{ "id": "1304.1907", "version": "v1", "published": "2013-04-06T15:54:32.000Z", "updated": "2013-04-06T15:54:32.000Z", "title": "Positive solutions to a supercritical elliptic problem which concentrate along a thin spherical hole", "authors": [ "Mónica Clapp", "Jorge Faya", "Angela Pistoia" ], "categories": [ "math.AP" ], "abstract": "We consider the supercritical problem \\[ -\\Delta v=|v|^{p-2}v in \\Theta_{\\epsilon}, v=0 on \\partial\\Theta_{\\epsilon}, \\] where $\\Theta$ is a bounded smooth domain in $\\mathbb{R}^{N}$, $N\\geq3$, $p>2^{\\ast}:=2N/(N-2)$, and $\\Theta_{\\epsilon}$ is obtained by deleting the $\\epsilon$-neighborhood of some sphere which is embedded in $\\Theta$. In some particular situations we show that, for $\\epsilon>0$ small enough, this problem has a positive solution $v_{\\epsilon}$ and that these solutions concentrate and blow up along the sphere as $\\epsilon$ tends to 0. Our approach is to reduce this problem to a critical problem of the form \\[ -\\Delta u=Q(x)|u|^{4/(n-2)}u in \\Omega_{\\epsilon}, u=0 on \\partial\\Omega_{\\epsilon}, \\] in a punctured domain $\\Omega_{\\epsilon}:=\\{x\\in\\Omega:|x-\\xi_{0}|>\\epsilon\\}$ of lower dimension, by means of some Hopf map. We show that, if $\\Omega$ is a bounded smooth domain in $\\mathbb{R}^{n}$, $n\\geq3$, $\\xi_{0} is in\\Omega,$ $Q is in C^{2}(\\b{\\Oarmega})$ is positive and $\\nabla Q(\\xi_{0})\\neq0$ then, for $\\epsilon>0$ small enough, this problem has a positive solution $u_{\\epsilon}$, and that these solutions concentrate and blow up at $\\xi_{0}$ as $\\epsilon$ goes to 0.", "revisions": [ { "version": "v1", "updated": "2013-04-06T15:54:32.000Z" } ], "analyses": { "subjects": [ "35J60", "35J20" ], "keywords": [ "positive solution", "thin spherical hole", "supercritical elliptic problem", "bounded smooth domain", "solutions concentrate" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013arXiv1304.1907C" } } }