Discovery of a non-Hermitian phase transition in a bulk condensed-matter system

TL;DR

This paper reports the first experimental observation of a non-Hermitian phase transition in a bulk condensed-matter system, revealing a new type of phase change driven by dynamical properties rather than static order.

Contribution

It demonstrates a non-Hermitian phase transition in a ferromagnetic semiconductor through time-resolved optical measurements, linking non-Hermitian physics to bulk condensed-matter systems.

Findings

Observation of a transition from bi-exponential to single-exponential decay.

Theoretical modeling confirms the non-Hermitian phase transition.

Potential for controlling bulk properties via non-Hermitian dynamics.

Abstract

Phase transitions are fundamental in nature. A small parameter change near a critical point leads to a qualitative change in system properties. Across a regular phase transition, the system remains in thermal equilibrium and, therefore, experiences a change of static properties, like the emergence of a magnetisation upon cooling a ferromagnet below the Curie temperature. When driving a system far from equilibrium, novel, otherwise inaccessible quantum states of matter may arise. Such states are typically non-Hermitian, that is, their dynamics break time-reversal symmetry, a basic law of equilibrium physics. Phase transitions in non-Hermitian systems are of fundamentally new nature in that the dynamical behaviour rather than static properties may undergo a qualitative change at a critical, here called exceptional point. Here we experimentally realize a non-Hermitian phase transition in a bulk condensed-matter system. Optical excitation creates charge carriers in the ferromagnetic semiconductor EuO. In a temperature-dependent interplay with the Hermitian transition to ferromagnetic order, a non-Hermitian change of the relaxation dynamics occurs, manifesting in our time-resolved reflection data as a transition from bi-exponential real to single-exponential complex decay. Our theory models this behavior and predicts non-Hermitian phase transitions for a large class of condensed-matter systems, where they may be exploited to sensitively control bulk-dynamic properties.