Concentration phenomena for a fractional relativistic Schrödinger equation with critical growth
arXiv:2105.13632 · doi:10.1515/anona-2023-0123
Abstract
In this paper, we are concerned with the following fractional relativistic Schrödinger equation with critical growth: \begin{equation*} \left\{ \begin{array}{ll} (-Δ+m^{2})^{s}u + V(\varepsilon x) u= f(u)+u^{2^{*}_{s}-1} \mbox{ in } \mathbb{R}^{N}, \\ u\in H^{s}(\mathbb{R}^{N}), \quad u>0 \, \mbox{ in } \mathbb{R}^{N}, \end{array} \right. \end{equation*} where is a small parameter, , , , is the fractional critical exponent, is the fractional relativistic Schrödinger operator, is a continuous potential, and is a superlinear continuous nonlinearity with subcritical growth at infinity. Under suitable assumptions on the potential , we construct a family of positive solutions , with exponential decay, which concentrates around a local minimum of as .
This is the final version (several modifications have been made with respect to the previous versions)