ScalingStacks

5. Applications

In this section, we apply the results of Section 4 to calculate the centers and traces (and their higher ℰn\mathcal{E}_{n}-analogues) of symmetric monoidal ∞\infty-categories of quasi-coherent sheaves. We also calculate centers and traces of ∞\infty-categories of linear endofunctors (equivalently by Corollary 4.10, quasi-coherent sheaves on fiber products) with monoidal structure given by composition (equivalently, convolution over the base).

5.1. Centers and traces

We begin with a discussion of the general notions of centers and traces of associative algebra objects in closed symmetric monoidal ∞\infty-categories. This is a general version of the approach to topological Hochschild homology developed in [EKMM, Sh]. We then calculate the center and trace of the symmetric monoidal ∞\infty-category of sheaves QC⁡(X)\qc(X) on a perfect stack XX (where we think of QC⁡(X)\qc(X) as an associative algebra object in the closed symmetric monoidal ∞\infty-category 𝒫​rL\mathcal{P}r^{\rm L} of presentable ∞\infty-categories).

Let 𝒮\mathcal{S} be a symmetric monoidal presentable ∞\infty-category. Recall that an associative algebra structure on A∈𝒮A\in\mathcal{S} is an object is equivalent to the structure of algebra over the ℰ1\mathcal{E}_{1} operad. We briefly recall the ∞\infty-category versions of two familiar facts from classical algebra.

First, there is the notion of the opposite associative algebra Aop∈𝒮A^{\rm op}\in\mathcal{S}. For this, recall that there is a map of operads τ:ℰ1→ℰ1\tau:\mathcal{E}_{1}\rightarrow\mathcal{E}_{1} determined by the action of the symmetric group Σ2\Sigma_{2} on the two contractible subspaces of ℰ1​(2)\mathcal{E}_{1}(2), and such that τ∘τ\tau\circ\tau is equivalent to the identity. Given an ℰ1\mathcal{E}_{1}-algebra AA, the pullback τ∗​A\tau^{*}A is by definition the opposite ℰ1\mathcal{E}_{1}-algebra AopA^{\rm op}.

Second, given two associative algebras A,B∈𝒮A,B\in\mathcal{S}, their monoidal product A⊗B∈𝒮A\otimes B\in\mathcal{S} carries a natural associative algebra structure. For this, recall that given two algebras AA, BB over any topological operad 𝒪\mathcal{O}, we have the structure of an 𝒪×𝒪\mathcal{O}\times\mathcal{O}-algebra on the monoidal product A⊗BA\otimes B. Since the term-wise diagonal map gives a map of operads 𝒪→𝒪×𝒪\mathcal{O}\rightarrow\mathcal{O}\times\mathcal{O}, we obtain an 𝒪\mathcal{O}-algebra structure on A⊗BA\otimes B by restriction along the diagonal.

Furthermore, any associative algebra A∈𝒮A\in\mathcal{S} is a left (as well as a right) module object over the associative algebra A⊗AopA\otimes A^{\rm op} via left and right multiplication.

Now assume further that 𝒮\mathcal{S} is a closed symmetric monoidal ∞\infty-category. Then we have internal hom objects [L4, 2.7], and given A⊗AopA\otimes A^{\rm op}-modules M,NM,N, we can define the A⊗AopA\otimes A^{\rm op}-linear morphism object ℋ​o​mA⊗Aop​(M,N)∈𝒮{\mathcal{H}om}_{A\otimes A^{\rm op}}(M,N)\in\mathcal{S}. Likewise, given left and right A⊗AopA\otimes A^{\rm op} modules M,N∈𝒮M,N\in\mathcal{S} we have a pairing M⊗A⊗AopN∈𝒮M\otimes_{A\otimes A^{\rm op}}N\in\mathcal{S} defined by the two-sided bar construction [L4, 4.5] over A⊗AopA\otimes A^{\rm op}.

0NYB

Definition 5.1. Let AA be an associative algebra object in a closed symmetric monoidal ∞\infty-category 𝒮\mathcal{S}.

  1. (1)

    The derived center or Hochschild cohomology 𝒵⁡(A)=HH∗⁡(A)∈𝒮\mathcal{Z}(A)=\hh^{*}(A)\in\mathcal{S} is the endomorphism object ℰ​n​dA⊗Aop​(A){\mathcal{E}nd}_{A\otimes A^{\rm op}}(A) of AA as an AA-bimodule.

  2. (2)

    The derived trace or Hochschild homology 𝒯​r​(A)=HH∗⁡(A)∈𝒮\mathcal{T}r(A)=\hh_{*}(A)\in\mathcal{S} is the pairing object A⊗A⊗AopA{A\otimes_{A\otimes A^{\rm op}}A} of AA with itself as an AA-bimodule.

In general, the center 𝒵⁡(A)\mathcal{Z}(A) is again an associative algebra object in 𝒮\mathcal{S}, and the trace 𝒯​r​(A)\mathcal{T}r(A) is an AA-module object in 𝒮\mathcal{S}. Furthermore, 𝒵⁡(A)\mathcal{Z}(A) comes with a canonical central morphism

𝔷:𝒵⁡(A)\textstyle{\mathfrak{z}:\mathcal{Z}(A)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}A\textstyle{A}F\textstyle{F\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F⁡(1A)\textstyle{F(1_{A})}

while 𝒯​r​(A)\mathcal{T}r(A) comes with a canonical trace morphism

𝔱​𝔯:A\textstyle{\mathfrak{tr}:A\ignorespaces\ignorespaces\ignorespaces\ignorespaces}𝒯​r​(A)\textstyle{\mathcal{T}r(A)}A\textstyle{A\ignorespaces\ignorespaces\ignorespaces\ignorespaces}A⊗A⊗A1A\textstyle{A\otimes_{A\otimes A}1_{A}}

coequalizing left and right multiplication. When AA is in fact symmetric, 𝒵⁡(A)\mathcal{Z}(A) and 𝒯​r​(A)\mathcal{T}r(A) are again naturally symmetric algebra objects in 𝒮\mathcal{S}, though the symmetric algebra structure on 𝒵⁡(A)\mathcal{Z}(A) is different from its general associative algebra structure.

