{ "id": "2306.14825", "version": "v1", "published": "2023-06-26T16:33:14.000Z", "updated": "2023-06-26T16:33:14.000Z", "title": "Mesoscale mode coupling theory for the weakly asymmetric simple exclusion process", "authors": [ "G. M. Schütz" ], "comment": "29 pages, 1 figure", "categories": [ "cond-mat.stat-mech", "math.PR" ], "abstract": "The asymmetric simple exclusion process and its analysis by mode coupling theory (MCT) is reviewed. To treat the weakly asymmetric case at large space scale $x\\varepsilon^{-1}$, %(corresponding to small Fourier momentum at scale $p\\varepsilon$), large time scale $t \\varepsilon^{-\\chi}$ and weak hopping bias $b \\varepsilon^{\\kappa}$ in the limit $\\varepsilon \\to 0$ we develop a mesoscale MCT that allows for studying the crossover at $\\kappa=1/2$ and $\\chi=2$ from Kardar-Parisi-Zhang (KPZ) to Edwards-Wilkinson (EW) universality. The dynamical structure function is shown to satisfy for all $\\kappa$ an integral equation that is independent of the microscopic model parameters and has a solution that yields a scale-invariant function with the KPZ dynamical exponent $z=3/2$ at scale $\\chi=3/2+\\kappa$ for $0\\leq\\kappa<1/2$ and for $\\chi=2$ the exact Gaussian EW solution with $z=2$ for $\\kappa>1/2$. At the crossover point it is a function of both scaling variables which converges at macroscopic scale to the conventional MCT approximation of KPZ universality for $\\kappa<1/2$. This fluctuation pattern confirms long-standing conjectures for $\\kappa \\leq 1/2$ and is in agreement with mathematically rigorous results for $\\kappa>1/2$ despite the numerous uncontrolled approximations on which MCT is based.", "revisions": [ { "version": "v1", "updated": "2023-06-26T16:33:14.000Z" } ], "analyses": { "subjects": [ "60K35", "82C22" ], "keywords": [ "weakly asymmetric simple exclusion process", "mesoscale mode coupling theory", "pattern confirms long-standing conjectures" ], "note": { "typesetting": "TeX", "pages": 29, "language": "en", "license": "arXiv", "status": "editable" } } }