ROTATIONAL SPECTROSCOPY AS A TOOL TO INVESTIGATE INTERACTIONS BETWEEN VIBRATIONAL POLYADS IN SYMMETRIC TOP MOLECULES: LOW-LYING STATES OF METHYL CYANIDE

Research Projects

Organizational Units

Journal Issue

Abstract

Recently, interactions between vibrational polyads were studied for propyne, H3CCCH; in particular those between v10=1 at 30,μm with the 15,μm dyad (v9=1, v10=2),} {\bf 216} (2002) 397$-Extra close brace or missing open brace407.}} {\bf 102} (2004) 1555407.}} {\bf 102} (2004) 1555-Extra close brace or missing open brace1568.} as well as between that dyad and the 10\,1568.} as well as between that dyad and the 10\,\mumtetrad(v_5 = 1$, v9=v10=1, v10=3, v8=1)b. Pronounced effects were caused by Δv10=±1, ΔK=0, Δl=±3 Fermi-type resonances at K≈12. Such resonances had not been found thus far for the isoelectronic methyl cyanide, H3CCN, molecule despite extensive previous spectroscopic work. As methyl cyanide is also an important interstellar molecule, in particular in hot and dense molecular cores, and as it may play a role in the atmospheres of planets or of Titan, we have recorded extensive rotational and rovibrational spectra up to ∼1.6,THz and ∼1500,cm−1, respectively. The present investigations focus on the v8=0, 1, and 2 states. The ν8 mode in methyl cyanide corresponds to the ν10 mode in propyne, and it is at a rather similar energy. While the infrared data pertaining to these states help to constrain their K level structures they do not reach K≈14 which are perturbed most; the l=0 component of 2,ν8 may be an exception. The pure rotational data on the other hand access K levels well beyond these perturbations which can be easily recognized in the spectra. Since the ν9=δ(CCH) mode in propyne is missing in methyl cyanide one would expect easier assignments and analyses. However, besides Δv8=±1, ΔK=0, Δl=±3 Fermi-type resonances around K of 14, additional fairly strong resonances occur at similar K values which are described by Δv8=±1, ΔK=∓2, Δl=±1. The latter type of resonance takes even place weakly between v=0 and v8=1; an indication for this was seen previously.}ime\v{c}kov{a} {\it et al.}, {\it J. Mol. Spectrosc.} (2004) 123$-$126.} The analyses of interactions between states with v8≤2 have been largely completed. The results will be compared with those in propyne.

Description

Author Institution: I. Physikalisches Institut, Univ. Koln, 50937 Koln; and MPIfR, 53121 Bonn, Germany; JPL, California Inst. of Technol., Pasadena, CA 91109, USA; LISA, Univ. Paris 12 & Paris 7 & CNRS, 94010 Cr{e}teil, France; PNNL, Richland, WA 99352, USA

Keywords

Citation