Departamento de Química Física I, Facultad de Ciencias Químicas, Universidad Complutense de Madrid, Madrid 28040, Spain.
J Chem Phys. 2009 Nov 7;131(17):174309. doi: 10.1063/1.3257692.
The photodissociation of methyl iodide at different wavelengths in the red edge of the A-band (286-333 nm) has been studied using a combination of slice imaging and resonance enhanced multiphoton ionization detection of the methyl fragment in the vibrational ground state (nu=0). The kinetic energy distributions (KED) of the produced CH(3)(nu=0) fragments show a vibrational structure, both in the I((2)P(3/2)) and I( *)((2)P(1/2)) channels, due to the contribution to the overall process of initial vibrational excitation in the nu(3)(C-I) mode of the parent CH(3)I. The structures observed in the KEDs shift toward upper vibrational excited levels of CH(3)I when the photolysis wavelength is increased. The I((2)P(3/2))/I( *)((2)P(1/2)) branching ratios, photofragment anisotropies, and the contribution of vibrational excitation of the parent CH(3)I are explained in terms of the contribution of the three excited surfaces involved in the photodissociation process, (3)Q(0), (1)Q(1), and (3)Q(1), as well as the probability of nonadiabatic curve crossing (1)Q(1)<--(3)Q(0). The experimental results are compared with multisurface wave packet calculations carried out using the available ab initio potential energy surfaces, transition moments, and nonadiabatic couplings, employing a reduced dimensionality (pseudotriatomic) model. A general qualitative good agreement has been found between theory and experiment, the most important discrepancies being in the I((2)P(3/2))/[I((2)P(3/2))+I( *)((2)P(1/2))] branching ratios. Inaccuracies of the available potential energy surfaces are the main reason for the discrepancies.
在 A 带(286-333nm)的红边,不同波长的碘化甲烷的光解已通过切片成像和共振增强多光子电离检测振动基态(nu=0)中的甲基片段的方法进行了研究。由于初始振动激发在母体 CH3I 的 nu(3)(C-I)模式下对整个过程的贡献,所产生的 CH(3)(nu=0)碎片的动能分布(KED)在 I((2)P(3/2))和 I( *)((2)P(1/2))通道中均显示出振动结构。当光解波长增加时,在 KED 中观察到的结构向 CH3I 的上振动激发能级移动。I((2)P(3/2))/I( *)((2)P(1/2))分支比、光碎片各向异性以及母体 CH3I 振动激发的贡献可以根据光解过程中涉及的三个激发表面(3)Q(0)、(1)Q(1)和(3)Q(1)以及非绝热曲线交叉(1)Q(1)<--(3)Q(0)的概率来解释。实验结果与使用可用从头算势能面、跃迁矩和非绝热耦合进行的多表面波包计算进行了比较,采用了简化的维度(拟三原子)模型。理论与实验之间存在很好的定性一致性,最重要的差异在于 I((2)P(3/2))/[I((2)P(3/2))+I( *)((2)P(1/2))]分支比。可用势能面的不准确性是差异的主要原因。