ScalingStacks

5. Commutative algebras, free algebras, and Lie algebras

Previously, we have described factorization homology for nn-disk algebras in spaces, chain complexes, and spectra, when the monoidal structure is given by products, and the resulting homology theories give rise to twisted mapping spaces and usual homology theories. Factorization homology behaves very differently, and with greater sensitivity to manifold topology, when the monoidal structure on chain complexes or spectra is given by tensor product or smash product – this case is closest to the physical motivation given in the introduction. We will consider this case in this section, focusing on some of the most common classes of nn-disk algebra structures, which are either commutative, freely generated by a module, or freely generated by a Lie algebra.

5.1. Factorization homology with coefficients in commutative algebras

We begin by examining commutative algebras in 𝒱\mathcal{V}, otherwise known as β„°βˆž\mathcal{E}_{\infty}-algebras in 𝒱\mathcal{V}. Note first that a commutative algebra in 𝒱\mathcal{V} is equivalent to a symmetric monoidal functor π–₯𝗂𝗇→𝒱{\sf Fin}\rightarrow\mathcal{V} from finite sets with disjoint union. So restriction along the connected components functor [βˆ’]:π’Ÿβ€‹π—‚π—Œπ—„π—‡π–‘β†’π’Ÿβ€‹π—‚π—Œπ—„π—‡β†’[βˆ’]π–₯𝗂𝗇[-]:\disk^{B}_{n}\rightarrow\disk_{n}\xrightarrow{[-]}{\sf Fin} defines a forgetful functor

𝖿𝗀𝗍:π– π—…π—€π–’π—ˆπ—†β‘(𝒱)βŸΆπ– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–‘β‘(𝒱).{\sf fgt}\colon\Alg_{\com}(\mathcal{V})\longrightarrow\Alg_{\disk^{B}_{n}}(\mathcal{V})~.

We have the following consequence of βŠ—\otimes-excision, where 𝒱\mathcal{V} is a symmetric monoidal ∞\infty-category which is βŠ—\otimes-presentable. To phrase this result we utilize that the ∞\infty-category π– π—…π—€π–’π—ˆπ—†β‘(𝒱)\Alg_{\com}(\mathcal{V}) is tensored over spaces:

π–²π—‰π–Ίπ–Όπ–Ύπ—ŒΓ—π– π—…π—€π–’π—ˆπ—†(𝒱)β†’βŠ—π– π—…π—€π–’π—ˆπ—†(𝒱),(X,A)β†¦π–Όπ—ˆπ—…π—‚π—†(π–·β†’βˆ—β†’{𝖠}π– π—…π—€π–’π—ˆπ—†(𝒱)).\spaces\times\Alg_{\com}(\mathcal{V})\xrightarrow{\otimes}\Alg_{\com}(\mathcal{V})~,\qquad(X,A)\mapsto\colim\bigl(X\to\ast\xrightarrow{\{A\}}\Alg_{\com}(\mathcal{V})\bigr)~.
0N53

Proposition 5.1. The following diagram among ∞\infty-categories commutes:

ℳ​𝖿𝗅𝖽nBΓ—π– π—…π—€π–’π—ˆπ—†β‘(𝒱)\textstyle{\mfld^{B}_{n}\times\Alg_{\com}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}U×𝗂𝖽\scriptstyle{U\times{\sf id}}𝗂𝖽×fgt\scriptstyle{{\sf id}\times{\rm fgt}}π–²π—‰π–Ίπ–Όπ–Ύπ—ŒΓ—π– π—…π—€π–’π—ˆπ—†β‘(𝒱)\textstyle{\Space\times\Alg_{\com}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}βŠ—\scriptstyle{\otimes}π– π—…π—€π–’π—ˆπ—†β‘(𝒱)\textstyle{\Alg_{\com}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ℳ​𝖿𝗅𝖽nBΓ—π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–‘β‘(𝒱)\textstyle{\mfld^{B}_{n}\times\Alg_{\disk^{B}_{n}}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}∫\scriptstyle{\int}𝒱\textstyle{\mathcal{V}}

where UU is the underlying space functor and the right downward arrow is the standard forgetful functor. In particular, there is a natural equivalence

∫MA≃MβŠ—A\int_{M}A~\simeq~M\otimes A

between the factorization homology of MM with coefficients in AA and the tensor of the commutative algebra AA with the underlying space of MM.

0N54

Proof. The functor βˆ’βŠ—A:ℳ​𝖿𝗅𝖽nB→𝒱-\otimes A\colon\mfld_{n}^{B}\to\mathcal{V} carries each contractible manifold to the underlying object of the commutative algebra AA. For (Ai)i∈I(A_{i})_{i\in I} a finite sequence of commutative algebras in 𝒱\mathcal{V}, the II-fold coproduct in π– π—…π—€π–’π—ˆπ—†β‘(𝒱)\Alg_{\com}(\mathcal{V}) is the pointwise tensor product ⨂i∈I​Ai\underset{i\in I}{\bigotimes}A_{i} (see PropositionΒ 3.2.4.7 ofΒ [Lu2]). It follows that this functor βˆ’βŠ—A-\otimes A is symmetric monoidal. From the defining expression of factorization homology as a colimit, there results a natural transformation

βˆ«βˆ’AβŸΆβˆ’βŠ—A\int_{-}A\longrightarrow-\otimes A

between symmetric monoidal functors ℳ​𝖿𝗅𝖽nB→𝒱\mfld_{n}^{B}\to\mathcal{V}, which evaluates as an equivalence on objects of π’Ÿβ€‹π—‚π—Œπ—„π—‡π–‘\disk_{n}^{B}. LemmaΒ 3.18 grants that the domain of this natural transformation satisfies βŠ—\otimes-excision. Because a collar-gluing M′​⋃M0×ℝ​Mβ€²β€²β‰…MM^{\prime}\underset{M_{0}\times\mathbb{R}}{\bigcup}M^{\prime\prime}\cong M determines a pushout of underlying spaces Mβ€²β€‹βˆM0​M′′≃MM^{\prime}\underset{M_{0}}{\coprod}M^{\prime\prime}\simeq M, the codomain of this natural transformation too satisfies βŠ—\otimes-excision. That the natural transformation evaluates on each BB-framed nn-manifold MM as an equivalence then follows by induction on a handle decomposition on MM.

∎

In other words, the factorization homology ∫MA\int_{M}A has a natural structure of a commutative algebra when AA is commutative, and this commutative algebra has a universal property: for each commutative algebra CC in 𝒱\mathcal{V} there is a natural equivalence from the space of commutative algebra maps

π–¬π–Ίπ—‰π–’π—ˆπ—†β‘(βˆ«π–¬π– ,𝖒)β‰ƒπ–¬π–Ίπ—‰π–’π—ˆπ—†β‘(𝖠,𝖒)𝖬,\Map_{\com}\bigl(\int_{M}A,C\bigr)~\simeq~\Map_{\com}(A,C)^{M}~,

to the space of maps from MM to the space of commutative algebra maps. By formal properties of left adjoints and tensors, this has the immediate corollary.

