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December 10, 2007

This Week’s Finds in Mathematical Physics (Week 259)

Posted by John Baez

In week259 of This Week’s Finds, hear what may be hiding in the Egg Nebula:



Then, learn how a mathematical phantom called the ‘field with one element’ is gradually becoming real. It may explain the deep inner meaning of q-deformation, and the 3-dimensional aspect of the integers!

Ever wonder what a ‘scheme’ is? You’ll learn that too.

Posted at December 10, 2007 12:17 AM UTC

TrackBack URL for this Entry:   http://golem.ph.utexas.edu/cgi-bin/MT-3.0/dxy-tb.fcgi/1531

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Nebulae and Meadows; Re: This Week’s Finds in Mathematical Physics (Week 259)

That was great!

The astrophotography, vision of the hot dusty electron-atmospheric future (don’t bother Al Gore, though, as he’s busy today in Oslo), and Field ponderings.

Anything to this?:

arXiv:0712.0917
Title: Some properties of finite meadows
Authors: Inge Bethke, Piet Rodenburg
Comments: 8 pages, 1 table
Subjects: Symbolic Computation (cs.SC)

Posted by: Jonathan Vos Post on December 10, 2007 1:37 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

You say

Durov’s framework generalizes Deitmar’s!

even though they disagree about vector spaces over F 1 .

For Deitmar

A “vector space over F 1 ” is just a … plain old set,

while for Durov it’s a pointed set. This must surely be an indication of a big difference which will show when they come to do algebraic geometry over F 1 .

Posted by: David Corfield on December 10, 2007 2:20 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Durov’s framework has a generalized ring whose modules are sets, and one whose modules are pointed sets. So, his framework generalizes Deitmar’s.

You make it sound like they disagree over the definition of ‘vector spaces over F 1 ’, but I don’t think Deitmar even talks about ‘vector spaces over F 1 ’. I wrote:

A ‘vector space over F 1 ’ is just a set on which this monoid acts via multiplication… but that amounts to just a plain old set. The ‘dimension of such a ‘vector space’ is just its cardinality.

but you shouldn’t really blame Deitmar for this. I was just trying to stretch his idea

ringsmonoids

to include

modulesofringsactionsofmonoids

and noting that a module over the 1-element monoid (which is what he calls F 1 ) is nothing but a set.

But you see, he’s an algebraic geometer in a hurry. He’s not interested in vector spaces over F 1 — he’s interested in going straight to schemes defined over F 1 . And, I think his example of the ‘projective line over F 1 ’ matches what Durov says that should be: a 2-point set.

To be blunt, I think Durov’s approach is more systematic and general. So, he talks a bit about both generalized rings: the one whose modules are pointed sets, and the one whose modules are sets. It’s probably good for algebraic geometers to deploy both, since the obvious ‘throw out the basepoint’ functor

[pointedsets][sets]

is just what algebraic geometers would call ‘projectivization’ — turning a ‘vector space’ for Durov’s F 1 into a ‘projective space’. It just so happens that a ‘projective space’ for Durov’s F 1 is a module of some other generalized ring… the one whose modules are just sets.

There’s also the obvious ‘keep the basepoint’ functor

[pointedsets][sets]

and the obvious ‘throw in a basepoint’ functor

[sets][pointedsets]

but I think it’s good to have a total of 3 functors around. After all, whenever we have a homomorphism of (generalized) rings f:RS we get the obvious pullback

f *:SModRMod

but also, one might hope, both a left and right adjoint to this — what Lawvere would call ‘free’ and ‘fascist’ functors.

In short, there’s room for plenty of fun and confusion here, but it should all make nice sense in the end. If I seem a bit casual about pointed sets versus sets, it’s because of my faith in that.

Posted by: John Baez on December 10, 2007 9:58 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Is there any reason to think more about my observation concerning the subobject classifier of the 2-topos of categories as scalar restriction of F 1 -modules to F -modules, i.e., pointed sets to sets?

Perhaps it’s more truthfully described as a discrete opfibration classifier, as Weber does. He also notes Lawvere’s idea: the category of sets is a generalised object of truth values.

Posted by: David Corfield on December 11, 2007 9:24 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

but something else, something more mysterious…

I am wondering: rings have a nice neat categorical description as categories enriched over abelian groups.

One problem with fields seems to be that they lack an equally neat characterization. This is a nuisance not only when looking for the field with one element, but also, for instance, when one tries to categorify the notion of a field.

Maybe somebody should think harder about what fields really are.

(And maybe somebody is already doing that. But then maybe somebody should think harder about what the first somebody is really doing. If you know what I mean.)

Posted by: Urs Schreiber on December 10, 2007 5:58 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

What if one tried to categorify a generalized field? Perhaps after doing the same for a generalized ring.

What do we know about algebraic 2-theories?

No doubt TWF won’t let us down. Ah yes, Week 170. So Noson Yanofsky gives us a definition of algebraic 2-theories in Coherence, Homotopy and 2-Theories.

