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Structural disorder in (Bi,M)2(Fe,Mn,Bi)2O6+x (M = Na or K) pyrochlores seen from reverse Monte Carlo analysis of neutron total scattering

机译:从中子总散射的反向蒙特卡洛分析中看到(Bi,M)2(Fe,Mn,Bi)2O6 + x(M = Na或K)烧绿石的结构无序

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摘要

The average structures of the polycrystalline pyrochlores (Na0.60Bi1.40)(Fe1.06Mn0.17Bi0.77)O6.87 and (K0.24Bi1.51)(Fe1.07Mn0.15Bi0.78)O6.86 can be refined through Rietveld refinement against Bragg scattering data using cubic space group Fd3 ̅m, with off-centred 96h and 32e positions describing the A2Oʹ network. Investigation of their local structures through neutron total scattering confirms the extent of disorder within these materials, and furthermore shows significant deviation from the average structure, which is not accounted for through analysis of Bragg data alone. Reverse Monte Carlo (RMC) analysis with a 6 × 6 × 6 supercell was used to model accurately this local disorder, revealing ellipsoidal distributions for A-site potassium, distinctly different to the hollow torus-shaped distributions for the sodium and bismuth cations. It is shown through bond valence sum analysis that whilst these atomic displacements allow for the steric preferences of Bi3+, they are also necessary to satisfy the valence of both the bismuth and the alkali metals on the A sites. Analysis of the final RMC configuration showed the BO6 octahedra for the separate B site metals to be more regular (O–B–O ≈ 90°) than those in the Rietveld model (O–B–O ≈ 85/95°) which describes an average of the three different environments.
机译:多晶烧绿石(Na0.60Bi1.40)(Fe1.06Mn0.17Bi0.77)O6.87和(K0.24Bi1.51)(Fe1.07Mn0.15Bi0.78)O6.86的平均结构可以通过Rietveld用立方空间群Fd3̅m对布拉格散射数据进行细化,偏心的96h和32e位置描述了A2Oʹ网络。通过中子全散射对其局部结构的研究证实了这些材料内部的无序程度,并且还显示出与平均结构的显着偏差,这不能仅通过分析布拉格数据来解释。使用具有6×6×6超级电池的反向蒙特卡洛(RMC)分析来精确地模拟这种局部紊乱,揭示A位钾的椭圆形分布,与钠和铋阳离子的空心圆环形分布明显不同。通过键合价和分析表明,尽管这些原子位移允许Bi3 +的空间偏好,但它们也必须满足A位上铋和碱金属的化合价。对最终RMC配置的分析表明,单独的B位金属的BO6八面体比Rietveld模型(OB–O≈85/95°)中的金属更规则(OB–O≈90°)。三种不同环境的平均值。

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