{"title":"Nanosecond-Pulsed Hybrid Thulium-Raman Fiber Amplifier at 2.1 $\\mu\\mathrm{m}$","authors":"André W. Edvardsen, L. G. Holmen","doi":"10.1109/cleo/europe-eqec57999.2023.10232726","DOIUrl":null,"url":null,"abstract":"Laser sources operating around 2.1 μm are attractive for a range of applications in areas such as remote sensing, free-space optical communication, defense and medicine. Most commonly, holmium-doped fibers pumped by thulium-doped fiber lasers at 1.95 μm are used to reach this spectral regime, but several studies have shown that holmium-doped fiber amplifiers have a much lower efficiency than theoretically possible [1]. Coincidentally, the wavelength 2.1μm lies close to the peak Raman shift (~ 13 THz in silica) of the 1.95μm pump. This means that amplifiers can be developed where 2.1 μm light (called Stokes) could be amplified through stimulated Raman scattering (SRS) in a passive fiber instead of through stimulated emission in a Ho-doped fiber.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"37 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Oceans","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/cleo/europe-eqec57999.2023.10232726","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Laser sources operating around 2.1 μm are attractive for a range of applications in areas such as remote sensing, free-space optical communication, defense and medicine. Most commonly, holmium-doped fibers pumped by thulium-doped fiber lasers at 1.95 μm are used to reach this spectral regime, but several studies have shown that holmium-doped fiber amplifiers have a much lower efficiency than theoretically possible [1]. Coincidentally, the wavelength 2.1μm lies close to the peak Raman shift (~ 13 THz in silica) of the 1.95μm pump. This means that amplifiers can be developed where 2.1 μm light (called Stokes) could be amplified through stimulated Raman scattering (SRS) in a passive fiber instead of through stimulated emission in a Ho-doped fiber.