0N55

Corollary 5.2. For each symmetric monoidal ∞\infty-category 𝒱\mathcal{V} which is βŠ—\otimes-presentable, there is a natural equivalence in 𝒱\mathcal{V}:

∫M𝖲𝗒𝗆⁑(𝖡)≃𝖲𝗒𝗆⁑(π–¬βŠ—π–΅).\int_{M}\sym(V)~\simeq~\sym(M\otimes V)~.

In particular, if 𝒱\mathcal{V} is the ∞\infty-category of chain complexes with tensor product, then there is an equivalence ∫M𝖲𝗒𝗆⁑(𝖡)≃𝖲𝗒𝗆⁑(π–’βˆ—β€‹(𝖬,𝖡))\int_{M}\sym(V)\simeq\sym(\mathsf{C}_{\ast}(M,V)) for each chain complex VV. We now push the above result slightly further for the two special classes of commutative algebras arising from the cohomology of spaces and the cohomology of Lie algebras. The study of the latter has benefitted greatly from conversations with Kevin Costello and Dennis Gaitsgory, and a full development of these ideas will amount to a forthcoming work.

0N56

Proposition 5.3. Let MM be an nn-manifold, and let XX be a nilpotent nn-connective space of finite type over RR such that Ο€n​X\pi_{n}X is finite. There is a natural equivalence of chain complexes

∫Mπ–’βˆ—β€‹(X,R)β‰ƒπ–’βˆ—β€‹(XM,R)\int_{M}\mathsf{C}^{\ast}(X,R)~\simeq~\mathsf{C}^{\ast}(X^{M},R)

between the factorization homology of MM with coefficient in the RR-cohomology of XX and the RR-cohomology of the space of maps from MM to XX.

0N57

Proof. The two sides are evidently equivalent in the case where MM is homeomorphic to ℝn\mathbb{R}^{n}, so to establish the result it suffices, as usual, to check by induction over a handle decomposition of MM. Given a handle decomposition N​⋃Sk×ℝnβˆ’k​ℝnβ‰…MN\underset{S^{k}\times\mathbb{R}^{n-k}}{\bigcup}\mathbb{R}^{n}\cong M, we have a homotopy pullback diagram of spaces

(8) XM\textstyle{X^{M}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Xℝn\textstyle{\ignorespaces\ignorespaces\ignorespaces\ignorespaces X^{\mathbb{R}^{n}}}XN\textstyle{X^{N}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XSk×ℝnβˆ’k\textstyle{X^{S^{k}\times\mathbb{R}^{n-k}}}

which gives rise to a natural map in RR-homology

π–’βˆ—β€‹(XM,R)βŸΆπ–’βˆ—β€‹(XN,R)β€‹β¨‚π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)β€‹π–’βˆ—β€‹(Xℝn,R)\mathsf{C}_{\ast}(X^{M},R)\longrightarrow\mathsf{C}_{\ast}(X^{N},R)\underset{\mathsf{C}_{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R)}{\bigotimes}\mathsf{C}_{\ast}(X^{\mathbb{R}^{n}},R)

from the homology of the mapping spaces to the cotensor product of the comodules π–’βˆ—β€‹(XN,R)\mathsf{C}_{\ast}(X^{N},R) and π–’βˆ—β€‹(Xℝn,R)\mathsf{C}_{\ast}(X^{\mathbb{R}^{n}},R) over the coalgebra π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)\mathsf{C}_{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R). This map is an equivalence exactly if the homological Eilenberg–Moore, or Rothenberg–Steenrod, spectral sequence for this homotopy Cartesian diagram converges. By Dwyer [Dw], the convergence of this Eilenberg–Moore spectral sequence is assured if the base XSk×ℝnβˆ’kX^{S^{k}\times\mathbb{R}^{n-k}} is connected and the action

Ο€1​(XSk×ℝnβˆ’k,f)β†»Ο€βˆ—β€‹(𝖿𝗂𝖻𝖾𝗋f​(Xℝnβ†’XSk×ℝnβˆ’k))\pi_{1}\bigl(X^{S^{k}\times\mathbb{R}^{n-k}},f\bigr)\circlearrowright\pi_{\ast}\bigl({\sf fiber}_{f}(X^{\mathbb{R}^{n}}\rightarrow X^{S^{k}\times\mathbb{R}^{n-k}})\bigr)

is nilpotent for a choice of basepoint f∈XSk×ℝnβˆ’kf\in X^{S^{k}\times\mathbb{R}^{n-k}}. Since XX is nn-connective, for k<nk<n any map f:Skβ†’Xf:S^{k}\rightarrow X is nullhomotopic, and therefore the base XSk×ℝnβˆ’k≃XSkX^{S^{k}\times\mathbb{R}^{n-k}}\simeq X^{S^{k}} is connected. We can thus take ff to be the constant map valued at the basepoint of XX, and so identify 𝖿𝗂𝖻𝖾𝗋f​(Xℝnβ†’XSk×ℝnβˆ’k)≃Ωk+1​X{\sf fiber}_{f}(X^{\mathbb{R}^{n}}\rightarrow X^{S^{k}\times\mathbb{R}^{n-k}})\simeq\Omega^{k+1}X. We now show the action of Ο€1​(XSk)\pi_{1}\bigl(X^{S^{k}}\bigr) on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X is nilpotent. Consider the fiber sequence Ξ©k+1​Xβ†’XSkβ†’π–Ύπ—βˆ—X\Omega^{k+1}X\to X^{S^{k}}\xrightarrow{{\sf ev}_{\ast}}X. This fibration admits a section, given by the constant maps. Consequently, there is an identification as a semi-direct product:

Ο€1​(XSk)β‰…Ο€1​X⋉π1​Ωk​Xβ‰…Ο€1​X⋉π0​Ωk+1​X.\pi_{1}\bigl(X^{S^{k}}\bigr)\cong\pi_{1}X\ltimes\pi_{1}\Omega^{k}X\cong\pi_{1}X\ltimes\pi_{0}\Omega^{k+1}X~.

Through this identification, the action of Ο€1​(XSk)\pi_{1}\bigl(X^{S^{k}}\bigr) on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X is the unique action that extends the standard actions of Ο€1​X\pi_{1}X and of Ο€0​Ωk+1​X\pi_{0}\Omega^{k+1}X on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X. By assumption, the action of Ο€1​X\pi_{1}X on Ο€βˆ—+k+1​Xβ‰…Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast+k+1}X\cong\pi_{\ast}\Omega^{k+1}X is nilpotent. In the case that k=0k=0, the same assumption grants that the action of Ο€0​Ωk+1​X\pi_{0}\Omega^{k+1}X on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X is nilpotent. In the case that k>0k>0, the action of Ο€0​Ωk+1​X\pi_{0}\Omega^{k+1}X on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X is automatically nilpotent due to commutativity. Nilpotence of the action of Ο€1​(XSk)\pi_{1}\bigl(X^{S^{k}}\bigr) on Ο€βˆ—β€‹Ξ©k+1​X\pi_{\ast}\Omega^{k+1}X follows. Consequently, the natural map in RR-homology above is an equivalence.

