dc.creator Hardwick, J. L. en_US dc.creator Brand, J. C. D. en_US dc.date.accessioned 2006-06-15T17:01:37Z dc.date.available 2006-06-15T17:01:37Z dc.date.issued 1973 en_US dc.identifier 1973-C-05 en_US dc.identifier.uri http://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, 136 en_US dc.description Author Institution: Department of Chemistry, University of Western Ontario, London en_US dc.description.abstract The 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.extent 151914 bytes dc.format.mimetype image/jpeg dc.language.iso English en_US dc.publisher Ohio State University en_US dc.title THE $^{2}B_{1}(^{2}\Pi_{u})$ STATE OF $NO_{2}$ en_US dc.type article en_US
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