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首页> 外文期刊>Physics and Chemistry of Minerals >Crystal structures of iron bearing tetrahedrite and tennantite at 25 and 250°C by means of Rietveld refinement of synchrotron data
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Crystal structures of iron bearing tetrahedrite and tennantite at 25 and 250°C by means of Rietveld refinement of synchrotron data

机译:通过同步加速器数据的Rietveld精炼,在25和250°C下含铁的四面体和球铁矿的晶体结构

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摘要

Rietveld refinement of X-ray synchrotron data was performed for two synthetic tetrahedrite samples, with 0.61 and 1.83 Fe atoms, and two synthetic tennantite samples with 0.10 and 1.23 Fe atoms p.f.u. M12(Sb,As)4S13. Measurements were performed at 25 and 250°C. For both the phases, increased Fe substitution is reflected in the increased tetrahedral ‘Cu1’–S distance (‘Cu1’ is a site of Fe substitution) and Cu2–S distances. Cu2 was refined as a split position; the Cu2–Cu2 split about the plane of the S12S2 triangle is about 0.56 and 0.65 ? for tetrahedrite and tennantite, respectively. Cu2–Cu2 distances in the structure cavity are 2.8–2.9 ?. Between 25 and 250°C, the lattice parameter a increased by 0.02–0.04 ? and the interatomic distances by 0.01 ? on an average. Thermal expansion coefficients of little-substituted samples are similar to those of unsubstituted samples, whereas thermal expansion appears to decrease with increasing substitution by Fe. The Cu2–Cu2 split increases at 250°C by about 0.1 ? for tetrahedrite and by more than 0.15 ? for tennantite but the cage expansion is minimal so that the Cu2–Cu2 distances in the cavity decrease with temperature. Difference Fourier maps indicate that there is little residual electron density left between the two Cu2 half-sites in tetrahedrite but this inter-site density is substantially higher in tennantite. It increases with temperature, especially in the little-substituted tennantite sample.
机译:对两个含0.61和1.83 Fe原子的合成四面体样品和两个含0.10和1.23 Fe原子的合成球粒体样品进行了X射线同步加速器数据的Rietveld改进。 M12 (Sb,As)4 S13 。在25和250℃下进行测量。对于这两个阶段,四面体“ Cu1” -S距离(“ Cu1”是Fe取代位点)和Cu2-S距离的增加都反映了Fe取代的增加。 Cu2被细化为拆分位置;围绕S12 S2三角形平面分裂的Cu2-Cu2约为0.56和0.65?分别用于四面体和球铁矿。结构腔中Cu2-Cu2的距离为2.8-2.9?。在25至250°C之间,晶格参数a增加0.02–0.04?原子间距离为0.01?平均而言。很少取代的样品的热膨胀系数与未取代的样品的热膨胀系数相似,而热膨胀似乎随着被Fe取代的增加而降低。在250°C下,Cu2-Cu2的裂隙增加了约0.1?四面体和大于0.15?对于钙钛矿,但笼扩展很小,因此腔中Cu2-Cu2的距离随温度降低。差分傅立叶图表明,在四面体中,两个Cu2半位之间几乎没有残留电子密度,但在钙锰矿中,这种位间密度显着更高。它随温度升高而增加,尤其是在取代度极低的钙钛矿样品中。

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