Spectral convergence of the Dirac operator on typical hyperbolic surfaces of high genus
Laura Monk, Rares Stan
TL;DR
The paper proves that the Dirac spectrum of typical high-genus hyperbolic surfaces with a nontrivial spin structure converges, in a probabilistic sense, to the Dirac spectrum of the hyperbolic plane. It achieves this via a Dirac-adapted Selberg trace formula and a carefully crafted family of test functions $h_t$, yielding a precise density limit $\frac{1}{4\pi}\int_a^b \lambda\coth(\pi\lambda)\,d\lambda$ with explicit remainder $O((b+1)/\sqrt{\log g})$. A uniform Weyl law and multiplicity bounds follow, valid uniformly for typical surfaces under the Weil--Petersson measure, while pathological examples show the Dirac spectrum can misbehave on certain non-typical surfaces. The results illuminate how Benjamini--Schramm convergence to the plane governs Dirac spectral statistics, with implications for quantum chaos and spectral geometry on random hyperbolic surfaces.
Abstract
In this article, we study the Dirac spectrum of typical hyperbolic surfaces of finite area, equipped with a nontrivial spin structure (so that the Dirac spectrum is discrete). For random Weil-Petersson surfaces of large genus $g$ with $o(\sqrt{g})$ cusps, we prove convergence of the spectral density to the spectral density of the hyperbolic plane, with quantitative error estimates. This result implies upper bounds on spectral counting functions and multiplicities, as well as a uniform Weyl law, true for typical hyperbolic surfaces equipped with any nontrivial spin structure.
