Abstract

In this paper we are concerned with the fractional Schrödinger equation ( − Δ ) α u+V(x)u=f(x,u), x∈ R N , where 0<α<1, N>2α, ( − Δ ) α stands for the fractional Laplacian of order α, V is a positive continuous potential, and f is a continuous subcritical nonlinearity. We obtain the existence of infinitely many weak solutions for the above problem by the fountain theorem in critical point theory.

Highlights

  • In this paper we consider the following fractional Schrödinger equation:(– )αu + V (x)u = f (x, u), x ∈ RN, ( . )where < α α, (– )α stands for the fractional Laplacian of order α, and the potential V : RN → R is a continuous function satisfying (V) < infx∈RN V (x) = V < lim inf|x|→∞ V (x) = V∞ < ∞

  • Where < α α, (– )α stands for the fractional Laplacian of order α, and the potential V : RN → R is a continuous function satisfying (V) < infx∈RN V (x) = V < lim inf|x|→∞ V (x) = V∞ < ∞

  • In [ ], Shang et al considered the existence of nontrivial solutions for ( . ) with f (u) = |u|q– u, where < q < ∗α

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Summary

Introduction

In this paper we consider the following fractional Schrödinger equation:. where < α < , N > α, (– )α stands for the fractional Laplacian of order α, and the potential V : RN → R is a continuous function satisfying (V) < infx∈RN V (x) = V < lim inf|x|→∞ V (x) = V∞ < ∞. In this paper we consider the following fractional Schrödinger equation:. In [ ], Shang and Zhang considered the critical fractional Schrödinger equation ε α(– )αu + V (x)u = |u| ∗α– u + λf (u), x ∈ RN , where ε and λ are positive parameters, V and f satisfy (V) and (H ), respectively. We can see that an alternative definition of the fractional Sobolev space Hα(RN ) via the Fourier transform is as follows: Hα RN = u ∈ L RN : + |ξ | α |F u| dξ < +∞.

Xj and
Then there exists k such that ρk
Now for any k
Thus we obtain
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