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通过高能X射线衍射、反向蒙特卡罗和Rietveld分析研究碲酸锶玻璃、反玻璃和晶相的结构。

Structure of strontium tellurite glass, anti-glass and crystalline phases by high-energy X-ray diffraction, reverse Monte Carlo and Rietveld analysis.

作者信息

Kaur Rajinder, Khanna Atul, Dippel Ann Christin, Gutowski Olof, González Fernando, González-Barriuso Marina

机构信息

Department of Physics, Guru Nanak Dev University, Amritsar, Punjab 143005, India.

Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg, Germany.

出版信息

Acta Crystallogr B Struct Sci Cryst Eng Mater. 2020 Feb 1;76(Pt 1):108-121. doi: 10.1107/S2052520620000025. Epub 2020 Jan 28.

DOI:10.1107/S2052520620000025
PMID:32831246
Abstract

The structures of xSrO-(100 - x)TeO (x = 5, 7.5, 8.5 and 10 mol.%) glass, anti-glass and crystalline samples were studied by high-energy X-ray diffraction (HEXRD), reverse Monte Carlo (RMC) simulations, atomic pair distribution function analysis and Fullprof Rietveld refinement. The atomic pair distributions show the first peak at 1.90 Å due to the Te-O equatorial bonds and the Te-O peak is asymmetrical due to the range of Te-O bond lengths in glass, anti-glass and crystalline samples. The short-range structural properties of glasses such as Te-O bond lengths, Te-O speciation, Te-Te distances and O-Te-O bond angle distributions were determined by RMC simulations. The average Te-O coordination number (N) for 5SrO-95TeO glass is 3.93 which decreases to 3.59 on increasing the SrO concentration to 10 mol.%. The changes in N revealed that the glass network predominantly contains TeO units with a small amount of TeO units and there is a structural transformation TeO → TeO with an increase in SrO concentration. The O-Te-O bond angle distributions have a peak at 79° and reveal that the O-Te-O bonds are the most abundant linkages in the tellurite network. Two glass samples containing 7.5 and 8.5 mol.% of SrO were annealed at 350°C for 1 h to produce anti-glass phases; they were further annealed at 450°C for 4 h to transform them into crystalline phases. The anti-glass samples are disordered cubic SrTeO and the disordered monoclinic SrTeO phases, whereas the crystalline samples contain monoclinic SrTeO and the orthorhombic TeO phases. The unit-cell parameters of the anti-glass and crystalline structures were determined by Fullprof Rietveld refinement. Thermal studies found that the glass transition temperature increases with an increase in SrO mol.% and the results on the short-range structure of glasses from Raman spectroscopy are in agreement with the RMC findings.

摘要

通过高能X射线衍射(HEXRD)、反向蒙特卡罗(RMC)模拟、原子对分布函数分析和Fullprof Rietveld精修,研究了xSrO-(100 - x)TeO(x = 5、7.5、8.5和10 mol.%)玻璃、反玻璃和晶体样品的结构。原子对分布显示,由于Te-O赤道键,第一个峰出现在1.90 Å处,并且由于玻璃、反玻璃和晶体样品中Te-O键长的范围,Te-O峰是不对称的。通过RMC模拟确定了玻璃的短程结构性质,如Te-O键长、Te-O形态、Te-Te距离和O-Te-O键角分布。5SrO-95TeO玻璃的平均Te-O配位数(N)为3.93,当SrO浓度增加到10 mol.%时,该值降至3.59。N的变化表明,玻璃网络主要包含TeO单元和少量的TeO单元,并且随着SrO浓度的增加,存在结构转变TeO → TeO。O-Te-O键角分布在79°处有一个峰,表明O-Te-O键是碲酸盐网络中最丰富的键合。将两个含有7.5和8.5 mol.% SrO的玻璃样品在350°C下退火1 h以产生反玻璃相;将它们进一步在450°C下退火4 h以将它们转变为晶相。反玻璃样品是无序立方SrTeO和无序单斜SrTeO相,而晶体样品包含单斜SrTeO和正交TeO相。通过Fullprof Rietveld精修确定了反玻璃和晶体结构的晶胞参数。热学研究发现,玻璃化转变温度随着SrO mol.%的增加而升高,并且拉曼光谱法对玻璃短程结构的研究结果与RMC的发现一致。

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