Flat Ehresmann connections in Cohesive HoTT
Posted by Urs Schreiber
This is to share a little observation about the formulation of flat Ehresmann connections in cohesive homotopy type theory.
For context, this can be understood as following up on two different threads on this blog:
You may think of this as part IV of the little series HoTT Cohesion (part I: de Rham cohomology, part II: differential cohomology, part III: geometric prequantization) in which we discussed very simple constructions in homotopy type theory that exist as soon as the axiom of cohesion is added and which, simple as they are, are interpreted as fundamental constructions in higher differential geometry.
You may think of this as a curious example of the theory of twisted principal ∞-bundles discussed in the previous entry. For I will describe how a flat Ehresmann connection on a -principal -bundle is formalized as a -twisted -bundle on its total space, where (“flat”) is one of the two reflectors in the definition of cohesive homotopy type theory.
Preliminaries and reminder
Recall from HoTT Cohesion - Exercise I and Exercise II that one of the fundamental consequences of cohesion in homotopy type theory is that for every -group – defined to be the identity type for some inhabited connected type which we will write – we have a long fiber sequence like this:
Here is the type of -principal bundles (a dependent term is interpreted as a -principal bundle over ) and similarly is that of -principal bundles with flat connection. The function forgets the flat connection and just remembers the underlying bundle. Next, is the type of flat (closed) -valued differential forms, in that a dependent term is a flat -valued differential form on .
Accordingly, the function
is such a flat -valued form: the Maurer-Cartan form on . Here we see it arise canonically as the homotopy fiber of the function that regards a flat -valued differential form as a flat connection on the trivial -principal -bundle.
All these items are discussed in more detail in the Lab entry cohesive (∞,1)-topos – structures.
Flat connections
We will now use the first stage of the above long fiber sequence and regard it as a local coefficient bundle, for that purpose suggestively drawn like this:
In the sense of section 4.1 of NSSa this exhibits the universal associated -bundle for the canonical --action by gauge transformations on -valued differential forms.
Suppose we start with a -principal bundle over some , modulated by the function .
Then we can ask for a lift of this through .
such a lift is a choice of flat connection on . Or rather, it classifies such a flat connection. Or better: it modulates a flat connection on .
Namely, by the discussion in section 4.2 of NSSa, is a cocycle in -twisted de Rham cohomology: there exists a cover
(a function such that ) over which lifts to a function with values in , hence to a differential form on the cover
So is a flat -valued form on TWISTED by the -principal bundle .
Traditionally we might say: “Yes, that’s a useful heuristics for thinking about flat connections”. In cohesive HoTT this statement is a formal fact.
Flat Ehresmann connections
There are many equivalent traditional incarnations of the notion of a connection on a bundle. One of them is that of an Ehresmann connection. This is the definition where a flat connection on the bundle as above is exhibited by a flat -valued differential form on that satisfies two conditions:
E I: The restriction of to any fiber is the Maurer-Cartan form ;
E II: Translating by under the -action on is the same as applying the adjoint action of on .
With the above cohesive homotopy type theory, we can naturally obtain such a structure from the connection . For if we regard this as a -twisted -valued de Rham cocycle, then by the discussion in section 4.3 of NSSa we are to consider the pasting of homotopy pullbacks
and regard the function
that appears here as modulating the geometric structure over which reflects the lift down on base space : the -twisted infinity-bundle corresponding to .
The way that this appears it is a morphism of -actions: it intertwines the -actions on and on . An with such properties we may call a flat Ehresmann connection on in cohesive homotopy type theory.
If the cohesive homotopy type theory is taken to be the internal language of Smooth∞Grpd and if happens to be an ordinary Lie group, then one can check that such are indeed Ehresmann connection 1-forms in the traditional sense. It is intuitively clear that the respect for the -action of corresponds to the second Ehresmann condition. In fact it also implies the first. This we can see manifestly already in the abstract language:
Let be any point of . Then we can form the pasting of homotopy pullbacks on the left of this equivalence
where the pasting law for pullbacks, this identifies on the right the restriction of to the fiber
with the Maurer-Cartan form.
Re: Flat Ehresmann connections in Cohesive HoTT
This may have been addressed elsewhere, but how does one define given in a general cohesive -topos? How much does look like a Lie algebra (or vector space with extra structure)?