Matrix factorizations and mirror symmetry
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\documentclass{article} \usepackage{amsmath,amsfonts,amssymb,epsfig,color} \newcommand{\C}{\mathbb{C}} \newcommand{\Z}{\mathbb{Z}} \newcommand{\R}{\mathbb{R}} \newcommand{\iso}{\cong} \parskip1em \parindent0em \begin{document} \underline{Matrix factorizations and mirror symmetry} The purpose of this talk is to introduce matrix factorizations (``sheaves with a potential''). These form categories which have general properties analogous to Fukaya categories, and indeed appear as mirrors in the non-Calabi-Yau case. A good informal reference is [Kapustin-Li, D-branes in LG models and algebraic geometry]. The most systematic approach is in [Orlov, Triangulated categories of singularities and D-branes in Landau-Ginzburg models]. A good exposition would cover both definitions, since each has its advantages. To read Orlov, one needs to know about triangulated categories at the level of [Gelfand-Manin, homological algebra]. \underline{Plan} {\it Definition.} Matrix factorizations for a potential $W$. They form a differential graded category, and the resulting homotopy category has mapping cones (technically, is triangulated). Older literature has a more commutative algebra viewpoint, going back to [Eisenbud, Homological algebra on a complete intersection, with an application to group representations] {\it Examples.} The nondegenerate potential $W = x_1^2 + \cdots + x_n^2$ is treated in [Kapustin-Li, op. cit.]. The relevant thing for us that there is a single basic matrix factorization, whose endomorphism algebra is semisimple (a Clifford algebra). There are a lot of other examples in the older literature, for instance [Knoerrer, The Cohen-Macaulay modules over simple hypersurface singularities]. {\it More theory.} This would be a good point to introduce Orlov's definition. It shows that if $W^{-1}(0)$ is smooth, the category of matrix factorizations is zero. Note also Orlov's recent preprint on idempotent completions, which shows that the Karoubi completion of the category of matrix factorizations only depends on the formal neighbourhood of the critical points. This is important, since it shows that up to Karoubi completion, we understand the category fully if $W^{-1}(0)$ has only ordinary double points (described in a formal neighbourhood by the nondegenerate potential above). {\it Mirror symmetry.} We should look at the mirror potentials for ${\mathbb C}P^1$ and ${\mathbb C}P^1 \times {\mathbb C}P^1$, and try to identify the matrix factorizations mirror to various important Lagrangian submanifolds. This is much easier to do in Orlov's picture, actually. For ${\mathbb C}P^1 \times {\mathbb C}P^1$, the main important point is to identify the standard Lagrangian torus (with its four different $Spin$ structures) and the anti-diagonal sphere. Unfortunately, this is unpublished work of Auroux-Katzarkov-Orlov, but it's not hard to at least guess the result. \underline{Notes} The important point about $\mathbb{C} P^1 \times \mathbb{C} P^1$ is that the two critical points lying in the same fibre interact nontrivially. Of course, if one passes to Karoubi completions, that interaction becomes trivial. In the mirror picture, this corresponds to the fact that various Lagrangian submanifolds will split as direct sums of simpler objects once one Karoubi-completes the Fukaya category. \underline{Dependencies} This depends on the talk about Lagrangian submanifolds in Fano varieties. It also uses derived categories of coherent sheaves. \end{document}
