Fisher-Hartwig asymptotics for non-Hermitian random matrices
Paul Bourgade, Guillaume Dubach, Lisa Hartung, Ahmet Keles
TL;DR
This work develops a full 2d Fisher–Hartwig theory for determinants of non-Hermitian random matrices with singular potentials, establishing precise asymptotics that connect to Gaussian multiplicative chaos on the limiting droplet. The authors combine Ward identities with a surgical decoupling of local singularities and a Ginibre/Kostlan comparison to prove emergence of GMC measures and log-correlated electric fields, revealing universality with respect to the confining potential. They provide explicit moment formulas, CLTs for linear statistics, and a freezing transition in the subcritical GMC regime, demonstrating a deep link between 2d free fermions, random normal matrices, and Liouville quantum gravity. The results unify 2d FH-type asymptotics with GMC limits, improving understanding of thick points, extreme values, and phase transitions in non-Hermitian random matrix models. The methods pave the way for further exploration of Painlevé-type phenomena and universality across general confining potentials.
Abstract
We prove the two-dimensional analogue of the asymptotics for Toeplitz determinants with Fisher-Hartwig singularities, for general real symbols. This formula has applications to random normal matrices with complex spectra: (i) the characteristic polynomial converges to a Gaussian multiplicative chaos random measure on the limiting droplet, in the subcritical phase; (ii) the electric potential converges pointwise to a logarithmically correlated field; (iii) the measure of its level sets (i.e. thick points) is identified; (iv) the associated free energy undergoes a freezing transition. This establishes emergence of the Liouville quantum gravity measure from free fermions in 2d, and universality with respect to the external potential.
