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Fermi surface “hot” spots in topological chiral semimetal CoSi

ORAL

Abstract

Materials with multifold band degeneracy provide a unique opportunity to study massless fermions without elementary particle counterparts. Recently CoSi has been shown to host both six- and four-fold band degenerate points[1,2].
Here we present a fermiology study of CoSi based on angle-resolved Shubnikov–de Haas oscillation measurements. The focused ion beam technique is used to fabricate microstructures with large length to cross section ratios to increase signal[3]. Two clear oscillation frequencies are observed at all angles. Despite the isotropic Fermi surface evident by the angle-independent oscillation frequency, the oscillation amplitude shows a sharp minimum with field applied along [100] direction, unexpected for the isotropic Fermi surfaces of a cubic material. Ab initio calculations reveal an angle-dependent electron-phonon lifetime, demonstrates the possible origin of the angle-dependent oscillation amplitude. These results indicate the existence of Fermi surface “hot” spots and its possible relation to band topology needs to be further investigated.

[1] Z. Rao et al., Nature 567, 496 (2019).
[2] D. S. Sanchez et al., Nature 567, 500–505 (2019).
[3] P. J. W. Moll, Annu. Rev. Condens. Matter Phys. 9, 147 (2018).

Presenters

  • Chunyu Guo

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

Authors

  • Chunyu Guo

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

  • Dennis Nenno

    John A. Paulson School of Engineering and Applied Sciences, Harvard University

  • Christina Garcia

    John A. Paulson School of Engineering & Applied Science, Harvard University, Harvard University, John A. Paulson School of Engineering and Applied Sciences, Harvard University

  • Kaustuv Manna

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

  • Jonas Diaz

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

  • Carsten Putzke

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

  • Feng-Ren Fan

    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

  • 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,

  • Prineha Narang

    Harvard University, SEAS, Harvard University, John A. Paulson School of Engineering & Applied Science, Harvard University, Harvard John A. Paulson School of Engineering and Applied Sciences, Harvard University, Physics, Harvard University, John A. Paulson School of Engineering and Applied Sciences, Harvard University

  • Philip Moll

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