Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, California 91125, USA.
J Phys Chem A. 2012 Jan 12;116(1):64-84. doi: 10.1021/jp2080379. Epub 2011 Dec 20.
The dynamics of O((3)P) + CO(2) collisions at hyperthermal energies were investigated experimentally and theoretically. Crossed-molecular-beams experiments at <E(coll)> = 98.8 kcal mol(-1) were performed with isotopically labeled (12)C(18)O(2) to distinguish products of nonreactive scattering from those of reactive scattering. The following product channels were observed: elastic and inelastic scattering ((16)O((3)P) + (12)C(18)O(2)), isotope exchange ((18)O + (16)O(12)C(18)O), and oxygen-atom abstraction ((18)O(16)O + (12)C(18)O). Stationary points on the two lowest triplet potential energy surfaces of the O((3)P) + CO(2) system were characterized at the CCSD(T)/aug-cc-pVTZ level of theory and by means of W4 theory, which represents an approximation to the relativistic basis set limit, full-configuration-interaction (FCI) energy. The calculations predict a planar CO(3)(C(2v), (3)A'') intermediate that lies 16.3 kcal mol(-1) (W4 FCI excluding zero point energy) above reactants and is approached by a C(2v) transition state with energy 24.08 kcal mol(-1). Quasi-classical trajectory (QCT) calculations with collision energies in the range 23-150 kcal mol(-1) were performed at the B3LYP/6-311G(d) and BMK/6-311G(d) levels. Both reactive channels observed in the experiment were predicted by these calculations. In the isotope exchange reaction, the experimental center-of-mass (c.m.) angular distribution, T(θ(c.m.)), of the (16)O(12)C(18)O products peaked along the initial CO(2) direction (backward relative to the direction of the reagent O atoms), with a smaller isotropic component. The product translational energy distribution, P(E(T)), had a relatively low average of <E(T)> = 35 kcal mol(-1), indicating that the (16)O(12)C(18)O products were formed with substantial internal energy. The QCT calculations give c.m. P(E(T)) and T(θ(c.m.)) distributions and a relative product yield that agree qualitatively with the experimental results, and the trajectories indicate that exchange occurs through a short-lived CO(3)* intermediate. A low yield for the abstraction reaction was seen in both the experiment and the theory. Experimentally, a fast and weak (16)O(18)O product signal from an abstraction reaction was observed, which could only be detected in the forward direction. A small number of QCT trajectories leading to abstraction were observed to occur primarily via a transient CO(3) intermediate, albeit only at high collision energies (149 kcal mol(-1)). The oxygen isotope exchange mechanism for CO(2) in collisions with ground state O atoms is a newly discovered pathway through which oxygen isotopes may be cycled in the upper atmosphere, where O((3)P) atoms with hyperthermal translational energies can be generated by photodissociation of O(3) and O(2).
在超热能量下,O((3)P) + CO(2) 碰撞的动力学通过实验和理论进行了研究。在 <E(coll)> = 98.8 kcal mol(-1) 下进行了具有同位素标记的 (12)C(18)O(2) 的交叉分子束实验,以区分非反应散射和反应散射的产物。观察到以下产物通道:弹性和非弹性散射 ((16)O((3)P) + (12)C(18)O(2))、同位素交换 ((18)O + (16)O(12)C(18)O) 和氧原子提取 ((18)O(16)O + (12)C(18)O)。在 CCSD(T)/aug-cc-pVTZ 理论水平和 W4 理论水平上,对 O((3)P) + CO(2) 体系的两个最低三重态势能表面上的驻点进行了表征,W4 理论代表了相对论基组极限的近似值,完全组态相互作用 (FCI) 能量。计算预测了一个平面 CO(3)(C(2v), (3)A'') 中间体,它位于反应物上方 16.3 kcal mol(-1)(W4 FCI 不包括零点能),并且通过能量为 24.08 kcal mol(-1) 的 C(2v) 过渡态接近。在 23-150 kcal mol(-1) 的碰撞能范围内进行了 B3LYP/6-311G(d) 和 BMK/6-311G(d) 水平的准经典轨迹 (QCT) 计算。实验中观察到的两种反应通道都被这些计算所预测。在同位素交换反应中,(16)O(12)C(18)O 产物的实验质心 (c.m.) 角分布 T(θ(c.m.)) 在初始 CO(2)方向(相对于试剂 O 原子的反方向)上呈峰值分布,具有较小的各向同性分量。产物平移能分布 P(E(T)) 的平均 <E(T)> = 35 kcal mol(-1) 相对较低,表明 (16)O(12)C(18)O 产物形成时具有大量的内部能量。QCT 计算给出了质心 P(E(T)) 和 T(θ(c.m.)) 分布以及相对产物产率,与实验结果定性一致,轨迹表明交换是通过短暂存在的 CO(3)* 中间体发生的。实验和理论都观察到提取反应的产率较低。在实验中,观察到来自提取反应的快速且微弱的 (16)O(18)O 产物信号,只能在正向检测到。观察到少量导致提取的 QCT 轨迹主要通过瞬态 CO(3)中间体发生,尽管仅在高碰撞能 (149 kcal mol(-1)) 下。CO(2)与基态 O 原子碰撞中的氧同位素交换机制是一种新发现的途径,通过这种途径,氧同位素可能在高层大气中循环,其中具有超热平移能的 O((3)P) 原子可以通过 O(3)和 O(2)的光解产生。