Neutral rare‐gas containing charge‐transfer molecules in solid matrices. II. HXeH, HXeD, and DXeD in Xe

Photolysis of hydrogen halides (and some other hydrogen containing small molecules) in solid Xe yields in a two step process charged centers, one of them being XeHXe+. Annealing of the irradiated doped solids produces, in addition to H–Xe–Y (Y=Cl, Br, or I) species characterized by us previously, a fairly strong doublet at 1181 and 1166 cm−1 and a weak absorption at 701 cm−1. Deuterated precursors yield a doublet at 846 and 856 cm−1. Also peaks belonging to mixed H/D form are found, indicating that the absorbing species contains two H/D atoms. The new species responsible for these absorptions are assigned as neutral linear centrosymmetric HXeH, HXeD, and DXeD. The nature of the bonding can be understood in terms of the resonance between the two ionic forms HXe+H− and H−Xe+H, analogously to the valence bond description of the well known XeF2. The pseudopotential (LANL1DZ) ab initio calculations at the MP2 level are in good agreement with the observed spectra.

[1]  W. M. Haynes CRC Handbook of Chemistry and Physics , 1990 .

[2]  P. Hay,et al.  The covalent and ionic states of the xenon halides , 1978 .

[3]  M. Räsänen,et al.  Photogeneration of ions via delocalized charge transfer states. II. HX2− (X=Cl,Br,I) in rare gas matrices , 1993 .

[4]  P. Rosmus,et al.  Calculation of Infrared Transition Probabilities for the 1Σ+Groundstate of XeH+ , 1984 .

[5]  V. A. Apkarian,et al.  Energy storage and thermoluminescence in halogen doped solid xenon. III. Photodynamics of charge separation, self‐trapping, and ion–hole recombination , 1988 .

[6]  Henrik Kunttu,et al.  Photogeneration of ions via delocalized charge transfer states. I. Xe2H+ and Xe2D+ in solid Xe , 1992 .

[7]  G. Tisone,et al.  Spectroscopic studies of diatomic noble gas halides: Analysis of spontaneous and stimulated emission from XeCl , 1976 .

[8]  J. Berkowitz,et al.  Diatomic ions of noble gas fluorides , 1970 .

[9]  V. A. Apkarian,et al.  Charge transfer photodynamics in halogen doped xenon matrices. II. Photoinduced harpooning and the delocalized charge transfer states of solid xenon halides (F, Cl, Br, I) , 1988 .

[10]  W. R. Wadt,et al.  Ab initio effective core potentials for molecular calculations. Potentials for K to Au including the outermost core orbitals , 1985 .

[11]  J. A. Seetula,et al.  Photogeneration of ionic species in Ar, Kr and Xe matrices doped with HCl, HBr and HI , 1994 .

[12]  F. Legay,et al.  Photochemistry in Hg doped matrices. Infrared spectra of mercury hydrides: HgH2, HgD2, HHgD, HgD , 1993 .

[13]  V. A. Apkarian,et al.  Cooperative photoabsorption induced charge transfer reaction dynamics in rare gas solids. I. Photodynamics of localized xenon chloride exciplexes , 1986 .

[14]  M. Pettersson,et al.  Neutral rare-gas containing charge-transfer molecules in solid matrices. I. HXeCl, HXeBr, HXeI, and HKrCl in Kr and Xe , 1995 .

[15]  W. R. Wadt,et al.  Ab initio effective core potentials for molecular calculations , 1984 .

[16]  W. R. Wadt,et al.  Ab initio effective core potentials for molecular calculations. Potentials for main group elements Na to Bi , 1985 .

[17]  T. George Electronic states of the XenHCl systems in gas and condensed phases , 1988 .