ScalingStacks

3.5. Homology theories

We give the following characterization, ร  la Eilenbergโ€“Steenrod, for factorization homology; this is the central conceptual result of this paper.

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Theorem 3.24. For ๐’ฑ\mathcal{V} a symmetric monoidal โˆž\oo-category which is โŠ—\otimes-presentable, there is an equivalence

โˆซ:๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโก(๐’ฑ)\textstyle{\displaystyle\int:\Alg_{\disk_{n}^{B}}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}๐‡โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝnB,๐’ฑ):๐–พ๐—โ„n\textstyle{\mathbf{H}(\mfld_{n}^{B},\mathcal{V}):{\sf ev}_{\mathbb{R}^{n}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

between ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–ก\disk^{B}_{n}-algebras in ๐’ฑ\mathcal{V} and homology theories of BB-framed nn-manifolds with coefficients in ๐’ฑ\mathcal{V}. This equivalence is implemented by the factorization homology functor โˆซ\int and the functor of evaluation on โ„n\mathbb{R}^{n}.

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Proof. Propositionย 3.7 recognizes factorization homology as a symmetric monoidal left Kan extensions, thereby implementing the left adjoint in an adjunction

i!:๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–ก(๐’ฑ)โ‡„๐–ฅ๐—Ž๐—‡โŠ—(โ„ณโ€‹๐–ฟ๐—…๐–ฝnB,๐’ฑ):iโˆ—.i_{!}\colon\Alg_{\disk_{n}^{B}}(\mathcal{V})\rightleftarrows\Fun^{\otimes}\bigl(\mfld_{n}^{B},\mathcal{V}\bigr)\colon i^{\ast}~.

The unit of this adjunction is an equivalence because ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโ†’โ„ณโ€‹๐–ฟ๐—…๐–ฝnB\disk_{n}^{B}\rightarrow\mfld_{n}^{B} is fully faithful, and the Kan extension along a fully faithful functor restricts as the original functor. The counit of this adjunction evaluates on a symmetric monoidal functor โ„ฑ\mathcal{F} as a morphism โˆซAโ†’โ„ฑ\int\!A\rightarrow\mathcal{F}, where A=โ„ฑ|โ„nA=\mathcal{F}_{|\mathbb{R}^{n}} is the ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–ก\disk^{B}_{n}-algebra defined by the values of โ„ฑ\mathcal{F} on disjoint unions of BB-framed Euclidean nn-spaces. It remains to verify that this counit is an equivalence.

Since both โ„ฑ\mathcal{F} and โˆซA\int\!A are symmetric monoidal and agree on โ„n\mathbb{R}^{n}, the map โˆซMAโ†’โ„ฑโก(M)\int_{M}A\rightarrow\mathcal{F}(M) is an equivalence for MM isomorphic to a disjoint union of Euclidean spaces, Mโ‰…โจ†Iโ„nM\cong\bigsqcup_{I}\mathbb{R}^{n}. Using induction, we will now see that the values of โ„ฑ\mathcal{F} and โˆซA\int\!A agree on thickened spheres Skร—โ„nโˆ’kS^{k}\times\mathbb{R}^{n-k}, the base case of k=0k=0 just having been shown. In the inductive step, assume the result for Siโˆ’1ร—โ„nโˆ’i+1S^{i-1}\times\mathbb{R}^{n-i+1}. Choose a standard collar-gluing Siโ†’๐‘“[โˆ’1,1]S^{i}\xrightarrow{f}[-1,1] with Siโˆ’1=fโˆ’1โ€‹(0)โŠ‚SiS^{i-1}=f^{-1}(0)\subset S^{i} an equator. There results a collar-gluing of Siร—โ„nโˆ’iS^{i}\times\mathbb{R}^{n-i}. For โ„ฑ\mathcal{F} a homology theory, we obtain the equivalence โˆซSiร—โ„nโˆ’iAโ‰ƒโ„ฑโก(Siร—โ„nโˆ’i)\int_{S^{i}\times\mathbb{R}^{n-i}}A\simeq\mathcal{F}(S^{i}\times\mathbb{R}^{n-i}) via the intermediate equvialences

