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dc.creatorTsuboi, M.en_US
dc.creatorHamada, Y.en_US
dc.creatorKawaguchi, K.en_US
dc.creatorYamada, Chikashien_US
dc.creatorNagai, Keiichien_US
dc.creatorHirota, Eizien_US
dc.date.accessioned2006-06-15T14:31:37Z
dc.date.available2006-06-15T14:31:37Z
dc.date.issued1980en_US
dc.identifier1980-RA-4en_US
dc.identifier.urihttp://hdl.handle.net/1811/11241
dc.description$^{1}$ Y. Hamada, A. Y. Hirakawa, K. Tamagake, and M. Tsuboi, J. Mol. Spectroscopy, 35, 420 (1970). $^{2}$ M. Tsuboi and J. Overend, J. Mol. Spectroscopy, 52, 256 (1974).en_US
dc.descriptionAuthor Institution:en_US
dc.description.abstractIn continuation of our $analysis^{1, 2}$ of the antisymmetric wagging band $(v_{a} = 1 \leftrightarrow 0$, 1020--860 $cm^{-1}$) of hydrazine, $NH_{2}NH_{2}$, an examination with $0.002 cm^{-1}$ resolution has recently been made by the use of infrared diode lasers. The J-structures of the $a-^{R}Q_{5}, b-^{R}Q_{5}, b-^{P}Q_{8}, b-^{P}Q_{9}, c-^{R}Q_{3}, c-^{P}Q_{8}, d-^{R}Q_{7}, d-^{R}Q_{5}, d-^{P}Q_{7}$, and $d-^{P}Q_{8}$ clusters have been analyzed, where a, b, c, and d are the components of the inversion splitting in each transition (C-type) (see the figure). It has been found that the inversion splitting becomes smaller with increasing J and with increasing K, both in the $v_{a}=0$ state (shown by b-c) and $v_{a}=1$ state (shown by a-d). An explanation is given for this finding. [FIGURE]en_US
dc.format.extent120401 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleINVERSION SPLITTING IN $NH_{2}NH_{2}$ AND ITS J, K-DEPENDENCEen_US
dc.typearticleen_US


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