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193纳米波长下丙炔的光解离动力学:轨迹表面跳跃研究

Photodissociation dynamics of propyne at 193 nm: a trajectory surface hopping study.

作者信息

Ghosh Subhendu, Rauta Akshaya Kumar, Maiti Biswajit

机构信息

Department of Chemistry, Institute of Science, Banaras Hindu University, Varanasi 221005, India.

出版信息

Phys Chem Chem Phys. 2016 Mar 21;18(11):8219-27. doi: 10.1039/c5cp07502e.

DOI:10.1039/c5cp07502e
PMID:26928947
Abstract

Photodissociation dynamics of propyne at 193 nm are studied using the fewest switches nonadiabatic trajectory surface hopping method on its first excited singlet electronic state (1(1)A''). The trajectories are propagated based on potential energies, gradients and nonadiabatic couplings calculated at the MRCIS(6,7) level with the 6-31++G(d,p) basis set. Our trajectory calculations have revealed that H + H3CCC is the major dissociation channel, which has also been predicted experimentally. For the primary photodissociation channel H + H3CCC we demonstrate that nonadiabatic dynamics do not play a significant role. This observation is however contradictory to most of the previously reported experimental predictions. The calculated product translation energy distribution for the acetylenic H atom elimination peaked at ∼ 18 kcal mol(-1), indicating that the dissociation occurs adiabatically on a moderately repulsive excited surface that correlates with the ground state products (CH3C ≡ C + H). The H atom elimination process from the methyl fragment involving a transition state, which has to compete with the acetylenic H atom dissociation channel with no barrier in the excited singlet surface, was found to be too less probable to make a contribution to product branching. We observed that a fewer but significant number of trajectories led to CH3 + CCH product formation which has not been observed experimentally when propyne is excited at 193 nm.

摘要

采用最少开关非绝热轨迹表面跳跃方法,在丙炔的第一激发单重态电子态(1(1)A'')上研究了其在193 nm处的光解离动力学。轨迹基于在MRCIS(6,7)水平并使用6-31++G(d,p)基组计算得到的势能、梯度和非绝热耦合进行传播。我们的轨迹计算表明,H + H3CCC是主要的解离通道,这也已通过实验预测到。对于主要的光解离通道H + H3CCC,我们证明非绝热动力学并不起显著作用。然而,这一观察结果与大多数先前报道的实验预测相矛盾。计算得到的炔氢原子消除的产物平动能分布在~18 kcal mol(-1)处达到峰值,表明解离是在与基态产物(CH3C≡C + H)相关的适度排斥激发表面上绝热发生的。发现从甲基片段消除氢原子的过程涉及一个过渡态,该过渡态必须与激发单重态表面上无势垒的炔氢原子解离通道竞争,其可能性太小以至于对产物分支没有贡献。我们观察到,当丙炔在193 nm处被激发时,有较少但数量可观的轨迹导致了CH3 + CCH产物的形成,而这在实验中尚未观察到。

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