Atomic loss and gain as a resource for non-equilibrium phase transitions in optical lattices

TL;DR

This paper explores how local incoherent atom loss and gain can drive non-equilibrium phase transitions in optical lattices, revealing complex dynamical behaviors and critical phenomena in Rydberg gases.

Contribution

It demonstrates that incoherent atom loss and gain can serve as sources of non-equilibrium phase transitions, expanding understanding of dynamical behaviors in Rydberg lattice systems.

Findings

Continuous and discontinuous phase transitions observed

Non-equilibrium transitions resemble stochastic processes with multiple absorbing states

Equilibrium transition of the 'model A' universality class identified

Abstract

Recent breakthroughs in the experimental manipulation of strongly interacting atomic Rydberg gases in lattice potentials have opened a new avenue for the study of many-body phenomena. Considerable efforts are currently being undertaken to achieve clean experimental settings that show a minimal amount of noise and disorder and are close to zero temperature. A complementary direction investigates the interplay between coherent and dissipative processes. Recent experiments have revealed a first glimpse into the emergence of a rich non-equilibrium behavior stemming from the competition of laser excitation, strong interactions and radiative decay of Rydberg atoms. The aim of the present theoretical work is to show that local incoherent loss and gain of atoms can in fact be the source of interesting out-of-equilibrium dynamics. This perspective opens new paths for the exploration of non-equilibrium critical phenomena and, more generally, phase transitions, some of which so far have been rather difficult to study. To demonstrate the richness of the encountered dynamical behavior we consider here three examples. The first two feature local atom loss and gain together with an incoherent excitation of Rydberg states. In this setting either a continuous or a discontinuous phase transition emerges with the former being reminiscent of genuine non-equilibrium transitions of stochastic processes with multiple absorbing states. The third example considers the regime of coherent laser excitation. Here the many-body dynamics is dominated by an equilibrium transition of the "model A" universality class.