Tossell J A, Horbach J
Department of Chemistry and Biochemistry, University of Maryland, College Park, Maryland 20742, USA.
J Phys Chem B. 2005 Feb 10;109(5):1794-7. doi: 10.1021/jp0454873.
The (17)O NMR spectrum of CaAl(2)Si(2)O(8) glass shows two types of O sites that are not present in the crystalline material. One of these, with (17)O NMR parameters C(Q) = 2.3 MHz and delta = +20 ppm, has been assigned to a "tricluster" O, a local geometry in which the O is coordinated to three tetrahedrally coordinated atoms, either Al or Si. For crystalline CaAl(4)O(7), a tricluster site (with three Al linkages to O, i.e., OAl(3)) has been characterized experimentally, with a C(Q) of 2.5 MHz and a delta of about +40 ppm. Thus, a C(Q) value of 2.5 MHz or less seems to be a characteristic of such sites, although they may show a range of delta values. However, several different quantum chemical cluster calculations employing energy-optimized geometries for various tricluster species have given C(Q) values considerably larger than that seen experimentally in the CaAl(2)Si(2)O(8) glass (with minimum C(Q) values of 3.0 MHz even for all Al species). We have recently shown that for edge-sharing geometries, in which the tricluster O atoms participate in "two-membered rings" of composition Al(2)O(2), the calculated C(Q) values are considerably lower, in the range identified in the glass. However, such two-membered ring geometries had been observed only in crystalline inorganic alumoxanes. Ab initio MD calculations on related compositions, such as the calcium aluminosilicate, CAS, (CaO)(0.21)(Al(2)O(3))(0.12)(SiO(2))(0.67), show a small percentage of O triclusters, but none in two-membered rings of the Al(2)O(2) type, and the calculated C(Q) values for the triclusters that do exist are higher than seen in the original experiments on CaAl(2)Si(2)O(8) glass and not significantly different from those for two-coordinate O in Si-O-Al sites. However, a classical MD simulation of the structure of glassy aluminum silicate AS2, (Al(2)O(3))2(SiO(2)), gave a predominance of O triclusters within two-membered rings, with structures much like those seen in the alumoxanes. We have now calculated (17)O nuclear quadrupole coupling constants and NMR shielding values for clusters extracted from these simulations, using standard quantum chemical methods. The calculated C(Q) values for these O triclusters are now in the range observed experimentally in the CaAl(2)Si(2)O(8) glass (around 2.3-2.6 MHz) when the tricluster O is surrounded by three Al, two of which are part of an Al(2)O(2) ring. This supports the experimentalists' contention that such tricluster O species do exist and have been seen by (17)O NMR.
CaAl₂Si₂O₈玻璃的¹⁷O NMR谱显示出两种在晶体材料中不存在的氧位点。其中一种,¹⁷O NMR参数C(Q) = 2.3 MHz且δ = +20 ppm,已被归为“三簇”氧,即一种局部几何结构,其中氧与三个四面体配位原子(Al或Si)配位。对于晶体CaAl₄O₇,已通过实验表征了一个三簇位点(氧与三个Al相连,即OAl₃),其C(Q)为2.5 MHz,δ约为 +40 ppm。因此,C(Q)值为2.5 MHz或更低似乎是此类位点的一个特征,尽管它们可能表现出一系列的δ值。然而,针对各种三簇物种采用能量优化几何结构进行的几种不同的量子化学簇计算给出的C(Q)值比在CaAl₂Si₂O₈玻璃中实验观察到的要大得多(即使对于所有Al物种,最小C(Q)值为3.0 MHz)。我们最近表明,对于三簇氧原子参与组成Al₂O₂的“二元环”的边共享几何结构,计算出的C(Q)值要低得多,处于在玻璃中确定的范围内。然而,这种二元环几何结构仅在晶体无机铝氧烷中被观察到。对相关组成(如钙铝硅酸盐,CAS,(CaO)₀.₂₁(Al₂O₃)₀.₁₂(SiO₂)₀.₆₇)进行的从头算分子动力学计算显示,只有一小部分氧三簇,但没有Al₂O₂型二元环中的氧三簇,并且对于确实存在的三簇计算出的C(Q)值高于在CaAl₂Si₂O₈玻璃的原始实验中观察到的值,并且与Si - O - Al位点中双配位氧的值没有显著差异。然而,对玻璃态硅酸铝AS2,(Al₂O₃)₂(SiO₂)结构进行的经典分子动力学模拟表明,二元环内的氧三簇占主导,其结构与在铝氧烷中看到的非常相似。我们现在使用标准量子化学方法计算了从这些模拟中提取的簇的¹⁷O核四极耦合常数和NMR屏蔽值。当三簇氧被三个Al包围,其中两个是Al₂O₂环的一部分时,这些氧三簇计算出的C(Q)值现在处于在CaAl₂Si₂O₈玻璃中实验观察到的范围内(约2.3 - 2.6 MHz)。这支持了实验者的观点,即这种三簇氧物种确实存在并且已通过¹⁷O NMR观察到。