{ "id": "1602.03354", "version": "v1", "published": "2016-02-10T12:45:34.000Z", "updated": "2016-02-10T12:45:34.000Z", "title": "On the Topological degree of the Mean field equation with two parameters", "authors": [ "Aleks Jevnikar", "Juncheng Wei", "Wen Yang" ], "categories": [ "math.AP" ], "abstract": "We consider the following class of equations with exponential nonlinearities on a compact surface $M$: $$ - \\Delta u = \\rho_1 \\left( \\frac{h_1 \\,e^{u}}{\\int_M h_1 \\,e^{u} } - \\frac{1}{|M|} \\right) - \\rho_2 \\left( \\frac{h_2 \\,e^{-u}}{\\int_M h_2 \\,e^{-u} } - \\frac{1}{|M|} \\right), $$ which is associated to the mean field equation of the equilibrium turbulence with arbitrarily signed vortices. Here $h_1, h_2$ are smooth positive functions and $\\rho_1, \\rho_2$ are two positive parameters. We start by proving a concentration phenomena for the above equation, which leads to a-priori bound for the solutions of this problem provided $\\rho_i\\notin 8\\pi\\mathbb{N}, \\, i=1,2$. Then we study the blow up behavior when $\\rho_1$ crosses $8\\pi$ and $\\rho_2 \\notin 8\\pi\\mathbb{N}$. By performing a suitable decomposition of the above equation and using the shadow system that was introduced for the $SU(3)$ Toda system, we can compute the Leray-Schauder topological degree for $\\rho_1 \\in (0,8\\pi) \\cup (8\\pi,16\\pi)$ and $\\rho_2 \\notin 8\\pi\\mathbb{N}$. As a byproduct our argument, we give new existence results when the underlying manifold is a sphere and a new proof for some known existence result.", "revisions": [ { "version": "v1", "updated": "2016-02-10T12:45:34.000Z" } ], "analyses": { "subjects": [ "35J20", "35J60", "35R01" ], "keywords": [ "mean field equation", "parameters", "existence result", "exponential nonlinearities", "leray-schauder topological degree" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2016arXiv160203354J" } } }