Brownian behaviour of the Riemann zeta function around the critical line
Louis Vassaux
TL;DR
This work proves a functional Brownian limit for the logarithm of the Riemann zeta function along horizontal perturbations near the critical line: the process $Z^{(T)}(\alpha) = (1/\sqrt{\log \log T}) \log \zeta(1/2 + 1/(\log T)^{\alpha} + i\tau)$ on $[0,1]$ converges in law to a standard complex Brownian motion as $T\to\infty$. The proof combines finite-dimensional Gaussian convergence (via Dirichlet polynomial approximations and Bourgade-type lemmas) with a Kolmogorov-type tightness argument, where zeros of $\zeta$ are carefully controlled. Consequences include a Brownian reflection principle for the maximum of $\log|\zeta|$ on horizontal lines, an arcsine law for the horizontal distribution of large values, and a Brownian-type law of the iterated logarithm for horizontal drift, together with local-time and occupation-measure descriptions of $\log|\zeta|$. These results deepen the probabilistic understanding of zeta-values in the critical strip and reveal a Brownian structure underlying horizontal fluctuations, paralleling random matrix and stochastic-process models.
Abstract
We establish a Brownian extension to Selberg's central limit theorem for the Riemann zeta function. This implies various limiting distributions for $ζ$, including an analogue of the reflection principle for the maximum of the Brownian motion: as $T$ diverges, for any $u>0$ we have \[ \frac{1}{T}\cdot {\rm meas}\Big\{0\leq t\leq T:\max_{σ\geq \tfrac{1}{2}}\log|ζ(σ+i t)|\geq u \sqrt{\tfrac{1}{2}\log \log T} \Big\}\to 2 \displaystyle\int_u^{\infty} \frac{e^{-\frac{x^2}{2}}}{\sqrt{2π}}\mathrm{d} x. \]
