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dc.creatorMoret-Bailly, J.en_US
dc.creatorCadot, J.en_US
dc.creatorBoquillon, J. P.en_US
dc.date.accessioned2006-06-15T14:00:27Z
dc.date.available2006-06-15T14:00:27Z
dc.date.issued1977en_US
dc.identifier1977-WE-4en_US
dc.identifier.urihttp://hdl.handle.net/1811/10303
dc.description$^{1}$ P. D. Maker and R. W. Terhune, Phys. Rev. 137, A801 (1965). $^{2}$ R. Y. Shen and N. Bloembergen, Phys. Rev. 137, 6A (1965).en_US
dc.descriptionAuthor Institution: Laboratoire de Spectronomie Mol\'{e}culaire, Universit\'{e} de Dijon, 6 Bd Gabriel, 21000en_US
dc.description.abstractIt has often been written that the observed intensity in externally stimulated Raman effect is proportional to the square of the $pressure.^{1,2}$ Precise measurements show, however, that at low pressure the intensity is proportional to the pressure. This result may be used for Stokes as well as for anti-Stokes lines. A theoretical explanation is given.en_US
dc.format.extent87052 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleINTENSITY OF THE LINES FOR EXTERNALLY STIMULATED RAMAN EFFECT (CARS) IN LOW PRESSURE GASESen_US
dc.typearticleen_US


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