F. Taher et al., SPIN-ORBIT TYPE PERTURBATIONS IN THE B(1)(1)PI STATE OF SCCL - CHARACTERIZATION OF THE INTERACTING (1)(3)SIGMA(+) STATE, Journal of molecular spectroscopy, 179(2), 1996, pp. 229-236
Citations number
6
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
An extensive study of the B(1)(1) Pi --> X(1) Sigma(+) system of (ScCl
)-Sc-45-Cl-35 and (ScCl)-Sc-45-Cl-37 observed in high resolution spect
ra of the molecular thermal emission is presented. The rotational anal
ysis reveals the presence of localized perturbations in almost all bra
nches of bands with upsilon' less than or equal to 5, associated with
hyperfine broadening of the perturbed Q lines. These effects are inter
preted as consequences of the avoided crossing between B(1)(1) Pi(upsi
lon) and (1)(3) Sigma(+)(upsilon + 2) levels due to spin-orbit interac
tion. It appears possible to enter the interacting levels for both iso
topomers in the same matrix representation, the energy term elements o
nly involving equilibrium parameters of the states (isotopically scale
d to (ScCl)-Sc-45-Cl-35). A semideperturbed model of the interacting s
tates, taking account of the (upsilon similar to upsilon + 2) perturba
tions only, is first envisaged. The simultaneous fit of some 6600 line
wavenumbers in 17 bands for (ScCl)-Sc-45-Cl-35 and 7 bands for (ScCl)
-Sc-45-Cl-37 With a total standard deviation of 0.005 cm(-1) makes it
possible to characterize the (1)(3) Sigma(+) state and precisely descr
ibe B(1)(1) Pi from upsilon = 0 to upsilon = 5. Spin-orbit interaction
parameters xi(u,v+2) are determined. A full deperturbation is then ca
rried out using a model describing the levels upsilon = 0 to upsilon =
7 of (ScCl)-Sc-45-Cl-35 and upsilon = 0 to upsilon = 4 of (ScCl)-Sc-4
5-Cl-37 for the two states, and taking account of all significant inte
ractions. The following principal equilibrium molecular constants (in
cm(-1)) are obtained: -for (1)(3) Sigma(+), T-e = 5388.23, omega(e) =
367.57, omega(e)x(e) = 1.29, B-e = 0.15550, alpha(e) = 0.00081, 10(6)D
(e) = 0.111; -for B(1)(1) Pi T-e = 6016.09, omega(e) = 381.89, omega(e
)x(e) = 1.37, B-e = 0.15511, alpha(e) = 0.00079, 10(6)D(e) = 0.103. Th
e vibration-independent spin-orbit interaction parameter is directly d
etermined, xi(el) = 53.02 cm(-1). (C) 1996 Academic Press, Inc.