What kind of 2-theory corresponds to a commutative theory? And what to the terminal theory?

Posted by: David Corfield on December 10, 2007 6:37 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

David wrote:

What if one tried to categorify a generalized field?

One shouldn’t — ones brain might explode!

Seriously, it’s an interesting idea, and it might serve to unify a bunch of work on ‘categories’ and ‘2-vector spaces’, just as generalized fields one notch down unify a bunch of work on ‘sets’ and ‘vector spaces’.

But, one notch down there’s a lot more evidence staring us in the face, making it incredibly obvious that we should unify a bunch of work about ‘sets’ and ‘vector spaces’. I’m not talking about the overall family resemblance of Set and Vect F for any field F, which existing category theory understands fairly well, and which we already know how to categorify to some extent. I’m talking about the much more detailed, exciting and mysterious sense in which Vect F q converges to Set as q1 .

If one found something like this one notch up, there’d really be a good reason to get excited about categorified generalized fields. Right now the idea seems a bit too ethereal to grab my interest.

(Right now I’m having fun trying to learn some basic algebraic geometry while simultaneously learning the far-out generalizations proposed by Durov, especially algebraic geometry over F 1 and algebra geometry over , which is all about ‘the real prime’ and ‘Arakelov geometry’.)

Posted by: John Baez on December 12, 2007 7:04 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

If one found something like this one notch up…

Hmmm. Shouldn’t we expect that the q1 limit of the 2-category of Vect F q-modules is the 2-category of (pointed sets)-modules?

I know Urs has talked about things like Vect-mod. But what is known? So we have Kapranov-Voevodsky 2-vector spaces as finitely generated free Vect-modules. And then further entities like Bim(Vect).

Is it even known what Set-mod looks like?

Is there an (abelian) algebraic 2-theory resembling Set Pointed set, which sends categories to pointed categories?

Hmmm, once more. Weren’t your lectures teeming with pointed categories?

Posted by: David Corfield on December 12, 2007 9:36 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Lots of good questions, David! Please help me out and answer some.

Posted by: John Baez on December 13, 2007 12:14 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

The odd thing about participating in this enterprise as an amateur is that one has much less sense of what ought to be already known. (Now which mathematician said something to the effect that what he could bring to the study of a field was a reliable sense of what ought to be already known? Oh yes, Ulam quoted on p. 107 of my book.)

If John Gray wrote about algebraic 2-theories in 1974, then surely there’s a whole heap of collected wisdom on them out there somewhere. Not that working things out for yourself should be avoided.

There ought to be a 2-adjunction between categories and pointed categories where the left adjoint merely adds a pointed object. So perhaps pointed categories are the 2-vector spaces for some generalized 2-ring.

On the other hand there are (Pointed Set)-modules, including those such as (PointedSet) n.

With FinSet-modules, we want a map FinSetEnd(C), for some category C. Is it that you couldn’t expect an equivalent of ’s module /2 ?

Maybe the groupoid FinSet 0 could have torsion modules.

Posted by: David Corfield on December 13, 2007 10:44 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

David wrote:

If John Gray wrote about algebraic 2-theories in 1974, then surely there’s a whole heap of collected wisdom on them out there somewhere.

Probably not a ‘whole heap’ — not in published form, anyway. I’m sure if you asked Martin Hyland he could tell you everything you wanted to know about algebraic 2-theories… but it’d mostly be in his head, not in papers.

You have to remember, John Gray was way ahead of his time when it came to n-categories. Also, category theory is a strongly deprecated field, especially in the USA — so not many people work on it, and not every idea gets followed up.

I bet you’ll find more published work on ‘2-monads’ or ‘pseudomonads’ than ‘2-theories’. That’s another way to skin the same cat. But again, the number of people actually working on these is darn small: Street, Hyland, Lack, Powers, a few more… mainly the usual suspects.

There may be a few people who have thought about ‘2-operads’, too.

Anyway, I should answer some of your questions, but I gotta go give a final exam!

Posted by: John Baez on December 13, 2007 6:55 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

I see the point that we need enough pressure to build up to prompt us to do the work.

one notch down there’s a lot more evidence staring us in the face, making it incredibly obvious that we should unify a bunch of work about ‘sets’ and ‘vector spaces’.

Then again perhaps this particularly way of pushing for a unification of ‘categories’ and ‘2-vector spaces’ might promote the generation of a similar bunch of work.

One of the things we lack is a parallel to the nice formula for the size of GL(n,F q) tending to that of S n, as q1 .

This is all very close to our 2-Klein geometry work.

As Urs has told us, your and Alissa’s 2-vector spaces are categories internal to Vect K. So we might expect that BC 2-vector spaces over F q will tend to categories internal to PointedSet as q1 .

Now what’s one of those? A pointed category (C,*) with id * a pointed arrow?

