Abstract

The real-time dynamics of equal-site correlation functions is studied for one-dimensional spin models with quenched disorder. Focusing on infinite temperature, we present a comparison between the dynamics of models with different quantum numbers $S = 1/2, 1, 3/2$, as well as of chains consisting of classical spins. Based on this comparison as well as by analyzing the statistics of energy-level spacings, we show that the putative many-body localization transition is shifted to considerably stronger values of disorder for increasing $S$. In this context, we introduce an effective disorder strength $W_\text{eff}$, which provides a mapping between the dynamics for different spin quantum numbers. For small $W_\text{eff}$, we show that the real-time correlations become essentially independent of $S$, and are moreover very well captured by the dynamics of classical spins. Especially for $S = 3/2$, the agreement between quantum and classical dynamics is remarkably observed even for very strong values of disorder. This behavior also reflects itself in the corresponding spectral functions, which are obtained via a Fourier transform from the time to the frequency domain. As an aside, we also comment on the self-averaging properties of the correlation function at weak and strong disorder. Our work sheds light on the correspondence between quantum and classical dynamics at high temperatures and extends our understanding of the dynamics in disordered spin chains beyond the well-studied case of $S=1/2$.

Highlights

  • Noninteracting particles in one and two spatial dimensions are localized even for arbitrarily small values of disorder [1,2]

  • As well as of chains consisting of classical spins. Based on this comparison as well as by analyzing the statistics of energy-level spacings, we show that the putative many-body localization transition is shifted to considerably stronger values of disorder for increasing S

  • We introduce an effective disorder strength Weff, which provides a mapping between the dynamics for different spin quantum numbers

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Summary

INTRODUCTION

Noninteracting particles in one and two spatial dimensions are localized even for arbitrarily small values of disorder [1,2]. We shed light onto this question by comparing the infinite-temperature dynamics of equal-site correlation functions for disordered classical and quantum spin chains with this comparison as well as by analyzing the statistics of energy-level spacings, we show that the putative many-body localization transition is shifted to considerably stronger values of disorder for increasing S. The occurrence of genuine MBL, is not expected for classical spin models This can be understood for instance from a rare-region argument, where small parts of the chain are only weakly disordered and exhibit chaotic dynamics, which eventually causes thermalization of the full system at sufficiently long timescales [27]. Not least due to the higher computational requirements, much less is known about the dynamics and the putative MBL transition for the Hamiltonian (1) between these two limiting cases, i.e., for

Equal-site correlation function
Quantum dynamics
Classical dynamics
Averaging
RESULTS
Clean model
Level-spacing distribution
Dynamics
Intermediate conclusion
Finite-size analysis and self-averaging
DISCUSSION
Full Text
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