5.1.1. Cyclic bar construction

It is very useful to have versions of the Hochschild chain and cochain complexes which calculate the trace and center. In the setting of an associative algebra object AA in a monoidal ∞\infty-category 𝒮\mathcal{S}, they will take the form of a simplicial object 𝐍∗c​y​c​(A)\mathbf{N}^{cyc}_{*}(A) and cosimplicial object 𝐍c​y​c∗​(A)\mathbf{N}_{cyc}^{*}(A) such that the geometric realization colim⁡𝐍∗c​y​c​(A)\colim\mathbf{N}^{cyc}_{*}(A) is the trace 𝒯​r​(A)\mathcal{T}r(A) and the totalization lim𝐍c​y​c∗​(A)\lim\mathbf{N}_{cyc}^{*}(A) is the center 𝒵⁡(A)\mathcal{Z}(A). (Note that simplicial and cosimplicial objects here are taken in the ∞\infty-categorical sense, and so the diagram identities hold up to coherent homotopies as in, e.g., [A], where the cyclic bar construction for A∞A_{\infty} H-spaces is developed.)

We construct the simplicial object 𝐍∗c​y​c​(A)\mathbf{N}^{cyc}_{*}(A) and cosimplicial object 𝐍c​y​c∗​(A)\mathbf{N}_{cyc}^{*}(A) as follows. Consider the adjunction

𝒮\textstyle{\mathcal{S}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F\scriptstyle{F}ModA​(𝒮)\textstyle{\mathrm{Mod}_{A}(\mathcal{S})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G\scriptstyle{G}

where F(−)=A⊗−F(-)=A\otimes- is the induction, and GG is the forgetful functor. It determines a comonad S≃F​GS\simeq FG acting on ModA​(𝒮)\mathrm{Mod}_{A}(\mathcal{S}).

As in classical algebra, for any AA-module MM, the comonad SS provides a canonical augmented simplicial object C∗​(M)C_{*}(M) with terms

Cn−1​(M)≃(F​G)n​(M)≃A⊗n⊗MC_{n-1}(M)\simeq(FG)^{n}(M)\simeq A^{\otimes n}\otimes M

such that the geometric realization of C∗​(M)C_{*}(M) is naturally equivalent to MM. We will say that C∗​(M)C_{*}(M) is a simplicial resolution of MM.

We can apply this technique to produce the familiar cyclic bar construction. Consider the special case of the above adjunction

ModAop​(𝒮)\textstyle{\mathrm{Mod}_{A^{\rm op}}(\mathcal{S})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F\scriptstyle{F}ModA⊗Aop​(𝒮)\textstyle{\mathrm{Mod}_{A\otimes A^{\rm op}}(\mathcal{S})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G\scriptstyle{G}

where F(−)=A⊗−F(-)=A\otimes- again is the induction, and GG is the forgetful functor from AA-bimodules to right AA-modules. Using the comonad S≃F​GS\simeq FG, we obtain a simplicial resolution C∗​(A)C_{*}(A) of the AA-bimodule AA whose terms Cn−1​(A)≃A⊗n+1C_{n-1}(A)\simeq A^{\otimes n+1} are AA-bimodules which are free as left AA-modules.

Now recall that the trace 𝒯​r​(A)\mathcal{T}r(A) is defined by the self-pairing A⊗A⊗AopAA\otimes_{A\otimes A^{\rm op}}A. Since the tensor product commutes with colimits, in particular geometric realizations, we calculate

𝒯​r​(A)=A⊗A⊗AopA≃A⊗A⊗Aop|C∗​(A)|≃|A⊗A⊗AopC∗​(A)|.\mathcal{T}r(A)=A\otimes_{A\otimes A^{\rm op}}A\simeq A\otimes_{A\otimes A^{\rm op}}|C_{*}(A)|\simeq|A\otimes_{A\otimes A^{\rm op}}C_{*}(A)|.

Thus the geometric realization of A⊗A⊗AopC∗​(A)A\otimes_{A\otimes A^{\rm op}}C_{*}(A) calculates the trace 𝒯​r​(A)\mathcal{T}r(A).

We write 𝐍∗c​y​c​(A)\mathbf{N}^{cyc}_{*}(A) for the simplicial object A⊗A⊗AopC∗​(A)A\otimes_{A\otimes A^{\rm op}}C_{*}(A) and refer to it as the Hochschild chain complex. Since AA is free as a right AA-module, the terms of the simplicial object C∗​(A)C_{*}(A) are free as AA-bimodules. Thus we can evaluate the terms of the Hochschild chain complex

𝐍nc​y​c​(A)=A⊗A⊗AopCn​(A)≃A⊗A⊗AopA⊗n+2≃A⊗n+1\mathbf{N}^{cyc}_{n}(A)=A\otimes_{A\otimes A^{\rm op}}C_{n}(A)\simeq A\otimes_{A\otimes A^{\rm op}}A^{\otimes n+2}\simeq A^{\otimes n+1}

In particular, there are equivalences 𝐍0c​y​c​(A)≃A\mathbf{N}^{cyc}_{0}(A)\simeq A and 𝐍1c​y​c​(A)≃A⊗A\mathbf{N}^{cyc}_{1}(A)\simeq A\otimes A, and the two simplicial maps A⊗A→AA\otimes A\rightarrow A are the multiplication and the opposite multiplication of AA.

Similarly, recall that the center 𝒵⁡(A)\mathcal{Z}(A) is defined by the endomorphisms ℰ​n​dA⊗Aop​(A){\mathcal{E}nd}_{A\otimes A^{\rm op}}(A). Since morphisms take colimits in the domain to limits, in particular geometric realizations to totalizations, we calculate

𝒵⁡(A)=ℰ​n​dA⊗Aop​(A)≃ℋ​o​mA⊗Ao​p​(|C∗​(A)|,A)≃|ℋ​o​mA⊗Ao​p​(C∗​(A),A)|\mathcal{Z}(A)={\mathcal{E}nd}_{A\otimes A^{\rm op}}(A)\simeq{\mathcal{H}om}_{A\otimes A^{op}}(|C_{*}(A)|,A)\simeq|{\mathcal{H}om}_{A\otimes A^{op}}(C_{*}(A),A)|

Thus the totalization of ℋ​o​mA⊗Ao​p​(C∗​(A),A){\mathcal{H}om}_{A\otimes A^{op}}(C_{*}(A),A) calculates the center 𝒵⁡(A)\mathcal{Z}(A).

