Khavinson's conjecture for hyperbolic harmonic functions on the unit ball

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Let n≥2n\geq 2 and let Bn{\mathbb B}^n and Sn−1{\mathbb S}^{n-1} denote the unit ball and unit sphere in Rn{\mathbb R}^n. For p∈(1,∞]p\in(1,\infty], let qq be its conjugate, let ϕ∈Lp(Sn−1,R)\phi\in L^p({\mathbb S}^{n-1},{\mathbb R}), and let u=Ph[ϕ]u=\mathcal{P}_h[\phi] be the invariant Poisson integral, where

Ph[ϕ](x)=∫Sn−1Ph(x,ζ)ϕ(ζ) dσ(ζ),\mathcal{P}_h[\phi](x)=\int_{{\mathbb S}^{n-1}}\mathcal{P}_h(x,\zeta)\phi(\zeta)\,d\sigma(\zeta),

and

Ph(x,ζ)=(1−∣x∣2∣x−ζ∣2)n−1.\mathcal{P}_h(x,\zeta)=\left(\frac{1-|x|^2}{|x-\zeta|^2}\right)^{n-1}.

For x∈Bn∖{0}x\in{\mathbb B}^n\setminus\{0\} and ℓ∈Sn−1\ell\in{\mathbb S}^{n-1}, let Cp(x)\mathcal{C}_p(x) and Cp(x;ℓ)\mathcal{C}_p(x;\ell) be the optimal constants in

∣∇u(x)∣≤Cp(x)∥ϕ∥p,|\nabla u(x)|\leq\mathcal{C}_p(x)\|\phi\|_p,

and

∣⟨∇u(x),ℓ⟩∣≤Cp(x;ℓ)∥ϕ∥p.|\langle\nabla u(x),\ell\rangle|\leq\mathcal{C}_p(x;\ell)\|\phi\|_p.

Khavinson's conjecture. Let p∈(1,∞]p\in(1,\infty], n≥3n\geq3, and x∈Bn∖{0}x\in{\mathbb B}^n\setminus\{0\}. Then

Cp(x)={Cp(x;nx),1<p<n,Cp(x;tx),p>n,\mathcal{C}_p(x)= \begin{cases} \mathcal{C}_p(x;n_x),&1<p<n,\\ \mathcal{C}_p(x;t_x),&p>n, \end{cases}

where nx=x∣x∣n_x=\frac{x}{|x|} and txt_x is any unit vector satisfying ⟨tx,x⟩=0\langle t_x,x\rangle=0. Moreover, if p=np=n or p=∞p=\infty, then Cp(x;ℓ)\mathcal{C}_p(x;\ell) does not depend on ℓ\ell.

This conjecture identifies the direction giving the sharp gradient estimate for hyperbolic harmonic Poisson integrals. The planar case n=2n=2 was solved by Kalaj and Marković, and the general conjecture is reported in the source as recently proved by Liu; consequently, the conjecture is solved.

References

Primary source

Adel Khalfallah, Fathi Haggui and Miodrag Mateljević, “Khavinson conjecture for hyperbolic harmonic functions on the unit ball”, arXiv:2103.00638 (2021).

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