INFRARED SPECTRUM OF PROTONATED ACETYLENE

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1985

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Ohio State University

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We have observed some 300 lines which are most likely due to protonated acetylene $H_{2}CCH^{+}$. The band origin is at $3141.4 cm^{-1}$. The rotational structure of the band fits approximately to a parallel ($\Delta K_{a} = 0$) band of the $H_{2}CO$-type classical structure but does not fit well to the usual asymmetric rotor pattern for high J levels. This is probably due to the theoretically predicted existence of the other (non-classical) structure and the very low barrier separating $them^{1,2,3}$. Based on the ab-initio prediction by Raine and $Schaeffer^{3}$, we assign the band tentatively to the CH stretching mode of the classical structure. The possibility of tunneling protons between the two equivalent classical forms through the non-classical form causes the ``splitting” of levels. When the whole problem is treated by using $D_{6h}$ symmetry, the ``internal rotation” around the c-axis is also feasible.

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$^{1}$J.A. Pople, Proceedings of the Robert A. Welch Foundation, XVI. Theoretical Chemistry, Houston, Texas (1973). $^{2}$J. Weber, M. Yoshimine and A.D. McLean, J. Chem. Phys. 64, 4159 (1976). $^{3}$G.P. Raine and H.F. Schaefer III, J. Chem. Phys. 81, 4034 (1984).
Author Institution: Department of Chemistry, The University of Chicago; Department of Chemistry, The University of Chicago

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