The
dissociation dynamics of the reaction CF2Br2+hνâCF2+2 Br have been studied for a variety of dissociation energies, Ediss=460â535 kJ molâ1
(corresponding to λ=260â223 nm). The laser induced fluorescence spectrum
of nascent CF2
products was measured for various dissociation energies within this range. Analysis
of the spectra yielded the CF2 vibrational distribution and average rotational energy. The translational energy of CF2 was measured ia the Doppler broadening of various fully resolved rovibronic
transitions. The most detailed analysis of energy disposal in the CF2 fragments was carried out at
Ediss=486 kJ molâ1 (or λ=246 nm). At this energy each degree of freedom of CF2 had an average energy of Evib=0.4±0.2 kJ molâ1, Erot=2.5±0.5 kJ molâ1, and Etrans=24±3 kJ molâ1. These CF2 energies, coupled with
the available thermochemical data, allow us to determine unambiguously that CF2 production must be accompanied by the production of two atomic Br fragments. A photofragment excitation spectrum of CF2Br2, probing for the production of CF2 fragments, provided a reaction threshold of 460±3 kJ molâ1
(corresponding
to 260±1.5 nm). The range of previously published reaction enthalpies varies from 392 to 438 kJ molâ1, all of
which are substantially below the observed threshold. Additionally, at Ediss=486 kJ molâ1, the energy of the CF2
fragment was 27 kJ molâ1 on average, already in excess of the available 26 kJ molâ1, and without considering the kinetic energy of the recoiling Br atoms. We rationalise these data by proposing that the reaction might have a small barrier in the exit channel. The observed threshold corresponds to the top of the barrier (460 kJ molâ1), while the final energy in the fragments is determined by the asymptotic reaction energy (â½424 kJ molâ1).
Simple dynamical models are presented to show that the proposed mechanism is reasonable. Key future experiments and calculations are identified that would enable a clearer picture of the dynamics of this reaction.
这
CF2Br2+hν–
CF2+2 Br 反应的解离动力学已针对各种解离能进行了研究,Ediss=460–535 kJ mol–1
(相当于 δ=260-223 nm)。激光诱导荧光光谱
新生
CF2
测量了产品在此范围内的各种离解能。分析
光谱分析得出
CF2 振动分布和平均旋转能。
CF2 的平移能量是通过各种完全分辨的 rovibronic 的多普勒展宽来测量的
过渡。对
CF2 碎片中的能量处置进行了最详细的分析
Ediss=486 kJ mol−1(或δ=246 nm)。在此能量下,
CF2每个自由度的平均能量为Evib=0.4±0.2 kJ mol-1,Erot=2.5±0.5 kJ mol-1,Etrans=24±3 kJ mol-1。这些
CF2 能量,加上
现有的热
化学数据使我们能够明确地确定
CF2 的产生必定伴随着两个原子 Br 碎片的产生。
CF2Br2 的光碎片激发光谱,探测
CF2 碎片的产生,提供了 460±3 kJ mol–1 的反应阈值
(相应的
至 260±1.5 nm)。先前发表的反应焓范围从 392 到 438 kJ mol·1 不等,全部
远低于观察到的阈值。此外,在 Ediss=486 kJ mol−1 时,
CF2 的能量
碎片平均为 27 kJ mol-1,已经超过了可用的 26 kJ mol-1,并且不考虑反冲 Br 原子的动能。我们通过提出反应在出口通道中可能有一个小障碍来合理化这些数据。观察到的阈值对应于势垒的顶部 (460 kJ mol-1),而碎片中的最终能量由渐近反应能 (-424 kJ mol-1) 决定。
简单的动力学模型表明所提出的机制是合理的。确定了未来的关键实验和计算,可以更清楚地了解该反应的动态。