Mean field equations, hyperelliptic curves and modular forms: II

preprint2016arXivOpen access

Abstract

A pre-modular form Zn(σ;τ)Z_n(σ; τ) of weight 12n(n+1)\tfrac{1}{2} n(n + 1) is introduced for each n∈Nn \in \Bbb N, where (σ,τ)∈C×H(σ, τ) \in \Bbb C \times \Bbb H, such that for Eτ=C/(Z+Zτ)E_τ= \Bbb C/(\Bbb Z + \Bbb Z τ), every non-trivial zero of Zn(σ;τ)Z_n(σ; τ), namely σ∉Eτ[2]σ\not\in E_τ[2], corresponds to a (scaling family of) solution to the mean field equation \begin{equation} \tag{MFE} \triangle u + e^u = ρ\, δ_0 \end{equation} on the flat torus EτE_τ with singular strength ρ=8πnρ= 8πn. In Part I (Cambridge J. Math. 3, 2015), a hyperelliptic curve Xˉn(τ)⊂SymnEτ\bar X_n(τ) \subset {\rm Sym}^n E_τ, the Lamé curve, associated to the MFE was constructed. Our construction of Zn(σ;τ)Z_n(σ; τ) relies on a detailed study on the correspondence P1←Xˉn(τ)→Eτ\Bbb P^1 \leftarrow \bar X_n(τ) \to E_τ induced from the hyperelliptic projection and the addition map. As an application of the explicit form of the weight 10 pre-modular form Z4(σ;τ)Z_4(σ; τ), a counting formula for Lamé equations of degree n=4n = 4 with finite monodromy is given in the appendix (by Y.-C. Chou).

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