We write 𝐍c​y​c∗​(A)\mathbf{N}_{cyc}^{*}(A) for the cosimplicial object ℋ​o​mA⊗Ao​p​(C∗​(A),A){\mathcal{H}om}_{A\otimes A^{op}}(C_{*}(A),A) and refer to it as the Hochschild cochain complex. As before, we can evaluate the terms of the Hochschild cochain complex

𝐍c​y​cn​(A)=ℋ​o​mA⊗Ao​p​(Cn​(A),A)≃ℋ​o​mA⊗Ao​p​(A⊗n+2,A)≃ℋ​o​m​(A⊗n,A).\mathbf{N}_{cyc}^{n}(A)={\mathcal{H}om}_{A\otimes A^{op}}(C_{n}(A),A)\simeq{\mathcal{H}om}_{A\otimes A^{op}}(A^{\otimes n+2},A)\simeq{\mathcal{H}om}(A^{\otimes n},A).

In particular, there are equivalences 𝐍c​y​c0​(A)≃A\mathbf{N}_{cyc}^{0}(A)\simeq A and 𝐍c​y​c1​(A)≃ℋ​o​m​(A,A)\mathbf{N}_{cyc}^{1}(A)\simeq{\mathcal{H}om}(A,A), and the two cosimplicial maps A→ℋ​o​m​(A,A)A\to{\mathcal{H}om}(A,A) are induced by the left and right multiplication of AA.

5.1.2. Centers and traces for monoidal ∞\infty-categories

We will apply the above constructions in the following setting. We will always take 𝒮\mathcal{S} to be the ∞\infty-category 𝒫​rL{\mathcal{P}r}^{\rm L} of presentable ∞\infty-categories (with morphisms left adjoints). Then a monoidal presentable ∞\infty-category 𝒞\mathcal{C} is an associative algebra object in 𝒫​rL\mathcal{P}r^{\rm L}. Thus we have the notion of its center (or Hochschild cohomology category) 𝒵⁡(𝒞)=Fun𝒞⊗𝒞op⁡(𝒞,𝒞)∈𝒫​rL\mathcal{Z}(\mathcal{C})=\Fun_{\mathcal{C}\otimes\mathcal{C}^{\rm op}}(\mathcal{C},\mathcal{C})\in\mathcal{P}r^{\rm L}, and its trace (or Hochschild homology category) 𝒯​r​(𝒞)=𝒞⊗𝒞⊗𝒞op𝒞∈𝒫​rL\mathcal{T}r(\mathcal{C})=\mathcal{C}\otimes_{\mathcal{C}\otimes\mathcal{C}^{\rm op}}\mathcal{C}\in\mathcal{P}r^{\rm L}.

Now we will specialize further to a geometric setting. Let XX be a perfect stack, and take 𝒞\mathcal{C} to be the presentable stable ∞\infty-category QC⁡(X)\qc(X) equipped with its (symmetric) monoidal tensor product. To calculate the center and trace of QC⁡(X)\qc(X), we introduce the loop space

ℒ​X=Map⁡(S1,X)≃X×X×XX\mathcal{L}X=\Map(S^{1},X)\simeq X\times_{X\times X}X

where the fiber product is along two copies of the diagonal map.

0NYC

Corollary 5.2. Let XX be a perfect stack, and equip QC⁡(X)\qc(X) with its (symmetric) monoidal algebra structure given by tensor product. Then there are canonical equivalences (of symmetric monoidal) ∞\infty-categories

QC⁡(ℒ​X)≃𝒵⁡(QC⁡(X))≃𝒯​r​(QC⁡(X))\qc(\mathcal{L}X)\simeq\mathcal{Z}(\qc(X))\simeq\mathcal{T}r(\qc(X))
0NYD

Proof. By Theorem 4.7, we know that 𝒯​r​(QC⁡(X))\mathcal{T}r(\qc(X)), which is a tensor product, is also calculated by a fiber product

𝒯​r​(QC⁡(X))≃QC⁡(X×X×XX).\mathcal{T}r(\qc(X))\simeq\qc(X\times_{X\times X}X).

On the other hand, by Corollary 4.10, we know that 𝒵⁡(QC⁡(X))\mathcal{Z}(\qc(X)), which consists of functors, is also calculated by a tensor product

𝒵⁡(QC⁡(X))≃𝒯​r​(QC⁡(X)).\mathcal{Z}(\qc(X))\simeq\mathcal{T}r(\qc(X)).

∎

5.2. Centers of convolution categories

Let p:X→Yp:X\to Y be a map of perfect stacks satisfying descent. Consider the convolution diagram

X×YX×YX\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces X\times_{Y}X\times_{Y}X}p12\scriptstyle{p_{12}}p23\scriptstyle{p_{23}}p13\scriptstyle{p_{13}}X×YX\textstyle{X\times_{Y}X}X×YX\textstyle{X\times_{Y}X}X×YX\textstyle{X\times_{Y}X}

Equip QC⁡(X×YX)\qc(X\times_{Y}X) with the monoidal product defined by convolution

M⋆N=p13∗(p12∗(M)⊗p23∗(N)).M\star N=p_{13*}(p_{12}^{*}(M)\otimes p_{23}^{*}(N)).

By Theorem 4.14, we have a monoidal equivalence

QC⁡(X×YX)≃FunY⁡(QC⁡(X),QC⁡(X)).\qc(X\times_{Y}X)\simeq\Fun_{Y}(\qc(X),\qc(X)).

Consider the fundamental correspondence

ℒ​Y=Y×Y×YY\textstyle{\mathcal{L}Y=Y\times_{Y\times Y}Y}ℒ​Y×YX=X×X×YX\textstyle{\mathcal{L}Y\times_{Y}X=X\times_{X\times Y}X\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π\scriptstyle{\pi}δ\scriptstyle{\delta}X×YX.\textstyle{X\times_{Y}X.}

where the maps are defined by the formulas

π=idℒ​Y×idYp=p×p×idYpδ=idX×πYidX.\pi={\rm id}_{\mathcal{L}Y}\times_{{\rm id}_{Y}}p=p\times_{p\times{\rm id}_{Y}}p\qquad\delta={\rm id}_{X}\times_{\pi_{Y}}{\rm id}_{X}.

where πY:X×Y→Y\pi_{Y}:X\times Y\to Y is the obvious projection.

