ScalingStacks

6. Epilogue: Topological Field Theory

For a perfect stack XX, the ∞\infty-category QC⁡(ℒ​X)\qc(\mathcal{L}X) of sheaves on its loop space carries a rich structure coming from topological field theory, generalizing the braided tensor category structure on the usual Drinfeld center and providing a categorified analogue of the Deligne conjecture on Hochschild cochains. In this section, we discuss these structures and their generalizations.

6.1. Topological Field Theory from perfect stacks

Let 2​Cob2{\rm Cob} denote the ∞\infty-category whose objects are compact oriented 11-manifolds, and whose morphisms 2​Cob​(C1,C2)2{\rm Cob}(C_{1},C_{2}) consist of the classifying spaces of oriented topological surfaces with fixed incoming and outgoing components C1,C2C_{1},C_{2}. This ∞\infty-category has a symmetric monoidal structure given by disjoint union of 1-manifolds. We will abuse notation by denoting the object consisting of the disjoint union of mm copies of S1S^{1} by mm.

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Definition 6.1. A 2-dimensional topological field theory valued in a symmetric monoidal ∞\infty-category 𝒞\mathcal{C} is a symmetric monoidal functor F:2​Cob→𝒞F:2{\rm Cob}\to\mathcal{C}.

Fix a base commutative derived ring kk.

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Definition 6.2. Let Cat∞ex{\rm Cat}_{\infty}^{\rm ex} denote the (∞,2)(\infty,2)-category of stable, presentable kk-linear ∞\infty-categories, with 1-morphisms consisting of continuous exact functors.

Note that Cat∞ex{\rm Cat}_{\infty}^{\rm ex} has a symmetric monoidal structure, the tensor product of presentable stable categories as studied in [L4, 4.2], and the unit of the monoidal structure is the ∞\infty-category of kk-modules. Since the empty 11-manifold is the unit of 2​Cob2{\rm Cob}, a topological field theory 𝒵\mathcal{Z} sends its endomorphisms, which are closed surfaces Σ\Sigma, to endomorphisms of the unit of the target ∞\infty-category 𝒞\mathcal{C}. When 𝒞=Cat∞ex\mathcal{C}={\rm Cat}_{\infty}^{\rm ex}, the unit is Modk\Mod_{k} and 𝒵⁡(Σ)\mathcal{Z}(\Sigma) is a kk-module.

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Proposition 6.3. For a perfect stack XX, there is a 2d TFT 𝒵X:2​Cob→Cat∞ex\mathcal{Z}_{X}:2{\rm Cob}\to{\rm Cat}_{\infty}^{\rm ex} with 𝒵X​(S1)=QC⁡(ℒ​X)\mathcal{Z}_{X}(S^{1})=\qc(\mathcal{L}X) and 𝒵X​(Σ)=Γ⁡(XΣ,𝒪XΣ)\mathcal{Z}_{X}(\Sigma)=\Gamma(X^{\Sigma},\mathcal{O}_{X^{\Sigma}}), for closed surfaces Σ\Sigma.

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Proof. We define 𝒵X\mathcal{Z}_{X} on objects by assigning 𝒵X​(m)=QC⁡((ℒ​X)m)\mathcal{Z}_{X}(m)=\qc((\mathcal{L}X)^{m}).

To define 𝒵X\mathcal{Z}_{X} on morphisms, observe first that since XX is perfect, (ℒ​X)m(\mathcal{L}X)^{m} is perfect, and for Σ∈2​Cob∘​(m,n)\Sigma\in 2{\rm Cob}^{\circ}(m,n), the mapping stack XΣ=Map⁡(Σ,X)X^{\Sigma}=\Map(\Sigma,X) is also perfect (special cases of Corollary 3.25). Now for each Σ∈2​Cob∘​(m,n)\Sigma\in 2{\rm Cob}^{\circ}(m,n), consider the correspondence

XΣ\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces X^{\Sigma}}(ℒ​X)m\textstyle{(\mathcal{L}X)^{m}}(ℒ​X)n\textstyle{(\mathcal{L}X)^{n}}

Since all of the stacks involved are perfect, pullback and pushforward of quasi-coherent sheaves along this correspondence defines a colimit-preserving functor

𝒵X​(Σ):QC⁡((ℒ​X)m)→QC⁡((ℒ​X)n).\mathcal{Z}_{X}(\Sigma):\qc((\mathcal{L}X)^{m})\to\qc((\mathcal{L}X)^{n}).

Thus applying this construction in families, we obtain a map of spaces

𝒵X​(m,n):2​Cob∘​(m,n)→Fun⁡(QC⁡((ℒ​X)m),QC⁡((ℒ​X)n)).\mathcal{Z}_{X}(m,n):2{\rm Cob}^{\circ}(m,n)\to\Fun(\qc((\mathcal{L}X)^{m}),\qc((\mathcal{L}X)^{n})).

