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Coulomb interactions and effective quantum inertia of charge carriers in a macroscopic conductor

A. Delgard1, B. Chenaud1, U. Gennser2, A. Cavanna2, D. Mailly2, P. Degiovanni3, and C. Chaubet1,*

  • 1Université Montpellier 2, CNRS, Laboratoire Charles Coulomb UMR5221, F-34095 Montpellier, France
  • 2Centre de Nanosciences et de Nanotechnologies (C2N), CNRS, Université Paris-Sud, Université Paris-Saclay, F-91120 Palaiseau, France
  • 3Université Lyon, Ens de Lyon, Université Claude Bernard Lyon 1, CNRS, Laboratoire de Physique, F-69342 Lyon, France

  • *Corresponding author: christophe.chaubet@umontpellier.fr

Phys. Rev. B 104, L121301 – Published 29 September, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L121301

Abstract

We study the low-frequency admittance of a quantum Hall bar of a size much larger than the electronic coherence length. We find that this macroscopic conductor behaves as an ideal quantum conductor with vanishing longitudinal resistance and purely inductive behavior up to f≲1MHz. Using several measurement configurations, we study the dependence of this inductance on the length of the edge channel and on the integer quantum Hall filling factor. The experimental data are well described by a scattering model for edge magnetoplasmons taking into account the effective long range Coulomb interactions within the sample. We find that the inductance's dependence on the filling factor arises predominantly from the effective quantum inertia of charge carriers induced by Coulomb interactions.

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