Gamma conjecture for asymptotics of mirror Lagrangian periods

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Let XX be a Calabi--Yau manifold equipped with a symplectic form ω\omega, and let {Zt}t∈Δ∗\{Z_t\}_{t\in \Delta^\ast} be a family of Calabi--Yau manifolds parametrized by tt in a small punctured disc Δ∗\Delta^\ast that corresponds to (X,ω)(X,\omega) under mirror symmetry. Let Ωt\Omega_t be a suitable holomorphic volume form on ZtZ_t, let tt be a suitable coordinate, and let Ct⊂ZtC_t\subset Z_t be a Lagrangian cycle mirror to a coherent sheaf EE on XX. Gamma conjecture. As t→0t\to 0 in a fixed angular sector, one should have

∫CtΩt=∫Xt−ω⋅Γ^X⋅(2π−1)deg⁡/2ch⁡(E)+O(tϵ),\int_{C_t} \Omega_t=\int_X t^{-\omega}\cdot \widehat{\Gamma}_X\cdot (2\pi\sqrt{-1})^{\deg/2}\operatorname{ch}(E)+O(t^\epsilon),

where ϵ>0\epsilon>0 is some constant. This conjectural asymptotic formula relates periods of Lagrangian cycles on the mirror family to the Gamma class and Chern character on the Calabi--Yau manifold, and is motivated by the mirror-symmetric correspondence between tropical or ordinary cycles and the Gamma conjecture. Its general validity remains open.

References

Primary source

Yuto Yamamoto, “Lifts of cycles in tropical hypersurfaces and the Gamma conjecture”, arXiv:2602.08666 (2026).

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