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    • CommentRowNumber1.
    • CommentAuthorUrs
    • CommentTimeNov 19th 2009

    wrote a fairly long Idea section at cohomology

    since the question keeps coming up and I noticed that the entry did a rather suboptimal job of describing the nice observation to be described here.

    • CommentRowNumber2.
    • CommentAuthorzskoda
    • CommentTimeNov 19th 2009
    I wrote few days ago at crossed product algebra some issues about "cocycled" case, where a generalization of a nonabelian group 2-cocycle to Hopf algebras appears ("factor system"). I do not really believe that such examples also come from standard model categories. Any idea how to generalize such cocycles for every n ?
    • CommentRowNumber3.
    • CommentAuthorUrs
    • CommentTimeNov 20th 2009

    I looked at crossed product algebra (also edited a bit, introducing some subsections). I don't see clearly yet.

    Could you remind me: do we have a simpler example of Hopf algebraic cocycles, where one could easier see what is going on? I would want to try to see if we can dualize all algebraic statements, at least morally, to get something that looks more like the familiar geometric examples, so that it would be easier to recognize a pattern.

    Currently I don't really see at all what is going on in the definition of that 2-cocycle  \sigma that you discuss. Do you have any intuition for what is going on here?

    • CommentRowNumber4.
    • CommentAuthorzskoda
    • CommentTimeNov 20th 2009
    • (edited Nov 20th 2009)
    But the generalization is mechanically almost trivial. I will now write it without checking (from memory) but the procedure is roughly the following. Take the usual group factor system G x G to B, say like in the case coming from 1->G->E->B->1 extension of groups (like in classical works of MacLane 1948 or so). Write down the linear extension of those to the group algebra (no dualization, this is linearization) i.e. to a bilinear map kG (x) kG to U=kB. Voila ! Now take this as a definition for every Hopf algebra H together with a measuring of H on U. The fact that we have measuring and not module is reflecting the generalization of the classical fact that we have a pseudofunctor.

    On the other hand, there are also special cases for Lie algebras and so on.