Departamento de Químicas Física, Facultad de Ciencias, Universidad Complutense de Madrid, 28040, Madrid, Spain.
Phys Chem Chem Phys. 2011 Sep 28;13(36):16404-15. doi: 10.1039/c1cp21378d. Epub 2011 Aug 17.
The photodissociation of CH(3)I in the blue edge (217-230 nm) of the A-band has been studied using a combination of slice imaging and resonance enhanced multiphoton ionization (REMPI) detection of the CH(3) fragment in the vibrational ground state (ν = 0). The profiles of the CH(3) (ν = 0) kinetic energy distributions and the photofragment anisotropies are interpreted in terms of the contribution of the excited surfaces involved in the photodissociation process, as well as the probability of non-adiabatic curve crossing between the (3)Q(0) and (1)Q(1) states. In the studied region, unlike in the central part of the A-band where absorption to the (3)Q(0) state dominates, the I((2)P(J)), with J = 1/2, 3/2, in correlation with CH(3) (ν = 0) kinetic energy distributions show clearly two contributions of different anisotropy, signature of the competing adiabatic and non-adiabatic dynamics, whose ratio strongly depends on the photolysis wavelength. The experimental results are compared with multisurface wave packet calculations carried out using the available ab initio potential energy surfaces, transition moments, and non-adiabatic couplings, employing a reduced dimensionality model. A good qualitative agreement is found between experiment and theory and both show evidence of reverse (3)Q(0)←(1)Q(1) non-adiabatic dynamics at the bluest excitation wavelengths both in the fragment kinetic energy and angular distributions.
CH(3)I 在 A 带蓝边(217-230nm)的光解研究采用切片成像和共振增强多光子电离(REMPI)检测 CH(3)碎片在振动基态(ν=0)的方法。CH(3)(ν=0)的动能分布和光碎片各向异性的分布,通过参与光解过程的激发表面的贡献,以及(3)Q(0)和(1)Q(1)态之间非绝热曲线交叉的概率来解释。在研究区域中,与 A 带中心部分(3)Q(0)态吸收占主导地位不同,I((2)P(J)),其中 J=1/2,3/2,与 CH(3)(ν=0)动能分布相关,清楚地显示了两种不同各向异性的贡献,这是竞争的绝热和非绝热动力学的特征,其比值强烈依赖于光解波长。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,采用了降维模型。实验和理论之间存在很好的定性一致性,两者都表明在最蓝的激发波长下存在反向(3)Q(0)←(1)Q(1)非绝热动力学,这在碎片动能和角分布中都有体现。