National Synchrotron Radiation Research Center (NSRRC), 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 30076, Taiwan.
J Chem Phys. 2011 Jul 28;135(4):044301. doi: 10.1063/1.3613636.
We investigated the dynamics of photodissociation of propenal (acrolein, CH(2)CHCHO) at 157 nm in a molecular beam and of migration and elimination of hydrogen atoms in systems C(3)H(4)O and C(3)H(3)O using quantum-chemical calculations. Compared with the previous results of photodissociation of propenal at 193 nm, the major difference is that the C(3)H(3)O fragment present at the 193-nm photolysis disappears at the 157-nm photolysis whereas the C(3)H(2)O fragment absent at 193 nm appears at 157 nm. Optimized structures and harmonic vibrational frequencies of molecular species with gross formula C(3)H(2-4)O were computed at the level of B3LYP/6-311G(d,p) and total energies of those molecules at optimized structures were computed at the level of CCSD(T)/6-311+G(3df,2p). Based on the calculated potential-energy surfaces, we deduce that the C(3)H(3)O fragment observed in the photolysis of propenal at 193 nm is probably CHCCHOH ((2)A") and/or CH(2)CCOH ((2)A") produced from an intermediate hydroxyl propadiene (CH(2)CCHOH) following isomerization. Adiabatic and vertical ionization potentials of eight isomers of C(3)H(3)O and two isomers of C(3)H(2)O were calculated; CHCCHOH ((2)A") and CH(2)CCOH ((2)A") have ionization potentials in good agreement with the experimental value of ∼7.4 eV. We also deduce that all the nascent C(3)H(3)O fragments from the photolysis of propenal at 157 nm spontaneously decompose mainly to C(2)H(3) + CO and C(3)H(2)O + H because of the large excitation energy. This work provides profound insight into the dynamics of migration and elimination of hydrogen atoms of propenal optically excited in the vacuum-ultraviolet region.
我们在分子束中研究了丙烯醛(CH(2)CHCHO)在 157nm 时的光解动力学,以及在 C(3)H(4)O 和 C(3)H(3)O 体系中氢原子的迁移和消除,使用量子化学计算。与丙烯醛在 193nm 时的光解的先前结果相比,主要区别在于在 193nm 光解时存在的 C(3)H(3)O 碎片在 157nm 光解时消失,而在 193nm 时不存在的 C(3)H(2)O 碎片出现在 157nm。采用 B3LYP/6-311G(d,p) 水平计算了具有通式 C(3)H(2-4)O 的分子物种的优化结构和简谐振动频率,并在优化结构的 CCSD(T)/6-311+G(3df,2p) 水平上计算了这些分子的总能量。基于计算得到的势能面,我们推断在 193nm 时丙烯醛光解中观察到的 C(3)H(3)O 碎片可能是 CHCCHOH((2)A")和/或 CH(2)CCOH((2)A"),它们是异构化后由中间体羟基丙二烯(CH(2)CCHOH)生成的。计算了 C(3)H(3)O 的八个异构体和 C(3)H(2)O 的两个异构体的绝热和垂直电离势;CHCCHOH((2)A")和 CH(2)CCOH((2)A")的电离势与实验值∼7.4eV 非常吻合。我们还推断,由于激发能较大,丙烯醛在 157nm 时光解产生的所有初生 C(3)H(3)O 碎片主要自发分解为 C(2)H(3)+CO 和 C(3)H(2)O+H。这项工作为理解真空紫外光激发下丙烯醛中氢原子的迁移和消除动力学提供了深刻的认识。