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dc.creatorLaufer, J. C.en_US
dc.creatorKopelman, Raoulen_US
dc.date.accessioned2006-06-15T13:23:38Z
dc.date.available2006-06-15T13:23:38Z
dc.date.issued1971en_US
dc.identifier1971-C-4en_US
dc.identifier.urihttp://hdl.handle.net/1811/8646
dc.description$^{1}$ C. Laufer and R. Kopelman, J. Chem. Phys. 53, 3674 (1970). $^{2}$ R. Bernstein, J. Chem. Phys. 50, 4842 (1969). $^{3}$ M. P. Marzocchi, H. Bonadeo, and G. Taddci, J. Chem. Phys. 53, 867 (1970).""en_US
dc.descriptionAuthor Institution: Department of Chemistry, University of Michiganen_US
dc.description.abstractThe benzene $C^{13}$ shift for the gas phase $a_{20}$ vibrational mode was calculated and found to be $0.37 cm^{-1}$. This value was combined with data from the exciton density-of-states and exciton interaction parameters for the isotopically pure $C_{6}H_{6}$ $crystal^{1}$ to calculate the density-of-states and spectral absorption functions for the natural abundance crystal. These calculations will be compared with recent experimental $data.^{2,3}$en_US
dc.format.extent86319 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE CARBON-13 SHIFT IN THE BENZENE $a_{2}$ MODE AND THE INFRARED EXCITION SPECTRUM OF THE NATURAL ABUNDANCE BENZENE CRYSTALen_US
dc.typearticleen_US


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