{ "id": "1712.03736", "version": "v1", "published": "2017-12-11T12:05:37.000Z", "updated": "2017-12-11T12:05:37.000Z", "title": "Wetting and layering for Solid-on-Solid II: Layering transitions, Gibbs states, and regularity of the free energy", "authors": [ "Hubert Lacoin" ], "comment": "55 pages, 3 Figures", "categories": [ "math-ph", "math.MP", "math.PR" ], "abstract": "We consider the Solid-On-Solid model interacting with a wall, which is the statistical mechanics model associated with the integer-valued field $(\\phi(x))_{x\\in \\mathbb Z^2}$, and the energy functional $$V(\\phi)=\\beta \\sum_{x\\sim y}|\\phi(x)-\\phi(y)|-\\sum_{x}\\left( h{\\bf 1}_{\\{\\phi(x)=0\\}}-\\infty{\\bf 1}_{\\{\\phi(x)<0\\}} \\right).$$ We prove that for $\\beta$ sufficiently large, there exists a decreasing sequence $(h^*_n(\\beta))_{n\\ge 0}$, satisfying $\\lim_{n\\to\\infty}h^*_n(\\beta)=h_w(\\beta),$ and such that: $(A)$ The free energy associated with the system is infinitely differentiable on $\\mathbb R \\setminus \\left(\\{h^*_n\\}_{n\\ge 1}\\cup h_w(\\beta)\\right)$, and not differentiable on $\\{h^*_n\\}_{n\\ge 1}$. $(B)$ For each $n\\ge 0$ within the interval $(h^*_{n+1},h^*_n)$ (with the convention $h^*_0=\\infty$), there exists a unique translation invariant Gibbs state which is localized around height $n$, while at a point of non-differentiability, at least two ergodic Gibbs state coexist. The respective typical heights of these two Gibbs states are $n-1$ and $n$. The value $h^*_n$ corresponds thus to a first order layering transition from level $n$ to level $n-1$. These results combined with those obtained in [23] provide a complete description of the wetting and layering transition for SOS.", "revisions": [ { "version": "v1", "updated": "2017-12-11T12:05:37.000Z" } ], "analyses": { "keywords": [ "free energy", "unique translation invariant gibbs state", "solid-on-solid", "regularity", "ergodic gibbs state coexist" ], "note": { "typesetting": "TeX", "pages": 55, "language": "en", "license": "arXiv", "status": "editable" } } }