Landau–Ginzburg/Calabi–Yau correspondence

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Consider the Lagrangian cones LFJRW⁡\mathcal L_{\operatorname{FJRW}} and LGW⁡\mathcal L_{\operatorname{GW}} in the symplectic spaces VFJRW⁡\mathcal V_{\operatorname{FJRW}} and VGW⁡\mathcal V_{\operatorname{GW}}, and let DFJRW⁡\mathcal D_{\operatorname{FJRW}} and DGW⁡\mathcal D_{\operatorname{GW}} denote the corresponding total potential functions. LG–CY correspondence. (1) There is a degree-preserving C[z,z−1]\mathbb C[z,z^{-1}]-valued linear symplectic isomorphism

ULG-CY⁡:VFJRW⁡→VGW⁡\mathbb U_{\operatorname{LG-CY}}:\mathcal V_{\operatorname{FJRW}}\to\mathcal V_{\operatorname{GW}}

and a choice of analytic continuation such that

ULG-CY⁡(LFJRW⁡)=LGW⁡.\mathbb U_{\operatorname{LG-CY}}(\mathcal L_{\operatorname{FJRW}})=\mathcal L_{\operatorname{GW}}.

(2) Up to an overall constant and a choice of analytic continuation, the total potentials satisfy

DGW⁡=U^LG-CY⁡(DFJRW⁡).\mathcal D_{\operatorname{GW}}=\widehat{\mathbb U}_{\operatorname{LG-CY}}(\mathcal D_{\operatorname{FJRW}}).

This geometric correspondence generalizes the quintic case to Calabi–Yau orbifold hypersurfaces and finite group quotients; genus-zero special cases are known, while the full statement remains open in the source.

References

Primary source

Alessandro Chiodo and Yongbin Ruan, “A global mirror symmetry framework for the Landau-Ginzburg/Calabi-Yau correspondence”, arXiv:1307.0939 (2013).

Additional references

2 papers in this index state this conjecture (2008–2013). The statement above is taken from the most recent of them; the others are arXiv:0812.4660.

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