Semi-classical states for fractional Schrödinger equations with magnetic fields and fast decaying potentials

This paper deals with the following fractional magnetic Schrödinger equations\begin{document}$ \varepsilon^{2s}(-\Delta)^s_{A/\varepsilon} u +V(x)u = |u|^{p-2}u, \ x\in{\mathbb R}^N, $\end{document}where \begin{document}$ \varepsilon>0 $\end{document} is a parameter, \begin{document}$ s\in(0,1) $\end{document} , \begin{document}$ N\geq3 $\end{document} , \begin{document}$ 2+2s/(N-2s)<p<2_s^*: = 2N/(N-2s) $\end{document} , \begin{document}$ A\in C^{0,\alpha}({\mathbb R}^N,{\mathbb R}^N) $\end{document} with \begin{document}$ \alpha\in(0,1] $\end{document} is a magnetic field, \begin{document}$ V:{\mathbb R}^N\to{\mathbb R} $\end{document} is a nonnegative continuous potential. By variational methods and penalized idea, we show that the problem has a family of solutions concentrating at a local minimum of \begin{document}$ V $\end{document} as \begin{document}$ \varepsilon\to 0 $\end{document} . There is no restriction on the decay rates of \begin{document}$ V $\end{document} . Especially, \begin{document}$ V $\end{document} can be compactly supported. The appearance of \begin{document}$ A $\end{document} and the nonlocal of \begin{document}$ (-\Delta)^s $\end{document} makes the proof more difficult than that in [ 7 ], which considered the case \begin{document}$ A\equiv 0 $\end{document} .