Magnetic phase transformations and magnetotransport phenomena in La0.7Sr0.3Mn1 – xCoxO3 perovskite compounds
- Autores: Troyanchuk I.O.1, Bushinsky M.V.1, Karpinsky D.V.1, Sikolenko V.V.2,3, Chobot A.N.1, Tereshko N.V.1, Mantytskaya O.S.1, Schorr S.3,4
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Afiliações:
- Scientific and Practical Materials Research Center
- Joint Institute for Nuclear Research
- Helmholtz-Zentrum Berlin
- Freie University Berlin
- Edição: Volume 125, Nº 2 (2017)
- Páginas: 290-297
- Seção: Order, Disorder, and Phase Transition in Condensed System
- URL: https://journals.rcsi.science/1063-7761/article/view/192456
- DOI: https://doi.org/10.1134/S1063776117070238
- ID: 192456
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Resumo
The compositions La0.7Sr0.3Mn1 – xCoxO3 (0.13 ≤ x ≤ 1) are studied by neutron diffraction, magnetometry, and measuring the magnetotransport properties. The substitution of cobalt ions for manganese ions is shown to decrease the magnetization and the Curie temperature from 270 K (x = 0.13) to 140 K (x = 0.33). As the cobalt ion content increases to x = 0.5, the Curie temperature increases to 190 K, the magnetization decreases, and the electrical resistivity increases. At x > 0.5, the temperature of transition into a paramagnetic state decreases to 68 K (x = 0.8) and then again increases to 225 K for the La0.7Sr0.3CoO3 composition. The magnetoresistive effect in the range 0.3 ≤ x ≤ 0.4 reaches 97% and decreases gradually with increasing temperature without anomalies near the Curie point. At x ≤ 0.2, the magnetoresistive effect increases near the Curie temperature. The composition at x = 0.6 is stoichiometric, and no coherent magnetic contribution to neutron scattering is detected. The magnetic properties near x ∼ 0.5 are assumed to be caused by partial ordering of Co3+ and Mn4+ ions, and the Co3+ ions can be in both low- and high-spin states. The magnetic interaction between Co3+ ions in a high-spin state and Mn4+ is predominantly ferromagnetic, and the ferromagnetic part of the exchange interactions is close to the ferromagnetic part. These data are used to plot a magnetic La0.7Sr0.3Mn1 – xCoxO3 phase diagram.
Sobre autores
I. Troyanchuk
Scientific and Practical Materials Research Center
Autor responsável pela correspondência
Email: troyan@physics.by
Belarus, Minsk, 220072
M. Bushinsky
Scientific and Practical Materials Research Center
Email: troyan@physics.by
Belarus, Minsk, 220072
D. Karpinsky
Scientific and Practical Materials Research Center
Email: troyan@physics.by
Belarus, Minsk, 220072
V. Sikolenko
Joint Institute for Nuclear Research; Helmholtz-Zentrum Berlin
Email: troyan@physics.by
Rússia, Dubna, Moscow oblast, 141980; Berlin, 12489
A. Chobot
Scientific and Practical Materials Research Center
Email: troyan@physics.by
Belarus, Minsk, 220072
N. Tereshko
Scientific and Practical Materials Research Center
Email: troyan@physics.by
Belarus, Minsk, 220072
O. Mantytskaya
Scientific and Practical Materials Research Center
Email: troyan@physics.by
Belarus, Minsk, 220072
S. Schorr
Helmholtz-Zentrum Berlin; Freie University Berlin
Email: troyan@physics.by
Alemanha, Berlin, 12489; Berlin, 14195
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