Active matter in infinite dimensions: Fokker-Planck equation and dynamical mean-field theory at low density
arXiv:2108.02407 · doi:10.1063/5.0065893
Abstract
We investigate the behavior of self-propelled particles in infinite space dimensions by comparing two powerful approaches in many-body dynamics: the Fokker-Planck equation and dynamical mean-field theory. The dynamics of the particles at low densities and infinite persistence time is solved in the steady-state with both methods, thereby proving the consistency of the two approaches in a paradigmatic out-of-equilibrium system. We obtain the analytic expression for the pair distribution function and the effective self-propulsion to first order in the density, confirming the results obtained in a previous paper and extending them to the case of a non-monotonous interaction potential. Furthermore, we obtain the transient behavior of active hard spheres when relaxing from equilibrium to the nonequilibrium steady-state. Our results show how collective dynamics is affected by interactions to first order in the density, and point out future directions for further analytical and numerical solutions of this problem.
25 pages, 5 figures
References in corpus (8)
- Motility-Induced Phase Separation
- Statistical Mechanics of Interacting Run-and-Tumble Bacteria
- Spontaneous velocity alignment in Motility-induced Phase Separation
- Perspective: Nonequilibrium glassy dynamics in dense systems of active particles
- Active matter: quantifying the departure from equilibrium
- Active hard-spheres in infinitely many dimensions
- Rheological similarities between dense self-propelled and sheared particulate systems
- Out-of-equilibrium dynamical equations of infinite-dimensional particle systems. II. The anisotropic case under shear strain