Some existence and nonexistence results for a Schrödinger-Poisson type system

preprint2014arXivOpen access

Abstract

In this paper, we study the Schrödinger-Poisson system {−Δu=pup−1v,u>0inRn,−Δv=pup,v>0inRn \left \{ \begin{array}{l} -Δu=\sqrt{p}u^{p-1}v, \quad u>0 \quad in \quad R^n, -Δv=\sqrt{p}u^p, \quad v>0 \quad in \quad R^n \end{array} \right. with n≥3n \geq 3 and p>1p>1. We investigate the existence and the nonexistence of positive classical solutions with the help of an integral system involving the Newton potential {u(x)=c1∫Rnup−1(y)v(y)dy∣x−y∣n−2,u>0inRn,v(x)=c2∫Rnup(y)dy∣x−y∣n−2v>0inRn. \left \{ \begin{array}{l} u(x)=c_1\displaystyle\int_{R^n}\frac{u^{p-1}(y)v(y)dy}{|x-y|^{n-2}}, \quad u>0 \quad in \quad R^n, v(x)=c_2\displaystyle\int_{R^n}\frac{u^p(y)dy}{|x-y|^{n-2}} \quad v>0 \quad in \quad R^n. \end{array} \right. First, the system has no solution when p≤nn−2p\leq \frac{n}{n-2}. When p>nn−2p>\frac{n}{n-2}, the system has a singular solution on Rn∖{0}R^n \setminus \{0\} with slow asymptotic rate 2p−1\frac{2}{p-1}. When p<n+2n−2p<\frac{n+2}{n-2}, the system has no solution in Ln(p−1)2(Rn)L^{\frac{n(p-1)}{2}}(R^n). In fact, if the system has solutions in Ln(p−1)2(Rn)L^{\frac{n(p-1)}{2}}(R^n), then p=n+2n−2p=\frac{n+2}{n-2} and all the positive classical solutions can be classified as u(x)=v(x)=c(tt2+∣x−x∗∣2)n−22u(x)=v(x)=c(\frac{t}{t^2+|x-x^*|^2})^{\frac{n-2}{2}}, where c,tc,t are positive constants. When p>n+2n−2p>\frac{n+2}{n-2}, by the shooting method and the Pohozaev identity, we find another pair of radial solution (u,v)(u,v) satisfying u≡vu \equiv v and decaying with slow rate 2p−1\frac{2}{p-1}.

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