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二硫分子(S2)的光解离成像。

Photodissociation imaging of diatomic sulfur (S2).

机构信息

Institute for Molecules and Materials, Radboud University Nijmegen, Heyendaalseweg 135, 6525 AJ Nijmegen, The Netherlands.

出版信息

J Phys Chem A. 2009 Dec 31;113(52):14995-5005. doi: 10.1021/jp905104u.

DOI:10.1021/jp905104u
PMID:19754091
Abstract

The photodissociation of diatomic sulfur, S(2), in the region of the first dissociation limit is studied with velocity map imaging. Correlated fine structure distributions P(J1,J2) for the two S((3)P(J)) fragments are determined at selected photolysis wavelengths. Image analysis of the speed distributions of the atomic fragments following product-state-specific detection results in a revision of the bond energy to D(0) = 35636.9 +/- 2.5 cm(-1) with respect to the lowest rovibrational level. This value arises from reinterpretation of previous spectroscopic data showing onset of predissociation in the B(3)Sigma(u)(-) state, as the measurements presented here demonstrate that the long-range correlation of the excited state invoked as causing the dissociation is S((3)P(2)) + S((3)P(2)) rather than S((3)P(2)) + S((3)P(1)). The wavelength dependence of data for the S((3)P(2)) + S((3)P(2)) channel suggests involvement of photoexcitation through the optically forbidden Herzberg continuum bands in addition to dissociation initiated via the optically allowed B(3)Sigma(u)(-)-X(3)Sigma(g)(-) and B''(3)Pi(u)-X(3)Sigma(g)(-) bands. Changes in product recoil velocity angular distributions and atomic angular momentum polarization were also measured as a function of dissociation wavelength. The results are compared with predictions from an adiabatic model for dissociation, which provides a basis for interpretation but does not explain quantitatively the experimental results.

摘要

双原子硫(S(2))在第一离解限区域的光解反应通过速度成像技术进行研究。在选定的光解波长下,确定了两个 S((3)P(J))碎片的相关精细结构分布 P(J1,J2)。通过对产物态特异性检测后原子碎片速度分布的图像分析,对键能进行了修订,得到 D(0) = 35636.9 +/- 2.5 cm(-1),相对于最低振转能级。这一数值源于对先前光谱数据的重新解释,表明在 B(3)Sigma(u)(-)态中出现了预离解的起始,而这里呈现的测量结果表明,引起离解的激发态的长程相关性是 S((3)P(2)) + S((3)P(2)),而不是 S((3)P(2)) + S((3)P(1))。对于 S((3)P(2)) + S((3)P(2))通道的数据的波长依赖性表明,除了通过光学允许的 B(3)Sigma(u)(-)-X(3)Sigma(g)(-)和 B''(3)Pi(u)-X(3)Sigma(g)(-)带引发的离解之外,还涉及通过光学禁戒的 Herzberg 连续带进行光激发。还测量了产物反冲速度角分布和原子角动量极化随离解波长的变化。结果与用于离解的绝热模型的预测进行了比较,该模型为解释提供了基础,但不能定量解释实验结果。

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