X-ray resonant magnetic scattering study of multiferroic $R$MnO$_{3 }(R$~=~Dy, Ho, Er) compounds

ORAL

Abstract

Element specific x-ray resonant magnetic scattering (XRMS) investigations were undertaken to determine the magnetic structure of multiferroic hexagonal RMnO$_{3}$ compounds. In the intermediate temperature phase (ITP) (8-68~K for the Dy$^{3+}$ and 4.5-40~K for Ho$^{3+})$ the moments are aligned and antiferromagnetically correlated in the \textbf{c }direction according to the same magnetic representation $\Gamma _{3}$. Below the ITP, the Dy$^{3+}$/Ho$^{3+}$ moments order differently and according to the magnetic representations $\Gamma _{2 }$/$\Gamma _{1}$. The temperature dependence of the observed intensity in the ITP can be modeled assuming the splitting of ground-state doublet/quasi-doublet crystal-field levels of Dy$^{3+}$/Ho$^{3+ }$by the exchange field of Mn$^{3+}$. No resonant signals could be found for Er$^{3+}$ from 2-80~K. Specific magnetic representations can be excluded for the magnetic order of Er$^{3+}$ moments but can not be uniquely determined within the sensitivity of XRMS. -- The support by U.S. DOE (DE-AC02-07CH11358 and DE-AC02-06 CH11357) is acknowledged.

Authors

  • Alan Goldman

    • Ames Laboratory and Physics Department and Astronomy, Iowa State University, Ames, IA
    • Ames Laboratory and Iowa State University
    • Ames Laboratory, US DOE and Iowa State University
    • Ames Laboratory
    • Ames Loboratory, US DOE and Iowa State University
    • Ames Laboratory/Department of Physics and Astronomy
    • Ames Laboratory, US DOE, Iowa State University, Ames, IA 5001, USA
  • S. Nandi$^{1}$

  • A. Kreyssig$^{1}$

  • L. Tan$^{1}$

  • J.W. Kim$^{1}$

  • J.Q. Yan$^{1}$

  • M.D. Vannette$^{1}$

  • J.C. Lang$^{3}$

  • D. Haskel$^{3}$

  • T.A. Lograsso$^{2}$

  • R.J. McQueeney$^{1}$

    • $^{1}$ Dept. of Physics and Astronomy, Iowa State University, Ames; $^{2}$Ames Laboratory US DOE, Ames ;$^{3}$Advanced Photon Souce, Argonne