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Structure of the fully ferroelectric/fully ferroelastic orthorhombic room-temperature phase of iron iodine boracite, Fe3B7O13I

机译:碘铁硼铁矿Fe 3 B 7 O 13 I的全铁电/全铁弹性正交晶室温相的结构

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摘要

FeBOI, M=578.13, orthorhombic, Pca2, a=8.6540(3), b=8.6481(3), c=12.2336(5) A, v=915.57(6) A, Z=4, D=4.19Mg m, A(Mo Ka)=0.7107A, u08.31 mm, F(000)=1080, T=298K, R=0.03 for 1936 reflexions from an optically controlled single-domain crystal. The metal surroundings of the three Fe atoms are analysed in detail; two of three metal sites (Fe2, Fe3) have similar chemical environments and equal displacement parameters. The averaged difference between the two Fe-I distances is compared with those of other non-cubic boracites. It decreases linearly as the ionic radius of the halogen increases, except for boracites containing Cr and Cu atoms with degenerate electronic states (showing Jahn-Teller effect).
机译:FeBOI,M = 578.13,正交,Pca2,a = 8.6540(3),b = 8.6481(3),c = 12.2336(5)A,v = 915.57(6)A,Z = 4,D = 4.19Mg m,对于来自光学控制的单畴晶体的1936年反射,A(Mo Ka)= 0.7107A,u08.31 mm,F(000)= 1080,T = 298K,R = 0.03。详细分析了三个Fe原子的金属周围环境;三个金属位点中的两个(Fe2,Fe3)具有相似的化学环境和相等的置换参数。将两个Fe-I距离之间的平均差异与其他非立方硼铁矿的平均差异进行比较。它随着卤素离子半径的增加而线性减小,除了含有Cr和Cu原子的简并电子态的硼铁矿(显示Jahn-Teller效应)。

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