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dc.creatorColin, R.en_US
dc.date.accessioned2006-06-15T16:41:47Z
dc.date.available2006-06-15T16:41:47Z
dc.date.issued1967en_US
dc.identifier1967-V-2en_US
dc.identifier.urihttp://hdl.handle.net/1811/15371
dc.descriptionAuthor Institution: Division of Pure Physics, National Research Council of Canada Ottawa 2, Ontario, Canadaen_US
dc.description$^{1}$ R. W. B. Pearse and A. G. Gaydon, ``The Identification of Molecular Spectra'', Chapman and Hall Ltd., 1963.
dc.description.abstractTwo new band systems of the SO molecule have been photographed with high dispersion spectrographs and have been analysed. The first system, composed of two strong red degraded double headed bands is observed in emission at 9,550 and $9,630 {\AA}$ in the afterglow produced when a mixture of COS and $O_{2}$ is pumped rapidly through a microwave discharge. The rotational analysis shows these bands to be respectively the (0,0) and (1,1) bands of the b $^{1}\Sigma^{+}-X ^{3}\Sigma^{-}$ transition of the SO molecule. Weak (2,2) and (0,1) bands are also observed at low dispersion at 9,710 and 10,800 {\AA} respectively. The second system is observed in absorption around $2400 {\AA}$ at short delay times after the flash photolysis of mixtures of COS, $O_{2}$ and Ar. This system previously attributed to $SO{_{2}}^{1}$ has been analysed and is shown to be due to a $^{3}II_{(a)}-X^{3}\Sigma$ transition of SO arising from the $v^{\prime \prime}=0$ level. The vibrational numbering of the upper $^{3}II$ state is so far undetermined.en_US
dc.format.extent147287 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTWO NEW BAND SYSTEMS OF THE SO MOLECULE.en_US
dc.typearticleen_US


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