Nonequilibrium phase transitions and violent relaxation in the Hamiltonian mean-field model

We discuss the nature of nonequilibrium phase transitions in the Hamiltonian mean-field model using detailed numerical simulations of the Vlasov equation and molecular dynamics. Starting from fixed magnetization water bag initial distributions and varying the energy, the states obtained after a viol...

Full description

Saved in:
Bibliographic Details
Published inPhysical review. E, Statistical, nonlinear, and soft matter physics Vol. 85; no. 6 Pt 1; p. 062103
Main Authors Rocha Filho, T M, Amato, M A, Figueiredo, A
Format Journal Article
LanguageEnglish
Published United States 28.06.2012
Subjects
Online AccessGet more information

Cover

Loading…
More Information
Summary:We discuss the nature of nonequilibrium phase transitions in the Hamiltonian mean-field model using detailed numerical simulations of the Vlasov equation and molecular dynamics. Starting from fixed magnetization water bag initial distributions and varying the energy, the states obtained after a violent relaxation undergo a phase transition from magnetized to nonmagnetized states when going from lower to higher energies. The phase transitions are either first order or are composed of a cascade of phase reentrances. This result is at variance with most previous results in the literature mainly based on the Lynden-Bell theory of violent relaxation. The latter is a rough approximation and, consequently, is not suited for an accurate description of nonequilibrium phase transition in long-range interacting systems.
ISSN:1550-2376
DOI:10.1103/physreve.85.062103