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    • CommentRowNumber1.
    • CommentAuthorUrs
    • CommentTimeJul 21st 2010
    • (edited Jul 21st 2010)

    I am a bit stuck/puzzled with the following. Maybe you have an idea:

    I have a group object GG and a morphism GQG \to Q. I have a model for the universal GG-bundle EG\mathbf{E}G (an object weakly equivalent to the point with a fibration EGBG\mathbf{E}G \to \mathbf{B}G).

    I have another object EQ\mathbf{E}Q weakly equivalent to the point such that I get a commuting diagram

    G Q EG EQ \array{ G &\to& Q \\ \downarrow && \downarrow \\ \mathbf{E}G &\to& \mathbf{E}Q }

    Here QQ is not groupal and i write EQ\mathbf{E}Q only for the heck of it and to indicate that this is contractible and the vertical morphisms above are monic (cofibrations if due care is taken).

    So I have GG acting on EG\mathbf{E}G and the coequalizer of that action exists and is BG\mathbf{B}G

    G×EGEGBG G \times \mathbf{E}G \stackrel{\to}{\to} \mathbf{E}G \to \mathbf{B}G

    I can also consider the colimit KK of the diagram

    G×EGEGEQ. G \times \mathbf{E}G \stackrel{\to}{\to} \mathbf{E}G \to \mathbf{E}Q \,.

    That gives me a canonical morphism BGK\mathbf{B}G \to K fitting in total into a diagram

    G Q EG EQ BG K. \array{ G &\to& Q \\ \downarrow && \downarrow \\ \mathbf{E}G &\to& \mathbf{E}Q \\ \downarrow && \downarrow \\ \mathbf{B}G &\to& K } \,.

    Now here comes finally the question: I know that the coequalizer of G×EGEGG \times \mathbf{E}G \stackrel{\to}{\to} \mathbf{E}G is a model for the homotopy colimit over the diagram

    G×GG* \cdots G \times G \stackrel{\to}{\stackrel{\to}{\to}} G \stackrel{\to}{\to} *

    as you can imagine. But I am stuck: what intrinsic (,1)(\infty,1)-categorical operation is KK a model of?

    I must be being dense….

    • CommentRowNumber2.
    • CommentAuthorUrs
    • CommentTimeJul 21st 2010
    • (edited Jul 21st 2010)

    Not sure if it helps to see the pattern or distract from its general structure: but my detailed setup is described in a bit more detail (though still in a rough fashion) here.

    • CommentRowNumber3.
    • CommentAuthorMike Shulman
    • CommentTimeJul 21st 2010

    I don’t understand the definition of K; is there a typo in the displayed equation after “I can also consider the colimit K of the diagram”?

    • CommentRowNumber4.
    • CommentAuthorUrs
    • CommentTimeJul 21st 2010
    • (edited Jul 21st 2010)

    KK was supposed to be the coequalizer of the two composite maps

    G×EGEQ G \times \mathbf{E}G \stackrel{\to}{\to} \mathbf{E}Q

    But wait, I guess I am being stupid….

    • CommentRowNumber5.
    • CommentAuthorUrs
    • CommentTimeJul 21st 2010

    Right, so I guess i simply mean that the square

    EG EQ BG K \array{ \mathbf{E}G &\to& \mathbf{E}Q \\ \downarrow && \downarrow \\ \mathbf{B}G &\to& K }

    is a pushout.

    • CommentRowNumber6.
    • CommentAuthorMike Shulman
    • CommentTimeJul 22nd 2010

    Is EGEQEG \to EQ a cofibration? If not, then it seems that that pushout has no homotopical meaning. If so, then it’s an acyclic cofibration, since both EG and EQ are contractible, hence BGKBG \to K is also an acyclic cofibration and thus a weak equivalence, so K is the same as BG. Regardless, it doesn’t seem that K can contain any information about Q, since that pushout doesn’t contain Q anywhere.

    • CommentRowNumber7.
    • CommentAuthorUrs
    • CommentTimeJul 22nd 2010

    Yeah, it looks puzzling.

    I should turn the question around:

    given a morphism in an (,1)(\infty,1)-category GQG \to Q, where GG happens to be a group object. Does this induce any canonical morphism out of the delooping BG\mathbf{B}G?

    (Feel free to assume some extra properties if that helps make you think of something.)

    • CommentRowNumber8.
    • CommentAuthorUrs
    • CommentTimeJul 22nd 2010
    • (edited Jul 22nd 2010)

    Well, I should maybe add the following: that morphsm GQG \to Q is part of a fiber sequence

    GQLBG. G \to Q \to L \to \mathbf{B}G \,.

    In the case that GG happens to be twice deloopable, this continues as

    GQLBGBQ G \to Q \to L \to \mathbf{B}G \to \mathbf{B}Q

    and that BGBQ\mathbf{B}G \to \mathbf{B}Q is what I need.

    So one way to ask what I am asking is: in the case that GG is not twice deloopable, what’s a reaonable universal approximation to the non-existent BGBQ\mathbf{B}G \to \mathbf{B}Q here?

    (Actually, I have a guess for that, too, using some extra structure I have availabke, but I can’t show that my guess reproduces the above ordinary pushout construciton.)

    • CommentRowNumber9.
    • CommentAuthorMike Shulman
    • CommentTimeJul 23rd 2010

    Should it be obvious that such a fiber sequence can be continued if G is twice deloopable? Or is this a special characteristic of your situation?

    • CommentRowNumber10.
    • CommentAuthorUrs
    • CommentTimeJul 23rd 2010
    • (edited Jul 23rd 2010)

    Should it be obvious that such a fiber sequence can be continued if G is twice deloopable? Or is this a special characteristic of your situation?

    This is special for my situation.

    The fiber sequence that i am considering is that induced by the counit

    LConstΓId LConst \Gamma \to Id

    of the terminal geometric morphism. I am working in an “locally \infty-connected” situation, so that :=LConstΓ\mathbf{\flat} := LConst \Gamma is a right adjoint. As such it preserves looping, and hence I get a fiber sequence

    G dRBGBGBG dRB 2GB 2GB 2G G \to \mathbf{\flat}_{dR} \mathbf{B}G \to \mathbf{\flat}\mathbf{B}G \to \mathbf{B}G \to \mathbf{\flat}_{dR} \mathbf{B}^2 G \to \mathbf{\flat}\mathbf{B}^2 G \to \mathbf{B}^2 G
    • CommentRowNumber11.
    • CommentAuthorMike Shulman
    • CommentTimeJul 23rd 2010

    Ok. I think I’m not going to be able to help you without spending a lot more time to understand your situation; sorry.