{ "id": "1610.07036", "version": "v1", "published": "2016-10-22T11:28:45.000Z", "updated": "2016-10-22T11:28:45.000Z", "title": "On the stability for Alexandrov's Soap Bubble theorem", "authors": [ "Rolando Magnanini", "Giorgio Poggesi" ], "comment": "20 pages, dedicated to prof. Shigeru Sakaguchi on the occasion of his $60^{th}$ birthday", "categories": [ "math.AP", "math.DG" ], "abstract": "Alexandrov's Soap Bubble theorem dates back to $1958$ and states that a compact embedded hypersurface in $\\mathbb{R}^N$ with constant mean curvature must be a sphere. For its proof, A.D. Alexandrov invented his reflection priciple. In $1982$, R. Reilly gave an alternative proof, based on integral identities and inequalities, connected with the torsional rigidity of a bar. In this article we study the stability of the spherical symmetry: the question is how much a hypersurface is near to a sphere, when its mean curvature is near to a constant in some norm. We present a stability estimate that states that a compact hypersurface $\\Gamma\\subset\\mathbb{R}^N$ can be contained in a spherical annulus whose interior and exterior radii, say $\\rho_i$ and $\\rho_e$, satisfy the inequality $$ \\rho_e - \\rho_i \\le C \\Vert H - H_0 \\Vert^{\\tau_N}_{L^1 (\\Gamma)}, $$ where $\\tau_N=1/2$ if $N=2, 3$, and $\\tau_N=1/(N+2)$ if $N\\ge 4$. Here, $H$ is the mean curvature of $\\Gamma$, $H_0$ is some reference constant and $C$ is a constant that depends on some geometrical and spectral parameters associated with $\\Gamma$. This estimate improves previous results in the literature under various aspects. We also present similar estimates for some related overdetermined problems.", "revisions": [ { "version": "v1", "updated": "2016-10-22T11:28:45.000Z" } ], "analyses": { "subjects": [ "53A10", "35N25", "35B35", "35A23" ], "keywords": [ "alexandrovs soap bubble theorem dates", "constant mean curvature", "compact embedded hypersurface" ], "note": { "typesetting": "TeX", "pages": 20, "language": "en", "license": "arXiv", "status": "editable" } } }