Rare thermal bubbles at the many-body localization transition from the Fock space point of view

TL;DR

This paper investigates the many-body localization transition from the Fock space perspective, introducing new probes and models to understand the transition's nature and its relation to ergodicity and localization phenomena.

Contribution

It introduces the radial probability distribution of eigenstate coefficients and relates it to the properties of quasi-local integrals of motion, providing new insights into the MBL transition.

Findings

Demonstrates non-self-averaging of the many-body fractal dimension D_q.

Shows the transition is consistent with the avalanche mechanism and Kosterlitz-Thouless scenario.

Provides bounds on disorder scaling for Anderson localization transition.

Abstract

In this work we study the many-body localization (MBL) transition and relate it to the eigenstate structure in the Fock space. Besides the standard entanglement and multifractal probes, we introduce the radial probability distribution of eigenstate coefficients with respect to the Hamming distance in the Fock space from the wave function maximum and relate the cumulants of this distribution to the properties of the quasi-local integrals of motion in the MBL phase. We demonstrate non-self-averaging property of the many-body fractal dimension $D_q$ and directly relate it to the jump of $D_q$ as well as of the localization length of the integrals of motion at the MBL transition. We provide an example of the continuous many-body transition confirming the above relation via the self-averaging of $D_q$ in the whole range of parameters. Introducing a simple toy-model, which hosts ergodic thermal bubbles, we give analytical evidences both in standard probes and in terms of newly introduced radial probability distribution that the MBL transition in the Fock space is consistent with the avalanche mechanism for delocalization, i.e., the Kosterlitz-Thouless scenario. Thus, we show that the MBL transition can been seen as a transition between ergodic states to non-ergodic extended states and put the upper bound for the disorder scaling for the genuine Anderson localization transition with respect to the non-interacting case.