F. Meguellati, G. Graner, K. Burczyk, and H. Bürger [J. Mol. Spectrosc. 185, 392-402 (1997)] reported in their paper on nu(3)(A(1)) bands of the (35,37)Cl and (16,18)O isotopomers of FClO(3) that the nu(3) bands, which, although weak, could be well observed for the (16)O isotopomers, disappear almos
Can Isotopic Substitution Change a Bright State into a Dark State? The Case of thev3= 1 State of FClO3
✍ Scribed by F. Meguellati; G. Graner; K. Burczyk; H. Bürger
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 302 KB
- Volume
- 185
- Category
- Article
- ISSN
- 0022-2852
No coin nor oath required. For personal study only.
✦ Synopsis
High-resolution infrared spectra of monoisotopic samples of F 35 Cl 18 O 3 and F 37 Cl 18 O 3 have been recorded with the purpose of analyzing the n 3 fundamental at 535 cm 01 . However, this band could not be observed whereas it had been seen and studied earlier in F 35 Cl 16 O 3 . To determine the parameters of the £ 3 Å 1 state, indirect methods were used. Hot bands n n / n 3 0 n 3 (n Å 1 or 2) were first analyzed and their LSCD (Lower State Combination Differences) yielded rotational parameters of n 3 . Then, with the help of n 1 / n 3 , all rovibrational parameters of n 3 were obtained. Similar methods were applied to spectra of F 35 Cl 16 O 3 and F 37 Cl 16 O 3 to prove that the parameters of n 3 obtained in this fashion are identical to those determined directly for these isotopomers and are even more comprehensive. It is shown that the different character of n 3 in the two 18 O and in the two 16 O isotopomers is due to the fact that the former are much closer to a spherical top molecule ((A 0 0 B 0 )/A 0 Å 0.015). This is not only reflected in intensities different by two orders of magnitude but also in the very different values of a B 3 in these two pairs.
📜 SIMILAR VOLUMES
## I989 1,3-hydrogen shifts in both the neutral and ionized states of formic, monothioformic and dithioformic acids are investigated using ab initio molecular-orbital methods. Geometries of stationary points are optimized at the UHF/6-3 1 G\*\* level while relative energies are determined employin
Two new pairs of singlet-triplet A 1 ⌺ u ϩ ϳ b 3 ⌸ u mixed levels of 7 Li 2 have been observed and used here as "window" levels in cw perturbation-facilitated optical-optical double-resonance (PFOODR) experiments. Previously, only one b 3 ⌸ u vibrational level, v ϭ 19, was known to mix with the sing