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Octahedrally coordinated vacancies in tourmaline: a theoretical approach

机译:电气石中的八面体协调的空位:一种理论方法

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Bond-valence theory is used to explore the local arrangements involving vacancies at the Y and Z sites in the tourmaline structure. The local bond-valence requirements of all possible local arrangements around the O8, O7, O6, O3 and O1 anion-sites have been determined for Y- and Z-site vacancies locally associated with Li~(1+), Mg~(2+), Al~(3+), Fe~(2+), Fe~(3+), B~(3+) and Si~(4+). The results show that arrangements involving tetrahedrally coordinated ~TR~(3+) -cations and octahedrally coordinated ~YR~(2+)- and ~ZR~(2+)-cations around O8, O7 and O6 can be ruled out, together with arrangements involving vacancies and ~YLi~(1+). As the occurrence of a Y-site vacancy (~Y□) is more in accord with the valence-sum rule than the occurrence of a Z-site vacancy (~Z□), ~Y□ is more likely to occur than ~Z□ in tourmaline. Local arrangements involving vacancies around O1- and O3-sites can be stable for OH~-, but not for O~(2-). Of particular interest in this regard are the arrangements[~YR~(3+) ~YR~(3+) ~Y□]-~(O1) and [~ZR~(3+) ~ZR~(3+) ~Y□]-~(O3)(OH~-), which yield the smallest deviations from the valence-sum rule. Coupling these stable arrangements with 2 x [~TSi~(4+) ~ZR~(3+) ~Y□]-~(O6)(O~(2-) forms larger vacancy clusters: [~Y(R~(3+))_2 -~(O1)(OH~-)-~Y(□)-~(O3)(OH~-)-~(O6)(O~(2-))_2-(~ZR~(3+) ~TSi~(4+))_2]. In tourmaline, vacancies are more favoured to occur at Y rather than at Z, in tandem with OH~-—at O3 and O1, R~(3+) at Y and Z and Si~(4+) at T.
机译:结合价理论被用于探索电气石结构中Y和Z位点涉及空位的局部排列。对于与Li〜(1 +),Mg〜(2)局部相关的Y和Z位置空位,已经确定了O8,O7,O6,O3和O1阴离子位置周围所有可能的局部排列的局部键合价要求。 +),Al〜(3 +),Fe〜(2 +),Fe〜(3 +),B〜(3+)和Si〜(4+)。结果表明,可以排除围绕O8,O7和O6的四面体配位〜TR〜(3 +)-阳离子和八面体配位〜YR〜(2 +)-和〜ZR〜(2 +)-阳离子的排列。包含空缺和〜YLi〜(1+)的安排。由于Y位空位(〜Y□)的出现比Z位空位(〜Z□)更符合价和规则,因此〜Y□比〜Z更有可能发生□在电气石中。涉及O1-和O3-位周围空位的局部安排对于OH〜-可能是稳定的,但对于O〜(2-)则不是稳定的。在这方面特别令人感兴趣的是[〜YR〜(3+)〜YR〜(3+)〜Y□]-〜(O1)和[〜ZR〜(3+)〜ZR〜(3+)〜 Y□]-〜(O3)(OH〜-),它与价和规则的偏差最小。将这些稳定排列与2 x [〜TSi〜(4+)〜ZR〜(3+)〜Y□]-〜(O6)(O〜(2-)耦合,形成较大的空位簇:[〜Y(R〜( 3 +))_ 2-〜(O1)(OH〜-)-〜Y(□)-〜(O3)(OH〜-)-〜(O6)(O〜(2-))_ 2-(〜ZR〜 (3+)〜TSi〜(4 +))_ 2]。在电气石中,空位更倾向于在Y而不是Z处发生,空位与OH〜-串联在O3和O1处,R〜(3+)在Y和Z以及T处的Si〜(4+)。

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