Mariana Haragus, Mathew A. Johnson, Wesley R. Perkins, Björn de Rijk
{"title":"Nonlinear Subharmonic Dynamics of Spectrally Stable Lugiato–Lefever Periodic Waves","authors":"Mariana Haragus, Mathew A. Johnson, Wesley R. Perkins, Björn de Rijk","doi":"10.1007/s00220-024-05104-5","DOIUrl":null,"url":null,"abstract":"<div><p>We study the nonlinear dynamics of perturbed, spectrally stable <i>T</i>-periodic stationary solutions of the Lugiato–Lefever equation (LLE), a damped nonlinear Schrödinger equation with forcing that arises in nonlinear optics. It is known that for each <span>\\(N\\in {\\mathbb {N}}\\)</span>, such a <i>T</i>-periodic wave train is asymptotically stable against <i>NT</i>-periodic, i.e. subharmonic, perturbations, in the sense that initially nearby data will converge at an exponential rate to a (small) spatial translation of the underlying wave. Unfortunately, in such results both the allowable size of initial perturbations as well as the exponential rates of decay depend on <i>N</i> and, in fact, tend to zero as <span>\\(N\\rightarrow \\infty \\)</span>, leading to a lack of uniformity in the period of the perturbation. In recent work, the authors performed a delicate decomposition of the associated linearized solution operator and obtained linear estimates which are uniform in <i>N</i>. The dynamical description suggested by this uniform linear theory indicates that the corresponding nonlinear iteration can only be closed if one allows for a spatio-temporal phase modulation of the underlying wave. However, such a modulated perturbation is readily seen to satisfy a quasilinear equation, yielding an inherent loss of regularity. We regain regularity by transferring a nonlinear damping estimate, which has recently been obtained for the LLE in the case of localized perturbations to the case of subharmonic perturbations. Thus, we obtain a nonlinear, subharmonic stability result for periodic stationary solutions of the LLE that is uniform in <i>N</i>. This in turn yields an improved nonuniform subharmonic stability result providing an <i>N</i>-independent ball of initial perturbations which eventually exhibit exponential decay at an <i>N</i>-dependent rate. Finally, we argue that our results connect in the limit <span>\\(N \\rightarrow \\infty \\)</span> to previously established stability results against localized perturbations, thereby unifying existing theories.</p></div>","PeriodicalId":522,"journal":{"name":"Communications in Mathematical Physics","volume":"405 10","pages":""},"PeriodicalIF":2.2000,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Communications in Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s00220-024-05104-5","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0
Abstract
We study the nonlinear dynamics of perturbed, spectrally stable T-periodic stationary solutions of the Lugiato–Lefever equation (LLE), a damped nonlinear Schrödinger equation with forcing that arises in nonlinear optics. It is known that for each \(N\in {\mathbb {N}}\), such a T-periodic wave train is asymptotically stable against NT-periodic, i.e. subharmonic, perturbations, in the sense that initially nearby data will converge at an exponential rate to a (small) spatial translation of the underlying wave. Unfortunately, in such results both the allowable size of initial perturbations as well as the exponential rates of decay depend on N and, in fact, tend to zero as \(N\rightarrow \infty \), leading to a lack of uniformity in the period of the perturbation. In recent work, the authors performed a delicate decomposition of the associated linearized solution operator and obtained linear estimates which are uniform in N. The dynamical description suggested by this uniform linear theory indicates that the corresponding nonlinear iteration can only be closed if one allows for a spatio-temporal phase modulation of the underlying wave. However, such a modulated perturbation is readily seen to satisfy a quasilinear equation, yielding an inherent loss of regularity. We regain regularity by transferring a nonlinear damping estimate, which has recently been obtained for the LLE in the case of localized perturbations to the case of subharmonic perturbations. Thus, we obtain a nonlinear, subharmonic stability result for periodic stationary solutions of the LLE that is uniform in N. This in turn yields an improved nonuniform subharmonic stability result providing an N-independent ball of initial perturbations which eventually exhibit exponential decay at an N-dependent rate. Finally, we argue that our results connect in the limit \(N \rightarrow \infty \) to previously established stability results against localized perturbations, thereby unifying existing theories.
我们研究了 Lugiato-Lefever 方程(LLE)的扰动、频谱稳定的 T 周期静态解的非线性动力学,LLE 是非线性光学中出现的带强迫的阻尼非线性薛定谔方程。众所周知,对于每个 \(N\in {\mathbb {N}}/),这样的 T 周期波列对于 NT 周期(即次谐波)扰动是渐近稳定的,即最初附近的数据将以指数速度收敛到基本波的(小)空间平移。不幸的是,在这类结果中,初始扰动的允许大小以及指数衰减率都取决于 N,而且事实上,随着 \(N\rightarrow \infty \)趋于零,导致扰动周期缺乏均匀性。在最近的工作中,作者对相关的线性化解算子进行了细致的分解,得到了在 N 中均匀的线性估计值。这种均匀线性理论提出的动力学描述表明,只有允许底层波的时空相位调制,相应的非线性迭代才能闭合。然而,这种调制扰动很容易被视为满足一个准线性方程,从而导致规律性的丧失。我们将最近在局部扰动情况下获得的 LLE 非线性阻尼估计值转移到次谐波扰动情况下,从而重新获得正则性。这反过来又产生了一个改进的非均匀亚谐波稳定性结果,它提供了一个与 N 无关的初始扰动球,这些扰动最终会以与 N 无关的速率呈现指数衰减。最后,我们认为我们的结果在极限(N \rightarrow \infty \)上与之前建立的针对局部扰动的稳定性结果相联系,从而统一了现有理论。
期刊介绍:
The mission of Communications in Mathematical Physics is to offer a high forum for works which are motivated by the vision and the challenges of modern physics and which at the same time meet the highest mathematical standards.