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dc.creatorBacis, R.en_US
dc.creatorEffantin, C.en_US
dc.creatorD'Incan, J.en_US
dc.date.accessioned2006-06-15T13:39:52Z
dc.date.available2006-06-15T13:39:52Z
dc.date.issued1975en_US
dc.identifier1975-Sigma-02en_US
dc.identifier.urihttp://hdl.handle.net/1811/9399
dc.descriptionAuthor Institution: Laboratoire de Spectrometrie Ionique et Mol\'{e}culaire, Universite Lyon Ien_US
dc.description.abstractThe utilization of a composite wall hollow cathode lamp and a Hypeac interferential spectrometer allows a far more precise study of diatomic molecular electronic spectra than with a large grating spectro-graph. From the profile of the first lines ((0-0)band of $B^{1}\Pi \rightarrow$ $X^{1}\Sigma$ transition of LuF), we were able to determine the quadrupolar constants of the fundamental and excited states, and the nuclear spin-electronic orbit constant a ($H_{IL} = a I \cdot $L) Then we show that the corresponding parameters allow us to calculate the slight dissymmeties observed for all the P, Q, and R lines.en_US
dc.format.extent81646 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE HYPERFINE STRUCTURE IN THE $B^{1}\Pi\rightarrow X^{1}\Sigma$ TRANSITION OF THE LuF MOLECULEen_US
dc.typearticleen_US


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