Abstract:A self-igniting DC-electric discharge of C 2 H 2 in Xe (matrix gas) or C 2 H 2 and Xe in Ar or Kr (matrix gas) is used to produce and study the XeC 2 molecule in these various rare gases at 12 K. Unlike in Ar and Kr, the wellknown electronic spectra of C 2 is completely absent in a Xe matrix. This together with annealing experiments in Ar matrices indicate that ground state Xe and C 2 react uniquely and without a barrier to form the XeC 2 molecule. The IRactive C-C stretch of this compound is found to be close… Show more
“…If H 2 molecules form upon photolysis, the formation of HXeCC needs global mobility of H atoms, which can be somewhat suppressed in the mixed matrices. Third, the Xe-CC molecule is computationally bent ͑148.6°͒, 30 which can produce a barrier for the formation of a linear HXeCC molecule, and this slows down the reaction at lower annealing temperatures in Ar and Kr matrices. We observed in solid Kr ͑C 2 H 2 /Xe/Kr͒ that the HCC and HCC¯Xe concentrations increase upon annealing.…”
HXeCCH molecule is prepared in Ar and Kr matrices and characterized by IR absorption spectroscopy. The experiments show that HXeCCH can be made in another host than the polarizable Xe environment. The H-Xe stretching absorption of HXeCCH in Ar and Kr is blueshifted from the value measured in solid Xe. The maximum blueshifts are +44.9 and +32.3 cm(-1) in Ar and Kr, respectively, indicating stabilization of the H-Xe bond. HXeCCH has a doublet H-Xe stretching absorption measured in Xe, Kr, and Ar matrices with a splitting of 5.7, 13, and 14 cm(-1), respectively. Ab initio calculations for the 1:1 HXeCCHcdots, three dots, centeredNg complexes (Ng = Ar, Kr, or Xe) are used to analyze the interaction of the hosts with the embedded molecule. These calculations support the matrix-site model where the band splitting observed experimentally is caused by specific interactions of the HXeCCH molecule with noble-gas atoms in certain local morphologies. However, the 1:1 complexation is unable to explain the observed blueshifts of the H-Xe stretching band in Ar and Kr matrices compared to a Xe matrix. More sophisticated computational approach is needed to account in detail the effects of solid environment.
“…If H 2 molecules form upon photolysis, the formation of HXeCC needs global mobility of H atoms, which can be somewhat suppressed in the mixed matrices. Third, the Xe-CC molecule is computationally bent ͑148.6°͒, 30 which can produce a barrier for the formation of a linear HXeCC molecule, and this slows down the reaction at lower annealing temperatures in Ar and Kr matrices. We observed in solid Kr ͑C 2 H 2 /Xe/Kr͒ that the HCC and HCC¯Xe concentrations increase upon annealing.…”
HXeCCH molecule is prepared in Ar and Kr matrices and characterized by IR absorption spectroscopy. The experiments show that HXeCCH can be made in another host than the polarizable Xe environment. The H-Xe stretching absorption of HXeCCH in Ar and Kr is blueshifted from the value measured in solid Xe. The maximum blueshifts are +44.9 and +32.3 cm(-1) in Ar and Kr, respectively, indicating stabilization of the H-Xe bond. HXeCCH has a doublet H-Xe stretching absorption measured in Xe, Kr, and Ar matrices with a splitting of 5.7, 13, and 14 cm(-1), respectively. Ab initio calculations for the 1:1 HXeCCHcdots, three dots, centeredNg complexes (Ng = Ar, Kr, or Xe) are used to analyze the interaction of the hosts with the embedded molecule. These calculations support the matrix-site model where the band splitting observed experimentally is caused by specific interactions of the HXeCCH molecule with noble-gas atoms in certain local morphologies. However, the 1:1 complexation is unable to explain the observed blueshifts of the H-Xe stretching band in Ar and Kr matrices compared to a Xe matrix. More sophisticated computational approach is needed to account in detail the effects of solid environment.
“…In 2012 the semicentential will be celebrated for the discovery of the very first Ng compound. (v) Xe-C n where n = 2, 3, 5, 7, 9, 104,105 have been discovered, and the issue of stability of a hypothetical 1D polymer (-Xe-C 2 -), 106 was immediately addressed; 107 (vi) using the isoelectronic analogy between C 2 and BN, as the yet unknown and quite strongly bound species Xe-BN, Xe-NB, HXeNBH and HXeBNH 108 have been considered;…”
Section: Going In New Directions: Prediction Of Novel Speciesmentioning
In this critical review I describe fascinating experimental and theoretical advances in 'noble gas' chemistry during the last twenty years, and have taken a somewhat unexpected course since 2000. I also highlight perspectives for further development in this field, including the prospective synthesis of compounds containing as yet unknown Xe-element and element-Xe-element bridging bonds, peroxide species containing Xe, adducts of XeF(2) with various metal fluorides, Xe-element alloys, and novel pressure-stabilized covalently bound and host-guest compounds of Xe. A substantial part of the essay is devoted to the-as yet experimentally unexplored-behaviour of the compounds of Xe under high pressure. The blend of science, history, and theoretical predictions, will be valued by inorganic and organic chemists, materials scientists, and the community of theoretical and experimental high-pressure physicists and chemists (151 references).
“…The remaining barrier might originate from the differences in geometries of the XeC 2 molecule and the corresponding fragment in the HXeCC radical. Indeed, computationally the XeC 2 molecule is bent with an angle of 147°, 22 whereas HXeCC is linear. In this situation, the activation of the XeC 2 bending motion ͑computationally 87 cm −1 ͒ can contribute to the process.…”
The light-induced H + XeC 2 ↔ HXeCC reaction is studied in solid Xe, and the full optical control of this reaction is demonstrated. By narrow-band excitation in the IR spectral region, HXeCC radicals can be decomposed to a local metastable configuration and then selectively recovered by resonant excitation of the XeC 2 vibrations. The novel recovery process is explained by short-range mobility of the reagents promoted by vibrational energy redistribution near the absorbing XeC 2 molecule. This means that a chemical reaction can be selectively promoted in a desired place where the chosen absorber locates. The obtained results make a strong case of solid-state reactive vibrational excitation spectroscopy of weak radiationless transitions.
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