A. Kvaran et al., (2-REMPI SPECTRA OF OMEGA=0 STATES OF THE HYDROGEN HALIDES - SPECTROSCOPY, PERTURBATIONS AND EXCITATION MECHANISMS(1)), The Journal of chemical physics, 109(14), 1998, pp. 5856-5867
(2 + I) REMPI spectra of HX (X=Cl, Br and I) have been recorded and an
alyzed by simulation calculations to derive rotational constants, band
origins and isotope shift values for a number of vibrational bands of
Omega = 0 states. Our data for HCl compare nicely with those derived
by Green et nl. by conventional analysis methods [D. S. Green et al.,
J. Mel. Spectrosc. 150, 303, 354, 388 (1991); D. S. Green and S. C. Wa
llace, J. Chem. Phys. 96, 5857 (1992)]. New spectroscopic parameters w
ere derived for eight vibrational bands which are assigned to the V((1
)Sigma(+)) state, for upsilon'=4 of the E((1)Sigma(+)) state, as well
as for five new bands in HBr. New spectroscopic parameters were derive
d for four vibrational bands which are assigned to the V state and for
upsilon'=1 of the E state in HI. Anomalies observed in energy level s
pacings, rotational parameters and isotope shift values are interprete
d as being largely due to homogeneous interactions between the V and t
he E states. It is argued that the interaction causes a compression of
rovibrational levels in the E state manifold but an expansion of leve
ls in the V stale manifold, something which might be expected for a Ry
dberg to ion-pair interaction. Variations observed in the intensity ra
tio of O and S line series to Q line series in vibrational bands of th
e E and V slates for HCl and HBr are discussed and mechanisms of two-p
hoton excitation processes are proposed. (C) 1998 American Institute o
f Physics.