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The fate of dynamical many-body localization in the presence of disorder

Dynamical localization is one of the most startling manifestations of quantum interference, where the evolution of a simple system is frozen out under a suitably tuned coherent periodic drive. Here, we show that, although any randomness in the interactions of a many body system kills dynamical localization eventually, spectacular remnants survive even when the disorder is strong. We consider a disordered quantum Ising chain where the transverse magnetization relaxes exponentially with time with a decay time-scale $τ$ due to random longitudinal interactions between the spins. We show that, under external periodic drive, this relaxation slows down ($τ$ shoots up) by orders of magnitude as the ratio of the drive frequency $ω$ and amplitude $h_{0}$ tends to certain specific values (the freezing condition). If $ω$ is increased while maintaining the ratio $h_0/ω$ at a fixed freezing value, then $τ$ diverges exponentially with $ω.$ The results can be easily extended for a larger family of disordered fermionic and bosonic systems.

preprint2015arXivOpen access

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