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非保守高阶流体动力学调制不稳定性

Nonconservative higher-order hydrodynamic modulation instability.

作者信息

Kimmoun O, Hsu H C, Kibler B, Chabchoub A

机构信息

Aix-Marseille University, CNRS, Centrale Marseille, IRPHE, Marseille, France.

Department of Marine Environment and Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan.

出版信息

Phys Rev E. 2017 Aug;96(2-1):022219. doi: 10.1103/PhysRevE.96.022219. Epub 2017 Aug 28.

Abstract

The modulation instability (MI) is a universal mechanism that is responsible for the disintegration of weakly nonlinear narrow-banded wave fields and the emergence of localized extreme events in dispersive media. The instability dynamics is naturally triggered, when unstable energy sidebands located around the main energy peak are excited and then follow an exponential growth law. As a consequence of four wave mixing effect, these primary sidebands generate an infinite number of additional sidebands, forming a triangular sideband cascade. After saturation, it is expected that the system experiences a return to initial conditions followed by a spectral recurrence dynamics. Much complex nonlinear wave field motion is expected, when the secondary or successive sideband pair that is created is also located in the finite instability gain range around the main carrier frequency peak. This latter process is referred to as higher-order MI. We report a numerical and experimental study that confirms observation of higher-order MI dynamics in water waves. Furthermore, we show that the presence of weak dissipation may counterintuitively enhance wave focusing in the second recurrent cycle of wave amplification. The interdisciplinary weakly nonlinear approach in addressing the evolution of unstable nonlinear waves dynamics may find significant resonance in other nonlinear dispersive media in physics, such as optics, solids, superfluids, and plasma.

摘要

调制不稳定性(MI)是一种普遍机制,它导致弱非线性窄带波场瓦解,并在色散介质中引发局部极端事件。当位于主能量峰值周围的不稳定能量边带被激发并遵循指数增长规律时,不稳定性动力学自然就会触发。由于四波混频效应,这些初级边带会产生无限数量的附加边带,形成一个三角形边带级联。饱和之后,预计系统会回到初始条件,随后出现频谱重现动力学。当产生的次级或连续边带对也位于主载波频率峰值周围的有限不稳定性增益范围内时,预计会出现许多复杂的非线性波场运动。后一过程被称为高阶MI。我们报告了一项数值和实验研究,证实了在水波中观察到高阶MI动力学。此外,我们表明,弱耗散的存在可能会出人意料地在波放大的第二个重现周期中增强波的聚焦。这种跨学科的弱非线性方法在处理不稳定非线性波动力学的演化时,可能会在物理学中的其他非线性色散介质(如光学、固体、超流体和等离子体)中引起显著共鸣。

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