{ "id": "2004.09102", "version": "v1", "published": "2020-04-20T07:35:52.000Z", "updated": "2020-04-20T07:35:52.000Z", "title": "Blow-up phenomena for positive solutions of semilinear diffusion equations in a half-space: the influence of the dispersion kernel", "authors": [ "Matthieu Alfaro", "Otared Kavian" ], "categories": [ "math.AP" ], "abstract": "We consider the semilinear diffusion equation $\\partial$ t u = Au + |u| $\\alpha$ u in the half-space R N + := R N --1 x (0, +$\\infty$), where A is a linear diffusion operator, which may be the classical Laplace operator, or a fractional Laplace operator, or an appropriate non regularizing nonlocal operator. The equation is supplemented with an initial data u(0, x) = u 0 (x) which is nonnegative in the half-space R N + , and the Dirichlet boundary condition u(t, x ' , 0) = 0 for x ' $\\in$ R N --1. We prove that if the symbol of the operator A is of order a|$\\xi$| $\\beta$ near the origin $\\xi$ = 0, for some $\\beta$ $\\in$ (0, 2], then any positive solution of the semilinear diffusion equation blows up in finite time whenever 0 < $\\alpha$ $\\le$ $\\beta$/(N + 1). On the other hand, we prove existence of positive global solutions of the semilinear diffusion equation in a half-space when $\\alpha$ > $\\beta$/(N + 1). Notice that in the case of the half-space, the exponent $\\beta$/(N + 1) is smaller than the so-called Fujita exponent $\\beta$/N in R N. As a consequence we can also solve the blow-up issue for solutions of the above mentioned semilinear diffusion equation in the whole of R N , which are odd in the x N direction (and thus sign changing).", "revisions": [ { "version": "v1", "updated": "2020-04-20T07:35:52.000Z" } ], "analyses": { "keywords": [ "positive solution", "blow-up phenomena", "dispersion kernel", "half-space", "semilinear diffusion equation blows" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }