Poisson transform and unipotent complex geometry

TL;DR

This paper characterizes the Poisson transform on non-compact Riemannian symmetric spaces using complex analysis, holomorphic extensions, and weighted Bergman spaces, providing a new functional-analytic description of eigenfunctions.

Contribution

It introduces a novel characterization of the Poisson transform's image in terms of weighted Bergman spaces and complex analysis, focusing on unipotent group actions and boundary behavior.

Findings

Eigenfunctions extend holomorphically to tube domains

Characterization of Poisson transform image via weighted Bergman spaces

A supremum norm condition involving boundary parameters

Abstract

Our concern is with Riemannian symmetric spaces $Z=G/K$ of the non-compact type and more precisely with the Poisson transform $\mathcal{P}_\lambda$ which maps generalized functions on the boundary $\partial Z$ to $\lambda$-eigenfunctions on $Z$. Special emphasis is given to a maximal unipotent group $N<G$ which naturally acts on both $Z$ and $\partial Z$. The $N$-orbits on $Z$ are parametrized by a torus $A=(\mathbb{R}_{>0})^r<G$ (Iwasawa) and letting the level $a\in A$ tend to $0$ on a ray we retrieve $N$ via $\lim_{a\to 0} Na$ as an open dense orbit in $\partial Z$ (Bruhat). For positive parameters $\lambda$ the Poisson transform $\mathcal{P}_\lambda$ is defined an injective for functions $f\in L^2(N)$ and we give a novel characterization of $\mathcal{P}_\lambda(L^2(N))$ in terms of complex analysis. For that we view eigenfunctions $\phi = \mathcal{P}_\lambda(f)$ as families $(\phi_a)_{a\in A}$ of functions on the $N$-orbits, i.e. $\phi_a(n)= \phi(na)$ for $n\in N$. The general theory then tells us that there is a tube domain $\mathcal{T}=N\exp(i\Lambda)\subset N_\mathbb{C}$ such that each $\phi_a$ extends to a holomorphic function on the scaled tube $\mathcal{T}_a=N\exp(i\operatorname{Ad}(a)\Lambda)$. We define a class of $N$-invariant weight functions ${\bf w}_\lambda$ on the tube $\mathcal{T}$, rescale them for every $a\in A$ to a weight ${\bf w}_{\lambda, a}$ on $\mathcal{T}_a$, and show that each $\phi_a$ lies in the $L^2$-weighted Bergman space $\mathcal{B}(\mathcal{T}_a, {\bf w}_{\lambda, a}):=\mathcal{O}(\mathcal{T}_a)\cap L^2(\mathcal{T}_a, {\bf w}_{\lambda, a})$. The main result of the article then describes $\mathcal{P}_\lambda(L^2(N))$ as those eigenfunctions $\phi$ for which $\phi_a\in \mathcal{B}(\mathcal{T}_a, {\bf w}_{\lambda, a})$ and $$\|\phi\|:=\sup_{a\in A} a^{\operatorname{Re}\lambda -2\rho} \|\phi_a\|_{\mathcal{B}_{a,\lambda}}<\infty$$ holds.