{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1363670318811998720.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1063/1.1653164"}},{"identifier":{"@type":"URI","@value":"https://pubs.aip.org/aip/apl/article-pdf/16/5/209/18423140/209_1_online.pdf"}}],"dc:title":[{"@value":"TRANSIENT STIMULATED ROTATIONAL AND VIBRATIONAL RAMAN SCATTERING IN GASES"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Using a mode-locked ruby laser, stimulated rotational and vibrational Raman scattering has been observed in a variety of high-pressure gases, where previously no stimulated scattering has been reported. Pulse energy conversion efficiencies as high as 70% have been obtained. Evidence for a strong optical Stark effect is seen in the gases producing rotational scattering. Self-focusing in a collimated beam is observed in N2O and CO2.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383670318811998721","@type":"Researcher","foaf:name":[{"@value":"M. E. Mack"}],"jpcoar:affiliationName":[{"@value":"United Aircraft Research Laboratories, East Hartford, Connecticut 06108"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670318811998723","@type":"Researcher","foaf:name":[{"@value":"R. L. Carman"}],"jpcoar:affiliationName":[{"@value":"Gordon McKay Research Laboratory, Harvard University, Cambridge, Massachusetts 02138"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670318811998722","@type":"Researcher","foaf:name":[{"@value":"J. Reintjes"}],"jpcoar:affiliationName":[{"@value":"Gordon McKay Research Laboratory, Harvard University, Cambridge, Massachusetts 02138"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670318811998720","@type":"Researcher","foaf:name":[{"@value":"N. Bloembergen"}],"jpcoar:affiliationName":[{"@value":"Gordon McKay Research Laboratory, Harvard University, Cambridge, Massachusetts 02138"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00036951"},{"@type":"EISSN","@value":"10773118"}],"prism:publicationName":[{"@value":"Applied Physics Letters"}],"dc:publisher":[{"@value":"AIP Publishing"}],"prism:publicationDate":"1970-03-01","prism:volume":"16","prism:number":"5","prism:startingPage":"209","prism:endingPage":"211"},"reviewed":"false","url":[{"@id":"https://pubs.aip.org/aip/apl/article-pdf/16/5/209/18423140/209_1_online.pdf"}],"createdAt":"2004-02-03","modifiedAt":"2024-02-05","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360565169058225920","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Effect of Pump and Probe Light Field on Picosecond Time-Resolved Resonance Raman Spectra of S1  <i>trans</i>-Stilbene. Disagreement between Stokes- and Anti-Stokes Scattering Frequencies"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1063/1.1653164"},{"@type":"CROSSREF","@value":"10.1246/bcsj.75.1075_references_DOI_Iq3Scoc3Bx05V70bOvROS2jyjF9"}]}