TOWARD A COMPLETE EQUILIBRIUM STRUCTURE OF BUTADIENE; HIGH-RESOLUTION INFRARED SPEC-TROSCOPY OF BUTADIENE-1-$^{13}C_{1}$

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2004

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Ohio State University

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Considerable progress has been made toward obtaining ground state rotational constants for butadiene (BDE) and its isotopomers for use in fitting an equilibrium structure. With the exception of a microwave investigation of the weakly polar BDE-$1,1-d_{2},{^{a}}$ studies of all of the other, nonpolar species have been done with high-resolution ($0.002 cm^{-1}$) infrared spectroscopy. Rotational constants are available for BDE and BDE$-2,3-d_{2}$ from one $study^{b}$ and for the three species of BDE$-1,4-d_{2}$ from another $study.^{c}$ The present report is on BDE$-1-^{13}C_{1}$. The rotational structure in the C-type bands at $524 cm^{-1}, 900 cm^{-1}$, and $908 cm^{-1}$ in the infrared spectrum has been analyzed. Rotational constants fit to 2191 ground state combination differences derived from all three bands are (in $cm^{-1}$) A = 1.3887919 (6), B = 0.1436683 (3), and C = 0.1302251 (3). In the parent molecule of $C_{2h}$ symmetry, a Raman-active $b_{g}$ mode occurs at $908 cm^{-1}$ and an infrared-active mode occurs at essentially the same frequency. In BDE$-1-^{13}C_{1}$ of reduced, $C_{s}$ symmetry, both modes have significant infrared intensity and occur at 908 and $900 cm^{-1}$. The higher frequency mode is $CH_{2}$ flapping; the lower frequency one is $^{13}CH_{2}$ flapping. $^{d}$

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$^{a}$W. Caminati, G. Grassi, and A. Bauder Chem. Phys. Letters 148, 13, (1988). $^{b}$N. C. Craig, J. L. Davis, K. A. Hanson, M. C. Moore, and M. Lock J. Mol. Struct. 00, 000, (2004). $^{c}$N. C. Craig, K. A. Hanson, R. W. Pierce, S. D. Saylor, and R. L. Sams J. Mol. Spectrosc., submitted. $^{d}$P. Huber-W\""{a}lchli and Hs. H. G\""{u}nthard Spectrochim. Acta, 37A, 285, (1981); Yu. N. Panchenko, private communication.
Author Institution: Department of Chemistry, Oberlin College; Department of Chemistry, Pacific Northwest National Laboratory

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