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通过MCN(M = Na、K、Rb)的超激发离子对态产生的CN(BΣ)的反向振动和转动激发

Inverted Vibrational and Rotational Excitation of CN(BΣ) Produced through Superexcited Ion-Pair States of MCN (M = Na, K, Rb).

作者信息

Yasumatsu Hisato, Jeung Gwang-Hi

机构信息

Cluster Research Laboratory, Toyota Technological Institute: in East Tokyo Laboratory, Genesis Research Institute, Inc., 717-86 Futamata, Ichikawa, Chiba 272-0001, Japan.

Institut des Sciences Moléculaires de Marseille, Service 561, Campus de Saint-Jérôme, Aix-Marseille Université, Marseille Cedex 20 13397, France.

出版信息

J Phys Chem A. 2020 Apr 9;124(14):2741-2745. doi: 10.1021/acs.jpca.9b11634. Epub 2020 Mar 30.

DOI:10.1021/acs.jpca.9b11634
PMID:32181653
Abstract

This paper reports an energy-partition mechanism in dissociative excitation of alkali cyanide molecules, MCN (M = Rb, K, Na), to produce CN(BΣ) and M(sS) ( = 5, 4, and 3 for Rb, K, and Na, respectively) in collision with Kr metastable atoms, Kr(P). Both the vibrational and rotational distributions of CN(BΣ) produced in the reactions of RbCN and KCN were inverted as being peaked at = 1 and ' = 35, respectively, where ' and ' are the vibrational and the rotational quantum numbers of CN(BΣ), respectively. According to a state crossing model, it was derived that CN(BΣ) is produced by predissociation through a superexcited ion-pair state, CN(3Σ)·M(S), followed by an adiabatic transition to a repulsive state correlating to the dissociation limit of CN(BΣ) + M(sS). The inverted distributions are driven by structural changes during the excitation and the adiabatic transition. The maximum vibrational population at ' = 1 originates from a large Franck-Condon overlap between the vibrational wavefunctions of CN(3Σ) and CN(BΣ) at ' = 1. The rotational excitation of the CN(BΣ) product is explained with changing from a T-shape geometry of MCN in the ground state to a linear one in the superexcited ion-pair state.

摘要

本文报道了碱金属氰化物分子MCN(M = Rb、K、Na)与氪亚稳态原子Kr(P)碰撞发生离解激发以产生CN(BΣ)和M(sS)(Rb、K、Na对应的s分别为5、4和3)时的能量分配机制。在RbCN和KCN反应中产生的CN(BΣ)的振动分布和转动分布都是反转的,分别在v' = 1和J' = 35处达到峰值,其中v'和J'分别是CN(BΣ)的振动量子数和转动量子数。根据态交叉模型推导得出,CN(BΣ)是通过一个超激发离子对态CN(3Σ)·M(S)预解离,然后绝热跃迁到一个与CN(BΣ) + M(sS)离解极限相关的排斥态而产生的。反转分布是由激发和绝热跃迁过程中的结构变化驱动的。v' = 1处的最大振动布居源于v' = 1时CN(3Σ)和CN(BΣ)的振动波函数之间较大的弗兰克 - 康登重叠。产物CN(BΣ)的转动激发可以用基态MCN的T形几何结构转变为超激发离子对态的线性几何结构来解释。

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