{ "id": "2007.04661", "version": "v1", "published": "2020-07-09T09:40:18.000Z", "updated": "2020-07-09T09:40:18.000Z", "title": "Upper bounds for the ground state energy of the Laplacian with zero magnetic field on planar domains", "authors": [ "Bruno Colbois", "Alessandro Savo" ], "categories": [ "math.AP", "math.DG" ], "abstract": "We obtain upper bounds for the first eigenvalue of the magnetic Laplacian associated to a closed potential $1$-form (hence, with zero magnetic field) acting on complex functions of a planar domain $\\Omega$, with magnetic Neumann boundary conditions. It is well-known that the first eigenvalue is positive whenever the potential admits at least one non-integral flux. By gauge invariance the lowest eigenvalue is simply zero if the domain is simply connected; then, we obtain an upper bound of the ground state energy depending only on the ratio between the number of holes and the area; modulo a numerical constant the upper bound is sharp and we show that in fact equality is attained (modulo a constant) for Aharonov-Bohm-type operators acting on domains punctured at a maximal $\\epsilon$-net. In the last part we show that the upper bound can be refined, provided that one can transform the given domain in a simply connected one by performing a number of cuts with sufficiently small total length; we thus obtain an upper bound of the lowest eigenvalue by the ratio between the number of holes and the area, multiplied by a Cheeger-type constant, which tends to zero when the domain is metrically close to a simply connected one.", "revisions": [ { "version": "v1", "updated": "2020-07-09T09:40:18.000Z" } ], "analyses": { "subjects": [ "58J50", "35P15" ], "keywords": [ "upper bound", "zero magnetic field", "ground state energy", "planar domain", "first eigenvalue" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }