* Institut für Physikalische Chemie, Abteilung Chemische Physik, Universität Kiel. Olshausenstrasse 40 60. D 24098 Kiel. Germany; + Laboratoire de Spectroscopie Hertzienne, URA CNRS 249. Bâtiment P5, Université de Lille I, 59655 Villeneuve D'Ascq Cedex. France; and \(\ddagger\) Department of Physica
Analysis of l-type resonance in the microwave spectrum of trioxane in states υ1(E) = 1 and υ2(E) = 1
✍ Scribed by A.P. Cox; D.J. Finnigan; M.J. Whittle
- Publisher
- Elsevier Science
- Year
- 1974
- Tongue
- English
- Weight
- 586 KB
- Volume
- 25
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
✦ Synopsis
the perturbation formula are evident even at the J= 6
Miliimetre wave spectra of trioxane, (CHzO)g , in its ground state and several excited vibrational states have been reported by Bellet-et al. [l] _ Measured rotational transitions of two degenerate states v,(E) = 1 and u2(E) = 1 were analysed using the perturbation formula of Grenier-Besson and Amat [2] _ Significant discrepancies between calculated and observed frequencies were obtained for both states, particularly for high J, low Kl -1 transitions of the u2(E) = 1 state. The perturbation treatment is only expected to be valid [2] if the following inequalities hold: * 7transition. Errors arise therefore through the use of the perturbation treatment due to Z-type resonance associated with the (Z, KIHVR1Z+2, K+ 2) matrix elements, where H& is the vibration-rotation hamil-.tonian. The presence of i-type resonance precludes rtype resonance effects, associated with the (1, KI HVR I I+ 2, K 7 1) elements, arising from inekprality (1 b). Other, higher order, off-diagonal elements might contribute, however, and to test this point we have treated the I-type resonance accurately by diagonalisation.
📜 SIMILAR VOLUMES
## IN HONOR OF PROF. DR. HANS B ÜRGER FOR HIS MANY VALUABLE CONTRIBUTIONS TO SCIENCE The υ 6 = 2 vibrational state of the main isotopomer of trifluorosilane, 28 SiHF 3 , has been investigated in the centimeter-and millimeter-wave ranges. Rotational spectra following the J = 1, k = l = 0 selection