts college, plus occasional conversations with his dog.</subtitle>
      <title>Uncertain Principles</title>
      <updated>2012-02-14T15:45:09Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://sbseminar.wordpress.com/?p=4442</id>
    <link href="http://sbseminar.wordpress.com/2012/01/29/a-way-to-discover-the-gamma-function/" rel="alternate" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/01/29/a-way-to-discover-the-gamma-function/#comments" rel="replies" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/01/29/a-way-to-discover-the-gamma-function/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">A way to discover the Gamma function</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">I was messing around this morning and I discovered the following, which seemed cute enough to share. In this post, I’ll make what strikes me as a very reasonable attempt to define for not an integer. Will I get the function? Wait and see! We have . So, by basic complex analysis, , where the [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4442&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>I was messing around this morning and I discovered the following, which seemed cute enough to share. In this post, I’ll make what strikes me as a very reasonable attempt to define <img alt="u!" class="latex" src="http://s0.wp.com/latex.php?latex=u%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="u!"/> for <img alt="u" class="latex" src="http://s0.wp.com/latex.php?latex=u&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="u"/> not an integer. Will I get the <img alt="\Gamma" class="latex" src="http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Gamma"/> function? Wait and see!</p>
<p><span id="more-4442"/></p>
<p>We have <img alt="e^z = \sum z^n/n!" class="latex" src="http://s0.wp.com/latex.php?latex=e%5Ez+%3D+%5Csum+z%5En%2Fn%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="e^z = \sum z^n/n!"/>. So, by basic complex analysis, <img alt="\frac{1}{2 \pi i} \oint e^z z^{-n} \frac{dz}{z} = \frac{1}{n!}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cfrac%7B1%7D%7B2+%5Cpi+i%7D+%5Coint+e%5Ez+z%5E%7B-n%7D+%5Cfrac%7Bdz%7D%7Bz%7D+%3D+%5Cfrac%7B1%7D%7Bn%21%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\frac{1}{2 \pi i} \oint e^z z^{-n} \frac{dz}{z} = \frac{1}{n!}"/>, where the integral is taken along a loop around the origin. This formula is also morally right for <img alt="n" class="latex" src="http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="n"/> a negative integer: <img alt="n!" class="latex" src="http://s0.wp.com/latex.php?latex=n%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="n!"/> wants to be $\infty$ when <img alt="n&lt;0" class="latex" src="http://s0.wp.com/latex.php?latex=n%3C0&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="n&lt;0"/> (because <img alt="0 \times (-1)! = 0! =1" class="latex" src="http://s0.wp.com/latex.php?latex=0+%5Ctimes+%28-1%29%21+%3D+0%21+%3D1&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="0 \times (-1)! = 0! =1"/>, so <img alt="(-1)!" class="latex" src="http://s0.wp.com/latex.php?latex=%28-1%29%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="(-1)!"/> should be infinity, and likewise for the other negative integers). So <img alt="1/n!" class="latex" src="http://s0.wp.com/latex.php?latex=1%2Fn%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="1/n!"/> wants to be zero for <img alt="n&lt;0" class="latex" src="http://s0.wp.com/latex.php?latex=n%3C0&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="n&lt;0"/> and, sure enough, this integral has no poles and vanishes in that case.</p>
<p>We can’t use this formula for <img alt="n" class="latex" src="http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="n"/> not an integer, because <img alt="z^n" class="latex" src="http://s0.wp.com/latex.php?latex=z%5En&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="z^n"/> has a branch cut and the path of integration would have to cross it. But we can fix that by taking the branch cut of <img alt="z^n" class="latex" src="http://s0.wp.com/latex.php?latex=z%5En&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="z^n"/> to be along the negative real axis, and drawing our loop out to stretch very far in the negative real direction. Then <img alt="e^z" class="latex" src="http://s0.wp.com/latex.php?latex=e%5Ez&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="e^z"/> will be very small at the point where the integration path crosses the real axis, so the branch cut will contribute very little. In the limit, we can define</p>
<p style="text-align: center;"><img alt="\displaystyle{ \frac{1}{u!} := \frac{1}{2 \pi i} \int_{\gamma} e^{z} z^{-u} \frac{dz}{z}}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B+%5Cfrac%7B1%7D%7Bu%21%7D+%3A%3D+%5Cfrac%7B1%7D%7B2+%5Cpi+i%7D+%5Cint_%7B%5Cgamma%7D+e%5E%7Bz%7D+z%5E%7B-u%7D+%5Cfrac%7Bdz%7D%7Bz%7D%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\displaystyle{ \frac{1}{u!} := \frac{1}{2 \pi i} \int_{\gamma} e^{z} z^{-u} \frac{dz}{z}}"/></p>
<p>where <img alt="\gamma" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cgamma&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\gamma"/> is a path that comes in from the negative real direction below the real axis, circles around the origin, and returns to infinity in the negative real direction above the axis. This integral will converge for all complex <img alt="u" class="latex" src="http://s0.wp.com/latex.php?latex=u&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="u"/></p>
<p>So, how does this do as a definition of <img alt="1/u!" class="latex" src="http://s0.wp.com/latex.php?latex=1%2Fu%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="1/u!"/>? Well, it obeys the right recursion. A quick integration by parts gives <img alt="\int_{\gamma} e^{z} z^{-u+1} dz = - \int_{\gamma} e^z \frac{z^u}{-u} dz = u  \int_{\gamma} e^z z^{-u} dz" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cint_%7B%5Cgamma%7D+e%5E%7Bz%7D+z%5E%7B-u%2B1%7D+dz+%3D+-+%5Cint_%7B%5Cgamma%7D+e%5Ez+%5Cfrac%7Bz%5Eu%7D%7B-u%7D+dz+%3D+u++%5Cint_%7B%5Cgamma%7D+e%5Ez+z%5E%7B-u%7D+dz&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\int_{\gamma} e^{z} z^{-u+1} dz = - \int_{\gamma} e^z \frac{z^u}{-u} dz = u  \int_{\gamma} e^z z^{-u} dz"/>, so <img alt="1/(u-1)! = u/u!" class="latex" src="http://s0.wp.com/latex.php?latex=1%2F%28u-1%29%21+%3D+u%2Fu%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="1/(u-1)! = u/u!"/>.</p>
<p>Let’s take our path <img alt="\gamma" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cgamma&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\gamma"/> and shrink it towards the negative real axis. As we approach <img alt="-r" class="latex" src="http://s0.wp.com/latex.php?latex=-r&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="-r"/> from above (for <img alt="r" class="latex" src="http://s0.wp.com/latex.php?latex=r&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="r"/> a positive real), <img alt="(-r)^{-u}" class="latex" src="http://s0.wp.com/latex.php?latex=%28-r%29%5E%7B-u%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="(-r)^{-u}"/> approaches <img alt="r^{-u} e^{i \pi u}" class="latex" src="http://s0.wp.com/latex.php?latex=r%5E%7B-u%7D+e%5E%7Bi+%5Cpi+u%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="r^{-u} e^{i \pi u}"/>. As we approach <img alt="-r" class="latex" src="http://s0.wp.com/latex.php?latex=-r&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="-r"/> from below, <img alt="(-r)^{-u}" class="latex" src="http://s0.wp.com/latex.php?latex=%28-r%29%5E%7B-u%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="(-r)^{-u}"/> approaches <img alt="r^{-u} e^{- i \pi u}" class="latex" src="http://s0.wp.com/latex.php?latex=r%5E%7B-u%7D+e%5E%7B-+i+%5Cpi+u%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="r^{-u} e^{- i \pi u}"/>. The difference between the two is <img alt="2 i r^{-u} \sin(\pi u)" class="latex" src="http://s0.wp.com/latex.php?latex=2+i+r%5E%7B-u%7D+%5Csin%28%5Cpi+u%29&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="2 i r^{-u} \sin(\pi u)"/>. So one might think that our integral was equal to <img alt="\frac{1}{\pi} \int_{0}^{\infty} r^{-u} \sin( \pi u) e^{-r} \frac{dr}{r}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cfrac%7B1%7D%7B%5Cpi%7D+%5Cint_%7B0%7D%5E%7B%5Cinfty%7D+r%5E%7B-u%7D+%5Csin%28+%5Cpi+u%29+e%5E%7B-r%7D+%5Cfrac%7Bdr%7D%7Br%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\frac{1}{\pi} \int_{0}^{\infty} r^{-u} \sin( \pi u) e^{-r} \frac{dr}{r}"/>. </p>
<p>If you are more careful, you’ll see that this argument only works for <img alt="\mathrm{Re}(u) &lt; 0" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cmathrm%7BRe%7D%28u%29+%3C+0&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\mathrm{Re}(u) &lt; 0"/>; otherwise, the pole at the origin is too wild to permit the limiting process. So we get that our previous definition is equivalent to</p>
<p style="text-align: center;"><img alt="\displaystyle{\frac{1}{u!} = \frac{1}{\pi} \sin(\pi u)  \int_{0}^{\infty} r^{-u} e^{-r} \frac{dr}{r}}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B%5Cfrac%7B1%7D%7Bu%21%7D+%3D+%5Cfrac%7B1%7D%7B%5Cpi%7D+%5Csin%28%5Cpi+u%29++%5Cint_%7B0%7D%5E%7B%5Cinfty%7D+r%5E%7B-u%7D+e%5E%7B-r%7D+%5Cfrac%7Bdr%7D%7Br%7D%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\displaystyle{\frac{1}{u!} = \frac{1}{\pi} \sin(\pi u)  \int_{0}^{\infty} r^{-u} e^{-r} \frac{dr}{r}}"/> for <img alt="\mathrm{Re}(u) &lt; 0" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cmathrm%7BRe%7D%28u%29+%3C+0&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\mathrm{Re}(u) &lt; 0"/>.</p>
<p>This is where a person who has seen the <img alt="\Gamma" class="latex" src="http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Gamma"/> function defined before will say “well, you’re on the right track, but that sure looks funky.” Writing <img alt="\Pi" class="latex" src="http://s0.wp.com/latex.php?latex=%5CPi&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Pi"/> for the standard complex extension of the factorial function<sup><a href="http://sbseminar.wordpress.com/2012/01/29/a-way-to-discover-the-gamma-function/#Footnote1">1</a></sup>, we have <img alt="\int_{0}^{\infty} r^{-u} e^{-r} \frac{dr}{r} = \Pi(-u-1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cint_%7B0%7D%5E%7B%5Cinfty%7D+r%5E%7B-u%7D+e%5E%7B-r%7D+%5Cfrac%7Bdr%7D%7Br%7D+%3D+%5CPi%28-u-1%29&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\int_{0}^{\infty} r^{-u} e^{-r} \frac{dr}{r} = \Pi(-u-1)"/>. So I’ve got the right integral, but it’s being evaluated at the wrong place, and there is this strange extra factor of <img alt="\frac{1}{\pi} \sin(\pi u)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cfrac%7B1%7D%7B%5Cpi%7D+%5Csin%28%5Cpi+u%29&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\frac{1}{\pi} \sin(\pi u)"/> floating around. </p>
<p>But it all works out! We have the functional equation of the <img alt="\Gamma" class="latex" src="http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Gamma"/> function:</p>
<p style="text-align: center;"><img alt="\displaystyle{\frac{1}{\pi} \sin(\pi u) \Pi(-1-u) = \frac{1}{\Pi(u)}.}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%7B%5Cfrac%7B1%7D%7B%5Cpi%7D+%5Csin%28%5Cpi+u%29+%5CPi%28-1-u%29+%3D+%5Cfrac%7B1%7D%7B%5CPi%28u%29%7D.%7D&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\displaystyle{\frac{1}{\pi} \sin(\pi u) \Pi(-1-u) = \frac{1}{\Pi(u)}.}"/></p>
<p>So the integral I have above really is the standard extension, but gotten at from the other side.</p>
<p>One wants to turn this into a proof of the functional equation, but as yet I don’t see how…</p>
<p><sup>1</sup><a name="Footnote1"/>For historical reasons, <img alt="\Gamma(1+u) = u!" class="latex" src="http://s0.wp.com/latex.php?latex=%5CGamma%281%2Bu%29+%3D+u%21&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Gamma(1+u) = u!"/>. So I’m writing <img alt="\Pi" class="latex" src="http://s0.wp.com/latex.php?latex=%5CPi&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Pi"/> for the function <img alt="\Gamma(1+u)" class="latex" src="http://s0.wp.com/latex.php?latex=%5CGamma%281%2Bu%29&amp;bg=ffffff&amp;fg=666666&amp;s=0" title="\Gamma(1+u)"/>.</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/sbseminar.wordpress.com/4442/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/sbseminar.wordpress.com/4442/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/sbseminar.wordpress.com/4442/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4442&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-13T16:49:04Z</updated>
    <published>2012-01-29T18:19:28Z</published>
    <category scheme="http://sbseminar.wordpress.com" term="complex analysis"/>
    <author>
      <name>David Speyer</name>
      <uri>http://www.math.lsa.umich.edu/~speyer</uri>
    </author>
    <source>
      <id>http://sbseminar.wordpress.com/feed/atom/</id>
      <link href="http://sbseminar.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://sbseminar.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://sbseminar.wordpress.com/osd.xml" rel="search" title="Secret Blogging Seminar" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://sbseminar.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Representation theory, geometry and whatever else we decide is worth writing about today.</subtitle>
      <title xml:lang="en">Secret Blogging Seminar</title>
      <updated>2012-02-14T21:21:39Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://blogs.discovermagazine.com/cosmicvariance/?p=7963</id>
    <link href="http://feedproxy.google.com/~r/CosmicVarianceBlog/~3/i_3fT1sDCVM/" rel="alternate" type="text/html"/>
    <title>Metaphysics Matters</title>
    <summary>Chattering classes here in the U.S. have recently been absorbed in discussions that dance around, but never quite address, a question that cuts to the heart of how we think about the basic architecture of reality: are human beings purely material, or something more? The first skirmish broke out when a major breast-cancer charity, Susan [...]</summary>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Chattering classes here in the U.S. have recently been absorbed in discussions that dance around, but never quite address, a question that cuts to the heart of how we think about <a href="http://blogs.discovermagazine.com/cosmicvariance/2009/06/04/abortion-and-the-architecture-of-reality/">the basic architecture of reality</a>: are human beings purely material, or something more?</p>
<p><a href="http://technorati.com/women/article/is-a-zygote-a-person/"><img alt="" class="alignright size-full wp-image-7964" height="241" src="http://blogs.discovermagazine.com/cosmicvariance/files/2012/02/zygote.jpeg" title="zygote" width="249"/></a> The first skirmish broke out when a major breast-cancer charity, Susan Komen for the Cure (the folks responsible for the ubiquitous pink ribbons), decided to cut their grants to Planned Parenthood, a decision they <a href="http://www.huffingtonpost.com/2012/02/03/susan-g-komen-planned-parenthood_n_1252651.html">quickly reversed</a> after facing an enormous public backlash.  Planned Parenthood provides a wide variety of women’s health services, including birth control and screening for breast cancer, but is widely associated with abortion services.  The Komen leaders offered numerous (mutually contradictory) reasons for their original action, but there is no doubt that their true motive was to end support to a major abortion provider, even if their grants weren’t being used to fund abortions.</p>
<p>Abortion, of course, is a perennial political hot potato, but the other recent kerfuffle focuses on a seemingly less contentious issue: birth control. Catholics, who officially are opposed to birth control of any sort, objected to rules promulgated by the Obama administration, under which birth control would have to be covered by employer-sponsored insurance plans. The original objection seemed to be that Catholic hospitals and other Church-sponsored institutions would essentially be paying for something they though was immoral, in response to which a <a href="http://www.religiondispatches.org/dispatches/sarahposner/5673/white_house_unveils_contraception_accommodation_plan_%5Bupdated%5D/">work-around compromise</a> was quickly adopted.  This didn’t satisfy everyone (anyone?), however, and now the ground has shifted to an argument that no individual Catholic employer should be forced to pay for birth-control insurance, whether or not the organization is sponsored by the Church.  This position has been staked out by the <a href="http://www.politico.com/news/stories/0212/72751.html">US Conference of Catholic Bishops</a>, and underlies <a href="http://motherjones.com/politics/2012/02/rubio-bill-limit-birth-control-access-millions">a new bill</a> proposed by Florida Senator Mark Rubio.</p>
<p>Topics like this are never simple, but they can be especially challenging for a secular democracy. <span id="more-7963"/> On the one hand, our society is based on religious pluralism.  We have freedom of conscience, and try to formulate our laws in such a way that everyone’s rights are protected.  But on the other hand, people have incompatible beliefs about fundamental issues.  Such beliefs are often of central importance, and the duct tape of political liberalism isn’t always sufficient to hold things together.</p>
<p>When it comes to abortion and birth control, there’s no question that down-and-dirty political and social aspects are front and center.  Different political parties want to score points with their constituencies by standing firm in the current culture wars.  And there’s also no question that restricting access to contraception and abortion is driven in part (we can argue about how big that part is) by a desire to control women’s sexuality.</p>
<p>But there is also a serious question about human life and the nature of reality.  What actually happens when that sperm and ovum get together to make a zygote?  Is it just one step of many in an enormously complex chemical reaction that ultimately gives rise to a new person, who is at heart just a complex chemical reaction him-or-herself?  Or is it the moment when an <a href="http://en.wikipedia.org/wiki/Ensoulment#Catholic_Church">immaterial soul</a>, distinct from the material body, first comes into being?  Question like this matter — but as a society we hardly ever discuss them, at least not in any serious and open way.  As a result, different sides talk past each other, trying to squeeze metaphysical stances into political boxes.</p>
<p>If it were really true that “a human life” was defined by the association of an immaterial soul with a physical body, and that association began at the moment of conception, then making abortion illegal would be perfectly sensible.  It would be murder, pure and simple.  (Very few people are actually consistent here, believing that mothers who have abortions should be treated like someone who has committed murder; but there are some.)  But this view of reality <a href="http://blogs.discovermagazine.com/cosmicvariance/2011/05/23/physics-and-the-immortality-of-the-soul/">is not true</a>.  </p>
<p>Naturalism, which describes human beings in the same physical terms as other objects in the universe, doesn’t actually provide a cut-and-dried answer to the abortion question, because it doesn’t draw a bright line between “a separate living person” and “a collection of cells.”  But it provides an utterly different context for addressing the question.  Naturalists are generally against murder, but it’s because they recognize certain collections of atoms as “people,” and endow those people with rights and privileges as part of the structure of society.  It all comes from distinctions that we human beings ultimately invent, not ones that are handed down from a higher authority.  Consequently, the appropriate rules are less clear.  A naturalist wants to know whether the purported person can think, feel, react, and so on.  They also will balance the interests of the fetus, whatever they may be, against the interests of the mother, who is unquestionably a living and functioning person.  It’s perfectly natural that those interests will seem more important than those of a fetus that isn’t even viable outside the womb.</p>
<p>Most everyone, religious believers and naturalists alike, agrees that killing innocent one-year-old children is morally wrong.  Consequently, we can happily live together in a society where that kind of action is illegal.  But our beliefs about aborting one-month-old embryos are understandably very different.  The disagreements about these issues aren’t simply political, they run much deeper than that.</p>
<p><a href="http://blogs.discovermagazine.com/cosmicvariance/2010/01/19/the-truth-still-matters/">It matters</a> how people <a href="http://blogs.discovermagazine.com/cosmicvariance/2007/06/04/it-does-matter-what-people-think-about-how-the-world-works/">think about the world</a>.  Political liberalism is a good system, but it only works insofar as the citizens can agree on a core set of values and push cultural/religious differences to the periphery.  Naturalism doesn’t answer all the value-oriented questions we might have; it simply provides a sensible framework in which they can be profitably discussed.  But between naturalists and non-naturalists, profitable discussion is much more difficult. Which is why we naturalists have to keep pressing, making the best case we can, trying to convince as many people as we can reach that there is only one realm of existence, governed by unbreakable laws, and that we are part of it. </p>

<p><a href="http://feedads.g.doubleclick.net/~a/dJKBHfZlwnvbb7-Mh2xnuvlhYvs/0/da"><img border="0" ismap="true" src="http://feedads.g.doubleclick.net/~a/dJKBHfZlwnvbb7-Mh2xnuvlhYvs/0/di"/></a><br/>
<a href="http://feedads.g.doubleclick.net/~a/dJKBHfZlwnvbb7-Mh2xnuvlhYvs/1/da"><img border="0" ismap="true" src="http://feedads.g.doubleclick.net/~a/dJKBHfZlwnvbb7-Mh2xnuvlhYvs/1/di"/></a></p><img height="1" src="http://feeds.feedburner.com/~r/CosmicVarianceBlog/~4/i_3fT1sDCVM" width="1"/></div>
    </content>
    <updated>2012-02-13T16:38:15Z</updated>
    <category term="Philosophy"/>
    <category term="Politics"/>
    <category term="Religion"/>
    <category term="Top Posts"/>
    <author>
      <name>Sean Carroll</name>
    </author>
    <source>
      <id>http://blogs.discovermagazine.com/cosmicvariance</id>
      <link href="http://blogs.discovermagazine.com/cosmicvariance" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/CosmicVarianceBlog" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <subtitle>Random samplings from a universe of ideas.</subtitle>
      <title>Cosmic Variance</title>
      <updated>2012-02-15T02:08:07Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/principles/2012/02/upcoming_appearances_boskone.php</id>
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/Wxr4fVrw_30/upcoming_appearances_boskone.php" rel="alternate" type="text/html"/>
    <title>Upcoming Appearances: Boskone</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>I've been falling down a little in the area of shameless self-promotion, but I will be at <a href="http://www.nesfa.org/boskone/index.html">Boskone</a> this coming weekend, where I'll be doing three program items:</p>

<p><strong>Reading: Chad Orzel (Reading), Fri 19:30 - 20:00</strong></p>

<p>This will be a section from the forthcoming book, probably involving Emmy and particle physics. Or possibly William Butler Yeats.</p>

<p><strong>How to Wreck Your Career with Social Media (Special Interest Group)
(M), Sat 16:00 - 17:00</strong><br/>
What are the new opportunities for public humiliation opened by the
Internet?  Join this entertaining discussion about authors getting
into nasty public spats with reviewers and fans, going off on long
unhinged political tirades, sharing a little too much of their
unfiltered id, and so on.</p>

<p>I was originally thinking of this as a panel, but they suggested it as a group discussion instead. Lacking any experience with this format, I'm going to hope that somebody's doing one before 4pm on Saturday that sounds interesting, so I can see what exactly I'm supposed to do. Also, suggestions of really entertaining wreckage on social media (blogs, LiveJournal, Twitter, etc.) are welcome in comments.</p>

<p><strong>What Every Dog Should Know About Quantum Physics (Solo Talk), Sun
14:00 - 15:00</strong><br/>
Author of <cite>How to Teach Physics to Your Dog</cite> and <cite>How to Teach
Relativity to Your Dog</cite>, Chad Orzel discusses the basics of quantum
physics for two- and four-legged audiences.</p>

<p>This is my public-lecture talk on quantum physics. It's also the last program slot on the schedule, which makes me wonder how many people will still be around to hear it... If you're going to be there, please do stop by.</p>

 <a href="http://scienceblogs.com/principles/2012/02/upcoming_appearances_boskone.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/Wxr4fVrw_30" width="1"/></div>
    </summary>
    <updated>2012-02-13T15:19:46Z</updated>
    <category term="Book Writing"/>
    <source>
      <id>http://scienceblogs.com/principles/</id>
      <author>
        <name>Chad Orzel</name>
      </author>
      <link href="http://scienceblogs.com/principles/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Thoughts on physics, politics, and pop culture, by a physics professor at a small liberal arts college, plus occasional conversations with his dog.</subtitle>
      <title>Uncertain Principles</title>
      <updated>2012-02-14T15:45:09Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://profmattstrassler.com/?p=2598</id>
    <link href="http://profmattstrassler.com/2012/02/13/why-a-lightweight-higgs-is-a-sensitive-creature-part-2/" rel="alternate" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/13/why-a-lightweight-higgs-is-a-sensitive-creature-part-2/#comments" rel="replies" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/13/why-a-lightweight-higgs-is-a-sensitive-creature-part-2/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Why a Lightweight Higgs is a Sensitive Creature — Part 2</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">[Note added:  It is official --- as expected, at this year's Chamonix workshop, where the Large Hadron Collider's [LHC's] future is planned out each year, it was decided that the LHC’s energy will be increased by 14% next year (from … <a href="http://profmattstrassler.com/2012/02/13/why-a-lightweight-higgs-is-a-sensitive-creature-part-2/">Continue reading <span class="meta-nav">→</span></a><img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2598&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p><em>[Note added:  It is official --- as expected, at this year's <a href="https://indico.cern.ch/conferenceDisplay.py?confId=164089" target="_blank">Chamonix workshop</a>, where the Large Hadron Collider's [LHC's] future is planned out each year, <a href="http://press.web.cern.ch/press/PressReleases/Releases2012/PR01.12E.html" target="_blank">it was decided</a> that the LHC’s energy will be increased by 14% next year (from 3.5 TeV energy per proton and 7 TeV energy per collision in 2010-2011 to 4 TeV per proton and 8 per collision.) Also the time between collisions will remain at 50 nanoseconds.  I’ll have some things to say about the pros and cons of this decision, in particular the challenges for the experiments, over the next few days.]</em></p>
<p>On Monday last week, I gave you half the explanation as to why a lightweight <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/360-2/" target="_blank" title="The Higgs FAQ&#xA0;1.0">Higgs particle</a> is a <strong>sensitive creature,</strong> one that is easily altered by new phenomena — by particles and/or forces that we might not yet know about.  It all had to do with an analogy between a violin string (or a guitar string or a xylophone key) and the properties of the Higgs particle.   Today, <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-standard-model-higgs/lightweight-higgs-a-sensitive-creature/" title="Lightweight Higgs: A `Sensitive&#xA0;Creature&#x2019;">on the same webpage as the first half, I have provided the second half of the story</a>. (If you have already read the first half, just look for the boldface words “<strong>The Diverse Modes of a Higgs’ Demise</strong>”, which separate last week’s prose from the new stuff.)  I’ve also added, for particle physicists and for those laypersons who want to go a little deeper, <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-standard-model-higgs/lightweight-higgs-a-sensitive-creature/a-quantitative-addendum-to-the-sensitive-creature/" title="A Quantitative Addendum to the Sensitive&#xA0;Creature">a short quantitative discussion of my main points</a>.</p>
<p>Also: <strong><em>I will have the honor to be interviewed</em></strong> on Wednesday at 5 p.m. Eastern time, at</p>
<p><a href="http://www.blogtalkradio.com/virtuallyspeaking/2012/02/15/matt-strassler-tom-levenson-virtually-speaking-science">http://www.blogtalkradio.com/virtuallyspeaking/2012/02/15/matt-strassler-tom-levenson-virtually-speaking-science</a></p>
<p>which you can listen to either live or later.  My interviewer, Tom Levenson, is an eminent science journalist who has written fascinating and surprising books on <a href="http://www.amazon.com/Einstein-Berlin-Thomas-Levenson/dp/055310344X" target="_blank">Einstein</a> and on <a href="http://www.amazon.com/Newton-Counterfeiter-Detective-Greatest-Scientist/dp/0151012784" target="_blank">Newton</a>, among <a href="http://www.amazon.com/Thomas-Levenson/e/B001HCU6CW/ref=ntt_athr_dp_pel_1" target="_blank">others</a>, <a href="http://web.mit.edu/newsoffice/2005/levenson-1130.html">won awards</a> for his work on television (e.g. NOVA), has <a href="http://inversesquare.wordpress.com/">a great blog</a> (and also <a href="http://www.balloon-juice.com/2012/02/01/none-dare-call-it-murder/">posts here</a>), and is a <a href="http://writing.mit.edu/people/faculty" target="_blank">professor of science writing at MIT</a>.  In short, he’s a bright and interesting dude whom you should <a href="https://twitter.com/#!/TomLevenson">consider following on Twitter</a>, or in whatever way floats your boat in the ocean of social media.  For this reason I suspect that the conversation is going to be a lot deeper and more interesting than the average interview, with the interviewer making at least as many interesting comments about the topic as the interviewee.</p>
<br/>Filed under: <a href="http://profmattstrassler.com/category/higgs/">Higgs</a>, <a href="http://profmattstrassler.com/category/lhc-background-info/">LHC Background Info</a>, <a href="http://profmattstrassler.com/category/public-outreach/">Public Outreach</a> Tagged: <a href="http://profmattstrassler.com/tag/decay/">decay</a>, <a href="http://profmattstrassler.com/tag/exoticdecays/">ExoticDecays</a>, <a href="http://profmattstrassler.com/tag/higgs/">Higgs</a>, <a href="http://profmattstrassler.com/tag/interviews/">interviews</a>, <a href="http://profmattstrassler.com/tag/lhc/">LHC</a>, <a href="http://profmattstrassler.com/tag/searches/">searches</a> <a href="http://feeds.wordpress.com/1.0/gocomments/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/profmattstrassler.wordpress.com/2598/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/profmattstrassler.wordpress.com/2598/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/profmattstrassler.wordpress.com/2598/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2598&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-13T14:50:50Z</updated>
    <published>2012-02-13T14:12:45Z</published>
    <category scheme="http://profmattstrassler.com" term="Higgs"/>
    <category scheme="http://profmattstrassler.com" term="LHC Background Info"/>
    <category scheme="http://profmattstrassler.com" term="Public Outreach"/>
    <category scheme="http://profmattstrassler.com" term="decay"/>
    <category scheme="http://profmattstrassler.com" term="ExoticDecays"/>
    <category scheme="http://profmattstrassler.com" term="interviews"/>
    <category scheme="http://profmattstrassler.com" term="LHC"/>
    <category scheme="http://profmattstrassler.com" term="searches"/>
    <author>
      <name>Matt Strassler</name>
      <uri>http://profmattstrassler.wordpress.com</uri>
    </author>
    <source>
      <id>http://profmattstrassler.com/feed/atom/</id>
      <link href="http://profmattstrassler.com" rel="alternate" type="text/html"/>
      <link href="http://profmattstrassler.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://profmattstrassler.com/osd.xml" rel="search" title="Of Particular Significance" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://profmattstrassler.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Conversations About Science with Theoretical Physicist Matt Strassler</subtitle>
      <title xml:lang="en">Of Particular Significance</title>
      <updated>2012-02-14T23:45:40Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.quantumdiaries.org/?p=20149</id>
    <link href="http://www.quantumdiaries.org/2012/02/13/immersion-totale-d%e2%80%99artistes-au-cenbg-prise-de-donnees/" rel="alternate" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/13/immersion-totale-d%e2%80%99artistes-au-cenbg-prise-de-donnees/#comments" rel="replies" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/13/immersion-totale-d%e2%80%99artistes-au-cenbg-prise-de-donnees/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Immersion totale d’artistes au CENBG : prise de données</title>
    <summary xml:lang="en">par Nathalie Aubin et Sylvie Massiot, artistes de la compagnie Nukku Matti Les zéolithes, le pic du spectre, disséquer les gonades, les nématodes, anaérobie, enzymatique, l’étuve agitante, interaction, j’ai du temps de faisceau, le pouième, la désintégration double béta des états excités, la soupe de quark, la magicité du noyau, TeV, KeV… Des mots imaginaires [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p><em>par Nathalie Aubin et Sylvie Massiot, artistes de la compagnie <a href="http://www.cienukkumatti.com/" target="_blank">Nukku Matti</a></em></p>
<p>Les zéolithes, le pic du spectre, disséquer les gonades, les nématodes, anaérobie, enzymatique, l’étuve agitante, interaction, j’ai du temps de faisceau, le pouième, la désintégration double béta des états excités, la soupe de quark, la magicité du noyau, TeV, KeV… Des mots imaginaires ? Non, le vocabulaire bien spécifique des scientifiques : leur « jargon » comme on dit. Parce que ces mots nous amusent, parce que les phénomènes qu’ils décrivent nous fascinent, et parce qu’ils nous inspirent tout simplement, nous venons de plonger dans l’univers de l’infiniment petit pour la création d’un spectacle sur la structure de la matière et les particules élémentaires. Nous terminons tout juste la deuxième phase : la prise de données…</p>
<div class="wp-caption alignleft" id="attachment_20150" style="width: 310px;"><img alt="" class="size-medium wp-image-20150" height="199" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/accordeon-copie-300x199.jpg" title="Les com&#xE9;diennes interpr&#xE8;tent une chanson devant un instrument de physique du CENBG. Photo : Service audiovisuel de Bordeaux 1" width="300"/><p class="wp-caption-text">Les comédiennes interprètent une chanson devant un instrument de physique du CENBG. Photo : Service audiovisuel de Bordeaux 1</p></div>
<p>Pour ce faire, nous nous sommes immergées, durant cinq jours, dans le monde de la recherche fondamentale et de la physique des particules. Notre expérience s’est déroulée plus précisément au <a href="http://www.cenbg.in2p3.fr" target="_blank">Centre d’Etudes Nucléaires de Bordeaux Gradignan (CENBG)</a>. Nous y avons passé une semaine exceptionnelle et nous avons découvert un univers extraordinaire… Christine Marquet, chercheuse au CENBG, nous a ouvert les portes d’un monde jusqu’alors invisible à nos yeux. Ici les chercheurs tentent de percer les mystères par la réflexion, la collaboration, l’échange de savoir, l’invention et la construction d’instruments insolites pour le néophyte. L’ensemble des professionnels s’est mis à notre portée sans compter son temps, ni son énergie pour partager ses connaissances et ses questionnements.</p>
<p>Ainsi, chercheurs, ingénieurs, techniciens nous ont parlé de noyaux exotiques, de mécanique, d’électronique, de chimie chaude, d’astrophysique, de biologie, d’informatique, de particules mais aussi de la place de la recherche dans notre société, de l’importance de la collaboration internationale, de la question de la rentabilité incompatible avec le principe même de la recherche fondamentale. Nous avons collecté beaucoup de données qu’il va nous falloir analyser et trier, mais comme le dit Stéphane, un physicien du CENBG : « le résultat n’est pas toujours là où on l’attend ».</p>
<p>Toutefois cette semaine d’immersion confirme notre envie de transmettre au plus grand nombre l’enthousiasme dans lequel nous avons été plongées. Notre souhait le plus cher est de réussir à traduire dans ce spectacle la même passion, la même curiosité, la même envie de partage que les chercheurs nous ont montrée.</p>
<p><br/>
<strong>Vidéo de la « Prise de données »</strong> (<em>réalisation : Service audiovisuel de l’Université Bordeaux 1</em>)</p>
<p>Pour le moment intitulé « Parce que 12 », ce nouveau spectacle sera en tournée cet automne. Le projet est soutenu par : l’IDDAC, le CENBG, le CNRS/IN2P3, l’Université Bordeaux 1, la Communauté de Communes du Vallon de l’Artolie, la ville de Villenave de Rions. Pour suivre l’évolution du projet, rendez-vous sur la rubrique “<a href="http://web.me.com/cienukkumatti/Creation-2012/Laboratoire.html" target="_blank">Création 2012</a>” de notre site web !</p></div>
    </content>
    <updated>2012-02-13T13:42:16Z</updated>
    <published>2012-02-13T13:42:16Z</published>
    <category scheme="http://www.quantumdiaries.org" term="Latest Posts"/>
    <category scheme="http://www.quantumdiaries.org" term="CENBG"/>
    <category scheme="http://www.quantumdiaries.org" term="physique des particules"/>
    <category scheme="http://www.quantumdiaries.org" term="th&#xE9;&#xE2;tre"/>
    <author>
      <name>CNRS-IN2P3</name>
      <uri>http://www.in2p3.fr/</uri>
    </author>
    <source>
      <id>http://www.quantumdiaries.org/feed/atom/</id>
      <link href="http://www.quantumdiaries.org" rel="alternate" type="text/html"/>
      <link href="http://www.quantumdiaries.org/feed/atom/" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">Thoughts on work and life from particle physicists from around the world.</subtitle>
      <title xml:lang="en">Quantum Diaries</title>
      <updated>2012-02-14T16:23:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.science20.com/86888 at http://www.science20.com</id>
    <link href="http://www.science20.com/quantum_diaries_survivor/universal_extra_dimensions_new_dzero_results-86888" rel="alternate" type="text/html"/>
    <title>Universal Extra Dimensions: New DZERO Results</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Of the dozens of new physics models which are currently on the market of Standard Model extensions and plug-ins, the ones hypothesizing the existence of additional dimensions of space-time beyond the 3+1 we know about are definitely among the most fascinating. <br/>

<p><a href="http://www.science20.com/quantum_diaries_survivor/universal_extra_dimensions_new_dzero_results-86888" target="_blank">read more</a></p></div>
    </summary>
    <updated>2012-02-13T13:03:38Z</updated>
    <category scheme="http://www.science20.com/physics" term="Physics"/>
    <author>
      <name>dorigo</name>
    </author>
    <source>
      <id>http://www.science20.com/quantum_diaries_survivor</id>
      <link href="http://www.science20.com/quantum_diaries_survivor" rel="alternate" type="text/html"/>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor/feed" rel="self" type="application/rss+xml"/>
      <subtitle>Science 2.0® - Science for the next 2,000 years</subtitle>
      <title>dorigo's blog</title>
      <updated>2012-02-15T04:45:03Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/principles/2012/02/links_for_2012-02-13.php</id>
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/TISM6soCVC0/links_for_2012-02-13.php" rel="alternate" type="text/html"/>
    <title>Links for 2012-02-13</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><ul>
<li><a href="http://thevirtuosi.blogspot.com/2012/02/time-keeps-on-slippin.html?utm_source=feedburner&amp;utm_medium=feed&amp;utm_campaign=Feed%3A+TheVirtuosi+%28The+Virtuosi%29">The Virtuosi: Time Keeps On Slippin'</a> <p>Alright, so how do we go about quantifying how "good" a watch is?  Well, there seem to be two main things we can test.  The first of these is accuracy.  That is, how close does this watch come to the actual time (according to some time system)?  If the official time is 3:00 pm and my watch claims it is 5:00 am, then it is not very accurate.  The second measure of "good-ness" is precision or, in watch parlance, stability.  This is essentially a measure of the consistency of the watch.  If I have a watch that is consistently off by 5 minutes from the official time, then it is not accurate but it is still stable.  In essence, a very consistent watch would be just as good as an accurate one, because we can always just subtract off the known offset.</p></li>

<li><a href="http://infoproc.blogspot.com/2012/02/class-and-race.html">Information Processing: Class and Race</a> <p>I don't have anything to add about the content of the post, but these graphs look like they came from a website spoofing confusing academic presentations, not an actual social-science paper. I'm not sure which I like more, the fade-to-invisibility technique used to distinguish some of the data series, or the way the legend implies they've done nine-parameter fits to (effectively) single data points.</p></li>

<li><a href="http://blog.markwshead.com/1148/design-problem/">Why You Need Domain Knowledge</a> <p>If you have a gun that runs on compressed air, it would be nice to know how much air you have left wouldn't it? I'm not sure the design was fully thought through. I don't know the story of the gun, but I do know that you shouldn't need to point the barrel toward your face to read a gauge.</p></li>
</ul>
 <a href="http://scienceblogs.com/principles/2012/02/links_for_2012-02-13.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/TISM6soCVC0" width="1"/></div>
    </summary>
    <updated>2012-02-13T12:38:21Z</updated>
    <category term="Links Dump"/>
    <source>
      <id>http://scienceblogs.com/principles/</id>
      <author>
        <name>Chad Orzel</name>
      </author>
      <link href="http://scienceblogs.com/principles/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Thoughts on physics, politics, and pop culture, by a physics professor at a small liberal arts college, plus occasional conversations with his dog.</subtitle>
      <title>Uncertain Principles</title>
      <updated>2012-02-14T15:45:09Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-22973357.post-4793859770697404394</id>
    <link href="http://backreaction.blogspot.com/feeds/4793859770697404394/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=22973357&amp;postID=4793859770697404394" rel="replies" title="31 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/4793859770697404394" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/4793859770697404394" rel="self" type="application/atom+xml"/>
    <link href="http://backreaction.blogspot.com/2012/02/does-science-need-universal-symbol.html" rel="alternate" title="Does science need a universal symbol?" type="text/html"/>
    <title>Does science need a universal symbol?</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://www.newscientist.com/article/mg21328460.300-science-needs-a-universal-symbol.html">Paul Root Wolpe is on the search for a universal symbol for science</a>. <a href="http://www.facebook.com/pages/Science-Symbol/230448310363375">He must be serious, because he has set up a Facebook page.</a> Though one can't say the success of that page is overwhelming.<br/><br/>I'm not sure we really need a universal symbol for science, but I don't think it would harm either. Either way, once the question was in my head, it got me thinking what would make a good symbol for science. Here's what I came up with:<br/><br/><a href="http://2.bp.blogspot.com/-HDPYhxGUmOg/TzadHRMAoGI/AAAAAAAABJw/nU3trte6LyM/s1600/sciencelogo.jpg"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5707922325937102946" src="http://2.bp.blogspot.com/-HDPYhxGUmOg/TzadHRMAoGI/AAAAAAAABJw/nU3trte6LyM/s400/sciencelogo.jpg" style="display: block; margin: 0px auto 10px; text-align: center; cursor: pointer; cursor: hand; width: 378px; height: 400px;"/></a><br/>It has the merit that you can put some electron orbits around it, or a galaxy in the middle. <a href="http://www.phinetune.com/2012/01/07/a-universal-symbol-for-science/">Here is somebody else who has made a suggestion</a>. It looks a little illuminati-ish to me though ;o) Something else that crossed my mind is to use an existing symbol, for example ∀ ("for all").<br/><br/>What do you think, would a symbol for science come in handy? Would you put it on your  bumper?<div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/22973357-4793859770697404394?l=backreaction.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-13T08:27:32Z</updated>
    <published>2012-02-12T13:00:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="Science and Society"/>
    <author>
      <name>Bee</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/06151209308084588985</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-22973357</id>
      <category term="Sociology of Science"/>
      <category term="This and That"/>
      <category term="Particle Physics"/>
      <category term="Physics"/>
      <category term="Useless Knowledge"/>
      <category term="Philosophy"/>
      <category term="Photo"/>
      <category term="Distraction"/>
      <category term="Art"/>
      <category term="Quantum Gravity"/>
      <category term="Academia"/>
      <category term="Comic"/>
      <category term="Science"/>
      <category term="Peer Review"/>
      <category term="Poll"/>
      <category term="Papers"/>
      <category term="Psychology"/>
      <category term="Politics"/>
      <category term="Germany"/>
      <category term="Baby"/>
      <category term="History of Science"/>
      <category term="Travel"/>
      <category term="Infotainment"/>
      <category term="Biology"/>
      <category term="Science and Society"/>
      <category term="Interna"/>
      <category term="Physicists"/>
      <category term="Random Thoughts"/>
      <category term="Canada"/>
      <category term="Humor"/>
      <category term="Astrophysics"/>
      <category term="Video"/>
      <category term="Blog"/>
      <category term="Books"/>
      <author>
        <name>Bee</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/06151209308084588985</uri>
      </author>
      <link href="http://backreaction.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://backreaction.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <title>Backreaction</title>
      <updated>2012-02-14T21:31:23Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://johncarlosbaez.wordpress.com/?p=8022</id>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/13/azimuth-on-google-plus-part-6/" rel="alternate" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/13/azimuth-on-google-plus-part-6/#comments" rel="replies" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/13/azimuth-on-google-plus-part-6/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Azimuth on Google Plus (Part 6)</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">News about energy on Google+.<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=8022&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Lately the distribution of hits per hour on this blog has become very <a href="http://en.wikipedia.org/wiki/Fat-tailed_distribution">fat-tailed</a>.  In other words: the readership shoots up immensely now and then.  I just noticed today’s statistics:</p>
<div align="center"><img alt="" src="http://math.ucr.edu/home/baez/azimuth-statistics_2-12-2012.jpg"/></div>
<p>That spike on the right is what I’m talking about: 338 hits per hour, while before it was hovering in the low 80′s, as usual for the weekend.  Why?   Someone on <i>Hacker News</i> posted an item saying: </p>
<blockquote><p>
John Baez will give his Google Talk tomorrow in the form of a robot.
</p></blockquote>
<p><a href="http://johncarlosbaez.wordpress.com/2012/01/24/i-robot/">That’s true!</a>   If you’re near Silicon Valley on Monday the 13th and you want to see me in the form of a robot, come to the Google campus and listen to my talk <i>Energy, the Environment and What We Can Do</i>.  </p>
<p>It starts at 4 pm in the Paramaribo Room (Building 42, Floor 2).  You’ll need to check in 15 minutes before that at the main visitor’s lounge in Building 43, and someone will escort you to the talk. </p>
<p>But if you can’t attend, don’t worry!  A video will appear on YouTube, and I’ll point you to it when it does.</p>
<div align="center">
<a href="http://johncarlosbaez.wordpress.com/2012/01/24/i-robot/"><img height="200" src="http://media.npr.org/assets/img/2011/12/31/anybot_custom.jpg?t=1325339121&amp;s=1"/></a>
</div>
<p>I tested out the robot a few days ago from a hotel room in Australia—it’s a strange sensation!  Suzanne Brocato showed me the ropes.  To talk to me easily, she lowered my ‘head’ until I was just 4 feet tall.  “You’re so short!” she laughed.  I rolled around the offices of Anybot and met the receptionist, who was also in the form of a robot.  Then we went to the office of the CEO, Trevor Blackwell, and planned out my talk a little.  I need to practice more today.  </p>
<p>But why did someone at <i>Hacker News</i> post that comment just then?  I suspect it’s because I reminded people about my talk on Google+ last night.  </p>
<p>The fat-tailed distribution of blog hits is also happening at the scale of days, not just hours:</p>
<div align="center"><img alt="" src="http://math.ucr.edu/home/baez/azimuth-statistics_1-2012.jpg"/></div>
<p>The spikes happen when I talk about a ‘hot topic’.  January 27th was my biggest day so far.   <i>Slashdot</i> discovered my post about the <a href="http://johncarlosbaez.wordpress.com/2012/01/26/ban-elsevier/">Elsevier boycott</a>, and send 3468 readers my way.   But a total 6499 people viewed that post, so a bunch must have come from other sources.</p>
<p>January 31st was also big: 3271 people came to read about <a href="http://johncarlosbaez.wordpress.com/2012/01/31/the-faculty-of-1000/">The Faculty of 1000</a>.  2140 of them were sent over by <i>Hacker News</i>.</p>
<p>If I were trying to make money from advertising on this blog, I’d be pushed toward more posts about hot topics.  Forget the mind-bending articles on <a href="http://johncarlosbaez.wordpress.com/2012/02/10/quantropy-part-2/">quantropy</a>, packed with complicated equations!  </p>
<p>But as it is, I’m trying to do some mixture of having fun, figuring out stuff, and getting people to save the planet.  (Open access publishing fits into that mandate: it’s tragic how climate crackpots post on popular blogs while experts on climate change publish their papers in journals hidden from public view!)  So, I don’t want to maximize readership: what matters more is getting people to do good stuff.  </p>
<p>Do you have any suggestions on how I could do this better, while still being me?  I’m not going to get a personality transplant, so there are limits on what I’ll do.</p>
<p>One good idea would be to make sure every post on a ‘hot topic’ offers readers <i>something they can do now</i>.  </p>
<p>Hmm, readership is still spiking:</p>
<div align="center"><img alt="" src="http://math.ucr.edu/home/baez/azimuth-statistics_2-12a-2012.jpg"/></div>
<p>But enough of this navel-gazing!  Here are some recent Azimuth articles about energy on Google+.  </p>
<h3> Energy </h3>
<p>1) In his State of the Union speech, Obama <a href="http://www.mnn.com/earth-matters/politics/blogs/sotu-2012-obama-touts-old-new-energy">talked a lot about energy</a>:</p>
<blockquote><p>
We’ve subsidized oil companies for a century. That’s long enough.  It’s time to end the taxpayer giveaways to an industry that rarely has been more profitable, and double-down on a clean energy industry that never has been more promising.
</p></blockquote>
<p>He acknowledged that differences on Capitol Hill are “too deep right now” to pass a comprehensive climate bill, but he added that “there’s no reason why Congress shouldn’t at least set a clean-energy standard that creates a market for innovation.”</p>
<p>However, lest anyone think he actually wants to stop global warming, he also pledged “to open more than 75 percent of our potential offshore oil and gas resources.” </p>
<p>2) This paper claims a ‘phase change’ hit the oil markets around 2005:</p>
<p>• James Murray and David King, <a href="http://www.nature.com/nature/journal/v481/n7382/full/481433a.html">Climate policy: Oil’s tipping point has passed</a>, <i>Nature</i> <b>481</b> (2011), 433–435. </p>
<div align="center">
<a href="http://math.ucr.edu/home/baez/murray_king_oil_market_phase_change.jpg"><br/>
<img src="http://math.ucr.edu/home/baez/murray_king_oil_market_phase_change.jpg" width="450"/></a></div>
<p>They write:</p>
<blockquote><p>
In 2005, global production of regular crude oil reached about 72 million barrels per day. From then on, production capacity seems to have hit a ceiling at 75 million barrels per day. A plot of prices against production from 1998 to today shows this dramatic transition, from a time when supply could respond elastically to rising prices caused by increased demand, to when it could not (see ‘Phase shift’). As a result, prices swing wildly in response to small changes in demand. Other people have remarked on this step change in the economics of oil around the year 2005, but the point needs to be lodged more firmly in the minds of policy-makers.
</p></blockquote>
<p>3) Help out the famous climate blogger Joe Romm!  He asks: <a href="http://thinkprogress.org/romm/2012/02/11/423484/us-energy-mix-in-2050-cut-co2-emissions-80/?mobile=nc">What will the U.S. energy mix look like in 2050 if we cut CO<sub>2</sub> emissions 80%?</a></p>
<blockquote><p>
How much total energy is consumed in 2050… How much coal, oil, and natural gas is being consumed (with carbon capture and storage of some coal and gas if you want to consider that)? What’s the price of oil? How much of our power is provided by nuclear power? How much by solar PV and how much by concentrated solar thermal? How much from wind power? How much from biomass? How much from other forms of renewable energy?  What is the vehicle fleet like? How much electric? How much next-generation biofuels?
</p></blockquote>
<p>As he notes, there are lots of studies on these issues.  Point him to the best ones!</p>
<p>4) Due to plunging prices for components, solar power prices in Germany <a href="http://www.trust.org/alertnet/news/falling-solar-prices-good-for-climate-bad-for-firms/">dropped by half in the last 5 years</a>.  Now solar generates electricity at levels only slightly above what consumers pay. The subsidies will disappear entirely within a few years, when solar will be as cheap as conventional fossil fuels.  Germany has added 14,000 megawatts capacity in the last 2 years and now has 24,000 megawatts in total—enough green electricity to meet nearly 4% the country’s power demand. That is expected to rise to 10% by 2020. Germany now has almost 10 times more installed capacity than the United States.</p>
<p>That’s all great—but, umm, what about the other 90%?   What’s their long-term plan?  Will they keep using coal-fired power plants?   Will they buy more nuclear power from France?</p>
<p>In May 2011, Britain claimed it would <a href="http://www.guardian.co.uk/environment/2011/may/17/uk-halve-carbon-emissions">halve carbon emissions by 2025</a>.  Is Germany making equally bold claims or not?<br/>
Of course what matters is deeds, not words, but I’m curious.</p>
<p>5) Stephen Lacey presents <a href="http://thinkprogress.org/romm/2012/01/23/408258/an-illustrated-guide-to-the-state-of-sustainability/">some interesting charts</a> showing the progress and problems with sustainability in the US.  For example, there’s been a striking drop in how much energy is being used per dollar of GNP:</p>
<div align="center"><a href="http://thinkprogress.org/romm/2012/01/23/408258/an-illustrated-guide-to-the-state-of-sustainability/"><br/>
<img src="http://thinkprogress.org/wp-content/uploads/2012/01/Screen-shot-2012-01-20-at-3.06.56-PM.png" width="450"/></a></div>
<p>Sorry for the archaic ‘British Thermal Units’: we no longer have a king, but for some reason the U.S. failed to throw off the old British system of measurement.  A <a href="http://en.wikipedia.org/wiki/British_thermal_unit">BTU</a> is a bit more than a kilojoule.</p>
<p>Despite these dramatic changes, Lacey says “we waste around 85% of the energy produced in the U.S.”  But he doesn’t say how that number was arrived at.  Does anyone know?</p>
<p>6) The American Council for an Energy-Efficient Economy (ACEEE) has a new report called <i><a href="http://aceee.org/research-report/e121">The Long-Term Energy Efficiency Potential: What the Evidence Suggests</a></i>.  It describes some scenarios, including one where the US encourages a greater level of productive investments in energy efficiency so that by the year 2050, it reduces overall energy consumption by 40 to 60 percent.  I’m very interested in how much efficiency can help.   Some, but not all, of the improvements will be eaten up by the <a href="http://www.azimuthproject.org/azimuth/show/Rebound+effect">rebound effect</a>.   </p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/johncarlosbaez.wordpress.com/8022/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/johncarlosbaez.wordpress.com/8022/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/johncarlosbaez.wordpress.com/8022/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=8022&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-13T05:34:13Z</updated>
    <published>2012-02-13T03:02:47Z</published>
    <category scheme="http://johncarlosbaez.wordpress.com" term="azimuth"/>
    <category scheme="http://johncarlosbaez.wordpress.com" term="climate"/>
    <category scheme="http://johncarlosbaez.wordpress.com" term="energy"/>
    <author>
      <name>John Baez</name>
      <uri>http://math.ucr.edu/home/baez/</uri>
    </author>
    <source>
      <id>http://johncarlosbaez.wordpress.com/feed/atom/</id>
      <link href="http://johncarlosbaez.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://johncarlosbaez.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/osd.xml" rel="search" title="Azimuth" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <title xml:lang="en">Azimuth</title>
      <updated>2012-02-14T12:46:26Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.scottaaronson.com/blog/?p=917</id>
    <link href="http://www.scottaaronson.com/blog/?p=917" rel="alternate" type="text/html"/>
    <link href="http://www.scottaaronson.com/blog/?p=917#comments" rel="replies" type="text/html"/>
    <link href="http://www.scottaaronson.com/blog/?feed=atom&amp;p=917" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Safari photos from Kenya</title>
    <summary xml:lang="en">(Credit for most of the photos: Dana) I was going to write a whole long essay about the differences between going to the zoo and visiting an ancestral environment of humanity, where elephants have grazed for millions of years; the weird sense of familiarity, as if you’re seeing how the surface of the earth is [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://www.scottaaronson.com/blog/?attachment_id=919" title="1"><img alt="1" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/11-150x150.jpg" title="1" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=920" title="2"><img alt="2" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/2-150x150.jpg" title="2" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=921" title="3"><img alt="3" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/3-150x150.jpg" title="3" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=922" title="4"><img alt="4" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/4-150x150.jpg" title="4" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=923" title="5"><img alt="5" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/5-150x150.jpg" title="5" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=924" title="6"><img alt="6" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/6-150x150.jpg" title="6" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=925" title="7"><img alt="7" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/7-150x150.jpg" title="7" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=926" title="8"><img alt="8" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/8-150x150.jpg" title="8" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=927" title="9"><img alt="9" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/9-150x150.jpg" title="9" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=928" title="10"><img alt="10" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/10-150x150.jpg" title="10" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=929" title="11"><img alt="11" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/111-150x150.jpg" title="11" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=930" title="12"><img alt="12" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/12-150x150.jpg" title="12" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=931" title="13"><img alt="13" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/13-150x150.jpg" title="13" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=932" title="14"><img alt="14" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/14-150x150.jpg" title="14" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=933" title="15"><img alt="15" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/15-150x150.jpg" title="15" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=934" title="16"><img alt="16" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/16-150x150.jpg" title="16" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=935" title="17"><img alt="17" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/17-150x150.jpg" title="17" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=936" title="18"><img alt="18" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/18-150x150.jpg" title="18" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=937" title="19"><img alt="19" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/19-150x150.jpg" title="19" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=938" title="20"><img alt="20" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/20-150x150.jpg" title="20" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=939" title="21"><img alt="21" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/21-150x150.jpg" title="21" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=940" title="22"><img alt="22" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/22-150x150.jpg" title="22" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=941" title="23"><img alt="23" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/23-150x150.jpg" title="23" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=942" title="24"><img alt="24" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/24-150x150.jpg" title="24" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=943" title="25"><img alt="25" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/25-150x150.jpg" title="25" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=944" title="26"><img alt="26" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/26-150x150.jpg" title="26" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=945" title="27"><img alt="27" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/27-150x150.jpg" title="27" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=946" title="28"><img alt="28" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/28-150x150.jpg" title="28" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=947" title="29"><img alt="29" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/29-150x150.jpg" title="29" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=948" title="30"><img alt="30" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/30-150x150.jpg" title="30" width="150"/></a>
<a href="http://www.scottaaronson.com/blog/?attachment_id=949" title="31"><img alt="31" class="attachment-thumbnail" height="150" src="http://www.scottaaronson.com/blog/wp-content/uploads/2012/02/31-150x150.jpg" title="31" width="150"/></a>

<p>(Credit for most of the photos: Dana)</p>
<p>I was going to write a whole long essay about</p>
<ul>
<li>the differences between going to the zoo and visiting an ancestral environment of humanity, where elephants have grazed for millions of years;</li>
<li>the weird sense of <em>familiarity</em>, as if you’re seeing how the surface of the earth is “supposed” to look, how it <em>did</em> look before humans started converting it into KFCs and parking lots;</li>
<li>how to tell whether an elephant charging your jeep is serious about wanting to trample you or, much more likely, just warning you to go away (apparently, it has to do with whether its ears are straight back or flapping);</li>
<li>the “airport” at Lake Naivasha (a strip of dirt in a grassy field filled with zebras, and a guy on a bicycle who shoos the zebras off the strip before a plane lands);</li>
<li>Britain’s failure, to this day, to issue any sort of apology for its detention, torture, and murder of tens of thousands of Kenyans during the waning years of its colonial rule in the 1950s;</li>
<li>the near-destruction by poaching, over the last century, of many of the majestic animal populations you see above;</li>
<li>the heroism of Richard Leakey (past director of the Kenya Wildlife Service) in overcoming decades of bureaucratic inertia to initiate a crackdown, where rangers were authorized to “poach the poachers,” shooting them on sight<em/> (!);</li>
<li>how, after Leakey almost-singlehandedly saved Kenya’s wild elephants, he lost both of his legs when his plane crashed (widely suspected to be due to sabotage), and was forced from his job months later;</li>
<li>the benefits of safari tourism in creating a serious economic incentive for conservation, but also the drawbacks (e.g., all the jeeps making it harder for the cheetahs to hunt);</li>
<li>the large, obvious, anything-but-”theoretical” changes being wrought by global warming on the rainfall in Kenya’s game parks (which changes are killing the trees, thereby eliminating the lions’ hiding places and making it harder for them to hunt—hey, at least the zebras are happy);</li>
<li>the Maasais’ innovative uses for cow dung; the resulting immature jokes on my part (homeowner to roofer: “this roof you sold me is <em>shit</em>!”);</li>
<li>my growing fascination, over the course of the trip, with the lesser-known corners of Mammalia (elands, dik-diks, kudus, waterbucks, topis, rock hyraxes); how this might mirror my fascination with lesser-known complexity classes like AWPP, QMA(2)/qpoly, SBP, C<sub>=</sub>P, and BPP<sub>path</sub>;</li>
<li>how parts of the African savannah have better cellphone reception than my office in Stata;</li>
<li>how it’s indeed possible to catch up on Jon Stewart and The Big Bang Theory over wifi, from a tent in the Maasai Mara, while hippos bellow loudly in the river below, and elephants graze and crocodiles sun themselves on the other side.</li>
</ul>
<p>But then I never got around to writing that essay.  So enjoy the photos, and ask in the comments if you want me to say something else.</p></div>
    </content>
    <updated>2012-02-13T03:16:48Z</updated>
    <published>2012-02-13T03:16:48Z</published>
    <category scheme="http://www.scottaaronson.com/blog" term="Adventures in Meatspace"/>
    <author>
      <name>Scott</name>
      <uri>http://www.scottaaronson.com</uri>
    </author>
    <source>
      <id>http://www.scottaaronson.com/blog/?feed=atom</id>
      <link href="http://www.scottaaronson.com/blog" rel="alternate" type="text/html"/>
      <link href="http://www.scottaaronson.com/blog/?feed=atom" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">The Blog of Scott Aaronson</subtitle>
      <title xml:lang="en">Shtetl-Optimized</title>
      <updated>2012-02-13T03:16:48Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://quomodocumque.wordpress.com/?p=3309</id>
    <link href="http://quomodocumque.wordpress.com/2012/02/12/is-there-a-noncommutative-siegels-lemma/" rel="alternate" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/12/is-there-a-noncommutative-siegels-lemma/#comments" rel="replies" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/12/is-there-a-noncommutative-siegels-lemma/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Is there a noncommutative Siegel’s Lemma?</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">Let f be the smallest function satisfying the following: Suppose given two matrices A and B in SL_3(Z), with all entries at most N.  If there is a word w(A,B,A^{-1},B^{-1}) which vanishes in SL_3(Z), then there is a word w’(A,B,A^{-1},B^{-1}) of length at most f(N) which vanishes in SL_3(Z). What are the asymptotics of f(N)? [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3309&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Let f be the smallest function satisfying the following:</p>
<p>Suppose given two matrices A and B in SL_3(Z), with all entries at most N.  If there is a word w(A,B,A^{-1},B^{-1}) which vanishes in SL_3(Z), then there is a word w’(A,B,A^{-1},B^{-1}) of length at most f(N) which vanishes in SL_3(Z).</p>
<p>What are the asymptotics of f(N)?</p>
<p>The reason for the title is that, if SL_3(Z) is replaced by Z^n, this is Siegel’s lemma:  if two (or, for that matter, k) vectors in [-N..N]^n are linearly dependent, then there is a linear dependency whose height is polynomial in N.  (Here k and n are constants and N is growing.)</p>
<p>I don’t have any particular need to know this — the question came up in conversation at the very stimulating <a href="http://www.msri.org/web/msri/scientific/show/-/event/Wm9222">MSRI Thin Groups workshop</a> just concluded.  <a href="http://www.msri.org/attachments/workshops/652_Sarnak-notes.pdf">Sarnak’s notes</a> are an excellent guide to the topics discussed there.</p>
<p> </p>
<p> </p>
<p> </p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/quomodocumque.wordpress.com/3309/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/quomodocumque.wordpress.com/3309/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/quomodocumque.wordpress.com/3309/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3309&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-12T20:13:21Z</updated>
    <published>2012-02-12T20:13:21Z</published>
    <category scheme="http://quomodocumque.wordpress.com" term="math"/>
    <category scheme="http://quomodocumque.wordpress.com" term="offhand"/>
    <category scheme="http://quomodocumque.wordpress.com" term="arithmetic groups"/>
    <category scheme="http://quomodocumque.wordpress.com" term="group theory"/>
    <category scheme="http://quomodocumque.wordpress.com" term="msri"/>
    <category scheme="http://quomodocumque.wordpress.com" term="sarnak"/>
    <category scheme="http://quomodocumque.wordpress.com" term="siegel's lemma"/>
    <category scheme="http://quomodocumque.wordpress.com" term="thin groups"/>
    <author>
      <name>JSE</name>
      <uri>http://quomodocumque.wordpress.com</uri>
    </author>
    <source>
      <id>http://quomodocumque.wordpress.com/feed/atom/</id>
      <link href="http://quomodocumque.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://quomodocumque.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://quomodocumque.wordpress.com/osd.xml" rel="search" title="Quomodocumque" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://quomodocumque.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Math, Madison, food, the Orioles, books, my kids.</subtitle>
      <title xml:lang="en">Quomodocumque</title>
      <updated>2012-02-15T00:49:06Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/principles/2012/02/syncretic_pre-schooler_bloggin.php</id>
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/KWZSXfgU5H4/syncretic_pre-schooler_bloggin.php" rel="alternate" type="text/html"/>
    <title>Syncretic Pre-Schooler Blogging</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>We send SteelyKid to preschool at the Jewish Community Center in Schenectady, because when we looked at day care programs back in the day, they had the one we liked best. This is a mixed blessing in a number of ways-- they close for a lot of religious holidays when nothing else closes, creating some awkwardness with child care and our jobs. On the plus side, though, it's a chance to learn about another culture, and as an extra bonus, most of what we learn is filtered through SteelyKid, making it extra cute.</p>

<p>For example, on the way home Friday, she was chattering quietly to herself in the back seat, and when I opened the door, announced "I was telling a story about Satsuki!"</p>

<p>"Satsuki from the Totoro movie?" She's a by fan of <cite>My Neighbor Totoro</cite>, which we have on DVD.</p>

<p>"Yeah. She was asking a question."</p>

<p>"What was the question?"</p>

<p>"Well, she was asking about... about... God gave the world to Abraham!"</p>

<p>"Really?"</p>

<p>"Yeah, He gave Abraham the whole world. And Jacob, too. God gave the world to Jacob, because he was a good boy."</p>

<p>A little later in the evening, at the dinner table, she explained that this picture was a painting of the whole world:</p>

