Issue
EPL
Volume 88, Number 3, November 2009
Article Number 30010
Number of page(s) 6
Section General
DOI http://dx.doi.org/10.1209/0295-5075/88/30010
Published online 17 November 2009
EPL, 88 (2009) 30010
DOI: 10.1209/0295-5075/88/30010

Unveiling the nature of out-of-equilibrium phase transitions in a system with long-range interactions

M.-C. Firpo

Laboratoire de Physique des Plasmas, CNRS-Ecole Polytechnique - 91128 Palaiseau cedex, France, EU

marie-christine.firpo@lpp.polytechnique.fr

received 19 May 2009; accepted in final form 16 October 2009; published November 2009
published online 17 November 2009

Abstract
Recently, there has been some vigorous interest in the out-of-equilibrium quasistationary states (QSSs), with lifetimes diverging with the number N of degrees of freedom, emerging from numerical simulations of the ferromagnetic XY Hamiltonian Mean Field (HMF) starting from some special initial conditions. Phase transitions have been reported between low-energy magnetized QSSs and large-energy unexpected, antiferromagnetic-like, QSSs with low magnetization. This issue is addressed here in the Vlasov $N\rightarrow \infty $ limit. It is argued that the time-asymptotic states emerging in the Vlasov limit can be related to simple generic time-asymptotic forms for the force field. The proposed picture unveils the nature of the out-of-equilibrium phase transitions reported for the ferromagnetic HMF: this is a bifurcation point connecting an effective integrable Vlasov one-particle time-asymptotic dynamics to a partly ergodic one which means a brutal open-up of the Vlasov one-particle phase space. Illustration is given by investigating the time-asymptotic value of the magnetization at the phase transition, under the assumption of a sufficiently rapid time-asymptotic decay of the transient force field.

PACS
05.70.Fh - Phase transitions: general studies.
05.45.-a - Nonlinear dynamics and chaos.
05.20.Dd - Kinetic theory.

© EPLA 2009