A. Demircan, M. Kroh, M. Pietrzyk, B. Huttl, U. Bandelow
{"title":"脉冲分裂的非拉曼红移","authors":"A. Demircan, M. Kroh, M. Pietrzyk, B. Huttl, U. Bandelow","doi":"10.1109/NUSOD.2007.4349043","DOIUrl":null,"url":null,"abstract":"While usually the generation of a Stokes component is attributed to Raman scattering, we present here experimentally and numerically a mechanism which can be explained by the nonlinear Schrodinger equation alone. It can be employed to excite new frequency components on the red side, by using pulse splitting in the normal dispersion regime.","PeriodicalId":255219,"journal":{"name":"2007 International Conference on Numerical Simulation of Optoelectronic Devices","volume":"72 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2007-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Non-Raman redshift by pulse splitting\",\"authors\":\"A. Demircan, M. Kroh, M. Pietrzyk, B. Huttl, U. Bandelow\",\"doi\":\"10.1109/NUSOD.2007.4349043\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"While usually the generation of a Stokes component is attributed to Raman scattering, we present here experimentally and numerically a mechanism which can be explained by the nonlinear Schrodinger equation alone. It can be employed to excite new frequency components on the red side, by using pulse splitting in the normal dispersion regime.\",\"PeriodicalId\":255219,\"journal\":{\"name\":\"2007 International Conference on Numerical Simulation of Optoelectronic Devices\",\"volume\":\"72 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2007-10-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2007 International Conference on Numerical Simulation of Optoelectronic Devices\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NUSOD.2007.4349043\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2007 International Conference on Numerical Simulation of Optoelectronic Devices","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NUSOD.2007.4349043","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
While usually the generation of a Stokes component is attributed to Raman scattering, we present here experimentally and numerically a mechanism which can be explained by the nonlinear Schrodinger equation alone. It can be employed to excite new frequency components on the red side, by using pulse splitting in the normal dispersion regime.
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