<p><img alt="sm_world_picture.jpg" height="435" src="http://scienceblogs.com/principles/upload/2012/02/syncretic_pre-schooler_bloggin/sm_world_picture.jpg" width="500"/></p>
 <a href="http://scienceblogs.com/principles/2012/02/syncretic_pre-schooler_bloggin.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/principles/2012/02/syncretic_pre-schooler_bloggin.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/KWZSXfgU5H4" width="1"/></div>
    </summary>
    <updated>2012-02-12T14:14:51Z</updated>
    <category term="The Pip"/>
    <source>
      <id>http://scienceblogs.com/principles/</id>
      <author>
        <name>Chad Orzel</name>
      </author>
      <link href="http://scienceblogs.com/principles/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Thoughts on physics, politics, and pop culture, by a physics professor at a small liberal arts college, plus occasional conversations with his dog.</subtitle>
      <title>Uncertain Principles</title>
      <updated>2012-02-14T15:45:09Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-2846514233477399562.post-2340980536698530047</id>
    <link href="http://resonaances.blogspot.com/feeds/2340980536698530047/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=2846514233477399562&amp;postID=2340980536698530047" rel="replies" title="12 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default/2340980536698530047" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default/2340980536698530047" rel="self" type="application/atom+xml"/>
    <link href="http://resonaances.blogspot.com/2012/02/higgs-stronger-and-more-exciting.html" rel="alternate" title="Higgs: stronger and more exciting" type="text/html"/>
    <title>Higgs: stronger and more exciting</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Today the CMS and ATLAS collaborations dumped into<a href="https://cdsweb.cern.ch/search?f=keyword&amp;p=Higgs%20physics&amp;ln=en"> public pages</a> a dozen publications describing the Higgs searches in the 2011 LHC data. In the first approximation, these are the same results that were presented on December 13. But there is one surprise...<br/><br/>The CMS collaboration had every reason to think that life was unfair.  For the last round of Higgs searches they made significantly more effort and analyzed more possible signatures than ATLAS.  The latter updated only 2  channels to the full dataset, and in principle had  worse sensitivity in the H→ZZ*→4l channel (due to slightly higher pT thresholds in the analysis). In spite of that, the significance of the Higgs-like excess near 125 GeV was much weaker in CMS than in ATLAS. Naturally,  the  CMS researchers  have spent the last 2 months scouring their drawers for strayed Higgs events. And they found.<br/><a href="http://4.bp.blogspot.com/-HGd0kIqlg9c/TzHA08T1kSI/AAAAAAAAAk4/oCfwX1eseKQ/s1600/vbf.png"/><br/><a href="http://4.bp.blogspot.com/-HGd0kIqlg9c/TzHA08T1kSI/AAAAAAAAAk4/oCfwX1eseKQ/s1600/vbf.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706554218630189346" src="http://4.bp.blogspot.com/-HGd0kIqlg9c/TzHA08T1kSI/AAAAAAAAAk4/oCfwX1eseKQ/s320/vbf.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 121px; height: 108px;"/></a>New interesting events are <a href="http://arxiv.org/abs/1202.1487">reported</a> <a href="https://cdsweb.cern.ch/record/1422388/files/HIG-11-033-arxiv-gen.pdf"/><span style="text-decoration: underline;"/>in the H → γγ channel. Compared to the December 13 presentation, CMS added a new category of events which, apart from 2 photons, contain  2 energetic jets in the forward (closer to  the beam pipe) region of the detector. Such  events could arise in the so-called vector boson fusion (VBF) process, where each of the  2 <a href="http://4.bp.blogspot.com/-L-_ruxB0K48/TzQ27R1YK5I/AAAAAAAAAlc/q-hN2lFP6xk/s1600/ggh.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5707247019812727698" src="http://4.bp.blogspot.com/-L-_ruxB0K48/TzQ27R1YK5I/AAAAAAAAAlc/q-hN2lFP6xk/s320/ggh.png" style="float: left; margin: 0pt 10px 10px 0pt; cursor: pointer; width: 119px; height: 105px;"/></a>colliding quarks emits a W or Z boson which coalesce to create a Higgs boson (right graph). The 2 original quark get deflected and may be seen in a detector as two forward jets.  On the other hand in gluon fusion (left graph), which is the dominant Higgs production process at the LHC,   the 2 colliding gluons "vanish" and the final state rarely contains 2 forward jets. Also background processes are less likely to produce 2 photons in association  with 2 such jets. Hence, by selecting diphoton events with 2 forward jets we can probe a distinct Higgs production process, with less signal (the VBF cross section is 10 times smaller than the gluon fusion one), but also with less background.<br/><br/><a href="http://2.bp.blogspot.com/-mf0bbqeKqEo/TzHAS9wftuI/AAAAAAAAAkg/a63lqWeLZR0/s1600/CMS_GaGa_dijet.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706553634903275234" src="http://2.bp.blogspot.com/-mf0bbqeKqEo/TzHAS9wftuI/AAAAAAAAAkg/a63lqWeLZR0/s320/CMS_GaGa_dijet.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 144px; height: 120px;"/></a>Now, in the VBF class CMS finds 7 diphoton events in a 1-GeV bin at  the invariant mass 124 GeV, where only about 2 events would be expected  from non-Higgs background. By itself it would be nothing, but together with the rest of events in the diphoton and 4-lepton channels it provides another support for the  existence of the  Higgs boson in the mass range 124-126 GeV.  All in all, the local significance of the excess near 125 GeV in the <a href="http://arxiv.org/abs/1202.1488">combined</a> CMS analysis is now over 3 sigma, very similar to <a href="http://arxiv.org/abs/1202.1408">that of</a> ATLAS.  While many small improvements have been  made, my feeling is that  significance was pumped up mostly by these additional VBF events.<br/><br/><a href="http://3.bp.blogspot.com/-LV0ZBDVzKzQ/TzHD2a5W-uI/AAAAAAAAAlE/gpeWsFtK7yU/s1600/CMS_HiggsCombined_pvalue.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706557542555384546" src="http://3.bp.blogspot.com/-LV0ZBDVzKzQ/TzHD2a5W-uI/AAAAAAAAAlE/gpeWsFtK7yU/s320/CMS_HiggsCombined_pvalue.png" style="float: left; margin: 0pt 10px 10px 0pt; cursor: pointer; width: 201px; height: 191px;"/></a><a href="http://3.bp.blogspot.com/-9u6xY75qf10/TzHD_5TQX1I/AAAAAAAAAlQ/ZgaRukTbfEQ/s1600/ATLAS_HiggsCombined_pvalue.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706557705335889746" src="http://3.bp.blogspot.com/-9u6xY75qf10/TzHD_5TQX1I/AAAAAAAAAlQ/ZgaRukTbfEQ/s320/ATLAS_HiggsCombined_pvalue.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 208px; height: 193px;"/></a><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/>But there is something intriguing here.  Now in both ATLAS and CMS the best fit of the Higgs rate in the H → γγ channel alone is about twice the Standard Model rate, with the standard rate being over 1 sigma away in both cases. Actually, with the present amount of data CMS would<span style="font-style: italic;"> not </span> expect to see any VBF events, as rate predicted by the Standard Model  is too small (see below that in this channel their fit is almost 4 times the standard rate, although  with a large error).    Could it be that we're seeing a non-Standard-Model Higgs boson with an enhanced decay rate and/or enhanced VBF production cross section? Of course, it is far too early for jumping into conclusions: the errors are still large and we may easily be observing an upward fluctuation. Besides,the combination of all channels doesn't show any dramatic enhancement of the Higgs rate.  In any case we're free to speculate while waiting for more data (and a word from ATLAS on the VBF events).<br/><a href="http://2.bp.blogspot.com/-yM6VYS8rIfI/TzHAbfsBv7I/AAAAAAAAAks/182yB2t3PBU/s1600/CMS_GaGaSigmaFit.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706553781450293170" src="http://2.bp.blogspot.com/-yM6VYS8rIfI/TzHAbfsBv7I/AAAAAAAAAks/182yB2t3PBU/s320/CMS_GaGaSigmaFit.png" style="float: left; margin: 0pt 10px 10px 0pt; cursor: pointer; width: 205px; height: 240px;"/></a><a href="http://3.bp.blogspot.com/-EyoRwlQAQkE/TzHAN2WQn9I/AAAAAAAAAkU/GG5IZpU52Qw/s1600/ATLAS_HiggsToGaGa_SigmaFit.png"><img alt="" border="0" id="BLOGGER_PHOTO_ID_5706553547014840274" src="http://3.bp.blogspot.com/-EyoRwlQAQkE/TzHAN2WQn9I/AAAAAAAAAkU/GG5IZpU52Qw/s320/ATLAS_HiggsToGaGa_SigmaFit.png" style="float: right; margin: 0pt 0pt 10px 10px; cursor: pointer; width: 272px; height: 197px;"/></a><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/><br/>See also <a href="http://profmattstrassler.com/2012/02/09/this-weeks-step-forward-in-the-search-for-the-higgs-particle/">Matt</a> for more details and more caution.<div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/2846514233477399562-2340980536698530047?l=resonaances.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-12T12:14:54Z</updated>
    <published>2012-02-08T00:11:00Z</published>
    <author>
      <name>Jester</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/08947218566941608850</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-2846514233477399562</id>
      <category term="Distraction"/>
      <category term="April Fools"/>
      <category term="Report"/>
      <category term="Jest"/>
      <category term="News"/>
      <category term="Musing"/>
      <category term="Review"/>
      <author>
        <name>Jester</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/16844247827820646813</uri>
      </author>
      <link href="http://resonaances.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://resonaances.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/2846514233477399562/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>Particle Physics Blog</subtitle>
      <title>RÉSONAANCES</title>
      <updated>2012-02-15T00:42:02Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.quantumdiaries.org/?p=20245</id>
    <link href="http://www.quantumdiaries.org/2012/02/12/maitriser-la-complexite/" rel="alternate" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/12/maitriser-la-complexite/#comments" rel="replies" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/12/maitriser-la-complexite/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Maîtriser la complexité</title>
    <summary xml:lang="en">Je reviens tout juste de la réunion annuelle du Forum économique mondial, à Davos. Durant ces quelques jours, je me suis attaché à faire comprendre que la science devrait occuper dans l’agenda politique et économique une place bien plus importante qu’elle ne le fait actuellement. C’est la deuxième fois seulement que je participe au Forum, [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Je reviens tout juste de la réunion annuelle du Forum économique mondial, à Davos. Durant ces quelques jours, je me suis attaché à faire comprendre que la science devrait occuper dans l’agenda politique et économique une place bien plus importante qu’elle ne le fait actuellement. C’est la deuxième fois seulement que je participe au Forum, mais j’ai l’impression que le message commence à être entendu. Cette année, j’ai insisté sur le fait qu’il est important d’établir des liens plus étroits entre les questions scientifiques évoquées au cours de la réunion et les discussions politiques, et je m’efforcerai de promouvoir cette idée en vue de la prochaine réunion du Forum.</p>
<p>La science est un sujet complexe. C’est ainsi. Mais il est essentiel que chacun l’aborde de manière constructive. C’est particulièrement vrai pour les hommes politiques et les chefs d’entreprise présents à Davos, dont les décisions en rapport avec des questions scientifiques peuvent influencer bien des choses, du bien-être de nos enfants à l’avenir de la planète. Il est fondamental que ces décisions soient prises de manière informée et rationnelle.</p>
<p>Le défi pour la science, c’est que nous vivons dans un monde où l’on se doit de connaître Shakespeare, Molière ou Goethe, mais où l’on peut avouer sans honte ne rien savoir de Faraday, de Pasteur ou d’Einstein. Cela n’a pas toujours été le cas et les choses pourraient être différentes. Aujourd’hui, la tendance est à l’indifférence, voire à l’hostilité envers la science. C’est une tendance dangereuse pour tous, et il est du devoir de la communauté scientifique d’y remédier.</p>
<p>Il n’y a encore pas si longtemps, la science faisait partie intégrante de la société. Elle faisait la une des journaux et on en parlait autant que des matches de football. Au début du XX<sup>e</sup> siècle, les découvertes d’Einstein étaient illustrées par des dessins de presse, et, dans les années 60, la science envahissait l’imaginaire populaire, en grande partie grâce au programme Apollo de la NASA. Mais, déjà, l’écart entre la science et la société se creusait, et cette tendance n’a fait que s’accentuer, laissant la société mal préparée pour prendre des décisions fondées scientifiquement.</p>
<p>Le changement climatique et l’énergie sont les deux grands défis auxquels la société doit aujourd’hui faire face. Ce sont là deux questions scientifiques et politiques extrêmement complexes. Le climat est en train de changer. Cela ne fait aucun doute, tout comme le fait que l’activité humaine y est pour quelque chose. Et pourtant, dans la sphère publique, la question reste débattue De la même façon, on ne peut que constater que les énergies renouvelables ne suffisent pas à l’heure actuelle pour satisfaire les besoins toujours croissants de la planète. Cela ne veut pas dire qu’elles n’ont pas leur place. Bien au contraire, et cette place prendra de l’ampleur au fil des ans. Mais il faudra du temps avant de pouvoir répondre à la demande. La société est-elle armée pour prendre les difficiles décisions qui s’imposent sur des questions d’importance planétaire comme celles-ci ? Je ne le pense pas.</p>
<p>Sur le plan individuel, un grand nombre de sujets laissent les citoyens perplexes, ce qui les amène à prendre des décisions en étant mal informés ; des décisions qui sont littéralement d’importance vitale : cela peut concerner la maladie de la vache folle, la peur du vaccin ROR, l’innocuité des téléphones portables, pour ne citer que ces quelques exemples.</p>
<p>Au CERN également nous avons bien sûr expérimenté ce phénomène. Lorsque le LHC a démarré en 2008, le monde a eu peur du trou noir. Une poignée d’individus prétendaient que notre accélérateur vedette allait créer un trou noir qui engloutirait notre planète. L’idée s’est répandue sur les réseaux sociaux et a été également largement reprise dans les médias traditionnels, dont un grand nombre ont cédé à la facilité, laissant de côté le code d’éthique journalistique et préférant exploiter l’aspect grotesque du scénario. Malheureusement, la science a trop longtemps négligé la société, et nombreux sont ceux qui n’ont pu voir tout ce que cela avait de risible. On a même signalé que des écoles avaient fermé le jour de l’inauguration de la machine pour permettre aux enfants d’être auprès de leurs parents, au cas où. Et tout cela, sur le témoignage d’un homme qui, interrogé à la télévision, a expliqué que, puisque le LHC allait peut-être détruire l’Univers, ou peut-être pas, la probabilité d’assister à un désastre était d’une chance sur deux. On pourrait en rire, si ce n’était pas si dramatique.</p>
<p>Que peuvent faire les scientifiques ? Selon moi, bien des choses Sur le plan institutionnel, des changements s’amorcent. Dans la toute nouvelle <em>Blavatnik School of Government</em> de l’Université d’Oxford, par exemple, la science fait partie intégrante des cours de politique publique. Nous devons utiliser des projets scientifiques passionnants comme le LHC pour amener les gens à s’intéresser à la science, pas uniquement par des articles scientifiques, mais aussi via de nouveaux canaux, comme le programme de résidence artistique qui vient d’être lancé au CERN. Et les scientifiques qui ont de l’influence doivent utiliser cette influence pour façonner le débat politique dans les capitales et dans des endroits comme Davos.</p>
<p>Depuis plusieurs années, le CERN privilégie l’ouverture, profitant de la mise en lumière du LHC pour dialoguer davantage avec le plus grand nombre (décideurs, population locale, grand public). Nos activités sont ainsi traitées de manière responsable et recommencent à faire la une des médias et à être suivies par le grand public. Parfois, les faits ne sont pas relatés exactement comme nous le voudrions, mais il est question de science, et c’est là l’essentiel.</p>
<p>Lorsque le LHC a démarré, le monde a continué d’exister, et un journal au moins n’a pas hésité à dire que le LHC serait le nouvel Apollo et conduirait toute une génération à s’intéresser à la science. Bien sûr, ce n’est pas à prendre au pied de la lettre, mais ce genre de commentaire a un effet positif. Plus récemment, un autre journal indiquait que la physique possède ce petit quelque chose en plus, cette qualité insaisissable qui le met dans l’air du temps.</p>
<p>La science dans son ensemble doit en profiter et faire en sorte que l’intérêt pour le LHC ne soit pas un simple feu de paille médiatique, et que les échanges avec le grand public se poursuivent. En tant que scientifiques, nous le devons à la planète. Nous devons aider les gens à maîtriser la complexité de leur vie quotidienne, qui dépend de questions scientifiques. Dans douze mois, c’est le message que je transmettrai à Davos.</p>
<p>Rolf Heuer</p></div>
    </content>
    <updated>2012-02-12T10:08:37Z</updated>
    <published>2012-02-12T10:08:37Z</published>
    <category scheme="http://www.quantumdiaries.org" term="Latest Posts"/>
    <author>
      <name>CERN (Francais)</name>
    </author>
    <source>
      <id>http://www.quantumdiaries.org/feed/atom/</id>
      <link href="http://www.quantumdiaries.org" rel="alternate" type="text/html"/>
      <link href="http://www.quantumdiaries.org/feed/atom/" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">Thoughts on work and life from particle physicists from around the world.</subtitle>
      <title xml:lang="en">Quantum Diaries</title>
      <updated>2012-02-14T16:23:31Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-10448119.post-8305550044079145771</id>
    <link href="http://hoggresearch.blogspot.com/feeds/8305550044079145771/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/publishing-implementations.html#comment-form" rel="replies" title="4 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/8305550044079145771" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/8305550044079145771" rel="self" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/publishing-implementations.html" rel="alternate" title="publishing implementations" type="text/html"/>
    <title>publishing implementations</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Foreman-Mackey and I got very close today to finishing a note for arXiv on his super-fast, parallel, ensemble sampler that we have been using in a range of projects (see recent papers by Lang and Bovy).  We will put it up as an arXiv-only paper, which is something I love to do.  But the fact that this is not a typical or normal kind of publication—for example, there is nowhere that it could appear in the peer-reviewed literature—is crazy:  A great implementation of a good algorithm that enables lots of science is itself an extremely important contribution to science, just like a telescope or a camera or a spectrograph.  How can we make these things count like publications?  And how can we change the language we all use that separates these contributions out into categories that are always contrasted with the category "science"?  Enough spouting; watch the arXiv this week for some block-busting code.</p><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/10448119-8305550044079145771?l=hoggresearch.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-12T02:40:45Z</updated>
    <published>2012-02-12T02:39:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="telescope"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="sample"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="code"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="MCMC"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="literature"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="writing"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="politics"/>
    <author>
      <name>Hogg</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/18398397408280534592</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-10448119</id>
      <category term="Willman 1"/>
      <category term="clustering"/>
      <category term="merging"/>
      <category term="galaxy"/>
      <category term="PHAT"/>
      <category term="HMF"/>
      <category term="proper motion"/>
      <category term="amateur"/>
      <category term="sdss"/>
      <category term="LSST"/>
      <category term="virtual observatory"/>
      <category term="tractor"/>
      <category term="robot"/>
      <category term="funding"/>
      <category term="telescope"/>
      <category term="digital camera"/>
      <category term="meta data"/>
      <category term="proposal"/>
      <category term="disk"/>
      <category term="fundamental astronomy"/>
      <category term="roweis"/>
      <category term="classification"/>
      <category term="practice"/>
      <category term="decision"/>
      <category term="travel"/>
      <category term="linear algebra"/>
      <category term="interstellar medium"/>
      <category term="web 2.0"/>
      <category term="email"/>
      <category term="bayes"/>
      <category term="scattering"/>
      <category term="atlas"/>
      <category term="quasar"/>
      <category term="confusion"/>
      <category term="minor planet"/>
      <category term="anthropology"/>
      <category term="gravitational lensing"/>
      <category term="reading"/>
      <category term="black hole"/>
      <category term="visualization"/>
      <category term="halo"/>
      <category term="cosmology"/>
      <category term="seminar"/>
      <category term="information"/>
      <category term="2mass"/>
      <category term="chemistry"/>
      <category term="HST"/>
      <category term="gravity"/>
      <category term="panstarrs"/>
      <category term="philosophy"/>
      <category term="experiment"/>
      <category term="WMAP"/>
      <category term="sample"/>
      <category term="baryon acoustic feature"/>
      <category term="radial velocity"/>
      <category term="ukidss"/>
      <category term="dark sector"/>
      <category term="parallax"/>
      <category term="spectroscopy"/>
      <category term="brown dwarf"/>
      <category term="LTFDFCF"/>
      <category term="kinematics"/>
      <category term="cosmography"/>
      <category term="transparency"/>
      <category term="flickr"/>
      <category term="calibration"/>
      <category term="optimization"/>
      <category term="editing"/>
      <category term="star formation"/>
      <category term="ultraviolet"/>
      <category term="statistics"/>
      <category term="testing"/>
      <category term="correlation"/>
      <category term="galex"/>
      <category term="intergalactic medium"/>
      <category term="noise"/>
      <category term="computing"/>
      <category term="dissertation"/>
      <category term="citizen science"/>
      <category term="nasa"/>
      <category term="planet"/>
      <category term="wise"/>
      <category term="talking"/>
      <category term="spitzer"/>
      <category term="cluster"/>
      <category term="CDM"/>
      <category term="astrometry"/>
      <category term="environment"/>
      <category term="imaging"/>
      <category term="press"/>
      <category term="MCMC"/>
      <category term="gaia"/>
      <category term="evolution"/>
      <category term="primus"/>
      <category term="compression"/>
      <category term="phase space"/>
      <category term="relativity"/>
      <category term="weapons"/>
      <category term="archive"/>
      <category term="Solar System"/>
      <category term="Milky Way"/>
      <category term="code"/>
      <category term="observing"/>
      <category term="learning"/>
      <category term="point-spread function"/>
      <category term="Euclid"/>
      <category term="hardware"/>
      <category term="catalog"/>
      <category term="science"/>
      <category term="database"/>
      <category term="thinking"/>
      <category term="gamma-ray burst"/>
      <category term="exoplanet"/>
      <category term="white dwarf"/>
      <category term="theory"/>
      <category term="hipparcos"/>
      <category term="radio"/>
      <category term="law"/>
      <category term="pulsar"/>
      <category term="Gaussian process"/>
      <category term="osss"/>
      <category term="politics"/>
      <category term="meeting"/>
      <category term="photometry"/>
      <category term="star"/>
      <category term="not research"/>
      <category term="API"/>
      <category term="cosmic ray"/>
      <category term="substructure"/>
      <category term="post-starburst"/>
      <category term="archetype"/>
      <category term="life"/>
      <category term="time"/>
      <category term="literature"/>
      <category term="dynamics"/>
      <category term="comet"/>
      <category term="anthropic"/>
      <category term="supernova"/>
      <category term="Earth"/>
      <category term="PTF"/>
      <category term="Fermi"/>
      <category term="search"/>
      <category term="usno-b"/>
      <category term="mathematics"/>
      <category term="dust"/>
      <category term="coffee"/>
      <category term="project management"/>
      <category term="model"/>
      <category term="data"/>
      <category term="writing"/>
      <author>
        <name>Hogg</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/18398397408280534592</uri>
      </author>
      <link href="http://hoggresearch.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://hoggresearch.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>galaxies, stellar dynamics, exoplanets, and fundamental astronomy</subtitle>
      <title>Hogg's Research</title>
      <updated>2012-02-14T20:52:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/catdynamics/2012/02/udi.php</id>
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/VzBMyhwCA7M/udi.php" rel="alternate" type="text/html"/>
    <title>UDI?</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
<a href="http://scienceblogs.com/catdynamics/upload/2012/02/udi/OldMain.jpg"><br/>
<img alt="OldMain.jpg" height="240" src="http://scienceblogs.com/catdynamics/upload/2012/02/udi/OldMain.jpg" width="320"/><br/>
Something missing...</a></p> <a href="http://scienceblogs.com/catdynamics/2012/02/udi.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/VzBMyhwCA7M" width="1"/></div>
    </summary>
    <updated>2012-02-11T22:53:04Z</updated>
    <category term="academia"/>
    <source>
      <id>http://scienceblogs.com/catdynamics/</id>
      <author>
        <name>Steinn Sigurðsson</name>
      </author>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Speculations on astronomy, astrophysics, news I find interesting, theoretical issues, science and science policy.  
I will digress into computational physics, science fiction and general issues and basically whatever I feel like whenever. 
And, of course, cats.</subtitle>
      <title>Dynamics of Cats</title>
      <updated>2012-02-14T17:08:27Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.science20.com/86861 at http://www.science20.com</id>
    <link href="http://www.science20.com/quantum_diaries_survivor/blog/sticks_and_stones_may_break_your_bones_words_will_really_put_you_trouble-86861" rel="alternate" type="text/html"/>
    <title>Sticks and Stones May Break Your Bones, But Words Will Really Put You In Trouble</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">That is what Hamza Kashgari, a 23 years old reporter and poet from Saudi Arabia, is realizing the hard way. He used twitter to write a poetic "dialogue" with prophet Muhammad, and this was enough to get him condemned to death by the salafi sheikhs. Hamza tried to escape, but was arrested in Malaysia. He now risks beheading for his words.

