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The photodissociation dynamics of CFBr exited into the A(~1A') state

机译:CFBr的光解离动力学进入A(〜1A“)状态

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The dynamics of the photolysis reaction, CFBr + h#upsilon# -> CF + Br, have been investigated for photolysis energies in the range, #upsilon# = 23 500 - 26 000 cm~(-1) (#lambda# = 385 - 435 nm). These energies correspond to excitation into the A(~1A") state of CFBr with 2500-5000 cm~(-1) of excess vibrational energy. Following dissociation of jet-cooled CFBr, the internal energy (#OMEGA#, #LAMBDA#, J) on the nascent CF fragments (X ~2#PI#, #upsilon# = 0) was probed by laser induced fluorescence spectroscopy. Two distinct types of product state distributions were observed. At energies above T_(00) + 3360 cm~(-1) the populations of the ~2#PI#_(1/2) and ~2#PI#_(3/2) spin-orbit states of CF were equal, while A" lambda doublet states were preferred over A'. These populations are consistent with a direct dissociation mechanism on the A state, over a barrer with a height of 3360 cm~(-1). The strong state mixing in the vicinity of the barrier ensures a statistical mixture of final spin-orbit states. The preference for the A" lambda doublet states is consistent with the two lone electrons in in-plane orbitals pairing up in the final CF product, leaving one unpaired electron in an out-of-plane orbital, lying parallel to the J vector of the recoiling fragment. For excitation at energies below T_(00) + 3360 cm~(-1) the ground spin-orbit state of CF (~2#PI#_(1/2)) is preferred, while the lambda doublet populations are equal. The interpretation of these populations is that at these energies A state CFBr is stable with respect to dissociation over the barrier. The molecule crosses to either the X or a state where it encounters a deep attractive potential well. The subsequent slower dissociation rate allows the molecule to follow a more adiabatic pathway producing the lowest spin-orbit state of CF, and for any preference for lambda doublet states to be lost.
机译:研究了光解反应的动力学,CFBr + h#upsilon#-> CF + Br,用于范围为#upsilon#= 23500-26 000 cm〜(-1)(#lambda#= 385)的光解能-435 nm)。这些能量对应于具有2500-5000 cm〜(-1)多余振动能的CFBr的A(〜1A“)态的激发。随着射流冷却的CFBr的解离,内部能量(#OMEGA#,#LAMBDA# ,J)用激光诱导荧光光谱法探测新生CF片段(X〜2#PI#,#upsilon#= 0),观察到两种不同类型的产物状态分布,能量在T_(00)+ 3360 cm以上〜(-1)CF的〜2#PI #_(1/2)和〜2#PI #_(3/2)自旋轨道的种群相等,而A“ lambda doublet态优于一种'。这些种群与高度为3360 cm〜(-1)的Barrer上A态的直接解离机制是一致的。势垒附近的强态混合确保了最终自旋轨道状态的统计混合。 A“λ双峰态的偏好与最终CF产物中平面内轨道中的两个孤电子成对一致,而一个未配对电子在平面外轨道中与电子的J向量平行对于低于T_(00)+ 3360 cm〜(-1)的能量激发,CF的自旋轨道状态(〜2#PI #_(1/2))是优选的,而Lambda双峰态是这些种群的解释是,在这些能量下,CFBr状态在势垒上方的解离是稳定的,分子穿过X或遇到深深吸引势的状态,随后的较慢解离速率使得该分子遵循更绝热的途径,产生最低的CF自旋轨道状态,并且任何情况下都会丢失lambda doublet状态。

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