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Three-dimensional quasiquantized Hall insulator phase in SrSi2

K. Manna1,2,*, N. Kumar2,3, S. Chattopadhyay4, J. Noky2, M. Yao2, J. Park4, T. Förster4, M. Uhlarz4, T. Chakraborty2 et al.

B. V. Schwarze4, J. Hornung4, V. N. Strocov5, H. Borrmann2, C. Shekhar2, Y. Sun2, J. Wosnitza4,6, C. Felser2, and J. Gooth2,6,†

  • 1Indian Institute of Technology-Delhi, Hauz Khas, New Delhi 110 016, India
  • 2Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Straße 40, 01187 Dresden, Germany
  • 3S. N. Bose National Centre for Basic Sciences, Salt Lake City, Kolkata 700 106, India
  • 4Hochfeld-Magnetlabor Dresden (HLD-EMFL) and Würzburg-Dresden Cluster of Excellence ct.qmat, Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • 5Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 6Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062 Dresden, Germany

  • *Kaustuv.Manna@physics.iitd.ac.in
  • †johannes.gooth@cpfs.mpg.de

Phys. Rev. B 106, L041113 – Published 18 July, 2022

DOI: https://doi.org/10.1103/PhysRevB.106.L041113

Abstract

In insulators, the longitudinal resistivity becomes infinitely large at zero temperature. For classical insulators, the Hall conductivity becomes zero at the same time. However, there are special systems, such as two-dimensional quantum Hall insulators, in which a more complex scenario is observed at high magnetic fields. Here, we report experimental evidence for a quasiquantized Hall insulator in the quantum limit of the three-dimensional compound SrSi2. Our measurements reveal a magnetic-field range, in which the longitudinal resistivity diverges with decreasing temperature, while the Hall conductivity approaches a quasiquantized value that is given only by the conductance quantum and the Fermi wave vector in the field direction. The quasiquantized Hall insulator appears in a magnetic field induced insulating ground state of three-dimensional materials and is deeply rooted in quantum Hall physics.

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