TY - JOUR
T1 - Long time asymptotic behavior of the focusing nonlinear Schrödinger equation
AU - Borghese, Michael
AU - Jenkins, Robert
AU - McLaughlin, Kenneth D.T.R.
N1 - Publisher Copyright:
© 2017 Elsevier Masson SAS
PY - 2018/7
Y1 - 2018/7
N2 - We study the Cauchy problem for the focusing nonlinear Schrödinger (fNLS) equation. Using the ∂‾ generalization of the nonlinear steepest descent method we compute the long-time asymptotic expansion of the solution ψ(x,t) in any fixed space-time cone C(x1,x2,v1,v2)={(x,t)∈R2:x=x0+vt with x0∈[x1,x2],v∈[v1,v2]} up to an (optimal) residual error of order O(t−3/4). In each cone C the leading order term in this expansion is a multi-soliton whose parameters are modulated by soliton–soliton and soliton–radiation interactions as one moves through the cone. Our results require that the initial data possess one L2(R) moment and (weak) derivative and that it not generate any spectral singularities.
AB - We study the Cauchy problem for the focusing nonlinear Schrödinger (fNLS) equation. Using the ∂‾ generalization of the nonlinear steepest descent method we compute the long-time asymptotic expansion of the solution ψ(x,t) in any fixed space-time cone C(x1,x2,v1,v2)={(x,t)∈R2:x=x0+vt with x0∈[x1,x2],v∈[v1,v2]} up to an (optimal) residual error of order O(t−3/4). In each cone C the leading order term in this expansion is a multi-soliton whose parameters are modulated by soliton–soliton and soliton–radiation interactions as one moves through the cone. Our results require that the initial data possess one L2(R) moment and (weak) derivative and that it not generate any spectral singularities.
KW - Focusing
KW - Integrable systems
KW - Long time asymptotics
KW - Nonlinear Schrödinger
KW - Riemann–Hilbert
KW - Soliton resolution
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U2 - 10.1016/j.anihpc.2017.08.006
DO - 10.1016/j.anihpc.2017.08.006
M3 - Article
AN - SCOPUS:85031316801
SN - 0294-1449
VL - 35
SP - 887
EP - 920
JO - Annales de l'Institut Henri Poincare (C) Analyse Non Lineaire
JF - Annales de l'Institut Henri Poincare (C) Analyse Non Lineaire
IS - 4
ER -