Jm. Flaud et al., H-2 SE-80 - HIGH-RESOLUTION STUDY OF THE 2-NU(1)-NU(1), 2-NU(1)+NU(3)AND NU(1)+2-NU(3) BANDS(NU(2), NU(1)+NU(2)+NU(3), 3), Journal of molecular spectroscopy, 168(2), 1994, pp. 556-566
Citations number
12
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
Using high-resolution Fourier transform spectra of monoisotopic (H2Se)
-Se-80 recorded in the 1.8- and 1.55-mu m regions, an extensive analys
is of the 2 nu(1) + nu(2), nu(1) + nu(2) + nu(3), 3 nu(1), 2 nu(1) + n
u(3), and nu(1), + 2 nu(3) bands of this molecule has been performed,
leading to a precise set of rotational levels for its {(210), (111)} a
nd {(300), (201), (102)} vibrational states. For the first set of stat
es, it was necessary to introduce the undetected (012) state in the Ha
miltonian model, and the observed levels of {(210), (111)} were least-
squares fit using a Hamiltonian which takes explicitly into account bo
th the Coriolis interactions between the levels of(210) and(111) and o
f(111)and (012), and the Darling-Dennison interaction between the leve
ls of(210) and (012). For the second set of states, namely, {(300), (2
01), (102)}, the same type of situation occurs and it was necessary as
well to introduce in the model the (003) vibrational state. In this w
ay, all the experimental levels of {(210), (111)}, and {(300), (201),
(102)} were calculated almost to within their experimental uncertainti
es and a precise set of vibrational energies and rotational and coupli
ng constants was derived with the band centers nu(0) (2 nu(1) + nu(2))
= 5612.7107, nu(0)(nu(1) + nu(2) + nu(3)) = 5613.7546, nu(0) (3 nu(1)
) = 6953.4607, nu(0) (2 nu(1) + nu(3)) = 6798.2084, and nu(0) (nu(1) 2 nu(3))= 6798.0967 cm(-1). (C) 1994 Academic Press, Inc.