How about this for a profound fact – a category is a BC 2-vector space over the field without elements.

Posted by: David Corfield on December 14, 2007 9:16 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Haven’t thought about 2-operads;, but what sort of thoughts are worth pursuing? There’s a whole bunch of `exercises’ one could perform - just using our experience with other 2-things.

Posted by: jim stasheff on December 14, 2007 1:44 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Jim writes:

Haven’t thought about 2-operads; but what sort of thoughts are worth pursuing?

It’s not instantly clear, so it might be worth noting the work that’s been done so far:

Batanin has a whole theory of ω-operads, such that his weak ω-categories are algebras of a certain ‘initial contractible’ ω-operad. There’s a marvelous relation to associahedra and their generalizations. I see David had some questions about this that never got answered… I know some answers.

Posted by: John Baez on December 14, 2007 8:47 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Maybe somebody should think harder about what fields really are.

(And maybe somebody is already doing that. But then maybe somebody should think harder about what the first somebody is really doing.)

Lol, this is brilliant!

Someone’s thinking my Lord, come to him,

Someone’s thinking my Lord, come to him,

Someone’s thinking my Lord, come to him,

Oh lord, kumbaya.

Posted by: Bruce Bartlett on December 10, 2007 9:16 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Bruce wrote:

Someone’s thinking my Lord, come to him,

Oh lord, kumbaya.

Interesting, a quote from Joan Baez here! (according to Wikip.) ;-)

Posted by: Urs Schreiber on December 11, 2007 6:08 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Indeed. You can’t keep a good Baez down.

Posted by: Bruce Bartlett on December 12, 2007 12:46 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Urs wrote:

I am wondering: rings have a nice neat categorical description as categories enriched over abelian groups.

One problem with fields seems to be that they lack an equally neat characterization. This is a nuisance not only when looking for the field with one element, but also, for instance, when one tries to categorify the notion of a field.

Maybe somebody should think harder about what fields really are.

Indeed!

In theory, algebraic geometers are the ones who should do this. Early on in algebraic geometry, the idea arose that the same equation, say

x n+y n=z n,

could have drastically different solutions depending on what field the variables (here x,y,z) lived in. This eventually led to the idea of a ‘scheme’ as something that could have ‘k-points’ for any field k.

But in the process, people realized that fields are in many ways less convenient to work with than commutative rings. Grothendieck can probably take a lot of credit for this. It’s a great example of a principle I attribue to him: ‘it’s better to work with a nice category containing some nasty objects, than a nasty category containing only nice objects’. While commutative rings can be ‘nasty’ compared to fields (e.g. they can contain nilpotents, which were traditionally considered ‘nasty’), the category of commutative rings is very ‘nice’ compared to the category of fields (basically because commutative rings involve only everywhere defined operations satisfying equational laws, so they’re models of an algebraic theory).

So, Grothendieck’s later approach to schemes (not the textbook one) is based on the idea that a scheme is nothing but a gadget that has ‘R-points’ for any commutative ring R. In this later definition, a scheme is just a functor

F:CommRingSet

assigning to each commutative ring R a set of ‘R-points’, F(R). In particular, any commutative ring S gives a scheme

hom(S,):CommRingSet

and these are what we call ‘affine schemes’.

This is very slick and beautiful, and I explained some of its virtues in week205 — for example, it gives a nice way of understanding topics in number theory like ‘inert primes’.

But, after posting week205 I got a reply from a well-known number theorist saying this stuff was useless.

I wasn’t convinced. But, I get the impression that many algebraic geometers and number theorists are still recovering from Grothendieck. They don’t really want further drastic reformulations of the subject, of the sort that might follow from pondering questions like ‘what are fields, really’.

I was reminded of this by something James wrote:

I think it is fair to say that the weirdness in scheme theory around closed points vs all points and maximal ideals vs prime ideals is really an artifact of scheme theory relying on point-set topology rather than topos theory. And things are this way because Grothendieck invented toposes after he invented schemes, and no one since then has bothered/wanted to rewrite the foundations in terms of topos theory.

and Tom’s reply:

That’s really bizarre! You’d think that algebraic geometry would be important enough that someone would have done it. Maybe it’s one of those things where people are afraid to rewrite foundations because they think people are too set in their ways. Or maybe people have tried to do it, but got the reaction ‘why are you telling me things I already know, just in some obscure language?’

It’s certainly forgivable to want to take a break from revamping the foundations of a subject, but I think eventually enough difficulties will build up to force algebraic geometry to further heights of abstraction. Some problems can only be solved that way.

In particular, Durov’s work shows there are lots of advantages of thinking of ‘commutative rings’ as a special case of ‘commutative algebraic theories’ — theories with a bunch of n-ary operations that all commute. We need this to understand what sort of thing the ‘field with one element’ is.

But, we may not need to decide which commutative algebraic theories deserve to be called ‘fields’! You can see Durov struggling with this question, but I’m not sure how important the answer is.