<br/>

<p><a href="http://www.science20.com/quantum_diaries_survivor/blog/sticks_and_stones_may_break_your_bones_words_will_really_put_you_trouble-86861" target="_blank">read more</a></p></div>
    </summary>
    <updated>2012-02-11T22:40:35Z</updated>
    <category scheme="http://www.science20.com/random_thoughts" term="Random Thoughts"/>
    <author>
      <name>dorigo</name>
    </author>
    <source>
      <id>http://www.science20.com/quantum_diaries_survivor</id>
      <link href="http://www.science20.com/quantum_diaries_survivor" rel="alternate" type="text/html"/>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor/feed" rel="self" type="application/rss+xml"/>
      <subtitle>Science 2.0® - Science for the next 2,000 years</subtitle>
      <title>dorigo's blog</title>
      <updated>2012-02-15T04:45:03Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://terrytao.wordpress.com/?p=5645</id>
    <link href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/" rel="alternate" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#comments" rel="replies" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">254B, Notes 4: The Bourgain-Gamburd expansion machine</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">We have now seen two ways to construct expander Cayley graphs . The first, discussed in Notes 2, is to use Cayley graphs that are projections of an infinite Cayley graph on a group with Kazhdan’s property (T). The second, discussed in Notes 3, is to combine a quasirandomness property of the group with a [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5645&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>
 We have now seen two ways to construct expander Cayley graphs <img alt="{Cay(G,S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28G%2CS%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(G,S)}"/>. The first, discussed in <a href="http://terrytao.wordpress.com/2011/12/06/254b-notes-2-cayley-graphs-and-kazhdans-property-t/">Notes 2</a>, is to use Cayley graphs that are projections of an infinite Cayley graph on a group with Kazhdan’s property (T). The second, discussed in <a href="http://terrytao.wordpress.com/2011/12/16/254b-notes-3-quasirandom-groups-expansion-and-selbergs-316-theorem/">Notes 3</a>, is to combine a quasirandomness property of the group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> with a flattening hypothesis for the random walk.
</p>
<p>
We now pursue the second approach more thoroughly. The main difficulty here is to figure out how to ensure flattening of the random walk, as it is then an easy matter to use quasirandomness to show that the random walk becomes mixing soon after it becomes flat. In the case of Selberg’s theorem, we achieved this through an explicit formula for the heat kernel on the hyperbolic plane (which is a proxy for the random walk). However, in most situations such an explicit formula is not available, and one must develop some other tool for forcing flattening, and specifically an estimate of the form <a name="muflat">
</a></p><p align="center"><a name="muflat"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \ll |G|^{-1/2+\epsilon} \ \ \ \ \ (1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cll+%7CG%7C%5E%7B-1%2F2%2B%5Cepsilon%7D+%5C+%5C+%5C+%5C+%5C+%281%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \ll |G|^{-1/2+\epsilon} \ \ \ \ \ (1)"/></a></p><a name="muflat">
</a><p><a name="muflat"/> for some <img alt="{n = O(\log |G|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+O%28%5Clog+%7CG%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = O(\log |G|)}"/>, where <img alt="{\mu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu}"/> is the uniform probability measure on the generating set <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/>.
</p>
<p>
In 2006, <a href="http://www.ams.org/mathscinet-getitem?mr=2227746">Bourgain and Gamburd</a> introduced a general method for achieving this goal. The intuition here is that the main obstruction that prevents a random walk from spreading out to become flat over the entire group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> is if the random walk gets <em>trapped</em> in some proper subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> (or perhaps in some coset <img alt="{xH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BxH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{xH}"/> of such a subgroup), so that <img alt="{\mu^{(n)}(xH)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%28xH%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}(xH)}"/> remains large for some moderately large <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>. Note that </p>
<p align="center"><img alt="\displaystyle  \mu^{(2n)}(H) \geq \mu^{(n)}(H x^{-1}) \mu^{(n)}(xH) = \mu^{(n)}(xH)^2," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%282n%29%7D%28H%29+%5Cgeq+%5Cmu%5E%7B%28n%29%7D%28H+x%5E%7B-1%7D%29+%5Cmu%5E%7B%28n%29%7D%28xH%29+%3D+%5Cmu%5E%7B%28n%29%7D%28xH%29%5E2%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(2n)}(H) \geq \mu^{(n)}(H x^{-1}) \mu^{(n)}(xH) = \mu^{(n)}(xH)^2,"/></p>
<p> since <img alt="{\mu^{(2n)} = \mu^{(n)} * \mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%282n%29%7D+%3D+%5Cmu%5E%7B%28n%29%7D+%2A+%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(2n)} = \mu^{(n)} * \mu^{(n)}}"/>, <img alt="{H = (H x^{-1}) \cdot (xH)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3D+%28H+x%5E%7B-1%7D%29+%5Ccdot+%28xH%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H = (H x^{-1}) \cdot (xH)}"/>, and <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> is symmetric. By iterating this observation, we seethat if <img alt="{\mu^{(n)}(xH)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%28xH%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}(xH)}"/> is too large (e.g. of size <img alt="{|G|^{-o(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%5E%7B-o%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|^{-o(1)}}"/> for some <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> comparable to <img alt="{\log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\log |G|}"/>), then it is not possible for the random walk <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> to converge to the uniform distribution in time <img alt="{O(\log |G|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%5Clog+%7CG%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(\log |G|)}"/>, and so expansion does not occur.</p>
<p>
A potentially more general obstruction of this type would be if the random walk gets trapped in (a coset of) an <em>approximate</em> group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>. Recall that a <em><img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate group</em> is a subset <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of a group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> which is symmetric, contains the identity, and is such that <img alt="{H \cdot H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%5Ccdot+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H \cdot H}"/> can be covered by at most <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> left-translates (or equivalently, right-translates) of <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>. Such approximate groups were studied extensively in last quarter’s course. A similar argument to the one given previously shows (roughly speaking) that expansion cannot occur if <img alt="{\mu^{(n)}(xH)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%28xH%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}(xH)}"/> is too large for some coset <img alt="{xH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BxH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{xH}"/> of an approximate group.
</p>
<p>
It turns out that this latter observation has a converse: if a measure does not concentrate in cosets of approximate groups, then some flattening occurs. More precisely, one has the following combinatorial lemma:
</p>
<blockquote><p><b>Lemma 1 (Weighted Balog-Szemerédi-Gowers lemma)</b> <a name="bsg"/> Let <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> be a group, let <img alt="{\mu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu}"/> be a finitely supported probability measure on <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> which is symmetric (thus <img alt="{\nu(g)=\nu(g^{-1})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%28g%29%3D%5Cnu%28g%5E%7B-1%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu(g)=\nu(g^{-1})}"/> for all <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>), and let <img alt="{K \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 1}"/>. Then one of the following statements hold: </p>
<ul>
<li>(i) (Flattening) One has <img alt="{\| \nu * \nu \|_{\ell^2(G)} \leq \frac{1}{K} \|\nu\|_{\ell^2(G)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C+%5Cnu+%2A+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%5Cfrac%7B1%7D%7BK%7D+%5C%7C%5Cnu%5C%7C_%7B%5Cell%5E2%28G%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\| \nu * \nu \|_{\ell^2(G)} \leq \frac{1}{K} \|\nu\|_{\ell^2(G)}}"/>. </li>
<li>(ii) (Concentration in an approximate group) There exists an <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> in <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> with <img alt="{|H| \ll K^{O(1)} / \| \nu \|_{\ell^2(G)}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cll+K%5E%7BO%281%29%7D+%2F+%5C%7C+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \ll K^{O(1)} / \| \nu \|_{\ell^2(G)}^2}"/> and an element <img alt="{x \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in G}"/> such that <img alt="{\nu(xH) \gg K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%28xH%29+%5Cgg+K%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu(xH) \gg K^{-O(1)}}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
This lemma is a variant of the more well-known <em>Balog-Szemerédi-Gowers lemma</em> in additive combinatorics <a href="http://www.ams.org/mathscinet-getitem?mr=1631259">due to Gowers</a> (which roughly speaking corresponds to the case when <img alt="{\mu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu}"/> is the uniform distribution on some set <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>), which in turn is a polynomially quantitative version of an earlier lemma of <a href="http://www.ams.org/mathscinet-getitem?mr=1305895">Balog and Szemerédi</a>. We will prove it below the fold.
</p>
<p>
The lemma is particularly useful when the group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> in question enjoys a <em>product theorem</em>, which roughly speaking says that the only medium-sized approximate subgroups of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> are trapped inside genuine proper subgroups of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> (or, contrapositively, medium-sized sets that generate the entire group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> cannot be approximate groups). The fact that some finite groups (and specifically, the bounded rank finite simple groups of Lie type) enjoy product theorems is a non-trivial fact, and will be discussed in later notes. For now, we simply observe that the presence of the product theorem, together with quasirandomness and a non-concentration hypothesis, can be used to demonstrate expansion:
</p>
<blockquote><p><b>Theorem 2 (Bourgain-Gamburd expansion machine)</b> <a name="bourgain"/> Suppose that <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> is a finite group, that <img alt="{S \subseteq G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS+%5Csubseteq+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S \subseteq G}"/> is a symmetric set of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> generators, and that there are constants <img alt="{0 &lt; \kappa &lt; 1 &lt; \Lambda}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%3C+%5Ckappa+%3C+1+%3C+%5CLambda%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 &lt; \kappa &lt; 1 &lt; \Lambda}"/> with the following properties. </p>
<ol>
<li> (Quasirandomness). The smallest dimension of a nontrivial representation <img alt="{\rho: G \rightarrow GL_d({\bf C})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Crho%3A+G+%5Crightarrow+GL_d%28%7B%5Cbf+C%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\rho: G \rightarrow GL_d({\bf C})}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> is at least <img alt="{|G|^{\kappa}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%5E%7B%5Ckappa%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|^{\kappa}}"/>; </li>
<li> (Product theorem). For all <img alt="{\delta &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cdelta+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\delta &gt; 0}"/> there is some <img alt="{\delta' = \delta'(\delta) &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cdelta%27+%3D+%5Cdelta%27%28%5Cdelta%29+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\delta' = \delta'(\delta) &gt; 0}"/> such that the following is true. If <img alt="{H \subseteq G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%5Csubseteq+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H \subseteq G}"/> is a <img alt="{|G|^{\delta'}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%5E%7B%5Cdelta%27%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|^{\delta'}}"/>-approximate subgroup with <img alt="{|G|^{\delta} \leq |H| \leq |G|^{1 - \delta}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%5E%7B%5Cdelta%7D+%5Cleq+%7CH%7C+%5Cleq+%7CG%7C%5E%7B1+-+%5Cdelta%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|^{\delta} \leq |H| \leq |G|^{1 - \delta}}"/> then <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> generates a proper subgroup of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>; </li>
<li> (Non-concentration estimate). There is some even number <img alt="{n \leq \Lambda\log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cleq+%5CLambda%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \leq \Lambda\log |G|}"/> such that
<p align="center"><img alt="\displaystyle  \sup_{H &lt; G}\mu^{(n)}(H) &lt; |G|^{-\kappa}," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7BH+%3C+G%7D%5Cmu%5E%7B%28n%29%7D%28H%29+%3C+%7CG%7C%5E%7B-%5Ckappa%7D%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{H &lt; G}\mu^{(n)}(H) &lt; |G|^{-\kappa},"/></p>
<p> where the supremum is over all proper subgroups <img alt="{H &lt; G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3C+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H &lt; G}"/>.
</p></li>
</ol>
<p> Then <img alt="{Cay(G,S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28G%2CS%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(G,S)}"/> is a two-sided <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for some <img alt="{\epsilon &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon &gt; 0}"/> depending only on <img alt="{k,\kappa, \Lambda}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C%5Ckappa%2C+%5CLambda%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k,\kappa, \Lambda}"/>, and the function <img alt="{\delta'(\cdot )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cdelta%27%28%5Ccdot+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\delta'(\cdot )}"/> (and this constant <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> is in principle computable in terms of these constants). </p></blockquote>
<p/>
<p>
This criterion for expansion is implicitly contained in <a href="http://www.ams.org/mathscinet-getitem?mr=2415383">this paper of Bourgain and Gamburd</a>, who used it to establish the expansion of various Cayley graphs in <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> for prime <img alt="{p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{p}"/>. This criterion has since been applied (or modified) to obtain expansion results in many other groups, as will be discussed in later notes.
</p>
<p>
<span id="more-5645"/>
</p>
<p/>
<p align="center"><b> —  1. The Balog-Szemerédi-Gowers lemma  — </b></p>
<p>
The Balog-Szemerédi-Gowers lemma (Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bsg">1</a>) is ostensibly a statement about group structure, but the main tool in its proof is a remarkable graph-theoretic lemma (also known as the Balog-Szemerédi-Gowers lemma) that allows one to upgrade a “statistical” structure (a structure which is only valid a small fraction of the time, say 1% of the time) to a “complete” structure (one which is valid 100% of the time), by shrinking the size of the structure slightly (and in particular, with losses of polynomial type, as opposed to exponential or worse). This is in contrast to other structure-improving results (such as <a href="http://en.wikipedia.org/wiki/Ramsey's_theorem">Ramsey’s theorem</a>, <a href="http://en.wikipedia.org/wiki/Szemer%C3%A9di%27s_theorem">Szemerédi’s theorem</a>, or <a href="http://en.wikipedia.org/wiki/Freiman's_theorem">Freiman’s theorem</a>), which are qualitatively similar in spirit, but have much worse quantitative bounds (though <a href="http://terrytao.wordpress.com/2007/03/11/ben-green-the-polynomial-freiman-ruzsa-conjecture/">there is some hope</a> in the case of Freiman’s theorem to only lose polynomial bounds with some improvement of existing arguments).
</p>
<p>
As we shall see later, the property of <img alt="{\|\nu*\nu\|_{\ell^2(G)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C%5Cnu%2A%5Cnu%5C%7C_%7B%5Cell%5E2%28G%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|\nu*\nu\|_{\ell^2(G)}}"/> being large is a statistical assertion about <img alt="{\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu}"/> (it asserts that <img alt="{\nu*\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%2A%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu*\nu}"/> collides with itself somewhat often), whereas approximate groups <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> represent a more complete sort of structure (<em>all</em> products of <img alt="{H \cdot H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%5Ccdot+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H \cdot H}"/> are trapped in a small set, whereas only <em>many</em> of the products in <img alt="{\nu * \nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu+%2A+%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu * \nu}"/> are so constrained). The graph-theoretic Balog-Szemerédi lemma is the key to moving from the former type of structure to the latter with only polynomial losses.
</p>
<p>
We need some notation. Define a <em>bipartite graph</em> <img alt="{G = G(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3D+G%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G = G(A,B,E)}"/> to be a graph whose vertex set <img alt="{V := A \cup B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV+%3A%3D+A+%5Ccup+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V := A \cup B}"/> is partitioned into two non-empty sets <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/>, and the edge set <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> consists only of edges between <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. If a finite bipartite graph <img alt="{G = G(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3D+G%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G = G(A,B,E)}"/> is <em>dense</em> in the sense that its edge density <img alt="{|E|/|A||B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C%2F%7CA%7C%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E|/|A||B|}"/> is large, then for many vertices <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/> and <img alt="{b \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B}"/>, <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> are connected by a path of length one (i.e. an edge). It is thus intuitive that many pairs of vertices <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/> and <img alt="{a' \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a' \in A}"/> will be connected by many paths of length two. Perhaps surprisingly, one can upgrade “many pairs” here to “almost all pairs”, provided that one is willing to shrink the set <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> slightly. More precisely, one has
</p>
<blockquote><p><b>Lemma 3 (Balog-Szemerédi-Gowers lemma: paths of length two)</b> <a name="two-path"/> Let <img alt="{G(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G(A,B,E)}"/> be a finite bipartite graph with <img alt="{|E| \geq |A| |B| / K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cgeq+%7CA%7C+%7CB%7C+%2F+K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \geq |A| |B| / K}"/>. Let <img alt="{\epsilon &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon &gt; 0}"/>. Then there exists a subset <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> with <img alt="{|A'| \geq \frac{|A|}{\sqrt{2} K}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgeq+%5Cfrac%7B%7CA%7C%7D%7B%5Csqrt%7B2%7D+K%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \geq \frac{|A|}{\sqrt{2} K}}"/> such that at least <img alt="{(1-\epsilon)|A'|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%281-%5Cepsilon%29%7CA%27%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(1-\epsilon)|A'|^2}"/> of the pairs <img alt="{(a,a') \in A' \times A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29+%5Cin+A%27+%5Ctimes+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a') \in A' \times A'}"/> are such that <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/> are connected by at least <img alt="{\frac{\epsilon}{2K^2} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%5Cepsilon%7D%7B2K%5E2%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{\epsilon}{2K^2} |B|}"/> paths of length two (i.e. there exists at least <img alt="{\frac{\epsilon}{2K^2} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%5Cepsilon%7D%7B2K%5E2%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{\epsilon}{2K^2} |B|}"/> vertices <img alt="{b \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B}"/> such that <img alt="{\{a,b\}, \{a',b\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7Ba%2Cb%5C%7D%2C+%5C%7Ba%27%2Cb%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{a,b\}, \{a',b\}}"/> both lie in <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/>). </p></blockquote>
<p/>
<blockquote><p><b>Remark 1</b>  It is not possible to remove the <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> entirely from this lemma; see Exercise 6.4.2 of <a href="http://www.ams.org/mathscinet-getitem?mr=2289012">my book with Van Vu</a> for a counterexample (involving Hamming balls). </p></blockquote>
<p/>
<p>
<em>Proof:</em>  The idea here is to use a probabilistic construction, picking <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> to be a neighbourhood of a randomly selected element <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. The rationale here is that if a pair <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/> of vertices in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> are not connected by many paths of length two, then they are unlikely to lie in the same neighbourhood, and so are unlikely to “wreck” the construction.
</p>
<p>
We turn to the details. Let <img alt="{b \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B}"/> be chosen uniformly at random, and let <img alt="{A' := \{ a \in A: (a,b) \in E \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%3A%3D+%5C%7B+a+%5Cin+A%3A+%28a%2Cb%29+%5Cin+E+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' := \{ a \in A: (a,b) \in E \}}"/> be the neighbourhood of <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/>. Observe that the expected size of <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> is </p>
<p align="center"><img alt="\displaystyle {\bf E} |A'| = \frac{1}{|B|} |E| \geq \frac{|A|}{K}. " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%7B%5Cbf+E%7D+%7CA%27%7C+%3D+%5Cfrac%7B1%7D%7B%7CB%7C%7D+%7CE%7C+%5Cgeq+%5Cfrac%7B%7CA%7C%7D%7BK%7D.+&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle {\bf E} |A'| = \frac{1}{|B|} |E| \geq \frac{|A|}{K}. "/></p>
<p> By Cauchy-Schwarz, we conclude in particular that <a name="ap-size">
</a></p><p align="center"><a name="ap-size"><img alt="\displaystyle  {\bf E} |A'|^2 \geq \frac{|A|^2}{K^2}. \ \ \ \ \ (2)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7B%5Cbf+E%7D+%7CA%27%7C%5E2+%5Cgeq+%5Cfrac%7B%7CA%7C%5E2%7D%7BK%5E2%7D.+%5C+%5C+%5C+%5C+%5C+%282%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  {\bf E} |A'|^2 \geq \frac{|A|^2}{K^2}. \ \ \ \ \ (2)"/></a></p><a name="ap-size">
</a><p><a name="ap-size"/></p>
<p>
Now, call a pair <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> <em>bad</em> if it is connected by fewer than <img alt="{\frac{\epsilon |B|}{2K^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%5Cepsilon+%7CB%7C%7D%7B2K%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{\epsilon |B|}{2K^2}}"/> paths of length two, and let <img alt="{N}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{N}"/> be the number of bad pairs <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> in <img alt="{A' \times A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%5Ctimes+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' \times A'}"/>. We consider the quantity <img alt="{{\bf E} N}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+E%7D+N%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf E} N}"/>. Observe that if <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> is a bad pair in <img alt="{A \times A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ctimes+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \times A}"/>, then there are at most <img alt="{\frac{\epsilon |B|}{2K^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%5Cepsilon+%7CB%7C%7D%7B2K%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{\epsilon |B|}{2K^2}}"/> values of <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> for which <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'}"/> will both lie in <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/>, and so this bad pair contributes at most <img alt="{\frac{\epsilon}{2K^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%5Cepsilon%7D%7B2K%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{\epsilon}{2K^2}}"/> to the expectation. Since there are at most <img alt="{|A|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^2}"/> bad pairs, we conclude that </p>
<p align="center"><img alt="\displaystyle  {\bf E} N \leq \frac{\epsilon |A|^2}{2K^2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7B%5Cbf+E%7D+N+%5Cleq+%5Cfrac%7B%5Cepsilon+%7CA%7C%5E2%7D%7B2K%5E2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  {\bf E} N \leq \frac{\epsilon |A|^2}{2K^2}."/></p>
<p> Combining this with <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#ap-size">(2)</a>, we see that
</p><p align="center"><img alt="\displaystyle  {\bf E} |A'|^2 - \frac{N}{\epsilon} - \frac{|A|^2}{2K^2} \geq 0." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7B%5Cbf+E%7D+%7CA%27%7C%5E2+-+%5Cfrac%7BN%7D%7B%5Cepsilon%7D+-+%5Cfrac%7B%7CA%7C%5E2%7D%7B2K%5E2%7D+%5Cgeq+0.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  {\bf E} |A'|^2 - \frac{N}{\epsilon} - \frac{|A|^2}{2K^2} \geq 0."/></p>
<p> In particular, there exists a choice of <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> for which the expression on the left-hand side is non-negative. This implies that
</p><p align="center"><img alt="\displaystyle  N \leq \epsilon |A'|^2" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++N+%5Cleq+%5Cepsilon+%7CA%27%7C%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  N \leq \epsilon |A'|^2"/></p>
<p> and
</p><p align="center"><img alt="\displaystyle  |A'|^2 \geq \frac{|A|^2}{2K^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%27%7C%5E2+%5Cgeq+%5Cfrac%7B%7CA%7C%5E2%7D%7B2K%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A'|^2 \geq \frac{|A|^2}{2K^2}"/></p>
<p> and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Given that almost all pairs <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/> in <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> are joined by many paths of length two, it is then plausible that almost all pairs <img alt="{a \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A'}"/>, <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/> are joined by many paths of length three, for some large subset <img alt="{B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B'}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Remarkably, one can now upgrade “almost all” pairs here to <em>all</em> pairs:
</p>
<blockquote><p><b>Lemma 4 (Balog-Szemerédi-Gowers lemma: paths of length three)</b> <a name="three-path"/> Let <img alt="{G(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G(A,B,E)}"/> be a finite bipartite graph with <img alt="{|E| \geq |A| |B| / K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cgeq+%7CA%7C+%7CB%7C+%2F+K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \geq |A| |B| / K}"/>. Then there exists subsets <img alt="{A', B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%2C+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A', B'}"/> of <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> respectively with <img alt="{|A'| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \gg K^{-O(1)} |A|}"/> and <img alt="{|B'| \gg K^{-O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'| \gg K^{-O(1)} |B|}"/>, such that for every <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/> and <img alt="{b \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B}"/>, <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> are joined by <img alt="{\gg K^{-O(1)} |A| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A| |B|}"/> paths of length three. </p></blockquote>
<p/>
<blockquote><p><b>Remark 2</b>  A lemma similar to this was first established <a href="http://www.ams.org/mathscinet-getitem?mr=1305895">by Balog and Szemerédi</a>, as a consequence of the <a href="http://en.wikipedia.org/wiki/Szemer%C3%A9di_regularity_lemma">Szemereédi regularity lemma</a>. However, as a consequence of using that lemma, the polynomial bounds <img alt="{K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^{-O(1)}}"/> in the above lemma had to be replaced by much worse bounds (of tower-exponential type in <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>), which turns out to be far too weak for the purposes of establishing expansion. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  The idea is to first prune a few “unpopular” vertices from <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> and then apply the preceding lemma.
</p>
<p>
Let <img alt="{A_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_1}"/> be the vertices in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of degree at least <img alt="{|B|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B|/2K}"/>, and let <img alt="{E_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E_1}"/> be the edges connecting <img alt="{A_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_1}"/> and <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Note that the vertices in <img alt="{A \backslash A_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Cbackslash+A_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \backslash A_1}"/> are connected to a total of at most <img alt="{|A| |B|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%7CB%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| |B|/2K}"/> edges, and so <img alt="{|E_1| \geq |A| |B|/2K \geq |A_1| |B|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE_1%7C+%5Cgeq+%7CA%7C+%7CB%7C%2F2K+%5Cgeq+%7CA_1%7C+%7CB%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E_1| \geq |A| |B|/2K \geq |A_1| |B|/2K}"/>. Since <img alt="{|E_1| \leq |A_1| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE_1%7C+%5Cleq+%7CA_1%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E_1| \leq |A_1| |B|}"/>, we conclude in particular that <img alt="{|A_1| \ge |A|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA_1%7C+%5Cge+%7CA%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A_1| \ge |A|/2K}"/>.
</p>
<p>
Let <img alt="{\epsilon &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon &gt; 0}"/> be a sufficiently small quantity (depending on <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>) to be chosen later. Applying Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#two-path">3</a>, one can find a subset <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/> of <img alt="{A_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_1}"/> of cardinality <img alt="{|A_2| \gg |A_1|/K \gg |A|/K^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA_2%7C+%5Cgg+%7CA_1%7C%2FK+%5Cgg+%7CA%7C%2FK%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A_2| \gg |A_1|/K \gg |A|/K^2}"/> such that at most <img alt="{\epsilon |A_2|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%7CA_2%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon |A_2|^2}"/> of the pairs <img alt="{(a,a') \in A_2 \times A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29+%5Cin+A_2+%5Ctimes+A_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a') \in A_2 \times A_2}"/> are <em>bad</em> in the sense that they are connected by <img alt="{\gg \epsilon/K^2 |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%5Cepsilon%2FK%5E2+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg \epsilon/K^2 |B|}"/> paths of length two.
</p>
<p>
Let <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> be those vertices <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> in <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/> for which there are at most <img alt="{\sqrt{\epsilon} |A_2|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csqrt%7B%5Cepsilon%7D+%7CA_2%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sqrt{\epsilon} |A_2|}"/> elements <img alt="{a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'}"/> of <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/> for which <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> is bad. By Markov’s inequality, <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> consists of all but at most <img alt="{\sqrt{\epsilon} |A_2|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csqrt%7B%5Cepsilon%7D+%7CA_2%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sqrt{\epsilon} |A_2|}"/> elements of <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/>.
</p>
<p>
Let <img alt="{E_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E_2}"/> be the edges connecting <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/> with <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Since each vertex in <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/> has degree at least <img alt="{|B|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B|/2K}"/>, one has </p>
<p align="center"><img alt="\displaystyle  |E_2| \geq |A_2| |B| / 2K \gg |A| |B| / K^3." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CE_2%7C+%5Cgeq+%7CA_2%7C+%7CB%7C+%2F+2K+%5Cgg+%7CA%7C+%7CB%7C+%2F+K%5E3.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |E_2| \geq |A_2| |B| / 2K \gg |A| |B| / K^3."/></p>
<p> We may thus find a subset <img alt="{B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B'}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> of cardinality <img alt="{|B'| \gg |B|/K^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C+%5Cgg+%7CB%7C%2FK%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'| \gg |B|/K^3}"/> such that each <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/> is adjacent to <img alt="{\gg |A|/K^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%2FK%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|/K^3}"/> elements of <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/>.</p>
<p>
Now let <img alt="{a \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A'}"/> and <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/>. We know that <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> is adjacent to <img alt="{\gg |A|/K^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%2FK%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|/K^3}"/> elements <img alt="{a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'}"/> of <img alt="{A_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2}"/>, and that at most <img alt="{\sqrt{\epsilon} |A_2|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csqrt%7B%5Cepsilon%7D+%7CA_2%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sqrt{\epsilon} |A_2|}"/> of these elements are such that <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> is bad. If we choose <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> to be a sufficiently small multiple of <img alt="{1/K^6}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2FK%5E6%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1/K^6}"/>, we conclude that there are <img alt="{\gg |A|/K^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%2FK%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|/K^3}"/> elements <img alt="{a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'}"/> which are adjacent to <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> and for which <img alt="{(a,a')}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Ca%27%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,a')}"/> is not bad. One thus has <img alt="{\gg (|A|/K^3) (\epsilon/K^2) |B| \gg |A| |B| / K^{11}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%28%7CA%7C%2FK%5E3%29+%28%5Cepsilon%2FK%5E2%29+%7CB%7C+%5Cgg+%7CA%7C+%7CB%7C+%2F+K%5E%7B11%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg (|A|/K^3) (\epsilon/K^2) |B| \gg |A| |B| / K^{11}}"/> paths of length three connecting <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> to <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/>, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
The exponents in <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> here can be improved slightly, but we will not attempt to obtain the optimal numerology here.
</p>
<blockquote><p><b>Remark 3</b>  The above results are analogous to a phenomenon in additive combinatorics, namely that a “1%-structured” set (such as a small density subset of a group) can often be upgraded to a “99%-structured” set (such as the complement of a small density subset of a group) by applying a single “convolution” or “sumset” operation, and then upgraded further to a “100%-structured” set (such as a genuine group) by applying a further convolution or sumset operation. (This is basically why, for instance, it is known that almost all even natural numbers are the sum of two primes, and all but finitely many odd natural numbers are the sum of three primes; but it is not known whether all but finitely many even natural numbers are the sum of two primes.) </p></blockquote>
<p/>
<blockquote><p><b>Exercise 1 (Weighted Balog-Szemerédi-Gowers theorem)</b>  Let <img alt="{(X,\mu)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28X%2C%5Cmu%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(X,\mu)}"/> and <img alt="{(Y,\nu)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28Y%2C%5Cnu%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(Y,\nu)}"/> be probability spaces, and let <img alt="{E \subset X \times Y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE+%5Csubset+X+%5Ctimes+Y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E \subset X \times Y}"/> have measure <img alt="{\mu \times \nu(E) \geq 1/K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu+%5Ctimes+%5Cnu%28E%29+%5Cgeq+1%2FK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu \times \nu(E) \geq 1/K}"/> for some <img alt="{K \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 1}"/>. </p>
<ul>
<li>(i) Show that for any <img alt="{\epsilon &gt; 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon &gt; 0}"/>, there exists a subset <img alt="{X'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BX%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{X'}"/> of <img alt="{X}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{X}"/> of measure <img alt="{\mu(X') \geq \frac{1}{\sqrt{2}K}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%28X%27%29+%5Cgeq+%5Cfrac%7B1%7D%7B%5Csqrt%7B2%7DK%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu(X') \geq \frac{1}{\sqrt{2}K}}"/> such that
<p align="center"><img alt="\displaystyle  \mu \times \mu( \{ (x,x') \in X' \times X': " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu+%5Ctimes+%5Cmu%28+%5C%7B+%28x%2Cx%27%29+%5Cin+X%27+%5Ctimes+X%27%3A+&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu \times \mu( \{ (x,x') \in X' \times X': "/></p>
<p align="center"><img alt="\displaystyle  \int_Y 1_E(x,y) 1_E(x',y)\ d\nu(y) &lt; \frac{\epsilon}{2K^2} \} ) \leq \epsilon \mu(X')^2." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cint_Y+1_E%28x%2Cy%29+1_E%28x%27%2Cy%29%5C+d%5Cnu%28y%29+%3C+%5Cfrac%7B%5Cepsilon%7D%7B2K%5E2%7D+%5C%7D+%29+%5Cleq+%5Cepsilon+%5Cmu%28X%27%29%5E2.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \int_Y 1_E(x,y) 1_E(x',y)\ d\nu(y) &lt; \frac{\epsilon}{2K^2} \} ) \leq \epsilon \mu(X')^2."/></p>
</li>
<li>(ii) Show that there exists subsets <img alt="{X', Y'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BX%27%2C+Y%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{X', Y'}"/> of <img alt="{X,Y}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BX%2CY%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{X,Y}"/> of measure <img alt="{\mu(X') \gg K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%28X%27%29+%5Cgg+K%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu(X') \gg K^{-O(1)}}"/> and <img alt="{\nu(Y') \gg K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%28Y%27%29+%5Cgg+K%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu(Y') \gg K^{-O(1)}}"/> such that
<p align="center"><img alt="\displaystyle  \int_X \int_Y 1_E(x,y') 1_E(x',y') 1_E(x',y)\ d\mu(x') d\nu(y') \gg K^{-O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cint_X+%5Cint_Y+1_E%28x%2Cy%27%29+1_E%28x%27%2Cy%27%29+1_E%28x%27%2Cy%29%5C+d%5Cmu%28x%27%29+d%5Cnu%28y%27%29+%5Cgg+K%5E%7B-O%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \int_X \int_Y 1_E(x,y') 1_E(x',y') 1_E(x',y)\ d\mu(x') d\nu(y') \gg K^{-O(1)}"/></p>
<p> for all <img alt="{x \in X'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+X%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in X'}"/> and <img alt="{y \in Y'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7By+%5Cin+Y%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{y \in Y'}"/>.
</p></li>
</ul>
</blockquote>
<p/>
<blockquote><p><b>Exercise 2 (99% Balog-Szemerédi theorem)</b>  Let <img alt="{G(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G(A,B,E)}"/> be a finite bipartite graph with <img alt="{|E| \geq (1-\epsilon) |A| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cgeq+%281-%5Cepsilon%29+%7CA%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \geq (1-\epsilon) |A| |B|}"/>. </p>
<ul>
<li>(i) Show that there exists a subset <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of size <img alt="{|A'| \geq (1-O(\sqrt{\epsilon})) |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgeq+%281-O%28%5Csqrt%7B%5Cepsilon%7D%29%29+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \geq (1-O(\sqrt{\epsilon})) |A|}"/> such that for every <img alt="{a,a' \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \in A'}"/>, <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a'}"/> are connected by at least <img alt="{(1-O(\sqrt{\epsilon})) |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%281-O%28%5Csqrt%7B%5Cepsilon%7D%29%29+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(1-O(\sqrt{\epsilon})) |B|}"/> paths of length <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>. (<em>Hint:</em> select <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> to be those vertices in <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> that are connected to “almost all” the vertices in <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>.) </li>
<li>(ii) Show that there also exists a subset <img alt="{B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B'}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> of size <img alt="{|B'| \geq (1-O(\sqrt{\epsilon})) |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C+%5Cgeq+%281-O%28%5Csqrt%7B%5Cepsilon%7D%29%29+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'| \geq (1-O(\sqrt{\epsilon})) |B|}"/> such that for every <img alt="{a \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A'}"/> and <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/>, <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> are connected by at least <img alt="{(1-O(\sqrt{\epsilon})) |A| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%281-O%28%5Csqrt%7B%5Cepsilon%7D%29%29+%7CA%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(1-O(\sqrt{\epsilon})) |A| |B|}"/> paths of length <img alt="{3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{3}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
We now apply the graph-theoretic lemma to the group context. The main idea here is to show that various sets (e.g. product sets <img alt="{A \cdot B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccdot+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cdot B}"/>) are small by showing that they are in the high-multiplicity region of some convolution (e.g. <img alt="{1_{A_1} * \ldots * 1_{A_k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_%7BA_1%7D+%2A+%5Cldots+%2A+1_%7BA_k%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_{A_1} * \ldots * 1_{A_k}}"/>), or equivalently that elements <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> of such sets have many representations as a product <img alt="{g = a_1 \ldots a_k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%3D+a_1+%5Cldots+a_k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g = a_1 \ldots a_k}"/> with <img alt="{a_1 \in A_1, \ldots, a_k \in A_k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_1+%5Cin+A_1%2C+%5Cldots%2C+a_k+%5Cin+A_k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_1 \in A_1, \ldots, a_k \in A_k}"/>. One can then use Markov’s inequality and the trivial identity <img alt="{\| 1_{A_1} * \ldots * 1_{A_k} \|_{\ell^1(G)} = |A_1| \ldots |A_k|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C+1_%7BA_1%7D+%2A+%5Cldots+%2A+1_%7BA_k%7D+%5C%7C_%7B%5Cell%5E1%28G%29%7D+%3D+%7CA_1%7C+%5Cldots+%7CA_k%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\| 1_{A_1} * \ldots * 1_{A_k} \|_{\ell^1(G)} = |A_1| \ldots |A_k|}"/> to get usable size bounds on such sets.
</p>
<blockquote><p><b>Corollary 5 (Balog-Szemerédi lemma, product set form)</b> <a name="bsps"/> let <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> be finite non-empty subsets of a group <img alt="{G = (G,\cdot)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3D+%28G%2C%5Ccdot%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G = (G,\cdot)}"/>, and suppose that
</p><p align="center"><img alt="\displaystyle  \|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/4} |B|^{3/4}/K" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C1_A+%2A+1_B+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%7CA%7C%5E%7B3%2F4%7D+%7CB%7C%5E%7B3%2F4%7D%2FK&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/4} |B|^{3/4}/K"/></p>
<p> for some <img alt="{K \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 1}"/>. (This hypothesis should be compared with the upper bound
</p><p align="center"><img alt="\displaystyle  \|1_A * 1_B \|_{\ell^2(G)} \leq \|1_A\|_{\ell^{4/3}(G)} \|1_B\|_{\ell^{4/3}(G)} = |A|^{3/4} |B|^{3/4}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C1_A+%2A+1_B+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%5C%7C1_A%5C%7C_%7B%5Cell%5E%7B4%2F3%7D%28G%29%7D+%5C%7C1_B%5C%7C_%7B%5Cell%5E%7B4%2F3%7D%28G%29%7D+%3D+%7CA%7C%5E%7B3%2F4%7D+%7CB%7C%5E%7B3%2F4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \|1_A * 1_B \|_{\ell^2(G)} \leq \|1_A\|_{\ell^{4/3}(G)} \|1_B\|_{\ell^{4/3}(G)} = |A|^{3/4} |B|^{3/4}"/></p>
<p> arising from Young’s inequality.) Then there exists subsets <img alt="{A', B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%2C+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A', B'}"/> of <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> respectively with <img alt="{|A'| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \gg K^{-O(1)} |A|}"/> and <img alt="{|B'| \gg K^{-O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'| \gg K^{-O(1)} |B|}"/> with <img alt="{|A' \cdot B'| \ll K^{O(1)} |A|^{1/2} |B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27+%5Ccdot+B%27%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A' \cdot B'| \ll K^{O(1)} |A|^{1/2} |B|^{1/2}}"/> and <img alt="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27+%5Ccdot+%28A%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}"/>. </p></blockquote>
<p/>
<p>
The quantity <img alt="{\|1_A *1_B\|_{\ell^2(G)}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C1_A+%2A1_B%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|1_A *1_B\|_{\ell^2(G)}^2}"/> (or equivalently, the number of solutions to the equation <img alt="{ab=a'b'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bab%3Da%27b%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ab=a'b'}"/> with <img alt="{a,a' \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \in A}"/> and <img alt="{b,b' \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%2Cb%27+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b,b' \in B}"/>) is also known as the <em>multiplicative energy</em> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>, and is sometimes denoted <img alt="{E(A,B)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%28A%2CB%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E(A,B)}"/> in the literature.
</p>
<p>
<em>Proof:</em>  By hypothesis, we have </p>
<p align="center"><img alt="\displaystyle  \sum_{(a,b) \in A \times B} 1_A * 1_B(ab) = \|1_A * 1_B \|_{\ell^2(G)}^2 \geq |A|^{3/2} |B|^{3/2} / K^2." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7B%28a%2Cb%29+%5Cin+A+%5Ctimes+B%7D+1_A+%2A+1_B%28ab%29+%3D+%5C%7C1_A+%2A+1_B+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2+%5Cgeq+%7CA%7C%5E%7B3%2F2%7D+%7CB%7C%5E%7B3%2F2%7D+%2F+K%5E2.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{(a,b) \in A \times B} 1_A * 1_B(ab) = \|1_A * 1_B \|_{\ell^2(G)}^2 \geq |A|^{3/2} |B|^{3/2} / K^2."/></p>
<p> Since
</p><p align="center"><img alt="\displaystyle  \sum_{(a,b) \in A \times B: 1_A * 1_B(ab) \leq |A|^{1/2} |B|^{1/2}/2K^2} 1_A * 1_B(ab) \leq |A|^{3/2} |B|^{3/2} / 2K^2," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7B%28a%2Cb%29+%5Cin+A+%5Ctimes+B%3A+1_A+%2A+1_B%28ab%29+%5Cleq+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%2F2K%5E2%7D+1_A+%2A+1_B%28ab%29+%5Cleq+%7CA%7C%5E%7B3%2F2%7D+%7CB%7C%5E%7B3%2F2%7D+%2F+2K%5E2%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{(a,b) \in A \times B: 1_A * 1_B(ab) \leq |A|^{1/2} |B|^{1/2}/2K^2} 1_A * 1_B(ab) \leq |A|^{3/2} |B|^{3/2} / 2K^2,"/></p>
<p> we conclude that
</p><p align="center"><img alt="\displaystyle  \sum_{(a,b) \in A \times B: 1_A * 1_B(ab) &gt; |A|^{1/2} |B|^{1/2}/2K^2} 1_A * 1_B(ab) \geq |A|^{3/2} |B|^{3/2} / 2K^2." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7B%28a%2Cb%29+%5Cin+A+%5Ctimes+B%3A+1_A+%2A+1_B%28ab%29+%3E+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%2F2K%5E2%7D+1_A+%2A+1_B%28ab%29+%5Cgeq+%7CA%7C%5E%7B3%2F2%7D+%7CB%7C%5E%7B3%2F2%7D+%2F+2K%5E2.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{(a,b) \in A \times B: 1_A * 1_B(ab) &gt; |A|^{1/2} |B|^{1/2}/2K^2} 1_A * 1_B(ab) \geq |A|^{3/2} |B|^{3/2} / 2K^2."/></p>
<p> Since, by Cauchy-Schwarz (or Young’s inequality), we have <img alt="{1_A*1_B(ab) \leq |A|^{1/2} |B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_A%2A1_B%28ab%29+%5Cleq+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_A*1_B(ab) \leq |A|^{1/2} |B|^{1/2}}"/>, we conclude that there is a set <img alt="{E \subset A \times B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE+%5Csubset+A+%5Ctimes+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E \subset A \times B}"/> with <img alt="{|E| \geq |A| |B|/2K^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cgeq+%7CA%7C+%7CB%7C%2F2K%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \geq |A| |B|/2K^2}"/> such that
</p><p align="center"><img alt="\displaystyle  1_A * 1_B(ab) &gt; |A|^{1/2} |B|^{1/2}/2K^2" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++1_A+%2A+1_B%28ab%29+%3E+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%2F2K%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  1_A * 1_B(ab) &gt; |A|^{1/2} |B|^{1/2}/2K^2"/></p>
<p> for all <img alt="{(a,b) \in E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%29+%5Cin+E%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b) \in E}"/>.</p>
<p>
By slight abuse of notation (arising from the fact that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> are not necessarily disjoint, and that <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> is a set of ordered pairs rather than unordered pairs), we can view the triplet <img alt="{(A,B,E)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A%2CB%2CE%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A,B,E)}"/> as a bipartite graph. Applying Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#three-path">4</a>, we can find subsets <img alt="{A', B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%2C+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A', B'}"/> of <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> respectively with <img alt="{|A'| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \gg K^{-O(1)} |A|}"/> and <img alt="{|B'| \gg K^{-O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'| \gg K^{-O(1)} |B|}"/> such that for all <img alt="{a \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A'}"/> and <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/>, one can find <img alt="{\gg K^{-O(1)} |A| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A| |B|}"/> elements <img alt="{a' \in A, b' \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27+%5Cin+A%2C+b%27+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a' \in A, b' \in B}"/> such that <img alt="{(a,b'), (a',b'), (a',b) \in E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%27%29%2C+%28a%27%2Cb%27%29%2C+%28a%27%2Cb%29+%5Cin+E%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b'), (a',b'), (a',b) \in E}"/>. In particular, we see that <a name="abba">
</a></p><p align="center"><a name="abba"><img alt="\displaystyle  \sum_{a' \in G} \sum_{b' \in G} 1_A * 1_B(ab') 1_A * 1_B(a'b') 1_A*1_B(a'b) \gg K^{-O(1)} |A|^{5/2} |B|^{5/2}. \ \ \ \ \ (3)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Ba%27+%5Cin+G%7D+%5Csum_%7Bb%27+%5Cin+G%7D+1_A+%2A+1_B%28ab%27%29+1_A+%2A+1_B%28a%27b%27%29+1_A%2A1_B%28a%27b%29+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B5%2F2%7D+%7CB%7C%5E%7B5%2F2%7D.+%5C+%5C+%5C+%5C+%5C+%283%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{a' \in G} \sum_{b' \in G} 1_A * 1_B(ab') 1_A * 1_B(a'b') 1_A*1_B(a'b) \gg K^{-O(1)} |A|^{5/2} |B|^{5/2}. \ \ \ \ \ (3)"/></a></p><a name="abba">
</a><p><a name="abba"/> Observe that <img alt="{1_A * 1_B(a'b') = 1_{B^{-1}}*1_{A^{-1}} ((b')^{-1} (a')^{-1} )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_A+%2A+1_B%28a%27b%27%29+%3D+1_%7BB%5E%7B-1%7D%7D%2A1_%7BA%5E%7B-1%7D%7D+%28%28b%27%29%5E%7B-1%7D+%28a%27%29%5E%7B-1%7D+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_A * 1_B(a'b') = 1_{B^{-1}}*1_{A^{-1}} ((b')^{-1} (a')^{-1} )}"/>. Using the identity <img alt="{(ab') ((b')^{-1} (a')^{-1}) (a' b) = ab}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28ab%27%29+%28%28b%27%29%5E%7B-1%7D+%28a%27%29%5E%7B-1%7D%29+%28a%27+b%29+%3D+ab%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(ab') ((b')^{-1} (a')^{-1}) (a' b) = ab}"/>, we note that triples <img alt="{(ab', (b')^{-1} (a')^{-1}, a'b)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28ab%27%2C+%28b%27%29%5E%7B-1%7D+%28a%27%29%5E%7B-1%7D%2C+a%27b%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(ab', (b')^{-1} (a')^{-1}, a'b)}"/> for <img alt="{a',b' \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27%2Cb%27+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a',b' \in G}"/> are precisely those triples <img alt="{(g_1,g_2,g_3) \in G \times G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28g_1%2Cg_2%2Cg_3%29+%5Cin+G+%5Ctimes+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(g_1,g_2,g_3) \in G \times G}"/> with <img alt="{g_1g_2g_3 = ab}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg_1g_2g_3+%3D+ab%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g_1g_2g_3 = ab}"/>. Thus the left-hand side of <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#abba">(3)</a> is equal to <img alt="{F(ab)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%28ab%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F(ab)}"/>, where </p>
<p align="center"><img alt="\displaystyle  F := 1_A * 1_B * 1_{B^{-1}} * 1_{A^{-1}} * 1_A * 1_B." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++F+%3A%3D+1_A+%2A+1_B+%2A+1_%7BB%5E%7B-1%7D%7D+%2A+1_%7BA%5E%7B-1%7D%7D+%2A+1_A+%2A+1_B.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  F := 1_A * 1_B * 1_{B^{-1}} * 1_{A^{-1}} * 1_A * 1_B."/></p>
<p> But since
</p><p align="center"><img alt="\displaystyle  \|F\|_{\ell^1} = |A| |B| |B^{-1}| |A^{-1}| |A| |B| = |A|^3 |B|^3," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7CF%5C%7C_%7B%5Cell%5E1%7D+%3D+%7CA%7C+%7CB%7C+%7CB%5E%7B-1%7D%7C+%7CA%5E%7B-1%7D%7C+%7CA%7C+%7CB%7C+%3D+%7CA%7C%5E3+%7CB%7C%5E3%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \|F\|_{\ell^1} = |A| |B| |B^{-1}| |A^{-1}| |A| |B| = |A|^3 |B|^3,"/></p>
<p> we see from Markov’s inequality that there are at most <img alt="{O(K^{O(1)} |A|^{1/2} |B|^{1/2})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)} |A|^{1/2} |B|^{1/2})}"/> possible values for <img alt="{ab}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bab%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ab}"/>, which gives the bound <img alt="{|A' \cdot B'| \ll K^{O(1)} |A|^{1/2} |B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27+%5Ccdot+B%27%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A' \cdot B'| \ll K^{O(1)} |A|^{1/2} |B|^{1/2}}"/>. </p>
<p>
The second bound <img alt="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27+%5Ccdot+%28A%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}"/> can be proven similarly to the first (noting that any <img alt="{a,a' \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a' \in A'}"/> are connected by <img alt="{\gg K^{-O(1)} |A|^2 |B|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E2+%7CB%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A|^2 |B|^2}"/> paths of length six), but can also from the former bound as follows. Observe that any element <img alt="{a (a')^{-1} \in A' \cdot (A')^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%28a%27%29%5E%7B-1%7D+%5Cin+A%27+%5Ccdot+%28A%27%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a (a')^{-1} \in A' \cdot (A')^{-1}}"/> has at least <img alt="{|B'|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%27%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B'|}"/> representations of the form <img alt="{a(a')^{-1} = (ab) (a'b)^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%28a%27%29%5E%7B-1%7D+%3D+%28ab%29+%28a%27b%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a(a')^{-1} = (ab) (a'b)^{-1}}"/> with <img alt="{b \in B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in B'}"/>, and hence <img alt="{ab,a'b \in A' \cdot B'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bab%2Ca%27b+%5Cin+A%27+%5Ccdot+B%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ab,a'b \in A' \cdot B'}"/>, thus </p>
<p align="center"><img alt="\displaystyle  1_{A'B'} * 1_{(A'B')^{-1}} \geq |B'| \gg K^{-O(1)} |B|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++1_%7BA%27B%27%7D+%2A+1_%7B%28A%27B%27%29%5E%7B-1%7D%7D+%5Cgeq+%7CB%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CB%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  1_{A'B'} * 1_{(A'B')^{-1}} \geq |B'| \gg K^{-O(1)} |B|"/></p>
<p> on <img alt="{A' (A')^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%28A%27%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' (A')^{-1}}"/>. On the other hand, the left-hand side has an <img alt="{\ell^1(G)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%5E1%28G%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell^1(G)}"/> norm of <img alt="{|A'B'| |(A'B')^{-1}| \ll K^{O(1)} |A| |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27B%27%7C+%7C%28A%27B%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'B'| |(A'B')^{-1}| \ll K^{O(1)} |A| |B|}"/>, and the bound <img alt="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27+%5Ccdot+%28A%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A' \cdot (A')^{-1}| \ll K^{O(1)} |A|}"/> then follows from Markov’s inequality. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 3</b> <a name="l2g"/> In the converse direction, show that if <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> are non-empty finite subsets of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> with <img alt="{|AB| \leq K |A|^{1/2} |B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CAB%7C+%5Cleq+K+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|AB| \leq K |A|^{1/2} |B|^{1/2}}"/>, then <img alt="{\|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/2} |B|^{3/2} / K^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C1_A+%2A+1_B+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%7CA%7C%5E%7B3%2F2%7D+%7CB%7C%5E%7B3%2F2%7D+%2F+K%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/2} |B|^{3/2} / K^{1/2}}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 4</b>  If <img alt="{A, B, C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%2C+C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B, C}"/> are three non-empty finite subsets of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, establish the <em>Ruzsa triangle inequality</em> <img alt="{|A \cdot C^{-1}| \leq \frac{|A \cdot B^{-1}| |B \cdot C^{-1}|}{|B|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccdot+C%5E%7B-1%7D%7C+%5Cleq+%5Cfrac%7B%7CA+%5Ccdot+B%5E%7B-1%7D%7C+%7CB+%5Ccdot+C%5E%7B-1%7D%7C%7D%7B%7CB%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cdot C^{-1}| \leq \frac{|A \cdot B^{-1}| |B \cdot C^{-1}|}{|B|}}"/>. (<em>Hint:</em> mimic the final part of the proof of Corollary <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bsps">5</a>.) </p></blockquote>
<p/>
<p>
We now give a variant of this corollary involving approximate groups.
</p>
<blockquote><p><b>Lemma 6 (Balog-Szemerédi lemma, approximate group form)</b> <a name="bzag"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite symmetric subset of a group <img alt="{G = (G,\cdot)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3D+%28G%2C%5Ccdot%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G = (G,\cdot)}"/>, and suppose that
</p><p align="center"><img alt="\displaystyle  \|1_A * 1_A \|_{\ell^2(G)} \geq |A|^3/K" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C1_A+%2A+1_A+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%7CA%7C%5E3%2FK&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \|1_A * 1_A \|_{\ell^2(G)} \geq |A|^3/K"/></p>
<p> for some <img alt="{K \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 1}"/>. Then there exists a <img alt="{K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^{O(1)}}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \ll K^{O(1)} |A|}"/> such that <img alt="{|A \cap gH| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gH%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gH| \gg K^{-O(1)} |A|}"/> for some <img alt="{g \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in H}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  By Corollary <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bsps">5</a>, we may find a subset <img alt="{A' \subset A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%5Csubset+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' \subset A}"/> with <img alt="{|A'| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%27%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A'| \gg K^{-O(1)} |A|}"/> such that <a name="apap">
</a></p><p align="center"><a name="apap"><img alt="\displaystyle  |A' (A')^{-1}| \ll K^{O(1)} |A|. \ \ \ \ \ (4)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%27+%28A%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C.+%5C+%5C+%5C+%5C+%5C+%284%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A' (A')^{-1}| \ll K^{O(1)} |A|. \ \ \ \ \ (4)"/></a></p><a name="apap">
</a><p><a name="apap"/> By Exercise <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#l2g">3</a>, this implies that </p>
<p align="center"><img alt="\displaystyle  \| 1_{A'} * 1_{(A')^{-1}} \|_{\ell^2(G)}^2 \gg K^{-O(1)} |A|^3." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+1_%7BA%27%7D+%2A+1_%7B%28A%27%29%5E%7B-1%7D%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E3.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| 1_{A'} * 1_{(A')^{-1}} \|_{\ell^2(G)}^2 \gg K^{-O(1)} |A|^3."/></p>
<p> Observe that the left-hand side is equal to
</p><p align="center"><img alt="\displaystyle  1_{A'} * 1_{(A')^{-1}} * 1_{A'} * 1_{(A')^{-1}} (1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++1_%7BA%27%7D+%2A+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D+%2A+1_%7B%28A%27%29%5E%7B-1%7D%7D+%281%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  1_{A'} * 1_{(A')^{-1}} * 1_{A'} * 1_{(A')^{-1}} (1)"/></p>
<p align="center"><img alt="\displaystyle  = 1_{(A')^{-1}} * 1_{A'} * 1_{(A')^{-1}} * 1_{A'}(1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%3D+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D+%2A+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%281%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  = 1_{(A')^{-1}} * 1_{A'} * 1_{(A')^{-1}} * 1_{A'}(1)"/></p>
<p align="center"><img alt="\displaystyle  = \| 1_{(A')^{-1}} * 1_{A'} \|_{\ell^2(G)}^2." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%3D+%5C%7C+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  = \| 1_{(A')^{-1}} * 1_{A'} \|_{\ell^2(G)}^2."/></p>
<p> We conclude that
</p><p align="center"><img alt="\displaystyle  \sum_{s \in G} (1_{(A')^{-1}} * 1_{A'}(s))^2 \gg K^{-O(1)} |A|^3." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bs+%5Cin+G%7D+%281_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29%29%5E2+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E3.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{s \in G} (1_{(A')^{-1}} * 1_{A'}(s))^2 \gg K^{-O(1)} |A|^3."/></p>
<p> On the other hand, we have
</p><p align="center"><img alt="\displaystyle  \sum_{s \in G} 1_{(A')^{-1}} * 1_{A'}(s) = |A'| |A'| \leq |A|^2." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bs+%5Cin+G%7D+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29+%3D+%7CA%27%7C+%7CA%27%7C+%5Cleq+%7CA%7C%5E2.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{s \in G} 1_{(A')^{-1}} * 1_{A'}(s) = |A'| |A'| \leq |A|^2."/></p>
<p> As a consequence, we see that if we set
</p><p align="center"><img alt="\displaystyle  S := \{ s \in G: 1_{(A')^{-1}} * 1_{A'}(s) \geq C^{-1} K^{-C} |A| \}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++S+%3A%3D+%5C%7B+s+%5Cin+G%3A+1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29+%5Cgeq+C%5E%7B-1%7D+K%5E%7B-C%7D+%7CA%7C+%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  S := \{ s \in G: 1_{(A')^{-1}} * 1_{A'}(s) \geq C^{-1} K^{-C} |A| \}"/></p>
<p> for some sufficiently large absolute constant <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/>, then
</p><p align="center"><img alt="\displaystyle  \sum_{s \in G \backslash S} (1_{(A')^{-1}} * 1_{A'}(s))^2 \leq C^{-1} K^{-C} |A|^3," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bs+%5Cin+G+%5Cbackslash+S%7D+%281_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29%29%5E2+%5Cleq+C%5E%7B-1%7D+K%5E%7B-C%7D+%7CA%7C%5E3%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{s \in G \backslash S} (1_{(A')^{-1}} * 1_{A'}(s))^2 \leq C^{-1} K^{-C} |A|^3,"/></p>
<p> and thus (for <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/> large enough)
</p><p align="center"><img alt="\displaystyle  \sum_{s \in S} (1_{(A')^{-1}} * 1_{A'}(s))^2 \gg K^{-O(1)} |A|^3." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bs+%5Cin+S%7D+%281_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29%29%5E2+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E3.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{s \in S} (1_{(A')^{-1}} * 1_{A'}(s))^2 \gg K^{-O(1)} |A|^3."/></p>
<p> Since <img alt="{1_{(A')^{-1}} * 1_{A'}(s) \leq|A'| \leq |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_%7B%28A%27%29%5E%7B-1%7D%7D+%2A+1_%7BA%27%7D%28s%29+%5Cleq%7CA%27%7C+%5Cleq+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_{(A')^{-1}} * 1_{A'}(s) \leq|A'| \leq |A|}"/>, we conclude that
</p><p align="center"><img alt="\displaystyle  |S| \gg K^{-O(1)} |A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CS%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |S| \gg K^{-O(1)} |A|."/></p>
<p> Also, <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> is clearly symmetric and contains the origin.</p>
<p>
Now let us consider an element <img alt="{g = a_0 s_1 \ldots s_5 b_6^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%3D+a_0+s_1+%5Cldots+s_5+b_6%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g = a_0 s_1 \ldots s_5 b_6^{-1}}"/> of the product <img alt="{(A') S^5 (A')^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A%27%29+S%5E5+%28A%27%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A') S^5 (A')^{-1}}"/>. By construction of <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/>, we can write each <img alt="{s_i}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bs_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{s_i}"/> as a product <img alt="{b_i^{-1} a_i}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb_i%5E%7B-1%7D+a_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b_i^{-1} a_i}"/> with <img alt="{a_i,b_i \in A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_i%2Cb_i+%5Cin+A%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_i,b_i \in A'}"/> in at least <img alt="{C^{-1} K^{-C} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%5E%7B-1%7D+K%5E%7B-C%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C^{-1} K^{-C} |A|}"/> ways. Doing so for each <img alt="{i=1,\ldots,5}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bi%3D1%2C%5Cldots%2C5%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{i=1,\ldots,5}"/> gives rise to a factorisation </p>
<p align="center"><img alt="\displaystyle  g = g_1 \ldots g_6" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++g+%3D+g_1+%5Cldots+g_6&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  g = g_1 \ldots g_6"/></p>
<p> where <img alt="{g_i := a_{i-1} b_i^{-1} \in A' (A')^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg_i+%3A%3D+a_%7Bi-1%7D+b_i%5E%7B-1%7D+%5Cin+A%27+%28A%27%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g_i := a_{i-1} b_i^{-1} \in A' (A')^{-1}}"/>; as the <img alt="{g_1,\ldots,g_6}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg_1%2C%5Cldots%2Cg_6%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g_1,\ldots,g_6}"/> uniquely determine the <img alt="{a_i,b_i}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_i%2Cb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_i,b_i}"/> (for fixed <img alt="{a_0,s_1,\ldots,s_5,b_6}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_0%2Cs_1%2C%5Cldots%2Cs_5%2Cb_6%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_0,s_1,\ldots,s_5,b_6}"/>), we conclude that each element <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> of <img alt="{(A') S^5 (A')^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A%27%29+S%5E5+%28A%27%29%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A') S^5 (A')^{-1}}"/> has at least <img alt="{\gg K^{-O(1)} |A|^5}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E5%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A|^5}"/> such factorisations. But by <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#apap">(4)</a>, there are at most <img alt="{O(K^{O(1)}|A|^6)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%7CA%7C%5E6%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)}|A|^6)}"/> such tuples <img alt="{g_1,\ldots,g_6}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg_1%2C%5Cldots%2Cg_6%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g_1,\ldots,g_6}"/>, and so there are at most <img alt="{O(K^{O(1)} |A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D+%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)} |A|)}"/> possible values for <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>, thus <a name="adul">
</a></p><p align="center"><a name="adul"><img alt="\displaystyle  |(A') S^5 (A')^{-1}| \ll K^{O(1)} |A|. \ \ \ \ \ (5)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%28A%27%29+S%5E5+%28A%27%29%5E%7B-1%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C.+%5C+%5C+%5C+%5C+%5C+%285%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |(A') S^5 (A')^{-1}| \ll K^{O(1)} |A|. \ \ \ \ \ (5)"/></a></p><a name="adul">
</a><p><a name="adul"/> In particular,
</p><p align="center"><img alt="\displaystyle  |S^5| \ll K^{O(1)} |S|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CS%5E5%7C+%5Cll+K%5E%7BO%281%29%7D+%7CS%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |S^5| \ll K^{O(1)} |S|."/></p>
<p> By the Ruzsa covering lemma (see the exercise below), this implies that <img alt="{S^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S^4}"/> is covered by <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> left-translates of <img alt="{S^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S^2}"/>, and so <img alt="{H := S^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3A%3D+S%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H := S^2}"/> is a <img alt="{K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^{O(1)}}"/>-approximate group. Finally, from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#adul">(5)</a> one has
</p><p align="center"><img alt="\displaystyle  |A' H| \ll K^{O(1)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%27+H%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A' H| \ll K^{O(1)} |A|"/></p>
<p> and thus by Exercise <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#l2g">3</a>
</p><p align="center"><img alt="\displaystyle  \| 1_{A'} * 1_H \|_{\ell^2(G)} \gg K^{-O(1)} |A|^{3/2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+1_%7BA%27%7D+%2A+1_H+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B3%2F2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| 1_{A'} * 1_H \|_{\ell^2(G)} \gg K^{-O(1)} |A|^{3/2}."/></p>
<p> In particular, since the support of <img alt="{1_{A'} * 1_H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_%7BA%27%7D+%2A+1_H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_{A'} * 1_H}"/> has size <img alt="{O(K^{O(1)} |A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D+%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)} |A|)}"/>, one has
</p><p align="center"><img alt="\displaystyle  1_{A'} * 1_H(g) \gg K^{-O(1)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++1_%7BA%27%7D+%2A+1_H%28g%29+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  1_{A'} * 1_H(g) \gg K^{-O(1)} |A|"/></p>
<p> for some <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>, or equivalently that
</p><p align="center"><img alt="\displaystyle  |A' \cap Hg| \gg K^{-O(1)} |A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%27+%5Ccap+Hg%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A' \cap Hg| \gg K^{-O(1)} |A|."/></p>
<p> Increasing <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> to <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and taking inverses, we conclude that <img alt="{|gH \cap A| \ll K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CgH+%5Ccap+A%7C+%5Cll+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|gH \cap A| \ll K^{-O(1)} |A|}"/>, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 5 (Ruzsa covering lemma)</b>  Let <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> be finite non-empty subsets of a group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. Show that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> can be covered by at most <img alt="{\frac{|AB|}{|B|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%7CAB%7C%7D%7B%7CB%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{|AB|}{|B|}}"/> left-translates of <img alt="{BB^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BBB%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{BB^{-1}}"/>. (<em>Hint:</em> consider a maximal disjoint collection of translates <img alt="{aB}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aB}"/> of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> with <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/>.) </p></blockquote>
<p/>
<blockquote><p><b>Exercise 6 (Converse to Balog-Szemerédi-Gowers)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite symmetric subset of a group <img alt="{G = (G,\cdot)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3D+%28G%2C%5Ccdot%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G = (G,\cdot)}"/>, and suppose there exists a <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| \leq K |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cleq+K+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \leq K |A|}"/> such that <img alt="{|A \cap gH| \geq |A|/K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gH%7C+%5Cgeq+%7CA%7C%2FK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gH| \geq |A|/K}"/> for some <img alt="{g \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in H}"/>. Show that
</p><p align="center"><img alt="\displaystyle  \|1_A * 1_A\|_{\ell^2(G)} \geq K^{-3} |A|^{3/2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C1_A+%2A+1_A%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+K%5E%7B-3%7D+%7CA%7C%5E%7B3%2F2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \|1_A * 1_A\|_{\ell^2(G)} \geq K^{-3} |A|^{3/2}."/></p>
</blockquote>
<p/>
<blockquote><p><b>Exercise 7</b>  Let <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> be finite non-empty subsets of a group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, and suppose that <img alt="{\|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/2} |B|^{3/2} / K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C1_A+%2A+1_B+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%7CA%7C%5E%7B3%2F2%7D+%7CB%7C%5E%7B3%2F2%7D+%2F+K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|1_A * 1_B \|_{\ell^2(G)} \geq |A|^{3/2} |B|^{3/2} / K}"/>. Show that there exists a <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| \leq K^{O(1)} |A|^{1/2} |B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cleq+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B1%2F2%7D+%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \leq K^{O(1)} |A|^{1/2} |B|^{1/2}}"/> and elements <img alt="{g, h \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%2C+h+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g, h \in G}"/> such that <img alt="{|A \cap gH| \gg K^{-O(1)} |H|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gH%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CH%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gH| \gg K^{-O(1)} |H|}"/> and <img alt="{|B \cap Hh| \gg K^{-O(1)} |H|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB+%5Ccap+Hh%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CH%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B \cap Hh| \gg K^{-O(1)} |H|}"/>. </p></blockquote>
<p/>
<p>
Finally, we can prove Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bsg">1</a>. Fix <img alt="{G, \nu, K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%2C+%5Cnu%2C+K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G, \nu, K}"/>. We may assume that <a name="noa">
</a></p><p align="center"><a name="noa"><img alt="\displaystyle  \| \nu * \nu \|_{\ell^2(G)} &gt; \frac{1}{K} \|\nu\|_{\ell^2(G)} \ \ \ \ \ (6)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu+%2A+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%3E+%5Cfrac%7B1%7D%7BK%7D+%5C%7C%5Cnu%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5C+%5C+%5C+%5C+%5C+%286%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu * \nu \|_{\ell^2(G)} &gt; \frac{1}{K} \|\nu\|_{\ell^2(G)} \ \ \ \ \ (6)"/></a></p><a name="noa">
</a><p><a name="noa"/> and we need to use this to locate an <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> in <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> with <img alt="{|H| \ll K^{O(1)} / \| \nu \|_{\ell^2(G)}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cll+K%5E%7BO%281%29%7D+%2F+%5C%7C+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \ll K^{O(1)} / \| \nu \|_{\ell^2(G)}^2}"/> and an element <img alt="{x \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in G}"/> such that <img alt="{\nu(xH) \gg K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%28xH%29+%5Cgg+K%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu(xH) \gg K^{-O(1)}}"/>.
</p>
<p>
Let us write <img alt="{M := 1/\|\nu\|_{\ell^2(G)}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM+%3A%3D+1%2F%5C%7C%5Cnu%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M := 1/\|\nu\|_{\ell^2(G)}^2}"/>. Intuitively, <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/> represents the “width” of the probability meaure <img alt="{\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu}"/>, as can be seen by considering the model example <img alt="{\nu = \frac{1}{M} 1_A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu+%3D+%5Cfrac%7B1%7D%7BM%7D+1_A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu = \frac{1}{M} 1_A}"/> where <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is a symmetric set of cardinality <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/> (i.e. <img alt="{\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu}"/> is the uniform probability measure on <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>). If we were actually in this model case, we could apply Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bzag">6</a> immediately and be done. Of course, in general, <img alt="{\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu}"/> need not be a uniform measure on a set of size <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>. However, it turns out that one can use <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#noa">(6)</a> to conclude that the “bulk” of <img alt="{\nu}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu}"/> is basically of this form.
</p>
<p>
More precisely, let us split <img alt="{\nu = \nu_{&lt;}+\nu_{&gt;}+\nu_=}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu+%3D+%5Cnu_%7B%3C%7D%2B%5Cnu_%7B%3E%7D%2B%5Cnu_%3D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu = \nu_{&lt;}+\nu_{&gt;}+\nu_=}"/>, where </p>
<p align="center"><img alt="\displaystyle  \nu_{&lt;} := \nu 1_{\nu \leq \frac{1}{100K^2M}}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cnu_%7B%3C%7D+%3A%3D+%5Cnu+1_%7B%5Cnu+%5Cleq+%5Cfrac%7B1%7D%7B100K%5E2M%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \nu_{&lt;} := \nu 1_{\nu \leq \frac{1}{100K^2M}}"/></p>
<p align="center"><img alt="\displaystyle  \nu_{&gt;} := \nu 1_{\nu \geq \frac{10K}{M}}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cnu_%7B%3E%7D+%3A%3D+%5Cnu+1_%7B%5Cnu+%5Cgeq+%5Cfrac%7B10K%7D%7BM%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \nu_{&gt;} := \nu 1_{\nu \geq \frac{10K}{M}}"/></p>
<p align="center"><img alt="\displaystyle  \nu_= := \nu - \nu_{&lt;} \nu_{&gt;}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cnu_%3D+%3A%3D+%5Cnu+-+%5Cnu_%7B%3C%7D+%5Cnu_%7B%3E%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \nu_= := \nu - \nu_{&lt;} \nu_{&gt;}."/></p>
<p> Observe that
</p><p align="center"><img alt="\displaystyle  \| \nu_{&lt;}\|_{\ell^2(G)}^2 \leq \frac{1}{100K^2M} \| \nu \|_{\ell^1(G)} = \frac{1}{100K^2M} " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu_%7B%3C%7D%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2+%5Cleq+%5Cfrac%7B1%7D%7B100K%5E2M%7D+%5C%7C+%5Cnu+%5C%7C_%7B%5Cell%5E1%28G%29%7D+%3D+%5Cfrac%7B1%7D%7B100K%5E2M%7D+&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu_{&lt;}\|_{\ell^2(G)}^2 \leq \frac{1}{100K^2M} \| \nu \|_{\ell^1(G)} = \frac{1}{100K^2M} "/></p>
<p> and so by Young’s inequality
</p><p align="center"><img alt="\displaystyle  \| \nu_{&lt;} * \nu \|_{\ell^2(G)} = \| \nu * \nu_{&gt;} \|_{\ell^2(G)} \leq \frac{1}{10KM^{1/2}}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu_%7B%3C%7D+%2A+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%3D+%5C%7C+%5Cnu+%2A+%5Cnu_%7B%3E%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%5Cfrac%7B1%7D%7B10KM%5E%7B1%2F2%7D%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu_{&lt;} * \nu \|_{\ell^2(G)} = \| \nu * \nu_{&gt;} \|_{\ell^2(G)} \leq \frac{1}{10KM^{1/2}}."/></p>
<p> In a similar vein, we have
</p><p align="center"><img alt="\displaystyle  \| \nu_{&gt;} \|_{\ell^1(G)} \leq \frac{M}{10K} \| \nu \|_{\ell^2(G)}^2 = \frac{1}{10K}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu_%7B%3E%7D+%5C%7C_%7B%5Cell%5E1%28G%29%7D+%5Cleq+%5Cfrac%7BM%7D%7B10K%7D+%5C%7C+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2+%3D+%5Cfrac%7B1%7D%7B10K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu_{&gt;} \|_{\ell^1(G)} \leq \frac{M}{10K} \| \nu \|_{\ell^2(G)}^2 = \frac{1}{10K}"/></p>
<p> and thus by Young’s inequality (and the normalisation <img alt="{\|\nu\|_{\ell^2(G)} = 1/M^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C%5Cnu%5C%7C_%7B%5Cell%5E2%28G%29%7D+%3D+1%2FM%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\|\nu\|_{\ell^2(G)} = 1/M^{1/2}}"/>)
</p><p align="center"><img alt="\displaystyle  \| \nu_{&gt;} * \nu \|_{\ell^2(G)} = \| \nu * \nu_{&lt;} \|_{\ell^2(G)} \leq \frac{1}{10KM^{1/2}}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu_%7B%3E%7D+%2A+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%3D+%5C%7C+%5Cnu+%2A+%5Cnu_%7B%3C%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%5Cfrac%7B1%7D%7B10KM%5E%7B1%2F2%7D%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu_{&gt;} * \nu \|_{\ell^2(G)} = \| \nu * \nu_{&lt;} \|_{\ell^2(G)} \leq \frac{1}{10KM^{1/2}}."/></p>
<p> Finally, from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#noa">(6)</a> one has
</p><p align="center"><img alt="\displaystyle  \| \nu * \nu \|_{\ell^2(G)} \geq \frac{1}{K M^{1/2}}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu+%2A+%5Cnu+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%5Cfrac%7B1%7D%7BK+M%5E%7B1%2F2%7D%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu * \nu \|_{\ell^2(G)} \geq \frac{1}{K M^{1/2}}."/></p>
<p> Subtracting using the triangle inequality (ignoring some slight double-counting), we conclude that
</p><p align="center"><img alt="\displaystyle  \| \nu_= * \nu_= \|_{\ell^2(G)} \gg \frac{1}{KM^{1/2}}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cnu_%3D+%2A+%5Cnu_%3D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgg+%5Cfrac%7B1%7D%7BKM%5E%7B1%2F2%7D%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \nu_= * \nu_= \|_{\ell^2(G)} \gg \frac{1}{KM^{1/2}}."/></p>
<p> If we then set <img alt="{A := \{ g \in G: \nu(g) &gt; \frac{1}{100K^2 M} \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3A%3D+%5C%7B+g+%5Cin+G%3A+%5Cnu%28g%29+%3E+%5Cfrac%7B1%7D%7B100K%5E2+M%7D+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A := \{ g \in G: \nu(g) &gt; \frac{1}{100K^2 M} \}}"/>, we conclude in particular that
</p><p align="center"><img alt="\displaystyle  \| 1_A * 1_A \|_{\ell^2(G)} \gg K^{-O(1)} M^{3/2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+1_A+%2A+1_A+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgg+K%5E%7B-O%281%29%7D+M%5E%7B3%2F2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| 1_A * 1_A \|_{\ell^2(G)} \gg K^{-O(1)} M^{3/2}."/></p>
<p> On the other hand, from Markov’s inequality one has <img alt="{|A| \ll K^2 M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cll+K%5E2+M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \ll K^2 M}"/>. Applying Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bzag">6</a>, we conclude the existence of a <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| \ll K^{O(1)} M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cll+K%5E%7BO%281%29%7D+M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \ll K^{O(1)} M}"/> such that <img alt="{|A \cap gH| \gg K^{-O(1)} M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gH%7C+%5Cgg+K%5E%7B-O%281%29%7D+M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gH| \gg K^{-O(1)} M}"/> for some <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>, which by definition of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> implies that <img alt="{\nu(gH) \gg K^{-O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cnu%28gH%29+%5Cgg+K%5E%7B-O%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\nu(gH) \gg K^{-O(1)}}"/>, and the claim follows.</p>
<p align="center"><b> —  2. The Bourgain-Gamburd expansion machine  — </b></p>
<p>
We can now prove Theorem <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bourgain">2</a>. We can assume that <img alt="{|G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G|}"/> is sufficiently large depending on the parameters <img alt="{k,\kappa,\Lambda,\delta'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C%5Ckappa%2C%5CLambda%2C%5Cdelta%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k,\kappa,\Lambda,\delta'}"/>, since the claim is trivial for bounded <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> (note that as <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> generates <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, the Cayley graph <img alt="{Cay(G,S)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BCay%28G%2CS%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Cay(G,S)}"/> will be an <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>-expander for some <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/>). Henceforth we allow all implied constants in the asymptotic notation to depend on <img alt="{k,\kappa,\Lambda,\delta'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%2C%5Ckappa%2C%5CLambda%2C%5Cdelta%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k,\kappa,\Lambda,\delta'}"/>.
</p>
<p>
To show expansion, it suffices from the quasirandomness hypothesis (and <a href="http://terrytao.wordpress.com/2011/12/16/254b-notes-3-quasirandom-groups-expansion-and-selbergs-316-theorem/">Proposition 4 from the preceding notes</a>), it will suffice to show that <a name="mundo">
</a></p><p align="center"><a name="mundo"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-1/2+\kappa/2} \ \ \ \ \ (7)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%7CG%7C%5E%7B-1%2F2%2B%5Ckappa%2F2%7D+%5C+%5C+%5C+%5C+%5C+%287%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-1/2+\kappa/2} \ \ \ \ \ (7)"/></a></p><a name="mundo">
</a><p><a name="mundo"/> for some <img alt="{n = O(\log |G|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+O%28%5Clog+%7CG%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = O(\log |G|)}"/>.
</p>
<p>
From Young’s inequality, <img alt="{\| \mu^{(n)}\|_{\ell^2(G)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7C+%5Cmu%5E%7B%28n%29%7D%5C%7C_%7B%5Cell%5E2%28G%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\| \mu^{(n)}\|_{\ell^2(G)}}"/> is decreasing in <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>, and is initially equal to <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> when <img alt="{n=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n=0}"/>. We need to “flatten” the <img alt="{\ell^2(G)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%5E2%28G%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell^2(G)}"/> norm of <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> as <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> increases. We first use the non-concentration hypothesis to obtain an initial amount of flattening:
</p>
<blockquote><p><b>Proposition 7</b>  For any <img alt="{n \geq \frac{1}{2} \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cgeq+%5Cfrac%7B1%7D%7B2%7D+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \geq \frac{1}{2} \Lambda \log |G|}"/>, one has <a name="mung">
</a></p><p align="center"><a name="mung"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-\kappa/4}. \ \ \ \ \ (8)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F4%7D.+%5C+%5C+%5C+%5C+%5C+%288%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-\kappa/4}. \ \ \ \ \ (8)"/></a></p><a name="mung">
</a><p><a name="mung"/> Furthermore, we have <a name="mugh">
</a></p><p align="center"><a name="mugh"><img alt="\displaystyle  \mu^{(n)}(gH) \leq |G|^{-\kappa/2} \ \ \ \ \ (9)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%28n%29%7D%28gH%29+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F2%7D+%5C+%5C+%5C+%5C+%5C+%289%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(n)}(gH) \leq |G|^{-\kappa/2} \ \ \ \ \ (9)"/></a></p><a name="mugh">
</a><p><a name="mugh"/> for all proper subgroups <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> and all <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  By the non-concentration hypothesis, we can find <img alt="{n_0 \leq \frac{1}{2} \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn_0+%5Cleq+%5Cfrac%7B1%7D%7B2%7D+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n_0 \leq \frac{1}{2} \Lambda \log |G|}"/> such that </p>
<p align="center"><img alt="\displaystyle  \mu^{(2n_0)}(H) \leq |G|^{-\kappa}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%282n_0%29%7D%28H%29+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(2n_0)}(H) \leq |G|^{-\kappa}"/></p>
<p> for all proper subgroups <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. If we write <img alt="{\mu^{(2n_0)}(H)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%282n_0%29%7D%28H%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(2n_0)}(H)}"/> as <img alt="{\mu^{(n_0)}*\mu^{(n_0)}( Hg g^{-1} H)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n_0%29%7D%2A%5Cmu%5E%7B%28n_0%29%7D%28+Hg+g%5E%7B-1%7D+H%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n_0)}*\mu^{(n_0)}( Hg g^{-1} H)}"/>, we see that
