2014/12/31 by J. Lenells, A. S. Fokas · 1 citation
Mathematics · Physics and Astronomy · #math.AP #nlin.SI #msc:35Q55 #msc:37K15
paper · pdf · doi:10.1098/rspa.2014.0925
23 pages
arxiv created 2015/09/19 · arxiv updated 2016/02/17
We consider the nonlinear Schrödinger equation on the half-line with a given Dirichlet (Neumann) boundary datum which for large t tends to the periodic function g0b(t) (g1b(t)). Assuming that the unknown Neumann (Dirichlet) boundary value tends for large t to a periodic function g1b(t) (g0b(t)), we derive an easily verifiable condition that the functions g0b(t) and g1b(t) must satisfy. Furthermore, we introduce two different methods, one based on the formulation of a Riemann-Hilbert problem, and one based on a perturbative approach, for constructing g1b(t) (g0b(t)) in terms of g0b(t) (g1b(t)).