INTERACTIONS IN SYMMETRIC TOP MOLECULES BETWEEN VIBRATIONAL POLYADS: ROTATIONAL AND ROVIBRATIONAL SPECTROSCOPY OF LOW-LYING STATES OF PROPYNE

Abstract

a^{a}P. Pracna, G. Graner, J. Cosl\'eou, J. Demaison, G. Wlodarczak, V.-M. Horneman, and M. Koivusaari, J. Mol. Spectrosc. 206, (2001) 150-157; H. S. P. M\""uller, P. Pracna, et al., unpublished b^{b}H. S. P. M\""uller, P. Pracna, and V.-M. Horneman, J. Mol. Spectrosc. 216, (2002) 397-407Author Institution: I. Physikalisches Institut, Universit\""at zu K\""oln; I. Physikalisches Institut, Academy of Sciences of the Czech Republic; I. Physikalisches Institut, 90014 University of Oulu; I. Physikalisches Institut, Justus-Liebig-Universit\""atA large body of very accurate (mostly 10-20 kHz) rotational transitions within the 10μm10 {\mu}m tetrad of the strongly prolate symmetric rotor propyne, H3C−C≡CHH_{3}C-C\equiv CH, had been recorded in order to analyze some weaker resonances.aresonances.^{a} The analysis, in particular for higher K transitions, indicated new problems: Interactions of members of the 10μm10 {\mu}m tetrad (v5=1,v9=v10=1,v10=3v_{5} = 1, v_{9} = v_{10} = 1, v_{10} = 3, and v8=1v_{8} = 1) with those of the 15μm15 {\mu}m dyad (v9=1v_{9} = 1 and v10=2v_{10} = 2). More than 300 rotational transitions within v10=1(Evib=330.9cm−1)v_{10} = 1 (E_{vib} = 330.9 cm^{-1}) have been recorded with J′′≤53J^{\prime\prime} \leq 53 and −11≤K⋅l10≤+16-11 \leq K \cdot l_{10} \leq +16 for a more systematic investigation into the lower excited vibrational states of propyne. Even the inclusion of many high order terms prevented the highest K transitions to be fit within experimental uncertainties, in particular those having K⋅l10≤0K \cdot l_{10} \leq 0. Inclusion of ν10\nu_{10} IR transitions from a reanalysis of the spectrum that was used in the study of the 10μm10 {\mu}m tetradatetrad^{a} confirmed these findings. It turned out that the first order energies of the K⋅l10=−12K \cdot l_{10} = -12 levels coincide to within 1cm−11 cm^{-1} with those of the overtone v10=2,K=12v_{10} = 2, K = 12 of the l10=+2l_{10} = +2 substate. A weaker Coriolis interaction occurs between v10=1,K⋅l10=−11v_{10} = 1, K \cdot l_{10} = -11 and v9=1,K⋅l9=+10.bv_{9} = 1, K \cdot l_{9} = +10.^{b} Meanwhile, the investigation of v10=1v_{10} = 1 has been completed, and those of v9=1v_{9} = 1 and v10=2v_{10} = 2 have begun. Fermi-type interactions occur between the states v10=2v_{10} = 2 and 3 and between v9=1v_{9} = 1 and v9=v10=1v_{9} = v_{10} = 1. Among the Coriolis resonances, the one between v10=2,l10=−2v_{10} = 2, l_{10} = -2 and v5=1v_{5} = 1 permitted intervibrational transitions to be detected in the submillimeter region. These interactions are expected to improve A,DKA, D_{K}, etc. for v=0v = 0. Selected details of our ongoing analyses will be presented. In addition, the relevance of these types of interactions for other symmetric top molecules will be discussed

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