<?xml version="1.0"?>
<feed xmlns:planet="http://planet.intertwingly.net/" xmlns:indexing="urn:atom-extension:indexing" xmlns="http://www.w3.org/2005/Atom" indexing:index="no">
  <title>Planet Musings</title>
  <updated>2009-11-07T19:25:26-06:00</updated>
  <generator uri="http://github.com/rubys/mars/tree/master">Mars</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>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://diracseashore.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>dberenstein</name>
						
      <uri>http://www.physics.ucsb.edu/People/person.php3?userid=dberens</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">A first time ever</div>
    </title>
		
    <link href="http://diracseashore.wordpress.com/2009/11/04/a-first-time-ever/" rel="alternate" type="text/html"/>
		
    <id>http://diracseashore.wordpress.com/?p=1642</id>
		
    <updated>2009-11-08T00:32:29+00:00</updated>
		
    <published>2009-11-04T22:08:17+00:00</published>
		
    <category term="Academia" scheme="http://diracseashore.wordpress.com/"/>
    <category term="Santa Barbara" scheme="http://diracseashore.wordpress.com/"/>
    <category term="science and society" scheme="http://diracseashore.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Yesterday night I attended a reception for the international scholars to UCSB. This was the first time that such a celebration took place in Santa Barbara, thanks to an anonymous donor. It was a lively event, and various important people from the UCSB campus showed up. I won’t bore you with the details.
Amongst the interesting [...]<img src="http://stats.wordpress.com/b.gif?host=diracseashore.wordpress.com&amp;blog=4754772&amp;post=1642&amp;subd=diracseashore&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://diracseashore.wordpress.com/2009/11/04/a-first-time-ever/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>Yesterday night I attended a reception for the international scholars to UCSB. This was the first time that such a celebration took place in Santa Barbara, thanks to an anonymous donor. It was a lively event, and various important people from the UCSB campus showed up. I won’t bore you with the details.</p>
<p>Amongst the interesting facts that I collected yesterday, was that most international students in the US come to study in the science and technology fields, while very few people from the US go out to study and when they do, the statistic is mostly on humanities. I also found out that there are about 640000 students from abroad in US Universities, and that US Universities graduate about 30000 PhD’s annually.</p>
<p>Not surprisingly, current cuts in US University funding (especially state Universities) will hurt the efforts to get the best (graduate) students to the US, with the consequent deterioration of the pool of people with talent contributing to the US economy. An interesting article regarding this issue can be found <a href="http://www.techcrunch.com/2009/08/23/foreigners-attending-us-grad-schools-way-down-wake-up-xenophobes/">here</a>.</p>
<p>If you couple all of this progressive <a href="http://www.nytimes.com/2009/11/01/education/edlife/01public-t.html?ref=education">lack of investment by the states into the education system</a>, the future starts looking pretty bad, not just for education, but for the US economy.</p>
<p>This year I am working on a University committee in charge of international education. So I have to learn quite a bit about this stuff.</p>
<p>Simple observation: if you lose <span style="text-decoration:line-through;">loose </span> the people from abroad (who are extremely good students), and you lose <span style="text-decoration:line-through;">loose</span> the local people (because they can not afford to go to school any longer), where is the human capital investment in the future development of technology going to come from?</p>
<p>Remember, modern economies depend on having the best and most innovative modern technology in order to compete. And, new ideas for technology come from people who know what the current technologies are, what they can do and how to make them. Ideas are not born from thin air.</p>
Posted in Academia, Santa Barbara, science and society  <a href="http://feeds.wordpress.com/1.0/gocomments/diracseashore.wordpress.com/1642/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/comments/diracseashore.wordpress.com/1642/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/diracseashore.wordpress.com/1642/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/delicious/diracseashore.wordpress.com/1642/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/diracseashore.wordpress.com/1642/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/stumble/diracseashore.wordpress.com/1642/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godigg/diracseashore.wordpress.com/1642/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/digg/diracseashore.wordpress.com/1642/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/diracseashore.wordpress.com/1642/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/reddit/diracseashore.wordpress.com/1642/" border="0" alt=""/></a> <img src="http://stats.wordpress.com/b.gif?host=diracseashore.wordpress.com&amp;blog=4754772&amp;post=1642&amp;subd=diracseashore&amp;ref=&amp;feed=1" border="0" alt=""/></div></div>
    </content>
		
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		<thr:total>5</thr:total>
	
    <source>
      <title type="text">Shores of the Dirac Sea</title>
      <subtitle type="text">A blog about physics... mostly.</subtitle>
      <updated>2009-11-08T00:32:29+00:00</updated>
      <generator uri="http://wordpress.com/">WordPress.com</generator>
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  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://diracseashore.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>dberenstein</name>
						
      <uri>http://www.physics.ucsb.edu/People/person.php3?userid=dberens</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Zurich in the summer</div>
    </title>
		
    <link href="http://diracseashore.wordpress.com/2009/09/15/zurich-in-the-summer/" rel="alternate" type="text/html"/>
		
    <id>http://diracseashore.wordpress.com/?p=1617</id>
		
    <updated>2009-11-08T00:28:25+00:00</updated>
		
    <published>2009-09-15T20:15:08+00:00</published>
		
    <category term="Conferences" scheme="http://diracseashore.wordpress.com/"/>
    <category term="string theory" scheme="http://diracseashore.wordpress.com/"/>
    <category term="travel" scheme="http://diracseashore.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">I have just attended the XV European Workshop on String Theory. It took place in Zürich, Switzerland. Here is the link to the conference information and the talk slides. The conference featured a lot of young speakers who I had not met before. I found it very entertaining. Curiously enough, I really got to feel [...]<img src="http://stats.wordpress.com/b.gif?host=diracseashore.wordpress.com&amp;blog=4754772&amp;post=1617&amp;subd=diracseashore&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://diracseashore.wordpress.com/2009/09/15/zurich-in-the-summer/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>I have just attended the XV European Workshop on String Theory. It took place in Zürich, Switzerland. Here is the link to the <a href="http://www.phys.ethz.ch/~swood/stringworkshop/index.html">conference information</a> and the <a href="http://www.phys.ethz.ch/~swood/stringworkshop/program.html">talk slides</a>. The conference featured a lot of young speakers who I had not met before. I found it very entertaining. Curiously enough, I really got to feel for the first time that different countries have their own way of doing physics. I think this reflects a bit on the attitudes of different cultures on what constitutes good taste. There is nothing wrong per se with any such preferences, it’s just an observation that I have heard many times before, but it had not really made itself so obvious to me as this time around. The menu of topics covered was rather formal and the hospitality of the event was incredible. I’m very grateful to Matthias and Matthias for providing such a welcoming environment. Here is a picture of Zürich (the best of the ones I took while wandering aimlessly through the streets of the city).</p>
<p><a href="http://diracseashore.files.wordpress.com/2009/09/zurichskyline.jpg"><img title="Zurichskyline" class="alignleft size-full wp-image-1619" src="http://diracseashore.files.wordpress.com/2009/09/zurichskyline.jpg?w=500&amp;h=375" height="375" alt="Zurichskyline" width="500"/></a></p>
<p>The weather was absolutely perfect and the town is truly a lovely place to loose oneself into.</p>
<p><span id="more-1617"/></p>
<p>Now, I’ll tell you a few anecdotes that happen occasionally to us, poor saps, who travel across the globe and find ourselves fighting this mysterious ailment called jet-lag. In particular, this is a story about myself.</p>
<p>I arrived at my hotel at about seven in the evening, not having slept well from the transatlantic flight from Los Angeles to Europe. I register and manage to get one or two hours of sleep. I woke up to the sound of the bells of the near clock tower at about 10 pm. Here is a picture, with a lovely moon casting its light on it.</p>
<p> </p><div class="wp-caption alignleft" id="attachment_1620" style="width: 510px"><a href="http://diracseashore.files.wordpress.com/2009/09/zurichclock.jpg"><img title="ZurichClock" class="size-full wp-image-1620" src="http://diracseashore.files.wordpress.com/2009/09/zurichclock.jpg?w=500&amp;h=666" height="666" alt="A machine for keeping people awake, that also manages to keep the time very well" width="500"/></a><p class="wp-caption-text">A machine for keeping people awake, that also manages to keep the time very well</p></div>
<p>It was a lovely bell tower with a beautiful clock and a rather loud set of bells. It rang every fifteen minutes. At the hour and fifteen it gave a short cry. At the hour and thirty, the cry of the bells was twice as long, and at forty five minutes it was three times as long. When the full hour came, it went extra long, and it finished with a lower rounder bell sound counting the hours. The clock rang all… night… long… My room was facing it directly.</p>
<p>Needless to say, first day of the conference, I was not better than a walking zombie. I’m sure you could hear me saying <em>brains… brains… branes…</em></p>
<p>The second night, it was the same again. I couldn’t hold it past four in the afternoon, and after taking a nap, I woke at 10 pm again and couldn’t sleep a wink at night. Fortunately, I used the time wisely to prepare my talk. By the third night, I forced myself to stay awake and after a nice dinner organized by the conference and a little bit of wine, I finally slept a whole night and was alert the next day. The bells never bothered me again.</p>
<p>Of course, we all laughed together at the episode and I received various pieces of advice on how to improve the success of a 9 hour change of schedule for my body.</p>
<p>Another interesting thing to notice is the price of items. Europe has become expensive, but Switzerland is much more so than other places in Europe. Fortunately, some items are much cheaper than in the US. Ordering wine at restaurants is much more common, and the markup is not as high as in the US. So if one is trying to have a good time, the food costs more, and the wine costs less, so one can balance the two against each other. There are also these coins of 5 CHF. Big coins at that. You get a lot of them in change. And one shouldn’t leave them behind. If one is not paying attention, it is a lot of money in coins. They have a nice solid weight to them, so your pockets notice the extra effort they have to make. This fact alone should give you an idea of the value of items. In the US, people don’t even like using one dollar coins. If they get them in change they collect them. I never understood why they don’t circulate much.</p>
<p>Finally, the Swiss train system is very nice, and dense. This made me think of all of Einstein’s special relativity trains running at great speeds in various directions and I can definitely see where his obsession with clocks and synchronization came from. I experienced them first hand: both the clocks, and the synchronization of events.</p>
Posted in Conferences, string theory, travel  <a href="http://feeds.wordpress.com/1.0/gocomments/diracseashore.wordpress.com/1617/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/comments/diracseashore.wordpress.com/1617/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/diracseashore.wordpress.com/1617/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/delicious/diracseashore.wordpress.com/1617/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/diracseashore.wordpress.com/1617/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/stumble/diracseashore.wordpress.com/1617/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godigg/diracseashore.wordpress.com/1617/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/digg/diracseashore.wordpress.com/1617/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/diracseashore.wordpress.com/1617/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/reddit/diracseashore.wordpress.com/1617/" border="0" alt=""/></a> <img src="http://stats.wordpress.com/b.gif?host=diracseashore.wordpress.com&amp;blog=4754772&amp;post=1617&amp;subd=diracseashore&amp;ref=&amp;feed=1" border="0" alt=""/></div></div>
    </content>
		
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		<thr:total>6</thr:total>
	
    <source>
      <title type="text">Shores of the Dirac Sea</title>
      <subtitle type="text">A blog about physics... mostly.</subtitle>
      <updated>2009-11-08T00:32:29+00:00</updated>
      <generator uri="http://wordpress.com/">WordPress.com</generator>
      <link href="http://diracseashore.wordpress.com/" rel="alternate" type="text/html"/>
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  </entry>

  <entry xml:lang="en">
    
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">MathML in Webkit</div>
    </title>
    
    <link href="http://golem.ph.utexas.edu/~distler/blog/archives/002105.html" rel="alternate" type="application/xhtml+xml"/>
    
    <updated>2009-11-08T00:03:26+00:00</updated>
    
    <published>2009-11-04T11:23:44-06:00</published>
    
    <id>tag:golem.ph.utexas.edu,2009:%2F~distler%2Fblog%2F1.2105</id>
    
    <summary type="text">Thanks to Alex Milowski</summary>
    
    <author>
      
      <name>distler</name>
      
      <uri>http://golem.ph.utexas.edu/~distler/blog/</uri>
      
      <email>distler@golem.ph.utexas.edu</email>
    
    </author>
    
    <category term="MathML"/>
    
    <content type="xhtml" xml:base="http://golem.ph.utexas.edu/~distler/blog/archives/002105.html">
      <div xmlns="http://www.w3.org/1999/xhtml">
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>

<p>There was a discussion about <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/">displaying math on the web</a>, over at Terry Tao’s blog. It was a little disheartening to learn where most peoples’ heads are at, in that regard. Many seems to be excited at the mere prospect of <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/#comment-42138">creating a web service</a> that would turn TeX equations into pictures. Such services are not exactly <a href="http://s2.wordpress.com/latex.php?latex=%5Cint_%7B-%5Cinfty%7D%5E%5Cinfty%20e%5E%7B-x%5E2%7D%20dx%20=%20%5Csqrt%7B%5Cpi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0">thin on the ground</a>, I <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/#comment-42143">retorted</a>, but hardly satisfactory, either. Fortunately, an actual <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/#comment-42119">blind user</a> showed up to explain at least <em>one reason</em> why that wasn’t the answer.</p>

<p>Still, being told, “You should use <acronym title="Mathematical Markup Language">MathML</acronym>.” is like being told, “Eat your vegetables.” and is just about as likely to be heeded.</p>

<p>One objection is the lack of browser support, which – these days – means that neither Opera, nor Webkit browsers (Safari, Chrome, …) support <acronym>MathML</acronym>. The latter, however, seems to be changing. There’s a <a href="http://trac.webkit.org/wiki/MathML%20Goals">plan</a> and, more importantly, there’s actually been <a href="https://bugs.webkit.org/show_bug.cgi?id=29158">code</a>  <a href="https://bugs.webkit.org/show_bug.cgi?id=29143">checked</a>  <a href="https://bugs.webkit.org/show_bug.cgi?id=29349">into</a>  <a href="https://bugs.webkit.org/show_bug.cgi?id=29529">trunk</a>.</p>

<p>Of course, it’s far too early to expect anything usable, but if Alex wants to prioritize, here’s a table of <acronym>MathML</acronym> elements and attributes used by <a href="http://golem.ph.utexas.edu/~distler/blog/itex2MML.html">itex2MML</a>. Things that aren’t yet supported by his patches are marked in bold.</p>

<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<div style="overflow:auto;">
<table class="plaintable" summary="Elements and attributes unimplemented in WebKit are marked in bold" style="width:35em;">
<caption>Presentational <acronym>MathML</acronym> Elements used in itex2MML</caption>
<thead>
<tr><th scope="col">Element</th><th scope="col">Attributes</th></tr>
</thead>
<tbody>
<tr><td>math</td><td>display</td></tr>
<tr><td>mi</td><td><b>mathvariant</b></td></tr>
<tr><td>mn</td><td/></tr>
<tr><td>mo</td><td><b>maxsize minsize lspace rspace stretchy</b></td></tr>
<tr><td>mrow</td><td><b>xmlns:xlink xlink:type xlink:href</b></td></tr>
<tr><td>mover</td><td/></tr>
<tr><td>munder</td><td/></tr>
<tr><td>munderover</td><td/></tr>
<tr><td>msub</td><td/></tr>
<tr><td>msup</td><td/></tr>
<tr><td>msubsup</td><td/></tr>
<tr><td><b>maction</b></td><td><b>actiontype( = toggle, statusline, tooltip)</b></td></tr>
<tr><td>mphantom</td><td/></tr>
<tr><td><b>mpadded</b></td><td><b>width lspace</b></td></tr>
<tr><td><b>mspace</b></td><td><b>height depth width</b></td></tr>
<tr><td>merror</td><td/></tr>
<tr><td>mtext</td><td/></tr>
<tr><td><b>mstyle</b></td><td><b>scriptlevel mathcolor mathbackground displaystyle mathvariant</b></td></tr>
<tr><td><b>mmultiscripts</b></td><td/></tr>
<tr><td><b>mprescripts</b></td><td/></tr>
<tr><td><b>none</b></td><td/></tr>
<tr><td>mfrac</td><td>linethickness</td></tr>
<tr><td><b>msqrt</b></td><td/></tr>
<tr><td><b>mroot</b></td><td/></tr>
<tr><td>mtable</td><td>rowalign columnalign <b>align rowspacing columnspacing equalrows equalcolumns</b> rowlines columnlines frame</td></tr>
<tr><td>mtr</td><td>rowalign columnalign</td></tr>
<tr><td>mtd</td><td>rowalign columnalign rowspan columnspan</td></tr>
<tr><td>semantics</td><td/></tr>
<tr><td><b>annotation-xml</b></td><td><b>encoding</b></td></tr>
</tbody>
</table>
</div>

<p>Other bits of the conversation were a little more heartening. <acronym>MathML</acronym>-in-<code>text/html</code> support is in <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/#comment-42096">Firefox nightlies</a>, though disabled by default. I don’t imagine it will be turned on before Firefox 3.7 at the earliest. Judging by the number of Firefox 3.0 users, it’ll be some years yet, before we can count on using <acronym>MathML</acronym>-in-<code>text/html</code>. And I did <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/#comment-42158">learn</a> about the very-cool-sounding <a href="http://www.mathjax.org/">MathJax project</a>.</p>

<p>Anyway, here’s a modest contribution to what the discussion could have been about: things you can do with math on the web, that you <em>couldn’t</em> do in print.   Hover your mouse over the right-hand side of </p>

<math xmlns="http://www.w3.org/1998/Math/MathML" display="block"><mi>A</mi><mo>=</mo><maction selection="2" actiontype="toggle"><maction actiontype="statusline"><mrow><mstyle displaystyle="false"><mfrac><mn>2</mn><msqrt><mi>π</mi></msqrt></mfrac></mstyle><msubsup><mo>∫</mo> <mn>0</mn> <mi>x</mi></msubsup><msup><mi>e</mi> <mrow><mo rspace="0em" lspace="verythinmathspace">−</mo><msup><mi>t</mi> <mn>2</mn></msup></mrow></msup><mi>d</mi><mi>t</mi></mrow><mtext>Click to hide.</mtext></maction> <maction actiontype="statusline"><mrow><mo rspace="thinmathspace" lspace="thinmathspace">erf</mo><mo stretchy="false">(</mo><mi>x</mi><mo stretchy="false">)</mo></mrow><mtext>The Error Function: click for the definition.</mtext></maction></maction></math>

<p>Unfortunately, due to a <a href="https://bugzilla.mozilla.org/show_bug.cgi?id=427990">year-old Mozilla bug</a>, the perhaps more-useful</p>

<math xmlns="http://www.w3.org/1998/Math/MathML" display="block"><mi>A</mi><mo>=</mo><maction actiontype="statusline"><mrow xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://en.wikipedia.org/wiki/Error_function" xlink:type="simple"><mrow><mo rspace="thinmathspace" lspace="thinmathspace">erf</mo><mo stretchy="false">(</mo><mi>x</mi><mo stretchy="false">)</mo></mrow></mrow><mtext>The Error Function: click to go to Wikipedia.</mtext></maction></math>

<p>doesn’t currently work.</p>

<p>These are created with itex’s <code>\statusline{}{}</code>, <code>\toggle{}{}</code> and <code>\href{}{}</code> <a href="http://golem.ph.utexas.edu/~distler/blog/itex2MMLcommands.html">commands</a>.</p>

<div class="update" id="WebkitU1"><h4>Update (11/6/2009):</h4> Since Frank Hecker was <a href="http://golem.ph.utexas.edu/~distler/blog/archives/002105.html#c028950">confused</a>, here’s the same equation, redone using itex’s <a href="http://golem.ph.utexas.edu/~distler/code/itexToMML/revision/40">new</a> <code>\tooltip{}{}</code> command:
<math xmlns="http://www.w3.org/1998/Math/MathML" display="block"><mi>A</mi><mo>=</mo><maction selection="2" actiontype="toggle"><maction actiontype="tooltip"><mrow><mstyle displaystyle="false"><mfrac><mn>2</mn><msqrt><mi>π</mi></msqrt></mfrac></mstyle><msubsup><mo>∫</mo> <mn>0</mn> <mi>x</mi></msubsup><msup><mi>e</mi> <mrow><mo rspace="0em" lspace="verythinmathspace">−</mo><msup><mi>t</mi> <mn>2</mn></msup></mrow></msup><mi>d</mi><mi>t</mi></mrow><mtext>Click to hide.</mtext></maction> <maction actiontype="tooltip"><mrow><mo rspace="thinmathspace" lspace="thinmathspace">erf</mo><mo stretchy="false">(</mo><mi>x</mi><mo stretchy="false">)</mo></mrow><mtext>The Error Function: click for the definition.</mtext></maction></maction></math>
Specifically, the itex code is
<blockquote><pre><code>A=\toggle{
    \tooltip{Click to hide.}{
   \tfrac{2}{\sqrt{\pi}}\int_0^x e^{-t^2} d t}  }{
    \tooltip{The Error Function: click for the definition.}{
   \mathop{erf}(x)}
  }</code></pre></blockquote>
</div>

      </div>
    
    </content>
  
    <source>
      <title>Musings</title>
      <link href="http://golem.ph.utexas.edu/~distler/blog/" rel="alternate" type="application/xhtml+xml"/>
      <link href="http://golem.ph.utexas.edu/~distler/blog/atom10.xml" rel="self"/>
      <link href="http://golem.ph.utexas.edu/~distler/blog/comments.atom" rel="replies" type="application/atom+xml"/>
      <updated>2009-11-08T00:03:26+00:00</updated>
      <subtitle>Thoughts on Science, Computing, and Life on Earth.</subtitle>
      <id>tag:golem.ph.utexas.edu,2003:Musings/1</id>
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  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://sbseminar.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>Scott Carnahan</name>
						
      <uri>http://math.mit.edu/~carnahan/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Classified problem</div>
    </title>
		
    <link href="http://sbseminar.wordpress.com/2009/11/04/classified-problem/" rel="alternate" type="text/html"/>
		
    <id>http://sbseminar.wordpress.com/?p=2575</id>
		
    <updated>2009-11-07T21:35:06+00:00</updated>
		
    <published>2009-11-05T07:26:49+00:00</published>
		
    <category term="combinatorics" scheme="http://sbseminar.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Today at tea, some grad students were discussing the following enumeration problem:
How many elements of  have zeroes in all diagonal entries?
I think they [Redacted].  The answer is apparently known but classified.  It’s a sort of q-analog of derangements (i.e., permutations without fixed points), but if you take the derangement formula and add [...]<img src="http://stats.wordpress.com/b.gif?host=sbseminar.wordpress.com&amp;blog=1217555&amp;post=2575&amp;subd=sbseminar&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://sbseminar.wordpress.com/2009/11/04/classified-problem/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>Today at tea, some grad students were discussing the following enumeration problem:</p>
<blockquote><p>How many elements of <img class="latex" title="GL_n(\mathbb{F}_q)" src="http://s3.wordpress.com/latex.php?latex=GL_n(%5Cmathbb%7BF%7D_q)&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="GL_n(\mathbb{F}_q)"/> have zeroes in all diagonal entries?</p></blockquote>
<p>I think they <i>[Redacted]</i>.  The answer is apparently known but classified.  It’s a sort of q-analog of derangements (i.e., permutations without fixed points), but if you take the derangement formula and add q-numbers in the naive way, the formula <img class="latex" title="(q-1)^n \sum_{k=0}^n (-1)^k \frac{[n]!}{[k]!}" src="http://s1.wordpress.com/latex.php?latex=(q-1)%5En+%5Csum_%7Bk=0%7D%5En+(-1)%5Ek+%5Cfrac%7B%5Bn%5D!%7D%7B%5Bk%5D!%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="(q-1)^n \sum_{k=0}^n (-1)^k \frac{[n]!}{[k]!}"/> doesn’t seem to work for n &gt; 2.</p>
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		<thr:total>16</thr:total>
	
    <source>
      <title type="text">Secret Blogging Seminar</title>
      <subtitle type="text">Representation theory, geometry and whatever else we decide is worth writing about today.</subtitle>
      <updated>2009-11-07T21:35:06+00:00</updated>
      <generator uri="http://wordpress.com/">WordPress.com</generator>
      <link href="http://sbseminar.wordpress.com/" rel="alternate" type="text/html"/>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://gowers.wordpress.com/wp-atom.php">
		
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      <name>gowers</name>
						
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    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Polymath and the origin of life</div>
    </title>
		
    <link href="http://gowers.wordpress.com/2009/11/07/polymath-and-the-origin-of-life/" rel="alternate" type="text/html"/>
		
    <id>http://gowers.wordpress.com/?p=1158</id>
		
    <updated>2009-11-07T17:31:40+00:00</updated>
		
    <published>2009-11-06T23:01:28+00:00</published>
		
    <category term="polymath" scheme="http://gowers.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">This is the first of a few posts I plan (one other of which is written and another of which is in draft form but in need of a few changes) in which I discuss various Polymath proposals in more detail than I did in my earlier post on possible projects. 
One of my suggestions, [...]<img src="http://stats.wordpress.com/b.gif?host=gowers.wordpress.com&amp;blog=1659011&amp;post=1158&amp;subd=gowers&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://gowers.wordpress.com/2009/11/07/polymath-and-the-origin-of-life/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>This is the first of a few posts I plan (one other of which is written and another of which is in draft form but in need of a few changes) in which I discuss various Polymath proposals in more detail than I did in <a href="http://gowers.wordpress.com/2009/09/16/possible-future-polymath-projects/">my earlier post on possible projects</a>. </p>
<p>One of my suggestions, albeit a rather tentative one, was to try to come up with a model that would show convincingly how life could emerge from non-life by purely naturalistic processes. But before this could become a sensible project it would be essential to have a more clearly defined mathematical question. By that I don’t mean a conjecture that Polymath would be trying to prove rigorously, but rather a list of properties that a model would have to have for it to count as successful. Such a list need not be fully precise, but in my view it should be reasonably precise, so that the task is reasonably well defined. It would of course be possible to change the desiderata as one went along.</p>
<p>In this post I’d like to make a preliminary list. It will undoubtedly be unsatisfactory in many ways, but I hope that there will be a subsequent discussion and that from it a better list will emerge. The purpose of this is not to start a Polymath project, but simply to attempt to define a Polymath proposal that might at some future date be an actual project. For two reasons I wouldn’t want this to be a serious project just yet: it seems a good idea to think quite hard about how it would actually work in practice, and someone who I hope will be a key participant is very busy for the next few months and less busy thereafter. <span id="more-1158"/> </p>
<p>As a starting point, let me mention two ideas that are already out there and have attracted a lot of attention. One is the idea of <a href="http://en.wikipedia.org/wiki/Cellular_automaton">cellular automata</a>. A fairly general type of cellular automaton can be defined as follows. You have a graph (usually something like an infinite two-dimensional lattice), and at some points you have 1s and at other points you have 0s. You then let the system evolve in rounds according to some simple rule that is usually the same for every vertex. It might be something like this: if at least two of my neighbours are 1s then I will become a 1, and otherwise I will become a 0. It turns out that very simple rules can lead to extremely complicated and interesting behaviour.</p>
<p>What counts as complicated and interesting? Well, perhaps it is better to say what counts as dull. One possible form of dullness is if a system evolves to some state such as the all-1s state, or perhaps a big rectangle full of 1s with 0s outside, or an oscillation between two configurations. Another form of dullness is a system that tends to disperse the 1s until they form some fairly random looking bunch of 1s that never stops looking fairly random. But in between, there are systems that tend to evolve towards some kind of criticality, where you get fractal structures with organization at many different distance scales. One thing that interests people about cellular automata is that there are very simple rules that seem to want to evolve towards these nice “edge of chaos” patterns.</p>
<p>The second idea is <a href="http://en.wikipedia.org/wiki/Self-organized_criticality">self-organized criticality</a>, which is a phenomenon exhibited by certain models in statistical physics — notably the so-called sandpile models. These are supposed to model what happens if you drop grains of sand one by one on to a pile. They will start to build up into a conical shape, but if the sides get too steep there are avalanches. The sizes of these avalanches vary, and if you plot the frequency of avalanches of various sizes, you find (experimentally at least) that they obey a power law. And power laws get people excited because they are what you find associated with critical phenomena. A typical sandpile model is something like this. You have a big square divided into a grid of small squares. You then set all squares equal to 0 except a few randomly chosen ones that you give small integers to. You then add 1 to the central square (let’s assume there is one), and after you have done so you have a rule that says that if any square has value at least 4 it must give 1 to each of its neighbours. This procedure you iterate until no square has value at least 4. (It can be shown that the order in which you do these operations doesn’t matter.) You then add 1 to the central square again, and keep going.</p>
<p>It turns out that the sizes of the “avalanches” that take place here (that is, how many iterations you have to do of the simple rule before all squares have value 0 to 3) also obey a power law, and also that systems such as these have a tendency to evolve towards interesting (that is, not too random and not too structured) configurations. That is, you can get critical phenomena without having to fine-tune some parameter. Again, this has got people excited as it seems to promise an explanation of how the complexity in nature could have started.</p>
<p>In the above description, I made the starting configuration random but after that the way the model evolved was deterministic. There are of course many different possible models, and in some of them the new “grains of sand” are dropped in random places. Again you get interesting critical behaviour. </p>
<p>Now as far as I know, with both cellular automata and sandpile models you get nice critical phenomena appearing, but while they give you pretty patterns they do not give you anything resembling an ecosystem. Yes, <a href="http://en.wikipedia.org/wiki/Conway's_Game_of_Life">Conway’s game of life</a> gives you glider guns and configurations that can reproduce themselves, but you have to set them up carefully in advance, and they don’t seem to do anything all that exciting. They also support universal computation, but again if you want to program the game of life to create an artificial-life simulator, you might as well use a much more powerful computer to do so. What a Polymath project would be looking for is a very simple system with the property that, regardless of the starting configuration, it would tend to develop and eventually produce something that looked like a complex ecosystem.</p>
<p>This brings me to a point that is worth making. The idea of this Polymath project would not be to produce yet another <a href="http://en.wikipedia.org/wiki/Artificial_life">artificial life</a> program, fascinating though those programs can be. One could think of it more like this: can one come up with a very simple model that almost always “self-organizes” and produces something that looks a bit like what you get with artificial life programs? In other words, we would be trying to model <a href="http://en.wikipedia.org/wiki/Abiogenesis">abiogenesis</a> rather than <a href="http://en.wikipedia.org/wiki/Evolution">evolution</a>. </p>
<p>After that discussion, I think I can have a stab at saying what the properties are that would make a truly interesting and new model. (I am much less sure about the “new” part, and would be interested to hear from people with more knowledge about this kind of topic what the state of the art is.) Some of the properties below seem to be more important than others, but for now I won’t bother to distinguish between those that I regard as essential and those that are merely desirable.</p>
<p>1. It should be a dynamic model that evolves according to simple rules.</p>
<p>2. It should have a tendency to evolve towards patterns with a “critical” character — not too random and not too simple, with interesting features at many distance scales.</p>
<p>3. Probably it should be a somewhat randomized model (to give it a certain robustness). Here I am referring to the rules by which the model develops rather than the initial conditions, but perhaps the initial conditions should be randomized as well.</p>
<p>4. It should have a tendency to produce identifiable macroscopic structures.</p>
<p>5. It should be possible to classify these macroscopic structures in interesting ways. (That is, we would like to be able to say that certain structures look more or less the same as certain others, and ideally this similarity would be a bit more flexible than one just being a translation of another.)</p>
<p>6. These structures should interact with one another, and the interaction should sometimes be destructive (thereby providing some selection pressure).</p>
<p>7. With high probability, self-reproducing structures should eventually emerge. (Before posting this I showed it to Michael Nielsen, who made some interesting points. One of them is that experience in the actual universe suggests that perhaps there should be some fine tuning of parameters before the probability becomes high: after all, life does not evolve on all planets.)</p>
<p>I could go on, but the idea is that once you’ve got 6 and 7, and perhaps a few other properties (for instance, one might decide to have major environmental changes from time to time just to stimulate the development of the system), then natural selection can begin to operate. </p>
<p>Of course, the major challenge is 7. The most plausible route I can see to 7 is a purely probabilistic one: almost all configurations are not self-reproducing, but if a self-reproducing one ever does arise, then it will reproduce itself and start appearing all over the place. But in that case 5 is also a huge challenge. The kinds of structures one would ideally like are not things like the bullets from Conway’s glider guns, but larger configurations that can move about and that are defined more topologically. Indeed, that could be a huge and general problem: the geometry of <img class="latex" title="\mathbb{Z}^3" src="http://s1.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E3&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{Z}^3"/> just isn’t the same as the geometry of <img class="latex" title="\mathbb{R}^3" src="http://s2.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D%5E3&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{R}^3"/>, but a continuous model would be very difficult to design and simulate (or would it?). But perhaps there could be some cleverly chosen simple rule that would tend to protect “clumps” of 1s and allow them to move, and to do complicated things like rotating (whatever that can be made to mean in <img class="latex" title="\mathbb{Z}^3" src="http://s3.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E3&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{Z}^3"/>). Or perhaps a complicated ecosystem could develop that was more <img class="latex" title="\mathbb{Z}^3" src="http://s1.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E3&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{Z}^3"/>-like than <img class="latex" title="\mathbb{R}^3" src="http://s2.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D%5E3&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{R}^3"/>-like. </p>
<p>Here, incidentally, is a paragraph from the Wikipedia article on Conway’s game of life, which shows that it is not already an example of what I am talking about:</p>
<blockquote><p>From a random initial pattern of living cells on the grid, observers will find the population constantly changing as the generations tick by. The patterns that emerge from the simple rules may be considered a form of beauty. Small isolated subpatterns with no initial symmetry tend to become symmetrical. Once this happens the symmetry may increase in richness, but it cannot be lost unless a nearby subpattern comes close enough to disturb it. In a very few cases the society eventually dies out, with all living cells vanishing, though this may not happen for a great many generations. Most initial patterns eventually “burn out”, producing either stable figures or patterns that oscillate forever between two or more states; many also produce one or more gliders or spaceships that travel indefinitely away from the initial location.</p></blockquote>
<p>We would be looking for something a bit like the Game of Life, possibly randomized, with the important difference that it almost always got more and more complicated and more and more interesting.</p>
<p><strong> Physics </strong></p>
<p>There is one other property that I think would make a model more convincing as an argument for the probability of life arising out of non-life without any magic processes operating. I partly owe this thought to Michael Nielsen, who included the following two questions in a comment he made on the post where I originally mentioned this problem.</p>
<blockquote><p>
(1) How would you go about recognizing self-replicating beings?</p>
<p>(2) What sort of models are “reasonable”, in the sense of both reflecting what we know of physics, and being simple enough to be tractable? The Game of Life isn’t very physical, in that it disobeys many basic physical principles, like conservation of energy, conservation of mass, conservation of momentum, and so on.
</p></blockquote>
<p>One of the things that people often say about life, evolution, biological systems and the like is that they are ways of locally combatting the second law of thermodynamics. So perhaps one could add the following property as one that it would be very nice to have.</p>
<p>8. The general tendency for the model is to become more and more disordered, and eventually to end in heat death, but for there to be many local <em>increases</em> in order. </p>
<p>Of course, one would need to be clear what that meant. The other physical principles that Michael mentioned would also be good to have.</p>
<p>Here is a subproblem that occurs to me as I am writing this. It is connected with the thought that one would like macroscopic structures to have some tendency to survive. In the Game of Life, it seems that structures that survive do so almost by accident — they settle down into some sort of periodicity, say. But structures in the biological world are held together by physical forces, and they have identifiable boundaries and things like that. So one might try to develop a model that captures just this behaviour. As with the main problem, I’m not sure how to formulate this subproblem precisely, but let me have a go. Does there exist a model with the following properties?</p>
<p>(i) If you draw some large-scale shape (think of the 0s and 1s as black and white pixels, say, so the shape is on a much larger distance scale than the distance between two neighbouring points of the grid), it has a tendency to move “continuously”.</p>
<p>(ii) There is a tendency for mass and momentum to be conserved.</p>
<p>To give an idea of the kind of thing I mean here, let’s suppose that “mass” is represented by 1s, and you take a large annulus, place it over <img class="latex" title="\mathbb{Z}^2" src="http://s3.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E2&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\mathbb{Z}^2"/>, and put a 1 at every grid point that lies in the annulus. Then in the interior circle of the annulus put a random scattering of not too many 1s. And then slightly move the annulus part, and slightly move all the little particles inside. If the first position of the annulus represents where some very simple structure is at time 1 and the second where it is at time 2, then conservation of mass and momentum would tell us to expect it to continue moving in the same direction (so it would be more sophisticated than a cellular automaton of the kind described earlier because its behaviour would depend not just on how it behaved an instant earlier), and to stay the same size. We might also have “forces” between neighbouring 1s that encouraged them to stay together somewhat, and so on.</p>
<p>Of course, as with Conway’s Game of Life, the idea would be to devise the simplest possible set of rules that did what one wanted (in this case preserve macroscopic shapes at least to some extent and allow them to move about reasonably flexibly but without distorting themselves too much). It would not be to try to create the most realistic model one could of the actual world. </p>
<p>Since writing the above paragraphs I’ve found out the following relevant facts. First this from the Wikipedia article on <a href="http://en.wikipedia.org/wiki/Life-like_cellular_automaton">Life-like cellular automata</a>:</p>
<blockquote><p>
Larger than Life is a family of cellular automata studied by Kellie Michele Evans. They have very large radius neighbourhoods, but perform `birth/death’ thresholding similar to Conway’s life. The LtL CA manifest eerily organic `glider’ and `blinker’ structures.</p>
<p>RealLife is the “continuum limit″ of Evan’s Larger Than Life CA, in the limit as the neighbourhood radius goes to infinity, while the lattice spacing goes to zero. Technically, they are not cellular automata at all, because the underlying “space” is the continuous Euclidean plane R2, not the discrete lattice Z2. They have been studied by Marcus Pivato.
</p></blockquote>
<p>Secondly, here is the <a href="http://arxiv.org/abs/math.DS/0503504">paper by Marcus Pivato</a> mentioned above.</p>
<p><strong>Chemistry and the problem of scale.</strong></p>
<p>By far the most famous contribution to our understanding of how life started is the <a href="http://en.wikipedia.org/wiki/Miller%E2%80%93Urey_experiment">Miller-Urey experiment</a>, in which Miller and Urey attempted to simulate the chemical conditions that might have prevailed early on in the life of the Earth. They used electrodes to create lightning-like sparks that passed through a vapour that was formed of water, methane, ammonia and hydrogen, and found that they produced complex amino acids, which are essential building blocks of life.</p>
<p>What relevance would this experiment have for a computer simulation? My view is that one should not necessarily try to produce a virtual Miller-Urey experiment (complete with virtual lightning, virtual ammonia, etc.) but that the experiment does raise a couple of questions that it is essential to address.</p>
<p>A fundamental fact about life as it exists in the physical world is that it is carbon based. The great virtue of carbon is that its particular bonding properties allow it to combine with other atoms to form molecules that are large and complicated enough to encode highly sophisticated information. So an obvious question is this.</p>
<p>Question 1: Should one design some kind of rudimentary virtual chemistry that would make complicated “molecules” possible in principle?</p>
<p>The alternative is to have some very simple physical rule and hope that the chemistry emerges from it (which would be more like the Game of Life approach). </p>
<p>This is just one example of a general tension. The more features you design into a model, the less “universal” it becomes and the less convincing it is as a demonstration of the inevitability of life. However, one can also argue for at least some designed features. After all, if we want to explain the origin of life, it is not necessary to start with a virtual Big Bang and get from there to the possibility of complex molecules. It may be that designing rules to make complex molecules possible (and then arguing that with probability 1 this possibility is actually realized) is attacking the problem at the correct level. </p>
<p>I do not have a strong view about what the right answer to this question is. Obviously I would prefer the chemistry to emerge as if by magic, but that may be an unrealistic hope.</p>
<p>The second question does not arise directly out of the Miller-Urey experiment, but it is related.</p>
<p>Question 2: How large and how complicated should we expect “organisms” to be?</p>
<p>A real-world organism, even a micro-organism, is made out of more atoms than one could hope to simulate on a computer. (I am not certain that that last sentence is correct, but I would be very surprised if it wasn’t. Added later: Michael Nielsen tells me that there are rudimentary organisms that are so small that they could perhaps be simulated in full.) Moreover, although it has many levels of complexity, there will also be distance scales at which it is relatively simple. For example, if I look at my hand from a distance of about a yard, my skin looks smooth. Similarly, if I were to look through a powerful microscope at one of the cells of my hand, then the boundary of that cell would be reasonably smooth, rather than fractal-like. In general, it seems that if you look at a typical organism, it is not equally complicated at all distance scales, but is more like  this: you take some small objects and put them together in a reasonably simple way to form bigger objects; you then use these bigger objects as building blocks for yet bigger objects; continuing this process for eight or nine (??) levels (perhaps if I knew more biology I would revise this number up considerably) you end up with a complex organism.</p>
<p>If that picture is roughly correct, then the number of “atoms” in a complex multicellular organism might be prohibitively large for a simulation. Is this a problem?</p>
<p>I think it shouldn’t be too problematic. Just as we are not trying to start with the Big Bang, neither are we trying to end with mammals. The main aim is to get to the point where evolution can take over. In particular, if a readily identifiable micro-organism appeared that could reproduce itself with small modifications, then the simulation would surely be declared a success.</p>
<p>Nevertheless, the question of scale remains. Would we want such a micro-organism to consist of a small handful of “pixels” that by some magic local rule gives rise to a copy of itself? Or would we want something much larger that had “smooth boundaries” at some distance scales and was composed of “complex molecules”? My inclination at the moment is to prefer the second for two reasons: it is less like the Game of Life (and therefore more likely to be novel and interesting) and it is closer to the life forms that we actually observe.</p>
<p>Added later: I haven’t quite made clear that one aim of such a project would be to come up with <em>theoretical</em> arguments. That is, it would be very nice if one could do more than have a discussion, based on intelligent guesswork, about how to design a simulation, followed (if we were lucky and found collaborators who were good at programming) by attempts to implement the designs, followed by refinements of the designs, etc. Even that could be pretty good, but some kind of theoretical (but probably not rigorous) argument  that gave one good reason to expect certain models to work well would be better still. Getting the right balance between theory and experiment could be challenging. The reason I am in favour of theory is that I feel that that is where mathematicians have more chance of making a genuinely new contribution to knowledge.</p>
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    <source>
      <title type="text">Gowers's Weblog</title>
      <subtitle type="text">Mathematics related discussions</subtitle>
      <updated>2009-11-07T17:31:40+00:00</updated>
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  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Great Moments in Targeted Advertising</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>We subscribe to <a href="http://www.locusmag.com/"><cite>Locus</cite></a>, the SF review and news magazine, and every month when it arrives, I flip through it quickly to look at the ads. This is a useful guide to what's coming out from various publishers, but it's also kind of fascinating to see how the different publishers market their stuff.</p>

<p>In particular, it's interesting to see how Baen pitches their books, because they are aimed with laser-like precision at people who aren't me. I'm sure their ads work very well for their target audience, but they make their forthcoming books sound absolutely horrifying to me. This month's ad may be the ultimate, featuring the following plug for a Tom Kratman book:</p>
<blockquote>
<p><b>Undercover Infidels!</b></p>

<p>Europe 2123. Dhimmitude-- assigning second-class citizenship to non-Muslims-- has dug its claws into the continent. Now a West Point grad must rescue a young girl sold into sexual slavery after her family could not pay the Christian Tax. U. S. Army vertean Tom Kratman notches up another controversial thriller!</p>
</blockquote>

<p>If that didn't scream "Run away!!!" loudly enough, there's a glowing quote from Mark Steyn. I'm not sure it would be possible to construct a more appalling book ad.</p>

<p>Oh, wait, I stand corrected: later in the same issue, there's a plug for <cite>The Science Behind the Secret</cite>, featuring a quote from noted <s>con man</s> tv psychic John Edward claiming that quantum mechanics is the basis for the "Law of Attraction." This is also a Baen book, coming in March. And it pretty much guarantees that even if they publish something I might like (hey, it could happen), I'll be getting it from the library, rather than giving them any of my beer money.</p>
 <a href="http://scienceblogs.com/principles/2009/11/great_moments_in_targeted_adve.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/qSd9EaPw984" height="1" width="1"/></div>
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    <published>2009-11-07T11:21:56-05:00</published>
      
    <updated>2009-11-07T11:21:56-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
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      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
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    <title>Links for 2009-11-07</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><ul class="delicious"><li>
                <div class="delicious-link"><a href="http://www.wipp.energy.gov/picsprog/articles/wipp%20exhibit%20message%20to%2012,000%20a_d.htm">WIPP Exhibit: Message to 12,000 A.D.</a></div>
                <div class="delicious-extended">"This place is not a place of honor.
No highly esteemed deed is commemorated here.
Nothing valued is here.
This place is a message and part of a system of messages.
Pay attention to it!
Sending this message was important to us.
We considered ourselves to be a powerful culture."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/science">science</a> <a href="http://delicious.com/orzelc/social-science">social-science</a> <a href="http://delicious.com/orzelc/nuclear">nuclear</a> <a href="http://delicious.com/orzelc/energy">energy</a> <a href="http://delicious.com/orzelc/culture">culture</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://www.amazon.com/gp/feature.html/ref=br_lf_m_1000446551_grlink_1?ie=UTF8&amp;plgroup=1&amp;docId=1000446551">Best Books of 2009: Science Top 10</a></div>
                <div class="delicious-extended">"Welcome to our Best of 2009 top 10 lists for Science. We've put our editors' picks and our 2009 bestsellers for each category on the same page together, so you can easily compare. Click on "Editors' Picks" to see our editors' list of the best science books of 2009, including our top pick, The Age of Wonder, Richard Holmes's delightfully masterful group biography of the adventurous scientists of Britain's Romantic age. And click on "Customer Favorites" to find the bestselling science books at Amazon.com during 2009"</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/science">science</a> <a href="http://delicious.com/orzelc/books">books</a> <a href="http://delicious.com/orzelc/writing">writing</a> <a href="http://delicious.com/orzelc/culture">culture</a> <a href="http://delicious.com/orzelc/internet">internet</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://suburbdad.blogspot.com/2009/11/transience.html">Confessions of a Community College Dean: Transience</a></div>
                <div class="delicious-extended">"We were talking about college preparation, and the various options and obstacles. In reference to a program that seems like it should work, but somehow doesn't, she mentioned that so many students move during the course of a year that it's not unusual for a majority of a class to turn over during the year. When students bounce from town to town -- it sounds like most of the moves are relatively local -- it's hard for any single program to gain serious traction, no matter how well-run it might be.

