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November 26, 2007

This Week’s Finds in Mathematical Physics (Week 258)

Posted by John Baez

In week258 of This Week’s Finds, learn what happens when sand grains flow. Read more about dust in the Red Rectangle:

and discover why some of it looks like this:

Then, find out about Deligne’s conjecture concerning Hochschild cohomology — and get a nice workout in homological algebra, categories and operads.

Café regulars will be pleased to know that the proof of Deligne’s conjecture is really just an infinitely categorified version of the Eckmann–Hilton argument!

Others may be pleased to know that I explain what that means, in terms so simple that any math PhD who studied homological algebra can understand it.

Posted at November 26, 2007 4:12 AM UTC

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Re: This Week’s Finds in Mathematical Physics (Week 258)

a nice workout in homological algebra, categories and operads.

Great cosmic coincidence! Let’s talk about this stuff.

Some more or less random questions and/or remarks, all spiraling in more or less on what you have been talking about in this TWF:

So let C be our abelian category.

The Dold-Kan correspondence says that we have an equivalence of categories Simp(C)Ch (C) between simplicial objects in C and non-negatively graded chain complexes in C. The direction Simp(C)Ch (C) is forming the “normalized chain complex” which corresponds to throwing away lots of face maps except for one at each level, restricting that to the kernel of some of the others, and regarding it as the differential in our complex.

Now, first question: how precisely do I connect this to higher categories now?

I want to combine this with the nerve functor ωCat(C)Simp(C) which sends an ω-category internal to C to its simplicial nerve. I want to get an equivalence ωCat(C)Ch (C) this way. Do I? If not, can you fix this?

This was the first question. Now comes the first big mystery™:

ω-categories correspond to non-negatively graded chain complexes (and nicely so: in degree k of the chain complex we have the space of k-morphisms starting at the 0 (k1 )-morphism, roughly).

These naturally sit in arbitrarily graded chain complexes. In particular, a couple of nice and natural operations on non-negatively graded chain complexes will produce not-necessarily-non-negatively graded chain complexes from them.

Most notably: forming the dual chain complex and forming the internal hom from that.

So: in the context that ω-categories correspond to non-negatively graded chain complexes, what corresponds to positively graded chain complexes?

Maybe ω-co-categories??

Is there a general way in which the “dual” of a category would be a co-category? (Probably like the “dual” of a group, namely functions on the group elements, has a co-algebra structure on it.) (And if so, preferably with ω everywhere.)

I have Weibel’s book sitting here (Danny’s copy, to be honest) and need to refresh my memory about a bunch of things. It’s been a while.

I’d be most pleased if somebody could give an exegesis of the standard homological algebra constructions entirely in terms of ωCat(C), as far as possible. I sense in John’s TWF the tendency to do just that.

It seems to me that I’d need such an interpretation in order to understand what some easy and obvious constructions in homological algebra mean.

For instance, looking at thet AKSZ paper one finds: they say we should look at two non-negatively graded cochain complexes (parameter space par and target space tar), but then form the space of fields (the hom object between these two) in the context of arbitrarily graded complexes, hence allowing the complex hom(par,tar) to be positively and negatively graded.

(positive = ghosts, negative = anti-xyz).

It’s a simple construction in the homological algebra context. But its true interpretation is quite mysterious (currently to me): both par and tar I know come from certain higher categories. But hom(par,tar) with negative degrees allowed does not – at least not in the same obvious manner.

So what’s going on??

Posted by: Urs Schreiber on November 26, 2007 6:49 PM | Permalink | Reply to this

dual categories and co-categories

Let’s see. Parts of my questions have an obvious answer. Let me try:

Let V be a closed monoidal category such that we can enrich over it. Assume in addition that V has duals on objects.

Then for C any V-category with composition x,y,z:Hom(x,y)Hom(y,z)Hom(x,z)

we obtain a dual co-catgeory enriched over V simply by hitting everything in sight with the duality operation. So we get a co-composition x,y,z *:Hom(x,z) *Hom(x,y) *Hom(y,z) * obviously.

Hm. And I guess if I do everything internal to V, the same general statement is true. And if I then imagine I have an ω-category internal to V, the same kind of statement is still true.

That was easy enough.

So next suppose that we have one ω-category acting on another. Say G is an ω-category with a single object and we have a morphism

GEnd(C).

Then, somehow, we want to dualize G, probably obtaining a co-ω-category this way , and then merge the result with C to some single new entity.

What might that be?

