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dc.creatorHill, R. A.en_US
dc.creatorEdwards, T. H.en_US
dc.date.accessioned2006-06-15T13:11:53Z
dc.date.available2006-06-15T13:11:53Z
dc.date.issued1963en_US
dc.identifier1963-E-8en_US
dc.identifier.urihttp://hdl.handle.net/1811/8224
dc.description$^{*}$Supported by the National Science Foundation. $^{1}$R.A. Hill and T.H. Edwards, J. Opt. Soc. Am. 53, 516, Abstract TB16. $^{2}$ R.A. Hill and T.H. Edwards, J. Mol. Spectroscopy 9, 494 (1962).en_US
dc.descriptionAuthor Institution: Department of Physics and Astronomy, Michigan State Universityen_US
dc.description.abstract“Ground state combination differences in four band’s, $2\nu_{1}$ and $\nu_{1} + \nu_{3}$ near $4600\;cm^{-1}$, and $2\nu_{1} + \nu_{2}$ and $\nu_{1} + \nu_{2} + \nu_{3}$ near $5600\;cm^{-1}$ have been analyzed simultaneously to obtain ground state constants for the two isotopic species $H_{2}{^{80}} Se^{1}$ and $H_{2}{^{78}} $Se, using an energy expression in which the centrifugal distortion energy is written in terms of the four distortion constants $\tau_{aaaa}, \tau_{bbbb_{1}}, \tau_{aabb}$ and $\tau_{abab}{^{2}}$.$^{2}$ Due to a Coriolis interaction between the bands $2\nu_{1}$ and $\nu_{1} + \nu_{3}$ (and also between the bands $2\nu_{1} + \nu_{2}$ and $\nu_{1} + \nu_{2} + \nu_{3})$ the first order energy expression is not able to fit either set of upper state rotational energy levels. However, buy coupling the sum rules for the interacting submatrices, $E^{+}$ with $E^{-}$ and $O^{+}$ with $O^{-}$, of the two vibrational states, we have obtained values for certain upper state constants.”en_US
dc.format.extent91331 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleNEAR INFRARED SPECTRUM OF HYDROGEN $SELENIDE^{*}$en_US
dc.typearticleen_US


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