ScalingStacks

5.1. An algebra for the lasagna operad

Throughout this section we assume familiarity with planar algebras [Jon99].

L1⊂S1{\color[rgb]{1,0,0}L_{1}}{\subset}S_{1}L2⊂S2{\color[rgb]{1,0,0}L_{2}}{\subset}S_{2}L3⊂S3{\color[rgb]{1,0,0}L_{3}}{\subset}S_{3}L⊂S{\color[rgb]{1,0,0}L}{\subset}SΣ{\color[rgb]{1,0.5,0}\Sigma}Σ{\color[rgb]{1,0.5,0}\Sigma}Σ{\color[rgb]{1,0.5,0}\Sigma}
Figure 2. A lasagna diagram, projected into 3d
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Definition 5.1. A lasagna algebra ℒ{\mathcal{L}} consists of

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    for each link LL in a 3-sphere SS, a (bigraded) abelian group ℒ⁡(S,L){\mathcal{L}}(S,L), which depends functorially on the pair (S,L)(S,L),

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    for each lasagna diagram DD, which, by definition, consists of a 4-ball BB, with a finite collection of disjoint 4-balls BiB_{i} removed from the interior, with boundary components SS (on the outside) and SiS_{i} (the boundaries of the removed interior balls BiB_{i}), and properly embedded framed oriented surface Σ\Sigma in the complementary region, meeting the boundary spheres in links LL and LiL_{i} (see Figure 2), a (homogeneous) homomorphism

    ℒ⁡(D):⨂iℒ⁡(Si,Li)→ℒ⁡(S,L),{\mathcal{L}}(D):\bigotimes_{i}{\mathcal{L}}(S_{i},L_{i})\to{\mathcal{L}}(S,L),

    such that

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    surfaces Σ\Sigma and Σ′\Sigma^{\prime} which are isotopic rel boundary induce identical homomorphisms,

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    if f:D→D′f:D\to D^{\prime} is a diffeomorphism between lasagna diagrams, then the square

    ⨂iℒ⁡(Si,Li){\lx@inpgf@ignorespaces\bigotimes_{i}{\mathcal{L}}(S_{i},L_{i})}ℒ⁡(S,L){\lx@inpgf@ignorespaces{\mathcal{L}}(S,L)}⨂iℒ⁡(f⁡(Si),f⁡(Li)){\lx@inpgf@ignorespaces\bigotimes_{i}{\mathcal{L}}(f(S_{i}),f(L_{i}))}ℒ⁡(f⁡(S),f⁡(L)){\lx@inpgf@ignorespaces{\mathcal{L}}(f(S),f(L))}ℒ⁡(D)\scriptstyle{\lx@inpgf@ignorespaces{\mathcal{L}}(D)}⨂iℒ⁡(f|Si)\scriptstyle{\lx@inpgf@ignorespaces\bigotimes_{i}{\mathcal{L}}(f|_{S_{i}})}ℒ⁡(f|S)\scriptstyle{\lx@inpgf@ignorespaces{\mathcal{L}}(f|_{S})}ℒ⁡(D′)\scriptstyle{\lx@inpgf@ignorespaces{\mathcal{L}}(D^{\prime})}

    commutes,

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    a ‘radial’ surface L×[0,1]⊂S×[0,1]L\times{[0,1]}\subset S\times{[0,1]} induces the identity map ℒ⁡(S,L)→ℒ⁡(S,L){\mathcal{L}}(S,L)\to{\mathcal{L}}(S,L) (or more precisely, mapping cylinders of diffeomorphisms induce the same map specified for that diffeomorphism by functoriality),

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    gluing of a ‘smaller’ lasagna diagram into one of the removed balls of a ‘larger’ lasagna diagram (with compatible boundaries) to obtain a single lasagna diagram is compatible with the corresponding composition of homomorphisms.

We won’t actually spell this out in detail, but one can easily extract from this definition the notion of the lasagna operad (actually a coloured operad, with colours corresponding to links), and that a lasagna algebra is an algebra for that operad. One can of course consider lasagna algebras valued in symmetric monoidal categories other than (bigraded) abelian groups.

The ‘one input ball’ part of a lasagna algebra is essentially equivalent to a functorial invariant of links in 3-spheres: we have an abelian group for each such link, and homomorphisms for cobordisms between them, which compose appropriately. It is not immediately clear that any such functorial invariant extends to a full lasagna algebra, with well-defined operations for multiple input balls. The goal in this section is to show that this is the case for Khovanov–Rozansky homology. In fact, our argument shows that any functorial invariant of links and cobordisms in 3-spheres which satisfies the monoidality property and sweep-around move extends to a lasagna algebra.

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Theorem 5.2. Khovanov–Rozansky homology affords the structure of a lasagna algebra.