</p><p align="center"><img alt="\displaystyle  \mu^{(2n_0)}(H) \geq \mu^{(n_0)}(Hg) \mu^{(n_0)}(g^{-1} H)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%282n_0%29%7D%28H%29+%5Cgeq+%5Cmu%5E%7B%28n_0%29%7D%28Hg%29+%5Cmu%5E%7B%28n_0%29%7D%28g%5E%7B-1%7D+H%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(2n_0)}(H) \geq \mu^{(n_0)}(Hg) \mu^{(n_0)}(g^{-1} H)"/></p>
<p> for all <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>. By symmetry, <img alt="{\mu^{(n_0)}(g^{-1} H) = \mu^{(n_0)}(Hg)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n_0%29%7D%28g%5E%7B-1%7D+H%29+%3D+%5Cmu%5E%7B%28n_0%29%7D%28Hg%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n_0)}(g^{-1} H) = \mu^{(n_0)}(Hg)}"/>, and thus
</p><p align="center"><img alt="\displaystyle  \sup_{g \in G} \mu^{(n_0)}(gH) \leq |G|^{-\kappa/2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csup_%7Bg+%5Cin+G%7D+%5Cmu%5E%7B%28n_0%29%7D%28gH%29+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sup_{g \in G} \mu^{(n_0)}(gH) \leq |G|^{-\kappa/2}."/></p>
<p> If <img alt="{n \geq \frac{1}{2} \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cgeq+%5Cfrac%7B1%7D%7B2%7D+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \geq \frac{1}{2} \Lambda \log |G|}"/>, then we may write <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/> as the convolution of a probability measure <img alt="{\mu^{(n-n_0)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n-n_0%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n-n_0)}}"/> and <img alt="{\mu^{(n_0)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n_0%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n_0)}}"/>. From this, we see that
</p><p align="center"><img alt="\displaystyle  \mu^{(n)}(g' H) \leq \sup_{g \in G} \mu^{(n_0)}(gH) \leq |G|^{-\kappa/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%28n%29%7D%28g%27+H%29+%5Cleq+%5Csup_%7Bg+%5Cin+G%7D+%5Cmu%5E%7B%28n_0%29%7D%28gH%29+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(n)}(g' H) \leq \sup_{g \in G} \mu^{(n_0)}(gH) \leq |G|^{-\kappa/2}"/></p>
<p> for all <img alt="{g' \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%27+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g' \in G}"/>, giving the claim <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mugh">(9)</a>. Specialising this to the case when <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> is the trivial group, one has
</p><p align="center"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^\infty(G)} \leq |G|^{-\kappa/2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E%5Cinfty%28G%29%7D+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^\infty(G)} \leq |G|^{-\kappa/2}."/></p>
<p> Since we also have
</p><p align="center"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^1(G)} = 1," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E1%28G%29%7D+%3D+1%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^1(G)} = 1,"/></p>
<p> the claim <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mung">(8)</a> then follows from Hölder’s inequality. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Now we obtain additional flattening using the product theorem hypothesis:
</p>
<blockquote><p><b>Lemma 8 (Flattening lemma)</b>  Suppose <img alt="{n \geq \frac{1}{2} \Lambda \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cgeq+%5Cfrac%7B1%7D%7B2%7D+%5CLambda+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \geq \frac{1}{2} \Lambda \log |G|}"/> is such that <a name="mumus">
</a></p><p align="center"><a name="mumus"><img alt="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \geq |G|^{-1/2+\kappa/2}. \ \ \ \ \ (10)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cgeq+%7CG%7C%5E%7B-1%2F2%2B%5Ckappa%2F2%7D.+%5C+%5C+%5C+%5C+%5C+%2810%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} \|_{\ell^2(G)} \geq |G|^{-1/2+\kappa/2}. \ \ \ \ \ (10)"/></a></p><a name="mumus">
</a><p><a name="mumus"/> Then one has
</p><p align="center"><img alt="\displaystyle  \| \mu^{(n)} * \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-\epsilon} \| \mu^{(n)} \|_{\ell^2(G)}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%2A+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%5Cleq+%7CG%7C%5E%7B-%5Cepsilon%7D+%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} * \mu^{(n)} \|_{\ell^2(G)} \leq |G|^{-\epsilon} \| \mu^{(n)} \|_{\ell^2(G)}"/></p>
<p> for some <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> depending only on <img alt="{\kappa}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa}"/> and <img alt="{\delta'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cdelta%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\delta'}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose the claim fails for some <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> to be chosen later, thus </p>
<p align="center"><img alt="\displaystyle  \| \mu^{(n)} * \mu^{(n)} \|_{\ell^2(G)} &gt; |G|^{-\epsilon} \| \mu^{(n)} \|_{\ell^2(G)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Cmu%5E%7B%28n%29%7D+%2A+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D+%3E+%7CG%7C%5E%7B-%5Cepsilon%7D+%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \mu^{(n)} * \mu^{(n)} \|_{\ell^2(G)} &gt; |G|^{-\epsilon} \| \mu^{(n)} \|_{\ell^2(G)}."/></p>
<p> Applying Lemma <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bsg">1</a>, we may thus find a <img alt="{O(|G|^{O(\epsilon)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CG%7C%5E%7BO%28%5Cepsilon%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|G|^{O(\epsilon)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with
</p><p align="center"><img alt="\displaystyle  |H| \ll |G|^{O(\epsilon)} / \| \mu^{(n)} \|_{\ell^2(G)}^2" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CH%7C+%5Cll+%7CG%7C%5E%7BO%28%5Cepsilon%29%7D+%2F+%5C%7C+%5Cmu%5E%7B%28n%29%7D+%5C%7C_%7B%5Cell%5E2%28G%29%7D%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |H| \ll |G|^{O(\epsilon)} / \| \mu^{(n)} \|_{\ell^2(G)}^2"/></p>
<p> and <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/> such that
</p><p align="center"><img alt="\displaystyle  \mu^{(n)}(gH) \gg |G|^{-O(\epsilon)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%28n%29%7D%28gH%29+%5Cgg+%7CG%7C%5E%7B-O%28%5Cepsilon%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(n)}(gH) \gg |G|^{-O(\epsilon)}."/></p>
<p> Since <img alt="{\mu^{(n)}\|_{\ell^\infty(G)} \leq |G|^{-\kappa/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%5C%7C_%7B%5Cell%5E%5Cinfty%28G%29%7D+%5Cleq+%7CG%7C%5E%7B-%5Ckappa%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}\|_{\ell^\infty(G)} \leq |G|^{-\kappa/2}}"/> by <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mugh">(9)</a>, we see that
</p><p align="center"><img alt="\displaystyle  |H| \gg |G|^{\kappa/2-O(\epsilon)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CH%7C+%5Cgg+%7CG%7C%5E%7B%5Ckappa%2F2-O%28%5Cepsilon%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |H| \gg |G|^{\kappa/2-O(\epsilon)}."/></p>
<p> Meanwhile, from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mumus">(10)</a> one has
</p><p align="center"><img alt="\displaystyle  |H| \ll |G|^{1-\kappa + O(\epsilon)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CH%7C+%5Cll+%7CG%7C%5E%7B1-%5Ckappa+%2B+O%28%5Cepsilon%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |H| \ll |G|^{1-\kappa + O(\epsilon)}."/></p>
<p> Applying the product hypothesis (assuming <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> sufficiently small depending on <img alt="{\kappa}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ckappa%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\kappa}"/> and <img alt="{\delta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cdelta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\delta}"/>), we conclude that <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> generates a proper subgroup <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, and thus
</p><p align="center"><img alt="\displaystyle  \mu^{(n)}(gK) \gg |G|^{-O(\epsilon)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cmu%5E%7B%28n%29%7D%28gK%29+%5Cgg+%7CG%7C%5E%7B-O%28%5Cepsilon%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \mu^{(n)}(gK) \gg |G|^{-O(\epsilon)}."/></p>
<p> But this contradicts <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mugh">(9)</a> (again if <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> is sufficiently small). <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Iterating the above lemma <img alt="{O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(1)}"/> times we obtain <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#mundo">(7)</a> for some <img alt="{n = O(\log |G|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+O%28%5Clog+%7CG%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = O(\log |G|)}"/>, as desired.
</p>
<blockquote><p><b>Remark 4</b>  Roughly speaking, the three hypotheses in Theorem <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/#bourgain">2</a> govern three separate stages of the life cycle of the random walk and its distributions <img alt="{\mu^{(n)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmu%5E%7B%28n%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\mu^{(n)}}"/>. In the early stage <img alt="{n = o(\log |G|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%3D+o%28%5Clog+%7CG%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n = o(\log |G|)}"/>, the non-concentration hypotheses creates some initial spreading of this random walk, in particular ensuring that the walk “escapes” from cosets of proper subgroups. In the middle stage <img alt="{n \sim \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Csim+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \sim \log |G|}"/>, the product theorem steadily flattens the distribution of the random walk, until it is very roughly comparable to the uniform distribution. Finally, in the late stage <img alt="{n \gg \log |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn+%5Cgg+%5Clog+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n \gg \log |G|}"/>, the quasirandomness property can smooth out the random walk almost completely to obtain the mixing necessary for expansion. </p></blockquote><p/>
<br/>Filed under: <a href="http://terrytao.wordpress.com/category/teaching/254b-expansion-in-groups/">254B - expansion in groups</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathco/">math.CO</a> Tagged: <a href="http://terrytao.wordpress.com/tag/additive-combinatorics/">additive combinatorics</a>, <a href="http://terrytao.wordpress.com/tag/balog-szemeredi-gowers-lemma/">Balog-Szemeredi-Gowers lemma</a>, <a href="http://terrytao.wordpress.com/tag/expander-graphs/">expander graphs</a>, <a href="http://terrytao.wordpress.com/tag/graph-theory/">graph theory</a> <a href="http://feeds.wordpress.com/1.0/gocomments/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/terrytao.wordpress.com/5645/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/terrytao.wordpress.com/5645/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/terrytao.wordpress.com/5645/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5645&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-11T19:58:23Z</updated>
    <published>2012-01-14T03:49:20Z</published>
    <category scheme="http://terrytao.wordpress.com" term="254B - expansion in groups"/>
    <category scheme="http://terrytao.wordpress.com" term="math.CO"/>
    <category scheme="http://terrytao.wordpress.com" term="additive combinatorics"/>
    <category scheme="http://terrytao.wordpress.com" term="Balog-Szemeredi-Gowers lemma"/>
    <category scheme="http://terrytao.wordpress.com" term="expander graphs"/>
    <category scheme="http://terrytao.wordpress.com" term="graph theory"/>
    <author>
      <name>Terence Tao</name>
      <uri>http://www.math.ucla.edu/~tao</uri>
    </author>
    <source>
      <id>http://terrytao.wordpress.com/feed/atom/</id>
      <link href="http://terrytao.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://terrytao.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://terrytao.wordpress.com/osd.xml" rel="search" title="What&amp;#039;s new" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://terrytao.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <title xml:lang="en">What's new</title>
      <updated>2012-02-15T04:28:30Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://terrytao.wordpress.com/?p=5714</id>
    <link href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/" rel="alternate" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#comments" rel="replies" type="text/html"/>
    <link href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">254B, Notes 5: Product theorems, pivot arguments, and the Larsen-Pink non-concentration inequality</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">In the previous set of notes, we saw that one could derive expansion of Cayley graphs from three ingredients: non-concentration, product theorems, and quasirandomness. Quasirandomness was discussed in Notes 3. In the current set of notes, we discuss product theorems. Roughly speaking, these theorems assert that in certain circumstances, a finite subset of a group [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5714&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>
 In the <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">previous set of notes</a>, we saw that one could derive expansion of Cayley graphs from three ingredients: non-concentration, product theorems, and quasirandomness. Quasirandomness was discussed in <a href="http://terrytao.wordpress.com/2011/12/16/254b-notes-3-quasirandom-groups-expansion-and-selbergs-316-theorem/">Notes 3</a>. In the current set of notes, we discuss product theorems. Roughly speaking, these theorems assert that in certain circumstances, a finite subset <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of a group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> either exhibits expansion (in the sense that <img alt="{A^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^3}"/>, say, is significantly larger than <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>), or is somehow “close to” or “trapped” by a genuine group.
</p>
<blockquote><p><b>Theorem 1 (Product theorem in <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>)</b> <a name="prod-slf"/> Let <img alt="{d \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d \geq 2}"/>, let <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> be a finite field, and let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subset of <img alt="{G := SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3A%3D+SL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G := SL_d(k)}"/>. Let <img alt="{\epsilon &gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon &gt;0}"/> be sufficiently small depending on <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>. Then at least one of the following statements holds: </p>
<ul>
<li> (Expansion) One has <img alt="{|A^3| \geq |A|^{1+\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E3%7C+%5Cgeq+%7CA%7C%5E%7B1%2B%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^3| \geq |A|^{1+\epsilon}}"/>. </li>
<li> (Close to <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>) One has <img alt="{|A| \geq |G|^{1-O_d(\epsilon)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cgeq+%7CG%7C%5E%7B1-O_d%28%5Cepsilon%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \geq |G|^{1-O_d(\epsilon)}}"/>. </li>
<li> (Trapping) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a proper subgroup of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
We will prove this theorem (which was proven first in the <img alt="{d=2,3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%2C3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2,3}"/> cases for fields <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> of prime order <a href="http://www.ams.org/mathscinet-getitem?mr=2415382">by</a> <a href="http://www.ams.org/mathscinet-getitem?mr=2781932">Helfgott</a>, and then for <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> and general <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> <a href="http://arxiv.org/abs/1001.5069">by Dinai</a>, and finally to general <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> and <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> independently <a href="http://arxiv.org/abs/1005.1858">by Pyber-Szabo</a> and <a href="http://arxiv.org/abs/1005.1881">by Breuillard-Green-Tao</a>) later in this notes. A more qualitative version of this proposition was also previously obtained <a href="http://www.ams.org/mathscinet-getitem?mr=2833482">by Hrushovski</a>. There are also generalisations of the product theorem of importance to number theory, in which the field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> is replaced by a cyclic ring <img alt="{{\bf Z}/q{\bf Z}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+Z%7D%2Fq%7B%5Cbf+Z%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf Z}/q{\bf Z}}"/> (with <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> not necessarily prime); this was achieved first for <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> and <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> square-free <a href="http://www.ams.org/mathscinet-getitem?mr=2587341">by Bourgain, Gamburd, and Sarnak</a>, <a href="http://arxiv.org/abs/1001.3664">by Varju</a> for general <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> and <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/> square-free, and finally by <a href="http://www.math.ias.edu/files/avi/BourgainVarju-1.pdf">this paper of Bourgain and Varju</a> for arbitrary <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> and <img alt="{q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{q}"/>.
</p>
<blockquote><p><b>Exercise 1 (Girth bound)</b>  Assuming Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#prod-slf">1</a>, show that whenever <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> is a symmetric set of generators of <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/> for some finite field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> and some <img alt="{d\geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d\geq 2}"/>, then any element of <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/> can be expressed as the product of <img alt="{O_d( \log^{O_d(1)} |k| )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_d%28+%5Clog%5E%7BO_d%281%29%7D+%7Ck%7C+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_d( \log^{O_d(1)} |k| )}"/> elements from <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/>. (Equivalently, if we add the identity element to <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/>, then <img alt="{S^m = SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%5Em+%3D+SL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S^m = SL_d(k)}"/> for some <img alt="{m = O_d( \log^{O_d(1)} |k| )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%3D+O_d%28+%5Clog%5E%7BO_d%281%29%7D+%7Ck%7C+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m = O_d( \log^{O_d(1)} |k| )}"/>.) This is a special case of a <a href="http://www.ams.org/mathscinet-getitem?mr=1179520">conjecture of Babai and Seress</a>, who conjectured that the bound should hold uniformly for all finite simple groups (in particular, the implied constants here should not actually depend on <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>. The methods used to handle the <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/> case can handle other finite groups of Lie type of bounded rank, but at present we do not have bounds that are independent of the rank. On the other hand, <a href="http://arxiv.org/abs/1109.3550">a recent paper of Helfgott and Seress</a> has almost resolved the conjecture for the permutation groups <img alt="{A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_n}"/>. </p></blockquote>
<p/>
<p>
A key tool to establish product theorems is an argument which is sometimes referred to as the <em>pivot argument</em>. To illustrate this argument, let us first discuss a much simpler (and older) theorem, which has a much weaker conclusion but is valid in any group <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>:
</p>
<blockquote><p><b>Theorem 2 (Baby product theorem)</b> <a name="baby"/> Let <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> be a group, and let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite non-empty subset of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Expansion) One has <img alt="{|A^{-1} A| \geq \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B-1%7D+A%7C+%5Cgeq+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{-1} A| \geq \frac{3}{2} |A|}"/>. </li>
<li> (Close to a subgroup) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a left-coset of a group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| &lt; \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%3C+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| &lt; \frac{3}{2} |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
To prove this theorem, we suppose that the first conclusion does not hold, thus <img alt="{|A^{-1} A| &lt;\frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B-1%7D+A%7C+%3C%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{-1} A| &lt;\frac{3}{2} |A|}"/>. Our task is then to place <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> inside the left-coset of a fairly small group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>.
</p>
<p>
To do this, we take a group element <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>, and consider the intersection <img alt="{A\cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A\cap gA}"/>. <em>A priori</em>, the size of this set could range from anywhere from <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/> to <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/>. However, we can use the hypothesis <img alt="{|A^{-1} A| &lt; \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B-1%7D+A%7C+%3C+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{-1} A| &lt; \frac{3}{2} |A|}"/> to obtain an important dichotomy, reminiscent of the classical fact that two cosets <img alt="{gH, hH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgH%2C+hH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gH, hH}"/> of a subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> are either identical or disjoint:
</p>
<blockquote><p><b>Proposition 3 (Dichotomy)</b> <a name="dich"/> If <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>, then exactly one of the following occurs: </p>
<ul>
<li> (Non-involved case) <img alt="{A \cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA}"/> is empty. </li>
<li> (Involved case) <img alt="{|A \cap gA| &gt; \frac{|A|}{2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gA%7C+%3E+%5Cfrac%7B%7CA%7C%7D%7B2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gA| &gt; \frac{|A|}{2}}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose we are not in the pivot case, so that <img alt="{A \cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA}"/> is non-empty. Let <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> be an element of <img alt="{A \cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA}"/>, then <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{g^{-1} a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} a}"/> both lie in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. The sets <img alt="{A^{-1} a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E%7B-1%7D+a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^{-1} a}"/> and <img alt="{A^{-1} g^{-1} a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E%7B-1%7D+g%5E%7B-1%7D+a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^{-1} g^{-1} a}"/> then both lie in <img alt="{A^{-1} A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E%7B-1%7D+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^{-1} A}"/>. As these sets have cardinality <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> and lie in <img alt="{A^{-1}A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E%7B-1%7DA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^{-1}A}"/>, which has cardinality less than <img alt="{\frac{3}{2}|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B3%7D%7B2%7D%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{3}{2}|A|}"/>, we conclude from the inclusion-exclusion formula that </p>
<p align="center"><img alt="\displaystyle |A^{-1} a \cap A^{-1} g^{-1} a| &gt; \frac{|A|}{2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%7CA%5E%7B-1%7D+a+%5Ccap+A%5E%7B-1%7D+g%5E%7B-1%7D+a%7C+%3E+%5Cfrac%7B%7CA%7C%7D%7B2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle |A^{-1} a \cap A^{-1} g^{-1} a| &gt; \frac{|A|}{2}."/></p>
<p> But the left-hand side is equal to <img alt="{|A \cap gA|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gA|}"/>, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
The above proposition provides a clear separation between two types of elements <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>: the “non-involved” elements, which have nothing to do with <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> (in the sense that <img alt="{A \cap gA = \emptyset}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA+%3D+%5Cemptyset%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA = \emptyset}"/>, and the “involved” elements, which have a lot to do with <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> (in the sense that <img alt="{|A \cap gA| &gt; |A|/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+gA%7C+%3E+%7CA%7C%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap gA| &gt; |A|/2}"/>. The key point is that there is a significant “gap” between the non-involved and involved elements; there are no elements that are only “slightly involved”, in that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gA}"/> intersect a little but not a lot. It is this gap that will allow us to upgrade approximate structure to exact structure. Namely,
</p>
<blockquote><p><b>Proposition 4</b>  The set <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of involved elements is a finite group, and is equal to <img alt="{A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A A^{-1}}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  It is clear that the identity element <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> is involved, and that if <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is involved then so is <img alt="{g^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1}}"/> (since <img alt="{A \cap g^{-1} A = g^{-1}(A \cap gA)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+g%5E%7B-1%7D+A+%3D+g%5E%7B-1%7D%28A+%5Ccap+gA%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap g^{-1} A = g^{-1}(A \cap gA)}"/>. Now suppose that <img alt="{g, h}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%2C+h%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g, h}"/> are both involved. Then <img alt="{A \cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA}"/> and <img alt="{A\cap hA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5Ccap+hA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A\cap hA}"/> have cardinality greater than <img alt="{|A|/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|/2}"/> and are both subsets of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, and so have non-empty intersection. In particular, <img alt="{gA \cap hA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgA+%5Ccap+hA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gA \cap hA}"/> is non-empty, and so <img alt="{A \cap g^{-1} hA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+g%5E%7B-1%7D+hA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap g^{-1} hA}"/> is non-empty. By Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich">3</a>, this makes <img alt="{g^{-1} h}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+h%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} h}"/> involved. It is then clear that <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> is a group.
</p>
<p>
If <img alt="{g \in A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A A^{-1}}"/>, then <img alt="{A \cap gA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA}"/> is non-empty, and so from Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich">3</a> <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is involved. Conversely, if <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is involved, then <img alt="{g \in A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A A^{-1}}"/>. Thus we have <img alt="{H = A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3D+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H = A A^{-1}}"/> as claimed. In particular, <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> is finite. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Now we can quickly wrap up the proof of Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#baby">2</a>. By construction, <img alt="{A \cap gA| &gt; |A|/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+gA%7C+%3E+%7CA%7C%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap gA| &gt; |A|/2}"/> for all <img alt="{g \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in H}"/>,which by double counting shows that <img alt="{|H| &lt; 2|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%3C+2%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| &lt; 2|A|}"/>. As <img alt="{H = A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3D+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H = A A^{-1}}"/>, we see that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a right coset <img alt="{Hg}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BHg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Hg}"/> of <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>; setting <img alt="{H' := g^{-1} H g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%27+%3A%3D+g%5E%7B-1%7D+H+g%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H' := g^{-1} H g}"/>, we conclude that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a left coset <img alt="{gH'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgH%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gH'}"/> of <img alt="{H'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H'}"/>. <img alt="{H'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H'}"/> is a conjugate of <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>, and so <img alt="{|H'| &lt; 2|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%27%7C+%3C+2%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H'| &lt; 2|A|}"/>. If <img alt="{h \in H'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh+%5Cin+H%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h \in H'}"/>, then <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{Ah}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BAh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Ah}"/> both lie in <img alt="{H'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H'}"/> and have cardinality <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/>, so must overlap; and so <img alt="{h \in A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh+%5Cin+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h \in A A^{-1}}"/>. Thus <img alt="{A A^{-1} = H'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+A%5E%7B-1%7D+%3D+H%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A A^{-1} = H'}"/>, and so <img alt="{|H'| &lt; \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%27%7C+%3C+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H'| &lt; \frac{3}{2} |A|}"/>, and Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#baby">2</a> follows.
</p>
<blockquote><p><b>Exercise 2</b>  Show that the constant <img alt="{3/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B3%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{3/2}"/> in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#baby">2</a> cannot be replaced by any larger constant. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 3</b>  Let <img alt="{A \subset G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Csubset+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \subset G}"/> be a finite non-empty set such that <img alt="{|A^2| &lt; 2|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2%7C+%3C+2%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2| &lt; 2|A|}"/>. Show that <img alt="{AA^{-1}=A^{-1} A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BAA%5E%7B-1%7D%3DA%5E%7B-1%7D+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{AA^{-1}=A^{-1} A}"/>. (<em>Hint:</em> If <img alt="{ab^{-1} \in A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bab%5E%7B-1%7D+%5Cin+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ab^{-1} \in A A^{-1}}"/>, show that <img alt="{ab^{-1} = c^{-1} d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bab%5E%7B-1%7D+%3D+c%5E%7B-1%7D+d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ab^{-1} = c^{-1} d}"/> for some <img alt="{c,d \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%2Cd+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c,d \in A}"/>.) </p></blockquote>
<p/>
<blockquote><p><b>Exercise 4</b>  Let <img alt="{A \subset G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Csubset+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \subset G}"/> be a finite non-empty set such that <img alt="{|A^2| &lt; \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2%7C+%3C+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2| &lt; \frac{3}{2} |A|}"/>. Show that there is a finite group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> with <img alt="{|H| &lt; \frac{3}{2} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%3C+%5Cfrac%7B3%7D%7B2%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| &lt; \frac{3}{2} |A|}"/> and a group element <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/> such that <img alt="{A \subset Hg \cap gH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Csubset+Hg+%5Ccap+gH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \subset Hg \cap gH}"/> and <img alt="{H = A A^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3D+A+A%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H = A A^{-1}}"/>. </p></blockquote>
<p/>
<p>
Below the fold, we give further examples of the pivot argument in other group-like situations, including Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#baby">2</a> and also the “sum-product theorem” of <a href="http://www.ams.org/mathscinet-getitem?mr=2053599">Bourgain-Katz-Tao</a> and <a href="http://www.ams.org/mathscinet-getitem?mr=2225493">Bourgain-Glibichuk-Konyagin</a>.
</p>
<p>
<span id="more-5714"/>
</p>
<p/>
<p align="center"><b> —  1. The sum-product theorem  — </b></p>
<p>
Consider a finite non-empty subset <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of a field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>. Then we may form the sumset </p>
<p align="center"><img alt="\displaystyle  A+A := \{a+b: a,b \in A \}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A%2BA+%3A%3D+%5C%7Ba%2Bb%3A+a%2Cb+%5Cin+A+%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A+A := \{a+b: a,b \in A \}"/></p>
<p> and the product set
</p><p align="center"><img alt="\displaystyle  A \cdot A := \{ab: ab \in A \}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A+%5Ccdot+A+%3A%3D+%5C%7Bab%3A+ab+%5Cin+A+%5C%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A \cdot A := \{ab: ab \in A \}."/></p>
<p> The minimal sizes of such sets are well understood:</p>
<blockquote><p><b>Exercise 5</b> <a name="sharp-sum"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite non-empty subset of a field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>. </p>
<ul>
<li>(i) Show that <img alt="{|A+A| \geq |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%2BA%7C+%5Cgeq+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A+A| \geq |A|}"/>, with equality occuring if and only if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is an additive coset <img alt="{A = x+H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+x%2BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = x+H}"/> of an finite additive subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> with some <img alt="{x \in k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in k}"/>. </li>
<li>(ii) Show that <img alt="{|A\cdot A|\geq |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5Ccdot+A%7C%5Cgeq+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A\cdot A|\geq |A|}"/>, with equality occuring if and only if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is either equal to a multiplicative coset <img alt="{A = gH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+gH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = gH}"/> of a finite multiplicative subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{k^\times := k \backslash \{0\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%5E%5Ctimes+%3A%3D+k+%5Cbackslash+%5C%7B0%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k^\times := k \backslash \{0\}}"/> with some <img alt="{g \in k^\times}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+k%5E%5Ctimes%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in k^\times}"/>, or the set <img alt="{\{0\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B0%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{0\}}"/>, or the set <img alt="{\{0\} \cup gH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B0%5C%7D+%5Ccup+gH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{0\} \cup gH}"/> where <img alt="{gH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gH}"/> is a multiplicative coset. </li>
<li>(iii) Show that <img alt="{\max(|A+A|, |A\cdot A|\geq |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmax%28%7CA%2BA%7C%2C+%7CA%5Ccdot+A%7C%5Cgeq+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\max(|A+A|, |A\cdot A|\geq |A|}"/>, with equality occuring if and only if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is either equal to a multiplicative dilate <img alt="{A = cF}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+cF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = cF}"/> of a finite subfield <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> with <img alt="{c \in k^\times}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc+%5Cin+k%5E%5Ctimes%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c \in k^\times}"/>, a singleton set, or an additive subgroup of order <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
The <em>sum-product phenomenon</em> is a robust version of the above observation, asserting that one of <img alt="{A+A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A+A}"/> or <img alt="{A\cdot A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5Ccdot+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A\cdot A}"/> must be significantly larger than <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is not somehow “close” to a genuine subfield of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>. Here is one formulation of this phenomenon:
</p>
<blockquote><p><b>Theorem 5 (Sum-product theorem)</b> <a name="spt"/> Let <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> be a sufficiently small number. Then for any field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> and any finite non-empty subset <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, one of the following statements hold: </p>
<ul>
<li> (Expansion) <img alt="{\max(|A+A|, |A\cdot A|) \geq |A|^{1+\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmax%28%7CA%2BA%7C%2C+%7CA%5Ccdot+A%7C%29+%5Cgeq+%7CA%7C%5E%7B1%2B%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\max(|A+A|, |A\cdot A|) \geq |A|^{1+\epsilon}}"/>. </li>
<li> (Close to a subfield) There is a dilate <img alt="{cF}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BcF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{cF}"/> of a subfield <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> with <img alt="{|F| \ll |A|^{1+O(\epsilon)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C+%5Cll+%7CA%7C%5E%7B1%2BO%28%5Cepsilon%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F| \ll |A|^{1+O(\epsilon)}}"/> and <img alt="{c\neq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bc%5Cneq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{c\neq 0}"/> which contains all but <img alt="{O(|A|^{O(\epsilon)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7BO%28%5Cepsilon%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{O(\epsilon)})}"/> elements of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. </li>
<li> (Smallness) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is an additive subgroup of order <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
If <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> has characteristic zero, then the second option here cannot occur, and we conclude that <img alt="{\max(|A+A|,|A \cdot A|) \geq |A|^{1+\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmax%28%7CA%2BA%7C%2C%7CA+%5Ccdot+A%7C%29+%5Cgeq+%7CA%7C%5E%7B1%2B%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\max(|A+A|,|A \cdot A|) \geq |A|^{1+\epsilon}}"/> for some absolute constant <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> as soon as <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> contains at least two non-zero elements, a claim first established in <img alt="{{\bf R}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf R}}"/> <a href="http://www.ams.org/mathscinet-getitem?mr=820223">by Erdos and Szemeredi</a>. When <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> is a finite field of prime order, the second option can only occur when <img alt="{F=k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%3Dk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F=k}"/>, and we conclude that <img alt="{\max(|A+A|,|A \cdot A|) \geq |A|^{1+\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cmax%28%7CA%2BA%7C%2C%7CA+%5Ccdot+A%7C%29+%5Cgeq+%7CA%7C%5E%7B1%2B%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\max(|A+A|,|A \cdot A|) \geq |A|^{1+\epsilon}}"/> as soon as <img alt="{|A| \leq |k|^{1-C\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cleq+%7Ck%7C%5E%7B1-C%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \leq |k|^{1-C\epsilon}}"/> whenever <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> is sufficiently small, <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/> is an absolute constant, and <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> has at least two non-zero elements. A preliminary version of this result (which required more size assumptions on <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, in particular a bound of the shape <img alt="{|A| \geq |k|^\delta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cgeq+%7Ck%7C%5E%5Cdelta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \geq |k|^\delta}"/>) was obtained by <a href="http://www.ams.org/mathscinet-getitem?mr=2053599">Bourgain, Katz, and Tao</a>, with the version stated above first obtained by <a href="http://www.ams.org/mathscinet-getitem?mr=2053599">Bourgain, Glibichuk, and Konyagin</a>. The proof given here is drawn from <a href="http://www.ams.org/mathscinet-getitem?mr=2289012">my book with Van</a>, and was originally inspired by <a href="http://www.ams.org/mathscinet-getitem?mr=1998834">this paper of Bourgain and Konyagin</a>.
</p>
<blockquote><p><b>Remark 1</b>  There has been a substantial amount of literature on trying to optimise the exponent <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> in the sum-product theorem. A relatively recent survey of this literature can be found in <a href="http://terrytao.wordpress.com/2008/06/17/the-sum-product-phenomenon-in-arbitrary-rings/">this paper of mine</a> (and in the references to the other papers cited in this remark). In <img alt="{{\bf R}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf R}}"/>, the best result currently in this direction is <a href="http://arxiv.org/abs/0806.1040">by Solymosi</a>, who established that one can take <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> arbitrarily close to <img alt="{1/3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2F3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1/3}"/>; for <img alt="{{\bf C}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf C}}"/>, the best result currently is <a href="http://arxiv.org/abs/1111.4977">by Rudnev</a>, who shows that one can take <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> arbitrarily close to <img alt="{19/69}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B19%2F69%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{19/69}"/>. For fields of prime order, one can take <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> arbitrarily close to <img alt="{1/11}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2F11%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1/11}"/>, a <a href="http://arxiv.org/abs/1011.2738">result of Rudnev</a>; an extension to arbitrary finite fields was then obtained <a href="http://arxiv.org/abs/1106.1148">by Li and Roche-Newton</a>. </p></blockquote>
<p/>
<p>
We now start proving Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spt">5</a>. As with Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#baby">2</a>, the engine of the proof is a dichotomy similar to that of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich">3</a>. Whilst the former proposition was modeled on the basic group-theoretic assertion that cosets <img alt="{gH}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BgH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{gH}"/> of a subgroup where either identical or disjoint, this proposition is modeled on the basic linear algebra fact that if <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> is a subfield of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> and <img alt="{\xi \in k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+%5Cin+k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi \in k}"/>, then <img alt="{F+\xi F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%2B%5Cxi+F%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F+\xi F}"/> is either of size <img alt="{|F|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|^2}"/>, or of size <img alt="{|F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|}"/>.
</p>
<blockquote><p><b>Lemma 6 (Dichotomy)</b> <a name="dich-sump"/> Let <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> be a field, let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite non-empty subset of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>, and let <img alt="{\xi \in k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+%5Cin+k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi \in k}"/>. Then at least one of the following statements hold: </p>
<ul>
<li> (Non-involved case) <img alt="{|A + \xi A| = |A|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%2B+%5Cxi+A%7C+%3D+%7CA%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A + \xi A| = |A|^2}"/>. </li>
<li> (Involved case) <img alt="{|A + \xi A| \leq |(A-A) A +(A-A) A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%2B+%5Cxi+A%7C+%5Cleq+%7C%28A-A%29+A+%2B%28A-A%29+A%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A + \xi A| \leq |(A-A) A +(A-A) A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose that we are not in the non-involved case, thus <img alt="{|A + \xi A| \neq |A|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%2B+%5Cxi+A%7C+%5Cneq+%7CA%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A + \xi A| \neq |A|^2}"/>. Then the map <img alt="{(a,b) \mapsto a+\xi b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%29+%5Cmapsto+a%2B%5Cxi+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b) \mapsto a+\xi b}"/> from <img alt="{A\times A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5Ctimes+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A\times A}"/> to <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> is not injective, and so there exists <img alt="{a,b,c,d \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d \in A}"/> with <img alt="{(a,b) \neq (c,d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%2Cb%29+%5Cneq+%28c%2Cd%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a,b) \neq (c,d)}"/> and </p>
<p align="center"><img alt="\displaystyle  a+\xi b = c+\xi d." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++a%2B%5Cxi+b+%3D+c%2B%5Cxi+d.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  a+\xi b = c+\xi d."/></p>
<p> In particular, <img alt="{b \neq d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cneq+d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \neq d}"/>. We then have <img alt="{\xi = (a-c)/(d-b)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+%3D+%28a-c%29%2F%28d-b%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi = (a-c)/(d-b)}"/> and so
</p><p align="center"><img alt="\displaystyle  |A + \xi A| = |(d-b) A + (a-c) A| \leq |(A-A) A +(A-A) A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA+%2B+%5Cxi+A%7C+%3D+%7C%28d-b%29+A+%2B+%28a-c%29+A%7C+%5Cleq+%7C%28A-A%29+A+%2B%28A-A%29+A%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A + \xi A| = |(d-b) A + (a-c) A| \leq |(A-A) A +(A-A) A|."/></p>
<p> <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Remark 2</b>  One can view <img alt="{A+\xi A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2B%5Cxi+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A+\xi A}"/> as measuring the extent to which the dilate <img alt="{\xi A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi A}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is “transverse” to <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. As the “slope” <img alt="{\xi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi}"/> varies, <img alt="{\xi A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi A}"/> “pivots” around the origin, encountering both the (relatively rare) involved slopes, and the (generic) non-involved slopes. It is this geometric picture which led to the term “pivot argument”, as used in particular <a href="http://arxiv.org/abs/0807.2027">by Helfgott</a> (who labeled the non-involved slopes as “pivots”). </p></blockquote>
<p/>
<p>
This dichotomy becomes useful if there is a significant gap between <img alt="{|(A-A) A +(A-A) A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7C%28A-A%29+A+%2B%28A-A%29+A%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|(A-A) A +(A-A) A|}"/> and <img alt="{|A|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^2}"/>. Let’s see how. To prove Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spt">5</a>, we may assume that <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> is larger than some large absolute constant <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/>, as the claim follows from Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#sharp-sum">5</a> otherwise (making <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/> small enough depending on <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/>). by deleting <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/> from <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, and tweaking <img alt="{\epsilon}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon}"/>, noting that we may then assume that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> does not contain <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/>. We suppose that </p>
<p align="center"><img alt="\displaystyle  |A+A|, |A\cdot A|\leq K|A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%2BA%7C%2C+%7CA%5Ccdot+A%7C%5Cleq+K%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A+A|, |A\cdot A|\leq K|A|"/></p>
<p> for some <img alt="{K \leq |A|^{\epsilon_0}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cleq+%7CA%7C%5E%7B%5Cepsilon_0%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \leq |A|^{\epsilon_0}}"/> and some sufficiently small absolute constant <img alt="{\epsilon_0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon_0}"/>. In particular we see that <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> will exceed any quantity of the form <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> if we make <img alt="{\epsilon_0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon_0}"/> small enough and <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/> large enough.</p>
<p>
We would like to boost this control of sums and products to more complex combinations of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. We will need some basic tools from additive combinatorics.
</p>
<blockquote><p><b>Lemma 7 (Ruzsa triangle inequality)</b>  If <img alt="{A,B,C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2CB%2CC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A,B,C}"/> are non-empty finite subsets of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>, then <img alt="{|A-C| \leq \frac{|A-B||B-C|}{|B|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA-C%7C+%5Cleq+%5Cfrac%7B%7CA-B%7C%7CB-C%7C%7D%7B%7CB%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A-C| \leq \frac{|A-B||B-C|}{|B|}}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  This is the additive version of Exercise 4 from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">Notes 4</a>. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Lemma 8 (Ruzsa covering lemma)</b>  If <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> are non-empty finite subsets of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>, then <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> can be covered by at most <img alt="{\frac{|A+B|}{|B|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%7CA%2BB%7C%7D%7B%7CB%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{|A+B|}{|B|}}"/> translates of <img alt="{B-B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB-B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B-B}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  This is the additive version of Exercise 5 from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">Notes 4</a>. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 6 (Sum set estimates)</b>  If <img alt="{A, B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, B}"/> are non-empty finite subsets of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> such that <img alt="{|A+B|\leq K |A|^{1/2}|B|^{1/2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%2BB%7C%5Cleq+K+%7CA%7C%5E%7B1%2F2%7D%7CB%7C%5E%7B1%2F2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A+B|\leq K |A|^{1/2}|B|^{1/2}}"/>, show that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> and <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> can both be covered by <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> translates of the same <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>-approximate group <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>, with <img alt="{|H| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \ll K^{O(1)} |A|}"/>. Conclude that
</p><p align="center"><img alt="\displaystyle  |n_1 A - n_2 A + n_3 B - n_4 B| \ll_{n_1,n_2,n_3,n_4} K^{O(|n_1|+|n_2|+|n_3|+|n_4|)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7Cn_1+A+-+n_2+A+%2B+n_3+B+-+n_4+B%7C+%5Cll_%7Bn_1%2Cn_2%2Cn_3%2Cn_4%7D+K%5E%7BO%28%7Cn_1%7C%2B%7Cn_2%7C%2B%7Cn_3%7C%2B%7Cn_4%7C%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |n_1 A - n_2 A + n_3 B - n_4 B| \ll_{n_1,n_2,n_3,n_4} K^{O(|n_1|+|n_2|+|n_3|+|n_4|)} |A|"/></p>
<p> for any natural numbers <img alt="{n_1,n_2,n_3,n_4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn_1%2Cn_2%2Cn_3%2Cn_4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n_1,n_2,n_3,n_4}"/>, where <img alt="{nA := A+\ldots+A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BnA+%3A%3D+A%2B%5Cldots%2BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{nA := A+\ldots+A}"/> denotes the sum set of <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> copies of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. (<em>Hint:</em> use the additive form of Exercise 7 from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">Notes 4</a>, and the preceding lemmas.) </p></blockquote>
<p/>
<p>
These lemmas allow us to improve the sum-product properties of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> by passing to a large subset <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> (cf. the Balog-Szemeredi-Gowers lemma from <a href="http://terrytao.wordpress.com/2012/01/13/254b-notes-4-the-bourgain-gamburd-expansion-machine/">Notes 4</a>):
</p>
<blockquote><p><b>Lemma 9 (Katz-Tao lemma)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be as above. Then there is a subset <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> with <img alt="{|B| \geq |A|/2K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%7C+%5Cgeq+%7CA%7C%2F2K%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B| \geq |A|/2K}"/> such that <img alt="{|B^2-B^2| \ll K^{O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%5E2-B%5E2%7C+%5Cll+K%5E%7BO%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B^2-B^2| \ll K^{O(1)} |B|}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  The dilates <img alt="{aA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aA}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> with <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/> all lie in a set <img alt="{A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2}"/> of cardinality at most <img alt="{K|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K|A|}"/>. Intuitively, this should force a lot of collision between the <img alt="{aA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aA}"/>, which we will exploit using the sum set estimates. More precisely, observe that </p>
<p align="center"><img alt="\displaystyle  \| \sum_{a \in A} 1_{aA}\|_{\ell^1}= |A|^2" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Csum_%7Ba+%5Cin+A%7D+1_%7BaA%7D%5C%7C_%7B%5Cell%5E1%7D%3D+%7CA%7C%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \sum_{a \in A} 1_{aA}\|_{\ell^1}= |A|^2"/></p>
<p> and hence by Cauchy-Schwarz
</p><p align="center"><img alt="\displaystyle  \| \sum_{a \in A} 1_{aA}\|_{\ell^2}^2 \geq |A|^3/K." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+%5Csum_%7Ba+%5Cin+A%7D+1_%7BaA%7D%5C%7C_%7B%5Cell%5E2%7D%5E2+%5Cgeq+%7CA%7C%5E3%2FK.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| \sum_{a \in A} 1_{aA}\|_{\ell^2}^2 \geq |A|^3/K."/></p>
<p> The left-hand side can be written as
</p><p align="center"><img alt="\displaystyle  \sum_{b \in A} \sum_{a\in A}|aA\cap bA|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bb+%5Cin+A%7D+%5Csum_%7Ba%5Cin+A%7D%7CaA%5Ccap+bA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{b \in A} \sum_{a\in A}|aA\cap bA|"/></p>
<p> and so by the pigeonhole principle we can find <img alt="{b_0 \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb_0+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b_0 \in A}"/> such that
</p><p align="center"><img alt="\displaystyle  \sum_{a\in A}|aA\cap b_0 A| \geq |A|^2/K." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Ba%5Cin+A%7D%7CaA%5Ccap+b_0+A%7C+%5Cgeq+%7CA%7C%5E2%2FK.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{a\in A}|aA\cap b_0 A| \geq |A|^2/K."/></p>
<p> We apply a dilation to set <img alt="{b_0=1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb_0%3D1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b_0=1}"/> (recall that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> does not contain <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/>). If we set <img alt="{B := \{a \in A: |aA\cap A| \geq |A|/2K\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB+%3A%3D+%5C%7Ba+%5Cin+A%3A+%7CaA%5Ccap+A%7C+%5Cgeq+%7CA%7C%2F2K%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B := \{a \in A: |aA\cap A| \geq |A|/2K\}}"/>, we conclude that
</p><p align="center"><img alt="\displaystyle  \sum_{a \in B}|aA\cap A| \geq |A|^2/2K" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Ba+%5Cin+B%7D%7CaA%5Ccap+A%7C+%5Cgeq+%7CA%7C%5E2%2F2K&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{a \in B}|aA\cap A| \geq |A|^2/2K"/></p>
<p> which implies in particular that
</p><p align="center"><img alt="\displaystyle  |B|\geq |A|/2K" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CB%7C%5Cgeq+%7CA%7C%2F2K&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |B|\geq |A|/2K"/></p>
<p> If <img alt="{a \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in B}"/>, then
</p><p align="center"><img alt="\displaystyle  |aA \cap A| \geq |A|/2K;" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CaA+%5Ccap+A%7C+%5Cgeq+%7CA%7C%2F2K%3B&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aA \cap A| \geq |A|/2K;"/></p>
<p> since <img alt="{|aA + aA| \leq K|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CaA+%2B+aA%7C+%5Cleq+K%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|aA + aA| \leq K|A|}"/> we also have
</p><p align="center"><img alt="\displaystyle  |aA + (aA \cap A)| \leq K|A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CaA+%2B+%28aA+%5Ccap+A%29%7C+%5Cleq+K%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aA + (aA \cap A)| \leq K|A|"/></p>
<p> and similarly
</p><p align="center"><img alt="\displaystyle  |A + (aA \cap A)| \leq K|A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA+%2B+%28aA+%5Ccap+A%29%7C+%5Cleq+K%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A + (aA \cap A)| \leq K|A|"/></p>
<p> and thus by the Ruzsa triangle inequality
</p><p align="center"><img alt="\displaystyle  |aA -A| \ll K^{O(1)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CaA+-A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aA -A| \ll K^{O(1)} |A|"/></p>
<p> whenever <img alt="{a \in B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in B}"/>. Informally, let us call a non-zero element <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> <em>good</em> if <img alt="{|aA - A| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CaA+-+A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|aA - A| \ll K^{O(1)} |A|}"/> (but note that this notion of “good” is a bit fuzzy, as it depends on the choice of implied constants in the <img alt="{O()}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O()}"/> notation). Observe that if <img alt="{a,a'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Ca%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,a'}"/> are good, then
</p><p align="center"><img alt="\displaystyle  |aa' A - a A|, |a A - A| \ll K^{O(1)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7Caa%27+A+-+a+A%7C%2C+%7Ca+A+-+A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aa' A - a A|, |a A - A| \ll K^{O(1)} |A|"/></p>
<p> and thus by the Ruzsa triangle inequality
</p><p align="center"><img alt="\displaystyle  |aa' A - A| \ll K^{O(1)} |A|," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7Caa%27+A+-+A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aa' A - A| \ll K^{O(1)} |A|,"/></p>
<p> thus the product of two good elements are good (with somewhat worse implied constants). Similarly, from the Ruzsa covering lemma we see that <img alt="{aA}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aA}"/> and <img alt="{a' A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%27+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a' A}"/> are both covered by <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> translates of <img alt="{A-A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA-A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A-A}"/>, and from this and sum set estimates we see that
</p><p align="center"><img alt="\displaystyle  |(a+a')A-A| \ll K^{O(1)} |A|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%28a%2Ba%27%29A-A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |(a+a')A-A| \ll K^{O(1)} |A|"/></p>
<p> and so the sum of two good elements is again good. Similarly the difference of good elements is good. Applying all these facts, we conclude that all the elements of <img alt="{B^2-B^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%5E2-B%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B^2-B^2}"/> are good, thus <img alt="{|gA-A| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CgA-A%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|gA-A| \ll K^{O(1)} |A|}"/> for all <img alt="{g \in B^2-B^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+B%5E2-B%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in B^2-B^2}"/>. In particular, since <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> exceeds <img alt="{K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^{O(1)}}"/>, we see from the Cauchy-Schwarz inequality that for each <img alt="{g \in B^2-B^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+B%5E2-B%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in B^2-B^2}"/>, there are <img alt="{\gg |A|^3/K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E3%2FK%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^3/K^{O(1)}}"/> solutions to the equation <img alt="{ga_1-a_2=ga_3-a_4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bga_1-a_2%3Dga_3-a_4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ga_1-a_2=ga_3-a_4}"/> with <img alt="{a_1 \neq a_3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_1+%5Cneq+a_3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_1 \neq a_3}"/> and <img alt="{a_1,a_2,a_3,a_4 \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_1%2Ca_2%2Ca_3%2Ca_4+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_1,a_2,a_3,a_4 \in A}"/>. However, there are only <img alt="{|A|^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^4}"/> possible choices for <img alt="{a_1,a_2,a_3,a_4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba_1%2Ca_2%2Ca_3%2Ca_4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a_1,a_2,a_3,a_4}"/>, and each such choice uniquely determines <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>, so there are at most <img alt="{O(K^{O(1)} |A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D+%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)} |A|)}"/> possible choices for <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Note that one could replace <img alt="{B^2-B^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%5E2-B%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B^2-B^2}"/> in the above lemma by any other homogeneous polynomial combination of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>.
</p>
<p>
By applying a dilation, we may assume that <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> contains <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/>. Applying Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich-sump">6</a> to this set <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> (and using sum set estimates), we arrive at the following dichotomy: every field element <img alt="{\xi \in k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+%5Cin+k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi \in k}"/> is either “non-involved” in the sense that <img alt="{|B+\xi B| = |B|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%2B%5Cxi+B%7C+%3D+%7CB%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B+\xi B| = |B|^2}"/>, or is “involved” in the sense that <img alt="{|B+\xi B| \leq C_1 K^{C_1} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%2B%5Cxi+B%7C+%5Cleq+C_1+K%5E%7BC_1%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B+\xi B| \leq C_1 K^{C_1} |B|}"/> for some fixed absolute constant <img alt="{C_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C_1}"/>. By sum set estimates we have <img alt="{|B+BB| \ll K^{O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%2BBB%7C+%5Cll+K%5E%7BO%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B+BB| \ll K^{O(1)} |B|}"/>; as we can assume that <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/>, and hence <img alt="{|B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B|}"/>, is larger than any quantity of the form <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>, this forces all elements of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> to be involved.
</p>
<p>
To exploit this, observe (by repeating the proof of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich-sump">6</a>) that if <img alt="{\xi_1,\xi_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi_1%2C%5Cxi_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi_1,\xi_2}"/> are involved, then the quantities <img alt="{\xi = \xi_1\xi_2, \xi_1+\xi_2, \xi_1-\xi_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi+%3D+%5Cxi_1%5Cxi_2%2C+%5Cxi_1%2B%5Cxi_2%2C+%5Cxi_1-%5Cxi_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi = \xi_1\xi_2, \xi_1+\xi_2, \xi_1-\xi_2}"/> are somewhat involved in the sense that </p>
<p align="center"><img alt="\displaystyle  |B + \xi B|\ll K^{O(1)} |B|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CB+%2B+%5Cxi+B%7C%5Cll+K%5E%7BO%281%29%7D+%7CB%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |B + \xi B|\ll K^{O(1)} |B|"/></p>
<p> for those choices of <img alt="{\xi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi}"/> (where the implied constants depend on <img alt="{C_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C_1}"/>). But as we can assume that <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/>, and hence <img alt="{|B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|B|}"/>, is larger than any quantity of the form <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/>, we see from Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich-sump">6</a> that this forces <img alt="{\xi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cxi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\xi}"/> to be involved as well (this is the crucial step at which approximate structure is improved to exact structure). We thussee that the set <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> of all involved elements is closed under multiplication, addition, and subtraction; as it also contains <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/>, it is a subring of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>. Arguing as in the proof of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich-sump">6</a>, we have that <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> is finite with <img alt="{|F|\ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|\ll K^{O(1)} |A|}"/>; in particular, <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> must now be a finite subfield of <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/>.</p>
<p>
Now we enter the “endgame”, in which we use this <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> to control <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. By previous discussion, <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> contains <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>, and thus <img alt="{|A \cap F| \gg K^{-O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+F%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap F| \gg K^{-O(1)} |A|}"/>. By the Ruzsa triangle inequality applied to <img alt="{A, A \cap F, F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%2C+A+%5Ccap+F%2C+F%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A, A \cap F, F}"/>, this implies that <img alt="{|A+F| \ll K^{O(1)} |F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%2BF%7C+%5Cll+K%5E%7BO%281%29%7D+%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A+F| \ll K^{O(1)} |F|}"/>, and so <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> can be covered by <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> translates of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>. A similar argument applied multiplicatively shows that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> can be covered by <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> dilates of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>. Since a non-trivial translate of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> and a non-trivial dilate of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> intersect in at most one point, we conclude that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> has at most <img alt="{O(K^{O(1)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)})}"/> elements outside of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>, and the claim follows.
</p>
<blockquote><p><b>Remark 3</b>  One can abstract this argument by replacing the multiplicative structure here by an abelian group action; see <a href="http://arxiv.org/abs/0807.2027">this paper of Helfgott</a> for details. The argument can also extend to non-commutative settings, such as division algebras or more generally to arbitrary rings (though in the latter case, the presence of non-trivial zero-divisors becomes a very significant issue); see <a href="http://terrytao.wordpress.com/2008/06/17/the-sum-product-phenomenon-in-arbitrary-rings/">this paper</a> for details. </p></blockquote>
<p/>
<p align="center"><b> —  2. Finite subgroups of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>  — </b></p>
<p>
We will shortly establish Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#prod-slf">1</a>, which can be viewed as a way to describe approximate subgroups of <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>. Before we do so, let us first warm up and digress slightly by by studying <em>genuine</em> finite subgroups <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>, in the model case <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/>, for which <em>ad hoc</em> explicit calculations are available. In order to make the algebraic geometry of the situation cleaner, it is convenient to embed the field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> in its algebraic closure <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>, and similarly embed <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> in <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. This is a group which is also an algebraic variety (identifying the space of <img alt="{2 \times 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2+%5Ctimes+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2 \times 2}"/> matrices with coefficients in <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> with <img alt="{\overline{k}^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^4}"/>), whose group operations are algebraic (in fact, polynomial) maps; in other words, <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> is an <a href="http://en.wikipedia.org/wiki/Algebraic_group">algebraic group</a>. We now consider the question of what finite subgroups of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> can look like. This is a classical question, with a complete classification obtained by Dickson in 1901. The precise classification is somewhat complicated; to give just a taste of this complexity, we observe that the symmetry group of the isocahedron is a finite subgroup of <img alt="{SO_3({\bf R})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSO_3%28%7B%5Cbf+R%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SO_3({\bf R})}"/>, which can be lifted to the spin group <img alt="{Spin_3({\bf R})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSpin_3%28%7B%5Cbf+R%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Spin_3({\bf R})}"/> (giving what is known as the <em>binary isocahedral group</em>, a group of order <img alt="{120}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B120%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{120}"/>), which is a subgroup of <img alt="{Spin_3({\bf C})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSpin_3%28%7B%5Cbf+C%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Spin_3({\bf C})}"/>, which can be identified with <img alt="{SL_2({\bf C})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+C%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf C})}"/>. Because of this, it is possible for some choices of finite field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> to embed the binary isocahedral group into <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> or <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>. Similar considerations obtain for the symmetry group of other Platonic solids. However, if one is willing to settle for a “rough” classification, in which one ignores groups of bounded size (and more generally, is willing just to describe a bounded index subgroup of the group <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>), the situation becomes much simpler. In the characteristic zero case <img alt="{k={\bf C}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%3D%7B%5Cbf+C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k={\bf C}}"/>, for instance, we have <a href="http://en.wikipedia.org/wiki/Jordan%27s_theorem_on_finite_linear_groups">Jordan’s theorem</a>, which asserts that given a finite subgroup <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of <img alt="{SL_d({\bf C})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%7B%5Cbf+C%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d({\bf C})}"/> for some <img alt="{d=O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3DO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=O(1)}"/>, a bounded index subgroup of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is abelian. (Jordan’s theorem was <a href="http://terrytao.wordpress.com/2011/08/27/254a-notes-0-hilberts-fifth-problem-and-related-topics/">discussed further in last quarter’s course</a>.) The finite characteristic case is inherently more complicated though (due in large part to the proliferation of finite subfields), with a satisfactory rough classification only becoming available for general <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> with the work <a href="http://www.ams.org/mathscinet-getitem?mr=2813339">of Larsen and Pink</a> (published in 2011, but which first appeared as a preprint in 1998). However, the <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> case is significantly simpler and can be treated by somewhat <em>ad hoc</em> methods, as we shall now do. The discussion here is loosely based on <a href="http://arxiv.org/abs/1201.1139">this paper of Kowalski</a>.
</p>
<p>
We pause to recall some basic structural facts about <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Elements of this group are <img alt="{2 \times 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2+%5Ctimes+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2 \times 2}"/> matrices with determinant one, and thus have two (algebraic, possibly repeated) eigenvalues <img alt="{t, t^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%2C+t%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t, t^{-1}}"/> for some <img alt="{t\in \overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%5Cin+%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t\in \overline{k}}"/> (note here that we are using the algebraically closed nature of <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>). This allows us to classify elements of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> into three classes: </p>
<ul>
<li> The <em>central</em> elements <img alt="{\pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm 1}"/>; </li>
<li> The <em>regular unipotent elements</em> and their negations, which are non-central elements with a double eigenvalue at <img alt="{+1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%2B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{+1}"/> (or a double eigenvalue at <img alt="{-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-1}"/>); and </li>
<li> The <em>regular semisimple elements</em>, which have two distinct eigenvalues.
</li>
</ul>
<p>
We collectively refer to regular unipotent elements and their negations as <em>regular projectively unipotent elements</em>.
</p>
<blockquote><p><b>Remark 4</b>  The presence of the non-identity central element <img alt="{-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-1}"/> leads to some slight technical annoyances (for instance, it means that <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/> merely an <em>almost simple</em> algebraic group rather than a simple one, in the sense that the only normal algebraic subgroups are finite). One can eliminate this element by working instead with the <em>projective special linear group</em> <img alt="{PSL_2:= SL_2/\{\pm 1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BPSL_2%3A%3D+SL_2%2F%5C%7B%5Cpm+1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{PSL_2:= SL_2/\{\pm 1\}}"/>, but we will not do so here. We remark that if one works in <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/> for <img alt="{d&gt;2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d&gt;2}"/> then the classification of elements becomes significantly more complicated, for instance there exist elements which are semisimple (i.e. diagonalisable) but neither regular nor central, because some but not all of the eigenvalues may be repeated. </p></blockquote>
<p/>
<p>
One can distinguish the unipotent elements from the semisimple ones using the trace: unipotent elements have trace <img alt="{+2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%2B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{+2}"/>, their negations have trace <img alt="{-2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-2}"/>, and the semisimple elements have traces distinct from <img alt="{\pm 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm 2}"/>. The ability to classify elements purely from the trace is a very special fact concerning <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/> which breaks down completely for higher rank matrix groups, but we will not hesitate to take advantage of this fact here.
</p>
<p>
Associated to the above classification are some natural algebraic subgroups of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, including the <a href="http://en.wikipedia.org/wiki/Maximal_torus">standard maximal torus</a> </p>
<p align="center"><img alt="\displaystyle  T(\overline{k}) := \{ \begin{pmatrix} t &amp; 0 \\ 0 &amp; t^{-1} \end{pmatrix}: t \in \overline{k}^\times \}," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++T%28%5Coverline%7Bk%7D%29+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+t+%26+0+%5C%5C+0+%26+t%5E%7B-1%7D+%5Cend%7Bpmatrix%7D%3A+t+%5Cin+%5Coverline%7Bk%7D%5E%5Ctimes+%5C%7D%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  T(\overline{k}) := \{ \begin{pmatrix} t &amp; 0 \\ 0 &amp; t^{-1} \end{pmatrix}: t \in \overline{k}^\times \},"/></p>
<p> the one-dimensional <em>standard unipotent group</em>
</p><p align="center"><img alt="\displaystyle  U(\overline{k}) := \{ \begin{pmatrix} 1 &amp; x \\ 0 &amp; 1 \end{pmatrix}: x \in \overline{k} \}," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++U%28%5Coverline%7Bk%7D%29+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+1+%26+x+%5C%5C+0+%26+1+%5Cend%7Bpmatrix%7D%3A+x+%5Cin+%5Coverline%7Bk%7D+%5C%7D%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  U(\overline{k}) := \{ \begin{pmatrix} 1 &amp; x \\ 0 &amp; 1 \end{pmatrix}: x \in \overline{k} \},"/></p>
<p> and the two-dimensional <a href="http://en.wikipedia.org/wiki/Borel_subgroup">standard Borel subgroup</a>
</p><p align="center"><img alt="\displaystyle  B(\overline{k}) := \{ \begin{pmatrix} t &amp; x \\ 0 &amp; t^{-1} \end{pmatrix}: x \in \overline{k}; t \in \overline{k}^\times \}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++B%28%5Coverline%7Bk%7D%29+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+t+%26+x+%5C%5C+0+%26+t%5E%7B-1%7D+%5Cend%7Bpmatrix%7D%3A+x+%5Cin+%5Coverline%7Bk%7D%3B+t+%5Cin+%5Coverline%7Bk%7D%5E%5Ctimes+%5C%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  B(\overline{k}) := \{ \begin{pmatrix} t &amp; x \\ 0 &amp; t^{-1} \end{pmatrix}: x \in \overline{k}; t \in \overline{k}^\times \}."/></p>
<p> More generally, we define a maximal torus of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> to be a conjugate (in <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>) of the standard maximal torus, a unipotent group to be a conjugate of the standard unipotent group, and a Borel subgroup to be a conjugate of the standard Borel subgroup. (This is not really the “right” way to define these groups, for the purpose of generalisation to other algebraic groups, but will suffice as long as we are only working with <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>.) Note that one can also think of a Borel subgroup as the stabiliser of a one-dimensional subspace of <img alt="{\overline{k}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^2}"/> (using the obvious action of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> on <img alt="{\overline{k}^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^2}"/>). Using the <a href="http://en.wikipedia.org/wiki/Jordan_normal_form">Jordan normal form</a> (again taking advantage of the algebraically closed nature of <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>), we can see how these groups interact with group elements:</p>
<p/><ul>
<li> The central elements lie in every maximal torus and every Borel subgroup. The identity <img alt="{+1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%2B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{+1}"/> lies in every unipotent group, but <img alt="{-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{-1}"/> lies in none of them. </li>
<li> Every regular unipotent element lies in exactly one unipotent group, which in turn lies in exactly one Borel subgroup (the normaliser of the unipotent group). Conversely, a unipotent group consists entirely of regular unipotent elements and the identity <img alt="{+1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%2B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{+1}"/>. </li>
<li> Every regular semisimple element lies in exactly one maximal torus, which in turn lies in exactly two Borel subgroups (the stabiliser of one of the eigenspaces of a regular semisimple element in the torus). Conversely, a maximal torus consists entirely of regular semisimple elements and the central elements <img alt="{\pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm 1}"/>.
</li>
</ul>
<blockquote><p><b>Remark 5</b>  If one was working in a non-algebraically closed field <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> instead of in <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>, one could subdivide the regular semisimple elements into two classes, the <em>split</em> case when the elements can be diagonalised inside <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>, and the <em>non-split</em> case when they can only be diagonalised in a quadratic extension of <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>. This similarly subdivides maximal tori into two families, the split tori and the non-split tori. In the case when one is working over the field <img alt="{{\bf R}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf R}}"/>, the unipotent, split semisimple, and non-split semisimple elements are referred to as parabolic, hyperbolic, and elliptic elements of <img alt="{SL_2({\bf R})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%7B%5Cbf+R%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2({\bf R})}"/> respectively. Fortunately, in our applications we can work in algebraically closed fields and avoid these sorts of finer distinctions. </p></blockquote>
<p/>
<p>
Ignoring the exceptional small examples of subgroups of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, such as the binary isocahedral group mentioned earlier, there are two obvious ways to generate subgroups of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. One is to pass from <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> to a subfield <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>, creating “arithmetic” subgroups of the form <img alt="{SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F)}"/> (or conjugates thereof). The other is to replace <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/> with an algebraic subgroup of the three-dimensional group <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>, such as the maximal tori, unipotent groups, and Borel subgroups mentioned earlier. (Actually, these are the only (connected) proper algebraic subgroups of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>, as can be seen by consideration of the associated Lie algebras.)
</p>
<p>
Observe that if <img alt="{A = SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+SL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = SL_2(F)}"/> is an arithmetic subgroup, then its intersections <img alt="{T(F) := A \cap T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%28F%29+%3A%3D+A+%5Ccap+T%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T(F) := A \cap T(\overline{k})}"/>, <img alt="{U(F) := A \cap U(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%28F%29+%3A%3D+A+%5Ccap+U%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U(F) := A \cap U(\overline{k})}"/>, <img alt="{B(F) := A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28F%29+%3A%3D+A+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(F) := A \cap B(\overline{k})}"/> capture a portion of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> proportionate to the dimensions involved, or more precisely that </p>
<p align="center"><img alt="\displaystyle  |A \cap T(\overline{k})| \ll |A|^{1/3}; |A \cap U(\overline{k})| \ll |A|^{1/3}; \quad |A \cap B(\overline{k})| \ll |A|^{2/3}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA+%5Ccap+T%28%5Coverline%7Bk%7D%29%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%3B+%7CA+%5Ccap+U%28%5Coverline%7Bk%7D%29%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%3B+%5Cquad+%7CA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7C+%5Cll+%7CA%7C%5E%7B2%2F3%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A \cap T(\overline{k})| \ll |A|^{1/3}; |A \cap U(\overline{k})| \ll |A|^{1/3}; \quad |A \cap B(\overline{k})| \ll |A|^{2/3}."/></p>
<p> Indeed, it is easy to see that <img alt="{|A| = |SL_2(F)| \sim |F|^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%3D+%7CSL_2%28F%29%7C+%5Csim+%7CF%7C%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| = |SL_2(F)| \sim |F|^3}"/>, <img alt="{|A \cap T(\overline{k})| = |T(F)| \sim |F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+T%28%5Coverline%7Bk%7D%29%7C+%3D+%7CT%28F%29%7C+%5Csim+%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap T(\overline{k})| = |T(F)| \sim |F|}"/>, and so forth. An important and general <a href="http://www.ams.org/mathscinet-getitem?mr=2781932">observation of Larsen and Pink</a> is that this sort of behaviour is shared by all other finite subgroups of algebraic groups such as <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, as long as these groups are not (mostly) trapped in a proper algebraic subgroup. We first illustrate this phenomenon for the torus groups:</p>
<blockquote><p><b>Proposition 10 (Larsen-Pink inequality, special case)</b> <a name="lpis"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Non-concentration) For any maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>, one has <img alt="{|A \cap T| \ll |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+T%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap T| \ll |A|^{1/3}}"/>. </li>
<li> (Trapping) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> such that <img alt="{|A \cap B| \gg |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose that the trapping hypothesis fails, thus <img alt="{|A \cap B| = o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%3D+o%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| = o(|A|)}"/> for all Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>, where we interpret <img alt="{o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bo%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{o(|A|)}"/> here to mean “less than <img alt="{\epsilon |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon |A|}"/> for an arbitrarily small constant <img alt="{\epsilon&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cepsilon%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\epsilon&gt;0}"/> which we are at liberty to choose”. (If one is uncomfortable with this type of definition, one can instead consider a sequence of potential counterexamples <img alt="{A = A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+A_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = A_n}"/> to the above proposition in various groups <img alt="{SL_2(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k_n})}"/>, in which <img alt="{\sup_B |A \cap B| = o_{n \rightarrow \infty}(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csup_B+%7CA+%5Ccap+B%7C+%3D+o_%7Bn+%5Crightarrow+%5Cinfty%7D%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sup_B |A \cap B| = o_{n \rightarrow \infty}(|A|)}"/>. Alternatively, one can also rephrase this argument if desired in the language of nonstandard analysis.) In particular, we see that any coset of <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> occupies a fraction <img alt="{o(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bo%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{o(1)}"/> at most of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. Thus, for instance, if we select an element <img alt="{\begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5C+c+%26+d+%5Cend%7Bpmatrix%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}"/> from <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> uniformly at random, then with probability <img alt="{1-o(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1-o%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1-o(1)}"/>, <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> is non-zero, and similarly for <img alt="{a,c,d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cc%2Cd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,c,d}"/>. To put it more informally, the matrix entries of an element of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> are “generically” non-zero. Similarly if we first conjugate <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> by a fixed group element.
