Normalized solutions for nonlinear Schrödinger equations with $L^2$-critical nonlinearity

Fuente: arXiv
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Autores principales: Cingolani, Silvia, Gallo, Marco, Ikoma, Norihisa, Tanaka, Kazunaga
Formato: Preprint
Publicado: 2024
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author Cingolani, Silvia
Gallo, Marco
Ikoma, Norihisa
Tanaka, Kazunaga
author_facet Cingolani, Silvia
Gallo, Marco
Ikoma, Norihisa
Tanaka, Kazunaga
contents We study the following nonlinear Schrödinger equation and we look for normalized solutions $(μ,u)\in {\bf R}\times H^1({\bf R}^N)$ for a given $m>0$ and $N\geq 2$ \[ -Δu + μu = g(u)\quad \text{in}\ {\bf R}^N, \qquad \frac{1}{2}\int_{{\bf R}^N} u^2 dx = m. \] We assume that $g$ has an $L^2$-critical growth, both at the origin and at infinity. That is, for $p=1+\frac{4}{N}$, $g(s)=|s|^{p-1}s +h(s)$, $h(s)=o(|s|^p)$ as $s\sim 0$ and $s\sim\infty$. The $L^2$-critical exponent $p$ is very special for this problem; in the power case $g(s) = |s|^{p-1}s$ a solution exists only for the specific mass $m=m_1$, where $m_1=\frac{1}{2}\int_{{\bf R}^N}ω_1^2\, dx$ is the mass of a least energy solution $ω_1$ of $-Δω+ω=ω^p$ in ${\bf R}^N$. We prove the existence of a positive solution for $m=m_1$ when $h$ has a sublinear growth at infinity, i.e., $h(s)=o(s)$ as $s\sim\infty$. In contrast, we show non-existence results for $h(s)\not=o(s)$ ($s\sim 0$) under a suitable monotonicity condition.
format Preprint
id arxiv_https___arxiv_org_abs_2410_23733
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Normalized solutions for nonlinear Schrödinger equations with $L^2$-critical nonlinearity
Cingolani, Silvia
Gallo, Marco
Ikoma, Norihisa
Tanaka, Kazunaga
Analysis of PDEs
35B33, 35B38, 35J20, 35Q55, 49J35, 35A01, 35J91, 47F10, 47J30
We study the following nonlinear Schrödinger equation and we look for normalized solutions $(μ,u)\in {\bf R}\times H^1({\bf R}^N)$ for a given $m>0$ and $N\geq 2$ \[ -Δu + μu = g(u)\quad \text{in}\ {\bf R}^N, \qquad \frac{1}{2}\int_{{\bf R}^N} u^2 dx = m. \] We assume that $g$ has an $L^2$-critical growth, both at the origin and at infinity. That is, for $p=1+\frac{4}{N}$, $g(s)=|s|^{p-1}s +h(s)$, $h(s)=o(|s|^p)$ as $s\sim 0$ and $s\sim\infty$. The $L^2$-critical exponent $p$ is very special for this problem; in the power case $g(s) = |s|^{p-1}s$ a solution exists only for the specific mass $m=m_1$, where $m_1=\frac{1}{2}\int_{{\bf R}^N}ω_1^2\, dx$ is the mass of a least energy solution $ω_1$ of $-Δω+ω=ω^p$ in ${\bf R}^N$. We prove the existence of a positive solution for $m=m_1$ when $h$ has a sublinear growth at infinity, i.e., $h(s)=o(s)$ as $s\sim\infty$. In contrast, we show non-existence results for $h(s)\not=o(s)$ ($s\sim 0$) under a suitable monotonicity condition.
title Normalized solutions for nonlinear Schrödinger equations with $L^2$-critical nonlinearity
topic Analysis of PDEs
35B33, 35B38, 35J20, 35Q55, 49J35, 35A01, 35J91, 47F10, 47J30
url https://arxiv.org/abs/2410.23733