Suppose now that Σ=Σ1​∐∐kS1Σ2∈2​Cob​(m,n)\Sigma=\Sigma_{1}\coprod_{\coprod_{k}{S^{1}}}\Sigma_{2}\in 2{\rm Cob}(m,n) is obtained by sewing two surfaces Σ1∈2​Cob​(m,k)\Sigma_{1}\in 2{\rm Cob}(m,k) and Σ2∈2​Cob​(k,n)\Sigma_{2}\in 2{\rm Cob}(k,n). Then we have a diagram of correspondences

XΣ\textstyle{X^{\Sigma}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XΣ1\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces X^{\Sigma_{1}}}XΣ2\textstyle{X^{\Sigma_{2}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(ℒ​X)m\textstyle{(\mathcal{L}X)^{m}}(ℒ​X)k\textstyle{(\mathcal{L}X)^{k}}(ℒ​X)n\textstyle{(\mathcal{L}X)^{n}}

Since all of the stacks involved are perfect, base change provides a canonical equivalence of functors

𝒵X​(Σ)≃𝒵X​(Σ2)∘𝒵X​(Σ1):QC⁡((ℒ​X)m)→QC⁡((ℒ​X)n).\mathcal{Z}_{X}(\Sigma)\simeq\mathcal{Z}_{X}(\Sigma_{2})\circ\mathcal{Z}_{X}(\Sigma_{1}):\qc((\mathcal{L}X)^{m})\to\qc((\mathcal{L}X)^{n}).

Similar diagrams define the higher compositions.

To complete the construction, note that 𝒵X\mathcal{Z}_{X} comes equipped with a canonical symmetric monoidal structure. Namely, by Theorem 4.7, there is a canonical equivalence

𝒵X​(m)=QC⁡((ℒ​X)m)≃QC⁡(ℒ​X)⊗m=𝒵X​(1)⊗m,\mathcal{Z}_{X}(m)=\qc((\mathcal{L}X)^{m})\simeq\qc(\mathcal{L}X)^{\otimes m}=\mathcal{Z}_{X}(1)^{\otimes m},

and it clearly extends to a symmetric monoidal structure. ∎

As an example, take X=B​GX=BG (in characteristic zero). Then 𝒵B​G​(S1)\mathcal{Z}_{BG}(S^{1}) is the ∞\infty-category of sheaves on the adjoint quotient G/G=LocG​(S1)G/G={\rm Loc}_{G}(S^{1}), while 𝒵B​G​(Σ)\mathcal{Z}_{BG}(\Sigma) is the cohomology of the structure sheaf of the moduli stack B​GΣ=LocG​(Σ)BG^{\Sigma}={\rm Loc}_{G}(\Sigma) of GG-local systems on Σ\Sigma.

More generally, the particular topological field theory operations we are considering are not sensitive to the structure of manifolds, and the same construction provides a field theory living over “bordisms” of spaces. In what follows, by a space we will mean a space homotopy equivalent to a finite simplicial set.

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Definition 6.4. Let BordSpaces{\rm Bord}_{\rm Spaces} denote the bordism (∞,1)(\infty,1)-category of spaces, with 1-morphisms from UU to VV given by spaces TU​VT_{UV} with maps U→TU​V←VU\rightarrow T_{UV}\leftarrow V, and composition of T:U→VT:U\to V and T′:V→WT^{\prime}:V\to W given by the homotopy pushout of spaces

T′∘T=T∐VT′.T^{\prime}\circ T=T\amalg_{V}T^{\prime}.

We endow BordSpaces{\rm Bord}_{\rm Spaces} with a symmetric monoidal structure given by disjoint union.

The proof of the previous proposition immediately extends to give the following:

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Proposition 6.5. For any perfect stack XX, there is a symmetric monoidal functor

SX:BordSpaces→Cat∞exS_{X}:{\rm Bord}_{\rm Spaces}\to{\rm Cat}_{\infty}^{\rm ex}

with SX​(U)=QC⁡(XU)S_{X}(U)=\qc(X^{U}) and SX(T:U→V)S_{X}(T:U\to V) the functor QC⁡(U)→QC⁡(V)\qc(U)\to\qc(V) given by pullback and pushforward along the correspondence

XU←XT→XV.X^{U}\leftarrow X^{T}\rightarrow X^{V}.

