{"title":"分布式反射激光器的研究进展","authors":"Y. Suematsu","doi":"10.1364/igwo.1984.tuc1","DOIUrl":null,"url":null,"abstract":"To overcome the effect of chromatic dispersion of single-mode fiber for high capacity optical fiber transmission at the lowest loss wavelength region of 1.55μm [1], semiconductor lasers with distributed reflectors operating in a fixed single-mode under rapid modulation have been developed [2]. Such DSM laser consists of tightly mode-controlled resonator, and is called as a dynamic-single-mode (DSM) laser or a single longitudinal mode laser[3].","PeriodicalId":208165,"journal":{"name":"Seventh Topical Meeting on Integrated and Guided-Wave Optics","volume":"26 3 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Progress in Distributed Reflector Lasers\",\"authors\":\"Y. Suematsu\",\"doi\":\"10.1364/igwo.1984.tuc1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"To overcome the effect of chromatic dispersion of single-mode fiber for high capacity optical fiber transmission at the lowest loss wavelength region of 1.55μm [1], semiconductor lasers with distributed reflectors operating in a fixed single-mode under rapid modulation have been developed [2]. Such DSM laser consists of tightly mode-controlled resonator, and is called as a dynamic-single-mode (DSM) laser or a single longitudinal mode laser[3].\",\"PeriodicalId\":208165,\"journal\":{\"name\":\"Seventh Topical Meeting on Integrated and Guided-Wave Optics\",\"volume\":\"26 3 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Seventh Topical Meeting on Integrated and Guided-Wave Optics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/igwo.1984.tuc1\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Seventh Topical Meeting on Integrated and Guided-Wave Optics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/igwo.1984.tuc1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
To overcome the effect of chromatic dispersion of single-mode fiber for high capacity optical fiber transmission at the lowest loss wavelength region of 1.55μm [1], semiconductor lasers with distributed reflectors operating in a fixed single-mode under rapid modulation have been developed [2]. Such DSM laser consists of tightly mode-controlled resonator, and is called as a dynamic-single-mode (DSM) laser or a single longitudinal mode laser[3].
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