{ "id": "2105.06103", "version": "v2", "published": "2021-05-13T06:49:23.000Z", "updated": "2021-07-21T06:50:15.000Z", "title": "Long-Range Ising Models: Contours, Phase Transitions and Decaying Fields", "authors": [ "Lucas Affonso", "Rodrigo Bissacot", "Eric O. Endo", "Satoshi Handa" ], "comment": "Preliminary Version, 27 pages", "categories": [ "math-ph", "cond-mat.stat-mech", "math.MP", "math.PR" ], "abstract": "Inspired by Fr\\\"{o}hlich-Spencer and subsequent authors who introduced the notion of contour for long-range systems, we provide a definition of contour and a direct proof for the phase transition for ferromagnetic long-range Ising models on $\\mathbb{Z}^d$, $d\\geq 2$. The argument, which is based on a multi-scale analysis, works for the sharp region $\\alpha>d$ and improves previous results obtained by Park for $\\alpha>3d+1$, and by Ginibre, Grossmann, and Ruelle for $\\alpha> d+1$, where $\\alpha$ is the power of the coupling constant. The key idea is to avoid a large number of small contours. As an application, we prove the persistence of the phase transition when we add a polynomial decaying magnetic field with power $\\delta>0$ as $h^*|x|^{-\\delta}$, where $h^* >0$. For $d<\\alphad-\\alpha$, and when $h^*$ is small enough over the critical line $\\delta=d-\\alpha$. For $\\alpha \\geq d+1$, $\\delta>1$ it is enough to prove the phase transition, and for $\\delta=1$ we have to ask $h^*$ small. The natural conjecture is that this region is also sharp for the phase transition problem when we have a decaying field.", "revisions": [ { "version": "v2", "updated": "2021-07-21T06:50:15.000Z" } ], "analyses": { "subjects": [ "82B05", "82B26", "82B20", "82Bxx" ], "keywords": [ "decaying field", "ferromagnetic long-range ising models", "polynomial decaying magnetic field", "phase transition occurs", "phase transition problem" ], "note": { "typesetting": "TeX", "pages": 27, "language": "en", "license": "arXiv", "status": "editable" } } }