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16.25 - 16.41电子伏特能量范围内N₂O的离子对解离:动力学与电子结构

Ion-pair dissociation of N2O in the 16.25-16.41 eV: dynamics and electronic structure.

作者信息

Zhou Chang, Mo Yuxiang

机构信息

Department of Physics and Key Laboratory for Atomic and Molecular Nanosciences, Tsinghua University, Beijing, 100084, China.

出版信息

J Chem Phys. 2008 Aug 14;129(6):064312. doi: 10.1063/1.2965593.

Abstract

The ion-pair dissociation dynamics of N(2)O -->(XUV) N(2)(+)(X (2)Sigma(g)(+), v) + O(-)((2)P(j)) at 16.248, 16.271, 16.389, and 16.411 eV have been studied using the velocity map imaging method and tunable XUV laser. The electronic structures of the ion-pair states have been studied by employing the ab initio quantum chemical calculation. The translational energy distributions and the angular distributions of the photofragments have been measured. The results show that about 40% of available energies are transformed into the translational energies, and the first excited vibrational states are populated most strongly for all four excitation energies. The anisotropy parameters beta are approximately 1. The ab initio calculations at the level of CASSCF6-311++g(3df) show that the equilibrium geometries of the ion-pair states are nonlinear with bond lengths R(N-N) = 1.10 A, R(N-O) = 2.15 A, and bond angle N-N-O = 103 degrees, respectively. The ion-pair states are formed by electron migration from the bonding sigma orbital of N[triple bond]N to the antibonding sigma orbital localized primarily on the O atom. Combining the experimental and theoretical results, it is concluded that the ion-pair dissociation occurs via predissociation of Rydberg states with (1)Sigma(+) symmetry, which converges to the ion-core N(2)O(+)(A (2)Sigma(+)).

摘要

利用速度成像方法和可调谐极紫外激光,研究了在16.248、16.271、16.389和16.411电子伏特能量下N(2)O -->(极紫外) N(2)(+)(X (2)Σg(+), v) + O(-)((2)P(j))的离子对解离动力学。采用从头算量子化学计算研究了离子对态的电子结构。测量了光碎片的平动能分布和角分布。结果表明,约40%的可用能量转化为平动能,并且在所有四种激发能量下,第一激发振动态的布居最为强烈。各向异性参数β约为1。在CASSCF6-311++g(3df)水平的从头算计算表明,离子对态的平衡几何结构是非线性的,键长R(N-N) = 1.10 Å,R(N-O) = 2.15 Å,键角N-N-O = 103°。离子对态是通过电子从N≡N的成键σ轨道迁移到主要定域在O原子上的反键σ轨道而形成的。结合实验和理论结果,得出离子对解离是通过具有(1)Σ+对称性的里德堡态预解离发生的,该态收敛到离子核N(2)O(+)(A (2)Σ+)。

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