Abstract

In this paper, we study the following nonlinear Schrödinger-Poisson system \begin{document}$\left\{\begin{array}{ll} -\Delta u+u+\epsilon K(x)\Phi(x)u = f(u),& x\in \mathbb{R}^{3} , \\ -\Delta \Phi = K(x)u^{2},\,\,& x\in \mathbb{R}^{3}, \\\end{array}\right.$ \end{document} where $K(x)$ is a positive and continuous potential and $f(u)$ is a nonlinearity satisfying some decay condition and some non-degeneracy condition, respectively. Under some suitable conditions, which are given in section 1, we prove that there exists some $\epsilon_{0}>0$ such that for $0<\epsilon<\epsilon_{0}$, the above problem has infinitely many positive solutions by applying localized energy method. Our main result can be viewed as an extension to a recent result Theorem 1.1 of Ao and Wei in [3] and a result of Li, Peng and Wang in [26].

Highlights

  • Introduction and the main resultIn this paper, we are mainly motivated by the following problem∂ψ i = − ∆ψ + (V (x) + E)ψ + K(x)Φ(x)ψ − f (x, ψ),∂t 2m (x, t) ∈ R3 × R+,−∆Φ = K(x)|ψ|2, x ∈ R3, where is the Planck constant, i is the imaginary unit, m is a positive constant, E is a real number, > 0, ψ : R3 × [0, T ] → C

  • This paper was partially supported by NSFC (No 11671162, No 11601194) and CCNU18CXTD04. ∗ Corresponding author: Chunhua Wang

  • (1.2) with f (x, u) = Q(x)|u|p−1u, 3 < p < 5. They have proved the existence of positive solutions to (1.2) when Q and K were nonsymmetric and nonnegative functions satisfying lim Q(x) = Q∞ and lim K(x) = 0

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Summary

CHUNHUA WANG AND JING YANG

In [5], the existence of ground state solutions for problem (1.2) has been proved in several situations, including the positive constant potential case. In [14], when = 1 and V (x) ≡ 1, Cerami and Vaira studied (1.2) with f (x, u) = Q(x)|u|p−1u, 3 < p < 5 They have proved the existence of positive solutions to (1.2) when Q and K were nonsymmetric and nonnegative functions satisfying lim Q(x) = Q∞ and lim K(x) = 0. F (x, u) = Q(x)|u|p−1u, 1 < p < 5, in [25], Li, Peng and Yan proved that (1.2) has infinitely many non-radial positive solutions under the assumptions that K(x), Q(x) were positive bounded radial functions in R3 satisfying some decaying conditions.

Noting that
Note that the support of
Now we consider
Since we have
KΦwPm wPm
Since we choose γ
So we have
Findings
Let rj

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