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00:32
What is "homology with local coefficients" really?

Cohomology with local coefficients is just sheaf cohomology which is just global sections (of sheaves of abelian groups or spectra), but what is homology?

In some cases homology is a special case of cohomology. For example: for a suitable class of spaces (Which include manifolds and varieties but am unsure what's the most general statement - hopefully finite type CW complexes) there's verdier duality which gives homology as a special class of cohomology.
correction - "special case" - first line in the third paragraph.
sorry third line in second paragraph
@SaalHardali As you say, for reasonable spaces you can see E-homology as $f_!f^!E$ where $f:X\to *$ is the morphism to the one-point space. I am not sure if there is a good definition of homology for unreasonable spaces, but if there is, it has to be equivalent to the procedure I gave
What I meant is that for CW-complexes $f_!f^!E = E\wedge \Sigma^∞_+X$
I meant if $X$ is a manifold $f_!f^!E=E\wedge \Sigma^∞_+X$, sorry
00:50
Wait, is $E$ a sheaf of spectra? Where is this smash product taking place then?
ah nevermind I got it.
It doesn't answer the question though
yours is a definition for homology with constant coefficients
To get homology with non-constant coefficients you just take a sheaf of $f^!E$-modules that is locally free of rank 1
And then push it with $f_!$?
Yes. I think that if X is not a manifold you have to mutter something related to the dualizing complex (a.k.a $f^!S$)
I'm really tempted to believe at this point that there's a coommon generalization of verdier duality and Spanier–Whitehead duality somewhere here
You are using SW duality in this (overly general) form of Verdier duality
00:57
Aha so it is
And $f^!S$ is the SW dual?
What do you mean?
I don't know exactly I'm asking. I've never seen such a general form of Verdier duality
Perhaps this is why I had no idea what is homology with local coefficients in the first place
Actually It would help me even if the case of HZ module is somehow explained.
So, that case is quite explicit
For example f^!HZ is the sheaf of Borel-Moore chains
Then it is clear that f_!f^!HZ is the complex of compactly supported B-M chains, a.k.a. C_*(X;Z)
Hmmm nice. What I'm trying to understand is this:
Suppose $F$ is a sheaf of $HZ$ modules. What does it mean to take homology with coefficients in $F$. I can calculate it via a procedure I learned way back but what is the meaning of these groups?
I am not sure I know how to define "homology with coefficients in HZ"
01:03
This is my point!
Wait what.
Homology in HZ just means homotopy groups of $HZ \wedge \sigma^{\infty}_+ X$?
Uh I mean in coefficients in F, sorry
Ah ok so now were on the same page
You said there's a verdier duality though so you might know how to define them (albeit in a not very direct way)?
One thing that happens is that (let's make everything HZ-linear) D(f_*F)=f_!(DF)
Ok this has to happen for it to be called verdier duality.
Where D=F(-,f^!HZ) is the Verdier dual
So in particular f_!F is dual to f_*(DF) and so I might be tempted to call it the homology of F
Going by general principles that the homology should be the cohomology of the dual, at least for dualizable objects
01:09
That's what I meant.
However f_!F is usually called the compactly supported cohomology so I am slightly uncomfortable calling it the homology
But I'm not so sure that the procedure I know calculates this thing even for very basic examples.
What's the procedure you know?
The only definition I know for local coefficients is when you have a local system of Z-modules
Yeah. It's messy
I don't like it
It's not, you can form the corresponding sheaf of B-M chains and that is a f^!HZ-module, which is the kind of thing I am comfortable taking homology of
Moreover I strongly suspect that this is just the Verdier dual of the sheaf computing the cohomology of the dual local system
I mean, the concrete definition with the explicit chains is fairly intuitive, isn't it?
01:16
Say $F$ is the sheaf of $HZ$ modules we can say $f_*\mathcal{Hom}(F,f^!HZ)=\mathcal{Hom}(f_!F,HZ)$
Is this what you meant?
The point is that Verdier duality works in situations where you can work interchangeably with homology and compactly supported cohomology
Yeah, this is what confuses me about homology with local coefficients. I understand there's a procedure and it's not very far fetched (nothing surprising). But somehow I can't find a way to justify it conceptually
In particular I can't "compose" functors that compute homology like you can compose sheaf cohomology (push $\circ$ push)
As a result there's a lot less to work with.
That's why I like having things conceptual
So, usually local coefficients are useful when you work homotopically. In that case a local system is just a functor $F:X\to HZ-Mod$ and homology is just the colimit and cohomology is just the limit
Ah so that's better already. Why haven't I thought about that.
In general a sheaf of spectra is just a functor $X \to Sp$ isn't it?
A local system of spectra, not a general sheaf
01:24
Yeah sorry abuse of terminology
I mean a homotopic sheaf
Or am I missing some crucial point here...
Isn't everything locally constant for infinity groupoids?
Well, I would never talk of a sheaf over an ∞-groupoid. It is bad terminology (although it has a meaning, it is simply confusing)
Sorry. Will not do this in the future.
So it is true that everything is locally constant over $\infty$-groupoids right?
So, a true statement is that a locally constant sheaf over a space is the same thing as a functor out of the corresponding ∞-groupoid (although it is a nontrivial theorem).
I am not sure which definition of "sheaf over an ∞-groupoid" you are using
Not sure what's the most concise way to say this but a "sheaf" of spaces for instance in my earlier terminology would just mean an $\infty$-groupoid over the my $\infty$-groupoid.
I'm told that one can stabilize the over category of an infinity groupoid to get parametrized spectra.
So, it turns out that this is equivalent to a functor from your ∞-groupoid to the category of ∞-groupoids. It is very much a special thing though. I think this terminology is more confusing than anything else and you should ditch it, but do as you feel comfortable
01:33
Already ditched it :)
Parametrized spectra again are local systems of spectra, not sheaves of spectra
Good Good.
So sheaves of spectra are something you say when there's a site right?
Yes. In general speaking of sheaves where there's not site (or topos) in sight is confusing
Got it. Thanks!
Although there is the obvious site for an infinity groupoid which gives the correct answer right?
The over category I mean.
Yes (that is a topos, not a site). That's why it is not strictly speaking an abuse of terminology
01:35
Sorry mean topos
I wouldn't recommend using it though
Yeah yeah, just wanted to make sure we were on the same page
I need to go to sleep now (4 am lol). Thanks for the help! If you have some epiphany about this homology thing please tag me here thanks!
 
