Mishra Shradha, Baskaran Aparna, Marchetti M Cristina
Physics Department, Syracuse University, Syracuse, New York 13244, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Jun;81(6 Pt 1):061916. doi: 10.1103/PhysRevE.81.061916. Epub 2010 Jun 16.
We consider a coarse-grained description of a collection of self-propelled particles given by hydrodynamic equations for the density and polarization fields. We find that the ordered moving or flocking state of the system is unstable to spatial fluctuations beyond a threshold set by the self-propulsion velocity of the individual units. In this region, the system organizes itself into an inhomogeneous state of well-defined propagating stripes of flocking particles interspersed with low-density disordered regions. Further, we find that even in the regime where the homogeneous flocking state is stable, the system exhibits large fluctuations in both density and orientational order. We study the hydrodynamic equations analytically and numerically to characterize both regimes.
我们考虑了由密度和极化场的流体动力学方程给出的自驱动粒子集合的粗粒度描述。我们发现,系统的有序移动或聚集状态对于超出单个单元自推进速度所设定阈值的空间涨落是不稳定的。在这个区域,系统会自行组织成一种不均匀状态,即由聚集粒子构成的定义明确的传播条纹与低密度无序区域相间分布。此外,我们发现即使在均匀聚集状态稳定的 regime 中,系统在密度和取向有序方面也表现出大幅涨落。我们通过解析和数值方法研究流体动力学方程,以刻画这两种 regime。