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Cl + CHD(v,v-I,v-II = 1)中拉伸激发的影响:当Cl原子攻击未激发的C-D键时。

Effects of Stretching Excitations in Cl + CHD( v, v-I, v-II = 1): As the Cl Atom Attacks the Unexcited C-D Bond.

作者信息

Mondal Sohidul, Liu Kopin

机构信息

Institute of Atomic and Molecular Sciences (IAMS), Academia Sinica , P.O. Box 23-166, Taipei , Taiwan 10699.

Department of Chemistry , National Sun Yat-sen University , Kaohsiung , Taiwan 80424.

出版信息

J Phys Chem A. 2019 Feb 28;123(8):1514-1520. doi: 10.1021/acs.jpca.8b11702. Epub 2019 Feb 20.

Abstract

The title reactions were studied at two collisional energies ( E) in a crossed-beam product-imaging experiment. We found that all three initial CH stretching excitations suppress the reactivity toward the abstraction of the unexcited D atom. In terms of vibrational suppression factor, σ/σ, the product channels of CH(0/4) + DCl and CH(1/3) + DCl show opposite mode-specific trends. However, the angular distributions of both channels are nearly identical to that of the ground-state reaction at the same E, regardless of the initial reactant states. Tentatively, we ascribed these two observations to a vibrationally induced narrowing effect of the attack angle near the barrier to reaction. As for the DCl coproduct state distributions, the two channels are distinct but show little mode-specific difference. When CH(0) is probed, the DCl coproduct peaks at v = 1 are accompanied by substantial rotational excitation, whereas the DCl products associated with CH(1/3) are both vibrationally and rotationally cold. We attributed the different (correlated) energy disposals to a manifestation of trajectory bifurcations in the postbarrier region, with a vibrationally nonadiabatic pathway leading to CH(0) + DCl( v = 1) and the other adiabatically to the CH(1/3) + DCl( v = 0) channel. For both pathways the initial CH stretching excitation acts as a conserved mode by preferentially retaining one quantum of vibrational excitation in the reaction.

摘要

在交叉束产物成像实验中,于两种碰撞能量(E)下研究了标题反应。我们发现,所有三种初始的CH伸缩振动激发都抑制了与未激发的D原子抽象反应的反应活性。就振动抑制因子σ/σ而言,CH(0/4) + DCl和CH(1/3) + DCl的产物通道呈现出相反的模式特异性趋势。然而,无论初始反应物状态如何,在相同的E下,两个通道的角分布都与基态反应的角分布几乎相同。初步地,我们将这两个观察结果归因于反应势垒附近攻击角的振动诱导变窄效应。至于DCl副产物的态分布,两个通道是不同的,但模式特异性差异很小。当探测CH(0)时,v = 1处的DCl副产物峰伴随着大量的转动激发,而与CH(1/3)相关的DCl产物在振动和转动方面都是冷的。我们将不同的(相关的)能量分配归因于势垒后区域轨迹分支的一种表现,其中一条振动非绝热路径通向CH(0) + DCl(v = 1),另一条绝热路径通向CH(1/3) + DCl(v = 0)通道。对于这两条路径,初始的CH伸缩振动激发都通过在反应中优先保留一个振动激发量子而作为一个守恒模式起作用。

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