Statistical mechanics of Floquet quantum matter: exact and emergent conservation laws

Equilibrium statistical mechanics rests on the assumption of chaotic 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 loc...

Full description

Bibliographic Details
Main Authors: Das, A. (Author), Haldar, A. (Author)
Format: Article
Language:English
Published: NLM (Medline) 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02363nam a2200229Ia 4500
001 10.1088-1361-648X-ac03d2
008 220425s2022 CNT 000 0 und d
020 |a 1361648X (ISSN) 
245 1 0 |a Statistical mechanics of Floquet quantum matter: exact and emergent conservation laws 
260 0 |b NLM (Medline)  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1088/1361-648X/ac03d2 
520 3 |a Equilibrium statistical mechanics rests on the assumption of chaotic 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 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 of Floquet systems has a much richer structure due to the existence ofemergentconservation laws: these are approximate but stable conservation laws arisingdue to the drive, and are not present in the undriven system. Extensive numerical and analytical results support perpetual stability of these emergent (though approximate) conservation laws, probably even in the thermodynamic limit. This banks on the recent finding of a sharp threshold for Floquet thermalization in clean, interacting non-integrable Floquet systems. This indicates to the possibility of stable Floquet phases of matter in disorder-free systems. This review intends to give a self-contained theoretical overview of these developments for a broad physics audience. We conclude by briefly surveying the current experimental scenario. © 2022 IOP Publishing Ltd. 
650 0 4 |a dynamical freezing 
650 0 4 |a emergent conservation law 
650 0 4 |a Floquet ETH 
650 0 4 |a Floquet MBL 
650 0 4 |a Floquet physics 
650 0 4 |a Floquet scars 
650 0 4 |a periodically driven quantum systems 
700 1 |a Das, A.  |e author 
700 1 |a Haldar, A.  |e author 
773 |t Journal of physics. Condensed matter : an Institute of Physics journal