Cates M E, Nardini C
DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom.
Service de Physique de l'Etat Condensé, CEA, CNRS Université Paris-Saclay, CEA-Saclay, 91191 Gif-sur-Yvette, France.
Rep Prog Phys. 2025 May 14;88(5). doi: 10.1088/1361-6633/add278.
In active systems, whose constituents have non-equilibrium dynamics at local level, fluid-fluid phase separation is widely observed. Examples include the formation of membraneless organelles within cells; the clustering of self-propelled colloidal particles in the absence of attractive forces, and some types of ecological segregation. A schematic understanding of such active phase separation was initially borrowed from what is known for the equilibrium case, in which detailed balance holds at microscopic level. However it has recently become clear that in active systems the absence of detailed balance, although it leave phase separation qualitatively unchanged in some regimes (for example domain growth driven by interfacial tension via Ostwald ripening), can in other regimes radically alter its phenomenology at mechanistic level. For example, microphase separation can be caused by reverse Ostwald ripening, a process that is hard to imagine from an equilibrium perspective. This and other new phenomena arise because, instead of having a single, positive interfacial tension like their equilibrium counterparts, the fluid-fluid interfaces created by active phase separation can have several distinct interfacial tensions governing different properties, some of which can be negative. These phenomena can be broadly understood by studying continuum field theories for a single conserved scalar order parameter (the fluid density), supplemented with a velocity field in cases where momentum conservation is also present. More complex regimes arise in systems described by multiple scalar order parameters (especially with nonreciprocal interactions between these); or when an order parameter undergoes both conserved and non-conserved dynamics (such that the combination breaks detailed balance); or in systems that support orientational long-range order in one or more of the coexisting phases. In this Review, we survey recent progress in understanding the specific role of activity in phase separation, drawing attention to many open questions. We focus primarily on continuum theories, especially those with a single scalar order parameter, reviewing both analytical and numerical work. We compare their predictions with particle-based models, which have mostly been studied numerically although a few have been explicitly coarse-grained to continuum level. We also compare, where possible, with experimental results. In the latter case, qualitative comparisons are broadly encouraging whereas quantitative ones are hindered by the dynamical complexity of most experimental systems relative that of simplified (particle-level or continuum) models of active matter.
在其组成部分在局部水平具有非平衡动力学的活性系统中,流体-流体相分离现象广泛存在。例如,细胞内无膜细胞器的形成;在没有吸引力的情况下自推进胶体颗粒的聚集,以及某些类型的生态隔离。对这种活性相分离的初步示意性理解最初借鉴了平衡情况下的已知情况,在平衡情况下微观层面存在细致平衡。然而,最近已经清楚的是,在活性系统中,尽管细致平衡的缺失在某些情况下(例如通过奥斯特瓦尔德熟化由界面张力驱动的畴生长)在定性上不会改变相分离,但在其他情况下会在机制层面从根本上改变其现象学。例如,微相分离可能由反向奥斯特瓦尔德熟化引起,从平衡的角度来看,这是一个难以想象的过程。出现这种以及其他新现象的原因是,与平衡状态下的对应物不同,活性相分离产生的流体-流体界面不是具有单一的正界面张力,而是可以有几个不同的界面张力来控制不同的性质,其中一些可能是负的。通过研究单一守恒标量序参量(流体密度)的连续场理论,并在存在动量守恒的情况下补充速度场,可以大致理解这些现象。在由多个标量序参量描述的系统中(特别是这些序参量之间存在非互易相互作用时);或者当序参量经历守恒和非守恒动力学时(使得这种组合打破细致平衡);或者在一个或多个共存相中支持取向长程有序的系统中,会出现更复杂的情况。在本综述中,我们概述了在理解活性在相分离中的具体作用方面的最新进展,同时提请注意许多未解决的问题。我们主要关注连续体理论,特别是那些具有单一标量序参量的理论,回顾分析和数值方面的工作。我们将它们的预测与基于粒子的模型进行比较,基于粒子的模型大多是通过数值方法研究的,尽管有一些已经明确粗粒化为连续体水平。在可能的情况下,我们还将其与实验结果进行比较。在后一种情况下,定性比较大致令人鼓舞,而定量比较则受到大多数实验系统相对于活性物质简化(粒子水平或连续体)模型的动力学复杂性的阻碍。