The remainder of this argument is checking that we have imposed sufficient finiteness conditions to ensure the convergence in cohomology as well as homology. Dualizing, we obtain an equivalence

(π–’βˆ—β€‹(XN,R)β€‹β¨‚π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)β€‹π–’βˆ—β€‹(Xℝn,R))βˆ¨β€‹βŸΆβˆΌβ€‹π–’βˆ—β€‹(XM,R).\Bigl(\mathsf{C}_{\ast}(X^{N},R)\underset{\mathsf{C}_{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R)}{\bigotimes}\mathsf{C}_{\ast}(X^{\mathbb{R}^{n}},R)\Bigr)^{\vee}\overset{\sim}{\longrightarrow}\mathsf{C}^{\ast}(X^{M},R)~.

Since Ο€n​X\pi_{n}X is finite, the mapping space XKX^{K} has finitely many components for any nn-dimensional finite CW complex KK. Because the source spaces, MM, NN, Sk×ℝnβˆ’kS^{k}\times\mathbb{R}^{n-k}, and ℝn\mathbb{R}^{n}, all have have the homotopy types of finite nn-dimensional CW complexes, we obtain that all these mapping spaces have finitely many components. Since they are additionally finite CW complexes and XX is finite type, the homology groups of the mapping spaces 𝖧i​(XK,R)\mathsf{H}_{i}(X^{K},R) are finite rank over RR, and therefore π–’βˆ—β€‹(XK,R)\mathsf{C}_{*}(X^{K},R) is its own double dual: the map π–’βˆ—β€‹(XK,R)β†’π–’βˆ—β€‹(XK,R)∨\mathsf{C}_{*}(X^{K},R)\rightarrow\mathsf{C}^{*}(X^{K},R)^{\vee} is an equivalence. Likewise, there is an equivalence between the dual of the tensor product and the cotensor product

(π–’βˆ—β€‹(XN,R)β€‹β¨‚π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)β€‹π–’βˆ—β€‹(Xℝn,R))βˆ¨β‰ƒπ–’βˆ—β€‹(XN,R)β€‹β¨‚π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)β€‹π–’βˆ—β€‹(Xℝn,R)β‰ƒπ–’βˆ—β€‹(XM,R)\Bigl(\mathsf{C}^{\ast}(X^{N},R)\underset{\mathsf{C}^{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R)}{\bigotimes}\mathsf{C}^{\ast}(X^{\mathbb{R}^{n}},R)\Bigr)^{\vee}\simeq\mathsf{C}_{\ast}(X^{N},R)\underset{\mathsf{C}_{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R)}{\bigotimes}\mathsf{C}_{\ast}(X^{\mathbb{R}^{n}},R)\simeq\mathsf{C}_{\ast}(X^{M},R)

– this can be seen by commuting duality with the colimit to obtain a limit of a cosimplicial object, then comparing termwise. Continuing, one then concludes the equivalence

π–’βˆ—β€‹(XM,R)β‰ƒπ–’βˆ—β€‹(XN,R)β€‹β¨‚π–’βˆ—β€‹(XSk×ℝnβˆ’k,R)β€‹π–’βˆ—β€‹(Xℝn,R),\mathsf{C}^{\ast}(X^{M},R)\simeq\mathsf{C}^{\ast}(X^{N},R)\underset{\mathsf{C}^{\ast}(X^{S^{k}\times\mathbb{R}^{n-k}},R)}{\bigotimes}\mathsf{C}^{\ast}(X^{\mathbb{R}^{n}},R)~,

thereby finishing the proof.

∎

0N58

Remark 5.4. See [GTZ1] for a closely related approach to the study of mapping spaces, in which one approaches the cohomology of a mapping space as a Hochschild homology-type invariant of the cohomology of the target.

5.2. Factorization homology with coefficients in free nn-disk algebras

We next turn to the factorization homology of free nn-disk algebras, a topic studied in more detail inΒ Β§2 ofΒ [AFT2].

Denote by π–₯𝗋𝖾𝖾𝗇⁑(𝖡)\free_{n}(V) the augmented nn-disk algebra freely generated by Vβˆˆπ’±V\in\mathcal{V}, regarded as a trivial π–³π—ˆπ—‰β‘(n)\Top(n)-module. Let π–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)\conf_{i}(M,\partial M) denote the quotient of π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(M) by the subspace of all configurations in which at least one point lies in the boundary of MM.

0N59

Proposition 5.5. Let MM be an nn-manifold, possibly with boundary. Let Vβˆˆπ’±V\in\mathcal{V} be an object of a symmetric monoidal ∞\oo-category which is βŠ—\otimes-presentable. There is an equivalence

∫Mπ–₯𝗋𝖾𝖾𝗇⁑(𝖡)β‰ƒβˆπ—‚β‰₯πŸ’π–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)β€‹βŠ—Ξ£i​VβŠ—i\int_{M}\free_{n}(V)~\simeq~\coprod_{i\geq 0}\conf_{i}(M,\partial M)\underset{\Sigma_{i}}{\otimes}V^{\otimes i}

between the factorization homology of an nn-manifold MM, possibly with boundary, with coefficients in π–₯𝗋𝖾𝖾𝗇⁑(𝖡)\free_{n}(V) and the coproduct of the configuration spaces of MM labeled by VV quotient the subspace where at least one point lies in the boundary of MM.

The argument below is a special case of one in [AF1].

0N5A

Proof. The following equivalences

∫Mπ–₯𝗋𝖾𝖾𝗇(𝖡)β‰ƒπ–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚βˆπ—‚β‰₯πŸ’π–’π—ˆπ—‡π–Ώi(U,βˆ‚U)βŠ—Ξ£iVβŠ—iβ‰ƒβˆiβ‰₯0π–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚π–’π—ˆπ—‡π–Ώi(U,βˆ‚U)βŠ—Ξ£iVβŠ—i\int_{M}\free_{n}(V)\simeq\colim_{U\in\disk^{\partial}_{n/M}}\coprod_{i\geq 0}\conf_{i}(U,\partial U)\underset{\Sigma_{i}}{\otimes}V^{\otimes i}\simeq\coprod_{i\geq 0}\colim_{U\in\disk^{\partial}_{n/M}}\conf_{i}(U,\partial U)\underset{\Sigma_{i}}{\otimes}V^{\otimes i}

follow from the commutativity of colimits. To conclude the result it therefore suffices to show that for each ii the canonical morphism

π–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚π–’π—ˆπ—‡π–Ώi​(U,βˆ‚U)β€‹βŠ—Ξ£i​VβŠ—iβŸΆπ–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)β€‹βŠ—Ξ£i​VβŠ—i\colim_{U\in\disk^{\partial}_{n/M}}\conf_{i}(U,\partial U)\underset{\Sigma_{i}}{\otimes}V^{\otimes i}\longrightarrow\conf_{i}(M,\partial M)\underset{\Sigma_{i}}{\otimes}V^{\otimes i}

in 𝒱\mathcal{V} is an equivalence. By the assumed distributivity in the βŠ—\otimes-presentability condition, this follows if the natural Ξ£i\Sigma_{i}-equivariant map of Ξ£i\Sigma_{i}-spaces

(9) π–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚π–’π—ˆπ—‡π–Ώi​(U,βˆ‚U)βŸΆπ–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)\colim_{U\in\disk^{\partial}_{n/M}}\conf_{i}(U,\partial U)\longrightarrow\conf_{i}(M,\partial M)

is an equivalence, which we now show.