That seemed hard to accept, so I asked around on campus for the last few days to see if others had heard or seen the same thing. They had. Apparently, one of the features of our local low-income community is extremely high transience. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/education">education</a> <a href="http://delicious.com/orzelc/class-war">class-war</a> <a href="http://delicious.com/orzelc/blogs">blogs</a> <a href="http://delicious.com/orzelc/dean-dad">dean-dad</a> <a href="http://delicious.com/orzelc/society">society</a> <a href="http://delicious.com/orzelc/culture">culture</a> <a href="http://delicious.com/orzelc/economics">economics</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://blogs.discovermagazine.com/cosmicvariance/2009/11/06/makers-of-universes/">Makers of Universes | Cosmic Variance | Discover Magazine</a></div>
                <div class="delicious-extended">"It can't be easy being the guy who has to introduce Albert Einstein. But it helps if you're George Bernard Shaw."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/science">science</a> <a href="http://delicious.com/orzelc/history">history</a> <a href="http://delicious.com/orzelc/culture">culture</a> <a href="http://delicious.com/orzelc/blogs">blogs</a> <a href="http://delicious.com/orzelc/cosmic-variance">cosmic-variance</a> <a href="http://delicious.com/orzelc/youtube">youtube</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://www.tor.com/index.php?option=com_content&amp;view=blog&amp;id=58193">Tor.com / Science fiction and fantasy / Blog posts / So good your head explodes every time: Ted Chiang's Stories of Your Life and Others</a></div>
                <div class="delicious-extended">"You know how some people are ideas writers, and their ideas are so amazingly brilliant that you don't care they can't really write character and plot? Ted Chiang is like that, except that his characters and plots are that good as well. His stories all arise out of astonishing SFnal ideas, they couldn't happen except in the contexts where they do happen, but they have characters with emotional trajectories that carry them along as well. He always gets the arc of story exactly right, so you know what you need to know when you need to know it and the end comes along in perfect timing and socks you in the jaw. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/sf">sf</a> <a href="http://delicious.com/orzelc/books">books</a> <a href="http://delicious.com/orzelc/tor">tor</a> <a href="http://delicious.com/orzelc/review">review</a>)</div>
            </li></ul> <a href="http://scienceblogs.com/principles/2009/11/links_for_2009-11-07.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/3c83_Q6li7I" height="1" width="1"/></div>
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    <published>2009-11-07T09:06:59-05:00</published>
      
    <updated>2009-11-07T09:06:59-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
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      <updated>2009-11-07T11:21:56-05:00</updated>
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    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Data mining</div>
    </title>
		
    <link href="http://gordonwatts.wordpress.com/2009/11/07/data-mining/" rel="alternate" type="text/html"/>
		
    <id>http://gordonwatts.wordpress.com/2009/11/07/data-mining/</id>
		
    <updated>2009-11-07T12:19:39+00:00</updated>
		
    <published>2009-11-07T12:19:39+00:00</published>
		
    <category term="Health" scheme="http://gordonwatts.wordpress.com/"/>
    <category term="computers" scheme="http://gordonwatts.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">In particle physics this is what we do. We have petabytes (1000 terrabytes!) datasets consisting of billions of physics interactions. For the particularly rare ones we need to pick out several 100 or 1000 and study them in detail. As you might expect, we are drowning in data and have developed many tools to help [...]<img src="http://stats.wordpress.com/b.gif?host=gordonwatts.wordpress.com&amp;blog=54078&amp;post=1205&amp;subd=gordonwatts&amp;ref=&amp;feed=1" border="0" alt=""/></div>
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    <content type="xhtml" xml:base="http://gordonwatts.wordpress.com/2009/11/07/data-mining/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>In particle physics this is what we do. We have petabytes (1000 terrabytes!) datasets consisting of billions of physics interactions. For the particularly rare ones we need to pick out several 100 or 1000 and study them in detail. As you might expect, we are drowning in data and have developed many <a href="http://root.cern.ch/">tools</a> to help us. Computers are central – without them we would not be able to do the science we currently do!</p>
<p>The most common public example of data mining I’ve heard about is looking at all the receipts from Wallmart purchases. This is why grocery stores like you to sign up for their frequent-use cards – they can track everything you buy, sell that data, and, more importantly, send you ads that are likely to get you in and get you to buy other things. It is an amazingly powerful tool. In business it has been getting a bit of a bad name recently because it has been connected to some fairly serious invasion of privacy issues (i.e. creepy things – like knowing what hour of the day you check your email, how much the average person in your zip code makes, etc.).</p>
<p>But one place that it could obviously be applied for the greater good that I’d never really given much thought to is medicine. Check out <a href="http://www.nytimes.com/2009/11/08/magazine/08Healthcare-t.html">this long article from the NYT on the topic</a> – Making Health Care Better. It starts with some history – and the bromide “The amount of death and disease would be less if all disease were left to itself.” from 1835… to the present day:</p>
<blockquote><p>“Medicine adopted the scientific method,” James said… “It transformed medicine, and it’s easy to make the case.”</p>
</blockquote>
<p>He talks about the testing and science applied to any new method, drug, procedure before it is allowed to be used by mainstream doctors. But…</p>
<blockquote><p>But there is one important way in which medicine never quite adopted the scientific method… …once a treatment enters the mainstream — once we know whether it works in certain situations — science is largely left behind. The next questions — when to use it and on which patients — become matters of judgment, not measurement.</p>
</blockquote>
<p>The article provides a dizzying array of treatments available to a doctor that is trying to treat heart disease. And what treatment is left up to the doctor’s judgment.</p>
<p>Cleary some hospitals and doctors have better average outcomes than others – so some doctors must have better judgment than others. Wouldn’t it be great if every doctor could start with a default procedure that has been shown to work for a patient that looks like the one the doctor is trying to treat and then modify it to fit the patient’s specifics?</p>
<p>Well…</p>
<blockquote><p>“I thought there wasn’t anybody better in the world at twiddling the knobs than I was,” Jim Orme, a critical-care doctor, told me later, “so I was skeptical that any protocol generated by a group of people could do better.”</p>
</blockquote>
<p>And that is just it – there are so many variations in treatments. Today’s instruments are quite complex and have many settings – so how do you know what works correctly? When the procedure is approved there is a fair amount of science recorded for each setting, and presumable most doctors follow it. But not all of them!</p>
<p>And this is where I think data-mining could come in. What if every single modern instrument was hooked into the network, and each adjustment was recorded? And linked to a patients medical file (so you could see history). Each time a nurse or doctor did something it was recorded. All of that in some standard format – and then shared across hospitals and doctors the country or world over?</p>
<p>This has, of course, been a dream for a while of electronic health care records. It always struck me as obvious that you would attach x-rays, CT scans, descriptions of medicine given, etc., but it never occurred to me the level of detail you could go into! From a technical point of view this is hard – the data is so non-uniform, unlike the particle physics experiments I work on, but the long term benefits could be quite good. The article describes when this data mining technique was applied ad-hoc in just a single hospital:</p>
<blockquote><p>One widely circulated national study overseen by doctors at Massachusetts General Hospital had found an ARDS [Acute respiratory distress syndrome] survival rate of about 10 percent. For those in Intermountain’s study, the rate was 40 percent.</p>
</blockquote>
<p>At any rate, this tickled my fancy, which is why I wrote about it. I found it ironic that on the <a href="http://www.nytimes.com/pages/health/index.html">Health</a> home page yesterday there was also the <a href="http://www.nytimes.com/2009/11/05/business/05device.html?_r=1&amp;ref=health">following article</a>:</p>
<blockquote><p>Five years later, Medicare underwrites more than half of the $4 billion the nation now spends annually on defibrillators, but the agency is no closer to knowing how many lives that big investment is saving.</p>
</blockquote>
<p>My impression of the health care bills working their way through congress right now is none of them really go after cost-savings. Science can help*.</p>
<p>* Ok – making devices that can spit out data in a common format will add to their cost. But you can do simple things like the Intermountain study to start as better devices come online!</p>
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    <source>
      <title type="text">Life as a Physicist</title>
      <subtitle type="text">Particle Physicist. In the wild.</subtitle>
      <updated>2009-11-07T12:19:39+00:00</updated>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-16693931.post-5412557661137450843</id>
    <published>2009-11-07T11:02:00+01:00</published>
    <updated>2009-11-07T11:34:29+01:00</updated>
    <category term="Galicia" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="Santiago de Compostela" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="Pub Fuco Luis" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="advertising" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="Cosmos" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="Carl Sagan" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="TV" scheme="http://www.blogger.com/atom/ns#"/>
    <title type="text">Carl Sagan day and a Cosmos coincidence</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">I was due to post an advert for a monthly event here in Santiago, part of the International Year of Astronomy, which has been going on for a few months and is due to continue into next year. Every month in Pub Fuco Lois the landlord has cleared the way for a showing of an episode of Carl Sagan's Cosmos. I attended the last event which was extremely enjoyable, though not as well attended as I'd hoped. After watching the episode (dubbed into Spanish) people chatted over drinks about the show before dispersing into the night. A fun evening but it will be improved by the inclusion of more people. So, come along next Tuesday and enjoy the show!<br/><div class="separator" style="clear: both; text-align: center;"><a href="http://4.bp.blogspot.com/_NtZfodDEoj0/SvVFMPgg7tI/AAAAAAAAAWs/bpBtu27c_bE/s1600-h/Untitled-1.jpg" style="margin-left: 1em; margin-right: 1em;"><img src="http://4.bp.blogspot.com/_NtZfodDEoj0/SvVFMPgg7tI/AAAAAAAAAWs/bpBtu27c_bE/s640/Untitled-1.jpg" border="0"/></a><br/></div><br/>The coincidence of course is that today is <a href="http://www.carlsaganday.com/">Carl Sagan day</a> and would have been his 75th birthday. For some words from a true Sagan oficionado go and <a href="http://toomanytribbles.blogspot.com/2009/11/happy-saganseve.html">see what TMT has to say</a> on the subject and watch the videos linked therein.<div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/16693931-5412557661137450843?l=jonstraveladventures.blogspot.com" height="1" width="1"/></div></div>
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    <author>
      <name>Jonathan Shock</name>
      <uri>http://www.blogger.com/profile/11667852535983804885</uri>
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      <id>tag:blogger.com,1999:blog-16693931</id>
      <updated>2009-11-07T11:34:29+01:00</updated>
      <title type="text">Jonstraveladventures</title>
      <link href="http://jonstraveladventures.blogspot.com/feeds/posts/default" rel="http://schemas.google.com/g/2005#feed" type="application/atom+xml"/>
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      <author>
        <name>Jonathan Shock</name>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-22973357.post-7226482298312565972</id>
    <published>2009-11-07T03:36:00-05:00</published>
    <updated>2009-11-07T03:42:29-05:00</updated>
    <category term="Physics" scheme="http://www.blogger.com/atom/ns#"/>
    <title type="text">Experimental Search for Quantum Gravity 2010</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://www.perimeterinstitute.ca/images/pifiles/searchqg.jpg"><img src="http://www.perimeterinstitute.ca/images/pifiles/searchqg.jpg" border="0" alt="" style="float:right; margin:0 0 10px 10px;cursor:pointer; cursor:hand;width: 200px; height: 200px;"/></a>I'm organizing a workshop!<br/><ul><a href="http://www.nordita.org/esqg2010/">Experimental Search for Quantum Gravity 2010</a></ul>will take place July 12-16 at <a href="http://www.nordita.org/">Nordita</a>, in the top intelligent city of the world, beautiful Stockholm, Sweden. This  is the 2010 installation of our <a href="http://backreaction.blogspot.com/2007/10/experimental-search-for-quantum-gravity.html">2007 PI workshop</a> of which you can find <a href="http://backreaction.blogspot.com/2007/11/esqg-2007-summary.html">my summary here.</a> <div><br/></div><div>We meanwhile have <a href="http://www.nordita.org/esqg2010/">the website up</a>, and a preliminary <a href="http://www.prime-spot.de/ESQG10/participants.html">list of participants</a>.<br/><br/>The purpose of the workshop is to bring together people who study various possibilities to experimentally test quantum gravity in order to assess these possibilities and encourage discussions. Some topics are:<div><br/><ul><li>Predictions for existent and planned earth based experiments (accelerators, high-precision measurements), possibly in scenarios with a lowered Planck scale.</li><li>Cosmological measurements: signatures from the universe's early quantum phase (in the cosmic microwave/neutrino/graviton background, large and small scale structure)</li><li>Astrophysical measurements: cosmic rays, gamma-ray bursts, supernovae.</li><li>Quantum effects caused by space-time fuzziness (decoherence), status and proposals for experiments.</li><li>Miscellaneous and other (emergent gravity, non-locality, etc.).</li></ul><br/>Yesterday, I submitted an application for conference support to the Swedish Research Council. (Many thanks to Thomas for helping with a Swedish title!) If this application goes through, most of the grant is meant to support students or postdocs in the early career stages, who have little or no travel grants available. I would really like to give these young researchers the opportunity to participate and learn something about what is still a very young field. So, if you feel addressed, mark the week July 12-16, and send me a note to be put on the waiting list (hossi at nordita dot org).<br/><br/>Since the topic touches on many different fields the workshop is bound to be interesting, and I'm very much looking forward to it.<p/><p/></div></div><div class="blogger-post-footer">"You do not really understand something unless you can explain it to your grandmother." ~ Albert Einstein<img src="https://blogger.googleusercontent.com/tracker/22973357-7226482298312565972?l=backreaction.blogspot.com" height="1" width="1"/></div></div>
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      <updated>2009-11-07T19:44:53-05:00</updated>
      <title type="text">Backreaction</title>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-2846514233477399562.post-3975800791031710181</id>
    <published>2009-10-30T22:10:00+01:00</published>
    <updated>2009-11-07T06:21:18+01:00</updated>
    <title type="text">Hail to Freedom</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Experimental collaborations display vastly different attitudes toward sharing their data. In my <a href="http://resonaances.blogspot.com/2009/10/whats-really-behind-dama.html">previous</a> post I described an extreme approach bordering on schizophrenia. On the other end of the spectrum is the Fermi collaboration (hail to Fermi).  After one year of taking and analyzing data they <a href="http://fermi.gsfc.nasa.gov/ssc/data/">posted</a> on a  public website the energy and direction of every gamma-ray photon they had detected. This is of course the standard procedure for all missions funded by NASA (hail to NASA). Now everybody, from a farmer in the Guangxi province to a professor in Harvard, has a chance to search for dark matter using real data.<br/><br/>The release of the Fermi data has already spawned two independent analyses by theorists. One is being widely discussed on blogs (<a href="http://blogs.discovermagazine.com/cosmicvariance/2009/10/28/has-fermi-seen-new-evidence-for-dark-matter/">here</a> and <a href="http://motls.blogspot.com/2009/10/fermi-sees-wmap-haze-too-dark-matter.html">here</a>) and in popular <a href="http://www.skyandtelescope.com/news/66968132.html">magazines</a>, whereas the other paper passed rather unnoticed. Both papers claim to have discovered an effect overlooked by the Fermi collaboration, and both hint to dark matter as the origin.<br/><br/>The <a href="http://www.slac.stanford.edu/spires/find/hep/www?eprint=arXiv:0910.4583">first</a> (chronologically, the second) of the two papers provides a new piece of evidence that the center of our galaxy hosts the so-called<span style="font-style: italic;"> haze</span> - a population of hard electrons (and/or positrons) whose spectrum is difficult to explain by conventional astrophysical processes. The haze was first observed by Jimi Hendrix ('Scuse me while I kiss the sky). Later, Doug Finkbeiner came across the haze when analyzing maps of cosmic microwave radiation provided by WMAP; in fact, that was also an independent analysis of  publicly released data (hail to WMAP). The WMAP haze is supposedly produced by synchrotron radiation of the electrons<a href="http://4.bp.blogspot.com/_xEaWDp7BS1Q/SutZCbKRhtI/AAAAAAAAAms/SFos6UvpbKU/s1600-h/FermiHaze.jpg"><img src="http://4.bp.blogspot.com/_xEaWDp7BS1Q/SutZCbKRhtI/AAAAAAAAAms/SFos6UvpbKU/s320/FermiHaze.jpg" border="0" id="BLOGGER_PHOTO_ID_5398506476519130834" alt="" style="margin: 0pt 0pt 10px 10px; float: right; cursor: pointer; width: 320px; height: 182px;"/></a>. But the same electrons should also produce gamma rays when interacting with the interstellar light in the process known as the inverse Compton scattering (Inverse Compton was the younger brother of Arthur), the ICS in short. The claim is that Fermi has detected these ICS photons. You can even see it yourself if you stare long enough into the picture.<br/><br/>The <a href="http://www.slac.stanford.edu/spires/find/hep/www?eprint=arXiv:0910.2998">second</a> paper also takes a look at the gamma rays arriving from the the galactic center, but uncovers a completely different signature. There seems to be a bumpy feature around a few GeV<a href="http://1.bp.blogspot.com/_xEaWDp7BS1Q/SutbOVzGvZI/AAAAAAAAAm0/Xutbv3T2r6M/s1600-h/dan.jpg"><img src="http://1.bp.blogspot.com/_xEaWDp7BS1Q/SutbOVzGvZI/AAAAAAAAAm0/Xutbv3T2r6M/s320/dan.jpg" border="0" id="BLOGGER_PHOTO_ID_5398508880261463442" alt="" style="margin: 0pt 0pt 10px 10px; float: right; cursor: pointer; width: 281px; height: 226px;"/></a> that does not fit a simple power-law spectrum expected from the background. The paper says that a dark matter particle of mass around 30 GeV annihilating into b quark pairs can fit the bump. The required annihilation cross section is fairly low, of order $10^{-25} cm^3/s$, only a factor of 3 larger than that needed to explain the observed abundance of dark matter via a thermal relic. That would put this dark matter particle closer to a standard WIMP, as opposed to the recently popular dark matter particles designed to explain the PAMELA positron excess who need a much larger mass and cross section.<br/><br/>Sadly, collider physics has a long way to go before reaching the same level of openness. Although collider experiments are 100% financed by public funds, and although acquired data have no commercial value, the data remains a property of the collaboration without ever being publicly released, not even after the collaboration has dissolved into nothingness. The only logical reason to explain that is <span style="font-style: italic;">inertia</span> - a quick and easy access to data and analysis tools has only quite recently become available to everybody. Another argument raised on that occasion is that only the collaboration who produced the data is able to  understand and properly handle them. That is of course irrelevant. Surely, the collaboration can make any analysis ten times better and more reliably. However, some analyses are simply never done either due to lack of manpower or laziness, and others are marred by theoretical prejudices. The LEP experiment is a perfect example here. Several important searches have never been done because, at the time,  there was no motivation from popular theories. In particular,  it is not excluded that the Higgs boson exist with a mass accessible to LEP (that is less than 115 GeV), but it was missed because some possible decay channels have not been studied.  It may well be  that ground breaking discoveries are stored on the LEP tapes rotting on dusty shelves in CERN catacombs. That danger could  be easily avoided if the LEP data were publicly available in an accessible form.<br/><br/>In the end, what do we have to lose? In the worst case scenario, the unrestricted access to data will just lead to more entries in my blog ;-)<br/><br/><span style="font-weight: bold;">Update:</span> At the<a href="http://fermi.gsfc.nasa.gov/science/symposium/2009/"> FERMI Symposium </a>this week  in Washington the collaboration trashed both of the above dark matter claims.<div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/2846514233477399562-3975800791031710181?l=resonaances.blogspot.com" height="1" width="1"/></div></div>
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    <author>
      <name>Jester</name>
      <uri>http://www.blogger.com/profile/16844247827820646813</uri>
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      <id>tag:blogger.com,1999:blog-2846514233477399562</id>
      <updated>2009-11-07T21:03:59+01:00</updated>
      <title type="text">RESONAANCES</title>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-2846514233477399562.post-6452307901936784</id>
    <published>2009-11-07T06:04:00+01:00</published>
    <updated>2009-11-07T06:15:16+01:00</updated>
    <title type="text">Higgs chased away from another hole</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">The hunt for the Higgs continues.  Tevatron is running at full steam hoping to catch a glimpse of the sucker before the LHC joins in the game. If the standard model is correct, the entire range of allowed Higgs masses will be covered within next 3-4 years. But there is one disturbing puzzle: indirect measurement indicate that we should have already found the Higgs! Indeed, precision measurements at LEP and Tevatron - mostly lepton asymmetries of Z decay and the value of the W boson mass - are best explained if the Higgs mass is some 80-90 GeV, whereas the direct limit from LEP implies that it must be heavier than 115 GeV. <br/><br/>There is one more reason, this time purely theoretical, to expect that the Higgs may be lighter than the naive LEP bound. If supersymmetry is relevant at the weak scale it is in general very uncomfortable with a heavy Higgs. Well, they keep telling you that the upper limit in the MSSM is 130 GeV. But that requires stretching the parameters of the model to the point of breaking, while the natural prediction is 90-100 GeV. Indeed, not finding the Higgs at LEP is probably the primary reason to disbelieve that supersymmetry is relevant at low energies.<br/><br/>Is it possible that Higgs is lighter than 115 GeV and LEP missed it? The answer is yes, because the LEP searches have left many loopholes. Sensitivity of LEP analyses deteriorates if the Higgs <a href="http://3.bp.blogspot.com/_xEaWDp7BS1Q/SvUBnghh7UI/AAAAAAAAAm8/OcucN--Rux0/s1600-h/HiggsTo4Tau.jpg"><img src="http://3.bp.blogspot.com/_xEaWDp7BS1Q/SvUBnghh7UI/AAAAAAAAAm8/OcucN--Rux0/s320/HiggsTo4Tau.jpg" border="0" id="BLOGGER_PHOTO_ID_5401225106357873986" alt="" style="margin: 0pt 0pt 10px 10px; float: right; cursor: pointer; width: 320px; height: 155px;"/></a>decays into a many-body final state, which is possible in some extensions of the standard model. One popular theory where this could happen is the NMSSM - the 2.0 version of the MSSM with an additional singlet. Roughly, the Higgs could first decay into the new singlet, who in turn decays into two tau leptons, which amounts to Higgs decaying into four tau leptons. This funny decay topology could escape LEP searches even if the Higgs is as light as 86 GeV! That is the case not because of deep physical reasons, but simply because LEP collaborations were too lazy to search for it (in comparison, Higgs decaying into four b-quarks, which was studied by LEP, is excluded for the Higgs mass up to 110 GeV).<br/><br/>But not anymore - this particular gaping hole has been recently sealed. A group of brave adventure-seekers  ventured into CERN caverns, excavated the ancient LEP data and analyzed them lookig for the Higgs-to-4tau signal.  The results were <a href="http://indico.cern.ch/conferenceDisplay.py?confId=71475">presented</a> this week at the ALEPH meeting celebrating the 20th anniversary and 9th anniversary of its demise. Of course, there is nothing there, in case you had any doubts. The new limit for the Higgs-to-4tau channel excludes the Higgs mass smaller than 105-110 GeV. Yet the beautiful thing in that analysis is that going back to the LEP data is still possible, if only there is reason, and will, and cheap work force.<br/><a href="http://2.bp.blogspot.com/_xEaWDp7BS1Q/SvUBztaEIjI/AAAAAAAAAnE/K4m4iVpIUG4/s1600-h/HiggsTo4Tau_Limit.jpg"><img src="http://2.bp.blogspot.com/_xEaWDp7BS1Q/SvUBztaEIjI/AAAAAAAAAnE/K4m4iVpIUG4/s320/HiggsTo4Tau_Limit.jpg" border="0" id="BLOGGER_PHOTO_ID_5401225315974652466" alt="" style="margin: 0px auto 10px; display: block; text-align: center; cursor: pointer; width: 320px; height: 183px;"/></a>So, is the idea of the hidden light Higgs dead? It has definitely received a serious blow, but it can still survive in some perverse models where Higgs decays into four light jets, at least until someone ventures to kill that too. Anyway, never say dead; there is no experimental results that theorists could not find a way around ;-)<div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/2846514233477399562-6452307901936784?l=resonaances.blogspot.com" height="1" width="1"/></div></div>
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      <name>Jester</name>
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      <id>tag:blogger.com,1999:blog-2846514233477399562</id>
      <updated>2009-11-07T21:03:59+01:00</updated>
      <title type="text">RESONAANCES</title>
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    <id>tag:blogger.com,1999:blog-10448119.post-1437087215744051926</id>
    <published>2009-11-06T21:24:00-05:00</published>
    <updated>2009-11-06T21:29:42-05:00</updated>
    <category term="seminar" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="galaxy" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="cosmology" scheme="http://www.blogger.com/atom/ns#"/>
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    <title type="text">galaxies, homogeneity</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>In the morning, Jeremy Tinker (Berkeley) led our group meeting with a discussion of information about galaxy evolution from clustering.  In the approximation that we know the dark matter model, the relationship between galaxies and dark matter can be parameterized and then the observed galaxy—galaxy clustering puts constraints on how the galaxies could possibly form and evolve.  He has some counterintuitive results, from the fact that at intermediate redshift, the large-scale clustering of red and blue galaxies is very similar.</p>

<p>In the afternoon, Marc Kamionkowski (Caltech) gave the Big Apple Colloquium about the isotropy and homogeneity of large-scale structure, and in particular the cosmic microwave background.  He is building non-natural models that permit anisotropy in the power spectrum while preserving isotropy in the temperature and density and all else.  There is a small amount of evidence for this statistical anisotropy situation in the current data; it is a long shot but if it holds up it is extremely important.</p><div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/10448119-1437087215744051926?l=hoggresearch.blogspot.com" height="1" width="1"/></div></div>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://terrytao.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>Terence Tao</name>
						
      <uri>http://www.math.ucla.edu/~tao</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Reading seminar 4: “Stable group theory and approximate subgroups”, by Ehud Hrushovski</div>
    </title>
		
    <link href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/" rel="alternate" type="text/html"/>
		