Posted by: John Baez on December 10, 2007 10:41 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

John wrote:
‘it’s better to work with a nice category containing some nasty objects, than a nasty category containing only nice objects’.

Some such generalisations of schemes:
Stacks and Artins algebraic spaces (or Knutsons book)

Best,
Thomas

Posted by: Thomas Riepe on December 14, 2007 8:14 AM | Permalink | Reply to this

Phield Theory: Phanton Fields; Re: This Week’s Finds in Mathematical Physics (Week 259)

How general should generalizations be, beyond the phantom Field with 1 element?

Should the general Phield theory include the phantom field with 0 elements? The phantom field with -1 elements? The phantom field with 1/2 elements? The phantom field with pi elements? The phantom field with i elements?

I have discussed with Michael Aschbacher to what extent the sporadic simple groups are examples of something deeper, which happen to be groups, and whose distribution reflect phantom sporadic groups that don’t quite make it into grouphood.

It seems to me that your periodic table of higher-order Lie algebras may be related.

Posted by: Jonathan Vos Post on December 10, 2007 7:06 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Typo: it’s Nikolai Durov, not Anton Durov.

Posted by: jon on December 10, 2007 8:31 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Whoops — thanks for catching that! I’ll fix it.

Posted by: John Baez on December 10, 2007 10:00 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

“They keys are, like, so close to one another”

;)

Posted by: Mikael Vejdemo Johansson on December 10, 2007 10:16 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Great, now I’ve gotta keep straight “ghosts” and “phantoms”. The fact that Gavin Wraith wrote up the article doesn’t help.

When we get to liches I quit.

Posted by: John Armstrong on December 10, 2007 10:05 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

That cracked me up while reading it as well.

Hmmmm… If we do have liches, then I’d like to dub the maximal lich a lich lord. At last! Mathematics that sounds like an AD&D-game!

Posted by: Mikael Vejdemo Johansson on December 10, 2007 10:17 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

If we do have liches, then I’d like to dub the maximal lich a lich lord. At last! Mathematics that sounds like an AD&D-game!

Would it come with a no-ghost theorem for attacking the Lich lattice?

(Sorry. :-P)

Posted by: Todd Trimble on December 11, 2007 12:20 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

If you like Halloween-themed mathematical concepts, you’ll love Dan Christensen’s paper on phantoms, ghosts, and skeleta. Too bad Gavin Wraith didn’t write it.

Posted by: John Baez on December 11, 2007 12:57 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

I was trying to figure out why Durov likes commutative generalized rings so much better than generalized rings in general. Of course this should be related to why algebraic geometers like commutative rings better than rings in general.

And, this morning while I was waiting for my pupils to dilate at the optometrist’s, I came up with some ideas. I’m hoping Tom Leinster or Todd Trimble or someone could say if these are new or not.

First, let’s stop calling them ‘generalized rings’ and call them what they are: ‘algebraic theories’.

Second, let’s start by seeing how much we can do using operads.

There’s a down-to-earth definition of what it means for an operad to be ‘commutative’. But the main thing this definition accomplishes, I think, is this:

Given an operad O we can talk about its algebras in any symmetric monoidal category C. We get a category of O-algebras in C, which I’ll call Oalg(C).

If O is commutative, all its operations act on any algebra A not just as morphisms

A nA

in C, but as O-algebra homomorphisms!

So, for O commutative, an O-algebra in C automatically becomes an O-algebra in Oalg(C)! We also have a forgetful functor going the other way, so we get an equivalence

Oalg(C)Oalg(Oalg(C))

There’s something very Eckmann–Hiltonesque about this. And in fact it seems to be Eckmann–Hiltonesque in two ways — two ways related by a curious ‘level shift’.

First, consider an operad with only unary operations. This is just a monoid in disguise. Further, the operad is commutative iff the monoid is commutative. We don’t usually talk about ‘algebras’ of a monoid, though — we call them ‘actions’. The above story, restricted to this special case, thus says ‘if M is a commutative monoid, an action of M in C is the same as an action of M in the category of actions of M in C’.

(And, if C=Set, this statement is an ‘if and only if’.)

Second, consider the operad O whose algebras are commutative monoids. This O is a commutative operad! So, we get

Oalg(C)Oalg(Oalg(C))

or in other words, ‘a commutative monoid in C is the same as a commutative monoid in the category of commutative monoids in C’.

Anyway, while all this is cute, I don’t yet see how to use it to give a slick definition of ‘commutative operad’. Or maybe I do: maybe we can say O is commutative if the forgetful functor

Oalg(Oalg(C))Oalg(C)

is an equivalence of categories! Does that seem right?

Also, I don’t see why this makes commutative operads better than general operads as a method of generalizing algebraic geometry. For that, I think I want something more like this:

There’s a tensor product of rings, but for commutative rings this tensor product is more interesting, since it makes CommRing op into a cartesian category. This is a fundamental sense in which affine schemes act like spaces.