We first consider the case that the boundary of MM is empty, so that the natural Ξ£i\Sigma_{i}-equivariant map π–’π—ˆπ—‡π–Ώi⁑(M)β†’β‰…π–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)\conf_{i}(M)\xrightarrow{\cong}\conf_{i}(M,\partial M) is a homeomorphism, and the natural functor π’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬β†’β‰ƒπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚\disk_{n/M}\xrightarrow{\simeq}\disk^{\partial}_{n/M} is an equivalence of ∞\infty-categories. In this case we are to show that the Ξ£i\Sigma_{i}-equivariant map of Ξ£i\Sigma_{i}-spaces

π–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬π–’π—ˆπ—‡π–Ώi​(U)βŸΆπ–’π—ˆπ—‡π–Ώi⁑(M)\colim_{U\in\disk_{n/M}}\conf_{i}(U)\longrightarrow\conf_{i}(M)

is an equivalence. After PropositionΒ 2.19, it is enough to show that the Ξ£i\Sigma_{i}-equivariant map of Ξ£i\Sigma_{i}-topological spaces

(10) π–Όπ—ˆπ—…π—‚π—†Uβˆˆπ–£π—‚π—Œπ—„n/Mβ€‹π–’π—ˆπ—‡π–Ώi⁑(U)βŸΆπ–’π—ˆπ—‡π–Ώi⁑(M)\underset{U\in{\sf Disk}_{n/M}}{\colim}\conf_{i}(U)\longrightarrow\conf_{i}(M)

is a weak homotopy equivalence from the homotopy colimit. Each map π–’π—ˆπ—‡π–Ώi⁑(U)β†’π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(U)\to\conf_{i}(M) comprising this homotopy colimit is an open embedding. Also, for each element {1,…,i}→𝑐M\{1,\dots,i\}\xrightarrow{c}M of π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(M), choosing mutually disjoint Euclidean neighborhoods about each c⁑(j)∈Mc(j)\in M demonstrates that cc lies in the image of at least one such open embedding. Therefore this augmented diagram is an open cover of π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(M). This open cover of MM has the property that each finite intersection of its terms is covered by terms contained in this finite intersection. This is to say that this open cover of π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(M) is in fact a hypercover. That the mapΒ (10) is a weak homotopy equivalence follows from Corollary 1.6 ofΒ [DI].

Now suppose βˆ‚M\partial M is not empty. Fix a collar-neighborhood βˆ‚M×ℝβ‰₯0β†ͺM\partial M\times\mathbb{R}_{\geq 0}\hookrightarrow M. Such a collar-neighborhood determines the top horizontal arrow in the diagram of topological spaces

π–Όπ—ˆπ—…π—‚π—†βˆ…β‰ IβŠ‚{1,…,i}β€‹π–’π—ˆπ—‡π–Ώ{1,…,i}βˆ–I⁑(βˆ‚M)Γ—π–’π—ˆπ—‡π–ΏI⁑(M̊)\textstyle{\underset{\emptyset\neq I\subset\{1,\dots,i\}}{\colim}\conf_{\{1,\dots,i\}\smallsetminus I}(\partial M)\times\conf_{I}(\mathring{M})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π–’π—ˆπ—‡π–Ώi⁑(M̊)\textstyle{\conf_{i}(\mathring{M})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}βˆ—\textstyle{\ast\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π–’π—ˆπ—‡π–Ώi⁑(M,βˆ‚M)\textstyle{\conf_{i}(M,\partial M)}

which commutes up to homotopy – here, the homotopy colimit is indexed by the opposite of the poset of non-empty subsets of {1,…,i}\{1,\dots,i\}. This collar-neighborhood also gives that this diagram is a weak homotopy pushout. The result for this case of non-empty boundary thus follows from the previous case of empty boundary applied to βˆ‚M\partial M and to M̊\mathring{M}, using that homotopy colimits commute with one another.

∎

0N5B

Remark 5.6. The preceding result has as a consequence that factorization homology is not a homotopy invariant of a closed nn-manifold, since the homotopy type of configuration spaces is known to be sensitive to simple homotopy equivalence by [LS].

From Proposition 5.5 and some reasoning on stable splittings of configuration spaces, one can deduce the following result. For the previous proposition, we required the monoidal structure of 𝒱\mathcal{V} to distribute over colimits; for convenience, we next assume the underlying ∞\infty-category of 𝒱\mathcal{V} is stable.

0N5C

Proposition 5.7. Let 𝒱\mathcal{V} be a symmetric monoidal ∞\infty-category which is βŠ—\otimes-presentable and whose underlying ∞\infty-category is stable. For any Vβˆˆπ’±V\in\mathcal{V} and any nonnegative integer m<nm<n, there is an equivalence in 𝒱\mathcal{V}:

∫Sm×ℝnβˆ’mπ–₯𝗋𝖾𝖾𝗇⁑(𝖡)≃π–₯𝗋𝖾𝖾𝗇⁑(𝖡)βŠ—π–₯π—‹π–Ύπ–Ύπ—‡βˆ’π—†β‘(Σ𝗆​𝖡).\int_{S^{m}\times\mathbb{R}^{n-m}}\free_{n}(V)~\simeq~\free_{n}(V)\otimes\free_{n-m}(\Sigma^{m}V)~.
0N5D

Proof. We first consider the case that 𝒱=(𝖲𝗉𝖾𝖼𝗍𝗋𝖺,∧)\mathcal{V}=\bigl({\sf Spectra},\wedge\bigr) and V=Ξ£βˆžβ€‹XV=\Sigma^{\infty}X is the suspension spectrum of a pointed connected space XX. There is a natural equivalence of spaces

