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dc.creatorHardwick, J. L.en_US
dc.creatorBrand, J. C. D.en_US
dc.date.accessioned2006-06-15T17:01:37Z
dc.date.available2006-06-15T17:01:37Z
dc.date.issued1973en_US
dc.identifier1973-C-05en_US
dc.identifier.urihttp://hdl.handle.net/1811/15921
dc.description$^{1}$ A.E Douglas and K. P. Huber, Can. J. Phys. 43, 74 (1965). $^{2}$ J. T. Hougen, P. R. Bunker and J.W.C. Johns, J. Mol. Spectrosc. 34, 136en_US
dc.descriptionAuthor Institution: Department of Chemistry, University of Western Ontario, Londonen_US
dc.description.abstractThe manifold of $^{2}\Sigma_{g}^{-}$ vibronic levels of the $^{2}B_{1}$ electronic state of $^{14}NO_{2}$ and $^{15}NO_{2}$ observed by Douglas and $Huber^{1}$ has been extended to lower energies and new observations added for $N^{18}O_{2}$. A potential function for the bending vibration of the excited state has been calculated using a Hamiltonian which employs a curvilinear bending $coordinate.^{2}$ The potential function is approximately invariant to isotopic substitution and is well represented by a rapidly-converging Taylor series expansions about a linear equilibrium configuration. There is little or no evidence that the excited state equilibrium configuration is other than linear.en_US
dc.format.extent151914 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE $^{2}B_{1}(^{2}\Pi_{u})$ STATE OF $NO_{2}$en_US
dc.typearticleen_US


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