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    Thermodynamic limit for isokinetic thermostats

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    Thermostat models in space dimension d=1,2,3 for nonequilibrium statistical mechanics are considered and it is shown that, in the thermodynamic limit, the motions of frictionless thermostats and isokinetic thermostats coincide. (C) 2010 American Institute of Physics. [doi:10.1063/1.3376659

    Small deviations from local equilibrium for a process which exhibits hydrodynamical behavior. I

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    The symmetric simple exclusion process where infinitely many particles move randomly on ~, jump with equal probability on nearest-neighbor sites, and interact by simple exclusion is considered. It is known that the only extremal invariant measures are Bernoulli, that each measure, in a suitable class, after a "macroscopic" time is locally described, at a zero-order approximation, by a Bernoulli measure with parameter depending on macroscopic space and time, and that the so-defined equilibrium profile satisfies the heat equation. Small deviations from local equilibrium in the hydrodynamical limit are investigated. It is proven, under suitable assumptions, that at first order the state is Gibbs with one- and two-body potentials whose strength depends only on macroscopic space and time and on the equilibrium profile. More precisely, the one-body potential is linear (on the microscopic positions of the particles) and proportional to the macroscopic space gradient of the equilibrium parameter at that time, so that Fourier law holds. The two-body potential varies on a macroscopic scale and does not depend on the microscopic positions of the particles; it is given by the value of the covariance of the Gaussian "macroscopic density fluctuation field.

    The weakly asymmetric simple exclusion process

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    The one dimensional n.n. simple exclusion process with generator \epsilon^{-2}L_0+\epsilon^{-1}1L_a, \epsilon > 0, is considered, L_0 and L_a respectively the generators of the symmetric and totally asymmetric simple exclusion processes. Propagation of chaos and convergence to the Burgers equation with viscosity are proven in the limit when \epsilon goes to zero. The density fluctuation field is shown to converge to a generalized Ornstein Uhlenbeck process with mean zero. The time asymptotic covariance kernel is explicitly computed for traveling wave profiles and the result indicates that the shock profile is stable while its space location fluctuates around its average position like a brownian motion. Its diffusion coefficient is explicitly computed

    Spectral properties of integral operators in problems of interface dynamic and metastability

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    In this paper we study some integral operators that are obtained by linearizations of a non local evolution equation for a non conserved order parameter which describes the phase of a fluid. We prove a Perron-Frobenius theorem by showing that there is an isolated, simple, maximal eigenvalue larger than 1 with a positive eigenvector and that the rest of the spectrum is strictly inside the unit ball. Such properties are responsible for the existence of invariant, attractive unstable one dimensional manifolds under the full, non linear evolution. This part of the analysis and the application to interface dynamics and metastability will be carried out in separate papers
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