Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub>
The phase content and sequence, the crystal structure, and the magnetic properties of perovskite solid solutions of the (1−<i>y</i>)BiFeO<sub>3</sub>–<i>y</i>BiZn<sub>0.5</sub>Ti<sub>0.5</sub>O<sub>3</sub> series (0.05 ≤ <i&g...
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oai:doaj.org-article:865ad8d936d14b6296b319ebb21aa8032021-11-25T18:12:33ZMagnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub>10.3390/magnetochemistry71101512312-7481https://doaj.org/article/865ad8d936d14b6296b319ebb21aa8032021-11-01T00:00:00Zhttps://www.mdpi.com/2312-7481/7/11/151https://doaj.org/toc/2312-7481The phase content and sequence, the crystal structure, and the magnetic properties of perovskite solid solutions of the (1−<i>y</i>)BiFeO<sub>3</sub>–<i>y</i>BiZn<sub>0.5</sub>Ti<sub>0.5</sub>O<sub>3</sub> series (0.05 ≤ <i>y</i> ≤ 0.90) synthesized under high pressure have been studied. Two perovskite phases, namely the rhombohedral <i>R</i>3<i>c</i> and the tetragonal <i>P</i>4<i>mm,</i> which correspond to the structural types of the end members, BiFeO<sub>3</sub> and BiZn<sub>0.5</sub>Ti<sub>0.5</sub>O<sub>3</sub>, respectively, were revealed in the as-synthesized samples. The rhombohedral and the tetragonal phases were found to coexist in the compositional range of 0.30 ≤ <i>y</i> ≤ 0.90. Magnetic properties of the BiFe<sub>1−<i>y</i></sub>[Zn<sub>0.5</sub>Ti<sub>0.5</sub>]<i><sub>y</sub></i>O<sub>3</sub> ceramics with <i>y</i> < 0.30 were measured as a function of temperature. The obtained compositional variations of the normalized unit-cell volume and the Néel temperature of the BiFe<sub>1−<i>y</i></sub>[Zn<sub>0.5</sub>Ti<sub>0.5</sub>]<i><sub>y</sub></i>O<sub>3</sub> perovskites in the range of their rhombohedral phase were compared with the respective dependences for the BiFe<sub>1−<i>y</i></sub><i>B</i><sup>3+</sup><i><sub>y</sub></i>O<sub>3</sub> perovskites (where <i>B</i><sup>3+</sup> = Ga, Co, Mn, Cr, and Sc). The role of the high-pressure synthesis in the formation of the antiferromagnetic states different from the modulated cycloidal one characteristic of the parent BiFeO<sub>3</sub> is discussed.Andrei N. SalakJoão Pedro V. CardosoJoaquim M. VieiraVladimir V. ShvartsmanDmitry D. KhalyavinElena L. FertmanAlexey V. FedorchenkoAnatoli V. PushkarevYury V. RadyushNikolai M. OlekhnovichRóbert TarasenkoAlexander FeherErik ČižmárMDPI AGarticleatomic substitutionNéel temperatureG-type antiferromagneticweak ferromagnetismcollinear magnetic ground stateChemistryQD1-999ENMagnetochemistry, Vol 7, Iss 151, p 151 (2021) |
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DOAJ |
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atomic substitution Néel temperature G-type antiferromagnetic weak ferromagnetism collinear magnetic ground state Chemistry QD1-999 |
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atomic substitution Néel temperature G-type antiferromagnetic weak ferromagnetism collinear magnetic ground state Chemistry QD1-999 Andrei N. Salak João Pedro V. Cardoso Joaquim M. Vieira Vladimir V. Shvartsman Dmitry D. Khalyavin Elena L. Fertman Alexey V. Fedorchenko Anatoli V. Pushkarev Yury V. Radyush Nikolai M. Olekhnovich Róbert Tarasenko Alexander Feher Erik Čižmár Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
description |
The phase content and sequence, the crystal structure, and the magnetic properties of perovskite solid solutions of the (1−<i>y</i>)BiFeO<sub>3</sub>–<i>y</i>BiZn<sub>0.5</sub>Ti<sub>0.5</sub>O<sub>3</sub> series (0.05 ≤ <i>y</i> ≤ 0.90) synthesized under high pressure have been studied. Two perovskite phases, namely the rhombohedral <i>R</i>3<i>c</i> and the tetragonal <i>P</i>4<i>mm,</i> which correspond to the structural types of the end members, BiFeO<sub>3</sub> and BiZn<sub>0.5</sub>Ti<sub>0.5</sub>O<sub>3</sub>, respectively, were revealed in the as-synthesized samples. The rhombohedral and the tetragonal phases were found to coexist in the compositional range of 0.30 ≤ <i>y</i> ≤ 0.90. Magnetic properties of the BiFe<sub>1−<i>y</i></sub>[Zn<sub>0.5</sub>Ti<sub>0.5</sub>]<i><sub>y</sub></i>O<sub>3</sub> ceramics with <i>y</i> < 0.30 were measured as a function of temperature. The obtained compositional variations of the normalized unit-cell volume and the Néel temperature of the BiFe<sub>1−<i>y</i></sub>[Zn<sub>0.5</sub>Ti<sub>0.5</sub>]<i><sub>y</sub></i>O<sub>3</sub> perovskites in the range of their rhombohedral phase were compared with the respective dependences for the BiFe<sub>1−<i>y</i></sub><i>B</i><sup>3+</sup><i><sub>y</sub></i>O<sub>3</sub> perovskites (where <i>B</i><sup>3+</sup> = Ga, Co, Mn, Cr, and Sc). The role of the high-pressure synthesis in the formation of the antiferromagnetic states different from the modulated cycloidal one characteristic of the parent BiFeO<sub>3</sub> is discussed. |
format |
article |
author |
Andrei N. Salak João Pedro V. Cardoso Joaquim M. Vieira Vladimir V. Shvartsman Dmitry D. Khalyavin Elena L. Fertman Alexey V. Fedorchenko Anatoli V. Pushkarev Yury V. Radyush Nikolai M. Olekhnovich Róbert Tarasenko Alexander Feher Erik Čižmár |
author_facet |
Andrei N. Salak João Pedro V. Cardoso Joaquim M. Vieira Vladimir V. Shvartsman Dmitry D. Khalyavin Elena L. Fertman Alexey V. Fedorchenko Anatoli V. Pushkarev Yury V. Radyush Nikolai M. Olekhnovich Róbert Tarasenko Alexander Feher Erik Čižmár |
author_sort |
Andrei N. Salak |
title |
Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
title_short |
Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
title_full |
Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
title_fullStr |
Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
title_full_unstemmed |
Magnetic Behaviour of Perovskite Compositions Derived from BiFeO<sub>3</sub> |
title_sort |
magnetic behaviour of perovskite compositions derived from bifeo<sub>3</sub> |
publisher |
MDPI AG |
publishDate |
2021 |
url |
https://doaj.org/article/865ad8d936d14b6296b319ebb21aa803 |
work_keys_str_mv |
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