Posted by: Urs Schreiber on November 26, 2007 7:14 PM | Permalink | Reply to this

Re: dual categories and co-categories

After being too verbose, as usual, I asked

What might that be?

More briefly: in a way I am asking:

What might the action ω-thing of an ω-groupoid acting on an ω-category be?

And I am looking for an answer which, when hit with some big Lie operation spits out a chain complex with the ω-groupoid in one part of its degrees, and the thing it acts on in the other.

Posted by: Urs Schreiber on November 26, 2007 8:15 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs wrote:

Great cosmic coincidence! Let’s talk about this stuff.

Okay, great! You seem to have sensed that “week258” was secretly about ω-categories — or maybe you just read the little hint in this blog entry. I didn’t want to get into that aspect explicitly in “week258”, since it would further clutter what was already an overly jargonesque explanation of what ultimately is a very simple idea.

But, whenever I think about chain complexes, I’m secretly thinking of them as specially nice strict ω-categories.

Okay…

So let C be our abelian category.

The Dold-Kan correspondence says that we have an equivalence of categories Simp(C)Ch (C) between simplicial objects in C and non-negatively graded chain complexes in C. The direction Simp(C)Ch (C) is forming the “normalized chain complex” which corresponds to throwing away lots of face maps except for one at each level, restricting that to the kernel of some of the others, and regarding it as the differential in our complex.

Right.

Now, first question: how precisely do I connect this to higher categories now?

I want to combine this with the nerve functor ωCat(C)Simp(C) which sends an ω-category internal to C to its simplicial nerve. I want to get an equivalence ωCat(C)Ch (C) this way. Do I?

Yes you do! Here I’m assuming you mean strict ω-categories.

You can use a nerve construction as you outline. But, it’s equally easy to see directly that the category

  • ωCat(C): strict ω-categories internal to the abelian category C, with strict ω-functors as morphisms.

is equivalent to the category

  • Ch (C): nonnegatively graded chain complexes in C, with chain maps as morphisms.

It’s fun and instructive to build this equivalence ‘by hand’, reinterpreting globes in terms of chains. But if you’re too busy, there’s a paper by Brown and Higgins that does it:

  • Ronald Brown and Philip J. Higgins, Cubical abelian groups with connections are equivalent to chain complexes.

    Abstract: The theorem of the title is deduced from the equivalence between crossed complexes and cubical ω-groupoids with connections proved by the authors in 1981. In fact we prove the equivalence of five categories defined internally to an additive category with kernels.

I believe that three of these five are ωCat(C), Ch (C) and Simp(C), while the others have a cubical flavor. But if you prefer octahedra and their higher-dimensional generalizations, you can probably use them too — this idea is incredibly robust!

You might enjoy this passage in HDA6 more now that you’re thinking about this stuff:

Since 2-vector spaces are equivalent to 2-term chain complexes, as described in Section 3, it should not be surprising that L -algebras are related to the categorified Lie algebras we are discussing here. An elegant but rather highbrow way to approach this is to use the theory of operads [MSS]. An L -algebra is actually an algebra of a certain operad in the symmetric monoidal category of chain complexes, called the ‘L operad’. Just as categories in Vect are equivalent to 2-term chain complexes, strict ω-categories in Vect can be shown equivalent to general chain complexes, by a similar argument [BH]. Using this equivalence, we can transfer the L operad from the world of chain complexes to the world of strict ω-category objects in Vect, and define a semistrict Lie ω-algebra to be an algebra of the resulting operad.

I also sketched how to see a chain complex in C as a strict ω-category in C starting at the bottom of page 18 here:

This is getting long, so I’ll quit this comment here and talk about other things in another comment. Your question:

So: in the context that ω-categories correspond to non-negatively graded chain complexes, what corresponds to positively graded chain complexes?

was very much on my mind while writing “week258”. Or at least it would have been if you meant to write “what corresponds to non-positively graded chain complexes?” Is that what you meant?

Posted by: John Baez on November 26, 2007 7:36 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Brown and Higgins wrote:

In fact we prove the equivalence of five categories defined internally to an additive category with kernels.

I wrote:

I believe that three of these five are ωCat(C), Ch (C) and Simp(C), while the others have a cubical flavor.

