On a class of semilinear fractional elliptic equations involving outside Dirac data
arXiv:1501.06242
Abstract
The purpose of this article is to give a complete study of the weak solutions of the fractional elliptic equation \begin{equation}\label{00} \arraycolsep=1pt \begin{array}{lll} (-Δ)^α u+u^p=0\ \ \ \ &\ {\rm in}\ \ B_1(e_N),\\[2mm]\phantom{(-Δ)^α +u^p} u=δ_{0}& \ {\rm in}\ \ \mathbb{R}^N\setminus B_1(e_N), \end{array} \end{equation} where , with denotes the fractional Laplacian operator in the principle value sense, is the unit ball centered at in with and is the Dirac mass concentrated at the origin. We prove that problem (\ref{00}) admits a unique weak solution when . Moreover, if in addition , the weak solution vanishes as . We also show that problem (\ref{00}) doesn't have any weak solution when . These results are very surprising since there are in total contradiction with the classical setting, i.e. $$ \arraycolsep=1pt \begin{array}{lll} -Δu+ u^p=0\ \ \ \ &\ {\rm in}\ \B_1(e_N),\\[2mm] \phantom{-Δ+u^{p} } u=δ_{0}& \ {\rm in}\ \ \R^N\setminus B_1(e_N), \end{array} $$ for which it has been proved that there are no solutions for .
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