โˆซSiร—โ„nโˆ’iโ€‹Aโ‰ƒโˆซโ„โˆ’1iร—โ„nโˆ’iโ€‹Aโ€‹โจ‚โˆซSiโˆ’1ร—โ„nโˆ’i+1โ€‹Aโ€‹โˆซโ„+1iร—โ„nโˆ’iโ€‹Aโ‰ƒโ„ฑโก(โ„โˆ’1iร—โ„nโˆ’i)โ€‹โจ‚โ„ฑโก(Siโˆ’1ร—โ„nโˆ’i+1)โ€‹โ„ฑโ€‹(โ„+1iร—โ„nโˆ’i)โ‰ƒโ„ฑโก(Siร—โ„j)\underset{S^{i}\times\mathbb{R}^{n-i}}{\int}\!A\simeq\underset{\mathbb{R}_{-1}^{i}\times\mathbb{R}^{n-i}}{\int}\!A\underset{\underset{S^{i-1}\times\mathbb{R}^{n-i+1}}{\int}\negthinspace A}{\bigotimes}\ \underset{\mathbb{R}_{+1}^{i}\times\mathbb{R}^{n-i}}{\int}\!A\ \simeq\ \mathcal{F}(\mathbb{R}_{-1}^{i}\times\mathbb{R}^{n-i})\underset{\mathcal{F}(S^{i-1}\times\mathbb{R}^{n-i+1})}{\bigotimes}\mathcal{F}(\mathbb{R}_{+1}^{i}\times\mathbb{R}^{n-i})\simeq\mathcal{F}(S^{i}\times\mathbb{R}^{j})

where the first equivalence is by the โŠ—\otimes-excision property of factorization homology, the last equivalence is by the assumption that โ„ฑ\mathcal{F} is a homology theory, and the middle equivalence is by induction.

We now restrict to the case of BB-framed nn-manifolds where nn is not equal to 4. By the handlebody theory for topological manifolds ([KS] for n>5n>5, [Qu] for n=5n=5, and [Mo] for n=3n=3) all such manifolds admits a handle decomposition. We now prove the result outside dimension 4 by induction on the handle decomposition. The base case is assured. To verify the inductive step, let MM be obtained from M0M_{0} by adding a handle of index q+1q+1. Therefore MM can be expressed as a collar-gluing Mโ‰…M0โ€‹โ‹ƒSqร—โ„nโˆ’qโ€‹โ„nM\cong M_{0}\underset{S^{q}\times\mathbb{R}^{n-q}}{\bigcup}\mathbb{R}^{n}, where โ„n\mathbb{R}^{n} is an open neighborhood of the (q+1)(q+1)-handle in MM. The values โ„ฑ\mathcal{F} and โˆซA\int\!A agree on the three constituent submanifolds of MM, and they both satisfy โŠ—\otimes-excision, so the values โ„ฑโก(M)โ‰ƒโˆซMA\mathcal{F}(M)\simeq\int_{M}A are equivalent.

This leaves the case of topological 4-manifolds, which do not admit handle decompositions in general. Because both โ„ฑ\mathcal{F} and โˆซA\int_{\!}A are symmetric monoidal, we can reduce to the case that MM is connected. Now, any connected topological 4-manifold MM admits a smooth structure on the complement Mโˆ–{x}M\smallsetminus\{x\} of a point xโˆˆMx\in M, [Qu]. Consequently, Mโˆ–{x}M\smallsetminus\{x\} admits a handle decomposition, which can be constructed from any Morse function on Mโˆ–{x}M\smallsetminus\{x\}, and the preceding argument thereby implies the equivalence โ„ฑโก(Mโˆ–{x})โ‰ƒโˆซMโˆ–{x}A\mathcal{F}(M\smallsetminus\{x\})\simeq\int_{M\smallsetminus\{x\}}A. Applying the โŠ—\otimes-excision property to the collar-gluing Mโˆ–{x}โ€‹โ‹ƒSnโˆ’1ร—โ„โ€‹โ„nโ‰…MM\smallsetminus\{x\}\underset{S^{n-1}\times\mathbb{R}}{\bigcup}\mathbb{R}^{n}\cong M, since โ„ฑ\mathcal{F} and โˆซA\int\!A agree on the constituent submanifolds, we obtain the equivalence โ„ฑโก(M)โ‰ƒโˆซMA\mathcal{F}(M)\simeq\int_{M}A. Therefore every homology theory โ„ฑ\mathcal{F} for nn-manifolds is equivalent to factorization homology with coefficients in โ„ฑโก(โ„n)\mathcal{F}(\mathbb{R}^{n}).

