Homogeneous Floquet time crystal from weak ergodicity breaking

H. Yarloo, A. Emami Kopaei, and A. Langari
Phys. Rev. B 102, 224309 – Published 28 December 2020

Abstract

Recent works on the observation of discrete time-crystalline signatures throw up major puzzles on the necessity of localization for stabilizing such out-of-equilibrium phases. Motivated by these studies, we delve into a clean interacting Floquet system whose quasi-spectrum conforms to the ergodic Wigner-Dyson distribution, yet with an unexpectedly robust, long-lived time-crystalline dynamics in the absence of disorder or fine-tuning. We relate such behavior to a measure zero set of nonthermal Floquet eigenstates with long-range spatial correlations, which coexist with otherwise thermal states at near-infinite temperature and develop a high overlap with a family of translationally invariant, symmetry-broken initial conditions. This resembles the notion of “dynamical scars” that remain robustly localized throughout a thermalizing Floquet spectrum with fractured structure. We dub such a long-lived discrete time crystal formed in partially nonergodic systems, “scarred discrete time crystal” which is distinct by nature from those stabilized by either many-body localization or prethermalization mechanism.

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  • Received 24 July 2020
  • Revised 6 December 2020
  • Accepted 8 December 2020

DOI:https://doi.org/10.1103/PhysRevB.102.224309

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsStatistical Physics & ThermodynamicsAtomic, Molecular & OpticalQuantum Information, Science & Technology

Authors & Affiliations

H. Yarloo*, A. Emami Kopaei, and A. Langari

  • Department of Physics, Sharif University of Technology, P.O. Box 11155-9161, Tehran, Iran

  • *yarloohadi@gmail.com
  • langari@sharif.edu

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Issue

Vol. 102, Iss. 22 — 1 December 2020

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