Magnetic Excitations in $\alpha$-RuCl$_{3}$

ORAL

Abstract

The layered material $\alpha$-RuCl$_{3}$ is composed of stacks of weakly coupled honeycomb lattices of octahedrally coordinated Ru$^{3+}$ ions. The Ru ion ground state has 5 d electrons in the low spin state, with spin-orbit coupling very strong compared to other terms in the single ion Hamiltonian. The material is therefore an excellent candidate for investigating possible Heisenberg-Kitaev physics. In addition, this compound is very amenable to investigation by neutron scattering to explore the magnetic ground state and excitations in detail. Here we discuss new time-of-flight inelastic neutron scattering data on $\alpha$-RuCl$_{3}$. A high energy excitation near 200 meV is identified as a transition from the single ion J=1/2 ground state to the J=3/2 excited state, yielding a direct measurement of the spin orbit coupling energy. Higher resolution measurements reveal two collective modes at much lower energy scales. The results are compared with the theoretical expectations for excitations in the Heisenberg - Kitaev model on a honeycomb lattice, and show that Kitaev interactions are important.

Authors

  • Stephen Nagler

    Quantum Condensed Matter Division, ORNL, USA, QCMD, Oak Ridge National Laboratory

  • Arnab Banerjee

    QCMD, Oak Ridge National Laboratory

  • Craig Bridges

    Chemical Sciences Division, ORNL, USA, CSD, Oak Ridge National Laboratory

  • Jiaqiang Yan

    Material Sciences Division, ORNL, USA, MSTD, Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • David Mandrus

    Department of Physics, University of Tennessee, Knoxville, USA, Dep. of Mat. Sci. and Eng., U. Tennessee, Oak Ridge National Laboratory / Univ of Tennessee, Department of Materials Science \& Engineering, University of Tennessee, Knoxville

  • Matthew Stone

    Quantum Condensed Matter Division, ORNL, Oak Ridge National Laboratory, Quantum Condensed Matter Division, ORNL, USA, QCMD, Oak Ridge National Laboratory, Oak Ridge National Lab

  • Adam Aczel

    Quantum Condensed Matter Division, ORNL, Quantum Condensed Matter Division, ORNL, USA, QCMD, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Quantum Condensed Matter Division, Oak Ridge National Laboratory

  • Ling Li

    Dep. of Mat. Sci. and Eng., U.Tennessee

  • Yuen Yiu

    Department of Physics, University of Tennessee, Knoxville, USA, Dep. of Physics, U. Tennessee

  • Mark Lumsden

    Quantum Condensed Matter Division, ORNL, USA, QCMD, Oak Ridge National Laboratory, Oak Ridge National Lab

  • Johannes Knolle

    Max-Planck-Institut, Dresden

  • Roderich Moessner

    Max-Planck-Institut, Dresden, MPI-PKS Dresden, Max-Planck-Institut f\"ur Physik komplexer Systeme, Germany, MPIPKS, Max Planck Institute for the Physics of Complex Systems, Dresden, Germany

  • Alan Tennant

    Neutron Sciences Directorate, ORNL, USA, NScD, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Oak Ridge, TN, USA