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dc.creatorButcher, Samuelen_US
dc.creatorCahill, P.en_US
dc.date.accessioned2006-06-15T13:08:19Z
dc.date.available2006-06-15T13:08:19Z
dc.date.issued1961en_US
dc.identifier1961-C-8en_US
dc.identifier.urihttp://hdl.handle.net/1811/8054
dc.description$^{*}$The research was made possible by support extended Harvard University by the Office of Naval Research under ONR Contract Nonr 1866, Task Order XIV. $^{\dagger}$National Science Foundation Predoctoral Fellow, 1958--1961. $^{\ddag}$Monsanto Chemical Company, Fellowship, 1959--1961. $^{1}$D. Lide, Jr., J. Chem. Phys., 19, 1605 (1956). $^{2}$D. Kivelson, J. Chem. Phys., 22, 1733 (1954).en_US
dc.descriptionAuthor Institution: Mallinckrodt Chemical Laboratory, Harvard Universityen_US
dc.description.abstractThe microwave spectrum of methyl stannane has been $reinvestigated.^{1}$ Ground state transitions for $J = 0\rightarrow 1$ were measured for seven tin isotopes (116 to 124). Three torsional states for each of the 116, 118 and 120 isotopes were observed to be split into doublets due to vibration-internal rotation interaction, and their frequencies were fitted to Kivelson’s $equation^{2}$ \[ \nu/2 ={B_{v}+G_{v}<m|\pi^{2}|m>+F_{v}< m|1-\cos 3 \theta|m>} \] Values $F_{v} =--17.568$ mc. And $G_{v} =--0.3525$ mc, were obtained, from which the torsional satellites of all the isotopes were calculated and agreed to within 0.3 mc. with observed transitions. From the observed splittings of the torsional states a barrier of $650 \pm 30$ calories was calculated. Correlations between molecules in this series will be discussed.en_US
dc.format.extent95173 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleBARRIER TO INTERNAL ROTATION IN METHYL $STANNANE^{*}$en_US
dc.typearticleen_US


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