Abstract

We investigate the steady-state entropy production rate (EPR) in the hydrodynamic Vicsek model (HVM) and diffusive flocking model (DFM). Both models display a transition from an isotropic gas to a polar liquid (flocking) phase, in addition to travelling polar clusters and microphase-separation in the miscibility gap. The phase diagram of the DFM, which may be considered an extension of the HVM, contains additional structure at low densities where we find a novel crystal phase in which a stationary hexagonal lattice of high-density ridges surround low density valleys. From an assessment of the scaling of the EPR at low noise, we uncover that the dynamics in this limit may be organised into three main classes based on the dominant contribution. Truly nonequilibrium dynamics is characterised by a divergent EPR in this limit, and sustains global time-reversal symmetry (TRS) violating currents at zero noise. On the other hand, marginally nonequilibrium and effectively equilibrium dynamics have a finite EPR in this limit, and TRS is broken only at the level of fluctuations. For the latter of these two cases, detailed balance is restored in the small noise limit and we recover effective Boltzmann statistics to lowest nontrivial order. We further demonstrate that the scaling of the EPR may change depending on the dynamical variables that are tracked when it is computed, and the protocol chosen for time-reversal. Results acquired from numerical simulations of the dynamics confirm both the asymptotic scaling relations we derive and our quantitative predictions.

Highlights

  • Nonequilibrium statistical physics deals with fluctuating dynamics that violate detailed balance, or equivalently time-reversal symmetry (TRS), driving the system away from the classical Boltzmann statistics [1,2,3,4,5]

  • We investigate the steady-state entropy production rate (EPR) in the hydrodynamic Vicsek model (HVM) and diffusive flocking model (DFM)

  • The phase diagram of the DFM, which may be considered an extension of the HVM, contains additional structure at low densities where we find a novel crystal phase in which a stationary hexagonal lattice of high-density ridges surround low density valleys

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Summary

Introduction

Nonequilibrium statistical physics deals with fluctuating dynamics that violate detailed balance, or equivalently time-reversal symmetry (TRS), driving the system away from the classical Boltzmann statistics [1,2,3,4,5]. This allows us to consider both the case of a time-even and time-odd polar density, and we explore how this choice changes our results from section 3.

The hydrodynamic Vicsek model
Entropy production at the fluctuating hydrodynamic level
Constant homogeneous ground-states
TRS violations in the generalised diffusive flocking model
The diffusive flocking model
Entropy production in the DFM
Conclusion
Polar liquid ground-state
Hydrodynamic Vicsek model
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