Asymptotic stability of small solitary waves for nonlinear Schrödinger equations with electromagnetic potential in R3 \mathbb{R}^3

preprint2010arXivOpen access

Abstract

We consider the nonlinear magnetic Schrödinger equation for u:R3×R→C u: \mathbb{R}^3 \times \mathbb{R} \to \mathbb{C} , iut=(i∇+A)2u+Vu+g(u),u(x,0)=u0(x), iu_t = (i \nabla + A)^2 u + V u + g(u), u(x,0) = u_0(x), where A:R3→R3 A :\mathbb{R}^3 \to \mathbb{R}^3 is the magnetic potential, V:R3→R V : \mathbb{R}^3 \to \mathbb{R} is the electric potential, and g=±∣u∣2u g = \pm | u |^2 u is the nonlinear term. We show that under suitable assumptions on the electric and magnetic potentials, if the initial data is small enough in H1 H^1 , then the solution of the above equation decomposes uniquely into a standing wave part, which converges as t→∞t \to \infty and a dispersive part, which scatters.

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