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Polyad quantum numbers and multiple resonances in anharmonic vibrational studies of polyatomic molecules

机译:多原子分子非谐振动研究中的双原子量子数和多重共振

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In the theory of anharmonic vibrations of a polyatomic molecule, mixing the zero-order vibrational states due to cubic, quartic and higher-order terms in the potential energy expansion leads to the appearance of more-or-less isolated blocks of states (also called polyads), connected through multiple resonances. Such polyads of states can be characterized by a common secondary integer quantum number. This polyad quantum number is defined as a linear combination of the zero-order vibrational quantum numbers, attributed to normal modes, multiplied by non-negative integer polyad coefficients, which are subject to definition for any particular molecule. According to Kellman's method [J. Chem. Phys. 93, 6630 (1990)], the corresponding formalism can be conveniently described using vector algebra. In the present work, a systematic consideration of polyad quantum numbers is given in the framework of the canonical Van Vleck perturbation theory (CVPT) and its numerical-analytic operator implementation for reducing the Hamiltonian to the quasi-diagonal form, earlier developed by the authors. It is shown that CVPT provides a convenient method for the systematic identification of essential resonances and the definition of a polyad quantum number. The method presented is generally suitable for molecules of significant size and complexity, as illustrated by several examples of molecules up to six atoms. The polyad quantum number technique is very useful for assembling comprehensive basis sets for the matrix representation of the Hamiltonian after removal of all non-resonance terms by CVPT. In addition, the classification of anharmonic energy levels according to their polyad quantum numbers provides an additional means for the interpretation of observed vibrational spectra.
机译:在多原子分子的非谐振动理论中,由于势能扩展中的立方,四次和更高阶项引起的零阶振动态的混合会导致出现或多或少的孤立状态块的出现(也称为双元共聚物),通过多个共振连接。这种状态的多元单元可以通过共同的次级整数量子数来表征。该多态量子数被定义为归因于正常模式的零级振动量子数的线性组合乘以非负整数多态性系数,该系数取决于任何特定分子的定义。根据凯尔曼的方法[J.化学物理93,6630(1990)],可以使用向量代数方便地描述相应的形式主义。在目前的工作中,在规范的范弗雷克微扰理论(CVPT)及其数值分析算子实现框架中,系统地考虑了多元子数,作者将其简化为准对角线形式。 。结果表明,CVPT为系统地识别基本共振和定义多元量子数提供了一种便捷的方法。所提出的方法通常适用于具有较大大小和复杂性的分子,如最多六个原子的分子的几个示例所示。在通过CVPT去除所有非共振项后,polyad量子数技术对于组装用于哈密顿量的矩阵表示的综合基础集非常有用。此外,根据非谐能级的多态量子数对其进行分类,为解释观测到的振动光谱提供了另一种手段。

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