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    • CommentRowNumber1.
    • CommentAuthorUrs
    • CommentTimeOct 20th 2010
    • CommentRowNumber2.
    • CommentAuthorMike Shulman
    • CommentTimeOct 18th 2012

    I just blogged about the recent Gepner-Kock paper which, among other things, proposes a more general definition of (infinity,1)-quasitopos than the one on the nLab. If no one objects, then in a little while I may modify the nLab’s definition.

    • CommentRowNumber3.
    • CommentAuthorUrs
    • CommentTimeOct 18th 2012
    • (edited Oct 18th 2012)

    If no one objects, then in a little while I may modify the nLab’s definition

    I certainly won’t object if we put in a comparative disussion as you do on the blog (And thanks for the summary! That’s useful. I haven’t found time to study the article in any detail).

    This all is related to a long standing question that I have been banging my head against with Dave Carchedi:

    is there a notion of concrete object in a local \infty-topos which is independent of some of these evident choices?

    We were looking at the nn-connected/nn-truncated factorization and trying to see if we could somehow “average over all nn” or the like to have not just a notion of “nn-concrete object” but just of “concrete object”.

    The same issue shows up when \infty-categorifying Lawvere’s axiom for cohesive 1-toposes that we call “discrete objects are concrete”.

    • CommentRowNumber4.
    • CommentAuthorMike Shulman
    • CommentTimeOct 18th 2012

    What are you looking to get out of such a definition?

    • CommentRowNumber5.
    • CommentAuthorUrs
    • CommentTimeOct 30th 2012
    • (edited Oct 30th 2012)

    Sorry for the slow reply.

    What are you looking to get out of such a definition?

    We never were really sure. It just somehow felt like the fact that in a local 1-topos there is a notion of concrete object – with the geometric meaning this has – should generalize to a local \infty-topos having a notion of concrete \infty-groupoids.

    Concretely, where in the local 1-topos over CartSp the concrete objects are just the diffeological spaces, a natural question seemed to be: can we intrinsically characterize the full sub-\infty-category of Sh (CartSp)Sh_\infty(CartSp) on those objects that are presented by simplicial diffeological spaces? Are these maybe somehow related to totally concrete objects in Sh (CartSp)Sh_\infty(CartSp)?

    These were the kinds of ideas that we were toying around with.

    But it may well be, I think now, that all these questions are going in the wrong direction. I did eventually find a major application for just nn-concrete objects, and maybe that’s all there is to it.

    (Namely just as 0-concreteness allows to formulate integration in differential cohomology/higher holonomy in a cohesive \infty-topos, so nn-concreteness allows to similarly formulate fiber integration in differential cohomology/transgression. I still need to write out the details of that, though. There is another aspect kicking in here for n1n \geq 1 that makes this statement be more than a blind generalization of the case for n=0n = 0.)

    • CommentRowNumber6.
    • CommentAuthorUrs
    • CommentTimeNov 29th 2012
    • (edited Nov 29th 2012)

    So I have now a better answer to the above. It comes in two parts:

    • the first is about explicit structures in differential geometry/cohomology,

    • the second is about general abstract higher modalities.

    Differential geometry, differential cohomology

    If GG is a braided \infty-group in a cohesive \infty-topos, write BG conn\mathbf{B}G_{conn}, as usual, for the coefficients for differential GG-cohomology and let XX be any other object.

    Then then mapping space object

    [X,BG conn]H [X, \mathbf{B}G_{conn}] \in \mathbf{H}

    looks a bit like the “moduli stack of GG-connections on XX”. Indeed, its global points are exactly the GG-connections on XX. But its cohesion is not quite what one needs for some applications:

    for some applications, we want the moduli \infty-stack of GG-connections to have UU-plots which are cohesive UU-parameterized collections of GG-connections on XX, of GG-gauge transformations on XX, etc. But the UU-plots of [X,BG conn][X, \mathbf{B}G_{conn}] are instead, of course, GG-connections on U×XU \times X, gauge transformations on U×XU \times X. That’s closely related, but is not quite the same.