Actually they don’t do Simp(C) — I guess the Dold-Kan theorem was too well-known to bother stating! They show these five are equivalent:

  1. chain complexes in C
  2. crossed complexes in C
  3. cubical sets with connections in C
  4. cubical ω-groupoids with connections in C
  5. globular strict ω-groupoids in C

It’s easy to see that globular strict ω-categories in C are the same as globular strict ω-groupoids in C. So, item 5 is just what you’re calling ωCat(C). And, of course, item 1 is your Ch (C).

Posted by: John Baez on November 26, 2007 7:46 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Thanks for that reply! Great.

You seem to have sensed that “week258” was secretly about ω-categories

Well, it almost seemed like you were responding to my questions here :-)

Or at least it would have been if you meant to write “what corresponds to non-positively graded chain complexes?” Is that what you meant?

Yes! These sign issues are a nuisance…

Posted by: Urs Schreiber on November 26, 2007 7:51 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

But if you prefer octahedra and their higher-dimensional generalizations, you can probably use them too

You could help fix yet another gap in my education here:

somehow I understand that Ross Street’s orientals, or probably some generalization of them, is supposed to make precise what you just indicated: a notion of ω-category based on a rather arbitrary geometric form (simplex, cube, etc.)

But I don’t really know the details.

Hm, while googling for this I ran into

Richard Steiner, Orientals

which even relates all that to chain complexes:

We show that the category of orientals is isomorphic to a subcategory of the category of chain complexes.

Hm, this is closely related to what I was talking about with Bruce in Bakewell. I wonder if Bruce is reading this here…

With Bruce I was chatting about this (not that our joint expertise was supposed to overcome the critical mass threshold):

dg-manifolds (linear approximation to smooth ω-groupoids) are modules over the endomorphisms of the odd line. This is a cool way of saying that most of their properties are encoded in the unique law of the universe, which reads d 2 =0 .

I was looking for an analogous way to describe ω-groupoids themselves. If I think of them as Kan-complexes, hence in particular as simplicial objects, I seem to be getting close: I could try to look at simplicial objects internal to -modules and then encode all face and degeneracy information in something like 2 =0 acting on that.

Does anyone see what I am trying to get at here? I’ll see what Richard Steiner has to say about this…

Posted by: Urs Schreiber on November 26, 2007 8:57 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs wrote:

Somehow I understand that Ross Street’s orientals, or probably some generalization of them, is supposed to make precise what you just indicated: a notion of ω-category based on a rather arbitrary geometric form (simplex, cube, etc.)

But I don’t really know the details.

The nth oriental is the free strict ω-category on an n-simplex.

Orientals are Street’s method of solving this problem: what is the simplicial nerve of a strict ω-category?

To answer this sort of problem, we need to take a strict ω-category C and figure out what the n-simplices in its nerve are.

An n-simplex in Nerve(C) is just a map from Δ[n] to Nerve(C). Here Δ[n] is the ‘walking n-simplex’ — the simplicial set that consists mainly of an n-simplex, but also of course its faces and degeneracies. Most people call this the ‘simplicial n-simplex’, but that sounds a bit scary at first.

So, the set of n-simplices in Nerve(C) is

hom(Δ[n],Nerve(C))

where we’re taking hom in the world of simplicial sets.

But the way these things work, the Nerve functor should be right adjoint to some functor — let’s call it Π — which takes a simplicial set and works out its ‘fundamental -category’. So, we should have

hom(X,Nerve(C))hom(Π (X),C)

and in particular

hom(Δ[n],Nerve(C))hom(Π (Δ[n]),C)

So, we’ll understand a lot about the nerve of C if we can understand Π (Δ[n]) — the fundamental ω-category of the walking n-simplex. And, this is what Street calls the nth oriental!

If you want to understand this stuff, I urge you to ponder Sreet’s Conspectus of Australian Category Theory, a nice paper which will eventually show up in the volume Peter May and I are editing.

In the section which describes his work on simplicial weak ω-categories, he says:

I decided to concentrate on one aspect of the problem. How do we rigorously define the nerve of an n-category? After unsuccessfully looking for an easy way out using multiple categories and multiply simplicial sets (I sent several letters to John Roberts about this), I realized that the problem came down to defining the free n-category O n on the n-simplex. Meaning had to be given to the term ‘free’ in this context: free on what kind of structure? How was an ‘n’-simplex an example of the structure? The structure required was an n-computad. The definition of n-computad and free n-category on an n-computad is done simultaneously by induction on n (see St17, Pw1, St21, St22, St29). An element of dimension n of the nerve NA of an ω-category A is an n-functor from O n to A. Things began to click once I drew the following picture of the 4 -simplex:

Click on the picture for a bigger version. It’s really a picture of the oriental O 4 , if you know how to look at it correctly. It should remind you of the ‘pentagonator’.