∫Sm×ℝnβˆ’mΞ©n​Σn​X​≃Cor​4.6​(Ξ©nβˆ’m​Σn​X)Sm≃Ωn​Σn​XΓ—Ξ©nβˆ’m​Σn​X\int_{S^{m}\times\mathbb{R}^{n-m}}\Omega^{n}\Sigma^{n}X~\underset{\rm Cor~\ref{non-abel}}{\simeq}~(\Omega^{n-m}\Sigma^{n}X)^{S^{m}}~\simeq~\Omega^{n}\Sigma^{n}X\times\Omega^{n-m}\Sigma^{n}X

where the first equivalence is by nonabelian PoincarΓ© duality and the second is by the standard trivialization of each fiber sequence π–¬π–Ίπ—‰βˆ—β‘(π–ͺ,𝖦)→𝖦π–ͺ→𝖦\Map_{*}(K,G)\rightarrow G^{K}\rightarrow G whose base is equipped with the structure of a group-like β„°1\mathcal{E}_{1}-space. (It is this second step that requires the strict inequality m<nm<n.) Passing to suspension spectra, PropositionΒ 5.5 begets the further equivalence

⋁kβ‰₯0π–’π—ˆπ—‡π–Ώk⁑(Sm×ℝnβˆ’m)β€‹βŠ—Ξ£kβ€‹Ξ£βˆžβ€‹XβŠ—k≃(⋁iβ‰₯0π–’π—ˆπ—‡π–Ώi⁑(ℝn)β€‹βŠ—Ξ£iβ€‹Ξ£βˆžβ€‹XβŠ—i)βŠ—(⋁jβ‰₯0π–’π—ˆπ—‡π–Ώj⁑(ℝnβˆ’m)β€‹βŠ—Ξ£jβ€‹Ξ£βˆžβ€‹(Ξ£m​X)βŠ—j).\bigvee_{k\geq 0}\conf_{k}(S^{m}\times\mathbb{R}^{n-m})\underset{\Sigma_{k}}{\otimes}\Sigma^{\oo}X^{\otimes k}\simeq\Bigl(\bigvee_{i\geq 0}\conf_{i}(\mathbb{R}^{n})\underset{\Sigma_{i}}{\otimes}\Sigma^{\oo}X^{\otimes i}\Bigr)\otimes\Bigl(\bigvee_{j\geq 0}\conf_{j}(\mathbb{R}^{n-m})\underset{\Sigma_{j}}{\otimes}\Sigma^{\oo}(\Sigma^{m}X)^{\otimes j}\Bigr)~.

Collecting coefficients of terms which are homogeneous in XX determines a Ξ£k\Sigma_{k}-equivariant stable homotopy equivalence

Ξ£βˆ—βˆžπ–’π—ˆπ—‡π–Ώk(Sm×ℝnβˆ’m)β‰ƒβˆi+j=k(Ξ£kΓ—Ξ£iΞ£βˆ—βˆžπ–’π—ˆπ—‡π–Ώi(ℝn))βŠ—(Ξ£kΓ—Ξ£jΞ£βˆ—βˆž(Ξ£+mjπ–’π—ˆπ—‡π–Ώj(ℝnβˆ’m)))\Sigma^{\infty}_{\ast}\conf_{k}(S^{m}\times\mathbb{R}^{n-m})\simeq\coprod_{i+j=k}\Bigl(\Sigma_{k}\underset{\Sigma_{i}}{\times}\Sigma^{\infty}_{\ast}\conf_{i}(\mathbb{R}^{n})\Bigr)\otimes\Bigr(\Sigma_{k}\underset{\Sigma_{j}}{\times}\Sigma^{\infty}_{\ast}\bigl(\Sigma^{mj}_{+}\conf_{j}(\mathbb{R}^{n-m})\bigr)\Bigl)

where Ξ£k​×Σlβˆ’\Sigma_{k}\underset{\Sigma_{l}}{\times}- is induction from Ξ£l\Sigma_{l}-spectra to Ξ£k\Sigma_{k}-spectra.

Now consider the general case for 𝒱\mathcal{V}, according to the hypothesis. After PropositionΒ 5.5, both sides of the equivalence split as coproducts in homogeneous terms VβŠ—kV^{\otimes k}, so it suffices to show that the coefficients of these terms are degreewise equivalent. Inspecting, we thus seek an equivalence in 𝒱\mathcal{V}:

π–’π—ˆπ—‡π–Ώk(Sm×ℝnβˆ’m)βŠ—Ξ£kVβŠ—k≃⨁i+j=k(π–’π—ˆπ—‡π–Ώi(ℝn)βŠ—Ξ£iVβŠ—i)βŠ—(π–’π—ˆπ—‡π–Ώj(ℝnβˆ’m)βŠ—Ξ£j(Ξ£mV)βŠ—j).\conf_{k}(S^{m}\times\mathbb{R}^{n-m})\underset{\Sigma_{k}}{\otimes}V^{\otimes k}~\simeq~\bigoplus_{i+j=k}\Bigl(\conf_{i}(\mathbb{R}^{n})\underset{\Sigma_{i}}{\otimes}V^{\otimes i}\Bigr)\otimes\Bigr(\conf_{j}(\mathbb{R}^{n-m})\underset{\Sigma_{j}}{\otimes}(\Sigma^{m}V)^{\otimes j}\Bigl)~.

This equivalence follows from the conclusion of the previous paragraph upon tensoring with VβŠ—kV^{\otimes k} and taking balanced Ξ£k\Sigma_{k}-coinvariants.

∎

0N5E

Remark 5.8. The equivalence in the above proposition can be upgraded to an equivalence of (nβˆ’m)(n-m)-disk algebras if the righthand side is given a twisted algebra structure, using a natural action of π–₯π—‹π–Ύπ–Ύπ—‡βˆ’π—†β‘(Σ𝗆​𝖡)\free_{n-m}(\Sigma^{m}V) on π–₯𝗋𝖾𝖾𝗇⁑(𝖡)\free_{n}(V).

The calculations to this point allow the following interesting description of the bar construction on a free nn-disk algebra. Let 𝒱\mathcal{V} be a symmetric monoidal ∞\oo-category which is βŠ—\otimes-presentable.

0N5F

Proposition 5.9. For any object Vβˆˆπ’±V\in\mathcal{V} in a symmetric monoidal ∞\infty-category which is βŠ—\otimes-presentable, there is an natural equivalence

𝖑𝖺𝗋⁑(π–₯𝗋𝖾𝖾𝗇⁑(𝖡))≃π–₯π—‹π–Ύπ–Ύπ—‡βˆ’πŸ£β‘(Σ​𝖡){\sf Bar}\bigl(\free_{n}(V)\bigr)~\simeq~\free_{n-1}(\Sigma V)

between the bar construction on the free nn-disk algebra on VV and the free (nβˆ’1)(n-1)-disk algebra generated by the suspension of VV.

0N5G

Proof. Via ExampleΒ 3.10, each augmented associative algebra Aβ†’πŸ™A\to\uno in 𝒱\mathcal{V} determines a symmetric monoidal functor A:π’Ÿβ€‹π—‚π—Œπ—„πŸ£βˆ‚,π—ˆπ—‹β†’π’±A\colon\disk^{\partial,\sf or}_{1}\to\mathcal{V}. Applying βŠ—\otimes-excision in this simplest case of the collar-gluing [βˆ’1,1)⋃(βˆ’1,1)(βˆ’1,1]β‰…[βˆ’1,1][-1,1)\underset{(-1,1)}{\bigcup}(-1,1]\cong[-1,1], we have that the bar construction 𝖑𝖺𝗋⁑(A){\sf Bar}(A) is identifiable as the factorization homology over the closed 1-disk:

𝖑𝖺𝗋⁑(A)β‰ƒβˆ«π”»1A.{\sf Bar}(A)~\simeq~\int_{\mathbb{D}^{1}}A~.

