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Out-of-Time-Order Correlation for Many-Body Localization (1608.01914v3)

Published 5 Aug 2016 in cond-mat.quant-gas, cond-mat.dis-nn, cond-mat.stat-mech, and cond-mat.str-el

Abstract: In this paper we first compute the out-of-time-order correlators (OTOC) for both a phenomenological model and a random-field XXZ model in the many-body localized phase. We show that the OTOC decreases in power law in a many-body localized system at the scrambling time. We also find that the OTOC can also be used to distinguish a many-body localized phase from an Anderson localized phase, while a normal correlator cannot. Furthermore, we prove an exact theorem that relates the growth of the second R\'enyi entropy in the quench dynamics to the decay of the OTOC in equilibrium. This theorem works for a generic quantum system. We discuss various implications of this theorem.

Citations (266)

Summary

  • The paper presents a comprehensive analysis showing a distinctive power-law decay of OTOCs in many-body localized systems, contrasting with exponential decay in chaotic models.
  • The paper develops and validates a robust theorem linking OTOC decay with entanglement growth using both analytical and numerical models in disordered quantum systems.
  • The findings enable clear differentiation between many-body and Anderson localized phases, offering an effective diagnostic tool for experimental investigations.

Out-of-Time-Order Correlation for Many-Body Localization

The paper "Out-of-Time-Order Correlation for Many-Body Localization" presents an extensive investigation into the behavior of out-of-time-order correlators (OTOCs) within the context of many-body localization (MBL). The authors, Ruihua Fan, Pengfei Zhang, Huitao Shen, and Hui Zhai, meticulously explore how OTOCs serve as a diagnostic tool for identifying and characterizing localized phases in disordered quantum systems.

Key Contributions

The paper undertakes both analytical and numerical computation of OTOCs in a phenomenological model and a random-field XXZ model, both within the many-body localized phase. The central result indicates a distinctive power-law decay of OTOCs in MBL systems, contrasting with the exponential decay typical of chaotic systems. This discovery provides a novel perspective on using OTOCs to distinguish MBL phases, which do not adhere to the Eigenstate Thermalization Hypothesis due to the presence of numerous local integrals of motion.

The paper posits that OTOCs can differentiate between MBL and Anderson localized (AL) phases, an achievement that conventional correlators cannot replicate. In the MBL phase, a decrease in OTOCs is observed concurrent with the logarithmic growth of entanglement entropy following a quench, while in the AL phase, OTOCs remain constant.

Theoretical Implications

The authors propose a robust theorem linking the growth of second Rényi entropy in quench dynamics to the decay of OTOCs in equilibrium. This theorem is applicable to any quantum mechanical system, providing a theoretical framework to relate equilibrium properties with dynamical processes quantitatively. It fosters a deeper understanding of the interplay between entanglement growth and dynamical correlations in localized systems.

Methodological Insights

Two models serve as the basis for empirical validation. The phenomenological model, characterized by local two-state degrees of freedom, gives rise to a clear analytical expression for OTOC decay. Numerical evaluations on the random-field XXZ model further substantiate these findings, exhibiting behavior consistent with theoretical predictions. The paper highlights the utility of OTOC as a crucial observable for identifying localized behaviors in varied quantum models.

Numerical Results

The authors validate their theoretical insights with simulations, presenting strong numerical evidence that supports the theorem. The simulations include calculations of the von Neumann and second Rényi entropies alongside OTOC analyses, highlighting their concurrent behaviors uniquely in MBL as opposed to AL phases.

Practical and Theoretical Impact

This research not only advances the understanding of many-body dynamics in localized systems but also provides a computational framework that can be readily applied in experimental settings. The explicit connection between OTOCs and entanglement entropy opens new avenues for exploring nonequilibrium quantum dynamics using current cold atom setups, where MBL phenomena have been observed.

Future Directions

Future studies could extend these results by examining OTOC behaviors across various interaction regimes and in higher dimensional systems, potentially exploring the transition dynamics between MBL and chaotic phases. Further research may also delve into optimizing measurement techniques for OTOCs in quantum computational contexts to leverage their theoretical potential fully.

In sum, this paper delivers a comprehensive examination of OTOC characteristics in many-body localized systems, encouraging a nuanced approach to studying localization phenomena in quantum mechanics. The proposed connections between dynamical and equilibrium properties broaden the theoretical horizons and establish a platform for continuing exploration in quantum statistical physics.