ScalingStacks

2.2. Gluing and cobordisms

Let us consider two four-manifolds WW and ZZ that have some part YY of their boundaries in common, as follows:

∂W=Y∐Y0,∂Z=(−Y)∐Y1,\partial W=Y\amalg Y_{0},\ \ \partial Z=(-Y)\amalg Y_{1},

where ∐\amalg denotes disjoint union. We can glue WW and ZZ along YY to form a new four-manifold W∪ZW\cup Z with boundary Y0∐Y1Y_{0}\amalg Y_{1}. Suppose we are also given links L0⊂Y0L_{0}\subset Y_{0}, L1⊂Y1L_{1}\subset Y_{1} and L⊂YL\subset Y. Let L¯⊂−Y\overline{L}\subset-Y denote the mirror reverse of LL. Then, we have a map

(3) Ψ:𝒮0N​(W,L∪L0)⊗𝒮0N​(Z,L¯∪L1)→𝒮0N​(W∪Z,L0∪L1)\Psi:\mathcal{S}_{0}^{N}(W;L\cup L_{0})\otimes\mathcal{S}_{0}^{N}(Z;\overline{L}\cup L_{1})\to\mathcal{S}_{0}^{N}(W\cup Z;L_{0}\cup L_{1})

obtained by gluing lasagna fillings along LL:

[F]⊗[G]↦[F∪G].[F]\otimes[G]\mapsto[F\cup G].

It is easy to see that if two lasagna fillings F1F_{1} and F2F_{2} are equivalent in WW, and G1G_{1} and G2G_{2} are equivalent in ZZ, then F1∪G1F_{1}\cup G_{1} and F2∪G2F_{2}\cup G_{2} are equivalent in W∪ZW\cup Z, so (3) is well-defined.

Starting from here, we see that skein lasagna modules are functorial under inclusions, in the following sense. We consider the case when Y0=∅Y_{0}=\emptyset, and we fix a lasagna filling GG of ZZ with boundary L¯∪L1\overline{L}\cup L_{1}. We can think of ZZ as a cobordism from Y=∂WY=\partial W to Y1Y_{1}. Then, there is an induced cobordism map

(4) ΨZ;G=Ψ(⋅⊗[G]):𝒮0N(W;L)→𝒮0N(W∪Z;L1).\Psi_{Z;G}=\Psi(\cdot\otimes[G]):\mathcal{S}_{0}^{N}(W;L)\to\mathcal{S}_{0}^{N}(W\cup Z;L_{1}).

Observe that the maps (4) behave well with respect to compositions:

(5) ΨZ′;G′∘ΨZ;G=ΨZ∪Z′;G∪G′.\Psi_{Z^{\prime};G^{\prime}}\circ\Psi_{Z;G}=\Psi_{Z\cup Z^{\prime};G\cup G^{\prime}}.

Furthermore, in terms of the decompositions (2), given α∈H2L​(W,ℤ)\alpha\in H^{L}_{2}(W;{\mathbb{Z}}), by attaching to it the class of GG in H2L∪L1​(Z,ℤ)H_{2}^{L\cup L_{1}}(Z;{\mathbb{Z}}) we get a class α1∈H2L1​(W∪Z,ℤ)\alpha_{1}\in H_{2}^{L_{1}}(W\cup Z;{\mathbb{Z}}). Then, ΨZ;G\Psi_{Z;G} maps 𝒮0N​(W,L,α)\mathcal{S}_{0}^{N}(W;L,\alpha) to 𝒮0N​(W∪Z,L1,α1)\mathcal{S}_{0}^{N}(W\cup Z;L_{1},\alpha_{1}). We let

(6) ΨZ;G,α:𝒮0N​(W,L,α)→𝒮0N​(W∪Z,L1,α1)\Psi_{Z;G,\alpha}:\mathcal{S}_{0}^{N}(W;L,\alpha)\to\mathcal{S}_{0}^{N}(W\cup Z;L_{1},\alpha_{1})

denote the restriction of ΨZ;G\Psi_{Z;G}.

When the lasagna filling GG consists of a surface SS (an embedded cobordism S⊂ZS\subset Z from LL to L1L_{1}) with no input balls, we will simply write ΨZ;S,α\Psi_{Z;S,\alpha} for ΨZ;G,α\Psi_{Z;G,\alpha}. Furthermore, we could decorate SS with nn dots at a chosen location, for 0≤n≤N−10\leq n\leq N-1, as usual in 𝔤​𝔩N\mathfrak{gl}_{N} foams; cf. [27, Example 2.3]. This corresponds to constructing a lasagna filling S(n∙)S(n\bullet) with nn input balls intersecting SS along unknots, each decorated with the generator

X∈KhRN⁡(U)≅ℤ⁡[X]/(XN).X\in\operatorname{KhR}_{N}(U)\cong{\mathbb{Z}}[X]/(X^{N}).

(This filling is equivalent to one where we consider a single input ball intersecting SS in an unknot, decorated with XnX^{n}.) When the chosen location of the dot placement is clear from the context, then we denote the corresponding map by

(7) ΨZ;S(n∙),α:𝒮0N(W;L,α)→𝒮0N(W∪Z;L1,α1).\Psi_{Z;S(n\bullet),\alpha}:\mathcal{S}_{0}^{N}(W;L,\alpha)\to\mathcal{S}_{0}^{N}(W\cup Z;L_{1},\alpha_{1}).

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