Posted by: John Baez on November 27, 2007 1:45 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

It IS the ur-pentagonator. Just take the tree corresponding to the triangulation. It continues to work for the associahedra. In fact I think ?Street? drew the picture for the 5-simplex.

Posted by: jim stasheff on November 27, 2007 2:35 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

If you read Street’s conspectus, you’ll see he even drew the picture for the 6-simplex — and you’ll see how long it took him!

Posted by: John Baez on November 27, 2007 7:34 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

“ah yes, I remember it well”

It’s similar pictures leading to Gordon, Power and Street that led me to realize that my former colleague Gordon and I had more in common than friendship.

Posted by: jim stasheff on November 28, 2007 1:55 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs meant to write:

So: in the context that ω-categories correspond to non-negatively graded chain complexes, what corresponds to non-positively graded chain complexes?

Maybe ω-co-categories??

One way to tackle this uses the fact that whenever C is an abelian category, so is C op. The people who invented this concept cleverly made the definition self-dual!

So, here goes:

First, a non-positively graded chain complex in some abelian category C is the same as a non-negatively graded cochain complex in C.

Second, a non-negatively graded cochain complex in C is the same as a non-negatively graded chain complex in C op.

Third, a non-negatively graded chain complex in C op is the same as a strict ω-category in C op.

So, a non-positively graded chain complex in C is the same as a strict ω-category in C op.

I suppose you could call this an ‘ω-co-category’ in C, but fewer people would understand you — like, 3 instead of 10.

However, we don’t always want to separate the positive and negative parts of a chain complex and treat them separately! What if we’ve got a full-fledged, -graded chain complex in C?

This gives a strict -category in C!

A -category has n-morphisms for n going down all the way to , as well as all the up to +.

Alas, the only people I know who have discussed -categories are James Dolan and myself. And, we haven’t written too much about them — just a few remarks in various papers.

It’s not hard to define strict -categories, internalize them, and prove that a -graded chain complex in C is the same as a strict -category in C.

The trickier part is to make sure that a strict -groupoid works out to be precisely a -graded chain complex of abelian groups. You need to make sure the Eckmann–Hilton theorem kicks in and makes everything abelian.

The really tricky thing would be to define weak -groupoids in a purely algebraic way, and then make sure they’re the same as spectra. In the field of ‘stable homotopy theory’, algebraic topologists use spectra as a generalization of chain complexes in precisely this way. The word ‘stable’ means ‘with homotopy groups going infinitely far down’. But, these guys don’t define spectra starting from a theory of weak -categories. Not yet, anyway.

There’s a lot more to say about this… Most things about weak -categories would be hard to make precise at present. But, many things involving strict -categories should be quite easy to make precise.

Posted by: John Baez on November 26, 2007 10:05 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

However, we don’t always want to separate the positive and negative parts of a chain complex and treat them separately! What if we’ve got a full-fledged, -graded chain complex in C?

Exactly, that’s what I keep asking. Starting here, continuing here and culminating here.

Back then I did receive a couple of helpful replies to this by David Ben-Zvi here, here and here.

I found these helpful, but wanted more: I wanted a conceptual understanding of what it means, ω-groupoid-wise, when I start with my Lie ω-groupoid, turn it into a non-negatively graded chain complex by linearizing it – and then adding stuff in the negative degrees.

In On Lie -modules and the BV complex I am starting to argue that having positive and negative degrees is the hallmark of having one ω-thing acting on another ω-thing.

This crucially involves some of the observations you mentioned, like

a non-positively graded chain complex in some abelian category C is the same as a non-negatively graded cochain complex in C.

Namely, when we form the Lie-Rinehart -pair with one Lie -algebra g (a chain complex, in particular!) acting on some module B (another chain complex!) this structure is encoded in the correspondonding Chevalley-Eilenberg algebra, which is defined on the complex

g *B.

Notice that, due to the fact that g here has been dualized, this is now a complex in arbitrary degree. And it’s a fact that equipping that complex with a dg-algebra structure encodes

- both the Lie -algebra structure of g

- as well as its action on B.

Therefore my conclusion was:

arbitrarily graded chain complexes (at least when carrying a dg-algebra structure) have to do with actions of ω-categories on each other.

But luckily you now provide the kind of interpretation I was hoping you would give:

What if we’ve got a full-fledged, -graded chain complex in C?

