Conductance noise in interacting Anderson insulators driven far from equilibrium

TL;DR

This study reveals a unique conductance noise characterized by downward spikes in strongly disordered, interacting Anderson insulators driven far from equilibrium, dependent on hopping transport and the liquid helium bath conditions.

Contribution

It introduces the observation of conductance spikes in Anderson insulators under high current, explaining their dependence on hopping transport and liquid helium interaction.

Findings

Conductance spikes occur only in hopping transport regime.

Spikes are controlled by sample parameters and current density.

The phenomenon depends on contact with the normal phase of liquid helium.

Abstract

The combination of strong disorder and many-body interactions in Anderson insulators lead to a variety of intriguing non-equilibrium transport phenomena. These include slow relaxation and a variety of memory effects characteristic of glasses. Here we show that when such systems are driven with sufficiently high current, and in liquid helium bath, a peculiar type of conductance noise can be observed. This noise appears in the conductance versus time traces as downward-going spikes. The characteristic features of the spikes (such as typical width) and the threshold current at which they appear are controlled by the sample parameters. We show that this phenomenon is peculiar to hopping transport and does not exist in the diffusive regime. Observation of conductance spikes hinges also on the sample being in direct contact with the normal phase of liquid helium; when this is not the case, the noise exhibits the usual 1/f characteristics independent of the current drive. A model based on the percolative nature of hopping conductance explains why the onset of the effect is controlled by current density. It also predicts the dependence on disorder as confirmed by our experiments. To account for the role of the bath, the hopping transport model is augmented by a heuristic assumption involving nucleation of cavities in the liquid helium in which the sample is immersed. The suggested scenario is analogous to the way high-energy particles are detected in a Glaser's bubble chamber.