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Large-time behaviour of solutions to the dissipative nonlinear Schrödinger equation

Published online by Cambridge University Press:  11 July 2007

N. Hayashi
Affiliation:
Department of Applied Mathematics, Science University of Tokyo, Tokyo 162-8601, Japan ([email protected])
E. I. Kaikina
Affiliation:
Departamento de Ciencias Básicas, Instituto Tecnológico de Morelia, CP 58120, Morelia, Michoacán, Mexico ([email protected])
P. I. Naumkin
Affiliation:
Instituto de Física y Matemáticas, Universidad Michoacana, AP 2-82, CP 58040, Morelia, Michoacán, Mexico ([email protected])

Abstract

We study the Cauchy problem for the nonlinear Schrödinger equation with dissipation where L is a linear pseudodifferential operator with dissipative symbol ReL(ξ) ≥ C1|ξ|2/(1 + ξ2) and |L′(ξ)| ≤ C2(|ξ|+ |ξ|n) for all ξ ∈ R. Here, C1, C2 > 0, n ≥ 1. Moreover, we assume that L(ξ) = αξ2 + O(|ξ|2+γ) for all |ξ| < 1, where γ > 0, Re α > 0, Im α ≥ 0. When L(ξ) = αξ2, equation (A) is the nonlinear Schrödinger equation with dissipation ut − αuxx + i|u|2u = 0. Our purpose is to prove that solutions of (A) satisfy the time decay estimate under the conditions that u0Hn,0H0,1 have the mean value and the norm ‖u0Hn,0 + ‖u0H0,1 = ε is sufficiently small, where σ = 1 if Im α > 0 and σ = 2 if Im α = 0, and Therefore, equation (A) is considered as a critical case for the large-time asymptotic behaviour because the solutions of the Cauchy problem for the equation ut − αuxx + i|u|p−1u = 0, with p > 3 have the same time decay estimate ‖uL∞ = O(t−½) as that of solutions to the linear equation. On the other hand, note that solutions of the Cauchy problem (A) have an additional logarithmic time decay. Our strategy of the proof of the large-time asymptotics of solutions is to translate (A) to another nonlinear equation in which the mean value of the nonlinearity is zero for all time.

Type
Research Article
Copyright
Copyright © Royal Society of Edinburgh 2000

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