{ "id": "1911.03018", "version": "v1", "published": "2019-11-08T03:35:41.000Z", "updated": "2019-11-08T03:35:41.000Z", "title": "On self-adjointness of symmetric diffusion operators", "authors": [ "Derek W Robinson" ], "categories": [ "math.FA" ], "abstract": "Let $\\Omega$ be a domain in $\\Ri^d$ with boundary $\\Gamma$ and let $d_\\Gamma$ denote the Euclidean distance to $\\Gamma$. Further let $H=-\\divv(C\\nabla)$ where $C=(\\,c_{kl}\\,)>0$ with $c_{kl}=c_{lk}$ are real, bounded, Lipschitz continuous functions and $D(H)=C_c^\\infty(\\Omega)$. Assume also that there is a $\\delta\\geq0$ such that $\\|C/d_\\Gamma^{\\,\\delta}-aI\\|\\to 0$ as $d_\\Gamma\\to0$ with $\\delta\\geq0$ where $a$ is a bounded Lipschitz continuous function with $a\\geq\\mu>0$ on a boundary layer $\\Gamma_{\\!\\!r}=\\{x\\in\\Omega: d_\\Gamma(x)2-(d-d_H)/2$ is sufficient for $H$ to be essentially self-adjoint as an operator on $L_2(\\Omega)$. In particular $\\delta>3/2$ suffices for $C^2$-domains. Finally we prove that $\\delta\\geq 3/2$ is necessary in the $C^2$-case.", "revisions": [ { "version": "v1", "updated": "2019-11-08T03:35:41.000Z" } ], "analyses": { "keywords": [ "symmetric diffusion operators", "self-adjointness", "convex set", "boundary layer", "bounded lipschitz continuous function" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }