Matrix‐Isolation Study of the Vacuum‐Ultraviolet Photolysis of Methyl Fluoride. The Infrared Spectra of the Free Radicals CF, HCF, and H2CF
摘要:
Upon vacuum-ultraviolet photolysis of methyl fluoride in an argon or a nitrogen matrix at 14°K, the free radicals CF, HCF, and H2CF are stabilized in sufficient concentration for observation of their infrared absorption spectra. Studies utilizing carbon-13 and deuterium substitution confirm the identification of these species. Visible-ultraviolet absorption spectra of photolyzed Ar:CF3F samples include bands which may be assigned to CH, to CF, and to HCF. The reaction of carbon atoms, produced by the photolysis of cyanogen azide isolated in an argon matrix, with HF trapped in the matrix has also been found to lead to the stabilization of sufficient HCF for infrared spectroscopic detection. Reaction of HCF with a second molecule of HF to form CH2F2 also occurs. The force constants and thermodynamic properties of HCF have been calculated, and a partial vibrational assignment is proposed for H2CF. Although these experiments do not determine the primary photodecomposition processes important for methyl fluoride, there is evidence that both H atom and F atom detachment may occur under the conditions of these experiments.
Infrared chemiluminescence using a SISAM spectrometer. Reactions producing vibrationally excited HF
作者:David Klenerman、I. W. M. Smith
DOI:10.1039/f29878300243
日期:——
03 for the Nv distribution from the primary reaction F + H2O2→ HF(v⩽ 4)+ HO2. Only weak emission from HF(v= 5), and none from higher levels, could be detected under conditions where the secondary reaction, F + HO2→ HF(v⩽ 9)+ O2, should occur. It seems that this reaction does not populate the higher HF levels preferentially, probably because it proceeds via an (HOOF)+ complex. The HF(v) emission in the
已使用SISAM(光谱干涉法选择振幅调制)来观察由F原子与H 2和H 2 O 2以及O原子与C 2 HF 3反应形成的振动激发的HF的红外化学发光。。在基于F + H实验2 →HF(v ⩽3)+ H,可以达成条件,其中初生相对振动人群可被确定为Ñ 3:Ñ 2:Ñ 1 = 0.31±0.03:0.48±0.03:0.21± 0.03,与之前的测量非常吻合。F + H上的类似测量2 ö 2系统得到Ñ 4: Ñ 3: Ñ 2: Ñ 1 = 0.15±0.03:0.25±0.03:0.31±0.03:0.30±0.03对Ñ v从初级反应分布函数F + H 2 ö 2 →HF( v ⩽4)+ HO 2。只有从HF弱发射( v = 5),并从较高水平的无,可以条件下检测,其中次级反应,F + HO 2 →HF( v ⩽9)+ O 2,应会发生。似乎该反应没有优先占据较高的HF水平,可能是因为它是通过(
The Elementary Reaction of CHF(X˜1A´) with Ozone
作者:Walter Hack、B. Wagner、Karlheinz Hoyermann
DOI:10.1524/zpch.2000.214.6.741
日期:2000.1.1
The reaction CHF(X
k
was obtained. No change in the rate constant was observed, substituting He by the quenchers N
反应CHF(X)已经获得。在用淬灭剂N替代He时,没有观察到速率常数的变化。
Laser-induced fluorescence of HCF and HCCl
作者:Yuanwu Qiu、Shikang Zhou、Jiliang Shi
DOI:10.1016/0009-2614(87)87304-9
日期:1987.4
We report the first observation of the laser-induced fluorescence excitation spectrum of the à 1A'(000)-X̃ 1A'(010) vibronic band of HCF and some subbands of the à 1A'(030) and à 1A'(040)-X̃ 1A'(000) vibronic bands of HCCl, using the technique of molecular beams.
Dissociations of Gas-Phase CHClF and CHCl<sub>2</sub> Radicals and Cations following Collisional Electron Transfer. A Variable-Time Neutralization−Reionization and ab Initio Study
作者:Martin Sadílek、František Tureček
DOI:10.1021/jp952416i
日期:1996.1.1
Variable-time neutralization−reionization massspectrometry is used to generate CHClF• and CHCl2• radicals and to study their unimolecular dissociations within 0.4−4.1 μs. Loss of Cl• is a major dissociation of CHClF• following collisional neutralizations with di-n-butyl ether, chlorobenzene, di-n-butylamine, aniline, and N,N-dimethylaniline, which range from 0.28 eV endoergic to 1.7 eV exoergic in
Products vibrational energy distributions in the O(3P) + CHF reaction
作者:D.S.Y. Hsu、R.G. Shortridge、M.C. Lin
DOI:10.1016/0301-0104(79)89002-3
日期:1979.5
The vibrational energy distributions of the HF and CO formed in flash-initiated SO2CHFX2 (X = Cl, Br) mixtures have been measured by laseremission and laser resonance absorption, respectively. Both excited products are believed to result mainly from the O(3P) + CHF reaction, which probably takes place via vibronically excited HFCO intermediates. The observed HF and COvibrational energy distributions