Beijing National Laboratory of Molecular Sciences, State Key Laboratory of Molecular Reaction Dynamics, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, P. R. China.
J Phys Chem A. 2011 Feb 24;115(7):1153-60. doi: 10.1021/jp106624q. Epub 2011 Jan 27.
The photodissociation dynamics of CH(3)I from 277 to 304 nm is studied with our mini-TOF photofragment translational spectrometer. A single laser beam is used for both photodissociation of CH(3)I and REMPI detection of iodine. Many resolved peaks in each photofragment translational spectrum reveal the vibrational states of the CH(3) fragment. There are some extra peaks showing the existence of the hot-band states of CH(3)I. After careful simulation with consideration of the hot-band effect, the distribution of vibrational states of the CH(3) fragment is determined. The fraction σ of photofragments produced from the hot-band CH(3)I varies from 0.07 at 277.38 nm to 0.40 at 304.02 nm in the I* channel and from 0.05 at 277.87 nm to 0.16 at 304.67 nm in the I channel . E(int)/E(avl) of photofragments from ground-state CH(3)I remains at about 0.03 in the I* channel for all four wavelengths, but E(int)/E(avl) decreases from 0.09 at 277.87 nm to 0.06 at 304.67 nm in the I channel . From the ground-state CH(3)I, the quantum yield Φ(I*) is determined to be 0.59 at 277 nm and 0.05 at 304 nm. The curve-crossing probability P(cc) from the hot-band CH(3)I is lower than that from the ground-state CH(3)I. The potential energy at the curve-crossing point is determined to be 32,740 cm(-1).
用我们的微型飞行时间光碎片翻译谱仪研究了 277 到 304nm 之间的 CH(3)I 的光解动力学。一束激光同时用于 CH(3)I 的光解和碘的 REMPI 检测。每个光碎片翻译谱中的许多分辨峰揭示了 CH(3)碎片的振动状态。还有一些额外的峰显示了 CH(3)I 的热带态的存在。经过仔细的模拟,考虑到热带效应,确定了 CH(3)碎片的振动状态分布。在 I通道中,来自热带 CH(3)I 的光碎片的分数σ从 277.38nm 的 0.07 变化到 304.02nm 的 0.40,在 I 通道中,从 277.87nm 的 0.05 变化到 304.67nm 的 0.16。来自基态 CH(3)I 的光碎片的 E(int)/E(avl)在 I通道中所有四个波长下保持在约 0.03,但在 I 通道中从 277.87nm 的 0.09 下降到 304.67nm 的 0.06。从基态 CH(3)I 确定 Φ(I*)的量子产率为 277nm 时为 0.59,304nm 时为 0.05。来自热带 CH(3)I 的曲线交叉概率 P(cc)低于来自基态 CH(3)I 的曲线交叉概率。在曲线交叉点的势能确定为 32740cm(-1)。