dc.creator Davidson, Ernest R. en_US dc.date.accessioned 2006-06-15T13:05:37Z dc.date.available 2006-06-15T13:05:37Z dc.date.issued 1960 en_US dc.identifier 1960-B-9 en_US dc.identifier.uri http://hdl.handle.net/1811/7925 dc.description $^{*}$Supported by the United States Air Force OSR and the National Science Foundation. en_US dc.description Author Institution: Chemistry Department, Indiana University en_US dc.description.abstract The 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.extent 72913 bytes dc.format.mimetype image/jpeg dc.language.iso English en_US dc.publisher Ohio State University en_US dc.title THE (ls2s) AND $(2p\Sigma)^{2}\ {^{1}} \Sigma_{g}{^{+}}$ STATES OF THE $H_{2}$ $MOLECULE^{*}$ en_US dc.type article en_US
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