Asymmetric exclusion process with long-range interactions

V. Belitsky, N. P. N. Ngoc, G. M. Schütz
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Abstract

We consider asymmetric simple exclusion processes with $N$ particles on the one-dimensional discrete torus with $L$ sites with following properties: (i) nearest-neighbor jumps on the torus, (ii) the jump rates depend only on the distance to the next particle in the direction of the jump, (iii) the jump rates are independent of $N$ and $L$. For measures with a long-range two-body interaction potential that depends only on the distance between neighboring particles we prove a relation between the interaction potential and particle jump rates that is necessary and sufficient for the measure to be invariant for the process. The normalization of the measure and the stationary current are computed both for finite $L$ and $N$ and in the thermodynamic limit. For a finitely many particles that evolve on $\mathbb{Z}$ with totally asymmetric jumps it is proved, using reverse duality, that a certain family of nonstationary measures with a microscopic shock and antishock evolves into a convex combination of such measures with weights given by random walk transition probabilities. On macroscopic scale this domain random walk is a travelling wave phenomenon tantamount to phase separation with a stable shock and stable antishock. Various potential applications of this result and open questions are outlined.
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具有长程相互作用的不对称排斥过程
我们考虑了一维离散环上具有 $L$ 位点的 $N$ 粒子的非对称简单排阻过程,该过程具有以下性质:(i) 环上的近邻跃迁;(ii) 跃迁率仅取决于跃迁方向上到下一个粒子的距离;(iii) 跃迁率与 $N$ 和 $L$ 无关。对于具有长程双体相互作用势的量度,其相互作用势只取决于相邻粒子之间的距离,我们证明了相互作用势与粒子跃迁率之间的关系,这种关系是量度对过程保持不变的必要条件和充分条件。我们计算了有限 $L$ 和 $N$ 以及热力学极限下的量纲归一化和静态电流。对于在$\mathbb{Z}$上以完全不对称跳跃演化的无限多粒子,利用反向对偶性证明了具有微观冲击和反冲击的非稳态度量的某一族会演化成此类度量的凸组合,其权重由随机漫步过渡概率给出。在宏观尺度上,这种域随机游走是一种游走波现象,相当于具有稳定冲击和稳定反冲击的相分离。本文概述了这一结果的各种潜在应用和有待解决的问题。
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