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Existence and multiplicity of nontrivial solutions for Schr??dinger-Poisson systems on bounded domains

机译:有界域上Schr ?? dinger-Poisson系统非平凡解的存在性和多重性

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In this paper, we concern with the following Schr??dinger-Poisson system: $$ extstyleegin{cases} -Delta u+phi u = f(x,u) , & xinOmega, -Deltaphi=u^{2}, & xinOmega, u=phi=0, & x inpartialOmega, end{cases} $$ where ?? is a smooth bounded domain in (mathbb{R}^{3}). Under more appropriate assumptions on??f, we obtain new results on the existence of nontrivial solutions and infinitely many solutions by using the mountain pass theorem and the symmetric mountain pass theorem, respectively. We extend and improve some recent results in the literature.KeywordsSchr??dinger-Poisson system??variational methods??mountain pass theorem??symmetric mountain pass theorem??MSC35J20??35J60??1 Introduction and preliminariesConsider the the following Schr??dinger-Poisson system: $$ extstyleegin{cases} -Delta u+phi u = f(x,u) , & xinOmega, -Deltaphi=u^{2}, & x inOmega, u=phi=0, & x inpartialOmega, end{cases} $$ (1.1) where ?? is a smooth bounded domain in (mathbb{R}^{3}), and (fin C(Omegaimesmathbb{R},mathbb{R})).System (1.1) is related to the stationary analogue of the nonlinear parabolic Schr??dinger-Poisson system $$ extstyleegin{cases} -irac{partialpsi}{partial t}=-Deltapsi+phi(x)psi- ert psi ert ^{p-2}psi & ext{in } Omega, -Deltaphi= ert psi ert ^{2} & ext{in }Omega, psi=phi=0 & ext{on } partialOmega. end{cases} $$ (1.2) The first equation in (1.2) is called the Schr??dinger equation, which describes quantum particles interacting with the electromagnetic field generated by the motion. An interesting class of Schr??dinger equations is the case where the potential (phi(x)) is determined by the charge of the wave function itself, that is, when the second equation in (1.2) (Poisson equation) holds. For more details as regards the physical relevance of the Schr??dinger-Poisson system, we refer to [1, 2, 3, 4].Recently, Schr??dinger-Poisson systems on unbounded domains or on the whole space (mathbb{R}^{N}) have attracted a lot of attention. Many solvability conditions on the nonlinearity have been given to obtain the existence and multiplicity of solutions for Schr??dinger-Poisson systems in (mathbb{R}^{N}), we refer the readers to [4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23] and references therein.
机译:在本文中,我们关注以下Schr ?? dinger-Poisson系统:$$ textstyle begin {cases}- Delta u + phi u = f(x,u),&x in Omega, - Delta phi = u ^ {2},&x in Omega, u = phi = 0,&x in partial Omega, end {cases} $$其中??是( mathbb {R} ^ {3} )中的光滑有界域。在更恰当的假设Δf上,我们分别通过使用山通过定理和对称山通过定理,获得了关于非平凡解和无限多个解的存在性的新结果。我们对文献中的最新结果进行了扩展和改进。关键词Schr,dinger-Poisson系统,变分方法,山路定理,对称山路定理,MSC35J20、35J60、1引言和初步考虑以下Schr? dinger-Poisson系统:$$ textstyle begin {cases}- Delta u + phi u = f(x,u),&x in Omega,- Delta phi = u ^ {2} ,&x in Omega, u = phi = 0,&x in partial Omega, end {cases} $$(1.1),其中??是( mathbb {R} ^ {3} )和(f in C( Omega times mathbb {R}, mathbb {R})))中的光滑有界域。系统(1.1 )与非线性抛物线Schr ?? dinger-Poisson系统的平稳类似物$$ textstyle begin {cases} -i frac { partial psi} { partial t} =- Delta psi + phi (x) psi- vert psi vert ^ {p-2} psi& text {in} Omega,- Delta phi = vert psi vert ^ {2}& text {in} Omega, psi = phi = 0和 text {on} partial Omega。 end {cases} $$(1.2)(1.2)中的第一个方程称为Schr ?? dinger方程,该方程描述了量子粒子与运动产生的电磁场相互作用。有趣的一类Schr ?? dinger方程是电势( phi(x))由波动函数本身的电荷决定的情况,也就是说,当(1.2)中的第二个方程(泊松方程)时持有。有关Schr ?? dinger-Poisson系统的物理相关性的更多详细信息,请参考[1,2,3,4]。最近,Schr ?? dinger-Poisson系统在无界域或整个空间上( mathbb {R} ^ {N} )吸引了很多关注。给出了许多关于非线性的可解性条件,以获得( mathbb {R} ^ {N} )中Schr ?? dinger-Poisson系统解的存在性和多重性,我们请读者参考[4,5, 6、7、8、9、10、11、12、13、14、15、16、17、18、19、20、21、22、23]及其引用。

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