Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature

The crystal structure and magnetic state of the (1 − x)BiFeO<sub>3</sub>-(x)BiMnO<sub>3</sub> solid solution has been analyzed by X-ray diffraction using lab-based and synchrotron radiation facilities, magnetization measurements, differential thermal analysis, and differentia...

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Main Authors: Dmitry V. Karpinsky, Maxim V. Silibin, Siarhei I. Latushka, Dmitry V. Zhaludkevich, Vadim V. Sikolenko, Hanan Al-Ghamdi, Aljawhara H. Almuqrin, M. I. Sayyed, Alexei A. Belik
Format: Article
Language:English
Published: MDPI AG 2022-05-01
Series:Nanomaterials
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Online Access:https://www.mdpi.com/2079-4991/12/9/1565
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author Dmitry V. Karpinsky
Maxim V. Silibin
Siarhei I. Latushka
Dmitry V. Zhaludkevich
Vadim V. Sikolenko
Hanan Al-Ghamdi
Aljawhara H. Almuqrin
M. I. Sayyed
Alexei A. Belik
author_facet Dmitry V. Karpinsky
Maxim V. Silibin
Siarhei I. Latushka
Dmitry V. Zhaludkevich
Vadim V. Sikolenko
Hanan Al-Ghamdi
Aljawhara H. Almuqrin
M. I. Sayyed
Alexei A. Belik
author_sort Dmitry V. Karpinsky
collection DOAJ
description The crystal structure and magnetic state of the (1 − x)BiFeO<sub>3</sub>-(x)BiMnO<sub>3</sub> solid solution has been analyzed by X-ray diffraction using lab-based and synchrotron radiation facilities, magnetization measurements, differential thermal analysis, and differential scanning calorimetry. Dopant concentration increases lead to the room-temperature structural transitions from the polar-active rhombohedral phase to the antipolar orthorhombic phase, and then to the monoclinic phase accompanied by the formation of two-phase regions consisting of the adjacent structural phases in the concentration ranges 0.25 < x<sub>1</sub> < 0.30 and 0.50 ≤ x<sub>2</sub> < 0.65, respectively. The accompanied changes in the magnetic structure refer to the magnetic transitions from the modulated antiferromagnetic structure to the non-colinear antiferromagnetic structure, and then to the orbitally ordered ferromagnetic structure. The compounds with a two-phase structural state at room temperature are characterized by irreversible temperature-driven structural transitions, which favor the stabilization of high-temperature structural phases. The magnetic structure of the compounds also exhibits an irreversible temperature-induced transition, resulting in an increase of the contribution from the magnetic phase associated with the high-temperature structural phase. The relationship between the structural parameters and the magnetic state of the compounds with a metastable structure is studied and discussed depending on the chemical composition and heating prehistory.
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spelling doaj.art-fa082371cb2e4cc1bc2e49305d82c9ff2023-11-23T08:56:11ZengMDPI AGNanomaterials2079-49912022-05-01129156510.3390/nano12091565Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by TemperatureDmitry V. Karpinsky0Maxim V. Silibin1Siarhei I. Latushka2Dmitry V. Zhaludkevich3Vadim V. Sikolenko4Hanan Al-Ghamdi5Aljawhara H. Almuqrin6M. I. Sayyed7Alexei A. Belik8Scientific-Practical Materials Research Centre of NAS of Belarus, 220072 Minsk, BelarusInstitute of Advanced Materials and Technologies, National Research University of Electronic Technology “MIET”, Zelenograd, 124498 Moscow, RussiaScientific-Practical Materials Research Centre of NAS of Belarus, 220072 Minsk, BelarusScientific-Practical Materials Research Centre of NAS of Belarus, 220072 Minsk, BelarusInstitute of Advanced Materials and Technologies, National Research University of Electronic Technology “MIET”, Zelenograd, 124498 Moscow, RussiaDepartment of Physics, College of Science, Princess Nourah Bint Abdulrahman University, P.O. Box 84428, Riyadh 11671, Saudi ArabiaDepartment of Physics, College of Science, Princess Nourah Bint Abdulrahman University, P.O. Box 84428, Riyadh 11671, Saudi ArabiaDepartment of Physics, Faculty of Science, Isra University, Amman 11622, JordanInternational Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science (NIMS), Namiki 1-1, Tsukuba, Ibaraki 305-0044, JapanThe crystal structure and magnetic state of the (1 − x)BiFeO<sub>3</sub>-(x)BiMnO<sub>3</sub> solid solution has been analyzed by X-ray diffraction using lab-based and synchrotron radiation facilities, magnetization measurements, differential thermal analysis, and differential scanning calorimetry. Dopant concentration increases lead to the room-temperature structural transitions from the polar-active rhombohedral phase to the antipolar orthorhombic phase, and then to the monoclinic phase accompanied by the formation of two-phase regions consisting of the adjacent structural phases in the concentration ranges 0.25 < x<sub>1</sub> < 0.30 and 0.50 ≤ x<sub>2</sub> < 0.65, respectively. The accompanied changes in the magnetic structure refer to the magnetic transitions from the modulated antiferromagnetic structure to the non-colinear antiferromagnetic structure, and then to the orbitally ordered ferromagnetic structure. The compounds with a two-phase structural state at room temperature are characterized by irreversible temperature-driven structural transitions, which favor the stabilization of high-temperature structural phases. The magnetic structure of the compounds also exhibits an irreversible temperature-induced transition, resulting in an increase of the contribution from the magnetic phase associated with the high-temperature structural phase. The relationship between the structural parameters and the magnetic state of the compounds with a metastable structure is studied and discussed depending on the chemical composition and heating prehistory.https://www.mdpi.com/2079-4991/12/9/1565crystal structuremagnetic statemultiferroicsphase transitionsmagnetometryX-ray diffraction
spellingShingle Dmitry V. Karpinsky
Maxim V. Silibin
Siarhei I. Latushka
Dmitry V. Zhaludkevich
Vadim V. Sikolenko
Hanan Al-Ghamdi
Aljawhara H. Almuqrin
M. I. Sayyed
Alexei A. Belik
Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
Nanomaterials
crystal structure
magnetic state
multiferroics
phase transitions
magnetometry
X-ray diffraction
title Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
title_full Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
title_fullStr Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
title_full_unstemmed Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
title_short Structural and Magnetic Phase Transitions in BiFe<sub>1 − x</sub>Mn<sub>x</sub>O<sub>3</sub> Solid Solution Driven by Temperature
title_sort structural and magnetic phase transitions in bife sub 1 x sub mn sub x sub o sub 3 sub solid solution driven by temperature
topic crystal structure
magnetic state
multiferroics
phase transitions
magnetometry
X-ray diffraction
url https://www.mdpi.com/2079-4991/12/9/1565
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