Your browser doesn't support javascript.
loading
Spin reorientation in antiferromagnetic Dy2FeCoO6 double perovskite.
Haripriya, G R; Heitmann, T W; Yadav, D K; Kaphle, G C; Ghimire, Madhav Prasad; Pradheesh, R; Joshi, J; Vora, P; Sethupathi, K; Sankaranarayanan, V; Nair, H S.
  • Haripriya GR; Low Temperature Physics Laboratory, Department of Physics, Indian Institute of Technology Madras, Chennai-600036, India.
  • Heitmann TW; University of Missouri Research Reactor, University of Missouri, Columbia, MO 65211, United States of America.
  • Yadav DK; Central Department of Physics, Tribhuvan University, Kirtipur, 44613 Kathmandu, Nepal.
  • Kaphle GC; Central Department of Physics, Tribhuvan University, Kirtipur, 44613 Kathmandu, Nepal.
  • Ghimire MP; Condensed Matter Physics Research Center (CMPRC), Butwal-11, Rupandehi, Lumbini, Nepal.
  • Pradheesh R; Central Department of Physics, Tribhuvan University, Kirtipur, 44613 Kathmandu, Nepal.
  • Joshi J; Condensed Matter Physics Research Center (CMPRC), Butwal-11, Rupandehi, Lumbini, Nepal.
  • Vora P; IFW Dresden, Helmholtzstr. 20, D-01069, Dresden, Germany.
  • Sethupathi K; Low Temperature Physics Laboratory, Department of Physics, Indian Institute of Technology Madras, Chennai-600036, India.
  • Sankaranarayanan V; Racah Institute of Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel.
  • Nair HS; Department of Physics and Astronomy, George Mason University, Fairfax, VA 22030, United States of America.
J Phys Condens Matter ; 33(2): 025802, 2021 Jan 13.
Article en En | MEDLINE | ID: mdl-33055379
ABSTRACT
We explored the electronic and magnetic properties of the lanthanide double perovskite Dy2FeCoO6 by combining magnetization, Raman and Mössbauer spectroscopy and neutron diffraction along with density functional theory (DFT) calculations. Our magnetization measurements revealed two magnetic phase transitions in Dy2FeCoO6. First, a paramagnetic to antiferromagnetic transition at T N = 248 K and subsequently, a spin reorientation transition at T SR = 86 K. In addition, a field-induced magnetic phase transition with a critical field of H c ≈ 20 kOe is seen at 2 K. Neutron diffraction data suggested cation-disordered orthorhombic structure for Dy2FeCoO6 in Pnma space group which is supported by Raman scattering results. The magnetic structures ascertained through representational analysis indicate that at T N, a paramagnetic state is transformed to Γ5(Cx, Fy, Az) antiferromagnetic structure while, at T SR, Fe/Co moments undergo a spin reorientation to Γ3(Gx, Ay, Fz). The refined magnetic moment of (Fe/Co) is 1.47(4) µ B at 7 K. The antiferromagnetic structure found experimentally is supported through the DFT calculations which predict an insulating electronic state in Dy2FeCoO6.

Texto completo: 1 Banco de datos: MEDLINE Idioma: En Año: 2021 Tipo del documento: Article

Texto completo: 1 Banco de datos: MEDLINE Idioma: En Año: 2021 Tipo del documento: Article