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    • CommentRowNumber1.
    • CommentAuthorUrs
    • CommentTimeSep 15th 2021

    for completeness, to go with U(ℋ), for the moment mainly in order to record references, such as:

    v1, current

    • CommentRowNumber2.
    • CommentAuthorUrs
    • CommentTimeSep 19th 2021
    • (edited Sep 19th 2021)

    added the statement that PU()PU(\mathcal{H}) is well-pointed, which is made explicit on p. 23 of

    but follows by a more general result due to Dardalat and Pennig.

    diff, v3, current

    • CommentRowNumber3.
    • CommentAuthorUrs
    • CommentTimeSep 19th 2021
    • (edited Sep 19th 2021)

    added statement that S 1U()PU()S^1 \to \mathrm{U}(\mathcal{H}) \to PU(\mathcal{H}) is a fiber bundle. Am copying this statement also to U(H) and to coset space coprojection admitting local sections

    diff, v5, current

    • CommentRowNumber4.
    • CommentAuthorUrs
    • CommentTimeOct 30th 2021

    added pointer to:

    • Ellen Maycock Parker, The Brauer Group of Graded Continuous Trace C *C^\ast-Algebras, Transactions of the American Mathematical Society 308 1 (1988) (jstor:2000953)

    diff, v6, current

    • CommentRowNumber5.
    • CommentAuthorUrs
    • CommentTimeDec 13th 2021

    for the graded version of PU()PU(\mathcal{H}) I have added pointer also to

    diff, v7, current

    • CommentRowNumber6.
    • CommentAuthorUrs
    • CommentTimeDec 13th 2021

    These authors also point (in addition to the reference in #4) to

    • E. Parker, Graded continuous trace C *C^\ast-algebras and duality, Operator algebras and topology (Craiova, 1989), 130–145, Pitman Res. Notes Math. Ser., 270.

    but I haven’t yet found any online trace of this article/book (I find the 1983 version of the series, but not the one from 1989).

    • CommentRowNumber7.
    • CommentAuthorperezl.alonso
    • CommentTimeApr 16th 2024
    • (edited Apr 16th 2024)

    The setting of NN\to \infty D-branes giving rise to an infinite-dimensional gauge bundle reminds me of the difference in presentations of the string group, where PU(H)PU(H) itself also appears in the construction by Stolz. In p.28 of 1201.5277 it is reviewed that the map of topological spaces dd:BPU(H)B 2U(1)dd:BPU(H)\to B^2 U(1) is actually the identity morphism, but surely its differential refinement dd of smooth stacks is not. But one can still have a fibration B 2U(1)BPU(H)BG\mathbf{B}^2 U(1)\to \mathbf{B} PU(H)\to \mathbf{B} G for BG=*BG=*, i.e. a nontrivial extension of 2-groups only visible at the smooth setting but not at the topological level, so that the NN\to \infty branes actually carry a nonabelian gerbe (with hopefully a finite-dimensional presentation). Do the arguments for quantization in differential K-theory rule out this possibility, or are they really just based on the need to incorporate the differential picture into the original hypothesis for quantization? The fact that those large NN matrix models describe some aspects of string and M-theory, which does feature these non-abelian gerbes, might suggest these already appear on D-branes, no?