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Computer simulation study of amorphous compounds: structural and vibrational properties

机译:非晶态化合物的计算机模拟研究:结构和振动特性

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Molecular dynamic (MD) simulations, both classical and ab initio, of amorphous GeO2 (germania), Al2O3 (alumina), and CdTeO compounds are presented. We focus our attention on the structural and vibrational properties, giving an atomic description of the short- and intermediate-range order. Amorphous germanium oxide under pressure was studied by means of classical MD simulations. At normal density, the analysis of the interatomic distances reveals that in the amorphous state there is a short-range order dominated by a slightly distorted (GeO4) tetrahedron. Beyond that, there is an intermediate-range order composed by vertex-sharing tetrahedra. As density increases, there is a structural transformation, from a short-range order defined by the basic tetrahedron to a basic octahedron. Consistent with this picture, the vibrational density of states also presents big changes, where the low frequency band shrinks, and the high frequency becomes wider and flatter. In the case of alumina, both classical and first principles MD calculations of amorphous Al2O3 are reported, comparing both methodologies. Interatomic correlations allow us to conclude that the short-range order is mainly composed by AlO4 tetrahedra, but in contrast to classical MD results, also an important number of AlO5 unit is present. The vibrational density of states presents two main bands, a low frequency one related to the inter-tetrahedron vibration and a high frequency band related to the intra-tetrahedron vibration. Finally, we present an ab initio MD calculation for the complex ternary material CdTeO3. According our calculations, the short-range order of this compound consists of a number of basic building blocks, greater than in the case of its crystalline counterpart. The compound is characterized using pair and angular distribution functions, coordination numbers, and a description of the molecular units of the compound. For example, Cd is coordinated by either six or five atoms. In the case of Te, the chemical unit is TeO3. The most frequent clusters are CdO6, CdO5, TeO3, and TeO4.
机译:非晶态GeO 2 (德国),Al 2 O 3 (氧化铝)的经典和从头算的分子动力学(MD)模拟,介绍了CdTeO化合物。我们将注意力集中在结构和振动特性上,对短程和中程顺序进行原子描述。通过经典的MD模拟研究了压力下的非晶态氧化锗。在正常密度下,原子间距离的分析表明,在非晶态下,存在一个短程有序的四面体,该四面体略微扭曲(GeO 4 )。除此之外,还有一个由顶点共享四面体组成的中间范围顺序。随着密度的增加,结构发生了变化,从基本四面体定义的短程有序转变为基本八面体。与这张图一致,状态的振动密度也呈现出很大的变化,即低频带缩小,而高频变得更宽,更平坦。对于氧化铝,报告了无定形Al 2 O 3 的经典和第一原理MD计算,并比较了两种方法。原子间的相关性使我们可以得出结论,短程顺序主要由AlO 4 四面体组成,但与经典的MD结果相反,AlO 5 单元也很重要存在。状态的振动密度呈现两个主要频带,一个与四面体间振动有关的低频频带和一个与四面体内振动有关的高频频带。最后,我们给出了复杂三元材料CdTeO 3 的从头算MD的计算。根据我们的计算,该化合物的短程顺序由许多基本结构单元组成,大于其晶体对应物。使用对和角分布函数,配位数和化合物分子单元的描述来表征化合物。例如,Cd由六个或五个原子配位。在Te的情况下,化学单元为TeO 3 。最常见的簇是CdO 6 ,CdO 5 ,TeO 3 和TeO 4

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