14 hours later…
15:16
Here's a question: some people (including me!) talk about (n,r)-categories, meaning n-categories in which all k-morphisms with k>r are invertible. Where does this terminology come from? Who invented it?
 
1 hour later…
16:39
Let $R\to T$ be a morphism of commutative S-algebras. If I have a T-algebra A, what is the relationship between THH^T(A) and THH^R(A) ? I'm particularly interested in the case where $R\to T$ is some Bousfield localization of $R$ at some spectrum $E$ (smashing, if this helps). This sounds like a classical problem but I can't seem to find much about it (even in the algebraic HH case). Perhaps I'm lacking some keyword
@BrunoStonek If R\to T is aTHH etale extension they are the same. The THH etale condition means that THH^R(T) is equivalent to T
In general they are related by equation 8 of arxiv.org/pdf/math/0306243v1.pdf
taking X=S^1 and using your notation you get the equation $THH^T(A)=THH^R(A)otimes_{THH^R(T)}T$
Smashing localizations are THH-étale, right?
16:54
so if T is obtained from R by a Bousfield loc L that is smashing
then THH^R(T) is L-locally equivalent to T
but since they are both local they are equivaelnt
does this sound correct ?
I think so. I was thinking more crudely, something like the simplicial diagram in the definition of THH^R(T) is (homotopically) constant
yes I agree
this seems to be the argument given by McCarthy-Minasian between remark 3.4 and example 3.5
@GeoffroyHorel thanks! it seems like the keyword I was lacking was "(thh)-étale"

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