    In a rough sense, the right moduli object should be obtained by degreewise concretification of [X,BG conn][X, \mathbf{B}G_{conn}]: it should be like [X,BG conn][X, \mathbf{B}G_{conn}] pointwise but otherwise just vary cohesively.

    I’ll write GConn(X)G\mathbf{Conn}(X) for that genuine object of differential moduli. There will be a canonical projection

    conc:[X,BG conn]GConn(X). conc \colon [X, \mathbf{B}G_{conn}] \to G \mathbf{Conn}(X) \,.

    In standard models, for XX an ordinary manifold etc. it is clear what this should be. The question is how to says this abstractly using just the cohesion, such as to know what this means for general XX and general GG and general ambient cohesive contexts.

    Higher modalities

    It was clear all along that the \sharp-modality of the cohesion should induce the construction of GConn(X)G \mathbf{Conn}(X). Now I think that I have proven that it indeed comes out, like this:

    By the construction of the forgetful map BG connBG\mathbf{B}G_{conn} \to \mathbf{B}G (that forgets the connection and only remembers the underlying bundle), it factors canonically as a tower

    BG connBG conn n1BG conn n2BG conn 0BG. \mathbf{B}G_{conn} \to \mathbf{B}G_{conn^{n-1}} \to \mathbf{B}G_{conn^{n-2 }} \to \cdots \to \mathbf{B}G_{conn^{0}} \simeq \mathbf{B}G \,.

    This tower “forgets connection data degreewise”, first the nn-form pieces, then then (n1)(n-1)-form pieces, and so on.

    For each stage [X,BG conn k][X, \mathbf{B}G_{conn^k}] we have the n-image/Postnikov system factorization of its \sharp-modality unit, which I write

    [X,BG conn k] [X,BG conn k] 2[X,BG conn k] 1[X,BG conn k] 0[X,BG conn k][X,BG conn k]. [X, \mathbf{B}G_{conn^k}] \simeq \sharp_\infty [X, \mathbf{B}G_{conn^k}] \to \cdots \to \sharp_2 [X, \mathbf{B}G_{conn^k}] \to \sharp_1 [X, \mathbf{B}G_{conn^k}] \to \sharp_0 [X, \mathbf{B}G_{conn^k}] \simeq \sharp [X, \mathbf{B}G_{conn^k}] \,.

    Now the claim is that the differential moduli object GConn(X)G\mathbf{Conn}(X) is the following iterated homotopy fiber product of “modality-images”

    GConn(X) 1[X,BG conn n]× 1[X,BG conn n1] 2[X,BG conn n1]× 2[X,BG conn n3]× n1[X,BG conn 1][X,BG]. G \mathbf{Conn}(X) \simeq \sharp_1[X, \mathbf{B}G_{conn^n}] \underset{\sharp_1 [X, \mathbf{B}G_{conn^{n-1}}]}{\times} \sharp_2[X, \mathbf{B}G_{conn^{n-1}}] \underset{\sharp_2 [X, \mathbf{B}G_{conn^{n-3}}]}{\times} \cdots \underset{\sharp_{n-1} [X, \mathbf{B}G_{conn^{1}}]}{\times} [X, \mathbf{B}G] \,.

    For instance for 1-truncated GG and hence n=2n = 2 this is the \infty-limit over

    1[X,BG conn] 2[X,BG conn 1] [X,BG] 1[X,BG conn 1] 2[X,BG]. \array{ \sharp_1[X, \mathbf{B}G_{conn}] && && \sharp_2[X, \mathbf{B}G_{conn^1}] && && [X, \mathbf{B}G] \\ & \searrow && \swarrow && \searrow && \swarrow && \\ && \sharp_1 [X, \mathbf{B}G_{conn^1}] && && \sharp_2[X, \mathbf{B}G] } \,.

    Clearly this construction is just a special case of a general construction that exists for any higher modality and a given tower of morphisms. A natural question seems to be: is this general construction something of more general relevance?

    • CommentRowNumber7.
    • CommentAuthorMike Shulman
    • CommentTimeNov 30th 2012

    Fascinating! But no, I don’t think I’ve ever seen anything like that before.