Quantized Fermi-arc-mediated transport in Weyl semimetal nanowires

Abstract

We study longitudinal transport in Weyl semimetal nanowires, both in the absence and in the presence of a magnetic flux threading the nanowires. We identify two qualitatively different regimes of transport with respect to the chemical potential in the nanowires. In the "surface regime", for low doping, most of the conductance occurs through the Fermi-arc surface states, and it rises in steps of one quantum of conductance as a function of the chemical potential; furthermore, with varying flux the conductance changes in steps of one quantum of conductance with characteristic Fabry-Pérot interference oscillations. In the "bulk-surface regime", for highly-doped samples, the dominant contribution to the conductance is quadratic in the chemical potential, and mostly conditioned by the bulk states; the flux dependence shows clearly that both the surface and the bulk states contribute. The two aforementioned regimes prove that the contribution of the Fermi-arc surface states is salient and, therefore, crucial for understanding transport properties of finite-size Weyl semimetal systems. Last but not least, we demonstrate that both regimes are robust to disorder.

13 pages, 6 figures

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• Multi higher-order Dirac and nodal line semimetals
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• Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction in Weyl semimetals with tilted energy dispersion
• Conductance oscillation in surface junctions of Weyl semimetals
• Magnetotransport across Weyl semimetal grain boundaries
• Magneto tunnel conductance across twisted Weyl semimetal junctions
• Chiral Anomaly Trapped in Weyl Metals: Nonequilibrium Valley Polarization at Zero Magnetic Field
• Aharanov-Bohm oscillations and perfectly transmitted mode in amorphous topological insulator nanowires