Abstract

We consider the number NθA(θ){\cal N}_{θ_A}(θ) of eigenvalues eiθje^{i θ_j} of a random unitary matrix, drawn from CUEβ(N)_β(N), in the interval θj∈[θA,θ]θ_j \in [θ_A,θ]. The deviations from its mean, NθA(θ)−E(NθA(θ)){\cal N}_{θ_A}(θ) - \mathbb{E}({\cal N}_{θ_A}(θ)), form a random process as function of θθ. We study the maximum of this process, by exploiting the mapping onto the statistical mechanics of log-correlated random landscapes. By using an extended Fisher-Hartwig conjecture for Toeplitz determinants, supplemented with the freezing duality conjecture for log-correlated fields, we obtain the cumulants of the distribution of that maximum for any β>0β>0. It exhibits combined features of standard counting statistics of fermions (free for β=2β=2 and with Sutherland-type interaction for β≠2β\ne 2) in an interval and extremal statistics of the fractional Brownian motion with Hurst index H=0H=0. The β=2β=2 results are expected to apply to the statistics of zeroes of the Riemann Zeta function

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