Passing to sheaves, we obtain a diagram

QC⁡(ℒ​Y)\textstyle{\qc(\mathcal{L}Y)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π∗\scriptstyle{\pi^{*}}QC⁡(ℒ​Y×YX)\textstyle{\qc(\mathcal{L}Y\times_{Y}X)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}δ∗\scriptstyle{\delta_{*}}QC⁡(X×YX)\textstyle{\qc(X\times_{Y}X)}

which by Theorem 4.14 admits the interpretation

FunY×Y⁡(QC⁡(Y),QC⁡(Y))\textstyle{\Fun_{Y\times Y}(\qc(Y),\qc(Y))\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π∗\scriptstyle{\pi^{*}}FunX×Y⁡(QC⁡(X),QC⁡(X))\textstyle{\Fun_{X\times Y}(\qc(X),\qc(X))\ignorespaces\ignorespaces\ignorespaces\ignorespaces}δ∗\scriptstyle{\delta_{*}}FunY⁡(QC⁡(X),QC⁡(X)).\textstyle{\Fun_{Y}(\qc(X),\qc(X)).}

where π∗\pi^{*} is the QC⁡(X)\qc(X)-linear induction, and δ∗\delta_{*} forgets the QC⁡(X)\qc(X)-linear structure.

The aim of this section is to prove the following.

0NYE

Theorem 5.3. Suppose p:X→Yp:X\to Y is a map of perfect stacks satisfying descent. Then there is a canonical equivalence

𝒵⁡(QC⁡(X×YX))≃QC⁡(ℒ​Y)\mathcal{Z}(\qc(X\times_{Y}X))\simeq\qc(\mathcal{L}Y)

such that the forgetful functor 𝔷:𝒵⁡(QC⁡(X×YX))→QC⁡(X×YX)\mathfrak{z}:\mathcal{Z}(\qc(X\times_{Y}X))\to\qc(X\times_{Y}X) is given by the correspondence δ∗​π∗:QC⁡(ℒ​Y)→QC⁡(X×YX)\delta_{*}\pi^{*}:\qc(\mathcal{L}Y)\to\qc(X\times_{Y}X).

The proof occupies the remainder of this section. We break up the argument into a general discussion and then its specific application.

At the end of the section, we also explain an analogous description of traces, conditional on a still to be developed version of Grothendieck duality in the derived setting. Namely, assuming further that p:X→Yp:X\to Y is proper with invertible dualizing sheaf and Grothendieck duality holds, we explain how to deduce an expected canonical equivalence

𝒯​r​(QC⁡(X×YX))≃QC⁡(ℒ​Y)\mathcal{T}r(\qc(X\times_{Y}X))\simeq\qc(\mathcal{L}Y)

such that the trace 𝔱​𝔯:QC⁡(X×YX)→𝒯​r​(QC⁡(X×YX))\mathfrak{tr}:\qc(X\times_{Y}X)\to\mathcal{T}r(\qc(X\times_{Y}X)) is given by the correspondence π∗​δ∗:QC⁡(X×YX)→QC⁡(ℒ​Y)\pi_{*}\delta^{*}:\qc(X\times_{Y}X)\to\qc(\mathcal{L}Y).

5.2.1. Relative cyclic bar construction

For the proof of Theorem 5.3, it will be useful to introduce relative versions of the Hochschild chain and cochain complexes. In general, the setup for the construction will be a map of associative algebra objects B→AB\to A in a monoidal ∞\infty-category 𝒮\mathcal{S}. The usual Hochschild chain and cochain complexes introduced in the previous section will correspond to the case when BB is the unit 1𝒮1_{\mathcal{S}}.

Consider the adjunction

ModB⊗Aop​(𝒮)\textstyle{\mathrm{Mod}_{B\otimes A^{\rm op}}(\mathcal{S})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}F\scriptstyle{F}ModA⊗Aop​(𝒮)\textstyle{\mathrm{Mod}_{A\otimes A^{\rm op}}(\mathcal{S})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G\scriptstyle{G}

where F(−)=A⊗B−F(-)=A\otimes_{B}- is the induction, and GG is the forgetful functor from AA-bimodules to B⊗AopB\otimes A^{\rm op}-modules. Using the comonad S≃F​GS\simeq FG, we obtain a simplicial resolution C∗B​(A)C^{B}_{*}(A) of the AA-bimodule AA with terms

Cn−1B(A)≃A⊗B⊗⋯⊗BA, with n+1 terms.C^{B}_{n-1}(A)\simeq A\otimes_{B}\otimes\cdots\otimes_{B}A,\quad\mbox{ with $n+1$ terms.}

To reduce the notation, we will denote the above expression by AB⊗n+1A_{B}^{\otimes n+1}.

As before, the geometric realization of A⊗A⊗AopC∗B​(A)A\otimes_{A\otimes A^{\rm op}}C^{B}_{*}(A) calculates the trace 𝒯​r​(A)\mathcal{T}r(A), and the totalization of ℋ​o​mA⊗Ao​p​(C∗B​(A),A){\mathcal{H}om}_{A\otimes A^{op}}(C^{B}_{*}(A),A) calculates the center 𝒵⁡(A)\mathcal{Z}(A). We write 𝐍∗B​(A)\mathbf{N}^{B}_{*}(A) for the simplicial object A⊗A⊗AopC∗B​(A)A\otimes_{A\otimes A^{\rm op}}C^{B}_{*}(A) and refer to it as the relative Hochschild chain complex. Similarly, we write 𝐍B∗​(A)\mathbf{N}_{B}^{*}(A) for the cosimplicial object ℋ​o​mA⊗Ao​p​(C∗B​(A),A){\mathcal{H}om}_{A\otimes A^{op}}(C^{B}_{*}(A),A) and refer to it as the relative Hochschild cochain complex.

