Marggi Poullain Sonia, Chicharro David V, Zanchet Alexandre, González Marta G, Rubio-Lago Luis, Senent María L, García-Vela Alberto, Bañares Luis
Departamento de Química Física I, Facultad de Ciencias Químicas, Universidad Complutense de Madrid (Unidad Asociada I+D+i CSIC), 28040 Madrid, Spain.
Instituto de Física Fundamental, CSIC, C/Serrano, 123, 28006 Madrid, Spain.
Phys Chem Chem Phys. 2016 Jun 22;18(25):17054-61. doi: 10.1039/c6cp01558a.
The photodissociation dynamics of the methyl radical from the 3s and 3pz Rydberg states have been studied using the velocity map and slice ion imaging in combination with pump-probe nanosecond laser pulses. The reported translational energy and angular distributions of the H((2)S) photofragment detected by (2+1) REMPI highlight different dissociation mechanisms for the 3s and 3pz Rydberg states. A narrow peak in the translational energy distribution and an anisotropic angular distribution characterize the fast 3s photodissociation, while for the 3pz state Boltzmann-type translational energy and isotropic angular distributions are found. High level ab initio calculations have been performed in order to elucidate the photodissociation mechanisms from the two Rydberg states and to rationalize the experimental results. The calculated potential energy curves highlight a typical predissociation mechanism for the 3s state, characterized by the coupling between the 3s Rydberg state and a valence repulsive state. On the other hand, the photodissociation on the 3pz state is initiated by a predissociation process due to the coupling between the 3pz Rydberg state and a valence repulsive state and constrained, later on, by two conical intersections that allow the system to relax to lower electronic states. Such a mechanism opens up different reaction pathways leading to CH2 photofragments in different electronic states and inducing a transfer of energy between translational and internal modes.
利用速度成像和切片离子成像技术,结合泵浦-探测纳秒激光脉冲,研究了甲基自由基在3s和3pz里德堡态的光解离动力学。通过(2 + 1)共振增强多光子电离(REMPI)检测到的H((2)S)光碎片的平动能和角分布表明,3s和3pz里德堡态的解离机制不同。平动能分布中的一个窄峰和各向异性的角分布是快速3s光解离的特征,而对于3pz态,则发现了玻尔兹曼型平动能分布和各向同性的角分布。为了阐明这两个里德堡态的光解离机制并合理解释实验结果,进行了高水平的从头算计算。计算得到的势能曲线突出了3s态典型的预解离机制,其特征是3s里德堡态与一个价排斥态之间的耦合。另一方面,3pz态的光解离是由一个预解离过程引发的,该过程是由于3pz里德堡态与一个价排斥态之间的耦合,随后受到两个锥形交叉点的限制,这使得系统能够弛豫到较低的电子态。这种机制开辟了不同的反应途径,导致处于不同电子态的CH2光碎片,并在平动和内禀模式之间诱导能量转移。