Signature of spin-fermion coupling in the magnetic excitations of Dirac semimetal YbMnBi<sub>2.</sub>

ORAL

Abstract

In Dirac semimetals, coupling of Dirac charge carriers with magnetism can lead to novel phenomena with potential for technological applications [1, 2]. From this perspective, 112 ternary pnictogens (A,R)MnX2 (A=Ca,Sr;R=Yb,Eu;X=Bi,Sb) represent an interesting family of Dirac materials where both the magnetism and Dirac electrons coexist, thereby providing an opportunity to study the spin-fermion coupling between Mn spins and Dirac electrons in Bi layer [2]. Previous studies of spin excitations in (Sr,Ca)MnBi2 using inelastic neutron scattering (INS) have found no indication of such coupling because anomalous broadening found in itinerant magnets was absent [2]. However, our recent INS measurements of spin waves on YbMnBi2 found a small and q-independent broadening in the spin waves, which is consistent with a significant spin-Dirac fermion coupling. Theoretical calculations show that the effect of coupling on the spin excitations is suppressed by a vanishing carrier density of states at the Dirac point. [1] A. Sapkota et al, arxiv 1908.08114 (2019), [2] M. C. Rahn et al, Phys. Rev. B 95, 134405 (2017).

*Work at BNL was supported by Office of BES, U.S. DOE under Contract No. DE-SC0012704. Research conducted at ORNL’s SNS was sponsored by SUFD, Office of BES, U.S. DOE.

Presenters

  • Aashish Sapkota

    • Brookhaven national lab
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
    • Ames Laboratory, Ames, IA 50011, USA; Iowa State University, Ames, IA 50011, USA

Authors

  • Aashish Sapkota

    • Brookhaven national lab
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
    • Ames Laboratory, Ames, IA 50011, USA; Iowa State University, Ames, IA 50011, USA
  • Igor Zaliznyak

    • Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
  • John Tranquada

    • Brookhaven national lab
    • Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
  • Laura Classen

    • University of Minnesota
    • Brookhaven National Laboratory; University of Minnesota
  • Cedomir Petrovic

    • Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory
    • Brookhaven National Laboratory
    • Condensed Matter Physics and Materials Science, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
    • Brookhaven National Laboratory, NY 11973, USA
  • Aifeng Wang

    • Condensed Matter Physics and Materials Science, Brookhaven National Laboratory
    • Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory
  • Matthew Stone

    • Oak Ridge National Lab
    • Neutron Scattering Division, Oak Ridge National Laboratory
    • Quantum Condensed Matter Div, Oak Ridge National Lab
    • Oak Ridge National Laboratory
    • Spallation Neutron Source, Oak Ridge National Laboratory
    • Neutron Scattering Division, Oak Ridge National Lab
    • Neutron Scattering Division, OakRidge National Laboratory
  • Andrei T Savici

    • Oak Ridge National Laboratory
  • Vasile O Garlea

    • Oak Ridge National Laboratory
    • Quantum Condensed Matter Div, Oak Ridge National Lab
    • Oak Ridge National Lab
    • Oak Ridge National Lab, Neutron Scattering Division