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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).

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