Kishimoto Naoki, Matsumura Eiichi, Ohno Koichi, Deleuze Michael S
Department of Chemistry, Graduate School of Science, Tohoku University, Aoba-ku, Sendai 980-8578, Japan.
J Chem Phys. 2004 Aug 15;121(7):3074-86. doi: 10.1063/1.1769367.
Ionization of bromomethanes (CH3Br, CH2Br2, and CHBr3) upon collision with metastable He*(2(3)S) atoms has been studied by means of collision-energy-resolved Penning ionization electron spectroscopy. Lone-pair (nBr) orbitals of Br4p characters have larger ionization cross sections than sigma(C-Br) orbitals. The collision-energy dependence of the partial ionization cross sections shows that the interaction potential between the molecule and the He*(2(3)S) atom is highly anisotropic around CH3Br or CH2Br2, while isotropic attractive interactions are found for CHBr3. Bands observed at electron energies of approximately 2 eV in the He*(2(3)S) Penning ionization electron spectra (PIES) of CH2Br2 and CHBr3 have no counterpart in ultraviolet (He I) photoionization spectra and theoretical (third-order algebraic diagrammatic construction) one-electron and shake-up ionization spectra. Energy analysis of the processes involved demonstrates that these bands and further bands overlapping with sigma(C-Br) or piCH2 levels are related to autoionization of dissociating (He+ - Br-) pairs. Similarly, a band at an electron energy of approximately 1 eV in the He*(2(3)S) PIES spectra of CH3Br has been ascribed to autoionizing Br** atoms released by dissociation of (unidentified) excited states of the target molecule. A further autoionization (S) band can be discerned at approximately 1 eV below the lone-pair nBr bands in the He*(2(3)S) PIES spectrum of CHBr3. This band has been ascribed to the decay of autoionizing Rydberg states of the target molecule (M**) into vibrationally excited states of the molecular ion. It was found that for this transition, the interaction potential that prevails in the entrance channel is merely attractive.
通过碰撞能量分辨彭宁电离电子能谱研究了溴甲烷(CH₃Br、CH₂Br₂和CHBr₃)与亚稳态He*(2(³)S)原子碰撞时的电离情况。具有Br4p特征的孤对(nBr)轨道比σ(C - Br)轨道具有更大的电离截面。部分电离截面的碰撞能量依赖性表明,分子与He*(2(³)S)原子之间的相互作用势在CH₃Br或CH₂Br₂周围是高度各向异性的,而对于CHBr₃则发现是各向同性的吸引相互作用。在CH₂Br₂和CHBr₃的He*(2(³)S)彭宁电离电子能谱(PIES)中,在电子能量约为2 eV处观察到的谱带在紫外(He I)光电离能谱以及理论(三阶代数图示构建)单电子和振激电离能谱中都没有对应物。对所涉及过程的能量分析表明,这些谱带以及与σ(C - Br)或πCH₂能级重叠的其他谱带与解离(He⁺ - Br⁻)对的自电离有关。类似地,在CH₃Br的He*(2(³)S) PIES能谱中,电子能量约为1 eV处的一个谱带被归因于目标分子(未确定)激发态解离释放出的自电离Br原子。在CHBr₃的He(2(³)S) PIES能谱中,可以在孤对nBr谱带下方约1 eV处辨别出另一个自电离(S)谱带。该谱带被归因于目标分子(M*)的自电离里德堡态衰变为分子离子的振动态激发态。研究发现,对于这种跃迁,在入射通道中占主导的相互作用势仅仅是吸引性的。