This gives a strict -category in C!

Ah!

Clearly my next question would be for references:

Alas, the only people I know who have discussed -categories are James Dolan and myself. And, we haven’t written too much about them — just a few remarks in various papers.

I guess I can imagine how to define them. What I would really like to know is:

- how are you thinking about -categories in the grand scheme of things?

- where do you apply them?

- do you at all see a connection with the situations in which you have been thinking about -categories and the situation I sketched, where we are dealing with actions of one ω-category on another?

Posted by: Urs Schreiber on November 27, 2007 9:51 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs wrote:

I guess I can imagine how to define them. What I would really like to know is:

- how are you thinking about -categories in the grand scheme of things?

They’re all about ‘stabilization’ — the process that occurs as you march down the periodic table.

A k-tuply monoidal n-category should be the same as a (k+1 )-tuply monoidal n-category when k gets big enough, I guess around k=2 n+2 . So at this point we can just call it a stable n-category.

But, a stable n-category is a special sort of stable (n+1 )-category: one with only identity morphisms. Conversely, we should be able to decategorify a stable (n+1 )-category and get a stable n-category. This suggests that we define a stable -category to be an -category equipped with extra structure such that whenever you decategorify it to get an n-category for any finite n, the result is stable.

You can think of a stable -category as having n-morphisms for each n0 , together with an ‘infinitely deep basement’ consisting of one identity n-morphism for each n<0 .

However, if you think about it this way, the indexing is a bit arbitrary. Why require that the interesting n-morphisms show up only for n>0 ? We can reindex them so they show up for n>k for any k, even negative k.

At this point we’re tempted to consider -categories — gadgets that can have nontrivial n-morphisms for all n. But, we want to retain the benefits of stability. So, we should define them carefully. I could explain how, but I prefer to let you ponder it a bit first, to see why it requires care.

The key point is: algebraic topologists have been thinking about this stuff for many decades already. However, instead of -categories, they think about -groupoids, which they call ‘spaces’. They call stable -groupoids ‘infinite loop spaces’. And, they call -groupoids ‘spectra’.

So, many of the clever tricks we need to perform can simply be stolen from them!

In particular, this business about needing to define -categories ‘carefully’ is very famous in the theory of spectra. It took algebraic topologists a long time to reach their current understanding of spectra.

- where do you apply them?

-categories are very important: they show up whenever algebraic topologists study stable homotopy theory — meaning things like -graded chain complexes (for babies) or spectra (for grownups). A spectrum is just a weak -groupoid. A chain complex is just a strict -groupoid!

Our job is simply to stop saying ‘groupoid’ all the time, and say ‘category’ instead.

- do you at all see a connection with the situations in which you have been thinking about -categories and the situation I sketched, where we are dealing with actions of one ω-category on another?

I don’t have time for a thoughtful answer now, but place -categories show up is this: if X and Y are nonnegatively graded chain complexes, the sensible notion of hom(X,Y) is -graded! The negative grades creep in even if you hadn’t wanted them. This is how cochain complexes snuck into “week258”.

And of course homs are closely related to actions…

Posted by: John Baez on November 27, 2007 8:00 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Thanks indeed for the detailed reply. Very helpful indeed.

Just remind me: when you say -groupoid, what precisely do you mean? Kan complex, quasi-category, ω-groupoid, complicial set, …? And does it matter?

but one place -categories show up is this: if X and Y are nonnegatively graded chain complexes, the sensible notion of hom(X,Y) is \mathbb{Z}-graded! The negative grades creep in even if you hadn’t wanted them.

Yes, that’s precisely the reason why I am trying to straighten this out:

AKSZ show say that when you quantize a thing that looks like X and propagates on Y, with X and Y -groupoids of sorts, then the space of fields should be taken as the hom(X,Y) of -categories! Instead of what you’d rather expect: the hom in -groupoids.

+) The positive degrees of hom(X,Y) are the ghosts.

0) The zero degrees of hom(X,Y) are the fields.

-) The negative degrees of hom(X,Y) are the anti-fields and anti-ghosts.

I could make my life easy and simply accept this as a fact, happily computing in this context. I understand this quite well operationally and it is an extremely cool fact - once you accept it.

But it bothers me. Even if I accept the fact that I need to consider -categories, it’s still strange:

why don’t we take X and Y to be -categories themselves? Probably we could. But then: what does it mean if we don’t?