โˆŽ

We record here this technical comparison of factorization homology with different target โˆž\oo-categories. (This result is also Propositionย 5.5.2.17 ofย [Lu2].)

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Lemma 3.25. For G:๐’ฑโ†’๐’ฑโ€ฒG:\mathcal{V}\rightarrow\mathcal{V}^{\prime} a symmetric monoidal functor between โŠ—\otimes-presentable โˆž\infty-categories whose restriction to underlying โˆž\infty-categories preserves geometric realizations, there is a canonical equivalence โˆซโˆ˜Gโ†’โ‰ƒGโˆ˜โˆซ\int\circ G\xrightarrow{\simeq}G\circ\int of functors ๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโก(๐’ฑ)โ†’๐–ฅ๐—Ž๐—‡โŠ—โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝnB,๐’ฑโ€ฒ)\Alg_{\disk_{n}^{B}}(\mathcal{V})\rightarrow\Fun^{\otimes}(\mfld_{n}^{B},\mathcal{V}^{\prime}).

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Proof. The two functors agree on disjoint unions of Euclidean spaces, so it suffices to check that Gโ€‹โˆซAG\int A is a homology theory with values in ๐’ฑโ€ฒ\mathcal{V}^{\prime}. This is immediate by the assumption on GG. โˆŽ

A result identical to Theorem 3.24 holds for topological nn-manifolds with boundary.

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Theorem 3.26. For ๐’ฑ\mathcal{V} a symmetric monoidal โˆž\oo-category which is โŠ—\otimes-presentable, and for Bโ†’๐–ก๐–ณ๐—ˆ๐—‰โก(๐—‡)B\to\BTop(n) a map of spaces, there is an equivalence between โˆž\infty-categories

โˆซ:๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡โˆ‚,๐–กโก(๐’ฑ)\textstyle{\displaystyle\int:\Alg_{\disk_{n}^{\partial,B}}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}๐‡โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝnโˆ‚,B,๐’ฑ):๐–พ๐—โ„n,โ„nโˆ’1ร—[0,1)\textstyle{\mathbf{H}(\mfld_{n}^{\partial,B},\mathcal{V}):{\sf ev}_{\mathbb{R}^{n},\mathbb{R}^{n-1}\times[0,1)}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

from ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡โˆ‚,๐–ก\disk^{\partial,B}_{n}-algebras in ๐’ฑ\mathcal{V} and homology theories of BB-framed nn-manifolds with coefficients in ๐’ฑ\mathcal{V}. This equivalence is implemented by the factorization homology functor โˆซ\int and evaluation on BB-framed Euclidean nn-spaces and half-spaces.

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Proof. After Propositionย 3.9 it is enough to consider the case where BB is equivalent to ๐–ก๐–ณ๐—ˆ๐—‰โก(๐—‡)\BTop(n), and so we omit it from the notation and discussion. Let โ„ฑ:โ„ณโ€‹๐–ฟ๐—…๐–ฝnโˆ‚โ†’๐’ฑ\mathcal{F}:\mfld_{n}^{\partial}\rightarrow\mathcal{V} be a symmetric monoidal functor satisfying the โŠ—\otimes-excision condition, and let AA be the restriction of โ„ฑ\mathcal{F} to ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡โˆ‚\disk_{n}^{\partial}. For a manifold with boundary Mยฏ\overline{M}, we prove that the canonical morphism โˆซMยฏAโ†’โ„ฑโก(Mยฏ)\int_{\overline{M}}A\rightarrow\mathcal{F}(\overline{M}) is an equivalence. By โŠ—\otimes-excision applied to the collar-gluing โˆ‚Mยฏร—[0,1)โ€‹โ‹ƒโˆ‚Mยฏร—โ„โ€‹Mโ‰…Mยฏ\partial\overline{M}\times[0,1)\underset{\partial\overline{M}\times\mathbb{R}}{\bigcup}M\cong\overline{M}, where MM is the interior of Mยฏ\overline{M}, we obtain a diagram in ๐’ฑ\mathcal{V}

