Hyperelliptic tangential covers and even elliptic finite-gap potentials, back and forth
Abstract
Let (X,ω0):=(C/,0) denote the elliptic curve associated to the lattice , X2:=\ω0,·s, ω3\ its set of half-periods and :X P1 the usual Weierstrass function, with a double pole at the origin ω0. Fix (α,m)∈ N4× N and consider a function u(x) = Σ03 αi(αi+1)(x\,-\,ωi) +2Σj=1m ((x\, -\, j)+(x+j)), where \j\ ∈ (X X2)(m). The latter is known to be a so-called (even, -periodic) finite-gap potential, if and only if \j\ satisfies the so-called (D-G) square system of equations. We let PotX(α,m) denote the set of such potentials. Any such potential corresponds to a unique spectral data (π,), where π: X is a hyperelliptic tangential cover of degree n:=12(Σiαi(αi+1)+4m) and a θ-characteristic of the spectral curve . The problem at stake is to find out all spectral data of the family PotX(m) := α∈ N4 PotX(α,m), for any m. The latter problem has been thoroughly studied for PotX(0) and PotX(1). In this article we go one step further, by studying all spectral data of each family PotX(α,2). We find the bound \#PotX(α,2)≤ 27, for any α∈ N4, with equality for a generic elliptic curve X. We also find a formula for the arithmetic geni of the corresponding spectral curves in terms of α, which we generalize to PotX(α,m) for any m. At last, we conclude with a natural conjecture, leading to a recursive formula in d∈ N, for the cardinals of PotX(α,d).
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