Ergodicity breaking phase transitions

Physical systems are both universal and special, depending on the physical property under consideration and the corresponding scale, such as the energy, time, or length scale. From the perspective of quantum dynamics, it has been recently established that the ability of isolated quantum systems to thermalize after being driven away from equilibrium is related to the emergence of universal properties that comply with random matrix theory. Specific indicators for the onset of ergodicity and quantum chaos are related to the statistical properties of energy spectrum, Hamiltonian eigenfunction properties, and the expectation values of observables in these states. At the same time, however, these indicators also carry fingerprints of nonuniversal properties of a given system. Remarkable examples of the latter include, e.g., quantitative information about energy and charge transport, and the scaling of characteristic relaxation times. One of the main conjectures of this project is that these indicators, despite complying with the universal predictions of the random matrix theory, also carry information about proximity of phase transitions. Here we focus on ergodicity breaking phase transitions, which represent a novel type of phase transitions at the boundaries of quantum chaos. We then extend the scope of the project to the critical properties at the ergodicity breaking transitions. We conjecture that they also exhibit certain universal properties, yet likely different from those described by the conventional random matrix theory. The outcome of the project is to establish a phenomenological theory of ergodicity breaking transitions that applies to a broad class of quantum systems, and to clarify the impact of dimensionality, symmetries, the nature of interactions, and other mechanisms on universal properties of ergodicity breaking transitions.