Continuing as before, we can evaluate the terms of the relative Hochschild chain complex

𝐍nB​(A)=A⊗A⊗AopCnB​(A)≃A⊗A⊗AopAB⊗n+2≃B⊗B⊗BopAB⊗n+1\mathbf{N}^{B}_{n}(A)=A\otimes_{A\otimes A^{\rm op}}C^{B}_{n}(A)\simeq A\otimes_{A\otimes A^{\rm op}}A_{B}^{\otimes n+2}\simeq B\otimes_{B\otimes B^{\rm op}}A_{B}^{\otimes n+1}

Similarly, we can evaluate the terms of the relative Hochschild cochain complex

𝐍Bn​(A)=ℋ​o​mA⊗Ao​p​(CnB​(A),A)≃ℋ​o​mA⊗Ao​p​(AB⊗n+2,A)≃ℋ​o​mB⊗Bop​(AB⊗n+1,B).\mathbf{N}_{B}^{n}(A)={\mathcal{H}om}_{A\otimes A^{op}}(C^{B}_{n}(A),A)\simeq{\mathcal{H}om}_{A\otimes A^{op}}(A_{B}^{\otimes n+2},A)\simeq{\mathcal{H}om}_{B\otimes B^{\rm op}}(A_{B}^{\otimes n+1},B).

5.2.2. Proof of Theorem 5.3

Now we will apply the preceding formalism to calculate the center of the monoidal ∞\infty-category QC⁡(X×YX)\qc(X\times_{Y}X). Recall that our aim is to show that there is a canonical equivalence

𝒵⁡(QC⁡(X×YX))≃QC⁡(ℒ​Y).\mathcal{Z}(\qc(X\times_{Y}X))\simeq\qc(\mathcal{L}Y).

where ℒ​Y\mathcal{L}Y is the loop space of YY.

Consider the symmetric monoidal ∞\infty-category QC⁡(X)\qc(X), together with the monoidal functor

Δ∗:QC⁡(X)→QC⁡(X×YX)\Delta_{*}:\qc(X)\to\qc(X\times_{Y}X)

obtained via pushforward along the relative diagonal Δ:X→X×YX\Delta:X\to X\times_{Y}X.

Set A=QC⁡(X×YX)A=\qc(X\times_{Y}X), and B=QC⁡(X)B=\qc(X). By the preceding discussion, the center 𝒵⁡(A)\mathcal{Z}(A) is the limit of the relative Hochschild cochain complex 𝐍B∗​(A)\mathbf{N}^{*}_{B}(A). Furthermore, its terms can be calculated

𝐍Bn​(A)≃ℋ​o​mB⊗Bop​(AB⊗n+1,B).\mathbf{N}_{B}^{n}(A)\simeq{\mathcal{H}om}_{B\otimes B^{\rm op}}(A_{B}^{\otimes n+1},B).

Applying the results of Section 4, we can rewrite each term in the form

𝐍Bn(A)≃QC(ℒY×YX×Y⋯×YX), with n+1 copies of X.\mathbf{N}_{B}^{n}(A)\simeq\qc(\mathcal{L}Y\times_{Y}X\times_{Y}\cdots\times_{Y}X),\quad\mbox{ with $n+1$ copies of $X$.}

Here we have used the elementary identification

ℒY×YX×Y⋯×YX≃X×X×X((X×YX)×X⋯×X(X×YX))\mathcal{L}Y\times_{Y}X\times_{Y}\cdots\times_{Y}X\simeq X\times_{X\times X}((X\times_{Y}X)\times_{X}\cdots\times_{X}(X\times_{Y}X))

where the left hand side has n+1n+1 copies of XX, and the right hand side has n+1n+1 copies of X×YXX\times_{Y}X.

We conclude that the terms of 𝐍B∗​(A)\mathbf{N}_{B}^{*}(A) are nothing more than the terms of the cosimplicial ∞\infty-category obtained by applying QC⁡(−)\qc(-) to the C̆ech simplicial stack induced by the map

p~:ℒ​Y×YX→ℒ​Y\tilde{p}:\mathcal{L}Y\times_{Y}X\to\mathcal{L}Y

obtained by base change from the original map p:X→Yp:X\to Y. It is straightforward to check that under this identification the coboundary maps are given by the usual C̆ech pullbacks. By assumption, pp satisfies descent, hence p~\tilde{p} satisfies descent, and thus the totalization lim𝐍B∗​(A)\lim\mathbf{N}_{B}^{*}(A) also calculates the ∞\infty-category QC⁡(ℒ​Y)\qc(\mathcal{L}Y).

Finally, note that under this identification, the composition δ∗​π∗:QC⁡(ℒ​Y)→QC⁡(X×YX)\delta_{*}\pi^{*}:\qc(\mathcal{L}Y)\to\qc(X\times_{Y}X) corresponds to the composition

QC⁡(ℒ​Y)≃lim𝐍B∗​(A)→𝐍B0​(A)→𝐍c​y​c0​(A)≃QC⁡(X×YX)\qc(\mathcal{L}Y)\simeq\lim\mathbf{N}_{B}^{*}(A)\to\mathbf{N}_{B}^{0}(A)\to\mathbf{N}_{cyc}^{0}(A)\simeq\qc(X\times_{Y}X)

which is precisely the central functor 𝔷\mathfrak{z}. This concludes the proof of Theorem 5.3.

5.2.3. Traces and Grothendieck duality

Finally, we explain here an analogous description of traces, conditional on a still to be developed version of Grothendieck duality in the derived setting. Namely, assuming further that p:X→Yp:X\to Y is proper with invertible dualizing sheaf and Grothendieck duality holds, we explain how to deduce an expected canonical equivalence

𝒯​r​(QC⁡(X×YX))≃QC⁡(ℒ​Y)\mathcal{T}r(\qc(X\times_{Y}X))\simeq\qc(\mathcal{L}Y)

such that the trace 𝔱​𝔯:QC⁡(X×YX)→𝒯​r​(QC⁡(X×YX))\mathfrak{tr}:\qc(X\times_{Y}X)\to\mathcal{T}r(\qc(X\times_{Y}X)) is given by the correspondence π∗​δ∗:QC⁡(X×YX)→QC⁡(ℒ​Y)\pi_{*}\delta^{*}:\qc(X\times_{Y}X)\to\qc(\mathcal{L}Y).

