Structural transition and magnetic properties of Mn doped Bi0.88Sm0.12FeO3 ceramics

We investigated the effects of Mn doping on the crystal structure, phonon vibration, and magnetic properties of Bi0.88Sm0.12FeO3 ceramics. Mn doping effectively modified the rhombohedral symmetry and induced a structural transition from an R3c rhombohedral to Pnam orthorhombic structure. Magnetic me...

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Veröffentlicht in:RSC advances 2020-03, Vol.10 (20), p.11957-11965
Hauptverfasser: Hien, N T, Vinh, N D, Dang, N V, Trang, T T, Van, H T, Thao, T T, Hue, L T, Tho, P T
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container_end_page 11965
container_issue 20
container_start_page 11957
container_title RSC advances
container_volume 10
creator Hien, N T
Vinh, N D
Dang, N V
Trang, T T
Van, H T
Thao, T T
Hue, L T
Tho, P T
description We investigated the effects of Mn doping on the crystal structure, phonon vibration, and magnetic properties of Bi0.88Sm0.12FeO3 ceramics. Mn doping effectively modified the rhombohedral symmetry and induced a structural transition from an R3c rhombohedral to Pnam orthorhombic structure. Magnetic measurements revealed a weak ferromagnetic behavior, which was related to the canted antiferromagnetic order of the Pnam structure. The cycloidal spin structure of the R3c phase could not be suppressed by substitution of Mn at the Fe site. Studies on the self-phase transition and electric field-induced structural transition revealed many changes in coercivity and remanent magnetization, which are believed to originate from the R3c/Pnam phase switching along with spin frustration. Observations of the field step-dependent hysteresis loop and the ferromagnetic-like hysteresis loop after poling in an electric field provided direct evidence of phase boundary (PB) ferromagnetism and magnetic coupling at the PB.
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Mn doping effectively modified the rhombohedral symmetry and induced a structural transition from an R3c rhombohedral to Pnam orthorhombic structure. Magnetic measurements revealed a weak ferromagnetic behavior, which was related to the canted antiferromagnetic order of the Pnam structure. The cycloidal spin structure of the R3c phase could not be suppressed by substitution of Mn at the Fe site. Studies on the self-phase transition and electric field-induced structural transition revealed many changes in coercivity and remanent magnetization, which are believed to originate from the R3c/Pnam phase switching along with spin frustration. 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subjects Antiferromagnetism
Ceramics
Chemistry
Coercivity
Crystal structure
Deoxidizing
Doping
Electric fields
Ferromagnetism
Hysteresis loops
Magnetic measurement
Magnetic properties
Magnetism
Manganese
Phase transitions
Spin structure
title Structural transition and magnetic properties of Mn doped Bi0.88Sm0.12FeO3 ceramics
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