Abstract

In this paper, we study the following fractional Schrödinger equation with electromagnetic fields and critical or supercritical nonlinearity: (−Δ)Asu+V(x)u=f(x,|u|2)u+λ|u|p−2u,x∈RN,\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$ (-\\Delta )_{A}^{s}u+V(x)u=f\\bigl(x, \\vert u \\vert ^{2}\\bigr)u+\\lambda \\vert u \\vert ^{p-2}u,\\quad x \\in \\mathbb{R}^{N}, $$\\end{document} where (-Delta )_{A}^{s} is the fractional magnetic operator with 0< s<1, N>2s, lambda >0, 2_{s}^{*}=frac{2N}{N-2s}, pgeq 2_{s}^{*}, f is a subcritical nonlinearity, and V in C(mathbb{R}^{N},mathbb{R}) and A in C(mathbb{R}^{N}, mathbb{R}^{N}) are the electric and magnetic potentials, respectively. Under some suitable conditions, by variational methods we prove that the equation has a nontrivial solution for small lambda >0. Our main contribution is related to the fact that we are able to deal with the case p>2_{s}^{*}.

Highlights

  • Introduction and preliminariesConsider the following fractional Schrödinger equation with electromagnetic fields and critical or supercritical nonlinearity:(– )sAu + V (x)u = f x, |u|2 u + λ|u|p–2u, x ∈ RN, (1.1) where (–, p ≥ 2∗s, f is a subcritical nonlinearity, and V ∈ C(RN, R) and A ∈ C(RN, RN ) are the electric and magnetic potentials, respectively.The fractional magnetic Laplacian is defined by (– u(x)CN,s lim r→0 u(x) ei(x–y)·A( x+y 2 )u(y) Bcr (x)

  • We study the following fractional Schrödinger equation with electromagnetic fields and critical or supercritical nonlinearity: (– )sAu + V(x)u = f (x, |u|2)u + λ|u|p–2u, x ∈ RN, where

  • The fractional magnetic Laplacian is defined by CN,s lim r→0 u(x) ei(x–y)·A(

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Summary

Introduction

We study the following fractional Schrödinger equation with electromagnetic fields and critical or supercritical nonlinearity: (– )sAu + V(x)u = f (x, |u|2)u + λ|u|p–2u, x ∈ RN, where By variational methods we prove that the equation has a nontrivial solution for small λ > 0. Introduction and preliminaries Consider the following fractional Schrödinger equation with electromagnetic fields and critical or supercritical nonlinearity: (– )sAu + V (x)u = f x, |u|2 u + λ|u|p–2u, x ∈ RN , (1.1)

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