2019
DOI: 10.1216/rmj-2019-49-7-2205
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Multiplicity results for a fractional Schrodinger equation with potentials

Abstract: This paper is devoted to study a class of nonlinear fractional Schrödinger equations:where s ∈ (0, 1), N > 2s, (−∆) s stands for the fractional Laplacian. The main purpose of this paper is to study the existence of infinitely many solutions for the aforementioned equation. By using variational methods and the genus properties in critical point theory, we establish the existence of at least one nontrivial solution as well as infinitely many solutions for the above equation with a general potential V (x) which i… Show more

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Cited by 4 publications
(5 citation statements)
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“…When V(x) is periodic, the existence of ground state solutions is investigated in [1,23,32,39]. For the case V(x) is allowed to be sign-changing, existence and multiplicity results of nontrivial solutions are given by [5,13,25].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…When V(x) is periodic, the existence of ground state solutions is investigated in [1,23,32,39]. For the case V(x) is allowed to be sign-changing, existence and multiplicity results of nontrivial solutions are given by [5,13,25].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The sequence {v n } ∞ n=1 is bounded in L p (R N ) by the boundness of it in X and Lemma 1, which, together with (12), implies that…”
mentioning
confidence: 89%
“…Schrödinger equations involving fractional Laplacians like (3) were largely studied. See [8][9][10][11][12] for instance.…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, mathematicians have displayed lively interest in the study of equations involving the fractional Laplacian. There are a variety of mathematical methods for the fractional Laplacian operators, such as Caffarelli-Silvestre extension method [12,28], variational method [14,17,20,22,27,32,34,36,40,43,47,48], direct method [8,10,11] and so on.…”
Section: Introductionmentioning
confidence: 99%
“…s u + u = |u| p−1 u in R N . Khoutir [27] gives multiplicity results of solutions to (−∆) s u + V (x) u = f (x, u) in R N with a general potential V (x) . Secchi [43] constructs solutions to (−∆) s u + V (x) u = f (x, u) in R N based on minimization on the Nehari manifold.…”
Section: Introductionmentioning
confidence: 99%