Categorifying the Dijkgraaf-Witten model
Posted by John Baez
The Dijkgraaf-Witten model is a simple sort of topological quantum field theory where the only field is a gauge field, and the gauge group G is finite:
Martins and Porter have a new paper on how to categorify this model, replacing the group G by a categorical group, or “2-group”.
I wrote about this stuff eleven years ago in week54 of This Week’s Finds - so if you want an elementary intro to these ideas, start there.
In the simplest version of the Dijkgraaf-Witten model, the path integral is just an integral over the moduli space of principal G-bundles, using the simplest possible measure on that space. It’s nice to formulate this theory on a triangulated manifold, where we assign a group element to each edge, and require that these group elements multiply to 1 around each triangle. This formulation makes it clear that we can also “twist” the Dijkgraaf-Witten model, which in n dimensions amounts to changing the action by any element of the nth cohomology of the gauge group.
I explained this stuff in the Winter 2005 Quantum Gravity Seminar. I also discussed the generalization where G is a Lie group - this gives 3d quantum gravity. And, I explained how the path integral in such theories can be rewritten as a sum over spin foams.
For people who like higher gauge theory, it’s tempting to “categorify” the Dijkgraaf-Witten model by replacing the gauge group by a 2-group. There’s already been some work on this, going back to a paper by Yetter:
-
David Yetter, TQFT’s from homotopy 2-types, Journal of Knot Theory and its Ramifications 2 (1993), 113-123.
and you can see more recent papers online:
Anyway, here’s a new one!
A categorical group or “crossed module” is the same as a strict 2-group. Note that this paper “twists” the categorified Dijkgraaf-Witten model using an element of the nth cohomology of the classifying space of our 2-group. So, it’s using the obvious generalization of group cohomology to 2-groups.
It would be nice to generalize this work from finite (or discrete) 2-groups to Lie 2-groups, and that’s sort of what I’m doing with Freidel and Baratin - we’re focusing on the case of the Poincaré 2-group.
Note that in all these theories, the connection or 2-connection is flat - it has to be when G is discrete, but it still is in these theories when we generalize G to a Lie group or Lie 2-group. Flat connections are a wee bit boring in physics, but good for getting TQFTs. Urs is busy working on more exciting theories that involve 2-connections or 3-connections with nontrivial curvature.
One can try to go further, replacing the group in the Dijkgraaf-Witten model by an -group, but the Homotopy Hypothesis conjectures that such things are the same as pointed connected homotopy -types, so at this point it’s more efficient to use simplicial techniques rather than -categories to make the ideas precise. For work along these lines, try:
Posted at August 24, 2006 7:16 AM UTC
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Re: Categorifying the Dijkgraaf-Witten model
Thanks, John, for inserting into my entry on Martins & Porter a link back to this entry here, which I forgot to point to.
At one point I want to get back and explain and emphasize again how really cool things happen when we replace here the finite group by our strict Fréchet Lie 2-group
without the central extension (so this is still equivalent to ) and then realize that putting in the central extension to the strict string 2-group amounts to introducing the “twist” here in the guise of a weak 2-functor
Transgressing this setup to loop space produces the Lie-analog of Simon Willerton’s baby FHT theorem as I once described in the entry with the funny title 2-Monoid of Observables on String-G.
In particular, the representations of the loop groupoid that we transgress to are twisted equivariant vector bundles on and we make contact with non-baby FHT.
Back then I was stopped by the fact that I wasn’t sure if I could handle the smooth structure on the quotient
where “” is supposed to denote the operation of identifying isomorphic 1-morphisms.
But now I think I actually can handle this, essentially by the standard smooth space Yoga.
I should try to find the time to do that. There is something interesting lurking here, which will connect all this combinatorial and homotopy theoretic reasoning to the real thing.
Re: Categorifying the Dijkgraaf-Witten model
Perhaps I can ask a question about this, which I haven’t been able to answer by browsing through the references provided. I thought that conventional finite-group Dijkgraaf-Witten only gave you 2+1 dimensional TQFTs. What about this categorified case? Does that give you 3+1 dimensional TQFTs, or doesn’t it work like that? I suspect it doesn’t, as John didn’t mention any dimensionality in his original post.
Re: Categorifying the Dijkgraaf-Witten model
I’m having quite a lot of luck banishing some of my higher-categorical gremlins here, so I’ll try again with one more.
I’ve lurked around enough by now to discover that a fundamental motivation for higher category theory is the relationship between -groupoids and the homotopies of compact topological spaces. For example, we can think of a 2-group as a connected compact topological space with , and so on all trivial.
But surely, the same topological space would be just as well-represented categorically by a 3-group created from by adding trivial 3-cells. Let’s call this , where the process adds trivial cells to an -category. It would also be just as well represented by , or even by .
Something else that’s of fundamental importance for -groups is their representation theory, given by unitary functors into . If and essentially represent the same topological space, wouldn’t we expect there to be a correspondence between the representations of and of , and in fact of and , for any -groupoid ? However, it seems to me that this isn’t the case, which I’ve tested at all the levels for which I know what ‘functor’ means.
Does this bother anybody else, or is there some deeper philosophy of -groupoids by which it all makes sense? The obvious conclusion is that a representation of an -groupoid doesn’t tell you something about the underlying topological space, but is sensitive to the way you’ve chosen to describe it as an -category… this seems a shame to me!
Re: Categorifying the Dijkgraaf-Witten model
Thanks, John, for inserting into my entry on Martins & Porter a link back to this entry here, which I forgot to point to.
At one point I want to get back and explain and emphasize again how really cool things happen when we replace here the finite group by our strict Fréchet Lie 2-group without the central extension (so this is still equivalent to ) and then realize that putting in the central extension to the strict string 2-group amounts to introducing the “twist” here in the guise of a weak 2-functor
Transgressing this setup to loop space produces the Lie-analog of Simon Willerton’s baby FHT theorem as I once described in the entry with the funny title 2-Monoid of Observables on String-G.
In particular, the representations of the loop groupoid that we transgress to are twisted equivariant vector bundles on and we make contact with non-baby FHT.
Back then I was stopped by the fact that I wasn’t sure if I could handle the smooth structure on the quotient where “” is supposed to denote the operation of identifying isomorphic 1-morphisms.
But now I think I actually can handle this, essentially by the standard smooth space Yoga.
I should try to find the time to do that. There is something interesting lurking here, which will connect all this combinatorial and homotopy theoretic reasoning to the real thing.