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Proof. For a lasagna diagram DD (as in Figure 2) we define a homomorphism

KhRN​(D):⨂iKhRN​(Si,Li)→KhRN​(S,L),\mathrm{KhR}_{N}(D):\bigotimes_{i}\mathrm{KhR}_{N}(S_{i},L_{i})\to\mathrm{KhR}_{N}(S,L),

as follows. We first choose points qj∈Sj∖Ljq_{j}\in S_{j}\setminus L_{j} and q∈S∖Lq\in S\setminus L and then a properly embedded 1-complex T⊂BT\subset B, disjoint from Σ\Sigma, such that the underlying graph of TT is a tree and the endpoints of the 1-complex are {qj,q}\{q_{j},q\}. Choose a small closed tubular neighborhood NN of TT, also disjoint from YY. The complement of NN in B∖⊔BiB\setminus\sqcup B_{i} is diffeomorphic to ℝ3×[0,1]{\mathbb{R}}^{3}\times[0,1] with some embedded surface Σ′\Sigma^{\prime}. We will view Σ′\Sigma^{\prime} as a bordism between two links in two copies of ℝ3{\mathbb{R}}^{3}. One copy is identified with Sq:=S∖{q}S^{q}:=S\setminus\{q\}, which contains the link LL. The other copy XX is the remainder of the boundary, and can be expressed as the boundary connect sum of the 3-balls Siqi:=Si∖{qi}S_{i}^{q_{i}}:=S_{i}\setminus\{q_{i}\}, connected along the tree TT. The 3-ball XX contains the split disjoint union of the links LiL_{i}. Khovanov–Rozansky homology for links in 3-balls gives us a map

KhRN(Σ′):KhRN(X,⊔iLi)→KhRN(Sq,L)\mathrm{KhR}_{N}(\Sigma^{\prime}):\mathrm{KhR}_{N}(X,\sqcup_{i}L_{i})\to\mathrm{KhR}_{N}(S^{q},L)

which, together with the monoidality maps from §4.3, specifies a map

KhRN​(D):⨂iKhRN​(Si,Li)\displaystyle\mathrm{KhR}_{N}(D):\bigotimes_{i}\mathrm{KhR}_{N}(S_{i},L_{i}) ≅⨂iKhRN(Siqi,Li)→TKhRN(X,⊔iLi)→KhRN(Sq,L)≅KhRN(S,L).\displaystyle\cong\bigotimes_{i}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\stackrel{{\scriptstyle T}}{{\to}}\mathrm{KhR}_{N}(X,\sqcup_{i}L_{i})\to\mathrm{KhR}_{N}(S^{q},L)\cong\mathrm{KhR}_{N}(S,L).

Here the first and last maps are the ‘evaluation’ isomorphisms discussed below Definition 4.12, and we highlight that the monoidality map depends on the tree TT.

We must check that the overall map above does not depend on the choices of qiq_{i} and TT. This is straightforward, so we merely sketch the argument. Isotoping the points qiq_{i} does not change the map, by the same argument that showed that KhRN\mathrm{KhR}_{N} is well-defined for links in 3-spheres; see §4.2. Isotoping TT disjointly from Σ\Sigma clearly does not affect the map. Changing the combinatorics of the underlying tree of TT can be done in such a way that NN varies continuously and remains far from Σ\Sigma, and so does not affect the map. Isotoping TT through Σ\Sigma does not affect the map, thanks to the sweep-around property (see Theorem 1.1 above). Thus KhRN​(Σ)\mathrm{KhR}_{N}(\Sigma) is well-defined.

Next we must show compatibility with the operad composition. For this we consider three lasagna diagrams:

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    D1D_{1} with output boundary (S1,L1,q1)(S_{1},L_{1},q_{1}), with input boundaries (Si,Li,qi)i∈J(S_{i},L_{i},q_{i})_{i\in J}, surface Σ1\Sigma_{1}, and tree T1T_{1},

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    D2D_{2} with output boundary (S2,L2,q2)(S_{2},L_{2},q_{2}), with input boundaries (S1,L1,q1)(S_{1},L_{1},q_{1}) along with (Si,Li,qi)i∈K(S_{i},L_{i},q_{i})_{i\in K}, surface Σ2\Sigma_{2}, and tree T2T_{2}

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    DD, the result of gluing D1D_{1} inside D2D_{2}, with outer boundary (S2,L2,q2)(S_{2},L_{2},q_{2}), input boundary (Si,Li,qi)i∈J∪K(S_{i},L_{i},q_{i})_{i\in J\cup K}, surface Σ=Σ1∪Σ2\Sigma=\Sigma_{1}\cup\Sigma_{2}, and tree T=T1∪T2T=T_{1}\cup T_{2}.