PropositionΒ 5.5 gives the first and last of the following identifications

βˆ«π”»1×ℝnβˆ’1​π–₯𝗋𝖾𝖾𝗇​(𝖡)\displaystyle\underset{\mathbb{D}^{1}\times\mathbb{R}^{n-1}}{\int}\free_{n}(V) ≃\displaystyle\simeq ∐iβ‰₯0π–’π—ˆπ—‡π–Ώi⁑(𝔻1×ℝnβˆ’1,βˆ‚π”»1×ℝnβˆ’1)β€‹βŠ—Ξ£i​VβŠ—i\displaystyle\coprod_{i\geq 0}\conf_{i}(\mathbb{D}^{1}\times\mathbb{R}^{n-1},\partial\mathbb{D}^{1}\times\mathbb{R}^{n-1})\underset{\Sigma_{i}}{\otimes}V^{\otimes i}
≃\displaystyle\simeq ∐iβ‰₯0Ξ£iβ€‹π–’π—ˆπ—‡π–Ώi⁑(ℝnβˆ’1)β€‹βŠ—Ξ£i​VβŠ—i\displaystyle\coprod_{i\geq 0}\Sigma^{i}\conf_{i}(\mathbb{R}^{n-1})\underset{\Sigma_{i}}{\otimes}V^{\otimes i}
≃\displaystyle\simeq ∐iβ‰₯0π–’π—ˆπ—‡π–Ώi⁑(ℝnβˆ’1)β€‹βŠ—Ξ£i​(Σ​V)βŠ—i\displaystyle\coprod_{i\geq 0}\conf_{i}(\mathbb{R}^{n-1})\underset{\Sigma_{i}}{\otimes}(\Sigma V)^{\otimes i}
≃\displaystyle\simeq π–₯π—‹π–Ύπ–Ύπ—‡βˆ’πŸ£β‘(Σ​𝖡).\displaystyle\free_{n-1}(\Sigma V)~.

The second identification follows from the Ξ£i\Sigma_{i}-equivariant equivalence of spaces

π–’π—ˆπ—‡π–Ώi⁑(𝔻1Γ—M,βˆ‚π”»1Γ—M)≃𝔻iΓ—π–’π—ˆπ—‡π–Ώi⁑(M)/βˆ‚π”»iΓ—π–’π—ˆπ—‡π–Ώi⁑(M)≃Σiβ€‹π–’π—ˆπ—‡π–Ώi⁑(M)\conf_{i}(\mathbb{D}^{1}\times M,\partial\mathbb{D}^{1}\times M)\simeq\mathbb{D}^{i}\times\conf_{i}(M)\big/\partial\mathbb{D}^{i}\times\conf_{i}(M)\simeq\Sigma^{i}\conf_{i}(M)

in the case M=ℝnβˆ’1M=\mathbb{R}^{n-1}. The third equivalence is a coproduct of a composite of two equivalences: Ξ£i​XβŠ—VβŠ—i≃XβŠ—Ξ£i​(VβŠ—i)≃XβŠ—(Σ​V)βŠ—i\Sigma^{i}X\otimes V^{\otimes i}\simeq X\otimes\Sigma^{i}(V^{\otimes i})\simeq X\otimes(\Sigma V)^{\otimes i}. The first of these equivalences uses that tensoring with spaces preserves colimits among spaces – an assertion which is direct from definitions. The second of these equivalences directly uses the assumption that the symmetric monoidal structure of 𝒱\mathcal{V} distributes over colimits.

∎

0N5H

Remark 5.10. In [Fra2], it was proved that 𝖑𝖺𝗋n​π–₯𝗋𝖾𝖾𝗇⁑(𝖡)β‰ƒπŸ™βŠ•Ξ£n​V{\sf Bar}^{n}\free_{n}(V)\simeq\uno\oplus\Sigma^{n}V, the free 00-disk algebra on the nnth suspension of VV. This can now be seen as an application of Proposition 5.9 iterated nn times. This result is well-known in the case of n=1n=1: the bar construction for the tensor algebra on VV is πŸ™βŠ•Ξ£β€‹V\uno\oplus\Sigma V. Our result is also entirely to be expected given the example of nn-fold loop space, where for a connected pointed space VV, we can calculate 𝖑𝖺𝗋⁑(π–₯𝗋𝖾𝖾𝗇⁑(𝖡))β‰ƒπ–‘β€‹Ξ©π—‡β€‹Ξ£π—‡β€‹π–΅β‰ƒΞ©π—‡βˆ’πŸ£β€‹Ξ£π—‡β€‹π–΅β‰ƒπ–₯π—‹π–Ύπ–Ύπ—‡βˆ’πŸ£β‘(Σ​𝖡){\sf Bar}\bigl(\free_{n}(V)\bigr)\simeq\mathsf{B}\Omega^{n}\Sigma^{n}V\simeq\Omega^{n-1}\Sigma^{n}V\simeq\free_{n-1}(\Sigma V). As such, this result could have been proved longed ago, as it fits naturally into works such as [Ma] and [Coh]. We note lastly that the limiting statement as nn increases gives the well-known equivalence 𝖑𝖺𝗋⁑(𝖲𝗒𝗆⁑(V))≃𝖲𝗒𝗆⁑(Σ​V){\sf Bar}\bigl({\sf Sym}(V)\bigr)\simeq{\sf Sym}(\Sigma V).

This result has an important consequence for the relation between the ∞\oo-categories of augmented nn-disk algebras and augmented (nβˆ’1)(n-1)-disk algebras:

0N5I

Theorem 5.11. Let 𝒱\mathcal{V} be a symmetric monoidal ∞\oo-category which is βŠ—\otimes-presentable. There is an adjunction

𝖑𝖺𝗋:π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)β‡†π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡βˆ’πŸ£π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱):Ξ©{\sf Bar}:\Alg_{\disk_{n}^{\fr}}^{\sf aug}(\mathcal{V})\leftrightarrows\Alg_{\disk_{n-1}^{\fr}}^{\sf aug}(\mathcal{V}):\Omega

where the functors are given by the bar construction and by a functor Ξ©\Omega which, on underlying objects of 𝒱\mathcal{V}, is the based loop functor.

