首页> 外文期刊>The Journal of Chemical Physics >MULTISTATE VIBRONIC COUPLING EFFECTS IN THE K-SHELL EXCITATION SPECTRUM OF ETHYLENE - SYMMETRY BREAKING AND CORE-HOLE LOCALIZATION
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MULTISTATE VIBRONIC COUPLING EFFECTS IN THE K-SHELL EXCITATION SPECTRUM OF ETHYLENE - SYMMETRY BREAKING AND CORE-HOLE LOCALIZATION

机译:乙烯K壳激发谱中的多态强子耦合效应-对称破裂和孔局部化。

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The vibrational fine structure of the prominent C1s-pi* absorption band of ethylene and some of its isotopomers has been investigated theoretically with the aid of a specific (linear) vibronic coupling model. The presence of two equivalent C1s levels gives rise to two nearly degenerate electronic states of g and u symmetry, respectively, which can Interact vibronically via the (planar) antisymmetric C-H stretching and bending modes (nu(11) and nu(12)). In addition to these states of immediate interest, the present model comprises three more:pairs of ''effective'' states at higher energy allowing one to describe the excitation of additional asymmetric (nonplanar) modes as a result of linear vibronic coupling. To a good approximation the intrapair vibronic coupling can be eliminated by using a representation in terms of localized C1s hole states. As a further result, the in-plane and out-of-plane modes become separable. The required vibronic coupling constants have been determined with the aid of ab initio calculations at various nuclear conformations using a second-order polarization propagator method: After slight readjustment of some of the parameters, the calculated spectral profiles are found to be in excellent agreement with the experimental findings. The theoretical spectra reflect strong excitation of nontotally symmetric modes (and the concomitant symmetry lowering), involving mainly the planar C-H stretching mode nu(11) and the out-of-plane C-H bending mode nu(8). While the planar distortion is a consequence of the equivalent core levels, the nonplanar symmetry lowering can be rationalized in chemical terms as a rehybridization effect in which the sp(2) bonding scheme in the ethylene ground state is changed to sp(3) in the excited state. (C) 1997 American Institute of Physics. [References: 48]
机译:借助特定的(线性)振动耦合模型,对乙烯和其某些同分异构体的突出的C1s-pi *吸收带的振动精细结构进行了理论研究。两个等效C1s的存在分别引起g和u对称性的两个简并的电子态,它们可以通过(平面)反对称C-H拉伸和弯曲模式(nu(11)和nu(12))进行电子相互作用。除了这些令人关注的状态外,本模型还包括三对:在较高能量下的“有效”状态对,允许人们描述由于线性振动耦合而引起的其他非对称(非平面)模式的激发。可以通过使用表示局部C1s空穴状态的表示来消除对内的振动耦合。结果,平面内和平面外模式变得可分离。使用二阶极化传播器方法,通过从头算来确定各种核构象,确定了所需的振动耦合常数:在对某些参数进行稍许调整后,发现计算出的光谱轮廓与重整度非常吻合。实验结果。理论光谱反映了非完全对称模式的强烈激发(以及随之而来的对称性降低),主要涉及平面C-H拉伸模式nu(11)和面外C-H弯曲模式nu(8)。虽然平面变形是等效核心水平的结果,但非平面对称性降低可以通过化学术语合理化为再混合效应,其中乙烯基态的sp(2)键合方案在结构中变为sp(3)。兴奋的状态。 (C)1997美国物理研究所。 [参考:48]

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