首页> 外文期刊>Diffusion and Defect Data. Solid State Data, Part B. Solid State Phenomena >Effects of Substitution in Barium hexaferritesBaFe_(12-x)X_xO_(19)(X=Co,Ti; Sc)
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Effects of Substitution in Barium hexaferritesBaFe_(12-x)X_xO_(19)(X=Co,Ti; Sc)

机译:BaFe_(12-x)X_xO_(19)(X = Co,Ti; Sc)取代在钡铁氧体中的作用

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The short and long-range atomic and magnetic order in BaFe_(12-x)Co_xTi_xO_(19)(x=0.4, 0.7,0.8) and BaFe_(10.4)Sc_(1.6)O_(19)prepared by soft chemistry routes were studied and compared with parentBaFe_(12)O_(19)prepared by solid-state reaction. ForBaFe_(10.3)Co_(0.85)Ti_(O_(19)neutron diffraction andmagnetic measurements revealed that (Co , Ti ) substitution causes significant distortions in thelocal oxygen surrounding of ferric cation sites, while the grain-size effect on the structuralparameters is considerably smaller. The thermal expansion coefficient exhibits a strong anisotropy.The refined magnetic moments for x=0.45 and 0.7 based on the five-cation sublattice block-typecollinear ferrimagnetic structure of uniaxial type known as Gorter type for BaFe_(12)O_(19), areconsiderably lower than the theoretical spin only moments, especially for the 4e and 12k sites,indicating for x = 0.7 a local noncollinearity with short-range ordering. For x 0.85, at 10 K ablock-type conical magnetic structure sets in. For BaFe_(10.4)Sc_(1.6)O_(19),combined neutron diffraction,field-dependent ~(57)FeMossbauer studies and magnetic measurements show that the collinear block-type structure remains effective at 300 K and below it down to about 190 K. In the 190 — 1.6 Krange we observe a temperature dependent incommensurate complex block-type conical structure.
机译:研究了通过软化学路线制备的BaFe_(12-x)Co_xTi_xO_(19)(x = 0.4,0.7,0.8)和BaFe_(10.4)Sc_(1.6)O_(19)的短程和长程原子和磁序并与固态反应制备的母体BaFe_(12)O_(19)进行了比较。对于BaFe_(10.3)Co_(0.85)Ti_(O_(19)中子衍射和磁测量表明,(Co,Ti)取代引起三价铁阳离子位点周围的局部氧的明显变形,而晶粒尺寸对结构参数的影响要小得多热膨胀系数表现出很强的各向异性。基于BaFe_(12)O_(19)的称为Gorter型的单轴型五阳离子亚晶格块型共线亚铁磁性结构,x = 0.45和0.7的精细磁矩相当可观低于理论上的仅自旋矩,特别是对于4e和12k位置,表明x = 0.7时具有短程有序的局部非共线性。对于x 0.85,在10 K时会出现块型圆锥形磁结构。对于BaFe_(10.4 Sc_(1.6)O_(19),组合中子衍射,与场有关的〜(57)FeMossbauer研究和磁测量表明,共线块状结构在300 K时仍有效,并且在低于300 K时有效0K。在190 — 1.6 Krange中,我们观察到温度相关的不对称复杂块型圆锥结构。

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