On Lipschitz continuity of solutions of hyperbolic Poisson's equation

preprint2021arXivOpen access

Abstract

In this paper, we investigate solutions of the hyperbolic Poisson equation Δhu(x)=ψ(x)Δ_{h}u(x)=ψ(x), where ψ∈L∞(Bn,Rn)ψ\in L^{\infty}(\mathbb{B}^{n}, \mathbb{R}^n) and Δhu(x)=(1−∣x∣2)2Δu(x)+2(n−2)(1−∣x∣2)∑i=1nxi∂u∂xi(x) Δ_{h}u(x)= (1-|x|^2)^2Δu(x)+2(n-2)(1-|x|^2)\sum_{i=1}^{n} x_{i} \frac{\partial u}{\partial x_{i}}(x) is the hyperbolic Laplace operator in the nn-dimensional space Rn\mathbb{R}^n for n≥2n\ge 2. We show that if n≥3n\geq 3 and u∈C2(Bn,Rn)∩C(Bn‾,Rn)u\in C^{2}(\mathbb{B}^{n},\mathbb{R}^n) \cap C(\overline{\mathbb{B}^{n}},\mathbb{R}^n ) is a solution to the hyperbolic Poisson equation, then it has the representation u=Ph[ϕ]−Gh[ψ]u=P_{h}[ϕ]-G_{ h}[ψ] provided that u∣Sn−1=ϕu\mid_{\mathbb{S}^{n-1}}=ϕ and ∫Bn(1−∣x∣2)n−1∣ψ(x)∣ dτ(x)<∞\int_{\mathbb{B}^{n}}(1-|x|^{2})^{n-1} |ψ(x)|\,dτ(x)<\infty. Here PhP_{h} and GhG_{h} denote Poisson and Green integrals with respect to ΔhΔ_{h}, respectively. Furthermore, we prove that functions of the form u=Ph[ϕ]−Gh[ψ]u=P_{h}[ϕ]-G_{h}[ψ] are Lipschitz continuous.

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