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首页> 外文期刊>Acta Crystallographica, Section B. Structural Science >Radial distribution of electron density in magnetite, Fe3O4
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Radial distribution of electron density in magnetite, Fe3O4

机译:磁铁矿Fe3O4中电子密度的径向分布

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Radial electron distributions and net atomic charges of magnetite Fe3O4 have been studied using single-crystal X-ray intensity data up to sin theta/lambda=1.22 Angstrom(-1). The number of electrons, C(R), was calculated against the radius of an atomic sphere for each atom by the Fourier summation method from the observed crystal structure factors. The radial distribution function was then obtained by differentiating the C(R) curve to derive an electron distribution radius, r(ED), which can give a clear separation between neighboring atoms. The effective atomic charges of Fe ions thus obtained are +1.93 (4) e (A site) and +1.47 (4) e (B site), with r(ED) = 1.13 and 1.19 Angstrom, respectively. Fe ions occupying the A site are more ionic than those at the B site. The charge difference between sites A and B is +0.46 e, which is comparable to an ideal difference of +0.5 e between Fe3+ and [Fe2+Fe3+]. It suggests the existence of valence fluctuation between Fe2+ and Fe3+ in the B site. Crystal data: Fe3O4, M-r = 231.54, cubic, Fd (3) over bar m, = 8.375 (2) Angstrom, V = 587.4 (4) Angstrom(3), Z = 8, D-x = 5.23 Mg m(-3), lambda(Mo K alpha) = 0.7107 Angstrom, mu(Mo K alpha) = 14.88 mm(-1), F(000) = 880, T = 296 K, final R = 0.016 wR = 0.010 for 78 reflections averaged out of 6049 within a hemisphere, with F > 3 sigma(F); u = 0.2555 (2).
机译:使用单晶X射线强度数据研究了磁铁矿Fe3O4的径向电子分布和净原子电荷,其正弦θ/λ= 1.22埃(-1)。根据观察到的晶体结构因子,通过傅里叶求和方法,针对每个原子,针对原子原子半径计算电子数C(R)。然后,通过微分C(R)曲线以得出电子分布半径r(ED)来获得径向分布函数,该分布可以使相邻原子之间实现清晰的分隔。由此获得的Fe离子的有效原子电荷为+1.93(4)e(A位)和+1.47(4)e(B位),r(ED)= 1.13和1.19埃。占据A位的Fe离子比位于B位的Fe离子更具离子性。位置A和B之间的电荷差为+0.46 e,相当于Fe3 +和[Fe2 + Fe3 +]之间的理想差+0.5 e。这表明在B位存在Fe2 +和Fe3 +之间的价态波动。晶体数据:Fe3O4,Mr = 231.54,立方,bar上的Fd(3),= 8.375(2)埃,V = 587.4(4)埃(3),Z = 8,Dx = 5.23 Mg m(-3) ,λ(Mo K alpha)= 0.7107埃,mu(Mo K alpha)= 14.88 mm(-1),F(000)= 880,T = 296 K,最终R = 0.016 wR = 0.010(平均78次反射)半球内6049,F> 3 sigma(F); u = 0.2555(2)。

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