Deformed Mirror Symmetry for Punctured Surfaces
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| Format: | Preprint |
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2023
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| _version_ | 1866909449119072256 |
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| author | Bocklandt, Raf van de Kreeke, Jasper |
| author_facet | Bocklandt, Raf van de Kreeke, Jasper |
| contents | Mirror symmetry originally envisions a correspondence between deformations of the A-side and deformations of the B-side. In this paper, we achieve an explicit correspondence in the case of punctured surfaces.
The starting point is the noncommutative mirror equivalence $ \operatorname{Gtl} Q \cong \operatorname{mf} (\operatorname{Jac} \check{Q}, \ell) $ for a punctured surface $ Q $. We pick a deformation $ \operatorname{Gtl}_q Q $ which captures a large part of the deformation theory and includes the relative Fukaya category. To find the corresponding deformation of $ \operatorname{mf} (\operatorname{Jac} \check{Q}, \ell) $, we deform work of Cho-Hong-Lau which interprets mirror symmetry as Koszul duality. As result we explicitly obtain the corresponding deformation $ \operatorname{mf} (\operatorname{Jac}_q \check{Q}, \ell_q) $ together with a deformed mirror functor $ \operatorname{Gtl}_q Q \xrightarrow{\sim} \operatorname{mf} (\operatorname{Jac}_q \check{Q}, \ell_q) $.
The bottleneck is to verify that the algebra $ \operatorname{Jac}_q \check{Q} $ is indeed a (flat) deformation of $ \operatorname{Jac} \check{Q} $. We achieve this by deploying a result of Berger-Ginzburg-Taillefer on deformations of CY3 algebras, which however requires the relations to be homogeneous. We show how to replace this homogeneity requirement by a simple boundedness condition and obtain flatness of $ \operatorname{Jac}_q \check{Q} $ for almost all $ Q $.
We finish the paper with examples, including a full treatment of the 3-punctured sphere and 4-punctured torus. With the help of our computations in arXiv:2305.09112, we describe $ \operatorname{Jac}_q \check{Q} $ explicitly. It turns out that the deformed potential $ \ell_q $ is still central in $ \operatorname{Jac}_q \check{Q} $, in contrast to the popular slogan that central elements do not survive under deformation. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2305_12608 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Deformed Mirror Symmetry for Punctured Surfaces Bocklandt, Raf van de Kreeke, Jasper Algebraic Geometry Representation Theory 14A22 (Primary), 53D37, 14J33, 16S38 (Secondary) Mirror symmetry originally envisions a correspondence between deformations of the A-side and deformations of the B-side. In this paper, we achieve an explicit correspondence in the case of punctured surfaces. The starting point is the noncommutative mirror equivalence $ \operatorname{Gtl} Q \cong \operatorname{mf} (\operatorname{Jac} \check{Q}, \ell) $ for a punctured surface $ Q $. We pick a deformation $ \operatorname{Gtl}_q Q $ which captures a large part of the deformation theory and includes the relative Fukaya category. To find the corresponding deformation of $ \operatorname{mf} (\operatorname{Jac} \check{Q}, \ell) $, we deform work of Cho-Hong-Lau which interprets mirror symmetry as Koszul duality. As result we explicitly obtain the corresponding deformation $ \operatorname{mf} (\operatorname{Jac}_q \check{Q}, \ell_q) $ together with a deformed mirror functor $ \operatorname{Gtl}_q Q \xrightarrow{\sim} \operatorname{mf} (\operatorname{Jac}_q \check{Q}, \ell_q) $. The bottleneck is to verify that the algebra $ \operatorname{Jac}_q \check{Q} $ is indeed a (flat) deformation of $ \operatorname{Jac} \check{Q} $. We achieve this by deploying a result of Berger-Ginzburg-Taillefer on deformations of CY3 algebras, which however requires the relations to be homogeneous. We show how to replace this homogeneity requirement by a simple boundedness condition and obtain flatness of $ \operatorname{Jac}_q \check{Q} $ for almost all $ Q $. We finish the paper with examples, including a full treatment of the 3-punctured sphere and 4-punctured torus. With the help of our computations in arXiv:2305.09112, we describe $ \operatorname{Jac}_q \check{Q} $ explicitly. It turns out that the deformed potential $ \ell_q $ is still central in $ \operatorname{Jac}_q \check{Q} $, in contrast to the popular slogan that central elements do not survive under deformation. |
| title | Deformed Mirror Symmetry for Punctured Surfaces |
| topic | Algebraic Geometry Representation Theory 14A22 (Primary), 53D37, 14J33, 16S38 (Secondary) |
| url | https://arxiv.org/abs/2305.12608 |