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dc.creatorDavidson, Ernest R.en_US
dc.date.accessioned2006-06-15T13:05:37Z
dc.date.available2006-06-15T13:05:37Z
dc.date.issued1960en_US
dc.identifier1960-B-9en_US
dc.identifier.urihttp://hdl.handle.net/1811/7925
dc.description$^{*}$Supported by the United States Air Force OSR and the National Science Foundation.en_US
dc.descriptionAuthor Institution: Chemistry Department, Indiana Universityen_US
dc.description.abstractThe electronic potential energy for the first two $1^\sigma_{g}{^{+}}$ excited stales of the hydrogen molecule has been computed as a function of internuclear distance using a twenty term expansion in elliptical coordinates with two non-linear parameters. The terms in the expansion were of the form \[ \xi^{n}_{1} \eta^{j}_{1} e^{-\alpha{_{1}} \xi{_{1}}} \xi^{\overline{n}}_{2} \eta^{\overline{1}}_{2} e^{-\alpha{_{2}}\xi{_{2}}}\quad (1+P_{12}). \]. Rather unusual potential curves were obtained which were difficult to compare directly with experimental data. Hence a method of numerical integration was devised for computing the vibrational-rotational levels arising from these curves. The results of this computation will be presented.en_US
dc.format.extent72913 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE (ls2s) AND $(2p\Sigma)^{2}\ {^{1}} \Sigma_{g}{^{+}}$ STATES OF THE $H_{2}$ $MOLECULE^{*}$en_US
dc.typearticleen_US


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