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Use of cohesive and/or fractured structures in synthetic algebraic geometry #33
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By the way, just a suggestion to @felixwellen : for this kind of open-ended questions, GitHub discussions seems to be a more appropriate tool than issues. Maybe you could enable discussions in the repo settings? |
Hi, |
It of course depends on what you mean by useful cohesive structure... |
It has the same limitations as discussed in #18: The flat modality cannot be as good as in cohesive HoTT, because that would imply the localization is a topos. This is even more direct for a sharp-modality, which, by being right adjoint, would be a lex monadic modality. |
Yeah, obviously I was a big misguided here. On a more basic level, I think this is related to some fundamental problems with |
The link you sent is interesting - I need some time to read through that though. But you are right that "cohesive" does mean "topological space-like" in many senses, and we already know very well that fails pretty badly on algebraic objects. |
I think the idea that things "are made from contractible blobs" is a good way to think about cohesion. In the thread I linked, it is also discussed that this is not sufficient to cover all topological spaces. On the other hand, it is sufficient to cover also lots of things which are topological but have complicated additional structure, like differential manifolds. And once you have cohesion (or a relevant part of it, like in |
Yeah, I guess when I was talking about topological spaces, I was thinking of "nice" spaces.
Doesn't covering require only the existence of a shape modality, so not full cohesion? Sure we can do everything that can be done in cohesive HoTT that does not require the flat or sharp modalities (that would be a tautological statement). I guess I was trying to see whether there is a more general setting in which we could look at |
BTW I found this answer written by Peter Scholze - indeed the problem comes from schemes not being locally contractible. He seems to suggest, though, that if one switches to the pro-etale (i.e. condensed) setting, things might start to work... |
Some follow up work. I think this suggests that we will get some form of cohesion (but not it!) once we move into the condensed world - I don't know what that will imply at the time being... |
Yes, a shape modality is a "relevant part" of cohesion I would say, even though it is just a modality ;-) |
Judging from the thesis I sent in the previous comment - cohesiveness is generally not a useful concept in an algebraic setting. On the other hand, fracturedness, developed by Lurie in the context of spectral algebraic geometry and used successfully by Clough (2023) to study differentiable sheaves, seem to be a much more useful concept. There is currently no synthetic account of fracturedness, but I expect to be useful in SAG once it is developed. It can't fix the problem that motivic spaces do not form a topos per se, but it should be useful in some way. |
I suggest leaving this issue open for further discussion, though. Maybe change the title? |
The (related) differential hexagon has been treated synthetically: |
This is a sort of continuation to #18.
Does the Nisnevich$(\infty, 1)$ -topos on $\mathbf{Sch}/S$ admit a useful cohesive structure?
The nLab page on motivic homotopy theory suggests that if one is working in the right topos (i.e., Nisnevich), then localizing at$\mathbb{A}^1$ will appropriately give one the motivic homotopy theory. Now, I'm probably interpreting it very wrong, but it seems to follow that if one is working in the Nisnevich topos (as one should be), then localization at $\mathbb{A}^1$ will give one the shape modality one wants, giving the higher Nisnevich topos the cohesive structure one wants.
I wonder what one can make out of this.
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