We continue with the notation from the proof of Theorem 5.3 and the preceding sections. We will show that the geometric realization colim⁡𝐍∗B​(A)\colim\mathbf{N}^{B}_{*}(A) of the relative Hochschild chain complex also calculates the ∞\infty-category QC⁡(ℒ​Y)\qc(\mathcal{L}Y). As before, applying the results of Section 4, we can rewrite the terms of 𝐍∗B​(A)\mathbf{N}^{B}_{*}(A) in the form

𝐍nB(A)≃QC(ℒY×YX×Y⋯×YX) with n+1 copies of X.\mathbf{N}^{B}_{n}(A)\simeq\qc(\mathcal{L}Y\times_{Y}X\times_{Y}\cdots\times_{Y}X)\quad\mbox{ with $n+1$ copies of $X$.}

Furthermore, it is straightforward to check that under this identification the boundary maps of 𝐍∗B​(A)\mathbf{N}^{B}_{*}(A) are given by the pushforwards 𝔭n∗\mathfrak{p}_{n*} which are right adjoints to the usual C̆ech pullbacks 𝔭n∗\mathfrak{p}_{n}^{*}.

To reduce notation, set Xn=X×Y⋯×YXX_{n}=X\times_{Y}\cdots\times_{Y}X with n+1n+1 copies of XX.

Now suppose that p:X→Yp:X\to Y is proper and has an invertible dualizing complex (Gorenstein). Then we expect Grothendieck duality to hold in the following form: the pushforwards 𝔭n∗\mathfrak{p}_{n*} are also left adjoints to the pullbacks

𝔭n!(−)≃𝔭n∗(−⊗ωℒ​Y×YXn−1/Y−1)⊗ωℒ​Y×YXn/Y,\mathfrak{p}_{n}^{!}(-)\simeq\mathfrak{p}_{n}^{*}(-\otimes\omega^{-1}_{\mathcal{L}Y\times_{Y}X_{n-1}/Y})\otimes\omega_{\mathcal{L}Y\times_{Y}X_{n}/Y},

where ωℒ​Y×YXn/Y\omega_{\mathcal{L}Y\times_{Y}X_{n}/Y} denotes the relative dualizing sheaf of ℒ​Y×YXn→Y\mathcal{L}Y\times_{Y}X_{n}\to Y. Under this assumption, we find that the limit QC⁡(ℒ​Y)\qc(\mathcal{L}Y) of the cosimplicial ∞\infty-category (QC⁡(ℒ​Y×YXn),𝔭n∗)(\qc(\mathcal{L}Y\times_{Y}X_{n}),\mathfrak{p}_{n}^{*}) admits the following alternative description.

First, we can identify the cosimplicial ∞\infty-category (QC⁡(ℒ​Y×YXn),𝔭n∗)(\qc(\mathcal{L}Y\times_{Y}X_{n}),\mathfrak{p}_{n}^{*}) with the cosimplicial ∞\infty-category (QC(ℒY×YXn,𝔭n!)(\qc(\mathcal{L}Y\times_{Y}X_{n},\mathfrak{p}_{n}^{!}) via tensoring by the inverse of the relative dualizing sheaf ωℒ​Y×YXn/Y\omega_{\mathcal{L}Y\times_{Y}X_{n}/Y} on each simplex. In particular, we obtain an identification of their limits.

Second, we can consider the cosimplicial ∞\infty-category (QC(ℒY×YXn),𝔭n!)(\qc(\mathcal{L}Y\times_{Y}X_{n}),\mathfrak{p}_{n}^{!}) as a diagram in the ∞\infty-category 𝒫​rR\mathcal{P}r^{\rm R} of presentable ∞\infty-categories (with morphisms right adjoints). By [L2, Theorem 5.5.3.18], the calculation of the limit of the diagram does not depend on this choice of context. Then we can pass to the opposite ∞\infty-category 𝒫​rL\mathcal{P}r^{\rm L} of presentable ∞\infty-categories (with morphisms left adjoints). To calculate a limit in 𝒫​rR\mathcal{P}r^{\rm R} is the same as to calculate a colimit in 𝒫​rL\mathcal{P}r^{\rm L}. But we have seen that the trace 𝒯​r​(ℋ)\mathcal{T}r(\mathcal{H}) is precisely the colimit of the dual simplicial diagram (QC(ℒY×YXn),𝔭n∗)(\qc(\mathcal{L}Y\times_{Y}X_{n}),\mathfrak{p}_{n*}). Thus we conclude that the geometric realization colim⁡𝐍∗B​(A)\colim\mathbf{N}_{*}^{B}(A) also calculates the ∞\infty-category QC⁡(ℒ​Y)\qc(\mathcal{L}Y).

Finally, note that under this identification, the composition π∗​δ∗:QC⁡(X×YX)→QC⁡(ℒ​Y)\pi_{*}\delta^{*}:\qc(X\times_{Y}X)\to\qc(\mathcal{L}Y) corresponds to the composition

QC⁡(X×YX)≃𝐍0c​y​c​(A)→𝐍0B​(A)→colim⁡𝐍∗c​y​c​(A)≃QC⁡(ℒ​Y)\qc(X\times_{Y}X)\simeq\mathbf{N}_{0}^{cyc}(A)\to\mathbf{N}_{0}^{B}(A)\to\colim\mathbf{N}_{*}^{cyc}(A)\simeq\qc(\mathcal{L}Y)

which is precisely the trace 𝔱​𝔯\mathfrak{tr}.

5.3. Higher centers

Unlike in classical algebra, for an algebra object in an ∞\infty-category, commutativity is an additional structure rather than a property. More precisely, the forgetful functor from ℰ∞\mathcal{E}_{\infty}-algebras to ℰ1\mathcal{E}_{1}-algebras is conservative but not fully faithful. Given an ℰ∞\mathcal{E}_{\infty}-algebra AA in a symmetric monoidal ∞\infty-category 𝒮\mathcal{S}, the center 𝒵⁡(A)\mathcal{Z}(A) that we have studied to this point does not involve the commutativity of AA. More precisely, it only depends upon the ℰ1\mathcal{E}_{1}-algebra underlying AA.

