n-Curvature
Posted by Urs Schreiber
We have learned that parallel -transport in an -bundle with connection over a base space is an -functor from the -path -groupoid of to some -category of fibers.
With every notion of connection we expect to obtain notions of
1) curvature;
2) Bianchi identity;
3) parallel sections;
4) covariant derivative.
Here we describe the functorial incarnation of these concepts. We find
1) To every transport -functor is canonically associated a curvature -functor The functor is flat precisely if is trivial on all -morphisms.
2)
The curvature -functor, regarded as an -transport itself,
is always flat.
3) Parallel sections of the -bundle with connection associated with are equivalent to morphisms from the trivial -transport into :
4) General sections together with their covariant derivative are equivalent to morphisms from the trivial curvature -transport into the curvature -transport
What is the curvature associated with a transport, really?
Whatever it is, it should vanish if our transport factors through the fundamental -groupoid of . As opposed to , whose -morphisms are thin homotopy classes of -paths, the -morphisms of are ordinary homotopy classes of -paths.
Hence we have a canonical projection that sends any -path to its homotopy class.
Definition. We say that is flat precisely if there is an -functor such that
Whatever the curvature of an -functor is, it should be an obstruction for this construction.
Proposition. Given any -transport , we canonically obtain an -category and an -functor such that is trivial on -morphisms (sends every -morphism to an identity -morphism) if and only if is flat.
When I wrote my first entry on this topic I think I had the right idea. But I did it by hand. This time I want to let the Dao do it by its own means:
Lifting gerbes?
Here is a problem whose solution I do not understand yet.
The way I have discussed curvature above, it is the obstruction to a descent problem:
we have some -thing on and want to push it down to by completing a square to the right
The obstruction is an -thing.
This curiously smells like it should be one aspect of a general mechanism of which lifting gerbes are another.
For lifting gerbes, the problem is essentially “the same but opposite”:
given an extension of groups, and given a principal -transport we want to know if we can lift by completing a square to the left
We know from pedestrian reasoning that this lift of 1-things is obstructed by a 2-thing: the lifting gerbe.
Therefore I expect that there is, as there was for curvature, a canonical arrow-theoretic construction that reads in the above extension problem and canonically spits out the parallel transport 2-functor of the lifting gerbe.
The entire problem here looks like that for curvature, with arrows reversed. Therefore I thought it would be simple to see how it works. But I still don’t see it.