There’s also a tensor product of operads. Is this more interesting for commutative operads? Does it make the opposite of the category of commutative operads into a cartesian category?

I thought of some other stuff too, but this is already more than anyone wants to read.

Posted by: John Baez on December 10, 2007 11:13 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Jim Dolan called with a few remarks.

I’d written:

So, for O commutative, an O-algebra in C automatically becomes an O-algebra in Oalg(C)! We also have a forgetful functor going the other way, so we get an equivalence

Oalg(C)Oalg(Oalg(C))

This is correct up to the phrase ‘so we get an equivalence’, which is wrong. For any operad O we have a ‘forgetful’ functor

Oalg(Oalg(C))Oalg(C)

and when O is commutative my argument gives a functor going the other way:

Oalg(C)Oalg(Oalg(C))

but these are not weak inverses of each other!

An abstract way to see this uses the tensor product of operads. This is defined by the property that an O 1 O 2 -algebra in C is the same as an O 1 -algebra in O 2 alg(C), or more precisely:

(O 1 O 2 )alg(C)O 1 alg(O 2 alg(C))

Syntactically, we generate the operad O 1 O 2 by throwing in all the operations of O 1 and all the operations of O 2 , and imposing relations saying that they commute.

If we really had

Oalg(Oalg(C))Oalg(C)

we would have

(OO)alg(C)Oalg(C)

But, it’s easy to find counterexamples, even when O is commutative. Why? Simply because OO is generated by two commuting copies of all the operations in O. And that can be a lot more operations than there are in O.

In fact, the easiest counterexamples arise when our commutative operad O has just unary operations, so that it’s a commutative monoid in disguise.

For example, suppose O is just in disguise, and take C=Set. Then an O-algebra in C is a set X with a function f:XX. An OO-algebra in C is a set X with two commuting functions f,g:XX. So, they’re very different.

So, the following ‘corollary’ of my false claim is also false:

First, consider an operad with only unary operations. This is just a monoid in disguise. Further, the operad is commutative iff the monoid is commutative. We don’t usually talk about ‘algebras’ of a monoid, though — we call them ‘actions’. The above story, restricted to this special case, thus says ‘if M is a commutative monoid, an action of M in C is the same as an action of M in the category of actions of M in C’.

(And, if C=Set, this statement is an ‘if and only if’.)

The rest of what I wrote seems true.

In particular, it seems correct that the tensor product of operads, restricted to commutative operads, is the coproduct of commutative operads. So, the answer to this:

Does it make the opposite of the category of commutative operads into a cartesian category?

seems to be ‘yes’.

Posted by: John Baez on December 11, 2007 12:49 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Jim adds:

by the way, about this business of why the “forgetful” functor from (o tensor o)-algebras to o-algebras isn’t an inverse to the (“co-diagonal”) functor going the other way that exists (precisely?) when o is commutative, it sort of has to do with the fact that there are _two_ forgetful functors; you can forget either the first (“inside”) o-algebra structure or the second (“outside”) one. again, this is the way it generally works; neither of the two projections from xXx to x is inverse to the diagonal x->xXx.

Posted by: John Baez on December 11, 2007 2:53 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

In particular, it seems correct that the tensor product of operads, restricted to commutative operads, is the coproduct of commutative operads.

Right, and I think the mistake that Jim pointed out can be understood in this language:

If O is a commutative operad, then there is a codiagonal map

:OOO

in the category of commutative operads since, as you say, the operadic tensor product becomes the coproduct there. By pulling back, this gives one direction

Oalg(OO)algOalg(Oalg)

of that “equivalence” you were conjecturing. The other direction, a forgetful functor

(OO)algOalg(Oalg)Oalg

can be seen as induced from the unique operad map IO, where I is the initial operad. That is, pulling back along this operad map is the forgetful functor

Oalg(C)Ialg(C)C.

In other words, the forgetful functor direction you were alluding to corresponds to the operad map

OIOi1 OO

which is nothing other than the second coproduct inclusion i 2 :OOO. Now of course i 2 is the identity by the way coproducts work, but the other composite i 2 is generally not the identity.

Are you unhappy with the standard way of defining the notion of commutative operad? If O is a Set-valued operad, we have a composite map

O(m)×O(n)1 ×δO(m)×O(n) mμO(mn)

which we may call α m,n, and another composite map

O(m)×O(n)O(n)×O(m)α n,mO(mn),

and commutativity of O is the condition that these maps agree for all m, n.

One thing that I can imagine might be slightly ‘irritating’ is that we are evidently using the presence of a diagonal map δ to define this notion (i.e., that the objects O(n) are cocommutative comonoids :-) ). Assuming our symmetric monoidal category C has coproducts which are preserved under tensoring, the change of base

SetC

is a strong symmetric monoidal functor which preserves such commutative comonoids, so the notion of commutative operad would cleanly carry over to C under such base change.

