Li Hongwei, Fang Yi, Kidwell Nathanael M, Beames Joseph M, Lester Marsha I
Department of Chemistry, University of Pennsylvania, Philadelphia Pennsylvania 19104-6323, United States.
J Phys Chem A. 2015 Jul 30;119(30):8328-37. doi: 10.1021/acs.jpca.5b05352. Epub 2015 Jul 20.
UV excitation of jet-cooled CH3CHOO on the B(1)A'-X(1)A' transition results in dissociation to two spin-allowed product channels: CH3CHO X(1)A' + O (1)D and CH3CHO a(3)A″ + O (3)P. The O (1)D and O (3)P products are detected using 2 + 1 REMPI at 205 and 226 nm, respectively, for action spectroscopy and velocity map imaging studies. The O (1)D action spectrum closely follows the previously reported UV absorption spectrum for jet-cooled CH3CHOO [Beames et al. J. Chem. Phys. 2013 , 138 , 244307]. Velocity map images of the O (1)D products following excitation of CH3CHOO at 305, 320, and 350 nm exhibit anisotropic angular distributions indicative of rapid (ps) dissociation, along with broad and unstructured total kinetic energy (TKER) distributions that reflect the internal energy distribution of the CH3CHO X(1)A' coproducts. The O (3)P action spectrum turns on near the peak of the UV absorption spectrum (ca. 324 nm) and extends to higher energy with steadily increasing O (3)P yield. Excitation of CH3CHOO at 305 nm, attributed to absorption of the more stable syn-conformer, also results in an anisotropic angular distribution of O (3)P products arising from rapid (ps) dissociation, but a narrower TKER distribution since less energy is available to the CH3CHO a(3)A″ + O (3)P products. The threshold for the higher energy CH3CHO a(3)A″ + O (3)P product channel is determined to be ca. 88.4 kcal mol(-1) from the termination of the TKER distribution and the onset of the O (3)P action spectrum. This threshold is combined with the singlet-triplet spacings of O atoms and acetaldehyde to establish the dissociation energy for syn-CH3HOO X(1)A' to the lowest spin-allowed product channel, CH3CHO X(1)A' + O (1)D, of ≤55.9 ± 0.4 kcal mol(-1). A harmonic normal-mode analysis is utilized to identify the vibrational modes of CH3CHO likely to be excited upon dissociation into the two product channels.
在B(1)A'-X(1)A'跃迁上对喷射冷却的CH3CHOO进行紫外激发会导致解离为两个自旋允许的产物通道:CH3CHO X(1)A' + O (1)D和CH3CHO a(3)A″ + O (3)P。分别使用2 + 1共振增强多光子电离(REMPI)在205和226 nm处检测O (1)D和O (3)P产物,用于作用光谱和速度映射成像研究。O (1)D作用光谱与先前报道的喷射冷却CH3CHOO的紫外吸收光谱[比姆斯等人,《化学物理杂志》2013年,138卷,244307]密切相关。在305、320和350 nm处激发CH3CHOO后,O (1)D产物的速度映射图像呈现出各向异性的角分布,表明快速(皮秒)解离,同时伴随着反映CH3CHO X(1)A'共产物内能分布的宽且无结构的总动能(TKER)分布。O (3)P作用光谱在紫外吸收光谱的峰值(约324 nm)附近开启,并随着O (3)P产率的稳步增加延伸到更高能量。在305 nm处激发CH3CHOO,归因于更稳定的顺式构象体的吸收,也导致了由快速(皮秒)解离产生的O (3)P产物的各向异性角分布,但由于CH3CHO a(3)A″ + O (3)P产物可获得的能量较少,TKER分布较窄。从TKER分布的终止和O (3)P作用光谱的起始确定,较高能量的CH3CHO a(3)A″ + O (3)P产物通道的阈值约为88.4 kcal mol(-1)。该阈值与O原子和乙醛的单重态 - 三重态间距相结合,以确定顺式 - CH3HOO X(1)A'到最低自旋允许产物通道CH3CHO X(1)A' + O (1)D的解离能≤55.9 ± 0.4 kcal mol(-1)。利用谐波简正模式分析来识别CH3CHO在解离为两个产物通道时可能被激发的振动模式。