{ "id": "1809.07911", "version": "v1", "published": "2018-09-21T01:47:36.000Z", "updated": "2018-09-21T01:47:36.000Z", "title": "Hydrodynamic Limit for the SSEP with a Slow Membrane", "authors": [ "Tertuliano Franco", "Mariana Tavares" ], "comment": "36 pages, 6 figures", "categories": [ "math.PR" ], "abstract": "In this paper we consider a symmetric simple exclusion process (SSEP) on the $d$-dimensional discrete torus $\\mathbb{T}^d_N$ with a spatial non-homogeneity given by a slow membrane. The slow membrane is defined here as the boundary of a smooth simple connected region $\\Lambda$ on the continuous $d$-dimensional torus $\\mathbb{T}^d$. In this setting, bonds crossing the membrane have jump rate $\\alpha/N^\\beta$ and all other bonds have jump rate one, where $\\alpha>0$, $\\beta\\in[0,\\infty]$, and $N\\in \\mathbb{N}$ is the scaling parameter. In the diffusive scaling we prove that the hydrodynamic limit presents a dynamical phase transition, that is, it depends on the regime of $\\beta$. For $\\beta\\in[0,1)$, the hydrodynamic equation is given by the usual heat equation on the continuous torus, meaning that the slow membrane has no effect in the limit. For $\\beta\\in(1,\\infty]$, the hydrodynamic equation is the heat equation with Neumann boundary conditions, meaning that the slow membrane $\\partial \\Lambda$ divides $\\mathbb{T}^d$ into two isolated regions $\\Lambda$ and $\\Lambda^\\complement$. And for the critical value $\\beta=1$, the hydrodynamic equation is the heat equation with certain Robin boundary conditions related to the Fick's Law.", "revisions": [ { "version": "v1", "updated": "2018-09-21T01:47:36.000Z" } ], "analyses": { "subjects": [ "60K35", "35K55" ], "keywords": [ "slow membrane", "hydrodynamic limit", "hydrodynamic equation", "symmetric simple exclusion process", "jump rate" ], "note": { "typesetting": "TeX", "pages": 36, "language": "en", "license": "arXiv", "status": "editable" } } }