ON THE ($\nu_{3} + \nu_{4}$) COMBINATION BAND OF METHANE $^{12}CH_{4}$
dc.creator | Bobin, B. | en_US |
dc.creator | Hilico, J. C. | en_US |
dc.date.accessioned | 2006-06-15T13:42:02Z | |
dc.date.available | 2006-06-15T13:42:02Z | |
dc.date.issued | 1975 | en_US |
dc.identifier | 1975-TG-07 | en_US |
dc.identifier.uri | http://hdl.handle.net/1811/9497 | |
dc.description | Author Institution: Laboratoire de Spectronomie Mol\'{e}culaire, Universit\'{e} de Dijon | en_US |
dc.description.abstract | Two ``tetrahedral” branches, In terms of the quantum number $R^{\prime}$, appear in the ($\nu_{3} + \nu_{4}$) band of methane. We assign them as the P and R branches of the transitions which reach the excited states ($R^{\prime}$ = $J^{\prime} - 2$) and ($R^{\prime}$ = $J^{\prime} + 2$), respectively. The symmetries of the lines are defined owing to a remarkable property of the 3-j symbols of type $F^{(3 {jj}^{\prime})}{A}_{2} {p p}$. The lines of the corresponding Q and R, or Q and P branches are obtained simply from differences between known ground-state levels. About 150 transitions have been assigned (see J. Physique, March 1975). A similar method is now applied to the transitions on the ($R^{\prime}$ = $j^{\prime}$, $j^{\prime}$ $\pm$ 1) excited states. The preliminary results are quite encouraging. | en_US |
dc.format.extent | 98056 bytes | |
dc.format.mimetype | image/jpeg | |
dc.language.iso | English | en_US |
dc.publisher | Ohio State University | en_US |
dc.title | ON THE ($\nu_{3} + \nu_{4}$) COMBINATION BAND OF METHANE $^{12}CH_{4}$ | en_US |
dc.type | article | en_US |
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