0N5J

Proof. We first show that the bar construction defines a functor 𝖑𝖺𝗋:π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)β†’π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡βˆ’πŸ£π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱){\sf Bar}\colon\Alg_{\disk_{n}^{\fr}}^{\sf aug}(\mathcal{V})\rightarrow\Alg_{\disk_{n-1}^{\fr}}^{\sf aug}(\mathcal{V}). This is so in as much as π–‘π–Ίπ—‹β‰ƒβˆ«π”»1×ℝnβˆ’1{\sf Bar}\simeq\int_{\mathbb{D}^{1}\times\mathbb{R}^{n-1}} is the object in 𝒱\mathcal{V} underlying the augmented β„°nβˆ’1\mathcal{E}_{n-1}-algebra π’Ÿβ€‹π—‚π—Œπ—„π—‡βˆ’πŸ£π–Ώπ—‹β†’π”»πŸ£Γ—βˆ’β„³β€‹π–Ώπ—…π–½nβˆ‚,π–Ώπ—‹β†’βˆ«A𝒱\disk^{\sf fr}_{n-1}\xrightarrow{\mathbb{D}^{1}\times-}\mfld^{\partial,\sf fr}_{n}\xrightarrow{\int A}\mathcal{V}. We will now argue that this functor carries colimit diagrams to colimit diagrams.

Proposition 5.9 gives a commutative diagram among ∞\infty-categories:

π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)\textstyle{\Alg_{\disk^{\fr}_{n}}^{\sf aug}(\mathcal{V})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}𝖑𝖺𝗋\scriptstyle{{\sf Bar}}π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡βˆ’πŸ£π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)\textstyle{\Alg_{\disk^{\fr}_{n-1}}^{\sf aug}(\mathcal{V})}𝒱\textstyle{\mathcal{V}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π–₯𝗋𝖾𝖾𝗇\scriptstyle{\free_{n}}Ξ£\scriptstyle{\Sigma}𝒱.\textstyle{\mathcal{V}\ignorespaces\ignorespaces\ignorespaces\ignorespaces.}π–₯π—‹π–Ύπ–Ύπ—‡βˆ’πŸ£\scriptstyle{\free_{n-1}}

As a consequence, the functor 𝖑𝖺𝗋{\sf Bar} preserves coproducts of free β„°n\mathcal{E}_{n}-algebras. We next argue that 𝖑𝖺𝗋{\sf Bar} preserves sifted colimits. Using that the symmetric monoidal structure of 𝒱\mathcal{V} distributes over colimits, it is enough to argue that factorization homology ∫M:π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)→𝒱\int_{M}\colon\Alg^{\sf aug}_{\disk^{\sf fr}_{n}}(\mathcal{V})\to\mathcal{V} carries sifted colimit diagrams to colimit diagrams, for each framed nn-manifold MM possibly with boundary.

So let A:Jβ†’π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹π–Ίπ—Žπ—€β‘(𝒱)A\colon J\to\Alg_{\disk^{\sf fr}_{n}}^{\sf aug}(\mathcal{V}) be a diagram of augmented β„°n\mathcal{E}_{n}-algebras in 𝒱\mathcal{V}, indexed by a sifted ∞\infty-category JJ. The canonical arrow π–Όπ—ˆπ—…π—‚π—†j∈J​𝖑𝖺𝗋​(𝖠𝗃)βŸΆπ–‘π–Ίπ—‹β‘(π–Όπ—ˆπ—…π—‚π—†π—ƒβˆˆπ–©β€‹π– π—ƒ)\underset{j\in J}{\colim}~{\sf Bar}(A_{j})\longrightarrow{\sf Bar}(\underset{j\in J}{\colim}A_{j}) in 𝒱\mathcal{V} is a composite

π–Όπ—ˆπ—…π—‚π—†π—ƒβˆˆπ–©π–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚,𝖿𝗋​𝖠𝗃​(𝖴)β‰ƒπ–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/(𝖬CLOSEβˆ‚,π–Ώπ—‹π–Όπ—ˆπ—…π—‚π—†π—ƒβˆˆπ–©β€‹π– π—ƒβ€‹(𝖴)βŸΆπ–Όπ—ˆπ—…π—‚π—†π–΄βˆˆπ’Ÿβ€‹π—‚π—Œπ—„π—‡/π–¬βˆ‚,𝖿𝗋(π–Όπ—ˆπ—…π—‚π—†π—ƒβˆˆπ–©π– π—ƒ)​(𝖴)\colim_{j\in J}\colim_{U\in\disk^{\partial,\sf fr}_{n/M}}A_{j}(U)~\simeq~\colim_{U\in\disk^{\partial,\sf fr}_{n/(M}}\colim_{j\in J}A_{j}(U)\longrightarrow\colim_{U\in\disk^{\partial,\sf fr}_{n/M}}(\colim_{j\in J}A_{j})(U)

where the outer objects are in terms of the defining expression for factorization homology, the left equivalence is through commuting colimits, and the right arrow is a colimit of canonical arrows. Again using that the symmetric monoidal structure of 𝒱\mathcal{V} distributes over colimits, each arrow π–Όπ—ˆπ—…π—‚π—†j∈J​𝖠𝗃​(𝖴)β†’(π–Όπ—ˆπ—…π—‚π—†π—ƒβˆˆπ–©β€‹π– π—ƒ)​(𝖴)\underset{j\in J}{\colim}A_{j}(U)\to(\underset{j\in J}{\colim}A_{j})(U) is an equivalence if and only if it is for UU connected. This is the case provided the forgetful functor 𝖾𝗏ℝn:𝖠𝗅𝗀nπ–Ίπ—Žπ—€β‘(𝒱)→𝒱{\sf ev}_{\mathbb{R}^{n}}\colon\Alg_{n}^{\sf aug}(\mathcal{V})\to\mathcal{V} preserves sifted colimits. This assertion is PropositionΒ 3.2.3.1 ofΒ [Lu2].

Continuing, we conclude that 𝖑𝖺𝗋{\sf Bar} preserves all coproducts, since any coproduct is a geometric realization of coproducts of free algebras (this is a consequence of the ∞\infty-categorical Barr–Beck TheoremΒ 4.7.4.5 ofΒ [Lu2]; seeΒ Β§4.7 thereof for a general discussion). Now, coproducts and geometric realizations generate all colimits, and we conclude that 𝖑𝖺𝗋{\sf Bar} is a colimit preserving functor from nn-disk algebras to (nβˆ’1)(n-1)-disk algebras.

To complete the proof, both of the ∞\infty-categories in the adjunction are presentable (see Corollary 3.2.3.3 ofΒ [Lu2]). The adjoint functor theorem (CorollaryΒ 5.5.2.9 ofΒ [Lu1]) can thus be applied to conclude that 𝖑𝖺𝗋{\sf Bar} is a left adjoint. The diagram above is therefore a commutative diagram of left adjoints, and therefore their right adjoints commute. Consequently, 𝖑𝖺𝗋{\sf Bar} has a right adjoint which, at the level of objects of 𝒱\mathcal{V}, agrees with based loops Ξ©\Omega, which is right adjoint to suspension Ξ£\Sigma.

