{ "id": "2112.05133", "version": "v2", "published": "2021-12-09T18:59:21.000Z", "updated": "2023-07-31T17:16:09.000Z", "title": "Entropic repulsion of 3D Ising interfaces conditioned to stay above a floor", "authors": [ "Reza Gheissari", "Eyal Lubetzky" ], "comment": "34 pages, 1 figure", "categories": [ "math.PR", "math-ph", "math.MP" ], "abstract": "We study the interface of the Ising model in a box of side-length $n$ in $\\mathbb Z^3$ at low temperature $1/\\beta$ under Dobrushin's boundary conditions, conditioned to stay in a half-space above height $h$ (a hard floor). Without this conditioning, Dobrushin showed in 1972 that typically most of the interface is flat at height $0$. With the floor, for small $h$, the model is expected to exhibit {\\it entropic repulsion}, where the typical height of the interface lifts off of $0$. Detailed understanding of the SOS model -- a more tractable height function approximation of 3D Ising -- due to Caputo et al., suggests that there is a single integer value $-h_n^* \\sim -c\\log n$ of the floor height, delineating the transition between rigidity at height $0$ and entropic repulsion. We identify an explicit $h_n^*=( c_\\star+o(1))\\log n$ such that, for the typical Ising interface above a hard floor at $h$, all but an $\\epsilon(\\beta)$-fraction of the sites are propelled to be above height $0$ if $h < h_n^*-1$, whereas all but an $\\epsilon(\\beta)$-fraction of the sites remain at height $0$ if $h\\geq h_n^*$. Further, $c_\\star$ is such that the typical height of the unconditional maximum is $(2c_\\star + o(1))\\log n$; this confirms scaling predictions from the SOS approximation.", "revisions": [ { "version": "v2", "updated": "2023-07-31T17:16:09.000Z" } ], "analyses": { "subjects": [ "60K35", "82B20", "82B24", "82B41" ], "keywords": [ "entropic repulsion", "3d ising interfaces", "hard floor", "tractable height function approximation", "dobrushins boundary conditions" ], "note": { "typesetting": "TeX", "pages": 34, "language": "en", "license": "arXiv", "status": "editable" } } }