</p>
<p>
We need to show that <img alt="{|A \cap T| \ll |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+T%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap T| \ll |A|^{1/3}}"/> for any maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>. By conjugation we may take <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> to be the standard maximal torus <img alt="{T = T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT+%3D+T%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T = T(\overline{k})}"/>. Set <img alt="{A' := A \cap T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%3A%3D+A+%5Ccap+T%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' := A \cap T(\overline{k})}"/>, then <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> is a subgroup of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of the form </p>
<p align="center"><img alt="\displaystyle  A' := \{ \begin{pmatrix} t &amp; 0 \ &amp; t^{-1} \end{pmatrix}: t\in H \}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A%27+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+t+%26+0+%5C+%26+t%5E%7B-1%7D+%5Cend%7Bpmatrix%7D%3A+t%5Cin+H+%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A' := \{ \begin{pmatrix} t &amp; 0 \ &amp; t^{-1} \end{pmatrix}: t\in H \}"/></p>
<p> for some finite multiplicative subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{\overline{k}^\times}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E%5Ctimes%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^\times}"/>. We may assume that <img alt="{|H|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H|}"/> is larger than any given absolute constant, as the claim is trivial otherwise. Our task is to show that <img alt="{|H|^3 \ll |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C%5E3+%5Cll+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H|^3 \ll |A|}"/>.</p>
<p>
Let <img alt="{g = \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%3D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5C+c+%26+d+%5Cend%7Bpmatrix%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g = \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}"/> be a typical element of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. By the preceding discussion, we may assume that <img alt="{a,b,c,d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d}"/> are all non-zero. Since <img alt="{A'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A'}"/> is a subgroup of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, we have <img alt="{A' g A' g A' \subset A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+g+A%27+g+A%27+%5Csubset+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' g A' g A' \subset A}"/>, thus </p>
<p align="center"><img alt="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_2 &amp; 0 \ &amp; t_2^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cbegin%7Bpmatrix%7D+t_1+%26+0+%5C+%26+t_1%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5Cc+%26+d+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+t_2+%26+0+%5C+%26+t_2%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5Cc+%26+d+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+t_3+%26+0+%5C+%26+t_3%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cin+A&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_2 &amp; 0 \ &amp; t_2^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A"/></p>
<p> for all <img alt="{t_1,t_2,t_3 \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2Ct_2%2Ct_3+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1,t_2,t_3 \in H}"/>. We evaluate the inner matrix products to obtain that
</p><p align="center"><img alt="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a^2 t_2 + bc t_2^{-1} &amp; ac t_2 + bd t_2^{-1} \\ ac t_2 + cd t_2^{-1} &amp; bc t_2 + d^2 t_2^{-1} \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cbegin%7Bpmatrix%7D+t_1+%26+0+%5C+%26+t_1%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+a%5E2+t_2+%2B+bc+t_2%5E%7B-1%7D+%26+ac+t_2+%2B+bd+t_2%5E%7B-1%7D+%5C%5C+ac+t_2+%2B+cd+t_2%5E%7B-1%7D+%26+bc+t_2+%2B+d%5E2+t_2%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+t_3+%26+0+%5C+%26+t_3%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cin+A&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a^2 t_2 + bc t_2^{-1} &amp; ac t_2 + bd t_2^{-1} \\ ac t_2 + cd t_2^{-1} &amp; bc t_2 + d^2 t_2^{-1} \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A"/></p>
<p> for <img alt="{t_1,t_2,t_3 \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2Ct_2%2Ct_3+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1,t_2,t_3 \in H}"/>.</p>
<p>
Because <img alt="{a,b,c,d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d}"/> are non-zero, we see that for all but <img alt="{O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(1)}"/> values of <img alt="{t_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_2}"/>, all four entries of the middle matrix here are non-zero. As a consequence, if one fixes <img alt="{t_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_2}"/> and lets <img alt="{t_1,t_3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2Ct_3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1,t_3}"/> vary, all of the triple products given above are distinct. Note that if one takes the above triple product and multiplies the diagonal entries together, the <img alt="{t_1, t_3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2C+t_3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1, t_3}"/> terms cancel and one obtains <img alt="{(a^2 t_2 + bc t_2^{-1}) (bc t_2 + d^2 t_2^{-1})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28a%5E2+t_2+%2B+bc+t_2%5E%7B-1%7D%29+%28bc+t_2+%2B+d%5E2+t_2%5E%7B-1%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(a^2 t_2 + bc t_2^{-1}) (bc t_2 + d^2 t_2^{-1})}"/>. This rational map (as a function of <img alt="{t_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_2}"/>) is at most four-to-one; each value of this map is associated to at most four values of <img alt="{t_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_2}"/>. Putting all this together, we conclude that there are <img alt="{\gg |H|^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CH%7C%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |H|^3}"/> different triple products one can form here as <img alt="{t_1,t_2,t_3 \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2Ct_2%2Ct_3+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1,t_2,t_3 \in H}"/> vary, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 7</b> <a name="lpis-alt"/> Establish a variant of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis">10</a> in which the maximal tori are replaced by unipotent groups. </p></blockquote>
<p/>
<p>
Given a group element <img alt="{g \in SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2(\overline{k})}"/>, let <img alt="{Conj(g) := \{ hgh^{-1}: h \in SL_2(\overline{k}) \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29+%3A%3D+%5C%7B+hgh%5E%7B-1%7D%3A+h+%5Cin+SL_2%28%5Coverline%7Bk%7D%29+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g) := \{ hgh^{-1}: h \in SL_2(\overline{k}) \}}"/> be the conjugacy class of <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>. The behaviour of this class depends on the nature of <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>:
</p>
<blockquote><p><b>Exercise 8</b> <a name="conjc"/> Let <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> be an element of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. </p>
<ul>
<li>(i) If <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is central, show that <img alt="{Conj(g) = \{\pm 1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29+%3D+%5C%7B%5Cpm+1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g) = \{\pm 1\}}"/>. </li>
<li>(ii) If <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is regular unipotent, show that <img alt="{Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g)}"/> is the space of all regular unipotent elements. </li>
<li>(iii) If <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is negative of a regular unipotent element, show that <img alt="{Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g)}"/> is the space of all negatives of regular unipotent elements. </li>
<li>(iv) If <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is regular semisimple, show that <img alt="{Conj(g) := \{ g'\in SL_2(\overline{k}): \hbox{tr}(g)= \hbox{tr}(g')\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29+%3A%3D+%5C%7B+g%27%5Cin+SL_2%28%5Coverline%7Bk%7D%29%3A+%5Chbox%7Btr%7D%28g%29%3D+%5Chbox%7Btr%7D%28g%27%29%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g) := \{ g'\in SL_2(\overline{k}): \hbox{tr}(g)= \hbox{tr}(g')\}}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
We can “dualise” the upper bound on maximal tori in Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis">10</a> into a lower bound on conjugacy classes:
</p>
<blockquote><p><b>Proposition 11 (Large conjugacy classes)</b> <a name="conj-large"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Large conjugacy classes) For any regular semisimple or regular projectively unipotent <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, one has <img alt="{|A \cap Conj(g)| \gg |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+Conj%28g%29%7C+%5Cgg+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap Conj(g)| \gg |A|^{2/3}}"/>. </li>
<li> (Trapping) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> such that <img alt="{|A \cap B| \gg |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  As before we may assume that <img alt="{|A \cap B| =o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%3Do%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| =o(|A|)}"/> for all Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Let <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/> be regular semisimple, and consider the map <img alt="{\phi: h \mapsto hgh^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%3A+h+%5Cmapsto+hgh%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi: h \mapsto hgh^{-1}}"/> from <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> to <img alt="{A \cap Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+Conj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap Conj(g)}"/>. For each <img alt="{g' \in A \cap Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%27+%5Cin+A+%5Ccap+Conj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g' \in A \cap Conj(g)}"/>, the preimage of <img alt="{g'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g'}"/> by <img alt="{\phi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi}"/> is contained in a coset of the centraliser <img alt="{C(g') := \{ h \in SL_2(\overline{k}): hg'=g'h\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%28g%27%29+%3A%3D+%5C%7B+h+%5Cin+SL_2%28%5Coverline%7Bk%7D%29%3A+hg%27%3Dg%27h%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C(g') := \{ h \in SL_2(\overline{k}): hg'=g'h\}}"/> of <img alt="{g'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g'}"/>. As <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> (and hence <img alt="{g'}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%27%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g'}"/>) is regular semisimple or regular projectively unipotent, this centraliser is a maximal torus or (two copies of) a unipotent group (this can be seen by placing <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> in Jordan normal form). By Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis">10</a> or Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-alt">7</a>, we conclude that each preimage of <img alt="{\phi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi}"/> has cardinality <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/>, which forces the range to have cardinality <img alt="{\gg |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{2/3}}"/> as claimed. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
We remark that this gives a dichotomy analogous to Lemma <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich">3</a> or Lemma <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#dich-sump">6</a> in the case <img alt="{|A\cap B| =o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5Ccap+B%7C+%3Do%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A\cap B| =o(|A|)}"/>. Namely, for any <img alt="{g \in SL_2({\overline{k}})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%7B%5Coverline%7Bk%7D%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2({\overline{k}})}"/>, either <img alt="{A \cap Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+Conj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap Conj(g)}"/> is empty, or <img alt="{|A \cap Conj(g)| \gg |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+Conj%28g%29%7C+%5Cgg+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap Conj(g)| \gg |A|^{2/3}}"/>. We will take advantage of a dichotomy similar to this (but for tori instead of conjugacy classes) in the next section.
</p>
<p>
We can match the lower bound in Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#conj-large">11</a> with an upper bound:
</p>
<blockquote><p><b>Proposition 12 (Larsen-Pink inequality, another special case)</b> <a name="lips-2"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Non-concentration) For any regular semisimple <img alt="{g \in SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2(\overline{k})}"/>, one has <img alt="{|A \cap Conj(g)| \ll |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+Conj%28g%29%7C+%5Cll+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap Conj(g)| \ll |A|^{2/3}}"/>. </li>
<li> (Trapping) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> such that <img alt="{|A \cap B| \gg |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  Again, we may assume that <img alt="{|A \cap B| = o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%3D+o%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| = o(|A|)}"/> for all Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. In particular, we may take <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> larger than any given absolute constant. Let <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> be regular semisimple, and let <img alt="{S:= A \cap Conj(g) =\{ s \in A: \hbox{tr}(s) = \hbox{tr}(g)\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%3A%3D+A+%5Ccap+Conj%28g%29+%3D%5C%7B+s+%5Cin+A%3A+%5Chbox%7Btr%7D%28s%29+%3D+%5Chbox%7Btr%7D%28g%29%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S:= A \cap Conj(g) =\{ s \in A: \hbox{tr}(s) = \hbox{tr}(g)\}}"/>; our task is to show that <img alt="{|S| \ll |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CS%7C+%5Cll+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|S| \ll |A|^{2/3}}"/>. Note from Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#conjc">8</a> that <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is conjugate to <img alt="{g^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1}}"/>, and so <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> is symmetric: <img alt="{S = S^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS+%3D+S%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S = S^{-1}}"/>. Also, <img alt="{Sa=aS}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSa%3DaS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Sa=aS}"/> for all <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/>.
</p>
<p>
Observe that whenever <img alt="{a, b \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2C+b+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a, b \in A}"/> and <img alt="{s \in S \cap a^{-1} S \cap b^{-1} S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bs+%5Cin+S+%5Ccap+a%5E%7B-1%7D+S+%5Ccap+b%5E%7B-1%7D+S%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{s \in S \cap a^{-1} S \cap b^{-1} S}"/>, then the triple <img alt="{(s,as, bs)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28s%2Cas%2C+bs%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(s,as, bs)}"/> lies in <img alt="{S^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S^3}"/>; conversely, every triple in <img alt="{S^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S^3}"/> arises in this manner. Thus we have the identity </p>
<p align="center"><img alt="\displaystyle  |S|^3 = \sum_{a,b \in A} |S \cap a^{-1} S \cap b^{-1} S|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CS%7C%5E3+%3D+%5Csum_%7Ba%2Cb+%5Cin+A%7D+%7CS+%5Ccap+a%5E%7B-1%7D+S+%5Ccap+b%5E%7B-1%7D+S%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |S|^3 = \sum_{a,b \in A} |S \cap a^{-1} S \cap b^{-1} S|."/></p>
<p> We will show that <a name="aba">
</a></p><p align="center"><a name="aba"><img alt="\displaystyle  \sum_{a,b \in A} |S \cap a^{-1} S \cap b^{-1} S| \ll |A|^2 + |A|^{4/3} |S|, \ \ \ \ \ (1)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Ba%2Cb+%5Cin+A%7D+%7CS+%5Ccap+a%5E%7B-1%7D+S+%5Ccap+b%5E%7B-1%7D+S%7C+%5Cll+%7CA%7C%5E2+%2B+%7CA%7C%5E%7B4%2F3%7D+%7CS%7C%2C+%5C+%5C+%5C+%5C+%5C+%281%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{a,b \in A} |S \cap a^{-1} S \cap b^{-1} S| \ll |A|^2 + |A|^{4/3} |S|, \ \ \ \ \ (1)"/></a></p><a name="aba">
</a><p><a name="aba"/> which will give <img alt="{|S| \ll |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CS%7C+%5Cll+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|S| \ll |A|^{2/3}}"/> as required.</p>
<p>
We now establish <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#aba">(1)</a>. We divide into several contributions. First suppose that <img alt="{a = \pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%3D+%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a = \pm 1}"/>. Then we bound the summand by <img alt="{|S|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CS%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|S|}"/>; there are <img alt="{O(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|)}"/> summands here, leading to a total contribution of <img alt="{O(|A| |S|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C+%7CS%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A| |S|)}"/>, which is acceptable. Similarly if <img alt="{b=\pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%3D%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b=\pm 1}"/>, or <img alt="{a = \pm b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%3D+%5Cpm+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a = \pm b}"/>, so we may restrict to the remaining cases when <img alt="{\pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm 1}"/>, <img alt="{\pm a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm a}"/>, <img alt="{\pm b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm b}"/> are distinct. In particular, <img alt="{a, b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2C+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a, b}"/> are now either regular unipotent or regular semisimple.
</p>
<p>
We now consider the case in which <img alt="{1,a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2Ca%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1,a,b}"/> are linearly dependent (in the space <img alt="{M_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M_2(\overline{k})}"/> of <img alt="{2\times 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%5Ctimes+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2\times 2}"/> matrices). For fixed <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/>, this constrains <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> to either a maximal torus or a unipotent group (depending on whether <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> is regular semisimple or regular projectively unipotent); this is easiest to see by placing <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> in Jordan canonical form. By the preceding results, we see that there are <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/> choices of <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> for each <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/>, leading to a contribution of <img alt="{O( |A|^{4/3} |S| )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28+%7CA%7C%5E%7B4%2F3%7D+%7CS%7C+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O( |A|^{4/3} |S| )}"/> in this case, which is acceptable. So we may now take <img alt="{1,a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2Ca%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1,a,b}"/> to be linearly independent.
</p>
<p>
The set <img alt="{S \cap a^{-1} S \cap b^{-1} S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS+%5Ccap+a%5E%7B-1%7D+S+%5Ccap+b%5E%7B-1%7D+S%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S \cap a^{-1} S \cap b^{-1} S}"/> is the intersection of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> with the affine line </p>
<p align="center"><img alt="\displaystyle  \ell := \{ s \in M_2(\overline{k}); \hbox{tr}(s) = \hbox{tr}(as) = \hbox{tr}(bs) = \hbox{tr}(g) \};" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cell+%3A%3D+%5C%7B+s+%5Cin+M_2%28%5Coverline%7Bk%7D%29%3B+%5Chbox%7Btr%7D%28s%29+%3D+%5Chbox%7Btr%7D%28as%29+%3D+%5Chbox%7Btr%7D%28bs%29+%3D+%5Chbox%7Btr%7D%28g%29+%5C%7D%3B&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \ell := \{ s \in M_2(\overline{k}); \hbox{tr}(s) = \hbox{tr}(as) = \hbox{tr}(bs) = \hbox{tr}(g) \};"/></p>
<p> this is indeed a line when <img alt="{1,a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2Ca%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1,a,b}"/> are linearly independent. In most cases, this line <img alt="{\ell}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell}"/> will intersect <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> (which we can view as a quadric surface in <img alt="{M_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M_2(\overline{k})}"/>) in at most two points, leading to a contribution of <img alt="{O(|A|^2)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E2%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^2)}"/> for this case, which is acceptable. The only cases left to treat are when the line <img alt="{\ell}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell}"/> are incident to <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. This only occurs when the line <img alt="{\ell}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell}"/> takes the form <img alt="{hU}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BhU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{hU}"/> for some <img alt="{h \in SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh+%5Cin+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h \in SL_2(\overline{k})}"/> and unipotent group <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/>; this is easiest to see by multiplying <img alt="{\ell}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cell%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\ell}"/> on the left so that it contains the identity, and then placing another element of the line in Jordan normal form. In that case, we have
</p><p align="center"><img alt="\displaystyle  \hbox{tr}(hu) = \hbox{tr}(ahu) = \hbox{tr}(bhu) = \hbox{tr}(g)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Chbox%7Btr%7D%28hu%29+%3D+%5Chbox%7Btr%7D%28ahu%29+%3D+%5Chbox%7Btr%7D%28bhu%29+%3D+%5Chbox%7Btr%7D%28g%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \hbox{tr}(hu) = \hbox{tr}(ahu) = \hbox{tr}(bhu) = \hbox{tr}(g)"/></p>
<p> for all <img alt="{u \in U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu+%5Cin+U%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u \in U}"/>. This forces <img alt="{h, ah, bh}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh%2C+ah%2C+bh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h, ah, bh}"/> to all lie in the Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> associated to <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/> (this is easiest to see by first conjugating <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/> into the standard unipotent group <img alt="{U(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U(\overline{k})}"/>). In particular, <img alt="{a, b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2C+b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a, b}"/> both lie in <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Furthermore, if we write <img alt="{\hbox{tr}(g) = t + t^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Btr%7D%28g%29+%3D+t+%2B+t%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{tr}(g) = t + t^{-1}}"/>, then the diagonal entries of <img alt="{h,ah,bh}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh%2Cah%2Cbh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h,ah,bh}"/> are <img alt="{t,t^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%2Ct%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t,t^{-1}}"/> or <img alt="{t^{-1},t}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%5E%7B-1%7D%2Ct%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t^{-1},t}"/>, and so the diagonal entries of <img alt="{a,b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b}"/> are either <img alt="{1,1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2C1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1,1}"/> or <img alt="{t^{-2},t^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%5E%7B-2%7D%2Ct%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t^{-2},t^2}"/> or <img alt="{t^2,t^{-2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt%5E2%2Ct%5E%7B-2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t^2,t^{-2}}"/>. In particular, <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/> is the stabiliser of one of the eigenvectors of <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> – so for fixed <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/>, there are at most two choices for <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/> (recall that <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> was regular). Furthermore, for fixed <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/> and <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/>, <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> is constrained to lie in at most three cosets of <img alt="{U}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U}"/>. As such, there are only <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/> choices of <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> here for each <img alt="{a}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a}"/>, giving another contribution of <img alt="{O(|A|^{4/3}|S|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B4%2F3%7D%7CS%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{4/3}|S|)}"/>, and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 9</b> <a name="chau"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, such that <img alt="{|A \cap B| = o(|A|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%3D+o%28%7CA%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| = o(|A|)}"/> for all Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>. Show that at most <img alt="{O(|A|^{2/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B2%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{2/3})}"/> of the elements of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> are unipotent. </p></blockquote>
<p/>
<p>
We can use the upper bound on conjugacy classes to obtain a lower bound on tori:
</p>
<blockquote><p><b>Proposition 13 (Large tori)</b> <a name="tori-large"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Large torus) For any regular semisimple <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, one has <img alt="{|A \cap T| \gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+T%7C+%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap T| \gg |A|^{1/3}}"/>, where <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is the unique maximal torus containing <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>. </li>
<li> (Trapping) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> such that <img alt="{|A \cap B| \gg |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  We can of course assume that the trapping case does not occur. We consider the map <img alt="{\phi: a\mapsto aga^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%3A+a%5Cmapsto+aga%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi: a\mapsto aga^{-1}}"/> from <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> to <img alt="{A \cap Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+Conj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap Conj(g)}"/>. By Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lips-2">12</a>, the range of <img alt="{\phi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi}"/> has cardinality <img alt="{O(|A|^{2/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B2%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{2/3})}"/>, so by the pigeonhole principle, there is a preimage of <img alt="{A \cap Conj(g)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+Conj%28g%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap Conj(g)}"/> of cardinality <img alt="{\gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{1/3}}"/>. But all preimages are conjugate to each other, so the preimage of <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> has cardinality <img alt="{\gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{1/3}}"/>. But this preimage is the intersection of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> with the centraliser of <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>, which two cosets of <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>, and so <img alt="{|A \cap T| \gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+T%7C+%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap T| \gg |A|^{1/3}}"/> as required. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 10</b> <a name="large-uni"/> Establish a variant of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#tori-large">13</a> in which <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> is regular unipotent instead of regular semisimple, and <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is replaced with the unique unipotent group containing <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>. </p></blockquote>
<p/>
<p>
This gives a second (and particularly useful) dichotomy: assuming <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is not trapped by a Borel subgroup, for a maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>, <img alt="{|A\cap T|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5Ccap+T%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A\cap T|}"/> is either zero or comparable to <img alt="{|A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^{1/3}}"/>.
</p>
<p>
To exploit this, we use the following counting argument <a href="http://www.ams.org/mathscinet-getitem?mr=2781932">of Larsen and Pink</a> (which is also reminiscent of an old argument of Jordan, used to prove <a href="http://en.wikipedia.org/wiki/Jordan%E2%80%93Schur_theorem">his theorem</a> mentioned previously), followed by some <em>ad hoc</em> arguments specific to <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>. We continue to assume that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is not trapped by a Borel subgroup. Let <img alt="{Z := A \cap\{+1,-1\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BZ+%3A%3D+A+%5Ccap%5C%7B%2B1%2C-1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Z := A \cap\{+1,-1\}}"/> denote the central elements of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, thus <img alt="{|Z|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CZ%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|Z|}"/> is either <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> or <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>. Observe that every element in <img alt="{A \backslash Z}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Cbackslash+Z%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \backslash Z}"/> is either regular projectively unipotent or regular semisimple; in the latter case, the element lies in a unique maximal torus, which also contains <img alt="{Z}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BZ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Z}"/>. We conclude that </p>
<p align="center"><img alt="\displaystyle |A|-|Z| = u|Z| + \sum_T (|A \cap T| - |Z|)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%7CA%7C-%7CZ%7C+%3D+u%7CZ%7C+%2B+%5Csum_T+%28%7CA+%5Ccap+T%7C+-+%7CZ%7C%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle |A|-|Z| = u|Z| + \sum_T (|A \cap T| - |Z|)"/></p>
<p> where <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> ranges over all the maximal tori that intersect <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, and <img alt="{u}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u}"/> is the number of regular projective unipotents in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>.</p>
<p>
If we conjugate a maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> by an element of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, we get another maximal torus, or the same maximal torus if the element used to conjugate <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> in was in the normaliser <img alt="{N_A(T) := \{ a \in A: a T=Ta\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BN_A%28T%29+%3A%3D+%5C%7B+a+%5Cin+A%3A+a+T%3DTa%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{N_A(T) := \{ a \in A: a T=Ta\}}"/> of <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>. Thus, by the <a href="http://en.wikipedia.org/wiki/Group_action#Orbit-stabilizer_theorem">orbit-stabilizer theorem</a>, there are exactly <img alt="{|A|/|N_A(T)|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%2F%7CN_A%28T%29%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|/|N_A(T)|}"/> tori conjugate to <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. We thus see that </p>
<p align="center"><img alt="\displaystyle |A|-|Z| = u + \sum_{T \in {\mathcal T}} \frac{|A|}{|N_A(T)|} (|A \cap T| - |Z|)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%7CA%7C-%7CZ%7C+%3D+u+%2B+%5Csum_%7BT+%5Cin+%7B%5Cmathcal+T%7D%7D+%5Cfrac%7B%7CA%7C%7D%7B%7CN_A%28T%29%7C%7D+%28%7CA+%5Ccap+T%7C+-+%7CZ%7C%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle |A|-|Z| = u + \sum_{T \in {\mathcal T}} \frac{|A|}{|N_A(T)|} (|A \cap T| - |Z|)"/></p>
<p> where <img alt="{{\mathcal T}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cmathcal+T%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\mathcal T}}"/> is a collection of representatives of conjugacy classes of maximal tori intersecting <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> in a regular semisimple element. We rearrange this as
</p><p align="center"><img alt="\displaystyle  1 = \frac{u|Z|+|Z|}{|A|} + \sum_{T \in {\mathcal T}} \frac{1}{[N_A(T):A \cap T]} (1 - \frac{|Z|}{|A \cap T|})." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++1+%3D+%5Cfrac%7Bu%7CZ%7C%2B%7CZ%7C%7D%7B%7CA%7C%7D+%2B+%5Csum_%7BT+%5Cin+%7B%5Cmathcal+T%7D%7D+%5Cfrac%7B1%7D%7B%5BN_A%28T%29%3AA+%5Ccap+T%5D%7D+%281+-+%5Cfrac%7B%7CZ%7C%7D%7B%7CA+%5Ccap+T%7C%7D%29.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  1 = \frac{u|Z|+|Z|}{|A|} + \sum_{T \in {\mathcal T}} \frac{1}{[N_A(T):A \cap T]} (1 - \frac{|Z|}{|A \cap T|})."/></p>
<p> Note that if <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is a maximal torus, the normaliser of <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> in <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> has index <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>. As such, <img alt="{A\cap T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5Ccap+T%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A\cap T}"/> has index at most two in <img alt="{N_A(T)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BN_A%28T%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{N_A(T)}"/>, and so <img alt="{\frac{1}{[N_A(T):A \cap T]}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B1%7D%7B%5BN_A%28T%29%3AA+%5Ccap+T%5D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{1}{[N_A(T):A \cap T]}}"/> is either equal to <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> or <img alt="{1/2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2F2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1/2}"/> for each <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>. From the preceding bounds on tori and unipotent elements, we also have <img alt="{\frac{|Z|}{|A \cap T|} \sim |A|^{-1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7B%7CZ%7C%7D%7B%7CA+%5Ccap+T%7C%7D+%5Csim+%7CA%7C%5E%7B-1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{|Z|}{|A \cap T|} \sim |A|^{-1/3}}"/> and <img alt="{\frac{u+|Z|}{|A|} = O( |A|^{-1/3} )}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7Bu%2B%7CZ%7C%7D%7B%7CA%7C%7D+%3D+O%28+%7CA%7C%5E%7B-1%2F3%7D+%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{u+|Z|}{|A|} = O( |A|^{-1/3} )}"/>. As we are assuming <img alt="{|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|}"/> to be large, the above equation is only consistent when <img alt="{{\mathcal T}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cmathcal+T%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\mathcal T}}"/> has cardinality <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> or <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>, and <img alt="{\frac{u|Z|+|Z|}{|A|}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cfrac%7Bu%7CZ%7C%2B%7CZ%7C%7D%7B%7CA%7C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\frac{u|Z|+|Z|}{|A|}}"/> is comparable to <img alt="{|A|^{-1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E%7B-1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^{-1/3}}"/>, or equivalently that <img alt="{u}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{u}"/> is comparable to <img alt="{|A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|^{2/3}}"/>. Thus, <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> has plenty of regular projective unipotents (matching the upper bound from Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#chau">9</a>); in particular, there is at least one regular unipotent.</p>
<p>
Applying a conjugation, we may assume that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> contains <img alt="{e := \begin{pmatrix} 1 &amp; 1 \\ 0 &amp; 1 \end{pmatrix}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Be+%3A%3D+%5Cbegin%7Bpmatrix%7D+1+%26+1+%5C%5C+0+%26+1+%5Cend%7Bpmatrix%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{e := \begin{pmatrix} 1 &amp; 1 \\ 0 &amp; 1 \end{pmatrix}}"/>, thus </p>
<p align="center"><img alt="\displaystyle  A \cap U(\overline{k}) = \{\begin{pmatrix} 1 &amp; t \\ 0 &amp; 1 \end{pmatrix}: t \in E\}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A+%5Ccap+U%28%5Coverline%7Bk%7D%29+%3D+%5C%7B%5Cbegin%7Bpmatrix%7D+1+%26+t+%5C%5C+0+%26+1+%5Cend%7Bpmatrix%7D%3A+t+%5Cin+E%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A \cap U(\overline{k}) = \{\begin{pmatrix} 1 &amp; t \\ 0 &amp; 1 \end{pmatrix}: t \in E\}"/></p>
<p> for some additive group <img alt="{E \subset \overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE+%5Csubset+%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E \subset \overline{k}}"/> containing <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/>. By Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-alt">7</a>, <img alt="{|E| \ll |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \ll |A|^{1/3}}"/>; by Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#large-uni">10</a>, we have <img alt="{|E|\gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E|\gg |A|^{1/3}}"/> also.</p>
<p>
The map <img alt="{a \mapsto a(A \cap U(\overline{k}))a^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cmapsto+a%28A+%5Ccap+U%28%5Coverline%7Bk%7D%29%29a%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \mapsto a(A \cap U(\overline{k}))a^{-1}}"/> maps <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> to unipotent groups that intersect <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> in <img alt="{\sim |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csim+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sim |A|^{1/3}}"/> regular unipotents. As there are <img alt="{\sim |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csim+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sim |A|^{2/3}}"/> regular unipotent elements in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, we see that there are only <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/> such unipotent groups available. From the pigeonhole principle and conjugation, we conclude that the preimage of <img alt="{U(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U(\overline{k})}"/> in this map has cardinality <img alt="{\gg |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{2/3}}"/>. But this preimage is simply <img alt="{A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap B(\overline{k})}"/>. In particular, the quotient <img alt="{(A\cap B(\overline{k}))/(A \cap U(\overline{k}))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A%5Ccap+B%28%5Coverline%7Bk%7D%29%29%2F%28A+%5Ccap+U%28%5Coverline%7Bk%7D%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A\cap B(\overline{k}))/(A \cap U(\overline{k}))}"/> has cardinality <img alt="{\gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{1/3}}"/>. Observe that each element of this quotient acts on <img alt="{A \cap U(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+U%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap U(\overline{k})}"/>, and hence on <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/>, by multiplication. As such, if we set </p>
<p align="center"><img alt="\displaystyle  F := \{ \xi \in \overline{k}: \xi E \subset E\}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++F+%3A%3D+%5C%7B+%5Cxi+%5Cin+%5Coverline%7Bk%7D%3A+%5Cxi+E+%5Csubset+E%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  F := \{ \xi \in \overline{k}: \xi E \subset E\}"/></p>
<p> to be the “multiplicative symmetry set” of <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/>, then we have <img alt="{|F|\gg |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%5Cgg+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|\gg |A|^{1/3}}"/>. As <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> is a finite additive group, <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> is a field of size at most <img alt="{|E| \ll|A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CE%7C+%5Cll%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|E| \ll|A|^{1/3}}"/>, thus <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> is a finite field of cardinality <img alt="{|F| \sim |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C+%5Csim+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F| \sim |A|^{1/3}}"/>. Also, <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> is a vector space over <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>; as <img alt="{E}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E}"/> contains <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/> and has cardinality <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/>, we see that <img alt="{E=F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BE%3DF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{E=F}"/>. Thus we have <a name="auk">
</a></p><p align="center"><a name="auk"><img alt="\displaystyle  A \cap U(\overline{k}) = \begin{pmatrix} 1 &amp; F \\ 0 &amp; 1 \end{pmatrix}. \ \ \ \ \ (2)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A+%5Ccap+U%28%5Coverline%7Bk%7D%29+%3D+%5Cbegin%7Bpmatrix%7D+1+%26+F+%5C%5C+0+%26+1+%5Cend%7Bpmatrix%7D.+%5C+%5C+%5C+%5C+%5C+%282%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A \cap U(\overline{k}) = \begin{pmatrix} 1 &amp; F \\ 0 &amp; 1 \end{pmatrix}. \ \ \ \ \ (2)"/></a></p><a name="auk">
</a><p><a name="auk"/> Also, as <img alt="{(A\cap B(\overline{k}))/(A \cap U(\overline{k}))}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A%5Ccap+B%28%5Coverline%7Bk%7D%29%29%2F%28A+%5Ccap+U%28%5Coverline%7Bk%7D%29%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A\cap B(\overline{k}))/(A \cap U(\overline{k}))}"/> has to stabilise <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>, we see that all elements of <img alt="{A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap B(\overline{k})}"/> have diagonal elements in <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>. Combining this with <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#auk">(2)</a>, we see that <img alt="{A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap B(\overline{k})}"/> takes the form <a name="fas">
</a></p><p align="center"><a name="fas"><img alt="\displaystyle  A \cap B(\overline{k}) = \{ \begin{pmatrix} t &amp; f(t) + x \\ 0 &amp; t^{-1} \end{pmatrix}: t \in H, x\in F\} \ \ \ \ \ (3)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A+%5Ccap+B%28%5Coverline%7Bk%7D%29+%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+t+%26+f%28t%29+%2B+x+%5C%5C+0+%26+t%5E%7B-1%7D+%5Cend%7Bpmatrix%7D%3A+t+%5Cin+H%2C+x%5Cin+F%5C%7D+%5C+%5C+%5C+%5C+%5C+%283%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A \cap B(\overline{k}) = \{ \begin{pmatrix} t &amp; f(t) + x \\ 0 &amp; t^{-1} \end{pmatrix}: t \in H, x\in F\} \ \ \ \ \ (3)"/></a></p><a name="fas">
</a><p><a name="fas"/> for some multiplicative subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{F^\times}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%5E%5Ctimes%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F^\times}"/>, and some function <img alt="{f: H \rightarrow \overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bf%3A+H+%5Crightarrow+%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{f: H \rightarrow \overline{k}}"/>; since <img alt="{A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap B(\overline{k})}"/> has cardinality <img alt="{\gg |A|^{2/3} \sim |F|^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B2%2F3%7D+%5Csim+%7CF%7C%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{2/3} \sim |F|^2}"/>, <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> must have cardinality <img alt="{\sim |F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csim+%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sim |F|}"/>. By taking the commutators of two matrices in <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#fas">(3)</a>, we see that <a name="fatch">
</a></p><p align="center"><a name="fatch"><img alt="\displaystyle  f(t) (s-s^{-1}) - f(s) (t-t^{-1}) \in F \ \ \ \ \ (4)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++f%28t%29+%28s-s%5E%7B-1%7D%29+-+f%28s%29+%28t-t%5E%7B-1%7D%29+%5Cin+F+%5C+%5C+%5C+%5C+%5C+%284%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  f(t) (s-s^{-1}) - f(s) (t-t^{-1}) \in F \ \ \ \ \ (4)"/></a></p><a name="fatch">
</a><p><a name="fatch"/> for all <img alt="{s,t \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bs%2Ct+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{s,t \in H}"/>.</p>
<p>
If we select <img alt="{t_0 \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_0+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_0 \in H}"/> such that <img alt="{t_0-t_0^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_0-t_0%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_0-t_0^{-1}}"/> is non-zero, then by conjugating <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> by a suitable element of <img alt="{U(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BU%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{U(\overline{k})}"/> (which does not affect any of the previous control established on <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>) we may normalise <img alt="{f(t_0)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bf%28t_0%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{f(t_0)}"/> to be zero. From <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#fatch">(4)</a> this makes <img alt="{f(t) \in F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bf%28t%29+%5Cin+F%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{f(t) \in F}"/> for all <img alt="{t \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t \in H}"/>. In particular, <a name="angst">
</a></p><p align="center"><a name="angst"><img alt="\displaystyle  A \cap B(\overline{k}) \subset B(F). \ \ \ \ \ (5)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A+%5Ccap+B%28%5Coverline%7Bk%7D%29+%5Csubset+B%28F%29.+%5C+%5C+%5C+%5C+%5C+%285%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A \cap B(\overline{k}) \subset B(F). \ \ \ \ \ (5)"/></a></p><a name="angst">
</a><p><a name="angst"/> Now for any <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, the subgroups <img alt="{A \cap B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Ccap+B%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \cap B(\overline{k})}"/> and <img alt="{g^{-1} (A \cap B(\overline{k})) g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+%28A+%5Ccap+B%28%5Coverline%7Bk%7D%29%29+g%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} (A \cap B(\overline{k})) g}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> have index <img alt="{O(|A|^{1/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7B1%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{1/3})}"/>, so their intersection must have cardinality <img alt="{\gg |A|^{1/3} \gg |F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7CA%7C%5E%7B1%2F3%7D+%5Cgg+%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |A|^{1/3} \gg |F|}"/>, thus </p>
<p align="center"><img alt="\displaystyle  |A \cap B(F) \cap g B(F) g^{-1}| \gg |F|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA+%5Ccap+B%28F%29+%5Ccap+g+B%28F%29+g%5E%7B-1%7D%7C+%5Cgg+%7CF%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A \cap B(F) \cap g B(F) g^{-1}| \gg |F|."/></p>
<p> In particular, there must exist either a regular unipotent or a regular semisimple element <img alt="{h \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h \in A}"/> of <img alt="{B(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(F)}"/> such that <img alt="{ghg^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bghg%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{ghg^{-1}}"/> also lies in <img alt="{B(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(F)}"/>. If <img alt="{h}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h}"/> is regular semisimple in <img alt="{B(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(F)}"/>, it has an eigenbasis in <img alt="{F^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F^2}"/>, and so <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> must map such an eigenbasis to another eigenbasis, and thus lies in <img alt="{SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F)}"/>. If instead <img alt="{h}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h}"/> is regular unipotent, it has the line <img alt="{\{0\} \times \overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B0%5C%7D+%5Ctimes+%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{0\} \times \overline{k}}"/> as the unique (geometric) eigenspace; <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> must preserve this eigenspace and thus lies in <img alt="{B(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(\overline{k})}"/>, and thus in <img alt="{B(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B(F)}"/> and therefore in <img alt="{SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F)}"/> by <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#angst">(5)</a>. Combining the cases, we conclude that <img alt="{A \subset SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%5Csubset+SL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A \subset SL_2(F)}"/>. We may therefore summarise our discussion as follows:</p>
<blockquote><p><b>Theorem 14 (Rough description of finite subgroups of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>)</b> <a name="subgroup"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then one of the following statements hold: </p>
<ul>
<li> (Arithmetic subgroup) There is a finite subfield <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> of <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> with <img alt="{|F| \sim |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C+%5Csim+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F| \sim |A|^{1/3}}"/> such that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a conjugate of <img alt="{SL_2(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F)}"/> (and is thus a subgroup of that conjugate of index <img alt="{O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(1)}"/>). </li>
<li> (Trapping) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> such that <img alt="{|A \cap B| \gg |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
In principle, the trapping case can be analysed further (using manipulations similar to those used to reach <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#angst">(5)</a>) but we will not pursue this here. We remark that while these computations were somewhat lengthy (and less elementary and precise than the more classical results of Dickson), they can extend to more complicated algebraic groups, such as <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, or more generally to any algebraic group of bounded rank; see <a href="http://www.ams.org/mathscinet-getitem?mr=2813339">this paper of Larsen and Pink</a> for details. In particular, Larsen and Pink were able to use these methods to establish an important subcase of the famous <a href="http://en.wikipedia.org/wiki/Classification_of_finite_simple_groups">classification of finite simple groups</a>, namely by verifying this classification for sufficiently large subgroups of a linear group of bounded rank over a field of arbitrary characteristic. It is conceivable that these methods may be extended in the future to give an alternate proof of the full classification (for sufficiently large groups, at least).
</p>
<p/>
<p align="center"><b> —  3. The product theorem in <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>  — </b></p>
<p>
In this section we prove the <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> case of Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#prod-slf">1</a>. This result was first established (for fields of prime order) <a href="http://www.ams.org/mathscinet-getitem?mr=2415382">by Helfgott</a> and then in the general case <a href="http://arxiv.org/abs/1001.5069">by Dinai</a>; we will present a variant of Helfgott’s argument which was developed <a href="http://arxiv.org/abs/1005.1881">by Breuillard, Green, and Tao</a> and independently <a href="http://arxiv.org/abs/1005.1858">by Pyber and Szabo</a>. It is convenient to rephrase the theorem as follows:
</p>
<blockquote><p><b>Theorem 15 (Product theorem in <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>, alternate form)</b> <a name="poid"/> Let <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> be a finite field, and let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate group in <img alt="{G := SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG+%3A%3D+SL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G := SL_2(k)}"/> that generates <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> for some <img alt="{K \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 2}"/>. Then one of the following holds: </p>
<ul>
<li> (Close to trivial) One has <img alt="{|A| \ll K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cll+K%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \ll K^{O(1)}}"/>. </li>
<li> (Close to <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>) One has <img alt="{|A| \geq K^{-O(1)} |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cgeq+K%5E%7B-O%281%29%7D+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \geq K^{-O(1)} |G|}"/>.
</li>
</ul>
</blockquote>
<p/>
<blockquote><p><b>Exercise 11</b>  Show that Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#prod-slf">1</a> follows from Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. (<em>Hint:</em> if <img alt="{|A^3| \leq |A|^{1+\epsilon}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E3%7C+%5Cleq+%7CA%7C%5E%7B1%2B%5Cepsilon%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^3| \leq |A|^{1+\epsilon}}"/>, use the multiplicative form of the Rusza triangle and covering lemmas to show that <img alt="{(A \cup \{1\} \cup A^{-1})^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28A+%5Ccup+%5C%7B1%5C%7D+%5Ccup+A%5E%7B-1%7D%29%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(A \cup \{1\} \cup A^{-1})^2}"/> is a <img alt="{O(|A|^{O(\epsilon)})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7CA%7C%5E%7BO%28%5Cepsilon%29%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|A|^{O(\epsilon)})}"/>-approximate group.) </p></blockquote>
<p/>
<p>
The problem now concerns the behaviour of finite approximate subgroups <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> of <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>. The first step will be to establish analogues of the Larsen-Pink non-concentration inequalities of the preceding section, but for approximate subgroups rather than genuine subgroups. (The observation that these inequalities could be usefully extended to the approximate group setting is <a href="http://www.ams.org/mathscinet-getitem?mr=2833482">due to Hrushovski</a>.) We begin by eliminating concentration in linear subgroups.
</p>
<blockquote><p><b>Lemma 16 (Escape from subspaces)</b> <a name="esc"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>, and let <img alt="{C&gt;0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%3E0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C&gt;0}"/>. Then one of the following holds: </p>
<ul>
<li> (Close to trivial) One has <img alt="{|A| \ll_C K^{O_C(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cll_C+K%5E%7BO_C%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \ll_C K^{O_C(1)}}"/>. </li>
<li> (Escape) For any <img alt="{d=0,1,2,3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D0%2C1%2C2%2C3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=0,1,2,3}"/> and any <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>-dimensional subspace <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> of <img alt="{\overline{k}^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^4}"/>, such that <img alt="{V\cap SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%5Ccap+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V\cap SL_2(\overline{k})}"/> is a subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, one has <img alt="{|A^2 \cap V| \leq K^{-C} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+V%7C+%5Cleq+K%5E%7B-C%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap V| \leq K^{-C} |A|}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
In practice, we will only apply the escape conclusion for Borel subgroups of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>, which are intersections of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> with three-dimensional subspaces; however, we need to work with the more general escape construction in the <em>proof</em> of the lemma, for inductive purposes. The claim can in fact be established for any <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>-dimensional subspace <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/>, or more generally for bounded complexity <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>-dimensional algebraic varieties; this will be discussed in the next section.
</p>
<p>
<em>Proof:</em>  We induct on <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>. For <img alt="{d=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=0}"/>, the claim is trivial, since <img alt="{|A^2 \cap V|=1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+V%7C%3D1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap V|=1}"/> in that case. Now suppose that <img alt="{d=1,2,3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D1%2C2%2C3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=1,2,3}"/>, and the claim has already been proven for smaller values of <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>.
</p>
<p>
Let <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> be a <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>-dimensional subspace of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> with <img alt="{V \cap SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV+%5Ccap+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V \cap SL_2(\overline{k})}"/> a group, and suppose for contradiction that <img alt="{|A^2 \cap V|&gt;K^{-C}|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+V%7C%3EK%5E%7B-C%7D%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap V|&gt;K^{-C}|A|}"/>. As <img alt="{A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2}"/> can be covered by <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> copies of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, we can find <img alt="{a\in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a\in A}"/> such that <a name="aav">
</a></p><p align="center"><a name="aav"><img alt="\displaystyle  |aA\cap V| &gt; K^{-C-1} |A|. \ \ \ \ \ (6)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CaA%5Ccap+V%7C+%3E+K%5E%7B-C-1%7D+%7CA%7C.+%5C+%5C+%5C+%5C+%5C+%286%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |aA\cap V| &gt; K^{-C-1} |A|. \ \ \ \ \ (6)"/></a></p><a name="aav">
</a><p><a name="aav"/>
</p>
<p>
Suppose that there exists an element <img alt="{b}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b}"/> of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> such that <img alt="{bVb^{-1} \neq V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BbVb%5E%7B-1%7D+%5Cneq+V%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{bVb^{-1} \neq V}"/>, so that <img alt="{bVb^{-1} \cap V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BbVb%5E%7B-1%7D+%5Ccap+V%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{bVb^{-1} \cap V}"/> has dimension strictly less than <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/>. From <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#aav">(6)</a> we have </p>
<p align="center"><img alt="\displaystyle  |A^4 \cap bVb^{-1}| \geq |baAb^{-1} \cap bVb^{-1}| &gt; K^{-C-1}|A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E4+%5Ccap+bVb%5E%7B-1%7D%7C+%5Cgeq+%7CbaAb%5E%7B-1%7D+%5Ccap+bVb%5E%7B-1%7D%7C+%3E+K%5E%7B-C-1%7D%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^4 \cap bVb^{-1}| \geq |baAb^{-1} \cap bVb^{-1}| &gt; K^{-C-1}|A|."/></p>
<p> Since <img alt="{A^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^4}"/> can be covered by <img alt="{K^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^3}"/> right translates of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, we can find <img alt="{g \in A^5}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%5E5%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A^5}"/> such that
</p><p align="center"><img alt="\displaystyle  |gA \cap bVb^{-1}| &gt; K^{-C-4}|A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CgA+%5Ccap+bVb%5E%7B-1%7D%7C+%3E+K%5E%7B-C-4%7D%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |gA \cap bVb^{-1}| &gt; K^{-C-4}|A|."/></p>
<p> Let <img alt="{A_1 :=aA \cap V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_1+%3A%3DaA+%5Ccap+V%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_1 :=aA \cap V}"/> and <img alt="{A_2 := gA \cap bVb^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_2+%3A%3D+gA+%5Ccap+bVb%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_2 := gA \cap bVb^{-1}}"/>. Then <img alt="{A_1 A_2^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_1+A_2%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_1 A_2^{-1}}"/> is contained in <img alt="{A^7}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E7%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^7}"/>, and so <img alt="{1_{A_1} * 1_{A_2^{-1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1_%7BA_1%7D+%2A+1_%7BA_2%5E%7B-1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1_{A_1} * 1_{A_2^{-1}}}"/> is supported on a set of cardinality at most <img alt="{K^6 |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%5E6+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K^6 |A|}"/>. Since
</p><p align="center"><img alt="\displaystyle  \| 1_{A_1} * 1_{A_2^{-1}} \|_{\ell^1} = |A_1||A_2| \geq K^{-2C-5} |A|^2" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5C%7C+1_%7BA_1%7D+%2A+1_%7BA_2%5E%7B-1%7D%7D+%5C%7C_%7B%5Cell%5E1%7D+%3D+%7CA_1%7C%7CA_2%7C+%5Cgeq+K%5E%7B-2C-5%7D+%7CA%7C%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \| 1_{A_1} * 1_{A_2^{-1}} \|_{\ell^1} = |A_1||A_2| \geq K^{-2C-5} |A|^2"/></p>
<p> we thus see from the pigeonhole principle that
</p><p align="center"><img alt="\displaystyle  |1_{A_1} * 1_{A_2^{-1}}(x)| \geq K^{-2C-11} |A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C1_%7BA_1%7D+%2A+1_%7BA_2%5E%7B-1%7D%7D%28x%29%7C+%5Cgeq+K%5E%7B-2C-11%7D+%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |1_{A_1} * 1_{A_2^{-1}}(x)| \geq K^{-2C-11} |A|."/></p>
<p> The left-hand side is <img alt="{|A_1 \cap x A_2|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA_1+%5Ccap+x+A_2%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A_1 \cap x A_2|}"/>, and thus
</p><p align="center"><img alt="\displaystyle  |(A_1\cap x A_2)^{-1} \cap (A_1 \cap x A_2)| \geq K^{-2C-11}|A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%28A_1%5Ccap+x+A_2%29%5E%7B-1%7D+%5Ccap+%28A_1+%5Ccap+x+A_2%29%7C+%5Cgeq+K%5E%7B-2C-11%7D%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |(A_1\cap x A_2)^{-1} \cap (A_1 \cap x A_2)| \geq K^{-2C-11}|A|."/></p>
<p> The set in the left-hand side is contained in both <img alt="{A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2}"/> and in <img alt="{V\cap (bVb^{-1})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%5Ccap+%28bVb%5E%7B-1%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V\cap (bVb^{-1})}"/> (here we use the group nature of <img alt="{V \cap SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV+%5Ccap+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V \cap SL_2(\overline{k})}"/>), and so
</p><p align="center"><img alt="\displaystyle  |A^2 \cap V\cap (bVb^{-1})| \geq K^{-2C-11} |A|." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E2+%5Ccap+V%5Ccap+%28bVb%5E%7B-1%7D%29%7C+%5Cgeq+K%5E%7B-2C-11%7D+%7CA%7C.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^2 \cap V\cap (bVb^{-1})| \geq K^{-2C-11} |A|."/></p>
<p> Applying the induction hypothesis, we conclude that <img alt="{|A| \leq K^{O_C(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cleq+K%5E%7BO_C%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \leq K^{O_C(1)}}"/>, and the claim follows.</p>
<p>
The only remaining case is when <img alt="{bVb^{-1}=V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BbVb%5E%7B-1%7D%3DV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{bVb^{-1}=V}"/> for all <img alt="{b \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bb+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{b \in A}"/>. As <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> generates <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>, this implies that <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> is normalised by <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>. But this is impossible if <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> has dimension <img alt="{1,2,3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%2C2%2C3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1,2,3}"/>; see Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#normal">12</a> below. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 12 (Almost simplicity of <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>)</b> <a name="normal"/> Let <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> be a subspace of <img alt="{\overline{k}^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^4}"/> of dimension <img alt="{1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{1}"/>, <img alt="{2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{2}"/>, or <img alt="{3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{3}"/>. Show that the group <img alt="{\{ g \in SL_2(k): gVg^{-1} = V\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+g+%5Cin+SL_2%28k%29%3A+gVg%5E%7B-1%7D+%3D+V%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ g \in SL_2(k): gVg^{-1} = V\}}"/> does not contain all of <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>. </p></blockquote>
<p/>
<p>
Now we can obtain an approximate version of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis">10</a>:
</p>
<blockquote><p><b>Proposition 17 (Larsen-Pink inequality, special case)</b> <a name="lpis-approx"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Then for any maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>, one has <img alt="{|A^2 \cap T| \ll K^{O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+T%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap T| \ll K^{O(1)} |A|^{1/3}}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  We may assume that <img alt="{|A| \geq K^C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cgeq+K%5EC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \geq K^C}"/> for any given constant <img alt="{C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{C}"/>, as the claim is trivial otherwise. Similarly, by Lemma <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#esc">16</a>, we may assume that <img alt="{|A^2 \cap B|\leq K^{-C}|B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+B%7C%5Cleq+K%5E%7B-C%7D%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap B|\leq K^{-C}|B|}"/> for all Borel subgroups <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/>.
</p>
<p>
We need to show that <img alt="{|A^2 \cap T| \ll |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+T%7C+%5Cll+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap T| \ll |A|^{1/3}}"/> for any maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>. By conjugation we may take <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> to be the standard maximal torus <img alt="{T = T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT+%3D+T%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T = T(\overline{k})}"/>. (This may make <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> generate a conjugate of <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/>, rather than <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> itself, but this will not impact our argument). Set <img alt="{A' := A^2 \cap T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+%3A%3D+A%5E2+%5Ccap+T%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' := A^2 \cap T(\overline{k})}"/>, then </p>
<p align="center"><img alt="\displaystyle  A' := \{ \begin{pmatrix} t &amp; 0 \ &amp; t^{-1} \end{pmatrix}: t\in H \}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++A%27+%3A%3D+%5C%7B+%5Cbegin%7Bpmatrix%7D+t+%26+0+%5C+%26+t%5E%7B-1%7D+%5Cend%7Bpmatrix%7D%3A+t%5Cin+H+%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  A' := \{ \begin{pmatrix} t &amp; 0 \ &amp; t^{-1} \end{pmatrix}: t\in H \}"/></p>
<p> for some finite subset <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{\overline{k}^\times}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5E%5Ctimes%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^\times}"/>. We may assume that <img alt="{|H| \geq K^C}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C+%5Cgeq+K%5EC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H| \geq K^C}"/>, as the claim is trivial otherwise. Our task is to show that <img alt="{|H|^3 \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CH%7C%5E3+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|H|^3 \ll K^{O(1)} |A|}"/>.</p>
<p>
As in the proof of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a>, we may find an element <img alt="{g = \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%3D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5C+c+%26+d+%5Cend%7Bpmatrix%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g = \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}}"/> of <img alt="{A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2}"/> with <img alt="{a,b,c,d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba%2Cb%2Cc%2Cd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a,b,c,d}"/> all non-zero. Since <img alt="{A' g A' g A' \subset A^{10}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%27+g+A%27+g+A%27+%5Csubset+A%5E%7B10%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A' g A' g A' \subset A^{10}}"/>, thus </p>
<p align="center"><img alt="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_2 &amp; 0 \ &amp; t_2^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A^{10}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cbegin%7Bpmatrix%7D+t_1+%26+0+%5C+%26+t_1%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5Cc+%26+d+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+t_2+%26+0+%5C+%26+t_2%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5Cc+%26+d+%5Cend%7Bpmatrix%7D+%5Cbegin%7Bpmatrix%7D+t_3+%26+0+%5C+%26+t_3%5E%7B-1%7D+%5Cend%7Bpmatrix%7D+%5Cin+A%5E%7B10%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \begin{pmatrix} t_1 &amp; 0 \ &amp; t_1^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_2 &amp; 0 \ &amp; t_2^{-1} \end{pmatrix} \begin{pmatrix} a &amp; b \\c &amp; d \end{pmatrix} \begin{pmatrix} t_3 &amp; 0 \ &amp; t_3^{-1} \end{pmatrix} \in A^{10}"/></p>
<p> for all <img alt="{t_1,t_2,t_3 \in H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bt_1%2Ct_2%2Ct_3+%5Cin+H%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{t_1,t_2,t_3 \in H}"/>. Arguing as in Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a>, we have
</p><p align="center"><img alt="\displaystyle  |H|^3\ll |A^{10}|," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CH%7C%5E3%5Cll+%7CA%5E%7B10%7D%7C%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |H|^3\ll |A^{10}|,"/></p>
<p> and the claim follows. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 13</b>  Show that if the non-concentration conclusion in Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a> holds, then for every maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> and every <img alt="{m \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m \geq 1}"/>, one has <img alt="{|A^m \cap T| \ll_m K^{O_m(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5Em+%5Ccap+T%7C+%5Cll_m+K%5E%7BO_m%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^m \cap T| \ll_m K^{O_m(1)} |A|^{1/3}}"/>. </p></blockquote>
<p/>
<p>
We can now establish variants of the other Larsen-Pink inequalities from the preceding section:
</p>
<blockquote><p><b>Exercise 14</b> <a name="lpis-alt-approx"/> Establish a variant of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a> in which the maximal tori are replaced by unipotent groups. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 15 (Large conjugacy classes)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Show that for any regular semisimple or regular projectively unipotent <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, one has <img alt="{|A^3 \cap Conj(g)| \gg K^{-O(1)} |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E3+%5Ccap+Conj%28g%29%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^3 \cap Conj(g)| \gg K^{-O(1)} |A|^{2/3}}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 16 (Larsen-Pink inequality, another special case)</b> <a name="lpis-again"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Show that for any regular semisimple <img alt="{g \in SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_2(\overline{k})}"/> and any <img alt="{m \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m \geq 1}"/>, one has <img alt="{|A^m \cap Conj(g)| \ll_m K^{O_m(1)} |A|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5Em+%5Ccap+Conj%28g%29%7C+%5Cll_m+K%5E%7BO_m%281%29%7D+%7CA%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^m \cap Conj(g)| \ll_m K^{O_m(1)} |A|^{2/3}}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 17 (Unipotent bound)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Show that <img alt="{O(K^{O(1)} |A|^{2/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D+%7CA%7C%5E%7B2%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)} |A|^{2/3})}"/> of the elements of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> are unipotent. </p></blockquote>
<p/>
<blockquote><p><b>Exercise 18 (Large tori)</b> <a name="tori-large-approxs"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Show that for any regular semisimple <img alt="{g \in A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A^2}"/>, one has <img alt="{|A^4 \cap T| \gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E4+%5Ccap+T%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^4 \cap T| \gg K^{-O(1)} |A|^{1/3}}"/>, where <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is the unique maximal torus containing <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>. In fact one has <img alt="{|A^2 \cap T| \gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+T%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap T| \gg K^{-O(1)} |A|^{1/3}}"/>. (For the latter claim, cover <img alt="{A^4}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^4}"/> by left translates of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>.) </p></blockquote>
<p/>
<p>
We now have a dichotomy: given a maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/>, either <img alt="{A^2\cap T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%5Ccap+T%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2\cap T}"/> has no regular semisimple elements (and thus contains only central elements), or else has cardinality <img alt="{\gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A|^{1/3}}"/>. We exploit this dichotomy as follows. Call a maximal torus <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> <em>involved</em> if <img alt="{A^2 \cap T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2+%5Ccap+T%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2 \cap T}"/> contains a regular semisimple element.
</p>
<blockquote><p><b>Lemma 18 (Key lemma)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/> be as in Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Then one of the following statements hold: </p>
<ul>
<li> (Invariance) If <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is an involved torus and <img alt="{a \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Ba+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{a \in A}"/>, then <img alt="{aTa^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaTa%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aTa^{-1}}"/> is an involved torus. </li>
<li> (Close to trivial) One has <img alt="{|A| \ll K^{O(1)}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%5Cll+K%5E%7BO%281%29%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| \ll K^{O(1)}}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  Let <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> be an involved torus, then by the preceding exercise we have <img alt="{|A^2 \cap T|\gg K^{-O(1)}|A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+T%7C%5Cgg+K%5E%7B-O%281%29%7D%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap T|\gg K^{-O(1)}|A|^{1/3}}"/>, and thus <img alt="{|A^4 \cap aTa^{-1}| \gg K^{-O(1)}|A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E4+%5Ccap+aTa%5E%7B-1%7D%7C+%5Cgg+K%5E%7B-O%281%29%7D%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^4 \cap aTa^{-1}| \gg K^{-O(1)}|A|^{1/3}}"/>. Thus, one has <img alt="{|gA \cap aTa^{-1}| \gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CgA+%5Ccap+aTa%5E%7B-1%7D%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|gA \cap aTa^{-1}| \gg K^{-O(1)} |A|^{1/3}}"/> for some <img alt="{g \in G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in G}"/>, which implies that <img alt="{|A^2 \cap aTa^{-1}| \gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+aTa%5E%7B-1%7D%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap aTa^{-1}| \gg K^{-O(1)} |A|^{1/3}}"/>. In particular, if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is not close to trivial, <img alt="{A^2 \cap aTa^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2+%5Ccap+aTa%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2 \cap aTa^{-1}}"/> contains a regular semisimple element and so <img alt="{aTa^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BaTa%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{aTa^{-1}}"/> is involved, as desired. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
We can now finish the proof of Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>. Suppose <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is not close to trivial. As there are at most <img alt="{O(K^{O(1)}|A|^{2/3})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28K%5E%7BO%281%29%7D%7CA%7C%5E%7B2%2F3%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(K^{O(1)}|A|^{2/3})}"/> unipotent elements and <img alt="{O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(1)}"/> central elements in <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> at least one regular semisimple element, and so there is at least one involved torus. By the above lemma, and the fact that <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> generates <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>, we see that the set of involved tori is invariant under conjugation by <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/>. As <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> has cardinality <img alt="{\gg |k|^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7Ck%7C%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |k|^3}"/>, and its intersection with the stabiliser of a single torus has cardinality <img alt="{O(|k|)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%7Ck%7C%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(|k|)}"/>, we conclude that there are <img alt="{\gg |k|^2 \ll |G|^{2/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+%7Ck%7C%5E2+%5Cll+%7CG%7C%5E%7B2%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg |k|^2 \ll |G|^{2/3}}"/> involved tori. By Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#tori-large-approxs">18</a>, each of these tori contains <img alt="{\gg K^{-O(1)} |A|^{1/3}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cgg+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\gg K^{-O(1)} |A|^{1/3}}"/> regular semisimple elements of <img alt="{A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2}"/>. Since each regular semisimple element belongs to a unique maximal torus, we conclude that </p>
<p align="center"><img alt="\displaystyle |A^2| \gg |G|^{2/3} K^{-O(1)} |A|^{1/3};" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%7CA%5E2%7C+%5Cgg+%7CG%7C%5E%7B2%2F3%7D+K%5E%7B-O%281%29%7D+%7CA%7C%5E%7B1%2F3%7D%3B&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle |A^2| \gg |G|^{2/3} K^{-O(1)} |A|^{1/3};"/></p>
<p> as <img alt="{|A^2| \leq K|A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2%7C+%5Cleq+K%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2| \leq K|A|}"/>, we conclude that <img alt="{|A|\gg K^{-O(1)} |G|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C%5Cgg+K%5E%7B-O%281%29%7D+%7CG%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A|\gg K^{-O(1)} |G|}"/>, as claimed.</p>
<blockquote><p><b>Exercise 19</b> <a name="spla"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a finite <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate subgroup of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> for some algebraically closed field <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>. Show that one of the following statements hold: </p>
<ul>
<li> (Close to group) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> generates a finite subgroup <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> with <img alt="{|G| \ll K^{O(1)} |A|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CG%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|G| \ll K^{O(1)} |A|}"/>. </li>
<li> (Concentrated in Borel) There is a Borel subgroup <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/> with <img alt="{|A \cap B| \gg K^{-O(1)} |B|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA+%5Ccap+B%7C+%5Cgg+K%5E%7B-O%281%29%7D+%7CB%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A \cap B| \gg K^{-O(1)} |B|}"/>.
</li>
</ul>
<p> (<em>Hint:</em> this does not follow directly from Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#poid">15</a>, but can be established by a modification of the proof of that theorem.) </p></blockquote>
<p/>
<p>
Note that the above exercise can be combined with Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#subgroup">14</a> to give a more detailed description of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. The Borel group <img alt="{B}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{B}"/> is solvable, and by using tools from additive combinatorics, such as <a href="http://terrytao.wordpress.com/2009/06/21/freimans-theorem-for-solvable-groups/">Freiman’s theorem in solvable groups</a> (or the Helfgott-Lindenstrauss conjecture, discussed in the <a href="http://terrytao.wordpress.com/2011/11/13/254a-notes-9-applications-of-the-structural-theory-of-approximate-groups/">previous quarter’s notes</a>), one can give even more precise descriptions of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> (at the cost of losing polynomial dependence of the bounds on <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>), but we will not discuss these topics here.
</p>
<blockquote><p><b>Exercise 20</b>  Use Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spla">19</a> to give an alternate proof of Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spt">5</a>. (<em>Hint:</em> there are a number of ways to embed the sum-product problem in a field <img alt="{k}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{k}"/> into a product problem in <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> (or <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>). For instance, one consider the tripling properties of sets of the form <img alt="{\{ \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}: a,b,c,d \in A \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+%5Cbegin%7Bpmatrix%7D+a+%26+b+%5C%5C+c+%26+d+%5Cend%7Bpmatrix%7D%3A+a%2Cb%2Cc%2Cd+%5Cin+A+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ \begin{pmatrix} a &amp; b \\ c &amp; d \end{pmatrix}: a,b,c,d \in A \}}"/> in terms of sets such as <img alt="{A^2+A^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E2%2BA%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^2+A^2}"/> or <img alt="{A^3+A^3+A^3+A^3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E3%2BA%5E3%2BA%5E3%2BA%5E3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^3+A^3+A^3+A^3}"/>, and then project this set onto <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> (or <img alt="{PSL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BPSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{PSL_2(k)}"/>), and combine this with the Katz-Tao lemma to obtain Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spt">5</a>. More details of this connection can be found in Section 8 of <a href="http://arxiv.org/abs/1005.1881">this paper</a>.) This is of course a much more complicated and inefficient way to establish the sum-product theorem, but it does illustrate the link between the two results (beyond the fact that both proofs exploit a dichotomy). Note alsot that the original proof of the product theorem in <img alt="{SL_2(F_p)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28F_p%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(F_p)}"/> by Helfgott actually used the sum-product theorem in <img alt="{F_p}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF_p%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F_p}"/> as a key tool. </p></blockquote>
<p/>
<p align="center"><b> —  4. The product theorem in <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>  — </b></p>
<p>
We now discuss the extension of the <img alt="{SL_2(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(k)}"/> product theory to the more general groups <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>. Actually, the arguments here will be valid in any almost simple connected algebraic group of bounded rank, but for sake of concreteness we will work with <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>. (This also has the (very) minor advantage that <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/> is an affine variety rather than a projective one, so we can work entirely in affine spaces such as <img alt="{{\bf A}^{d^2}(\overline{k}) :=\overline{k}^{d^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29+%3A%3D%5Coverline%7Bk%7D%5E%7Bd%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k}) :=\overline{k}^{d^2}}"/>; related to this, the only regular maps we need to consider will be polynomial in nature.) There is also some recent work on product theorems in other algebraic groups than the almost simple ones; see for instance the papers of <a href="http://arxiv.org/abs/1005.1858">Pyber-Szabo</a>, <a href="http://arxiv.org/abs/1008.5264">Gill-Helfgott</a>, and <a href="http://arxiv.org/abs/1005.1881">Breuillard-Green-Tao</a> for some examples of this. It is conceivable that a satisfactory understanding of approximate subgroups of arbitrary algebraic groups of bounded dimension will be available in the near future.
</p>
<p>
The treatment of the <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> case relied on a number of <em>ad hoc</em> computations which were only valid in <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>, and also on the pleasant fact that the only non-regular elements of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/> were the central elements <img alt="{\pm 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cpm+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\pm 1}"/>, which is certainly false for higher values of <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>. In <a href="http://www.ams.org/mathscinet-getitem?mr=2781932">this paper</a>, Helfgott was able to push his original <img alt="{d=2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=2}"/> arguments to the <img alt="{d=3}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%3D3%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d=3}"/> case, but again the arguments were somewhat <em>ad hoc</em> in nature and did not seem to extend to the general setting. However, the arguments based on the Larsen-Pink concentration estimates have proven to be quite general, and in particular can handle the situation <img alt="{SL_d(k)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28k%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(k)}"/>. The one catch is that instead of working with very concrete and explicit subsets of <img alt="{SL_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2}"/>, such as Borel subgroups or other intersections <img alt="{SL_2 \cap V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2+%5Ccap+V%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2 \cap V}"/> with linear spaces <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/>, one has to work with more general algebraic subvarieties of <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/>. As such, a certain amount of basic algebraic geometry becomes necessary. Also, because we are seeking results with quantitative bounds, we will need to keep some track of the “complexity” of the varieties that one encounters in the course of the argument.
</p>
<p>
We now very quickly review some algebraic geometry notions, though for reasons of space we will not attempt to develop the full theory of algebraic geometry here, referring instead to standard texts such as <a href="http://www.ams.org/mathscinet-getitem?mr=1416564">Harris</a>, <a href="http://www.ams.org/mathscinet-getitem?mr=1748380">Mumford</a>, or <a href="http://www.ams.org/mathscinet-getitem?mr=1288523">Griffiths-Harris</a>. As usual, algebraic geometry is cleanest when working over an algebraically closed field, so we will work primarily over <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>.
</p>
<blockquote><p><b>Definition 19 (Variety)</b>  Let <img alt="{M \geq d \geq 0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM+%5Cgeq+d+%5Cgeq+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M \geq d \geq 0}"/> be integers, and let <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> be an algebraically closed field. We write <img alt="{{\bf A}^d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5Ed%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^d(\overline{k})}"/> for the affine space <img alt="{\overline{k}^d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5Ed%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^d}"/>. </p>
<ul>
<li> An (affine) <a href="http://en.wikipedia.org/wiki/Algebraic_variety">variety</a> <img alt="{V = V(\overline{k}) \subset {\bf A}^d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV+%3D+V%28%5Coverline%7Bk%7D%29+%5Csubset+%7B%5Cbf+A%7D%5Ed%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V = V(\overline{k}) \subset {\bf A}^d(\overline{k})}"/> of complexity at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/> is a set of the form
<p align="center"><img alt="\displaystyle  V = \{ x \in \overline{k}^d: P_1(x) =\ldots = P_m(x) = 0 \}," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++V+%3D+%5C%7B+x+%5Cin+%5Coverline%7Bk%7D%5Ed%3A+P_1%28x%29+%3D%5Cldots+%3D+P_m%28x%29+%3D+0+%5C%7D%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  V = \{ x \in \overline{k}^d: P_1(x) =\ldots = P_m(x) = 0 \},"/></p>
