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过氧亚硝酸的二次羟基泛频激发与统计解离动力学

Second OH overtone excitation and statistical dissociation dynamics of peroxynitrous acid.

作者信息

Konen Ian M, Li Eunice X J, Stephenson Thomas A, Lester Marsha I

机构信息

Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104-6323, USA.

出版信息

J Chem Phys. 2005 Nov 22;123(20):204318. doi: 10.1063/1.2126968.

Abstract

The second OH overtone transition of the trans-perp conformer of peroxynitrous acid (tp-HOONO) is identified using infrared action spectroscopy. HOONO is produced by the recombination of photolytically generated OH and NO(2) radicals, and then cooled in a pulsed supersonic expansion. The second overtone transition is assigned to tp-HOONO based on its vibrational frequency (10 195.3 cm(-1)) and rotational band contour, which are in accord with theoretical predictions and previous observations of the first overtone transition. The transition dipole moment associated with the overtone transition is rotated considerably from the OH bond axis, as evident from its hybrid band composition, indicating substantial charge redistribution upon OH stretch excitation. The overtone band exhibits homogeneous line broadening that is attributed to intramolecular vibrational redistribution, arising from the coupling of the initially excited OH stretch to other modes that ultimately lead to dissociation. The quantum state distributions of the OH X (2)Pi (nu=0) products following first and second OH overtone excitation of tp-HOONO are found to be statistical by comparison with three commonly used statistical models. The product state distributions are principally determined by the tp-HOONO binding energy of 16.2(1) kcal mol(-1). Only a small fraction of the OH products are produced in nu=1 following the second overtone excitation, consistent with statistical predictions.

摘要

利用红外光声光谱法确定了过氧亚硝酸(tp-HOONO)反式垂直构象体的第二个OH泛频跃迁。HOONO由光解产生的OH和NO(2)自由基复合而成,然后在脉冲超声速膨胀中冷却。基于其振动频率(10195.3 cm(-1))和转动带轮廓,第二个泛频跃迁被归属于tp-HOONO,这与理论预测和先前对第一个泛频跃迁的观测结果一致。从其混合带组成可以明显看出,与泛频跃迁相关的跃迁偶极矩相对于OH键轴有很大旋转,这表明在OH伸缩激发时电荷有大量重新分布。泛频带呈现出均匀的谱线展宽,这归因于分子内振动再分配,它是由最初激发的OH伸缩与其他最终导致解离的模式的耦合引起的。通过与三种常用的统计模型比较,发现tp-HOONO的第一个和第二个OH泛频激发后OH X(2)Pi(ν = 0)产物的量子态分布是统计性的。产物态分布主要由tp-HOONO的结合能16.2(1) kcal mol(-1)决定。在第二个泛频激发后,只有一小部分OH产物以ν = 1产生,这与统计预测一致。

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