Antiferromagnetic Resonance and Terahertz Continuum in α-RuCl<sub>3</sub>

ORAL

Abstract

We report time-domain THz spectroscopy measurements of α-RuCl3 as a function of temperature and applied in-plane magnetic field, H, in the energy range 0.3 to 8.3 meV. Polarized measurements show that at zero field, 3-fold rotational symmetry is broken in the honeycomb plane from 2 K to 300 K. Below TN, and with B(t) parallel H, we observe an antiferromagnetic resonance (AFMR) peak at 2.56 meV atop a large broadband continuum which can attributed largely to electric dipole absorption. We track the evolution of the AMFR peak from H = 0 T to 7 T as it broadens and shifts to lower frequency. From spectral weight analysis of this peak, we place an upper bound on the contribution to the dc susceptibility from a magnetic excitation continuum. Ref. arxiv:1704.07357

*Terahertz spectroscopy was performed at Lawrence Berkeley National Laboratory in the Spin Physics program supported by the Director, Office of Science, Office of Basic Energy Sciences, Materials Sciences and Engineering Division, of the U.S. Department of Energy under Contract No. DE-AC02-76SF00515. This

Presenters

  • Arielle Little

    • Univ of California - Berkeley

Authors

  • Arielle Little

    • Univ of California - Berkeley
  • Liang Wu

    • Univ of California - Berkeley
  • Paula Lampen-Kelley

    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
  • Arnab Banerjee

    • Quantum Condensed Matter Division, Oak Ridge National Laboratory
    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
  • Shreyas Patankar

    • Physics, Univ of California - Berkeley
    • Univ of California - Berkeley
    • Physics, University of California, Berkeley
  • Dylan Rees

    • Univ of California - Berkeley
  • Craig Bridges

    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
  • Jiaqiang Yan

    • Materials Science and Technology Division, Oak Ridge National Laboratory
    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
    • Ames Laboratory, Iowa State University
  • David Mandrus

    • Department of Materials Science and Engineering, The University of Tennessee
    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
    • Department of Materials Science and Engineering, University of Tennessee
    • University of Tennessee
    • Materials Science and Technology, Oak Ridge National Laboratory
    • Materials Science and Engineering, The University of Tennessee
    • Materials Science and Engineering, University of Tennessee
    • Material Science and Technology Division, Oak Ridge National Laboratory
    • Oakridge National Laboratory
    • University of Tennessee, Knoxville
    • Univ of Tennessee, Knoxville
  • Stephen Nagler

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

    • Physics, Univ of California - Berkeley
    • Univ of California - Berkeley
    • Physics, University of California, Berkeley