The influence of composition on the local structure around yttrium in quenched silicate melts — Insights from EXAFS

The influence of composition on the local structure around yttrium in quenched silicate melts — Insights from EXAFS
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成分对淬火硅酸盐熔体中钇周围局部结构的影响 â 来自 EXAFS 的见解

DOI:
10.1016/j.chemgeo.2012.09.017
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发表时间:
2013
期刊:
影响因子:
3.9
通讯作者:
Hennet L.
Hennet L.
中科院分区:
地球科学2区
文献类型:
--
作者:
Simon S;Wilke M;Chernikov R;Klemme S;Hennet L.

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用扩展X射线吸收精细结构(EXAFS)谱研究了含5000 ppm Y的硅酸盐和铝硅酸盐玻璃中Y周围的结构环境随熔体组成和聚合反应的变化。所使用的玻璃组合物取自Prowatke和Klemme(2005),铝饱和指数(ASI,Al 2 O3/(Na 2 O + K2 O +CaO)的摩尔比)从0.115变化到0.768。此外,使用了来自CaO-Al 2 O3-SiO2(CAS)系统的一组玻璃组合物,其结构数据来自计算机模拟(Haigis等人,2013--本期)。第一配位壳层的Y-O对关联的结构参数是根据解释大的静态无序和非高斯对分布的类γ分布函数从EXAFS确定的。分析表明,对于Prowatke和Klemme(2005)的组合物,配位数从6增加到8,沿着,平均Y-O距离增加0.13 π。对于CAS-组合物,随着平均Y-O距离增加0.06 π,配位数从6增加到7,沿着。这些参数的变化与Y-O对分布的不对称性和宽度的显著增加有关。由于其尺寸和电荷,6重配位Y将优先键合到聚合物熔体网络的非桥接氧上以形成稳定的构型,对于具有低ASI的较少聚合的熔体也是如此。在ASI值接近1的高度聚合熔体中,Y的6倍配位是不可能的,因为几乎只有桥氧可用。因此,通过增加配位数和Y-O距离来平衡Y周围的桥氧的过度键合,以满足局部电荷平衡要求。
The structural environment around Y in silicate and aluminosilicate glasses containing 5000ppm Y was investigated as a function of melt composition and polymerization using Extended X-ray Absorption Fine Structure (EXAFS) spectroscopy. The used glass compositions were taken from Prowatke and Klemme (2005) varying in the aluminum saturation index (ASI, molar ratio of Al2O3/(Na2O+K2O+CaO)) from 0.115 to 0.768. Furthermore, a set of glass compositions from the system CaO–Al2O3–SiO2(CAS) was used, for which structural data from computer simulations are available (Haigis et al., 2013--this issue). Structural parameters of the Y–O pair correlation of the first coordination shell were determined from the EXAFS based on a gamma-like distribution function that accounts for the large static disorder and non-Gaussian pair distributions. The analysis shows an increase in the coordination number from 6 to 8, along with an increase of the average Y–O distance by 0.13Å for the composition of Prowatke and Klemme (2005). For the CAS-composition an increase of the coordination number from 6 to 7, along with an increase of the average Y–O distance by 0.06Å is obtained. The change of these parameters is associated with a considerable increase in the asymmetry and width of the Y–O pair distribution. Due to its size and charge, 6-fold coordinated Y will preferentially bond to non-bridging oxygens of the polymeric melt network to form a stable configuration, as is the case for the less polymerized melts with low ASI. In highly polymerized melts with ASI values close to one, 6-fold coordination of Y is not possible because almost only bridging oxygens are available. Consequently, over-bonding of bridging oxygens around Y is counterbalanced by an increase of coordination number and Y–O distance to satisfy local charge balance requirements.
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