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Calabi–Yau structures on topological Fukaya categories

Published online by Cambridge University Press:  27 August 2025

Vivek Shende
Affiliation:
Department of Mathematics, University of California, Berkeley, Berkeley, CA, 94720-3840, USA Current address: Centre for Quantum Mathematics, University of Southern Denmark, 5230, Odense M, Denmark vivek@math.berkeley.edu
Alex Takeda
Affiliation:
Department of Mathematics, Uppsala University, Uppsala, 752 37, Sweden alex.takeda@math.uu.se
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Abstract

We develop a local-to-global formalism for constructing Calabi–Yau structures for global sections of constructible sheaves or cosheaves of differential graded categories. The required data (a morphism between the sheafified Hochschild homology with the topological dualizing sheaf, satisfying a nondegeneracy condition) specializes to the classical notion of orientation when applied to the category of local systems on a manifold. We apply this construction to the cosheaves on arboreal skeleta arising in the microlocal approach to the A-model.

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Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original article is properly cited.
Copyright
© The Author(s), 2025.
Figure 0

Figure 1. Arboreal singularity $\overline {{\mathbb {A}}_2}$. For simplicity we use the notation described above for each correspondence.

Figure 1

Figure 2. Arboreal singularity $\overline {{\mathbb {A}}_3}$. This singularity is homeomorphic to a union of three 2-discs, along half-discs; in the figure above the grey disc is horizontal and the two white half-discs discs are glued to it along two perpendicular diameters, one to the top and another to the bottom. We only labelled the 0-simplices; the labels on all other simplices can be deduced from their vertices. The link ${\mathbb {A}}_3^{\mathrm {{link}}}$ can be seen to be homeomorphic to the 1-skeleton of a tetrahedron.

Figure 2

Figure 3. Stratification of the arboreal singularity $\overline {\mathbb {A}}_2$, by the strata ${\mathbb {A}}_2(\mathfrak p)$.

Figure 3

Figure 4. Gluing of $\overline {\mathbb {A}}_3$ from the discs ${\mathbb {A}}_3(\bullet )$. ${\mathbb {A}}_3(\alpha )$ and ${\mathbb {A}}_3(\gamma )$ are shown creased, with half-disc flaps pointing up and down, respectively.

Figure 4

Figure 5. The subsets ${\mathbb {A}}_3(\bullet ,\bullet )$ where ${\mathbb {A}}_3$ has the quiver structure $\alpha \rightarrow \beta \leftarrow \gamma$. The subsets ${\mathbb {A}}_3(\alpha ),{\mathbb {A}}_3(\beta ),{\mathbb {A}}_3(\gamma )$ are homeomorphic to closed discs, and the arboreal singularity is obtained by gluing them appropriately; on the left ${\mathbb {A}}_3(\alpha ),{\mathbb {A}}_3(\gamma )$ are shown with folded flaps up and down, and are glued along the horizontal parts to ${\mathbb {A}}_3(\beta )$. Note that the subsets ${\mathbb {T}}(\lambda _1,\lambda _2)$ depend on the directions of the arrows in $T$, and, moreover, as in the proof above for any vertices $\lambda _1,\lambda _2$, the difference between ${\mathbb {T}}(\lambda _1,\lambda _2)$ and ${\mathbb {T}}(\lambda _1) \cap {\mathbb {T}}(\lambda _2)$ is at most deletion of some boundary strata.

Figure 5

Figure 6. The generalized arboreal singularity corresponding to the singleton quiver $\vec {T} = \alpha$ with the vertex also a marked leaf $\ell = \{\alpha \}$. We delete two open subsets to get $\overline {\mathbb {T}}^*$; also shown is ${\mathbb {T}}^* = \overline {\mathbb {T}}^* \cap {\mathbb {T}}^+$.

Figure 6

Figure 7. The generalized arboreal singularity corresponding to the $A_2$ quiver $\vec T = \alpha \to \beta$ with marked leaf $\ell = \{\alpha \}$. Here we obtain $\overline {\mathbb {T}}^*$ from deleting some of the strata in the arboreal singularity $\overline {\mathbb {T}}^+$ corresponding to the augmented quiver $\alpha ^+ \to \alpha \to \beta$. The bottom right corner shows ${\mathbb {T}}^*$; note that it contains part of its boundary.

Figure 7

Figure 8. The pairs $({\mathbb {T}}(\alpha ),Z_\alpha )$ appearing in the Mayer–Vietoris decomposition. The complements $Z_\alpha = {\mathbb {T}}(\alpha )\setminus U_\alpha$ are in dark grey. The intersection pairs $({\mathbb {T}}(\alpha )\cap {\mathbb {T}}(\beta ),Z_\alpha \cap Z_\beta )$ have vanishing relative homology.

Figure 8

Figure 9. The case $d=2$. The neighbourhood of a point in the front projection of the Legendrian $\Lambda$ is homeomorphic to either ${\mathbb {A}}_2 \times {\mathbb {R}} = {\mathbb {S}} tar_1 \times {\mathbb {R}}$ or ${\mathbb {A}}_3 = {\mathbb {S}} tar_2$. Note that in general it is the star quivers $Star_k$ that appear, and not the $A_k$ series.

Figure 9

Figure 10. The coorientation of the front projection $\pi (\Lambda )$ defines a decomposition of $U \simeq {\mathbb {A}}_3$ into discs ${\mathbb {A}}_3(\alpha )$ labelled by each vertex of $A_3$. The choice of rooting is given by picking the centre vertex of the quiver (which labels the disc along $M$) to be the root.

Figure 10

Figure 11. The comb $\mathbb {X}$. We pick a decomposition of $\mathbb {X}$ into overlapping intervals; in this case the $i$th interval has endpoints $p_i$ and $+\infty$, and, extending the positive orientation on $\mathbb {R}$, its boundary is $(+\infty ) - (p_i)$.

Figure 11

Figure 12. On the surface $\Sigma$ with two punctures, and with fixed microlocal rank along the concentric circles of $\Lambda$. If we look at the substack of $\textrm{Sh}_\Lambda (\Sigma )$ of objects with rank zero at the punctures, the microlocal rank conditions mean we have rank-three local systems equipped with invariant filtrations near each puncture; in this particular case we have two filtrations respectively of the form $0\subset k\subset k^2 \subset k^3$ and $0\subset k \subset k^3$.

Figure 12

Figure 13. The restriction to the upper boundary components can be assembled into a map to $[{L}/{L}]$ where $L$ is a Levi subgroup of $G = GL_m$ given by the integers $\{m_i\}$. The restriction to the lower boundary components is a map to $[{G}/{G}]$ giving the monodromy of the $G$-local system.

Figure 13

Figure 14. The Legendrian link for the irregular type $( \begin{smallmatrix}1&0\\0&1 \end{smallmatrix})$$({1}/{z^3})$. The Legendrian link $\Lambda \subset T^\infty \Sigma$ is obtained by lifting the projection using the outward coorientation. The dashed lines are the Stokes rays, where the asymptotics of the formal solution changes. Note that each component of the link is unknotted with itself: this is true of all the examples of this form.

Figure 14

Figure 15. The Legendrian link for the irregular type $( \begin{smallmatrix}1&0\\0&1 \end{smallmatrix})$$(1/z^{3/2})$. The microlocal rank on the link $\Lambda$ is 1.