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碘甲烷的电离和光解离:CH3I 的确定实验生成焓。

On the ionization and dissociative photoionization of iodomethane: a definitive experimental enthalpy of formation of CH3I.

机构信息

Paul Scherrer Institut, Villigen 5232, Switzerland.

出版信息

Phys Chem Chem Phys. 2009 Dec 14;11(46):11013-21. doi: 10.1039/b915400k. Epub 2009 Oct 16.

DOI:10.1039/b915400k
PMID:19924337
Abstract

The dissociative photoionization onset energy of the CH(3)I --> CH(3)(+) + I reaction was studied at the vacuum ultraviolet (VUV) beamline of the Swiss Light Source (SLS) using a new imaging photoelectron photoion coincidence (iPEPICO) apparatus operating with a photon resolution of 2 meV and a threshold electron kinetic energy resolution of about 1 meV. Three previous attempts at establishing this value accurately, namely a pulsed field ionization (PFI)-PEPICO measurement, ab initio calculations and a mass-analyzed threshold ionization (MATI) experiment, in which the onset energy was bracketed by state-selected excitation to vibrationally excited (2)A(1) A states of the parent ion, have yielded contradictory results. It is shown that dimers and adducts formed in the supersonic molecular beam affected the PFI-PEPICO onset energy. The room temperature iPEPICO experiment yields an accurate 0 K onset of 12.248 +/- 0.003 eV, from which we derive a Delta(f)H(o)(298 K)(CH(3)I) = 15.23 +/- 0.3 kJ mol(-1), and the C-I bond energy in CH(3)I is 232.4 +/- 0.4 kJ mol(-1). The room temperature breakdown diagram shows a fine structure that corresponds to the threshold photoelectron spectrum (TPES) of the A state. Low internal energy neutrals seem to be preferentially ionized in the A state when compared with the X state, and A state peaks in the TPES are Stark-shifted as a function of the DC field, whereas the dissociative photoionization of X state ions is not affected. This suggests that there are different competing mechanisms at play to produce ions in the A state vs. ions in the X state. The competition between field ionization and autoionization in CH(3)I is compared with that in Ar, N(2) and in the H-atom loss energy region in CH(4)(+). The binding energies of the neutral and ionic Ar-CH(3)I clusters were found to be 26 and 66 meV, respectively.

摘要

CH(3)I 的离解光电子电离起始能量的研究在瑞士光源(SLS)的真空紫外(VUV)光束线上进行,使用了一种新的成像光电子光离子符合(iPEPICO)装置,其光子分辨率为 2 毫电子伏特,阈值电子动能分辨率约为 1 毫电子伏特。之前有三次试图准确确定该值,即脉冲场电离(PFI)-PEPICO 测量、从头算计算和质量分析的阈值电离(MATI)实验,其中起始能量通过对母体离子的振动激发(2)A(1)A 态的状态选择激发来限制,得出了相互矛盾的结果。结果表明,在超音速分子束中形成的二聚体和加合物影响了 PFI-PEPICO 的起始能量。室温 iPEPICO 实验得出了准确的 0 K 起始值 12.248 +/- 0.003 eV,由此我们得出了 Delta(f)H(o)(298 K)(CH(3)I) = 15.23 +/- 0.3 kJ mol(-1),并且在 CH(3)I 中的 C-I 键能为 232.4 +/- 0.4 kJ mol(-1)。室温击穿图显示出与 A 态阈值光电子能谱(TPES)相对应的精细结构。与 X 态相比,低内能中性似乎优先在 A 态中被电离,并且 A 态中的峰在 Stark 位移中作为 DC 场的函数,而 X 态离子的离解光电子电离不受影响。这表明在 A 态中产生离子与在 X 态中产生离子之间存在不同的竞争机制。CH(3)I 中的场电离和自电离的竞争与 Ar、N(2)以及 CH(4)(+)中的 H-原子损失能量区域中的竞争进行了比较。中性和离子 Ar-CH(3)I 团簇的结合能分别为 26 和 66 毫电子伏特。

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