Incomplete equilibrium in long-range interacting systems
arXiv:cond-mat/0603659 · doi:10.1103/PhysRevLett.97.100601
Abstract
We use a Hamiltonian dynamics to discuss the statistical mechanics of long-lasting quasi-stationary states particularly relevant for long-range interacting systems. Despite the presence of an anomalous single-particle velocity distribution, we find that the Central Limit Theorem implies the Boltzmann expression in Gibbs' -space. We identify the nonequilibrium sub-manifold of -space characterizing the anomalous behavior and show that by restricting the Boltzmann-Gibbs approach to this sub-manifold we obtain the statistical mechanics of the quasi-stationary states.
Title changed, throughout revision of the text
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Cited by in corpus (10)
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