Sahoo Jayakrushna, Mahapatra S
School of Chemistry, University of Hyderabad, Hyderabad, 500 046, India.
Phys Chem Chem Phys. 2023 Oct 25;25(41):28309-28325. doi: 10.1039/d3cp02409a.
Out of the many major breakthroughs that the hydrogen-exchange reaction has led to, electronic nonadiabatic effects that are mainly due to the geometric phase has intrigued many. In this work we investigate such effects in the state-to-state dynamics of the H + H ( = 3, 4, = 0) → H (', ') + H reaction with a vibrationally excited reagent at energies corresponding to thermal conditions. The dynamical calculations are performed by a time-dependent quantum mechanical method both on the lower adiabatic potential energy surface (PES) and also using a two-states coupled diabatic theoretical model to explicitly include all the nonadiabatic couplings present in the 1' ground electronic manifold of the H system. The nonadiabatic couplings are considered here up to the quadratic term; however, the effect of the latter on the reaction dynamics is found to be very small. Adiabatic population analysis showed a minimal participation of the upper adiabatic surface even for the vibrationally excited reagent. A strong nonadiabatic effect appears in the state-to-state reaction probabilities and differential cross sections (DCSs). This effect is manifested as "out-of-phase" oscillations in the DCSs between the results of the uncoupled and coupled surface situations. The oscillations persist as a function of both scattering angle and collision energy in both the backward and forward scattering regions. The origins of these oscillations are examined in detail. The oscillations that appear in the forward direction are found to be different from those due to glory scattering, where the latter showed a negligibly small nonadiabatic effect. The nonadiabatic effects are reduced to a large extent when summed over all product quantum states, in addition to the cancellation due to integration over the scattering angle and partial wave summation.
在氢交换反应所带来的众多重大突破中,主要源于几何相位的电子非绝热效应引发了许多人的兴趣。在这项工作中,我们研究了在与热条件相对应的能量下,具有振动激发试剂的H + H( = 3, 4, = 0)→H (', ') + H反应的态对态动力学中的此类效应。动力学计算通过含时量子力学方法在较低绝热势能面(PES)上进行,并且还使用双态耦合 diabatic 理论模型来明确包含H系统1'基电子流形中存在的所有非绝热耦合。这里考虑非绝热耦合直至二次项;然而,发现后者对反应动力学的影响非常小。绝热布居分析表明,即使对于振动激发试剂,上绝热面的参与也极小。在态对态反应概率和微分截面(DCS)中出现了强烈的非绝热效应。这种效应表现为在未耦合和耦合表面情况的结果之间,DCS 中的“异相”振荡。在向后和向前散射区域中,这些振荡都作为散射角和碰撞能量的函数持续存在。详细研究了这些振荡的起源。发现在向前方向出现的振荡与由于荣耀散射引起的振荡不同,后者显示出可忽略不计的小非绝热效应。除了由于在散射角上的积分和分波求和导致的抵消之外,当对所有产物量子态求和时,非绝热效应在很大程度上减小。