The 2d topological field theory 𝒵X\mathcal{Z}_{X} above is a categorified analogue of the 2d TFTs defined by string topology on a compact oriented manifold, or the topological B-model defined by a Calabi-Yau variety [C]. Namely, we assign to the circle the ∞\infty-category of quasi-coherent sheaves, rather than the complex of chains, on the loop space. This has the advantage that we may construct maps for arbitrary correspondences without the assumption that XX is a Calabi-Yau or satisfies Poincaré duality. On the other hand, we have gone up a level of categoricity, pushing off the problems of duality and orientation to the definition of operations between Γ⁡(XΣ,𝒪XΣ)\Gamma(X^{\Sigma},\mathcal{O}_{X^{\Sigma}}) for cobordisms between surfaces or invariants for 3-manifolds. Recall [BK] that an extended 3-dimensional topological field theory assigns a braided (in fact ribbon) category to the circle. This category must however satisfy a strong finiteness and nondegeneracy condition (modularity) coming from its extension to three-manifolds. It would be interesting to see what conditions need to be imposed on the sheaves we consider and on the stack XX in order to extend 𝒵X\mathcal{Z}_{X} in such a fashion. Note that Corollary 4.8 shows that QC⁡(X)\qc(X) for XX perfect satisfies an analogue of the Calabi-Yau or Frobenius property: namely it is self-dual as a Modk\Mod_{k}-module.

6.2. Deligne-Kontsevich conjectures for derived centers

The notion of Drinfeld center for monoidal stable categories is a categorical analogue of Hochschild cohomology of associative (or A∞A_{\infty}) algebras (or more precisely of Hochschild cochains, or its spectral analogue, topological Hochschild cohomology). In the case of algebras, Deligne’s conjecture states that the Hochschild cochain complex has the structure of an ℰ2\mathcal{E}_{2}-algebra (lifting the Gerstenhaber algebra, or H∗​(ℰ2)H_{*}(\mathcal{E}_{2})-algebra, structure on Hochschild cohomology). There is also a cyclic version of the conjecture which states that the Hochschild cochains for a Frobenius algebra possesses the further structure of a framed ℰ2\mathcal{E}_{2}, or ribbon, algebra. See [T1, K1, KS1, MS, C, KS2] for various proofs of the Deligne conjecture and [Ka, TZ] for its cyclic version. The Kontsevich conjecture (see [T2, HKV]) generalizes this picture to higher algebras, asserting that the Hochschild cochains on an ℰn\mathcal{E}_{n}-algebra have a natural ℰn+1\mathcal{E}_{n+1}-structure.

The work of Costello [C] and Kontsevich-Soibelman [KS2] explains how a strong form of the Deligne conjecture follows from the structure of topological field theory – specifically, by constructing a topological field theory 𝒵A\mathcal{Z}_{A} from an algebra AA such that 𝒵A​(S1)\mathcal{Z}_{A}(S^{1}) is the Hochschild cochain complex of AA. Observe that the configuration space of mm-tuples of circles in the disk (the mm-th space of the ℰ2\mathcal{E}_{2}-operad) maps to the space of functors 𝒵​(S1)⊗m→𝒵⁡(S1)\mathcal{Z}(S^{1})^{\otimes m}\to\mathcal{Z}(S^{1}) compatibly with

compositions.

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Proposition 6.6. In any 2d TFT 𝒵\mathcal{Z}, the object 𝒵⁡(S1)∈𝒞\mathcal{Z}(S^{1})\in\mathcal{C} is an algebra over the framed ℰ2\mathcal{E}_{2}-operad (in particular, over the ℰ2\mathcal{E}_{2}-operad).

A natural categorified analogue of the Deligne conjecture states that the Drinfeld center of a monoidal ∞\infty-category is an ℰ2\mathcal{E}_{2}-category. For dualizable and self-dual kk-linear ∞\infty-categories, one can ask if this structure comes from a natural framed ℰ2\mathcal{E}_{2}, or ribbon, structure. We observe that our identification of the Drinfeld center of QC⁡(X)\qc(X) with sheaves on the loop space, combined with the construction of the topological field theory 𝒵X\mathcal{Z}_{X}, automatically solves this conjecture in the applicable cases:

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Corollary 6.7. For XX a perfect stack, the center 𝒯​r​(QC⁡(X))≃QC⁡(ℒ​X)\mathcal{T}r(\qc(X))\simeq\qc(\mathcal{L}X) has the structure of a stable framed ℰ2\mathcal{E}_{2}-category. For a map X→YX\to Y of perfect stacks, the same holds for the center 𝒯​r​(QC⁡(X×YX))≃QC⁡(ℒ​X)\mathcal{T}r(\qc(X\times_{Y}X))\simeq\qc(\mathcal{L}X).

In fact, the same arguments prove a case of the categorified form of the Kontsevich conjecture. We consider QC⁡(XSn)\qc(X^{S^{n}}) as part of an n+1n+1-dimensional topological field theory, with operations given by cobordisms of nn-manifolds.

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Corollary 6.8. For XX a perfect stack, the ℰn\mathcal{E}_{n}-Hochschild cohomology of the stable ℰn\mathcal{E}_{n}-category QC⁡(X)\qc(X) has the structure of a stable (framed) ℰn+1\mathcal{E}_{n+1}-category.

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