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Let be a Lie group and let be the smooth stack of principal -bundles. Then we have a natural equivalence . If we apply the internal hom to the homotopy pullback diagram defining (and if internal homs preserve homotopy pullbacks, something I need be reassured about) then we get a homotopy pullback diagram realizing the free loop space object as the based loop space of . On the other hand, since is a smooth group, then so is and we can consider the smooth stack , whose based loop space is again .
What is the relation between and ? (if any)
From what I read in the lines after equation (3.2) in Konrad Waldorf’s Spin structures on loop spaces that characterize string manifolds I guess that for a connected the two stacks and should actually be equivalent, but I don’t clearly see this yet.
I guess simple-connectedness would play a role here, no?
Could be: Konrad Waldorf writes “Since is connected, is a principal -bundle over , see etc. etc.”, which is the sentence I derived my guess from (here is a spin manifold, is its frame bundle (i.e., the total space of the associated principal Spin-bundle) and stands for “loop space”). But since is actually simply connected (Konrad work with high enough ), it may well be that the sentence should actually have read “Since is simply connected…”.
I don’t know about the stacky-part, but in terms of Lie groups and their classifying spaces then and commute. Indeed, and commute. For a Lie group , we have the fibration sequence with contractible. Then this maps to which is still a fibration sequence. Moreover, the contraction of maps to a contraction of whence the base of the fibration is . This argument works with -maps or with -complexes or whatever you require. There’s no requirement of connectivity or simple connectivity.
Hmm, and we should use the fact we can take to be a group, so that is perfectly well-defined as a homogeneous space and is a model for . And shouldn’t this be just ?
You don’t need it to be a group, just a principle -bundle.
Hi,
I guess the connectivity assumption is needed in order for to be connected. If not, then it is only the conneceted component of the basepoint to be a . But connected should be enough, with no need of simple connectedness.
Yes, that the two stacks (-stacks) are equivalent follows directly from preserving all -limits, which gives
and hence by definition of as the inverse equivalence in
we have
as soon as is connected, which it is precisely if for all there is an essentially unique -principal infinity-bundle on the circle times the germ of an -disk .
(I am including some links just for the sake of eventual bystanders.)
I’ve thought about this some more, and the connectivity assumptions are there to ensure that is connected since it is the identity component of this which is .
The reason being that a point of must have a lift to . Now a point of classifies a -bundle over and a lift of this to is a section, whence a trivialisation. Thus a point of is in if (and only if) the associated bundle is trivial, which occurs if and only if it is in the identity component of .
Thus the general statement is that:
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