Kinetic energy analysis of O(3P0) and O2(b 1Σg+) fragments produced by photolysis of ozone in the Huggins bands

The velocity profile of O2(b 1Σg+,v=0) produced by photolysis of O3 in the Huggins band region at 351.4 nm has been measured using a delayed pulsed field extraction time-of-flight technique confirming that this fragment is formed by single-photon absorption. The velocity profile of O(3P0) produced by photolysis at 322.64 nm has also been obtained. O(3P0) fragments are shown to be produced in coincidence with O2(X 3Σg−), O2(a 1Δg), and O2(b 1Σg+). The relative contribution of each of these channels to the total O(3P0) signal is reported and it is shown that spin-forbidden channels dominate the dissociation process at this wavelength. Two quite different primary crossings of the initially excited state are suggested to account for the change in the relative contribution of these three channels when photolysis is changed from resonance with a vibronic band of ozone to an off-resonance wavelength. The determination of the anisotropy parameter, β(v), for these dissociation processes suggests that the transitio...

[1]  P. O’Keeffe,et al.  Photodissociation of ozone between 335 and 352 nm to give O2(b1Σ+g)+O(3PJ) , 1998 .

[2]  M. Kawasaki,et al.  Wavelength and temperature dependence of the absolute O(1D) production yield from the 305–329 nm photodissociation of ozone , 1998 .

[3]  David H. Parker,et al.  ANGULAR DISTRIBUTIONS FOR PHOTODISSOCIATION OF O2 IN THE HERZBERG CONTINUUM , 1998 .

[4]  G. Hancock,et al.  Spin-forbidden dissociation of ozone in the Huggins bands , 1998 .

[5]  M. Kawasaki,et al.  Photochemistry of Ozone: Surprises and Recent Lessons , 1998, Science.

[6]  A. Ravishankara,et al.  Quantum yields of O(¹D) in the photolysis of ozone between 289 and 329 nm as a function of temperature , 1998 .

[7]  P. Houston,et al.  SPEED-DEPENDENT ANISOTROPY PARAMETERS IN THE UV PHOTODISSOCIATION OF OZONE , 1997 .

[8]  M. Kawasaki,et al.  Photofragment excitation spectrum for O(1D) from the photodissociation of jet-cooled ozone in the wavelength range 305–329 nm , 1997 .

[9]  G. Hancock,et al.  A DIRECT MEASUREMENT OF THE O(1D) QUANTUM YIELDS FROM THE PHOTODISSOCIATION OF OZONE BETWEEN 300 AND 328 NM , 1997 .

[10]  R. C. Richter,et al.  Relative quantum yields for O1D production in the photolysis of ozone between 301 and 336 nm: evidence for the participation of a spin-forbidden channel , 1997 .

[11]  M. Kawasaki,et al.  Observation of the spin-forbidden O(1D) + O2(X3Σg-) channel in the 317-327 nm photolysis of ozone , 1996 .

[12]  J. Syage Photofragment imaging by sections for measuring state‐resolved angle‐velocity differential cross sections , 1996 .

[13]  M. Kawasaki,et al.  Photodissociation Processes of Ozone in the Huggins Band at 308−326 nm: Direct Observation of O(1D2) and O(3Pj) Products , 1996 .

[14]  C. M. Sadowski,et al.  Time-of-flight measurements of the kinetic energies of the O2(a1Δg) fragment from the photolysis of ozone between 287 and 331 nm , 1995 .

[15]  F. Comes,et al.  O(1D) QUANTUM YIELDS OF OZONE PHOTOLYSIS IN THE UV FROM 300 NM TO ITS THRESHOLD AND AT 355 NM , 1995 .

[16]  J. Joens Reassignment of the vibrational structure of the Huggins absorption band of ozone , 1994 .

[17]  M. El-Sayed,et al.  The one dimensional photofragment translational spectroscopic technique: intramolecular clocking of energy redistribution for molecules falling apart , 1994 .

[18]  T. Slanger,et al.  Oxygen spectroscopy below 5.1 eV , 1988 .

[19]  H. Levene,et al.  The effect of parent internal motion on photofragment rotational distributions: Vector correlation of angular momenta and C2v symmetry breaking in dissociation of AB2 molecules , 1987 .

[20]  D. Katayama New vibrational quantum number assignments for the UV absorption bands of ozone based on the isotope effect , 1979 .

[21]  K. Wilson,et al.  Triatomic Photofragment Spectra. II. Angular Distributions from NO2 Photodissociation , 1972 .

[22]  G. Hancock,et al.  Product channels in the near-UV photodissociation of ozone , 1995 .