English

Circular Jacobi Ensembles and deformed Verblunsky coefficients

Probability 2010-01-11 v3 Mathematical Physics math.MP

Abstract

Using the spectral theory of unitary operators and the theory of orthogonal polynomials on the unit circle, we propose a simple matrix model for the following circular analogue of the Jacobi ensemble: cδ,β(n)1k<lne\iiθke\iiθlβj=1n(1e\iiθj)δ(1e\iiθj)δc_{\delta,\beta}^{(n)} \prod_{1\leq k<l\leq n}| e^{\ii\theta_k}-e^{\ii\theta_l}|^\beta\prod_{j=1}^{n}(1-e^{-\ii\theta_j})^{\delta} (1-e^{\ii\theta_j})^{\overline{\delta}} with δ>1/2\Re \delta > -1/2. If ee is a cyclic vector for a unitary n×nn\times n matrix UU, the spectral measure of the pair (U,e)(U,e) is well parameterized by its Verblunsky coefficients (α0,...,αn1)(\alpha_0, ..., \alpha_{n-1}). We introduce here a deformation (γ0,>...,γn1)(\gamma_0, >..., \gamma_{n-1}) of these coefficients so that the associated Hessenberg matrix (called GGT) can be decomposed into a product r(γ0)...r(γn1)r(\gamma_0)... r(\gamma_{n-1}) of elementary reflections parameterized by these coefficients. If γ0,...,γn1\gamma_0, ..., \gamma_{n-1} are independent random variables with some remarkable distributions, then the eigenvalues of the GGT matrix follow the circular Jacobi distribution above. These deformed Verblunsky coefficients also allow to prove that, in the regime δ=δ(n)\delta = \delta(n) with δ(n)/n\dd\delta(n)/n \to \dd, the spectral measure and the empirical spectral distribution weakly converge to an explicit nontrivial probability measure supported by an arc of the unit circle. We also prove the large deviations for the empirical spectral distribution.

Keywords

Cite

@article{arxiv.0804.4512,
  title  = {Circular Jacobi Ensembles and deformed Verblunsky coefficients},
  author = {Paul Bourgade and Ashkan Nikeghbali and Alain Rouault},
  journal= {arXiv preprint arXiv:0804.4512},
  year   = {2010}
}

Comments

New section on large deviations for the empirical spectral distribution, Corrected value for the limiting free energy

R2 v1 2026-06-21T10:35:24.084Z