ScalingStacks

1.4. Heegaard Floer homology

Heegaard Floer homology, defined by Ozsváth–Szabó [OsSz1, OsSz2, OsSz3], is a set of invariants for 3- and 4-dimensional manifolds. For a 3-manifold YY, the Heegaard Floer invariant of YY (an abelian group) is defined by choosing a Heegaard decomposition of YY as two handlebodies glued along a genus-gg surface ℋ\mathcal{H}, then computing a Lagrangian intersection Floer homology group between two Lagrangian submanifolds in Symg​(ℋ)\mathrm{Sym}^{g}(\mathcal{H}) induced by the two handlebodies.

In bordered Heegaard Floer homology [LiOzTh1, Za], there are also extended Heegaard Floer invariants for 2d surfaces and 3d cobordisms. Let FF be the data of a surface (Σ,M)(\Sigma,M) with a set of points M⊂∂ΣM\subset\partial\Sigma as above, equipped with a choice of arc decomposition. To such a surface, bordered Heegaard Floer associates a differential algebra A⁡(F)A(F). Auroux [Au2] has shown that the algebra A⁡(F)A(F) is the endomorphism algebra of a generating object of ℱ​(Sym∗​(Σ),M)\mathcal{F}(\mathrm{Sym}^{*}(\Sigma),M) determined by the arc decomposition.

Our constructions are based on the combinatorics of A⁡(F)A(F) and we do not work directly with ℱ​(Sym∗​(Σ),M)\mathcal{F}(\mathrm{Sym}^{*}(\Sigma),M). Given a component of ∂Σ∖M\partial\Sigma\setminus M, we define a differential bimodule EE over A⁡(F)A(F), and a bimodule endomorphism τ\tau of E⊗A⁡(F)EE\otimes_{A(F)}E, that yield a higher representation of 𝔤​𝔩​(1|1)+\mathfrak{gl}(1|1)^{+}.

Theorem 1.3.1 follows now from the following result.

0P4J

Theorem 1.4.1. If F1F_{1} and F2F_{2} are surfaces with arc decompositions glued as in Theorem 1.3.1 to form FF, then

A(F)≅A(F1)⊗○A(F2)A(F)\cong A(F_{1}){\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}A(F_{2})

as higher representations of 𝔤​𝔩​(1|1)+\mathfrak{gl}(1|1)^{+}.

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2