Photoassociation of Kr-F collision pairs in the ultraviolet

The bound←free absorption (photoassociation) of thermalized Kr(4p6 1S0)–F(2p5 2P) collision pairs has been studied in the ultraviolet in Kr/F2 gas mixtures by laser pump–probe techniques. Experiments carried out at 248 nm with two time‐delayed excimer laser pulses demonstrate that KrF(B2 Σ1/2+) molecules are produced by the photodissociation of F2, followed by the photoassociation of Kr–F collision pairs by a single ∼5 eV photon. The saturation behavior of this photoassociation process indicates that the currently accepted value for the KrF(B→X) stimulated emission cross section (2.6×10−16 cm2) is too large by at least a factor of 2. A revised value for σSE of (1.2±0.6)×10−16 cm2 is suggested. By indirectly monitoring the temporal decay of the atomic fluorine number density owing to reformation of F2, the rate constant for the recombination of F atoms in a Kr background by three‐body (2F+Kr) collisions has been determined to be kr=2×10−32 cm6 s−1.

[1]  J. H. Schloss,et al.  Excitation spectra for the photoassociation of Kr–F and Xe–I collision pairs in the ultraviolet (208–258 nm) , 1993 .

[2]  T. Nelson,et al.  Quenching constants of KrF(B, C) by Kr and Xe and the KrF(B, C) equilibrium constant , 1992 .

[3]  J. Eden,et al.  Bound→free emission spectra and photoassociation of 114Cd2 and 64Zn2 , 1991 .

[4]  T. Nelson,et al.  Cooperative two-photon-induced chemical bond formation during a Kr + F2 collision to form KrF , 1990 .

[5]  K. Hakuta,et al.  Photoassociation of KrF Excimer at 248 nm , 1988 .

[6]  D. Geohegan,et al.  Absorption spectrum of Kr2F(4 2Γ) in the near ultraviolet and visible (335≤λ≤600 nm): Comparison with Kr+2(1( 1/2 )u) measurements , 1988 .

[7]  A. W. McCown,et al.  Spectroscopy Of Absorbers In Rare Gas-Halide Laser Plasmas , 1988, Photonics West - Lasers and Applications in Science and Engineering.

[8]  D. Geohegan,et al.  Xe2Cl and Kr2F excited state (4 2Γ) absorption spectra: measurements of absolute cross sections , 1987 .

[9]  T. Ho,et al.  Laser photolysis study of the recombination reactions of atomic chlorine in inert gases , 1987 .

[10]  R. F. Holland,et al.  Ultraviolet absorption spectrum of molecular fluorine , 1987 .

[11]  A. McCown,et al.  Absorption at 248 nm by Kr2F , 1987 .

[12]  R. Jiang,et al.  Measurements of the diffusion coefficients of atomic chlorine in rare gases , 1986 .

[13]  Geohegan,et al.  Resonantly enhanced three-photon ionization of krypton. , 1986, Physical review. A, General physics.

[14]  Minoru Obara,et al.  An advanced kinetic model of electron‐beam‐excited KrF lasers including the vibrational relaxation in KrF*(B) and collisional mixing of KrF*(B,C) , 1985 .

[15]  W. H. Beattie,et al.  The Homogeneous rate constant for the recombination of fluorine atoms with F2 as the third body , 1984 .

[16]  J. Ku,et al.  Laser photoassociation of Xe and Br(2P3/2) atoms and generation of aligned XeBr(B) molecules , 1984 .

[17]  J. Ku,et al.  Photoassociative laser‐induced fluorescence of XeCl* and kinetics of XeCl(B) and XeCl(C) in Xe , 1984 .

[18]  F. Schäfer,et al.  Picosecond gain dynamics of KrF , 1984 .

[19]  J. Eden,et al.  Ultraviolet photoassociative production of XeCl(B,C) molecules in Xe/Cl2 gas mixtures: Radiative lifetime of Xe2Cl(4 2Γ) , 1984 .

[20]  J. Ku,et al.  Photoassociative laser induced fluorescence of XeCl , 1982 .

[21]  K. Kompa,et al.  Formation of Xe∗2 by collision pair absorption at 158 nm , 1981 .

[22]  R. Waynant,et al.  Destruction of ground state XeCl molecules by HCl and rare gas collisions , 1980 .

[23]  S. L. Shostak,et al.  Transient absorpion following flash photodissociation of halogens in rare gases , 1979 .

[24]  D. Ehrlich,et al.  Condon internal diffraction in the O/sub u//sup +/. -->. O/sub g//sup +/ fluorescence of photoassociated Hg/sub 2/ , 1978 .

[25]  R. Waynant,et al.  New quenching rates applicable to the KrF laser , 1978 .

[26]  G. Quigley,et al.  Lifetime and quenching rate constants for Kr2F* and Kr2* , 1978 .

[27]  S. Searles,et al.  Radiative lifetime of KrF , 1977 .

[28]  A. Hawryluk,et al.  Gain and absorption measurements in a KrF* laser , 1977 .

[29]  H. Scheingraber,et al.  Discrete and continuous Franck Condon factors of the Mg2A1Σ+u–X1Σ+g system and their J dependence , 1977 .

[30]  C. Ultee The homogeneous recombination rate constant of F atoms at room temperature , 1977 .

[31]  G. Tisone,et al.  Spectroscopic studies of diatomic noble gas halides. II. Analysis of bound-free emission from XeBr, XeI, and KrF , 1976 .

[32]  P. Ganguli,et al.  The rate of homogeneous recombination of fluorine atoms , 1974 .

[33]  R. Vogel,et al.  The Absorption Spectrum of Fluorine1 , 1956 .

[34]  John Crank,et al.  The Mathematics Of Diffusion , 1956 .