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Autore principale: Athanassoulis, Agissilaos
Natura: Preprint
Pubblicazione: 2026
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Accesso online:https://arxiv.org/abs/2604.16998
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author Athanassoulis, Agissilaos
author_facet Athanassoulis, Agissilaos
contents The Alber equation is the mixed-state nonlinear Schrödinger equation with singular ($δ$-interaction) kernel. It is used in the modeling of stochastic ocean waves, where it appears with the focusing sign in the nonlinearity, on $d=1.$ The main result of the paper is global well-posedness for self-adjoint, non-negative data in the Schatten-Sobolev space $H^1\mathfrak{S}^1(\mathbb{T}),$ for both the focusing and defocusing cases. The Schatten class norms achieve control of the position density without derivative loss, and a systematic Fourier-Galerkin argument tailored to the $δ$ kernel allows us to establish several qualitative properties of the solution, including energy conservation. In the focusing case, Hoffmann-Ostenhof and Gagliardo-Nirenberg estimates yield a global a priori $H^1\mathfrak{S}^1$ bound with no smallness condition. Non-negativity is a structural requirement for the energy argument to work. The propagation of higher Sobolev regularity $H^s\mathfrak{S}^1$ follows. As an application, small perturbations around Penrose-stable backgrounds are shown to grow at most polynomially in $H^1\mathfrak{S}$ over long timescales.
format Preprint
id arxiv_https___arxiv_org_abs_2604_16998
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Global solutions for the Alber equation in $H^1\mathfrak{S}^1(\mathbb{T})$
Athanassoulis, Agissilaos
Analysis of PDEs
35Q55, 35B35, 47B10, 37A60
The Alber equation is the mixed-state nonlinear Schrödinger equation with singular ($δ$-interaction) kernel. It is used in the modeling of stochastic ocean waves, where it appears with the focusing sign in the nonlinearity, on $d=1.$ The main result of the paper is global well-posedness for self-adjoint, non-negative data in the Schatten-Sobolev space $H^1\mathfrak{S}^1(\mathbb{T}),$ for both the focusing and defocusing cases. The Schatten class norms achieve control of the position density without derivative loss, and a systematic Fourier-Galerkin argument tailored to the $δ$ kernel allows us to establish several qualitative properties of the solution, including energy conservation. In the focusing case, Hoffmann-Ostenhof and Gagliardo-Nirenberg estimates yield a global a priori $H^1\mathfrak{S}^1$ bound with no smallness condition. Non-negativity is a structural requirement for the energy argument to work. The propagation of higher Sobolev regularity $H^s\mathfrak{S}^1$ follows. As an application, small perturbations around Penrose-stable backgrounds are shown to grow at most polynomially in $H^1\mathfrak{S}$ over long timescales.
title Global solutions for the Alber equation in $H^1\mathfrak{S}^1(\mathbb{T})$
topic Analysis of PDEs
35Q55, 35B35, 47B10, 37A60
url https://arxiv.org/abs/2604.16998