On the weighted logarithmic potential operator

Abstract

For a bounded open set $Ω\subset \mathbb{R}^N$ with $N\geq 2$, and for positive continuous functions $w,g$ on $\overlineΩ$, we consider the weighted eigenvalue problem \begin{equation*} \mathcal{L}_{w} u =τgu, \end{equation*} where $\mathcal{L}_{w}$ is the weighted logarithmic potential operator on $L^2(Ω)$ as defined below: \begin{equation*} \mathcal{L}_{w} u(x)=\int_Ω\log\left(\frac{w(x)w(y)}{|x-y|}\right)u(y)dy. \end{equation*} We study the monotonicity and continuity of the largest positive eigenvalue $τ_{w,g}^+(Ω)$ with respect to $Ω$, $w$, and $g$. We also establish that $τ_{w,g}^+(Ω)$ satisfies a reverse Faber Krahn inequality under polarization. We provide a sufficient condition for the existence of a negative eigenvalue in terms of the weighted transfinite diameter of $Ω$, under the assumption that $\log w$ is superharmonic. For $Ω\subset \mathbb{R}^2$, if $Δ\log w $ is a constant $C$, we show that 0 can be an eigenvalue of $\mathcal{L}_{w}$ only when $C=\frac{2π}{|Ω|}$. For such domains, if $\log w$ is a harmonic function on $Ω$, we provide a representation formula for the eigenfunctions. Using this representation, we establish variants of the maximum principles that give some insight into the geometry of these eigenfunctions.

Figures (2)

• Figure 1: $\Omega$
• Figure 2: $P_H(\Omega)$

Theorems & Definitions (45)

• Theorem 1.1
• Theorem 1.2
• Theorem 1.3
• Definition 1.4
• Definition 1.5
• Theorem 1.6
• Remark 1.7
• Remark 1.8
• Theorem 1.9
• Theorem 1.10