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Main Author: Matsutani, Shigeki
Format: Preprint
Published: 2024
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Online Access:https://arxiv.org/abs/2403.06156
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author Matsutani, Shigeki
author_facet Matsutani, Shigeki
contents It is known that the elliptic function solutions of the nonlinear Schrödinger equation are reduced to the algebraic differential relation in terms of the Weierstrass sigma function, $\displaystyle{ \left[-{\frak{i}}\frac{\partial}{\partial t} +α\frac{\partial}{\partial u}\right]Ψ-\frac{1}{2} \frac{\partial^2}{\partial u^2}Ψ+(Ψ^* Ψ) Ψ= \frac12 (2β+α^2-3\wp(v))Ψ}$, where $Ψ(u;v, t):=\mathrm{e}^{αu+{\frak{i}}βt+c}$ $\displaystyle{\frac{\mathrm{e}^{-ζ(v)u}σ(u+v)}{σ(u)σ(v)}}$, its dual $Ψ^*(u; v,t)$, and certain complex numbers $α, β$ and $c$. In this paper, we generalize the algebraic differential relation to those of genera two and three in terms of the hyperelliptic sigma functions.
format Preprint
id arxiv_https___arxiv_org_abs_2403_06156
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Nonlinear Schrödinger equation in terms of elliptic and hyperelliptic $σ$ functions
Matsutani, Shigeki
Exactly Solvable and Integrable Systems
Algebraic Geometry
It is known that the elliptic function solutions of the nonlinear Schrödinger equation are reduced to the algebraic differential relation in terms of the Weierstrass sigma function, $\displaystyle{ \left[-{\frak{i}}\frac{\partial}{\partial t} +α\frac{\partial}{\partial u}\right]Ψ-\frac{1}{2} \frac{\partial^2}{\partial u^2}Ψ+(Ψ^* Ψ) Ψ= \frac12 (2β+α^2-3\wp(v))Ψ}$, where $Ψ(u;v, t):=\mathrm{e}^{αu+{\frak{i}}βt+c}$ $\displaystyle{\frac{\mathrm{e}^{-ζ(v)u}σ(u+v)}{σ(u)σ(v)}}$, its dual $Ψ^*(u; v,t)$, and certain complex numbers $α, β$ and $c$. In this paper, we generalize the algebraic differential relation to those of genera two and three in terms of the hyperelliptic sigma functions.
title Nonlinear Schrödinger equation in terms of elliptic and hyperelliptic $σ$ functions
topic Exactly Solvable and Integrable Systems
Algebraic Geometry
url https://arxiv.org/abs/2403.06156