Smolin Andrey G, Vasyutinskii Oleg S, Vieuxmaire Olivier P J, Ashfold Michael N R, Balint-Kurti Gabriel G, Orr-Ewing Andrew J
Ioffe Physico-Technical Institute, Russian Academy of Sciences, 194021 Saint Petersburg, Russia.
J Chem Phys. 2006 Mar 7;124(9):94305. doi: 10.1063/1.2168149.
Resonance-enhanced multiphoton ionization and velocity map imaging of the Cl(2P(3/2)0) fragments of BrCl photolysis at 467.16 nm have been used to obtain a complete set of orientation parameters (with ranks K = 1 and 3) describing the polarization of the electronic angular momentum. The experiments employ two geometries distinguished only by the circular or linear polarization of the photolysis laser beam. Normalized difference images constructed from the data accumulated using a right or left circularly polarized probe-laser beam, counterpropagating with the photolysis laser, were fitted to basis images corresponding to contributions from various odd-rank anisotropy parameters. Expressions are given for the difference images in terms of the K = 1 and 3 anisotropy parameters, which describe coherent and incoherent parallel and perpendicular excitation and dissociation mechanisms. The nonzero values of the anisotropy parameters are indicative of nonadiabatic dissociation dynamics, with likely contributions from flux on the A 3Pi1,B 3Pi(0+),C 1Pi1, and X 1sigma+(0+) states as well as one further omega = 1 state, all of which correlate adiabatically to Cl(2P(3/2)0) + Br(2P(3/2)0) photofragments. The magnitudes of the parameters depend both on the amplitudes of dissociative flux in these states, and also on the phases accumulated by the nuclear wave functions for different dissociation pathways.
利用在467.16 nm处BrCl光解产生的Cl(2P(3/2)0)碎片的共振增强多光子电离和速度映射成像,获得了一套完整的描述电子角动量极化的取向参数(秩K = 1和3)。实验采用了两种仅由光解激光束的圆偏振或线偏振区分的几何构型。由使用与光解激光反向传播的右旋或左旋圆偏振探测激光束积累的数据构建的归一化差分图像,被拟合到对应于各种奇秩各向异性参数贡献的基图像。给出了用K = 1和3各向异性参数表示的差分图像的表达式,这些参数描述了相干和非相干的平行和垂直激发及解离机制。各向异性参数的非零值表明非绝热解离动力学,可能来自A 3Pi1、B 3Pi(0+)、C 1Pi1和X 1sigma+(0+)态以及另一个ω = 1态上的通量贡献,所有这些态都绝热关联到Cl(2P(3/2)0) + Br(2P(3/2)0)光碎片。这些参数的大小既取决于这些态中解离通量的幅度,也取决于不同解离途径的核波函数积累的相位。