3-DIMENSIONAL INFINITE-ORDER SUDDEN QUANTUM-THEORY FOR INDIRECT PHOTODISSOCIATION PROCESSES - APPLICATION TO THE PHOTOFRAGMENT YIELD SPECTRUM OF NOCL IN THE REGION OF THE T-1(1(3)A'')[-S-0(1(1)A') TRANSITION -FRAGMENT ROTATIONAL DISTRIBUTIONS AND THERMAL AVERAGES
H. Grinberg et al., 3-DIMENSIONAL INFINITE-ORDER SUDDEN QUANTUM-THEORY FOR INDIRECT PHOTODISSOCIATION PROCESSES - APPLICATION TO THE PHOTOFRAGMENT YIELD SPECTRUM OF NOCL IN THE REGION OF THE T-1(1(3)A'')[-S-0(1(1)A') TRANSITION -FRAGMENT ROTATIONAL DISTRIBUTIONS AND THERMAL AVERAGES, The Journal of chemical physics, 107(6), 1997, pp. 1849-1860
The analytical infinite order sudden (IOS) quantum theory of triatomic
photodissociation, developed in paper I, is applied to study the indi
rect photodissociation of NOCl through a real or virtual intermediate
state. The theory uses the IOS approximation for the dynamics in the f
inal dissociative channels and an Airy function approximation for the
continuum functions, The transition is taken as polarized in the plane
of the molecule; symmetric top wave functions are used for both the i
nitial and intermediate bound states; and simple semiempirical model p
otentials are employed for each state. The theory provides analytical
expressions for the photofragment yield spectrum for producing particu
lar final fragment re-vibrational states as a function of the photon e
xcitation energy, Computations are made of the photofragment excitatio
n spectrum of NOCl in the region of the T-1(1(3)A '') <-- S-0(1(1)A')
transition for producing the NO fragment in the vibrational states n(N
O)=0, 1, and 2. The computed spectra for the unexcited n(NO)= =0 and e
xcited n(NO)=2 states are in reasonable agreement with experiment, How
ever, some discrepancies are observed for the singly excited n(NO)=1 v
ibrational state, indicating deficiencies in the semiempirical potenti
al energy surface. Computations for two different orientations of the
in-plane transition dipole moment produce very similar excitation spec
tra, Calculations of fragment rotational distributions are performed f
or high values of the total angular momentum J, a feature that would b
e very difficult to perform with close-coupled methods, Computations a
re also made of the thermally averaged rotational energy distributions
to simulate the conditions in actual supersonic jet experiments. (C)
1997 American Institute of Physics.