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Photodissociation Dynamics of 2-Bromopropane Using Velocity Map Imaging Technique

机译:速度图成像技术研究2-溴丙烷的光解离动力学

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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 (~2P_(3/2)) and Br* (~2P_(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_3H_7 moiety than the channel leading to Br*. The anisotropy parameters of β (Br) were obtained to be between 0.68 and 1.49, and β (Br*) between 0.73 and 1.96, indicating that the Br* product originates from direct excitation of the ~3Q_0 state and the ~1Q_1 → ~3Q_0 nonadiabatic transition, and the Br product from direct excitation of the ~1Q_1 or ~3Q_1 state and the ~3Q_0 → ~1Q_1 nonadiabatic transition. The curve crossing probabilities were determined to be increase with the wavelength. As compared with the case of CH_3Br, the two heavier branched CH_3 groups significantly enhance the Br (~2P_(3/2)) production from nonadiabatic contribution. The curve crossing from the ~3Q_0 to the ~1Q_1 surface is much higher than that of the reverse from the ~1Q_1 to the ~3Q_0 surface, which may have resulted from the difference in shape between the potential energy surfaces of the ~3Q_0 and ~1Q_1 states. Finally, based on the experimental data, the partial absorption cross sections of the A band for the ~3Q_0, ~3Q_1, and ~1Q_1 states were extracted.
机译:使用共振增强多光子电离技术结合速度图离子成像检测技术,研究了在232和267 nm之间的多个波长下,A波段2-溴丙烷的光解离动力学。分析了Br(〜2P_(3/2))和Br *(〜2P_(1/2))的离子图像,以产生相应的总平移能和角度分布。总的平移能分布表明,导致Br的通道在2-C_3H_7部分携带的内部能量比导致Br *的通道更多。获得的β(Br)的各向异性参数在0.68至1.49之间,并且β(Br *)在0.73至1.96之间,表明Br *产物源自〜3Q_0状态和〜1Q_1→〜3Q_0的直接激发。非绝热跃迁,以及〜1Q_1或〜3Q_1状态和〜3Q_0→〜1Q_1非绝热跃迁的直接激发产生的Br产物。确定曲线交叉概率随波长增加。与CH_3Br的情况相比,两个较重的支链CH_3基团显着增强了非绝热作用产生的Br(〜2P_(3/2))。从〜3Q_0到〜1Q_1表面的曲线比从〜1Q_1到〜3Q_0表面的曲线高得多,这可能是由〜3Q_0和〜的势能面之间的形状差异引起的。 1Q_1状态。最后,根据实验数据,提取了〜3Q_0,〜3Q_1和〜1Q_1状态的A波段的部分吸收截面。

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