ScalingStacks

The process of gluing a lasagna filling works as follows. Let F′F^{\prime} be a lasagna filling of B4B^{4} with boundary link LTL_{T} as above; i.e., inside S3=∂B4S^{3}=\partial B^{4} we have mm pairs of embedded 3-balls Bi∪Bi¯B_{i}\cup\overline{B_{i}}, such that LT∩Bi=TiL_{T}\cap B_{i}=T_{i} and LT∩Bi¯=T¯iL_{T}\cap\overline{B_{i}}=\overline{T}_{i} for 1≤i≤m1\leq i\leq m. Denote the numbers of boundary points by 2​pi:=|∂Ti|2p_{i}:=|\partial T_{i}|. Now we attach mm 1-handles with core-parallel lasagna sheets I×Ti⊂I×B3I\times T_{i}\subset I\times B^{3} along the Bi∪Bi¯≅S0×B3B_{i}\cup\overline{B_{i}}\cong S^{0}\times B^{3} to obtain a lasagna filling of W1W_{1} with boundary LL. Since the relations in 𝒮0N\mathcal{S}_{0}^{N} are local, this induces a map:

(17) glueLT:𝒮0N​(B4,LT,𝕜)​{(∑ipi)​(N−1)}→𝒮0N​(W1,L,𝕜)\mathrm{glue}_{L_{T}}\colon\mathcal{S}_{0}^{N}(B^{4};L_{T},\mathbbm{k})\{(\textstyle\sum_{i}p_{i})(N-1)\}\to\mathcal{S}_{0}^{N}(W_{1};L,\mathbbm{k})

The grading shift is there to compensate the change in Euler characteristic of the surfaces in lasagna fillings upon gluing.

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