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Overlap distributions under the Gibbs measure of a Haar model of log⁡∣ζ∣\log|ζ| on and near the critical line

Frédéric Ouimet

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Source: arXiv

Published: Oct 10, 2026

arXiv: 2610.14901

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Source abstract

We study the Gibbs measure of H(h)=ℜ∑pj≤XUpj/(jpj(σ+ih))H(h) = \Re\sum_{p^{j} \leq X}U_{p}^{j}/(j p^{j(σ+ i h)}), a random field modeling large values of the log-modulus of the Riemann zeta function on and near the critical line, where the UpU_{p} are independent and uniformly distributed on the complex unit circle. Writing t=log⁡log⁡Tt = \log \log T, the cutoff XX and real part σσ may vary with TT subject to T1/tΦ≤X≤T1/tφT^{1/t^Φ} \leq X \leq T^{1/t^φ} and 0≤σ−1/2≤CσtΦ/log⁡T0 \leq σ- 1/2 \leq C_σt^Φ/\log T, for fixed Φ≥φ>1/2Φ\geq φ> 1/2 and Cσ>0C_σ > 0. On Iθ=[−(log⁡T)θ,(log⁡T)θ]I_θ = [ - (\log T)^θ,(\log T)^θ], define the Gibbs measure Gβ,σ,TH(dh):=eβH(h)dh/∫IθeβH(h′)dh′G_{β,σ,T}^{\mathrm{H}}(\mathrm{d}h) := e^{βH(h)}\mathrm{d}h/\int_{I_θ}e^{βH(h')}\mathrm{d}h'. For every fixed θ>−1θ> - 1 and inverse temperature β>0β> 0, the limiting joint distributions of correlations (overlaps) among points sampled from this measure are determined after averaging over the Haar phases. At and below βc(θ)=21+(θ∨0)β_{c}(θ) = 2\sqrt{1 + (θ\vee 0)}, the limiting two-overlap distribution is concentrated at q0=∣θ∧0∣q_{0} = |θ\wedge 0|. Above this threshold, it assigns masses βc(θ)/ββ_{c}(θ)/β and 1−βc(θ)/β1 - β_{c}(θ)/β to q0q_{0} and 11, respectively, and the limiting joint overlap distribution is described by a Poisson-Dirichlet process of parameter βc(θ)/ββ_{c}(θ)/β. Approximate Ghirlanda-Guerra identities are shown to hold uniformly for bounded deterministic functions of the sampled positions. This paper is the first in a series devoted to extending these results to log⁡∣ζ∣\log|ζ| near the critical line.

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