Abstract

In this paper, we study the following critical system with fractional Laplacian: \t\t\t{(−Δ)su+λ1u=μ1|u|2∗−2u+αγ2∗|u|α−2u|v|βin Ω,(−Δ)sv+λ2v=μ2|v|2∗−2v+βγ2∗|u|α|v|β−2vin Ω,u=v=0in RN∖Ω,\\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}$$\\textstyle\\begin{cases} (-\\Delta)^{s}u+\\lambda_{1}u=\\mu_{1}|u|^{2^{\\ast}-2}u+\\frac{\\alpha \\gamma}{2^{\\ast}}|u|^{\\alpha-2}u|v|^{\\beta} & \\text{in } \\Omega, \\\\ (-\\Delta)^{s}v+\\lambda_{2}v= \\mu_{2}|v|^{2^{\\ast}-2}v+\\frac{\\beta \\gamma}{2^{\\ast}}|u|^{\\alpha}|v|^{\\beta-2}v & \\text{in } \\Omega, \\\\ u=v=0 & \\text{in } \\mathbb{R}^{N}\\setminus\\Omega, \\end{cases} $$\\end{document} where (-Delta)^{s} is the fractional Laplacian, 0< s<1, mu_{1},mu_{2}>0, 2^{ast}=frac{2N}{N-2s} is a fractional critical Sobolev exponent, N>2s, 1<alpha, beta<2, alpha+beta=2^{ast}, Ω is an open bounded set of mathbb{R}^{N} with Lipschitz boundary and lambda_{1},lambda_{2}>-lambda_{1,s}(Omega), lambda_{1,s}(Omega) is the first eigenvalue of the non-local operator (-Delta)^{s} with homogeneous Dirichlet boundary datum. By using the Nehari manifold, we prove the existence of a positive ground state solution of the system for all gamma>0. Via a perturbation argument and using the topological degree and a pseudo-gradient vector field, we show that this system has a positive higher energy solution. Then the asymptotic behaviors of the positive ground state solutions are analyzed when gammarightarrow0.

Highlights

  • The fractional Laplacian operator and fractional Sobolev space arise in a quite natural way in many different contexts, such as the thin obstacle problem, finance, phase transitions, anomalous diffusion, flame propagation and many others

  • By using the Nehari manifold, we prove the existence of a positive ground state solution of the system for all γ > 0

  • Via a perturbation argument and using the topological degree and a pseudo-gradient vector field, we show that this system has a positive higher energy solution

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Summary

Introduction

The fractional Laplacian operator and fractional Sobolev space arise in a quite natural way in many different contexts, such as the thin obstacle problem, finance, phase transitions, anomalous diffusion, flame propagation and many others (see [1–4] and the references therein). Proved the existence and multiplicity of solutions for equation (2) under suitable conditions of s and q. Luo and Zou [11], showed that when λ1, λ2 ∈ (–λ1,s( ), 0), (3) has a positive ground state solution for all γ > 0. Passing to a subsequence, (uγn , vγn ) → (u, v) strongly in Ds( ) × Ds( ) as n → +∞, and one of the following conclusions holds: (1) (u, 0) is a positive ground state solution of. Remark 1.1 the method in this paper to obtain the ground state solution is different from Z. In order to prove Theorem 1.1, we use the classical mountain pass theorem, due to each equation in this system is critical exponent, so the embedding for Ds( ) → L2∗ ( ).

Some preliminaries For the following fractional Brézis–Nirenberg problem
Methods
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