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arXiv 2409.17543math.AP
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通过局部Pohozaev恒等式构造具有Sobolev临界增长的非线性椭圆系统的解

Construction of solutions to a nonlinear critical elliptic system via local Pohozaev identities

Qidong Guo, Qingfang Wang, Wenju Wu

AI总结:

本文研究具有Sobolev临界增长的非线性椭圆系统,通过结合有限约化论证和局部Pohozaev恒等式,在特定条件下构造出能量可任意大的同步型非径ial正向量解的无界序列,推广了单一临界问题的结论。

摘要:

本文研究具有Sobolev临界增长的椭圆系统:$-Δu+P(|y'|,y'')u=u^{2^*-1}+\fracβ{2} u^{\frac{2^*}{2}-1}v^{\frac{2^*}{2}},\\ y\in R^N$,$-Δv+Q(|y'|,y'')v=v^{2^*-1}+\fracβ{2} v^{\frac{2^*}{2}-1}u^{\frac{2^*}{2}}$,$y\in R^N$,$u,v>0$,$u,v\in H^1(R^N)$。其中$(y',y'')\in R^2 \times R^{N-2}$,$P(|y'|,y'')$和$Q(|y'|,y'')$是$R^+\times R^{N-2}$中的有界非负函数,$2^*=\frac{2N}{N-2}$。通过结合有限约化论证和局部Pohozaev型恒等式,在假设$N\geq 5$且$r^2(P(r,y'')+κ^2Q(r,y''))$具有共同的拓扑非平凡临界点的条件下,构造出同步型非径向正向量解的无界序列,其能量可任意大。结果推广了[Peng, Wang and Yan, J. Funct. Anal. 274: 2606-2633, 2018]单一临界问题的结论。创新点主要有两方面:一方面,当$N\geq5$时,耦合指数$\frac{2}{N-2}<1$,给直接应用扰动论证造成极大困难,这是耦合系统与单一方程的主要差异;另一方面,$P(y)$和$Q(y)$较弱的对称性条件使我们无法直接估计约化泛函的相应导数来定位解的集中点,故采用局部Pohozaev恒等式进行定位。

英文摘要:

In this paper, we investigate the following elliptic system with Sobolev critical growth $-Δu+P(|y'|,y'')u=u^{2^*-1}+\fracβ{2} u^{\frac{2^*}{2}-1}v^{\frac{2^*}{2}},\ y\in R^N$, $-Δv+Q(|y'|,y'')v=v^{2^*-1}+\fracβ{2} v^{\frac{2^*}{2}-1}u^{\frac{2^*}{2}}$, $y\in R^N ,u,v>0,u,\,v\in H^1(R^N), $ where~$(y',y'')\in R^2 \times R^{N-2}$, $P(|y'|,y''), Q(|y'|,y'')$ are bounded non-negative function in $R^+\times R^{N-2}$, $2^*=\frac{2N}{N-2}$. By combining a finite reduction argument and local Pohozaev type of identities, assuming that $N\geq 5$ and $r^2(P(r,y'')+κ^2Q(r,y''))$ have a common topologically nontrivial critical point, we construct an unbounded sequence of non-radial positive vector solutions of synchronized type, whose energy can be made arbitrarily large. Our result extends the result of a single critical problem by [Peng, Wang and Yan,J. Funct. Anal. 274: 2606-2633, 2018]. The novelties mainly include the following two aspects. On one hand, when $N\geq5$, the coupling exponent $\frac{2}{N-2}<1$, which creates a great trouble for us to apply the perturbation argument directly. This constitutes the main difficulty different between the coupling system and a single equation. On the other hand, the weaker symmetry conditions of $P(y)$ and $Q(y)$ make us not estimate directly the corresponding derivatives of the reduced functional in locating the concentration points of the solutions, we employ some local Pohozaev identities to locate them.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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