Posted by: Todd Trimble on December 11, 2007 3:37 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Pipped by Jim. Curses, foiled again…

Posted by: Todd Trimble on December 11, 2007 3:38 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Pipped?
and Jim = me?

Posted by: jim stasheff on December 11, 2007 1:59 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Jim Stasheff asked:

and Jim = me?

I am pretty sure that the Jim meant was Jim Dolan. Todd was referring , I guess, to this and this forwarded comment from Jim Dolan, which beat his own comment by, let’s see, apparently some 40 minutes or so.

Posted by: Urs Schreiber on December 11, 2007 3:57 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

So what’s a commutative (or do we want some other term, like symmetric?) algebraic 2-theory? Presumably a 2-theory made up of things like n-ary Vect-linear combinations would count.

Posted by: David Corfield on December 11, 2007 9:18 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Though Todd was pipped by Jim, Todd’s post is probably easier to understand, since it’s more detailed. So, it’s all for the best in this best of all possible worlds.

Todd wrote:

Are you unhappy with the standard way of defining the notion of commutative operad?

I was at the time, mainly because it seemed too ‘syntactical’, as opposed to ‘semantic’. I was trying to figure out why Durov prefers to do algebraic geometry with commutative operads (or really, algebraic theories). And, it seemed to me that one of the the main things he does with an operad O is play around with their categories of algebras Oalg(C). (Not having read all of his 568-page time, I’m not sure how true this really is, but anyway, this is one of the main things everyone always does with operads, so I was willing to guess it’s true for him too.) So, I was seeking a characterization of commutative operads solely in terms of their categories of algebras!

And so, I was slowly blundering my way towards a realization that you and Jim had more clearly.

Namely: while Op (the category of operads) has a tensor product, this becomes the coproduct when restricted to CommOp (the category of commutative operads). A tensor product is a coproduct when it has a codiagonal

:OOO

and a unit

!:1 O

satisfying some nice properties. In paarticular, they make O into a commutative monoid in Op. So, Jim also hazarded a speculation that perhaps a commutative operad is the same as a commutative monoid in Op. Is anyone up to figuring this out?

Anyway, in terms of categories of models, our operad being commutative gives us

Δ *:Oalg(C)(OO)alg(C)Oalg(Oalg(C))

as we have been discussing. It also gives us

! *:1 alg(C)Oalg(C)

Hmm. Since the algebras of the terminal operad 1 are just commutative monoids, 1 alg(C) is the category of commutative monoids in C. So, we’re saying any commutative monoid in C becomes an algebra of O in C, which is quite familiar to me — just a turned-around, semantic way of saying 1 is the terminal operad.

Anyway, trying to assemble these observations into something a bit more cogent, I’d like to say that O being commutative makes it a commmutative monoid in Op, so that Oalg(C) gets a kind of ‘cocommutative comonoid’ structure. But, I’m not quite sure how to make that precise, because what symmetric monoidal 2-category is Oalg(C) an object in, exactly?

To be frank, I’m not sure where all this stuff is going. It now seems to me that something else is more important. We’re trying to generalize algebraic geometry. Algebraic geometers are called ‘geometers’ because CommRing op (the category of affine schemes) has many of the features typical of a category of ‘spaces’. For starters, it’s cartesian! But CommRing op lacks some nice features: namely, we can’t always glue together affine schemes to get other affine schemes. So, algebraic geometers embed CommRing op in a larger category, the category of schemes, which has more colimits. (All colimits?)

Now we’re seeing that CommOp is a bit similar to CommRing. In particular, CommOp op — the punster in me wants to call this the category of commutative ‘erads’ — is cartesian, just like the category of affine schemes.

I’d like to know exactly how far the similarity goes.

And then, I’d like to see Deitmar and Durov’s tricks for generalizing the concept of ‘scheme’ as very general tricks, applicable whenever we have a cartesian category with some extra features, and want to be able to from new objects by ‘gluing together’ objects form this cartesian category.

(We could take presheaves on our cartesian category, to get arbitrary colimits, or we could do something weirder, analogous to the textbook definition of ‘scheme’.)

When I’m done, I’ll probably discover that this stuff is already well-known among experts in topos theory. But that’s okay.

Posted by: John Baez on December 11, 2007 7:18 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Namely: while Op (the category of operads) has a tensor product, this becomes the coproduct when restricted to CommOp (the category of commutative operads). A tensor product is a coproduct when it has a codiagonal :OOO and a unit !:1 O satisfying some nice properties. In paarticular, they make O into a commutative monoid in Op. So, Jim also hazarded a speculation that perhaps a commutative operad is the same as a commutative monoid in Op. Is anyone up to figuring this out?

Two things. One, there seems to be a typo, where you have ‘1’ (the terminal operad) instead of ‘I’ (the initial operad). (Later, you do mention 1 again as the operad for commutative monoids; I is the operad for general objects.)

