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    • CommentRowNumber1.
    • CommentAuthorDavid_Corfield
    • CommentTimeOct 26th 2013

    Somehow I’m reminded of that Temptations song ’Ball of confusion’. Anyway, a thread to jot down ideas on how the different varieties of cohesion relate to each other. Anyone welcome to join in.

    There’s a question of how to organise cohesion. Do we see it as a relative notion and then gather together pairs of \infty-toposes, one cohesive over the other, or do we see enough from cohesion over Grpd\infty Grpd?

    We have

    SmoothGrpdEuclideanTopGrpdGrpd. Smooth \infty Grpd \to Euclidean Top \infty Grpd \to \infty Grpd.

    Then a cluster of infinitesimal extensions: super, synthetic, synthetic super imposed on them, except super does no work on Euclidean Top. Is there a synthetic Euclidean Top?

    The synthetic extension of Grpd\infty Grpd is InfGrpdInf \infty Grpd. Is there a SuperInfGrpdSuper Inf \infty Grpd?

    On everything we can act by () I(-)^I, and its approximations, J n()J^n(-). J 1=TJ^1 = T on Grpd\infty Grpd is infinitesimal. Grpd I\infty Grpd^I is not, so at some point in the interpolation this property must fail.

    Then there’s global cohesion.

    • CommentRowNumber2.
    • CommentAuthorDavid_Corfield
    • CommentTimeOct 27th 2013

    In section 4.6.1 of dcct, Urs represents some of the above in terms of { ps|q} p,s,q\{\mathbb{R}^{p \oplus s| q}\}_{p, s, q}. There we see six versions of this with various combinations of pp, qq, and ss sent to zero. But there are eight combinations possible for three quantities. There could be { 0s|q} s,q\{\mathbb{R}^{0 \oplus s| q}\}_{s, q} and { 0s} s\{\mathbb{R}^{0 \oplus s}\}_{s}. These would give rise to synthetic versions of the right hand pair: InfGrpdInf \infty Grpd and SuperInfGrpdSuper Inf \infty Grpd.

    This relates to that discussion on Manin’s three dimensions

    • CommentRowNumber3.
    • CommentAuthorUrs
    • CommentTimeNov 5th 2013

    Yes! That could be and eventially should be made explicit somewhere.

    • CommentRowNumber4.
    • CommentAuthorDavid_Corfield
    • CommentTimeNov 6th 2013

    Is there a theory about these dimensions? I mean, given \mathbb{R}, how do I get to { ps|q} p,s,q\{\mathbb{R}^{p \oplus s| q}\}_{p, s, q}?

    Could I replace \mathbb{R}, and find similar extensions?

    • CommentRowNumber5.
    • CommentAuthorUrs
    • CommentTimeNov 6th 2013

    That the { p} p\{\mathbb{R}^p\}_p themselves support a cohesive geometry rests ultimately on the fact that the Cartesian spaces are locally and globally contractible (and “supported on points”, but that’s so traditional a condition one hardly notices it). From this, the two extensions by even and by odd-graded infinitesimals is pretty automatic and just works.

    So as in earlier discussion, the real question is what other kinds of useful geometric spaces we have that are locally contractible.

    I still have the feeling that polydiscs should work, supporting cohesive analytic geometry. I even suspect that this is pretty obviously so. But sadly I still haven’t gotten around to doing anything substantial along these lines. Somebody should.

    • CommentRowNumber6.
    • CommentAuthorDavid_Corfield
    • CommentTimeNov 6th 2013

    OK, so you’d probably get odd and even-infinitesimal extensions whichever contractible spaces were found.

    I’ve probably asked before, but does using rather than make a difference?