4.8 Article

Theory for the Charge-Density-Wave Mechanism of 3D Quantum Hall Effect

Journal

PHYSICAL REVIEW LETTERS
Volume 125, Issue 20, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.125.206601

Keywords

-

Funding

  1. National Natural Science Foundation of China [11534001, 11974249, 11925402]
  2. Strategic Priority Research Program of Chinese Academy of Sciences [XDB28000000]
  3. Guangdong province [2016ZT06D348, 2017ZT0 7C062, 2020KCXTD001]
  4. National Key RD Program [2016YFA0301700]
  5. Natural Science Foundation of Shanghai [19ZR1437300]
  6. Shenzhen High-level Special Fund [G02206304, G02206404]
  7. Science, Technology and Innovation Commission of Shenzhen Municipality [ZDSYS20190 902092905285, ZDSYS20170303165926217, JCYJ20170412152620376, KYTDPT201810 11104202253]
  8. China Postdoctoral Science Foundation [2019M662150, 2020 T130635]
  9. SUSTech Presidential Postdoctoral Fellowship
  10. Center for Computational Science and Engineering of Southern University of Science and Technology

Ask authors/readers for more resources

The charge-density-wave (CDW) mechanism of the 3D quantum Hall effect has been observed recently in ZrTe5 [Tang et al., Nature 569, 537 (2019)]. Different from previous cases, the CDW forms on a one-dimensional (1D) band of Landau levels, which strongly depends on the magnetic field. However, its theory is still lacking. We develop a theory for the CDW mechanism of 3D quantum Hall effect. The theory can capture the main features in the experiments. We find a magnetic field induced second-order phase transition to the CDW phase. We find that electron-phonon interactions, rather than electron-electron interactions, dominate the order parameter. We extract the electron-phonon coupling constant from the non-Ohmic I - V relation. We point out a commensurate-incommensurate CDW crossover in the experiment. More importantly, our theory explores a rare case, in which a magnetic field can induce an order-parameter phase transition in one direction but a topological phase transition in other two directions, both depend on one magnetic field.

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