Aharonov-Bohm oscillations in disordered topological insulator nanowires

TL;DR

This paper investigates Aharonov-Bohm oscillations in disordered topological insulator nanowires, explaining experimental observations and how flux oscillation patterns depend on doping and disorder.

Contribution

It provides a theoretical framework for understanding flux oscillations in disordered topological insulator nanowires, reconciling experimental results with theory.

Findings

Flux oscillations depend on doping and disorder.

Explanation for observed h/e and h/2e oscillations.

Proposed experiments to verify the theory.

Abstract

A direct signature of electron transport at the metallic surface of a topological insulator is the Aharonov-Bohm oscillation observed in a recent study of Bi_2Se_3 nanowires [Peng et al., Nature Mater. 9, 225 (2010)] where conductance was found to oscillate as a function of magnetic flux $\phi$ through the wire, with a period of one flux quantum $\phi_0=h/e$ and maximum conductance at zero flux. This seemingly agrees neither with diffusive theory, which would predict a period of half a flux quantum, nor with ballistic theory, which in the simplest form predicts a period of $\phi_0$ but a minimum at zero flux due to a nontrivial Berry phase in topological insulators. We show how h/e and h/2e flux oscillations of the conductance depend on doping and disorder strength, provide a possible explanation for the experiments, and discuss further experiments that could verify the theory.