A maximum entropy principle explains quasi-stationary states in systems with long-range interactions: the example of the Hamiltonian Mean Field model

Abstract

A generic feature of systems with long-range interactions is the presence of {\it quasi-stationary} states with non-Gaussian single particle velocity distributions. For the case of the Hamiltonian Mean Field (HMF) model, we demonstrate that a maximum entropy principle applied to the associated Vlasov equation explains known features of such states for a wide range of initial conditions. We are able to reproduce velocity distribution functions with an analytical expression which is derived from the theory with no adjustable parameters. A normal diffusion of angles is detected and a new dynamical effect, two oscillating clusters surrounded by a halo, is also found and theoretically justified.

4 pages, 3 figs, submitted to Phys. Rev. Lett

References in corpus (3)

• Lynden-Bell and Tsallis distributions for the HMF model
• On the diffusive anomalies in a long-range Hamiltonian system
• Absence of Domain Wall Roughening in a Transverse Field Ising Model with Long-Range Interactions

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