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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 degrees 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 degrees 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摄氏度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. M-12(Sb,As)(4)S-13. Measurements were performed at 25 and 250 degrees 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 S1(2)S2 triangle is about 0.56 and 0.65 angstrom for tetrahedrite and tennantite, respectively. Cu2-Cu2 distances in the structure cavity are 2.8-2.9 angstrom. Between 25 and 250 degrees C, the lattice parameter a increased by 0.02-0.04 angstrom and the interatomic distances by 0.01 angstrom 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 degrees C by about 0.1 angstrom for tetrahedrite and by more than 0.15 angstrom 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:对两个具有0.61和1.83 Fe原子的合成四面体样品以及两个具有0.10和1.23 Fe原子p.f.u的合成球铁矿样品进行X射线同步加速器数据的Rietveld改进。 M-12(Sb,As)(4)S-13。在25和250摄氏度下进行测量。对于这两个相,增加的Fe取代都反映在增加的四面体“ Cu1” -S距离(“ Cu1”是Fe取代的位置)和Cu2-S距离上。 Cu2被精制为分裂位置;对于四面体和球铁矿,围绕S1(2)S2三角形平面分裂的Cu2-Cu2分别约为0.56和0.65埃。结构腔中的Cu 2 -Cu 2距离为2.8-2.9埃。在25到250摄氏度之间,晶格参数a平均增加0.02-0.04埃,原子间距离平均增加0.01埃。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。对于四面体,Cu 2 -Cu 2裂隙在250℃下增加约0.1埃,对于球铁矿,Cu 2 -Cu 2裂隙增加超过0.15埃,但是笼形膨胀最小,使得腔中的Cu 2 -Cu 2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,此位间密度显着更高。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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