Normalized ground states for Kirchhoff equations in R3{\mathbb{R}}^{3} with a critical nonlinearity

preprint2021arXivOpen access

Abstract

This paper is concerned with the existence of ground states for a class of Kirchhoff type equation with combined power nonlinearities \begin{equation*} -\left(a+b\int_{\mathbb{R}^{3}}|\nabla u(x)|^{2}\right) Δu =λu+|u|^{p-2}u+u^{5}\quad \ \text{for some} \ λ\in\mathbb{R},\quad x\in\mathbb{R}^{3}, \end{equation*} with prescribed L2L^{2}-norm mass \begin{equation*} \int_{\mathbb{R}^{3}}u^{2}=c^{2} \end{equation*} in Sobolev critical case and proves that the equation has a couple of solutions (uc,λc)∈S(c)×R(u_{c},λ_{c})\in S(c)\times \mathbb{R} for any c>0c>0, a,b>0a,b >0 and 143≤p<6,\frac{14}{3}\leq p< 6, where S(c)={u∈H1(R3):∫R3u2=c2}.S(c)=\{u\in H^{1}(\mathbb{R}^{3}):\int_{\mathbb{R}^{3}}u^{2}=c^{2}\}. \textbf{Keywords:} Kirchhoff type equation; Critical nonlinearity; Normalized ground states \noindent{AMS Subject Classification:\, 37L05; 35B40; 35B41.}

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