Nonequilibrium phase transitions in a Brownian $p$-state clock model

TL;DR

This paper introduces a two-dimensional Brownian p-state clock model to study nonequilibrium phase transitions, revealing a robust BKT transition and novel nonequilibrium effects on symmetry-breaking transitions.

Contribution

The study presents a novel nonequilibrium extension of the p-state clock model with particle diffusion, analyzing its phase transitions and critical behaviors.

Findings

Identifies three phases: disordered, critical, and ordered for p>4.

Finds the BKT transition exponent is universal and robust against diffusion.

Shows the symmetry-breaking transition exponent deviates from equilibrium predictions due to nonequilibrium effects.

Abstract

We introduce a Brownian $p$-state clock model in two dimensions and investigate the nature of phase transitions numerically. As a nonequilibrium extension of the equilibrium lattice model, the Brownian $p$-state clock model allows spins to diffuse randomly in the two-dimensional space of area $L^2$ under periodic boundary conditions. We find three distinct phases for $p>4$: a disordered paramagnetic phase, a quasi-long-range-ordered critical phase, and an ordered ferromagnetic phase. In the intermediate critical phase, the magnetization order parameter follows a power law scaling $m \sim L^{-\tilde{\beta}}$, where the finite-size scaling exponent $\tilde{\beta}$ varies continuously. These critical behaviors are reminiscent of the double Berezinskii-Kosterlitz-Thouless~(BKT) transition picture of the equilibrium system. At the transition to the disordered phase, the exponent takes the universal value $\tilde\beta = 1/8$ which coincides with that of the equilibrium system. This result indicates that the BKT transition driven by the unbinding of topological excitations is robust against the particle diffusion. On the contrary, the exponent at the symmetry-breaking transition to the ordered phase deviates from the universal value $\tilde{\beta} = 2/p^2$ of the equilibrium system. The deviation is attributed to a nonequilibrium effect from the particle diffusion.