Magnetic properties of La and (La, Zr) doped BiFeO3 ceramics

Bi 0.9 La 0.1 FeO 3 (BLF) and Bi 0.9 La 0.1 Fe 0.98 Zr 0.02 O 3 (BLFZ) ceramics were synthesized by conventional solid state reaction method. X-ray diffraction studies and Rietveld refinements indicated that both of the samples possessed rhombohedrally distorted perovskite structure. The average gra...

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Veröffentlicht in:Journal of materials science 2011-02, Vol.46 (3), p.734-738
Hauptverfasser: Lan, Changyong, Jiang, Yuwen, Yang, Shaoguang
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creator Lan, Changyong
Jiang, Yuwen
Yang, Shaoguang
description Bi 0.9 La 0.1 FeO 3 (BLF) and Bi 0.9 La 0.1 Fe 0.98 Zr 0.02 O 3 (BLFZ) ceramics were synthesized by conventional solid state reaction method. X-ray diffraction studies and Rietveld refinements indicated that both of the samples possessed rhombohedrally distorted perovskite structure. The average grain size of BLFZ (~700 nm) was greatly reduced in comparison with BLF (~6 μm). The remanent magnetization of BLFZ was greatly enhanced compared with BLF. The enhancement of remanent magnetization was attributed to the collapse of the spiral spin structure. Both samples showed exchange bias. The possible reason for the appearance of exchange bias was attributed to the inhomogeneity in doping. The measurements of magnetization as a function of temperature indicated that BLF and BLFZ had almost the same magnetic transition temperature (~355 °C).
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X-ray diffraction studies and Rietveld refinements indicated that both of the samples possessed rhombohedrally distorted perovskite structure. The average grain size of BLFZ (~700 nm) was greatly reduced in comparison with BLF (~6 μm). The remanent magnetization of BLFZ was greatly enhanced compared with BLF. The enhancement of remanent magnetization was attributed to the collapse of the spiral spin structure. Both samples showed exchange bias. The possible reason for the appearance of exchange bias was attributed to the inhomogeneity in doping. 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X-ray diffraction studies and Rietveld refinements indicated that both of the samples possessed rhombohedrally distorted perovskite structure. The average grain size of BLFZ (~700 nm) was greatly reduced in comparison with BLF (~6 μm). The remanent magnetization of BLFZ was greatly enhanced compared with BLF. The enhancement of remanent magnetization was attributed to the collapse of the spiral spin structure. Both samples showed exchange bias. The possible reason for the appearance of exchange bias was attributed to the inhomogeneity in doping. 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X-ray diffraction studies and Rietveld refinements indicated that both of the samples possessed rhombohedrally distorted perovskite structure. The average grain size of BLFZ (~700 nm) was greatly reduced in comparison with BLF (~6 μm). The remanent magnetization of BLFZ was greatly enhanced compared with BLF. The enhancement of remanent magnetization was attributed to the collapse of the spiral spin structure. Both samples showed exchange bias. The possible reason for the appearance of exchange bias was attributed to the inhomogeneity in doping. The measurements of magnetization as a function of temperature indicated that BLF and BLFZ had almost the same magnetic transition temperature (~355 °C).</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1007/s10853-010-4805-9</doi><tpages>5</tpages></addata></record>
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subjects Bias
Bismuth ferrite
Ceramics
Characterization and Evaluation of Materials
Chemistry and Materials Science
Classical Mechanics
Collapse
Crystallography and Scattering Methods
Diffraction
Distortion
Exchanging
Grain size
Inhomogeneity
Magnetic properties
Magnetic transitions
Magnetism
Magnetization
Materials Science
Perovskite structure
Perovskites
Polymer Sciences
Solid Mechanics
Spin structure
Transition temperature
Zirconium
title Magnetic properties of La and (La, Zr) doped BiFeO3 ceramics
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