Existence Result for Non-linearly Perturbed Hardy-Schr\"odinger Problems: Local and Non-local cases

Let $\Omega \subset \mathbb{R}^n$ be a smooth bounded domain having zero in its interior $0 \in \Omega.$ We fix $0 < \alpha \le 2$ and $0 \le s <\alpha.$ We investigate a sufficient condition for the existence of a positive solution for the following perturbed problem associated with the Hardy...

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Bibliographic Details
Main Author: Shakerian, Shaya
Format: Journal Article
Language:English
Published: 23-11-2017
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Summary:Let $\Omega \subset \mathbb{R}^n$ be a smooth bounded domain having zero in its interior $0 \in \Omega.$ We fix $0 < \alpha \le 2$ and $0 \le s <\alpha.$ We investigate a sufficient condition for the existence of a positive solution for the following perturbed problem associated with the Hardy-Schr\"odinger operator $ L_{\gamma,\alpha,}: = ({-}{ \Delta})^{\frac{\alpha}{2}}- \frac{\gamma}{|x|^{\alpha}}$ on $\Omega:$ \begin{equation*} \left\{\begin{array}{rl} \displaystyle ({-}{ \Delta})^{\frac{\alpha}{2}}u- \gamma \frac{u}{|x|^{\alpha}} - \lambda u= {\frac{u^{2_{\alpha}^*(s)-1}}{|x|^s}}+ h(x) u^{q-1} & \text{in } {\Omega}\\ u=0 \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, & \text{in } \mathbb{R}^n \setminus \Omega, \end{array}\right. \end{equation*} where ${2_{\alpha}^*(s)}:=\frac{2(n-s)}{n-{\alpha}},$ $\lambda \in \mathbb{R} $, $h \in C^0(\overline{\Omega}),$ $h \ge 0,$ $q \in (2, 2^*_\alpha)$ with $2^*_\alpha:=2^*_\alpha(0),$ and $\gamma < \gamma_H(\alpha),$ the latter being the best constant in the Hardy inequality on $\mathbb{R}^n.$ We prove that there exists a threshold $ \gamma_{crit}(\alpha)$ in $( - \infty, \gamma_H(\alpha)) $ such that the existence of solutions of the above problem is guaranteed by the non-linear perturbation $(i.e., h(x) u^{q-1})$ whenever $ \gamma \le \gamma_{crit}(\alpha),$ while for $\gamma_{crit}(\alpha)<\gamma <\gamma_H(\alpha)$, it is determined by a subtle combination of the geometry of the domain and the size of the nonlinearity of the perturbations.
DOI:10.48550/arxiv.1711.08839