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From coherent shocklets to giant collective incoherent shock waves in nonlocal turbulent flows

机译:从相干小波到非局部湍流中的巨大集体非相干激波

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摘要

Understanding turbulent flows arising from random dispersive waves that interact strongly through nonlinearities is a challenging issue in physics. Here we report the observation of a characteristic transition: strengthening the nonlocal character of the nonlinear response drives the system from a fully turbulent regime, featuring a sea of coherent small-scale dispersive shock waves (shocklets) towards the unexpected emergence of a giant collective incoherent shock wave. The front of such global incoherent shock carries most of the stochastic fluctuations and is responsible for a peculiar folding of the local spectrum. Nonlinear optics experiments performed in a solution of graphene nano-flakes clearly highlight this remarkable transition. Our observations shed new light on the role of long-range interactions in strongly nonlinear wave systems operating far from thermodynamic equilibrium, which reveals analogies with, for example, gravitational systems, and establishes a new scenario that can be common to many turbulent flows in photonic quantum fluids, hydrodynamics and Bose–Einstein condensates.
机译:理解由通过非线性强烈相互作用的随机色散波产生的湍流是物理学中一个具有挑战性的问题。在这里,我们报告观察到一个特征性的转变:增强非线性响应的非局部特性将系统从一个完全湍流的状态驱使出来,该系统以相干的小规模色散冲击波(小波)为特征,向着巨大的集体不相干的意外出现激波。这种全局非相干震荡的前部携带了大多数随机波动,并导致局部频谱的特殊折叠。在石墨烯纳米薄片溶液中进行的非线性光学实验清楚地表明了这一非凡的转变。我们的观察为远距离相互作用在远非热力学平衡的强非线性波系统中的作用提供了新的线索,这揭示了与引力系统的类比,并建立了光子中许多湍流共同的新情况。量子流体,流体力学和玻色-爱因斯坦凝聚物。

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