    <id>http://terrytao.wordpress.com/?p=3081</id>
		
    <updated>2009-11-07T00:48:46+00:00</updated>
		
    <published>2009-11-06T05:10:53+00:00</published>
		
    <category term="Logic reading seminar" scheme="http://terrytao.wordpress.com/"/>
    <category term="math.CO" scheme="http://terrytao.wordpress.com/"/>
    <category term="math.LO" scheme="http://terrytao.wordpress.com/"/>
    <category term="definability" scheme="http://terrytao.wordpress.com/"/>
    <category term="Ehud Hrushovski" scheme="http://terrytao.wordpress.com/"/>
    <category term="henry towsner" scheme="http://terrytao.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">This week, Henry Towsner concluded his portion of reading seminar of the Hrushovski paper, by discussing (a weaker, simplified version of) main model-theoretic theorem (Theorem 3.4 of Hrushovski), and described how this theorem implied the combinatorial application in Corollary 1.2 of Hrushovski. The presentation here differs slightly from that in Hrushovski’s paper, for instance [...]<img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=3081&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div>
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    <content type="xhtml" xml:base="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>
 This week, <a href="http://www.math.ucla.edu/~hpt/">Henry Towsner</a> concluded his portion of <a href="http://terrytao.wordpress.com/category/teaching/logic-reading-seminar/">reading seminar</a> of the <a href="http://arxiv.org/abs/0909.2190">Hrushovski paper</a>, by discussing (a weaker, simplified version of) main model-theoretic theorem (Theorem 3.4 of Hrushovski), and described how this theorem implied the combinatorial application in Corollary 1.2 of Hrushovski. The presentation here differs slightly from that in Hrushovski’s paper, for instance by avoiding mention of the more general notions of S1 ideals and forking.
</p>
<p>
Here is a collection of resources so far on the Hrushovski paper: </p>
<ul>
<li> <a href="http://terrytao.files.wordpress.com/2009/11/hrushovskinotes-2.pdf">Henry Towsner’s notes</a> (which most of Notes 2-4 have been based on); </li>
<li> <a href="http://www.math.ucla.edu/~alexus/papers/talks/udi1.pdf">Alex Usvyatsov’s notes</a> on the derivation of Corollary 1.2 (broadly parallel to the notes here); </li>
<li> <a href="http://www.math.uiuc.edu/~vddries/approx.pdf">Lou van den Dries’ notes</a> (covering most of what we have done so far, and also material on stable theories); and </li>
<li> <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#comment-42065">Anand Pillay’s sketch</a> of a simplified proof of Theorem 1.1.
</li>
</ul>
<p>
<span id="more-3081"/>
</p>
<p/>
<p align="center"><b> —  1. Theorem 3.4  — </b></p>
<p>
Here is a weakened version of Hrushovski’s Theorem 3.4:
</p>
<blockquote><p><b>Theorem 1</b> <a name="main"/> Let <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> be a countable model of a language extending the language of groups, with a universal extension <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/>. Let <img class="latex" title="{\mu}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu}"/> be a continuous, invariant Keisler measure that is also invariant under translations. Let <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> be a symmetric definable subset of <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> with <img class="latex" title="{\mu(X) = 1}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(X)+=+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X) = 1}"/> and <img class="latex" title="{\mu(X \cdot X)}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(X+%5Ccdot+X)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X \cdot X)}"/> finite, and let <img class="latex" title="{\tilde G}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/> be the group generated by <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>. Let <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> be a wide type over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> contained in <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>, and suppose that for every <img class="latex" title="{a \in q(G)}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+q(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in q(G)}"/>, there exists <img class="latex" title="{b \in q(G)}" src="http://s2.wordpress.com/latex.php?latex=%7Bb+%5Cin+q(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b \in q(G)}"/> such that <img class="latex" title="{tp(a/M \cup \{b\})}" src="http://s3.wordpress.com/latex.php?latex=%7Btp(a/M+%5Ccup+%5C%7Bb%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M \cup \{b\})}"/> and <img class="latex" title="{tp(b/M \cup \{a\})}" src="http://s1.wordpress.com/latex.php?latex=%7Btp(b/M+%5Ccup+%5C%7Ba%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(b/M \cup \{a\})}"/> are both wide. </p>
<p>
Then the set <img class="latex" title="{S := q^{-1} q q^{-1} q}" src="http://s2.wordpress.com/latex.php?latex=%7BS+:=+q%5E%7B-1%7D+q+q%5E%7B-1%7D+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S := q^{-1} q q^{-1} q}"/> is a normal subgroup of <img class="latex" title="{\tilde G}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/>. </p>
</blockquote>
<p/>
<blockquote><p><b>Remark 1</b>  The condition about <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> and <img class="latex" title="{b}" src="http://s2.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> seems to be a statement that there exist plenty of pairs <img class="latex" title="{(a,b)}" src="http://s3.wordpress.com/latex.php?latex=%7B(a,b)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(a,b)}"/> in <img class="latex" title="{q(G)}" src="http://s1.wordpress.com/latex.php?latex=%7Bq(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q(G)}"/> that are in “general position” somehow. In the case of abelian groups, it seems that this hypothesis not necessary. The hypothesis is for all <img class="latex" title="{a \in q(G)}" src="http://s2.wordpress.com/latex.php?latex=%7Ba+%5Cin+q(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in q(G)}"/>, but by homogeneity it suffices to verify it for a single <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> (since the action of the automorphism group of <img class="latex" title="{G}" src="http://s1.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is transitive on <img class="latex" title="{q(G)}" src="http://s2.wordpress.com/latex.php?latex=%7Bq(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q(G)}"/>). </p></blockquote>
<p/>
<blockquote><p><b>Remark 2</b>  Interestingly, it seems that no doubling condition on <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> is needed to prove this theorem, but the doubling condition arises when one wants to put <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> to use. </p></blockquote>
<p/>
<blockquote><p><b>Remark 3</b>  As <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> is wide, <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is wide also. If we also assume that every finite product <img class="latex" title="{X^{\cdot n} = X \cdot \ldots \cdot X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%5E%7B%5Ccdot+n%7D+=+X+%5Ccdot+%5Cldots+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^{\cdot n} = X \cdot \ldots \cdot X}"/> has finite measure, this leads to the consequence that the index of <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> in <img class="latex" title="{\tilde G}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/> does not exceed <img class="latex" title="{2^{\aleph_0}}" src="http://s1.wordpress.com/latex.php?latex=%7B2%5E%7B%5Caleph_0%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^{\aleph_0}}"/> in cardinality (i.e. has <em>bounded index</em>, see Lemma 1 of <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 2</a>). Indeed, if this were not the case, then one could find more than <img class="latex" title="{2^{\aleph_0}}" src="http://s2.wordpress.com/latex.php?latex=%7B2%5E%7B%5Caleph_0%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^{\aleph_0}}"/> disjoint cosets <img class="latex" title="{Sa_i}" src="http://s3.wordpress.com/latex.php?latex=%7BSa_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Sa_i}"/> in <img class="latex" title="{\tilde G}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/>, and hence in some finite product <img class="latex" title="{X^{\cdot n}}" src="http://s2.wordpress.com/latex.php?latex=%7BX%5E%7B%5Ccdot+n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^{\cdot n}}"/>. By Section 4 of <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 2</a>, <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is <img class="latex" title="{\bigwedge}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable, and so is the intersection of countably many definable sets <img class="latex" title="{S_n}" src="http://s2.wordpress.com/latex.php?latex=%7BS_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n}"/>. For any distinct <img class="latex" title="{i,j}" src="http://s3.wordpress.com/latex.php?latex=%7Bi,j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{i,j}"/>, <img class="latex" title="{Sa_i, Sa_j}" src="http://s1.wordpress.com/latex.php?latex=%7BSa_i,+Sa_j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Sa_i, Sa_j}"/> are disjoint, thus by saturation we have <img class="latex" title="{S_{n(i,j)} a_i \cap S_{n(i,j)} a_j}" src="http://s2.wordpress.com/latex.php?latex=%7BS_%7Bn(i,j)%7D+a_i+%5Ccap+S_%7Bn(i,j)%7D+a_j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_{n(i,j)} a_i \cap S_{n(i,j)} a_j}"/> non-empty for some integer <img class="latex" title="{n(i,j)}" src="http://s3.wordpress.com/latex.php?latex=%7Bn(i,j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n(i,j)}"/>. By the <a href="http://en.wikipedia.org/wiki/Infinitary_combinatorics">Erdös-Rado theorem</a> (an infinitary analogue of Ramsey’s theorem), we can then ass to a countable set of indices <img class="latex" title="{i}" src="http://s1.wordpress.com/latex.php?latex=%7Bi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{i}"/> in which the <img class="latex" title="{n(i,j) = n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn(i,j)+=+n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n(i,j) = n}"/> are constant, thus we have a countable set of disjoint translates <img class="latex" title="{S_n a_i}" src="http://s3.wordpress.com/latex.php?latex=%7BS_n+a_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n a_i}"/>, which live in some finite product <img class="latex" title="{X^{\cdot n}}" src="http://s1.wordpress.com/latex.php?latex=%7BX%5E%7B%5Ccdot+n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^{\cdot n}}"/>. But as <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is wide, <img class="latex" title="{S_n}" src="http://s3.wordpress.com/latex.php?latex=%7BS_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n}"/> has positive measure, while <img class="latex" title="{X^{\cdot n}}" src="http://s1.wordpress.com/latex.php?latex=%7BX%5E%7B%5Ccdot+n%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^{\cdot n}}"/> has finite leasure, leading to a contradiction. </p></blockquote>
<p/>
<blockquote><p><b>Remark 4</b>  The set <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> can also be defined in a more “<a href="http://en.wikipedia.org/wiki/Characteristic_subgroup">characteristic</a>” fashion as the smallest <img class="latex" title="{\bigwedge}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable subgroup of <img class="latex" title="{\tilde G}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/> of bounded index; we’ll return to this point in a later note (I think). </p></blockquote>
<p/>
<blockquote><p><b>Remark 5</b>  Here is one example of how the group <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> emerges. Start with a finite combinatorial model, in which <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> is a discrete interval <img class="latex" title="{\{-N,\ldots,N\}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7B-N,%5Cldots,N%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{-N,\ldots,N\}}"/> and the group is the integers; we normalise <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> to have measure <img class="latex" title="{1}" src="http://s3.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/>. Taking ultralimits, we end up with a non-standard discrete interval <img class="latex" title="{X = \{-N,\ldots,N\}}" src="http://s1.wordpress.com/latex.php?latex=%7BX+=+%5C%7B-N,%5Cldots,N%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X = \{-N,\ldots,N\}}"/> in the non-standard integers, with <img class="latex" title="{\mu}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu}"/> being the counting measure normalised to give <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> a measure of <img class="latex" title="{1}" src="http://s1.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/>. (This is not yet a saturated model, but yet us ignore this issue.) Note that the subsets <img class="latex" title="{\{-N/k,\ldots,N/k\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7B-N/k,%5Cldots,N/k%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{-N/k,\ldots,N/k\}}"/> are definable for any standard natural number <img class="latex" title="{k}" src="http://s3.wordpress.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k}"/>. Their intersection <img class="latex" title="{S := \bigcap_k \{-N/k,\ldots,N/k\}}" src="http://s1.wordpress.com/latex.php?latex=%7BS+:=+%5Cbigcap_k+%5C%7B-N/k,%5Cldots,N/k%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S := \bigcap_k \{-N/k,\ldots,N/k\}}"/> is a wide subgroup; if <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> was a “generic” type in <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> then <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> would be wide, and <img class="latex" title="{q^{-1} q q^{-1} q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%5E%7B-1%7D+q+q%5E%7B-1%7D+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q^{-1} q q^{-1} q}"/> would generate <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> (this is vaguely reminiscent of the “Bogulybov theorem” in additive combinatorics). </p></blockquote>
<p/>
<p>
To apply Theorem <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#main">1</a>, we need the following auxiliary lemma (a weakened version of Hrushovski Lemma 2.15):
</p>
<blockquote><p><b>Lemma 2</b> <a name="sub"/> Let <img class="latex" title="{B}" src="http://s1.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/> be a definable set of positive measure. Then we can refine <img class="latex" title="{B}" src="http://s2.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/> to a wide type <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> such that for every <img class="latex" title="{a \in q(G)}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+q(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in q(G)}"/>, there exists <img class="latex" title="{b \in q(G)}" src="http://s2.wordpress.com/latex.php?latex=%7Bb+%5Cin+q(G)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b \in q(G)}"/> such that <img class="latex" title="{tp(a/M \cup \{b\})}" src="http://s3.wordpress.com/latex.php?latex=%7Btp(a/M+%5Ccup+%5C%7Bb%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M \cup \{b\})}"/> and <img class="latex" title="{tp(b/M \cup \{a\})}" src="http://s1.wordpress.com/latex.php?latex=%7Btp(b/M+%5Ccup+%5C%7Ba%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(b/M \cup \{a\})}"/> are both wide. </p></blockquote>
<p/>
<p>
This lemma can be viewed as a more technical variant of Lemma 2 from <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 2</a>.
</p>
<p>
To prove this lemma we need a technical sublemma:
</p>
<blockquote><p><b>Lemma 3</b> <a name="subsub"/> Let <img class="latex" title="{P}" src="http://s2.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> be a definable set of positive measure, and suppose that the product <img class="latex" title="{P \times P}" src="http://s3.wordpress.com/latex.php?latex=%7BP+%5Ctimes+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \times P}"/> is covered by two definable sets <img class="latex" title="{C, D}" src="http://s1.wordpress.com/latex.php?latex=%7BC,+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C, D}"/> (these are sets of pairs, of course). Then one can refine <img class="latex" title="{P}" src="http://s2.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> to a definable subset <img class="latex" title="{P'}" src="http://s3.wordpress.com/latex.php?latex=%7BP'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P'}"/> of positive measure, such that at least one of the following holds: </p>
<ul>
<li> (i) For every <img class="latex" title="{a \in P'}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+P'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in P'}"/>, the set <img class="latex" title="{C_a := \{ b: (a,b) \in C \}}" src="http://s2.wordpress.com/latex.php?latex=%7BC_a+:=+%5C%7B+b:+(a,b)+%5Cin+C+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a := \{ b: (a,b) \in C \}}"/> has positive measure; or </li>
<li> (ii) For every <img class="latex" title="{b \in P'}" src="http://s3.wordpress.com/latex.php?latex=%7Bb+%5Cin+P'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b \in P'}"/>, the set <img class="latex" title="{D^b := \{ a: (a,b) \in D \}}" src="http://s1.wordpress.com/latex.php?latex=%7BD%5Eb+:=+%5C%7B+a:+(a,b)+%5Cin+D+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D^b := \{ a: (a,b) \in D \}}"/> has positive measure.
</li>
</ul>
</blockquote>
<p/>
<p>
<em>Proof:</em>  We can refine <img class="latex" title="{C, D}" src="http://s2.wordpress.com/latex.php?latex=%7BC,+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C, D}"/> to be contained in <img class="latex" title="{P \times P}" src="http://s3.wordpress.com/latex.php?latex=%7BP+%5Ctimes+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \times P}"/>. At least one of <img class="latex" title="{C, D}" src="http://s1.wordpress.com/latex.php?latex=%7BC,+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C, D}"/> must have positive measure; let’s say that <img class="latex" title="{\mu(C)=0}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(C)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C)=0}"/>. We can find a definable set <img class="latex" title="{Q_n}" src="http://s3.wordpress.com/latex.php?latex=%7BQ_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q_n}"/> between <img class="latex" title="{\{ a: \mu(C_a) &gt; 1/n \}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7B+a:+%5Cmu(C_a)+%3E+1/n+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ a: \mu(C_a) &gt; 1/n \}}"/> and <img class="latex" title="{\{ a: \mu(C_a) \geq 1/n \}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7B+a:+%5Cmu(C_a)+%5Cgeq+1/n+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ a: \mu(C_a) \geq 1/n \}}"/>. If any of these <img class="latex" title="{Q_n}" src="http://s3.wordpress.com/latex.php?latex=%7BQ_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q_n}"/> has positive measure, then we can just take <img class="latex" title="{P' := Q_n}" src="http://s1.wordpress.com/latex.php?latex=%7BP'+:=+Q_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P' := Q_n}"/>, so we may assume instead that <img class="latex" title="{\mu(Q_n)=0}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(Q_n)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(Q_n)=0}"/> for all <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, which implies that <img class="latex" title="{\mu(C) = 0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(C)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C) = 0}"/> by Fubini’s theorem (which can be extended to Kiesler measures, at least in the weak form we need here), giving the desired contradiction. <img class="latex" title="\Box" src="http://s2.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
Now we prove Lemma <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#sub">2</a>. By starting with <img class="latex" title="{B}" src="http://s3.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/> and refining repeatedly using Lemma <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#subsub">3</a> (enumerating all the definable sets, <img class="latex" title="{P}" src="http://s1.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> and pairs of definable sets <img class="latex" title="{C,D}" src="http://s2.wordpress.com/latex.php?latex=%7BC,D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C,D}"/>, so that each pair is revisited infinitely often) one can find a type <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> refining <img class="latex" title="{B}" src="http://s1.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/> with the property that whenever <img class="latex" title="{P}" src="http://s2.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> is a definable set containing <img class="latex" title="{q({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Bq(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q({\Bbb U})}"/>, and <img class="latex" title="{P \times P}" src="http://s1.wordpress.com/latex.php?latex=%7BP+%5Ctimes+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \times P}"/> is covered by two definable sets <img class="latex" title="{C, D}" src="http://s2.wordpress.com/latex.php?latex=%7BC,+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C, D}"/>, then either <img class="latex" title="{C_a}" src="http://s3.wordpress.com/latex.php?latex=%7BC_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a}"/> has positive measure for all <img class="latex" title="{a \in P}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in P}"/>, or <img class="latex" title="{D^b}" src="http://s2.wordpress.com/latex.php?latex=%7BD%5Eb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D^b}"/> has positive measure for all <img class="latex" title="{b \in P}" src="http://s3.wordpress.com/latex.php?latex=%7Bb+%5Cin+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b \in P}"/>. In particular (setting <img class="latex" title="{C=P \times P}" src="http://s1.wordpress.com/latex.php?latex=%7BC=P+%5Ctimes+P%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C=P \times P}"/> and <img class="latex" title="{D}" src="http://s2.wordpress.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D}"/> empty) this implies that <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> is wide.
</p>
<p>
Now let <img class="latex" title="{a \in q({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+q(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in q({\Bbb U})}"/>, and define <img class="latex" title="{q_a}" src="http://s2.wordpress.com/latex.php?latex=%7Bq_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q_a}"/> to be the type <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>, refined using the complement of all the sets of the form <img class="latex" title="{C_a}" src="http://s1.wordpress.com/latex.php?latex=%7BC_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a}"/> for definable <img class="latex" title="{C}" src="http://s2.wordpress.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C}"/> with <img class="latex" title="{\mu(C_a)=0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(C_a)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C_a)=0}"/>, and the complement of the sets of the form <img class="latex" title="{D_a}" src="http://s1.wordpress.com/latex.php?latex=%7BD_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D_a}"/> for definable <img class="latex" title="{D}" src="http://s2.wordpress.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D}"/> with <img class="latex" title="{\mu(D^a)=0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(D%5Ea)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(D^a)=0}"/> (note the asymmetry here!). We claim that this collection of sentences is still finitely satisfiable. Indeed, if this were not the case, <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> would have to be covered by <img class="latex" title="{C_a \cup D_a}" src="http://s2.wordpress.com/latex.php?latex=%7BC_a+%5Ccup+D_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a \cup D_a}"/> for some definable <img class="latex" title="{C, D}" src="http://s3.wordpress.com/latex.php?latex=%7BC,+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C, D}"/> with <img class="latex" title="{\mu(C_a)=\mu(D^a)=0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(C_a)=%5Cmu(D%5Ea)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C_a)=\mu(D^a)=0}"/>. Write <img class="latex" title="{P := C_a \cup D_a}" src="http://s2.wordpress.com/latex.php?latex=%7BP+:=+C_a+%5Ccup+D_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P := C_a \cup D_a}"/>, then the set <img class="latex" title="{\{ x: P = C_x \cup D_x \}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7B+x:+P+=+C_x+%5Ccup+D_x+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ x: P = C_x \cup D_x \}}"/> is definable and contains <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/>, and thus contains <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>. If we set <img class="latex" title="{P' := \{ x \in P: P = C_x \cup D_x \}}" src="http://s3.wordpress.com/latex.php?latex=%7BP'+:=+%5C%7B+x+%5Cin+P:+P+=+C_x+%5Ccup+D_x+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P' := \{ x \in P: P = C_x \cup D_x \}}"/>, we thus see that <img class="latex" title="{P'}" src="http://s1.wordpress.com/latex.php?latex=%7BP'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P'}"/> is a definable set containing <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> and <img class="latex" title="{P' \times P' \subset C \cup D}" src="http://s3.wordpress.com/latex.php?latex=%7BP'+%5Ctimes+P'+%5Csubset+C+%5Ccup+D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P' \times P' \subset C \cup D}"/>, contradicting the construction of <img class="latex" title="{q'}" src="http://s1.wordpress.com/latex.php?latex=%7Bq'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'}"/>.
</p>
<p>
As <img class="latex" title="{q_a}" src="http://s2.wordpress.com/latex.php?latex=%7Bq_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q_a}"/> is finitely satisfiable, we may extend it to a type <img class="latex" title="{q'_a}" src="http://s3.wordpress.com/latex.php?latex=%7Bq'_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'_a}"/> over <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/>. Now let <img class="latex" title="{b}" src="http://s2.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> be any realisation of <img class="latex" title="{q'_a}" src="http://s3.wordpress.com/latex.php?latex=%7Bq'_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'_a}"/>. We claim that <img class="latex" title="{tp(b/M \cup \{a\})}" src="http://s1.wordpress.com/latex.php?latex=%7Btp(b/M+%5Ccup+%5C%7Ba%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(b/M \cup \{a\})}"/> is wide. For if not, then <img class="latex" title="{b}" src="http://s2.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> would be contained in a set <img class="latex" title="{C_a}" src="http://s3.wordpress.com/latex.php?latex=%7BC_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a}"/> of measure zero for some definable <img class="latex" title="{C}" src="http://s1.wordpress.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C}"/>, but by construction <img class="latex" title="{q_a({\Bbb U})}" src="http://s2.wordpress.com/latex.php?latex=%7Bq_a(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q_a({\Bbb U})}"/> and hence <img class="latex" title="{q'_a({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Bq'_a(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'_a({\Bbb U})}"/> is contained in the complement of <img class="latex" title="{C_a}" src="http://s1.wordpress.com/latex.php?latex=%7BC_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_a}"/>, a contradiction.
</p>
<p>
We similarly claim that <img class="latex" title="{tp(a/M \cup \{b\})}" src="http://s2.wordpress.com/latex.php?latex=%7Btp(a/M+%5Ccup+%5C%7Bb%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M \cup \{b\})}"/> is wide. For if not, then <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> is contained in a set <img class="latex" title="{D^b}" src="http://s1.wordpress.com/latex.php?latex=%7BD%5Eb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D^b}"/> of measure zero for some definable <img class="latex" title="{D}" src="http://s2.wordpress.com/latex.php?latex=%7BD%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D}"/>. since <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> and <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> have the same type over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, <img class="latex" title="{D^a}" src="http://s3.wordpress.com/latex.php?latex=%7BD%5Ea%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D^a}"/> has measure zero also, and so <img class="latex" title="{q_a}" src="http://s1.wordpress.com/latex.php?latex=%7Bq_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q_a}"/> is contained in the complement of <img class="latex" title="{D_a}" src="http://s2.wordpress.com/latex.php?latex=%7BD_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D_a}"/> by construction. In particular, <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> lies outside <img class="latex" title="{D_a}" src="http://s1.wordpress.com/latex.php?latex=%7BD_a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D_a}"/>, which is inconsistent with <img class="latex" title="{a}" src="http://s2.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> lying in <img class="latex" title="{D^b}" src="http://s3.wordpress.com/latex.php?latex=%7BD%5Eb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{D^b}"/>. This proves Lemma <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#sub">2</a>.
</p>
<blockquote><p><b>Remark 6</b>  As I understand it, the argument simplifies in the stable case, when the wideness of <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> over <img class="latex" title="{b}" src="http://s2.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> is equivalent to the wideness of <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> over <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/>. </p></blockquote>
<p/>
<p align="center"><b> —  2. Corollary 1.2  — </b></p>
<p>
Assuming Theorem <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#main">1</a>, we now establish the following combinatorial consequence, which is (a slightly weaker version of) Corollary 1.2 of Hrushovski:
</p>
<blockquote><p><b>Corollary 4</b> <a name="12"/> Let <img class="latex" title="{k,l,m}" src="http://s2.wordpress.com/latex.php?latex=%7Bk,l,m%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k,l,m}"/> be positive integers. Then for <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> sufficiently close to <img class="latex" title="{1}" src="http://s1.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/>, the following statement is true: whenever <img class="latex" title="{X_0}" src="http://s2.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> is a finite subset of a group <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> with the bounded quintipling property <img class="latex" title="{|X_0 X X| \leq k |X_0|}" src="http://s1.wordpress.com/latex.php?latex=%7B%7CX_0+X+X%7C+%5Cleq+k+%7CX_0%7C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{|X_0 X X| \leq k |X_0|}"/>, where <img class="latex" title="{X := X_0^{-1} X_0}" src="http://s2.wordpress.com/latex.php?latex=%7BX+:=+X_0%5E%7B-1%7D+X_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X := X_0^{-1} X_0}"/>, and for a proportion at least <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> of the <img class="latex" title="{l}" src="http://s1.wordpress.com/latex.php?latex=%7Bl%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{l}"/>-tuples <img class="latex" title="{(a_1,\ldots,a_l) \in (X \cdot X)^l}" src="http://s2.wordpress.com/latex.php?latex=%7B(a_1,%5Cldots,a_l)+%5Cin+(X+%5Ccdot+X)%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(a_1,\ldots,a_l) \in (X \cdot X)^l}"/>, one has <img class="latex" title="{|a_1^X \ldots a_l^X| \geq |X|/m}" src="http://s3.wordpress.com/latex.php?latex=%7B%7Ca_1%5EX+%5Cldots+a_l%5EX%7C+%5Cgeq+%7CX%7C/m%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{|a_1^X \ldots a_l^X| \geq |X|/m}"/> (recall that <img class="latex" title="{a^X := \{ x^{-1}ax: x \in X \}}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%5EX+:=+%5C%7B+x%5E%7B-1%7Dax:+x+%5Cin+X+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a^X := \{ x^{-1}ax: x \in X \}}"/>). Then there exists a subgroup <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> of <img class="latex" title="{X \cdot X}" src="http://s3.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X}"/> such that <img class="latex" title="{X_0}" src="http://s1.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> is contained in at most <img class="latex" title="{k(m+1)}" src="http://s2.wordpress.com/latex.php?latex=%7Bk(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k(m+1)}"/> cosets of <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>. </p></blockquote>
<p/>
<p>
We have weakened things a bit here by drawing the <img class="latex" title="{a_i}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_i}"/> from <img class="latex" title="{X \cdot X}" src="http://s2.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X}"/> rather than <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> (and also weakening bounded tripling to bounded quintipling); this is in order to achieve some minor simplifications in the proof.
</p>
<p>
We now prove the corollary, by the usual “compactness and contradiction” method. If the corollary failed for some <img class="latex" title="{k,l,m}" src="http://s1.wordpress.com/latex.php?latex=%7Bk,l,m%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k,l,m}"/>, then one can find a sequence of groups <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> with subsets <img class="latex" title="{X_0}" src="http://s3.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> of tripling uniformly bounded by <img class="latex" title="{k}" src="http://s1.wordpress.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k}"/>, such that the proportion of <img class="latex" title="{l}" src="http://s2.wordpress.com/latex.php?latex=%7Bl%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{l}"/>-tuples <img class="latex" title="{(a_1,\ldots,a_l)}" src="http://s3.wordpress.com/latex.php?latex=%7B(a_1,%5Cldots,a_l)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(a_1,\ldots,a_l)}"/> in <img class="latex" title="{(X \cdot X)^l}" src="http://s1.wordpress.com/latex.php?latex=%7B(X+%5Ccdot+X)%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(X \cdot X)^l}"/> with <img class="latex" title="{|a_1^X \ldots a_l^X| \geq |X|/m}" src="http://s2.wordpress.com/latex.php?latex=%7B%7Ca_1%5EX+%5Cldots+a_l%5EX%7C+%5Cgeq+%7CX%7C/m%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{|a_1^X \ldots a_l^X| \geq |X|/m}"/> approaches <img class="latex" title="{1}" src="http://s3.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/>, but such that there is no subgroup <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> of <img class="latex" title="{X \cdot X}" src="http://s2.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X}"/> which can cover <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> by <img class="latex" title="{k(m+1)}" src="http://s1.wordpress.com/latex.php?latex=%7Bk(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k(m+1)}"/> cosets.
</p>
<p>
Taking an ultralimit (and using counting measure normalised so that <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> has mass <img class="latex" title="{1}" src="http://s3.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/>), we obtain a subset <img class="latex" title="{X_0}" src="http://s1.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> of a group <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> and a continuous, invariant, translation-invariant Keisler measure <img class="latex" title="{\mu}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu}"/> so that <img class="latex" title="{\mu(X) = 1}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(X)+=+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X) = 1}"/>, <img class="latex" title="{\mu(X_0 X X) \leq k \mu(X_0)}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(X_0+X+X)+%5Cleq+k+%5Cmu(X_0)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X_0 X X) \leq k \mu(X_0)}"/>, and such that the set <img class="latex" title="{Q := \{ (a_1,\ldots,a_l) \in (X \cdot X)^l: \mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+0.5) \}}" src="http://s3.wordpress.com/latex.php?latex=%7BQ+:=+%5C%7B+(a_1,%5Cldots,a_l)+%5Cin+(X+%5Ccdot+X)%5El:+%5Cmu(+a_1%5EX+%5Cldots+a_l%5EX+)+%5Cgeq+%5Cmu(X)/(m+0.5)+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q := \{ (a_1,\ldots,a_l) \in (X \cdot X)^l: \mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+0.5) \}}"/> (say) has measure <img class="latex" title="{\mu(X \cdot X)^l}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(X+%5Ccdot+X)%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X \cdot X)^l}"/>. (Strictly speaking, one has to replace <img class="latex" title="{\mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(+a_1%5EX+%5Cldots+a_l%5EX+)+%5Cgeq+%5Cmu(X)/(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)}"/> by a definable predicate between <img class="latex" title="{\mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(+a_1%5EX+%5Cldots+a_l%5EX+)+%5Cgeq+%5Cmu(X)/(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)}"/> and <img class="latex" title="{\mu( a_1^X \ldots a_l^X ) &gt; \mu(X)/(m+1)}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(+a_1%5EX+%5Cldots+a_l%5EX+)+%3E+%5Cmu(X)/(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu( a_1^X \ldots a_l^X ) &gt; \mu(X)/(m+1)}"/>, but let’s ignore this technicality.) We then extend <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> to a universal model <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/>.
</p>
<p>
The set <img class="latex" title="{X_0}" src="http://s1.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> has positive measure (at least <img class="latex" title="{1/k}" src="http://s2.wordpress.com/latex.php?latex=%7B1/k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1/k}"/>, in fact), so by Lemma <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#sub">2</a>, we may refine it to a wide type <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> obeying the hypotheses of Theorem <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#main">1</a>, so that the set <img class="latex" title="{S := q^{-1} q q^{-1} q}" src="http://s1.wordpress.com/latex.php?latex=%7BS+:=+q%5E%7B-1%7D+q+q%5E%7B-1%7D+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S := q^{-1} q q^{-1} q}"/> is a group. Note that this set is contained in <img class="latex" title="{X \cdot X}" src="http://s2.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X}"/>.
</p>
<p>
Since <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> contains the wide type <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>, it is itself wide. By Section 4 of <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 2</a>, <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is <img class="latex" title="{\bigwedge}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable, and is thus the intersection of definable sets <img class="latex" title="{S_n}" src="http://s1.wordpress.com/latex.php?latex=%7BS_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n}"/>, which have positive measure as <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is wide; we can place this inside the definable set <img class="latex" title="{X \cdot X}" src="http://s3.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X}"/>. As <img class="latex" title="{Q}" src="http://s1.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> has full measure in <img class="latex" title="{(X \cdot X)^l}" src="http://s2.wordpress.com/latex.php?latex=%7B(X+%5Ccdot+X)%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(X \cdot X)^l}"/>, we see that <img class="latex" title="{Q}" src="http://s3.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> intersects <img class="latex" title="{S_n^l}" src="http://s1.wordpress.com/latex.php?latex=%7BS_n%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n^l}"/> for every <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, by saturation, <img class="latex" title="{Q}" src="http://s3.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> must also intersect <img class="latex" title="{S^l}" src="http://s1.wordpress.com/latex.php?latex=%7BS%5El%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S^l}"/>. In particular, there exists <img class="latex" title="{a_1,\ldots,a_l}" src="http://s2.wordpress.com/latex.php?latex=%7Ba_1,%5Cldots,a_l%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,\ldots,a_l}"/> in <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> such that </p>
<p align="center"><img class="latex" title="\displaystyle  \mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)." src="http://s1.wordpress.com/latex.php?latex=%5Cdisplaystyle++%5Cmu(+a_1%5EX+%5Cldots+a_l%5EX+)+%5Cgeq+%5Cmu(X)/(m+1).&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\displaystyle  \mu( a_1^X \ldots a_l^X ) \geq \mu(X)/(m+1)."/></p>
<p> On the other hand, as <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is normal in <img class="latex" title="{\tilde G}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Ctilde+G%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde G}"/>, the set <img class="latex" title="{a_1^X \ldots a_l^X}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_1%5EX+%5Cldots+a_l%5EX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1^X \ldots a_l^X}"/> lies in <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>. This implies that we cannot find more than <img class="latex" title="{\mu(X_0 X X) (m+1) / \mu(X) \leq k(m+1)}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(X_0+X+X)+(m+1)+/+%5Cmu(X)+%5Cleq+k(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X_0 X X) (m+1) / \mu(X) \leq k(m+1)}"/> disjoint translates <img class="latex" title="{xS}" src="http://s1.wordpress.com/latex.php?latex=%7BxS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{xS}"/>, <img class="latex" title="{x \in X_0}" src="http://s2.wordpress.com/latex.php?latex=%7Bx+%5Cin+X_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x \in X_0}"/>. As a consequence, <img class="latex" title="{X_0}" src="http://s3.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> is covered by at most <img class="latex" title="{k(m+1)}" src="http://s1.wordpress.com/latex.php?latex=%7Bk(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k(m+1)}"/> translates of <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, and so <img class="latex" title="{X^2}" src="http://s3.wordpress.com/latex.php?latex=%7BX%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^2}"/> can be covered by <img class="latex" title="{k^4 (m+1)^4}" src="http://s1.wordpress.com/latex.php?latex=%7Bk%5E4+(m+1)%5E4%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k^4 (m+1)^4}"/> such translates, including <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> itself. In particular, <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is both <img class="latex" title="{\bigwedge}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable and <img class="latex" title="{\bigvee}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cbigvee%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigvee}"/>-definable (it is the complement of all the other cosets in <img class="latex" title="{X^2}" src="http://s3.wordpress.com/latex.php?latex=%7BX%5E2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X^2}"/>). But any set <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> which is both <img class="latex" title="{\bigwedge}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable and <img class="latex" title="{\bigvee}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cbigvee%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigvee}"/>-definable has to be definable. (Proof: we can write <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> as the intersection of definable sets <img class="latex" title="{S_n}" src="http://s2.wordpress.com/latex.php?latex=%7BS_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S_n}"/> and also as the union of definable sets <img class="latex" title="{U_n}" src="http://s3.wordpress.com/latex.php?latex=%7BU_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{U_n}"/>. By saturation, <img class="latex" title="{U_n \backslash S_n}" src="http://s1.wordpress.com/latex.php?latex=%7BU_n+%5Cbackslash+S_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{U_n \backslash S_n}"/> must be empty for at least one <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, and the claim follows.) </p>
<p>
To summarise, <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is now a definable group which can cover <img class="latex" title="{X_0}" src="http://s1.wordpress.com/latex.php?latex=%7BX_0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X_0}"/> by at most <img class="latex" title="{k(m+1)}" src="http://s2.wordpress.com/latex.php?latex=%7Bk(m+1)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k(m+1)}"/> cosets. This is a first-order statement and so descends back to the original finitary models, but this then contradicts the construction of such sets, and proves the Corollary.
</p>
<blockquote><p><b>Remark 7</b>  The argument not only shows the existence of the set <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, but shows that this set is “definable”, in the sense that there are a finite number of first-order expressions using <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> and normalised cardinality, one of which is guaranteed to generate <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> whenever the hypotheses of Corollary <a href="http://terrytao.wordpress.com/2009/11/05/reading-seminar-4-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#12">4</a> are satisfied. Indeed, if this were not the case, one could construct a sequence of counterexamples for which no such recipe for constructing <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> would work for sufficiently late elements of this sequence, and then run the above argument to obtain a contradiction. </p></blockquote><p/>
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    <source>
      <title type="text">What's new</title>
      <subtitle type="text">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <updated>2009-11-07T00:48:46+00:00</updated>
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    <title>Glorious Dawn Record</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>I get a lot of press releases forward to me which usually get forwarded directly into my gmail archive.  But this one I'm happy to pass along: Third Man Records is <a href="http://www.thirdmanrecords.com/news.html">releasing</a> <a href="http://www.youtube.com/watch?v=zSgiXGELjbc">A Glorious Dawn</a>.  You know the Carl Sagan remix (w/ guest appearance of the Hawkmeister) that I've been looping over and over again while I work:</p><blockquote>Third Man Records is over the moon to announce the 7-inch release of "A Glorious Dawn" on November 9th.<br/>
...<br/>
The release is timed to coincide with the 75th anniversary of Sagan's birth. Also happening that day is a reception in United States' Congress with speeches by senators, NASA officials and assorted scientists, all hosted by the Planetary Society, which was co-founded by Sagan.<p/>

<p>Third Man Records, in conjunction with United Record Pressing, fabricated a special "Cosmos Colored Vinyl" of which 150 copies will be available...50 randomly inserted into mail orders for "A Glorious Dawn" and the remainder to be made available at the Third Man Records Nashville store front at noon on November 9th.</p>

<p>The one-sided single features a very special etching on the flipside. Reproduced from the original artwork, the etching copies the etching included with the Voyager Golden Record, set off into space in 1977 as the most elaborate message-in-a-bottle idea ever imagined. With its inclusion of Blind Willie Johnson's "Dark Was The Night" it goes without saying that the Voyager Golden Record is one of Third Man's favorite releases of all-time..</p></blockquote>I fell asleep last night listening to an episode of Cosmos.  Maybe that explains da alienz in my dreamz?<p/> <a href="http://scienceblogs.com/pontiff/2009/11/glorious_dawn_record.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/TheQuantumPontiff/~4/96o5dAuDpFs" height="1" width="1"/></div>
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    <id>http://scienceblogs.com/pontiff/2009/11/glorious_dawn_record.php</id>
         
    <category term="Astronomy"/>
         
         
    <published>2009-11-06T18:00:07-05:00</published>
      
    <updated>2009-11-06T18:00:07-05:00</updated>
    <source>
      <title>The Quantum Pontiff</title>
      <link href="http://scienceblogs.com/pontiff/" rel="alternate"/>
      <subtitle>Theoretical Musings</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T18:00:07-05:00</updated>
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    <title>Friday Random Ten, 11/06</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><ol>
<li><b>Porcupine Tree, "Kneel and Disconnect"</b>: New Porcupine Tree! It's
  always great to get new stuff from these guys. It's good, but it's not
  up to the quality of their last two albums. (But given that their last two
  were utterly amazing, that's not much of a criticism.)</li>
<li><b>Mind Games, "Royalty in Jeopardy"</b>: Some prog that I recently found
  via eMusic. They've got a sound that I describe as being sort of like a 
  mix between Yes and Marillion. They're very good - I wouldn't put them
  in the top ranks of neo-prog, but they're not at the bottom either.
</li><li><b>Riverside, "Cybernetic Pillow"</b>: Now, these guys, I would
  definitely put in the top ranks of neo-prog. Riverside is a 
  Polish prog-rock band, formed by members of a couple of other
  heavy metal bands. They're absolutely <em>brilliant</em>. This track
  is off their album "Rapid Eye Movement", which I'd recommend as a first
  Riverside album.</li>
<li><b>Marillion, "Hard as Love (acoustic)"</b>: This is the version of "Hard as
  Love"" from their recent acoustic album. HaL was one of their louder,
  poppier, catchier tunes - a Marillion rocker. To call this just an acoustic
  mix doesn't do it justice. They took the basic bones of the song,
  and completely rebuilt it. It's an amazing change. The acoustic
  version swaps the bridge and the chorus, completely changing the fell
  of the structure, and turning it into something that's almost a ballad.
  Amazing, and <em>much</em> better than the original version of the song.</li>
<li><b>Thinking Plague, "This Weird Wind"</b>: Thinking Plague is a group
  that I have a hard time describing. To me, they sound like a very out-there
  post-rock group with classical influences, but I've been told that 
  they call themselves a "Rock in Opposition" band. What they are is
  a distinctly peculiar ensemble. They've got vocals, but they use
  the singers voice like it's just another instrument in the mix - it's
  not leading the song in any way, it's just part of the music. The music
  itself is frequently atonal, with a very peculiar sound. The guitarist
  sounds <em>very</em> much like one of Robert Fripp's GuitarCraft students - but
  when I mentioned that in the past, he showed up in the comments saying
  "Who's Robert Fripp?" I love Thinking Plague, but I have a hard time
  recommending them - they're so strange that most people won't like
  them. If you're a big fan of both neo-progressive rock and 20th
  century classical, then definitely give them a listen.</li>
<li><b>EQ, "Closer"</b>: IQ is back! IQ is a progressive band that
  got started around the same time as Marillion. Also like Marillion, they
  started off sounding like a Peter Gabriel-era Genesis rip-off, but
  they've evolved their own very distinct sound over the years. They're
  absolutely fantastic - I'd put them up in the top of neo-progressive
  bands with Marillion and the Flower Kings. And they just released a new
  album, which is absolutely fantastic.</li>
<li><b>Sonic Youth, "Rain King (live)"</b>: Very typical Sonic Youth - strange
  tonality. Loud. Tons of hidden complexity. Brilliant. And performed
  live! No studio tricks here.</li>
<li><b>Kayo Dot, "The Useless Ladder"</b>: Another very hard-to-describe
  band. Roughly, they're what you get when a progressive metal band 
  decides to start writing 21st century classical chamber music. Very,
  very highly recommended.</li>

<li><b>Red Sparrowes, "And By Our Own Hand Did Every Last Bird Lie Silent In
Their Puddles, The Air Barren Of Songs As The Clouds Drifted Away. For Killing
Their Greatest Enemy, The Locusts Noisily Thanked Us And Turned Their Jaws
Toward Our Crops, Swallowing Our Greed Whole"</b>: It took me longer to type
the title of that than it did to listen to it. Red Sparrowes is a really
excellent post-rock band. But frankly, this track just annoys be because
of the damn title.</li>
<li><b>Rachel's, "A French Gallease"</b>: A beautiful track by my favorite
of the classically-leaning post-rock ensembles.</li> 
</ol> <a href="http://scienceblogs.com/goodmath/2009/11/friday_random_ten_1106.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/CyKN/~4/EYOBR7YlrNs" height="1" width="1"/></div>
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    <id>http://scienceblogs.com/goodmath/2009/11/friday_random_ten_1106.php</id>
         
    <category term="Music"/>
         
         
    <published>2009-11-06T14:58:50-05:00</published>
      
    <updated>2009-11-06T14:58:50-05:00</updated>
    <source>
      <title>Good Math, Bad Math</title>
      <link href="http://scienceblogs.com/goodmath/" rel="alternate"/>
      <subtitle>Finding the fun in good math; Shredding bad math and squashing the crackpots who espouse it.</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T14:58:50-05:00</updated>
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    <title>You Can’t Make This Stuff Up</title>
		
    <link href="http://feedproxy.google.com/~r/CosmicVarianceBlog/~3/psocdR8JxM0/" rel="alternate"/>
		
    <link href="http://blogs.discovermagazine.com/cosmicvariance/2009/11/06/you-cant-make-this-stuff-up/#comments" rel="replies" type="text/html"/>
		
    <published>2009-11-06T19:23:45+00:00</published>
		
    <author>
      <name>Julianne</name>
    </author>
				
    <category term="Science"/>
		
    <category term="Science and the Media"/>
		
    <category term="baguette thwarts science"/>
		
    <category term="LHC"/>

		
    <id>http://blogs.discovermagazine.com/cosmicvariance/?p=3135</id>
		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Lead paragraph from the Times Online UK about the latest LHC snafu:
The rehabilitation of the beleaguered Large Hadron Collider was on hold tonight after the failure of one of its powerful cooling units caused by an errant chunk of baguette.</div>
    </summary>
			
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Lead paragraph from the <a href="http://www.timesonline.co.uk/tol/news/science/physics/article6905250.ece">Times Online UK</a> about the latest LHC snafu:</p>
<blockquote><p>The rehabilitation of the beleaguered Large Hadron Collider was on hold tonight after the failure of one of its powerful cooling units caused by an errant chunk of baguette.</p></blockquote>

<p><a href="http://feedads.g.doubleclick.net/~a/Yqs0WIybg-5R9eKm1BXmRtsZVX8/0/da"><img ismap="true" src="http://feedads.g.doubleclick.net/~a/Yqs0WIybg-5R9eKm1BXmRtsZVX8/0/di" border="0"/></a><br/>
<a href="http://feedads.g.doubleclick.net/~a/Yqs0WIybg-5R9eKm1BXmRtsZVX8/1/da"><img ismap="true" src="http://feedads.g.doubleclick.net/~a/Yqs0WIybg-5R9eKm1BXmRtsZVX8/1/di" border="0"/></a></p><img src="http://feeds.feedburner.com/~r/CosmicVarianceBlog/~4/psocdR8JxM0" height="1" width="1"/></div>
    </content>
			<wfw:commentRss>http://blogs.discovermagazine.com/cosmicvariance/2009/11/06/you-cant-make-this-stuff-up/feed/</wfw:commentRss>
		<slash:comments>18</slash:comments>
		
    <updated>2009-11-06T19:23:45+00:00</updated>
    <source>
      <title>Cosmic Variance</title>
      <link href="http://blogs.discovermagazine.com/cosmicvariance" rel="alternate"/>
      <subtitle>Random samplings from a universe of ideas.</subtitle>
      <updated>2009-11-06T19:23:45+00:00</updated>
      <generator>http://wordpress.org/?v=2.8.4</generator><sy:updatePeriod>hourly</sy:updatePeriod><sy:updateFrequency>1</sy:updateFrequency>
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      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Poll: A Question of Character</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>"It's a question of character, of friendship. Hell, Leo, I ain't afraid to say it, it's a question of ethics." --Giovanni Gaspari</p>

<p>I'm back to lunchtime hoops after a two-week layoff due to teaching responsibilities. And this has reminded me of one of the great character tests that sports provide. Imagine that you're playing basketball, but are too tired to keep running with the fast break in both directions. You can't quit without pissing everybody off, though, and there's no-one you can have sub in for you. What do you do?</p>

<p>
&lt;a href="http://answers.polldaddy.com/poll/2219332/"&gt;What do you do when you're too tired to run the floor in a basketball game, but can't leave?&lt;/a&gt;&lt;span style="font-size:9px;"&gt;(&lt;a href="http://answers.polldaddy.com"&gt;opinion&lt;/a&gt;)&lt;/span&gt;
</p>

<p>This question is a nearly infallible test of a person's character. Except for those annoying bastards who are in such good shape that they never get tired of running. You never can tell what those guys will do.</p>
 <a href="http://scienceblogs.com/principles/2009/11/poll_a_question_of_character.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/Z2_TtY7MG7I" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/Z2_TtY7MG7I/poll_a_question_of_character.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/principles/2009/11/poll_a_question_of_character.php</id>
         
    <category term="Basketball"/>
         
         
    <published>2009-11-06T13:26:40-05:00</published>
      
    <updated>2009-11-06T13:26:40-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-07T11:21:56-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
      <id>http://scienceblogs.com/principles/</id>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>A Tactic Named Sue</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>A <del>puppet</del> <a href="http://scienceblogs.com/pontiff/2008/12/nature_on_el_naschie.php#comment-2053328">commenter</a> informs me that <a href="http://www.pressgazette.co.uk/story.asp?sectioncode=1&amp;storycode=44545&amp;c=1">El Naschie is suing Nature</a>.  El Naschie, you may remember, was the journal editor of Chaos, Solitons and Fractals who was accused of not reviewing his own papers in the journal.  To be expected, I suppose.   But the <a href="http://scienceblogs.com/pontiff/2008/12/nature_on_el_naschie.php#comment-2053328">commenter</a> that pointed this out is entertaining:</p><blockquote>Sarah Limbrick [Pontiff: writer of the above linked article about the suit] would surely be interested to know what the leading libel expert in England had to say about the Nature article complained of. He said he is in a state of disbelief that the worlds most respectable scientific journal Nature should publish an article which bears all the hallmarks of the tabloid press.  Another interesting point is the conspiracy theory linking the plagiarism of El Naschies work published in Scientific American with the Nature article as well as a far worse article published in Die Zeit. Interestingly all of these three publications are owned by Macmillan. I understand from confidential sources that a mega surprise will be released at the trial engulfing highly reputed names some of whom are Nobel laureates.</blockquote>OOooh, Nobel laureates in a libel case and conspiracy theories to boot!  That's bigger than the Scopes monkey trial!<p/> <a href="http://scienceblogs.com/pontiff/2009/11/a_tactic_named_sue.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/TheQuantumPontiff/~4/3mdGckmiIaE" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/TheQuantumPontiff/~3/3mdGckmiIaE/a_tactic_named_sue.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/pontiff/2009/11/a_tactic_named_sue.php</id>
         
    <category term="Off The Deep End"/>
         
         
    <published>2009-11-06T13:14:44-05:00</published>
      
    <updated>2009-11-06T13:14:44-05:00</updated>
    <source>
      <title>The Quantum Pontiff</title>
      <link href="http://scienceblogs.com/pontiff/" rel="alternate"/>
      <subtitle>Theoretical Musings</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T18:00:07-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/TheQuantumPontiff" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
      <id>http://scienceblogs.com/pontiff/</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://asymptotia.com/wp-atom.php">
		
    <author>
			
      <name>Clifford</name>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Presidential Star Party</div>
    </title>
		
    <link href="http://asymptotia.com/2009/11/06/presidential-star-party/" rel="alternate" type="text/html"/>
		
    <id>http://asymptotia.com/?p=5347</id>
		
    <updated>2009-11-06T18:08:45+00:00</updated>
		
    <published>2009-11-06T17:43:59+00:00</published>
		
    <category term="astronomy" scheme="http://asymptotia.com/"/>
    <category term="black people in science" scheme="http://asymptotia.com/"/>
    <category term="minorities in science" scheme="http://asymptotia.com/"/>
    <category term="science" scheme="http://asymptotia.com/"/>
    <category term="science education" scheme="http://asymptotia.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://asymptotia.com/wp-images/2009/11/star_party_white_house_dara_norman.jpg"><img class="alignleft size-full wp-image-5349" title="star_party_white_house_dara_norman" src="http://asymptotia.com/wp-images/2009/11/star_party_white_house_dara_norman.jpg" alt="star_party_white_house_dara_norman" width="250"/></a>This is a photo I borrowed from Dara Norman's <a href="http://blogs.nsbp.org/vector/2009/10/12/the-first-white-house-star-party/">blog post over on NSBP's Vector</a>. It is about the star party held over at hhe White House in October of this year. It looks like it was a lot of fun! Er, you may recognize one or two of  those people at the telescope...




