Hao Yusong, Zhou Chang, Mo Yuxiang
Department of Physics, Key Laboratory for Atomic and Molecular Nanosciences, Tsinghua University, Beijing 100084, China.
J Phys Chem A. 2007 Nov 1;111(43):10887-90. doi: 10.1021/jp074780a. Epub 2007 Oct 11.
We studied the ion-pair formation dynamics of F2 at 18.385 eV (67.439 nm) using the velocity map imaging method. It was found that there are two dissociation channels corresponding to production of F(+)((1)D(2)) + F(-)((1)S(0)) and F(+)((3)P(j)) + F(-)((1)S(0)). The measured center-of-mass translational energy distribution shows that about 98% of the dissociation occurs via the F(+)((1)D(2)) channel. The measured angular distributions of the photofragments indicate that dissociation for the F(+)((3)P(j)) channel occurs via predissociation of Rydberg states converging to F(2)(+)(A(2)Pi(u)) and dissociation for the F(+)((1)D(2)) channel involves mainly a direct perpendicular transition into the ion-pair state, or X(1)Sigma(g)(+) --> 2(1)Pi(u), which is also supported by the transition dipole moment calculations .
我们使用速度成像方法研究了18.385电子伏特(67.439纳米)下F2的离子对形成动力学。结果发现,存在两个分别对应于生成F(+)((1)D(2)) + F(-)((1)S(0))和F(+)((3)P(j)) + F(-)((1)S(0))的解离通道。测量得到的质心平动能量分布表明,约98%的解离通过F(+)((1)D(2))通道发生。光碎片的测量角分布表明,F(+)((3)P(j))通道的解离是通过收敛到F(2)(+)(A(2)Pi(u))的里德堡态预解离发生的,而F(+)((1)D(2))通道的解离主要涉及直接垂直跃迁到离子对态,即X(1)Sigma(g)(+) --> 2(1)Pi(u),这也得到了跃迁偶极矩计算的支持。