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自驱动硬磁盘动力学蒙特卡洛模型中的聚类与非均匀动力学

Clustering and heterogeneous dynamics in a kinetic Monte Carlo model of self-propelled hard disks.

作者信息

Levis Demian, Berthier Ludovic

机构信息

Laboratoire Charles Coulomb, UMR 5221 CNRS, and Université Montpellier 2, Montpellier, France.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2014 Jun;89(6):062301. doi: 10.1103/PhysRevE.89.062301. Epub 2014 Jun 9.

Abstract

We introduce a kinetic Monte Carlo model for self-propelled hard disks to capture with minimal ingredients the interplay between thermal fluctuations, excluded volume, and self-propulsion in large assemblies of active particles. We analyze in detail the resulting (density, self-propulsion) nonequilibrium phase diagram over a broad range of parameters. We find that purely repulsive hard disks spontaneously aggregate into fractal clusters as self-propulsion is increased and rationalize the evolution of the average cluster size by developing a kinetic model of reversible aggregation. As density is increased, the nonequilibrium clusters percolate to form a ramified structure reminiscent of a physical gel. We show that the addition of a finite amount of noise is needed to trigger a nonequilibrium phase separation, showing that demixing in active Brownian particles results from a delicate balance between noise, interparticle interactions, and self-propulsion. We show that self-propulsion has a profound influence on the dynamics of the active fluid. We find that the diffusion constant has a nonmonotonic behavior as self-propulsion is increased at finite density and that activity produces strong deviations from Fickian diffusion that persist over large time scales and length scales, suggesting that systems of active particles generically behave as dynamically heterogeneous systems.

摘要

我们引入了一个用于自驱动硬磁盘的动力学蒙特卡罗模型,以用最少的要素捕捉热涨落、排除体积和自推进在大量活性粒子集合体中的相互作用。我们在广泛的参数范围内详细分析了由此产生的(密度、自推进)非平衡相图。我们发现,随着自推进的增加,纯排斥性硬磁盘会自发聚集成分形簇,并通过建立一个可逆聚集的动力学模型来解释平均簇尺寸的演变。随着密度的增加,非平衡簇会渗流形成一种类似于物理凝胶的分支结构。我们表明,需要添加有限量的噪声来触发非平衡相分离,这表明活性布朗粒子中的相分离是由噪声、粒子间相互作用和自推进之间的微妙平衡导致的。我们表明,自推进对活性流体的动力学有深远影响。我们发现,在有限密度下,随着自推进的增加,扩散常数具有非单调行为,并且活性会导致与菲克扩散的强烈偏差,这种偏差在长时间尺度和长度尺度上持续存在,这表明活性粒子系统通常表现为动态非均匀系统。

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