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For the complex ball $|z|^2\le 1$ in $\mathbb{C}^n$, there is a Poisson kernel proportional to $|x-z|^{-2n}$. This is generalized to the unitary group $U(N)$ so that in the complex matrix ball $Z^\dagger Z\le1$ we have the Poisson kernel proportional to $|\det(X-Z)|^{-2N}$, which can be written in terms of Schur polynomials using the Cauchy identity for $\sum_\lambda s_\lambda(X)s_\lambda(Z)$.

For the real ball $z^2<1$ in $\mathbb{R}^n$, there is also a Poisson kernel, but this is proportional to $|x-z|^{-n}$. Just from analogy, I would imagine that this could be generalized to the (special?) orthogonal group $O(N)$ so that in the real matrix ball $Z^TZ\le1$ we would have a Poisson kernel proportional to $|\det(X-Z)|^{-N}$, which in turn could be written in terms of orthogonal characters using some version of the Cauchy identity.

However, I cannot find anything about this, neither in the literature about symmetric functions and Cauchy identities, nor in literature about analysis on matrix spaces. Why?

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  • $\begingroup$ What exactly do you mean by a "Poisson kernel" for a compact group? $\endgroup$
    – R W
    Commented May 9 at 19:40
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    $\begingroup$ @RW Some $P(X,Z)\ge 0$ such that $\int P(X,Z) f(X)=f(Z)$, with integration over the group and $Z$ inside the ball. Along the lines of the book by Hua. $\endgroup$
    – thedude
    Commented May 9 at 19:46
  • $\begingroup$ How is "the ball" related to "the group" and which book do you refer to? $\endgroup$
    – R W
    Commented May 9 at 20:52
  • $\begingroup$ @RW the ball is defined by $Z^\dagger Z\le 1$ and the group is its boundary, $Z^\dagger Z=1$. The book is "Harmonic analysis of functions of several complex variables in the classical domains". $\endgroup$
    – thedude
    Commented May 9 at 20:55

1 Answer 1

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The Poisson kernel for the orthogonal group was calculated by Benjamin Béri in Generalization of the Poisson kernel to the superconducting random-matrix ensembles. This is in the context where $X$ is the scattering matrix of a superconductor in the Cartan symmetry class D (broken time-reversal and spin-rotation symmetries).

The result for $X\in{\rm SO}(N)$ (real unitary matrices with determinant $+1$) is $$P_{\rm SO}(X)\propto\frac{1}{|\operatorname{det}(X-Z)|^{N-1}},$$ to be contrasted with $$P_{\rm U}(X)\propto\frac{1}{|\operatorname{det}(X-Z)|^{2N}}$$ for $X\in{\rm U}(N)$.


Since the exponent $N-1$ differs from the expectation in the OP, let me check the reproducing property for ${\rm SO}(2)$ and $Z=zI_2$ (with $-1<z<1$). In that case the Poisson kernel is $$P_{\rm SO}(X)d\mu(X)=f(\theta)\,d\theta,\;\;f(\theta)=\frac{1-z^2}{2 \pi \left(z^2-2 z \cos \theta+1\right)}, $$ $$\text{in the parameterization}\;\;X(\theta)=\begin{pmatrix}\cos\theta&\sin\theta\\ -\sin\theta&\cos\theta\end{pmatrix}\;\;0<\theta<2\pi,$$ and one readily checks that $$\langle X^p\rangle\equiv\int_0^{2\pi} X^p(\theta)f(\theta)\,d\theta=z^p I_2=Z^p.$$ The reproducing property for the orthogonal Poisson kernel fails if $Z$ is not proportional to the unit matrix, for example, if $Z={{z\;0}\choose{0\,-z}}$ one has $\operatorname{det}(X-Z)=1-z^2$, independent of $X$ and $\langle X\rangle=0\neq Z$.


To generalize the Poisson kernel to all three classical groups ${\rm U}(N)$, ${\rm SO}(N)$, ${\rm Sp}(N)$, one defines an $N\times N$ subunitary matrix $Z$ as the submatrix of the $2N\times 2N$ unitary matrix $$\Omega=\begin{pmatrix}Z&T'\\ T&Z'\end{pmatrix}.$$ The $N\times N$ unitary matrix $X$ is then constructed by $$X=Z+T'X_0(1-Z'X_0)^{-1}T,$$ with $X_0$ an $N\times N$ unitary matrix distributed according to the Haar measure on the unitary, orthogonal, or symplectic group. The Poisson kernel is then defined as the corresponding probability distribution function $P(X)$ for a given $Z$. The result is $P(X)\propto|\operatorname{det}(X-Z)|^{-\beta N+\gamma}$, with $\beta=2,\gamma=0$ for ${\rm U}(N)$, $\beta=1,\gamma=1$ for ${\rm SO}(N)$, and $\beta=1,\gamma=-1$ for ${\rm Sp}(N)$. $$\mbox{}$$ The reproducing property, $\int P(X)f(X)d\mu(X)=f(Z)$, is ensured if the average of the matrix product $X_0(Z'X_0)^p$ vanishes for all $p=0,1,2\ldots$, which happens for any integer $N$ and any $Z$ in the unitary group, and for even $N$ and $Z\propto I_N$ in the orthogonal or symplectic groups.
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  • $\begingroup$ By $O_\pm(N)$ you mean I take either the +, i.e. $SO(N)$, or the $-$? $\endgroup$
    – thedude
    Commented May 13 at 20:41
  • $\begingroup$ Also, have you ever seen a discussion about expanding this kernel as an infinite series using irreducible characters? $\endgroup$
    – thedude
    Commented May 13 at 20:42
  • $\begingroup$ yes, the orthogonal group is disconnected, you average over either sector; I am unsure about the expansion you mention; one complication is that for the orthogonal group the reproducing property only holds for $Z$ proportional to the unit matrix. $\endgroup$ Commented May 13 at 20:46
  • $\begingroup$ I have restricted the answer to ${\rm SO}(N)={\rm O}_+(N)$; for ${\rm O}_-(N)$ the reproducing property fails even for the Haar measure, so for $Z=0$, since $\int_{{\rm O}_-}X^2 d\mu(X)\neq 0$, while $Z^2=0$. $\endgroup$ Commented May 14 at 6:14

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