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    Existence of positive ground state solutions of Schrödinger–Poisson system involving negative nonlocal term and critical exponent on bounded domain

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    Abstract(#br)In this paper, we prove the existence of positive ground state solutions of the Schrödinger–Poisson system involving a negative nonlocal term and critical exponent on a bounded domain. The main tools are the mountain pass theorem and the concentration compactness principle

    Quantitative Properties on the Steady States to A Schr\"odinger-Poisson-Slater System

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    A relatively complete picture on the steady states of the following Schro¨\ddot{o}dinger-Poisson-Slater (SPS) system \begin{cases} -\Delta Q+Q=VQ-C_{S}Q^{2}, & Q>0\text{ in }\mathbb{R}^{3}\\ Q(x)\to0, & \mbox{as }x\to\infty,\\ -\Delta V=Q^{2}, & \text{in }\mathbb{R}^{3}\\ V(x)\to0 & \mbox{as }x\to\infty. \end{cases} is given in this paper: existence, uniqueness, regularity and asymptotic behavior at infinity, where CS>0C_{S}>0 is a constant. To the author's knowledge, this is the first uniqueness result on SPS system

    Concentration phenomena for critical fractional Schr\"odinger systems

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    In this paper we study the existence, multiplicity and concentration behavior of solutions for the following critical fractional Schr\"odinger system \begin{equation*} \left\{ \begin{array}{ll} \varepsilon^{2s} (-\Delta)^{s}u+V(x) u=Q_{u}(u, v)+\frac{1}{2^{*}_{s}}K_{u}(u, v) &\mbox{ in } \mathbb{R}^{N}\varepsilon^{2s} (-\Delta)^{s}u+W(x) v=Q_{v}(u, v)+\frac{1}{2^{*}_{s}}K_{v}(u, v) &\mbox{ in } \mathbb{R}^{N} u, v>0 &\mbox{ in } \R^{N}, \end{array} \right. \end{equation*} where ε>0\varepsilon>0 is a parameter, s∈(0,1)s\in (0, 1), N>2sN>2s, (−Δ)s(-\Delta)^{s} is the fractional Laplacian operator, V:RN→RV:\mathbb{R}^{N}\rightarrow \mathbb{R} and W:RN→RW:\mathbb{R}^{N}\rightarrow \mathbb{R} are positive H\"older continuous potentials, QQ and KK are homogeneous C2C^{2}-functions having subcritical and critical growth respectively. We relate the number of solutions with the topology of the set where the potentials VV and WW attain their minimum values. The proofs rely on the Ljusternik-Schnirelmann theory and variational methods.Comment: arXiv admin note: text overlap with arXiv:1704.0060
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