Fingerprint of topology in high-temperature quantum oscillations, Part 2

ORAL

Abstract

A robust methodology to detect Dirac-Weyl fermions in topological semimetals by transport or thermodynamic measurements remains an open problem. It is often argued that a $\pi$ phase in quantum oscillations directly corresponds to the nontrivial Berry phase of topological semimetals. However, the oscillation phase is complicated by multiple contributing factors including the orbital magnetic moment, rendering such correspondences ambiguous for a substantial fraction of topological semimetals. Here, we propose to utilize the temperature dependence of the frequency, F(T), rather than the oscillation phase, as a hallmark signature of topology in quantum oscillations. At temperatures that are comparable to the cyclotron energy, F(T) encodes the energy-derivative of the cyclotron mass - a quantity that vanishes for conventional Schroedinger-type fermions, yet equals the inverse square of the Fermi velocity for Dirac-Weyl fermions. Cd$_3$As$_2$, Bi$_2$O$_2$Se and LaRhIn$_5$ serve as testing grounds confirming our methodology. Our approach requires no ab-initio calculation as input, and is able to identify topological Fermi pockets which are small compared to the Brillouin-zone volume - both attributes being ideally suited to identify topological heavy-fermion materials.

Presenters

  • Aris Alexandradinata

    • University of Illinois at Urbana-Champaign
    • Department of Physics and Institute for Condensed Matter Theory, University of Illinois at Urbana-Champaign

Authors

  • Chunyu Guo

    • Ecole Polytechnique Federale de Lausanne
    • Laboratory of Quantum Materials (QMAT), Institute of Materials (IMX), Ecole Polytechnique Federale de Lausanne (EPFL)
  • Aris Alexandradinata

    • University of Illinois at Urbana-Champaign
    • Department of Physics and Institute for Condensed Matter Theory, University of Illinois at Urbana-Champaign
  • Carsten Putzke

    • Ecole Polytechnique Federale de Lausanne
    • Laboratory of Quantum Materials (QMAT), Institute of Materials (IMX), Ecole Polytechnique Federale de Lausanne (EPFL)
  • Amelia K Estry

    • Ecole Polytechnique Federale de Lausanne
  • Feng-Ren Fan

    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
    • Max Planck Institute for Chemical Physics of Solids
  • Shengnan Zhang

    • Ecole Polytechnique Federale de Lausanne
    • Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL)
  • QuanSheng Wu

    • Ecole Polytechnique Fédérale de Lausanne (EPFL), Switzerland
    • Ecole Polytechnique Federale de Lausanne
    • Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL)
  • Oleg Yazyev

    • Ecole Polytechnique Federale de Lausanne (EPFL), Switzerland
    • Ecole Polytechnique Fédérale de Lausanne (EPFL), Switzerland
    • Ecole Polytechnique Federale de Lausanne
    • Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL)
    • École Polytechnique Fédérale de Lausanne (EPFL), Switzerland
  • Kent R Shirer

    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
    • Max Planck Institute for Chemical Physics of Solids
  • Maja Bachmann

    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
  • Eric D Bauer

    • Los Alamos National Laboratory
    • Los Alamos National Lab
    • Los Alamos National laboratory
    • Los Alamos Natl Lab
    • Condensed Matter and Magnet Science Group, Los Alamos National Laboratory
    • Los Alamos National LAborator
  • Filip Ronning

    • Los Alamos National Lab
    • Los Alamos National Laboratory
    • Los Alamos National laboratory
    • Condensed Matter and Magnet Science Group, Los Alamos National Laboratory
  • Chandra Shekhar

    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute for the Chemical Physics of Solids
    • Max Planck, Dresden
    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
  • Claudia Felser

    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute for the Chemical Physics of Solids
    • Solid State Chemistry, Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute, Dresden, Germany
    • Max Planck, Dresden
    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
    • Max Planck Institute for Chemical Physics of Solids,
  • Yan Sun

    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck, Dresden
    • Max Planck Institute for Chemical Physics of Solids, 01187 Dresden
  • Philip Moll

    • Ecole Polytechnique Federale de Lausanne
    • Laboratory of Quantum Materials (QMAT), Institute of Materials (IMX), Ecole Polytechnique Federale de Lausanne (EPFL)