Baskaran A, Marchetti M C
Martin Fisher School of Physics, Brandeis University, Waltham, MA, USA.
Eur Phys J E Soft Matter. 2012 Sep;35(9):95. doi: 10.1140/epje/i2012-12095-8. Epub 2012 Sep 28.
We consider the hydrodynamic theory of an active fluid of self-propelled particles with nematic aligning interactions. This class of materials has polar symmetry at the microscopic level, but forms macrostates of nematic symmetry. We highlight three key features of the dynamics. First, as in polar active fluids, the control parameter for the order-disorder transition, namely the density, is dynamically convected by the order parameter via active currents. The resulting dynamical self-regulation of the order parameter is a generic property of active fluids and destabilizes the uniform nematic state near the mean-field transition. Secondly, curvature-driven currents render the system unstable deep in the nematic state, as found previously. Finally, and unique to self-propelled nematics, nematic order induces local polar order that in turn leads to the growth of density fluctuations. We propose this as a possible mechanism for the smectic order of polar clusters seen in numerical simulations.
我们考虑具有向列排列相互作用的自驱动粒子活性流体的流体动力学理论。这类材料在微观层面具有极性对称性,但会形成向列对称性的宏观状态。我们强调动力学的三个关键特征。首先,与极性活性流体一样,有序 - 无序转变的控制参数,即密度,通过活性流由序参量进行动态对流。序参量由此产生的动态自我调节是活性流体的普遍特性,并使均匀向列态在平均场转变附近变得不稳定。其次,如先前发现的那样,曲率驱动流使系统在向列态深处变得不稳定。最后,对于自驱动向列相而言独特的是,向列序会诱导局部极性序,进而导致密度涨落的增长。我们提出这可能是数值模拟中所见极性团簇近晶序的一种机制。