Onset of Floquet Thermalisation
Asmi Haldar, Roderich Moessner, Arnab Das

TL;DR
This paper investigates the onset of heating and non-ergodic behavior in an interacting Floquet system, revealing a threshold-driven transition to non-thermal states that are robust across various parameters and initial conditions.
Contribution
It demonstrates that Floquet heating only occurs above a certain drive amplitude threshold, with non-ergodic states exhibiting emergent conserved quantities and partial freezing.
Findings
Heating onset only below a drive amplitude threshold
Existence of non-ergodic states with finite entropy
Partial freezing of magnetization in initial states
Abstract
In presence of interactions, a closed, homogeneous (disorder-free) many-body system is believed to generically heat up to an `infinite temperature' ensemble when subjected to a periodic drive: in the spirit of the ergodicity hypothesis underpinning statistical mechanics, this happens as no energy or other conservation law prevents this. Here we present an interacting Ising chain driven by a field of time-dependent strength, where such heating onsets only below a threshold value of the drive amplitude, above which the system exhibits non-ergodic behaviour. The onset appears at {\it strong, but not fast} driving. This in particular puts it beyond the scope of high-frequency expansions. The onset location shifts, but it is robustly present, across wide variations of the model Hamiltonian such as driving frequency and protocol, as well as the initial state. The portion of nonergodic states…
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