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Competing Exchange Interactions and Multiferroic Behavior of a Molecule-Based Magnet

Invited

Abstract

Multiferroic behavior sensitively depends on the microscopic interactions between spins. The molecule-based magnet (NH4)2FeCl5 (H2O) exhibits a complex magnetic-field or pressure versus temperature phase diagram with three multiferroic phases observed by magnetization, neutron diffraction, and Raman spectroscopy measurements. Both low-field phases contain spin cycloids with electric polarization P along the a axis produced by the inverse Dzyalloshinskii-Moriya interaction. Above the spin-reorientation transition at roughly 4 T, the spins form a canted antiferromagnetic state and P rotates to the c axis. The electric polarization at high fields is believed to be caused by p-d orbital hybridization. We evaluate the magnetic interactions in the low-field multiferroic phase by comparing inelastic neutron scattering spectra of a single crystal with a simple Heisenberg model containing five exchange interactions mediated by intermolecular hydrogen and halogen bonds. Two competing exchange interactions in every bc plane produce a cycloid with spins in the ac plane, helicity Si x Sj along the b axis, and ordering wavevector Q = (0, 0, 0.23) r.l.u. along the c axis. Using this wavevector as a constraint, we obtain excellent agreement between the observed and predicted inelastic spectra at zero field. With some small but clear differences, the zero-field exchange and anisotropy parameters also provide excellent agreement with the inelastic neutron-scattering spectra of the high-field phase. The resulting exchange and anisotropy parameters are compared with the predictions of first-principle calculations.

Presenters

  • Randy Fishman

    Oak Ridge National Lab, Oak Ridge National Laboratory

Authors

  • Randy Fishman

    Oak Ridge National Lab, Oak Ridge National Laboratory

  • Xiaojian Bai

    Oak Ridge National Lab

  • Vasile Garlea

    Oak Ridge National Laboratory, Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN, Oak Ridge National Lab, Neutron Scattering Division, Oak Ridge National Laboratory

  • Tao Hong

    Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge National Laboratory, Oak Ridge National Lab

  • Jaime Fernandez-Baca

    Oak Ridge National Lab, Oak Ridge National Laboratory

  • Huibo Cao

    Oak Ridge National Lab, Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA, Neutron Scattering, Oak Ridge National Laboratory, Oak Ridge National Laboratory

  • Wei Tian

    Oak Ridge National Laboratory, Oak Ridge, Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA, Oak Ridge National Lab

  • Minseong Lee

    National High Magnetic Field Laboratory, Pulsed Field Facility, Los Alamos National Lab, National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos National Lab, Los Alamos National Laboratory

  • Vivien Zapf

    Los Alamos Natl Lab, National High Magnetic Field Lab, Los Alamos National Lab, Pulsed Field Facility, Los Alamos National Lab, Los Alamos National Lab, Los Alamos National Laboratory

  • Junhee Lee

    Ulsan National Institute of Science and Technology

  • Amanda J Clune

    University of Tennessee

  • Kendall D Hughey

    Department of Chemistry, University of Tennessee, University of Tennessee

  • Janice Musfeldt

    University of Tennessee, Department of Physics and Astronomy, Rutgers University, Department of Chemistry, University of Tennessee