In this section, we discuss higher versions of the center where we forget less commutativity. For a perfect stack XX, we calculate the ℰn\mathcal{E}_{n}-center of the ℰn\mathcal{E}_{n}-category underlying the ℰ∞\mathcal{E}_{\infty}-category QC⁡(X)\qc(X). A detailed treatment of the foundations of the subject may be found in Chapter 2 of [F1]. Here we summarize only what is required for our consideration of the ℰn\mathcal{E}_{n}-center of QC⁡(X)\qc(X).

0NYF

Remark 5.4. As noted in the introduction, after the completion of this manuscript, the paper [L5] was revised to include a thorough treatment of ∞\infty-categorical operads and their algebras, and the paper [L7] treats in great detail the specific case of the ℰn\mathcal{E}_{n}-operads. We refer the reader to these preprints for further details.

Let FF be a topological operad. We define a topological category ℱ\mathcal{F} with objects finite pointed sets and morphism spaces given by

Mapℱ(J∗,I∗)=∐f:J∗→I∗∏IF(f−1{i}).\Map_{\mathcal{F}}(J_{*},I_{*})=\coprod_{f:J_{*}\rightarrow I_{*}}\prod_{I}F(f^{-1}\{i\}).

We then obtain an ∞\infty-category, also denoted by ℱ\mathcal{F}, by applying the singular functor to the mapping spaces to get a simplicial category and then taking the simplicial nerve.

0NYG

Definition 5.5 ([F1]). An ℱ\mathcal{F}-monoidal structure on an ∞\infty-category 𝒞\mathcal{C} consists of a functor p:ℱ→Cat∞p:\mathcal{F}\rightarrow{\rm Cat}_{\infty} with an identification 𝒞≃p⁡(1∗)\mathcal{C}\simeq p(1_{*}) such that the natural maps p⁡(J∗)→∏Jp⁡(1∗)p(J_{*})\rightarrow\prod_{J}p(1_{*}) resulting from a choice of a point x∈F⁡(J)x\in F(J) is an equivalence.

We will refer to the ∞\infty-category 𝒞\mathcal{C} equipped with an ℱ\mathcal{F}-monoidal structure as an ℱ\mathcal{F}-category. This construction will be of particular interest to us when ℱ\mathcal{F} is the little nn-disks operad ℰn\mathcal{E}_{n}.

To discuss Hochschild cohomology, we must next introduce the notion of operadic modules.

To this end, let Fin∗{{\rm Fin}_{*}} be the category of finite based sets. Let Fin+{\rm Fin}_{+} be the category of “doubly-based sets” with objects finite based sets I∗I_{*} and (I∐+)∗(I\amalg+)_{*}, and morphisms α\alpha of the underlying based sets such that +∈α−1(+)+\in\alpha^{-1}(+), and either α(+)=+\alpha(+)=+ or α(+)=∗\alpha(+)=*.

Given a topological operad FF, recall the ∞\infty-category ℱ\mathcal{F} introduced above. We also define the ∞\infty-category ℱ+\mathcal{F}_{+} to be the fiber product of ∞\infty-categories

ℱ+=ℱ×Fin∗Fin+.\mathcal{F}_{+}=\mathcal{F}\times_{{\rm Fin}_{*}}{\rm Fin}_{+}.
0NYH

Definition 5.6. Let 𝒞\mathcal{C} be an ℱ\mathcal{F}-category. An ℱ\mathcal{F}-𝒞\mathcal{C}-module structure on an ∞\infty-category ℳ\mathcal{M} is a functor q:ℱ+→Cat∞q:\mathcal{F}_{+}\rightarrow{\rm Cat}_{\infty} extending the ℱ\mathcal{F}-monoidal structure on 𝒞\mathcal{C}, together with an identification q⁡(+)≃ℳq(+)\simeq\mathcal{M} such that the natural map q((I∐+)∗)→𝒞I×ℳq((I\amalg+)_{*})\rightarrow\mathcal{C}^{I}\times\mathcal{M} is an equivalence for any II.

0NYI

Example 5.7. When ℱ\mathcal{F} is the ℰ1\mathcal{E}_{1} operad, the notion of an ℱ\mathcal{F}-𝒞\mathcal{C}-module coincides with that of a 𝒞\mathcal{C}-bimodule: it is an ∞\infty-category left and right tensored over 𝒞\mathcal{C}. When ℱ\mathcal{F} is the ℰ∞\mathcal{E}_{\infty} operad, the notion coincides with that of a left (or equivalently right) module.

There is a similar definition of an ℱ\mathcal{F}-algebra and an ℱ\mathcal{F}-AA-module in a symmetric monoidal or ℱ\mathcal{F}-monoidal ∞\infty-category ℳ\mathcal{M} generalizing the definition given above. This requires the notion of an ℱ\mathcal{F}-lax monoidal functor (see [F1, Chapter 2, Definition 3.10]). The simplification of the previous definition is available because Cat∞{\rm Cat}_{\infty} is equipped with the Cartesian monoidal structure. We will avail ourselves of this greater generality in the following definition, although the only case that will concern us in the following is when ℳ\mathcal{M} is either Cat∞{\rm Cat}_{\infty} or 𝒫​rL\mathcal{P}r^{\rm L}.

Now let ℳ\mathcal{M} be a presentable symmetric monoidal ∞\infty-category whose monoidal structure distributes over colimits. Let AA be an ℱ\mathcal{F}-algebra in ℳ\mathcal{M}, and let ModAℱ​(ℳ)\mathrm{Mod}_{A}^{\mathcal{F}}(\mathcal{M}) be the ∞\infty-category of ℱ\mathcal{F}-AA-modules in ℳ\mathcal{M} (see [F1, Chapter 2, Definition 4.3]). Under the above assumptions, the ∞\infty-category ModAℱ​(ℳ)\mathrm{Mod}_{A}^{\mathcal{F}}(\mathcal{M}) is naturally tensored over ℳ\mathcal{M}.

