Abstract

We consider the empirical eigenvalue distribution of an $m\times m$ principle submatrix of an $n\times n$ random unitary matrix distributed according to Haar measure. Earlier work of Petz and Réffy identified the limiting spectral measure if $\frac{m} {n}\to \alpha $, as $n\to \infty $; under suitable scaling, the family $\{\mu _{\alpha }\}_{\alpha \in (0,1)}$ of limiting measures interpolates between uniform measure on the unit disc (for small $\alpha $) and uniform measure on the unit circle (as $\alpha \to 1$). In this note, we prove an explicit concentration inequality which shows that for fixed $n$ and $m$, the bounded-Lipschitz distance between the empirical spectral measure and the corresponding $\mu _{\alpha }$ is typically of order $\sqrt{\frac {\log (m)}{m}} $ or smaller. The approach is via the theory of two-dimensional Coulomb gases and makes use of a new “Coulomb transport inequality” due to Chafaï, Hardy, and Maïda.

Highlights

  • Let U be an n × n Haar-distributed unitary matrix

  • We prove an explicit concentration inequality which shows that for fixed n and m, the bounded-Lipschitz distance between the empirical spectral measure and the corresponding μα is typically of order log(m) m or smaller

  • In the case that m = o( n), the truncated matrix is close to a matrix of independent, identically distributed Gaussian random variables; the circular law for the Ginibre ensemble would lead one to expect that the eigenvalue distribution was approximately uniform in a disc, and this was verified by Jiang in [5]

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Summary

Réffy identified the limiting spectral measure if m n

∞; under suitable scaling, the family {μα}α∈(0,1) of limiting measures interpolates between uniform measure on the unit disc (for small α) and uniform measure on the unit circle (as α → 1). We prove an explicit concentration inequality which shows that for fixed n and m, the bounded-Lipschitz distance between the empirical spectral measure and the corresponding μα is typically of order log(m) m or smaller. The approach is via the theory of two-dimensional Coulomb gases and makes use of a new “Coulomb transport inequality” due to Chafaï, Hardy, and Maïda

Introduction
On the eigenvalues of truncations of random unitary matrices
Let μm be the empirical spectral measure given by
Then with probability
Then for any
Coulomb gas model with potential
Given r
Now take
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