Department of physics, Xiaogan University, Xiaogan City, Hubei Province, 432100, P. R. China.
J Phys Chem A. 2010 Jun 3;114(21):6188-93. doi: 10.1021/jp101260d.
Photodissociation dynamics of 2-bromopropane in the A band was investigated at several wavelengths between 232 and 267 nm using resonance-enhanced multiphoton ionization technique combined with velocity map ion-imaging detection. The ion images of Br ((2)P(3/2)) and Br* ((2)P(1/2)) were analyzed to yield corresponding total translational energy and angular distributions. The total translational energy distributions showed that the channel leading to Br carried more internal energy in the 2-C(3)H(7) moiety than the channel leading to Br*. The anisotropy parameters of beta (Br) were obtained to be between 0.68 and 1.49, and beta (Br*) between 0.73 and 1.96, indicating that the Br* product originates from direct excitation of the (3)Q(0) state and the (1)Q(1) --> (3)Q(0) nonadiabatic transition, and the Br product from direct excitation of the (1)Q(1) or (3)Q(1) state and the (3)Q(0) --> (1)Q(1) nonadiabatic transition. The curve crossing probabilities were determined to be increase with the wavelength. As compared with the case of CH(3)Br, the two heavier branched CH(3) groups significantly enhance the Br ((2)P(3/2)) production from nonadiabatic contribution. The curve crossing from the (3)Q(0) to the (1)Q(1) surface is much higher than that of the reverse from the (1)Q(1) to the (3)Q(0) surface, which may have resulted from the difference in shape between the potential energy surfaces of the (3)Q(0) and (1)Q(1) states. Finally, based on the experimental data, the partial absorption cross sections of the A band for the (3)Q(0), (3)Q(1), and (1)Q(1) states were extracted.
在 232nm 至 267nm 之间的几个波长处,使用共振增强多光子电离技术结合速度映射离子成像检测,研究了 A 带中 2-溴丙烷的光解动力学。分析 Br((2)P(3/2))和 Br*((2)P(1/2))的离子图像,得到相应的总平动能量和角分布。总平动能量分布表明,导致 Br 的通道在 2-C(3)H(7)部分具有比导致 Br的通道更多的内部能量。获得的 Br 的各向异性参数β(Br)在 0.68 到 1.49 之间,β(Br)在 0.73 到 1.96 之间,表明 Br*产物源自(3)Q(0)态的直接激发和(1)Q(1)-->(3)Q(0)非绝热跃迁,而 Br 产物源自(1)Q(1)或(3)Q(1)态的直接激发和(3)Q(0)-->(1)Q(1)非绝热跃迁。确定曲线交叉概率随波长增加而增加。与 CH(3)Br 的情况相比,两个较重的分支 CH(3)基团显著增强了来自非绝热贡献的 Br((2)P(3/2))的产生。从(3)Q(0)到(1)Q(1)表面的曲线交叉比从(1)Q(1)到(3)Q(0)表面的曲线交叉高得多,这可能是由于(3)Q(0)和(1)Q(1)态的势能面之间的形状差异所致。最后,基于实验数据,提取了 A 带中(3)Q(0)、(3)Q(1)和(1)Q(1)态的部分吸收截面。