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引用次数: 0
摘要
我们考虑了一维唐克斯-吉拉尔多气体与空间相关的失衡势。我们推导出该系统被划分为 n 个方框并在每个方框内分解为能量特征状态时的精确动力学。这是一种介于实空间和动量空间之间的混合波函数表示法,其基元由定位在方框中的平面波组成,这就是 "小波 "一词的由来。利用这种表示法,我们推导出了在适当极限下出现的广义流体力学,而无需假设局部松弛。我们强调,除了更常见的大空间和晚时间极限(类似于半经典扩展)外,广义流体力学行为还出现在高动量和短时间极限中。在这个极限中,守恒电荷不需要用广义流体力学来描述众多粒子。我们还证明,这种小波表示法为完整描述铁核玻色子的失衡动力学提供了一种高效的数值算法。
We consider the one-dimensional Tonks–Girardeau gas with a space-dependent potential out of equilibrium. We derive the exact dynamics of the system when divided into n boxes and decomposed into energy eigenstates within each box. It is a representation of the wave function that is a mixture between real space and momentum space, with basis elements consisting of plane waves localized in a box, giving rise to the term ‘wavelet’. Using this representation, we derive the emergence of generalized hydrodynamics in appropriate limits without assuming local relaxation. We emphasize that a generalized hydrodynamic behaviour emerges in a high-momentum and short-time limit, in addition to the more common large-space and late-time limit, which is akin to a semi-classical expansion. In this limit, conserved charges do not require numerous particles to be described by generalized hydrodynamics. We also show that this wavelet representation provides an efficient numerical algorithm for a complete description of the out-of-equilibrium dynamics of hardcore bosons.
期刊介绍:
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