Stability of standing waves for nonlinear Schrödinger equations with unbounded potentials (Q1572868)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Stability of standing waves for nonlinear Schrödinger equations with unbounded potentials |
scientific article; zbMATH DE number 1484715
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Stability of standing waves for nonlinear Schrödinger equations with unbounded potentials |
scientific article; zbMATH DE number 1484715 |
Statements
Stability of standing waves for nonlinear Schrödinger equations with unbounded potentials (English)
0 references
22 May 2002
0 references
The author considers the Cauchy problem of the following nonlinear Schrödinger equations: \[ ih\psi_t=-\frac{h^2}{2m}\triangle \psi+V(x)\psi-\gamma|\psi|^{p-1}\psi,\quad t \geq 0,\;x \in \mathbb{R}^N, \tag{1} \] \[ \psi(0,x)=\psi_0(x),\quad x \in \mathbb{R}^n, \tag{2} \] where \(h\), \(m\), \(\gamma\) and \(p\) are positive constants. As his result and proof do not rely on the parameters \(h\), \(m\), \(\gamma\), he assumes that without loss of generality, \(h=m=\gamma=1.\) Let \[ H:=\left\{\varphi \in H^1(\mathbb{R}^N),\int_{\mathbb{R}^N}V(x)|\varphi|^2 dx < \infty \right\}. \] \(H\) becomes a Hilbert space, continuously embedded in \(H^1(\mathbb{R}^N)\), when endowed with the inner product \[ \langle \varphi,\varphi \rangle_H=\int_{\mathbb{R}^N}[\nabla \varphi \nabla \overline{\varphi}+(V-\inf V)\varphi\overline{\varphi}+ \varphi\overline{\varphi}]dx. \] Let \(\|\cdot\|_H\) be the associated norm and for any \(\mu \geq 0\) let \(S_\mu\) be the set of minimizers of the minimization problem \[ \inf_{\left\{u \in H,\int_{\mathbb{R}^N}|u|^2 dx=\mu \right\}} E(u), \] where \[ E(\varphi):=\int_{\mathbb{R}^N}\Biggl[\frac{1}{4}|\nabla \varphi|^2+\frac{1}{2}|V(x)\varphi|^2-\frac{1}{p+1}|\varphi|^{p+1}\Biggr] dx,\quad\varphi \in H. \] The author proves the following stability theorem by the method of Cazenave and Lions. Theorem. Assume that \(V\) satisfies \(\inf V >-\infty\), \(V(x) \rightarrow \infty\) as \(|x|\rightarrow \infty\) and for each \(|\alpha|\geq 2\), \(|D^{\alpha}V|\) is bounded. Let \(1<p<\frac{4}{N}\), \(\mu>0.\) Then for arbitrary \(\varepsilon\), there exists \(\sigma>0\) such that for any \(\psi_0 \in H,\) if \[ \inf_{u \in {\mathcal S}_{\mu}}\|\psi_0 -u \|_H < \sigma, \] then the solution \(\psi(t,\cdot)\) of the Cauchy problem (1),(2) satisfies \[ \inf_{u \in {\mathcal S}_{\mu}}\|\psi(t,\cdot)-u(\cdot) \|_H < \varepsilon,\quad \text{for all }t \geq 0. \] The author also mentions the physical background of this problem.
0 references
nonlinear Schrödinger equation
0 references
unbounded potential
0 references
variational argument
0 references
standing wave
0 references
stability
0 references