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溴碘甲烷在第一和第二吸收带的光解离动力学。速度映射与切片成像联合研究。

Photodissociation dynamics of bromoiodomethane from the first and second absorption bands. A combined velocity map and slice imaging study.

作者信息

Marggi Poullain Sonia, Chicharro David V, Navarro Eduardo, Rubio-Lago Luis, González-Vázquez Jesús, Bañares Luis

机构信息

Departamento de Qumica Fsica I, Facultad de Ciencias Qumicas, Universidad Complutense de Madrid, 28040 Madrid, Spain.

出版信息

Phys Chem Chem Phys. 2018 Jan 31;20(5):3490-3503. doi: 10.1039/c7cp07077b.

DOI:10.1039/c7cp07077b
PMID:29335697
Abstract

The photodissociation dynamics of bromoiodomethane (CHBrI) have been investigated at the maximum of the first A and second A' absorption bands, at 266 and 210 nm excitation wavelengths, respectively, using velocity map and slice imaging techniques in combination with a probe detection of both iodine and bromine fragments, I(P), I*(P), Br(P) and Br*(P) via (2 + 1) resonance enhanced multiphoton ionization. Experimental results, i.e. translational energy and angular distributions, are reported and discussed in conjunction with high level ab initio calculations of potential energy curves and absorption spectra. The results indicate that in the A-band, direct dissociation through the 5A' excited state leads to the I(P) channel while I*(P) atoms are produced via the 5A' → 4A'/4A'' nonadiabatic crossing. The presence of Br and Br* fragments upon excitation to the A-band is attributed to indirect dissociation via a curve crossing between the 5A' with upper excited states such as the 9A'. The A'-band is characterized by a strong photoselectivity leading exclusively to the Br(P) and Br*(P) channels, which are likely produced by dissociation through the 9A' excited state. Avoided crossings between several excited states from both the A and A' bands entangle however the possible reaction pathways.

摘要

利用速度成像和切片成像技术,结合通过(2 + 1)共振增强多光子电离对碘和溴碎片I(P)、I*(P)、Br(P)和Br*(P)的探测,分别在266和210 nm激发波长下,于第一个A吸收带和第二个A'吸收带的峰值处研究了溴碘甲烷(CHBrI)的光解离动力学。结合势能曲线和吸收光谱的高水平从头算计算,报告并讨论了实验结果,即平动能和角分布。结果表明,在A带中,通过5A'激发态的直接解离导致I(P)通道,而I*(P)原子则通过5A'→4A'/4A''非绝热跃迁产生。激发到A带时Br和Br碎片的存在归因于通过5A'与诸如9A'等较高激发态之间的曲线交叉进行的间接解离。A'带的特征是具有很强的光选择性,仅导致Br(P)和Br(P)通道,这可能是通过9A'激发态的解离产生的。然而,A带和A'带中几个激发态之间的避免交叉使可能的反应途径变得复杂。

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