<p> where <img alt="{0 \leq m \leq M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%5Cleq+m+%5Cleq+M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 \leq m \leq M}"/> and <img alt="{P_1,\ldots,P_m: {\bf A}^d(\overline{k}) \rightarrow\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BP_1%2C%5Cldots%2CP_m%3A+%7B%5Cbf+A%7D%5Ed%28%5Coverline%7Bk%7D%29+%5Crightarrow%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{P_1,\ldots,P_m: {\bf A}^d(\overline{k}) \rightarrow\overline{k}}"/> are polynomials of degree at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>. (Thus the complexity parameter <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/> controls the dimension, degree, and number of polynomials needed to cut out the variety. Note that we do not assume our varieties to be irreducible, and as such what we call a variety corresponds to what is sometimes known as an <em>algebraic set</em> in the literature.) Note that the union or intersection of two varieties of complexity at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>, is another variety of complexity at most <img alt="{O_M(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_M%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_M(1)}"/>. </p></li>
<li> A variety is <em>irreducible</em> if it cannot be expressed as the union of two proper (i.e. strict) subvarieties. </li>
</ul>
</blockquote>
<p/>
<p>
Thus, for instance, <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> is a variety of complexity <img alt="{O_d(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_d%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_d(1)}"/> in <img alt="{{\bf A}^{d^2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k})}"/> (after identifying this latter affine space with the space of <img alt="{d \times d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%5Ctimes+d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d \times d}"/> matrices over <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>).
</p>
<p>
It is known that any variety can be expressed as the union of a finite number of irreducible components, and this decomposition is unique if we require that no component is contained in any other. Furthermore, to each irreducible variety <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> one can assign a <em>dimension</em> <img alt="{\hbox{dim}(V)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Bdim%7D%28V%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{dim}(V)}"/>, defined as the maximal integer <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> for which there exists a chain </p>
<p align="center"><img alt="\displaystyle  \emptyset \neq V_0 \subsetneq \ldots \subsetneq V_D = V" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Cemptyset+%5Cneq+V_0+%5Csubsetneq+%5Cldots+%5Csubsetneq+V_D+%3D+V&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \emptyset \neq V_0 \subsetneq \ldots \subsetneq V_D = V"/></p>
<p> of irreducible varieties; this will be an integer between <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/> and <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>. For instance, it can be shown that <img alt="{{\bf A}^d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5Ed%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^d(\overline{k})}"/> has dimension <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> (as expected). We define the dimension of a non-irreducible variety <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> to be the least integer <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> such that <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> can be covered by finitely many irreducible varieties of dimension <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>. If a (non-empty) variety <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> can be cut out from an irreducible variety <img alt="{W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{W}"/> by setting <img alt="{m}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m}"/> polynomials to zero, then one has <img alt="{\hbox{dim}(W) - m \leq \hbox{dim}(V) \leq \hbox{dim}(W)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Bdim%7D%28W%29+-+m+%5Cleq+%5Chbox%7Bdim%7D%28V%29+%5Cleq+%5Chbox%7Bdim%7D%28W%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{dim}(W) - m \leq \hbox{dim}(V) \leq \hbox{dim}(W)}"/>. Since <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> can be cut out from <img alt="{{\bf A}^{d^2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k})}"/> by a single polynomial, and is not equal to all of <img alt="{{\bf A}^{d^2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k})}"/>, we conclude in particular that <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> has dimension <img alt="{d^2-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5E2-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d^2-1}"/>. </p>
<p>
One can show that the image of a <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-dimensional variety by a polynomial map <img alt="{P: {\bf A}^{d_1}\rightarrow {\bf A}^{d_2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BP%3A+%7B%5Cbf+A%7D%5E%7Bd_1%7D%5Crightarrow+%7B%5Cbf+A%7D%5E%7Bd_2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{P: {\bf A}^{d_1}\rightarrow {\bf A}^{d_2}}"/> is contained in a variety of dimension at most <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>. One can thus produce upper bounds on the dimension of varieties, by covering them by polynomial images of varieties already known to be bounded by the same dimension.
</p>
<p>
An <em>algebraic subgroup</em> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> is a subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> which is also a subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. For instance, the <em>standard maximal torus</em> <img alt="{T(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T(\overline{k})}"/>, consisting of all the diagonal elements of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, is an algebraic subgroup; more generally, any <em>maximal torus</em>, by which we mean a conjugate of the standard maximal torus, is an algebraic subgroup.
</p>
<blockquote><p><b>Exercise 21</b>  Show that every maximal torus has dimension <img alt="{d-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d-1}"/> and complexity <img alt="{O_d(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_d%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_d(1)}"/>. </p></blockquote>
<p/>
<p>
Dual to the maximal tori are the conjugacy classes <img alt="{Conj(g) := \{ hgh^{-1}: h \in SL_d(\overline{k})\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BConj%28g%29+%3A%3D+%5C%7B+hgh%5E%7B-1%7D%3A+h+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Conj(g) := \{ hgh^{-1}: h \in SL_d(\overline{k})\}}"/> of regular semisimple elements. We call a element <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> <em>regular semisimple</em> if it has <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/> distinct eigenvalues, and is thus diagonalisable. Observe that each regular semisimple element lies in precisely one maximal torus.
</p>
<blockquote><p><b>Exercise 22</b>  Show that every conjugacy class of a regular semisimple element has dimension <img alt="{d^2-d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5E2-d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d^2-d}"/> and complexity <img alt="{O_d(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_d%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_d(1)}"/>. </p></blockquote>
<p/>
<p>
If <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> is a finite subfield of <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>, then <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/> is a finite subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, and is thus technically a <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/>-dimensional algebraic subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. However, the complexity of this algebraic group is huge (comparable to the cardinality of <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/>). It turns out that <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/> is “effectively Zariski-dense” in the sense that it cannot be captured in a low complexity algebraic variety:
</p>
<blockquote><p><b>Lemma 20 (Schwartz-Zippel lemma for <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/>)</b> <a name="szl"/> Let <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> be a proper subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> of complexity at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>. Let <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> be a finite subfield of <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/>. Then
</p><p align="center"><img alt="\displaystyle  |SL_d(F) \cap V| \ll_{M,d} |F|^{d^2-2}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CSL_d%28F%29+%5Ccap+V%7C+%5Cll_%7BM%2Cd%7D+%7CF%7C%5E%7Bd%5E2-2%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |SL_d(F) \cap V| \ll_{M,d} |F|^{d^2-2}."/></p>
</blockquote>
<p/>
<p>
<em>Proof:</em>  <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> is the hypersurface in <img alt="{{\bf A}^{d^2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k})}"/> cut out by the determinant polynomial. As <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> is a proper subvariety, we can find a polynomial <img alt="{P: \overline{k}^{d^2} \rightarrow \overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BP%3A+%5Coverline%7Bk%7D%5E%7Bd%5E2%7D+%5Crightarrow+%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{P: \overline{k}^{d^2} \rightarrow \overline{k}}"/> which is not a multiple of the determinant polynomial, but which vanishes on <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/>; by the complexity hypothesis we may take <img alt="{P}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{P}"/> to have degree <img alt="{O_{M,d}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_%7BM%2Cd%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_{M,d}(1)}"/>. Our task is then to show that </p>
<p align="center"><img alt="\displaystyle  |\{ x \in SL_d(F): P(x)=0 \}| \ll_{M,d} |F|^{d^2-2}. " class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%5C%7B+x+%5Cin+SL_d%28F%29%3A+P%28x%29%3D0+%5C%7D%7C+%5Cll_%7BM%2Cd%7D+%7CF%7C%5E%7Bd%5E2-2%7D.+&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |\{ x \in SL_d(F): P(x)=0 \}| \ll_{M,d} |F|^{d^2-2}. "/></p>
<p>
Let us write the <img alt="{d^2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d^2}"/> coordinates of <img alt="{{\bf A}^{d^2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7B%5Cbf+A%7D%5E%7Bd%5E2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{{\bf A}^{d^2}(\overline{k})}"/> arbitrarily as <img alt="{x_1,\ldots,x_{d^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx_1%2C%5Cldots%2Cx_%7Bd%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x_1,\ldots,x_{d^2}}"/>. In a given element of <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/>, not all of the <img alt="{x_i}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x_i}"/> can be zero; thus by symmetry and relabeling if necessary it suffices to show that <a name="pad">
</a></p><p align="center"><a name="pad"><img alt="\displaystyle  |\{ x \in SL_d(F): P(x)=0; x_{d^2} \neq 0 \}| \ll_{M,d} |F|^{d^2-2}. \ \ \ \ \ (7)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%5C%7B+x+%5Cin+SL_d%28F%29%3A+P%28x%29%3D0%3B+x_%7Bd%5E2%7D+%5Cneq+0+%5C%7D%7C+%5Cll_%7BM%2Cd%7D+%7CF%7C%5E%7Bd%5E2-2%7D.+%5C+%5C+%5C+%5C+%5C+%287%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |\{ x \in SL_d(F): P(x)=0; x_{d^2} \neq 0 \}| \ll_{M,d} |F|^{d^2-2}. \ \ \ \ \ (7)"/></a></p><a name="pad">
</a><p><a name="pad"/> But then one can express <img alt="{x_{d^2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx_%7Bd%5E2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x_{d^2}}"/> as a rational function of the other <img alt="{d^2-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5E2-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d^2-1}"/> coordinates, and the left-hand side of <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#pad">(7)</a> is contained in a set of the form <img alt="{\{ x \in F^{d^2-1}: Q(x)=0\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+x+%5Cin+F%5E%7Bd%5E2-1%7D%3A+Q%28x%29%3D0%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ x \in F^{d^2-1}: Q(x)=0\}}"/> for some polynomial <img alt="{Q}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Q}"/> of degree <img alt="{O_{M,d}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_%7BM%2Cd%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_{M,d}(1)}"/> that is not identically zero. The claim then follows from the <a href="http://en.wikipedia.org/wiki/Schwartz%E2%80%93Zippel_lemma">Schwartz-Zippel lemma</a>, which we give as an exercise below. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<blockquote><p><b>Exercise 23 (Schwartz-Zippel lemma)</b>  Let <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> be a finite field, and let <img alt="{Q:F^d \rightarrow F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BQ%3AF%5Ed+%5Crightarrow+F%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Q:F^d \rightarrow F}"/> be a polynomial of degree <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> that is not identically zero. Show that
</p><p align="center"><img alt="\displaystyle  |\{ x \in F^d: Q(x) = 0 \}| \ll_d D |F|^{d-1}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%5C%7B+x+%5Cin+F%5Ed%3A+Q%28x%29+%3D+0+%5C%7D%7C+%5Cll_d+D+%7CF%7C%5E%7Bd-1%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |\{ x \in F^d: Q(x) = 0 \}| \ll_d D |F|^{d-1}."/></p>
<p> For an additional challenge, obtain the sharper bound
</p><p align="center"><img alt="\displaystyle  |\{ x \in F^d: Q(x) = 0 \}| \leq D |F|^{d-1}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%5C%7B+x+%5Cin+F%5Ed%3A+Q%28x%29+%3D+0+%5C%7D%7C+%5Cleq+D+%7CF%7C%5E%7Bd-1%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |\{ x \in F^d: Q(x) = 0 \}| \leq D |F|^{d-1}."/></p>
</blockquote>
<p/>
<p>
We contrast this with the size of <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/> itself:
</p>
<blockquote><p><b>Exercise 24</b> <a name="szl-a"/> Let <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/> be a finite field. Show that <img alt="{|F|^{d^2-1} \ll_d |SL_d(F)|\ll_d |F|^{d^2-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%5E%7Bd%5E2-1%7D+%5Cll_d+%7CSL_d%28F%29%7C%5Cll_d+%7CF%7C%5E%7Bd%5E2-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|^{d^2-1} \ll_d |SL_d(F)|\ll_d |F|^{d^2-1}}"/>. </p></blockquote>
<p/>
<p>
The key non-concentration inequality we will need is the following.
</p>
<blockquote><p><b>Proposition 21 (Larsen-Pink inequality)</b> <a name="lpi-big"/> Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> for some <img alt="{K \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 2}"/>, and let <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> be a subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> of complexity at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>. Let <img alt="{m \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m \geq 1}"/>. Then one of the following is true: </p>
<ul>
<li> (Non-concentration) One has <a name="amvf">
<p align="center"><img alt="\displaystyle  |A^m \cap V| \ll_{M,d,m} K^{O_{M,d,m}(1)} |A|^{dim(V)/dim(SL_d)}. \ \ \ \ \ (8)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5Em+%5Ccap+V%7C+%5Cll_%7BM%2Cd%2Cm%7D+K%5E%7BO_%7BM%2Cd%2Cm%7D%281%29%7D+%7CA%7C%5E%7Bdim%28V%29%2Fdim%28SL_d%29%7D.+%5C+%5C+%5C+%5C+%5C+%288%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^m \cap V| \ll_{M,d,m} K^{O_{M,d,m}(1)} |A|^{dim(V)/dim(SL_d)}. \ \ \ \ \ (8)"/></p>
</a><p><a name="amvf"/> </p></li>
<li> (Trapping) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a proper algebraic subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> of complexity <img alt="{O_{M,d,m}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_%7BM%2Cd%2Cm%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_{M,d,m}(1)}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
This inequality subsumes results such as Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a>, Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-alt-approx">14</a>, and Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-again">16</a>. Note from Lemma <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#szl">20</a> (and Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#szl-a">24</a>) that the trapping option of the above proposition cannot occur if <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> generates <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/> and <img alt="{|F|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F|}"/> is sufficiently large depending on <img alt="{M, d, m}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%2C+d%2C+m%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M, d, m}"/>, while the non-concentration claim is trivial when <img alt="{|F| = O_{M,d,m}(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CF%7C+%3D+O_%7BM%2Cd%2Cm%7D%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|F| = O_{M,d,m}(1)}"/>; thus in this case we have <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#amvf">(9)</a> unconditionally.
</p>
<p>
The proof of Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big">21</a> is somewhat complicated and is deferred to the next section. We record some particular consequences of this inequality.
</p>
<blockquote><p><b>Exercise 25 (Consequences of the non-concentration inequality)</b>  Let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> for some <img alt="{K \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K \geq 2}"/>, which generates <img alt="{SL_d(F)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28F%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(F)}"/> for some finite field <img alt="{F}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BF%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{F}"/>. </p>
<ul>
<li>(i) If <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> is a maximal torus (and thus of dimension <img alt="{d-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d-1}"/>), show that <img alt="{|A^{10} \cap T| \ll_d K^{O_d(1)} |A|^{\frac{1}{d+1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B10%7D+%5Ccap+T%7C+%5Cll_d+K%5E%7BO_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7B1%7D%7Bd%2B1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{10} \cap T| \ll_d K^{O_d(1)} |A|^{\frac{1}{d+1}}}"/>. </li>
<li>(ii) If <img alt="{T_0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T_0}"/> denotes the elements of <img alt="{T}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{T}"/> which are not regular semisimple, show that <img alt="{|A^{10} \cap T| \ll_d K^{O_d(1)} |A|^{\frac{d-2}{d^2-1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B10%7D+%5Ccap+T%7C+%5Cll_d+K%5E%7BO_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7Bd-2%7D%7Bd%5E2-1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{10} \cap T| \ll_d K^{O_d(1)} |A|^{\frac{d-2}{d^2-1}}}"/>. </li>
<li>(iii) If <img alt="{g \in SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_d(\overline{k})}"/> is regular semisimple, show that <img alt="{|A^{10} \cap Conj(g)|\ll_d K^{O_d(1)} |A|^{\frac{d}{d+1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7B10%7D+%5Ccap+Conj%28g%29%7C%5Cll_d+K%5E%7BO_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7Bd%7D%7Bd%2B1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{10} \cap Conj(g)|\ll_d K^{O_d(1)} |A|^{\frac{d}{d+1}}}"/>. </li>
<li>(iv) Show that at most <img alt="{O_d(K^{O_d(1)} |A|^{\frac{d^2-2}{d^2-1}})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO_d%28K%5E%7BO_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7Bd%5E2-2%7D%7Bd%5E2-1%7D%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O_d(K^{O_d(1)} |A|^{\frac{d^2-2}{d^2-1}})}"/> of the elements of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> are not regular semisimple. </li>
<li>(v) For any regular semisimple <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, show that <img alt="{|A^3 \cap Conj(g)| \gg_d K^{-O_d(1)} |A|^{\frac{d}{d+1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E3+%5Ccap+Conj%28g%29%7C+%5Cgg_d+K%5E%7B-O_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7Bd%7D%7Bd%2B1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^3 \cap Conj(g)| \gg_d K^{-O_d(1)} |A|^{\frac{d}{d+1}}}"/>. </li>
<li>(vi) For any regular semisimple <img alt="{g \in A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A}"/>, show that <img alt="{|A^2 \cap T| \gg_d K^{-O_d(1)} |A|^{\frac{1}{d+1}}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E2+%5Ccap+T%7C+%5Cgg_d+K%5E%7B-O_d%281%29%7D+%7CA%7C%5E%7B%5Cfrac%7B1%7D%7Bd%2B1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^2 \cap T| \gg_d K^{-O_d(1)} |A|^{\frac{1}{d+1}}}"/>.
</li>
</ul>
</blockquote>
<p/>
<blockquote><p><b>Exercise 26</b>  By repeating the arguments of the preceding section, establish Theorem <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#prod-slf">1</a> for general <img alt="{d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d}"/>. </p></blockquote>
<p/>
<blockquote><p><b>Remark 6</b>  There is an analogue of Exercise <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#spla">19</a>, in which the role of the Borel subgroups is replaced by proper algebraic subgroups of bounded complexity; see Theorem 5.5 of <a href="http://arxiv.org/abs/1005.1881">the paper of Breuillard, Green, and Tao</a> for a more precise statement. </p></blockquote>
<p/>
<p align="center"><b> —  5. Proof of the Larsen-Pink inequality (optional)  — </b></p>
<p>
We now prove Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big">21</a>. In order to escape the burden of having to keep track of the complexity of everything, we will use the tool of <a href="http://en.wikipedia.org/wiki/Ultraproduct">ultraproducts</a> (which we will phrase in the language of <a href="http://en.wikipedia.org/wiki/Nonstandard_analysis">nonstandard analysis</a>). See <a href="http://terrytao.wordpress.com/2011/10/15/254a-notes-6-ultraproducts-as-a-bridge-between-hard-analysis-and-soft-analysis/">this previous blog post</a> for a discussion of ultraproducts and how they can be used to turn quantitative (or “hard”) analysis tasks into qualitative (or “soft”) analysis tasks. One can also use the machinery of schemes and inverse limits as a substitute for the ultraproduct formalism; this is the approach taken in the <a href="http://www.ams.org/mathscinet-getitem?mr=2813339">paper of Larsen and Pink</a>. The <a href="http://arxiv.org/abs/1005.1881">paper of Breuillard, Green, and Tao</a> has a slightly reduced reliance on ultraproducts, at the cost of more complexity bookkeeping, while <a href="http://arxiv.org/abs/1005.1858">the Pyber-Szabo paper</a> avoids ultraproducts altogether but has perhaps the most bookkeeping of all the papers mentioned here (but, by the same token, is the only argument currently known which gives effective bounds). We will thus presume some familiarity both with ultraproducts (and nonstandard analysis) and with algebraic geometry in this section.
</p>
<p>
As in the <a href="http://terrytao.wordpress.com/2011/10/15/254a-notes-6-ultraproducts-as-a-bridge-between-hard-analysis-and-soft-analysis/">previously mentioned blog post</a>, we select a non-principal ultrafilter <img alt="{\alpha \in \beta {\bf N} \backslash {\bf N}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Calpha+%5Cin+%5Cbeta+%7B%5Cbf+N%7D+%5Cbackslash+%7B%5Cbf+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\alpha \in \beta {\bf N} \backslash {\bf N}}"/>, and use it to construct ultraproducts and nonstandard objects. (To ensure the existence of such an object, we shall assume the <a href="http://en.wikipedia.org/wiki/Axiom_of_choice">axiom of choice</a>, as we have already been doing implicitly throughout this course.) We also use the usual nonstandard asymptotic notation, thus for instance <img alt="{O(1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%281%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O(1)}"/> denotes a nonstandard quantity bounded in magnitude by a standard number.
</p>
<p>
The quantitative Larsen-Pink inequality (Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big">21</a>) can then be deduced from the following nonstandard version, in which all references to complexity are now absent:
</p>
<blockquote><p><b>Proposition 22 (Larsen-Pink inequality)</b> <a name="lpi-big-nonst"/> Let <img alt="{d \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d \geq 2}"/> be standard. Let <img alt="{\overline{k} = \prod_{n \rightarrow\alpha} \overline{k_n}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D+%3D+%5Cprod_%7Bn+%5Crightarrow%5Calpha%7D+%5Coverline%7Bk_n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k} = \prod_{n \rightarrow\alpha} \overline{k_n}}"/> be a nonstandard algebraically complete field (i.e. an ultraproduct of standard algebraically complete fields). Let <img alt="{K = \lim_{n \rightarrow\alpha} K_n \geq 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%3D+%5Clim_%7Bn+%5Crightarrow%5Calpha%7D+K_n+%5Cgeq+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K = \lim_{n \rightarrow\alpha} K_n \geq 2}"/> be a nonstandard natural number, and let <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> be a nonstandard <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> (i.e. an ultraproduct <img alt="{A = \prod_{n \rightarrow \alpha} A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3D+%5Cprod_%7Bn+%5Crightarrow+%5Calpha%7D+A_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A = \prod_{n \rightarrow \alpha} A_n}"/> of standard <img alt="{K_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K_n}"/>-approximate subgroups of <img alt="{SL_d(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k_n})}"/>), and let <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> be a subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. Then one of the following is true: </p>
<ul>
<li> (Non-concentration) One has <a name="amvf">
<p align="center"><img alt="\displaystyle  |A^m \cap V| \ll K^{O(1)} |A|^{dim(V)/dim(SL_d)} \ \ \ \ \ (9)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5Em+%5Ccap+V%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7Bdim%28V%29%2Fdim%28SL_d%29%7D+%5C+%5C+%5C+%5C+%5C+%289%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^m \cap V| \ll K^{O(1)} |A|^{dim(V)/dim(SL_d)} \ \ \ \ \ (9)"/></p>
</a><p><a name="amvf"/> for all standard <img alt="{m \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m \geq 1}"/>, where <img alt="{|A| := \lim_{n \rightarrow \alpha} |A_n|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%7C+%3A%3D+%5Clim_%7Bn+%5Crightarrow+%5Calpha%7D+%7CA_n%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A| := \lim_{n \rightarrow \alpha} |A_n|}"/> is the nonstandard cardinality of <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>. </p></li>
<li> (Trapping) <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a proper algebraic subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
Let us see why Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big-nonst">22</a> implies Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big">21</a>. Suppose for contradiction that Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big">21</a> failed. Carefully negating all the quantifiers (and using the axiom of choice), this means that there is a sequence <img alt="{\overline{k_n}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk_n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k_n}}"/> of standard algebraically closed fields, a sequence <img alt="{K_n \ge 2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK_n+%5Cge+2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K_n \ge 2}"/> of standard numbers, a sequence <img alt="{A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_n}"/> of <img alt="{K_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K_n}"/>-approximate subgroups of <img alt="{SL_d(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k_n})}"/>, and a standard <img alt="{M \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M \geq 1}"/>, a sequence <img alt="{V_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_n}"/> of subvarieties of <img alt="{SL_d(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k_n})}"/> of complexity at most <img alt="{M}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{M}"/>, and a standard <img alt="{m \geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm+%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m \geq 1}"/>, such that for each <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>, <img alt="{A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_n}"/> is not contained in a proper algebraicd subgroup of <img alt="{SL_d(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k_n})}"/> of complexity <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> or less, and one has </p>
<p align="center"><img alt="\displaystyle  |A_n^m \cap V_n| \geq n K^n |A|^{dim(V_n)/dim(SL_d)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA_n%5Em+%5Ccap+V_n%7C+%5Cgeq+n+K%5En+%7CA%7C%5E%7Bdim%28V_n%29%2Fdim%28SL_d%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A_n^m \cap V_n| \geq n K^n |A|^{dim(V_n)/dim(SL_d)}."/></p>
<p> Now one forms the ultralimit <img alt="{K :=\lim_{n \rightarrow\alpha} K_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK+%3A%3D%5Clim_%7Bn+%5Crightarrow%5Calpha%7D+K_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K :=\lim_{n \rightarrow\alpha} K_n}"/> and the ultraproducts <img alt="{\overline{k} := \prod_{n \rightarrow \alpha} \overline{k_n}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D+%3A%3D+%5Cprod_%7Bn+%5Crightarrow+%5Calpha%7D+%5Coverline%7Bk_n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k} := \prod_{n \rightarrow \alpha} \overline{k_n}}"/>, <img alt="{A := \prod_{n \rightarrow \alpha} A_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA+%3A%3D+%5Cprod_%7Bn+%5Crightarrow+%5Calpha%7D+A_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A := \prod_{n \rightarrow \alpha} A_n}"/>, <img alt="{V := \prod_{n \rightarrow \alpha} V_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV+%3A%3D+%5Cprod_%7Bn+%5Crightarrow+%5Calpha%7D+V_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V := \prod_{n \rightarrow \alpha} V_n}"/>. Then <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> is an algebraically closed field, <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is a nonstandard <img alt="{K}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BK%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{K}"/>-approximate subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, and <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> is an algebraic subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> (here we use the uniform complexity bound). One can also show that <img alt="{\hbox{dim}(V) = \lim_{n \rightarrow \alpha}\hbox{dim}(V_n)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Bdim%7D%28V%29+%3D+%5Clim_%7Bn+%5Crightarrow+%5Calpha%7D%5Chbox%7Bdim%7D%28V_n%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{dim}(V) = \lim_{n \rightarrow \alpha}\hbox{dim}(V_n)}"/>; see Lemma 3 of <a href="http://terrytao.wordpress.com/2010/01/30/the-ultralimit-argument-and-quantitative-algebraic-geometry/">this blog post</a>. As such, we have
</p><p align="center"><img alt="\displaystyle  |A^m \cap V| \not \ll K^{O(1)} |A|^{dim(V)/dim(SL_d)}," class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5Em+%5Ccap+V%7C+%5Cnot+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7Bdim%28V%29%2Fdim%28SL_d%29%7D%2C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^m \cap V| \not \ll K^{O(1)} |A|^{dim(V)/dim(SL_d)},"/></p>
<p> so by Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big-nonst">22</a>, <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/> is contained in a proper algebraic subgroup <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. By unpacking the coefficients of all the polynomials over <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> used to cut out <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/>, we see that <img alt="{H}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H}"/> is itself an ultraproduct <img alt="{H = \prod_{n \rightarrow \alpha} H_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BH+%3D+%5Cprod_%7Bn+%5Crightarrow+%5Calpha%7D+H_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{H = \prod_{n \rightarrow \alpha} H_n}"/> of proper algebraic subgroups of <img alt="{SL_d(\overline{k_n})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk_n%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k_n})}"/>, of complexity bounded uniformly in <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/>. By <a href="http://en.wikipedia.org/wiki/Ultraproduct#.C5.81o.C5.9B.27s_theorem">Los’s theorem</a>, one has <img alt="{A_n \subset H_n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA_n+%5Csubset+H_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A_n \subset H_n}"/> for all <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> sufficiently close to <img alt="{\alpha}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Calpha%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\alpha}"/>, which gives a contradiction for <img alt="{n}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{n}"/> large enough.</p>
<p>
It remains to establish Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpi-big-nonst">22</a>. By Los’s theorem, the ultraproduct <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> of algebraically closed fields is again algebraically closed, which allows us to use algebraic geometry in the nonstandard field <img alt="{\overline{k}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}}"/> without difficulty.
</p>
<p>
Let <img alt="{\langle A\rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+A%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle A\rangle}"/> be the group generated by <img alt="{A}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A}"/>, and consider the Zariski closure <img alt="{\overline{\langle A \rangle}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7B%5Clangle+A+%5Crangle%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{\langle A \rangle}}"/> of this group, that is to say the intersection of all the varieties containing <img alt="{\langle A \rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+A+%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle A \rangle}"/>. This is again an algebraic variety (here we use the Noetherian property of varieties, that there does not exist any infinite descending chain of varieties), and is also a group (exercise!), and is thus an algebraic subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. If this subgroup is proper then we have the trapping propertly, so we may assume that the closure is all of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. In other words, <img alt="{\langle A\rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+A%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle A\rangle}"/> is <em>Zariski dense</em> in <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>.
</p>
<p>
For any dimension <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> between <img alt="{0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0}"/> and <img alt="{\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{dim}(SL_d)}"/> inclusive, and any standard real <img alt="{\sigma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sigma}"/>, let us call <img alt="{\sigma}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\sigma}"/> <em><img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-admissible</em> if one has the bound </p>
<p align="center"><img alt="\displaystyle  |A^m \cap V| \ll K^{O(1)} |A|^{\sigma}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5Em+%5Ccap+V%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^m \cap V| \ll K^{O(1)} |A|^{\sigma}"/></p>
<p> whenever <img alt="{m\geq 1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm%5Cgeq+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m\geq 1}"/> is standard and <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> is a <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-dimensional subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>. Our task is to show that <img alt="{D/\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%2F%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D/\hbox{dim}(SL_d)}"/> is admissible for all <img alt="{0 \leq D \leq \hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%5Cleq+D+%5Cleq+%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 \leq D \leq \hbox{dim}(SL_d)}"/>. This claim is trivial at the two endpoints <img alt="{D=0}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%3D0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D=0}"/> and <img alt="{D=\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%3D%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D=\hbox{dim}(SL_d)}"/>; the difficulty is to somehow “interpolate” between these two endpoints. We need the following combinatorial observation.</p>
<blockquote><p><b>Exercise 27 (Extreme dimensions)</b>  Suppose for sake of contradiction that <img alt="{D/\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%2F%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D/\hbox{dim}(SL_d)}"/> is inadmissible for some <img alt="{0 &lt; D&lt; \hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%3C+D%3C+%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 &lt; D&lt; \hbox{dim}(SL_d)}"/>. Show that we can find dimensions
</p><p align="center"><img alt="\displaystyle  0 &lt; D_1 \leq D_2 &lt; \hbox{dim}(SL_d)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++0+%3C+D_1+%5Cleq+D_2+%3C+%5Chbox%7Bdim%7D%28SL_d%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  0 &lt; D_1 \leq D_2 &lt; \hbox{dim}(SL_d)"/></p>
<p> and a real number <img alt="{\theta \geq 1/\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Ctheta+%5Cgeq+1%2F%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\theta \geq 1/\hbox{dim}(SL_d)}"/> such that </p>
<ul>
<li> <img alt="{D_1 \theta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1+%5Ctheta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1 \theta}"/> is not <img alt="{D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1}"/>-admissible; </li>
<li> <img alt="{D_2 \theta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2+%5Ctheta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2 \theta}"/> is not <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>-admissible; </li>
<li> <img alt="{D\theta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%5Ctheta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D\theta}"/> is <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-admissible whenever <img alt="{0 \leq D &lt; D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%5Cleq+D+%3C+D_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 \leq D &lt; D_1}"/> or <img alt="{D_2 &lt; D \leq \hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2+%3C+D+%5Cleq+%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2 &lt; D \leq \hbox{dim}(SL_d)}"/>; </li>
<li> <img alt="{(D+1)\theta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%28D%2B1%29%5Ctheta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{(D+1)\theta}"/> is <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-admissible for any <img alt="{0 \leq D \leq \hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0+%5Cleq+D+%5Cleq+%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0 \leq D \leq \hbox{dim}(SL_d)}"/>.
</li>
</ul>
</blockquote>
<p/>
<p>
Let <img alt="{D_1,D_2,\theta}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2CD_2%2C%5Ctheta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1,D_2,\theta}"/> be as in the above exercise. By construction, we can then find subvarieties <img alt="{V_1, V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%2C+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1, V_2}"/> of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> of dimension <img alt="{D_1,D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2CD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1,D_2}"/> respectively and standard positive integers <img alt="{m_1,m_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm_1%2Cm_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m_1,m_2}"/> such that <a name="elo">
</a></p><p align="center"><a name="elo"><img alt="\displaystyle  |A^{m_1} \cap V_1| \not \ll K^{O(1)} |A|^{\theta D_1} \ \ \ \ \ (10)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm_1%7D+%5Ccap+V_1%7C+%5Cnot+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+D_1%7D+%5C+%5C+%5C+%5C+%5C+%2810%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m_1} \cap V_1| \not \ll K^{O(1)} |A|^{\theta D_1} \ \ \ \ \ (10)"/></a></p><a name="elo">
</a><p><a name="elo"/> and <a name="elo-2">
</a></p><p align="center"><a name="elo-2"><img alt="\displaystyle  |A^{m_2} \cap V_2| \not \ll K^{O(1)} |A|^{\theta D_2}. \ \ \ \ \ (11)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm_2%7D+%5Ccap+V_2%7C+%5Cnot+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+D_2%7D.+%5C+%5C+%5C+%5C+%5C+%2811%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m_2} \cap V_2| \not \ll K^{O(1)} |A|^{\theta D_2}. \ \ \ \ \ (11)"/></a></p><a name="elo-2">
</a><p><a name="elo-2"/> On the other hand, we have <a name="vax">
</a></p><p align="center"><a name="vax"><img alt="\displaystyle  |A^{m} \cap V| \ll K^{O(1)} |A|^{\theta (\hbox{dim}(V)+1)} \ \ \ \ \ (12)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm%7D+%5Ccap+V%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+%28%5Chbox%7Bdim%7D%28V%29%2B1%29%7D+%5C+%5C+%5C+%5C+%5C+%2812%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m} \cap V| \ll K^{O(1)} |A|^{\theta (\hbox{dim}(V)+1)} \ \ \ \ \ (12)"/></a></p><a name="vax">
</a><p><a name="vax"/> whenever <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> is a subvariety of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, with the improvement <a name="vax-2">
</a></p><p align="center"><a name="vax-2"><img alt="\displaystyle  |A^{m} \cap V| \ll K^{O(1)} |A|^{\theta \hbox{dim}(V)} \ \ \ \ \ (13)" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm%7D+%5Ccap+V%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+%5Chbox%7Bdim%7D%28V%29%7D+%5C+%5C+%5C+%5C+%5C+%2813%29&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m} \cap V| \ll K^{O(1)} |A|^{\theta \hbox{dim}(V)} \ \ \ \ \ (13)"/></a></p><a name="vax-2">
</a><p><a name="vax-2"/> whenever <img alt="{V}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V}"/> has dimension strictly less than <img alt="{D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1}"/>, or strictly greater than <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>.
</p>
<p>
We can use <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax">(12)</a>, <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax-2">(13)</a> to show that <img alt="{A^{m_1} \times A^{m_2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BA%5E%7Bm_1%7D+%5Ctimes+A%5E%7Bm_2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{A^{m_1} \times A^{m_2}}"/> is “quantitatively Zariski dense” in <img alt="{V_1 \times V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ctimes+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \times V_2}"/>:
</p>
<blockquote><p><b>Lemma 23 (Quantitative Zariski density)</b> <a name="zardens"/> For any proper subvariety <img alt="{W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{W}"/> of <img alt="{V_1 \times V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ctimes+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \times V_2}"/>, we have
</p><p align="center"><img alt="\displaystyle  |(A^{m_1} \times A^{m_2}) \cap W|\ll K^{O(1)} |A|^{\theta (D_1+D_2)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7C%28A%5E%7Bm_1%7D+%5Ctimes+A%5E%7Bm_2%7D%29+%5Ccap+W%7C%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+%28D_1%2BD_2%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |(A^{m_1} \times A^{m_2}) \cap W|\ll K^{O(1)} |A|^{\theta (D_1+D_2)}."/></p>
</blockquote>
<p/>
<p>
<em>Proof:</em>  <img alt="{W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{W}"/> has dimension at most <img alt="{D_1+D_2-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2BD_2-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1+D_2-1}"/>. By standard algebraic geometry, we see that for each <img alt="{0\leq D \leq D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B0%5Cleq+D+%5Cleq+D_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{0\leq D \leq D_1}"/>, the set of <img alt="{y \in V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7By+%5Cin+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{y \in V_2}"/> for which the slice <img alt="{\{ x \in V_1: (x,y) \in W\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+x+%5Cin+V_1%3A+%28x%2Cy%29+%5Cin+W%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ x \in V_1: (x,y) \in W\}}"/> has dimension <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>, has dimension at most <img alt="{D_1+D_2-D-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2BD_2-D-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1+D_2-D-1}"/>. In particular, if <img alt="{D &lt; D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD+%3C+D_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D &lt; D_1}"/>, then by <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax">(12)</a>, <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax-2">(13)</a> the contribution of such <img alt="{x}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x}"/> to <img alt="{|(A^{m_1} \times A^{m_2}) \cap W|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7C%28A%5E%7Bm_1%7D+%5Ctimes+A%5E%7Bm_2%7D%29+%5Ccap+W%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|(A^{m_1} \times A^{m_2}) \cap W|}"/> is at most </p>
<p align="center"><img alt="\displaystyle  K^{O(1)} \times |A|^{\theta D} \times K^{O(1)} |A|^{\theta (D_1+D_2-D-1+1)}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++K%5E%7BO%281%29%7D+%5Ctimes+%7CA%7C%5E%7B%5Ctheta+D%7D+%5Ctimes+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+%28D_1%2BD_2-D-1%2B1%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  K^{O(1)} \times |A|^{\theta D} \times K^{O(1)} |A|^{\theta (D_1+D_2-D-1+1)}"/></p>
<p> while if <img alt="{D = D_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD+%3D+D_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D = D_1}"/>, then the contribution is at most
</p><p align="center"><img alt="\displaystyle  K^{O(1)} \times |A|^{\theta (D+1)} \times K^{O(1)} |A|^{\theta (D_1+D_2-D-1)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++K%5E%7BO%281%29%7D+%5Ctimes+%7CA%7C%5E%7B%5Ctheta+%28D%2B1%29%7D+%5Ctimes+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+%28D_1%2BD_2-D-1%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  K^{O(1)} \times |A|^{\theta (D+1)} \times K^{O(1)} |A|^{\theta (D_1+D_2-D-1)}."/></p>
<p> (One may wonder about the question of uniformity in the <img alt="{O()}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BO%28%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{O()}"/> notation, but in nonstandard analysis one can automatically gain such uniformity through countable saturation; see Exercise 20 of <a href="http://terrytao.wordpress.com/2011/10/15/254a-notes-6-ultraproducts-as-a-bridge-between-hard-analysis-and-soft-analysis/">this blog post</a>.) Summing over all <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> we obtain the claim. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
We will now use a counting argument (which is, unsurprisingly, related to the counting argument used to establish Proposition <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#lpis-approx">17</a>, or any of the other Larsen-Pink inequalities in preceding sections) to obtain a contradiction from these four estimates.
</p>
<p>
First, by decomposing <img alt="{V_1,V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%2CV_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1,V_2}"/> into irreducible components (and using <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax">(12)</a> to eliminate all lower-dimensional components) we may assume that <img alt="{V_1,V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%2CV_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1,V_2}"/> are both irreducible.
</p>
<p>
The product <img alt="{V_1 \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \cdot V_2}"/> is not necessarily a variety, but it is still a constructible set (i.e. a finite boolean combination of varieties), and can still be assigned a dimension (by equating the dimension of a constructible set with the dimension of its Zariski closure). As it contains a translate of <img alt="{V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_2}"/>, it has dimension at least <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>. It would be convenient if <img alt="{V_1 \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \cdot V_2}"/> had dimension strictly greater than <img alt="{V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_2}"/>. This is not necessarily the case, but it turns out that it becomes so after a generic conjugation, thanks to the almost simplicity of <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/>:
</p>
<blockquote><p><b>Exercise 28 (Almost simplicity)</b>  Show that the only proper normal subgroups of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> are those contained in the centre of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, i.e. in the identity matrix multipled by the <img alt="{d^{th}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bd%5E%7Bth%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{d^{th}}"/> roots of unity. (<em>Hint:</em> Let <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> be a normal subgroup of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> that contains an element which is not a multiple of the identity. Place that element in Jordan normal form and divide it by one of its conjugates to make it fix a subspace of <img alt="{\overline{k}^d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Coverline%7Bk%7D%5Ed%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\overline{k}^d}"/>; iterate this procedure until one finds an element in <img alt="{G}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{G}"/> that is the direct sum of the identity in <img alt="{SL_{d-2}(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_%7Bd-2%7D%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_{d-2}(\overline{k})}"/> and a non-central element of <img alt="{SL_2(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_2%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_2(\overline{k})}"/>. Then use this to generate all of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>.) </p></blockquote>
<p/>
<blockquote><p><b>Proposition 24 (Generic skewness)</b>  For generic <img alt="{g \in SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_d(\overline{k})}"/> (i.e. for all <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/> in <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/> outside of a lower-dimensional variety), the set <img alt="{V_1 \cdot g \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \cdot g \cdot V_2}"/> has dimension strictly greater than <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Let <img alt="{g \in SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_d(\overline{k})}"/>, and assume that <img alt="{V_1 \cdot g \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \cdot g \cdot V_2}"/> has dimension exactly <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>. This set contains all the translates <img alt="{xg V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bxg+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{xg V_2}"/> with <img alt="{x \in V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+V_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in V_1}"/>, which are each <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>-dimensional irreducible varieties. By splitting up <img alt="{V_1\cdot g \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%5Ccdot+g+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1\cdot g \cdot V_2}"/> into components, we conclude that there are only finitely many distinct translates <img alt="{xg V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bxg+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{xg V_2}"/>. If we denote one of these translates as <img alt="{W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{W}"/>, the set <img alt="{\{ x \in SL_d(\overline{k}): xgV_2 = W \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+x+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%3A+xgV_2+%3D+W+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ x \in SL_d(\overline{k}): xgV_2 = W \}}"/> is easily seen to be a variety (as it is the intersection of varieties <img alt="{Wy^{-1}g^{-1}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BWy%5E%7B-1%7Dg%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{Wy^{-1}g^{-1}}"/> for <img alt="{y \in V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7By+%5Cin+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{y \in V_2}"/>); as a finite number of these sets cover <img alt="{V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1}"/>, at least one of them has to be all of <img alt="{V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1}"/>; thus there is a <img alt="{W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{W}"/> such that <img alt="{xgV_2=W}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BxgV_2%3DW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{xgV_2=W}"/> for all <img alt="{x \in V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+V_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in V_1}"/>. In particular, this implies that <img alt="{g^{-1} y^{-1} x g V_2 = V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+y%5E%7B-1%7D+x+g+V_2+%3D+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} y^{-1} x g V_2 = V_2}"/> for all <img alt="{x,y \in V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx%2Cy+%5Cin+V_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x,y \in V_1}"/>.
</p>
<p>
Let <img alt="{S := \{ h \in SL_d(\overline{k}): hV_2 = V_2\}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS+%3A%3D+%5C%7B+h+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%3A+hV_2+%3D+V_2%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S := \{ h \in SL_d(\overline{k}): hV_2 = V_2\}}"/>. Arguing as before, <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> is a variety, and is also a group; it is thus an algebraic group, and by the preceding discussion we have <img alt="{g^{-1} V_1^{-1} V_1 g \subset S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+V_1%5E%7B-1%7D+V_1+g+%5Csubset+S%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} V_1^{-1} V_1 g \subset S}"/>.
</p>
<p>
The set <img alt="{\{ g \in SL_d(\overline{k}): g^{-1} V_1^{-1} V_1 g \subset S \}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5C%7B+g+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%3A+g%5E%7B-1%7D+V_1%5E%7B-1%7D+V_1+g+%5Csubset+S+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\{ g \in SL_d(\overline{k}): g^{-1} V_1^{-1} V_1 g \subset S \}}"/> is a variety. If it has dimension strictly less than that of <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/>, we are done, so we may assume this set is all of <img alt="{SL_d}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d}"/>; thus <img alt="{g^{-1} V_1^{-1} V_1 g \subset S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%5E%7B-1%7D+V_1%5E%7B-1%7D+V_1+g+%5Csubset+S%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g^{-1} V_1^{-1} V_1 g \subset S}"/> for all <img alt="{g \in SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in SL_d(\overline{k})}"/>. By almost simplicity, the normal subgroup generated by <img alt="{V_1^{-1} V_1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1%5E%7B-1%7D+V_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1^{-1} V_1}"/> is all of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>; thus <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> must be all of <img alt="{SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BSL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{SL_d(\overline{k})}"/>, thus <img alt="{hV_2 = V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BhV_2+%3D+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{hV_2 = V_2}"/> for all <img alt="{h \in SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bh+%5Cin+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{h \in SL_d(\overline{k})}"/>. But this forces <img alt="{V_2 = SL_d(\overline{k})}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_2+%3D+SL_d%28%5Coverline%7Bk%7D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_2 = SL_d(\overline{k})}"/>, a contradiction since <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/> is strictly less than <img alt="{\hbox{dim}(SL_d)}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Chbox%7Bdim%7D%28SL_d%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\hbox{dim}(SL_d)}"/>. <img alt="\Box" class="latex" src="http://s0.wp.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\Box"/></p>
<p>
Combining this proposition with the Zariski density of <img alt="{\langle A\rangle}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Clangle+A%5Crangle%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\langle A\rangle}"/>, we see that we can find <img alt="{g \in A^m}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg+%5Cin+A%5Em%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g \in A^m}"/> for some standard <img alt="{m}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bm%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{m}"/> such that <img alt="{V_1 \cdot g \cdot V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \cdot g \cdot V_2}"/> has dimension <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/> strictly greater than <img alt="{D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_2}"/>.
</p>
<p>
Fix this <img alt="{g}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bg%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{g}"/>. Let <img alt="{\phi: V_1 \times V_2 \rightarrow \overline{V_1 \cdot g \cdot V_2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%3A+V_1+%5Ctimes+V_2+%5Crightarrow+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi: V_1 \times V_2 \rightarrow \overline{V_1 \cdot g \cdot V_2}}"/> be the twisted product map <img alt="{\phi(x,y) := xgy}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%28x%2Cy%29+%3A%3D+xgy%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi(x,y) := xgy}"/>. We have the double counting identity </p>
<p align="center"><img alt="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\})| = |A^{m_1} \cap V_1| |A^{m_2} \cap V_2|" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bz+%5Cin+A%5E%7Bm_1%2Bm%2Bm_2%7D+%5Ccap+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D+%7CA%5E%7Bm_1%7D%5Ctimes+A%5E%7Bm_2%7D+%5Ccap+%5Cphi%5E%7B-1%7D%28%5C%7Bz%5C%7D%29%7C+%3D+%7CA%5E%7Bm_1%7D+%5Ccap+V_1%7C+%7CA%5E%7Bm_2%7D+%5Ccap+V_2%7C&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\})| = |A^{m_1} \cap V_1| |A^{m_2} \cap V_2|"/></p>
<p> and thus by <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#elo">(10)</a>, <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#elo-2">(11)</a>
</p><p align="center"><img alt="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\})| \not \ll K^{O(1)} |A|^{\theta(D_1+D_2)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bz+%5Cin+A%5E%7Bm_1%2Bm%2Bm_2%7D+%5Ccap+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D+%7CA%5E%7Bm_1%7D%5Ctimes+A%5E%7Bm_2%7D+%5Ccap+%5Cphi%5E%7B-1%7D%28%5C%7Bz%5C%7D%29%7C+%5Cnot+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta%28D_1%2BD_2%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\})| \not \ll K^{O(1)} |A|^{\theta(D_1+D_2)}."/></p>
<p>
Now, <img alt="{\phi}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi}"/> is a map from an irreducible <img alt="{D_1+D_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2BD_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1+D_2}"/>-dimensional variety to a <img alt="{D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D}"/>-dimensional variety with Zariski-dense image, and is thus a <em>dominant map</em>. Among other things, this implies that there is a subvariety <img alt="{S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{S}"/> of <img alt="{V_1 \times V_2}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BV_1+%5Ctimes+V_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{V_1 \times V_2}"/> of dimension at most <img alt="{D_1+D_2-1}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2BD_2-1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1+D_2-1}"/> such that for all <img alt="{x \in \overline{V_1 \cdot g \cdot V_2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bx+%5Cin+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{x \in \overline{V_1 \cdot g \cdot V_2}}"/>, the set <img alt="{\phi^{-1}(\{x\}) \backslash S}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%5Cphi%5E%7B-1%7D%28%5C%7Bx%5C%7D%29+%5Cbackslash+S%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{\phi^{-1}(\{x\}) \backslash S}"/> has dimension <img alt="{D_1+D_2-D}" class="latex" src="http://s0.wp.com/latex.php?latex=%7BD_1%2BD_2-D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{D_1+D_2-D}"/>. By <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax-2">(13)</a>, we then have </p>
<p align="center"><img alt="\displaystyle  |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\}) \backslash S| \ll K^{O(1)} |A|^{\theta(D_1+D_2-D)}" class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm_1%7D%5Ctimes+A%5E%7Bm_2%7D+%5Ccap+%5Cphi%5E%7B-1%7D%28%5C%7Bz%5C%7D%29+%5Cbackslash+S%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta%28D_1%2BD_2-D%29%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\}) \backslash S| \ll K^{O(1)} |A|^{\theta(D_1+D_2-D)}"/></p>
<p> for all <img alt="{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}}" class="latex" src="http://s0.wp.com/latex.php?latex=%7Bz+%5Cin+A%5E%7Bm_1%2Bm%2Bm_2%7D+%5Ccap+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}}"/>; by another application of <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#vax-2">(13)</a>, we have
</p><p align="center"><img alt="\displaystyle  |A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}| \ll K^{O(1)} |A|^{\theta D}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%7CA%5E%7Bm_1%2Bm%2Bm_2%7D+%5Ccap+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7C+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta+D%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  |A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}| \ll K^{O(1)} |A|^{\theta D}."/></p>
<p> Combining these estimates we see that
</p><p align="center"><img alt="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\}) \cap S| \not \ll K^{O(1)} |A|^{\theta(D_1+D_2)}." class="latex" src="http://s0.wp.com/latex.php?latex=%5Cdisplaystyle++%5Csum_%7Bz+%5Cin+A%5E%7Bm_1%2Bm%2Bm_2%7D+%5Ccap+%5Coverline%7BV_1+%5Ccdot+g+%5Ccdot+V_2%7D%7D+%7CA%5E%7Bm_1%7D%5Ctimes+A%5E%7Bm_2%7D+%5Ccap+%5Cphi%5E%7B-1%7D%28%5C%7Bz%5C%7D%29+%5Ccap+S%7C+%5Cnot+%5Cll+K%5E%7BO%281%29%7D+%7CA%7C%5E%7B%5Ctheta%28D_1%2BD_2%29%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="\displaystyle  \sum_{z \in A^{m_1+m+m_2} \cap \overline{V_1 \cdot g \cdot V_2}} |A^{m_1}\times A^{m_2} \cap \phi^{-1}(\{z\}) \cap S| \not \ll K^{O(1)} |A|^{\theta(D_1+D_2)}."/></p>
<p> The left-hand side simplifies to <img alt="{|A^{m_1} \times A^{m_2} \cap S|}" class="latex" src="http://s0.wp.com/latex.php?latex=%7B%7CA%5E%7Bm_1%7D+%5Ctimes+A%5E%7Bm_2%7D+%5Ccap+S%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" title="{|A^{m_1} \times A^{m_2} \cap S|}"/>. But this then contradicts Lemma <a href="http://terrytao.wordpress.com/2012/02/05/254b-notes-5-product-theorems-pivot-arguments-and-the-larsen-pink-non-concentration-inequality/#zardens">23</a>.</p>
<br/>Filed under: <a href="http://terrytao.wordpress.com/category/teaching/254b-expansion-in-groups/">254B - expansion in groups</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathag/">math.AG</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathco/">math.CO</a>, <a href="http://terrytao.wordpress.com/category/mathematics/mathgr/">math.GR</a> Tagged: <a href="http://terrytao.wordpress.com/tag/larsen-pink-inequality/">Larsen-Pink inequality</a>, <a href="http://terrytao.wordpress.com/tag/product-theorems/">product theorems</a>, <a href="http://terrytao.wordpress.com/tag/special-linear-group/">special linear group</a>, <a href="http://terrytao.wordpress.com/tag/sum-product-theorems/">sum-product theorems</a>, <a href="http://terrytao.wordpress.com/tag/ultraproducts/">ultraproducts</a> <a href="http://feeds.wordpress.com/1.0/gocomments/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/terrytao.wordpress.com/5714/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/terrytao.wordpress.com/5714/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/terrytao.wordpress.com/5714/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=5714&amp;subd=terrytao&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-11T18:04:57Z</updated>
    <published>2012-02-05T19:32:41Z</published>
    <category scheme="http://terrytao.wordpress.com" term="254B - expansion in groups"/>
    <category scheme="http://terrytao.wordpress.com" term="math.AG"/>
    <category scheme="http://terrytao.wordpress.com" term="math.CO"/>
    <category scheme="http://terrytao.wordpress.com" term="math.GR"/>
    <category scheme="http://terrytao.wordpress.com" term="Larsen-Pink inequality"/>
    <category scheme="http://terrytao.wordpress.com" term="product theorems"/>
    <category scheme="http://terrytao.wordpress.com" term="special linear group"/>
    <category scheme="http://terrytao.wordpress.com" term="sum-product theorems"/>
    <category scheme="http://terrytao.wordpress.com" term="ultraproducts"/>
    <author>
      <name>Terence Tao</name>
      <uri>http://www.math.ucla.edu/~tao</uri>
    </author>
    <source>
      <id>http://terrytao.wordpress.com/feed/atom/</id>
      <link href="http://terrytao.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://terrytao.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://terrytao.wordpress.com/osd.xml" rel="search" title="What&amp;#039;s new" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://terrytao.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <title xml:lang="en">What's new</title>
      <updated>2012-02-15T04:28:30Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://quomodocumque.wordpress.com/?p=3305</id>
    <link href="http://quomodocumque.wordpress.com/2012/02/10/would-the-death-of-the-journal-system-be-good-for-women-in-math/" rel="alternate" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/10/would-the-death-of-the-journal-system-be-good-for-women-in-math/#comments" rel="replies" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/10/would-the-death-of-the-journal-system-be-good-for-women-in-math/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Would the death of the journal system be good for women in math?</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">I am not one of the most radical signatories to the “Cost of Knowledge” statement:  there are certainly some among us who look forward to a world without commercial journals, or even a world without journals at all.  I don’t yet see a clear path to that world. Nonetheless, I want to add one possible [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3305&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>I am not one of the most radical signatories to <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf">the “Cost of Knowledge” statement</a>:  there are certainly some among us who look forward to a world without commercial journals, or even a world without journals at all.  I don’t yet see a clear path to that world.</p>
<p>Nonetheless, I want to add one possible item to the case against journals.</p>
<p>There is lots of inequity in the way mathematicians are assigned status — we all have researchers we think are underappreciated (and some people are quite willing to talk about who they think is overappreciated.)</p>
<p>One very simple source of inequity — but I’ll bet a pretty large one — is that <em>authors decide what journal to submit to</em>.  Some people “aim high” — their method is to ask “what’s the best journal where this paper would fit?”  Others “aim low,” asking something more like “what’s the median journal where papers like this appear?”  You can’t get in the Annals unless you submit to the Annals, and you won’t submit to the Annals very often if you aim low.</p>
<p>Women in the workplace <a href="http://www.nytimes.com/2008/04/06/jobs/06pre.html">are socialized not to ask for things</a>.  I wouldn’t be surprised to learn that there are disproportionately many men in the “aim high, why shouldn’t my paper be in the Annals?” group.  (And of course, for those who get het up whenever I talk about women in math, this applies just as well to any group of mathematicians disinclined to push for their own work.)</p>
<p>Would things be different if papers in the Annals were selected from <em>all</em> papers, not just those whose authors decided to nominate themselves?  Then publication in a top journal would be a little more like being invited to speak at a prestigious conference.  Would that be an improvement?</p>
<p> </p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/quomodocumque.wordpress.com/3305/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/quomodocumque.wordpress.com/3305/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/quomodocumque.wordpress.com/3305/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3305&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-11T05:18:12Z</updated>
    <published>2012-02-11T05:18:12Z</published>
    <category scheme="http://quomodocumque.wordpress.com" term="academia"/>
    <category scheme="http://quomodocumque.wordpress.com" term="math"/>
    <category scheme="http://quomodocumque.wordpress.com" term="journals"/>
    <category scheme="http://quomodocumque.wordpress.com" term="publishing"/>
    <category scheme="http://quomodocumque.wordpress.com" term="women in math"/>
    <author>
      <name>JSE</name>
      <uri>http://quomodocumque.wordpress.com</uri>
    </author>
    <source>
      <id>http://quomodocumque.wordpress.com/feed/atom/</id>
      <link href="http://quomodocumque.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://quomodocumque.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://quomodocumque.wordpress.com/osd.xml" rel="search" title="Quomodocumque" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://quomodocumque.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Math, Madison, food, the Orioles, books, my kids.</subtitle>
      <title xml:lang="en">Quomodocumque</title>
      <updated>2012-02-15T00:49:06Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-10448119.post-5998071383265765690</id>
    <link href="http://hoggresearch.blogspot.com/feeds/5998071383265765690/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/electromagnetism-and-massive-stars.html#comment-form" rel="replies" title="3 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/5998071383265765690" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/5998071383265765690" rel="self" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/electromagnetism-and-massive-stars.html" rel="alternate" title="electromagnetism and massive stars" type="text/html"/>
    <title>electromagnetism and massive stars</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Inspired in part by our meetings yesterday about Fergus's modeling of imaging data in a coronograph, I worked on a physically motivated re-factor of my physically motivated code to model electromagnetic fields (phase and amplitude) in astronomical telescopes and cameras.  I am just a few dozen lines of code away from having a full model (highly approximate) of a simple coronograph.</p><p>In the afternoon, Selma de Mink (STScI) gave a nice seminar about extremely massive star evolution.  Among many other things, she noted that there is a possibility that low-metallicity, rapidly rotating, massive stars could evolve to very hot temperatures and very high luminosities where no other kinds of stars can be.  I think we can find these things in <i>PHAT</i> data on Andromeda; I need to email the team.</p><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/10448119-5998071383265765690?l=hoggresearch.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-11T03:29:23Z</updated>
    <published>2012-02-11T03:29:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="seminar"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="telescope"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="PHAT"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="star"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="code"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="model"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="imaging"/>
    <author>
      <name>Hogg</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/18398397408280534592</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-10448119</id>
      <category term="Willman 1"/>
      <category term="clustering"/>
      <category term="merging"/>
      <category term="galaxy"/>
      <category term="PHAT"/>
      <category term="HMF"/>
      <category term="proper motion"/>
      <category term="amateur"/>
      <category term="sdss"/>
      <category term="LSST"/>
      <category term="virtual observatory"/>
      <category term="tractor"/>
      <category term="robot"/>
      <category term="funding"/>
      <category term="telescope"/>
      <category term="digital camera"/>
      <category term="meta data"/>
      <category term="proposal"/>
      <category term="disk"/>
      <category term="fundamental astronomy"/>
      <category term="roweis"/>
      <category term="classification"/>
      <category term="practice"/>
      <category term="decision"/>
      <category term="travel"/>
      <category term="linear algebra"/>
      <category term="interstellar medium"/>
      <category term="web 2.0"/>
      <category term="email"/>
      <category term="bayes"/>
      <category term="scattering"/>
      <category term="atlas"/>
      <category term="quasar"/>
      <category term="confusion"/>
      <category term="minor planet"/>
      <category term="anthropology"/>
      <category term="gravitational lensing"/>
      <category term="reading"/>
      <category term="black hole"/>
      <category term="visualization"/>
      <category term="halo"/>
      <category term="cosmology"/>
      <category term="seminar"/>
      <category term="information"/>
      <category term="2mass"/>
      <category term="chemistry"/>
      <category term="HST"/>
      <category term="gravity"/>
      <category term="panstarrs"/>
      <category term="philosophy"/>
      <category term="experiment"/>
      <category term="WMAP"/>
      <category term="sample"/>
      <category term="baryon acoustic feature"/>
      <category term="radial velocity"/>
      <category term="ukidss"/>
      <category term="dark sector"/>
      <category term="parallax"/>
      <category term="spectroscopy"/>
      <category term="brown dwarf"/>
      <category term="LTFDFCF"/>
      <category term="kinematics"/>
      <category term="cosmography"/>
      <category term="transparency"/>
      <category term="flickr"/>
      <category term="calibration"/>
      <category term="optimization"/>
      <category term="editing"/>
      <category term="star formation"/>
      <category term="ultraviolet"/>
      <category term="statistics"/>
      <category term="testing"/>
      <category term="correlation"/>
      <category term="galex"/>
      <category term="intergalactic medium"/>
      <category term="noise"/>
      <category term="computing"/>
      <category term="dissertation"/>
      <category term="citizen science"/>
      <category term="nasa"/>
      <category term="planet"/>
      <category term="wise"/>
      <category term="talking"/>
      <category term="spitzer"/>
      <category term="cluster"/>
      <category term="CDM"/>
      <category term="astrometry"/>
      <category term="environment"/>
      <category term="imaging"/>
      <category term="press"/>
      <category term="MCMC"/>
      <category term="gaia"/>
      <category term="evolution"/>
      <category term="primus"/>
      <category term="compression"/>
      <category term="phase space"/>
      <category term="relativity"/>
      <category term="weapons"/>
      <category term="archive"/>
      <category term="Solar System"/>
      <category term="Milky Way"/>
      <category term="code"/>
      <category term="observing"/>
      <category term="learning"/>
      <category term="point-spread function"/>
      <category term="Euclid"/>
      <category term="hardware"/>
      <category term="catalog"/>
      <category term="science"/>
      <category term="database"/>
      <category term="thinking"/>
      <category term="gamma-ray burst"/>
      <category term="exoplanet"/>
      <category term="white dwarf"/>
      <category term="theory"/>
      <category term="hipparcos"/>
      <category term="radio"/>
      <category term="law"/>
      <category term="pulsar"/>
      <category term="Gaussian process"/>
      <category term="osss"/>
      <category term="politics"/>
      <category term="meeting"/>
      <category term="photometry"/>
      <category term="star"/>
      <category term="not research"/>
      <category term="API"/>
      <category term="cosmic ray"/>
      <category term="substructure"/>
      <category term="post-starburst"/>
      <category term="archetype"/>
      <category term="life"/>
      <category term="time"/>
      <category term="literature"/>
      <category term="dynamics"/>
      <category term="comet"/>
      <category term="anthropic"/>
      <category term="supernova"/>
      <category term="Earth"/>
      <category term="PTF"/>
      <category term="Fermi"/>
      <category term="search"/>
      <category term="usno-b"/>
      <category term="mathematics"/>
      <category term="dust"/>
      <category term="coffee"/>
      <category term="project management"/>
      <category term="model"/>
      <category term="data"/>
      <category term="writing"/>
      <author>
        <name>Hogg</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/18398397408280534592</uri>
      </author>
      <link href="http://hoggresearch.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://hoggresearch.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>galaxies, stellar dynamics, exoplanets, and fundamental astronomy</subtitle>
      <title>Hogg's Research</title>
      <updated>2012-02-14T20:52:31Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-6912603287930240451.post-944448927498833856</id>
    <link href="http://noncommutativegeometry.blogspot.com/feeds/944448927498833856/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=6912603287930240451&amp;postID=944448927498833856" rel="replies" title="0 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/6912603287930240451/posts/default/944448927498833856" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/6912603287930240451/posts/default/944448927498833856" rel="self" type="application/atom+xml"/>
    <link href="http://noncommutativegeometry.blogspot.com/2012/02/new-book-noncommutative-geometry.html" rel="alternate" title="A new book: Noncommutative geometry,  arithmetic, and related topics" type="text/html"/>
    <title>A new book: Noncommutative geometry,  arithmetic, and related topics</title>
    <summary>Proceedings of the  JAMI 2009 meeting on ``Noncommutative geometry, arithmetic, and related topics" Just published by Johns Hopkins University Press is available in the market now.Happy reading!</summary>
    <updated>2012-02-11T00:38:43Z</updated>
    <published>2012-02-10T22:22:00Z</published>
    <author>
      <name>Masoud Khalkhali</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/03769072750559219167</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-6912603287930240451</id>
      <category term="information"/>
      <category term="quantization"/>
      <category term="function fields"/>
      <category term="number-theory"/>
      <category term="general"/>
      <category term="multimedia"/>
      <category term="number theory"/>
      <author>
        <name>Arup</name>
        <email>noreply@blogger.com</email>
      </author>
      <link href="http://noncommutativegeometry.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/6912603287930240451/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://noncommutativegeometry.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/6912603287930240451/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <title>Noncommutative geometry</title>
      <updated>2012-02-13T16:10:51Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.quantumdiaries.org/?p=20232</id>
    <link href="http://www.quantumdiaries.org/2012/02/10/peer-review/" rel="alternate" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/10/peer-review/#comments" rel="replies" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/10/peer-review/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Peer Review: A Cornerstone of Science</title>
    <summary xml:lang="en">Ah yes, peer review; one of the more misunderstood parts of the scientific method. Peer review is frequently treated as an incantation to separate the wheat from the chaff. What has been peered reviewed is good; what hasn’t is bad. But life is never so simple. In the late 1960s, Joseph Weber (1919 – 2000) [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Ah yes, peer review; one of the more misunderstood parts of the scientific method. Peer review is frequently treated as an incantation to separate the wheat from the chaff. What has been peered reviewed is good; what hasn’t is bad. But life is never so simple. In the late 1960s, Joseph Weber (1919 – 2000) published two Physical Review Letters were he claimed to have detected gravitational waves. Although there are a few holdouts who believed he did, the general consensus is that he did not, since his results have not been reproduced. Rather it is generally believed that his results were an experimental artifact. His results were peer reviewed and accepted at a “prestigious” journal but that does not guarantee that they are correct. Even the Nobel committee occasionally makes mistakes, most notably giving the award to the discoverer of lobotomies.</p>
<p>Conversely, consider the case of Alfred Wegener (1880 – 1930). In 1912 he proposed the idea of continental drift. To say the least, it was not enthusiastically received. It did not help that Wegener was meteorologist, not a geologist. This theory was largely rejected by his peers in geology. For example, the University of Chicago geologist Rollin T. Chamberlin said, <em>If we are to believe in Wegener’s hypothesis we must forget everything which has been learned in the past 70 years and start all over again</em>. In 1926, the American Association of Petroleum Geologists (AAPG) held a special <em>symposium</em> on the hypothesis of <em>continental drift</em> and rejected it. After that, the hypothesis was strictly on the fringe until the late 1950s and early ‘60s when it finally became mainstream.</p>
<p>Thus, we see that peer review cannot <em>definitively</em> be relied on to give the final answer. So what use is peer review? The problem is that, as pointed out in previous posts, in science there is no one person who can serve as the ultimate authority; rather, observation is. As a school student, the teacher knows more than the student and can be considered the final authority. In university, the professor plays that role, sometimes with gusto. But when it comes to research, frequently it is the researcher him/herself who is the world expert. So how can research be judged and how do we make decisions about that research? And decisions do have to be made. We cannot publish everything—the useful results would get lost in the noise. We must maintain the collective wisdom that has been laboriously developed. Similarly, decisions have to be made on who gets research grants. Do we use a random number generator? Ok, no snide remarks, I admit that it does <strong>occasionally</strong> look like we do.  As there is no single human to serve as the final authority, we turn to the people who know the most about the topic, namely the peers of the person. If we want a decision related to sheep farming, we consult sheep farmers; if about nuclear physics, we consult nuclear physicists. Peer review is simply the idea that when we have to make a decision, we consult those people most likely to be able to make an informed decision. Is it perfect? No. Is there a better process? Perhaps, but no one seems to know what it is.</p>
<p>Peer review is also used as a bulwark against bull…, oops, material, that is of questionable validity. The expression, <em>that has not been peer reviewed, </em>is used as a euphemism for, <em>that is complete and utter crap and I am not going to waste my time dealing with it.</em> In this case it tends to come across as closed minded: <em>Not</em> <em>peer reviewed?  It’s nonsense!</em> Needless to say, cranks take great exception and tend to regard peer review as a new priesthood who stifles innovation.  And indeed, as noted above, sometimes peer review does get it wrong. There is always this tension between accepting nonsense and rejecting the next big thing. As the case of continental drift illustrates, it is sometimes only in retrospect, when we have more data, that we can tell what the correct answer is. However, it is better to reject or delay the acceptance of something that has a good chance of being wrong than to have the literature overrun with wrong results (think lobotomies). However, contrary to popular conception, Copernicus and Wegener are the exception, not the rule. That is why Copernicus is still used as the example of the suppression of ideas half a millennium later—there are just not that many good examples. And I might add that both Copernicus and Wegener were initially rejected for good reasons and were accepted once sufficient supporting data came to light.  Most people, who the peer review process deems to be cranks, are indeed cranks. Never heard of <a href="http://en.wikipedia.org/wiki/Immanuel_Velikovsky">Immanuel Velikovsky</a> (1895 – 1979)? Well, there is a reason. The few who were right are remembered, but the multitudes that were wrong are, like Velikovsky, forgotten.</p>
<p>Peer review is one of the cornerstones of science and is an essential part of its error control process. At every level in science we use peers to check for errors. Within well-run collaborations, results are reviewed by the peers within the collaboration before submitting for publication. I will get my peers to read my papers before submission. Even the editing of these posts before being put on line can be considered peer review. Then there is the formal peer review a paper receives when it is submitted to a journal. In many ways this is the least important peer review because it is after a paper is published that it receives its most vigorous peer review. I can be quite sure there is no fundamental flaw in special relativity, not because Einstein was a genius, not because it was published in a prestigious journal, but because after it was published many very clever people tried very hard to find flaws in it and failed. Any widely read scientific paper will be subject to this thorough scrutiny by the author’s peers.  That is the reason we can have confidence in the results of science and why secrecy is the enemy of scientific progress. Given enough eyeballs, <em>all</em><em> </em><em>bugs</em><em> </em>are <em>shallow</em><a href="http://www.quantumdiaries.org/2012/02/10/peer-review/#_ftn1">[1]</a>.</p>
<p><strong><em>Additional posts in this series will appear most Friday afternoons at 3:30 pm Vancouver time. </em><em>To receive a reminder follow me on Twitter: @musquod.</em></strong></p>
<p> </p>
<div>
<hr size="1"/>
<div>
<p><a href="http://www.quantumdiaries.org/2012/02/10/peer-review/#_ftnref1">[1]</a> <a href="http://en.wikipedia.org/wiki/The_Cathedral_and_the_Bazaar">The Cathedral and the Bazaar</a>, Eric Raymond</p>
</div>
</div></div>
    </content>
    <updated>2012-02-10T23:15:09Z</updated>
    <published>2012-02-10T23:30:17Z</published>
    <category scheme="http://www.quantumdiaries.org" term="Latest Posts"/>
    <category scheme="http://www.quantumdiaries.org" term="Peer Review"/>
    <category scheme="http://www.quantumdiaries.org" term="Philosophy of science"/>
    <author>
      <name>Byron</name>
      <uri>http://www.triumf.ca/theory/byron-jennings</uri>
    </author>
    <source>
      <id>http://www.quantumdiaries.org/feed/atom/</id>
      <link href="http://www.quantumdiaries.org" rel="alternate" type="text/html"/>
      <link href="http://www.quantumdiaries.org/feed/atom/" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">Thoughts on work and life from particle physicists from around the world.</subtitle>
      <title xml:lang="en">Quantum Diaries</title>
      <updated>2012-02-14T16:23:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://gowers.wordpress.com/?p=3940</id>
    <link href="http://gowers.wordpress.com/2012/01/29/whats-wrong-with-electronic-journals/" rel="alternate" type="text/html"/>
    <link href="http://gowers.wordpress.com/2012/01/29/whats-wrong-with-electronic-journals/#comments" rel="replies" type="text/html"/>
    <link href="http://gowers.wordpress.com/2012/01/29/whats-wrong-with-electronic-journals/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">What’s wrong with electronic journals?</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">It probably sounds disingenuous of me to say this, but when I sat down to write a post about Elsevier I wasn’t really trying to start a campaign. My intention was merely to make public, and a little more rigid, a policy that I and many others had already been applying, in my case without [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=gowers.wordpress.com&amp;blog=1659011&amp;post=3940&amp;subd=gowers&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>It probably sounds disingenuous of me to say this, but when I sat down to write a post about Elsevier I wasn’t really trying to start a campaign. My intention was merely to make public, and a little more rigid, a policy that I and many others had already been applying, in my case without much difficulty, for several years. The idea of setting up a website occurred to me as I was writing the post: I considered it (and still consider it) not as a petition to Elsevier to change its ways — since I don’t believe there is any realistic chance of that — but as a simple way to bring out into the open all the private boycotts and semi-boycotts that were going on, and thereby to encourage others to do the same. </p>
<p>By accident, the post seems to have been quite well timed. Probably it’s not an accident at all, and that whatever atmosphere it was that prompted me to get round to writing the post (for example, certain discussions I had had with other mathematicians, some of them online) was the same as what made it a good moment. Anyhow, accident or no, the result is that some people have talked about “momentum”, and I’m starting to feel a responsibility, not particularly welcome (because it threatens to involve work), not to squander that momentum.<br/>
<span id="more-3940"/></p>
<p>I’ve actually been ill in bed for much of the last few days, so most of the rest of this post will be reporting on some feverish thoughts, which I’ll try to organize into a more coherent form. I’ll also try not to write too much, though that may be quite difficult.</p>
<p><strong>What next?</strong></p>
<p>What I really mean is more like, “How much next?” Do we just let the number of signatures at <a href="http://thecostofknowledge.com/" target="_blank">Tyler Neylon’s website</a> continue to grow at its currently healthy rate and sit back and hope that at some point there will be a phase change? That was something like my original plan — or rather non-plan. But there are reasons to suppose that provoking a phase change will take a bit more effort.  </p>
<p>I felt I had at least to think about that when <a href="http://gowers.wordpress.com/2012/01/23/httpthecostofknowledge-com/#comment-14789">Michael Harris made a comment</a> of which here is the beginning.</p>
<blockquote><p>When the number of signatures reaches a certain target figure — 500, say, or 1000 — the next step is to send an open letter to the members of the editorial board of one of the Elsevier journals, explaining why they might want either to look into changing publishers or, if this is impossible for contractual reasons, to resign. Since the editors are colleagues, the tone should not be confrontational. Instead, one should make the point that their remaining on the editorial board in the face of such a massive show of rejection will naturally be interpreted as a defense of Elsevier’s business practices; and more pragmatically, it will be more difficult to maintain the quality of a journal subject to boycott.</p>
<p>I’m willing to draft such a letter if there is sufficient interest and if no one else volunteers, though I’m hardly the most qualified to do so. It would need at least 20 signatures from a broad sampling of mathematical specialties.</p></blockquote>
<p>My initial impulse on reading this was to think that maybe that was moving a bit fast. I also latched on eagerly to the words “the tone should not be confrontational” and started mentally drafting letters full of assurances that they were not in any sense a criticism etc. etc. Meanwhile, it soon became clear that the 1000-signatures mark would be quickly passed, as it now has been. (However, the proportion of mathematicians has dropped. For a while it was almost 100% but now it is a lot less than that. So a target that might be appropriate is 1000 mathematicians. Restricting the list by subject is not yet possible, but Tyler Neylon assures me that it will become so. With a bit of effort, I’ve done a not terribly reliable count and concluded that there are 430 mathematicians so far.) </p>
