2010/12/01 by Eva Koo, Koo, Eva
Mathematics · Physics and Astronomy · #35Bxx #35Pxx #Advanced Mathematical Physics Problems #Analysis of PDEs (math.AP) #FOS: Mathematics #Nonlinear Photonic Systems #Spectral Theory in Mathematical Physics #math.AP #msc:35Bxx #msc:35Pxx
paper · pdf · doi:10.48550/arxiv.1012.0092
34 pages
arxiv created 2010/12/01 · openalex publication_date 2010/12/01 · arxiv updated 2010/12/02 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
We consider the nonlinear magnetic Schrödinger equation for u: ℝ3 × ℝ → ℂ , iut = (i ∇ + A)2 u + V u + g(u), u(x,0) = u0(x), where A :ℝ3 → ℝ3 is the magnetic potential, V : ℝ3 → ℝ is the electric potential, and g = ± | 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 , then the solution of the above equation decomposes uniquely into a standing wave part, which converges as t → ∞ and a dispersive part, which scatters.