流体动力二维晶体熔化动态路线中的集体晶格激发

Mikheil Kharbedia, Niccolò Caselli, Macarena Calero, Lara H. Moleiro, Jesús F. Castillo, José A. Santiago, Diego Herráez-Aguilar, Francisco Monroy
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引用次数: 0

摘要

表面刚度产生了稳定的法拉第波(FW)模式,即所谓的流体力学晶体,相当于单色驱动下由离散次谐波组成的有序波晶格。主控规则既包括用于调频的惯性施加参数共振,也包括用于波场自聚焦的刚性驱动非线性。它们利用了相干 FW 包在空间和时间上定位所需的离散性。集体晶格激发被观测到为无色散传播定位,它导致了明确的对称性破缺所产生的周期性调制。从场论的角度来看,集合扭曲模式的减半成因被揭示为流体力学晶体熔化的自然途径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Collective lattice excitations in the dynamic route for melting hydrodynamic 2D-crystals
Surface stiffnesses engender steady patterns of Faraday waves (FWs), so called hydrodynamic crystals as correspond to ordered wave lattices made of discrete subharmonics under monochromatic driving. Mastering rules are both inertia-imposed parametric resonance for frequency-halving together with rigidity-driven nonlinearity for wavefield self-focusing. They harness the discretization needed for coherent FW-packets to localize in space and time. Collective lattice excitations are observed as dispersionless propagating dislocations that lead periodic modulations arising from explicit symmetry breaking. In a field theory perspective, a halving genesis for the collective distorting modes is revealed as the natural pathway for hydrodynamic crystal melting.
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