-cvj</div>
    </summary>
		
    <link href="http://asymptotia.com/2009/11/06/presidential-star-party/#comments" rel="replies" type="text/html" thr:count="0"/>
		
    <link href="http://asymptotia.com/2009/11/06/presidential-star-party/feed/atom/" rel="replies" type="application/atom+xml" thr:count="0"/>
		<thr:total>0</thr:total>
	
    <source>
      <title type="text">Asymptotia</title>
      <updated>2009-11-06T18:08:45+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.7.1">WordPress</generator>
      <link href="http://asymptotia.com/" rel="alternate" type="text/html"/>
      <id>http://asymptotia.com/feed/atom/</id>
      <link href="http://asymptotia.com/feed/atom/" rel="self" type="application/atom+xml"/>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">UB40 - U3</div>
    </title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
statistical reminder<br/>
</p> <a href="http://scienceblogs.com/catdynamics/2009/11/ub40_-_u3.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2009/11/ub40_-_u3.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/jUfR5rV_SfE" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/jUfR5rV_SfE/ub40_-_u3.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/catdynamics/2009/11/ub40_-_u3.php</id>
         
    <category term="random"/>
         
         
    <published>2009-11-06T12:58:30-05:00</published>
      
    <updated>2009-11-06T12:58:30-05:00</updated>
    <source>
      <title>Dynamics of Cats</title>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate"/>
      <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>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T12:58:30-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
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      <id>http://scienceblogs.com/catdynamics/</id>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Plot Threads</div>
    </title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
Plot complexity is not, in and of itself, a measure of the quality of a work of communication, but it is surely a measure of something:</p> <a href="http://scienceblogs.com/catdynamics/2009/11/plot_threads.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2009/11/plot_threads.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/Xyrksuj8kq4" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/Xyrksuj8kq4/plot_threads.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/catdynamics/2009/11/plot_threads.php</id>
         
    <category term="random"/>
         
         
    <published>2009-11-06T11:50:20-05:00</published>
      
    <updated>2009-11-06T11:50:20-05:00</updated>
    <source>
      <title>Dynamics of Cats</title>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate"/>
      <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>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T12:58:30-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
      <id>http://scienceblogs.com/catdynamics/</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://blogs.uslhc.us/wp-atom.php">
		
    <author>
			
      <name>Vivek Jain</name>
						
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">ATLAS Upgrade</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2869" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2869</id>
		
    <updated>2009-11-06T16:48:23+00:00</updated>
		
    <published>2009-11-06T16:48:23+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>
    <category term="ATLAS" scheme="http://blogs.uslhc.us/"/>
    <category term="LHC" scheme="http://blogs.uslhc.us/"/>
    <category term="upgrade" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">You might think it odd that work has already started to upgrade parts of the ATLAS detector, even before the LHC has started running!
As I wrote in a previous post, one of the key operating parameters for the LHC is luminosity, i.e., the beam intensity. The design calls for a luminosity of 1034/cm2/sec; this means [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2869"><div xmlns="http://www.w3.org/1999/xhtml"><p>You might think it odd that work has already started to upgrade parts of the ATLAS detector, even before the LHC has started running!</p>
<p>As I wrote in <a href="http://blogs.uslhc.us/?p=2447">a previous post</a>, one of the key operating parameters for the LHC is luminosity, i.e., the beam intensity. The design calls for a luminosity of 10<sup>34</sup>/cm<sup>2</sup>/sec; this means that if you look at the beam head-on, it will contain 10<sup>34</sup> protons/sec spread over an area of 1 sq. cm. In reality, each beam consists of 2800 bunches each containing ~10<sup>11</sup> protons and about 0.03 mm in radius. Two such bunches collide every 25 nanoseconds, i.e., 40 million times/second; this is known as a bunch crossing.</p>
<p>The number of events that we collect is directly proportional to the luminosity. I had also written that the most common type of events that occur have a very large rate. What this implies is that when two proton bunches collide, most of the time we produce these “ordinary” events. For instance, when the luminosity is 10<sup>34</sup>, at each bunch crossing we get an average of 23 such events; they are easy to recognize, in the sense that they produce mainly low energy particles. So, when we produce an interesting event, say, a pair of top quarks or a Higgs boson, that event will be sitting atop this low-level “fuzz”. This background produces detectable signals in ATLAS, causing higher load on the trigger system and readout electronics, and pattern recognition problems in the reconstruction software. For instance, the <a href="http://blogs.uslhc.us/?p=1964">(TRT) sub-detector</a>, could have an occupancy rate as high as 10-20%, i.e., a non-negligible fraction of all wires will register hits; pattern recognition will be tough, but manageable. Other tracking sub-detectors are not a problem since they have much finer granulation (see Seth’s <a href="http://blogs.uslhc.us/?p=481">post on tracking</a>).  In addition, as particles produced in these “ordinary” events travel through the various sub-systems that are made out of silicon, they cause a slow degradation in them; detectors and electronics are made to resist this deterioration, but they do eventually fail.</p>
<p>When the luminosity starts to increase, as the LHC program calls for, these problems become much more serious. For instance, at a luminosity of 10<sup>35</sup>, each interesting event will be sitting atop a background of about 400 of these “junk” events; there is no way around it. As for the TRT, you can see that it will be useless.</p>
<p>The upgrade is planned in two phases. In the first phase, corresponding to a luminosity of 3*10<sup>34</sup>, currently scheduled for 2015 (but will depend on well the LHC performs), we plan to insert an extra layer of silicon sensors between the beam-pipe and the first silicon layer; by then, the first layer’s performance will have deteriorated enough to be noticeable. We will also upgrade some other detectors and electronics that sit close to the beam.</p>
<p>In the second phase, corresponding to a luminosity of 10<sup>35</sup>, all of the sub-systems that are used for tracking charged particles, i.e., the silicon layers and the TRT, will be replaced. All electronic readout for the detector will be replaced with more sophisticated stuff; the trigger logic and associated electronics will undergo a big overhaul, etc. This is scheduled for 2020.</p>
<p>These upgrades take time and effort, hence the early start. Most groups in the US and UK are already steering resources, in the form of people and money, towards the Phase I upgrade, e.g., my colleague, Hal Evans at Indiana University, is looking at some trigger improvements, and other countries are also joining in. We are used to this mode of operation; at one of my previous experiments (at the accelerator at Cornell University), we were simultaneously, analyzing data collected with version II of the experiment, starting to commission version II.5, and doing R\&amp;D on version III!</p>
<p>–Vivek Jain, Indiana University</p>
<a href="http://www.addtoany.com/share_save?linkurl=http://blogs.uslhc.us/?p=2869&amp;linkname=ATLAS%20Upgrade" class="a2a_dd addtoany_share_save"><img src="http://blogs.uslhc.us/wp-content/plugins/add-to-any/share_save_120_16.png" height="16" alt="Share/Bookmark" width="120"/></a></div>
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		<thr:total>3</thr:total>
	
    <source>
      <title type="text">US LHC Blog</title>
      <subtitle type="text">US LHC Blogs</subtitle>
      <updated>2009-11-06T16:48:23+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.8.4">WordPress</generator>
      <link href="http://blogs.uslhc.us/" rel="alternate" type="text/html"/>
      <id>http://blogs.uslhc.us/?feed=atom</id>
      <link href="http://blogs.uslhc.us/?feed=atom" rel="self" type="application/atom+xml"/>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">LHC: toast</div>
    </title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><br/>
LHC started overheating when a cooling unit cut out<br/>
</p> <a href="http://scienceblogs.com/catdynamics/2009/11/lhc_toast.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2009/11/lhc_toast.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/55SHDs3fxMk" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/55SHDs3fxMk/lhc_toast.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/catdynamics/2009/11/lhc_toast.php</id>
         
    <category term="astro"/>
         
         
    <published>2009-11-06T11:37:09-05:00</published>
      
    <updated>2009-11-06T11:37:09-05:00</updated>
    <source>
      <title>Dynamics of Cats</title>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate"/>
      <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>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T12:58:30-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
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      <id>http://scienceblogs.com/catdynamics/</id>
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  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://diracseashore.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>dberenstein</name>
						
      <uri>http://www.physics.ucsb.edu/People/person.php3?userid=dberens</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Turning of the seasons</div>
    </title>
		
    <link href="http://diracseashore.wordpress.com/2009/11/06/turning-of-the-seasons/" rel="alternate" type="text/html"/>
		
    <id>http://diracseashore.wordpress.com/?p=1647</id>
		
    <updated>2009-11-06T15:54:53+00:00</updated>
		
    <published>2009-11-06T15:54:53+00:00</published>
		
    <category term="Random" scheme="http://diracseashore.wordpress.com/"/>
    <category term="Santa Barbara" scheme="http://diracseashore.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Time keeps on passing by. Right now, apples, pumpkins, squashes and persimmons are in season, amongst other vegetables and fruits. The fall weather has settled in nicely, and the usual seasonal events are happening. For example, this is the season when postdoctoral applications are made, and I find myself writing a lot of letters of [...]<img src="http://stats.wordpress.com/b.gif?host=diracseashore.wordpress.com&amp;blog=4754772&amp;post=1647&amp;subd=diracseashore&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://diracseashore.wordpress.com/2009/11/06/turning-of-the-seasons/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>Time keeps on passing by. Right now, apples, pumpkins, squashes and persimmons are in season, amongst other vegetables and fruits. The fall weather has settled in nicely, and the usual seasonal events are happening. For example, this is the season when postdoctoral applications are made, and I find myself writing a lot of letters of recommendation. In over a month, I will be reading these applications with the rest of the folks here, to make decisions on who we are going to hire.</p>
<p>Imagine my surprise this week when going to a grocery store, they are already setting up their Christmas decorations. Isn’t it a bit early for that? I was hoping that they wold be setting up the `Turkey day’ decorations after Hallowe’en. This is not the only place. To me, it’s too early for the end of year Holiday decorations. Seems to me they want to rush the end of the year. Or maybe they have nothing to be thankful for.</p>
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    <author>
			
      <name>Terence Tao</name>
						
      <uri>http://www.math.ucla.edu/~tao</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">The “no self-defeating object” argument</div>
    </title>
		
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    <category term="expository" scheme="http://terrytao.wordpress.com/"/>
    <category term="math.LO" scheme="http://terrytao.wordpress.com/"/>
    <category term="cantor's theorem" scheme="http://terrytao.wordpress.com/"/>
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    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">A fundamental tool in any mathematician’s toolkit is that of reductio ad absurdum: showing that a statement  is false by assuming first that  is true, and showing that this leads to a logical contradiction. A particulary pure example of reductio ad absurdum occurs when establishing the non-existence of a hypothetically overpowered object [...]<img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=2828&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>
 A fundamental tool in any mathematician’s toolkit is that of <a href="http://en.wikipedia.org/wiki/Reductio_ad_absurdum">reductio ad absurdum</a>: showing that a statement <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> is false by assuming first that <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> is true, and showing that this leads to a logical contradiction. A particulary pure example of <em>reductio ad absurdum</em> occurs when establishing the non-existence of a hypothetically overpowered object or structure <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>, by showing that <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>’s powers are “self-defeating”: the very existence of <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> and its powers can be used (by some clever trick) to construct a counterexample to that power. Perhaps the most well-known example of a self-defeating object comes from the <a href="http://en.wikipedia.org/wiki/Omnipotence_paradox">omnipotence paradox</a> in philosophy (“Can an omnipotent being create a rock so heavy that He cannot lift it?”); more generally, a large number of other paradoxes in logic or philosophy can be reinterpreted as a proof that a certain overpowered object or structure does not exist.
</p>
<p>
In mathematics, perhaps the first example of a self-defeating object one encounters is that of a largest natural number:
</p>
<blockquote><p><b>Proposition 1 (No largest natural number)</b> <a name="nolarge"/> There does not exist a natural number <img class="latex" title="{N}" src="http://s3.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/> which is larger than all other natural numbers. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that there was such a largest natural number <img class="latex" title="{N}" src="http://s1.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/>. Then <img class="latex" title="{N+1}" src="http://s2.wordpress.com/latex.php?latex=%7BN+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N+1}"/> is also a natural number which is strictly larger than <img class="latex" title="{N}" src="http://s3.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/>, contradicting the hypothesis that <img class="latex" title="{N}" src="http://s1.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/> is the largest natural number. <img class="latex" title="\Box" src="http://s2.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
Note the argument does not apply to the <em>extended natural number system</em> in which one adjoins an additional object <img class="latex" title="{\infty}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cinfty%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\infty}"/> beyond the natural numbers, because <img class="latex" title="{\infty+1}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cinfty+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\infty+1}"/> is defined equal to <img class="latex" title="{\infty}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cinfty%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\infty}"/>. However, the above argument does show that the existence of a largest number is not compatible with the <a href="http://en.wikipedia.org/wiki/Peano_axioms">Peano axioms</a>.
</p>
<p>
This argument, by the way, is perhaps the only mathematical argument I know of which is routinely taught to primary school children <em>by other primary school children</em>, thanks to the schoolyard game of naming the largest number. It is arguably one’s first exposure to a mathematical <em>non-existence result</em>, which seems innocuous at first but can be surprisingly deep, as such results preclude in advance all future attempts to establish existence of that object, no matter how much effort or ingenuity is poured into this task. One sees this in a typical instance of the above schoolyard game; one player tries furiously to cleverly construct some impressively huge number <img class="latex" title="{N}" src="http://s3.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/>, but no matter how much effort is expended in doing so, the player is defeated by the simple response “… plus one!” (unless, of course, <img class="latex" title="{N}" src="http://s1.wordpress.com/latex.php?latex=%7BN%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N}"/> is infinite, ill-defined, or otherwise not a natural number).
</p>
<p>
It is not only individual objects (such as natural numbers) which can be self-defeating; structures (such as orderings or enumerations) can also be self-defeating. (In modern set theory, one considers structures to themselves be a kind of object, and so the distinction between the two concepts is often blurred.) Here is one example (related to, but subtly different from, the previous one):
</p>
<blockquote><p><b>Proposition 2 (The natural numbers cannot be finitely enumerated)</b> <a name="naff"/> The natural numbers <img class="latex" title="{{\Bbb N} = \{0,1,2,3,\ldots\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+N%7D+=+%5C%7B0,1,2,3,%5Cldots%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb N} = \{0,1,2,3,\ldots\}}"/> cannot be written as <img class="latex" title="{\{ a_1,\ldots,a_n\}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7B+a_1,%5Cldots,a_n%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ a_1,\ldots,a_n\}}"/> for any finite collection <img class="latex" title="{a_1,\ldots,a_n}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_1,%5Cldots,a_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,\ldots,a_n}"/> of natural numbers. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that such an enumeration <img class="latex" title="{{\Bbb N} = \{a_1,\ldots,a_n\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+N%7D+=+%5C%7Ba_1,%5Cldots,a_n%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb N} = \{a_1,\ldots,a_n\}}"/> existed. Then consider the number <img class="latex" title="{a_1+\ldots+a_n+1}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_1+%5Cldots+a_n+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1+\ldots+a_n+1}"/>; this is a natural number, but is larger than (and hence not equal to) any of the natural numbers <img class="latex" title="{a_1,\ldots,a_n}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_1,%5Cldots,a_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,\ldots,a_n}"/>, contradicting the hypothesis that <img class="latex" title="{{\Bbb N}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb N}}"/> is enumerated by <img class="latex" title="{a_1,\ldots,a_n}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_1,%5Cldots,a_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,\ldots,a_n}"/>. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
Here it is the <em>enumeration</em> which is self-defeating, rather than any individual natural number such as <img class="latex" title="{a_1}" src="http://s2.wordpress.com/latex.php?latex=%7Ba_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1}"/> or <img class="latex" title="{a_n}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_n}"/>. (For this post, we allow enumerations to contain repetitions.)
</p>
<p>
The above argument may seem trivial, but a slight modification of it already gives an important result, namely <a href="http://en.wikipedia.org/wiki/Euclid's_theorem">Euclid’s theorem</a>:
</p>
<blockquote><p><b>Proposition 3 (The primes cannot be finitely enumerated)</b> <a name="euclid"/> The prime numbers <img class="latex" title="{{\mathcal P} = \{2,3,5,7,\ldots\}}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5Cmathcal+P%7D+=+%5C%7B2,3,5,7,%5Cldots%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathcal P} = \{2,3,5,7,\ldots\}}"/> cannot be written as <img class="latex" title="{\{p_1,\ldots,p_n\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7Bp_1,%5Cldots,p_n%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{p_1,\ldots,p_n\}}"/> for any finite collection of prime numbers. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that such an enumeration <img class="latex" title="{{\mathcal P} = \{p_1,\ldots,p_n\}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5Cmathcal+P%7D+=+%5C%7Bp_1,%5Cldots,p_n%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathcal P} = \{p_1,\ldots,p_n\}}"/> existed. Then consider the natural number <img class="latex" title="{p_1 \times \ldots \times p_n + 1}" src="http://s1.wordpress.com/latex.php?latex=%7Bp_1+%5Ctimes+%5Cldots+%5Ctimes+p_n+++1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p_1 \times \ldots \times p_n + 1}"/>; this is a natural number larger than <img class="latex" title="{1}" src="http://s2.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/> which is not divisible by any of the primes <img class="latex" title="{p_1,\ldots,p_n}" src="http://s3.wordpress.com/latex.php?latex=%7Bp_1,%5Cldots,p_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p_1,\ldots,p_n}"/>. But, by the <a href="http://en.wikipedia.org/wiki/Fundamental_theorem_of_arithmetic">fundamental theorem of arithmetic</a> (or by the method of <a href="http://en.wikipedia.org/wiki/Infinite_descent">Infinite descent</a>, which is another classic application of <em>reductio ad absurdum</em>), every natural number larger than <img class="latex" title="{1}" src="http://s1.wordpress.com/latex.php?latex=%7B1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1}"/> must be divisible by some prime, contradicting the hypothesis that <img class="latex" title="{{\mathcal P}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5Cmathcal+P%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathcal P}}"/> is enumerated by <img class="latex" title="{p_1,\ldots,p_n}" src="http://s3.wordpress.com/latex.php?latex=%7Bp_1,%5Cldots,p_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p_1,\ldots,p_n}"/>. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 1</b>  Continuing the number-theoretic theme, the “dueling conspiracies” arguments in a <a href="http://terrytao.wordpress.com/2009/09/24/the-prime-number-theorem-in-arithmetic-progressions-and-dueling-conspiracies/">previous blog post</a> can also be viewed as an instance of this type of “no-self-defeating-object”; for instance, a zero of the Riemann zeta function at <img class="latex" title="{1+it}" src="http://s2.wordpress.com/latex.php?latex=%7B1+it%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1+it}"/> implies that the primes anti-correlate almost completely with the multiplicative function <img class="latex" title="{n^{it}}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%5E%7Bit%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n^{it}}"/>, which is self-defeating because it also implies complete anti-correlation with <img class="latex" title="{n^{-it}}" src="http://s1.wordpress.com/latex.php?latex=%7Bn%5E%7B-it%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n^{-it}}"/>, and the two are incompatible. Thus we see that the <a href="http://en.wikipedia.org/wiki/Prime_number_theorem">prime number theorem</a> (a much stronger version of Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#euclid">3</a>) also emerges from this type of argument. </p></blockquote>
<p/>
<p>
In this post I would like to collect several other well-known examples of this type of “no self-defeating object” argument. Each of these is well studied, and probably quite familiar to many of you, but I feel that by collecting them all in one place, the commonality of theme between these arguments becomes more apparent. (For instance, as we shall see, many well-known “paradoxes” in logic and philosophy can be interpreted mathematically as a rigorous “no self-defeating object” argument.)
</p>
<p>
<span id="more-2828"/>
</p>
<p/>
<p align="center"><b> —  1. Set theory  — </b></p>
<p>
Many famous foundational results in set theory come from a “no self-defeating object” argument. (Here, we shall be implicitly be using a standard axiomatic framework for set theory, such as <a href="http://en.wikipedia.org/wiki/Zermelo%E2%80%93Fraenkel_set_theory">Zermelo-Frankel set theory</a>.) The basic idea here is that any sufficiently overpowered set-theoretic object is capable of encoding a version of the <a href="http://en.wikipedia.org/wiki/Liar_paradox">liar paradox</a> (“this sentence is false”, or more generally a statement which can be shown to be logically equivalent to its negation) and thus lead to a contradiction. Consider for instance this variant of <a href="http://en.wikipedia.org/wiki/Russell's_paradox">Russell’s paradox</a>:
</p>
<blockquote><p><b>Proposition 4 (No universal set)</b> <a name="nous"/> There does not exist a set which contains all sets (including itself). </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that there existed a universal set <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> which contained all sets. Using the <a href="http://en.wikipedia.org/wiki/Axiom_schema_of_specification">axiom schema of specification</a>, one can then construct the set </p>
<p align="center"><img class="latex" title="\displaystyle  Y := \{ A \in X: A \not \in A\}" src="http://s3.wordpress.com/latex.php?latex=%5Cdisplaystyle++Y+:=+%5C%7B+A+%5Cin+X:+A+%5Cnot+%5Cin+A%5C%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\displaystyle  Y := \{ A \in X: A \not \in A\}"/></p>
<p> of all sets in the universe which did not contain themselves. As <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> is universal, <img class="latex" title="{Y}" src="http://s2.wordpress.com/latex.php?latex=%7BY%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y}"/> is contained in <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>. But then, by definition of <img class="latex" title="{Y}" src="http://s1.wordpress.com/latex.php?latex=%7BY%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y}"/>, one sees that <img class="latex" title="{Y \in Y}" src="http://s2.wordpress.com/latex.php?latex=%7BY+%5Cin+Y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y \in Y}"/> if and only if <img class="latex" title="{Y \not \in Y}" src="http://s3.wordpress.com/latex.php?latex=%7BY+%5Cnot+%5Cin+Y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y \not \in Y}"/>, a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 2</b>  As a corollary, there also does not exist any set <img class="latex" title="{Z}" src="http://s2.wordpress.com/latex.php?latex=%7BZ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Z}"/> which contains all <em>other</em> sets (not including itself), because the set <img class="latex" title="{X := Z \cup \{Z\}}" src="http://s3.wordpress.com/latex.php?latex=%7BX+:=+Z+%5Ccup+%5C%7BZ%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X := Z \cup \{Z\}}"/> would then be universal. </p></blockquote>
<p/>
<p>
One can “localise” the above argument to a smaller domain than the entire universe, leading to the important
</p>
<blockquote><p><b>Proposition 5 (Cantor’s theorem)</b> <a name="cantor"/> Let <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> be a set. Then the power set <img class="latex" title="{2^X := \{ A: A \subset X \}}" src="http://s2.wordpress.com/latex.php?latex=%7B2%5EX+:=+%5C%7B+A:+A+%5Csubset+X+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^X := \{ A: A \subset X \}}"/> of <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> cannot be enumerated by <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>, i.e. one cannot write <img class="latex" title="{2^X := \{ A_x: x \in X \}}" src="http://s2.wordpress.com/latex.php?latex=%7B2%5EX+:=+%5C%7B+A_x:+x+%5Cin+X+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^X := \{ A_x: x \in X \}}"/> for some collection <img class="latex" title="{(A_x)_{x \in X}}" src="http://s3.wordpress.com/latex.php?latex=%7B(A_x)_%7Bx+%5Cin+X%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(A_x)_{x \in X}}"/> of subsets of <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>. </p></blockquote>
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<p>
<em>Proof:</em>  Suppose for contradiction that there existed a set <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> whose power set <img class="latex" title="{2^X}" src="http://s3.wordpress.com/latex.php?latex=%7B2%5EX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^X}"/> could be enumerated as <img class="latex" title="{\{ A_x: x \in X \}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7B+A_x:+x+%5Cin+X+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ A_x: x \in X \}}"/> for some <img class="latex" title="{(A_x)_{x \in X}}" src="http://s2.wordpress.com/latex.php?latex=%7B(A_x)_%7Bx+%5Cin+X%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(A_x)_{x \in X}}"/>. Using the axiom schema of specification, one can then construct the set </p>
<p align="center"><img class="latex" title="\displaystyle  Y := \{ x \in X: x \not \in A_x \}." src="http://s3.wordpress.com/latex.php?latex=%5Cdisplaystyle++Y+:=+%5C%7B+x+%5Cin+X:+x+%5Cnot+%5Cin+A_x+%5C%7D.&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\displaystyle  Y := \{ x \in X: x \not \in A_x \}."/></p>
<p> The set <img class="latex" title="{Y}" src="http://s1.wordpress.com/latex.php?latex=%7BY%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y}"/> is an element of the power set <img class="latex" title="{2^X}" src="http://s2.wordpress.com/latex.php?latex=%7B2%5EX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^X}"/>. As <img class="latex" title="{2^X}" src="http://s3.wordpress.com/latex.php?latex=%7B2%5EX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^X}"/> is enumerated by <img class="latex" title="{\{ A_x: x \in X \}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7B+A_x:+x+%5Cin+X+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ A_x: x \in X \}}"/>, we have <img class="latex" title="{Y = A_y}" src="http://s2.wordpress.com/latex.php?latex=%7BY+=+A_y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y = A_y}"/> for some <img class="latex" title="{y \in Y}" src="http://s3.wordpress.com/latex.php?latex=%7By+%5Cin+Y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{y \in Y}"/>. But then by the definition of <img class="latex" title="{Y}" src="http://s1.wordpress.com/latex.php?latex=%7BY%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Y}"/>, one sees that <img class="latex" title="{y \in A_y}" src="http://s2.wordpress.com/latex.php?latex=%7By+%5Cin+A_y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{y \in A_y}"/> if and only if <img class="latex" title="{y \not \in A_y}" src="http://s3.wordpress.com/latex.php?latex=%7By+%5Cnot+%5Cin+A_y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{y \not \in A_y}"/>, a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
As is well-known, one can adapt Cantor’s argument to the real line, showing that the reals are uncountable:
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<blockquote><p><b>Proposition 6 (The real numbers cannot be countably enumerated)</b> <a name="countex"/> The real numbers <img class="latex" title="{{\mathbb R}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5Cmathbb+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathbb R}}"/> cannot be written as <img class="latex" title="{\{ x_n: n \in {\mathbb N} \}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7B+x_n:+n+%5Cin+%7B%5Cmathbb+N%7D+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ x_n: n \in {\mathbb N} \}}"/> for any countable collection <img class="latex" title="{x_1,x_2,\ldots}" src="http://s1.wordpress.com/latex.php?latex=%7Bx_1,x_2,%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_1,x_2,\ldots}"/> of real numbers. </p></blockquote>
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<p>
<em>Proof:</em>  Suppose for contradiction that there existed a countable enumeration of <img class="latex" title="{{\mathbb R}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5Cmathbb+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathbb R}}"/> by a sequence <img class="latex" title="{x_1,x_2,\ldots}" src="http://s3.wordpress.com/latex.php?latex=%7Bx_1,x_2,%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_1,x_2,\ldots}"/> of real numbers. Consider the decimal expansion of each of these numbers. Note that, due to the well-known “<img class="latex" title="{0.999\ldots=1.000\ldots}" src="http://s1.wordpress.com/latex.php?latex=%7B0.999%5Cldots=1.000%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{0.999\ldots=1.000\ldots}"/>” issue, the decimal expansion may be non-unique, but each real number <img class="latex" title="{x_n}" src="http://s2.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/> has at most two decimal expansions. For each <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, let <img class="latex" title="{a_n \in \{0,1,\ldots,9\}}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_n+%5Cin+%5C%7B0,1,%5Cldots,9%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_n \in \{0,1,\ldots,9\}}"/> be a digit which is not equal to the <img class="latex" title="{n^{th}}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%5E%7Bth%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n^{th}}"/> digit of any of the decimal expansions of <img class="latex" title="{x_n}" src="http://s3.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/>; this is always possible because there are ten digits to choose from and at most two decimal expansions of <img class="latex" title="{x_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/>. (One can avoid any implicit invocation of the <a href="http://en.wikipedia.org/wiki/Axiom_of_choice">axiom of choice</a> here by setting <img class="latex" title="{a_n}" src="http://s2.wordpress.com/latex.php?latex=%7Ba_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_n}"/> to be (say) the <em>least</em> digit which is not equal to the <img class="latex" title="{n^{th}}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%5E%7Bth%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n^{th}}"/> digit of any of the decimal expansions of <img class="latex" title="{x_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/>.) Then the real number given by the decimal expansion <img class="latex" title="{0.a_1a_2a_3\ldots}" src="http://s2.wordpress.com/latex.php?latex=%7B0.a_1a_2a_3%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{0.a_1a_2a_3\ldots}"/> differs in the <img class="latex" title="{n^{th}}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%5E%7Bth%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n^{th}}"/> digit from any of the decimal expansions of <img class="latex" title="{x_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/> for each <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, and so is distinct from every <img class="latex" title="{x_n}" src="http://s3.wordpress.com/latex.php?latex=%7Bx_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x_n}"/>, a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 3</b>  One can of course deduce Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#countex">6</a> directly from Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#cantor">5</a>, by using the decimal representation to embed <img class="latex" title="{2^{\mathbb N}}" src="http://s2.wordpress.com/latex.php?latex=%7B2%5E%7B%5Cmathbb+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{2^{\mathbb N}}"/> into <img class="latex" title="{{\mathbb R}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5Cmathbb+R%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathbb R}}"/>. But notice how the two arguments have a slightly different (though closely related) basis; the former argument proceeds by encoding the liar paradox, while the second proceeds by exploiting Cantor’s diagonal argument. The two perspectives are indeed a little different: for instance, Cantor’s diagonal argument can also be modified to establish the <a href="http://en.wikipedia.org/wiki/Arzel%C3%A0%E2%80%93Ascoli_theorem">Arzela-Ascolí theorem</a>, whereas I do not see any obvious way to prove that theorem by encoding the liar paradox. </p></blockquote>
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<blockquote><p><b>Remark 4</b>  It is an interesting psychological phenomenon that Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#countex">6</a> is often considered far more unintuitive than any of the other propositions here, despite being in the same family of arguments; most people have no objection to the fact that every effort to finitely enumerate the natural numbers, for instance, is doomed to failure, but for some reason it is much harder to let go of the belief that, at some point, some sufficiently ingenious person will work out a way to countably enumerate the real numbers. I am not exactly sure why this disparity exists, but I suspect it is at least partly due to the fact that the rigorous construction of the real numbers is quite sophisticated and often not presented properly until the advanced undergraduate level. (Or perhaps it is because we do not play the game “enumerate the real numbers” often enough in schoolyards.) </p></blockquote>
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<blockquote><p><b>Remark 5</b>  One can also use the diagonal argument to show that any reasonable notion of a “constructible real number” must itself be non-constructive (this is related to the <a href="http://en.wikipedia.org/wiki/Interesting_number_paradox">interesting number paradox</a>). Part of the problem is that the question of determining whether a proposed construction of a real number is actually well-defined is a variant of the <a href="http://en.wikipedia.org/wiki/Halting_problem">halting problem</a>, which we will discuss below. </p></blockquote>
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<p>
While a genuinely universal set is not possible in standard set theory, one at least has the notion of an <a href="http://en.wikipedia.org/wiki/Ordinal_number">ordinal</a>, which contains all the ordinals less than it. (In the discussion below, we assume familiarity with the theory of ordinals.) One can modify the above arguments concerning sets to give analogous results about the ordinals. For instance:
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<blockquote><p><b>Proposition 7 (Ordinals do not form a set)</b>  There does not exist a set that contains all the ordinals. </p></blockquote>
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<p>
<em>Proof:</em>  Suppose for contradiction that such a set existed. By the axiom schema of specification, one can then find a set <img class="latex" title="{\Omega}" src="http://s1.wordpress.com/latex.php?latex=%7B%5COmega%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega}"/> which consists precisely of all the ordinals and nothing else. But then <img class="latex" title="{\Omega \cup \{\Omega\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5COmega+%5Ccup+%5C%7B%5COmega%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega \cup \{\Omega\}}"/> is an ordinal which is not contained in <img class="latex" title="{\Omega}" src="http://s3.wordpress.com/latex.php?latex=%7B%5COmega%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega}"/> (by the <a href="http://en.wikipedia.org/wiki/Axiom_of_regularity">axiom of foundation</a>, also known as the <em>axiom of regularity</em>), a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 6</b>  This proposition(together with the theory of ordinals) can be used to give a quick proof of <a href="http://en.wikipedia.org/wiki/Zorn's_lemma">Zorn’s lemma</a>: see <a href="http://terrytao.wordpress.com/2009/01/28/245b-notes-7-well-ordered-sets-ordinals-and-zorns-lemma-optional/">these lecture notes of mine</a> for further discussion. Notice the similarity between this argument and the proof of Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#nolarge">1</a>. </p></blockquote>
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<blockquote><p><b>Remark 7</b>  Once one has Zorn’s lemma, one can show that various other classes of mathematical objects do not form sets. Consider for instance the class of all vector spaces. Observe that any chain of (real) vector spaces (ordered by inclusion) has an upper bound (namely the union or limit of these spaces); thus, if the class of all vector spaces was a set, then Zorn’s lemma would imply the existence of a maximal vector space <img class="latex" title="{V}" src="http://s2.wordpress.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{V}"/>. But one can simply adjoin an additional element not already in <img class="latex" title="{V}" src="http://s3.wordpress.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{V}"/> (e.g. <img class="latex" title="{\{V\}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7BV%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{V\}}"/>) to <img class="latex" title="{V}" src="http://s2.wordpress.com/latex.php?latex=%7BV%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{V}"/>, and contradict this maximality. (An alternate proof: every object is an element of some vector space, and in particular every set is an element of some vector space. If the class of all vector spaces formed a set, then by the <a href="http://en.wikipedia.org/wiki/Axiom_of_union">axiom of union</a>, we see that union of all vector spaces is a set also, contradicting Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#nous">4</a>.) </p></blockquote>
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<p>
One can localise the above argument to smaller cardinalities, for instance:
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<blockquote><p><b>Proposition 8 (Countable ordinals are uncountable)</b>  There does not exist a countable enumeration <img class="latex" title="{\omega_1, \omega_2, \ldots}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Comega_1,+%5Comega_2,+%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\omega_1, \omega_2, \ldots}"/> of the countable ordinals. (Here we consider finite sets and countably infinite sets to both be countable.) </p></blockquote>
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<p>
<em>Proof:</em>  Suppose for contradiction that there exists a countable enumeration <img class="latex" title="{\omega_1, \omega_2, \ldots}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Comega_1,+%5Comega_2,+%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\omega_1, \omega_2, \ldots}"/> of the countable ordinals. Then the set <img class="latex" title="{\Omega := \bigcup_n \omega_n}" src="http://s2.wordpress.com/latex.php?latex=%7B%5COmega+:=+%5Cbigcup_n+%5Comega_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega := \bigcup_n \omega_n}"/> is also a countable ordinal, as is the set <img class="latex" title="{\Omega \cup \{\Omega \}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5COmega+%5Ccup+%5C%7B%5COmega+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega \cup \{\Omega \}}"/>. But <img class="latex" title="{\Omega \cup \{\Omega \}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5COmega+%5Ccup+%5C%7B%5COmega+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega \cup \{\Omega \}}"/> is not equal to any of the <img class="latex" title="{\omega_n}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Comega_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\omega_n}"/> (by the axiom of foundation), a contradiction. <img class="latex" title="\Box" src="http://s3.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 8</b>  With the axiom of choice, one can show the existence of uncountable ordinals (e.g. by well-ordering the reals), and then there exists a least uncountable ordinal <img class="latex" title="{\Omega}" src="http://s1.wordpress.com/latex.php?latex=%7B%5COmega%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\Omega}"/>. By construction, this ordinal consists precisely of all the countable ordinals, but is itself uncountable, much as <img class="latex" title="{{\mathbb N}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5Cmathbb+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\mathbb N}}"/> consists precisely of all the finite natural numbers, but is itself infinite (Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#naff">2</a>). The least uncountable ordinal is notorious, among other things, for providing a host of counterexamples to various intuitively plausible assertions in point set topology, and in particular in showing that the topology of sufficiently uncountable spaces cannot always be adequately explored by countable objects such as sequences. </p></blockquote>
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<blockquote><p><b>Remark 9</b>  The existence of the least uncountable ordinal can explain why one cannot contradict Cantor’s theorem on the uncountability of the reals simply by iterating the diagonal argument (or any other algorithm) in an attempt to “exhaust” the reals. From <a href="http://en.wikipedia.org/wiki/Transfinite_induction">transfinite induction</a> we see that the diagonal argument allows one to assign a different real number to each countable ordinal, but this does not establish countability of the reals, because the set of all countable ordinals is itself uncountable. (This is similar to how one cannot contradict Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#nous">4</a> by iterating the <img class="latex" title="{N \rightarrow N+1}" src="http://s3.wordpress.com/latex.php?latex=%7BN+%5Crightarrow+N+1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{N \rightarrow N+1}"/> map, as the set of all finite natural numbers is itself infinite.) In any event, even once one reaches the first uncountable ordinal, one may not yet have completely exhausted the reals; for instance, using the diagonal argument given in the proof of Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#countex">6</a>, only the real numbers in the interval <img class="latex" title="{[0,1]}" src="http://s1.wordpress.com/latex.php?latex=%7B%5B0,1%5D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{[0,1]}"/> will ever be enumerated by this procedure. (Also, the question of whether <em>all</em> real numbers in <img class="latex" title="{[0,1]}" src="http://s2.wordpress.com/latex.php?latex=%7B%5B0,1%5D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{[0,1]}"/> can be enumerated by the iterated diagonal algorithm requires the <a href="http://en.wikipedia.org/wiki/Continuum_hypothesis">continuum hypothesis</a>, and even with this hypothesis I am not sure whether the statement is decidable.) </p></blockquote>
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<p align="center"><b> —  2. Logic  — </b></p>
<p>
The “no self-defeating object” argument leads to a number of important non-existence results in logic. Again, the basic idea is to show that a sufficiently overpowered logical structure will eventually lead to the existence of a self-contradictory statement, such as the liar paradox. To state examples of this properly, one unfortunately has to invest a fair amount of time in first carefully setting up the language and theory of logic. I will not do so here, and instead use informal English sentences as a proxy for precise logical statements to convey a taste (but not a completely rigorous description) of these logical results here.
</p>
<p>
The liar paradox itself – the inability to assign a consistent truth value to “this sentence is false” – can be viewed as an argument demonstrating that there is no consistent way to interpret (i.e. assign a truth value to) sentences, when the sentences are (a) allowed to be self-referential, and (b) allowed to invoke the very notion of truth given by this interpretation. One’s first impulse is to say that the difficulty here lies more with (a) than with (b), but there is a clever trick, known as <a href="http://en.wikipedia.org/wiki/Quining">Quining</a> (or <em>indirect self-reference</em>), which allows one to modify the liar paradox to produce a non-self-referential statement to which one still cannot assign a consistent truth value. The idea is to work not with fully formed sentences <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, which have a single truth value, but instead with <a href="http://en.wikipedia.org/wiki/Predicate_(mathematical_logic)">predicates</a> <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, whose truth value depends on a variable <img class="latex" title="{x}" src="http://s2.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> in some range. For instance, <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> may be “<img class="latex" title="{x}" src="http://s1.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> is thirty-two characters long.”, and the range of <img class="latex" title="{x}" src="http://s2.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> may be the set of strings (i.e. finite sequences of characters); then for every string <img class="latex" title="{T}" src="http://s3.wordpress.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T}"/>, the statement <img class="latex" title="{S(T)}" src="http://s1.wordpress.com/latex.php?latex=%7BS(T)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(T)}"/> (formed by replacing every appearance of <img class="latex" title="{x}" src="http://s2.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> in <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> with <img class="latex" title="{T}" src="http://s1.wordpress.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T}"/>) is either true or false. For instance, <img class="latex" title="{S(``a'')}" src="http://s2.wordpress.com/latex.php?latex=%7BS(%60%60a'')%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(``a'')}"/> is true, but <img class="latex" title="{S(``ab'')}" src="http://s3.wordpress.com/latex.php?latex=%7BS(%60%60ab'')%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(``ab'')}"/> is false. Crucially, predicates are themselves strings, and can thus be fed into themselves as input; for instance, <img class="latex" title="{S(S)}" src="http://s1.wordpress.com/latex.php?latex=%7BS(S)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(S)}"/> is false. If however <img class="latex" title="{U}" src="http://s2.wordpress.com/latex.php?latex=%7BU%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{U}"/> is the predicate “<img class="latex" title="{x}" src="http://s3.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> is sixty-five characters long.”, observe that <img class="latex" title="{U(U)}" src="http://s1.wordpress.com/latex.php?latex=%7BU(U)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{U(U)}"/> is true.
</p>
<p>
Now consider the <em>Quine predicate</em> <img class="latex" title="{Q}" src="http://s2.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> given by
</p>
<p>
“<img class="latex" title="{x}" src="http://s3.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> is a predicate whose range is the set of strings, and <img class="latex" title="{x(x)}" src="http://s1.wordpress.com/latex.php?latex=%7Bx(x)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x(x)}"/> is false.”
</p>
<p>
whose range is the set of strings. Thus, for any string <img class="latex" title="{T}" src="http://s2.wordpress.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T}"/>, <img class="latex" title="{Q(T)}" src="http://s3.wordpress.com/latex.php?latex=%7BQ(T)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q(T)}"/> is the sentence
</p>
<p>
“<img class="latex" title="{T}" src="http://s1.wordpress.com/latex.php?latex=%7BT%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T}"/> is a predicate whose range is the set of strings, and <img class="latex" title="{T(T)}" src="http://s2.wordpress.com/latex.php?latex=%7BT(T)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T(T)}"/> is false.”
</p>
<p>
This predicate is defined non-recursively, but the sentence <img class="latex" title="{Q(Q)}" src="http://s3.wordpress.com/latex.php?latex=%7BQ(Q)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q(Q)}"/> captures the essence of the liar paradox: it is true if and only if it is false. This shows that there is no consistent way to interpret sentences in which the sentences are allowed to come from predicates, are allowed to use the concept of a string, and also allowed to use the concept of truth as given by that interpretation.
</p>
<p>
Note that the proof of Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#nous">4</a> is basically the set-theoretic analogue of the above argument, with the connection being that one can identify a predicate <img class="latex" title="{T(x)}" src="http://s1.wordpress.com/latex.php?latex=%7BT(x)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{T(x)}"/> with the set <img class="latex" title="{\{x: T(x) \hbox{ true} \}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7Bx:+T(x)+%5Chbox%7B+true%7D+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{x: T(x) \hbox{ true} \}}"/>.
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<p>
By making one small modification to the above argument – replacing the notion of truth with the related notion of provability – one obtains the celebrated <a href="http://en.wikipedia.org/wiki/G%C3%B6del's_incompleteness_theorems">Gödel’s (second) incompleteness theorem</a>:
</p>
<blockquote><p><b>Theorem 9 (Gödel’s incompleteness theorem)</b>  (Informal statement) No consistent logical system which has the notion of a string, can provide a proof of its own logical consistency. (Note that a proof can be viewed as a certain type of string.) </p></blockquote>
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<blockquote><p><b>Remark 10</b>  Because one can encode strings in numerical form (e.g. using the ASCII code), it is also true (informally speaking) that no consistent logical system which has the notion of a natural number, can provide a proof of its own logical consistency. </p></blockquote>
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<p>
<em>Proof:</em>  (Informal sketch only) Suppose for contradiction that one had a consistent logical system inside of which its consistency could be proven. Now let <img class="latex" title="{Q}" src="http://s3.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> be the predicate given by
</p>
<p>
“<img class="latex" title="{x}" src="http://s1.wordpress.com/latex.php?latex=%7Bx%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x}"/> is a predicate whose range is the set of strings, and <img class="latex" title="{x(x)}" src="http://s2.wordpress.com/latex.php?latex=%7Bx(x)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x(x)}"/> is not provable”
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<p>
and whose range is the set of strings. Define the <em>Gödel sentence</em> <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> to be the string <img class="latex" title="{G := Q(Q)}" src="http://s1.wordpress.com/latex.php?latex=%7BG+:=+Q(Q)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G := Q(Q)}"/>. Then <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is logically equivalent to the assertion “<img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is not provable”. Thus, if <img class="latex" title="{G}" src="http://s1.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> were false, then <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> would be provable, which (by the consistency of the system) implies that <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is true, a contradiction; thus, <img class="latex" title="{G}" src="http://s1.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> must be true. Because the system is provably consistent, the above argument can be placed inside the system itself, to <em>prove</em> inside that system that <img class="latex" title="{G}" src="http://s2.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> must be true; thus <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is provable and <img class="latex" title="{G}" src="http://s1.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> is then false, a contradiction. (It becomes quite necessary to carefully distinguish the notions of truth and provability (both inside a system and externally to that system) in order to get this argument straight!) <img class="latex" title="\Box" src="http://s2.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 11</b>  It is not hard to show that a consistent logical system cannot <em>disprove</em> its own consistency either; thus the consistency of such a system is undecidable within that system. Thus this theorem strengthens the (more well known) first Gödel incompleteness theory, which asserts the existence of undecidable statements inside a consistent logical system which contains the concept of a string (or a natural number). On the other hand, the incompleteness theorem does not preclude the possibility that the consistency of a weak theory could be proven in a strictly stronger theory (e.g. the consistency of Peano arithmetic is provable in Zermelo-Frankel set theory). </p></blockquote>
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<blockquote><p><b>Remark 12</b>  One can use the incompleteness theorem to establish the undecidability of other overpowered problems. For instance, <a href="http://en.wikipedia.org/wiki/Matiyasevich's_theorem">Matiyasevich’s theorem</a> demonstrates that the problem of determining the solvability of a system of Diophantine equations is, in general, undecidable, because one can encode statements such as the consistency of set theory inside such a system. </p></blockquote>
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<p align="center"><b> —  3. Computability  — </b></p>
<p>
One can adapt these arguments in logic to analogous arguments in the theory of computation; the basic idea here is to show that a sufficiently overpowered computer program cannot exist, by feeding the source code for that program into the program itself (or some slight modification thereof) to create a contradiction. As with logic, a properly rigorous formalisation of the theory of computation would require a fair amount of preliminary machinery, for instance to define the concept of Turing machine (or some other universal computer), and so I will once again use informal English sentences as an informal substitute for a precise programming language.
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<p>
A fundamental “no self-defeating object” argument in the subject, analogous to the other liar paradox type arguments encountered previously, is the <a href="http://en.wikipedia.org/wiki/Halting_Theorem">Turing halting theorem</a>:
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<blockquote><p><b>Theorem 10 (Turing halting theorem)</b>  There does not exist a program <img class="latex" title="{P}" src="http://s3.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> which takes a string <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> as input, and determines in finite time whether <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is a program (with no input) that halts in finite time. </p></blockquote>
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<p>
<em>Proof:</em>  Suppose for contradiction that such a program <img class="latex" title="{P}" src="http://s3.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> existed. Then one could easily modify <img class="latex" title="{P}" src="http://s1.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> to create a variant program <img class="latex" title="{Q}" src="http://s2.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/>, which takes a string <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> as input, and halts if and only if <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> is a program (with <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> itself as input) that does not halts in finite time. Indeed, all <img class="latex" title="{Q}" src="http://s3.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> has to do is call <img class="latex" title="{P}" src="http://s1.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> with the string <img class="latex" title="{S(S)}" src="http://s2.wordpress.com/latex.php?latex=%7BS(S)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(S)}"/>, defined as the program (with no input) formed by declaring <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> to be the input string for the program <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>. If <img class="latex" title="{P}" src="http://s2.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> determines that <img class="latex" title="{S(S)}" src="http://s3.wordpress.com/latex.php?latex=%7BS(S)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(S)}"/> does not halt, then <img class="latex" title="{Q}" src="http://s1.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> halts; otherwise, if <img class="latex" title="{P}" src="http://s2.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> determines that <img class="latex" title="{S(S)}" src="http://s3.wordpress.com/latex.php?latex=%7BS(S)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S(S)}"/> does halt, then <img class="latex" title="{Q}" src="http://s1.wordpress.com/latex.php?latex=%7BQ%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q}"/> performs an infinite loop and does not halt. Then observe that <img class="latex" title="{Q(Q)}" src="http://s2.wordpress.com/latex.php?latex=%7BQ(Q)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Q(Q)}"/> will halt if and only if it does not halt, a contradiction. <img class="latex" title="\Box" src="http://s3.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 13</b>  As one can imagine from the proofs, this result is closely related to, but not quite identical with, the Gödel incompleteness theorem. That latter theorem implies that the question of whether a given program halts or not in general is undecidable (consider a program designed to search for proofs of the inconsistency of set theory). By contrast, the halting theorem (roughly speaking) shows that this question is <em>uncomputable</em> (i.e. there is no algorithm to decide halting in general) rather than <em>undecidable</em> (i.e. there are programs whose halting can neither be proven nor disproven). </p>
<p>
On the other hand, the halting theorem can be used to establish the incompleteness theorem. Indeed, suppose that all statements in a suitably strong and consistent logical system were either provable or disprovable. Then one could build a program that determined whether an input string <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, when run as a program, halts in finite time, simply by searching for all proofs or disproofs of the statement “<img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> halts in finite time”; this program is guaranteed to terminate with a correct answer by hypothesis. </p>
</blockquote>
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<blockquote><p><b>Remark 14</b>  While it is not possible for the halting problem for a given computing language to be computable in that language, it is certainly possible that it is computable in a strictly stronger language. When that is the case, one can then invoke <a href="http://en.wikipedia.org/wiki/Newcomb's_paradox">Newcomb’s paradox</a> to argue that the weaker language does not have unlimited “free will” in some sense. </p></blockquote>
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<blockquote><p><b>Remark 15</b>  In the language of <a href="http://en.wikipedia.org/wiki/Recursion_theory">recursion theory</a>, the halting theorem asserts that the set of programs that do not halt is not a <a href="http://en.wikipedia.org/wiki/Recursive_set">decidable set</a> (or a <em>recursive set</em>). In fact, one can make the slightly stronger assertion that the set of programs that do not halt is not even a <a href="http://en.wikipedia.org/wiki/Recursively_enumerable">semi-decidable set</a> (or a <em>recursively enumerable set</em>), i.e. there is no algorithm which takes a program as input and halts in finite time if and only if the input program does not halt. This is because the complementary set of programs that do halt is clearly semi-decidable (one simply runs the program until it halts, running forever if it does not), and so if the set of programs that do not halt is also semi-decidable, then it is decidable (by running both algorithms in parallel). </p></blockquote>
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<blockquote><p><b>Remark 16</b>  One can use the halting theorem to exclude overly general theories for certain types of mathematical objects. For instance, one cannot hope to find an algorithm to determine the existence of smooth solutions to arbitrary nonlinear partial differential equations, because it is possible to simulate a Turing machine using the laws of classical physics, which in turn can be modeled using (a moderately complicated system of) nonlinear PDE. Instead, progress in nonlinear PDE has instead proceeded by focusing on much more specific classes of such PDE (e.g. elliptic PDE, parabolic PDE, hyperbolic PDE, gauge theories, etc.). </p></blockquote>
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<p>
One can place the halting theorem in a more “quantitative” form. Call a function <img class="latex" title="{f: {\mathbb N} \rightarrow {\mathbb N}}" src="http://s3.wordpress.com/latex.php?latex=%7Bf:+%7B%5Cmathbb+N%7D+%5Crightarrow+%7B%5Cmathbb+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{f: {\mathbb N} \rightarrow {\mathbb N}}"/> <em>computable</em> if there exists a computer program which, when given a natural number <img class="latex" title="{n}" src="http://s1.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> as input, returns <img class="latex" title="{f(n)}" src="http://s2.wordpress.com/latex.php?latex=%7Bf(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{f(n)}"/> as output in finite time. Define the <a href="http://en.wikipedia.org/wiki/Busy_beaver_function">Busy Beaver function</a> <img class="latex" title="{BB: {\mathbb N} \rightarrow {\mathbb N}}" src="http://s3.wordpress.com/latex.php?latex=%7BBB:+%7B%5Cmathbb+N%7D+%5Crightarrow+%7B%5Cmathbb+N%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB: {\mathbb N} \rightarrow {\mathbb N}}"/> by setting <img class="latex" title="{BB(n)}" src="http://s1.wordpress.com/latex.php?latex=%7BBB(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n)}"/> to equal the largest output of any program of at most <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> characters in length (and taking no input), which halts in finite time. Note that there are only finitely many such programs for any given <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, so <img class="latex" title="{BB(n)}" src="http://s1.wordpress.com/latex.php?latex=%7BBB(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n)}"/> is well-defined. On the other hand, it is uncomputable, even to upper bound:
</p>
<blockquote><p><b>Proposition 11</b>  There does not exist a computable function <img class="latex" title="{f}" src="http://s2.wordpress.com/latex.php?latex=%7Bf%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{f}"/> such that one has <img class="latex" title="{BB(n) \leq f(n)}" src="http://s3.wordpress.com/latex.php?latex=%7BBB(n)+%5Cleq+f(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n) \leq f(n)}"/> for all <img class="latex" title="{n}" src="http://s1.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that there existed a computable function <img class="latex" title="{f(n)}" src="http://s2.wordpress.com/latex.php?latex=%7Bf(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{f(n)}"/> such that <img class="latex" title="{BB(n) \leq f(n)}" src="http://s3.wordpress.com/latex.php?latex=%7BBB(n)+%5Cleq+f(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n) \leq f(n)}"/> for all <img class="latex" title="{n}" src="http://s1.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>. We can use this to contradict the halting theorem, as follows. First observe that once the Busy Beaver function can be upper bounded by a computable function, then for any <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, the run time of any halting program of length at most <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> can also be upper bounded by a computable function. This is because if a program of length <img class="latex" title="{n}" src="http://s1.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> halts in finite time, then a trivial modification of that program (of length larger than <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>, but by a computable factor) is capable of outputting the run time of that program (by keeping track of a suitable “clock” variable, for instance). Applying the upper bound for Busy Beaver to that increased length, one obtains the bound on run time.
</p>
<p>
Now, to determine whether a given program <img class="latex" title="{S}" src="http://s3.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/> halts in finite time or not, one simply simulates (runs) that program for time up to the computable upper bound of the possible running time of <img class="latex" title="{S}" src="http://s1.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>, given by the length of <img class="latex" title="{S}" src="http://s2.wordpress.com/latex.php?latex=%7BS%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{S}"/>. If the program has not halted by then, then it never will. This provides a program <img class="latex" title="{P}" src="http://s3.wordpress.com/latex.php?latex=%7BP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P}"/> obeying the hypotheses of the halting theorem, a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 17</b>  A variant of the argument shows that <img class="latex" title="{BB(n)}" src="http://s2.wordpress.com/latex.php?latex=%7BBB(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n)}"/> grows faster than any computable function: thus if <img class="latex" title="{f}" src="http://s3.wordpress.com/latex.php?latex=%7Bf%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{f}"/> is computable, then <img class="latex" title="{BB(n) &gt; f(n)}" src="http://s1.wordpress.com/latex.php?latex=%7BBB(n)+%3E+f(n)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{BB(n) &gt; f(n)}"/> for all sufficiently large <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>. We leave the proof of this result as an exercise to the reader. </p></blockquote>
<p/>
<blockquote><p><b>Remark 18</b>  Sadly, the most important unsolved problem in complexity theory, namely the <a href="http://en.wikipedia.org/wiki/P_=_NP_problem"><img class="latex" title="{P \neq NP}" src="http://s3.wordpress.com/latex.php?latex=%7BP+%5Cneq+NP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \neq NP}"/> problem</a>, does not seem to be susceptible to the no-self-defeating-object argument, basically because such arguments tend to be <em>relativisable</em> whereas the <img class="latex" title="{P \neq NP}" src="http://s1.wordpress.com/latex.php?latex=%7BP+%5Cneq+NP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \neq NP}"/> problem is not; see <a href="http://terrytao.wordpress.com/2009/08/01/pnp-relativisation-and-multiple-choice-exams/">this earlier blog post</a> for more discussion. On the other hand, one has the curious feature that many proposed <em>proofs</em> that <img class="latex" title="{P \neq NP}" src="http://s2.wordpress.com/latex.php?latex=%7BP+%5Cneq+NP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \neq NP}"/> appear to be self-defeating; this is most strikingly captured in the celebrated work of Razborov and Rudich, who showed (very roughly speaking) that any sufficiently “natural” proof that <img class="latex" title="{P \neq NP}" src="http://s3.wordpress.com/latex.php?latex=%7BP+%5Cneq+NP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \neq NP}"/> could be used to disprove the existence of an object closely related to the belief that <img class="latex" title="{P \neq NP}" src="http://s1.wordpress.com/latex.php?latex=%7BP+%5Cneq+NP%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{P \neq NP}"/>, namely the existence of pseudorandom number generators. (I am told, though, that diagonalisation arguments can be used to prove some other inclusions or non-inclusions in complexity theory that are not subject to the relativisation barrier, though I do not know the details.) </p></blockquote>
<p/>
<p align="center"><b> —  4. Game theory  — </b></p>
<p>
Another basic example of the no-self-defeating-objects argument arises from game theory, namely the <a href="http://en.wikipedia.org/wiki/Strategy-stealing_argument">strategy stealing argument</a>. Consider for instance a generalised version of naughts and crosses (tic-tac-toe), in which two players take turns placing naughts and crosses on some game board (not necessarily square, and not necessarily two-dimensional), with the naughts player going first, until a certain pattern of all naughts or all crosses is obtained, with the naughts player winning if the pattern is all naughts, and the crosses player winning if the pattern is all crosses. (If all positions are filled without either pattern occurring, the game is a draw.) We assume that the winning patterns for the cross player are exactly the same as the winning patterns for the naughts player (but with naughts replaced by crosses, of course).
</p>
<blockquote><p><b>Proposition 12</b> <a name="so"/> In any generalised version of naughts and crosses, there is no strategy for the second player (i.e. the crosses player) which is guaranteed to ensure victory. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose for contradiction that the second player had such a winning strategy <img class="latex" title="{W}" src="http://s2.wordpress.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W}"/>. The first player can then <em>steal</em> that strategy by placing a naught arbitrarily on the board, and then pretending to be the second player and using <img class="latex" title="{W}" src="http://s3.wordpress.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W}"/> accordingly. Note that occasionally, the <img class="latex" title="{W}" src="http://s1.wordpress.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W}"/> strategy will compel the naughts player to place a naught on the square that he or she has already occupied, but in such cases the naughts player may simply place the naught somewhere else instead. (It is not possible that the naughts player would run out of places, thus forcing a draw, because this would imply that <img class="latex" title="{W}" src="http://s2.wordpress.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W}"/> could lead to a draw as well, a contradiction.) If we denote this stolen strategy by <img class="latex" title="{W'}" src="http://s3.wordpress.com/latex.php?latex=%7BW'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W'}"/>, then <img class="latex" title="{W'}" src="http://s1.wordpress.com/latex.php?latex=%7BW'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W'}"/> guarantees a win for the naughts player; playing the <img class="latex" title="{W'}" src="http://s2.wordpress.com/latex.php?latex=%7BW'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W'}"/> strategy for the naughts player against the <img class="latex" title="{W}" src="http://s3.wordpress.com/latex.php?latex=%7BW%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{W}"/> strategy for the crosses player, we obtain a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<blockquote><p><b>Remark 19</b>  The key point here is that in naughts and crosses games, it is possible to play a <em>harmless move</em> – a move which gives up the turn of play, but does not actually decrease one’s chance of winning. In games such as chess, there does not appear to be any analogue of the harmless move, and so it is not known whether black actually has a strategy guaranteed to win or not in chess, though it is suspected that this is not the case. </p></blockquote>
<p/>
<blockquote><p><b>Remark 20</b>  The <a href="http://en.wikipedia.org/wiki/Hales%E2%80%93Jewett_theorem">Hales-Jewett theorem</a> shows that for any fixed board length, an <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>-dimensional game of naughts and crosses is unable to end in a draw if <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> is sufficiently large. An induction argument shows that for any two-player game that terminates in bounded time in which draws are impossible, one player must have a guaranteed winning strategy; by the above proposition, this strategy must be a win for the naughts player. Note, however, that Proposition <a href="http://terrytao.wordpress.com/2009/11/05/the-no-self-defeating-object-argument/#so">12</a> provides no information as to <em>how</em> to locate this winning strategy, other than that this strategy belongs to the naughts player. Nevertheless, this gives a second example in which the no-self-defeating-object argument can be used to ensure the <em>existence</em> of some object, rather than the <em>non-existence</em> of an object. (The first example was the prime number theorem, discussed earlier.) </p></blockquote>
<p/>
<p>
The strategy-stealing argument can be applied to real-world economics and finance, though as with any other application of mathematics to the real world, one has to be careful as to the implicit assumptions one is making about reality and how it conforms to one’s mathematical model when doing so. For instance, one can argue that in any market or other economic system in which the net amount of money is approximately constant, it is not possible to locate a universal trading strategy which is guaranteed to make money for the user of that strategy, since if everyone applied that strategy then the net amount of money in the system would increase, a contradiction. Note however that there are many loopholes here; it may be that the strategy is difficult to copy, or relies on exploiting some other group of participants who are unaware or unable to use the strategy, and would then lose money (though in such a case, the strategy is not truly universal as it would stop working once enough people used it). Unfortunately, there can be strong psychological factors that can cause people to override the conclusions of such strategy-stealing arguments with their own rationalisations, as can be seen, for instance, in the perennial popularity of pyramid schemes, or to a lesser extent, market bubbles (though one has to be careful about applying the strategy-stealing argument in the latter case, since it is possible to have net wealth creation through external factors such as advances in technology).
</p>
<p>
Note also that the strategy-stealing argument also limits the universal predictive power of <a href="http://en.wikipedia.org/wiki/Technical_analysis">technical analysis</a> to provide predictions other than that the prices obey a <a href="http://en.wikipedia.org/wiki/Martingale_(probability_theory)">martingale</a>, though again there are loopholes in the case of markets that are illiquid or highly volatile.
</p>
<p/>
<p align="center"><b> —  5. Physics  — </b></p>
<p>
In a similar vein, one can try to adapt the no-self-defeating-object argument from mathematics to physics, but again one has to be much more careful with various physical and metaphysical assumptions that may be implicit in one’s argument. For instance, one can argue that under the laws of special relativity, it is not possible to construct a totally immovable object. The argument would be that if one could construct an immovable object <img class="latex" title="{O}" src="http://s1.wordpress.com/latex.php?latex=%7BO%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{O}"/> in one inertial reference frame, then by the <a href="http://en.wikipedia.org/wiki/Principle_of_relativity">principle of relativity</a> it should be possible to construct an object <img class="latex" title="{O'}" src="http://s2.wordpress.com/latex.php?latex=%7BO'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{O'}"/> which is immovable in another inertial reference frame which is moving with respect to the first; setting the two on a collision course, we obtain the classic contradiction between an irresistible force and an immovable object. Note however that there are several loopholes here which allow one to avoid contradiction; for instance, the two objects <img class="latex" title="{O, O'}" src="http://s3.wordpress.com/latex.php?latex=%7BO,+O'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{O, O'}"/> could simply pass through each other without interacting.
</p>
<p>
In a somewhat similar vein, using the laws of special relativity one can argue that it is not possible to systematically generate and detect tachyon particles – particles traveling faster than the speed of light – because these could be used to transmit localised information faster than the speed of light, and then (by the principle of relativity) to send localised information back into the past, from one location to a distant one. Setting up a second tachyon beam to reflect this information back to the original location, one could then send localised information back to one’s own past (rather than to the past of an observer at a distant location), allowing one to set up a classic <a href="http://en.wikipedia.org/wiki/Grandfather_paradox">grandfather paradox</a>. However, as before, there are a large number of loopholes in this argument which could let one avoid contradiction; for instance, if the apparatus needed to set up the tachyon beam may be larger than the distance the beam travels (as is for instance the case in <a href="http://en.wikipedia.org/wiki/Mexican_wave">Mexican wave</a>-type tachyon beams) then there is no causality paradox; another loophole is if the tachyon beam is not fully localised, but propagates in spacetime in a manner to interfere with the second tachyon beam. A third loophole occurs if the universe exhibits quantum behaviour (in particular, the ability to exist in entangled states) instead of non-quantum behaviour, which allows for such superluminal mechanisms as wave function collapse to occur without any threat to causality or the principle of relativity. A fourth loophole occurs if the effects of relativistic gravity (i.e. general relativity) become significant. Nevertheless, the paradoxical effect of time travel is so strong that this physical argument is a fairly convincing way to rule out many commonly imagined types of faster-than-light travel or communication (and we have a number of other arguments too that exclude more modes of faster-than-light behaviour, though this is an entire blog post topic in its own right).
</p><p/>
Posted in expository, math.LO Tagged: cantor's theorem, godel incompleteness theorem, halting problem <a href="http://feeds.wordpress.com/1.0/gocomments/terrytao.wordpress.com/2828/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/comments/terrytao.wordpress.com/2828/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/terrytao.wordpress.com/2828/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/delicious/terrytao.wordpress.com/2828/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/terrytao.wordpress.com/2828/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/stumble/terrytao.wordpress.com/2828/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godigg/terrytao.wordpress.com/2828/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/digg/terrytao.wordpress.com/2828/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/terrytao.wordpress.com/2828/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/reddit/terrytao.wordpress.com/2828/" border="0" alt=""/></a> <img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=2828&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div></div>
    </content>
		
