Mass-Spectrometric Study of Ions in Xe, Kr, Ar, Ne at Pressures up to 40 torr: Termolecular Formation of the Rare-Gas Molecular Ions. Bond Dissociation Energy of Ar2+ and Ne2+
- 1 September 1967
- journal article
- research article
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 47 (5), 1684-1691
- https://doi.org/10.1063/1.1712150
Abstract
The positive ions obtained from alpha‐particle irradiation of the rare gases Xe, Kr, Ar, Ne were studied in the pressure range 5–40 torr. In all cases both the rare‐gas molecular ion R2+ and the atomic ion R+ could be observed. The R2+/R+ ratio could be decreased by the addition of gases which react with R2+ and R+ through charge transfer. This technique led to a determination of the rate constant for the termolecular reaction R++2R→R2++R. The rate constant for argon is 6×10−32 cm6 atom−2·sec−1. The ratio of Hornbeck—Molnar ionization to direct ionization in Ar was found equal to 0.4. Xe2+ is a major ion in Kr (at 20 torr) containing 10 ppm xenon. The kinetics of the efficient formation of Xe2+ is examined. It is concluded that Xe2+ is formed by Kr2++Xe→KrXe++Kr followed by KrXe++Xe→Xe2++Kr. The rate constants for these two reactions are estimated at 10−10 cm3 molecule−1·sec−1. Both reactions must be exothermic. A schematic representation of the energies of formation of the Kr, Xe, homo‐ and heteronuclear ions is given. Changes in the charge‐transfer spectrum of ethylene with change of the concentration ratio of R2+ and R+ are used to derive the ethylene charge‐transfer spectrum due to R+ and R2+. The charge‐transfer spectrum with R+ is in agreement with that obtained from experiments using low pressures and near‐thermal velocity R+. The charge‐transfer spectrum due to R2+ is used in conjunction with the breakdown graph of ethylene to obtain the recombination energy R.E. of R2+. The bond dissociation energy of R2+ is then estimated from D(R+—R)=I.P.(R)—R.E.(R2+). Values between 1.5–2 eV are obtained for the dissociation energies of Ar2+ and Ne2+.Keywords
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