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created equivariant homotopy theory – table displaying the various cohesive ∞-toposes and their bases ∞-toposes (for inclusion in “Related entries” at the relevant entries)
I remember you told me once that there was no interesting super version of ETop∞Grpd. Does then ETopGrpdcell=PSh∞(Orb) prevent any interesting mixture of equivariance with super-extensions?
So Orb is an enhanced version of the full sub-∞-category of Smooth∞Grpd on the objects of the form BG for G a compact Lie group. That sub-∞-category genuinely knows smooth structure and does have non-trivial superifications.
Passing to Orb here means replacing external hom-groupoids between these BGs with geometic realization of internal hom-groupoids. That is a curious step which somehow governs the whole theory, but which remains a bit subtle, to my mind. I am not sure if superification goes along with this. I really wish I had a better concrete feeling for this step…
I see. Yes, curious. I wonder why that’s seen as the natural thing to do.
I suppose one way to think of this is that this is the natural way to have the geometry enter the hom-spaces, so that it is in a way “more geoemtric” than not doing it.
As I remarked elswhere once when we discussed this, this is inded one of the very things that Lawvere pointed out cohesion is good for back in “axiomatic cohesion”: given a cohesive topos (or ∞-topos, same story): then it has three kinds of hom-objects:
the external hom space H(X,A)∈∞Grpd;
the internal one [X,A]∈H (so far as for any topos);
the realization Π[X,A]∈∞Grpd.
It’s the fact that Π preserves products which says that Π[X,A] gives a secondary enrichment of H in ∞-groupoids. The self-enrichment in point 2 contains “more information” than both 1 and 3, but leads us to enriched ∞-category theory. The third point retains as much of the geometric information in 2 as possible while still staying non-trivially enriched.
So that’s what the global equivariant indexing category is: the full sub-∞-category of that secondary enrichment of ETop∞Grpd on the deloopings of compact Lie groups.
From that perspective it is quite natural to consider this.
But even if conceptually naturally, I still find it hard (harder) to reason about this, to work with it.
On the other hand, depending on what you have in mind with supergeometry here:
you can take the ∞-topos SmoothSuper∞Grpd and then make it G-equivariant by passing to the ∞-topos [Orb,SmoothSuper∞Grpd].
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