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		<thr:total>31</thr:total>
	
    <source>
      <title type="text">What's new</title>
      <subtitle type="text">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <updated>2009-11-07T00:48:46+00:00</updated>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://empg.maths.ed.ac.uk/blog/wp-atom.php">
		
    <author>
			
      <name>Patricia</name>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Amir-Kian Kashani-Poor’s EMPJ-talk</div>
    </title>
		
    <link href="http://empg.maths.ed.ac.uk/blog/?p=884" rel="alternate" type="text/html"/>
		
    <id>http://empg.maths.ed.ac.uk/blog/?p=884</id>
		
    <updated>2009-11-06T15:37:55+00:00</updated>
		
    <published>2009-11-05T17:31:43+00:00</published>
		
    <category term="Maths&amp;Physics" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="Uncategorized" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="EMPJ" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="EMPJunior" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="introductory talk" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="matrix models" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="preseminar" scheme="http://empg.maths.ed.ac.uk/blog"/>
    <category term="student" scheme="http://empg.maths.ed.ac.uk/blog"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Here we are again, to summarize yesterday’s  EMPJ  introductory seminar. Once again, I’d like to take this opportunity to thank all the speakers who agree to give us these “pre-seminar” talks on behalf of all of us EMPJunior members! I think this activity is going very well, I find it extremely helpful to [...]</div>
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		<thr:total>2</thr:total>
	
    <source>
      <title type="text">EMPG Blog</title>
      <subtitle type="text">Mathematical Physics in Edinburgh</subtitle>
      <updated>2009-11-06T15:37:55+00:00</updated>
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    <title>Makers of Universes</title>
		
    <link href="http://feedproxy.google.com/~r/CosmicVarianceBlog/~3/F0JH0PlKOmk/" rel="alternate"/>
		
    <link href="http://blogs.discovermagazine.com/cosmicvariance/2009/11/06/makers-of-universes/#comments" rel="replies" type="text/html"/>
		
    <published>2009-11-06T15:27:58+00:00</published>
		
    <author>
      <name>Sean</name>
    </author>
				
    <category term="Humor"/>
		
    <category term="Science and Society"/>

		
    <id>http://blogs.discovermagazine.com/cosmicvariance/?p=3131</id>
		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">It can’t be easy being the guy who has to introduce Albert Einstein.  But it helps if you’re George Bernard Shaw.

You have to love YouTube, although this is only an excerpt from a somewhat longer speech.  Most of the text is here.</div>
    </summary>
			
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>It can’t be easy being the guy who has to introduce Albert Einstein.  But it helps if you’re George Bernard Shaw.</p>
<p/>
<p>You have to love YouTube, although this is only an excerpt from a somewhat longer speech.  Most of the text is <a href="http://is.gd/4Ny8W">here</a>.</p>

<p><a href="http://feedads.g.doubleclick.net/~a/Gnerj-6d8ZAndgeje-rWnTt3_PU/0/da"><img ismap="true" src="http://feedads.g.doubleclick.net/~a/Gnerj-6d8ZAndgeje-rWnTt3_PU/0/di" border="0"/></a><br/>
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		<slash:comments>6</slash:comments>
		
    <updated>2009-11-06T15:27:58+00:00</updated>
    <source>
      <title>Cosmic Variance</title>
      <link href="http://blogs.discovermagazine.com/cosmicvariance" rel="alternate"/>
      <subtitle>Random samplings from a universe of ideas.</subtitle>
      <updated>2009-11-06T19:23:45+00:00</updated>
      <generator>http://wordpress.org/?v=2.8.4</generator><sy:updatePeriod>hourly</sy:updatePeriod><sy:updateFrequency>1</sy:updateFrequency>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://blogs.uslhc.us/wp-atom.php">
		
    <author>
			
      <name>Flip Tanedo</name>
						
      <uri>http://www.lepp.cornell.edu/~pt267/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Symmetry in Physcs, Pt. 4</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2492" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2492</id>
		
    <updated>2009-11-06T15:19:51+00:00</updated>
		
    <published>2009-11-06T15:19:51+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>
    <category term="higgs" scheme="http://blogs.uslhc.us/"/>
    <category term="Symmetry" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Alright, it’s time to start wrapping things up a bit. I’ve been going on for some time now about how symmetries play a central role in our understanding of physics. Here’s a lightning review:

In part 1, we thought about how the symmetries of space(time) restrict the form of our theories.
In part 2, we saw how [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2492"><div xmlns="http://www.w3.org/1999/xhtml"><p>Alright, it’s time to start wrapping things up a bit. I’ve been going on for some time now about how symmetries play a central role in our understanding of physics. Here’s a lightning review:</p>
<ul>
<li>In <a href="http://blogs.uslhc.us/?p=2247">part 1</a>, we thought about how the symmetries of space(time) restrict the form of our theories.</li>
<li>In <a href="http://blogs.uslhc.us/?p=2275">part 2</a>, we saw how antimatter comes from a <strong>discrete</strong> symmetry of spacetime (Charge-Parity)</li>
<li>In <a href="http://blogs.uslhc.us/?p=2486">part 3</a>, we introduced <strong>internal</strong> symmetries that have nothing to do with spacetime, but that lead to a replication in the number of particles. This “explains,” for example, why there are three copies of the electron.</li>
</ul>
<p>Here’s a summary in graphical form:</p>
<p style="text-align: center"><img class="aligncenter size-full wp-image-2852" src="http://blogs.uslhc.us/wp-content/uploads/2009/11/symmetrynotes.png" height="360" alt="symmetrynotes" width="480"/></p>
<p>If you wanted a nice summary in the format of a nice TED talk, (I know <a href="http://blogs.uslhc.us/?p=2816">Mike A.</a> is a fan), then I recommend <a href="http://www.ted.com/talks/marcus_du_sautoy_symmetry_reality_s_riddle.html">Marcus du Sautoy’s talk</a> earlier this year:</p>
<p>[There is a video that cannot be displayed in this feed. <a href="http://blogs.uslhc.us/?p=2492">Visit the blog entry to see the video.]</a></p>
<p><span> </span></p>
<p>Now I’d like to go over some more formal results with far-reaching effects in physics, i.e. some “advanced topics.” These are usually things which are derived rigorously in successively more advanced physics courses, but here we’ll just give heuristic explanations that highlight the physical relevance. Though the topics are somewhat high brow in their nature, they address very simple questions that I think should be very accessible.</p>
<p><span style="font-size: medium"><strong>Where do conservation laws come from?<br/>
</strong></span></p>
<p>Emmy Noether was a prominent physicist and mathematician in the early 1900s when those fields were dramatically dominated by men. Today every undergraduate physics student learns <strong>Noether’s Theorem</strong> as part of analytic mechanics. The theorem can be summarized as this:</p>
<blockquote><p>For every continuous symmetry, there is a conserved charge.</p></blockquote>
<p>What does this mean? The first part refers to a continuous symmetry. These are like the spacetime symmetries that we discussed in <a href="http://blogs.uslhc.us/?p=2247">part 1</a>: rotations, translations and their relativistic generalizations (Lorentz transformations). The word <strong>continuous</strong> means that you can perform the symmetry by any arbitrary amount, as opposed to discrete symmetries (such as those in <a href="http://blogs.uslhc.us/?p=2275">part 2</a>).</p>
<p>The second part says that if you have a continuous symmetry, then you have a conserved quantity which we call <strong>charge</strong>. This is something you’re already familiar with: we know that electrons carry electric charge and that this charge is conserved: it is neither created nor destroyed, and every interaction between particles must have the same charge going out as it did going in. For example, if ten physicists entered a bar and only nine left by closing time, then the number of physicists is not conserved. (Maybe one of them had a change of heart and became a mathematician.)</p>
<p>This is really neat, because now we can <strong>explain</strong> the existence of conserved charges in terms of the existence of a symmetry in nature. Here are a few well known examples from non-relativistic classical physics:</p>
<ul>
<li>The laws of physics are the same over time (time translation symmetry). This implies the existence of a conserved quantity that doesn’t change with time. We call this <strong>energy</strong>. i.e. the energy of a system of constant in time.</li>
<li>The laws of physics are the same at every point in space (space translation symmetry). This implies the existence of a conserved quantity that doesn’t change with space. We call this <strong>momentum</strong>.</li>
<li>The laws of physic are the same no matter how we change the direction of or coordinates, this leads to the conservation of <strong>angular momentum</strong>.</li>
</ul>
<p>(I once convinced myself that if you think about this for a while, it makes sense ‘intuitively’ without any mathematics. However,  this depends on what you mean by ‘intuitive.’) This is now really useful because physicists building theories can generate conserved charges just by imposing that the theory obeys some symmetry.<span id="more-2492"/></p>
<p><span style="font-size: medium"><strong>Where do forces come from?</strong></span></p>
<p>There’s a particular kind of symmetry that particle physicists are particularly interested in: <strong>gauge symmetries</strong>. These symmetries are special because they give us <strong>gauge bosons</strong>, otherwise known as force particles. Thus we can also say that symmetry is the reason why we have forces between particles.</p>
<p>There are two complementary ways in which one can view gauge symmetry. The first way is to think of it as an additional feature of a regular global symmetry. For example, we can say that there is an internal symmetry that causes us to have three ‘colors’ of each quark. We can then “promote” this symmetry  to a gauge symmetry and this forces us to introduce a new force particle (the gluon) which connects particles which have color charge. (This color charge, of course, comes from Noether’s theorem above.) This works by saying that we are promoting a global symmetry into a local symmetry, meaning that we allow ourselves to do different symmetry transformations at different points in space(time).</p>
<p>For example, electric charge comes from a simple symmetry called <strong>U(1)</strong>. This is the symmetry of a circle. So we can imagine a little circle living at every point in spacetime, and at every point there is some point on the circle which tells a property of the electron field. What is this property? It’s a complex phase, basically a complex number of length 1 that multiplies the electron variable in our theories.  This isn’t a “real” circle since it’s an internal symmetry, we’re just imagining this to help us understand what’s going on. A <strong>global</strong> symmetry would tell us that if we move the point on the circle by the <em>same </em>amount <em>everywhere</em> in space, then the laws of physics should be the same:</p>
<p><img class="aligncenter size-medium wp-image-2855" src="http://blogs.uslhc.us/wp-content/uploads/2009/11/gauge_1-300x148.png" height="148" alt="gauge_1" width="300"/></p>
<p>A <strong>gauge</strong> symmetry, however, is one where we can do an <em>independent</em> rotation at <em>each </em>point in space (i.e. a <strong>local</strong> transformation):</p>
<p><img class="aligncenter size-medium wp-image-2856" src="http://blogs.uslhc.us/wp-content/uploads/2009/11/gauge_2-300x148.png" height="148" alt="gauge_2" width="300"/></p>
<p>If a symmetry is a gauge symmetry, then this transformation should still leave the laws of physics the same. Note that the <strong>local</strong> symmetry is much more restrictive than the <strong>global</strong> symmetry. Why does this give us force particles? If all of the arrows are mutually misaligned, it turns out that we need to define a way to go from the orientation of an arrow at point <em>x </em>to the orientation of the arrow at point <em>y</em>. In differential geometry this is called a <strong>connection</strong>. In physics it’s called a <strong>gauge field</strong>. This “gauge field” object which tells us how the arrows point is precisely what we call force particles! So the photon is just the “gauge field” which connects the U(1) orientations of electrically charged particles. Particles that aren’t charged don’t have a U(1) orientation, and so the photon doesn’t “see” them.</p>
<p>As a side note, the second way to think of this is to say that if the arrows can point in any direction then this piece of information is actually a redundancy in our theory. In other words, gauge symmetries can be thought of as not arising from some natural principle, but as a human-made invention that introduces redundancy to makes nature more mathematically tractable. If you think about this for a while this becomes something of an ontological question, which is <em>not </em>what we want to get into; but the point is that quantum effects tend to break lots of symmetries. If we create a gauge symmetry that is redundant, we ought to make sure that quantum effects don’t mess it up or else our theory in completely inconsistent. The quantum effects are called <strong>anomalies</strong>, and this leads to a powerful tool in theoretical physics called <strong>anomaly cancellation</strong>. (It was a cancellation of anomalies in 1984 by Green and Schwarz that led to the first superstring revolution.)</p>
<p><span style="font-size: medium"><strong>Where do massless particles come from?<br/>
</strong></span></p>
<p>These are a weird questions Why should I ask where massless particles come from? Why is this different from asking where <em>any</em> particle comes from?</p>
<p>Massless particles are somewhat special in quantum field theory. It turns out that they can lead to apparent theoretical inconsistencies (so-called “infrared divergences”) and quantum mechanics usually conspires to give particles mass unless (ta-da) such masses are protected against by some symmetry. (An example of this is chiral symmetry, i.e. the left-handed and right-handed structure of the Standard Model fermions, that prevents fermions from getting mass other than by the Higgs mechanism. If that didn’t make sense, then don’t worry about it.)</p>
<p>This is related to <strong>Goldstone’s theorem</strong>, which tells us that:</p>
<blockquote><p>If a continuous global symmetry is broken, then there are massless particles in the theory.</p></blockquote>
<p>By “continuous global symmetry” we mean something like the U(1) symmetry of the circle described above or its higher-dimensional generalizations. I’ll have to be necessarily sketchy here, but the picture that everyone always draws is the so-called “Mexican hat potential”:</p>
<p><img class="aligncenter size-medium wp-image-2865" src="http://blogs.uslhc.us/wp-content/uploads/2009/11/higgspot-300x230.gif" height="230" alt="higgspot" width="300"/></p>
<p>The idea is that we can imagine a quantum field as a marble rolling around in that Mexican-hat-shaped bowl. The position of the marble represents the “vacuum expectation value” of the field. Here ‘<strong>vacuum expectation value</strong>‘<strong> </strong>(vev) is code for whether or not the particle exists everywhere in space without any additional quantum effects. Most potentials don’t have that dimple in the middle, so the ‘marble’ wants to sit right in the center where the field takes zero vacuum expectation value. This is what most particles do. For the <strong>Higgs</strong>, however the vacuum expectation value is nonzero — the Mexican-hat shaped bowl pushes the Higgs to live on the ring where the hat is flat. This means that the Higgs “exists everywhere” in space even without having to be created through quantum interactions. Indeed, it is the interaction of particles with this “omnipresent” Higgs field that gives those particles mass.</p>
<p>Now, Goldstone’s theorem is the observation that the shape of the bowl actually corresponds to the mass of the particle rolling around in it. This is part of the structure of all quantum field theories, and you can take it as a stated fact. The key observation is that the Higgs particle still has a direction where it is free to roll around, namely the angular direction. Goldstone tells us that these directions (in “field space,” i.e. in the space of possible Higgs vacuum values, not physical space) correspond to massless excitations of the Higgs field.</p>
<p>So you can think about it this way: the fact that the Higgs field doesn’t live at the center of the potential (it’s pushed out by the dimple) tells us that the Higgs lives everywhere in space. Particles interactions with this “everywhere in space” field gives them mass. In addition, however, there is a certain way that we can jiggle this “everywhere in space” field that corresponds to massless particles. This is just like the ripples one gets from throwing a rock into a pond.</p>
<p><span style="font-size: medium"><strong>Where do massive force particles come from?</strong></span></p>
<p>This massless Higgs field coming form Goldstone’s theorem relates to a different problem in field theory related to gauge bosons, i.e. force particles. It turns out that if we write a theory with <em>massive</em> force particles (as we observe with the <em>W</em> and <em>Z</em> bosons), this usually leads to apparent theoretical inconsistencies (a “breakdown of unitarity”), e.g. probabilities that are greater than 100%. However, it turns out that if the force particles get their masses in a very specific way, i.e. via a process called <strong>spontaneous symmetry breaking</strong>, then everything is okay. Further, it turns out that everything is okay because—you guess it—there is symmetry in the theory.</p>
<p>The point is this: the <em>W</em> and <em>Z</em> bosons get their masses from “eating” the massless Higgs particles. What this means is that the physical <em>W</em> and <em>Z</em> bosons actually contain part of the Higgs field! More technically, the <em>W </em>and <em>Z</em> fields mix quantum mechanically with the massless Higgs particles. This becomes a rather technical point, so I’ll leave it at that. Don’t worry if you’re unhappy with the word “eat” in this context. It is commonly used even in quantum field theory textbooks and bugged me for a long time until I felt like I properly understood what was going on.</p>
<p><span style="font-size: medium"><strong>Summary and Outlook<br/>
</strong></span></p>
<p>I’ve been going on for quite some time now about symmetries and how they’re important in particle physics. Let me close with the following summary:</p>
<ul>
<li>Symmetries play a key role in how we define our theories and, in turn, restrict their structure.</li>
<li>Antiparticles are related by charge-parity conjugation, a discrete symmetry of spacetime.</li>
<li>The Standard Model is composed of several symmetries: spacetime, family, color, electroweak.</li>
<li>Symmetries can be very interesting when they break. The Higgs boson is intimately connected to <strong>electroweak symmetry breaking</strong>, which ends up giving the <em>W</em> and <em>Z</em> bosons mass through its Goldstone particles and gives mass to the matter particles through interactions between left and right handed fermions.</li>
<li>Local, or “gauge,” symmetries are responsible for the existence of force particles.</li>
<li>Symmetries are responsible for conservation laws, such as the conservation of momentum or the conservation of electric charge.</li>
</ul>
<p>In future posts I’ll spend more time talking about my research, in which the theoretical physics community has been using symmetry in novel ways to go beyond the Standard Model. To whet your appetite, this includes extending spacetime symmetry (extra dimensions), imposing a matter particle/force particle symmetry (supersymmetry), and incorporating all of the Standard Model gauge symmetries into a single symmetry (grand unification).</p>
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    <title>Poll: The Computers of the Future</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Today's Quantum Optics lecture is about quantum computing experiments, and how different types of systems stack up. Quantum computing, as you probably know if you're reading this blog, is based on building a computer whose "bits" can not only take on "0" and "1" states, but arbitrary superpositions of "0" and "1". Such a computer would be able to out-perform any classical computer on certain types of problems, and would open the exciting possibility of a windows installation that is both working and hung up at the same time.</p>

<p>There are roughly as many types of proposed quantum computers as there are people working on quantum computation. It's not clear which of them, if any, will eventually prove to be useful, meaning that this is the perfect subject for a blog poll:</p>

<p>
&lt;a href="http://answers.polldaddy.com/poll/2217973/"&gt;The quantum computers of the future will be based on:&lt;/a&gt;&lt;span style="font-size:9px;"&gt;(&lt;a href="http://www.polldaddy.com"&gt;survey&lt;/a&gt;)&lt;/span&gt;
</p>

<p>While this is a poll about quantum computing, the machines running the poll are strictly classical, so you can only choose one option.</p>
 <a href="http://scienceblogs.com/principles/2009/11/poll_the_computers_of_the_futu.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/yQwwQvpyag8" height="1" width="1"/></div>
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    <published>2009-11-06T08:50:20-05:00</published>
      
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    <title>Links for 2009-11-06</title>
          
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                <div class="delicious-link"><a href="http://www.avclub.com/articles/philip-k-dick,35021/?utm_medium=RSS&amp;utm_campaign=feeds&amp;utm_source=avclub_rss_daily">Philip K. Dick | Books | The A.V. Club</a></div>
                <div class="delicious-extended">"Why it's daunting: Science fiction and fantasy get a lot of mileage out of taking their readers to new worlds, but most classic genre fiction is really about making new worlds seem like home. The Lord Of The Rings would lose a lot of its appeal if the hobbits had no Shire to return to, and Isaac Asimov's Foundation series wouldn't be nearly as effective if the heroes weren't bent on protecting a sane, prosperous status quo. Philip K. Dick doesn't play by the same rules. While his work has clear genre roots, using such familiar tropes as androids, time travel, precognition, and space travel, he operates by a surreal common sense that's simultaneously lucid and fever-dream absurd. In 36 novels and more than 120 stories, he used fiction to work out his own particular philosophy, and the results aren't always immediately accessible."</div>
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                <div class="delicious-link"><a href="http://www.midmajority.com/2009/11/that-teenage-feeling.php">The Mid-Majority : That Teenage Feeling</a></div>
                <div class="delicious-extended">"College basketball is about college, and it's about basketball. Our Game belongs to those who are still young enough to play it.

College basketball is an experience that's only fully understood by actual students. There's a special bond between a student section and players (especially walk-ons) that's hardly ever captured in published words, much less "Coke Madness." As you watch from the bleachers, you know those players made the same choice as you did. You might not have been actively recruited like they were. But those are your friends and representatives, working on your behalf to validate a shared, life-altering decision about where to get educated. "</div>
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                <div class="delicious-extended">"Inside his lighted, glassed-in command post, the captain of the East German border guard, a beefy guy with a square jaw and the dark bristly air of a Doberman, stood dialing and redialing his telephone. For hours he vainly sought instructions. Certainly he was confused. Most likely he was frightened. The crowds before him had broiled out of nowhere, grown so fast, unlike anything he had ever seen, and now they pushed so close that their breath, frosting in the night, mingled with that of his increasingly anxious men."</div>
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                <div class="delicious-link"><a href="http://www.themorningnews.org/archives/opinions/a_common_nomenclature_for_lego_families.php">A Common Nomenclature for Lego Families by Giles Turnbull - The Morning News</a></div>
                <div class="delicious-extended">"This language of Lego isn't just something our family has invented; every Lego-building family must have its own vocabulary. And the words they use (mostly invented by the children, not the adults) are likely to be different every time. But how different? And what sort of words?

Hence, a survey. I asked fellow parents to donate their children for a few minutes, and name a selection of Lego pieces culled from the Lego parts store."</div>
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                <div class="delicious-extended">"Does everyone see a little bit of themselves in animated cartoon characters? Or do the artists actually draw the characters to look more generic, less racially distinctive? There have been few studies about the perceived race and ethnicity of animated cartoon characters, and none focusing on the unique Japanese anime style."</div>
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                <div class="delicious-link"><a href="http://pimpmynovel.blogspot.com/2009/11/nanowrimohno.html">Pimp My Novel: NaNoWriMOhNo</a></div>
                <div class="delicious-extended">"[I]t seems that a lot of people are missing the point of NaNoWriMo altogether. Despite Chris Baty's invitation to "write laughably awful yet lengthy prose together," a lot of folks are getting really amped up about having finally written a piece of fiction of substantial length and are more concerned about FINALLY BECOMING AUTHORS ZOMG than about having fun writing crap, which is what the contest is really about. If even one sentence of whatever you concoct in the spirit of NaNoWriMo leads you into a publishable novel somewhere down the road (with substantial editing and revision, of course), you should count yourself lucky."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/books">books</a> <a href="http://delicious.com/orzelc/publishing">publishing</a> <a href="http://delicious.com/orzelc/business">business</a> <a href="http://delicious.com/orzelc/pimp-novel">pimp-novel</a>)</div>
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                <div class="delicious-link"><a href="http://killingthebuddha.com/mag/dogma/spaceship-jesus-will-come-back-and-whisk-us-away/">Spaceship Jesus Will Come Back and Whisk Us Away &lt; Killing the Buddha</a></div>
                <div class="delicious-extended">"The words left behind are ironically what the books are about, but not in the way their authors intended. The evangelical/fundamentalists, from their crudest egocentric celebrities to their "intellectuals" touring college campuses trying to make evangelicalism respectable, have been left behind by modernity. They won't change their literalistic anti-science, anti-education, anti-everything superstitions, so now they nurse a deep grievance against "the world." This has led to a profound fear of the "other.""</div>
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                <div class="delicious-link"><a href="http://www.insidehighered.com/news/2009/11/05/survey">News: Technology Gap - Inside Higher Ed</a></div>
                <div class="delicious-extended">"[W]hen students were asked whether their professors understand technology and have integrated it into their courses, only 38 percent said Yes. Further, when students were asked about the top impediment to using technology, the top answer was "lack of faculty technology knowledge," an answer that drew 45 percent of respondents, up from 25 percent only a year ago.

