Abstract

In this paper, we study the following nonlinear Klein–Gordon–Maxwell system: \t\t\t{−Δu+V(x)u−(2ω+ϕ)ϕu=f(x,u)+λh(x)|u|q−2u,x∈R3,Δϕ=(ω+ϕ)u2,x∈R3,(Pλ)\\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}$$ \\textstyle\\begin{cases} -\\Delta u+ V(x)u-(2\\omega +\\phi )\\phi u = f(x,u)+\\lambda h(x) \\vert u \\vert ^{q-2}u, & x\\in \\mathbb{R}^{3},\\\\ \\Delta \\phi = (\\omega +\\phi )u^{2}, & x\\in \\mathbb{R}^{3}, \\end{cases}\\displaystyle \\quad (\\mathrm{P_{\\lambda }}) $$\\end{document} where ω and λ are positive constants, V is a continuous function with negative infimum, qin (1,2), hin L^{frac{2}{2-q}}(mathbb{R}^{3}) is a positive potential function. Under the classic Ambrosetti–Rabinowitz condition, nontrivial solutions are obtained via the symmetric mountain pass theorem and the mountain pass theorem. In our paper, the nonlinearity F can also change sign and does not need to satisfy any 4-superlinear condition. We extend and improve some existing results to some extent.

Highlights

  • Introduction and main results A KleinGordon–Maxwell system arises in a very interesting physical context: a model describing the nonlinear Klein–Gordon field interacting with the electromagnetic field

  • In this paper, we study the following nonlinear Klein–Gordon–Maxwell system:

  • Ambrosetti–Rabinowitz condition, nontrivial solutions are obtained via the symmetric mountain pass theorem and the mountain pass theorem

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Summary

Under the classic

Ambrosetti–Rabinowitz condition, nontrivial solutions are obtained via the symmetric mountain pass theorem and the mountain pass theorem. Many solutions for a type of Klein–Gordon–Maxwell system with a coercive potential were got via a variant fountain theorem and the symmetric mountain pass theorem in [17]. Superlinear condition, infinitely many solutions for a nonlinear Klein–Gordon–Maxwell system with sign-changing potential were got by Ding and Li via the symmetric mountain pass theorem. Theorem 1.1 Let (V), (F1)–(F3) and (H) hold, there exists λ∗ > 0 such that the system (Pλ) has a sequence of weak solutions {(un, φn)} ⊂ E × D1,2(R3) satisfying. Lemma 3.1 Let (F1) and (F2) be satisfied, (i) there exist constants c1, c2 ∈ (0, ∞) such that. Lemma 3.2 Assume that (V ), (F1), (F2) and (H) hold, the functional I satisfies the (PS) condition.

Since the sequence
Xi and
4Cλ q
Methods

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