Structures of Ca5(VO4)3Cl and Ca4.78(1)Na0.22(PO4)3Cl0.78: positions of channel anions and repulsion on the anion in apatite-type compounds

Mimiko Matsuura, H. Okudera
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Abstract

Single crystal specimens of apatite-type compounds Ca5(VO4)3Cl and Ca4.78 (1)Na0.22(PO4)3Cl0.78 were prepared with a flux-growth technique and their structures were examined with single-crystal X-ray diffraction. The anion channel is defined by a face-sharing array of nearly regular Ca octahedra, which run along c, together with flat O3 trigonal antiprisms that are concentric with the Ca octahedra and highly oblate in [001]. The position of the channel anion in Ca5(VO4)3Cl is split into two at [0, 0, ±0.1691 (6)] with half occupancies. Dynamic disorder among these two positions is suggested from a saddle-shaped electron density distribution through the Ca regular triangle, i.e. the shared face of the Ca octahedra at z = ¼. The position of Cl− was too close to Ca2+ under bond-valence consideration. This is due to repulsion on Cl− from the flat O3 trigonal antiprism which is located at z = 0, namely, in between pairs of split Cl site positions. Ca4.78 (1)Na0.22(PO4)3Cl0.78 crystallizes as a disordered hexagonal structure in which the crystallographic pattern is not an intermediate state but a projection of two distinct halves of the monoclinic pattern [doubled in b; Mackie, Elliot & Young (1972). Acta Cryst. B28, 1840–1848] in one hexagonal cell. In spite of quite different environments, the bond-valence sums for Cl− in these structures are large and similar to each other. The repulsion between O2− and Cl− and a demand for keeping Ca2+ and Cl− apart are balanced at the positions where bond-valence sums for Cl− are around 1.2.
Ca5(VO4)3Cl和Ca4.78(1)Na0.22(PO4)3Cl0.78的结构:通道阴离子的位置和对阴离子的排斥力
采用通量生长法制备了磷灰石型化合物Ca5(VO4)3Cl和Ca4.78 (1)Na0.22(PO4)3Cl0.78的单晶样品,并用x射线单晶衍射对其结构进行了表征。阴离子通道由沿c方向排列的几乎规则的Ca八面体组成的面共享阵列以及与Ca八面体同心且在[001]中高度扁圆的平面O3三角形反棱镜定义。Ca5(VO4)3Cl中通道阴离子的位置在[0,0,±0.1691(6)]处被一分为二,占据率为一半。通过Ca正则三角形(即Ca八面体在z =¼处的共享面)的鞍状电子密度分布,可以推测出这两个位置之间的动态无序性。考虑到键价,Cl−的位置过于接近Ca2+。这是由于位于z = 0的平面O3三角形反棱镜对Cl−的排斥作用,即在分裂的Cl位对之间。Ca4.78 (1)Na0.22(PO4)3Cl0.78结晶为无序的六方结构,其晶体模式不是中间状态,而是单斜模式的两个不同半的投影[在b中翻倍];Mackie, Elliot & Young(1972)。Acta结晶。[B28, 1840-1848]在一个六边形的格子里。尽管环境完全不同,但这些结构中Cl−的键价和都很大,而且彼此相似。O2 -和Cl -之间的斥力以及保持Ca2+和Cl -分开的需求在Cl -的键价和约为1.2的位置上达到平衡。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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