Abstract

We study the finite-time dynamics of an initially localized wave-packet in the Anderson model on the random regular graph (RRG). Considering the full probability distribution Π(x,t)Π(x,t) of a particle to be at some distance xx from the initial state at time tt, we give evidence that Π(x,t)Π(x,t) spreads sub-diffusively over a range of disorder strengths, wider than a putative non-ergodic phase. We provide a detailed analysis of the propagation of Π(x,t)Π(x,t) in space-time (x,t)(x,t) domain, identifying four different regimes. These regimes in (x,t)(x,t) are determined by the position of a wave-front Xfront(t)X_{\text{front}}(t), which moves sub-diffusively to the most distant sites Xfront(t)∼tβX_{\text{front}}(t) \sim t^β with an exponent β<1β< 1. We support our numerical results by a self-consistent semiclassical picture of wavepacket propagation relating the exponent ββ with the relaxation rate of the return probability Π(0,t)∼e−ΓtβΠ(0,t) \sim e^{-Γt^β}. 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.

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