Proceedings of the London Mathematical Society· 2013Q1
Existence and instability of standing waves with prescribed norm for a class of Schrödinger-Poisson equations
- 263citations
- Q1SCImago
- 2013year
Short summary
Researchers proved the existence of standing wave solutions for a class of Schrödinger-Poisson-Slater equations when the L2-norm is sufficiently small, and demonstrated that these solutions are strongly unstable.
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Key points
- Existence of standing waves proven for Schrödinger-Poisson-Slater equations with prescribed L2-norm (c > 0) when c is sufficiently small.
- A mountain-pass argument on the energy functional is used to find critical points.
- Standing waves at the mountain-pass energy level are shown to be strongly unstable.
- The mountain-pass energy level serves as a threshold for global existence of solutions to the Cauchy problem.
AI-generated from the title and abstract; the full text is not read.
Abstract
In this paper, we study the existence and the instability of standing waves with prescribed L2-norm for a class of Schrödinger–Poisson–Slater equations in ℝ3 ( * ) i ψ t + Δ ψ − ( | x | − 1 * | ψ | 2 ) ψ + | ψ | p − 2 ψ = 0 when p ∈ ( 10 3 , 6 ) . To obtain such solutions, we look into critical points of the energy functional F ( u ) = 1 2 ‖ ∇ u ‖ L 2 ( R 3 ) 2 + 1 4 ∫ R 3 ∫ R 3 | u ( x ) | 2 | u ( y ) | 2 | x − y | d x d y − 1 p ∫ R 3 | u | p d x , on the constraints given by S ( c ) = { u ∈ H 1 ( R ) 3 : ‖ u ‖ L 2 ( R 3 ) 2 = c , c > 0 } . For the values p ∈ ( 10 3 , 6 ) considered, the functional F is unbounded from below on S(c) and the existence of critical points is obtained by a mountain-pass argument developed on S(c). We show that critical points exist provided that c > 0 is sufficiently small and that when c > 0 is not small a nonexistence result is expected. Regarding the dynamics, we show for initial condition u0∈H1(ℝ3) of the associated Cauchy problem with ‖ u 0 ‖ 2 2 = c that the mountain-pass energy level γ(c) gives a threshold for global existence. Also, the strong instability of standing waves at the mountain pass energy level is proved. Finally, we draw a comparison between the Schrödinger–Poisson–Slater equation and the classical nonlinear Schrödinger equation.
The authors' abstract, as published at the source. Proceedings of the London Mathematical Society, 2013 · DOI ↗
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Field: Mathematical Physics
Mathematical PhysicsMathematics