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甲烷光解动力学的轨迹表面跳跃研究。

Trajectory surface-hopping study of methane photodissociation dynamics.

机构信息

Department of Chemistry, Northwestern University, Evanston, Illinois 60208-3113, USA.

出版信息

J Chem Phys. 2009 Dec 14;131(22):224320. doi: 10.1063/1.3271242.

Abstract

We use the fewest switches nonadiabatic trajectory surface hopping approach to study the photodissociation of methane on its lowest singlet excited state potential surface (1 (1)T(2)) at 122 nm, with emphasis on product state branching and energy partitioning. The trajectories and couplings are based on CASSCF(8,9) calculations with an aug-cc-pvdz basis set. We demonstrate that nonadiabatic dynamics is important to describe the dissociation processes. We find that CH(3)(X (2)A(2) ("))+H and CH(2)(a (1)A(1))+H(2) are the major dissociation channels, as have been observed experimentally. CH(3)+H is mostly formed by direct dissociation that is accompanied by hopping to the ground state. CH(2)+H(2) can either be formed by hopping to the ground state to give CH(2)(a (1)A(1))+H(2) or by adiabatic dissociation to CH(2)(b (1)B(1))+H(2). In the latter case, the CH(2)(b (1)B(1)) can then undergo internal conversion to the ground singlet state by Renner-Teller induced hopping. Less important dissociation mechanisms lead to CH(2)+H+H and to CH+H(2)+H. Intersystem crossing effects, which are not included, do not seem essential to describe the experimentally observed branching behavior. About 5% of trajectories involve a roaming atom mechanism which can eventually lead to formation of products in any of the dissociation channels. Branching fractions to give H and H(2) are in good agreement with experiment, and the H atom translational energy distribution shows bimodal character which also matches observations.

摘要

我们使用最少的开关非绝热轨迹表面跳跃方法来研究甲烷在其最低单重激发态势能面上(1 (1)T(2)) 在 122nm 处的光解,重点是产物态分支和能量分配。轨迹和耦合基于带有 aug-cc-pvdz 基组的 CASSCF(8,9) 计算。我们证明非绝热动力学对于描述解离过程很重要。我们发现 CH(3)(X (2)A(2) ("))+H 和 CH(2)(a (1)A(1))+H(2) 是主要的解离通道,这与实验观察到的结果一致。CH(3)+H 主要是通过直接解离形成的,同时伴随着跳跃到基态。CH(2)+H(2) 可以通过跳跃到基态形成 CH(2)(a (1)A(1))+H(2),也可以通过绝热解离形成 CH(2)(b (1)B(1))+H(2)。在后一种情况下,CH(2)(b (1)B(1)) 可以通过 Renner-Teller 诱导跳跃转化为基态单重态。不太重要的解离机制导致 CH(2)+H+H 和 CH+H(2)+H。未包括的系间窜越效应似乎对于描述实验观察到的分支行为不是必需的。大约 5%的轨迹涉及漫游原子机制,该机制最终可以导致任何解离通道中产物的形成。给出 H 和 H(2) 的分支分数与实验吻合较好,H 原子的平移能分布呈双峰特征,与观察结果一致。

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