Compatibility with the operad composition now boils down to the claim:

KhRN​(D)=KhRN​(D2)∘(KhRN​(D1)⊗𝟏)\mathrm{KhR}_{N}(D)=\mathrm{KhR}_{N}(D_{2})\circ(\mathrm{KhR}_{N}(D_{1})\otimes\mathbf{1})

as maps

(⨂i∈JKhRN​(Si,Li))⊗(⨂i∈KKhRN​(Si,Li))→KhRN​(S2,L2)\left(\bigotimes_{i\in J}\mathrm{KhR}_{N}(S_{i},L_{i})\right)\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i},L_{i})\right)\to\mathrm{KhR}_{N}(S_{2},L_{2})

We compare these two homomorphisms on the level of 3-ball link homologies, that is, with respect to a fixed choice of basepoints qiq_{i} and qq, and we suppress associators. On this level KhRN​(D)\mathrm{KhR}_{N}(D) is determined by the homomorphism

(5.1) (⨂i∈JKhRN(Siqi,Li))⊗(⨂i∈KKhRN(Siqi,Li))→𝑇KhRN(X,⊔iLi)→KhRN(S2q,L2)\left(\bigotimes_{i\in J}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\xrightarrow{T}\mathrm{KhR}_{N}(X,\sqcup_{i}L_{i})\to\mathrm{KhR}_{N}(S_{2}^{q},L_{2})

where XX denotes the boundary connect sum of the 3-balls SiqiS_{i}^{q_{i}} for i∈J∪Ki\in J\cup K along the tree TT, and the first map is provided by lax monoidality. On the other hand, the homomorphism KhRN​(D2)∘(KhRN​(D1)⊗𝟏)\mathrm{KhR}_{N}(D_{2})\circ(\mathrm{KhR}_{N}(D_{1})\otimes\mathbf{1}) is determined by the composite

(⨂i∈JKhRN​(Siqi,Li))⊗(⨂i∈KKhRN​(Siqi,Li))→T1⊗𝟏\displaystyle\left(\bigotimes_{i\in J}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\xrightarrow{T_{1}\otimes\mathbf{1}} KhRN(XJ,⊔i∈JLi)⊗(⨂i∈KKhRN(Siqi,Li))\displaystyle\;\mathrm{KhR}_{N}(X_{J},\sqcup_{i\in J}L_{i})\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)
→KhRN​(Σ1′)⊗𝟏\displaystyle\xrightarrow{\mathrm{KhR}_{N}(\Sigma^{\prime}_{1})\otimes\mathbf{1}} KhRN​(S1q1,L1)⊗(⨂i∈KKhRN​(Siqi,Li))\displaystyle\;\mathrm{KhR}_{N}(S_{1}^{q_{1}},L_{1})\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)
→T2\displaystyle\xrightarrow{T_{2}} KhRN(XK,⊔i∈{1}∪KLi)\displaystyle\;\mathrm{KhR}_{N}(X_{K},\sqcup_{i\in\{1\}\cup K}L_{i})
→KhRN​(Σ2′)\displaystyle\xrightarrow{\mathrm{KhR}_{N}(\Sigma^{\prime}_{2})} KhRN​(S2q,L2).\displaystyle\;\mathrm{KhR}_{N}(S_{2}^{q},L_{2}).

Here we write XJX_{J} for the boundary connect sum of the 3-balls Siqi:=Si∖{qi}S_{i}^{q_{i}}:=S_{i}\setminus\{q_{i}\} for i∈Ji\in J that is determined by T1T_{1}, and XKX_{K} for the boundary connect sum of the SiqiS_{i}^{q_{i}} for i∈{1}∪Ki\in\{1\}\cup K along T2T_{2}. After commuting the map induced by Σ1′\Sigma^{\prime}_{1} past the second monoidality map, we arrive at

(5.2) (⨂i∈JKhRN(Siqi,Li))⊗(⨂i∈KKhRN(Siqi,Li))→𝑇KhRN(X,⊔i∈J∪KLi)→KhRN​(Σ2′∘(Σ1′∪𝟏))KhRN(S2q,L2).\left(\bigotimes_{i\in J}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\otimes\left(\bigotimes_{i\in K}\mathrm{KhR}_{N}(S_{i}^{q_{i}},L_{i})\right)\xrightarrow{T}\mathrm{KhR}_{N}(X,\sqcup_{i\in J\cup K}L_{i})\xrightarrow{\mathrm{KhR}_{N}(\Sigma^{\prime}_{2}\circ(\Sigma^{\prime}_{1}\cup\mathbf{1}))}\mathrm{KhR}_{N}(S_{2}^{q},L_{2}).

Since the link cobordism Σ2′∘(Σ1′∪𝟏)\Sigma^{\prime}_{2}\circ(\Sigma^{\prime}_{1}\cup\mathbf{1}) is isotopic to Σ\Sigma, the functoriality of KhRN\mathrm{KhR}_{N} implies that the maps in (5.1) and (5.2) are equal. This proves the claim. ∎

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

Scott Morrison, Kevin Walker, Paul Wedrich

Original source: arXiv:1907.12194v5