Generalized maximum entropy approach to quasi-stationary states in long range systems
Gabriele Martelloni, Gianluca Martelloni, Pierre de Buyl, Duccio, Fanelli

TL;DR
This paper introduces a generalized maximum entropy method incorporating additional conserved quantities to better describe quasi-stationary states in long-range interacting systems, successfully explaining complex velocity distributions.
Contribution
It develops a generalized Gibbs ensemble approach that accounts for pseudo-conserved moments, improving the theoretical understanding of QSS in long-range systems.
Findings
Accurately predicts multiple bumps in velocity distributions.
Matches simulation results both above and below phase transition.
Resolves previously unexplained features of QSS.
Abstract
Systems with long-range interactions display a short-time relaxation towards Quasi Stationary States (QSS) whose lifetime increases with the system size. In the paradigmatic Hamiltonian Mean-field Model (HMF) out-of-equilibrium phase transitions are predicted and numerically detected which separate homogeneous (zero magnetization) and inhomogeneous (nonzero magnetization) QSS. In the former regime, the velocity distribution presents (at least) two large, symmetric, bumps, which cannot be self-consistently explained by resorting to the conventional Lynden-Bell maximum entropy approach. We propose a generalized maximum entropy scheme which accounts for the pseudo-conservation of additional charges, the even momenta of the single particle distribution. These latter are set to the asymptotic values, as estimated by direct integration of the underlying Vlasov equation, which formally holds…
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