{"title":"光放大器的平板波导三电平模型","authors":"H. Kalinowski, Á. Guzmán","doi":"10.1109/SBMO.1993.587233","DOIUrl":null,"url":null,"abstract":"Continuous wave optical amplification in a slab waveguide can be simulated by means of the scalar Beam Propagation Method, taking in account signal and pump field propagahon through t,he waveguide. We nsed a t,hree-level scheme for the pump ~ amplification process, which reproduces the main experimental features of Erbium Doped Fiber Amplifiers pumped at 1.48pm, as reported by the COST 217 Project Group, for both short and long amplifier lengths. An alternative procedure, ablr t o reduce computational time by a large factor, is presented.","PeriodicalId":219944,"journal":{"name":"SBMO International Microwave Conference/Brazil,","volume":"70 6","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1993-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Slab Waveguide Three-Level Model For An Optical Amplifier\",\"authors\":\"H. Kalinowski, Á. Guzmán\",\"doi\":\"10.1109/SBMO.1993.587233\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Continuous wave optical amplification in a slab waveguide can be simulated by means of the scalar Beam Propagation Method, taking in account signal and pump field propagahon through t,he waveguide. We nsed a t,hree-level scheme for the pump ~ amplification process, which reproduces the main experimental features of Erbium Doped Fiber Amplifiers pumped at 1.48pm, as reported by the COST 217 Project Group, for both short and long amplifier lengths. An alternative procedure, ablr t o reduce computational time by a large factor, is presented.\",\"PeriodicalId\":219944,\"journal\":{\"name\":\"SBMO International Microwave Conference/Brazil,\",\"volume\":\"70 6\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1993-08-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"SBMO International Microwave Conference/Brazil,\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/SBMO.1993.587233\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"SBMO International Microwave Conference/Brazil,","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SBMO.1993.587233","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Slab Waveguide Three-Level Model For An Optical Amplifier
Continuous wave optical amplification in a slab waveguide can be simulated by means of the scalar Beam Propagation Method, taking in account signal and pump field propagahon through t,he waveguide. We nsed a t,hree-level scheme for the pump ~ amplification process, which reproduces the main experimental features of Erbium Doped Fiber Amplifiers pumped at 1.48pm, as reported by the COST 217 Project Group, for both short and long amplifier lengths. An alternative procedure, ablr t o reduce computational time by a large factor, is presented.
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