Department of Chemistry, University of Pennsylvania, Philadelphia, Pennsylvania 19104-6323, USA.
J Chem Phys. 2011 Oct 14;135(14):144303. doi: 10.1063/1.3644763.
The H- and D-atom products from collisional quenching of OD A (2)Σ(+) by H(2) are characterized through Doppler spectroscopy using two-photon (2 (2)S ←← 1 (2)S) laser-induced fluorescence. Partial deuteration enables separation of the channel forming H + HOD products, which accounts for 75% of reactive quenching events, from the D + H(2)O product channel. The Doppler profiles, along with those reported previously for other isotopic variants, are transformed into product translational energy distributions using a robust fitting procedure based on discrete velocity basis functions. The product translational energy distribution for the H-atom channel is strongly peaked at low energy (below 0.5 eV) with a long tail extending to the energetic limit. By contrast, the D-atom channel exhibits a small peak at low translational energy with a distinctive secondary peak at higher translational energy (approximately 1.8 eV) before falling off to higher energy. In both cases, most of the available energy flows into internal excitation of the water products. Similar distributions are obtained upon reanalysis of D- and H-atom Doppler profiles, respectively, from reactive quenching of OH A (2)Σ(+) by D(2). The sum of the translational energy distributions for H- and D-atom channels is remarkably similar to that obtained for OH A (2)Σ(+) + H(2), where the two channels cannot be distinguished from one another. The product translational energy distributions from reactive quenching are compared with those obtained from a previous experiment performed at higher collision energy, quasiclassical trajectory calculations of the post-quenching dynamics, and a statistical model.
通过双光子(2²S ←← 1²S)激光诱导荧光的多普勒光谱学,对 OD A(2)Σ(+)与 H2 的碰撞猝灭产生的 H 和 D 原子产物进行了表征。部分氘化使得可以将形成 H + HOD 产物的通道与 D + H2O 产物通道分离,这占反应猝灭事件的 75%。多普勒轮廓以及以前报道的其他同位素变体的轮廓,使用基于离散速度基函数的强大拟合程序转化为产物平移能分布。H-原子通道的产物平移能分布在低能量(低于 0.5 eV)下强烈集中,长尾延伸到能量极限。相比之下,D-原子通道在低平移能下表现出一个小峰,在更高的平移能(约 1.8 eV)下有一个独特的次峰,然后在更高的能量下下降。在这两种情况下,大部分可用能量都流入水产物的内部激发。对 OH A(2)Σ(+)与 D2 的反应猝灭的 D-和 H-原子多普勒轮廓分别进行重新分析时,也得到了类似的分布。H-和 D-原子通道的平移能分布之和与 OH A(2)Σ(+)+ H2 获得的分布非常相似,其中两个通道无法相互区分。反应猝灭产生的产物平移能分布与以前在更高碰撞能下进行的实验、后猝灭动力学的准经典轨迹计算和统计模型的结果进行了比较。