Two, yes to Jim’s surmise, but I think you can also say that a commutative operad is an operad O equipped with just a monoid structure with respect to ; that is, monoids here are automatically commutative. This for approximately the same reason that a commutative group is a group equipped with a monoid structure with respect to ×, and a commutative ring is a ring equipped with a monoid structure with respect to (commutation of operations being built into the definitions of these monoidal products).

Posted by: Todd Trimble on December 11, 2007 9:24 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Thanks for catching the mistakes, Todd — and thanks for confirming Jim’s guess!

As for this thing I wrote…

(We could take presheaves on our cartesian category, to get arbitrary colimits, or we could do something weirder, analogous to the textbook definition of ‘scheme’.)

When I’m done, I’ll probably discover that this stuff is already well-known among experts in topos theory.

… maybe this ‘something weirder’ is just called forming a topos of sheaves on a site — in which case it’s very well-known, and not weird at all.

I don’t know. I guess I need some kindly soul to answer the following two questions:

Every scheme X gives a functor

F:CommRingSet

where F X(R) is the set of ‘R-points’ of X — this being just another name for scheme morphisms Spec(R)X.

Which functors F:CommRingSet come from a schemes in this way?

A functor F:CommRingSet is called a ‘presheaf on CommRing op’. Could there be some Grothendieck topology on CommRing op such that F comes from a scheme iff F is a sheaf with respect to this topology?

If this is true, I bet Deitmar’s ‘schemes over F 1 ’ are really just sheaves on CommMon op with respect to some Grothendieck topology on CommMon op.

And, maybe this is part of a big pattern…

Posted by: John Baez on December 12, 2007 3:12 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Which functors F:CommRingSet come from a scheme in this way?

James said something about this back here. The topology he was referring to (“closure under adjoining quotients by equivalence relations which are covers in your topology”) is the Zariski topology on affine schemes, where covers E αE are covering families by Zariski open affine subschemes.

I’m sure he (among others) could answer this question definitively:

A functor F:CommRingSet is called a ‘presheaf on CommRing op’. Could there be some Grothendieck topology on CommRing op such that F comes from a scheme iff F is a sheaf with respect to this topology?

That is, do schemes form a topos? I doubt it: I thought I heard somewhere that they don’t even admit all coequalizers. James?

But maybe it doesn’t matter. The sheaf-theoretic characterization of schemes James mentioned is of a general nature which would probably apply to this speculation:

If this is true, I bet Deitmar’s ‘schemes over F 1 ’ are really just sheaves on CommMon op with respect to some Grothendieck topology on CommMon op.

So maybe we just tweak that, referring to a Zariski topology on CommMon op, and close up coproducts of objects in this category under quotients of equivalence relations which are covers?

Posted by: Todd Trimble on December 12, 2007 7:22 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Todd wrote:

The topology he was referring to… is the Zariski topology on affine schemes, where covers E αE are covering families by Zariski open affine subschemes.

Good. I think I get this idea of using the Zariski topology on affine schemes to define general schemes. I was wondering about a more ‘global’ way to pick out the schemes from among the presheaves on CommRing op.

That is, do schemes form a topos? I doubt it: I thought I heard somewhere that they don’t even admit all coequalizers. James?

We’ll have to wait until that masked man returns.

If schemes don’t even admit all coequalizers, no wonder Grothendieck became dissatisfied with them and wanted to switch to general presheaves over CommRing. I didn’t think they were that bad. (But maybe it’s easy to find two topological spaces that locally look like spectra of rings, and glue them together in a way to get a space that’s not like this?)

Anyway, while I’d like to know the slickest and most up-to-date approach to algebraic geometry before generalizing it, it seems most people are sticking with the usual approach to schemes…

So maybe we just tweak that, referring to a Zariski topology on CommMon op, and close up coproducts of objects in this category under quotients of equivalence relations which are covers?

If I understand what’s going on, that’s what Deitmar is already doing here (from week259):

He starts by defining a “commutative ring over F1” to be simply a commutative monoid. The simplest example is F1 itself.

Now, watch how he gets away with never using addition:

He defines an “ideal” in a commutative monoid R to be a subset I for which the product of something in I with anything in R again lies in I. He says an ideal P is “prime” if whenever a product of two elements in R is in P, at least one of them is in P.

He defines the “spectrum” Spec(R) of a commutative monoid R to be the set of its prime ideals. He gives this the “Zariski topology”. That’s the topology where the closed sets are the whole space, or any set of prime ideals that contain a given ideal.

He then shows how to get a sheaf of commutative monoids on Spec(R). He defines a “scheme” to be a space equipped with a sheaf of commutative monoids that’s locally isomorphic to one of this sort.

Does that sound right?

I spent some time reading Durov’s paper last night, and it seems he does the same sort of thing for commutative algebraic theories. But, he has to work a bit harder. It’s all in section 6, “Localization, Spectra and Schemes”, starting on page 269.

