Origin of the Butterfly Magnetoresistance in a Dirac Nodal-line System

ORAL

Abstract

We report a study on the geometry of the Fermi surface (FS) of ZrSi(Se,Te) \emph{via} the de Haas-van Alphen effect (dHvA), whose electronic dispersion was reported to display a line of Dirac nodes within their Brillouin zone. For both compounds we find that their FSs agree well with Density Functional Theory (DFT) calculations. In contrast to ZrSiTe, DFT finds that the nodal Dirac line is close to the Fermi level in ZrSiSe which displays a very small residual resistivity and pronounced four-fold symmetric magnetoresistivity as a function of field orientation. The transport lifetime in ZrSiSe is found to be 10E2-10E3 times larger than its quasiparticle lifetime indicating that its charge carriers are protected against backscattering under zero-field, as previously reported for Cd3As2. The quasiparticle lifetime in ZrSiSe is found to be angle-dependent displaying a minimum for fields along the \emph{c}-axis. Therefore, the ``butterfly" magnetoresistivity observed in ZrSiSe, but not in ZrSiTe, seems to result from the magnetic field-induced suppression of this protection against backscattering, with this effect becoming particularly effective as the field is aligned along the inter-planar direction.

Presenters

  • Yu-Che Chiu

    Natl. High Magnetic Field Lab, Florida State University, Natl High Magnetic Field Lab, National High Magnetic Field Laboratory, Physics, Florida State University

Authors

  • Yu-Che Chiu

    Natl. High Magnetic Field Lab, Florida State University, Natl High Magnetic Field Lab, National High Magnetic Field Laboratory, Physics, Florida State University

  • Kuan-Wen Chen

    Physics, Florida State University, Natl High Magnetic Field Lab

  • Rico Schoenemann

    Natl. High Magnetic Field Lab, Florida State University, Natl High Magnetic Field Lab, National High Magnetic Field Laboratory

  • Qiong Zhou

    Natl. High Magnetic Field Lab, Florida State University, Natl High Magnetic Field Lab, Physics, Florida State University

  • David Graf

    NHMFL Tallahassee, NHMFL, National High Magnetic Field Lab, National High Magnetic Field Laboratory, National High Magnetic Field Laboratory/Florida State University, Natl High Magnetic Field Lab, NHMFL at Florida State University, Florida State University, National High Magnetic Field Laboratory, Florida State University, Condensed Matter Science, NHMFL

  • Erik Kampert

    Dresden High Magnetic Field Laboratory

  • Tobias Förster

    Dresden High Magnetic Field Laboratory, High Magnetic Field Laboratory

  • Gregory McCandless

    Department of Chemistry and Biochemistry, The University of Texas at Dallas, University of Texas at Dallas, Chemistry and Biochemistry, The University of Texas at Dallas

  • Julia Chan

    Department of Chemistry and Biochemistry, The University of Texas at Dallas, University of Texas at Dallas, Chemistry and Biochemistry, The University of Texas at Dallas

  • Ryan Baumbach

    National High Magnetic Field Laboratory, Florida State University, National High Magnetic Field Lab, Florida State University, National High Magnetic Field Laboratory, NHMFL, National High Magnetic Field Laboratory/Florida State University, Natl High Magnetic Field Lab, NHMFL at Florida State University

  • Michelle Johannes

    Naval Research Lab, Center for Computational Materials Science, Naval Research Lab, Naval Research Laboratory

  • Luis Balicas

    Natl High Magnetic Field Lab, Nat. High Magn. Field Lab., Florida State University, FSU-NHMFL, National High Magnetic Field Lab, National High Magnetic Field Laboratory, Natl. High Magnetic Field Lab, Florida State University, High Field Magnet Lab, 1800 E. Paul Dirac Drive, National High Magnetic Field Laboratory, Natl High Magnetic Field Lab