โˆซโˆ‚Mยฏร—[0,1)โ€‹Aโ€‹โจ‚โˆซโˆ‚Mยฏร—โ„โ€‹Aโ€‹โˆซMA\textstyle{\displaystyle\underset{{\partial\overline{M}\times[0,1)}}{\int}A\underset{\underset{\partial\overline{M}\times\mathbb{R}}{\int}A}{\bigotimes}\int_{M}A\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}โ„ฑโก(โˆ‚Mยฏร—[0,1))โ€‹โจ‚โ„ฑโก(โˆ‚Mยฏร—โ„)โ€‹โ„ฑโ€‹(M)\textstyle{\mathcal{F}(\partial\overline{M}\times[0,1))\underset{\mathcal{F}(\partial\overline{M}\times\mathbb{R})}{\bigotimes}\mathcal{F}(M)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}โˆซMยฏA\textstyle{\displaystyle\int_{\overline{M}}A\ignorespaces\ignorespaces\ignorespaces\ignorespaces}โ„ฑโก(Mยฏ)\textstyle{\mathcal{F}(\overline{M})}

in which the vertical morphisms are equivalences. It now suffices to show that the top horizontal morphism is an equivalence. The equivalences of โˆซMAโ†’โ„ฑโก(M)\int_{M}A\rightarrow\mathcal{F}(M) and โˆซโˆ‚Mยฏร—โ„Aโ†’โ„ฑโก(โˆ‚Mยฏร—โ„)\int_{\partial\overline{M}\times\mathbb{R}}A\rightarrow\mathcal{F}(\partial\overline{M}\times\mathbb{R}) are given by Theorem 3.24; the last equivalence โˆซโˆ‚Mยฏร—[0,1)Aโ†’โ„ฑโก(โˆ‚Mยฏร—[0,1))\int_{\partial\overline{M}\times[0,1)}A\rightarrow\mathcal{F}({\partial\overline{M}\times[0,1)}) by follows by Theorem 3.24 and Proposition 2.16. โˆŽ

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Remark 3.27. There is an analogous theorem available for stratified spaces proved in ยง2 ofย [AFT2], where embeddings are conically smooth and preserve the stratifications. The previous theorems hold if the โŠ—\otimes-presentable condition is weakened to the condition that the monoidal structure distributes over sifted colimits.

The following example describes how factorization homology specializes to usual homology.

