Abstract

We numerically investigate the distribution of Drude weights DD of many-body states in disordered one-dimensional interacting electron systems across the transition to a many-body localized phase. Drude weights are proportional to the spectral curvatures induced by magnetic fluxes in mesoscopic rings. They offer a method to relate the transition to the many-body localized phase to transport properties. In the delocalized regime, we find that the Drude weight distribution at a fixed disorder configuration agrees well with the random-matrix-theory prediction P(D)∝(γ2+D2)−3/2P(D) \propto (γ^2+D^2)^{-3/2}, although the distribution width γγ strongly fluctuates between disorder realizations. A crossover is observed towards a distribution with different large-DD asymptotics deep in the many-body localized phase, which however differs from the commonly expected Cauchy distribution. We show that the average distribution width ⟨γ⟩\langle γ\rangle , rescaled by LΔLΔ, ΔΔ being the average level spacing in the middle of the spectrum and LL the systems size, is an efficient probe of the many-body localization transition, as it increases/vanishes exponentially in the delocalized/localized phase.

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