Statistical Mechanics of Floquet Quantum Matter: Exact and Emergent Conservation Laws
Asmi Haldar, Arnab Das

TL;DR
This paper reviews the development of statistical mechanics for Floquet quantum systems, highlighting the role of emergent conservation laws and their implications for stable Floquet engineering.
Contribution
It provides a comprehensive overview of the theoretical advances in understanding emergent conservation laws in periodically driven quantum systems.
Findings
Emergent conservation laws are stable and approximate, arising due to periodic drive.
Existence of a sharp ergodicity threshold for Floquet thermalization.
Potential for stable Floquet engineering in non-integrable systems.
Abstract
Equilibrium statistical mechanics rests on the assumption of ergodic dynamics of a system modulo the conservation laws of local observables: extremization of entropy immediately gives Gibbs' ensemble (GE) for energy conserving systems and a generalized version of it (GGE) when the number of local conserved quantities (LCQ) is more than one. Through the last decade, statistical mechanics has been extended to describe the late-time behaviour of periodically driven (Floquet) quantum matter starting from a generic state. The structure built on the fundamental assumptions of ergodicity and identification of the relevant "conservation laws" in this inherently non-equilibrium setting. More recently, it has been shown that the statistical mechanics has a much richer structure due to the existence of {\it emergent} conservation laws: these are approximate but stable conservation laws arising…
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