Liu Shu, Chen Qun, Shao Kejie, Fu Bina, Zhang Dong H
State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences Dalian Liaoning 116023 China
University of Chinese Academy of Sciences Beijing 100049 China.
Chem Sci. 2025 Jul 10. doi: 10.1039/d5sc03277f.
Previous experimental and theoretical studies have shown that direct reactive systems typically exhibit backward-peaked differential cross sections (DCS) at relatively low collision energies, while complex-forming reactive systems tend to display forward-backward symmetric DCS. Is this a universal phenomenon in all direct reactions, especially those proceeding through non-collinear transition states? In this work, we developed the quantum wave packet method to calculate the full-dimensional state-to-state DCSs for the title exchange reaction with DO in the ground rovibrational state on a highly accurate neural network potential energy surface. For the first time, we obtain a sideward-scattered angle distribution just above the threshold, which directly reflects the C transition state geometry of this reaction. As the collision energy increases, the DCS broadens and undergoes a series of notable changes, culminating in the dominance of backward scattering at = 1.4 eV, accompanied by an early-sideward scattering peak. Although trajectory analysis can explain most of the DCS variations, significant differences persist between the quantum and quasiclassical trajectory DCSs, arising from quantum interference between the contributions from low and high partial waves. Additionally, the collision energy dependent DCSs at the scattering angle of 107° exhibit two clear step-like features around = 0.91 and 1.16 eV, which can be attributed to the shape resonance states trapped in the C well. In the energy region considered here, the majority of the available energy goes into the translational motion of the products, and the reaction exhibits low vibrational mode-specific behavior.
先前的实验和理论研究表明,直接反应体系通常在相对较低的碰撞能量下呈现后向峰值微分截面(DCS),而形成复合物的反应体系则倾向于表现出前后对称的DCS。这在所有直接反应中,尤其是那些通过非共线过渡态进行的反应中,是一种普遍现象吗?在这项工作中,我们开发了量子波包方法,以在高精度神经网络势能面上计算与处于基振转态的DO发生标题交换反应的全维态-态DCS。首次,我们获得了略高于阈值的侧向散射角分布,它直接反映了该反应的C过渡态几何结构。随着碰撞能量增加,DCS变宽并经历一系列显著变化,最终在碰撞能量为1.4 eV时后向散射占主导,同时伴有一个早期侧向散射峰。尽管轨迹分析可以解释大部分DCS变化,但量子和准经典轨迹DCS之间仍存在显著差异,这源于低部分波和高部分波贡献之间的量子干涉。此外,在散射角为107°时,依赖于碰撞能量的DCS在碰撞能量约为0.91和1.16 eV处呈现出两个明显的阶梯状特征,这可归因于被困在C阱中的形状共振态。在此处考虑的能量区域内,大部分可用能量进入产物的平动,并且该反应表现出低振动模式特异性行为。