波动表面上的轻粒子和重粒子:束状平衡、不可约序列和局部密度高度相关性

S. Mahapatra, K. Ramola, M. Barma
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引用次数: 3

摘要

我们研究了由两种粒子(轻粒子和重粒子)耦合到波动表面(用倾斜场描述)的系统的早期时间和粗化动力学。粒子的动力学和倾斜度通过局部更新规则耦合,并根据微观速率导致不同的有序和无序稳态相。我们在非平衡系统中引入了一种广义的平衡机制,即束状平衡,其中输入和输出的过渡电流在组态之间是平衡的。这使我们能够精确地确定这个模型相图的子空间中的稳态。在该模型中引入了界面和弯曲不可约序列的概念。这些序列是非局部的,我们发现它们在后期的有序相中提供了一个粗糙的长度尺度。最后,我们提出了一个$局部$相关函数($\mathcal{S}$),它与不可约序列的数量有直接关系,并且能够通过其粗化特性来区分该系统的几个阶段。$\mathcal{S}$从一个完全无序的初始配置开始,显示一个初始线性上升和一个宽最大值。随着系统向有序稳态演化,$\mathcal{S}$在后期进一步表现出幂律衰减,这编码了接近有序相的粗化特性。着眼于早期动力学,我们假设了控制粒子和倾斜的耦合平均场演化方程,这些方程在短时间内由一组线性化方程很好地近似,我们解析求解了这些方程。在紫外线(晶格)截止设定的时间尺度之外,在粗化开始之前,我们的线性化理论预测了中间扩散(幂律)拉伸的存在,我们也在系统的有序状态的模拟中发现了这一点。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Light and heavy particles on a fluctuating surface: Bunchwise balance, irreducible sequences, and local density-height correlations
We study the early time and coarsening dynamics in a system consisting of two species of particles ($light$ and $heavy$) coupled to a fluctuating surface (described by tilt fields). The dynamics of particles and tilts are coupled through local update rules, and lead to different ordered and disordered steady state phases depending on the microscopic rates. We introduce a generalised balance mechanism in non-equilibrium systems, namely $bunchwise~balance$, in which incoming and outgoing transition currents are balanced between groups of configurations. This allows us to exactly determine the steady state in a subspace of the phase diagram of this model. We introduce the concept of $irreducible~sequences$ of interfaces and bends in this model. These sequences are non-local, and we show that they provide a coarsening length scale in the ordered phases at late times. Finally, we propose a $local$ correlation function ($\mathcal{S}$) that has a direct relation to the number of irreducible sequences, and is able to distinguish between several phases of this system through its coarsening properties. Starting from a totally disordered initial configuration, $\mathcal{S}$ displays an initial linear rise and a broad maximum. As the system evolves towards the ordered steady states, $\mathcal{S}$ further exhibits power law decays at late times that encode coarsening properties of the approach to the ordered phases. Focusing on early time dynamics, we posit coupled mean-field evolution equations governing the particles and tilts, which at short times are well approximated by a set of linearized equations, which we solve analytically. Beyond a timescale set by an ultraviolet (lattice) cutoff and preceding the onset of coarsening, our linearized theory predicts the existence of an intermediate diffusive (power-law) stretch, which we also find in simulations of the ordered regime of the system.
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