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I have added to groupoid convolution algebra the beginning of an Examples-section titled Higher groupoid convolution algebras and n-vector spaces/n-modules.
Conservatively, you can regard this indeed as just some examples of applications of the groupoid convolution algebra construction. But the way it is presented is supposed to be suggestive of a “higher C*-algebra” version of convolution algebras of higher Lie groupoids.
I have labelled it as “under construction” to reflect the fact that this latter aspect is a bit experimental for the moment.
The basic idea is that to the extent that we do have groupoid convolution as a (2,1)-functor
(as do do for discrete geometry and conjecturally do for smooth geometry), then this immediately means that it sends double groupoids to convolution sesquialgebras, hence to 3-modules with basis (3-vector spaces).
As the simplest but instructive example of this I have spelled out how the ordinary dual(commutative and non-co-commutative) Hopf algebra of a finite group arises this way as the “horizontally constant” double groupoid incarnation of , while the convolution algebra of is the algebra of the “vertically discrete” double groupoid incarnation of .
But next, if we simply replace the bare with the 2-category of -algebras and Hilbert bimodules between them and assume (as seems to be the case) that -algebraic groupoid convolution is a 2-functor
then the same argument goes through as before and yields convolution “-2-algebras” that look like Hopf-C*-algebras. Etc. Seems to go in the right direction…
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