paper

Nonequilibrium mode-coupling theory for dense active systems of self-propelled particles

arXiv:1708.05222 · doi:10.1039/C7SM01648D

Abstract

The physics of active systems of self-propelled particles, in the regime of a dense liquid state, is an open puzzle of great current interest, both for statistical physics and because such systems appear in many biological contexts. We develop a nonequilibrium mode-coupling theory (MCT) for such systems, where activity is included as a colored noise with the particles having a self-propulsion foce and persistence time . Using the extended MCT and a generalized fluctuation-dissipation theorem, we calculate the effective temperature of the active fluid. The nonequilibrium nature of the systems is manifested through a time-dependent that approaches a constant in the long-time limit, which depends on the activity parameters and . We find, phenomenologically, that this long-time limit is captured by the potential energy of a single, trapped active particle (STAP). Through a scaling analysis close to the MCT glass transition point, we show that , the -relaxation time, behaves as , where is the MCT exponent for the passive system. may increase or decrease as a function of depending on the type of active force correlations, but the behavior is always governed by the same value of the exponent . Comparison with numerical solution of the nonequilibrium MCT as well as simulation results give excellent agreement with the scaling analysis.

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Nonequilibrium mode-coupling theory for dense active systems of self-propelled particles · wovepaper