Synthesis, structure, and magnetic properties of the layered bismuth transition metal oxide solid solution Bi sub 2 Fe sub 4 minus x Ga sub x O sub 9

The solid solution Bi{sub 2}Fe{sub 4{minus}x}Ga{sub x}O{sub 9} (0 {le} x {le} 4) was synthesized and investigated by X-ray diffraction, Moessbauer spectroscopy, and susceptibility measurements. The system was found essentially to follow Vegard's law. The crystal structure of the x = 2 member, B...

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Veröffentlicht in:Journal of solid state chemistry 1992-07, Vol.99:1
Hauptverfasser: Giaquinta, D.M., Papaefthymiou, G.C., Davis, W.M., Loye, H.C. zur
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Papaefthymiou, G.C.
Davis, W.M.
Loye, H.C. zur
description The solid solution Bi{sub 2}Fe{sub 4{minus}x}Ga{sub x}O{sub 9} (0 {le} x {le} 4) was synthesized and investigated by X-ray diffraction, Moessbauer spectroscopy, and susceptibility measurements. The system was found essentially to follow Vegard's law. The crystal structure of the x = 2 member, Bi{sub 2}Fe{sub 2}Ga{sub 2}O{sub 9}, was solved. The structure is orthorhombic with space group Pbam (No. 55), a = 7.946(1) {angstrom}, b = 8.355(1){angstrom}, and c = 5.929(1) {angstrom}. Iron and gallium were nonstatistically distributed over two octahedral and two tetrahedral sites. The iron displayed a 60% preference for the octahedral positions. Magnetic susceptibility and Moessbauer measurements showed antiferromagnetic behavior. The ordering temperature, T{sub N}, exhibited a strong dependence on x, decreasing rapidly with gallium doping from T{sub N} = 245 {plus minus} 5 K for x = 0 to T{sub N} {lt} 4.2 K for x = 3. Spin-glass-like behavior was observed in the gallium-substituted compounds, and a previously undetected spin rearrangement at 220 K for the x = 0 compound is reported.
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The system was found essentially to follow Vegard's law. The crystal structure of the x = 2 member, Bi{sub 2}Fe{sub 2}Ga{sub 2}O{sub 9}, was solved. The structure is orthorhombic with space group Pbam (No. 55), a = 7.946(1) {angstrom}, b = 8.355(1){angstrom}, and c = 5.929(1) {angstrom}. Iron and gallium were nonstatistically distributed over two octahedral and two tetrahedral sites. The iron displayed a 60% preference for the octahedral positions. Magnetic susceptibility and Moessbauer measurements showed antiferromagnetic behavior. The ordering temperature, T{sub N}, exhibited a strong dependence on x, decreasing rapidly with gallium doping from T{sub N} = 245 {plus minus} 5 K for x = 0 to T{sub N} {lt} 4.2 K for x = 3. Spin-glass-like behavior was observed in the gallium-substituted compounds, and a previously undetected spin rearrangement at 220 K for the x = 0 compound is reported.</abstract><cop>United States</cop><doi>10.1016/0022-4596(92)90296-8</doi></addata></record>
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subjects 360204 - Ceramics, Cermets, & Refractories- Physical Properties
400201 - Chemical & Physicochemical Properties
ANTIFERROMAGNETIC MATERIALS
BISMUTH COMPOUNDS
BISMUTH OXIDES
CHALCOGENIDES
CHEMICAL PREPARATION
COHERENT SCATTERING
CRYSTAL LATTICES
CRYSTAL STRUCTURE
DATA
DIFFRACTION
DISPERSIONS
EXPERIMENTAL DATA
GALLIUM COMPOUNDS
GALLIUM OXIDES
INFORMATION
INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY
IRON COMPOUNDS
IRON OXIDES
LATTICE PARAMETERS
MAGNETIC MATERIALS
MAGNETIC PROPERTIES
MAGNETIC SUSCEPTIBILITY
MATERIALS
MATERIALS SCIENCE
MIXTURES
MOESSBAUER EFFECT
NUMERICAL DATA
ORTHORHOMBIC LATTICES
OXIDES
OXYGEN COMPOUNDS
PHYSICAL PROPERTIES
SCATTERING
SOLID SOLUTIONS
SOLUTIONS
SYNTHESIS
TRANSITION ELEMENT COMPOUNDS
X-RAY DIFFRACTION
title Synthesis, structure, and magnetic properties of the layered bismuth transition metal oxide solid solution Bi sub 2 Fe sub 4 minus x Ga sub x O sub 9
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