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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 -toposes, one cohesive over the other, or do we see enough from cohesion over ?
We have
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 is . Is there a ?
On everything we can act by , and its approximations, . on is infinitesimal. is not, so at some point in the interpolation this property must fail.
Then there’s global cohesion.
In section 4.6.1 of dcct, Urs represents some of the above in terms of . There we see six versions of this with various combinations of , , and sent to zero. But there are eight combinations possible for three quantities. There could be and . These would give rise to synthetic versions of the right hand pair: and .
This relates to that discussion on Manin’s three dimensions
Yes! That could be and eventially should be made explicit somewhere.
Is there a theory about these dimensions? I mean, given , how do I get to ?
Could I replace , and find similar extensions?
That the 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.
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?
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