Pritchard Marisian, Parr Jessica, Li Guosheng, Reisler Hanna, McCaffery Anthony J
Department of Chemistry, University of Sussex, Brighton, UKBN19QJ.
Phys Chem Chem Phys. 2007 Dec 21;9(47):6241-52. doi: 10.1039/b710967a. Epub 2007 Oct 5.
Pair correlated fragment rovibrational distributions are presented following vibrational predissociation of the C2H2-DCl van der Waals dimer initiated by excitation of the asymmetric (asym) C-H stretch. The only observed fragmentation pathways are DCl (v= 0; j= 6-9)+ C2H2(nu2= 1; j= 1-5). These and previously reported data on the related C2H2-HCl species are analysed using the angular momentum (AM) method. Calculations accurately reproduce fragment rovibrational distributions following dissociation of the C2H2-HCl dimer initiated either by excitation of the asym C-H stretch or via the HCl stretch, and those from C2H2-DCl initiated via asym C-H stretch excitation. The calculations demonstrate that the dimer is bent at the moment of dissociation. Several geometries are found that lead to H-bond breakage via a clearly identified set of fragment quantum states. The results suggest a hierarchy in the disposal of excess energy and angular momentum between fragment vibration, rotation and recoil. Deposition of the largest portion of energy into a C2H2 vibrational state sets an upper limit on HCl rotation, which then determines the energy and AM remaining for C2H2 rotation and fragment recoil. Acceptor C2H2 vibrational modes follow a previously noted propensity, implying that the dissociating impulse must be able to induce appropriate nuclear motions both in the acceptor vibration and in rotation of the C2H2 fragment.
通过不对称(asym)C-H伸缩振动激发引发C2H2-DCl范德华二聚体的振动预解离后,给出了成对相关碎片的振转分布。唯一观察到的碎裂途径是DCl(v = 0;j = 6 - 9)+ C2H2(ν2 = 1;j = 1 - 5)。使用角动量(AM)方法分析了这些以及先前报道的关于相关C2H2-HCl物种的数据。计算准确地再现了通过不对称C-H伸缩振动激发或通过HCl伸缩振动引发的C2H2-HCl二聚体解离后的碎片振转分布,以及通过不对称C-H伸缩振动激发引发的C2H2-DCl的碎片振转分布。计算表明,二聚体在解离瞬间是弯曲的。发现了几种几何构型,它们通过一组明确确定的碎片量子态导致氢键断裂。结果表明在碎片振动、转动和反冲之间的多余能量和角动量分配上存在层次结构。将大部分能量沉积到C2H2振动态中为HCl转动设定了上限,这进而决定了C2H2转动和碎片反冲剩余的能量和角动量。受体C2H2振动态遵循先前指出的倾向,这意味着解离冲量必须能够在受体振动和C2H2碎片转动中诱导适当的核运动。