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Example 3.28. Let ๐’ฑโŠ•\mathcal{V}^{\oplus} be either the โˆž\oo-category of chain complexes or of spectra equipped with the direct sum monoidal structure. Since every object VV therein has an essentially unique morphism VโŠ•Vโ†’VV\oplus V\rightarrow V, there is an equivalence ๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–ฟ๐—‹โก(๐’ฑโŠ•)โ‰ƒ๐’ฑ\Alg_{\disk_{n}^{\sf fr}}(\mathcal{V}^{\oplus})\simeq\mathcal{V}. The factorization homology of a framed nn-manifold MM with coefficients in VV is then equivalent to โˆซMVโ‰ƒ๐–ขโˆ—โ€‹(M,V)\int_{M}V\simeq\mathsf{C}_{\ast}(M,V), or ฮฃโˆ—โˆžโ€‹MโŠ—V\Sigma^{\infty}_{\ast}M\otimes V for spectra, the stabilization of MM smashed with VV. There is a natural functor limโ†’โกโ„ณโ€‹๐–ฟ๐—…๐–ฝn๐–ฟ๐—‹โ†’๐–ฒ๐—‰๐–บ๐–ผ๐–พ๐—Œ๐–ฟ๐—‚๐—‡\varinjlim\mfld_{n}^{\fr}\rightarrow\spaces^{\sf fin}, and this functor is an equivalence because: it is fully faithful since limโ†’kโก๐–ค๐—†๐–ป๐–ฟ๐—‹โก(Mร—โ„k,Nร—โ„k)โ†’๐–ฌ๐–บ๐—‰โก(๐–ฌร—โ„โˆž,๐–ญร—โ„โˆž)โ‰ƒ๐–ฌ๐–บ๐—‰โก(๐–ฌ,๐–ญ)\varinjlim_{k}\Emb^{\fr}(M\times\mathbb{R}^{k},N\times\mathbb{R}^{k})\rightarrow\Map(M\times\mathbb{R}^{\infty},N\times\mathbb{R}^{\infty})\simeq\Map(M,N) is a weak homotopy equivalence for every MM and NN; it is essentially surjective since every finite CW complex XX can be embedded into โ„m\mathbb{R}^{m} for mm sufficiently large, and thus it is homotopy equivalent to a framed nn-manifold, namely an open regular neighborhood of the embedding. Theorem 3.24 thereby specializes to the formulation of the Eilenbergโ€“Steenrod axioms given in the introduction. If one sets ๐’ฑ\mathcal{V} to be the opposite ๐–ข๐—๐—ˆ๐—‰{\sf Ch}^{\op}, then one likewise recovers the Eilenbergโ€“Steenrod axioms for cohomology.

To this point, we have worked with topological manifolds and embeddings with the compact-open topology, but other choices could have been made, for instance, to work with smooth manifolds, or to have regarded the embeddings spaces as discrete. We next remark on as to how these alternate choices play out.

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Remark 3.29. One could replace the โˆž\oo-category of topological nn-manifolds and embeddings with that of smooth nn-manifolds and smooth embeddings, โ„ณโ€‹๐–ฟ๐—…๐–ฝn๐—Œ๐—†\mfld^{\sm}_{n}, or piecewise linear nn-manifolds and piecewise linear embeddings, โ„ณโ€‹๐–ฟ๐—…๐–ฝn๐–ฏ๐–ซ\mfld^{\sf PL}_{n}, and Theoremย 3.24 is still valid. The proof, in fact, is even simpler, as the existence of handlebody structures is much easier than in the case of topological manifolds. However, a consequence of smoothing theory [KS] is an equivalence

โ„ณโ€‹๐–ฟ๐—…๐–ฝn๐—Œ๐—†โ‰ƒโ„ณโ€‹๐–ฟ๐—…๐–ฝn๐–ก๐–ฎโก(n)\mfld^{\sm}_{n}\simeq\mfld_{n}^{{\sf BO}(n)}

between smooth nn-manifolds and ๐–กโ€‹Oโก(n)\BO(n)-framed topological nn-manifolds, so long as nn is not equal 44, so nothing new is obtained by considering smooth or piecewise linear manifolds rather than BB-framed topological manifolds. In the case of smooth 4-manifolds, there is still an equivalence ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐Ÿฆ๐—Œ๐—†โ‰ƒ๐’Ÿโ€‹๐—‚๐—Œ๐—„๐Ÿฆ๐–ก๐–ฎโก(๐Ÿฆ)\disk_{4}^{\sm}\simeq\disk_{4}^{{\sf BO}(4)}, and so combining the smooth and topological versions of Theorem 3.24 gives an equivalence

๐‡โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝn๐—Œ๐—†,๐’ฑ)โ‰ƒ๐‡โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝ4๐–ก๐–ฎโก(4),๐’ฑ)\mathbf{H}(\mfld_{n}^{\sm},\mathcal{V})\simeq\mathbf{H}(\mfld_{4}^{{\sf BO}(4)},\mathcal{V})

between homology theories for smooth 4-manifolds and homology theories for ๐–ก๐–ฎโก(4){\sf BO}(4)-framed topological 4-manifolds. Since the ๐–ก๐–ฎโก(4){\sf BO}(4)-framing on the tangent microbundle is only a very weak measure of a smooth structure in dimension 4 (e.g., there is a single ๐–ก๐–ฎโก(4){\sf BO}(4)-framing of โ„4\mathbb{R}^{4}, in contrast to the uncountably many smooth structures), this form of factorization homology is not a refined invariant of smooth 4-manifolds.