First he tries to copy the cases we’ve just talked about (commutative rings and commutative monoids), defining a ‘prime ideal’ for a commutative algebraic theory in a way that only depends on its unary operations. He uses this to define the ‘prime spectrum’ of a commutative algebraic theory.

But then he seems to decide this is misguided. Which makes sense: there’s obviously something fishy about focusing too much attention on the unary operations in a general algebraic theory!

He then defines a ‘total spectrum’ and works with that.

You can get a vague flavor of what he’s up to in section 6.4.14, on page 301, where he says:

Whenever we want to consider spectra of generalized rings, and generalized schemes, obtained from such spectra by gluing, we have to fix a localization theory T ? and a topology (weak or finite; strong topology won’t do for schemes since quasicoherence is not local for strong topology). We have just seen that these choices do not affect spectra of classical rings and classical schemes, so any choice would be compatible with the classical theory of Grothendieck schemes in this respect.

Posted by: John Baez on December 12, 2007 5:55 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

We’ll have to wait until that masked man returns.

While we’re waiting, I’ll blab a little about the rumor I’d thought I’d heard that the category of schemes does not admit all coequalizers. It’s just that I got the impression that that to some extent is why algebraic spaces were invented – to repair this difficulty, at least in some cases of interest to algebraic geometers. James would be able to tell us instantly, I’m sure.

Reading the wikipedia article on algebraic spaces, I gather that it’s possible to have a scheme Y and an equivalence relation

EY

where the maps involved are étale coverings but not coverings in the Zariski topology, and which doesn’t have good descent (i.e., there’s no scheme Y/E which would play the role of coequalizer of the pair of maps from E to Y above). (But by how algebraic spaces are defined, there’s always an algebraic space which fits the bill.)

Besides James, surely there are other people knowledgeable in algebraic geometry who can help out! (David Ben-Zvi? Someone from the Secret Blogging Seminar?)

Posted by: Todd Trimble on December 12, 2007 7:33 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Yet another James, James Borger, works on this kind of problem. At the Morgan-Phoa workshop he gave a talk entitled Algebraic spaces, what are they categorically? , but it was actually about Lambda rings.

Posted by: Kea on December 12, 2007 8:32 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

Todd,

Yes, algebraic stacks add certain colimits - namely quotients by etale equivalence relations - to the world of schemes. But if we want a good theory of quotients or more general colimits - for example quotients by (nonfree) algebraic group actions - then we are naturally led to the world of algebraic stacks and higher stacks.

Put another way, we can replace schemes by sheaves of sets on the category of schemes, (sometimes known as “spaces” in algebraic geometry), thereby adding colimits while retaining some of the ones we already had in our
category (namely those captured by whatever topology we are using, Zariski, etale, flat etc). Algebraic spaces come from closing up schemes in this world under simple colimits.

But if we want to do more complicated operations, like quotients by groups, we know the world of sets is not a great world to work in — we are used to replacing sets
by one of the equivalent worlds: topological spaces/homotopy, simplicial sets, or higher groupoids. e.g. we can take the quotient pt/G in the world of sets, and just stay with a point, but for most applications we might want to retain information about stabilizers and end up with BG, as an object in one of the above equivalent worlds. Likewise in the world of schemes to have a reasonable theory of moduli spaces, quotients and general colimits we should replace functors of points valued in sets by those valued in one of the above equivalent worlds. This is the world of (higher) stacks, which has a good notion of all colimits (e.g. it underlies a model category). This is explained very nicely in Toen’s survey article on higher and derived stacks. (Usually algebraic geometers don’t deal with simplicial sets but only with 1-truncated spaces, or 1-groupoids, leading to usual Artin stacks, but the above is more natural and more in the spirit of this blog…)

Of course next one should be asking about a good theory of LIMITS, which is where derived stacks originate, but I’ll
refer you to Toen’s article for that…

Posted by: David Ben-Zvi on December 13, 2007 6:44 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 259)

David,

Thanks for the confirmation and your succinct explanations.

So from what you say, higher stacks and derived stacks seem to be the right framework for a lot of basic constructions one wants in algebraic geometry (moduli spaces, good descent objects for group actions, …) – could it then be said that the language of higher/derived stacks provide the most up-to-date working foundations for algebraic geometry (supplanting schemes or algebraic spaces as good foundations, as these are not yet rich enough to carry out all the geometric operations one would like)?

Recalling John Baez’s comment here, it sounds like the world of stacks is a “nice category containing some nasty objects, [rather] than a nasty category containing only nice objects”. John’s comment was paying out more of a thread (mainly between Tom Leinster and James) on foundations for algebraic geometry, but it almost sounds like stacks already constitute a de facto technical foundation for much of modern algebraic geometry (as I think Thomas Riepe may have been suggesting as well), thus prompting my (probably naively expressed) question.

Posted by: Todd Trimble on December 14, 2007 11:07 PM | Permalink |