ScalingStacks

4.6. Comparison with the Rozansky–Willis invariant

In [31], Rozansky defined a Khovanov-type homology theory for (null-homologous) links in S1×S2S^{1}\times S^{2}. His construction was generalized by Willis in [33] to null-homologous links in Y=#m​(S1×S2)Y=\#^{m}(S^{1}\times S^{2}) for any mm. We will denote the Rozansky-Willis homology of L⊂YL\subset Y by HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L). Just like the skein lasagna module 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L), the invariant HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) can be computed from a Kirby diagram for W1=♮m​(S1×B3)W_{1}=\natural^{m}(S^{1}\times B^{3}) including the link LL, so it is a natural question whether they are related.

The first observation is that the two invariants are not always isomorphic. Indeed, in any specific bidegree, HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) is defined as the Khovanov homology of the link in S3S^{3} obtained from LL by adding sufficiently many twists in place of the 1-handles. It follows that HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) has finite rank in each bidegree, whereas this may not hold for 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L), as we have seen in Theorem 4.23. Another concrete example is for m=1m=1, where L=S1×P1L=S^{1}\times P_{1} yields a 44-dimensional lasagna skein module according to Proposition 4.15, but HRW∗,∗​(L)≅HH∙⁡(𝕜⁡[X]/(X2))H^{*,*}_{\operatorname{RW}}(L)\cong\operatorname{HH}_{\bullet}(\mathbbm{k}[X]/(X^{2})) is infinite-dimensional.

However, HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) and 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L) are conceptually similar, as both arise as the Hochschild homology of a chain complex associated to a tangle TT that closes to the link LL:

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    HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) is computed as the Hochschild homology of a dg bimodule (for a tensor product of mm of Khovanov’s arc rings) associated to the tangle TT, as defined for m=1m=1 by Khovanov in [18] and extended by parabolic induction to m>1m>1. Here the homological degree of the dg bimodule gets mixed with the Hochschild degree, and so the resulting invariant is a bigraded vector space.

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    𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L) can be computed via Theorem 4.7 (and for m=1m=1 even more concretely in Corollary 4.10) as the zeroth Hochschild homology of an equivalent dg bimodule; see Remark 4.13 for the comparison. In fact, the higher blob homology from [27], which does not play a role for skein lasagna modules, corresponds to higher Hochschild homology. The main difference, however, is that the dg bimodule is not considered as an object of a dg or triangulated category, but of the linear cohomology category. Accordingly, the full blob homology is triply-graded, with the blob/Hochschild grading separated from the homological grading.

Based on this comparison, one may expect 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L) and, more generally, the full blob homology 𝒮∗N​(W1,L)\mathcal{S}^{N}_{*}(W_{1};L) to appear on the E2E_{2} page of a spectral sequence converging to HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L). Suppose that one can find a suitable projective resolution in terms of tangle complexes, which simultaneously allows the computation of blob homology as well as the dg version of Hochschild homology. Then, by tensoring with the dg bimodule associated to the tangle, one obtains a double complex of (quantum) graded vector spaces, where the vertical differential carries Hochschild degree and the horizontal differential carries homological degree. The homology of the total complex would compute HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L). To obtain 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L), one first takes homology in the rows (thus computing the Khovanov homologies of links of the form Ti∪T¯T_{i}\cup\overline{T} where TiT_{i} appears in the resolution), and only then the zeroth homology of the induced differential coming from the resolution. We will not pursue this comparison further in the present paper, but remark that there is precedent for interesting invariants appearing on E2E_{2} pages of spectral sequences that come from separating Hochschild and homological degrees, namely the triply-graded HOMFLYPT link homology; see [29, Section 6].

In general, one does not expect a map from the E2E_{2} page of a spectral sequence to its E∞E_{\infty} page. However, since 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L) appears as the lowest row on the E2E_{2} page, the above discussion suggests the existence of a natural map

𝒮02​(W1,L)→HRW∗,∗​(L).\mathcal{S}_{0}^{2}(W_{1},L)\to H^{*,*}_{\operatorname{RW}}(L).

In the following we propose a candidate for such a map.

In Willis’s construction of HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L), we represent ∂W1=Y\partial W_{1}=Y by mm pairs of spheres in the plane, with the spheres in each pair being identified (that is, we add a handle). This is the same as the usual Kirby diagram of W1W_{1}. The link LL may intersect each handle a number of times, as in this picture:

L Original paper diagram

Let L⁡(n1,…,nm)L(n_{1},\dots,n_{m}) be the link in S3S^{3} obtained from LL by inserting nin_{i} full twists in place of the ithi^{\operatorname{th}} handle, as shown here:

n i Original paper diagram

The homology HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) can be computed as the Khovanov homology of the link L⁡(n1,…,nm)L(n_{1},\dots,n_{m}) for ni≫0n_{i}\gg 0, with some suitable shifts in grading. Note that L⁡(n1,…,nm)L(n_{1},\dots,n_{m}) depends on the choice of a path between the attaching spheres of each 1-handle; however, it can be shown that HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L) is independent of these choices up to isomorphism.

Consider now the skein lasagna module 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L). Let us attach an nin_{i}-framed 2-handle through the ithi^{\operatorname{th}} 1-handle:

L Original paper diagram n i Original paper diagram

The 2-handles cancel the corresponding 1-handles, so the result is a Kirby diagram for B4B^{4}, whose boundary is S3S^{3}. The link LL becomes L⁡(n1,…,nm)⊂S3L(n_{1},\dots,n_{m})\subset S^{3}, as can be seen by doing a series of handle slides of the arcs of LL over the 2-handle:

Original paper diagram n i Original paper diagram n i Original paper diagram n i Original paper diagram n i

where in the last step we cancelled the handles. (Compare Figure 5.13 in [10].)

The 2-handle attachments give a cobordism ZZ from Y=#m​(S1×S2)Y=\#^{m}(S^{1}\times S^{2}) to S3S^{3}. There is also an embedded annular cobordism S⊂ZS\subset Z from LL to L⁡(n1,…,nm)L(n_{1},\dots,n_{m}). As discussed in Section 2.2, these cobordisms induce a map on skein lasagna modules:

ΨZ;S:𝒮02​(W1,L)→𝒮02​(B4,L⁡(n1,…,nm))≅Kh⁡(L⁡(n1,…,nm)).\Psi_{Z;S}:\mathcal{S}_{0}^{2}(W_{1};L)\to\mathcal{S}_{0}^{2}(B^{4};L(n_{1},\dots,n_{m}))\cong\operatorname{Kh}(L(n_{1},\dots,n_{m})).

Our conjecture is that these maps stabilize as ni→∞n_{i}\to\infty, giving a well-defined morphism from 𝒮02​(W1,L)\mathcal{S}_{0}^{2}(W_{1},L) to HRW∗,∗​(L)H^{*,*}_{\operatorname{RW}}(L).

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

Ciprian Manolescu, Kevin Walker, Paul Wedrich

Original source: arXiv:2206.04616v2