<p>I then read this (written, as you can see, in response to <a href="http://gowers.wordpress.com/2012/01/21/elsevier-my-part-in-its-downfall/#comment-14659">another comment</a>).</p>
<blockquote><p>Stan,</p>
<p>We agree that technology is making publishing an electronic journal easy without technical expertise.</p>
<p>A group of current UChicago and forner grad students and alums have created Scholastica, (http://www.scholasticahq.com), an academic journal management platform and scholarly community. Anyone can create their own peer reviewed journal, manage their peer review process, and ultimately publish without the need for publishing companies like Elsevier. There’s also a section of the application called ‘The Conversation’ (http://scholasticahq.com/conversation) that is very similar to Mathoverflow that allows academics to build reputation points that can be used to be recruited as a referee.</p>
<p>We hope that this is seen as more than a shameless plug as we’ve been working tirelessly over the last year with no pay to provide something to address the problems with academic publishing that Tim and others describe here.</p>
<p>We would love your support.</p>
<p>- Rob Walsh<br/>
Scholastica</p></blockquote>
<p>A little later, I had an exchange of emails with Brian Cody, another member of the Scholastica team, and it became clear that one of their aims was to make it almost effort free for the editors of a journal to do what the editors of Topology did: resign en masse and start again somewhere else with a modified name. Scholastica may well not be the only venture of its kind, and perhaps one can argue about whether it is the best, but what one can say now, with confidence, is that there is a web tool out there that makes the mechanics of starting up a new (but secretly not so new) journal almost trivial. I’d add that the site is in beta at the moment, with an eager team of developers who are ready to add features if there is a demand for them. I urge people to have a look.</p>
<p>It seems to me that if lots of mathematicians feel that enough is enough with Elsevier, and if it is easy to move a journal, then one really can start to think that something might happen sooner rather than later. But there is one snag, which brings me to the title of this post: a journal set up with Scholastica is electronic. [I write that without being 100% certain that it is correct -- I have written to them to check.]</p>
<p><strong>Electronic Journals.</strong></p>
<p>What’s wrong with that, you might ask? I don’t have a good answer, but I do have a bad answer, which is that I, and probably many other people, have an irrational prejudice against them. (There’s also a potentially better answer to do with whether electronic archives are likely to be as durable as paper ones have shown themselves to be, but I’m going to ignore that issue.) I grew up with the paper journal, I remember the thrill of seeing my first paper <em>in print</em>, I enjoyed browsing in libraries, I liked the long traditions that accompanied certain journals, and so on, and when the first electronic journals started, there just didn’t seem to be any point in submitting to them: why sacrifice that lovely paper when you didn’t have to? Somehow, electronic journals weren’t the real thing.</p>
<p>Recently, however, my prejudice has weakened. An obvious reason is that I don’t actually have any of the experiences that I enjoyed when I was starting out in my career: I can’t remember when I last set foot in a maths library, I think people have stopped sending me fifty offprints whenever a paper of mine comes out (which is a relief, as the ones I do have are a silly waste of shelf space, though I can’t bear to throw them away), the moment a paper “comes out” is nowadays the day I put it on the arXiv rather than the almost irrelevant day a couple of years later when it is published. In short, I do pretty well everything on my computer these days, so the idea of an electronic publication has lost the “unreal” feeling it used to have. </p>
<p>However, I do think that kind of prejudice probably still survives to a significant extent, and that it would be good to try to combat it. Here it seems to me that electronic journals have missed a trick. When I see the name “Electronic Journal of Combinatorics”, for example, my instinct is to read it as something like, “Journal of Combinatorics — except it’s only electronic”. In other words, the word “electronic” has entirely negative associations. (At this point I should say that yesterday out of curiosity I browsed the archive of the Electronic Journal of Combinatorics for the first time ever, and discovered to my surprise, and slight shame, that it was full of excellent papers by excellent mathematicians. Moreover, in the sample I looked at every single paper made me think, “Hmm, that looks interesting.” By way of apology, I shall submit to them when I next have a suitable paper. I was also shocked to discover that <a href="http://www.math.upenn.edu/~wilf/">Herb Wilf</a>, who founded the journal, died a few weeks ago. That news had passed me by.)</p>
<p>There must surely be ways that an electronic journal could exploit its electronic character in order to have a <em>positive</em> appeal. Why not have an electronic journal that isn’t run on quite the same lines as a conventional journal? Let me describe an imaginary new journal that would be close enough to conventional journals not to ruffle too many feathers but different enough that at least some people might find it dynamic, forward-looking, and somewhere one would love to be published. </p>
<hr/>
<p><strong>Breakthroughs in Mathematics.</strong></p>
<p>The journal Breakthroughs in Mathematics is set up with one main aim: to accept papers only if they are outstanding. As its name suggests, the editors will be looking for papers that open up new areas, get past seemingly impregnable barriers, or solve long-standing open problems.</p>
<p>If you have written such a paper, why might you wish to submit it to Breakthroughs rather than to, say, Annals, Acta or the Journal of the AMS? Here are a few reasons.</p>
<p>1. Our attitude is that if you publish with us, then we are doing you a favour rather than the other way round. The journal does not have a print version, so there is no need to fill issues with papers that do not meet its exacting standards. If a few months go by without a breakthrough, then that’s fine by us. The average number of papers published so far has been about ten per year, so publication in Breakthroughs is something of an event in the way that publication in a conventional journal, however prestigious, is not.</p>
<p>2. We have a large, youthful and diverse editorial board, consisting mainly of mathematicians who are active on the internet. If that is not your thing, then by all means submit to a conventional journal, but if you are part of the internet generation of mathematicians, then you may feel more at home at Breakthroughs. </p>
<p>3. The submission and refereeing process works as follows. Authors are required to submit not just their papers but also a short account of their work, in which they should explain their result in terms that are comprehensible to mathematicians outside their speciality, paying particular attention to what it is that makes it more than just an ordinary piece of very good mathematics. There is then an initial filtering process by the editorial board, helped by quick opinions solicited from experts in the relevant areas, which is based more on the short account of the paper than on the paper itself and is intended to establish whether the result is sufficiently interesting to sufficiently many editors to be publishable in Breakthroughs. In the rare event that it is, the paper then goes to a technical referee, whose job is not to evaluate the paper, but simply to comment on how it is written and to check that the author has done what he or she claims to have done. </p>
<p>4. The technical referee is not anonymous. Indeed, he or she is positively encouraged to interact with the author, asking for help in understanding difficult parts of a paper, and so on. Authors can even nominate their own technical referee if they wish, though Breakthroughs has the final say.</p>
<p>5. When the paper is published, it appears along with an explanation, written by a suitable member of the editorial board, of why it is deemed important enough to appear in Breakthroughs. This will typically be based on the short account provided by the author, as well as on remarks made by the referees, and possibly on other sources such as online discussion of the result (which will typically by this time be quite well known, though we aim to deal with our papers quickly). It also comes with a comments page, to which anybody can contribute remarks about the paper — such as alternative proofs of certain steps, notification of applications, and the like. The author can respond to these remarks. In these ways, we attempt to give a bit of publicity to the papers we publish, and to provide some context for the general reader.</p>
<p>6. We have made a serious attempt to be precise about what is required of a paper for it to be published in Breakthroughs. For details, see our page, “What is a breakthrough?” Of course, it is impossible to give exact necessary and sufficient conditions, but the fact that we at least try makes it clearer what it means to have a Breakthroughs in Mathematics paper on your CV than it would if we simply said that we had very high standards. </p>
<hr/>
<p><strong>But still: what now?</strong></p>
<p>A journal like that is not going to answer the need for new journals to replace the overpriced conventional ones, but it could at least make electronic journals sexy in a way that they aren’t at the moment. It would also have the great virtue of not requiring much work of the editors. (It would require quite a lot of work per accepted paper, but the number of accepted papers would be very small.) </p>
<p>I’m aware though that I haven’t really faced up to the question of whether the editors of an Elsevier journal should be gently encouraged to consider switching publishers. As a matter of fact, I heard from an Elsevier editor recently. Let me call him/her X. X had approached a potential referee and had just received a refusal in which my earlier blog post was mentioned. X was somewhat critical of encouraging people not to referee for Elsevier journals, but said that he/she had some sympathy with the reasons. My guess is that on any journal there will be a small handful of very active editors, often just the official main editors, who in a sense “are” the journal and whose lives could be a little disrupted, and a much wider set of editors who wouldn’t at all mind moving if there were good reasons to do so. </p>
<p>How much of an imposition this would be would depend on a number of factors. One factor I find hard to judge because of my lack of experience running journals is probably the most important: the extent to which the smooth running of a journal depends on a good relationship between the managing editors and certain representatives, who may have genuine mathematical sympathies and expertise, of the publishers. Giving up a relationship like that would be a genuine sacrifice unless there was a realistic prospect of a new and similar relationship to take its place. Asking a print journal to go electronic would also be asking quite a lot, though, for reasons I indicated above, perhaps not too much.</p>
<p><strong>Combinatorics journals.</strong></p>
<p>In the course of writing the last couple of paragraphs I found myself thinking about the situation in combinatorics, and I have come to realize that I am on the editorial boards of at least two Springer journals: the Annals of Combinatorics, which is not really my kind of combinatorics and has involved zero work, and Combinatorica, which is one of my favourite maths journals. Since the general view seems to be that Springer has become a problem company as well, I should perhaps consider my position. I find it quite hard to get comprehensible information about the prices of these journals, but I think that if I could sell the back numbers that I’ve received from them at their official cost price, I could go on a round-the-world cruise and still have plenty of change. </p>
<p>What are the options if you want to publish a good result in combinatorics? (Here, I’m mainly talking about Hungarian-style combinatorics rather than enumerative or algebraic combinatorics.) If the result is interesting enough, you could of course publish in a general-interest journal, but let’s suppose you want it to appear in a specialist journal. The list of journals that would naturally spring to my mind is this. I’ll also give my associations with each one, which should not be taken seriously because I haven’t made any effort to test whether they are correct. I’m sure other people have different pecking orders.</p>
<p>Combinatorica: used to be regarded as the number one journal in combinatorics, and very possibly still is; quite slow and with a big backlog (that was true once but may be out of date). [Springer]</p>
<p>Discrete Mathematics: good solid journal; not of the absolute top rank. [Elsevier]</p>
<p><strong>Edit. The assessments of the next two journals were based on ignorance and were wrong: I am told by those in the know that JCT is roughly on a par with Combinatorica, or perhaps just the tiniest bit behind. So they are very good.</strong></p>
<p>Journal of Combinatorial Theory A: good solid journal; not of the absolute top rank. [Elsevier]</p>
<p>Journal of Combinatorial Theory B: good solid journal; not of the absolute top rank. [Elsevier]</p>
<p>European Journal of Combinatorics: OK, but not as good as I thought it was when I submitted a paper I very much liked to it twenty years ago. [Elsevier]</p>
<p>Random Structures and Algorithms: very good; lots of interesting papers. [Wiley]</p>
<p>Combinatorics, Probability and Computing: a personal favourite; set up recently(ish) by Béla Bollobás and maintains a high standard. [Cambridge University Press]</p>
<p>Electronic Journal of Combinatorics: now that I’ve actually looked into it … good.</p>
<p>I’ve probably missed some obvious further possibilities there, but the fact remains that that is my mental list of good combinatorial journals, and if I want to avoid the big publishing houses then my list goes down from eight to two. It’s not as bad as it sounds though. The only one of those journals that I’ve actually submitted to is Combinatorics, Probability and Computing, and the only one of the first six that I’d feel sad about boycotting is Combinatorica, though I also feel quite positive about Random Structures and Algorithms.   </p>
<p>So if anything is to be done about outrageously high journal prices in combinatorics, it looks as though new journals, or migration of existing ones, will be needed. (Incidentally, I’m writing all this on the assumption that we stick with something close to the current system of journals providing varying stamps of quality. Obviously other systems are possible, but persuading large numbers of mathematicians to move to those systems would be much more of a challenge.) </p>
<p><strong>Are there two kinds of mathematician?</strong></p>
<p>I was quite surprised that the reaction to the idea of a boycott was as positive as it was: I had expected a more divided response. I still wonder whether the true response <em>is</em> more divided. Could it be that the kind of mathematician who participates fully in online discussions on blogs, Mathoverflow etc. is naturally enthusiastic, whereas a more traditionally-minded mathematician just wants to be left alone to continue with a way of doing things that seems perfectly satisfactory? If so, then the apparently strong support could be misleading. I think it is this thought that makes me want to tread carefully after reading Michael Harris’s suggestion. But treading carefully doesn’t necessarily mean not treading at all. I’d be very interested to know what other people think about this: is there some moment that needs to be seized, or should we simply sit back and watch the number of signatures grow?</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/gowers.wordpress.com/3940/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/gowers.wordpress.com/3940/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/gowers.wordpress.com/3940/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=gowers.wordpress.com&amp;blog=1659011&amp;post=3940&amp;subd=gowers&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-10T22:15:28Z</updated>
    <published>2012-01-29T15:41:16Z</published>
    <category scheme="http://gowers.wordpress.com" term="Mathematics on the internet"/>
    <author>
      <name>gowers</name>
      <uri>http://gowers.wordpress.com</uri>
    </author>
    <source>
      <id>http://gowers.wordpress.com/feed/atom/</id>
      <link href="http://gowers.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://gowers.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://gowers.wordpress.com/osd.xml" rel="search" title="Gowers's Weblog" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://gowers.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Mathematics related discussions</subtitle>
      <title xml:lang="en">Gowers's Weblog</title>
      <updated>2012-02-14T13:41:23Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.quantumdiaries.org/?p=20194</id>
    <link href="http://www.quantumdiaries.org/2012/02/10/physicists-eat/" rel="alternate" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/10/physicists-eat/#comments" rel="replies" type="text/html"/>
    <link href="http://www.quantumdiaries.org/2012/02/10/physicists-eat/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Physicists Eat!</title>
    <summary xml:lang="en">CERN is a pretty interesting place to work, probably more so than other physics laboratories around the world, due to its highly international nature. Here is a nice graphic of the nationalities of all CERN users: In no place is the international nature of the laboratory more evident than in the main cafeteria on site. [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>CERN is a pretty interesting place to work, probably more so than other physics laboratories around the world, due to its highly international nature. Here is a nice graphic of the nationalities of all CERN users:</p>
<p><a href="http://www.quantumdiaries.org/wp-content/uploads/2012/02/1106170_01-A4-at-144-dpi.jpg"><img alt="" class="aligncenter size-large wp-image-20199" height="386" src="http://www.quantumdiaries.org/wp-content/uploads/2012/02/1106170_01-A4-at-144-dpi-1024x772.jpg" title="CERN Users" width="512"/></a><br/>
In no place is the international nature of the laboratory more evident than in the main cafeteria on site. While most of the conversations are in English, you can usually hear bits of conversation in other languages. I personally like to play the ‘guess what language that table is speaking’ game, though it’s a little frustrating as I can’t just go over and ask to check if I have it right or not.</p>
<p>Whatever the language the conversation is in, you can be sure that the most discussed topic is physics. In fact, a lot of important discussions occur over a drink or a bite to eat. It’s just easier to discuss issues in an informal setting with less people than a more formal video conference.</p>
<p>Probably due to this fact, I think there is a slight fascination with the cafeteria from the media. Every couple of weeks there is usually a film crew in there, filming people eating and talking for whatever feature they are producing.</p>
<p>USLHC has decided to join in on the cafeteria action, having intern Amy Dusto set up <a href="http://www.uslhc.us/LHC_Lunch">LHC Lunch</a>, a series of articles and videos sourced from lunch time interviews with members of the LHC experiments working for US institutes. </p>
<p>Why do I bring all of this up? Well, I was one of the physicists whom she interviewed, and my article and video has just been published. Check it out <a href="http://www.uslhc.us/LHC_Lunch/Anna_Phan">here</a>. Enjoy!</p></div>
    </content>
    <updated>2012-02-10T10:47:46Z</updated>
    <published>2012-02-10T10:47:46Z</published>
    <category scheme="http://www.quantumdiaries.org" term="Latest Posts"/>
    <author>
      <name>Anna Phan</name>
    </author>
    <source>
      <id>http://www.quantumdiaries.org/feed/atom/</id>
      <link href="http://www.quantumdiaries.org" rel="alternate" type="text/html"/>
      <link href="http://www.quantumdiaries.org/feed/atom/" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">Thoughts on work and life from particle physicists from around the world.</subtitle>
      <title xml:lang="en">Quantum Diaries</title>
      <updated>2012-02-14T16:23:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://johncarlosbaez.wordpress.com/?p=7885</id>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/08/the-cost-of-knowledge/" rel="alternate" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/08/the-cost-of-knowledge/#comments" rel="replies" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/08/the-cost-of-knowledge/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">The Cost of Knowledge</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">As of this moment, 4760 scholars have joined a boycott of the publishing company Elsevier. Of these, only 20% are mathematicians. But since the boycott was started by a mathematician, 34 of us wrote and signed an official statement explaining the boycott: • The Cost of Knowledge. It’s also below. Please check it out and [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7885&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>As of this moment, 4760 scholars have joined <a href="http://thecostofknowledge.com/">a boycott of the publishing company Elsevier</a>.  Of these, only 20% are mathematicians.  But since the boycott was started by a mathematician, 34 of us wrote and signed an official statement explaining the boycott:</p>
<p>• <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf">The Cost of Knowledge</a>.  </p>
<p>It’s also below.  Please check it out and join the boycott!  I’m sure more than 34 mathematicians would be happy to sign, but we wanted to get the statement out soon.  </p>
<h3> THE COST OF KNOWLEDGE </h3>
<p>This is an attempt to describe some of the background to the current boycott of Elsevier by many mathematicians (and other academics) at <a href="http://thecostofknowledge.com">http://thecostofknowledge.com</a>, and to present some of the issues that confront the boycott movement.  Although the movement is anything but monolithic, we believe that the points we make<br/>
here will resonate with many of the signatories to the boycott.</p>
<h4> The role of journals (1): dissemination of research.</h4>
<p>  The role of journals in professional mathematics has been under discussion for some time now.</p>
<p>Traditionally, while journals served several purposes, their primary purpose was the dissemination of research papers.  The journal publishers were charging for the cost of typesetting (not a trivial matter in general before the advent of electronic typesetting, and particularly non-trivial for mathematics), the cost of physically publishing copies of the journals, and the cost of distributing the journals to subscribers (primarily academic libraries).</p>
<p>The editorial board of a journal is a group of professional<br/>
mathematicians. Their editorial work is undertaken as part of their scholarly duties, and so is paid for by their employer, typically a university. Thus, from the publisher’s viewpoint the editors are volunteers. (The editor in chief of a journal sometimes receives modest compensation from the publisher.) When a paper is submitted to the journal, by an author who is again typically a university-employed mathematician, the editors select the referee or referees for the paper, evaluate the referees’ reports, decide whether or not to accept the submission, and organize the submitted papers into volumes.  These are passed on to the publisher, who then undertakes the job of actually publishing them. The publisher supplies some administrative assistance in handling the papers, as well as some copy-editing assistance, which is often quite minor but sometimes more substantial. The referees are again volunteers from the point of view of the publisher: as with editing, refereeing is regarded as part of the service component of a mathematician’s academic work. Authors are not paid by the publishers for their published papers, although they are usually asked to sign over the copyright to the publisher.</p>
<p>This system made sense when the publishing and dissemination of papers was a difficult and expensive undertaking.  Publishers supplied a valuable service in this regard, for which they were paid by subscribers to the journals, which were mainly academic libraries. The academic institutions whose libraries subscribe to mathematics journals are broadly speaking the same institutions that employ the mathematicians who are writing for, refereeing for, and editing the journals. Therefore, the cost of the whole process of producing research papers is borne by these institutions (and the outside entities that partially fund them, such as the National Science Foundation in the United States): they pay for their academic mathematician employees to do research and to organize the publications of the results of their research in journals; and then (through their libraries) they pay the publishers to disseminate these results among all the world’s mathematicians. Since these institutions employ research faculty in order to foster research, it certainly used to make sense for them to pay for the dissemination of this research as well. After all, the sharing of scientific ideas and research results is unquestionably a key component for making progress in science.</p>
<p>Now, however, the world has changed in significant ways.<br/>
Authors typeset their own papers, using electronic typesetting. Publishing and distribution costs are not<br/>
as great as they once were.  And most importantly,<br/>
dissemination of scientific ideas no longer takes place via the physical distribution of journal volumes. Rather, it takes place mainly electronically. While this means of dissemination is not free, it is much less expensive, and much of it happens quite independently of mathematical journals.</p>
<p>In conclusion, the cost of journal publishing has gone down<br/>
because the cost of typesetting has been shifted from<br/>
publishers to authors and the cost of publishing and distribution is significantly lower than it used to be.<br/>
By contrast, the amount of money being spent by university libraries on journals seems to be growing with no end in sight.  Why do mathematicians contribute all this volunteer labor, and their employers pay all this money, for a service whose value no longer justifies its cost?</p>
<h4> The role of journals (2): peer review and professional<br/>
evaluation</h4>
<p>There are some important reasons that mathematicians haven’t just abandoned journal publishing. In particular, peer review plays an essential role in ensuring the correctness and readability of mathematical papers, and publishing papers in research journals is the main way of achieving professional recognition. Furthermore, not all journals count equally from this point of view: journals are (loosely) ranked, so that publications in top journals will often count more than publications in lower ranked ones. Professional mathematicians typically have a good sense of the relative prestige of the journals that publish papers in their area, and they will usually submit a paper to the highest ranked journal that they judge is likely to accept and publish it.</p>
<p>Because of this evaluative aspect of traditional journal publishing, the problem of switching to a different model<br/>
is much more difficult than it might appear at first.  For<br/>
example, it is not easy just to begin a new journal (even an electronic one, which avoids the difficulties of printing and distribution), since mathematicians may not want to publish in it, preferring to submit to journals with known reputations. Secondly, although the reputation of various journals has been created through the efforts of the authors, referees, and editors who have worked (at no cost to the publishers) on it over the years, in many cases the <i>name</i> of the journal is owned by the publisher, making it difficult for the mathematical community to separate this valuable object that they have constructed from its present publisher.</p>
<h4> The role of Elsevier</h4>
<p>Elsevier, Springer, and a number of other commercial publishers (many of them large companies but less significant for their mathematics publishing, e.g., Wiley) all exploit our volunteer labor to extract very large profits from the academic community. They supply some value in the process, but nothing like enough to justify their prices.</p>
<p>Among these publishers, Elsevier may not be the most expensive, but in the light of other factors, such as scandals, lawsuits, lobbying, etc. (discussed further below), we consider them a good initial focus for our discontent. A boycott should be substantial enough to be meaningful, but not so broad that the choice of targets becomes controversial or the boycott becomes an unmanageable burden.  Refusing to submit papers to all overpriced publishers is a reasonable further step, which some of us have taken, but the focus of this boycott is on Elsevier because of the widespread feeling among mathematicians that they are the worst offender.</p>
<p>Let us begin with the issue of journal costs. Unfortunately, it is difficult to make cost comparisons: journals differ greatly in quality, in number of pages per volume, and even in amount of text per page.  As measured by list prices, Elsevier mathematics journals are amongst the most expensive. For instance, in the <a href="http://www.ams.org/membership/mem-journal-survey">AMS mathematics journal price survey</a>, seven of the ten most expensive journals (by 2007 volume list price) were published by Elsevier.   (All prices are as of 2007 because both prices and page counts are easily available online.)  However, that is primarily because Elsevier publishes the largest volumes. Price per page is a more meaningful measure that can be easily computed.  By this standard, Elsevier is certainly not the worst publisher, but its prices do on the face of it look very high. The <i>Annals of Mathematics</i>, published by Princeton University Press, is one of the absolute top mathematics journals and quite affordably priced: $0.13/page as of 2007.  By contrast, ten Elsevier journals (not including one that has since ceased publication) cost $1.30/page or more; they and three others cost more per page than <i>any</i> journal published by a university press or learned society. For comparison, three other top journals competing with the <i>Annals</i> are <i>Acta Mathematica</i>, published by the Institut Mittag Leffler for $0.65/page, <i>Journal of the American Mathematical Society</i>, published by the American Mathematical Society for $0.24/page, and <i>Inventiones Mathematicae</i>, published by Springer for $1.21/page.  Note that none of Elsevier’s mathematics journals is generally considered comparable in quality to these journals.</p>
<p>However, there is an additional aspect which makes it hard to compute the true cost of mathematics journals. This is the widespread practice among large commercial publishers of “bundling” journals, which allows libraries to subscribe to large numbers of journals in order to avoid paying the exorbitant list prices for the ones they need. Although this means that the average price libraries pay per journal is less than the list prices might suggest, what really matters is the average price that they pay per journal (or page of journal) <i>that they actually want</i>, which is hard to assess, but clearly higher. We would very much like to be able to offer more concrete data regarding the actual costs to libraries of Elsevier journals compared with those of Springer or other publishers. Unfortunately, this is difficult, because publishers often make it a contractual requirement that their institutional customers should not disclose the financial details of their contracts. For example, Elsevier sued Washington State University to try to prevent release of this information. One common consequence of these arrangements, though, is that in many cases a library cannot actually save any money by cancelling a few Elsevier journals: at best the money can sometimes be diverted to pay for other Elsevier subscriptions.</p>
<p>One reason for focusing on Elsevier rather than, say, Springer is that Springer has had a rich and productive history with the mathematical community. As well as journals, it has published important series of textbooks, monographs, and lecture notes; one could perhaps regard the prices of its journals as a means of subsidizing these other, less profitable, types of publications. Although all these types of publications have become less important with the advent of the internet and the resulting electronic distribution of texts, the long and continuing presence of Springer in the mathematical world has resulted in a store of goodwill being built up in the mathematical community towards them.  This store is being rapidly depleted, but has not yet reached zero.  See for instance the <a href="http://www-fourier.ujf-grenoble.fr/petitions/index.php?petition=3">recent petition to Springer</a> by a number of French mathematicians and departments.</p>
<p>Elsevier does not have a comparable tradition of involvement in mathematics publishing.  Many of the mathematics journals that it publishes have been acquired comparatively recently as it has bought up other, smaller publishers.   Furthermore, in recent years it has been involved in various scandals regarding the scientific content, or lack thereof, of its journals. One in particular involved the journal <i>Chaos, Solitons &amp; Fractals</i>,  which, at the time the scandal broke in 2008–2009, was one of the highest impact factor  mathematics journals that Elsevier published.   (Elsevier currently reports the five-year impact factor of this journal at 1.729.  For sake of comparison, <i>Advances in Mathematics</i>, also published by Elsevier, is reported as having a five-year impact factor of 1.575.)  It turned out that the high impact factor was at least partly the result of the journal publishing many papers full of mutual citations.  (See  <a href="http://www.siam.org/news/news.php?id=1663">Arnold</a> for more information on this and other troubling examples that show the limitations of bibliometric measures of scholarly quality.) Furthermore, <i>Chaos, Solitons &amp; Fractals</i> published many papers that, in our professional judgement, have little or no scientific merit and should not have been published in any reputable journal.</p>
<p>In another notorious episode, this time in medicine, for at least five years Elsevier “published a series of sponsored article compilation publications, on behalf of pharmaceutical clients, that were made to look like journals and lacked the proper disclosures”, as noted by <a href="http://www.elsevier.&lt;br /&gt; com/wps/find/authored_newsitem.cws_home/companynews05_01203&#x2033;&gt;the CEO of Elsevier&#x2019;s Health Sciences Division&lt;/a&gt;.&lt;/p&gt; &lt;p&gt;Recently, Elsevier has lobbied for the Research Works Act, a proposed U.S. law that would undo the National Institutes of Health&#x2019;s public access policy, which guarantees public access to published research papers based on NIH funding within twelve months of publication (to give publishers time to make a profit). Although most lobbying occurs behind closed doors, Elsevier&#x2019;s vocal support of this act shows their opposition to a popular and effective open access policy.&lt;/p&gt; &lt;p&gt;These scandals, taken together with the bundling practices, exorbitant prices, and lobbying activities, suggest a publisher motivated purely by profit, with no genuine interest in or commitment to mathematical knowledge and the community of academic mathematicians that generates it.  Of course, many Elsevier employees are reasonable people doing their best to contribute to scholarly publishing, and we bear them no ill will.  However, the organization as a whole does not seem to have the interests of the mathematical community at heart.&lt;/p&gt; &lt;h4&gt; The boycott &lt;/h4&gt; &lt;p&gt;Not surprisingly, many mathematicians have in recent years lost patience with being involved in a system in which commercial publishers make profits based on the free labor of mathematicians and subscription fees from their institutions&#x2019; libraries, for a service that has become largely unnecessary.  (See &lt;a href="><br/>
com/wps/find/authored_newsitem.cws_home/companynews05_01203″&gt;the CEO of Elsevier’s Health Sciences Division</a>.</p>
<p>Recently, Elsevier has lobbied for the Research Works Act, a proposed U.S. law that would undo the National Institutes of Health’s public access policy, which guarantees public access to published research papers based on NIH funding within twelve months of publication (to give publishers time to make a profit). Although most lobbying occurs behind closed doors, Elsevier’s vocal support of this act shows their opposition to a popular and effective open access policy.</p>
<p>These scandals, taken together with the bundling practices, exorbitant prices, and lobbying activities, suggest a publisher motivated purely by profit, with no genuine interest in or commitment to mathematical knowledge and the community of academic mathematicians that generates it.  Of course, many Elsevier employees are reasonable people doing their best to contribute to scholarly publishing, and we bear them no ill will.  However, the organization as a whole does not seem to have the interests of the mathematical community at heart.</p>
<h4> The boycott </h4>
<p>Not surprisingly, many mathematicians have in recent years lost patience with being involved in a system in which commercial publishers make profits based on the free labor of mathematicians and subscription fees from their institutions’ libraries, for a service that has become largely unnecessary.  (See <a href="http://www.scottaaronson.com/writings/journal.pdf">Scott Aaronson’s scathing but all-too-true satirical description</a> of the publishers’ business model.)  Among all the commercial publishers, the behavior of Elsevier seemed to many to be the most egregious, and a number of mathematicians had made personal commitments to avoid any involvement with Elsevier journals.  (Some journals were also successfully moved from Elsevier to other publishers; e.g., <i>Annales Scientifiques de l’école Normale Supérieure</i> which until recent years was published by Elsevier, is now published by the Société Mathématique de France.)</p>
<p>One of us (Timothy Gowers) decided that it might be useful to<br/>
publicize his own personal boycott of Elsevier, thus encouraging others to do the same.   This led to the current boycott movement at <a href="http://thecostofknowledge.com">http://thecostofknowledge.com</a>, the success of which has far exceeded his initial expectations.</p>
<p>Each participant in the boycott can choose which activities they intend to avoid: submitting to Elsevier journals, refereeing for them, and serving on editorial boards.  Of course, submitting papers and editing journals are purely voluntary activities, but refereeing is a more subtle issue.  The entire peer review system depends on the availability of suitable referees, and its success is one of the great traditions of science: refereeing is felt to be both a burden and an honor, and practically every member of the community willingly takes part in it. However, while we respect and value this tradition, many of us do not wish to see our labor used to support Elsevier’s business model.</p>
<h4> What next?</h4>
<p>As suggested at the very beginning, different participants in the boycott have different goals, both in the short and long term.  Some people would like to see the journal system eliminated completely and replaced by something else more adapted to the internet and the possibilities of electronic distribution.  Others see journals as continuing to play a role, but with commercial publishing being replaced by open access models. Still others imagine a more modest change, in which commercial publishers are replaced by non-profit entities such as professional societies (e.g., the American Mathematical Society, the London Mathematical Society, and the Société Mathématique de France, all of which already publish a number of journals) or university presses; in this way the value generated by the work of authors, referees, and editors would be returned to the academic and scientific community. These goals need not be mutually exclusive: the world of mathematics journals, like the world of mathematics itself, is large, and open access journals can coexist with traditional journals, as well as with other, more novel means of dissemination and evaluation.</p>
<p>What all the signatories do agree on is that Elsevier is an exemplar of everything that is wrong with the current system of commercial publication of mathematics journals, and we will no longer acquiesce to Elsevier’s harvesting of the value of our and our colleagues’ work.</p>
<p>What future do we envisage for all the papers that would<br/>
otherwise be published in Elsevier journals? There are many<br/>
other journals being published; perhaps they can pick up at<br/>
least some of the slack. Many successful new journals have been founded in recent years, too, including several that are electronic (thus completely eliminating printing and physical distribution costs), and no doubt more will follow. Finally, we hope that the mathematical community will be able to reclaim for itself some of the value that it has given to Elsevier’s journals by moving some of these journals (in name, if possible, and otherwise in spirit)  from Elsevier to other publishers.  One notable example  is the August 10, 2006 resignation of the entire editorial board of the Elsevier journal <i>Topology</i> and their founding of the <i>Journal of Topology</i>, owned by the London Mathematical Society.  </p>
<p>None of these changes will be easy; editing a journal is hard work, and founding a new journal, or moving and relaunching an existing journal, is even harder. But the alternative is to continue with the status quo, in which Elsevier harvests ever larger profits from the work of us and our colleagues, and this is both unsustainable and unacceptable.</p>
<p>Signed by:</p>
<p>Scott Aaronson <br/>
Massachusetts Institute of Technology</p>
<p>Douglas N. Arnold<br/>
University of Minnesota</p>
<p>Artur Avila<br/>
IMPA and Institut de Mathématiques de Jussieu</p>
<p>John Baez<br/>
University of California, Riverside</p>
<p>Folkmar Bornemann<br/>
Technische Universität München</p>
<p>Danny Calegari<br/>
Caltech/Cambridge University</p>
<p>Henry Cohn<br/>
Microsoft Research New England</p>
<p>Jordan Ellenberg<br/>
University of Wisconsin, Madison</p>
<p>Matthew Emerton<br/>
University of Chicago</p>
<p>Marie Farge<br/>
École Normale Supérieure Paris</p>
<p>David Gabai<br/>
Princeton University</p>
<p>Timothy Gowers<br/>
Cambridge University</p>
<p>Ben Green<br/>
Cambridge University</p>
<p>Martin Grötschel<br/>
Technische Universität Berlin</p>
<p>Michael Harris<br/>
Université Paris-Diderot Paris 7</p>
<p>Frédéric Hélein<br/>
Institut de Mathéatiques de Jussieu</p>
<p>Rob Kirby<br/>
University of California, Berkeley</p>
<p>Vincent Lafforgue<br/>
CNRS and Université d’Orléans</p>
<p>Gregory F. Lawler<br/>
University of Chicago</p>
<p>Randall J. LeVeque<br/>
University of Washington</p>
<p>László Lovász<br/>
Eötvös Lor´nd University</p>
<p>Peter J. Olver<br/>
University of Minnesota</p>
<p>Olof Sisask<br/>
Queen Mary, University of London</p>
<p>Terence Tao<br/>
University of California, Los Angeles</p>
<p>Richard Taylor<br/>
Institute for Advanced Study</p>
<p>Bernard Teissier<br/>
Institut de Mathématiques de Jussieu</p>
<p>Burt Totaro<br/>
Cambridge University</p>
<p>Lloyd N. Trefethen<br/>
Oxford University</p>
<p>Takashi Tsuboi<br/>
University of Tokyo</p>
<p>Marie-France Vigneras<br/>
Institut de Mathématiques de Jussieu </p>
<p>Wendelin Werner<br/>
Université Paris-Sud</p>
<p>Amie Wilkinson<br/>
University of Chicago</p>
<p>Günter M. Ziegler<br/>
Freie Universität Berlin</p>
<h4> Appendix: recommendations for mathematicians.</h4>
<p>All mathematicians must decide for themselves whether, or to what extent, they wish to participate in the boycott.  Senior<br/>
mathematicians who have signed the boycott bear some<br/>
responsibility towards junior colleagues who are forgoing the<br/>
option of publishing in Elsevier journals, and should do their<br/>
best to help minimize any negative career consequences.</p>
<p>Whether or not you decide to join the boycott, there are some<br/>
simple actions that everyone can take, which seem to us to be<br/>
uncontroversial:</p>
<p>1)  Make sure that the final versions of all your papers, particularly new ones, are freely available online—  ideally both on the arXiv.  (Elsevier’ electronic preprint policy is    unacceptable, because it explicitly does not allow authors to update their papers on the arXiv to incorporate changes made during peer review). When signing copyright transfer forms, we recommend amending them (if necessary) to reserve the right to make the author’s final version of the text available free online from servers such as the arXiv, and on your home page.</p>
<p>2) If you are submitting a paper and there is a choice between an expensive journal and a cheap (or free) journal of the same standard, then always submit to the cheap one.</p>
<h4> Note </h4>
<p>The <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf">PDF version</a> of this statement has many useful references not included here.</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/johncarlosbaez.wordpress.com/7885/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/johncarlosbaez.wordpress.com/7885/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/johncarlosbaez.wordpress.com/7885/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7885&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-10T09:02:08Z</updated>
    <published>2012-02-08T23:57:56Z</published>
    <category scheme="http://johncarlosbaez.wordpress.com" term="mathematics"/>
    <category scheme="http://johncarlosbaez.wordpress.com" term="publishing"/>
    <author>
      <name>John Baez</name>
      <uri>http://math.ucr.edu/home/baez/</uri>
    </author>
    <source>
      <id>http://johncarlosbaez.wordpress.com/feed/atom/</id>
      <link href="http://johncarlosbaez.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://johncarlosbaez.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/osd.xml" rel="search" title="Azimuth" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <title xml:lang="en">Azimuth</title>
      <updated>2012-02-14T12:46:26Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-9163501679982013672.post-1760436714087238535</id>
    <link href="http://cosmic-horizons.blogspot.com/feeds/1760436714087238535/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://cosmic-horizons.blogspot.com/2012/02/mapping-growth-and-gravity-with-robust.html#comment-form" rel="replies" title="0 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/9163501679982013672/posts/default/1760436714087238535" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/9163501679982013672/posts/default/1760436714087238535" rel="self" type="application/atom+xml"/>
    <link href="http://cosmic-horizons.blogspot.com/2012/02/mapping-growth-and-gravity-with-robust.html" rel="alternate" title="Mapping Growth and Gravity with Robust Redshift Space Distortions" type="text/html"/>
    <title>Mapping Growth and Gravity with Robust Redshift Space Distortions</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">A quick post this evening, as I have been at a workshop for the <a href="http://arxiv.org/abs/1112.3367">SAMI</a> instrument, and am off to Santa Barbara for the <a href="http://www.itp.ucsb.edu/activities/dbdetails?acro=dwarfgal12">First Galaxies and Faint Dwarfs: First Galaxies and Faint Dwarfs </a>conference next week, but a couple of things to post. The first is a paper by my ex-phd student, Juliana Kwan, who is now a postdoc in the US at the <a href="http://www.anl.gov/">Argonne National Laboratory.</a><br/><br/>The paper is quite complex, and focuses on <a href="http://relativity.livingreviews.org/open?pubNo=lrr-2004-8&amp;amp;page=articlesu20.html">redshift space distortions.</a> This can be difficult to understand, but here goes. We've mentioned a couple of times that matter in the Universe is arranged on a cosmic web, with clusters, clumps, filaments and voids. In fact, it looks something like this:<br/><div class="separator" style="clear: both; text-align: center;"><a href="http://www.lsw.uni-heidelberg.de/users/mcamenzi/images/Cosmic_web.jpg" style="margin-left: 1em; margin-right: 1em;"><img border="0" height="230" src="http://www.lsw.uni-heidelberg.de/users/mcamenzi/images/Cosmic_web.jpg" width="320"/></a></div>Our Milky Way galaxy is just a little dot in there. But the detail of the way the mass is distributed is a probe of our Universe, as its present structure carries the imprint of the forces that created it, including the make up of the Universe, the cosmic evolution, and even the nature of gravity itself.<br/><br/>What do we see when we look out into the Universe? Well, we can measure the position to a galaxy on the sky very accurately, but distance is not. But we can easily measure the redshift, or the amount features in the spectrum are moving to longer wavelength, and use our cosmology to turn this into a distance using the famous <a href="http://en.wikipedia.org/wiki/Hubble%27s_law">Hubble law</a>.<br/><br/>However, there is a problem. The redshift we see is a mixture of two parts, one due to the cosmic expansion (the Hubble law bit) and one due to the `<a href="http://en.wikipedia.org/wiki/Peculiar_motion">peculiar velocity</a>, or how much the galaxy is whizzing about. By comparing to the Microwave Background, we know that our Milky Way is moving with a speed of <a href="http://hypertextbook.com/facts/1999/PatriciaKong.shtml">about 500 km/s.</a><br/><br/>As we measure redshifts, not distances, these peculiar velocities distort the distances we calculate via the Hubble law. So, this happens<br/><div class="separator" style="clear: both; text-align: center;"><a href="http://ej.iop.org/images/1367-2630/10/12/125015/Full/nj289273fig4.jpg" style="margin-left: 1em; margin-right: 1em;"><img border="0" height="160" src="http://ej.iop.org/images/1367-2630/10/12/125015/Full/nj289273fig4.jpg" width="320"/></a></div>The blue on the right is the actual positions of galaxies in the cosmic web (in a simulation of the Universe). The green on the left show the effects of peculiar velocity, and things are stretched and squished from the space position.<br/><br/>In fact, clusters of galaxies, where velocities are typically several thousands of km/s, get stretched out into what are known as <a href="http://en.wikipedia.org/wiki/Fingers_of_god">Fingers of God</a> - although what they have to do with the Higgs boson, I don't know (and no, that's not a serious statement). Here's a real set of observations;<br/><div class="separator" style="clear: both; text-align: center;"><a href="http://bustard.phys.nd.edu/Phys171/lectures/cfa2.n30.gif" style="margin-left: 1em; margin-right: 1em;"><img border="0" height="247" src="http://bustard.phys.nd.edu/Phys171/lectures/cfa2.n30.gif" width="320"/></a></div>Now, the details of these Redshift Space Distortions allow us learn even more information about the Universe, but it is very hard to untangle. What Juliana's paper does is to look at the possible ways that can be used to extract science, and shows what needs to be done if you want to get "robust" measures. I'll write more on on what robust means later, but for now, I'll finish by saying "Well done Juliana!"<br/><br/><span style="font-size: large;"><a href="http://arxiv.org/abs/1105.1194">Mapping Growth and Gravity with Robust Redshift Space Distortions</a></span><br/> <br/> <a href="http://arxiv.org/find/astro-ph/1/au:+Kwan_J/0/1/0/all/0/1">Juliana Kwan</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Lewis_G/0/1/0/all/0/1">Geraint F. Lewis</a>, <a href="http://arxiv.org/find/astro-ph/1/au:+Linder_E/0/1/0/all/0/1">Eric V. Linder</a><br/><div class="dateline">(Submitted on 6 May 2011 (<a href="http://arxiv.org/abs/1105.1194v1">v1</a>), last revised 3 Feb 2012 (this version, v2))</div><blockquote class="abstract"> Redshift space distortions caused by galaxy peculiar velocities provide awindow onto the growth rate of large scale structure and a method for testinggeneral relativity. We investigate through a comparison of N-body simulationsto various extensions of perturbation theory beyond the linear regime, therobustness of cosmological parameter extraction, including the gravitationalgrowth index, \gamma. We find that the Kaiser formula and some perturbationtheory approaches bias the growth rate by 1-sigma or more relative to thefiducial at scales as large as k &gt; 0.07 h/Mpc. This bias propagates toestimates of the gravitational growth index as well as \Omega_m and theequation of state parameter and presents a significant challenge to modellingredshift space distortions. We also determine an accurate fitting function fora combination of line of sight damping and higher order angular dependence thatallows robust modelling of the redshift space power spectrum to substantiallyhigher k.</blockquote><br/><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/9163501679982013672-1760436714087238535?l=cosmic-horizons.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-10T07:53:15Z</updated>
    <published>2012-02-10T07:53:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="Big Bang"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="Dark Matter"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="Cosmology"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="Astro-ph"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="Dark Energy"/><geo:lat xmlns:geo="http://www.w3.org/2003/01/geo/wgs84_pos#">-33.873651</geo:lat><geo:long xmlns:geo="http://www.w3.org/2003/01/geo/wgs84_pos#">151.206890</geo:long>
    <author>
      <name>Cusp</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/12515740423567038683</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-9163501679982013672</id>
      <category term="Quasars"/>
      <category term="The Conversation"/>
      <category term="Dark Matter"/>
      <category term="Intermission"/>
      <category term="Big Bang"/>
      <category term="Observing"/>
      <category term="Cosmology"/>
      <category term="Conversation"/>
      <category term="Gyroscope"/>
      <category term="GPGPUs"/>
      <category term="Physics"/>
      <category term="History"/>
      <category term="Astro-ph"/>
      <category term="Numerical Methods"/>
      <category term="2-d Universe"/>
      <category term="Movies"/>
      <category term="Dark Energy"/>
      <category term="Zombies"/>
      <category term="papers"/>
      <category term="PAndAS"/>
      <category term="Media"/>
      <author>
        <name>Cusp</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/12515740423567038683</uri>
      </author>
      <link href="http://cosmic-horizons.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/9163501679982013672/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://cosmic-horizons.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/9163501679982013672/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>My personal take on what's going on within our Event Horizon. Mostly astronomical, often cosmological, usually quite grumpy.</subtitle>
      <title>Cosmic Horizons</title>
      <updated>2012-02-10T07:53:15Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/catdynamics/2012/02/ominous_signs_for_nasa.php</id>
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/L1lmVakuHW4/ominous_signs_for_nasa.php" rel="alternate" type="text/html"/>
    <title>Ominous signs for NASA</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
There are several signs o'doom for NASA bubbling up out there</p> <a href="http://scienceblogs.com/catdynamics/2012/02/ominous_signs_for_nasa.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2012/02/ominous_signs_for_nasa.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/L1lmVakuHW4" width="1"/></div>
    </summary>
    <updated>2012-02-10T06:32:47Z</updated>
    <category term="astro"/>
    <source>
      <id>http://scienceblogs.com/catdynamics/</id>
      <author>
        <name>Steinn Sigurðsson</name>
      </author>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Speculations on astronomy, astrophysics, news I find interesting, theoretical issues, science and science policy.  
I will digress into computational physics, science fiction and general issues and basically whatever I feel like whenever. 
And, of course, cats.</subtitle>
      <title>Dynamics of Cats</title>
      <updated>2012-02-14T17:08:27Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://johncarlosbaez.wordpress.com/?p=7914</id>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/the-federal-research-public-access-act/" rel="alternate" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/the-federal-research-public-access-act/#comments" rel="replies" type="text/html"/>
    <link href="http://johncarlosbaez.wordpress.com/2012/02/10/the-federal-research-public-access-act/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">The Federal Research Public Access Act</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">The Federal Research Public Access Act would make science funded by U.S. taxpayers freely available to all. <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7914&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>As of this minute, 5030 scholars have joined the <a href="http://thecostofknowledge.com/">Elsevier boycott</a>.  You should too!  But now is the time to go further and take <i>positive</i> steps to develop <i>new, better</i> systems for refereeing and distributing scholarly papers.</p>
<p>Everyone I know is talking about this now.  Today, quantum physicist <a href="http://dabacon.org/pontiff/?p=6040">Steve Flammia</a> pointed out to me that <a href="http://doyle.house.gov/press-releases-1/2012/02/doyle-introduces-bill-to-ensure-public-access-to-federally-funded-research.shtml">U.S. Representative Mike Doyle</a> has a good idea:</p>
<p>• <a href="http://doyle.house.gov/FRPA112FINAL.pdf">The Federal Research Public Access Act</a>. </p>
<p>It’s simple: <i>we should get to see the research we paid for with our tax dollars</i>. We shouldn’t have to pay for it twice: once to have it done, and once more to see the results.</p>
<p>As Doyle puts it:</p>
<blockquote><p>
Americans have the right to see the results of research funded with taxpayer dollars.  Yet such research too often gets locked away behind a pay-wall, forcing those who want to learn from it to pay expensive subscription fees for access.</p>
<p>The Federal Research Public Access Act will encourage broader collaboration among scholars in the scientific community by permitting widespread dissemination of research findings.  Promoting greater collaboration will inevitably lead to more innovative research outcomes and more effective solutions in the fields of biomedicine, energy, education, and health care.
</p></blockquote>
<p>But what does the bill actually do?  It says this: any federal agency that spends more than $100 million per year funding research must make that research freely available in a public repository no later than 6 months after the research has been published in a peer-review journal. </p>
<p>This is <i>already done</i> by the National Institute of Health: the bill would expand this practice to the National Science Foundation, the Department of Energy, and other agencies.</p>
<h3> What we should do </h3>
<p>Someone with technical brains should make it easy for US citizens to contact Congress and support this bill.  Google got 4.5 million people to sign their <a href="http://www.forbes.com/sites/erikkain/2012/01/19/4-5-million-people-signed-googles-anti-sopa-petition/">petition against SOPA</a>, the so-called <a href="http://en.wikipedia.org/wiki/Stop_Online_Piracy_Act">Stop Online Piracy Act</a>.  But we’ve been playing defense for too long.  Let’s go on the offense and do something like this for a bill that’s <i>good!</i> </p>
<p>Emailing your congressperson <a href="https://writerep.house.gov/writerep/welcome.shtml">incredibly easy</a>, but <i><a href="http://w2.eff.org/congress/#phonefax">telephone calls</a></i> are even better, precisely because they’re a bit more work.  </p>
<p>Here’s a sample of what you could write or say:</p>
<blockquote><p>
I am your constituent, and I urge you to support the Federal Research Public Access Act.  As a taxpayer, I help support scientific research out of my own pocket.  I deserve to see the results!  The National Institute of Health already demands this for all the research they support, and the system works well.  Broadening this policy will advance science and improve the lives and welfare of all Americans.
</p></blockquote>
<p>I believe an emphasis on ‘taxpayers getting their money worth’ and ‘improving the lives of all Americans’ may resonate well with the U.S. Congress: that’s why I’ve worded the message this way.  Taxes and patriotism are hot-button issues.  But of course you should feel free to modify this text!</p>
<h3> Why it’s important </h3>
<p>I think this bill is important: even if it doesn’t pass, it changes the debate and puts the publishers on the defensive.  </p>
<p>Remember: the Association of American Publishers is still supporting the <a href="http://en.wikipedia.org/wiki/Research_Works_Act">Research Works Act</a>, a bill that would <i>prevent</i> federal agencies from requiring that the research they fund be made freely available online.  It seems this bill would even <i>roll back</i> the existing requirement that research funded by the National Institute of Health be made freely available at <a href="http://publicaccess.nih.gov/">PubMed Central</a>!</p>
<p>There’s a built-in imbalance at work here.  Publishers pays lobbyists to work full-time on advancing their agenda.  Scientists and other scholars prefer to spend their time thinking about more interesting things.  So, we’re usually <i>reactive</i>: we wait until something becomes intolerable before taking action.  That’s why we’re fighting against a <a href="http://www.lib.utk.edu/~jon/crisis.html">crisis of journal prices that bankrupt our libraries</a>, and battling bad bills like the Research Works Act, when we should be developing better systems for communicating the results of our research, and supporting good bills… </p>
<p>… like the Federal Research Public Access Act!</p>
<h3> For more </h3>
<p>For more, see:</p>
<p>• David Dobbs, <a href="http://www.wired.com/wiredscience/2012/02/open-science-revolt-occupies-congress/">Open science revolt occupies Congress</a>, <i>Wired</i>, 9 February 2012.</p>
<p>• <a href="http://www.taxpayeraccess.org/action/FRPAA2012.shtml">Call to action: Tell Congress you support the Bipartisan Federal Research Public Access Act (FRPAA)</a>, Alliance for Taxpayer Access, 9 February 2012.</p>
<p>• Scholarly Publishing &amp; Academic Resources Council, <a href="http://www.arl.org/sparc/advocacy/frpaa/frpaafaq.shtml">SPARC FAQ for university administrators and faculty: Federal Research Public Access Act (FRPAA)</a>.</p>
<p>The original sponsors of the Federal Research Public Access Act were Reps. Kevin Yoder (R-KS) and Wm. Lacy Clay (D-MO).  Identical legislation is also being introduced in the U.S. Senate by Sens. John Cornyn (R-TX), Ron Wyden (D-OR), and Kay Bailey Hutchison (R-TX).   </p>
<p> </p>
<div align="center"><a href="http://en.wikipedia.org/wiki/Public_Library_of_Science"><img src="http://upload.wikimedia.org/wikipedia/commons/thumb/f/f3/Open_Access_PLoS.svg/300px-Open_Access_PLoS.svg.png"/></a></div>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/johncarlosbaez.wordpress.com/7914/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/johncarlosbaez.wordpress.com/7914/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/johncarlosbaez.wordpress.com/7914/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=johncarlosbaez.wordpress.com&amp;blog=12777403&amp;post=7914&amp;subd=johncarlosbaez&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-10T06:11:46Z</updated>
    <published>2012-02-10T05:26:58Z</published>
    <category scheme="http://johncarlosbaez.wordpress.com" term="publishing"/>
    <author>
      <name>John Baez</name>
      <uri>http://math.ucr.edu/home/baez/</uri>
    </author>
    <source>
      <id>http://johncarlosbaez.wordpress.com/feed/atom/</id>
      <link href="http://johncarlosbaez.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://johncarlosbaez.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/osd.xml" rel="search" title="Azimuth" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://johncarlosbaez.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <title xml:lang="en">Azimuth</title>
      <updated>2012-02-14T12:46:26Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://quomodocumque.wordpress.com/?p=3301</id>
    <link href="http://quomodocumque.wordpress.com/2012/02/09/blackboard-panorama/" rel="alternate" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/09/blackboard-panorama/#comments" rel="replies" type="text/html"/>
    <link href="http://quomodocumque.wordpress.com/2012/02/09/blackboard-panorama/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Blackboard panorama</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">Thanks to Emmanuel Kowalski for this action shot.  As you can no doubt tell from my happy expression in the photo, I am about to say something about mapping class groups.  <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3301&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Thanks to <a href="http://blogs.ethz.ch/kowalski/">Emmanuel Kowalski</a> for this action shot.  As you can no doubt tell from my happy expression in the photo, I am about to say something about mapping class groups.</p>
<p> </p>
<p><a href="http://quomodocumque.files.wordpress.com/2012/02/pano_20120209_154331_2.jpg"><img alt="" class="aligncenter size-full wp-image-3302" height="208" src="http://quomodocumque.files.wordpress.com/2012/02/pano_20120209_154331_2.jpg?w=500&amp;h=208" title="PANO_20120209_154331_2" width="500"/></a></p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/quomodocumque.wordpress.com/3301/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/quomodocumque.wordpress.com/3301/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/quomodocumque.wordpress.com/3301/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=quomodocumque.wordpress.com&amp;blog=1236000&amp;post=3301&amp;subd=quomodocumque&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-10T04:40:06Z</updated>
    <published>2012-02-10T04:40:06Z</published>
    <category scheme="http://quomodocumque.wordpress.com" term="math"/>
    <category scheme="http://quomodocumque.wordpress.com" term="panorama"/>
    <category scheme="http://quomodocumque.wordpress.com" term="photos"/>
    <author>
      <name>JSE</name>
      <uri>http://quomodocumque.wordpress.com</uri>
    </author>
    <source>
      <id>http://quomodocumque.wordpress.com/feed/atom/</id>
      <link href="http://quomodocumque.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://quomodocumque.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://quomodocumque.wordpress.com/osd.xml" rel="search" title="Quomodocumque" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://quomodocumque.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Math, Madison, food, the Orioles, books, my kids.</subtitle>
      <title xml:lang="en">Quomodocumque</title>
      <updated>2012-02-15T00:49:06Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://profmattstrassler.com/?p=2561</id>
    <link href="http://profmattstrassler.com/2012/02/09/this-weeks-step-forward-in-the-search-for-the-higgs-particle/" rel="alternate" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/09/this-weeks-step-forward-in-the-search-for-the-higgs-particle/#comments" rel="replies" type="text/html"/>
    <link href="http://profmattstrassler.com/2012/02/09/this-weeks-step-forward-in-the-search-for-the-higgs-particle/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">This Week’s Step Forward in the Search for the Higgs Particle</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">I’ve been busy with some pressing work in service of the triggering strategy at the Large Hadron Collider [LHC] experiments for the last few days… (and if you understand what the trigger does, you know that stuff having to do … <a href="http://profmattstrassler.com/2012/02/09/this-weeks-step-forward-in-the-search-for-the-higgs-particle/">Continue reading <span class="meta-nav">→</span></a><img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2561&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>I’ve been busy with some pressing work in service of the triggering strategy at the <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/introduction-to-the-large-hadron-collider/" target="_blank" title="Introduction to the&#xA0;LHC">Large Hadron Collider</a> [LHC] experiments for the last few days… (and if you understand <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/the-trigger-discarding-all-but-the-gold/" title="The Trigger: Discarding All But the&#xA0;Gold">what the trigger does</a>, you know that stuff having to do with triggering pretty much takes priority over almost anything else, including sleep.) So my apologies that I’ve been a little slow to sum up this week’s updated results on the search for the <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/360-2/" target="_blank" title="The Higgs FAQ&#xA0;1.0">Higgs particle</a>.   Today I hope to make amends.</p>
<p>In <a href="http://profmattstrassler.com/2012/02/07/some-higgs-news-coming-in-a-few-hours/" target="_blank" title="Some Higgs News&#xA0;NOW">Tuesday’s post </a>I reported that the ATLAS and CMS experiments at the LHC had updated their <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/holiday-higgs-hints-confidence-inspiring-or-not/" title="Holiday Higgs Hints: Confidence-Inspiring or&#xA0;Not?">preliminary results on the Higgs search presented on December 13th</a>, through the release of documents intended for publication [so-called ``preprints,'' intended for submission to a journal for peer review.]  In updates to that post, I highlighted two issues which I found particularly interesting in comparing the updated information to the presentations in December. The first of these represents additional evidence from CMS, which strengthens their case for a signal of a Higgs-like particle with a mass around 124 <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/some-technical-concepts/a-technical-concept-gev-and-tev/" target="_blank" title="GeV and&#xA0;TeV">GeV</a>/c<sup>2</sup>. The second of these involves the lack of any improvement in the concordance between ATLAS and CMS, which one might have hoped for, and in whose absence the results still remain almost as inconclusive as they were back in December. Today I want to explain these in a bit more detail.</p>
<p><strong>The New Result From CMS</strong></p>
<div class="wp-caption alignright" id="attachment_2562" style="width: 370px;"><a href="http://profmattstrassler.files.wordpress.com/2012/02/smhiggsmakeit.png"><img alt="" class=" wp-image-2562  " height="275" src="http://profmattstrassler.files.wordpress.com/2012/02/smhiggsmakeit.png?w=360&amp;h=275" title="SMHiggsMakeIt" width="360"/></a><p class="wp-caption-text">Fig. 1: The mechanisms by which a Standard Model Higgs can be produced, from largest to smallest.  The largest (p p --&gt; H, also known as g g --&gt; H, where p stands for proton and g for a gluon inside the proton) produces a Higgs and (naively -- see the text!) nothing else except remnants of the protons.  The next largest ( p p --&gt; q q H, or q q --&gt; q q H, where q stands for quark) produces a Higgs plus two quarks, each of which appears in the detector as a jet.  The disturbances in the W and Z fields are often called "virtual particles", though they are not really particles at all.</p></div>
<p>CMS, like ATLAS, has been searching for Standard Model (or Standard-Model-like) <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-standard-model-higgs/decays-of-the-standard-model-higgs/" target="_blank" title="Decays of the Standard Model&#xA0;Higgs">Higgs particles decaying</a> to two photons, independent of how they are produced.  [Recall that the ``<a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-standard-model-higgs/" target="_blank" title="The Standard Model&#xA0;Higgs">Standard Model Higgs particle</a>'' is the simplest form of Higgs particle that might be present in nature.]  But there are <a href="http://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-standard-model-higgs/production-of-the-standard-model-higgs-particle/" target="_blank" title="Production of the Standard Model Higgs&#xA0;Particle">several ways to produce Standard Model Higgs particles</a> (see Figure 1), the two largest of which are (1) g g –&gt; H, two gluons (one from each proton `p’, so this is also called p p –&gt; H) colliding to make a Higgs particle, and (2) q q –&gt; q q H, two quarks scattering off each other and producing W and Z <a href="http://profmattstrassler.com/articles-and-posts/particle-physics-basics/virtual-particles-what-are-they/" target="_blank" title="Virtual Particles: What are&#xA0;they?">“virtual particles” (disturbances in the W and Z fields which aren’t particles at all)</a>, which meet in the middle and fuse to create a Higgs particle. The rate at which q q –&gt; q q H occurs is about 10-15 times smaller than the rate for g g –&gt; H. Now if there is a Standard Model Higgs particle at around 125 GeV/c<sup>2</sup>, the number of these Higgs particles already produced in ATLAS and CMS (each) and decaying to two photons is about 150 or so via g g –&gt; H, and about 10 or so produced in q q –&gt; q q H. Not all of these would be detected, so the numbers observed would be  somewhat smaller.</p>
<p>Let me start by making a simple and naive (and wrong) comment about these two production processes. The conclusion we’ll draw from the naive viewpoint will turn out to be correct, but the details will change, in an important way, when I correct these initial statements toward the end of this section.</p>
<p>From Figure 1, you can see that the thing which makes q q –&gt; q q H different from the g g –&gt; H process is that there are two outgoing quarks, which turn into two outgoing <a href="http://profmattstrassler.com/articles-and-posts/particle-physics-basics/the-known-apparently-elementary-particles/jets-the-manifestation-of-quarks-and-gluons/" target="_blank" title="Jets: The Manifestation of Quarks and&#xA0;Gluons">jets (sprays of hadrons)</a>. In other words, what the experiments will observe is collisions with two photons (from the decaying Higgs) along with two jets. So (naively) they should be able to look for the q q –&gt; q q H process and measure it separately from the g g –&gt; H process by <em>separating the events with two photons into those that have two jets and those that don’t</em>.</p>
<div class="wp-caption alignleft" id="attachment_2563" style="width: 510px;"><a href="http://profmattstrassler.files.wordpress.com/2012/02/cmsnewdiphoton.png"><img alt="" class="size-full wp-image-2563" height="247" src="http://profmattstrassler.files.wordpress.com/2012/02/cmsnewdiphoton.png?w=500&amp;h=247" title="CMSNewDiphoton" width="500"/></a><p class="wp-caption-text">Fig. 2: CMS updated results, showing the number of events with two photons that have a particular invariant mass. Left: all collisions with two photons. Right: all collisions with two photons and two jets (subject to additional criteria; see text.) In red is the shape of the background; black dots are data, and the blue curves show the size and shape of an expected signal that is *twice* as big as expected for a Standard Model Higgs particle of mass 120 GeV.</p></div>
<p>Now why would that buy you anything? Because the backgrounds (processes that mimic a Higgs signal but have nothing to do with a Higgs at all) to these two classes of events are very different. In particular, although the signal for q q –&gt; q q H is about 10 or so times smaller than that of g g –&gt; H, the background is a <strong>lot</strong> smaller, by a factor of 100. Roughly speaking, in the g g –&gt; H case one is looking for tens of events on a background of many hundreds, while in the q q –&gt; q q H case one is looking for a few events on a background of a few.</p>
<p>This is clear from the CMS results, which are shown in Figure 2. On the left is the <a href="http://profmattstrassler.com/articles-and-posts/largehadroncolliderfaq/some-technical-concepts/a-technical-concept-invariant-mass/" target="_blank" title="Invariant&#xA0;Mass">invariant mass</a> of the two photons in <em><strong>all</strong></em> observed collisions with two photons.  That includes any generated either by g g –&gt; H or q q –&gt; q q H.  However, the majority of the events in any bin are due to background (collisions that generate photon pairs for reasons that have nothing to do with the Higgs particle. ) You can see that the size of any expected excess from a Standard Model Higgs (half the size of the blue bump at the bottom of the plot) is very small compared to the sheer number of events above the bump. That’s why you have to look really closely to see the small excess that CMS claims to observe, running from 121 to 126 GeV and centered around 123-124 GeV.  The background is hundreds of events per bin, and the expected signal is just a few dozen per bin.</p>
<p>On the right of Figure 2 is the same plot for those collisions that (roughly — see below) have two jets and two photons. You see that the background is about 2 events per bin, and the expected signal is one or two events per bin. The fact that the number of background events per bin is really small means that statistical fluctuations, bin to bin, are large; that’s why the data is all over the place on the right-hand plot. But you can see by eye that there are some extra events in the 123-124 GeV bin. Now you have to be a little careful; we don’t expect all of the signal events to be in one bin. They should be spread out over three or four, because the experimental measurement, though precise, still has its limitations. So you should look at the three or four bins around 124, and ask if you see extra events. And you do — more than you would expect from a Standard Model Higgs particle, in fact.</p>
<p>Now the statistical significance of the excess isn’t very large. But if the small excess seen on the left-hand plot of Figure 2 were a pure statistical fluctuation of the background,<em><strong> there would be no particular reason for the small fraction of these collisions that appear in the right-hand plot of Figure 2 to show an excess in the same place</strong></em>. On the other hand, that is <em>exactly</em> what you would expect if there were a Higgs particle of Standard Model type at this mass. So the observed excess in the right-hand plot makes the CMS case for a Higgs particle — which was a circumstantial case involving several different measurements with very little evidence on their own — somewhat stronger. Although the statistical significance of the combination of all their measurements doesn’t change much, the statistical significance of the part of the signal that I feel most comfortable trusting — the part that comes from the two-photon search and the four-lepton search — has certainly increased.</p>
<div class="wp-caption alignright" id="attachment_2570" style="width: 510px;"><a href="http://profmattstrassler.files.wordpress.com/2012/02/ggh_g_gg.png"><img alt="" class="size-full wp-image-2570" height="255" src="http://profmattstrassler.files.wordpress.com/2012/02/ggh_g_gg.png?w=500&amp;h=255" title="ggH_g_gg" width="500"/></a><p class="wp-caption-text">Fig. 3: Proton-proton collisions that make a Higgs via the collision of two gluons can (with lower probability) also produce one or more gluons along the way. These gluons turn into jets. The last process cannot be distinguished from the p p --&gt; q q H process shown in Figure 1 (also known as q q --&gt; q q H). Thus the right hand plot in Figure 2, if indeed it contains a Higgs signal, contains a poorly known admixture of q q --&gt; q q H and g g --&gt; g g H .</p></div>
<p>Ok: let me correct the naive aspects of what I’ve told you. Simply requiring two jets is not nearly enough to separate g g –&gt; H from q q –&gt; q q H, because there is a certain probability that a gluon or two will be produced in g g –&gt; H.  In other words, there is a chance that rather than merely being g g –&gt; H, the collision of two gluons will lead to g g –&gt; g H or g g –&gt; g g H.  (See Figure 3.)  Gluons, quarks and antiquarks all make <a href="http://profmattstrassler.com/articles-and-posts/particle-physics-basics/the-known-apparently-elementary-particles/jets-the-manifestation-of-quarks-and-gluons/" title="Jets: The Manifestation of Quarks and&#xA0;Gluons">jets</a>, and gluon jets look a lot like quark jets and cannot typically be distinguished. So g g –&gt; g g H  looks a lot like q q –&gt; q q H. Now there are tricks to try to separate these processes to a degree (involving a requirement on where the jets and photons are actually heading relative to one another) but (a) these tricks only allow <em>partial</em> separation of q q –&gt; q q H and g g –&gt; g g H , and worse (b) <em><strong>the ability of theorists to calculate how well the tricks work in separating the two is very limited</strong></em>. The CMS experimenters assign a 70% systematic uncertainty to how much g g –&gt; g g H remains after they play their tricks, but I can easily imagine this is a significant underestimate.  I would like to know more about how they came up with this number; if someone told me the systematic uncertainty was twice this big I would not flinch, given how intricate their tricks for selecting events are, and how little I would trust existing theoretical calculations in that context.  We need to hear from the world’s experts on these calculations, and see if they agree with each other that this 70% number is large enough.</p>
<p>If my concerns were valid, what that would mean is that once you play these intricate tricks (as was done for the plot on the right side of Figure 2) you would be left with a very uncertain theoretical prediction for exactly how many events a Standard Model Higgs particle would give you. The error bar on the theoretical prediction would probably be a factor of 2, possibly worse.  And if I were right, CMS might then be underestimating the Standard Model prediction, leading them to over-interpret their result in Figure 2 as additional evidence for an excess above Standard Model expectations.</p>
<p>Indeed there has been some excitement among some of my theoretical colleagues about this suggestion that the number of events observed by CMS is larger than would be expected from a Standard Model Higgs particle. This is because the number of events at ATLAS also seems to be larger than expected. But aside from the fact that the number of events in the excess seen in the right-hand plot is very low (and therefore subject to large fluctuations: if you expect 2 or 3 events, the statistical probability of getting 8 is not as small as you would think), the expectation is itself quite uncertain (and thus perhaps the 2 or 3 events expected should actually be 5 or 6.) And there’s another reason — see below — to be suspicious of any excess above the Standard Model at both ATLAS and CMS. So I would be very, very cautious about reading anything into the larger number of events.  Of course it is intriguing and fun to think about, but it is far too early to get excited.</p>
<p><em>In particular, to my excited colleagues: let’s recall that over the years the rate for the process g g –&gt; H changed by a factor of 3 as theorists did more accurate calculations. What do we currently know about the process g g –&gt; g g H, <em>especially in this very limited kinematic region, given that it has been cal</em>culated only to leading order in perturbation theory?  Even if there *is* an excess above the expectations for a Standard Model Higgs in CMS’s data, we could perhaps just as well interpret it as an excess in g g –&gt; H only, along with an underestimate of the contribution of g g –&gt; g g H to this kinematic region, and with NO excess in q q –&gt; q q H at all.</em></p>
<p><strong>Why don’t CMS and ATLAS two-photon results line up better?</strong></p>
<p>Now, let’s talk about the second issue: the fact that there was no improvement in the discrepancy in the preferred mass for ATLAS and CMS’s excesses (if interpreted as due to a new particle.)  The inconsistency isn’t so large as to make the measurements clearly contradictory, but neither is it small enough that one can ignore it.</p>
<div class="wp-caption alignright" id="attachment_2564" style="width: 510px;"><a href="http://profmattstrassler.files.wordpress.com/2012/02/digamatlascmswindow.png"><img alt="" class="size-full wp-image-2564" height="381" src="http://profmattstrassler.files.wordpress.com/2012/02/digamatlascmswindow.png?w=500&amp;h=381" title="DigamATLASCMSWindow" width="500"/></a><p class="wp-caption-text">Fig. 4: The two-photon data from 115 to 135 GeV, with a vertical line drawn in at 125 GeV to help the eye. Data are dots (statistical uncertainties are shown as vertical bars) and background is a red line. Left: CMS, all events (as in left of Figure 2); note the excess which runs from 121 to 126. Center: CMS, selected events with two jets (as in right of Figure 2); note the overall excess in the same region. Right: ATLAS; note the excess from 124 to 127.</p></div>
<p>First, let me bring your attention to the discrepancy; in Figure 4 I’ve pulled out the region from 115 to 135 GeV for the left and right plots in Figure 2, and put them next to an excerpt from ATLAS’s most recent plot covering the same region.  Note the line that I have drawn on all three plots dividing events above 125 GeV from events below 125 GeV.  What you notice is that ATLAS’s largest excess (126-127) is at a point where CMS has a deficit, and that ATLAS has a deficit across some of CMS’s excess.  I do not want to overstate the importance of this observation; it may easily be a consequence of small statistics. But neither should it be understated.  If anyone tells you that the case for the Higgs is firm, ask them about this discrepancy, which (when the case actually <em>does</em> become firm) had better go away.</p>
<p>There are three possible reasons for this discrepancy.</p>
<ol>
<li>There is no Higgs signal at all; ATLAS is seeing some fluctuations in its data, and separately, CMS is seeing some fluctuations in its data. By chance they happen to be close together, but the lack of consistency is reflective of the fact that they are actually independent effects that have nothing to do with each other.</li>
<li>There is a signal, but the shape and location of the signal are distorted because either ATLAS’s or CMS’s signal peak is sitting on top of a large background fluctuation. For example, this could easily explain why ATLAS has a peak that is larger and narrower than expected from a pure Standard Model signal, an example of which (the dotted red line centered around 120 GeV) is shown on the ATLAS plot at right in Figure 4.  Were this true, by the way, then the excess at ATLAS would be a signal plus a background fluctuation, which combine to give an excess that seems too large for a Standard Model Higgs, but which will return toward the expected size as more data is gathered and the fluctuation in the background is smoothed away.</li>
<li>There is a signal, and either ATLAS or CMS has its photon energy measurement wrong by 1-2%. Calibrating photon energies is not easy, and the mass measurement needs to be accurate to about 1%. I certainly thought it was possible that when the preliminary results of December turned into preprints we’d see a small shift in the mass measurement, up or down, at either CMS or ATLAS,  one that might move their two-photon measurements together (or apart) by as much as 1 GeV/c<sup>2</sup> or even more. It appears we did not. The preprints show essentially no difference in the two-photon distributions compared to the Dec. 13th presentations. And this suggests that the experiments are reasonably confident in their energy measurements. <em>That said, it appears that when the two-photon measurements are combined with the four-lepton measurements, the result for ATLAS and the result for CMS, whose preferred values were separated by about 2 GeV/<em>c<sup>2</sup></em>, have now moved slightly further apart, by less than half a GeV/c<sup>2</sup>. [I think this is due to a shift in the four-lepton measurement of ATLAS, but I could be wrong; I haven't been able to fully track this down yet.]</em></li>
</ol>
<p>I don’t know how to evaluate which of these possibilities is most likely, and even if I did, the truth doesn’t care what I (or you) think. We’ll just have to wait and see.</p>
<p><strong>Summary of the Update</strong></p>
<p>To sum up: the finalizing of the preliminary results from Dec. 13th has had the following effects (so far)</p>
<ul>
<li>The CMS excess at 123-124 GeV/c<sup>2</sup> in events with two photons and two jets means a moderate but notable improvement in the credibility of their case, which previously relied on combining a small excess in two photons with a very small excess in four other measurements. The case is more robust now. Meanwhile the preferred value of the mass has drifted just a tiny bit higher.</li>
<li>The ATLAS result is essentially unchanged, though the preferred value of the mass has drifted a bit higher.</li>
<li>The discrepancy between the preferred masses for the ATLAS and CMS measurements has slightly increased, not enough to cause a reevaluation of the situation, but eliminating any possibility that they might in the near term shift in such a way to become more consistent. Consistency (or clear inconsistency) will have to await a lot more data.</li>
<li>Both experiments appear to see excesses that are larger than would be expected for a Standard Model Higgs particle of this mass, by perhaps as much as a factor of 2, but given the large statistical uncertainties and (for the most recent CMS result) large systematic uncertainties, one should not be surprised if all such indications disappear over time.</li>
</ul>
<p>The excesses in the measurements remain, within the uncertainties, consistent with a Standard Model Higgs, or something rather similar, of around 125 GeV/c<sup>2</sup>.  Due to the new CMS result, I am somewhat more optimistic that this is a real signal than I was in December, but we still have a long way to go before this all begins to settle down.</p>
<br/>Filed under: <a href="http://profmattstrassler.com/category/higgs/">Higgs</a>, <a href="http://profmattstrassler.com/category/lhc-news/">LHC News</a>, <a href="http://profmattstrassler.com/category/particle-physics/">Particle Physics</a>  <a href="http://feeds.wordpress.com/1.0/gocomments/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/profmattstrassler.wordpress.com/2561/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/profmattstrassler.wordpress.com/2561/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/profmattstrassler.wordpress.com/2561/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=profmattstrassler.com&amp;blog=24633746&amp;post=2561&amp;subd=profmattstrassler&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-10T00:32:10Z</updated>
    <published>2012-02-10T00:26:30Z</published>
    <category scheme="http://profmattstrassler.com" term="Higgs"/>
    <category scheme="http://profmattstrassler.com" term="LHC News"/>
    <category scheme="http://profmattstrassler.com" term="Particle Physics"/>
    <author>
      <name>Matt Strassler</name>
      <uri>http://profmattstrassler.wordpress.com</uri>
    </author>
    <source>
      <id>http://profmattstrassler.com/feed/atom/</id>
      <link href="http://profmattstrassler.com" rel="alternate" type="text/html"/>
      <link href="http://profmattstrassler.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://profmattstrassler.com/osd.xml" rel="search" title="Of Particular Significance" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://profmattstrassler.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Conversations About Science with Theoretical Physicist Matt Strassler</subtitle>
      <title xml:lang="en">Of Particular Significance</title>
      <updated>2012-02-14T23:45:40Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>tag:golem.ph.utexas.edu,2012:%2Fcategory%2F3.2495</id>
    <link href="http://golem.ph.utexas.edu/category/2012/02/the_cost_of_knowledge.html" rel="alternate" type="application/xhtml+xml"/>
    <title xml:lang="en">The Cost of Knowledge</title>
    <summary xml:lang="en">An explanation of the Elsevier boycott, from the mathematician's point of view.</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img alt="MathML-enabled post (click for more details)." class="mathlogo" src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" title="MathML-enabled post (click for details)."/></a></div>
<p>As of this moment, 4760 scholars have joined a <a href="http://thecostofknowledge.com/"> boycott of the publishing company Elsevier</a>.  Of these, only 20% are mathematicians.  But since the boycott was started by a mathematician, 34 of us wrote and signed  <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf"> statement</a> explaining the boycott.  Here it is.</p>
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img alt="MathML-enabled post (click for more details)." class="mathlogo" src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" title="MathML-enabled post (click for details)."/></a></div>
<h4> THE COST OF KNOWLEDGE </h4>

