Quantization property of n-Laplacian mean field equation and sharp Moser-Onofri inequality (2406.00743v2)
Abstract: In this paper, we are concerned with the following $n$-Laplacian mean field equation [ \left{ {\begin{array}{*{20}{c}} { - \Delta_n u = \lambda eu} & {\rm in} \ \ \Omega, \ {\ \ \ \ u = 0} &\ {\rm on}\ \partial \Omega, \end{array}} \right. ] [] where $\Omega$ is a smooth bounded domain of $\mathbb{R}n \ (n\geq 2)$ and $- \Delta_n u =-{\rm div}(|\nabla u|{n-2}\nabla u)$. We first establish the quantization property of solutions to the above $n$-Laplacian mean field equation. As an application, combining the Pohozaev identity and the capacity estimate, we obtain the sharp constant $C(n)$ of the Moser-Onofri inequality in the $n$-dimensional unit ball $Bn:=Bn(0,1)$, $$\mathop {\inf }\limits_{u \in W_0{1,n}(Bn)}\frac{1}{ n C_n}\int_{Bn} | \nabla u|n dx- \ln \int_{Bn} {eu} dx\geq C(n),$$ which extends the result of Caglioti-Lions-Marchioro-Pulvirenti in \cite{Caglioti} to the case of $n$-dimensional ball. Here $C_n=(\frac{n2}{n-1}){n-1} \omega_{n-1}$ and $\omega_{n-1}$ is the surface measure of $Bn$. For the Moser-Onofri inequality in a general bounded domain of $\mathbb{R}n$, we apply the technique of $n$-harmonic transplantation to give the optimal concentration level of the Moser-Onofri inequality and obtain the criterion for the existence and non-existence of extremals for the Moser-Onofri inequality.
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