A stable argon compound

The noble gases have a particularly stable electronic configuration, comprising fully filled s and p valence orbitals. This makes these elements relatively non-reactive, and they exist at room temperature as monatomic gases. Pauling predicted in 1933 that the heavier noble gases, whose valence electrons are screened by core electrons and thus less strongly bound, could form stable molecules. This prediction was verified in 1962 by the preparation of xenon hexafluoroplatinate, XePtF6, the first compound to contain a noble-gas atom. Since then, a range of different compounds containing radon, xenon and krypton have been theoretically anticipated and prepared. Although the lighter noble gases neon, helium and argon are also expected to be reactive under suitable conditions, they remain the last three long-lived elements of the periodic table for which no stable compound is known. Here we report that the photolysis of hydrogen fluoride in a solid argon matrix leads to the formation of argon fluorohydride (HArF), which we have identified by probing the shift in the position of vibrational bands on isotopic substitution using infrared spectroscopy. Extensive ab initio calculations indicate that HArF is intrinsically stable, owing to significant ionic and covalent contributions to its bonding, thus confirming computational predictions that argon should form a stable hydride species with properties similar to those of the analogous xenon and krypton compounds reported before.

[1]  E. G. Hope,et al.  Recent Advances in Noble-Gas Chemistry , 1998 .

[2]  A. Serra,et al.  Thermally activated glide of small dislocation loops in metals , 1999 .

[3]  M. Pettersson,et al.  Photochemistry of HNCO in Solid Xenon: Photoinduced and Thermally Activated Formation of HXeNCO † , 2000 .

[4]  D. Rodney,et al.  Dislocation Pinning by Small Interstitial Loops: A Molecular Dynamics Study , 1999 .

[5]  D. Cremer,et al.  The chemistry of the noble gas elements helium, neon, and argon — Experimental facts and theoretical predictions , 1990 .

[6]  Guinan,et al.  New mechanism of defect production in metals: A molecular-dynamics study of interstitial-dislocation-loop formation in high-energy displacement cascades. , 1991, Physical review letters.

[7]  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 .

[8]  Michael C. L. Gerry,et al.  Noble gas–metal chemical bonding? The microwave spectra, structures, and hyperfine constants of Ar–CuX(X=F, Cl, Br) , 2000 .

[9]  J. Gauss,et al.  Neon and argon bonding in first-row cations NeX+ and ArX+ (X = Li-Ne) , 1989 .

[10]  Lester Andrews,et al.  Noble Gas Complexes with BeO: Infrared Spectra of NG-BeO (NG = Ar, Kr, Xe) , 1994 .

[11]  R. Hunt,et al.  Photolysis of hydrogen and fluorine in solid argon. Matrix infrared spectra of (HF)2, (HF) (DF), and (DF)2 , 1985 .

[12]  P. Hay,et al.  The covalent and ionic states of the rare gas monofluorides , 1978 .

[13]  H. Zbib,et al.  The stress field of a general circular Volterra dislocation loop: Analytical and numerical approaches , 2000 .

[14]  B. N. Singh,et al.  Segregation of cascade induced interstitial loops at dislocations: possible effect on initiation of plastic deformation , 1997 .

[15]  A. Bement FUNDAMENTAL MATERIALS PROBLEMS IN NUCLEAR REACTORS. , 1970 .

[16]  M. Victoria,et al.  Defect cluster structure and tensile properties of copper single crystals irradiated with 600 MeV protons , 1997 .

[17]  J. J. Turner,et al.  Krypton Fluoride: Preparation by the Matrix Isolation Technique , 1963, Science.

[18]  M. Pettersson,et al.  A theoretical study of HArF, a newly observed neutral argon compound , 2001 .

[19]  J. M. Perlado,et al.  Comparative study of radiation damage accumulation in Cu and Fe , 2000 .

[20]  Michael C. L. Gerry,et al.  The microwave spectra and structures of Ar–AgX (X=F,Cl,Br) , 2000 .

[21]  L. Pauling The Formulas of Antimonic Acid and the Antimonates , 1933 .

[22]  Neil Bartlett,et al.  Concerning the nature of XePtF6 , 2000 .

[23]  G. Chaban,et al.  Ab initio calculation of anharmonic vibrational states of polyatomic systems: Electronic structure combined with vibrational self-consistent field , 1999 .

[24]  N. M. Ghoniema,et al.  Interaction and accumulation of glissile defect clusters near dislocations , 1999 .

[25]  N. Soneda,et al.  Defect production, annealing kinetics and damage evolution in α-Fe: An atomic-scale computer simulation , 1998 .

[26]  S. Zinkle,et al.  Defect accumulation in pure fcc metals in the transient regime: a review , 1993 .

[27]  M. Pettersson,et al.  On self-limitation of UV photolysis in rare-gas solids and some of its consequences for matrix studies , 1998 .

[28]  Hussein M. Zbib,et al.  3D dislocation dynamics: stress–strain behavior and hardening mechanisms in fcc and bcc metals , 2000 .

[29]  G. E. Lucas,et al.  Recent progress in understanding reactor pressure vessel steel embrittlement , 1998 .

[30]  Molecular dynamics simulation of irradiation damage cascades in copper using a many-body potential , 1994 .

[31]  M. Lorenz,et al.  Neutral Xenon Hydrides in Solid Neon and Their Intrinsic Stability , 2000 .

[32]  Mika Pettersson,et al.  The mechanism of formation and infrared-induced decomposition of HXeI in solid Xe , 1997 .

[33]  E. E. Bloom The challenge of developing structural materials for fusion power systems , 1998 .

[34]  L. Stein Removal of Xenon and Radon from Contaminated Atmospheres with Dioxygenyl Hexafluoroantimonate, O2SbF6 , 1973, Nature.

[35]  M. Pettersson,et al.  New Rare-Gas-Containing Neutral Molecules , 1999 .

[36]  N. Baluc,et al.  The microstructure and associated tensile properties of irradiated fcc and bcc metals , 2000 .

[37]  J. Johns Spectra of the protonated rare gases , 1984 .

[38]  B. Wirth,et al.  Atomistic simulation of stacking fault tetrahedra formation in Cu , 2000 .

[39]  W. Lawrence,et al.  Spectroscopy of argon fluoride and krypton fluoride exciplexes in rare gas matrices , 1996 .

[40]  M. W. Wong Prediction of a Metastable Helium Compound: HHeF , 2000 .

[41]  Wolfram Koch,et al.  Stabilities and nature of the attractive interactions in HeBeO, NeBeO, and ArBeO and a comparison with analogs NGLiF, NGBN, and NGLiH (NG = He, Ar). A theoretical investigation , 1988 .

[42]  H. Heinisch Computer simulation of high energy displacement cascades , 1990 .

[43]  Mika Pettersson,et al.  A Chemical Compound Formed from Water and Xenon: HXeOH , 1999 .

[44]  G. Pimentel,et al.  Infrared detection of xenon dichloride , 1967 .

[45]  H. Trinkaus,et al.  Radiation hardening revisited: role of intracascade clustering , 1997 .