Posted by: Urs Schreiber on November 27, 2007 10:38 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs wrote:

Just remind me: when you say -groupoid, what precisely do you mean? Kan complex, quasi-category, ω-groupoid, complicial set,..? And does it matter?

There’s a big difference between strict and weak -grouopids, of course.

By a ‘strict -groupoid’ I mean a strict globular ω-category with all n-morphisms (n>0 ) strictly invertible. Maybe this is what you’re calling an ω-groupoid.

(I don’t particularly like the use of ‘ω-’ to mean ‘strict -‘, but perhaps it’s entrenched enough that we should go with it.)

There are lots of different models of weak -groupoids that have all been proved equivalent, at least at the level of model categories. That is, there are a bunch of model categories which are all Quillen equivalent, and I’m perfectly happy to call an object of any of these a weak -groupoid.

The two most obvious choices are:

  • simplicial sets (with Kan complexes as the fibrant objects, so we may use just Kan complexes)
  • nice topological spaces (let us say compactly generated weak Hausdorff spaces)

Quasicategories are not at all intended to be a model of weak -groupoids; they’re a model of weak (,1 )-categories, which are significantly more general! There are lots of other models of weak (,1 )-categories, and any of these can be restricted to give a model of -groupoids, by demanding that the 1-morphisms are weakly invertible.

Complicial sets are also not a model for weak -groupoids. They’re a simplicial formulation of strict -categories.

Posted by: John Baez on November 28, 2007 7:05 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Okay, thanks a lot.

So this was a really important piece of information for me:

They call stable -groupoids ‘infinite loop spaces’. And, they call -groupoids ‘spectra’. #

even though I gather it is maybe supposed to be more or less a tautology.

If I understand correctly, the point is this: an infinite loop space is a space which allows to apply B to it arbitrarily often. But we can apply B n times to things that are n-tuply monoidal. So infinite loop spaces correspond to -tuply monoidal things. And another word for that is stable things.

Then I also get the point about spectra and -categories, I guess.

Hm, now suppose we’d considered ring spectra. These would correspond to monoidal -categories.

But… Hm. There shouldn’t be anything preventing us from considering monoidal -categories, then double monoidal -categories, then k-tuply monoidal -categories.

Then stable -categories??

Suppose I were not just saying these words but could actually handle this: would I just go in a circle and stay withing -categories – or would I arrive at, say, 2 -categories, or maybe -categories or…

Somehow dg-algebras are supposed to be equivalent to (hope I get this right) modules over Eilenberg-MacLane ring spectra? Or something like that, I am probably misremembering what somebody told me over lunch. But maybe I need to better understand that statement. And what it means in terms of -categories.

Posted by: Urs Schreiber on November 28, 2007 7:25 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Urs wrote:

If I understand correctly, the point is this: an infinite loop space is a space which allows to apply B to it arbitrarily often. But we can apply B n times to things that are n-tuply monoidal. So infinite loop spaces correspond to -tuply monoidal things. And another word for that is stable things.

You’re almost exactly right. James Dolan and I discuss this starting on page 21 of Categorification. It’s standard material in topology; what we do is sketch how to talk about it in the language of n-category theory.

But, you may enjoy this slight correction: there’s a difference between a k-tuply monoidal -groupoid and a k-tuply groupal -groupoid. In the latter, the k extra multiplication operations have weak inverses.

In topology, a k-tuply monoidal -groupoid corresponds to an E k space. (To be precise, an E k space is a space that’s an algebra of the little k-cubes operad.)

Among the E k spaces are the k-fold loop spaces. These are the ones that correspond to k-tuply groupal -groupoids.

It’s easy to exhibit lots of very interesting E k spaces that that aren’t k-fold loop spaces. The easiest one is the ‘free E k space on a point’. For details, see page 27 of our paper.

Then I also get the point about spectra and -categories, I guess.

You probably do. But: spectra correspond to -groupoids.

I don’t actually know truly interesting examples of -categories that aren’t -groupoids. (By ‘truly interesting’, I mean ones that aren’t just shifted -categories.) There must be lots of fun examples; I just haven’t tried to find any.

Hm, now suppose we’d considered ring spectra. These would correspond to monoidal -categories.

You mean monoidal -groupoids.

Yes, ring spectra are -groupoids with a new monoidal structure which we should think of as ‘multiplication’, since it distributes over the previous ‘additive’ stable monoidal structure.

But… Hm. There shouldn’t be anything preventing us from considering monoidal -categories, then double monoidal -categories, then k-tuply monoidal -categories.

