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首页> 外文期刊>International Journal of Quantum Chemistry >APPLICATIONS OF THE GROUP-FUNCTION THEORY TO THE FIELD OF MATERIALS SCIENCE [Review]
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APPLICATIONS OF THE GROUP-FUNCTION THEORY TO THE FIELD OF MATERIALS SCIENCE [Review]

机译:群函数理论在材料科学领域的应用[综述]

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The group-function theory, as proposed by McWeeny for the study of weak intermolecular interactions and developed by Huzinaga in the context of valence-electron methods, is shown to be applicable to the ab initio study of tunable solid-state laser materials made of defective ionic crystals. The applicability of the theory relies on the existence of local electronic states (to which the demonstrated/potential laser activity is ascribed), which are essentially localized in a small cluster of atoms including the defect and whose electron correlation interactions with the surrounding crystal components are negligible. According to the group-function formalism, it is possible (a) to neglect electron correlation effects beyond the defect cluster and (b) to define a quantum mechanical embedding potential which embodies the rest of the so-called host effects. Computationally, the theory becomes applicable as the embedding potential is approximated through ab initio model potentials (AIMP). The results of AIMP embedded-cluster calculations demonstrate that it is possible to calculate the local structure and spectroscopy of the active defect at an ab initio level, the attainable accuracy being comparable to the usual one in molecular ab initio studies in the gas phase. Also, in this article, we present a systematic study of the local distortions produced upon doping divalent first-series transition-metal ions in rock-salt oxides, MO:Me(2+) (M = Mg, Ca, Sr; Me = Sc-Zn) and Tl+ in KMgF3 and KF hosts. This study leads to the calculation of the local structures of the defects in these materials, which have not been measured. The results suggest that the use of the mismatch of the empirical ionic radii of the impurity and the substituted ion in order to predict local distortions in doped ionic crystals is not significant when it is smaller than 0.1 Angstrom, and when it is larger, it should be weighted by a reduction factor depending on the host. For the first-series divalent transition-metal ion impurities, this factor is shown to be 0.15 for SrO, 0.25 for CaO, and around 0.50 for MgO. (C) 1996 John Wiley & Sons, Inc. [References: 102]
机译:McWeeny提出的用于研究弱分子间相互作用的群函数理论,由Huzinaga在价电子方法的背景下提出,被证明可用于从头开始研究由缺陷制成的可调固态激光材料。离子晶体。该理论的适用性取决于局部电子状态的存在(归因于其所证明的/潜在的激光活性),该状态基本上位于包括缺陷的小原子簇中,并且其与周围晶体成分的电子相关性相互作用为微不足道。根据族函数形式主义,有可能(a)忽略缺陷簇以外的电子相关效应,以及(b)定义体现其余所谓主体效应的量子机械嵌入势。计算上,该理论变得适用,因为嵌入电位是通过从头算模型电位(AIMP)进行近似的。 AIMP嵌入式集群计算的结果表明,可以从头算级别计算活性缺陷的局部结构和光谱,可以达到的精度与气相分子从头算研究中的常规精度相当。同样,在本文中,我们对掺杂在盐岩氧化物MO:Me(2+)中的二价第一系列过渡金属离子产生的局部畸变进行了系统研究(M = Mg,Ca,Sr; Me = KMgF3和KF宿主中的Sc-Zn)和Tl +。这项研究导致对这些材料中尚未测量的缺陷局部结构的计算。结果表明,当杂质离子和取代离子的经验离子半径小于0.1埃时,使用杂质的经验离子半径的不匹配来预测掺杂离子晶体中的局部畸变并不重要。可以根据主机的减少因子进行加权。对于第一系列二价过渡金属离子杂质,该因数对于SrO而言显示为0.15,对于CaO而言为0.25,对于MgO而言约为0.50。 (C)1996 John Wiley&Sons,Inc. [参考:102]

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