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dc.creatorCook, Thomas J.en_US
dc.creatorLevy, Donald H.en_US
dc.date.accessioned2006-06-15T17:06:04Z
dc.date.available2006-06-15T17:06:04Z
dc.date.issued1973en_US
dc.identifier1973-Q-03en_US
dc.identifier.urihttp://hdl.handle.net/1811/16090
dc.descriptionAuthor Institution: The James Franck Institute and Department of Chemistry, The University of Chicagoen_US
dc.description.abstractThe dipole moment of the electronically excited $A^{2} \Pi$ state of the CN radical has been measured as 0.56 $\pm$ 0.03 D by analyzing the electric field dependence of the level anti-crossing spectral linewidth. The theory of the Stark effect indicates that the broadening depends upon two parameters, the $A^{2}\Pi$ dipole moment and the electric dipole transition moment between the $A^{2}\Pi$ and $B^{2}\Sigma^{+}$ states. The spectral linewidth is rather insensitive to the value of the transition moment, and this quantity is not well determined from the experimental data.en_US
dc.format.extent128075 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleTHE ELECTRIC DIPOLE MOMENT OF THE $A^{2} \Pi$ STATE OF CN AS MEASURED BY LEVEL ANTI-CROSSING SPECTROSCOPYen_US
dc.typearticleen_US


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