And only 32 percent of students said that they believed their college was adequately preparing them to use technology in their careers."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/education">education</a> <a href="http://delicious.com/orzelc/technology">technology</a> <a href="http://delicious.com/orzelc/inside-higher-ed">inside-higher-ed</a>)</div>
            </li></ul> <a href="http://scienceblogs.com/principles/2009/11/links_for_2009-11-06.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/TWgfIVCvqbc" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/TWgfIVCvqbc/links_for_2009-11-06.php" rel="alternate"/>
         
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    <category term="Links Dump"/>
         
         
    <published>2009-11-06T07:37:27-05:00</published>
      
    <updated>2009-11-06T07:37:27-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
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      <updated>2009-11-07T11:21:56-05:00</updated>
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  <entry xml:lang="en">
    
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Fraïssé Limits</div>
    </title>
    
    <link href="http://golem.ph.utexas.edu/category/2009/11/fraisse_limits.html" rel="alternate" type="application/xhtml+xml"/>
    
    <updated>2009-11-06T11:57:10+00:00</updated>
    
    <published>2009-11-06T11:47:54+00:00</published>
    
    <id>tag:golem.ph.utexas.edu,2009:%2Fcategory%2F3.2106</id>
    
    <summary type="text">How should we understand a Fraïssé Limit category theoretically?</summary>
    
    <author>
      
      <name>david</name>
      
      <uri>http://www.dcorfield.pwp.blueyonder.co.uk/</uri>
      
      <email>d.corfield@kent.ac.uk</email>
    
    </author>
    
    <category term="Categories"/>
    
    <content type="xhtml" xml:base="http://golem.ph.utexas.edu/category/2009/11/fraisse_limits.html">
      <div xmlns="http://www.w3.org/1999/xhtml">
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>The <a href="http://en.wikipedia.org/wiki/Rado_graph">Rado graph</a>, or <i>random graph</i>, seems to be an extraordinary entity. Take countably many nodes, then for each pair of nodes flip a coin and if it shows heads, draw an edge between them. Almost surely you will have generated the Rado graph, <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math>.</p>

<p>Any finite graph (and indeed any countable graph) is contained in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math>, not just in the sense of being embeddedable, but in the sense of being an induced subgraph, that is, it is the full subgraph on a subset of nodes. Along with this <i>universality</i>, <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math> is also <i>homogenous</i> in the sense that any isomorphism between finite induced subgraphs extends to an automorphism of all of <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math>.</p>

<p><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math> is very robust, you can delete finitely many vertices, add or remove finitely many edges, or interchange edges and non-edges, and you still end up with a graph isomorphic to <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math>. Furthermore, the odd thing about the construction of this graph is that I didn’t have to tell you the probability <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>p</mi></math> of the coin showing heads. So long as <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>p</mi></math> is in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mo stretchy="false">(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo stretchy="false">)</mo></math> and the tosses are independent, the Rado graph almost surely emerges.</p>

<p>Not only this, there are many ways to generate it without using random devices. Rado himself took the nodes to be the natural numbers, and an edge between <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>m</mi></math> and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>n</mi></math> whenever either the <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>m</mi></math>th bit of the binary representation of <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>n</mi></math> is nonzero, or the <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>n</mi></math>th bit of the binary representation of <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>m</mi></math> is nonzero. Yet another method has us take as nodes the prime numbers equal to 1 mod 4. Then we join <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>p</mi></math> and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>q</mi></math> if they are quadratic residues of each other.</p>
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>I find myself interested in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>R</mi></math> because it is an example of a Fraïssé limit. This is nicely explained in Artem Chernikov’s slides – <a href="http://chernikov.files.wordpress.com/2008/12/whatis_fraisseconstruction.pdf">What is…Fraïssé construction?</a> We want a countable category, <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>K</mi></math>, of finitely generated structures (for a countable signature) whose morphisms are embeddings, which satisfies the three properties:</p>

<ul>
<li>Hereditary: if <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>A</mi></math> embeds into <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>B</mi></math> and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>B</mi></math> is in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>K</mi></math>, then so is <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>A</mi></math>.</li>
<li>Joint embedding property: for any <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>A</mi><mo>,</mo><mi>B</mi><mo>∈</mo><mi>K</mi></math>, there exists a <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>C</mi><mo>∈</mo><mi>K</mi></math> and morphisms <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>A</mi><mo>→</mo><mi>C</mi><mo>←</mo><mi>B</mi></math>.</li>
<li>Amalgamation property: for arrows <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>f</mi><mo>:</mo><mi>A</mi><mo>→</mo><mi>B</mi><mo>,</mo><mi>g</mi><mo>:</mo><mi>A</mi><mo>→</mo><mi>C</mi></math> in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>K</mi></math>, there exist <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>r</mi><mo>:</mo><mi>B</mi><mo>→</mo><mi>D</mi></math> and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>s</mi><mo>:</mo><mi>C</mi><mo>→</mo><mi>D</mi></math> in <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>K</mi></math>, such that <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>r</mi><mo>∘</mo><mi>f</mi><mo>=</mo><mi>s</mi><mo>∘</mo><mi>g</mi></math>.</li>
</ul>
 
Then <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>K</mi></math> is the category of substructures of a countable structure <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>M</mi></math> which is universal and homogeneous. Examples include the Rado graph as the Fraïssé limit of the category of finite graphs and embeddings, and <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mo stretchy="false">⟨</mo><mi>ℚ</mi><mo>,</mo><mo>&lt;</mo><mo stretchy="false">⟩</mo></math> as the Fraïssé limit of the category of finite linearly ordered sets and order preserving injections.

<p>So now some questions: Can this kind of limit be given a natural category theoretic description? Is it related to any of the completions we have listed <a href="http://ncatlab.org/nlab/show/completion">here</a>? It seems to be a kind of <a href="http://ncatlab.org/nlab/show/ind-object">Ind-completion</a>, pretty close to an <a href="http://ncatlab.org/nlab/show/ideal+completion">ideal completion</a>. Can we understand the homogeneity category theoretically?</p>

<p>I should imagine I need to get a look at this thesis – Trevor Irwin, <a href="http://gradworks.umi.com/32/97/3297082.html">Fraïssé limits and colimits with applications to continua</a>:</p>

<blockquote>

<p>The classical Fraïssé construction is a method of taking a direct limit of a family of finite models of a language provided the family fulfills certain amalgamation conditions. The limit is a countable model of the same language which can be characterized by its (injective) homogeneity and universality with respect to the initial family of models. A standard example is the family of finite linear orders for which the Fraïssé limit is the rational numbers with the usual ordering.</p>

<p>We present this classical construction via category theory, and within this context we introduce the dual construction. This respectively constitutes the Fraïssé colimits and limits indicated in the title. We provide several examples.</p>

<p>We then present the projective Fraïssé limit as a special case of the dual construction, and as such it is the categorical dual to the classical (injective) Fraïssé limit. In this dualization we use a notion of model theoretic structure which has a topological ingredient. This results in the countable limit structures being replaced by structures which are zero-dimensional, compact, second countable spaces with the property that the relations are closed and the functions are continuous.</p>

<p>We apply the theory of projective Fraïssé limits to the pseudo-arc by first representing the pseudo-arc as a natural quotient of a projective Fraïssé limit. Using this representation we derive topological properties of the pseudo-arc as consequences of the properties of projective Fraïssé limits. We thereby obtain a new proof of Mioduszewski’s result that the pseudo-arc is surjectively universal among chainable continua, and also a homogeneity theorem for the pseudo-arc which is a strengthening of a result due to Lewis and Smith. We also find a new characterization of the pseudo-arc via the homogeneity property.</p>

<p>We continue with further applications of these methods to a class of continua known as pseudo-solenoids, and achieve analogous results for the universal pseudo-solenoid.</p>

</blockquote>

<p>Available treatments include Wieslaw Kubiś, <a href="http://arxiv.org/abs/0711.1683">Fraisse sequences - a category-theoretic approach to universal homogeneous structures</a>:</p>

<blockquote>

<p>We present a category-theoretic approach to universal homogeneous objects, with applications in the theory of Banach spaces and in set-theoretic topology,</p>

</blockquote>

<p>and Olivia Caramello, <a href="http://arxiv.org/abs/0805.2778">Fraïssé’s construction from a topos-theoretic perspective</a>:</p>

<blockquote>

<p>We present a topos-theoretic interpretation of (a categorical generalization of) Fraisse’s construction in model theory, with applications to countably categorical theories.</p>

</blockquote>
      </div>
    
    </content>
  
    <source>
      <title>The n-Category Café</title>
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      <updated>2009-11-06T11:57:10+00:00</updated>
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    <title>Biweekly links for 11/06/2009</title>
		
    <link href="http://feedproxy.google.com/~r/michaelnielsen/wmna/~3/EPjtV6bhuXQ/" rel="alternate"/>
		
    <link href="http://michaelnielsen.org/blog/biweekly-links-for-11062009/#comments" rel="replies" type="text/html"/>
		
    <published>2009-11-06T10:53:14+00:00</published>
		
    <author>
      <name>Michael Nielsen</name>
    </author>
				
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    <id>http://michaelnielsen.org/blog/biweekly-links-for-11062009/</id>
		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Lo and Behold: the Internet

“Forty years ago today, a team led by Leonard Kleinrock typed the “Lo” of “Login” into a Stanford computer, which promptly crashed before the command could be entered. But because Kleinrock’s team was sending this message from a UCLA machine, he had just taken part in one of the great milestones [...]</div>
    </summary>
			
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><ul>
<li><a href="http://seedmagazine.com/content/article/lo_and_behold_the_internet">Lo and Behold: the Internet</a>
<ul>
<li>“Forty years ago today, a team led by Leonard Kleinrock typed the “Lo” of “Login” into a Stanford computer, which promptly crashed before the command could be entered. But because Kleinrock’s team was sending this message from a UCLA machine, he had just taken part in one of the great milestones in communication history.”</li>
</ul>
</li>
<li><a href="http://www.synthesis.cc/2009/11/igem-2009-in-the-thick-of-it.html">iGEM 2009: In the thick of it. – synthesis</a>
<ul>
<li>Rob Carlson on current progress in synthetic biology.</li>
</ul>
</li>
<li><a href="http://bixolabs.com/2009/11/01/announcing-the-public-terabyte-dataset-project/">The Public Terabyte Dataset project « Elastic Web Mining | Bixolabs</a>
<ul>
<li>“This is a high quality crawl of top web sites, using AWS’s Elastic Map Reduce, Concurrent’s Cascading workflow API, and Bixolab’s elastic web mining platform.<p/>
<p>Hosting for the resulting dataset will be provided by Amazon in S3, and freely available to all EC2 users.</p>
<p>In addition, the code used to create and process the dataset will be available for download”</p></li>
</ul>
</li>
</ul>
<p>Click <a href="http://delicious.com/nielsen/">here</a> for all of my del.icio.us bookmarks.</p>
<img src="http://feeds.feedburner.com/~r/michaelnielsen/wmna/~4/EPjtV6bhuXQ" height="1" width="1"/></div>
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    <updated>2009-11-06T10:53:14+00:00</updated>
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  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://asymptotia.com/wp-atom.php">
		
    <author>
			
      <name>Clifford</name>
						
      <uri>http://asymptotia.com/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Time Bandit</div>
    </title>
		
    <link href="http://asymptotia.com/2009/11/05/time-bandit/" rel="alternate" type="text/html"/>
		
    <id>http://asymptotia.com/?p=5334</id>
		
    <updated>2009-11-06T07:46:29+00:00</updated>
		
    <published>2009-11-06T07:28:35+00:00</published>
		
    <category term="personal" scheme="http://asymptotia.com/"/>
    <category term="travel" scheme="http://asymptotia.com/"/>
    <category term="work" scheme="http://asymptotia.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><a href="http://asymptotia.com/wp-images/2009/11/dining_at_vijs_3.jpg"><img class="alignleft size-medium wp-image-5339" title="dining_at_vijs_3" src="http://asymptotia.com/wp-images/2009/11/dining_at_vijs_3-225x300.jpg" alt="dining_at_vijs_3" width="180"/></a>Well, <a href="http://asymptotia.com/2009/11/04/remote-office/">that</a> was not altogether terrible, I gather, but I was so tired and a little bit out of sorts* when I started giving the talk that I was running very slowly. So by time I got to the end (even though I hit my right pace later on) I was some 15 minutes over. Ugh. People seemed to like it, but I definitely need to whittle out a few of the more superfluous slides  (which I'd always intended to) and strike the intended pace I wanted to hit earlier than 3/4 of the way through the talk. My reward (besides some nice remarks at the end of the talk that sort of made my day) was a visit to another excellent restaurant  for dinner, with some good company. The extraordinarily good Vij's. The hour's wait for the food was perfectly fine given the nibbles they bring you while you wait, and the  food itself once you get it.  Here's a shot or two of some of the excellent food just after its arrival, and the empty dishes and satisfied hosts just after polishing it all off: [...]</div>
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    <source>
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    <author>
			
      <name>Flip Tanedo</name>
						
      <uri>http://www.lepp.cornell.edu/~pt267/</uri>
					
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    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">LHC vs. baguette bombardier bird</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2861" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2861</id>
		
    <updated>2009-11-06T06:11:56+00:00</updated>
		
    <published>2009-11-06T06:11:56+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">I don’t really know what to think of this, but apparently there’s a news story going around that a piece of bread found its way onto an electrical connection in one of the LHC’s above-ground buildings leading to a failure of a cooling unit. The buildings are protected by high security fences so the story [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2861"><div xmlns="http://www.w3.org/1999/xhtml"><p>I don’t really know what to think of this, but apparently there’s a news story going around that a piece of bread found its way onto an electrical connection in one of the LHC’s above-ground buildings leading to a failure of a cooling unit. The buildings are protected by high security fences so the story is that it was probably dropped by a bird. The upside is that they don’t expect this to make a dent in the current LHC start up schedule.</p>
<p>[As someone who has yet to visit CERN, I have to wonder how such a think could actually occur. Is it so easy for a bird to get into one of these buildings? Should someone make silly references to <em>Spiderman 3</em>?]</p>
<p>I did my best to try to track this story down to a reputable source, hopefully the US/LHC bloggers currently at CERN might be able to comment? (Mike? Seth? See any birds lately? <img class="wp-smiley" src="http://blogs.uslhc.us/wp-includes/images/smilies/icon_smile.gif" alt=":-)"/>  )</p>
<p>I first saw this story reported on the social news site Reddit, where it gathered plenty of <a href="http://www.reddit.com/r/science/comments/a1c3d/baguette_dropped_from_birds_beak_shuts_down_the/">rather funny comments</a>, e.g. “So… what IS the average flight velocity of a baguette-laden swallow?” Reddit linked to a <a href="http://www.popsci.com/science/article/2009-11/bread-loving-bird-shuts-down-lhc">report in Popular Science</a>, which in turn linked to <a href="http://www.theregister.co.uk/2009/11/05/lhc_bread_bomb_dump_incident/">The Register</a> which claimed as its source a press briefing by Mike Lamont, the LHC Machine Coordinator.  At the time of this writing, most of the Google News references to this incident point to the article at <em>The Register</em>, though some spiced it up with some of their own illustrations, e.g.  the <a href="http://www.crunchgear.com/2009/11/05/breaking-large-hadron-collider-shut-down-by-precision-bird-strike/"><em>Crunch Gear</em></a> blog.</p>
<p>Knowing <em>The Register</em>’s history of making tongue-in-cheek statements, I dug a little bit deeper and I was finally able to track down a <a href="http://www.upi.com/Odd_News/2009/11/05/Errant-baguette-chunk-shuts-down-collider/UPI-54651257482954/">story from United Press International</a> under their “Odd News” section with some details. This story finally references <em>The Times</em> of London, which has a nice <a href="http://www.timesonline.co.uk/tol/news/science/physics/article6905250.ece">write up by Nico Hines</a>. It sounds like the fail-safes kicked in properly and it is expected that the LHC can stick to its scheduled restart (keeping in mind that this schedule gets regular minor updates).</p>
<p>So, on the one hand, it sounds like the story is legit. On the other hand, I maybe I should feel guilty that by posting this since I’m playing the role of “<em>yet another blogger posting on a breaking news item and contributing nothing new other than a few snarky comments</em>.” (What does this say about the state of blog-based journalism these days?)</p>
<p>[Hey, at least I provided a paper trail of references like an honest academic.]</p>
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		<thr:total>3</thr:total>
	
    <source>
      <title type="text">US LHC Blog</title>
      <subtitle type="text">US LHC Blogs</subtitle>
      <updated>2009-11-06T16:48:23+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.8.4">WordPress</generator>
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  </entry>

  <entry xml:lang="en-us">
		
    <author>
			
      <name>PhilipJ</name>
		
    </author>
		
    <published>2009-11-06T04:43:02+00:00</published>
		
    <updated>2009-11-06T04:50:12+00:00</updated>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Molecule of the Month: Designed DNA crystals</div>
    </title>
		
    <link href="http://biocurious.com/2009/11/06/molecule-of-the-month-designed-dna-crystals" rel="alternate" type="text/html"/>
		
    <id>tag:biocurious.com,2009-11-06:890bf13c9ae848a71af2301e445ce4d6/8c1324207a51050a7550a8bba74e38b8</id>
		
    <category term="Molecule-of-the-Month"/>
		
		
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p><img class="alignright" src="http://biocurious.com/images/MotM/dnaCrystal.png" alt="DNA crystal"/></p><blockquote><span class="caps">DNA</span> is a perfect raw material for constructing nanoscale structures. Since base-pairing has been selected by evolution to be highly specific, it is easy to design sequences that will link up with their proper mates. In this way, we can treat small pieces of <span class="caps">DNA</span> like Tinkertoys, designing individual components and then allowing them to assemble when we put them together. In addition, the chemistry of <span class="caps">DNA</span> synthesis has been completely automated, so custom pieces of <span class="caps">DNA</span> can be easily constructed, or even ordered from commercial biotech companies. This puts <span class="caps">DNA</span> nanotechnology in the hands of any modest laboratory, and many laboratories have taken advantage of this, creating nanoscale scaffolds, tweezers, polyhedra, computers, and even tiny illustrations composed entirely of <span class="caps">DNA</span>.<br/><br/><span class="caps">DNA</span> has the characteristic mix of flexibility and rigidity that is the hallmark of biological molecules. If the sequence of bases is correct, it zips up into a double helix that, at least in short lengths, is a sturdy cylinder. Longer stretches, however, start to show flexibility, and the <span class="caps">DNA</span> helix curves and bends. The trick in designing a <span class="caps">DNA</span> infrastructure is to develop ways to rigidify the overall structure. In most cases, this has been done by having the <span class="caps">DNA</span> strand weave back and forth between many parallel double helices. In this way, the bundle of helices form a structure that is far more rigid than a single helix.<br/><br/>Nadrian Seeman pioneered the use of <span class="caps">DNA</span> for building nanoscale structures. After decades of work, the structure shown here, from <span class="caps">PDB</span> entry <a href="http://www.pdb.org/pdb/explore.do?structureId=3gbi">3gbi</a>, is the first crystal structure of a <span class="caps">DNA</span> lattice completely designed from scratch. It is built of small 3D triangular subunits, each composed of three separate types of <span class="caps">DNA</span> strands. The base sequences are carefully chosen so that they assemble into this one particular structure, and not any others. At the corners of the 3D triangle, there are sticky ends that link to other triangles, stacking up in a predicable way into a three-dimensional scaffold.</blockquote><p/>

	<p>Read the rest from David Goodsell at the <span class="caps">RCSB</span> <span class="caps">PDB</span> <a href="http://dx.doi.org/10.2210/rcsb_pdb/mom_2009_11">here</a>.  We’ve covered some of  <a href="http://biocurious.com/2006/02/21/dna-lego">this kind</a> <a href="http://biocurious.com/2006/01/17/dna-pyramids">of work</a> before, too.</p></div>
    </content>

    <source>
      <title type="text">Biocurious</title>
      <subtitle type="text">a biophysics blog</subtitle>
      <link href="http://biocurious.com/atom/" rel="self"/>
      <link href="http://biocurious.com/" rel="alternate" type="text/html"/>
      <id>tag:biocurious.com,2005:890bf13c9ae848a71af2301e445ce4d6</id>
      <generator uri="http://textpattern.com/" version="4.0.6">Textpattern</generator>
      <updated>2009-11-07T18:33:23+00:00</updated>
      <author>
		
        <name>PhilipJ</name>
		
		
        <uri>http://biocurious.com/</uri>

      </author>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://blogs.uslhc.us/wp-atom.php">
		
    <author>
			
      <name>Mike Anderson</name>
						
      <uri>http://www.hep.wisc.edu/~mbanderson/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Note to Readers</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2859" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2859</id>
		
    <updated>2009-11-06T04:49:38+00:00</updated>
		
    <published>2009-11-06T04:49:38+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">These LHC posts appear in two places: the main blog site, and the facebook page.  The main site supports video, which currently don’t show up in the facebook posts.
Two of my previous posts had video, so check those out on the main site!
Also notice the “View Original Post” link at the bottom of these which [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2859"><div xmlns="http://www.w3.org/1999/xhtml"><p>These LHC posts appear in two places: the <a href="http://blogs.uslhc.us/">main blog site</a>, and the <a href="http://www.facebook.com/pages/Large-Hadron-Collider-LHC/29436227675">facebook page</a>.  The main site supports video, which currently don’t show up in the facebook posts.</p>
<p>Two of my previous posts had video, so check those out on the main site!</p>
<p>Also notice the “<span>View Original Post” link at the bottom of these which takes you to the main site. </span></p>
<a href="http://www.addtoany.com/share_save?linkurl=http://blogs.uslhc.us/?p=2859&amp;linkname=Note%20to%20Readers" class="a2a_dd addtoany_share_save"><img src="http://blogs.uslhc.us/wp-content/plugins/add-to-any/share_save_120_16.png" height="16" alt="Share/Bookmark" width="120"/></a></div>
    </content>
		
    <link href="http://blogs.uslhc.us/?p=2859#comments" rel="replies" type="text/html" thr:count="0"/>
		
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		<thr:total>0</thr:total>
	
    <source>
      <title type="text">US LHC Blog</title>
      <subtitle type="text">US LHC Blogs</subtitle>
      <updated>2009-11-06T16:48:23+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.8.4">WordPress</generator>
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    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Diamond Encrusted Dragon's Egg</div>
    </title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>A long time ago,  a massive star about 10,000 light years from Earth went kaboom.<br/>
329 years ago, we think, in 1680, the light from the supernova explosion reached Earth and was recorded as a new star by the Flamsteed, then the Astronomer Royal, looking relatively dim as nearby supernove go, due to the layers of dust in the galaxy between us and the site of the explosion.</p>

<p>Now, digging into archival x-ray data, a couple of astronomers may finally have figured out what is going on in Cass A.</p> <a href="http://scienceblogs.com/catdynamics/2009/11/diamond_encrusted_degenerate_s.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/catdynamics/2009/11/diamond_encrusted_degenerate_s.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/DynamicsOfCats/~4/har8UyOc72Q" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/DynamicsOfCats/~3/har8UyOc72Q/diamond_encrusted_degenerate_s.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/catdynamics/2009/11/diamond_encrusted_degenerate_s.php</id>
         
    <category term="astro"/>
         
         
    <published>2009-11-05T23:22:59-05:00</published>
      
    <updated>2009-11-05T23:22:59-05:00</updated>
    <source>
      <title>Dynamics of Cats</title>
      <link href="http://scienceblogs.com/catdynamics/" rel="alternate"/>
      <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>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T12:58:30-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/DynamicsOfCats" rel="self" type="application/rss+xml"/>
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      <id>http://scienceblogs.com/catdynamics/</id>
    </source>
  </entry>

  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-13869903.post-8535203775791341482</id>
    <published>2009-11-05T21:18:00-06:00</published>
    <updated>2009-11-05T21:18:57-06:00</updated>
    <title type="text">Inspirational speech</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><span style="font-family: Verdana,sans-serif;"><span style="font-size: 85%;">I can't recall if I've posted this before.  If you're feeling down (e.g., because just about every story in the news today is horrifying to some degree), <a href="http://www.youtube.com/watch?v=d6wRkzCW5qI">this</a> might cheer you up.</span></span><div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/13869903-8535203775791341482?l=nanoscale.blogspot.com" height="1" width="1"/></div></div>
    </content>
    <link href="http://nanoscale.blogspot.com/feeds/8535203775791341482/comments/default" title="Post Comments" rel="replies" type="application/atom+xml"/>
    <link href="https://www.blogger.com/comment.g?blogID=13869903&amp;postID=8535203775791341482" title="1 Comments" rel="replies" type="text/html"/>
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    <link href="http://nanoscale.blogspot.com/2009/11/inspirational-speech.html" title="Inspirational speech" rel="alternate" type="text/html"/>
    <author>
      <name>Doug Natelson</name>
      <uri>http://www.blogger.com/profile/13340091255404229559</uri>
      <email>noreply@blogger.com</email><gd:extendedProperty xmlns:gd="http://schemas.google.com/g/2005" name="OpenSocialUserId" value="08062051348608340110"/>
    </author><thr:total xmlns:thr="http://purl.org/syndication/thread/1.0">1</thr:total>
    <source>
      <id>tag:blogger.com,1999:blog-13869903</id>
      <updated>2009-11-06T01:41:53-06:00</updated>
      <title type="text">nanoscale views</title>
      <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"/>
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      <link href="http://www.blogger.com/feeds/13869903/posts/default?start-index=26&amp;max-results=25" rel="next" type="application/atom+xml"/>
      <author>
        <name>Doug Natelson</name>
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        <email>noreply@blogger.com</email>
      </author>
      <generator uri="http://www.blogger.com/" version="7.00">Blogger</generator><openSearch:totalResults>377</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>25</openSearch:itemsPerPage>
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  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Thursday Baby Blogging 110509</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>For this week's Baby Blogging, we have a shot of Kate helping SteelyKid with her new favorite game:</p>

<p><img src="http://scienceblogs.com/principles/upload/2009/11/sm_week65.jpg" height="381" alt="sm_week65.jpg" width="500"/></p>

<p>It's called "Take off my shoes, and put them back on." She can play this for hours. It would be even cuter if she could do the putting on and taking off herself, but alas, she's still kind of unclear on the solidity of objects, and doesn't really grasp that her feet can only get into the shoes from the open end. She'll get there, though.</p>

<p>SteelyKid officially moved out of the infant room at day care this week. She's now in the next age/ development group, termed "Waddlers" (an intermediate step between "Infants" and "Toddlers"). I very briefly considered going for the alliterative "Wednesday Waddler Blogging," but regained my senses in time. We're going to stick with "Thursday Baby Blogging" for a while yet.</p>
 <a href="http://scienceblogs.com/principles/2009/11/thursday_baby_blogging_110509.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/QpTPTB3Bucc" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/QpTPTB3Bucc/thursday_baby_blogging_110509.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/principles/2009/11/thursday_baby_blogging_110509.php</id>
         
    <category term="Steelykid!"/>
         
         
    <published>2009-11-05T21:32:58-05:00</published>
      
    <updated>2009-11-05T21:32:58-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-07T11:21:56-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
      <id>http://scienceblogs.com/principles/</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://terrytao.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>Terence Tao</name>
						
      <uri>http://www.math.ucla.edu/~tao</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Reading seminar 3: “Stable group theory and approximate subgroups”, by Ehud Hrushovski</div>
    </title>
		
    <link href="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/" rel="alternate" type="text/html"/>
		
    <id>http://terrytao.wordpress.com/?p=3052</id>
		
    <updated>2009-11-06T01:22:15+00:00</updated>
		
    <published>2009-10-30T01:54:18+00:00</published>
		
    <category term="Logic reading seminar" scheme="http://terrytao.wordpress.com/"/>
    <category term="math.LO" scheme="http://terrytao.wordpress.com/"/>
    <category term="global types" scheme="http://terrytao.wordpress.com/"/>
    <category term="invariant types" scheme="http://terrytao.wordpress.com/"/>
    <category term="Keisler measure" scheme="http://terrytao.wordpress.com/"/>
    <category term="wide types" scheme="http://terrytao.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">This week, Henry Towsner continued some model-theoretic preliminaries for the reading seminar of the Hrushovski paper, particularly regarding the behaviour of wide types, leading up to the main model-theoretic theorem (Theorem 3.4 of Hrushovski) which in turn implies the various combinatorial applications (such as Corollary 1.2 of Hrushovski). Henry’s notes can be found here.


