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具有短程排列和远程反排列相互作用的欠阻尼活性物质中动态模式形成的平均场方法。

Mean field approach of dynamical pattern formation in underdamped active matter with short-ranged alignment and distant anti-alignment interactions.

作者信息

Arold Dominic, Schmiedeberg Michael

机构信息

Institut für Theoretische Physik I, Friedrich-Alexander-Universität Erlangen-Nürnberg, Staudtstraße 7, 91058 Erlangen, Germany.

出版信息

J Phys Condens Matter. 2020 May 11;32(31). doi: 10.1088/1361-648X/ab849b.

Abstract

Many active matter systems, especially on the microscopic scale, are well approximated as overdamped, meaning that any inertial momentum is immediately dissipated by the environment. On the other hand, especially for macroscopic active systems but also for many mesoscopic systems the time scale of translational inertial motion can become large enough to be relevant for the dynamics. This raises the question how collective dynamics and the resulting states in active matter are influenced by inertia. Therefore, we propose a coarse-grained continuum model for underdamped active matter based on a mean field description for passive systems. Furthermore, as an example, we apply the model to a system with interactions that support an alignment on short distances and an anti-alignment on longer length scales as known in the context of pattern formation due to orientational interactions. Our numerical calculations of the under- and overdamped dynamics both predict a structured laning state. However, activity induced convective flows that are only present in the underdamped model destabilize this state when the anti-alignment is weakened, leading to a collective motion state which does not occur in the overdamped limit. A turbulent transition regime between the two states can be characterized by strong density fluctuations and the absence of global ordering.

摘要

许多活性物质系统,尤其是在微观尺度上,都可以很好地近似为过阻尼系统,这意味着任何惯性动量都会立即被环境耗散。另一方面,特别是对于宏观活性系统以及许多介观系统,平动惯性运动的时间尺度可能会变得足够大,从而与动力学相关。这就引出了一个问题:活性物质中的集体动力学以及由此产生的状态是如何受到惯性影响的。因此,我们基于对被动系统的平均场描述,提出了一个用于欠阻尼活性物质的粗粒化连续介质模型。此外,作为一个例子,我们将该模型应用于一个具有相互作用的系统,这种相互作用在短距离上支持对齐,而在较长长度尺度上支持反对齐,这在由于取向相互作用而形成图案的背景中是已知的。我们对欠阻尼和过阻尼动力学的数值计算都预测了一种结构化的车道状态。然而,仅在欠阻尼模型中存在的活性诱导对流在反对齐减弱时会使这种状态不稳定,从而导致一种在过阻尼极限中不会出现的集体运动状态。这两种状态之间的湍流转变区域可以通过强烈的密度波动和缺乏全局有序性来表征。

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