Fermat-hypersurface superpotential conjecture

Let VV be the subspace spanned by the immersed-point generators X1,,Xn+2X_1,\ldots,X_{n+2}, and write a deformation as b=i=1n+2xiXib=\sum_{i=1}^{n+2}x_iX_i. Let WW be the mirror superpotential obtained from the immersed Lagrangian construction, and let checkq(q)check{q}(q) denote the inverse mirror map for the Fermat hypersurface tildeXtilde{X}. Superpotential conjecture. The elements of VV should be weak bounding cocycles, and, after a change of coordinates in (x1,,xn+2)(x_1,\ldots,x_{n+2}), the superpotential should be equivalent to

W=i=1n+2xin+2+checkq(q)x1xn+2.W=\sum_{i=1}^{n+2}x_i^{n+2}+check{q}(q)x_1\cdots x_{n+2}.

In dimension one the weak unobstructedness and the equality of the generalized SYZ map with the mirror map are established; the conjecture proposes that these statements persist in general dimensions and gives an explicit form for the higher-dimensional mirror superpotential.

Sources & referencesView supporting material

Primary source

Cheol-Hyun Cho, Hansol Hong and Siu-Cheong Lau, “Localized mirror functor for Lagrangian immersions, and homological mirror symmetry for P^1_a,b,c”, arXiv:1308.4651 (2015).

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