A [...]<img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=3052&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>
 This week, <a href="http://www.math.ucla.edu/~hpt/">Henry Towsner</a> continued some model-theoretic preliminaries for the <a href="http://terrytao.wordpress.com/category/teaching/logic-reading-seminar/">reading seminar</a> of the <a href="http://arxiv.org/abs/0909.2190">Hrushovski paper</a>, particularly regarding the behaviour of wide types, leading up to the main model-theoretic theorem (Theorem 3.4 of Hrushovski) which in turn implies the various combinatorial applications (such as Corollary 1.2 of Hrushovski). Henry’s notes can be found <a href="http://terrytao.files.wordpress.com/2009/10/hrushovskinotes-1.pdf">here</a>.
</p>
<p>
A key theme here is the phenomenon that any pair of large sets contained inside a definable set of finite measure (such as <img class="latex" title="{X \cdot X^{-1}}" src="http://s2.wordpress.com/latex.php?latex=%7BX+%5Ccdot+X%5E%7B-1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X \cdot X^{-1}}"/>) must intersect if they are sufficiently “generic”; the notion of a wide type is designed, in part, to capture this notion of genericity.
</p>
<p>
<span id="more-3052"/>
</p>
<p/>
<p align="center"><b> —  1. Global types  — </b></p>
<p>
Throughout this post, we begin with a countable structure <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> of a language <img class="latex" title="{L}" src="http://s1.wordpress.com/latex.php?latex=%7BL%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{L}"/>, and then consider a universal elementary extension <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> of <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> (i.e. one that obeys the saturation and homogeneity properties as discussed in <a href="http://terrytao.wordpress.com/2009/10/15/reading-seminar-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 1</a>. Later on, <img class="latex" title="{L}" src="http://s1.wordpress.com/latex.php?latex=%7BL%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{L}"/> will contain the language of groups, and then we will rename <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> as <img class="latex" title="{G}" src="http://s3.wordpress.com/latex.php?latex=%7BG%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{G}"/> to emphasise this.
</p>
<p>
Recall from <a href="http://terrytao.wordpress.com/2009/10/15/reading-seminar-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">Notes 1</a> that a <em>partial type</em> over a set <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> is a set of formulae (with <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> variables for some fixed <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>) using <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> as constant symbols, which is consistent and contains the theory of <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>; if the set of formulae is maximal (i.e. complete), then it is a <em>type</em>. One can also think of a type as an ultrafilter over the <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/>-definable sets; if <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is a type and <img class="latex" title="{B}" src="http://s2.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/> is an <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/>-definable set given by some formula <img class="latex" title="{\phi}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\phi}"/>, then either <img class="latex" title="{\phi}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\phi}"/> lies in <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> (in which case we write <img class="latex" title="{p \subset B}" src="http://s1.wordpress.com/latex.php?latex=%7Bp+%5Csubset+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset B}"/>) or <img class="latex" title="{\neg \phi}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cneg+%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\neg \phi}"/> lies in <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> (in which case we write <img class="latex" title="{p \subset \overline{B}}" src="http://s1.wordpress.com/latex.php?latex=%7Bp+%5Csubset+%5Coverline%7BB%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset \overline{B}}"/>) but not both.
</p>
<p>
When the set <img class="latex" title="{A}" src="http://s2.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> is small (i.e. has cardinality less than that of <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, which in particular would be true of <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> consisted of <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> union with a finite set, which is a very typical situation), then by saturation one can identify types (or partial types) with the subset <img class="latex" title="{p({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U})}"/> of <img class="latex" title="{{\Bbb U}^n}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%5En%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}^n}"/> that they cut out. In particular, these sets are non-empty. Adding more formulae to a partial type corresponds to shrinking the set that they cut out, and vice versa.
</p>
<p>
However, if we have a <em>global</em> type <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> – a type defined over the entire model <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> – then one can no longer identify types with the set <img class="latex" title="{p({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U})}"/> that they cut out, because these sets are usually empty! However, what we can do is <em>restrict</em> <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> to some smaller set <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> of constants to create a type <img class="latex" title="{p\downharpoonright_A}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%5Cdownharpoonright_A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p\downharpoonright_A}"/> over <img class="latex" title="{A}" src="http://s2.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/>, defined as the set of all formulae in <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> that only involve the constants in <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/>. It is easy to see that this is still a type, and if <img class="latex" title="{A}" src="http://s2.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> is small, it cuts out a non-empty set in <img class="latex" title="{{\Bbb U}^n}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%5En%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}^n}"/>.
</p>
<p>
A global type <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is said to be <em><img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-invariant</em>, or <em>invariant</em> for short, if the set of formulae in <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is invariant under any automorphism <img class="latex" title="{\sigma}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma}"/> of <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> that fixes <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. In particular, given any <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable set <img class="latex" title="{A \subset {\Bbb U}^n \times {\Bbb U}^m}" src="http://s2.wordpress.com/latex.php?latex=%7BA+%5Csubset+%7B%5CBbb+U%7D%5En+%5Ctimes+%7B%5CBbb+U%7D%5Em%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A \subset {\Bbb U}^n \times {\Bbb U}^m}"/> and <img class="latex" title="{b \in {\Bbb U}^m}" src="http://s3.wordpress.com/latex.php?latex=%7Bb+%5Cin+%7B%5CBbb+U%7D%5Em%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b \in {\Bbb U}^m}"/>, we see that <img class="latex" title="{p \subset A_b}" src="http://s1.wordpress.com/latex.php?latex=%7Bp+%5Csubset+A_b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset A_b}"/> if and only if <img class="latex" title="{p \subset A_{\sigma(b)}}" src="http://s2.wordpress.com/latex.php?latex=%7Bp+%5Csubset+A_%7B%5Csigma(b)%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset A_{\sigma(b)}}"/>, where <img class="latex" title="{A_b := \{ a \in {\Bbb U}^n: (a,b) \in A \}}" src="http://s3.wordpress.com/latex.php?latex=%7BA_b+:=+%5C%7B+a+%5Cin+%7B%5CBbb+U%7D%5En:+(a,b)+%5Cin+A+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A_b := \{ a \in {\Bbb U}^n: (a,b) \in A \}}"/> is a slice of <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/>. (Indeed, this gives an equivalent definition of invariance.)
</p>
<p>
A trivial example of an invariant global type would be the type of an element <img class="latex" title="{m \in M}" src="http://s2.wordpress.com/latex.php?latex=%7Bm+%5Cin+M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{m \in M}"/> (or in <img class="latex" title="{M^n}" src="http://s3.wordpress.com/latex.php?latex=%7BM%5En%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M^n}"/>). This cuts out a singleton set <img class="latex" title="{\{m\}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7Bm%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{m\}}"/>. This is in fact the only invariant global type that cuts out anything at all:
</p>
<blockquote><p><b>Lemma 1</b>  Let <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> be a global invariant type. Then <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is realisable in <img class="latex" title="{{\Bbb U}}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> (i.e. <img class="latex" title="{p({\Bbb U})}" src="http://s2.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U})}"/> is non-empty) if and only if it is realisable in <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> (and is the type of a single element in <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>). </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is realisable in <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> by some <img class="latex" title="{a \in p({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Ba+%5Cin+p(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a \in p({\Bbb U})}"/>. Since the formula <img class="latex" title="{x=a}" src="http://s2.wordpress.com/latex.php?latex=%7Bx=a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x=a}"/> is definable in <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, we see that <img class="latex" title="{p \subset \{ x: x = a \}}" src="http://s1.wordpress.com/latex.php?latex=%7Bp+%5Csubset+%5C%7B+x:+x+=+a+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset \{ x: x = a \}}"/>, i.e. <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> cuts out precisely the singleton set <img class="latex" title="{\{a\}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{a\}}"/>. As <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is invariant, <img class="latex" title="{\{a\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{a\}}"/> must then be invariant under all <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-fixing automorphisms of <img class="latex" title="{{\Bbb U}}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>. By homogeneity, this means that there is no element distinct from <img class="latex" title="{a}" src="http://s2.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> which is elementarily indistinguishable from <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>; in other words, <img class="latex" title="{\{a\}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{a\}}"/> is the set cut out by the type <img class="latex" title="{tp(a/M)}" src="http://s3.wordpress.com/latex.php?latex=%7Btp(a/M)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M)}"/> of <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>.
</p>
<p>
By saturation, the formula <img class="latex" title="{x \neq a}" src="http://s3.wordpress.com/latex.php?latex=%7Bx+%5Cneq+a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x \neq a}"/> together with the formulae in <img class="latex" title="{tp(a/M)}" src="http://s1.wordpress.com/latex.php?latex=%7Btp(a/M)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M)}"/> is not satisfiable, hence not finitely satisfiable. Thus there is a finite set of formulae in <img class="latex" title="{tp(a/M)}" src="http://s2.wordpress.com/latex.php?latex=%7Btp(a/M)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M)}"/> that cut out <img class="latex" title="{\{a\}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{a\}}"/>, i.e. <img class="latex" title="{\{a\}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{a\}}"/> is definable over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. But as <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> is an elementary extension of <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, these formulae must also be realisable in <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, i.e. <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> lies in <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, and the claim follows. <img class="latex" title="\Box" src="http://s2.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
(Because of this, one should regard the notation <img class="latex" title="{p \subset B}" src="http://s3.wordpress.com/latex.php?latex=%7Bp+%5Csubset+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset B}"/> carefully; the set <img class="latex" title="{p({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U})}"/> that <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> cuts out in the model <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> may in fact be empty, but when we write <img class="latex" title="{p \subset B}" src="http://s1.wordpress.com/latex.php?latex=%7Bp+%5Csubset+B%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p \subset B}"/> for some definable <img class="latex" title="{B}" src="http://s2.wordpress.com/latex.php?latex=%7BB%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B}"/>, we interpret this syntactically rather than semantically (or equivalently, that <img class="latex" title="{p({\Bbb U}') \subset B({\Bbb U}')}" src="http://s3.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D')+%5Csubset+B(%7B%5CBbb+U%7D')%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U}') \subset B({\Bbb U}')}"/> holds in all extensions <img class="latex" title="{{\Bbb U}'}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}'}"/> of <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, and not just in <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> itself.)
</p>
<p>
On the other hand, invariant global types exist in abundance:
</p>
<blockquote><p><b>Lemma 2</b> <a name="ext"/> Let <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> be a type over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. Then there exists an invariant global type <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> that refines <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> (i.e. it contains all the formulae that <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> does). </p></blockquote>
<p/>
<p>
<em>Proof:</em>  We view <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> as a collection of logically consistent formulae. We enlarge this collection to a larger one <img class="latex" title="{p'}" src="http://s1.wordpress.com/latex.php?latex=%7Bp'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p'}"/> by adding in the negations of all the formulae definable over <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> that are not realisable in <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. Observe that this collection remains logically consistent, because any finite set of formulae in <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> were realisable in <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, hence in <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> (which is an elementary substructure). Hence, by Zorn’s lemma, one can extend <img class="latex" title="{p'}" src="http://s1.wordpress.com/latex.php?latex=%7Bp'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p'}"/> to a global type <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>.
</p>
<p>
We now claim that <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> is invariant. Indeed, let <img class="latex" title="{\phi}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cphi%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\phi}"/> be a sentence over <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> that is contained in <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>, and let <img class="latex" title="{\sigma}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma}"/> be an automorphism that fixes <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. If <img class="latex" title="{\sigma(\phi)}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Csigma(%5Cphi)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma(\phi)}"/> is not in <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>, then <img class="latex" title="{\neg \sigma(\phi)}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cneg+%5Csigma(%5Cphi)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\neg \sigma(\phi)}"/> must be in <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> (by completeness), and hence <img class="latex" title="{\phi \wedge \neg \sigma(\phi)}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cphi+%5Cwedge+%5Cneg+%5Csigma(%5Cphi)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\phi \wedge \neg \sigma(\phi)}"/> is in <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> also, and hence must be realisable in <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> (otherwise its negation would be in <img class="latex" title="{p'}" src="http://s1.wordpress.com/latex.php?latex=%7Bp'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p'}"/>, and hence in <img class="latex" title="{q}" src="http://s2.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>). But this is absurd since <img class="latex" title="{\sigma}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma}"/> fixes <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. Thus <img class="latex" title="{\sigma(\phi)}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Csigma(%5Cphi)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma(\phi)}"/> does lie in <img class="latex" title="{q}" src="http://s3.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/>, yielding invariance. </p>
<p/>
<p>
A major use of invariant global types for us will be that they can be used to generate sequences of indiscernibles (as defined in <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">previous notes</a>):
</p>
<blockquote><p><b>Lemma 3</b> <a name="lob"/> Let <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> be a global invariant type of some arity <img class="latex" title="{d}" src="http://s2.wordpress.com/latex.php?latex=%7Bd%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{d}"/>, and construct recursively a sequence <img class="latex" title="{b_1, b_2, \ldots \in {\Bbb U}^d}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_1,+b_2,+%5Cldots+%5Cin+%7B%5CBbb+U%7D%5Ed%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1, b_2, \ldots \in {\Bbb U}^d}"/> by requiring <img class="latex" title="{b_n \in p\downharpoonright_{M \cup \{b_1,\ldots,b_{n-1}\}}({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_n+%5Cin+p%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Bb_1,%5Cldots,b_%7Bn-1%7D%5C%7D%7D(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_n \in p\downharpoonright_{M \cup \{b_1,\ldots,b_{n-1}\}}({\Bbb U})}"/> for all <img class="latex" title="{n=1,2,\ldots}" src="http://s2.wordpress.com/latex.php?latex=%7Bn=1,2,%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n=1,2,\ldots}"/>. (This is always possible since types are satisfiable once restricted to small sets, by saturation, as discussed earlier). Then <img class="latex" title="{b_1,b_2,\ldots}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_1,b_2,%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,b_2,\ldots}"/> are indiscernible over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, i.e. the tuples <img class="latex" title="{(b_{i_1},\ldots,b_{i_k})}" src="http://s2.wordpress.com/latex.php?latex=%7B(b_%7Bi_1%7D,%5Cldots,b_%7Bi_k%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_{i_1},\ldots,b_{i_k})}"/> for <img class="latex" title="{i_1 &lt; \ldots &lt; i_k}" src="http://s3.wordpress.com/latex.php?latex=%7Bi_1+%3C+%5Cldots+%3C+i_k%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{i_1 &lt; \ldots &lt; i_k}"/> are elementarily indistinguishable (over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>) for any fixed <img class="latex" title="{k}" src="http://s2.wordpress.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k}"/>. </p></blockquote>
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<p>
<em>Proof:</em>  This is achieved by an induction on <img class="latex" title="{k}" src="http://s3.wordpress.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k}"/>. The <img class="latex" title="{k=1}" src="http://s1.wordpress.com/latex.php?latex=%7Bk=1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k=1}"/> case is clear since the <img class="latex" title="{b_n}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_n}"/> all have type <img class="latex" title="{p\downharpoonright_M}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%5Cdownharpoonright_M%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p\downharpoonright_M}"/> over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. Now we do the <img class="latex" title="{k=2}" src="http://s2.wordpress.com/latex.php?latex=%7Bk=2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k=2}"/> case. It suffices to show that <img class="latex" title="{(b_1,b_2)}" src="http://s3.wordpress.com/latex.php?latex=%7B(b_1,b_2)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,b_2)}"/> and <img class="latex" title="{(b_i,b_j)}" src="http://s1.wordpress.com/latex.php?latex=%7B(b_i,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_i,b_j)}"/> are elementarily indistinguishable over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> for all <img class="latex" title="{i &lt; j}" src="http://s3.wordpress.com/latex.php?latex=%7Bi+%3C+j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{i &lt; j}"/>.
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<p>
By construction, <img class="latex" title="{b_2}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_2}"/> and <img class="latex" title="{b_j}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_j}"/> have the same type over <img class="latex" title="{M \cup \{b_1\}}" src="http://s3.wordpress.com/latex.php?latex=%7BM+%5Ccup+%5C%7Bb_1%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M \cup \{b_1\}}"/>, and so <img class="latex" title="{(b_1,b_2)}" src="http://s1.wordpress.com/latex.php?latex=%7B(b_1,b_2)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,b_2)}"/> and <img class="latex" title="{(b_1,b_j)}" src="http://s2.wordpress.com/latex.php?latex=%7B(b_1,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,b_j)}"/> are elementarily indistinguishable over <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>. So it remains to show that <img class="latex" title="{(b_1,b_j)}" src="http://s1.wordpress.com/latex.php?latex=%7B(b_1,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,b_j)}"/> and <img class="latex" title="{(b_i,b_j)}" src="http://s2.wordpress.com/latex.php?latex=%7B(b_i,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_i,b_j)}"/> are elementarily indistinguishable.
</p>
<p>
Let <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> be an <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable relation that contains <img class="latex" title="{(b_1,b_j)}" src="http://s2.wordpress.com/latex.php?latex=%7B(b_1,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,b_j)}"/>; we need to show that <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> contains <img class="latex" title="{(b_i,b_j)}" src="http://s1.wordpress.com/latex.php?latex=%7B(b_i,b_j)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_i,b_j)}"/> also.
</p>
<p>
Since <img class="latex" title="{b_1}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1}"/> and <img class="latex" title="{b_i}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_i}"/> have the same type over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, by homogeneity there exists an automorphism <img class="latex" title="{\sigma}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Csigma%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma}"/> of <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> fixing <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> that maps <img class="latex" title="{b_1}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1}"/> to <img class="latex" title="{b_i}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_i}"/>. Since <img class="latex" title="{b_j}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_j}"/> realises <img class="latex" title="{p\downharpoonright_{M \cup \{b_1\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Bb_1%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p\downharpoonright_{M \cup \{b_1\}}}"/>, we see that <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> contains the sentence <img class="latex" title="{(b_1,x) \in A}" src="http://s1.wordpress.com/latex.php?latex=%7B(b_1,x)+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_1,x) \in A}"/>, hence by invariance <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> contains <img class="latex" title="{(b_i,x) \in A}" src="http://s3.wordpress.com/latex.php?latex=%7B(b_i,x)+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_i,x) \in A}"/> also. Since <img class="latex" title="{b_j}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_j}"/> realises <img class="latex" title="{p\downharpoonright_{M \cup \{b_i\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Bb_i%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p\downharpoonright_{M \cup \{b_i\}}}"/>, we conclude <img class="latex" title="{(b_i,b_j) \in A}" src="http://s3.wordpress.com/latex.php?latex=%7B(b_i,b_j)+%5Cin+A%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{(b_i,b_j) \in A}"/>, as required.
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<p>
This concludes the <img class="latex" title="{k=2}" src="http://s1.wordpress.com/latex.php?latex=%7Bk=2%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k=2}"/> case. The higher <img class="latex" title="{k}" src="http://s2.wordpress.com/latex.php?latex=%7Bk%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{k}"/> case is similar and is left as an exercise. <img class="latex" title="\Box" src="http://s3.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
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<p align="center"><b> —  2. Intersections of wide types  — </b></p>
<p>
Now we assume that the structure <img class="latex" title="{{\Bbb U}}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/> is equipped with an <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-invariant Kiesler measure <img class="latex" title="{\mu}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu}"/>. This leads to the notion of a <em>wide type</em> – a type such that all the <img class="latex" title="{{\Bbb U}}" src="http://s1.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>-definable sets containing this type have positive measure. Intuitively, elements of a wide type are distributed “generically” in the structure.
</p>
<p>
In the <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">previous notes</a> we showed that wide types can be “split” amongst indiscernables, as follows:
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<blockquote><p><b>Lemma 4</b> <a name="indiscern"/> Let <img class="latex" title="{b}" src="http://s2.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> be an element or tuple in <img class="latex" title="{{\Bbb U}}" src="http://s3.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, let <img class="latex" title="{a}" src="http://s1.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> be a wide type over <img class="latex" title="{M \cup \{b\}}" src="http://s2.wordpress.com/latex.php?latex=%7BM+%5Ccup+%5C%7Bb%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M \cup \{b\}}"/> for some set of constants <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, and let <img class="latex" title="{b_1,b_2,\ldots}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_1,b_2,%5Cldots%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,b_2,\ldots}"/> be a sequence of indiscernibles (over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>) that has the same type as <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> (over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>). Then for any finite number <img class="latex" title="{b_1,\ldots,b_n}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_1,%5Cldots,b_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,\ldots,b_n}"/> in this sequence, one can find a type <img class="latex" title="{a'}" src="http://s3.wordpress.com/latex.php?latex=%7Ba'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a'}"/> such that <img class="latex" title="{a'}" src="http://s1.wordpress.com/latex.php?latex=%7Ba'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a'}"/> has the same type over <img class="latex" title="{b_i}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_i}"/> as <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> does over <img class="latex" title="{b}" src="http://s1.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/>, for all <img class="latex" title="{1 \leq i \leq n}" src="http://s2.wordpress.com/latex.php?latex=%7B1+%5Cleq+i+%5Cleq+n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1 \leq i \leq n}"/>. </p></blockquote>
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We now use this lemma to show that sets defined by wide types intersect each other in a uniform fashion.
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<blockquote><p><b>Lemma 5</b> <a name="slosh"/> Let <img class="latex" title="{p,q}" src="http://s3.wordpress.com/latex.php?latex=%7Bp,q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p,q}"/> be types over <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, and let <img class="latex" title="{a,a' \in p({\Bbb U})}" src="http://s2.wordpress.com/latex.php?latex=%7Ba,a'+%5Cin+p(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a,a' \in p({\Bbb U})}"/>, <img class="latex" title="{b,b' \in q({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Bb,b'+%5Cin+q(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b,b' \in q({\Bbb U})}"/> be realisations of <img class="latex" title="{a,b}" src="http://s1.wordpress.com/latex.php?latex=%7Ba,b%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a,b}"/> such that <img class="latex" title="{tp(a/M \cup \{b\})}" src="http://s2.wordpress.com/latex.php?latex=%7Btp(a/M+%5Ccup+%5C%7Bb%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a/M \cup \{b\})}"/> and <img class="latex" title="{tp(a'/M \cup \{b'\})}" src="http://s3.wordpress.com/latex.php?latex=%7Btp(a'/M+%5Ccup+%5C%7Bb'%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a'/M \cup \{b'\})}"/> are wide. Let <img class="latex" title="{A_x}" src="http://s1.wordpress.com/latex.php?latex=%7BA_x%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A_x}"/>, <img class="latex" title="{B_y}" src="http://s2.wordpress.com/latex.php?latex=%7BB_y%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{B_y}"/> be <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable sets with parameters, contained inside an <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable set <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> of finite measure; then <img class="latex" title="{\mu(A_a \cap B_b) &gt; 0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_b)+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_b) &gt; 0}"/> if and only if <img class="latex" title="{\mu(A_{a'} \cap B_{b'}) &gt; 0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba'%7D+%5Ccap+B_%7Bb'%7D)+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a'} \cap B_{b'}) &gt; 0}"/>. </p></blockquote>
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<em>Proof:</em>  By homogeneity, there is an automorphism fixing <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> that sends <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/> to <img class="latex" title="{b'}" src="http://s1.wordpress.com/latex.php?latex=%7Bb'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b'}"/>, and maps <img class="latex" title="{a}" src="http://s2.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> to another element of <img class="latex" title="{p({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Bp(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p({\Bbb U})}"/>. Thus without loss of generality we may assume <img class="latex" title="{b=b'}" src="http://s1.wordpress.com/latex.php?latex=%7Bb=b'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b=b'}"/>.
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We assume for contradiction that <img class="latex" title="{\mu(A_a \cap B_b) &gt; \delta &gt; 0}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_b)+%3E+%5Cdelta+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_b) &gt; \delta &gt; 0}"/> and <img class="latex" title="{\mu(A_{a'} \cap B_{b'}) = 0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba'%7D+%5Ccap+B_%7Bb'%7D)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a'} \cap B_{b'}) = 0}"/>.
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By Lemma <a href="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#ext">2</a>, we may extend <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> to an invariant global type <img class="latex" title="{q'}" src="http://s2.wordpress.com/latex.php?latex=%7Bq'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'}"/>. Observe that for any <img class="latex" title="{\epsilon &gt; 0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cepsilon+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\epsilon &gt; 0}"/>, either one has <img class="latex" title="{\mu(A_a \cap B_x) \geq \epsilon}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_x)+%5Cgeq+%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_x) \geq \epsilon}"/> for all <img class="latex" title="{x \in q'\downharpoonright_{M \cup \{a\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bx+%5Cin+q'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x \in q'\downharpoonright_{M \cup \{a\}}}"/>, or one has <img class="latex" title="{\mu(A_a \cap B_x) \leq \epsilon}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_x)+%5Cleq+%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_x) \leq \epsilon}"/> for all <img class="latex" title="{x \in q'\downharpoonright_{M \cup \{a\}}}" src="http://s1.wordpress.com/latex.php?latex=%7Bx+%5Cin+q'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x \in q'\downharpoonright_{M \cup \{a\}}}"/> (since there is a <img class="latex" title="{M \cup \{a\}}" src="http://s2.wordpress.com/latex.php?latex=%7BM+%5Ccup+%5C%7Ba%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M \cup \{a\}}"/>-definable set between <img class="latex" title="{\{ x: \mu(A_a \cap B_x) \geq \epsilon \}}" src="http://s3.wordpress.com/latex.php?latex=%7B%5C%7B+x:+%5Cmu(A_a+%5Ccap+B_x)+%5Cgeq+%5Cepsilon+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ x: \mu(A_a \cap B_x) \geq \epsilon \}}"/> and <img class="latex" title="{\{ x: \mu(A_a \cap B_x) &gt; \epsilon \}}" src="http://s1.wordpress.com/latex.php?latex=%7B%5C%7B+x:+%5Cmu(A_a+%5Ccap+B_x)+%3E+%5Cepsilon+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ x: \mu(A_a \cap B_x) &gt; \epsilon \}}"/>. Suppose first that the former option holds for some <img class="latex" title="{\epsilon}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\epsilon}"/>, thus there is a uniform lower bound <img class="latex" title="{\mu(A_a \cap B_x) &gt; \epsilon}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_x)+%3E+%5Cepsilon%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_x) &gt; \epsilon}"/>. We now define a sequence <img class="latex" title="{a_1,a_2,\ldots \in p({\Bbb U})}" src="http://s1.wordpress.com/latex.php?latex=%7Ba_1,a_2,%5Cldots+%5Cin+p(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,a_2,\ldots \in p({\Bbb U})}"/> and an indiscernible sequence <img class="latex" title="{b_1,b_2,\ldots \in q({\Bbb U})}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_1,b_2,%5Cldots+%5Cin+q(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,b_2,\ldots \in q({\Bbb U})}"/> as follows:
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<li> We initialise <img class="latex" title="{a_1=a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_1=a%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1=a}"/> and <img class="latex" title="{b_1}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1}"/> to be a realisation of <img class="latex" title="{q'\downharpoonright_{M \cup \{a_1\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bq'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba_1%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'\downharpoonright_{M \cup \{a_1\}}}"/>. </li>
<li> Now suppose that <img class="latex" title="{a_1,\ldots,a_n,b_1,\ldots,b_n}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_1,%5Cldots,a_n,b_1,%5Cldots,b_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1,\ldots,a_n,b_1,\ldots,b_n}"/> have been chosen with <img class="latex" title="{b_1,\ldots,b_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_1,%5Cldots,b_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,\ldots,b_n}"/> indiscernible. By Lemma <a href="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#indiscern">4</a>, we can find <img class="latex" title="{a_{n+1} \in p({\Bbb U})}" src="http://s2.wordpress.com/latex.php?latex=%7Ba_%7Bn+1%7D+%5Cin+p(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_{n+1} \in p({\Bbb U})}"/> that has the same type over <img class="latex" title="{b_i}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_i}"/> that <img class="latex" title="{a'}" src="http://s1.wordpress.com/latex.php?latex=%7Ba'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a'}"/> has over <img class="latex" title="{b'}" src="http://s2.wordpress.com/latex.php?latex=%7Bb'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b'}"/> for all <img class="latex" title="{1 \leq i \leq n}" src="http://s3.wordpress.com/latex.php?latex=%7B1+%5Cleq+i+%5Cleq+n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1 \leq i \leq n}"/>. Since <img class="latex" title="{\mu(A_{a'} \cap B_{b'}) = 0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba'%7D+%5Ccap+B_%7Bb'%7D)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a'} \cap B_{b'}) = 0}"/>, this implies that <img class="latex" title="{\mu( A_{a_{n+1}} \cap B_{b_i} ) = 0}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(+A_%7Ba_%7Bn+1%7D%7D+%5Ccap+B_%7Bb_i%7D+)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu( A_{a_{n+1}} \cap B_{b_i} ) = 0}"/> for all <img class="latex" title="{1 \leq i \leq n}" src="http://s3.wordpress.com/latex.php?latex=%7B1+%5Cleq+i+%5Cleq+n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1 \leq i \leq n}"/>. (Here we use the fact that <img class="latex" title="{\mu( A_x \cap B_b )=0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(+A_x+%5Ccap+B_b+)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu( A_x \cap B_b )=0}"/> is a type-definable formula over <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> and <img class="latex" title="{b}" src="http://s3.wordpress.com/latex.php?latex=%7Bb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b}"/>.) </li>
<li> Now, let <img class="latex" title="{b_{n+1}}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_%7Bn+1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_{n+1}}"/> be a realisation of <img class="latex" title="{q'\downharpoonright_{M \cup \{a_1,\ldots,a_{n+1},b_1,\ldots,b_n\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bq'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba_1,%5Cldots,a_%7Bn+1%7D,b_1,%5Cldots,b_n%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'\downharpoonright_{M \cup \{a_1,\ldots,a_{n+1},b_1,\ldots,b_n\}}}"/>. With this construction and Lemma <a href="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#lob">3</a> we see by induction that <img class="latex" title="{b_1,\ldots,b_{n+1}}" src="http://s3.wordpress.com/latex.php?latex=%7Bb_1,%5Cldots,b_%7Bn+1%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_1,\ldots,b_{n+1}}"/> is also indiscernible; now we iterate the procedure.
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Let <img class="latex" title="{C_i}" src="http://s1.wordpress.com/latex.php?latex=%7BC_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_i}"/> be the set <img class="latex" title="{C_i := A_{a_i} \cap B_{b_i}}" src="http://s2.wordpress.com/latex.php?latex=%7BC_i+:=+A_%7Ba_i%7D+%5Ccap+B_%7Bb_i%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_i := A_{a_i} \cap B_{b_i}}"/>, then observe from the above construction that <img class="latex" title="{C_i}" src="http://s3.wordpress.com/latex.php?latex=%7BC_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_i}"/> lies in <img class="latex" title="{X}" src="http://s1.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/> and <img class="latex" title="{\mu(C_i \cap C_j) = 0}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(C_i+%5Ccap+C_j)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C_i \cap C_j) = 0}"/> for all <img class="latex" title="{i &lt; j}" src="http://s3.wordpress.com/latex.php?latex=%7Bi+%3C+j%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{i &lt; j}"/>. On the other hand, we claim that <img class="latex" title="{\mu(C_i)}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(C_i)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(C_i)}"/> is uniformly bounded away from zero, this contradicts the finite measure of <img class="latex" title="{\mu(X)}" src="http://s2.wordpress.com/latex.php?latex=%7B%5Cmu(X)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(X)}"/> by the pigeonhole principle.
</p>
<p>
To see the uniform lower bound, find an automorphism <img class="latex" title="{\sigma_i}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Csigma_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\sigma_i}"/> fixing <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/> that maps <img class="latex" title="{a_1}" src="http://s2.wordpress.com/latex.php?latex=%7Ba_1%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1}"/> to <img class="latex" title="{a_i}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_i}"/>. By hypothesis, <img class="latex" title="{\mu(A_{a_1} \cap B_{b_1}) &gt; 0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba_1%7D+%5Ccap+B_%7Bb_1%7D)+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a_1} \cap B_{b_1}) &gt; 0}"/>, thus there exists a rational <img class="latex" title="{r &gt; 0}" src="http://s2.wordpress.com/latex.php?latex=%7Br+%3E+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{r &gt; 0}"/> such that the predicate that models <img class="latex" title="{\mu(A_{a_1} \cap B_x) &gt; r}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba_1%7D+%5Ccap+B_x)+%3E+r%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a_1} \cap B_x) &gt; r}"/> is in <img class="latex" title="{\tilde q}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Ctilde+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\tilde q}"/>, hence in <img class="latex" title="{q'}" src="http://s2.wordpress.com/latex.php?latex=%7Bq'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'}"/>. By invariance, the predicate <img class="latex" title="{\mu(A_{a_i} \cap B_x) &gt; r}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba_i%7D+%5Ccap+B_x)+%3E+r%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a_i} \cap B_x) &gt; r}"/> is in <img class="latex" title="{q'}" src="http://s1.wordpress.com/latex.php?latex=%7Bq'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'}"/> also, hence by construction of <img class="latex" title="{b_i}" src="http://s2.wordpress.com/latex.php?latex=%7Bb_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_i}"/>, <img class="latex" title="{\mu(A_{a_i} \cap B_{b_i}) &gt; r}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba_i%7D+%5Ccap+B_%7Bb_i%7D)+%3E+r%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a_i} \cap B_{b_i}) &gt; r}"/>, and the claim follows.
</p>
<p>
Now we consider the opposite case, in which <img class="latex" title="{\mu(A_a \cap B_x) = 0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_a+%5Ccap+B_x)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_a \cap B_x) = 0}"/> for all <img class="latex" title="{x \in q'\downharpoonright_{M \cup \{a\}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bx+%5Cin+q'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba%5C%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{x \in q'\downharpoonright_{M \cup \{a\}}}"/>. Then we run the construction slightly differently: for each <img class="latex" title="{n}" src="http://s3.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/> in turn, set <img class="latex" title="{b_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_n}"/> to be a realisation of <img class="latex" title="{q'\downharpoonright_{M \cup \{a_1,\ldots,a_{n-1},b_1,\ldots,b_{n-1}}}" src="http://s2.wordpress.com/latex.php?latex=%7Bq'%5Cdownharpoonright_%7BM+%5Ccup+%5C%7Ba_1,%5Cldots,a_%7Bn-1%7D,b_1,%5Cldots,b_%7Bn-1%7D%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q'\downharpoonright_{M \cup \{a_1,\ldots,a_{n-1},b_1,\ldots,b_{n-1}}}"/>, then set <img class="latex" title="{a_n \in p({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_n+%5Cin+p(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_n \in p({\Bbb U})}"/> so that <img class="latex" title="{\mu(A_{a_n} \cap B_{b_n}) &gt; \delta}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A_%7Ba_n%7D+%5Ccap+B_%7Bb_n%7D)+%3E+%5Cdelta%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A_{a_n} \cap B_{b_n}) &gt; \delta}"/>. (This is possible because for any definable set <img class="latex" title="{C}" src="http://s2.wordpress.com/latex.php?latex=%7BC%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C}"/> containing <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/>, the <img class="latex" title="{\bigwedge}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cbigwedge%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\bigwedge}"/>-definable set <img class="latex" title="{\{ x \in C: \mu(A_x \cap B_b) \geq \delta \}}" src="http://s2.wordpress.com/latex.php?latex=%7B%5C%7B+x+%5Cin+C:+%5Cmu(A_x+%5Ccap+B_b)+%5Cgeq+%5Cdelta+%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\{ x \in C: \mu(A_x \cap B_b) \geq \delta \}}"/> contains <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> and thus has positive measure, and so the same is true for <img class="latex" title="{b_n}" src="http://s1.wordpress.com/latex.php?latex=%7Bb_n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{b_n}"/>; now use saturation.) Then again we see that the <img class="latex" title="{C_i}" src="http://s2.wordpress.com/latex.php?latex=%7BC_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{C_i}"/> lie in <img class="latex" title="{X}" src="http://s3.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>, have intersection of measure zero, and have measure uniformly bounded from below, and we again obtain a contradiction. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
Now we place a group structure on <img class="latex" title="{{\Bbb U}}" src="http://s2.wordpress.com/latex.php?latex=%7B%7B%5CBbb+U%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{{\Bbb U}}"/>, and obtain a variant of the above result:
</p>
<blockquote><p><b>Proposition 6</b>  Let <img class="latex" title="{p, q}" src="http://s3.wordpress.com/latex.php?latex=%7Bp,+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p, q}"/> be types in <img class="latex" title="{M}" src="http://s1.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>, with <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> wide. Suppose that <img class="latex" title="{p}" src="http://s3.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/>, <img class="latex" title="{q}" src="http://s1.wordpress.com/latex.php?latex=%7Bq%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{q}"/> are contained in <img class="latex" title="{M}" src="http://s2.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable sets <img class="latex" title="{X, X'}" src="http://s3.wordpress.com/latex.php?latex=%7BX,+X'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X, X'}"/> such that <img class="latex" title="{XX'}" src="http://s1.wordpress.com/latex.php?latex=%7BXX'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{XX'}"/> has finite measure. Let <img class="latex" title="{a,b \in q}" src="http://s2.wordpress.com/latex.php?latex=%7Ba,b+%5Cin+q%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a,b \in q}"/> be such that the type of <img class="latex" title="{a}" src="http://s3.wordpress.com/latex.php?latex=%7Ba%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a}"/> over <img class="latex" title="{M \cup \{b\}}" src="http://s1.wordpress.com/latex.php?latex=%7BM+%5Ccup+%5C%7Bb%5C%7D%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M \cup \{b\}}"/> is wide. Assume also that the Keisler measure is translation-invariant. Then <img class="latex" title="{pa \cap pb}" src="http://s2.wordpress.com/latex.php?latex=%7Bpa+%5Ccap+pb%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{pa \cap pb}"/> is also wide. </p></blockquote>
<p/>
<p>
<em>Proof:</em>  Suppose this is not the case, so that there exists an <img class="latex" title="{M}" src="http://s3.wordpress.com/latex.php?latex=%7BM%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{M}"/>-definable set <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> containing <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> such that <img class="latex" title="{Aa \cap Ab}" src="http://s3.wordpress.com/latex.php?latex=%7BAa+%5Ccap+Ab%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Aa \cap Ab}"/> has zero measure. (Initially, one would need two different definable sets containing <img class="latex" title="{p}" src="http://s1.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/>, but one can simply take their intersection.) On the other hand, as <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> is wide, <img class="latex" title="{A}" src="http://s3.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> itself has positive measure. We can place <img class="latex" title="{A}" src="http://s1.wordpress.com/latex.php?latex=%7BA%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{A}"/> in <img class="latex" title="{X}" src="http://s2.wordpress.com/latex.php?latex=%7BX%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{X}"/>.
</p>
<p>
By using the fact that wide types over one set of constants can be refined to wide types over larger sets of constants (Lemma 2 from the <a href="http://terrytao.wordpress.com/2009/10/22/reading-seminar-2-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/">previous notes</a>), we see that we can recursively construct a sequence <img class="latex" title="{a_1, a_2, \ldots \in q({\Bbb U})}" src="http://s3.wordpress.com/latex.php?latex=%7Ba_1,+a_2,+%5Cldots+%5Cin+q(%7B%5CBbb+U%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{a_1, a_2, \ldots \in q({\Bbb U})}"/> with <img class="latex" title="{tp(a_n/M \cup \{a_1,\ldots,a_{n-1}\})}" src="http://s1.wordpress.com/latex.php?latex=%7Btp(a_n/M+%5Ccup+%5C%7Ba_1,%5Cldots,a_%7Bn-1%7D%5C%7D)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{tp(a_n/M \cup \{a_1,\ldots,a_{n-1}\})}"/> wide for all <img class="latex" title="{n}" src="http://s2.wordpress.com/latex.php?latex=%7Bn%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{n}"/>. Since <img class="latex" title="{\mu(Aa \cap Ab) = 0}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(Aa+%5Ccap+Ab)+=+0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(Aa \cap Ab) = 0}"/>, we conclude from Lemma <a href="http://terrytao.wordpress.com/2009/10/29/reading-seminar-3-stable-group-theory-and-approximate-subgroups-by-ehud-hrushovski/#slosh">5</a> that <img class="latex" title="{\mu(A a_n \cap A a_i)=0}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A+a_n+%5Ccap+A+a_i)=0%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A a_n \cap A a_i)=0}"/> for all <img class="latex" title="{1 \leq i &lt; n}" src="http://s2.wordpress.com/latex.php?latex=%7B1+%5Cleq+i+%3C+n%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{1 \leq i &lt; n}"/>. On the other hand, the <img class="latex" title="{\mu(Aa_i)}" src="http://s3.wordpress.com/latex.php?latex=%7B%5Cmu(Aa_i)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(Aa_i)}"/> all have the same measure as <img class="latex" title="{\mu(A)}" src="http://s1.wordpress.com/latex.php?latex=%7B%5Cmu(A)%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{\mu(A)}"/>, which is positive. Finally, the <img class="latex" title="{Aa_i}" src="http://s2.wordpress.com/latex.php?latex=%7BAa_i%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{Aa_i}"/> are all contained in <img class="latex" title="{XX'}" src="http://s3.wordpress.com/latex.php?latex=%7BXX'%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{XX'}"/>, which has finite measure; this leads to a contradictoin. <img class="latex" title="\Box" src="http://s1.wordpress.com/latex.php?latex=%5CBox&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\Box"/></p>
<p>
This “generic intersection” property of translates of <img class="latex" title="{p}" src="http://s2.wordpress.com/latex.php?latex=%7Bp%7D&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="{p}"/> will be important in later arguments when creating near-groups.
</p><p/>
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      <subtitle type="text">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
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    <title type="text">highly parameterized models of data</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>As my loyal reader knows, I have no fear when it comes to models with huge numbers of parameters; indeed the <a href="http://arxiv.org/abs/astro-ph/0703454">ubercalibration</a> project is effectively a fit with hundreds of millions of parameters, and we can <i>prove</i> that we got the global optimum (in the sense that we made sure the problem is guaranteed to be convex).  Today Roweis pitched a generalization of all this, in which one creates a very flexible linear model space, where parameters are tied to or in a hierarchy of meta-data, such that some parameters are tied to, say, the date, some to the airmass, some to the seeing, some to the camera column, and so on.  Then the model <i>discovers</i> which parameters are necessary for accurate modeling of the data and thereby discovers important meta-data, dependencies of the data on artificial issues, and bad data.  We tentatively agreed to run this on the new BOSS spectra from <a href="http://sdss3.org/">SDSS-III</a>.</p><div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/10448119-1573064702063646441?l=hoggresearch.blogspot.com" height="1" width="1"/></div></div>
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    <updated>2009-11-05T16:16:57-05:00</updated>
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    <category term="data" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="sample" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="model" scheme="http://www.blogger.com/atom/ns#"/>
    <category term="bayes" scheme="http://www.blogger.com/atom/ns#"/>
    <title type="text">more sampling</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Iain Murray gave another nice talk today, this time in the machine learning group, about a high-end sampling method called <q>elliptical slice sampling</q>, optimized for gaussian process modeling, where calls to the prior probability distribution function are more expensive than likelihood calls.  It was a very nice talk and got me thinking about slice sampling in general, which might be very useful to us.</p><div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/10448119-3111575521792225969?l=hoggresearch.blogspot.com" height="1" width="1"/></div></div>
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    <author>
      <name>Hogg</name>
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      <id>tag:blogger.com,1999:blog-10448119</id>
      <updated>2009-11-06T21:29:42-05:00</updated>
      <title type="text">Hogg's Research</title>
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  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Orbits, Periodic Orbits, and Dense Orbits - Oh My!</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p> Another one of the fundamental properties of a chaotic system is
<em>dense periodic orbits</em>.  It's a bit of an odd one: a chaotic
system doesn't have to have periodic orbits <em>at all</em>. But if it
does, then they have to be dense.</p>

<p> The dense periodic orbit rule is, in many ways, very similar to the
sensitivity to initial conditions. But personally, I find it rather more
interesting a way of describing key concept. The idea is, when you've got a
dense periodic orbit, it's an odd thing. It's a repeating system, which will
cycle through the same behavior, over and over again. But when you look at a
state of the system, you can't tell which fixed path it's on. In fact,
miniscule differences in the position, differences so small that you can't
measure them, can put you onto dramatically different paths. There's
the similarity with the initial conditions rule: you've got the same 
basic idea of tiny changes producing dramatic results.</p> <a href="http://scienceblogs.com/goodmath/2009/11/orbits_periodic_orbits_and_den.php">Read the rest of this post...</a> | <a href="http://scienceblogs.com/goodmath/2009/11/orbits_periodic_orbits_and_den.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/CyKN/~4/JJO5yPh82Fo" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/CyKN/~3/JJO5yPh82Fo/orbits_periodic_orbits_and_den.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/goodmath/2009/11/orbits_periodic_orbits_and_den.php</id>
         
    <category term="Chaos"/>
         
         
    <published>2009-11-05T12:16:18-05:00</published>
      
    <updated>2009-11-05T12:16:18-05:00</updated>
    <source>
      <title>Good Math, Bad Math</title>
      <link href="http://scienceblogs.com/goodmath/" rel="alternate"/>
      <subtitle>Finding the fun in good math; Shredding bad math and squashing the crackpots who espouse it.</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-06T14:58:50-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
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      <id>http://scienceblogs.com/goodmath/</id>
    </source>
  </entry>

  <entry xmlns:dc="http://purl.org/dc/elements/1.1/" xml:base="http://www.scientificblogging.com">
 
    <title>The Say of the Week: Lederman's Shoulder</title>
 
    <link href="http://www.scientificblogging.com/quantum_diaries_survivor/blog/say_week_ledermans_shoulder" rel="alternate"/>
 
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">"The yield of muon pairs decreased rapidly from 1 GeV to the kinematic limit of nearly 6 GeV with the exception of a curious shoulder near 3GeV. The measurement of muons was by <em>range</em> as determined by liquid and plastic scintillation counters interspersed with steel shielding. Each angular bin (there were 18) had four range bins, and for two muons this made a total of only 5000 mass bins into which to sort the data. Multiple scattering in the minimum of 10 feet of steel<br/>made finer binning useless. Thus we could only note that "Indeed, in the mass region near 3.5 GeV, the observed spectrum may be reproduced by a composite of a resonance and a steeper continuum." This 1968-1969 experiment was repeated in 1974 by Aubert et al. (1974), with a<br/><br/>
<p><a href="http://www.scientificblogging.com/quantum_diaries_survivor/blog/say_week_ledermans_shoulder" target="_blank">read more</a></p></div>
    </summary>
 
    <link href="http://www.scientificblogging.com/quantum_diaries_survivor/blog/say_week_ledermans_shoulder#comments" rel="replies" type="text/html"/>
 
    <category term="Physics" scheme="http://www.scientificblogging.com/physics"/>
 
    <published>2009-11-05T16:13:26+00:00</published>
 
    <author>
      <name>dorigo</name>
    </author>
 
    <id>urn:feed-entry-id:61280 at http://www.scientificblogging.com</id>

    <updated>2009-11-05T16:13:26+00:00</updated>
    <source>
      <title>dorigo's blog</title>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor" rel="alternate"/>
      <subtitle>Science 2.0</subtitle>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor/feed" rel="self"/>
      <id>http://www.scientificblogging.com/quantum_diaries_survivor</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://asymptotia.com/wp-atom.php">
		
    <author>
			
      <name>Clifford</name>
						
      <uri>http://asymptotia.com/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Remote Office</div>
    </title>
		
    <link href="http://asymptotia.com/2009/11/04/remote-office/" rel="alternate" type="text/html"/>
		
    <id>http://asymptotia.com/?p=5326</id>
		
    <updated>2009-11-05T16:05:20+00:00</updated>
		
    <published>2009-11-05T06:26:42+00:00</published>
		
    <category term="personal" scheme="http://asymptotia.com/"/>
    <category term="travel" scheme="http://asymptotia.com/"/>
    <category term="work" scheme="http://asymptotia.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">I'm in remote office mode again. I've to give two colloquia while visiting two physics departments in Vancouver area over the next two days. (Subject matter will be essentially the same as the one I gave <a href="http://asymptotia.com/2009/10/01/there-goes-the-weekend/">a month ago</a>.) So tonight, I'm eating dinner at the splendid  restaurant <em>Banana Leaf</em> not far from my hotel while reviewing the slides of my presentations on my pda <small>(my iTouch <a href="http://asymptotia.com/wp-images/2009/11/dining_at_banana_leaf.jpg"><img class="alignleft size-medium wp-image-5327" title="dining_at_banana_leaf" src="http://asymptotia.com/wp-images/2009/11/dining_at_banana_leaf-300x225.jpg" alt="dining_at_banana_leaf" width="180"/></a>-  I dump lots of files I want to read on it using an application called filemagnet. Very useful. See <a href="http://asymptotia.com/2009/07/31/testing-testing/">here</a>. In this case I'm looking at the pdf output from the keynote presentation software I use. )</small> I'm making a few notes on changes I'll make when I get back to my hotel. I'm also reviewing a few other documents that were sent to me for response, and tying off various loose ends here and there before the evening ends.

I sometimes worry that it might be considered rude that I'm apparently doing a bit of work and so not fully paying attention to the food, but I'm not too worried, really. Once the actual food arrives  I've been quite appreciative of it, giving it my full [...]</div>
    </summary>
		
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		<thr:total>4</thr:total>
	
    <source>
      <title type="text">Asymptotia</title>
      <updated>2009-11-06T18:08:45+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.7.1">WordPress</generator>
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    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Sports Poll: Yankees Win</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>I have a lab all morning, so I won't get to more substantive blogging before this afternoon. The Yankees won their 27th World Series title last night, though, and given their status as the most polarizing team in baseball, this seems like a good excuse for a poll:</p>

<p>
&lt;a href="http://answers.polldaddy.com/poll/2213713/"&gt;What do you think about the Yankees winning the World Series?&lt;/a&gt;&lt;span style="font-size:9px;"&gt;(&lt;a href="http://www.polldaddy.com"&gt;surveys&lt;/a&gt;)&lt;/span&gt;
</p>

<p>Choose only one.</p>
 <a href="http://scienceblogs.com/principles/2009/11/sports_poll_yankees_win.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/nwjYyyuajBo" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/nwjYyyuajBo/sports_poll_yankees_win.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/principles/2009/11/sports_poll_yankees_win.php</id>
         
    <category term="Polls"/>
         
         
    <published>2009-11-05T09:55:40-05:00</published>
      
    <updated>2009-11-05T09:55:40-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-07T11:21:56-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
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      <id>http://scienceblogs.com/principles/</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://blogs.uslhc.us/wp-atom.php">
		
    <author>
			
      <name>Seth Zenz</name>
						
      <uri>http://cern.ch/sethzenz/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Much Ado About 2.2 TeV</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2825" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2825</id>
		
    <updated>2009-11-05T14:16:05+00:00</updated>
		
    <published>2009-11-05T13:07:13+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">It was reported last week by Dennis Overbye at the New York Times that the LHC is only going to reach a center-of-mass energy of 2.2 TeV (i.e. an energy of 1.1 TeV per beam) before the winter shutdown.  I was asked about this previously, and at the time I thought it was “in [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2825"><div xmlns="http://www.w3.org/1999/xhtml"><p>It was reported <a href="http://topics.blogs.nytimes.com/2009/10/27/the-cosmic-countdown-in-geneva-goes-on/">last week by Dennis Overbye at the New York Times</a> that the LHC is only going to reach a center-of-mass energy of 2.2 TeV (i.e. an energy of 1.1 TeV per beam) before the winter shutdown.  I was asked about this previously, and at the time I thought it was “in a schedule somewhere.”  After looking around, though, it’s much less clear to me where the information actually come from — maybe I heard it from people who had read the New York Times blog, and maybe Overbye originally learned it from <a href="http://www.nytimes.com/2009/10/13/science/space/13lhc.html">magical time-traveling Higgs Bosons</a>!  So we might have to demote the whole thing to the category of rumor — but it’s a rumor that appeared in the news, so I can certainly say what I’d think about it <em>if</em> it were true.</p>
<p>If indeed the LHC only achieves an energy of 2.2 TeV by the time it’s shut down in mid-December, some might be tempted to characterize it as a serious setback or defeat; in fact, it’s nothing of the kind.  Here’s what’s really going on: the LHC is in the middle of an ongoing start-up process, and has to take a quick break in December and January, but will then pick up where it left off.  That means that the point the accelerator startup happens to reach before shutdown doesn’t mean anything special at all — the really important thing is where it gets to when the process continues next year.</p>
<p>What we do know from CERN is that there are <a href="http://cdsweb.cern.ch/journal/article?name=CERNBulletin&amp;issue=43/2009&amp;number=3&amp;category=News%20Articles&amp;ln=en">three stages of LHC magnet commisionning</a>: to 2000, 4000, and 6000 amps of current.  We also know that reaching 2000 amps <a href="http://cdsweb.cern.ch/journal/article?name=CERNBulletin&amp;issue=45/2009&amp;number=1&amp;category=News%20Articles&amp;ln=en">“allow[s] the passage and guidance of beams at about 1.2 TeV”</a> (which sounds close enough to the 1.1 TeV figure to be rounding uncertainty).  So if there were only time to commission to 2000 amps before the end of the year, that could certainly explain the limited beam energy.</p>
<p>Is running at 2.2 TeV good for the physics program?  Oddly enough, if we only have a few days of running, there are two lower energies that would be more fun for physicists.  The best option might be to continue at the energy at which the center-of-mass energy achieved by the previous accelerator stage, 0.9 TeV.  This is the energy that the first collisions will happen at, and longer running at a single energy would let those of us who work on the detectors get a better handle on how our data looks.  (For example, I could attempt to do an early, quick version of <a href="http://blogs.uslhc.us/?p=2445">my track jet analysis</a>.  In fact, I’ll try to do that no matter what; it will be good practice, if nothing else.)  Another option might be to run at exactly 1.96 TeV, which is the energy of the Tevatron accelerator at Fermilab; that would give us a rare chance to look at the differences between proton-proton and proton-<em>anti</em>proton collisions at the same energy.</p>
<p>But the physics program isn’t the top priority this year, it’s getting the LHC fully up and running.  Whatever the rumors say, we don’t yet know how far accelerator commissioning will get this year.  Even 2.2 TeV would be enough to make the LHC the highest-energy collider in the world, which is an accomplishment to be proud of.  No matter what, there will be much more to do next year, and we can start making discoveries!  — <a href="http://blogs.uslhc.us/?author=9">Seth</a></p>
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		<thr:total>8</thr:total>
	
    <source>
      <title type="text">US LHC Blog</title>
      <subtitle type="text">US LHC Blogs</subtitle>
      <updated>2009-11-06T16:48:23+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.8.4">WordPress</generator>
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  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Beyond Rocket Science</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>It's not getting as much press as the "X Prize" for private rocket launches, but NASA has quietly been running a contest for work toward a "space elevator," offering up to $2 million for a scheme to transmit power to a small robot climbing a 1km cable. Yesterday, the team from <a href="http://www.lasermotive.com/blog/">LaserMotive</a>, including certified rocket scientist and friend of the blog Jordin Kare, <a href="http://www.ajc.com/news/nation-world/success-in-space-elevator-185413.html">successfully powered a robot up a 900m cable</a> using diode laser arrays to send power to solar panels on the robot. They managed an average speed of 3.73 m/s, which doesn't get them the full $2 million prize, but qualified them for the $900,000 prize for an average speed above 2 m/s.</p>

<p>There are still two other teams in the competition, which will continue today. The Kansas City Space Pirates team got within 50 m of the top, but not fast enough to be in the money, and a team from the University of Saskatchewan has yet to compete at all. LaserMotive can apparently take another crack as well, and over on Twitter, <a href="http://twitter.com/mkkare">Mary Kay Kare</a> says that Jordin has some ideas of how to speed their climber up, and go for the grand prize.</p>

<p>This is a long, long way from an actual space elevator, of course-- working out the power beaming is arguably less of a challenge than finding a material to build the thing out of, which nobody has come close to doing. Still, it's cool to see, and a reminder that while rockets are flashier, there's work going on on other ways to get stuff into space in an economical manner.</p>
 <a href="http://scienceblogs.com/principles/2009/11/beyond_rocket_science.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/Cjr0uJFzuU4" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/Cjr0uJFzuU4/beyond_rocket_science.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/principles/2009/11/beyond_rocket_science.php</id>
         
    <category term="Science"/>
         
         
    <published>2009-11-05T08:45:09-05:00</published>
      
    <updated>2009-11-05T08:45:09-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-07T11:21:56-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
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      <id>http://scienceblogs.com/principles/</id>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>Links for 2009-11-05</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><ul class="delicious"><li>
                <div class="delicious-link"><a href="http://www.philosophypress.co.uk/?p=802">TPM: The Philosophers' Magazine | My philosophy: Alan Sokal</a></div>
                <div class="delicious-extended">"Physicists, when they do philosophy, often do it badly. They're often confused about the conceptual foundations of their own physics, because sometimes you can compute and get the right results even if you don't understand conceptually very well what you're doing. That's a criticism that not only philosophers but also mathematicians make of physics. Because I'm half a mathematician I respect that criticism too. So it's absolutely true that physicists often make a botch of the conceptual foundations of physics, especially when it comes to quantum mechanics, because quantum mechanics is simply much harder than any other physics we know. Everybody makes a botch of it because we don't really know what's going on.

"I think there is also something in physicists' complaints about philosophers that often what they do is so sterile that it's of virtually no relevance to any working scientist, even at the level of conceptually clarifying important things in their fields."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/philosophy">philosophy</a> <a href="http://delicious.com/orzelc/physics">physics</a> <a href="http://delicious.com/orzelc/science">science</a> <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/humanities">humanities</a> <a href="http://delicious.com/orzelc/social-science">social-science</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://crookedtimber.org/2009/11/04/applications/">Applications -- Crooked Timber</a></div>
                <div class="delicious-extended">"In more recent years, the number of positions advertised in English has hovered around 1600-1700.  This year, one of my students told me that she'd heard the number would be something like 250.  "WTF," I calmly replied. "Where did that number come from?"  It came from a wiki of some kind, which is apparently what These Kids Today use when they're not twittering on the FaceSpace.  "That would be a Depression-era number," I said, "because I don't believe there's been a time since the MLA started keeping stats when the number was below 1,000."  Well, it's now looking like 250 is indeed a very low estimate.  But it's quite possible that the number will wind up being below 1,000, which is a problem, because all the MLA charts run from 1,000 to 2,000, so that 2009-10 might require the MLA to redesign the things or face the prospect of publishing one of those cartoon-charts where the plummeting line runs right off the page."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/jobs">jobs</a> <a href="http://delicious.com/orzelc/economics">economics</a> <a href="http://delicious.com/orzelc/humanities">humanities</a> <a href="http://delicious.com/orzelc/blogs">blogs</a> <a href="http://delicious.com/orzelc/crooked-timber">crooked-timber</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://www.insidehighered.com/news/2009/11/04/harass">News: The Curious 'Sexual Harassment' Charge - Inside Higher Ed</a></div>
                <div class="delicious-extended">"East Georgia College has dropped an unspecified sexual harassment charge against an English professor who, ironically, had openly criticized the lack of protections for the falsely accused in its sexual harassment policy.

