STRUCTURE OF THE CARBON-CHAIN RADICALS CCCN AND CCCCH

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1995

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Ohio State University

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The millimeter-wave rotational spectra of $CCC^{15}N$ and the single $^{13}C$ isotopic species of the CCCN and CCCCH radicals were measured and the same set of rotational, centrifugal distortion, and spin-rotation constants used to describe the normal species [Gottlieb et al., Astrophys. j. 275, 916 (1983)] were determined. Owing to a large Fermi-contact interaction at the terminal carbon, hyperfine structure was resolved in $^{13}CCCCH.$ Measurements of the fundamental $N = 1 \rightarrow 0$ rotational transition of CCCCH with a Fourier transform spectrometer described in the accompanying talk by $Chen et al.^{1}$ yielded precise values of the Fermi-contact and dipole-dipole hyperfine coupling constants in all four $^{13}C$ species. The Fermi-contact interaction is of order a factor of two larger in CCCN, allowing determination of hyperfine coupling constant b in $^{13}CCCN$ and $C^{13}CCN$ from the millimeter-wave rotational spectra. Substitution $(r_{s})$ structures were determined for both radicals. The equilibrium geometry of CCCN has been determined both from large-scale coupled cluster calculations including connected triple substitutions [RCCSD(T)] as well as by a mixed experimental-theoretical procedure. Less extensive RCCSD(T) calculations were also carried out for CCCCH.

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1. W. Chen. S.T. Novick, M. C. McCarthy, C.A. Gottlieb, and P. Thaddeus, accompanying paper presented during this Symposium.
Author Institution: Harvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138; Harvard University, Cambridge, MA 02138.; Universität Göttingen, Tammannstr. 6, D-37077 Göttingen, Germany.

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