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dc.creatorVan Vaals, J. J.en_US
dc.creatorMeerts, W. Leoen_US
dc.creatorDymanus, A.en_US
dc.date.accessioned2006-06-15T14:40:39Z
dc.date.available2006-06-15T14:40:39Z
dc.date.issued1981en_US
dc.identifier1981-RC-7en_US
dc.identifier.urihttp://hdl.handle.net/1811/11606
dc.description$^{1}$ T. T\""{o}rring, J.P. Bekooy, W.L. Meerts, J. Hoeft, E. Tiemann and A. Dymanus, J. Chem. Phys. 73, 4875 (1980)en_US
dc.descriptionAuthor Institution:en_US
dc.description.abstractThe microwave spectra of the isotopic species $K^{13} $CN and $KC^{15}N$ have been determined by molecular beam electric resonance spectroscopy. The seeded beam technique was used to concentrate the population in the lower rotational and vibrational levels. For both isotopic species we observed about 20 rotational transitions originating in the ground vibrational state in the frequency range 12 to 38 GHz and determined the three rotational, as well as the five quartic centrifugal distortion constants. The rotational constants of the normal isotopic species $^{1}$ and of the $^{13}C$ and $^{15}N$ substituted species were used to determine the effective structure for the ground vibrational state and the substitution structure. The substitution structural parameters in {\AA} are $r_{CN}= 1.171(2), r_{CK} = 2.711(5), r_{KN} = 2.532(5)$.en_US
dc.format.extent77573 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE STRUCTURE OF KCN: ISOTOPIC SUBSTITUTION OF $^{13}C \ AND \ ^{15}N$en_US
dc.typearticleen_US


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