Abstract
We consider an open one dimensional lattice gas on sites i=1,..., N, with particles jumping independently with rate 1 to neighboring interior empty sites, the simple symmetric exclusion process. The particle fluxes at the left and right boundaries, corresponding to exchanges with reservoirs at different chemical potentials, create a stationary nonequilibrium state (SNS) with a steady flux of particles through the system. The mean density profile in this state, which is linear, describes the typical behavior of a macroscopic system, i.e., this profile occurs with probability 1 when N→∞. The probability of microscopic configurations corresponding to some other profile ρ(x), x=i/N, has the asymptotic form exp[−N \(F\)({ρ})]; \(F\) is the large deviation functional. In contrast to equilibrium systems, for which \(F\) eq({ρ}) is just the integral of the appropriately normalized local free energy density, the \(F\) we find here for the nonequilibrium system is a nonlocal function of ρ. This gives rise to the long range correlations in the SNS predicted by fluctuating hydrodynamics and suggests similar non-local behavior of \(F\) in general SNS, where the long range correlations have been observed experimentally.
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Derrida, B., Lebowitz, J.L. & Speer, E.R. Large Deviation of the Density Profile in the Steady State of the Open Symmetric Simple Exclusion Process. Journal of Statistical Physics 107, 599–634 (2002). https://doi.org/10.1023/A:1014555927320
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DOI: https://doi.org/10.1023/A:1014555927320