<p>This is an attempt to describe some of the background to the current
boycott of Elsevier by many mathematicians (and other academics) at
<a href="http://thecostofknowledge.com">http://thecostofknowledge.com</a>, and to present some of the issues that
confront the boycott movement.  Although the movement is anything but
monolithic, we believe that the points we make
here will resonate with many of the signatories to the boycott.</p>

<h4> The role of journals (1): dissemination of research.</h4>  The role of
journals in professional mathematics has been under discussion for some
time now.

<p>Traditionally, while journals served several purposes, their primary
purpose was the dissemination of research papers.  The journal
publishers were charging for the cost of typesetting (not a trivial
matter in general before the advent of electronic typesetting, and
particularly non-trivial for mathematics), the cost of physically
publishing copies of the journals, and the cost of distributing the
journals to subscribers (primarily academic libraries).</p>

<p>The editorial board of a journal is a group of professional
mathematicians. Their editorial work is undertaken as part of
their scholarly duties, and so is paid for by their employer,
typically a university. Thus, from the publisher’s viewpoint
the editors are volunteers. (The editor in chief of a
journal sometimes receives modest compensation from the
publisher.) When a paper is submitted to the journal, by an
author who is again typically a university-employed
mathematician, the editors select the referee or referees for
the paper, evaluate the referees’ reports, decide whether or
not to accept the submission, and organize the submitted papers
into volumes.  These are passed on to the publisher, who then
undertakes the job of actually publishing them. The publisher
supplies some administrative assistance in handling the papers,
as well as some copy-editing assistance, which is often quite
minor but sometimes more substantial. The referees are again
volunteers from the point of view of the publisher: as with
editing, refereeing is regarded as part of the service
component of a mathematician’s academic work. Authors are not
paid by the publishers for their published papers, although
they are usually asked to sign over the copyright to the
publisher.</p>

<p>This system made sense when the publishing and dissemination of
papers was a difficult and expensive undertaking.  Publishers
supplied a valuable service in this regard, for which they were
paid by subscribers to the journals, which were mainly academic
libraries. The academic institutions whose libraries subscribe
to mathematics journals are broadly speaking the same
institutions that employ the mathematicians who are writing
for, refereeing for, and editing the journals. Therefore, the
cost of the whole process of producing research papers is borne
by these institutions (and the outside entities that partially
fund them, such as the National Science Foundation in the
United States): they pay for their academic mathematician
employees to do research and to organize the publications of
the results of their research in journals; and then (through their
libraries) they pay the publishers to disseminate these results
among all the world’s mathematicians. Since these institutions
employ research faculty in order to foster research, it
certainly used to make sense for them to pay for the
dissemination of this research as well. After all, the sharing
of scientific ideas and research results is unquestionably a
key component for making progress in science.</p>

<p>Now, however, the world has changed in significant ways.
Authors typeset their own papers, using electronic typesetting.
Publishing and distribution costs are not
as great as they once were.  And most importantly,
dissemination of scientific ideas no longer takes place via the
physical distribution of journal volumes. Rather, it
takes place mainly electronically. While this means of dissemination
is not free, it is much less expensive, and much of it happens quite
independently of mathematical journals.</p>

<p>In conclusion, the cost of journal publishing has gone down
because the cost of typesetting has been shifted from
publishers to authors and the cost of
publishing and distribution is significantly lower than it used to be.
By contrast, the amount of money being spent by university libraries on
journals seems to be growing with no end in sight.  Why do mathematicians
contribute all this volunteer labor, and their employers pay all this money, for
a service whose value no longer justifies its cost?</p>

<h4> The role of journals (2): peer review and professional
evaluation</h4>

<p>There are some important reasons that mathematicians
haven’t just abandoned journal publishing. In particular, peer review plays an
essential role in ensuring the correctness and readability of
mathematical papers, and publishing papers in research journals
is the main way of achieving professional recognition.
Furthermore, not all journals count equally from this point of
view: journals are (loosely) ranked, so that publications
in top journals will often count more than publications in
lower ranked ones. Professional mathematicians typically have a
good sense of the relative prestige of the journals that
publish papers in their area, and they will usually submit a
paper to the highest ranked journal that they judge is likely
to accept and publish it.</p>

<p>Because of this evaluative aspect of traditional journal publishing, the
problem of switching to a different model
is much more difficult than it might appear at first.  For
example, it is not easy just to begin a new journal (even an
electronic one, which avoids the difficulties of printing
and distribution), since mathematicians may not want to publish
in it, preferring to submit to journals with known reputations.
Secondly, although the reputation of various journals has been
created through the efforts of the authors, referees, and editors
who have worked (at no cost to the publishers) on it over the
years, in many cases the <i>name</i> of the journal is owned by
the publisher, making it difficult for the mathematical
community to separate this valuable object that they have
constructed from its present publisher.</p>

<h4> The role of Elsevier</h4>  

<p>Elsevier, Springer, and a number
of other commercial publishers (many of them large companies
but less significant for their mathematics publishing, e.g.,
Wiley) all exploit our volunteer labor to extract very large profits from
the academic community. They supply some value in the process,
but nothing like enough to justify their prices.</p>

<p>Among these publishers, Elsevier may not be the most expensive,
but in the light of other factors, such as scandals,
lawsuits, lobbying, etc. (discussed further below), we consider
them a good initial focus for our discontent. A boycott should
be substantial enough to be meaningful, but
not so broad that the choice of targets becomes controversial
or the boycott becomes an unmanageable burden.  Refusing to
submit papers to all overpriced publishers is a reasonable
further step, which some of us have taken, but the focus of
this boycott is on Elsevier because of the widespread feeling
among mathematicians that they are the worst offender.</p>

<p>Let us begin with the issue of journal costs.  Unfortunately, it is
difficult to make cost comparisons: journals differ greatly in quality,
in number of pages per volume, and even in amount of text per page.  As
measured by list prices, Elsevier mathematics journals are amongst the
most expensive. For instance, in the <a href="http://www.ams.org/membership/mem-journal-survey">AMS mathematics journal price
survey</a>, seven
of the ten most expensive journals (by 2007 volume list
price) were published by Elsevier.   (All prices are as of 2007 because both prices and page counts are easily available online.) 
However, that is primarily because Elsevier publishes the largest
volumes. Price per page is a more meaningful measure that can be easily
computed.  By this standard, Elsevier is certainly not the worst
publisher, but its prices do on the face of it look very high. The
<i>Annals of Mathematics</i>, published by Princeton University Press,
is one of the absolute top mathematics journals and quite affordably
priced: $0.13/page as of 2007.  By contrast, ten Elsevier
journals (not including one that has since ceased publication)
 cost $1.30/page or more; they and three others cost more per page than
<i>any</i> journal published by a university press or learned society.
For comparison, three other top journals competing with the
<i>Annals</i> are <i>Acta Mathematica</i>, published by the Institut
Mittag Leffler for $0.65/page, <i>Journal of the American
Mathematical Society</i>, published by the American Mathematical Society
for $0.24/page, and <i>Inventiones Mathematicae</i>, published by
Springer for $1.21/page.  Note that none of Elsevier’s mathematics
journals is generally considered comparable in quality to these
journals.</p>

<p>However, there is an additional aspect which makes it hard to
compute the true cost of mathematics journals. This is the
widespread practice among large commercial publishers of
“bundling” journals, which allows libraries to subscribe to
large numbers of journals in order to avoid paying the
exorbitant list prices for the ones they need. Although
this means that the average price libraries
pay per journal is less than the list prices might suggest,
what really matters is the average price that they pay per
journal (or page of journal) <i>that they actually want</i>, which
is hard to assess, but clearly higher. We
would very much like to be able to offer more concrete data
regarding the actual costs to libraries of Elsevier journals
compared with those of Springer or other publishers.
Unfortunately, this is difficult, because publishers often make
it a contractual requirement that their institutional customers
should not disclose the financial details of their contracts.
For example, Elsevier sued Washington State University to try
to prevent release of this information. One
common consequence of these arrangements, though, is that in
many cases a library cannot actually save any money by
cancelling a few Elsevier journals: at best the money can
sometimes be diverted to pay for other Elsevier subscriptions.</p>

<p>One reason for focusing on Elsevier rather than, say, Springer
is that Springer has had a rich and productive
history with the mathematical community. As well as journals,
it has published important series of textbooks,
monographs, and lecture notes; one could perhaps regard the prices
of its journals as a means of subsidizing these other, less
profitable, types of publications. Although all these types of
publications have become less important with the advent of the
internet and the resulting electronic distribution of texts,
the long and continuing presence of Springer in the mathematical world
has resulted in a store of goodwill being built up in the
mathematical community towards them.  This store is
being rapidly depleted, but has not yet reached zero.  See for instance the <a href="http://www-fourier.ujf-grenoble.fr/petitions/index.php?petition=3">recent petition to Springer</a> by a number of French mathematicians and departments.</p>

<p>Elsevier does not have a comparable
tradition of involvement in mathematics publishing.  Many of
the mathematics journals that it publishes have been acquired
comparatively recently as it has bought up other, smaller
publishers.   Furthermore, in recent years it has been involved
in various scandals regarding the scientific content, or lack
thereof, of its journals. One in particular involved
the journal <i>Chaos, Solitons &amp; Fractals</i>,  which, at the
time the scandal broke in 2008–2009, was one of the highest
impact factor  mathematics journals that Elsevier published.   (Elsevier currently reports the five-year impact factor of this journal at <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mn>1.729</mn></math>.  For sake of
comparison, <i>Advances in Mathematics</i>, also published by
Elsevier, is reported as having a five-year impact factor of
<math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mn>1.575</mn></math>.)  It
turned out that the high impact factor was at least partly the
result of the journal publishing many papers full of mutual
citations.  (See  <a href="http://www.siam.org/news/news.php?id=1663">Arnold</a> for more information on
this and other troubling examples that show the limitations of
bibliometric measures of scholarly quality.) Furthermore, <i>
Chaos, Solitons &amp; Fractals</i> published many papers that, in
our professional judgement, have little or no scientific merit
and should not have been published in any reputable journal.</p>

<p>In another notorious episode, this time in medicine, for at least five years
Elsevier “published a series of sponsored article compilation
publications, on behalf of pharmaceutical clients, that were made to
look like journals and lacked the proper disclosures”, as noted by <a href="http://www.elsevier. com/wps/find/authored_newsitem.cws_home/companynews05_01203">the CEO of Elsevier’s Health Sciences Division</a>.</p>

<p>Recently, Elsevier has lobbied for the Research Works Act,
a proposed U.S. law that would undo the National Institutes of
Health’s public access policy, which guarantees public access to
published research papers based on NIH funding within twelve months of
publication (to give publishers time to make a profit). Although most
lobbying occurs behind closed doors, Elsevier’s vocal support of this
act shows their opposition to a popular and effective open access
policy.</p>

<p>These scandals, taken together with the bundling practices,
exorbitant prices, and lobbying activities, suggest
a publisher motivated purely by profit, with no genuine
interest in or commitment to mathematical knowledge and the
community of academic mathematicians that generates it.  Of
course, many Elsevier employees are reasonable people doing
their best to contribute to scholarly publishing, and we bear
them no ill will.  However, the organization as a whole does not
seem to have the interests of the mathematical community
at heart.</p>

<h4> The boycott </h4>

<p>Not surprisingly, many mathematicians have
in recent years lost patience with being involved in a system
in which commercial publishers make profits based on the free
labor of mathematicians and subscription fees from their
institutions’ libraries, for a service that has become largely
unnecessary.  (See <a href="http://www.scottaaronson.com/writings/journal.pdf">Scott Aaronson’s scathing but all-too-true satirical
description</a> of the publishers’ business model.)  Among all the
commercial publishers, the behavior of Elsevier seemed to many
to be the most egregious, and a number of mathematicians had
made personal commitments to avoid any involvement with
Elsevier journals.  (Some journals were also
successfully moved from Elsevier to other publishers; e.g.,
<i>Annales Scientifiques de l’école Normale Supérieure</i>
which until recent years was published by Elsevier, is now
published by the Société Mathématique de France.)</p>

<p>One of us (Timothy Gowers) decided that it might be useful to
publicize his own personal boycott of Elsevier, thus
encouraging others to do the same.   This led to the current
boycott movement at <a href="http://thecostofknowledge.com">http://thecostofknowledge.com</a>, the success of which has far exceeded his initial expectations.</p>

<p>Each participant in the boycott can choose which activities they intend
to avoid: submitting to Elsevier journals, refereeing for them, and
serving on editorial boards.  Of course, submitting papers and editing
journals are purely voluntary activities, but refereeing is a more
subtle issue.  The entire peer review system depends on the
availability of suitable referees, and its success is one of the great
traditions of science: refereeing is felt to be both a burden and an
honor, and practically every member of the community willingly takes
part in it. However, while we respect and value this tradition, many of us do
not wish to see our labor used to support Elsevier’s business
model.</p>

<h4> What next?</h4>

<p>As suggested at the very beginning, different participants
in the boycott have different
goals, both in the short and long term.  Some people would like to see
the journal system eliminated completely and replaced by something
else more adapted to the internet and the possibilities of electronic
distribution.  Others see journals as continuing to play a role, but
with commercial publishing being replaced by open access models. Still
others imagine a more modest change, in which commercial publishers are
replaced by non-profit entities such as professional societies (e.g.,
the American Mathematical Society, the London Mathematical Society, and
the Société Mathématique de France, all of which already publish
a number of journals) or university presses; in this way the value
generated by the work of authors, referees, and editors would be
returned to the academic and scientific community. These goals need not
be mutually exclusive: the world of mathematics journals, like the
world of mathematics itself, is large, and open access journals can
coexist with traditional journals, as well as with other, more novel
means of dissemination and evaluation.</p>

<p>What all the signatories do agree on is that Elsevier is an exemplar of
everything that is wrong with the current system of commercial
publication of mathematics journals, and we will no longer acquiesce to
Elsevier’s harvesting of the value of our and our colleagues’ work.</p>

<p>What future do we envisage for all the papers that would
otherwise be published in Elsevier journals? There are many
other journals being published; perhaps they can pick up at
least some of the slack. Many successful new journals have been
founded in recent years, too, including several that are
electronic (thus completely eliminating printing and physical
distribution costs), and no doubt more will follow. Finally, we
hope that the mathematical community will be able to reclaim
for itself some of the value that it has given to Elsevier’s
journals by moving some of these journals (in name, if
possible, and otherwise in spirit)  from Elsevier to other publishers.  One notable example  is the August 10, 2006 resignation of the entire editorial
board of the Elsevier journal <i>Topology</i> and their
founding of the <i>Journal of Topology</i>, owned by the London
Mathematical Society.  </p>

<p>None of these changes will be easy; editing a journal is hard work, and
founding a new journal, or moving and relaunching an existing journal,
is even harder. But the alternative is to continue with the status quo,
in which Elsevier harvests ever larger profits from the work of us and
our colleagues, and this is both unsustainable and unacceptable.</p>

<p>Signed by:</p>

<p>Scott Aaronson <br/>
Massachusetts Institute of Technology</p>

<p>Douglas N. Arnold<br/>
University of Minnesota</p>

<p>Artur Avila<br/>
IMPA and Institut de Mathématiques de Jussieu</p>

<p>John Baez<br/>
University of California, Riverside</p>

<p>Folkmar Bornemann<br/>
Technische Universität München</p>

<p>Danny Calegari<br/>
Caltech/Cambridge University</p>

<p>Henry Cohn<br/>
Microsoft Research New England</p>

<p>Jordan Ellenberg<br/>
University of Wisconsin, Madison</p>

<p>Matthew Emerton<br/>
University of Chicago</p>

<p>Marie Farge<br/>
École Normale Supérieure Paris</p>

<p>David Gabai<br/>
Princeton University</p>

<p>Timothy Gowers<br/>
Cambridge University</p>

<p>Ben Green<br/>
Cambridge University</p>

<p>Martin Grötschel<br/>
Technische Universität Berlin</p>

<p>Michael Harris<br/>
Université Paris-Diderot Paris 7</p>

<p>Frédéric Hélein<br/>
Institut de Mathéatiques de Jussieu</p>

<p>Rob Kirby<br/>
University of California, Berkeley</p>

<p>Vincent Lafforgue<br/>
CNRS and Université d’Orléans</p>

<p>Gregory F. Lawler<br/>
University of Chicago</p>

<p>Randall J. LeVeque<br/>
University of Washington</p>

<p>László Lovász<br/>
Eötvös Lor´nd University</p>

<p>Peter J. Olver<br/>
University of Minnesota</p>

<p>Olof Sisask<br/>
Queen Mary, University of London</p>

<p>Terence Tao<br/>
University of California, Los Angeles</p>

<p>Richard Taylor<br/>
Institute for Advanced Study</p>

<p>Bernard Teissier<br/>
Institut de Mathématiques de Jussieu</p>

<p>Burt Totaro<br/>
Cambridge University</p>

<p>Lloyd N. Trefethen<br/>
Oxford University</p>

<p>Takashi Tsuboi<br/>
University of Tokyo</p>

<p>Marie-France Vigneras<br/>
Institut de Mathématiques de Jussieu </p>

<p>Wendelin Werner<br/>
Université Paris-Sud</p>

<p>Amie Wilkinson<br/>
University of Chicago</p>

<p>Günter M. Ziegler<br/>
Freie Universität Berlin</p>

<h4> Appendix: recommendations for mathematicians.</h4>  All
mathematicians must decide for themselves whether, or to what
extent, they wish to participate in the boycott.  Senior
mathematicians who have signed the boycott bear some
responsibility towards junior colleagues who are forgoing the
option of publishing in Elsevier journals, and should do their
best to help minimize any negative career consequences.

<p>Whether or not you decide to join the boycott, there are some
simple actions that everyone can take, which seem to us to be
uncontroversial:</p>

<ol>
<li>
Make sure that the final versions of all your papers,
    particularly new ones, are freely available online –
    ideally both on the arXiv.  (Elsevier’s
    electronic preprint policy is
    unacceptable, because it explicitly does not allow
    authors to update their papers on the arXiv to
    incorporate changes made during peer review). When signing copyright transfer
    forms, we recommend amending them (if necessary) to
    reserve the right to make the author’s final version of
    the text available free online from servers such as the
    arXiv, and on your home page.
</li>
<li>
 If you are submitting a paper and there is a choice between
     an expensive journal and a cheap (or free) journal of the same
     standard, then always submit to the cheap one.
</li>
</ol>

<h4> Note </h4>

<p>The <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf"><abbr title="Portable Document Format">PDF</abbr> version</a> of this statement has many useful references not included here.</p></div>
    </content>
    <updated>2012-02-10T00:05:29Z</updated>
    <published>2012-02-09T01:51:37Z</published>
    <author>
      <name>john</name>
      <email>baez@math.ucr.edu</email>
      <uri>http://math.ucr.edu/home/baez/</uri>
    </author>
    <source>
      <id>tag:golem.ph.utexas.edu,2006:nCategoryCafe/3</id>
      <icon>http://golem.ph.utexas.edu/category/images/favicon.ico</icon>
      <link href="http://golem.ph.utexas.edu/category/" rel="alternate" type="application/xhtml+xml"/>
      <link href="http://golem.ph.utexas.edu/category/atom10.xml" rel="self" type="application/atom+xml"/>
      <link href="http://golem.ph.utexas.edu/category/comments.atom" rel="replies" type="application/atom+xml"/>
      <rights xml:lang="en">Copyright (c) 2012, The n-Category Collective</rights>
      <subtitle xml:lang="en">A group blog on math, physics and philosophy</subtitle>
      <title xml:lang="en">The n-Category Café</title>
      <updated>2012-02-14T21:19:22Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://dabacon.org/pontiff/?p=6040</id>
    <link href="http://dabacon.org/pontiff/?p=6040" rel="alternate" type="text/html"/>
    <link href="http://dabacon.org/pontiff/?p=6040#comments" rel="replies" type="text/html"/>
    <link href="http://dabacon.org/pontiff/?feed=atom&amp;p=6040" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">A Federal Mandate for Open Science</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">Witness the birth of the Federal Research Public Access Act: “The Federal Research Public Access Act will encourage broader collaboration among scholars in the scientific community by permitting widespread dissemination of research findings.  Promoting greater collaboration will inevitably lead to … <a href="http://dabacon.org/pontiff/?p=6040">Continue reading <span class="meta-nav">→</span></a></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Witness the birth of the <a href="http://doyle.house.gov/press-releases-1/2012/02/doyle-introduces-bill-to-ensure-public-access-to-federally-funded-research.shtml">Federal Research Public Access Act</a>:</p>
<blockquote><p>“The Federal Research Public Access Act will encourage broader collaboration among scholars in the scientific community by permitting widespread dissemination of research findings.  Promoting greater collaboration will inevitably lead to more innovative research outcomes and more effective solutions in the fields of biomedicine, energy, education, quantum information theory and health care.”</p>
<h6>[Correction: it didn't really mention quantum information theory---SF.]</h6>
</blockquote>
<p>You can read the full text of FRPAA <a href="http://doyle.house.gov/FRPA112FINAL.pdf">here</a>.</p>
<p>The bill states that any federal agency which budgets more than $100 million per year for funding external research must make that research available in a public online repository for free download now later than 6 months after the research has been published in a peer-reviewed journal.</p>
<p>This looks to me like a big step in the right direction for open science. Of course, it’s still <a href="http://www.youtube.com/watch?v=tyeJ55o3El0">just a bill</a>, and needs to successfully navigate the Straights of the Republican-controlled House, through the Labyrinth of Committees and the Forest of Filibuster, and run the Gauntlet of Presidential Vetos. How can you help it survive this harrowing journey? Write your <a href="http://www.senate.gov/general/contact_information/senators_cfm.cfm">senators</a> and your <a href="https://writerep.house.gov/writerep/welcome.shtml">congresscritter</a> today, and tell them that you support FRPAA and open science!</p>
<p>Hat tip to Robin Blume-Kohout.</p></div>
    </content>
    <updated>2012-02-09T22:56:03Z</updated>
    <published>2012-02-09T22:38:41Z</published>
    <category scheme="http://dabacon.org/pontiff" term="Open Science"/>
    <category scheme="http://dabacon.org/pontiff" term="Politics"/>
    <category scheme="http://dabacon.org/pontiff" term="Science 2.0"/>
    <category scheme="http://dabacon.org/pontiff" term="Scientific Publishing"/>
    <category scheme="http://dabacon.org/pontiff" term="Society"/>
    <author>
      <name>sflammia</name>
    </author>
    <source>
      <id>http://dabacon.org/pontiff/?feed=atom</id>
      <link href="http://dabacon.org/pontiff" rel="alternate" type="text/html"/>
      <link href="http://dabacon.org/pontiff/?feed=atom" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">A College of Quantum Cardinals</subtitle>
      <title xml:lang="en">The Quantum Pontiff</title>
      <updated>2012-02-13T23:02:04Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-10448119.post-1063042427423591228</id>
    <link href="http://hoggresearch.blogspot.com/feeds/1063042427423591228/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/exoplanets-and-speckles.html#comment-form" rel="replies" title="1 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/1063042427423591228" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/1063042427423591228" rel="self" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/exoplanets-and-speckles.html" rel="alternate" title="exoplanets and speckles" type="text/html"/>
    <title>exoplanets and speckles</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Fergus did a set of demonstrations today for Oppenheimer, Brenner, and me of his planet-finding code for Oppenheimer's P1640 high dynamic-range imager.  The imager blocks out most of the light of the star in an intermediate focal plane, but a combination of atmosphere and optical distortions plus physical optics means that still huge amounts of light hits the focal plane and in a very speckly pattern of blobs.  Fergus showed us that he can (potentially) find planets among those speckles, even planets that are percent-level distortions of the speckle pattern!  If this holds up it could have huge impact on high dynamic-range imaging, now and in the near future.  For the past week or two I have also been playing around with modeling electromagnetic fields in imperfect cameras to see if we can make a more physically motivated model (Fergus's model is data-driven rather than physics-driven).</p><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/10448119-1063042427423591228?l=hoggresearch.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-09T21:26:57Z</updated>
    <published>2012-02-09T21:26:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="exoplanet"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="telescope"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="point-spread function"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="star"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="talking"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="code"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="imaging"/>
    <author>
      <name>Hogg</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/18398397408280534592</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-10448119</id>
      <category term="Willman 1"/>
      <category term="clustering"/>
      <category term="merging"/>
      <category term="galaxy"/>
      <category term="PHAT"/>
      <category term="HMF"/>
      <category term="proper motion"/>
      <category term="amateur"/>
      <category term="sdss"/>
      <category term="LSST"/>
      <category term="virtual observatory"/>
      <category term="tractor"/>
      <category term="robot"/>
      <category term="funding"/>
      <category term="telescope"/>
      <category term="digital camera"/>
      <category term="meta data"/>
      <category term="proposal"/>
      <category term="disk"/>
      <category term="fundamental astronomy"/>
      <category term="roweis"/>
      <category term="classification"/>
      <category term="practice"/>
      <category term="decision"/>
      <category term="travel"/>
      <category term="linear algebra"/>
      <category term="interstellar medium"/>
      <category term="web 2.0"/>
      <category term="email"/>
      <category term="bayes"/>
      <category term="scattering"/>
      <category term="atlas"/>
      <category term="quasar"/>
      <category term="confusion"/>
      <category term="minor planet"/>
      <category term="anthropology"/>
      <category term="gravitational lensing"/>
      <category term="reading"/>
      <category term="black hole"/>
      <category term="visualization"/>
      <category term="halo"/>
      <category term="cosmology"/>
      <category term="seminar"/>
      <category term="information"/>
      <category term="2mass"/>
      <category term="chemistry"/>
      <category term="HST"/>
      <category term="gravity"/>
      <category term="panstarrs"/>
      <category term="philosophy"/>
      <category term="experiment"/>
      <category term="WMAP"/>
      <category term="sample"/>
      <category term="baryon acoustic feature"/>
      <category term="radial velocity"/>
      <category term="ukidss"/>
      <category term="dark sector"/>
      <category term="parallax"/>
      <category term="spectroscopy"/>
      <category term="brown dwarf"/>
      <category term="LTFDFCF"/>
      <category term="kinematics"/>
      <category term="cosmography"/>
      <category term="transparency"/>
      <category term="flickr"/>
      <category term="calibration"/>
      <category term="optimization"/>
      <category term="editing"/>
      <category term="star formation"/>
      <category term="ultraviolet"/>
      <category term="statistics"/>
      <category term="testing"/>
      <category term="correlation"/>
      <category term="galex"/>
      <category term="intergalactic medium"/>
      <category term="noise"/>
      <category term="computing"/>
      <category term="dissertation"/>
      <category term="citizen science"/>
      <category term="nasa"/>
      <category term="planet"/>
      <category term="wise"/>
      <category term="talking"/>
      <category term="spitzer"/>
      <category term="cluster"/>
      <category term="CDM"/>
      <category term="astrometry"/>
      <category term="environment"/>
      <category term="imaging"/>
      <category term="press"/>
      <category term="MCMC"/>
      <category term="gaia"/>
      <category term="evolution"/>
      <category term="primus"/>
      <category term="compression"/>
      <category term="phase space"/>
      <category term="relativity"/>
      <category term="weapons"/>
      <category term="archive"/>
      <category term="Solar System"/>
      <category term="Milky Way"/>
      <category term="code"/>
      <category term="observing"/>
      <category term="learning"/>
      <category term="point-spread function"/>
      <category term="Euclid"/>
      <category term="hardware"/>
      <category term="catalog"/>
      <category term="science"/>
      <category term="database"/>
      <category term="thinking"/>
      <category term="gamma-ray burst"/>
      <category term="exoplanet"/>
      <category term="white dwarf"/>
      <category term="theory"/>
      <category term="hipparcos"/>
      <category term="radio"/>
      <category term="law"/>
      <category term="pulsar"/>
      <category term="Gaussian process"/>
      <category term="osss"/>
      <category term="politics"/>
      <category term="meeting"/>
      <category term="photometry"/>
      <category term="star"/>
      <category term="not research"/>
      <category term="API"/>
      <category term="cosmic ray"/>
      <category term="substructure"/>
      <category term="post-starburst"/>
      <category term="archetype"/>
      <category term="life"/>
      <category term="time"/>
      <category term="literature"/>
      <category term="dynamics"/>
      <category term="comet"/>
      <category term="anthropic"/>
      <category term="supernova"/>
      <category term="Earth"/>
      <category term="PTF"/>
      <category term="Fermi"/>
      <category term="search"/>
      <category term="usno-b"/>
      <category term="mathematics"/>
      <category term="dust"/>
      <category term="coffee"/>
      <category term="project management"/>
      <category term="model"/>
      <category term="data"/>
      <category term="writing"/>
      <author>
        <name>Hogg</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/18398397408280534592</uri>
      </author>
      <link href="http://hoggresearch.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://hoggresearch.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>galaxies, stellar dynamics, exoplanets, and fundamental astronomy</subtitle>
      <title>Hogg's Research</title>
      <updated>2012-02-14T20:52:31Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-10448119.post-8724012768392541789</id>
    <link href="http://hoggresearch.blogspot.com/feeds/8724012768392541789/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/hst-target-selection.html#comment-form" rel="replies" title="0 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/8724012768392541789" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/10448119/posts/default/8724012768392541789" rel="self" type="application/atom+xml"/>
    <link href="http://hoggresearch.blogspot.com/2012/02/hst-target-selection.html" rel="alternate" title="HST target selection" type="text/html"/>
    <title>HST target selection</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Tsalmantza and I discussed how we might winnow down our list of potentially lensed quasars into a set of sensible targets for <i>HST</i> imaging.  It is essential to look for marginal evidence of extension; that is, do the quasars depart from our expectation of point-source morphology.  A more speculative path is to look at luminosity indicators:  Are any of the quasars brighter than you would expect given line strengths and ratios, possibly indicating gravitational magnification?</p><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/10448119-8724012768392541789?l=hoggresearch.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-09T21:21:01Z</updated>
    <published>2012-02-09T04:59:00Z</published>
    <category scheme="http://www.blogger.com/atom/ns#" term="spectroscopy"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="quasar"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="talking"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="imaging"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="gravitational lensing"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="proposal"/>
    <category scheme="http://www.blogger.com/atom/ns#" term="HST"/>
    <author>
      <name>Hogg</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/18398397408280534592</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-10448119</id>
      <category term="Willman 1"/>
      <category term="clustering"/>
      <category term="merging"/>
      <category term="galaxy"/>
      <category term="PHAT"/>
      <category term="HMF"/>
      <category term="proper motion"/>
      <category term="amateur"/>
      <category term="sdss"/>
      <category term="LSST"/>
      <category term="virtual observatory"/>
      <category term="tractor"/>
      <category term="robot"/>
      <category term="funding"/>
      <category term="telescope"/>
      <category term="digital camera"/>
      <category term="meta data"/>
      <category term="proposal"/>
      <category term="disk"/>
      <category term="fundamental astronomy"/>
      <category term="roweis"/>
      <category term="classification"/>
      <category term="practice"/>
      <category term="decision"/>
      <category term="travel"/>
      <category term="linear algebra"/>
      <category term="interstellar medium"/>
      <category term="web 2.0"/>
      <category term="email"/>
      <category term="bayes"/>
      <category term="scattering"/>
      <category term="atlas"/>
      <category term="quasar"/>
      <category term="confusion"/>
      <category term="minor planet"/>
      <category term="anthropology"/>
      <category term="gravitational lensing"/>
      <category term="reading"/>
      <category term="black hole"/>
      <category term="visualization"/>
      <category term="halo"/>
      <category term="cosmology"/>
      <category term="seminar"/>
      <category term="information"/>
      <category term="2mass"/>
      <category term="chemistry"/>
      <category term="HST"/>
      <category term="gravity"/>
      <category term="panstarrs"/>
      <category term="philosophy"/>
      <category term="experiment"/>
      <category term="WMAP"/>
      <category term="sample"/>
      <category term="baryon acoustic feature"/>
      <category term="radial velocity"/>
      <category term="ukidss"/>
      <category term="dark sector"/>
      <category term="parallax"/>
      <category term="spectroscopy"/>
      <category term="brown dwarf"/>
      <category term="LTFDFCF"/>
      <category term="kinematics"/>
      <category term="cosmography"/>
      <category term="transparency"/>
      <category term="flickr"/>
      <category term="calibration"/>
      <category term="optimization"/>
      <category term="editing"/>
      <category term="star formation"/>
      <category term="ultraviolet"/>
      <category term="statistics"/>
      <category term="testing"/>
      <category term="correlation"/>
      <category term="galex"/>
      <category term="intergalactic medium"/>
      <category term="noise"/>
      <category term="computing"/>
      <category term="dissertation"/>
      <category term="citizen science"/>
      <category term="nasa"/>
      <category term="planet"/>
      <category term="wise"/>
      <category term="talking"/>
      <category term="spitzer"/>
      <category term="cluster"/>
      <category term="CDM"/>
      <category term="astrometry"/>
      <category term="environment"/>
      <category term="imaging"/>
      <category term="press"/>
      <category term="MCMC"/>
      <category term="gaia"/>
      <category term="evolution"/>
      <category term="primus"/>
      <category term="compression"/>
      <category term="phase space"/>
      <category term="relativity"/>
      <category term="weapons"/>
      <category term="archive"/>
      <category term="Solar System"/>
      <category term="Milky Way"/>
      <category term="code"/>
      <category term="observing"/>
      <category term="learning"/>
      <category term="point-spread function"/>
      <category term="Euclid"/>
      <category term="hardware"/>
      <category term="catalog"/>
      <category term="science"/>
      <category term="database"/>
      <category term="thinking"/>
      <category term="gamma-ray burst"/>
      <category term="exoplanet"/>
      <category term="white dwarf"/>
      <category term="theory"/>
      <category term="hipparcos"/>
      <category term="radio"/>
      <category term="law"/>
      <category term="pulsar"/>
      <category term="Gaussian process"/>
      <category term="osss"/>
      <category term="politics"/>
      <category term="meeting"/>
      <category term="photometry"/>
      <category term="star"/>
      <category term="not research"/>
      <category term="API"/>
      <category term="cosmic ray"/>
      <category term="substructure"/>
      <category term="post-starburst"/>
      <category term="archetype"/>
      <category term="life"/>
      <category term="time"/>
      <category term="literature"/>
      <category term="dynamics"/>
      <category term="comet"/>
      <category term="anthropic"/>
      <category term="supernova"/>
      <category term="Earth"/>
      <category term="PTF"/>
      <category term="Fermi"/>
      <category term="search"/>
      <category term="usno-b"/>
      <category term="mathematics"/>
      <category term="dust"/>
      <category term="coffee"/>
      <category term="project management"/>
      <category term="model"/>
      <category term="data"/>
      <category term="writing"/>
      <author>
        <name>Hogg</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/18398397408280534592</uri>
      </author>
      <link href="http://hoggresearch.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://hoggresearch.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/10448119/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <subtitle>galaxies, stellar dynamics, exoplanets, and fundamental astronomy</subtitle>
      <title>Hogg's Research</title>
      <updated>2012-02-14T20:52:31Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://sbseminar.wordpress.com/?p=4487</id>
    <link href="http://sbseminar.wordpress.com/2012/02/09/a-forum-on-mathematical-publishing/" rel="alternate" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/02/09/a-forum-on-mathematical-publishing/#comments" rel="replies" type="text/html"/>
    <link href="http://sbseminar.wordpress.com/2012/02/09/a-forum-on-mathematical-publishing/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">A forum on mathematical publishing</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml">There’s been lots of great discussion on the future of mathematical publishing in recent weeks, largely inspired by the boycott of Elsevier (1) (2) (3). Mostly this has been happening on blogs, particularly Tim Gower’s, but also here and a number of other places. There’s a nice index of this discussion in a wiki page [...]<img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4487&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>There’s been lots of great discussion on the future of mathematical publishing in recent weeks, largely inspired by the boycott of Elsevier (<a href="https://gowers.wordpress.com/2012/01/21/elsevier-my-part-in-its-downfall/">1</a>) (<a href="http://thecostofknowledge.com/">2</a>) (<a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf">3</a>). Mostly this has been happening on blogs, particularly Tim Gower’s, but also here and a number of other places. There’s a nice index of this discussion in <a href="http://michaelnielsen.org/polymath1/index.php?title=Journal_publishing_reform">a wiki page</a> on Michael Nielsen’s site, to the extent that it’s possible to index a discussion happening all over the internet!</p>
<p>I think a lot of people find it somewhat frustrating that this discussion is predominantly happening in blog comment threads, however. It’s hard to maintain conversations, and almost impossible to coordinate people with similar interests and concerns. Andrew Stacey and I thought that it might be helpful to set up a forum (like the <a href="http://www.math.ntnu.no/~stacey/Mathforge/nForum">nForum</a>, associated the to nCafe, or <a href="http://meta.mathoverflow.net/">meta.mathoverflow.net</a>) to alleviate this.</p>
<p>Thus, please check out <a href="http://www.math.ntnu.no/~stacey/Mathforge/Math2.0">Math 2.0</a>! We’ll see what sticks. :-)</p>
<p>Our hope is that this might provide a better home for more focused discussion, and a place for people who want to coordinate concrete next steps in reforming mathematical publishing. Come in and join us!</p>
<br/>  <a href="http://feeds.wordpress.com/1.0/gocomments/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/comments/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/delicious/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/gofacebook/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/facebook/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/gotwitter/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/twitter/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/stumble/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/godigg/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/digg/sbseminar.wordpress.com/4487/"/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/sbseminar.wordpress.com/4487/" rel="nofollow"><img alt="" border="0" src="http://feeds.wordpress.com/1.0/reddit/sbseminar.wordpress.com/4487/"/></a> <img alt="" border="0" height="1" src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=4487&amp;subd=sbseminar&amp;ref=&amp;feed=1" width="1"/></div>
    </content>
    <updated>2012-02-09T20:21:45Z</updated>
    <published>2012-02-09T20:19:37Z</published>
    <category scheme="http://sbseminar.wordpress.com" term="elsevier"/>
    <category scheme="http://sbseminar.wordpress.com" term="publishing"/>
    <category scheme="http://sbseminar.wordpress.com" term="websites"/>
    <author>
      <name>Scott Morrison</name>
      <uri>http://tqft.net/</uri>
    </author>
    <source>
      <id>http://sbseminar.wordpress.com/feed/atom/</id>
      <link href="http://sbseminar.wordpress.com" rel="alternate" type="text/html"/>
      <link href="http://sbseminar.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <link href="http://sbseminar.wordpress.com/osd.xml" rel="search" title="Secret Blogging Seminar" type="application/opensearchdescription+xml"/>
      <link href="http://wordpress.com/opensearch.xml" rel="search" title="WordPress.com" type="application/opensearchdescription+xml"/>
      <link href="http://sbseminar.wordpress.com/?pushpress=hub" rel="hub" type="text/html"/>
      <subtitle xml:lang="en">Representation theory, geometry and whatever else we decide is worth writing about today.</subtitle>
      <title xml:lang="en">Secret Blogging Seminar</title>
      <updated>2012-02-14T21:21:39Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://asymptotia.com/?p=11191</id>
    <link href="http://asymptotia.com/2012/02/07/incomplete-subtractions/" rel="alternate" type="text/html"/>
    <link href="http://asymptotia.com/2012/02/07/incomplete-subtractions/#comments" rel="replies" type="text/html"/>
    <link href="http://asymptotia.com/2012/02/07/incomplete-subtractions/feed/atom/" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">Incomplete Subtractions</title>
    <summary type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://asymptotia.com/wp-images/2012/02/three_subtraction_studies_6_feb_2012_small.jpg"><img alt="" class="alignright size-full wp-image-11192" src="http://asymptotia.com/wp-images/2012/02/three_subtraction_studies_6_feb_2012_small.jpg" title="three_subtraction_studies_6_feb_2012_small" width="499"/></a>


Well, it has been well over two months since I popped into the studio I sometimes visit to to a "drop in and draw" session. (I've spoken about the value of such practice here <a href="http://asymptotia.com/2011/01/28/nude/">before</a>.)  Although I've been drawing a bit here and there on the bus and subway to keep practicing, and also doing some work on some pages of <a href="http://asymptotia.com/the-project/">The Project</a> (actually, some pretty detailed finish work on a few pages I'm quite happy with), I was not sure whether I'd have the right chops to do a good job at the session, and expected that if I went I'd have a frustrating -but of course valuable- evening of knocking off some rust  and oiling the wheels again. So I went along yesterday.


 Strangely, it felt like it was going to be a good session  as I approached, and as I settled down and began to try to capture the 2 minute poses, and then the 5 minute poses, I felt like I was flowing along pretty well. It helped that the model on duty  is  [...]</div>
    </summary>
    <updated>2012-02-09T18:24:43Z</updated>
    <published>2012-02-08T07:56:57Z</published>
    <category scheme="http://asymptotia.com" term="art"/>
    <category scheme="http://asymptotia.com" term="craft"/>
    <category scheme="http://asymptotia.com" term="Los Angeles"/>
    <category scheme="http://asymptotia.com" term="personal"/>
    <category scheme="http://asymptotia.com" term="sketches"/>
    <category scheme="http://asymptotia.com" term="work"/>
    <author>
      <name>Clifford</name>
      <uri>http://asymptotia.com</uri>
    </author>
    <source>
      <id>http://asymptotia.com/feed/atom/</id>
      <link href="http://asymptotia.com" rel="alternate" type="text/html"/>
      <link href="http://asymptotia.com/feed/atom/" rel="self" type="application/atom+xml"/>
      <title xml:lang="en">Asymptotia</title>
      <updated>2012-02-14T20:53:49Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>tag:golem.ph.utexas.edu,2012:%2Fcategory%2F3.2496</id>
    <link href="http://golem.ph.utexas.edu/category/2012/02/the_moduli_3stack_of_the_cfiel.html" rel="alternate" type="application/xhtml+xml"/>
    <title type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><em>The Moduli 3-Stack of the C-Field</em></div>
    </title>
    <summary xml:lang="en">An article discussing the moduli 3-stack of the C-field in 11-dimensional supergravity.</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img alt="MathML-enabled post (click for more details)." class="mathlogo" src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" title="MathML-enabled post (click for details)."/></a></div>

<p>We are in the process of finalizing a little article</p>

<p>Domenico Fiorenza, Hisham Sati, U.S.,  <em><strong><a href="http://ncatlab.org/schreiber/show/The%20moduli%203-stack%20of%20the%20C-field">The <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><msub><mi>E</mi> <mn>8</mn></msub></math> moduli 3-stack of the C-field in M-theory</a></strong></em></p>

<p><strong>Abstract</strong> The higher <a href="http://ncatlab.org/nlab/show/gauge+theory">gauge field</a> in <a href="http://ncatlab.org/nlab/show/11-dimensional+supergravity">11-dimensional supergravity</a> – the <a href="http://ncatlab.org/nlab/show/supergravity+C-field">C-field</a> – is constrained by quantum effects 
to be a <a href="http://ncatlab.org/nlab/show/cocycle">cocycle</a> in some <a href="http://ncatlab.org/nlab/show/twisted+cohomology">twisted</a> version of <a href="http://ncatlab.org/nlab/show/ordinary+differential+cohomology">ordinary differential cohomology</a>. We argue that it should indeed be a cocycle in a certain 
<a href="http://ncatlab.org/nlab/show/twisted+differential+c-structure">twisted nonabelian differential cohomology</a>. 
We give a simple and natural characterization of the full 
<a href="http://ncatlab.org/nlab/show/smooth+infinity-groupoid">smooth</a> <a href="http://ncatlab.org/nlab/show/moduli+stack">moduli 3-stack</a> of configurations of the <a href="http://ncatlab.org/nlab/show/supergravity+C-field">C-field</a>, the field of <a href="http://ncatlab.org/nlab/show/gravity">gravity</a> and the (auxiliary) <a href="http://ncatlab.org/nlab/show/E8">E8</a>-<a href="http://ncatlab.org/nlab/show/Yang-Mills+field">Yang-Mills field</a>.
We show that the <a href="http://ncatlab.org/nlab/show/truncated+object">truncation</a> of this moduli 3-stack to a <a href="http://ncatlab.org/nlab/show/discrete+infinity-groupoid">bare 1-groupoid</a> of field configurations reproduces the differential integral <a href="http://ncatlab.org/nlab/show/twisted+Wu+structure">Wu structures</a> that Hopkins-Singer had shown (<a href="http://ncatlab.org/nlab/show/Quadratic+Functions+in+Geometry,+Topology,+and+M-Theory">HS02</a>) to formalize Witten’s argument (<a href="http://arxiv.org/abs/hep-th/9609122">Wi96</a>) on the nature of the C-field. Finally we give a similarly simple and natural characterization of the moduli 2-stack of boundary C-field configurations and show that it is equivalent to the <a href="http://ncatlab.org/nlab/show/smooth+infinity-groupoid">smooth</a> <a href="http://ncatlab.org/nlab/show/moduli+stack">moduli 2-stack</a> of <a href="http://ncatlab.org/nlab/show/Green-Schwarz+mechanism">anomaly free</a> <a href="http://ncatlab.org/nlab/show/heterotic+string+theory">heterotic supergravity</a> field configurations (<a href="http://ncatlab.org/schreiber/show/Twisted+Differential+String+and+Fivebrane+Structures">SSS12</a>).</p>

<p>This may be read as a companion to the article that I mentioned last time, at <a href="http://golem.ph.utexas.edu/category/2012/01/multiple_m5branes_string_2conn.html">Multiple M5-branes, String 2-connections, and  7d  nonabelian   Chern-Simons theory</a></p>

<math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mspace width="thinmathspace"/></math>

<p>A pdf of the article is behind the <a href="http://ncatlab.org/schreiber/show/The%20moduli%203-stack%20of%20the%20C-field">above link</a>. Any comment you might have would be most welcome.</p></div>
    </content>
    <updated>2012-02-09T17:59:31Z</updated>
    <published>2012-02-09T09:11:46Z</published>
    <category term="Math"/>
    <author>
      <name>urs</name>
      <email>urs.schreiber@math.uni-hamburg.de</email>
      <uri>http://www.math.uni-hamburg.de/home/schreiber</uri>
    </author>
    <source>
      <id>tag:golem.ph.utexas.edu,2006:nCategoryCafe/3</id>
      <icon>http://golem.ph.utexas.edu/category/images/favicon.ico</icon>
      <link href="http://golem.ph.utexas.edu/category/" rel="alternate" type="application/xhtml+xml"/>
      <link href="http://golem.ph.utexas.edu/category/atom10.xml" rel="self" type="application/atom+xml"/>
      <link href="http://golem.ph.utexas.edu/category/comments.atom" rel="replies" type="application/atom+xml"/>
      <rights xml:lang="en">Copyright (c) 2012, The n-Category Collective</rights>
      <subtitle xml:lang="en">A group blog on math, physics and philosophy</subtitle>
      <title xml:lang="en">The n-Category Café</title>
      <updated>2012-02-14T21:19:22Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.science20.com/86826 at http://www.science20.com</id>
    <link href="http://www.science20.com/quantum_diaries_survivor/top_quark_production_studied_detail-86826" rel="alternate" type="text/html"/>
    <title>Top Quark Production Studied In Detail</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">A new result by the CMS collaboration has been produced today on top quark physics. For those of you who only get triggered by the search of new particles or new forces, the study of "yesterday's signals", such as top quarks, is boring and uninformative; but high-energy physics is a rich field of research, and we extend our understanding of subnuclear physics no less by getting to know how exactly top quarks get produced in proton-proton collisions, than we do by placing limits on ephemeral particles (SUSY ones, e.g.).<br/><br/>So I salute the new measurement as an important advance. Using over one inverse femtobarn of data collected in 2011 (about a hundred trillion proton-proton collisions), CMS was able to study top quark pairs in great detail. <br/>

<p><a href="http://www.science20.com/quantum_diaries_survivor/top_quark_production_studied_detail-86826" target="_blank">read more</a></p></div>
    </summary>
    <updated>2012-02-09T15:08:20Z</updated>
    <category scheme="http://www.science20.com/physics" term="Physics"/>
    <author>
      <name>dorigo</name>
    </author>
    <source>
      <id>http://www.science20.com/quantum_diaries_survivor</id>
      <link href="http://www.science20.com/quantum_diaries_survivor" rel="alternate" type="text/html"/>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor/feed" rel="self" type="application/rss+xml"/>
      <subtitle>Science 2.0® - Science for the next 2,000 years</subtitle>
      <title>dorigo's blog</title>
      <updated>2012-02-15T04:45:03Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://www.scottaaronson.com/blog/?p=912</id>
    <link href="http://www.scottaaronson.com/blog/?p=912" rel="alternate" type="text/html"/>
    <link href="http://www.scottaaronson.com/blog/?p=912#comments" rel="replies" type="text/html"/>
    <link href="http://www.scottaaronson.com/blog/?feed=atom&amp;p=912" rel="replies" type="application/atom+xml"/>
    <title xml:lang="en">The battle against Elsevier gains momentum</title>
    <summary xml:lang="en">Check out this statement on “The Cost of Knowledge” released today, which (besides your humble blogger) has been signed by Ingrid Daubechies (President of the International Mathematical Union), Timothy Gowers, Terence Tao, László Lovász, and 29 others.  The statement carefully explains the rationale for the current Elsevier boycott, and answers common questions like “why single [...]</summary>
    <content type="xhtml" xml:lang="en"><div xmlns="http://www.w3.org/1999/xhtml"><p>Check out this <a href="http://gowers.files.wordpress.com/2012/02/elsevierstatementfinal.pdf">statement on “The Cost of Knowledge” released today</a>, which (besides your humble blogger) has been signed by Ingrid Daubechies (President of the International Mathematical Union), Timothy Gowers, Terence Tao, László Lovász, and 29 others.  The statement carefully explains the rationale for the current Elsevier boycott, and answers common questions like “why single out Elsevier?” and “what comes next?”</p>
<p>Also check out <a href="http://gowers.wordpress.com/2012/02/08/a-more-formal-statement-about-mathematical-publishing/#more-3986">Timothy Gowers’ blog post</a> announcing the statement.  The post includes a hilarious report by investment firm Exane Paribas, explaining that the current boycott has caused Reed Elsevier’s stock price to fall, but presenting that as a <em>great investment opportunity</em>, since they fully expect the price to rebound once this boycott fails like all the previous ones.  I ask you: does that not want to make you boycott Elsevier, <em>for no other reason than to see the people who follow Exane Paribas’ cynical advice lose their money?</em></p>
<p>In related news, the <a href="http://thecostofknowledge.com/">boycott petition</a> now has 4600+ signatures and counting.  If you’ve already signed, great!  If you haven’t, why not?</p>
<p><span style="color: #ff0000;"><strong>Update (Feb. 9):</strong></span> There’s now a <a href="http://www.bostonglobe.com/opinion/2012/02/12/why-scientists-are-boycotting-publisher/9sCpDEP7BkkX1INfakn3NL/story.html">great editorial</a> by Gareth Cook in the <em>Boston Globe</em> supporting the Elsevier boycott (and analogizing it to both the Tahrir Square uprising and the Boston Tea Party!).</p></div>
    </content>
    <updated>2012-02-09T13:33:59Z</updated>
    <published>2012-02-08T17:54:51Z</published>
    <category scheme="http://www.scottaaronson.com/blog" term="Announcements"/>
    <category scheme="http://www.scottaaronson.com/blog" term="Nerd Interest"/>
    <category scheme="http://www.scottaaronson.com/blog" term="Rage Against Doofosity"/>
    <author>
      <name>Scott</name>
      <uri>http://www.scottaaronson.com</uri>
    </author>
    <source>
      <id>http://www.scottaaronson.com/blog/?feed=atom</id>
      <link href="http://www.scottaaronson.com/blog" rel="alternate" type="text/html"/>
      <link href="http://www.scottaaronson.com/blog/?feed=atom" rel="self" type="application/atom+xml"/>
      <subtitle xml:lang="en">The Blog of Scott Aaronson</subtitle>
      <title xml:lang="en">Shtetl-Optimized</title>
      <updated>2012-02-13T03:16:48Z</updated>
    </source>
  </entry>

  <entry>
    <id>tag:blogger.com,1999:blog-22973357.post-5505720402002382927</id>
    <link href="http://backreaction.blogspot.com/feeds/5505720402002382927/comments/default" rel="replies" title="Post Comments" type="application/atom+xml"/>
    <link href="http://www.blogger.com/comment.g?blogID=22973357&amp;postID=5505720402002382927" rel="replies" title="12 Comments" type="text/html"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/5505720402002382927" rel="edit" type="application/atom+xml"/>
    <link href="http://www.blogger.com/feeds/22973357/posts/default/5505720402002382927" rel="self" type="application/atom+xml"/>
    <link href="http://backreaction.blogspot.com/2012/02/when-i-grow-up-i-want-to-be-physicist.html" rel="alternate" title="When I grow up I want to be a physicist" type="text/html"/>
    <title>When I grow up I want to be a physicist</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://2.bp.blogspot.com/_ws8XY4ubvXg/Ss3yv_A345I/AAAAAAAAAyo/qLoKdbDUkn0/s200/scarecrow.png"><img alt="" border="0" src="http://2.bp.blogspot.com/_ws8XY4ubvXg/Ss3yv_A345I/AAAAAAAAAyo/qLoKdbDUkn0/s200/scarecrow.png" style="float: right; margin: 0 0 10px 10px; cursor: pointer; cursor: hand; width: 196px; height: 200px;"/></a>The other day I talked to a young women who is about to finish high school, so the time is coming to decide what education to pursue after that. What does a theoretical physicist actually do?, she asked. And while I was babbling away, I recalled how little I knew myself what a physicist does when I was a young student.<br/><br/>Of course I knew that professors give lectures. And I had read a bunch of popular science books and biographies, from which I concluded that theoretical physics requires a lot of thinking. The physicists I had read about, they also wrote many books, and articles and, most of all, letters. They really wrote a lot of letters, these people. There also was the occasional mentioning of a conference, where talks had to be given. And I could have learned from these historical narratives that, even back then, the physicists moved a lot, but I blamed that on one or the other war. I never asked who organized these conferences or hired these people.<br/><br/>While one could say that my family is scientifically minded, when I grew up I didn't know anybody who worked in scientific research or in academia who I could have asked what their daily life looks like. Today, it is easier for young people with an interest in science to find out what a profession entails in practice, and if you are thinking about a career in science, I really encourage you too look around. <a href="http://www.phdcomics.com/">Piled higher and deeper</a> has documented the sufferings of PhD students as humorously as aptly, and postdocs from many areas of science write blogs. When I finished high school, I didn't even know what a postdoc is! At the higher career levels, bloggers are still sparse, but they are there, and they tell you what theoretical physicists do.<br/><br/>Yes, they give lectures. They also give seminars, and attend seminars. They write articles and read articles, and review articles. They also write the occasional book, though that isn't very common in the early career stages. They attend conferences and workshops, and also organize conferences and workshops. They travel a lot. They sit in committees for all sorts of organizational and administrational purposes.<br/><br/>To some extend, the books I had read contained a little of all of that. What they did not tell me anything about was one thing that theoretical physicists today spend a lot of time on: writing proposals. They write and write and write proposals, to fund their own research or their research group, their students and postdocs, or their conferences, or maybe just their own book, or long-term stays. If you want to be a theoretical physicist, you better get used to the idea that a big part of your job will consist of asking for money, again and again and again. And then, somebody also has to review these proposals...<br/><br/>You will not be surprised to hear that theoretical physicists do no longer write a lot of letters. I don't know how their email frequency compares to that of the general population, but this touches on one aspect of research in theoretical physics that you read about very, very little on blogs. That is how tightly knit the community really is, and how much people talk to each other and exchange ideas.<br/><br/>At least on the blogs that I read, it's like an unwritten code. You don't blog about conversations with your peers, except possibly under special circumstances (like for an interview). Most of these conversations are considered private and sharing inappropriate, even if confidentiality was not explicitly asked for. I think this is good because there needs to be room for privacy. However, this might give the reader a somewhat distorted picture of what research looks like. It is really a lot about exchanging ideas, it is a lot about asking questions, and about building up on other people's argument. A lot of research is communication with colleagues. So, if you try to catch a taste of theoretical physics from reading blogs, keep in mind that most bloggers will not pull their nonblogging colleagues into a public discussion.<br/><br/>Oh, yes, and in the remaining time - the time not spent on reading papers, sitting in seminars, organizing conferences or writing proposals or reports or blogging - in that time, they think.<br/><br/>If you are considering to become a scientist: Check out this <a href="http://lookslikescience.tumblr.com/">wonderful tumblr site that shows you some photos of real scientists!</a><div class="blogger-post-footer"><img alt="" height="1" src="https://blogger.googleusercontent.com/tracker/22973357-5505720402002382927?l=backreaction.blogspot.com" width="1"/></div></div>
    </content>
    <updated>2012-02-09T10:03:08Z</updated>
    <published>2012-02-09T10:02:00Z</published>
    <author>
      <name>Bee</name>
      <email>noreply@blogger.com</email>
      <uri>http://www.blogger.com/profile/06151209308084588985</uri>
    </author>
    <source>
      <id>tag:blogger.com,1999:blog-22973357</id>
      <category term="Sociology of Science"/>
      <category term="This and That"/>
      <category term="Particle Physics"/>
      <category term="Physics"/>
      <category term="Useless Knowledge"/>
      <category term="Philosophy"/>
      <category term="Photo"/>
      <category term="Distraction"/>
      <category term="Art"/>
      <category term="Quantum Gravity"/>
      <category term="Academia"/>
      <category term="Comic"/>
      <category term="Science"/>
      <category term="Peer Review"/>
      <category term="Poll"/>
      <category term="Papers"/>
      <category term="Psychology"/>
      <category term="Politics"/>
      <category term="Germany"/>
      <category term="Baby"/>
      <category term="History of Science"/>
      <category term="Travel"/>
      <category term="Infotainment"/>
      <category term="Biology"/>
      <category term="Science and Society"/>
      <category term="Interna"/>
      <category term="Physicists"/>
      <category term="Random Thoughts"/>
      <category term="Canada"/>
      <category term="Humor"/>
      <category term="Astrophysics"/>
      <category term="Video"/>
      <category term="Blog"/>
      <category term="Books"/>
      <author>
        <name>Bee</name>
        <email>noreply@blogger.com</email>
        <uri>http://www.blogger.com/profile/06151209308084588985</uri>
      </author>
      <link href="http://backreaction.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default" rel="self" type="application/atom+xml"/>
      <link href="http://backreaction.blogspot.com/" rel="alternate" type="text/html"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <link href="http://www.blogger.com/feeds/22973357/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <title>Backreaction</title>
      <updated>2012-02-14T21:31:23Z</updated>
    </source>
  </entry>

  <entry xml:lang="en">
    <id>http://scienceblogs.com/catdynamics/2012/02/i_have_never_seen_a_purple_squ.php</id>
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/cp6V2lQ5mNA/i_have_never_seen_a_purple_squ.php" rel="alternate" type="text/html"/>
    <title>I have never seen a purple squirrel...</title>
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>but now I hope to see one:</p> <a href="http://scienceblogs.com/catdynamics/2012/02/i_have_never_seen_a_purple_squ.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2012/02/i_have_never_seen_a_purple_squ.php#commentsArea">Read the comments on this post...</a><img height="1" src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/cp6V2lQ5mNA" width="1"/></div>
    </summary>
    <updated>2012-02-09T05:59:37Z</updated>
    <category term="random"/>
    <source>
      <id>http://scienceblogs.com/catdynamics/</id>
      <author>
        <name>Steinn Sigurðsson</name>
      </author>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate" type="text/html"/>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub" type="text/html"/>
      <rights>Copyright 2012</rights>
      <subtitle>Speculations on astronomy, astrophysics, news I find interesting, theoretical issues, science and science policy.  
I will digress into computational physics, science fiction and general issues and basically whatever I feel like whenever. 
And, of course, cats.</subtitle>
      <title>Dynamics of Cats</title>
      <updated>2012-02-14T17:08:27Z</updated>
    </source>
  </entry></feed>

