15min:
ANALYSIS AND FIT OF THE HIGH-RESOLUTION VISIBLE SPECTRUM OF THE TWO-EQUIVALENT-TOP MOLECULE BIACETYL.

NOBUKIMI OHASHI, Department of Physics, Kanazawa University, Kakuma, Kanazawa 920-1192, Japan; JON T. HOUGEN, Optical Technology Division, NIST, Gaithersburg, MD 20899-8441, USA; CHENG-LIANG HUANG, Department of Applied Chemistry, National Chiayi University, Chiayi, Taiwan; CHEN-LIN LIU, CHI-KUNG NI, Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei 106, P.O. Box 23-166, Taiwan.

The A 1\!Au(S1)-X 1\!Ag(S0) LIF spectrum of biacetyl (CH3C(=O)C(=O)CH3) shows a long progression in the torsional vibrations of the two methyl tops. The S1 torsional level pattern can be qualitatively understood using local mode ideas applied to the two equivalent methyl rotors and symmetry ideas from the PI group G36. For the present rotational analysis, we assigned a G36 symmetry species, two local-mode torsional quantum numbers, and rotational quantum numbers JKa,Kc to each observed torsion-rotation level. Transitions were globally fit with a two-equivalent-top computer program, which uses the molecular principal axis system, a free-rotor basis set for each top, a symmetric-top basis set for the rotational functions, and a single-step diagonalization procedure. The program is similar to our two-inequivalent-top program for N-methylacetamide. Last year, we refit 179 previously published rotational lines involving 7 torsional tunneling sublevels with zero or one quantum of torsional excitation in the S1 state of biacetyl, using 14 parameters (5 for S0, 9 for S1) to obtain a standard deviation of 0.0041 cm-1. We have now extended that fit by adding 131 unpublished lines involving 5 tunneling sublevels with two quanta of torsional excitation, using 19 parameters to obtain a standard deviation of 0.0040 cm-1. Including transitions with still higher torsional excitation leads to a degraded standard deviation. We thus suspect that a number of higher-order terms describing top-top-overall-rotation interactions are missing from the present model, but the possibility of misassignments in the higher-energy regions must also be considered.