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利用同步辐射对气态和凝聚态 HCCl3 的芯级正离子和负离子碎裂的研究。

Core-level positive-ion and negative-ion fragmentation of gaseous and condensed HCCl3 using synchrotron radiation.

机构信息

National Synchrotron Radiation Research Center (NSRRC), Hsinchu 30076, Taiwan.

出版信息

J Chem Phys. 2011 Jul 28;135(4):044303. doi: 10.1063/1.3615626.

Abstract

We investigated the dissociation dynamics of positive-ion and negative-ion fragments of gaseous and condensed HCCl(3) following photoexcitation of Cl 2p electrons to various resonances. Based on ab initio calculations at levels HF/cc-pVTZ and QCISD/6-311G∗, the first doublet structures in Cl L-edge x-ray absorption spectrum of HCCl(3) are assigned to transitions from the Cl (2P(3/2),(1/2)) initial states to the 10a(1)(∗) orbitals. The Cl 2p → 10a(1)(∗) excitation of HCCl(3) induces a significant enhancement of the Cl(+) desorption yield in the condensed phase and a small increase in the HCCl(+) yield in the gaseous phase. Based on the resonant photoemission of condensed HCCl(3), excitations of Cl 2p electrons to valence orbitals decay predominantly via spectator Auger transitions. The kinetic energy distributions of Cl(+) ion via the Cl 2p → 10a(1)(∗) excitation are shifted to higher energy ∼0.2 eV and ∼0.1 eV relative to those via the Cl 2p → 10e(∗) excitation and Cl 2p → shape resonance excitation, respectively. The enhancement of the yields of ionic fragments at specific core-excited resonance states is assisted by a strongly repulsive surface that is directly related to the spectator electrons localized in the antibonding orbitals. The Cl(-) anion is significantly reinforced in the vicinity of Cl 2p ionization threshold of gaseous HCCl(3), mediated by photoelectron recapture through post-collision interaction.

摘要

我们研究了 Cl 2p 电子光激发到各种共振态后气态和凝聚态 HCCl(3)中正离子和负离子碎片的离解动力学。基于 HF/cc-pVTZ 和 QCISD/6-311G∗水平的从头算计算,HCCl(3)的 Cl L 边 X 射线吸收光谱中的第一个双线结构被分配给从 Cl(2P(3/2),(1/2))初始态到 10a(1)(∗)轨道的跃迁。Cl 2p→10a(1)(∗)激发 HCCl(3)导致凝聚相中 Cl(+)脱附产率显著增强,气相中 HCCl(+)产率略有增加。基于凝聚态 HCCl(3 的共振光发射,Cl 2p 电子激发到价轨道主要通过旁观者俄歇跃迁衰减。通过 Cl 2p→10a(1)(∗)激发的 Cl(+)离子的动能分布分别向更高的能量(约 0.2 eV 和 0.1 eV)偏移,相对于 Cl 2p→10e(∗)激发和 Cl 2p→形状共振激发的 Cl(+)离子。在特定的核心激发共振态下,离子碎片产率的增强是由一个直接与局域在反键轨道中的旁观者电子相关的强烈排斥表面辅助的。气态 HCCl(3 中 Cl 2p 电离阈值附近的 Cl(-)阴离子通过光电电子通过后碰撞相互作用的捕获而显著增强。

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