Resonance-induced nonlinear bound states

Fuente: arXiv
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Autori principali: Turner, Jackson C., Weinstein, Michael I.
Natura: Preprint
Pubblicazione: 2025
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author Turner, Jackson C.
Weinstein, Michael I.
author_facet Turner, Jackson C.
Weinstein, Michael I.
contents We study nonlinear bound states -- time-harmonic and spatially decaying ($L^2$) solutions -- of the nonlinear Schrödinger / Gross--Pitaevskii equations (NLS/GP) with a compactly supported linear potential. Such solutions are known to bifurcate from the $L^2$ bound states of an underlying Schrödinger operator $H_V=-\partial_x^2+V$. In this article we prove an extension of this result: for the 1D NLS/GP, nonlinear bound states also arise via bifurcation from the scattering resonance states and transmission resonance states of $H_V$, associated with the poles and zeros, respectively, of the reflection coefficients, $r_\pm(k)$, of $H_V$. The corresponding resonance states are non-decaying and only $L^2_{\rm loc}$. In contrast to nonlinear states arising from $L^2$ bound states of $H_V$, these resonance bifurcations initiate at a strictly positive $L^2$ threshold which is determined by the position of the complex scattering resonance pole or transmission resonance zero.
format Preprint
id arxiv_https___arxiv_org_abs_2510_19538
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Resonance-induced nonlinear bound states
Turner, Jackson C.
Weinstein, Michael I.
Mathematical Physics
Analysis of PDEs
Pattern Formation and Solitons
We study nonlinear bound states -- time-harmonic and spatially decaying ($L^2$) solutions -- of the nonlinear Schrödinger / Gross--Pitaevskii equations (NLS/GP) with a compactly supported linear potential. Such solutions are known to bifurcate from the $L^2$ bound states of an underlying Schrödinger operator $H_V=-\partial_x^2+V$. In this article we prove an extension of this result: for the 1D NLS/GP, nonlinear bound states also arise via bifurcation from the scattering resonance states and transmission resonance states of $H_V$, associated with the poles and zeros, respectively, of the reflection coefficients, $r_\pm(k)$, of $H_V$. The corresponding resonance states are non-decaying and only $L^2_{\rm loc}$. In contrast to nonlinear states arising from $L^2$ bound states of $H_V$, these resonance bifurcations initiate at a strictly positive $L^2$ threshold which is determined by the position of the complex scattering resonance pole or transmission resonance zero.
title Resonance-induced nonlinear bound states
topic Mathematical Physics
Analysis of PDEs
Pattern Formation and Solitons
url https://arxiv.org/abs/2510.19538