A mean-field theory of nearly many-body localized metals
Sarang Gopalakrishnan, Rahul Nandkishore

TL;DR
This paper develops a mean-field theory for nearly many-body localized metals, explaining how slow dynamics and spectral properties evolve near the MBL transition, with results aligning with recent experiments.
Contribution
It introduces a self-consistent mean-field framework modeling the transition from metallic to localized phases using slow bath dynamics.
Findings
Spectral linewidth is proportional to DC conductivity.
Linewidth and conductivity vanish near the transition with calculable scaling.
The theory agrees with recent experimental observations.
Abstract
We develop a mean-field theory of the metallic phase near the many-body localization (MBL) transition, using the observation that a system near the MBL transition should become an increasingly slow heat bath for its constituent parts. As a first step, we consider the properties of a many-body localized system coupled to a generic ergodic bath whose characteristic dynamical timescales are much slower than those of the system. As we discuss, a wide range of experimentally relevant systems fall into this class; we argue that relaxation in these systems is dominated by collective many-particle rearrangements, and compute the associated timescales and spectral broadening. We then use the observation that the self-consistent environment of any region in a nearly localized metal can itself be modeled as a slowly fluctuating bath to outline a self-consistent mean-field description of the nearly…
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