Two weeks ago, Thomas Thibeault was informed in a letter from John Black, president of East Georgia, that "the evidence" in the mysterious complaint filed against him in August "does not warrant the charge of sexual harassment" and that he was reinstated to his position, ending a nearly two-month suspension. Black and other East Georgia officials did not respond to requests for comment regarding this about-face. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/gender">gender</a> <a href="http://delicious.com/orzelc/politics">politics</a> <a href="http://delicious.com/orzelc/inside-higher-ed">inside-higher-ed</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://science-professor.blogspot.com/2009/11/45-45-10.html">FemaleScienceProfessor: 45 : 45 : 10</a></div>
                <div class="delicious-extended">"A visiting colleague and I recently discussed a perennial topic of obsession among some academics: how our departments/universities assign teaching loads.

Some departments (either by choice or by requirement from an external source) have rigid teaching loads that are the same for all faculty. Some departments assign different teaching loads to different faculty as a function of seniority; in recent years, I have seen some departments assign less teaching to assistant professors and more to associate and full professors, but in days of yore, it was the other way around (and may still be in some departments). Some departments assign different teaching loads to different faculty as a function of faculty research activity."</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/academia">academia</a> <a href="http://delicious.com/orzelc/education">education</a> <a href="http://delicious.com/orzelc/culture">culture</a> <a href="http://delicious.com/orzelc/jobs">jobs</a> <a href="http://delicious.com/orzelc/fsp">fsp</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://mediadecoder.blogs.nytimes.com/2009/10/19/the-robots-are-coming-oh-theyre-here/">The Robots Are Coming! Oh, They're Here. - Media Decoder Blog - NYTimes.com</a></div>
                <div class="delicious-extended">"Sportswriting has long played host to some of the most glorious, along with the most cliché-ridden, exercises in journalism. As anybody on a sports beat can tell you, making game stories interesting day in and day out can be a brutal challenge, but for those with lesser ambitions, it can be something that you do in your sleep. Now some kids at the Intelligent Information Laboratory at Northwestern University are suggesting that an average game day story can be bolted together without human intervention. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/sports">sports</a> <a href="http://delicious.com/orzelc/journalism">journalism</a> <a href="http://delicious.com/orzelc/technology">technology</a> <a href="http://delicious.com/orzelc/media">media</a> <a href="http://delicious.com/orzelc/silly">silly</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://twistedphysics.typepad.com/cocktail_party_physics/2009/11/the-science-of-skymall.html">Cocktail Party Physics: the science of skymall</a></div>
                <div class="delicious-extended">"Here's a handy travel tip: be sure to pack sufficient reading material for your six-hour return flight to Los Angeles. After whipping through a new (forthcoming) biography of reclusive mathematician Grigory Perelman, I found myself at loose ends halfway through my flight home, even after perusing the in-flight magazine detailing glorious three-day vacations in exotic locales I could never afford. So I found myself browsing the Skymall catalog in desperation. You know the one: it features merchandise you never realized you needed, from a variety of outlets, all readily available for order on the in-flight phone. It also features no small measure of Science!"</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/science">science</a> <a href="http://delicious.com/orzelc/gadgets">gadgets</a> <a href="http://delicious.com/orzelc/blogs">blogs</a> <a href="http://delicious.com/orzelc/cocktail-party">cocktail-party</a> <a href="http://delicious.com/orzelc/technology">technology</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://www.midmajority.com/">The Mid-Majority</a></div>
                <div class="delicious-extended">"You might be an alumnus of one of the 251 colleges and universities below the Red Line. You might even be attending one now, and living in that pleasant time-window before the student loan bills start coming. If you didn't go to a small college, or if you didn't go to college at all, it doesn't matter -- you can still join in. But this -- right now -- is the time to jump on board, when the slate is clean and opportunities seem boundless. Even if you've never heard of these schools and don't know where they are, this is the time to adopt. Choose your allegiance now, and definitely not later.

But who's going to believe you five months from now? Don't worry. For the first time ever, TMM has a way for you to prove that you were here, at the beginning. It's fast, fun... and unlike most of the stuff on this site, free. You will be a confirmed and certified fan, with a document as real as anything Price Waterhouse has ever issued. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/basketball">basketball</a> <a href="http://delicious.com/orzelc/sports">sports</a> <a href="http://delicious.com/orzelc/blogs">blogs</a> <a href="http://delicious.com/orzelc/mid-majority">mid-majority</a>)</div>
            </li><li>
                <div class="delicious-link"><a href="http://www.theonion.com/content/news_briefs/barack_obama_names_alan?utm_source=onion_rss_daily">Barack Obama Names Alan Moore Official White House Biographer | The Onion - America's Finest News Source</a></div>
                <div class="delicious-extended">""As evidenced by his epic run on Swamp Thing #21-64, Moore's deft hand with both sociopolitical commentary and metaphysical violence makes him an ideal choice to chronicle my time in office," Obama said of the author of Watchmen and From Hell, whom he reportedly chose over others on a short list of potential biographers that included Warren Ellis, Grant Morrison, and Bob Woodward. "</div>
                <div class="delicious-tags">(tags: <a href="http://delicious.com/orzelc/comics">comics</a> <a href="http://delicious.com/orzelc/silly">silly</a> <a href="http://delicious.com/orzelc/politics">politics</a> <a href="http://delicious.com/orzelc/onion">onion</a>)</div>
            </li></ul> <a href="http://scienceblogs.com/principles/2009/11/links_for_2009-11-05.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/ZyxpnjOx8Yk" height="1" width="1"/></div>
    </summary>
         
    <link href="http://feedproxy.google.com/~r/scienceblogs/uncertainprinciples/~3/ZyxpnjOx8Yk/links_for_2009-11-05.php" rel="alternate"/>
         
    <id>http://scienceblogs.com/principles/2009/11/links_for_2009-11-05.php</id>
         
    <category term="Links Dump"/>
         
         
    <published>2009-11-05T06:41:14-05:00</published>
      
    <updated>2009-11-05T06:41:14-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
      <link href="http://scienceblogs.com/principles/" rel="alternate"/>
      <subtitle>Physics, Politics, Pop Culture</subtitle>
      <rights>Copyright 2009</rights>
      <updated>2009-11-07T11:21:56-05:00</updated>
      <generator>http://www.sixapart.com/movabletype/?v=4.261</generator>
      <link href="http://feeds.feedburner.com/scienceblogs/uncertainprinciples" rel="self" type="application/rss+xml"/>
      <link href="http://pubsubhubbub.appspot.com/" rel="hub"/>
      <id>http://scienceblogs.com/principles/</id>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://blogs.uslhc.us/wp-atom.php">
		
    <author>
			
      <name>Mike Anderson</name>
						
      <uri>http://www.hep.wisc.edu/~mbanderson/</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">What Went Wrong Last Year</div>
    </title>
		
    <link href="http://blogs.uslhc.us/?p=2816" rel="alternate" type="text/html"/>
		
    <id>http://blogs.uslhc.us/?p=2816</id>
		
    <updated>2009-11-05T05:25:41+00:00</updated>
		
    <published>2009-11-04T21:23:54+00:00</published>
		
    <category term="Uncategorized" scheme="http://blogs.uslhc.us/"/>
    <category term="LHC" scheme="http://blogs.uslhc.us/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Brian Cox explains in this 3 minute talk from Feb 2009 what went wrong at CERN last year, and why continuing this work, despite setbacks, is worth it.
It has been over a year since that accident, and many repairs and improvements have been made including:

Replacing 53 magnets  (out of 9,000)
Installing extra  pressure relief valves
Installing [...]</div>
    </summary>
		
    <content type="xhtml" xml:base="http://blogs.uslhc.us/?p=2816"><div xmlns="http://www.w3.org/1999/xhtml"><p> </p>
<p>Brian Cox explains in this 3 minute talk from Feb 2009 what went wrong at CERN last year, and why continuing this work, despite setbacks, is worth it.</p>
<p>It has been over a year since that accident, and many repairs and improvements have been made including:</p>
<ul>
<li>Replacing 53 magnets  (out of 9,000)</li>
<li>Installing extra  pressure relief valves</li>
<li>Installing monitors to ensure  this can’t happen again</li>
</ul>
<p>This has made me more confident, but at the same time, the problem we hit happened just after one week of running – maybe there are problems we would have hit only after a few weeks of running, or a few months?</p>
<p>We don’t know everything that might happen, so I’m glad we are playing it safer this time.</p>
<a href="http://www.addtoany.com/share_save?linkurl=http://blogs.uslhc.us/?p=2816&amp;linkname=What%20Went%20Wrong%20Last%20Year" class="a2a_dd addtoany_share_save"><img src="http://blogs.uslhc.us/wp-content/plugins/add-to-any/share_save_120_16.png" height="16" alt="Share/Bookmark" width="120"/></a></div>
    </content>
		
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		<thr:total>0</thr:total>
	
    <source>
      <title type="text">US LHC Blog</title>
      <subtitle type="text">US LHC Blogs</subtitle>
      <updated>2009-11-06T16:48:23+00:00</updated>
      <generator uri="http://wordpress.org/" version="2.8.4">WordPress</generator>
      <link href="http://blogs.uslhc.us/" rel="alternate" type="text/html"/>
      <id>http://blogs.uslhc.us/?feed=atom</id>
      <link href="http://blogs.uslhc.us/?feed=atom" rel="self" type="application/atom+xml"/>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://terrytao.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>Terence Tao</name>
						
      <uri>http://www.math.ucla.edu/~tao</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Displaying maths online, II</div>
    </title>
		
    <link href="http://terrytao.wordpress.com/2009/11/04/displaying-maths-online-ii/" rel="alternate" type="text/html"/>
		
    <id>http://terrytao.wordpress.com/?p=3068</id>
		
    <updated>2009-11-04T22:56:12+00:00</updated>
		
    <published>2009-11-04T22:52:09+00:00</published>
		
    <category term="non-technical" scheme="http://terrytao.wordpress.com/"/>
    <category term="question" scheme="http://terrytao.wordpress.com/"/>
    <category term="html" scheme="http://terrytao.wordpress.com/"/>
    <category term="mathematical formatting" scheme="http://terrytao.wordpress.com/"/>
    <category term="MathML" scheme="http://terrytao.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">As the previous discussion on displaying mathematics on the web has become quite lengthy, I am opening a fresh post to continue the topic.  I’m leaving the previous thread open for those who wish to respond directly to some specific comments in that thread, but otherwise it would be preferable to start afresh on this [...]<img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=3068&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://terrytao.wordpress.com/2009/11/04/displaying-maths-online-ii/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>As the previous discussion on <a href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/">displaying mathematics on the web</a> has become quite lengthy, I am opening a fresh post to continue the topic.  I’m leaving the previous thread open for those who wish to respond directly to some specific comments in that thread, but otherwise it would be preferable to start afresh on this thread to make it easier to follow the discussion.</p>
<p>It’s not easy to summarise the discussion so far, but the comments have identified several existing formats for displaying (and marking up) mathematics on the web (<a href="http://en.wikipedia.org/wiki/MathML">mathML</a>, <a href="http://www.math.union.edu/~dpvc/jsMath/">jsMath</a>, <a href="http://www.mathjax.com/">MathJax</a>, <a href="http://en.wikipedia.org/wiki/OpenMath">OpenMath</a>), as well as a surprisingly large number of tools for converting mathematics into web friendly formats (e.g.  <a href="http://www.latex2html.org/">LaTeX2HTML</a>, <a href="http://math.etsu.edu/LaTeXMathML/">LaTeXMathML</a>, <a href="http://lucatrevisan.wordpress.com/latex-to-wordpress/">LaTeX2WP</a>, <a href="http://www.gottabemobile.com/2008/10/29/windows-7-math-input-panel-screenshots">Windows 7 Math Input</a>, <a href="http://golem.ph.utexas.edu/~distler/blog/itex2MML.html">itex2MML</a>, <a href="http://ritex.rubyforge.org/">Ritex</a>, <a href="http://www.albany.edu/~hammond/gellmu/">Gellmu</a>, <a href="http://www.forkosh.dreamhost.com/source_mathtex.html">mathTeX</a>, <a href="http://wordpress.org/extend/plugins/wp-latex/">WP-LaTeX</a>, <a href="http://www.cse.ohio-state.edu/~gurari/TeX4ht/">TeX4ht</a>, <a href="http://www.blahtex.org/">blahtex</a>, <a href="http://plastex.sourceforge.net/">plastex</a>, <a href="http://hutchinson.belmont.ma.us/tth/">TtH</a>, <a href="http://www.dessci.com/webmath/webeq/">WebEQ</a>, <a href="http://www.integretechpub.com/techexplorer/">techexplorer</a>, etc.).  Some of the formats are not widely supported by current software, and by current browsers in particular, but it seems that the situation will improve with the next generation of these browsers.</p>
<p>It seems that the tools that already exist are enough to improvise a passable way of displaying mathematics in various formats online, though there are still significant issues with accessibility, browser support, and ease of use.  Even if all these issues are resolved, though, I still feel that something is still missing.    Currently, if I want to transfer some mathematical content from one location to another (e.g. from a LaTeX file to a blog, or from a wiki to a PDF, or from email to an online document, or whatever), or to input some new piece of mathematics, I have to think about exactly what format I need for the task at hand, and what conversion tool may be needed.  In contrast, if one looks at non-mathematical content such as text, links, fonts, non-Latin alphabets, colours, tables, images, or even video, the formats here have been standardised, and one can manipulate this type of content in both online and offline formats more or less seamlessly (in principle, at least – there is still room for improvement), without the need for any particularly advanced technical expertise.  It doesn’t look like we’re anywhere near that level currently with regards to mathematical content, though presumably things will improve when a single mathematics presentation standard, such as mathML, becomes universally adopted and supported in browsers, in operating systems, and in other various pieces of auxiliary software.</p>
<p>Anyway, it has been a very interesting and educational discussion for me, and hopefully for others also; I look forward to any further thoughts that readers have on these topics.  (Also, feel free to recapitulate some of the points from the previous thread; the discussion has been far too multifaceted for me to attempt a coherent summary by myself.)</p>
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    </content>
		
    <link href="http://terrytao.wordpress.com/2009/11/04/displaying-maths-online-ii/#comments" rel="replies" type="text/html" thr:count="12"/>
		
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		<thr:total>12</thr:total>
	
    <source>
      <title type="text">What's new</title>
      <subtitle type="text">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <updated>2009-11-07T00:48:46+00:00</updated>
      <generator uri="http://wordpress.com/">WordPress.com</generator>
      <link href="http://terrytao.wordpress.com/" rel="alternate" type="text/html"/>
      <id>http://terrytao.wordpress.com/feed/atom/</id>
      <link href="http://terrytao.wordpress.com/feed/atom/" rel="self" type="application/atom+xml"/>
    </source>
  </entry>

  <entry xmlns:dc="http://purl.org/dc/elements/1.1/" xml:base="http://www.scientificblogging.com">
 
    <title>Learn To Compute Higgs Limits On The Fly</title>
 
    <link href="http://www.scientificblogging.com/quantum_diaries_survivor/learn_compute_higgs_limits_fly" rel="alternate"/>
 
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">I am presently into the second week of my lessons of Subnuclear Physics for the 2nd year of specialization in Physics, and I have just finished a lesson discussing the current searches for the Higgs boson at the Tevatron collider. Since the course has a focus on experimental techniques, I found it useful today to give as an exercise the determination of an order-of-magnitude estimate of cross section limits that the CDF experiments can set on a 160 GeV Higgs boson, with the data so far analyzed. It is an exercise I worked out by heart during my walk to the Physics Department: this should tell you it is not of overpowering difficulty.<br/><br/><br/>
<p><a href="http://www.scientificblogging.com/quantum_diaries_survivor/learn_compute_higgs_limits_fly" target="_blank">read more</a></p></div>
    </summary>
 
    <link href="http://www.scientificblogging.com/quantum_diaries_survivor/learn_compute_higgs_limits_fly#comments" rel="replies" type="text/html"/>
 
    <category term="Physics" scheme="http://www.scientificblogging.com/physics"/>
 
    <published>2009-11-04T21:00:36+00:00</published>
 
    <author>
      <name>dorigo</name>
    </author>
 
    <id>urn:feed-entry-id:61249 at http://www.scientificblogging.com</id>

    <updated>2009-11-04T21:00:36+00:00</updated>
    <source>
      <title>dorigo's blog</title>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor" rel="alternate"/>
      <subtitle>Science 2.0</subtitle>
      <link href="http://www.scientificblogging.com/quantum_diaries_survivor/feed" rel="self"/>
      <id>http://www.scientificblogging.com/quantum_diaries_survivor</id>
    </source>
  </entry>

  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0" xmlns:sy="http://purl.org/rss/1.0/modules/syndication/" xmlns:content="http://purl.org/rss/1.0/modules/content/" xmlns:slash="http://purl.org/rss/1.0/modules/slash/" xmlns:wfw="http://wellformedweb.org/CommentAPI/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:atom="http://www.w3.org/2005/Atom">
		
    <title>Are You a Cognitive Miser?</title>
		
    <link href="http://feedproxy.google.com/~r/CosmicVarianceBlog/~3/rIcd2L7aDpY/" rel="alternate"/>
		
    <link href="http://blogs.discovermagazine.com/cosmicvariance/2009/11/04/are-you-a-cognitive-miser/#comments" rel="replies" type="text/html"/>
		
    <published>2009-11-04T19:14:34+00:00</published>
		
    <author>
      <name>Sean</name>
    </author>
				
    <category term="Humanity"/>

		
    <id>http://blogs.discovermagazine.com/cosmicvariance/?p=3125</id>
		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Jack is looking at Anne, but Anne is looking at George.  Jack is married, but George is not.  Is a married person looking at an unmarried person?
A)  Yes.
B)  No.
C)  Cannot be determined.
This is from this month’s Scientific American — article unfortunately costs money.  It’s about “dysrationalia,” which is what [...]</div>
    </summary>
			
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>Jack is looking at Anne, but Anne is looking at George.  Jack is married, but George is not.  Is a married person looking at an unmarried person?</p>
<blockquote><p>A)  Yes.</p>
<p>B)  No.</p>
<p>C)  Cannot be determined.</p></blockquote>
<p><span id="more-3125"/>This is from this month’s <a href="http://www.scientificamerican.com/sciammind/?contents=2009-11"><em>Scientific American</em></a> — article unfortunately <a href="http://www.scientificamerican.com/article.cfm?id=rational-and-irrational-thought">costs money</a>.  It’s about “dysrationalia,” which is what happens when people with nominally high IQ’s end up thinking irrationally.  A phenomenon I’m sure we’ve all encountered, especially in certain corners of the blogosphere.</p>
<p>And the answer is the first option.  But over 80 percent of people choose the third option.  Here’s the solution: the puzzle doesn’t say whether Anne is married or not, but she either is or she isn’t.  If Anne is married, she’s looking at George, so the answer is “yes”; if she’s unmarried, Jack is looking at her, so the answer is still “yes.”  The underlying reason why smart people get the wrong answer is (according to the article) that they simply don’t take the time to go carefully through all of the possibilities, instead taking the easiest inference.  The patience required to go through all the possibilities doesn’t correlate very well with intelligence.</p>

<p><a href="http://feedads.g.doubleclick.net/~a/wI70xfs7gwHHjj4Kk2ywcMXp8Qo/0/da"><img ismap="true" src="http://feedads.g.doubleclick.net/~a/wI70xfs7gwHHjj4Kk2ywcMXp8Qo/0/di" border="0"/></a><br/>
<a href="http://feedads.g.doubleclick.net/~a/wI70xfs7gwHHjj4Kk2ywcMXp8Qo/1/da"><img ismap="true" src="http://feedads.g.doubleclick.net/~a/wI70xfs7gwHHjj4Kk2ywcMXp8Qo/1/di" border="0"/></a></p><img src="http://feeds.feedburner.com/~r/CosmicVarianceBlog/~4/rIcd2L7aDpY" height="1" width="1"/></div>
    </content>
			<wfw:commentRss>http://blogs.discovermagazine.com/cosmicvariance/2009/11/04/are-you-a-cognitive-miser/feed/</wfw:commentRss>
		<slash:comments>85</slash:comments>
		
    <updated>2009-11-04T19:14:34+00:00</updated>
    <source>
      <title>Cosmic Variance</title>
      <link href="http://blogs.discovermagazine.com/cosmicvariance" rel="alternate"/>
      <subtitle>Random samplings from a universe of ideas.</subtitle>
      <updated>2009-11-06T19:23:45+00:00</updated>
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  </entry>

  <entry xml:lang="en">
    
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Notions of Space</div>
    </title>
    
    <link href="http://golem.ph.utexas.edu/category/2009/11/notions_of_space.html" rel="alternate" type="application/xhtml+xml"/>
    
    <updated>2009-11-04T18:45:16+00:00</updated>
    
    <published>2009-11-04T14:43:14+00:00</published>
    
    <id>tag:golem.ph.utexas.edu,2009:%2Fcategory%2F3.2103</id>
    
    <summary type="text">A survey of Jacob Lurie's "Structured Spaces".</summary>
    
    <author>
      
      <name>urs</name>
      
      <uri>http://www.math.uni-hamburg.de/home/schreiber</uri>
      
      <email>urs.schreiber@math.uni-hamburg.de</email>
    
    </author>
    
    <category term="Math"/>
    
    <content type="xhtml" xml:base="http://golem.ph.utexas.edu/category/2009/11/notions_of_space.html">
      <div xmlns="http://www.w3.org/1999/xhtml">
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>Today is my turn in our <a href="http://golem.ph.utexas.edu/category/2009/09/a_seminar_on_a_survey_of_ellip.html">Seminar on A Survey of Elliptic Cohomology</a>.</p>

<p>I attempted to write a survey of some central ideas in Jacob Lurie’s <a href="http://ncatlab.org/nlab/show/Structured+Spaces">Structured Spaces</a>.</p>

<p>You can find it here: <a href="http://ncatlab.org/nlab/show/A+Survey+of+Elliptic+Cohomology+-+the+derived+moduli+stack+of+derived+elliptic+curves#notions_of_space_4">Notions of Space</a>.</p>
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>You may think of this post also as a continuation of our discussion about <a href="http://golem.ph.utexas.edu/category/2008/01/comparative_smootheology.html">Comparative Smootheology I </a> <a href="http://golem.ph.utexas.edu/category/2008/04/comparative_smootheology_ii.html">II</a> <a href="http://golem.ph.utexas.edu/category/2008/09/comparative_smootheology_iii.html">III</a>.</p>
      </div>
    
    </content>
  
    <source>
      <title>The n-Category Café</title>
      <link href="http://golem.ph.utexas.edu/category/" rel="alternate" type="application/xhtml+xml"/>
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      <updated>2009-11-06T11:57:10+00:00</updated>
      <subtitle>A group blog on math, physics and philosophy</subtitle>
      <id>tag:golem.ph.utexas.edu,2006:nCategoryCafe/3</id>
      <generator uri="http://www.movabletype.org/" version="3.36">Movable Type</generator>
      <icon>http://golem.ph.utexas.edu/category/images/favicon.ico</icon>
      <rights>Copyright (c) 2009, The n-Category Collective</rights>
    </source>
  </entry>

  <entry xmlns:thr="http://purl.org/syndication/thread/1.0" xml:lang="en" xml:base="http://terrytao.wordpress.com/wp-atom.php">
		
    <author>
			
      <name>Terence Tao</name>
						
      <uri>http://www.math.ucla.edu/~tao</uri>
					
    </author>
		
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Displaying mathematics on the Web</div>
    </title>
		
    <link href="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/" rel="alternate" type="text/html"/>
		
    <id>http://terrytao.wordpress.com/?p=3030</id>
		
    <updated>2009-11-04T18:06:24+00:00</updated>
		
    <published>2009-10-29T18:52:31+00:00</published>
		
    <category term="non-technical" scheme="http://terrytao.wordpress.com/"/>
    <category term="question" scheme="http://terrytao.wordpress.com/"/>
    <category term="html" scheme="http://terrytao.wordpress.com/"/>
    <category term="mathematical formatting" scheme="http://terrytao.wordpress.com/"/>
    <category term="MathML" scheme="http://terrytao.wordpress.com/"/>		
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">The various languages and formats that make up modern web pages (HTML, XHTML, CSS, etc.) work wonderfully for most purposes, but there is one place where they are still somewhat clunky, namely in the presentation of mathematical equations and diagrams on web pages.  While web formats do support very simple mathematical typesetting (such as [...]<img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=3030&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div>
    </summary>
		
    <content type="xhtml" xml:base="http://terrytao.wordpress.com/2009/10/29/displaying-mathematics-on-the-web/"><div xmlns="http://www.w3.org/1999/xhtml"><div class="snap_preview"><br/><p>The various languages and formats that make up modern web pages (<a href="http://en.wikipedia.org/wiki/HTML">HTML</a>, <a href="http://en.wikipedia.org/wiki/XHTML">XHTML</a>, <a href="http://en.wikipedia.org/wiki/Cascading_Style_Sheets">CSS</a>, etc.) work wonderfully for most purposes, but there is one place where they are still somewhat clunky, namely in the presentation of mathematical equations and diagrams on web pages.  While web formats do support very simple mathematical typesetting (such as the usage of basic symbols such as π, or superscripts such as <em>x<sup>2</sup></em>), it is difficult to create more sophisticated (and non-ugly) mathematical displays, such as</p>
<p style="text-align:center;"><img class="latex" title="\displaystyle \hbox{det} \begin{pmatrix} 1 &amp; x_1 &amp; \ldots &amp; x_1^{n-1} \\ 1 &amp; x_2 &amp; \ldots &amp; x_2^{n-1} \\ \vdots &amp; \vdots &amp; \ddots &amp; \vdots \\ 1 &amp; x_n &amp; \ldots &amp; x_n^{n-1} \end{pmatrix} = \prod_{1 \leq i &lt; j \leq n} (x_j - x_i) " src="http://s1.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Chbox%7Bdet%7D+%5Cbegin%7Bpmatrix%7D+1+&amp;+x_1+&amp;+%5Cldots+&amp;+x_1%5E%7Bn-1%7D+%5C%5C+1+&amp;+x_2+&amp;+%5Cldots+&amp;+x_2%5E%7Bn-1%7D+%5C%5C+%5Cvdots+&amp;+%5Cvdots+&amp;+%5Cddots+&amp;+%5Cvdots+%5C%5C+1+&amp;+x_n+&amp;+%5Cldots+&amp;+x_n%5E%7Bn-1%7D+%5Cend%7Bpmatrix%7D+=+%5Cprod_%7B1+%5Cleq+i+%3C+j+%5Cleq+n%7D+(x_j+-+x_i)+&amp;bg=ffffff&amp;fg=000000&amp;s=0" alt="\displaystyle \hbox{det} \begin{pmatrix} 1 &amp; x_1 &amp; \ldots &amp; x_1^{n-1} \\ 1 &amp; x_2 &amp; \ldots &amp; x_2^{n-1} \\ \vdots &amp; \vdots &amp; \ddots &amp; \vdots \\ 1 &amp; x_n &amp; \ldots &amp; x_n^{n-1} \end{pmatrix} = \prod_{1 \leq i &lt; j \leq n} (x_j - x_i) "/></p>
<p>without some additional layer of software (in this case, WordPress’s LaTeX renderer).   These type of <em>ad hoc</em> fixes work, up to a point, but several difficulties still remain.  For instance:</p>
<ol>
<li>There is no standardisation with regard to mathematics displays.  For instance, WordPress uses $<span/>latex and $ to indicate a mathematics display, Wikipedia uses &lt;math&gt; and &lt;/math&gt;, the current experimental Google Wave plugins use $$ and $$, and so forth.</li>
<li>Mathematical formulae need to be compiled from a plain text language (much as with LaTeX), rather than edited directly on a visual editor. This is in contrast to other HTML elements, such as <a href="http://en.wikipedia.org/wiki/Hyperlink">links</a>, <strong>boldface</strong>,  <span style="color:#ff0000;">colors</span>, etc.</li>
<li>One cannot easily cut and paste a portion of a web page containing maths displays into another page or file  (although with WordPress’s format, things are not so bad as the raw LaTeX code will be captured as plain text).  Again, this is in contrast to other HTML elements, which can be cut and pasted quite easily.</li>
<li>Currently, mathematical displays are usually rendered as static images and thus cannot be easily edited without recompiling the source code for that display.  A related issue is that the images do not automatically resize when the browser scale changes; also, in some cases they do not blend well with the background colour scheme for the page.</li>
<li>It is difficult to take an extended portion of LaTeX and convert it into a web page or vice versa, although tools such as Luca Trevisan’s <a href="http://lucatrevisan.wordpress.com/latex-to-wordpress/">LaTeX to WordPress converter</a> achieve a heroic (and very useful) level of partial success in this regard.</li>
</ol>
<p>There are a number of extensions to the existing web languages that have been proposed to address some of these difficulties, the most well known of which is probably <a href="http://www.w3.org/Math/">MathML</a>, which is used for instance in <a href="http://golem.ph.utexas.edu/category/" title="A group blog on math, physics and philosophy">the n-Category Café</a>.  So far, though, adoption of the MathML standard (and development of editors and other tools to take advantage of this standard) seems to not be too widespread at present.</p>
<p>I’d like to open a discussion, then, about what kinds of changes to the current web standards could help facilitate the easier use of mathematical displays on web pages.  (I’m indirectly in contact with some people involved in these standards, so if some interesting discussions arise here, I can try to pass them on.)</p>
Posted in non-technical, question Tagged: html, mathematical formatting, MathML <a href="http://feeds.wordpress.com/1.0/gocomments/terrytao.wordpress.com/3030/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/comments/terrytao.wordpress.com/3030/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godelicious/terrytao.wordpress.com/3030/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/delicious/terrytao.wordpress.com/3030/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/gostumble/terrytao.wordpress.com/3030/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/stumble/terrytao.wordpress.com/3030/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/godigg/terrytao.wordpress.com/3030/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/digg/terrytao.wordpress.com/3030/" border="0" alt=""/></a> <a href="http://feeds.wordpress.com/1.0/goreddit/terrytao.wordpress.com/3030/" rel="nofollow"><img src="http://feeds.wordpress.com/1.0/reddit/terrytao.wordpress.com/3030/" border="0" alt=""/></a> <img src="http://stats.wordpress.com/b.gif?host=terrytao.wordpress.com&amp;blog=817149&amp;post=3030&amp;subd=terrytao&amp;ref=&amp;feed=1" border="0" alt=""/></div></div>
    </content>
		
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		<thr:total>99</thr:total>
	
    <source>
      <title type="text">What's new</title>
      <subtitle type="text">Updates on my research and expository papers, discussion of open problems, and other maths-related topics.  By Terence Tao</subtitle>
      <updated>2009-11-07T00:48:46+00:00</updated>
      <generator uri="http://wordpress.com/">WordPress.com</generator>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-13869903.post-4593928741038440740</id>
    <published>2009-11-04T11:44:00-06:00</published>
    <updated>2009-11-04T11:44:46-06:00</updated>
    <title type="text">3He</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><span style="font-size: 85%;"><span style="font-family: Verdana,sans-serif;">The lighter helium isotope, <sup>3</sup>He, is not something that most people have ever heard of.  <sup>3</sup>He is one neutron shy of the typical helium atom, and is present at a level of around 13 atoms per 10 million atoms of regular helium.  Every now and then there is some discussion out there in the sci-fi/futurist part of the world that we should mine the moon for <sup>3</sup>He as a potential fuel for fusion reactors.  However, it turns out that <sup>3</sup>He has uses that are much more down to earth.  </span></span><br/><br/><span style="font-size: 85%;"><span style="font-family: Verdana,sans-serif;">For example, in its pure form it can be used as the working fluid in an evaporative refrigerator.  Just as you cool off your tea by blowing across the top and allowing the most energetic water molecules to be carried away, it is possible to cool liquid helium by pumping away the gas above it.  In the case of regular <sup>4</sup>He, the lowest temperature that you can reach this way ends up being about 1.1 K.  (Remember, helium is special in that at low pressures in bulk it remains a liquid all the way down as far as you care to go.)  This limit happens because the vapor pressure of <sup>4</sup>He drops exponentially at very low temperatures - it doesn't matter how big a vacuum pump you have; you simply can't pull any more gas molecules away.  In contrast, <sup>3</sup>He is lighter, as well as being a fermion (and thus obeying different quantum statistics than its heavier sibling).  This difference in properties means that it can get down to more like 0.26 K before its vapor pressure is so low that further pumping is useless.  (You don't throw away the pumped <sup>3</sup>He.  You recycle it.)  This is the principle behind the <sup>3</sup>He refrigerator.<br/></span></span><br/><br/><span style="font-size: 85%;"><span style="font-family: Verdana,sans-serif;">You can do even better than that.  If you cool a mixture of <sup>3</sup>He and <sup>4</sup>He down well below 1 K, it will spontaneously separate into a <sup>3</sup>He-rich phase (the concentrated phase, nearly pure), and a dilute phase of 6% <sup>3</sup>He dissolved in 94% <sup>4</sup>He.  At these temperatures the <sup>4</sup>He is a superfluid, meaning that in many ways it acts like vacuum as far as the <sup>3</sup>He atoms are concerned.  If you pump away the (nearly pure <sup>3</sup>He) gas above the dilute phase, more <sup>3</sup>He atoms are pulled out of the concentrated phase and into the dilute phase to maintain the 6% solubility.  This lets you evaporatively cool the concentrated phase much further, all the way down to milliKelvin temperatures.  (The trick is to run this in closed-cycle, so that the <sup>3</sup>He atoms eventually end up back in the concentrated phase.)  This is the principle behind the dilution refrigerator, or "dil fridge".</span></span><br/><br/><span style="font-size: 85%;"><span style="font-family: Verdana,sans-serif;">Unfortunately, right now there is a <i>major</i> shortage of <sup>3</sup>He.  Its price has shot up by something like a factor of 20 in the last year, and it's hard to get any <i>at all</i>.  This is a huge problem for a large number of (mostly) condensed matter physicists, as reported in the October issue of <a href="http://dx.doi.org/10.1063/1.3248465">Physics Today</a> (reprinted here (<a href="http://www.eas.slu.edu/People/DJCrossley/energy/articles/nuclear/helium3_shortfall.pdf">pdf</a>)).  The reasons are complicated, but the proximate causes are an increase in demand (it's great for neutron detectors, which are handy if you're looking for nuclear weapons) and a decrease in supply (it comes from decay of tritium, mostly from triggers for nuclear warheads).  There are ways to fix this issue, but it will take time and cost money.  In the meantime, my sympathies go out to experimentalists who have spent their startups on fridges that they can't get running.</span></span><div class="blogger-post-footer"><img src="https://blogger.googleusercontent.com/tracker/13869903-4593928741038440740?l=nanoscale.blogspot.com" height="1" width="1"/></div></div>
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    <author>
      <name>Doug Natelson</name>
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      <title type="text">nanoscale views</title>
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  <entry xml:lang="en">
    
    <title type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Who Discovered the Icosahedron?</div>
    </title>
    
    <link href="http://golem.ph.utexas.edu/category/2009/11/who_discovered_the_icosahedron.html" rel="alternate" type="application/xhtml+xml"/>
    
    <updated>2009-11-04T17:18:07+00:00</updated>
    
    <published>2009-11-04T17:02:49+00:00</published>
    
    <id>tag:golem.ph.utexas.edu,2009:%2Fcategory%2F3.2104</id>
    
    <summary type="text">Was it Theaetetus or the Scots?</summary>
    
    <author>
      
      <name>john</name>
      
      <uri>http://math.ucr.edu/home/baez/</uri>
      
      <email>baez@math.ucr.edu</email>
    
    </author>
    
    <category term="Geometry"/>
    
    <content type="xhtml" xml:base="http://golem.ph.utexas.edu/category/2009/11/who_discovered_the_icosahedron.html">
      <div xmlns="http://www.w3.org/1999/xhtml">
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>This weekend we’re having a <a href="http://www.ams.org/amsmtgs/2163_program.html">meeting of the American Mathematical Society</a> here at Riverside.  Julie Bergner and I are running a special session on <a href="http://golem.ph.utexas.edu/category/2009/09/homotopy_theory_and_higher_alg.html">Homotopy Theory and Higher Algebraic Structures</a>, and there will also be two special sessions on knot theory, one run by Alissa Crans and Sam Nelson.  It should be fun!  And it’s starting already: Khovanov will be giving a colloquium talk today.  </p>
<div><a href="http://golem.ph.utexas.edu/~distler/blog/mathml.html"><img class="mathlogo" title="MathML-enabled post (click for details)." src="http://golem.ph.utexas.edu/~distler/blog/images/MathML.png" alt="MathML-enabled post (click for more details)."/></a></div>
<p>But I’m giving a talk in another session — the session on <a href="http://www.ams.org/amsmtgs/2163_program_ss4.html#title">History and Philosophy of Mathematics</a>, run by Shawnee McMurran and James J. Tattersall.  Shawnee was a grad student here at UCR back when I first arrived.</p>

<p>My talk is not very profound or professional, but I hope it’s at least fun:</p>

<ul>
<li>
John Baez, <a href="http://math.ucr.edu/home/baez/icosahedron/">Who Discovered the Icosahedron?</a>
</li>
</ul>

<p>It’s designed to look best in full screen mode, at least on my small laptop.</p>

<p>As usual, comments and corrections are eagerly awaited!  I hope to keep delving into these issues as the years go by.  I’m already trying to recruit my Scottish friends to investigate the mysterious stone balls at the <a href="http://www.nms.ac.uk/our_museums/national_museum.aspx">National Museum of Scotland</a> in Edinburgh and the <a href="http://clyde-valley.com/Glasgow/kelvingr.htm">Glasgow Art Gallery and Museum</a>.  And I’m going to find out more about Scholium 1 in Book XIII of Euclid’s <i>Elements</i>.</p>
      </div>
    
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    <source>
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      <updated>2009-11-06T11:57:10+00:00</updated>
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  <entry xmlns:georss="http://www.georss.org/georss" xmlns:openSearch="http://a9.com/-/spec/opensearchrss/1.0/">
    <id>tag:blogger.com,1999:blog-22973357.post-3038674140160061018</id>
    <published>2009-11-04T10:15:00-05:00</published>
    <updated>2009-11-04T10:19:36-05:00</updated>
    <title type="text">The Waterloo Institute for Complexity &amp; Innovation</title>
    <content type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml">Waterloo, Ontario, <a href="http://www.intelligentwaterloo.com/en/">once named the Top Intelligent Community of the world</a>, home of the <a href="http://perimeterinstitute.ca/">Perimeter Institute for Theoretical Physics</a> and the <strike>Center</strike> <a href="http://www.cigionline.org/">Centre for International Governance Innovation</a>, makes another shot at solving all problems of mankind: The <a href="http://www.sig.uwaterloo.ca/WICI.html">Waterloo Institute for Complexity &amp; Innovation</a> (WICI).<br/><br/>Presently in its planning phase, the WICI's is an interdisciplinary effort, located at the University of Waterloo. According to the website, its goals are to<br/><ul><li> Develop a common, transdisciplinary language and methodology and an integrated, coherent theory for the study and pedagogy of complex adaptive systems; and,</li><br/><li> Apply these tools to stimulate rapid and beneficial innovation that will increase the resilience of complex adaptive systems worldwide – including social, political, economic, and ecological systems – that are currently under threat.</li></ul><br/>So far, the activities consist of <a href="http://www.sig.uwaterloo.ca/WICI_Seminars.html">a seminar series</a>, which, innovation etc, has the talks recorded and uploaded to Google videos. You find there, among others, Stuart Kauffman speaking on <a href="http://video.google.com/videoplay?docid=792139949574688521&amp;ei=dIgQSYmkDIXE-wGditChCg&amp;q=stuart+Kauffman+economics&amp;hl=en#"><i>"The Evolution of Economic Wealth and Innovation,"</i></a> Thomas Homer-Dixon on <a href="http://video.google.ca/videoplay?docid=1176509918001434074#"><i>"Ingenuity Theory: Adaptation Failure and Societal Crisis,"</i></a> and if you have been waiting for a summary of <a href="http://arxiv.org/abs/0902.4274v1">Lee Smolin's last year's q-fin paper</a>, here's his talk on <a href="http://video.google.ca/videoplay?docid=-6937900269058875401#"><i>"Symmetries in Economic Models and their Consequences"</i></a>.<div><br/></div><div>Unfortunately, they have forgotten about another complex system currently under threat, the academic system. Which plays a central role for <a href="http://backreaction.blogspot.com/2008/10/lightcone-institute.html">my virtual institute</a>, and that for a good reason.</div><div><br/></div><div><a href="http://www.intelligentcommunity.org/index.php?src=gendocs&amp;ref=Top7_by_Year&amp;category=Events">The top intelligent community of the year 2009 btw is Stockholm</a>.</div><div class="blogger-post-footer">"You do not really understand something unless you can explain it to your grandmother." ~ Albert Einstein<img src="https://blogger.googleusercontent.com/tracker/22973357-3038674140160061018?l=backreaction.blogspot.com" height="1" width="1"/></div></div>
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      <name>Bee</name>
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      <updated>2009-11-07T19:44:53-05:00</updated>
      <title type="text">Backreaction</title>
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  <entry xmlns:feedburner="http://rssnamespace.org/feedburner/ext/1.0">
         
    <title>A Question About Frost</title>
          
    <summary type="xhtml"><div xmlns="http://www.w3.org/1999/xhtml"><p>It's November now, which means we're edging into winter, and my morning ritual has been expanded to include scraping the frost off the cars when I get back from walking the dog. I've had to do this half a dozen times already, and I've noticed a puzzling pattern.</p>

<p>Our driveway is aligned almost exactly east-west, with the cars facing east when they're pulled in at night. This means that one set of side windows faces north, and the other south. And here's the thing that puzzles me: the frost layer is significantly thicker on the south-facing side windows than on the north-facing side windows. I have to actively scrape the south-facing windows, but the north-facing ones I can just about wipe off with my hand.</p>

<p>I have no idea why that should be the case (the cars are symmetric under reflection about the axis, after all), but it's very repeatable. But then, I'm not all that clear on the science of frost formation in the first place. I'm sure that some of my wise and worldly readers know more about weather-related matters than I do, though, so maybe one of you can explain it to me. Why <em>do</em> the south-facing car windows collect more frost than the north-facing car windows?</p>
 <a href="http://scienceblogs.com/principles/2009/11/a_question_about_frost.php#commentsArea">Read the comments on this post...</a><img src="http://feeds.feedburner.com/~r/scienceblogs/uncertainprinciples/~4/n0bekXJfil8" height="1" width="1"/></div>
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    <published>2009-11-04T09:58:36-05:00</published>
      
    <updated>2009-11-04T09:58:36-05:00</updated>
    <source>
      <title>Uncertain Principles</title>
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      <updated>2009-11-07T11:21:56-05:00</updated>
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