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Higher harmonics of quantum oscillations uncover Dirac Fermons in LaRhIn<sub>5</sub>

ORAL

Abstract

Quantum oscillations are commonly used to experimentally diagnose the band topology of a semimetal. When the cyclotron orbit encloses a topological defect, it is often presumed that the nontrivial Berry phase results in a π-phase shift of the fundamental harmonic. However, this presumption neglects how spin-orbit coupling renders the Berry phase a continuously varying quantity, and ignores the Zeeman interaction with the spin-orbit-induced magnetic moment. Here, we overcome these shortcomings and demonstrate how to rigorously identify three-dimensional Dirac fermions from the higher harmonics of quantum oscillations. Applying this method to the intermetallic LaRhIn5, we unambiguously identify the nontrivial Berry phase of a topological Fermi pocket with a small frequency ≈ 7T, despite the presence of large, trivial Fermi pockets which dominate transport by orders of magnitude. Our analysis identifies LaRhIn5 as a 3D Dirac-point metal, revising a previous proposal of LaRhIn5 as a nodal-line semimetal by Mikitik et. al. [Phys. Rev. Lett. 93, 106403 (2004)]. The electronic similarity of LaRhIn5 to the prototypical heavy-fermion superconductors Ce(Co,Rh,Ir)In5 further suggests them as prime candidates for strongly-correlated Dirac systems.

Presenters

  • Aris Alexandradinata

    University of Illinois at Urbana-Champaign, Department of Physics, University of Illinois at Urbana-Champaign

Authors

  • Aris Alexandradinata

    University of Illinois at Urbana-Champaign, Department of Physics, University of Illinois at Urbana-Champaign

  • Chunyu Guo

    Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne, Ecole Polytechnique Federale de Lausanne

  • Carsten Putzke

    Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne, Ecole Polytechnique Federale de Lausanne, École Polytechnique Fédéral de Lausanne, University of Bristol

  • Fengren Fan

    Max Planck Institute for Chemical Physics of Solids, Max-Planck Institute for Chemical Physics of Solids

  • Shengnan Zhang

    Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne

  • QuanSheng Wu

    EPFL Lausanne, Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne, Ecole Polytechnique Federale de Lausanne

  • Oleg V. Yazyev

    Ecole Polytechnique Federale de Lausanne, Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne

  • Kent Shirer

    Max Planck Institute for Chemical Physics of Solids

  • Maja Bachmann

    Max Planck Institute for Chemical Physics of Solids, Physics, Stanford University

  • Eric Bauer

    Los Alamos National Laboratory, Los Alamos Natl Lab, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory, Los Alamos National Laboratory, Los Alamos

  • Filip Ronning

    Los Alamos National Laboratory, Los Alamos Natl Lab, Condensed Matter and Magnet Science Group, Los Alamos National Laboratory

  • Claudia Felser

    Max Planck Institute for Chemical Physics of Solids, MPI-CPfS Dresden, Max Planck Institute For Chemical and Physical Solids, MPI for chemical physics of solids, Dresden, Solid State Chemistry, Max Planck Institute Chemical Physics of Solids, Max Planck Institute, Max-Planck-Institute for Chemical Physics of Solids , Nöthnitzer Straße-40, 01187 Dresden, Germany, Max Planck Inst, Max Planck Dresden, Chemical Physics of Solids, Max Planck Institute

  • Yan Sun

    Max Planck Institute for Chemical Physics of Solids, Max Planck Dresden

  • Philip Moll

    Institute of Material Science and Engineering, Ecole Polytechnique Federale de Lausanne, Ecole Polytechnique Federale de Lausanne, École Polytechnique Fédéral de Lausanne, Institute of Materials (IMX), EPFL, Ecole polytechnique federale de Lausanne