∎

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Remark 5.12. We interpret TheoremΒ 5.11 in terms of Koszul duality, after [GiK] and [Pr]. Given the calculation of the Koszul dual operad 𝔻​ℰn≃ℰn​[βˆ’n]\mathbb{D}\mathcal{E}_{n}\simeq\mathcal{E}_{n}[-n], computed at the level of homology by Getzler and Jones [GJ] and computed in chain complexes by Fresse [Fre], these functors should be equivalent to restriction and induction along the Koszul dual of the map β„°nβˆ’1β†’β„°n\mathcal{E}_{n-1}\rightarrow\mathcal{E}_{n}. However, Theorem 5.11 is more general: it holds unstably (for instance, when 𝒱\mathcal{V} is π–²π—‰π–Ίπ–Όπ–Ύπ—Œ\spaces), whereas this operadic form of Koszul duality would require 𝒱\mathcal{V} to be stable.

5.3. Factorization homology from Lie algebras

We now discuss factorization homology of nn-disk algebras coming from Lie algebras. Our results are closely analogous to those above about the factorization homology of nn-disk algebras coming from topological spaces. For simplicity, we assume our Lie algebras are defined over a fixed field kk of characteristic zero.

As we proceed, we make use of the fact that Lie algebras in π–¬π—ˆπ–½k{\sf Mod}_{k} admit totalizations, and therefore the ∞\infty-category of such is cotensored over pointed spaces in a natural and standard way: (X,𝔀)↦𝔀X(X,\mathfrak{g})\mapsto{\mathfrak{g}}^{X}. For MM an nn-manifold, we notate 𝖬𝖺𝗉𝖼⁑(𝖬,𝔀):=𝔀𝖬+\Map_{\sf c}(M,\mathfrak{g}):={\mathfrak{g}}^{M^{+}}, where M+M^{+} is the 1-point compactification. One can describe this as 𝖬𝖺𝗉𝖼⁑(M,𝔀)β‰ƒπ–’π–Όβˆ—β€‹(M,𝔀)\Mapc(M,\mathfrak{g})\simeq\mathsf{C}_{\sf c}^{\ast}(M,\mathfrak{g}), the compactly supported cochains of MM with coefficients in 𝔀\mathfrak{g}. See also [Gw] and [CG] for a discussion of the following.

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Proposition 5.13. For 𝔀\mathfrak{g} a Lie algebra over kk, there is a natural equivalence of chain complexes over kk,

∫Mπ–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(ℝn,𝔀))β‰ƒπ–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(M,𝔀)),\int_{M}\mathsf{C}_{\ast}^{\Lie}\bigl(\Mapc(\mathbb{R}^{n},\mathfrak{g})\bigr)~\simeq~\mathsf{C}^{\Lie}_{\ast}\bigl(\Mapc(M,\mathfrak{g})\bigr)~,

between the factorization homology of the Lie algebra chains of Ξ©n​𝔀\Omega^{n}{\mathfrak{g}} and the Lie algebra chains of the Lie algebra 𝔀M+\mathfrak{g}^{M^{+}}.

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Proof. Lie algebra chains defines a functor between ∞\infty-categories π–’βˆ—π–«π—‚π–Ύ:𝖠𝗅𝗀𝖫𝗂𝖾⁑(π–¬π—ˆπ–½k)β†’π–¬π—ˆπ–½k\mathsf{C}^{\Lie}_{\ast}:\Alg_{\Lie}({\sf Mod}_{k})\rightarrow{\sf Mod}_{k}. This functor carries finite products of Lie algebras to finite tensor products of kk-modules, which is to say that it is symmetric monoidal. Furthermore, this functor preserves geometric realizations, so Lemma 3.25 applies to give a natural identification: ∫Mπ–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(ℝn,𝔀))β‰ƒπ–’βˆ—π–«π—‚π–Ύβ€‹(∫M𝖬𝖺𝗉𝖼⁑(ℝn,𝔀))\int_{M}\mathsf{C}_{\ast}^{\Lie}\bigl(\Mapc(\mathbb{R}^{n},\mathfrak{g})\bigr)\simeq\mathsf{C}_{\ast}^{\Lie}\bigl(\int_{M}\Mapc(\mathbb{R}^{n},\mathfrak{g})\bigr). The equivalence ∫M𝖬𝖺𝗉𝖼⁑(ℝn,𝔀)≃𝖬𝖺𝗉𝖼⁑(M,𝔀)\int_{M}\Mapc(\mathbb{R}^{n},\mathfrak{g})\simeq\Mapc(M,\mathfrak{g}) now follows from the argument of nonabelian PoincarΓ© duality (CorollaryΒ 4.6), only here we apply it in the usual abelian setting.66 6 See [AF2] for a complete account, where nonabelian PoincarΓ© duality is an instance of a version of PoincarΓ©/Koszul duality for Cartesian-presentable ∞\infty-categories.

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Remark 5.14. The nn-disk algebra π–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(ℝn,𝔀))\mathsf{C}_{\ast}^{\Lie}\bigl(\Mapc(\mathbb{R}^{n},\mathfrak{g})\bigr) has an interesting separate interpretation that we state here, and prove as a separate work. There is a forgetful functor from β„°n\mathcal{E}_{n}-algebras in chain complexes over kk to Lie algebras over kk (seeΒ [Coh] for an account at the level of homology). The adjoint functor theorem (CorollaryΒ 5.5.2.9 ofΒ [Lu1]) applies to this functor, and so there is an adjunction

𝖴n:𝖠𝗅𝗀𝖫𝗂𝖾⁑(π–¬π—ˆπ–½k)β‡„π– π—…π—€π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹β‘(π–¬π—ˆπ–½k):𝖿𝗀𝗍.\mathsf{U}_{n}\colon\Alg_{\Lie}({\sf Mod}_{k})~\rightleftarrows~\Alg_{\disk_{n}^{\sf fr}}({\sf Mod}_{k})\colon{\sf fgt}~.

In the case n=1n=1, this left adjoint 𝖴1\mathsf{U}_{1} agrees with the familiar universal enveloping algebra functor. In general, there is an identification of π’Ÿβ€‹π—‚π—Œπ—„π—‡π–Ώπ—‹\disk_{n}^{\sf fr}-algebras,

𝖴nβ€‹π”€β‰ƒπ–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(ℝn,𝔀)),\mathsf{U}_{n}\mathfrak{g}~\simeq~\mathsf{C}_{\ast}^{\Lie}\bigl(\Mapc(\mathbb{R}^{n},\mathfrak{g})\bigr)~,

through which PropositionΒ 5.13 can be reformulated as an equivalence of chain complexes over kk:

∫M𝖴nβ€‹π”€β‰ƒπ–’βˆ—π–«π—‚π–Ύβ€‹(𝖬𝖺𝗉𝖼⁑(M,𝔀)).\int_{M}\mathsf{U}_{n}\mathfrak{g}~\simeq~\mathsf{C}^{\Lie}_{\ast}\bigl(\Mapc(M,\mathfrak{g})\bigr)~.

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

David Ayala, John Francis

Original source: arXiv:1206.5522v6