Yes. In the world of topology, k-tuply monoidal -groupoids are very important. They’re called ‘E k ring spectra’.

Then stable -categories??

Stable -groupoids are also very important in topology. They’re called ‘E ring spectra’. Many of the most popular spectra are E ring spectra.

In short; when we replace abelian groups by -groupoids (aka spectra), rings go to ring spectra and commutative rings go to E ring spectra.

This set of analogies is the foundation of brave new algebra. People are starting to redo all of algebraic geometry with E ring spectra replacing commutative rings! You can think of this as some sort of ‘-groupoidification’ of algebraic geometry.

It’s about time! The basic ideas are not new:

  • J. P. May, F. Quinn, N. Ray and J. Tornehave, E Ring Spaces and E Ring Spectra, Lecture Notes in Mathematics 577, Springer Verlag, Berlin, 1977.

But, important technical advances have only recently made it practical to do algebraic geometry with E ring spectra — and this is what makes brave new algebra a hot topic.

Hmm — it’s time for dinner.

Posted by: John Baez on November 29, 2007 5:29 AM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

somehow dg-algebras are supposed to be equivalent to (hope I get this right) modules over Eilenberg-MacLane ring spectra?

The statement is apparently:

dg-algebras (of -modules i.e. of abelian groups) are equivalent to

monoids in the category of symmetric spectra that are modules over the Eilenberg-MacLance spectrum H.

Since dg-algebras are also monoids in (co)chain complexes I was wondering whether that means that (co)chain complexes themselves are equivcalent to H-modules.

But this we couldn’t figure out.

Posted by: Urs Schreiber on November 29, 2007 5:30 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

John wrote:

but one place -categories show up is this: if X and Y are nonnegatively graded chain complexes, the sensible notion of hom(X,Y) is -graded! The negative grades creep in even if you hadn’t wanted them.

And I said:

Yes, that’s precisely the reason why I am trying to straighten this out:

AKSZ show say that when you quantize a thing that looks like X and propagates on Y, with X and X -groupoids of sorts, then the space of fields should be taken as the hom(X,Y) of -categories! Instead of what you’d rather expect: the hom in -groupoids.

+) The positive degrees of hom(X,Y) are the ghosts.

0) The zero degrees of hom(X,Y) are the fields.

-) The negative degrees of hom(X,Y) are the anti-fields and anti-ghosts.

I am about to get into that in more detail in my notes. Here is a figure emphasizing this (important, I think) point a little more:

And now good night!

Posted by: Urs Schreiber on November 28, 2007 11:55 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

In search for hints concerning my conjecture that coalgebra structures on positively and negatively graded chain complexes correspond to Lie -algebras (in positive degree) together with an -vector space (in negative degree) which they act on, I asked John:

- do you at all see a connection with the situations in which you have been thinking about -categories and the situation I sketched, where we are dealing with actions of one ω-category on another?

After giving plenty of thoughtful answers, John replied to this particular question:

I don’t have time for a thoughtful answer now, but place -categories show up is this: if X and Y are nonnegatively graded chain complexes, the sensible notion of hom(X,Y) is -graded! The negative grades creep in even if you hadn’t wanted them. This is how cochain complexes snuck into “week258”.

And of course homs are closely related to actions…

That was after he explained that -categories are all about stabilization.

I thought about this for a while. Here is the conclusion at which I arrived:

take a 1-tuply monoidal 0-groupoid. That’s a group. It lives in degree 0.

The fact that it is 1-tuply monoidal means we can suspend it to a 1-groupoid with a single object.

Now the group itself is in degree 1. And the single object is in degree 0.

But let’s think about this: it is unfair to regard that single object just as a dot .

Rather, we should think of the group as being the group of automorphisms of that single object. The shifting process in which we regard a monoidal n-thing as an (n+1 )-thing here really makes manifest that a monoidal thing usually arises as the endomorphisms of some other thing.

A doubly monoidal 0-groupoid is an abelian group. We shift it up twice to obtain a 2-category with a single object and a single 1-morphism. And we should think of the abelian group really as being the automorphism group of that single morphism.

I am probably (hopyfully, even) stating a triviality in a verbose way. But it took me some thought process to arrive at this:

the game we are plaing here can be regarded as saying this:

if I have a k-tuply monoidal n-category, I can, instead of shifting it up to a k+n-category with single p-cells for p<k, think of it as being something with cells in degree 0 up to n, with something sitting in degree -1 to p.

