卢嘉图-勒弗尔方程中孤波解的稳定性

Lukas Bengel
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摘要

我们分析了Lugiato-Lefever方程在\(\mathbb {R}\)上的孤波解的频谱和动力学稳定性。我们的兴趣在于非线性薛定谔方程的相移亮孤子通过分岔产生的解。这些解是高度非线性、局部化、远离平衡的波,是模拟克尔频梳的物理相关解。我们证明,当相位角满足(\theta \in (0,\pi )\)时,分岔孤波在光谱上是稳定的,而当相位角满足(\theta \in (\pi ,2\pi )\)时,会出现不稳定波。此外,我们还建立了频谱稳定孤波对局部扰动的渐近轨道稳定性。我们的分析利用了Lyapunov-Schmidt还原法、为线性哈密顿系统开发的不稳定指数计数以及解析估计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

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Stability of solitary wave solutions in the Lugiato–Lefever equation

We analyze the spectral and dynamical stability of solitary wave solutions to the Lugiato–Lefever equation on \(\mathbb {R}\). Our interest lies in solutions that arise through bifurcations from the phase-shifted bright soliton of the nonlinear Schrödinger equation. These solutions are highly nonlinear, localized, far-from-equilibrium waves, and are the physical relevant solutions to model Kerr frequency combs. We show that bifurcating solitary waves are spectrally stable when the phase angle satisfies \(\theta \in (0,\pi )\), while unstable waves are found for angles \(\theta \in (\pi ,2\pi )\). Furthermore, we establish asymptotic orbital stability of spectrally stable solitary waves against localized perturbations. Our analysis exploits the Lyapunov–Schmidt reduction method, the instability index count developed for linear Hamiltonian systems, and resolvent estimates.

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