K. H. Tow, Y. Léguillon, P. Besnard, L. Brilland, D. Mechin, D. Tregoat, J. Troles, P. Toupin
{"title":"Ge10As24Se68硫系光纤中1阶和2阶布里渊斯托克斯阶的激光阈值分别为6mw和30mw","authors":"K. H. Tow, Y. Léguillon, P. Besnard, L. Brilland, D. Mechin, D. Tregoat, J. Troles, P. Toupin","doi":"10.1364/ECEOC.2012.TU.4.F.3","DOIUrl":null,"url":null,"abstract":"A compact second-order Stokes Brillouin fiber laser made of microstructured chalcogenide glass is reported for the first time. This laser has very low optical pump-power threshold for Stokes conversion: 6 mW for first order and only 30 mW for second order with nonresonant pumping.","PeriodicalId":270552,"journal":{"name":"2012 38th European Conference and Exhibition on Optical Communications","volume":"21 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2012-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"6 mW and 30 mW laser threshold for respectively 1st and 2nd Brillouin Stokes order in a Ge10As24Se68 chalcogenide fiber\",\"authors\":\"K. H. Tow, Y. Léguillon, P. Besnard, L. Brilland, D. Mechin, D. Tregoat, J. Troles, P. Toupin\",\"doi\":\"10.1364/ECEOC.2012.TU.4.F.3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A compact second-order Stokes Brillouin fiber laser made of microstructured chalcogenide glass is reported for the first time. This laser has very low optical pump-power threshold for Stokes conversion: 6 mW for first order and only 30 mW for second order with nonresonant pumping.\",\"PeriodicalId\":270552,\"journal\":{\"name\":\"2012 38th European Conference and Exhibition on Optical Communications\",\"volume\":\"21 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2012-09-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2012 38th European Conference and Exhibition on Optical Communications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/ECEOC.2012.TU.4.F.3\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2012 38th European Conference and Exhibition on Optical Communications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/ECEOC.2012.TU.4.F.3","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
6 mW and 30 mW laser threshold for respectively 1st and 2nd Brillouin Stokes order in a Ge10As24Se68 chalcogenide fiber
A compact second-order Stokes Brillouin fiber laser made of microstructured chalcogenide glass is reported for the first time. This laser has very low optical pump-power threshold for Stokes conversion: 6 mW for first order and only 30 mW for second order with nonresonant pumping.