And moreover, as we have seen above, this stuff in the negative degrees is really nicely thought of as something that the stuff in the non-negative degrees acts on.

Now, as John explains, when both k and n go all the way through infinity, we arrive at -categories.

But if the above is right, it would mean that a good way to think of a stable -groupoid is as the automorphisms of some infinity-thing hidded in the negative degrees.

Okay, that’s what i wanted to say. When the thought occurred to me I found it useful. Now that I have typed it into a comment box it feels a little pointless. But I’ll post it anyway.

Posted by: Urs Schreiber on December 5, 2007 10:37 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

I could try to claim that I’m starting to become an expert on things A , but given that Jim Stasheff is an avid commenter here, I don’t quite dare to. :)

However, I have read the Lu-Palmieri-Wu-Zhang [LPWZh] paper mentioned in the exposition backwards and forwards. On the face, what LPWZh try to do is to take the survey articles by Bernhard Keller, outlining the use of A -algebras in representation theory, and widening the scope of their proven usability while actually proving the many unproven and interesting statements that Keller makes.

At the core of this lies two different theorems. One is the Kadeishvili theorem (which in various guises has been proven by everyone involved with A -algebras, and a few more, in my impression ;) that says that you can carry A -algebras across taking homology. Kadeishvili’s argument specializes to the case where you start with an A -algebra with only m 1 and m 2 are non-trivial – i.e. a plain old dg-algebra. For higher generality, you’d probably want to turn to the Homology Perturbation Theory crowd with Stasheff, Gugenheim and Huebschmann among the more famous names…

Hence, since if we take graded endomorphism algebra of a resolution of M and introduce the “homotopy differential”: f=df+fd, then cycles are chain maps and the homology picks out exactly the algebra cohomology over the appropriate module category. Thus, we get Ext as the homology of a dg-algebra, and thus, Ext has an A -algebra structure.

The second cornerstone of these papers is the Keller higher multiplication theorem: if the ring R is sufficiently nice, then the A -algebra structure on Ext R *(M,M) for some appropriate module M will allow you to recover a presentation of R explicitly.

I hope this answers your question about the origin of their A -algebra structure.

Posted by: Mikael Vejdemo Johansson on November 26, 2007 8:00 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

Thanks, Mikael — that’s extremely helpful!

I think this means that the A -algebra structure that everyone uses on Ext R *(M,M) agrees with the ‘conceptually simple’ one that I proposed in “week258”.

My way — for which the details haven’t been worked out — was to associate an A -category to any sufficiently nice abelian category. For simplicity, let’s start with the category of R-modules for some ring R. Then my idea was to build an A -category with R-modules as objects, but a new hom, the ‘derived function complex’

HOM(x,y)=hom(Px,y)

Here Px is a nice functorial projective resolution of x, say the free resolution. We think of Px and y as chain complexes of R-modules, and let hom(Px,y) be the cochain complex of abelian groups where the n-chains are degree-(n) maps of graded R-modules from Px to y… not necessarily chain maps!

I believe there’s a reasonable way to define a composition

:HOM(x,y)HOM(y,z)HOM(x,z)

and I think this gives an A -category. It could in fact be a mere differential graded category, which would make what I’m saying sound a bit pompous. But either way, this would make

HOM(x,x)

into an A -algebra (for example a dg algebra). Then, taking cohomology and using the Kadeishvili theorem, we see that

Ext *(x,x)=H *(HOM(x,x))

is an A -algebra.

I guess the only difference between this stuff and what you’re saying is that I’m using

hom(Px,x)

where you are using

hom(Px,Px)

Hmm! These should be equivalent as A -algebras, but the multiplication is obviously associative ‘on the nose’ in yours, so yours is simpler.

So, instead of defining

HOM(x,y)=hom(Px,y)

maybe I should define

HOM(x,y)=hom(Px,Py)

to make composition easier to define, and get a dg category instead of an A -category. It’s probably ‘equivalent’ (in some relaxed sense of equivalence suited to A -categories), but more manageable.

Indeed, everything I’m doing has probably been done better already by the experts.

Posted by: John Baez on November 26, 2007 11:21 PM | Permalink | Reply to this

Re: This Week’s Finds in Mathematical Physics (Week 258)

I’m not sure I understand precisely what you’re saying in this comment, but this is what I think you’re getting at. As you guessed, what you want to do is the dg-version of derived categories. (I’m not working on so much sleep, so don&