0NYJ

Definition 5.8. For an ℱ\mathcal{F}-algebra AA in ℳ\mathcal{M}, we define the ℱ\mathcal{F}-Hochschild cohomology

HHℱ∗⁡(A)=ℋ​o​mModAℱ​(A,A)\hh^{*}_{\mathcal{F}}(A)={\mathcal{H}om}_{\mathrm{Mod}_{A}^{\mathcal{F}}}(A,A)

to be the object of ℳ\mathcal{M} representing the endomorphisms of AA as an object of ModAℱ​(ℳ)\mathrm{Mod}_{A}^{\mathcal{F}}(\mathcal{M}).

In particular, when ℳ=𝒫​rL\mathcal{M}=\mathcal{P}r^{\rm L}, the ℱ\mathcal{F}-Hochschild cohomology of an ℱ\mathcal{F}-category 𝒞\mathcal{C} is the ∞\infty-category of ℱ\mathcal{F}-𝒞\mathcal{C}-module functors

HHℱ∗⁡(𝒞)=FunMod𝒞ℱ⁡(𝒞,𝒞).\hh^{*}_{\mathcal{F}}(\mathcal{C})=\Fun_{\mathrm{Mod}_{\mathcal{C}}^{\mathcal{F}}}(\mathcal{C},\mathcal{C}).

We now specialize to the case where ℱ\mathcal{F} is the ℰn\mathcal{E}_{n}-operad. Intuitively, an ℰn\mathcal{E}_{n}-algebra structure on an object AA is equivalent to a family of associative algebra structures on AA parameterized by Sn−1S^{n-1} such that antipodal points are associated to opposite multiplications on AA. An ℰn\mathcal{E}_{n}-AA-module structure on MM admits a similar intuitive interpretation as a family of compatible left AA-module structures on MM parameterized by Sn−1S^{n-1}. This intuition leads to the following (to appear in [F2], see also [L7]).

0NYK

Proposition 5.9 ([F2]). Let 𝒞\mathcal{C} be a presentable symmetric monoidal ∞\infty-category whose monoidal structure distributes over colimits.

To an ℱ\mathcal{F}-algebra AA in 𝒞\mathcal{C} there is functorially assigned associative algebra UAU_{A} such that there is a canonical equivalence ModAℱ​(𝒞)≃ModUA​(𝒞)\mathrm{Mod}_{A}^{\mathcal{F}}(\mathcal{C})\simeq\mathrm{Mod}_{U_{A}}(\mathcal{C}) between ℱ\mathcal{F}-AA-modules and left UAU_{A}-modules.

If ℱ\mathcal{F} is the ℰn\mathcal{E}_{n} operad, and the ℰn\mathcal{E}_{n}-algebra structure on AA is obtained by restriction from an ℰ∞\mathcal{E}_{\infty}-algebra structure, then there is a canonical equivalence of associative algebras UA≃Sn−1⊗AU_{A}\simeq S^{n-1}\otimes A.

For n=1n=1, the proposition reduces to the familiar statement that for an ℰ∞\mathcal{E}_{\infty}-algebra AA, an A⊗AopA\otimes A^{\rm op}-module structure (in the form of an ℰ1\mathcal{E}_{1}-AA-module structure) is equivalent to an A⊗AA\otimes A-module structure (in the form of a left UAU_{A}-module structure).

For our current purposes, one can interpret the proposition as furnishing the definition of an ℰn\mathcal{E}_{n}-AA-module. Namely, the reader uncomfortable with the abstractions can take left Sn−1⊗AS^{n-1}\otimes A-modules as the definition of ℰn\mathcal{E}_{n}-AA-modules

0NYL

Example 5.10. Let 𝒞\mathcal{C} be an ℰ1\mathcal{E}_{1}-algebra in 𝒫​rL\mathcal{P}r^{\rm L} (so 𝒞\mathcal{C} is a presentable monoidal ∞\infty-category whose monoidal structure distributes over colimits). Then left modules for the monoidal ∞\infty-category U𝒞U_{\mathcal{C}} are equivalent to 𝒞\mathcal{C}-bimodules. In particular, we have an equivalence U𝒞≃𝒞⊗𝒞opU_{\mathcal{C}}\simeq\mathcal{C}\otimes\mathcal{C}^{\rm op}, where here 𝒞op\mathcal{C}^{\rm op} denotes the ∞\infty-category 𝒞\mathcal{C} equipped with the opposite monoidal structure. As a consequence, we see that in this case, the preceding general definition of ℱ\mathcal{F}-Hochschild cohomology recaptures the notion of the Drinfeld center introduced earlier.

Let AA be an ℰ∞\mathcal{E}_{\infty}-algebra and UAU_{A} be as above. We have a companion definition of ℰn\mathcal{E}_{n}-Hochschild homology.

0NYM

Definition 5.11. For an ℰ∞\mathcal{E}_{\infty}-algebra AA, we define the ℰn\mathcal{E}_{n}-Hochschild homology

HH∗ℰn⁡(A)=A⊗UAA\hh_{*}^{\mathcal{E}_{n}}(A)=A\otimes_{U_{A}}A

to be the tensor product of AA with itself over the algebra UAU_{A}.

We now have the following contribution of this paper to the story.

0NYN

Corollary 5.12. For a perfect stack XX, consider the stable ∞\infty-category QC⁡(X)\qc(X) equipped with its ℰn\mathcal{E}_{n}-tensor product. Then with XSn=Map⁡(Sn,X)X^{S^{n}}=\Map(S^{n},X), there are canonical equivalences

QC⁡(XSn)≃HHℰn∗⁡(QC⁡(X))≃HH∗ℰn⁡(QC⁡(X))\qc(X^{S^{n}})\simeq\hh^{*}_{\mathcal{E}_{n}}(\qc(X))\simeq\hh_{*}^{\mathcal{E}_{n}}(\qc(X))
0NYP

Proof. The result follows from an inductive application of Theorem 4.7 and Corollary 4.12 to the Cartesian diagrams

XSn\textstyle{X^{S^{n}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}X\textstyle{X\ignorespaces\ignorespaces\ignorespaces\ignorespaces}X\textstyle{X\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XSn−1\textstyle{X^{S^{n-1}}}

where the two maps X→XSn−1X\to X^{S^{n-1}} assign to a point of XX the corresponding constant map. ∎

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

David Ben-Zvi, John Francis, David Nadler

Original source: arXiv:0805.0157v5