In the subsequent sections, we will be solely concerned with the homology theories of Definition 3.15. There do, however, exist very interesting functors in ๐–ฅ๐—Ž๐—‡โŠ—โก(โ„ณโ€‹๐–ฟ๐—…๐–ฝn,๐’ฑ)\Fun^{\otimes}(\mfld_{n},\mathcal{V}) which do not satisfy the โŠ—\otimes-excision property. In [BFN] the authors were particularly concerned with one such construction: given a stack XX over kk, one can define a functor โ„ณโ€‹๐–ฟ๐—…๐–ฝnโ†’๐–ฒ๐—๐–บ๐–ผ๐—„๐—Œโ†’๐–ฌ๐—ˆ๐–ฝ๐—„\mfld_{n}\rightarrow{\sf Stacks}\rightarrow\m_{k} given by sending a manifold MM to the cotensor with XX, Mโ†XMM\rightsquigarrow X^{M}, and then taking sheaf cohomology of the structure sheaf of this stack. In the case of the circle, M=S1M=S^{1}, this gives the Hochschild homology of XX: ๐’ชโก(XS1)โ‰ƒ๐–ง๐–ขโˆ—โก(๐–ท)\mathcal{O}(X^{S^{1}})\simeq\hh_{*}(X). As soon as XX is nonaffine, this construction will generically fail to satisfy โŠ—\otimes-excision. While the cotensor only depends on the homotopy type of MM, as we shall see in Proposition 5.1, it has a more refined generalization taking as input a derived stack defined over nn-disk algebras, rather than commutative algebras, as in [Fra1].

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Definition 3.30. Let ๐’ฑ\mathcal{V} be a symmtric monoidal โˆž\infty-category which is โŠ—\otimes-presentable. For a BB-framed nn-manifold MM and a functor X:๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโก(๐’ฑ)โ†’๐–ฒ๐—‰๐–บ๐–ผ๐–พ๐—ŒX:\Alg_{\disk^{B}_{n}}(\mathcal{V})\rightarrow\spaces, the factorization homology of MM with coefficients in XX is the object in ๐’ฑ\mathcal{V}

โˆซMX:=๐—…๐—‚๐—†๐– โˆˆ๐– ๐–ฟ๐–ฟ/๐–ท๐—ˆ๐—‰โˆซ๐–ฌ๐– \int_{M}X:=\limit_{A\in{\sf Aff}^{\op}_{/X}}\int_{M}A

where ๐– ๐–ฟ๐–ฟโ‰ƒ๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโก(๐’ฑ)๐—ˆ๐—‰{\sf Aff}\simeq\Alg_{\disk^{B}_{n}}(\mathcal{V})^{\op} is the image of the Yoneda embedding in ๐–ฅ๐—Ž๐—‡โก(๐– ๐—…๐—€๐’Ÿโ€‹๐—‚๐—Œ๐—„๐—‡๐–กโก(๐’ฑ),๐–ฒ๐—‰๐–บ๐–ผ๐–พ๐—Œ)\Fun\bigl(\Alg_{\disk_{n}^{B}}(\mathcal{V}),\spaces\bigr).

Intuitively, the object โˆซMX\int_{M}X is ฮ“โก(X,โˆซM๐’ช)\Gamma(X,\int_{M}\mathcal{O}), the global sections of the presheaf on XX obtained by applying factorization homology of MM to the structure sheaf of XX. From the vantage offered by Costello and Gwilliam in [CG], this generalization of factorization homology serves as a candidate for the structure of observables in a topological quantum field theory which is not necessarily perturbative, a direction we will pursue in future work.

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

David Ayala, John Francis

Original source: arXiv:1206.5522v6