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arXiv:1908.11388 · Physical review. B./Physical review. B

Subdiffusion in the Anderson model on the random regular graph

Giuseppe De Tomasi, Soumya Bera, Antonello Scardicchio, Ivan M. Khaymovich

Published Mar 3, 2020• 71 citations
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Abstract

We study the finite-time dynamics of an initially localized wave packet in the Anderson model on the random regular graph (RRG) and show the presence of a subdiffusion phase coexisting both with ergodic and putative nonergodic phases. The full probability distribution $\mathrm{\ensuremath{\Pi}}(x,t)$ of a particle to be at some distance $x$ from the initial state at time $t$ is shown to spread subdiffusively over a range of disorder strengths. The comparison of this result with the dynamics of the Anderson model on ${\mathbb{Z}}^{d}$ lattices, $d>2$, which is subdiffusive only at the critical point implies that the limit $d\ensuremath{\rightarrow}\ensuremath{\infty}$ is highly singular in terms of the dynamics. A detailed analysis of the propagation of $\mathrm{\ensuremath{\Pi}}(x,t)$ in space-time $(x,t)$ domain identifies four different regimes determined by the position of a wave front ${X}_{\text{front}}(t)$, which moves subdiffusively to the most distant sites ${X}_{\text{front}}(t)\ensuremath{\sim}{t}^{\ensuremath{\beta}}$ with an exponent $\ensuremath{\beta}<1$. Importantly, the Anderson model on the RRG can be considered as proxy of the many-body localization transition (MBL) on the Fock space of a generic interacting system. In the final discussion, we outline possible implications of our findings for MBL.

