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Magnetism
Magnetic phase diagrams of R$_{1-x}$Sr$_{x}$(Mn$_{1-x/2}$Sb$_{x/2}$)O$_{3}$ ($R$ = La, Pr, Nd, Sm, Eu) with trivalent manganese ions
I. O. Troyanchuka, M. V. Bushinskya, N. V. Tereshkoa, V. V. Sikolenkob, C. Ritterc, S. Schorrde a Scientific-Practical Materials Research Centre of NAS of Belarus, Minsk, Belarus
b Joint Institute for Nuclear Research, Dubna, Moscow region
c Institut Laue-Langevin, Grenoble, France
d Helmholtz-Zentrum Berlin, Berlin, Germany
e Freie University Berlin, Berlin, Germany
Abstract:
The results of neutron-diffraction, magnetic, and magnetotransport studies of La$_{1-x}$Sr$_{x}$(Mn$_{1-x/2}^{3+}$Sb$_{x/2}^{5+}$)O$_{3}$ ($x\le$ 0.7) pervoskites, which contain only Mn$^{3+}$ ions, are reported. It is demonstrated that the system undergoes a transition from the antiferromagnetic state to the ferromagnetic one at $x\sim$ 0.2. Its structure then changes from $O'$-orthorombic to $O$-orthorombic, which is attributable to orbital disordering. At $x\ge$ 0.6, the competition between antiferromagnetic and ferromagnetic interactions and strong diamagnetic dilution trigger the emergence of the cluster spin-glass phase. As the ionic radius of rare-earth ions in $R_{0.7}$Sr$_{0.3}$Mn$_{0.85}$Sb$_{0.15}$O$_{3}$ decreases, the ferromagnetic state transforms gradually into spin glass ($R$ = Sm). All ferromagnetic compositions are dielectric in the magnetically ordered phase with strong magnetoresistive effects. It is assumed that ferromagnetism is induced by the strong covalency and orbital disordering.
Received: 10.01.2018 Revised: 31.01.2018
Citation:
I. O. Troyanchuk, M. V. Bushinsky, N. V. Tereshko, V. V. Sikolenko, C. Ritter, S. Schorr, “Magnetic phase diagrams of R$_{1-x}$Sr$_{x}$(Mn$_{1-x/2}$Sb$_{x/2}$)O$_{3}$ ($R$ = La, Pr, Nd, Sm, Eu) with trivalent manganese ions”, Fizika Tverdogo Tela, 60:9 (2018), 1717–1722; Phys. Solid State, 60:9 (2018), 1762–1767
Linking options:
https://www.mathnet.ru/eng/ftt9075 https://www.mathnet.ru/eng/ftt/v60/i9/p1717
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