Hao Yusong, Zhou Chang, Mo Yuxiang
Department of Physics and Key Laboratory for Atomic and Molecular Nanosciences, Tsinghua University, Beijing 100084, China.
J Phys Chem A. 2009 Mar 19;113(11):2294-303. doi: 10.1021/jp8097878.
The ion-pair dissociation dynamics of Cl2 in the range 13.26-13.73 eV have been studied employing coherent extreme ultraviolet radiation (XUV) and the velocity map imaging method. The Cl- (1S(0)) ion-pair yield spectrum has been measured, and 80 velocity map images of Cl- (1S(0)) have been recorded for the strong peaks in the spectrum. From the images, two dissociation channels corresponding to Cl- (1S(0)) + Cl+ (3P(j)) and Cl- (1S(0)) + Cl+ (1D(2)) have been found. The branching ratios among the fragments Cl+ (3P(0,1)), Cl+ (3P(2)), and Cl+ (1D(2)) and their corresponding anisotropy parameters beta have been determined. It is concluded that the ion-pair dissociation occurs via the predissociation of Rydberg states and its dynamics strongly depend on the excitation energies. The perpendicular and parallel transitions correspond to the excitation to two major Rydberg series converging to ion-core Cl2+ (A2Pi(u)), ...sigma(g)2pi(u)3pi(g)4[A2Pi(u)]ns sigma(g), 1Pi(u) (n = 6,7), and ...sigma(g)2pi(u)3pi(g)4[A2Pi(u)]nd pi(g), 1Sigma(u)+ (n = 4,5), respectively. For the production of fragments Cl+ (1D(2)), it is proposed that the perpendicular transitions are from the excitation to Rydberg states [A2Pi(u)]ns sigma(g), 1Pi(u) that is predissociated by ion-pair state 2 1Pi(u), while the parallel transitions are from the excitation to [A2Pi(u)]nd pi(g), 1Sigma(u)+ that interacts with ion-pair states 0(u)+ (1D(2)), 0(u)+ (3P(2)), and 0(u)+ (3P(0)).
利用相干极紫外辐射(XUV)和速度成像方法研究了13.26 - 13.73 eV范围内Cl2的离子对解离动力学。测量了Cl- (1S(0))离子对产率谱,并针对谱中的强峰记录了80张Cl- (1S(0))的速度成像图。从这些图像中,发现了两个对应于Cl- (1S(0)) + Cl+ (3P(j))和Cl- (1S(0)) + Cl+ (1D(2))的解离通道。确定了碎片Cl+ (3P(0,1))、Cl+ (3P(2))和Cl+ (1D(2))之间的分支比及其相应的各向异性参数β。得出结论,离子对解离通过里德堡态的预解离发生,其动力学强烈依赖于激发能。垂直和平行跃迁分别对应于激发到两个主要的里德堡系列,它们汇聚到离子核Cl2+ (A2Pi(u)),...σg2πu3πg4[A2Pi(u)]nsσg,1Pi(u)(n = 6,7),以及...σg2πu3πg4[A2Pi(u)]ndπg,1Σu+(n = 4,5)。对于碎片Cl+ (1D(2))的产生,提出垂直跃迁是由激发到被离子对态2 1Pi(u)预解离的里德堡态[A2Pi(u)]nsσg,1Pi(u)引起的,而平行跃迁是由激发到与离子对态0(u)+ (1D(2))、0(u)+ (3P(2))和0(u)+ (3P(0))相互作用的[A2Pi(u)]ndπg,1Σu+引起的。