DOI
10.1103/physrevb.101.100201

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We study the finite-time dynamics of an initially localized wave packet in the Anderson model on the random regular graph (RRG) and show the presence of a subdiffusion phase coexisting both with ergodic and putative nonergodic phases. The full probability distribution \ensuremathΠ(x,t)\mathrm{\ensuremath{\Pi}}(x,t)\ensuremathΠ(x,t) of a particle to be at some distance xxx from the initial state at time ttt is shown to spread subdiffusively over a range of disorder strengths. The comparison of this result with the dynamics of the Anderson model on Zd{\mathbb{Z}}^{d}Zd lattices, d>2d>2d>2, which is subdiffusive only at the critical point implies that the limit d\ensuremath→\ensuremath∞d\ensuremath{\rightarrow}\ensuremath{\infty}d\ensuremath→\ensuremath∞ is highly singular in terms of the dynamics. A detailed analysis of the propagation of \ensuremathΠ(x,t)\mathrm{\ensuremath{\Pi}}(x,t)\ensuremathΠ(x,t) in space-time (x,t)(x,t)(x,t) domain identifies four different regimes determined by the position of a wave front Xfront(t){X}_{\text{front}}(t)Xfront​(t), which moves subdiffusively to the most distant sites Xfront(t)\ensuremath∼t\ensuremathβ{X}_{\text{front}}(t)\ensuremath{\sim}{t}^{\ensuremath{\beta}}Xfront​(t)\ensuremath∼t\ensuremathβ with an exponent \ensuremathβ<1\ensuremath{\beta}<1\ensuremathβ<1. Importantly, the Anderson model on the RRG can be considered as proxy of the many-body localization transition (MBL) on the Fock space of a generic interacting system. In the final discussion, we outline possible implications of our findings for MBL.
A disordered quantum system can be driven, e.g., by increasing disorder, through the Anderson transition between a delocalized and localized phase. Recently, Anderson localization on treelike graphs has attracted much attention in view of its connections with problems of many-body localization. One of the central questions in this context is that of ergodicity of eigenstates. The authors of this paper perform a numerical study of Anderson transition on random regular graphs (RRGs) with diagonal disorder. The problem can be described as a tight-binding model on a lattice with NNN sites that is locally a tree with constant connectivity. Focusing on the delocalized side of the transition, they show that the data can be interpreted in terms of the finite-size crossover from a small ($N\ensuremath{\ll}{N}_{c}$) to a large ($N\ensuremath{\gg}{N}_{c}$) system, where Nc{N}_{c}Nc​ is the correlation volume diverging exponentially at the transition. A distinct feature of this crossover is a nonmonotonicity of the spectral and wave-function statistics, which is related to properties of the critical phase in the studied model and renders the finite-size analysis highly nontrivial. The results support an analytical prediction that states in the delocalized phase (and at $N\ensuremath{\gg}{N}_{c}$) are ergodic.
Anderson localization on random regular graphs (RRG) serves as a toy-model of many-body localization (MBL). We explore the transition from ergodicity to localization on RRG with large connectivity mmm. In the analytical part, we focus on the inverse participation ratio of eigenstates and identify several regimes on the ergodic side of the transition---self-consistent golden rule, golden rule, precritical, and critical---that the system consecutively goes through when the disorder increases toward the point Wc{W}_{c}Wc​ of the localization transition. We also perform exact-diagonalization numerics as well as a population-dynamics analysis combining analytical and numerical techniques. Results of all the approaches are in excellent mutual agreement. We further explore the evolution from ergodicity to localization in two models of Fock-space MBL: fermionic and spin quantum dots. Large-connectivity RRG models serve as an approximation for this class of many-body problems; one of our central goals is to better understand the status of this approximation. Our numerical simulations support the conjecture that, in the limit of a large system, there is a sharp ergodicity-to-localization transition in the quantum-dot models. Furthermore, our results are consistent with the RRG-like scaling of the critical disorder, ${W}_{c}\ensuremath{\sim}mlnm$. While in the golden-rule range the behavior of quantum-dot models is in agreement with analytical predictions based on the RRG model, substantial deviations occur in the precritical regime. Our results indicate that the precritical and critical behavior (as well as the numerical coefficient in the formula for Wc{W}_{c}Wc​) in the quantum-dot models may be different from what one would expect from the RRG-like approximation.
We present a renormalization group (RG) analysis of the problem of Anderson localization on a random regular graph (RRG) which generalizes the RG of Abrahams, Anderson, Licciardello, and Ramakrishnan to infinite-dimensional graphs. The RG equations necessarily involve two parameters (one being the changing connectivity of subtrees), but we show that the one-parameter scaling hypothesis is recovered for sufficiently large system sizes for both eigenstates and spectrum observables. We also explain the nonmonotonic behavior of dynamical and spectral quantities as a function of the system size for values of disorder close to the transition, by identifying two terms in the beta function of the running fractal dimension of different signs and functional dependence. Our theory provides a simple and coherent explanation for the unusual scaling behavior observed in numerical data of the Anderson model on RRG and of many-body localization.
Anderson localization on random regular graphs (RRG) attracts much attention as a toy model of many-body localization. Here, the critical behavior at the localization transition on RRG, related to that on infinite Bethe lattices, is studied numerically by means of a population dynamics approach. Proceeding up to correlation volumes as large as 1019{10}^{19}1019, the authors obtain the value of one half for the correlation-length critical exponent, in agreement with analytical predictions. They find very well pronounced corrections to scaling, similar to those in models with high spatial dimensionality and with many-body localization transitions.
We discuss the dependence of the critical properties of the Anderson model on the dimension d in the language of β -function and renormalization group recently introduced in Vanoni et al. [C. Vanoni et al. , Proc. Natl. Acad. Sci. U.S.A. 121 , e2401955121 (2024)] in the context of Anderson transition on random regular graphs. We show how in the delocalized region, including the transition point, the one-parameter scaling part of the β -function for the fractal dimension D 1 evolves smoothly from its d = 2 form, in which β 2 ≤ 0 , to its β ∞ ≥ 0 form, which is represented by the random regular graph (RRG) result. We show how the ϵ = d − 2 expansion and the 1 / d expansion around the RRG result can be reconciled and how the initial part of a renormalization group trajectory governed by the irrelevant exponent y depends on dimensionality. We also show how the irrelevant exponent emerges out of the high-gradient terms of expansion in the nonlinear sigma model and put forward a conjecture about a lower bound for the fractal dimension. The framework introduced here may serve as a basis for investigations of disordered many-body systems and of more general nonequilibrium quantum systems.