Smooth 2-Functors and Differential Forms
Posted by Urs Schreiber
We have now a detailed description and proof of the relation between
- strict smooth 2-functors on 2-paths in a manifold with values in a strict Lie 2-group
and
- differential forms with values in the corresponding Lie 2-algebra :
U.S. and Konrad Waldorf
Smooth Functors vs. Differential Forms
arXiv:0802.0663v1
Abstract: We establish a relation between smooth 2-functors defined on the path 2-groupoid of a smooth manifold and differential forms on this manifold. This way we set up a dictionary between fundamental notions from category theory and differential geometry. We show that smooth 2-functors appear in several fields, namely as connections on (non-abelian) gerbes, as the curvature of smooth functors and as critical points in BF theory. We demonstrate further that our dictionary provides a powerful tool to discuss the transgression of geometric objects to loop spaces.
This is finally the detailed worked-out version of the stuff I talk about in the entry On -Transport, Part II.
This result is the bridge between the description of ordinary (1-)bundles with connection in terms of parallel transport functors
U.S. and K. Waldorf
Parallel Transport and Functors
(arXiv, blog)
and the corresponding description of 2-bundles with connection as indicated in
John Baez, U.S.
Higher Gauge Theory
arXiv:math/0511710v2.
The further detailed development of this to a full-blown theory of 2-Transport will be the content of a followup article which is in preparation. This will sum up various things that Konrad and me have been talking about for a while now, for instance here:
Konrad Waldorf, Parallel Transport Functors of Principal Bundles and (non-abelian) Bundle Gerbes (pdf, blog)
Konrad Waldorf, Parallel Transport and Functors (pdf slides)
U. S., Parallel Transport in Low Dimensions (pdf, blog)
U.S., On String- and Chern-Simons -Transport (pdf slides, blog)
The last one also indicates how all this is related to a description where smooth -functors between Lie -groupoids are replaced by morphisms of Lie -algebras/Lie -algebroids. Since the latter are more easily handled for all , on this differential side the entire program has already proceeded past all the way to :
Hisham Sati, U.S., Jim Stasheff
-Connections and Applications to String- and Chern-Simons -Transport
(pdf, blog, arXiv).
(The big theorem in the Lie 2-groupoid case in Smooth Functors vs. Differential Forms becomes, in the differential world of Lie 2-algebras, a simple example (see for instance section 6.5.1). Of course then the problem is to integrate that back to the world of Lie -groupoids. Dicussion of that can be found here on the blog at On Lie -tegration and Rational Homotopy Theory and Differential Forms and Smooth Spaces.)
As the title suggests, all this is headed towards understanding String- and Chern-Simons -transport (and their higher dimensional generalizations) and their quantization (their image under the “quantization edge” of the cube): in the end we want to hit a classical Chern-Simons parallel 3-transport with the quantization functor to obtain the Chern-Simons quantum 3-transport and the holographically related WZW theory, as described in
Jens Fjelstad and U.S.
Towards 2-Functorial CFT
(blog).
I started to describe this step using the Lie -algebraic description in the series of entries States of Chern-Simons Theory (I, II, III).
This so far concentrates on just the kinematics: the value of the TFT 3-functor on -dimensional manifolds. For its value on -dimensional manifolds (i.e. for the “path integral”) one will need BV-quantization.
How BV quantization arises in the context of -transport is indicated in the last section of -connections as well as in the notes
U.S., On the BV-Formalism (pdf, blog).
But clearly more work is necessary here.
Re: Smooth 2-Functors and Differential Forms
Wow, it’s really coming together at last, isn’t it?