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dc.creatorMcDiarmid, R.en_US
dc.date.accessioned2006-06-15T16:37:28Z
dc.date.available2006-06-15T16:37:28Z
dc.date.issued1967en_US
dc.identifier1967-H-10en_US
dc.identifier.urihttp://hdl.handle.net/1811/15229
dc.descriptionAuthor Institution: National Institutes of Healthen_US
dc.description.abstractThe quantum defect calculated when the origin of the sharply structured system of intense absorption bands lying to the blue of the broad $\pi^{\ast} \leftarrow \pi$ transition of trans-butene-2 is fitted to the Rydberg equation with an assumed ionization potential of 9,11 eV is found to be comparable with that obtained for transitions to ns Rydberg states of ethylene: t-butene-1.16; ethylene-1.09. The zero point energy shift between the systems origins in t-butene and perdeutero-t-butene is also comparable with that observed between light and heavy ethylene: $-230 cm^{-1} vs - 180 cm^{-1}$. From these we conclude that the $1670 {\AA}$ transition of t-butene-2 is the transition to the 4s Rydberg state of this molecule. A comparison between the vibrational frequency intervals observed in t-butene-2 and perdeutero-t-butene-2 affords an approximate description of the motions responsible for the stronger vibronic bands. A further comparison between the frequency intervals observed in the 4s Rydberg state and those reported for the ground state of the light compound indicates that the carbon-carbon double bond and the $sp^{2}$ carbon-hydrogen bonds are weaker in the 4s Rydberg state than in the ground state but that the $sp^{2}$ $carbon-sp^{3}$ carbon bonds are stronger in the Rydberg state. The vibrational structure of the $1670 {\AA}$ transition was observed to differ from that observed in the $2000 {\AA}$ transition, suggesting that the latter is not the missing first member of the Rydberg series.en_US
dc.format.extent184702 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE 1670 {\AA} TRANSITION OF trans-BUTENE-2en_US
dc.typearticleen_US


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