THE HYPERFINE STRUCTURE IN THE $B^{1}\Pi\rightarrow X^{1}\Sigma$ TRANSITION OF THE LuF MOLECULE

dc.creator	Bacis, R.	en_US
dc.creator	Effantin, C.	en_US
dc.creator	D'Incan, J.	en_US
dc.date.accessioned	2006-06-15T13:39:52Z
dc.date.available	2006-06-15T13:39:52Z
dc.date.issued	1975	en_US
dc.identifier	1975-Sigma-02	en_US
dc.identifier.uri	http://hdl.handle.net/1811/9399
dc.description	Author Institution: Laboratoire de Spectrometrie Ionique et Mol\'{e}culaire, Universite Lyon I	en_US
dc.description.abstract	The 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.extent	81646 bytes
dc.format.mimetype	image/jpeg
dc.language.iso	English	en_US
dc.publisher	Ohio State University	en_US
dc.title	THE HYPERFINE STRUCTURE IN THE $B^{1}\Pi\rightarrow X^{1}\Sigma$ TRANSITION OF THE LuF MOLECULE	en_US
dc.type	article	en_US