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可见光光解 CO 二聚体阳离子:激发态中的快速和慢速离解动力学。

Visible photodissociation of the CO dimer cation: fast and slow dissociation dynamics in the excited state.

机构信息

Department of Chemistry, Graduate School of Science, Tohoku University, 6-3 Aoba, Aramaki, Aoba-ku, Sendai 980-8578, Japan.

出版信息

Phys Chem Chem Phys. 2019 Feb 6;21(6):3083-3091. doi: 10.1039/c8cp07068g.

Abstract

Velocity and angular distributions of photofragment CO2+ ions produced from mass-selected (CO2)2+ at 532 nm excitation were observed in an ion imaging experiment. The velocity distribution was assigned to two components, fast and slow velocity components, which was consistent with the previous study by Bowers et al. The anisotropy parameters of the angular distributions for the fast and slow velocity components were experimentally determined to be βfast = 1.52 ± 0.14 and βslow = 0.46 ± 0.10, respectively. In the theoretical approach, potential energy surfaces (PESs) of (CO2)2+ were calculated along two coordinates, the intermolecular distance and mutual orientations of the CO2 monomers. In addition, molecular dynamics simulations were performed. The visible transition of the most stable staggered structure of (CO2)2+ was attributed to C[combining tilde]2Ag ← X[combining tilde]2Bu by an excited state calculation. On the PES of the C[combining tilde] state, a potential well was found in which the two CO2 monomers lay side by side to each other, in addition to a repulsive slope along the intermolecular distance. The results of the simulations confirmed that the fragment CO2+ ions with fast velocity and large anisotropy originated from the rapid dissociation of (CO2)2+ on the repulsive slope. Meanwhile, the fragment CO2+ ions with slow velocity and small anisotropy were expected to emerge from statistical dissociation after large amplitude libration of CO2 molecules which was caused by the potential well in the excited state PES.

摘要

在离子成像实验中,观察到在 532nm 激发下从质量选择的 (CO2)2+ 产生的光碎片 CO2+ 离子的速度和角分布。速度分布被分配为两个分量,快和慢速度分量,这与 Bowers 等人的先前研究一致。快和慢速度分量的角分布各向异性参数通过实验确定为 βfast = 1.52 ± 0.14 和 βslow = 0.46 ± 0.10。在理论方法中,沿着两个坐标,分子间距离和 CO2 单体的相互取向,计算了 (CO2)2+ 的势能面 (PES)。此外,还进行了分子动力学模拟。(CO2)2+ 的最稳定交错结构的可见跃迁归因于通过激发态计算的 C[combining tilde]2Ag ← X[combining tilde]2Bu。在 C[combining tilde] 态的 PES 上,发现了一个势能阱,其中两个 CO2 单体彼此并排排列,此外还有沿着分子间距离的排斥斜率。模拟结果证实,具有快速速度和大各向异性的碎片 CO2+ 离子源自 (CO2)2+ 在排斥斜率上的快速解离。同时,具有慢速度和小各向异性的碎片 CO2+ 离子预计将在 CO2 分子的大振幅摆动后从统计解离中出现,这是由激发态 PES 中的势能阱引起的。

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