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A photodissociation study of CH2BrCl in the A-band using the time-sliced ion velocity imaging method

机译:时分离子速度成像法研究A波段CH2BrCl的光解离

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Employing a high-resolution (velocity resolution Delta nuu < 1.5%) time-sliced ion velocity imaging apparatus, we have examined the photodissociation of CH2BrCl in the photon energy range of 448.6-618.5 kJ/mol (193.3-266.6 nm). Precise translational and angular distributions for the dominant Br(P-2(3/2)) and Br(P-2(1/2)) channels have been determined from the ion images observed for Br(P-2(3/2)) and Br(P-2(1/2)). In confirmation with the previous studies, the kinetic-energy distributions for the Br(P-2(1/2)) channel are found to fit well with one Gaussian function, whereas the kinetic- energy distributions for the Br(P-2(3/2)) channel exhibit bimodal structures and can be decomposed into a slow and a fast Gaussian component. The observed kinetic-energy distributions are consistent with the conclusion that the formation of the Br(P-2(3/2)) and Br(P-2(1/2)) channels takes place on a repulsive potential-energy surface, resulting in a significant fraction (0.40-0.47) of available energy to appear as translational energy for the photofragments. On the basis of the detailed kinetic-energy distributions and anisotropy parameters obtained in the present study, together with the specific features and relative absorption cross sections of the excited 2A('), 1A('), 3A('), 4A('), and 2A(') states estimated in previous studies, we have rationalized the dissociation pathways of CH2BrCl in the A-band, leading to the formation of the Br(P-2(3/2)) and Br(P-2(1/2)) channels. The analysis of the ion images observed at 235 nm for Cl(P-2(3/2,1/2)) provides strong evidence that the formation of Cl mainly arises from the secondary photodissociation process CH2Cl+h nu -> CH2+Cl.
机译:使用高分辨率(速度分辨率Delta nu / nu <1.5%)的时间切片离子速度成像设备,我们检查了CH2BrCl在448.6-618.5 kJ / mol(193.3-266.6 nm)光子能量范围内的光解离。从观察到的Br(P-2(3/2)离子图像确定了主导Br(P-2(3/2))和Br(P-2(1/2))通道的精确平移和角度分布))和Br(P-2(1/2))。与先前的研究确认,发现Br(P-2(1/2))通道的动能分布与一个高斯函数非常吻合,而Br(P-2(1/2) 3/2))通道呈现双峰结构,可以分解为慢和快高斯分量。观测到的动能分布与以下结论一致:Br(P-2(3/2))和Br(P-2(1/2))通道的形成是在排斥势能表面上进行的,导致相当一部分(0.40-0.47)的可用能量以光碎片的平移能量形式出现。根据本研究获得的详细动能分布和各向异性参数,以及激发的2A('),1A('),3A('),4A(')的特定特征和相对吸收截面)和先前研究中估计的2A(')状态,我们已经合理化了CH2BrCl在A波段的解离途径,导致形成了Br(P-2(3/2))和Br(P-2 (1/2))个频道。对Cl(P-2(3 / 2,1 / 2))在235 nm处观察到的离子图像的分析提供了有力的证据,表明Cl的形成主要来自二次光解离过程CH2Cl + h nu-> CH2 + Cl 。

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