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Cation ordering of {110} and {211} sectors in grandite garnet from Mali

机译:马里的石榴石石榴石中{110}和{211}扇区的阳离子排序

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The cation ordering of the {110}_(c) and {211}_(c) growth sectors in birefringent garnet from Kayas, Mali was investigated by means of single–crystal X–ray diffraction (SC–XRD) method The chemical compositions of the {110}_(c) and {211}_(c) sectors were determined as (Ca_(2.96)Mg_(0.04)Mn_(0.04))_(Σ3.04)(Fe_(0.97)Al_(0.95)Ti_(0.11))_(Σ2.03)Si_(2.93)O_(12), and (Ca_(2.91)Mg_(0.05)Mn_(0.03))_(Σ2.99)(Fe_(1.01)Al_(0.90)Ti_(0.14))_(Σ2.05)Si_(2.93)O_(12), respectively. Reflections that violate the extinction rule for the space group Ia 3d were observed, and crystal structure models for both the {110}_(c) and {211}_(c) sectors should have triclinic symmetry with the space group I 1. The unit–cell parameters of both growth sectors were a = 11.9739(13), b = 11.9742(14), c = 11.9737(13) ?, α = 90.001(9), β = 90.098(9) and γ = 90.014 (10)° for the {110}_(c) sector; a = 11.952(6), b = 11.952(6), c = 11.957(6) ?, α = 90.06(4), β = 90.01(4) and γ = 89.94(4)° for the {211}_(c) sector. Structure refinements for I 1 models of both sectors were convergent with R 1 = 3.02 and 3.36%, respectively. There were significant differences in the Fe~(3+) distribution trend in the Y sites between the {110}_(c) and {211}_(c) sectors. The Fe~(3+) occupancies of the eight Y sites in the {110}_(c) sector were 66.9(8), 66.0(8), 63.2(8), 60.0(8), 49.8(8), 49.5(8), 47.8(8), and 46.7(8)%. The octahedral Y sites of {110}_(c) sector can be divided into two groups. In terms of symmetry, Fe~(3+) distribution in the Y site of the {110}_(c) sector appeared to be pseudo–orthorhombic. In contrast, the Fe~(3+) distributions in the eight Y sites of the {211}_(c) sector as follows: 60.0(10), 41.9(10), 62.7(10), 69.1(10), 55.5(10), 53.2(10), 55.7(10), and 43.5(10)%. The Fe~(3+) occupancies in the Y sites of the {211}_(c) sector were random and different from that of the {110}_(c) sector. Different cation distributions between the growth sectors in the Mali garnet indicate that cation ordering in the crystal structure was formed during growth. These observations suggest that the differences in the Fe~(3+) distribution between the {110}_(c) and {211}_(c) sectors are strongly affected by the growth process in each sector.
机译:通过单晶X射线衍射(SC-XRD)方法研究了来自马里卡亚斯的双折射石榴石中{110} _(c)和{211} _(c)生长区的阳离子有序性{110} _(c)和{211} _(c)中的部分被确定为(Ca_(2.96)Mg_(0.04)Mn_(0.04))_(Σ3.04)(Fe_(0.97)Al_(0.95) Ti_(0.11))_(Σ2.03)Si_(2.93)O_(12)和(Ca_(2.91)Mg_(0.05)Mn_(0.03))_(Σ2.99)(Fe_(1.01)Al_(0.90) Ti_(0.14))_(Σ2.05)Si_(2.93)O_(12)。观察到违反空间群 Ia 3d的消光规则的反射,{110} _(c)和{211} _(c)扇区的晶体结构模型应具有三斜对称性,且空间群 I1。两个增长部门的单位-细胞参数分别为 a = 11.9739(13), b = 11.9742(14), c = 11.9737(13)?,对于{110} _(c)扇区,α= 90.001(9),β= 90.098(9)和γ= 90.014(10)°; a = 11.952(6), b = 11.952(6), c = 11.957(6)?,α= 90.06(4),β= 90.01(4) {211} _(c)扇区的γ= 89.94(4)°。两个部门的I 1模型的结构优化分别收敛于R 1 = 3.02和3.36%。 {110} _(c)和{211} _(c)扇区之间Y位的Fe〜(3+)分布趋势存在显着差异。 {110} _(c)扇区中八个 Y站点的Fe〜(3+)占有率分别为66.9(8),66.0(8),63.2(8),60.0(8),49.8(8) ),49.5(8),47.8(8)和46.7(8)%。 {110} _(c)扇区的八面体 Y位置可以分为两组。就对称性而言,{110} _(c)扇形的 Y部位的Fe〜(3+)分布似乎是伪斜方晶。相反,{211} _(c)扇区的八个 Y位置中的Fe〜(3+)分布如下:60.0(10),41.9(10),62.7(10),69.1(10) ),55.5(10),53.2(10),55.7(10)和43.5(10)%。 {211} _(c)扇区的 Y位置中的Fe〜(3+)占据是随机的,并且不同于{110} _(c)扇区。马里石榴石的生长区域之间的阳离子分布不同,表明在生长过程中形成了晶体结构中的阳离子有序。这些观察结果表明,{110} _(c)和{211} _(c)部门之间的Fe〜(3+)分布差异受各个部门增长过程的强烈影响。

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