Extended slow dynamical regime close to the many-body localization transition

By D. J. Luitz, N. Laflorencie, Fabien Alet. 2015

241 citations recorded by the source corpus.

Many-body localization is characterized by a slow logarithmic growth of the entanglement entropy after a global quantum quench while the local memory of an initial density imbalance remains at infinite time. We investigate how much the proximity of a many-body localized phase can influence the dynamics in the delocalized ergodic regime where thermalization is expected. Using an exact Krylov space technique, the out-of-equilibrium dynamics of the random-field Heisenberg chain is studied up to L=28 sites, starting from an initially unentangled high-energy product state. Within most of the delocalized phase, we find a sub-ballistic entanglement growth $S(t)\propto t^{1/z}$ with a disorder-dependent exponent $z\ge1$, in contrast with the pure ballistic growth $z=1$ of clean systems. At the same time, anomalous relaxation is also observed for the spin imbalance $I(t) \propto t^{-\zeta}$ with a continuously varying disorder-dependent exponent $\zeta$, vanishing at the transition. This provides a clear experimental signature for detecting this non-conventional regime.

Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/3b84a50a5bb92688ee9afa5fc6c273862ba18a93

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In Atomic and Molecular Physics, and Optics

  1. A. Nahum
  2. J. Ruhman
  3. S. Gopalakrishnan
  4. S. Vijay
  5. V. Khemani
  6. V. Ros
  7. Romain Vasseur
  8. D. Huse

In Condensed Matter Physics

  1. A. Nahum
  2. J. Ruhman
  3. S. Gopalakrishnan
  4. Romain Vasseur
  5. S. Vijay
  6. Antonello Scardicchio
  7. V. Ros
  8. I. Bloch

In Statistical and Nonlinear Physics

  1. J. Ruhman
  2. A. Nahum
  3. Romain Vasseur
  4. Antonello Scardicchio
  5. V. Ros
  6. S. Vijay
  7. I. Bloch
  8. J. Moore

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