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Large Deviation of the Density Profile in the Steady State of the Open Symmetric Simple Exclusion Process

机译:开放对称简单排除过程稳态下密度分布的大偏差

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摘要

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.
机译:我们考虑在位置i = 1,...,N上存在一个开放的一维晶格气体,其中粒子以速率1独立地跳到相邻的内部空位,这是简单的对称排除过程。左边界和右边界处的粒子通量(与在不同化学势下与储层的交换相对应)创建了稳定的非平衡态(SNS),其中稳定的粒子通量穿过系统。在这种状态下,线性的平均密度分布图描述了宏观系统的典型行为,即,当N→∞时,该分布图以概率1出现。对应于某些其他轮廓ρ(x),x = i / N的微观构形的概率具有渐近形式exp [-N $ F $({ρ})]; $ F $是大偏差函数。与平衡系统相反,对于平衡系统,$ F $ eq ({ρ})只是适当归一化的局部自由能密度的积分,我们在这里为非平衡系统找到的$ F $是的非局部函数。 ρ。这引起了通过波动流体动力学预测的SNS中的远距离相关性,并暗示了在普通SNS中类似$ F $的非局部行为,其中已通过实验观察到了远距离相关性。

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