Mean field equations, hyperelliptic curves and modular forms: I

preprint2015arXivOpen access

Abstract

We develop a theory connecting the following three areas: (a) the mean field equation (MFE) △u+eu=ρ δ0\triangle u + e^u = ρ\, δ_0, ρ∈R>0ρ\in \mathbb R_{>0} on flat tori Eτ=C/(Z+Zτ)E_τ= \mathbb C/(\mathbb Z + \mathbb Zτ), (b) the classical Lamé equations and (c) modular forms. A major theme in part I is a classification of developing maps ff attached to solutions uu of the mean field equation according to the type of transformation laws (or monodromy) with respect to ΛΛ satisfied by ff. We are especially interested in the case when the parameter ρρ in the mean field equation is an integer multiple of 4π4π. In the case when ρ=4π(2n+1)ρ= 4π(2n + 1) for a non-negative integer nn, we prove that the number of solutions is n+1n + 1 except for a finite number of conformal isomorphism classes of flat tori, and we give a family of polynomials which characterizes the developing maps for solutions of mean field equations through the configuration of their zeros and poles. Modular forms appear naturally already in the simplest situation when  ρ=4π\,ρ=4π. In the case when ρ=8πnρ= 8πn for a positive integer nn, the solvability of the MFE depends on the \emph{moduli} of the flat tori EτE_τ and leads naturally to a hyperelliptic curve Xˉn=Xˉn(τ)\bar X_n=\bar X_{n}(τ) arising from the Hermite-Halphen ansatz solutions of Lamé's differential equation d2wdz2−(n(n+1)℘(z;Λτ)+B)w=0\frac{d^2 w}{dz^2}-(n(n+1)\wp(z;Λ_τ) + B) w=0. We analyse the curve Xˉn\bar X_n from both the analytic and the algebraic perspective, including its local coordinate near the point at infinity, which turns out to be a smooth point of Xˉn\bar{X}_n. We also specify the role of the branch points of the hyperelliptic projection Xˉn→P1\bar X_n \to \mathbb P^1 when the parameter ρρ varies in a neighborhood of ρ=8πnρ= 8πn.

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