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arXiv:1402.0502 · Physical Review B

Dynamics of many-body localization

Yevgeny Bar Lev, David R. Reichman

Published Jun 23, 2014• 130 citations
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Abstract

Following the field theoretic approach of Basko et al. [Ann. Phys. 321, 1126 (2006)], we study in detail the real-time dynamics of a system expected to exhibit many-body localization. In particular, for time scales inaccessible to exact methods, we demonstrate that within the second-Born approximation the temporal decay of the density-density correlation function is consistent with a finite value for $t\ensuremath{\rightarrow}\ensuremath{\infty}$, as expected in a nonergodic state. This behavior persists over a wide range of disorder and interaction strengths and suggests that the nonergodic phase is surprisingly robust compared to the prediction of Basko et al. We argue that this discrepancy may be resolved by the presence of a nonergodic, but metallic, phase.

DOI
10.1103/physrevb.89.220201

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Following the field theoretic approach of Basko et al. [Ann. Phys. 321, 1126 (2006)], we study in detail the real-time dynamics of a system expected to exhibit many-body localization. In particular, for time scales inaccessible to exact methods, we demonstrate that within the second-Born approximation the temporal decay of the density-density correlation function is consistent with a finite value for t\ensuremath→\ensuremath∞t\ensuremath{\rightarrow}\ensuremath{\infty}t\ensuremath→\ensuremath∞, as expected in a nonergodic state. This behavior persists over a wide range of disorder and interaction strengths and suggests that the nonergodic phase is surprisingly robust compared to the prediction of Basko et al. We argue that this discrepancy may be resolved by the presence of a nonergodic, but metallic, phase.
We study the real-time dynamics of a two-dimensional Anderson-Hubbard model using nonequilibrium self-consistent perturbation theory within the second-Born approximation. When compared with exact diagonalization performed on small clusters, we demonstrate that for strong disorder this technique approaches the exact result on all available timescales, while for intermediate disorder, in the vicinity of the many-body localization transition, it produces quantitatively accurate results up to nontrivial times. Our method allows for the treatment of system sizes inaccessible by any numerically exact method and for the complete elimination of finite-size effects for the times considered. We show that for a sufficiently strong disorder the system becomes nonergodic, while for intermediate disorder strengths and for all accessible timescales transport in the system is strictly subdiffusive. We argue that these results are incompatible with a simple percolation picture, but are consistent with the heuristic random resistor network model where subdiffusion may be observed for long times until a crossover to diffusion occurs. The prediction of slow finite-time dynamics in a two-dimensional interacting and disordered system can be directly verified in future cold-atoms experiments.
An analytical theory, based on the perturbative treatment of the disorder and extended into a self-consistent set of equations for the dynamical density correlations, is developed and applied to the prototype one-dimensional model of many-body localization. Results show a qualitative agreement with numerically obtained dynamical structure factor in the whole range of frequencies and wavevectors, as well as across the transition to the nonergodic behavior. The theory reveals the singular nature of the one-dimensional problem, whereby on the ergodic side the dynamics is subdiffusive with a dynamical exponent varying with the disorder.
An analytical theory, based on the perturbative treatment of the disorder and extended into a self-consistent set of equations for the dynamical density correlations, is developed and applied to the prototype one-dimensional model of many-body localization. Results show a qualitative agreement with the numerically obtained dynamical structure factor in the whole range of frequencies and wave vectors, as well as across the transition to nonergodic behavior. The theory reveals the singular nature of the one-dimensional problem, whereby on the ergodic side the dynamics is subdiffusive with dynamical conductivity $\ensuremath{\sigma}(\ensuremath{\omega})\ensuremath{\propto}{|\ensuremath{\omega}|}^{\ensuremath{\alpha}}$, i.e., with vanishing dc limit ${\ensuremath{\sigma}}_{0}=0$ and $\ensuremath{\alpha}<1$ varying with disorder, while we get $\ensuremath{\alpha}>1$ in the localized phase.
What happens in an isolated quantum system when both disorder and interactions are present? Over the recent years, the picture of a non-thermalizing phase of matter, the many-localized phase, has emerged as a stable solution. We present a basic introduction to the topic of many-body localization, using the simple example of a quantum spin chain that allows us to illustrate several of the properties of this phase. We then briefly review the current experimental research efforts probing this physics. The largest part of this review is a selection of more specialized questions, some of which are currently under active investigation. We conclude by summarizing the connections between many-body localization and quantum simulations.
We study the infinite temperature dynamics of a prototypical one-dimensional system expected to exhibit many-body localization. Using numerically exact methods, we establish the dynamical phase diagram of this system based on the statistics of its eigenvalues and its dynamical behavior. We show that the nonergodic phase is reentrant as a function of the interaction strength, illustrating that localization can be reinforced by sufficiently strong interactions even at infinite temperature. Surprisingly, within the accessible time range, the ergodic phase shows subdiffusive behavior, suggesting that the diffusion coefficient vanishes throughout much of the phase diagram in the thermodynamic limit. Our findings strongly suggest that Wigner-Dyson statistics of eigenvalue spacings may appear in a class of ergodic but subdiffusive systems.