1 research outputs found
Magnetic Interactions in the Double Perovskites R<sub>2</sub>NiMnO<sub>6</sub> (R = Tb, Ho, Er, Tm) Investigated by Neutron Diffraction
R<sub>2</sub>NiMnO<sub>6</sub> (R = Tb, Ho, Er, Tm) perovskites have been
prepared by soft-chemistry techniques followed by high oxygen-pressure
treatments; they have been investigated by X-ray diffraction, neutron
powder diffraction (NPD), and magnetic measurements. In all cases
the crystal structure is defined in the monoclinic <i>P</i>2<sub>1</sub>/<i>n</i> space group, with an almost complete
order between Ni<sup>2+</sup> and Mn<sup>4+</sup> cations in the octahedral
perovskite sublattice. The low temperature NPD data and the macroscopic
magnetic measurements indicate that all the compounds are ferrimagnetic,
with a net magnetic moment different from zero and a distinct alignment
of Ni and Mn spins depending on the nature of the rare-earth cation.
The magnetic structures are different from the one previously reported
for La<sub>2</sub>NiMnO<sub>6</sub>, with a ferromagnetic structure
involving Mn<sup>4+</sup> and Ni<sup>2+</sup> moments. This spin alignment
can be rationalized taking into account the Goodenough–Kanamori
rules. The magnetic ordering temperature (<i>T</i><sub>CM</sub>) decreases abruptly as the size of the rare earth decreases, since <i>T</i><sub>CM</sub> is mainly influenced by the superexchange
interaction between Ni<sup>2+</sup> and Mn<sup>4+</sup> (Ni<sup>2+</sup>–O–Mn<sup>4+</sup> angle) and this angle decreases
with the rare-earth size. The rare-earth magnetic moments participate
in the magnetic structures immediately below <i>T</i><sub>CM</sub>