CO2的c1s→nsσg Rydberg激发态中的振动耦合

IF 2.781
Jun-ichi Adachi, Nobuhiro Kosugi, Eiji Shigemasa, Akira Yagishita
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引用次数: 30

摘要

在相对于线偏振光电矢量的90°和0°方向上,测量了CO2的c1s→Rydberg激发区的片段离子产率。c1s→ns (n = 3,4), npπ和npσ (n = 3?7),和nd (n = 3,4) Rydberg跃迁均表现出明显的振动结构。偶极禁止的c1s (σg)→3sσg Rydberg转变是所有Rydberg转变中最强的,90°方向的离子产额占主导地位。这表明弯曲振动主要与3sσg里德伯态耦合,并且借给强度的偶极子允许态是很强的π*共振,仅比3sσg态低2 eV。另一方面,在4sσg Rydberg态中,通过反对称拉伸模式在0°方向上观察到强烈的振动耦合。这可能是因为4sσg状态接近另一个具有Σu+对称性的借给强度状态,并且远离π*共振。角分辨离子产额技术是研究振动耦合机理的有力手段。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Vibronic Couplings in the C 1s → nsσg Rydberg Excited States of CO2

Fragment ion yields in the C 1s → Rydberg excitation region of CO2 were measured in the 90° and 0° directions relative to the electric vector of the linearly polarized light. The C 1s → ns (n = 3, 4), npπ and npσ (n = 3?7), and nd (n = 3, 4) Rydberg transitions are clearly observed and show some vibrational structures. The dipole-forbidden C 1s(σg) → 3sσg Rydberg transition is the strongest of all the Rydberg transitions, and the ion yield in the 90° direction is dominant. This indicates that the bending vibration is predominantly coupled with the 3sσg Rydberg state and the intensity-lending dipole-allowed state is a very strong π* resonance, only 2 eV lower than the 3sσg state. On the other hand, in the 4sσg Rydberg state the vibronic coupling through the antisymmetric stretching mode is strongly observed in the 0° direction. This is probably because the 4sσg state approaches another intensity-lending state with Σu+ symmetry and goes away from the π* resonance. The angle-resolved ion-yield technique is very powerful for elucidating the vibronic coupling mechanism.

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