Fourier analysis on finite groups is well known to be useful for probability theory and combinatorics — consider for example the Fourier analysis on $(\mathbb Z/2\mathbb Z)^n$ which can be used to get interesting results about sharp thresholds and noise stability and so on. It is, fortunately, concrete and easy enough that you don't need to be much of an algebraist to do something interesting.

Now, unfortunately, sometimes objects can't be easily coded by a sequence of independent bits, even if the bits are allowed to take more values. For a simple example, consider the set of graphs with n vertices and m edges. We can no longer consider a “small perturbation” of this to be rerandomizing some bits.

What we can do instead is this: Pick a pair of vertices between which there is an edge, and a pair which do not have an edge between them. Move the edge from the first pair to the second, getting a new graph with the same amount of vertices and edges, which is very similar.

I just noticed that this actually naturally creates a groupoid: Consider the category of graphs with $n$ vertices and $m$ edges, with morphisms being these switchings and compositions thereof. The same construction of course gives a groupoid for other classes of objects and switchings between them as well.

So since Fourier analysis is useful for studying perturbations in other contexts, I was wondering if there is some such thing here as well. Google tells me that abstractly there is, but is it possible to work out what it concretely is for a concretely given finite groupoid like this?