M. Likhachev, S. Aleshkina, A. V. Shubin, M. Bubnov, E. Dianov, D. Lipatov, A. Guryanov
{"title":"大模面积高掺镱无光变暗al2o3 - p2o5 - sio2基光纤","authors":"M. Likhachev, S. Aleshkina, A. V. Shubin, M. Bubnov, E. Dianov, D. Lipatov, A. Guryanov","doi":"10.1109/CLEOE.2011.5943202","DOIUrl":null,"url":null,"abstract":"Large-mode area (LMA) Yb-doped fibers are routinely used in high-power CW and pulsed fiber lasers and amplifiers. Solubility of Yb<sup>3+</sup> ions in pure silica glass is rather small; therefore co-doping with Al<inf>2</inf>O<inf>3</inf> is required to suppress clustering. Single-mode operation in LMA fibers (core diameter ∼ 20 µm) is possible, when the refractive index difference between the core and the cladding (Δn) is about 0.002 or less. Both Al<inf>2</inf>O<inf>3</inf> and Yb<inf>2</inf>O<inf>3</inf> have a relatively high molar refractivity (∼0.0025/mol.% and 0.001/wt.%, respectively), and therefore only a small Al<inf>2</inf>O<inf>3</inf> concentration can be incorporated into a highly Yb-doped LMA fiber. Clustering of Yb<sup>3+</sup> ions results in photodarkening (PD) - degradation of the laser properties with time due to a grey loss increase. Utilization of the phosphorosilicate glass matrix allows one to suppress PD almost completely (the grey loss due to PD is 10–100 times smaller in comparison with that in the aluminosilicate fiber) [1], but a typical Δn in such fibers is about 0.005–0.015.","PeriodicalId":6331,"journal":{"name":"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)","volume":"76 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2011-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"25","resultStr":"{\"title\":\"Large-mode-area highly Yb-doped photodarkening-free Al2O3-P2O5-SiO2-Based fiber\",\"authors\":\"M. Likhachev, S. Aleshkina, A. V. Shubin, M. Bubnov, E. Dianov, D. Lipatov, A. Guryanov\",\"doi\":\"10.1109/CLEOE.2011.5943202\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Large-mode area (LMA) Yb-doped fibers are routinely used in high-power CW and pulsed fiber lasers and amplifiers. Solubility of Yb<sup>3+</sup> ions in pure silica glass is rather small; therefore co-doping with Al<inf>2</inf>O<inf>3</inf> is required to suppress clustering. Single-mode operation in LMA fibers (core diameter ∼ 20 µm) is possible, when the refractive index difference between the core and the cladding (Δn) is about 0.002 or less. Both Al<inf>2</inf>O<inf>3</inf> and Yb<inf>2</inf>O<inf>3</inf> have a relatively high molar refractivity (∼0.0025/mol.% and 0.001/wt.%, respectively), and therefore only a small Al<inf>2</inf>O<inf>3</inf> concentration can be incorporated into a highly Yb-doped LMA fiber. Clustering of Yb<sup>3+</sup> ions results in photodarkening (PD) - degradation of the laser properties with time due to a grey loss increase. Utilization of the phosphorosilicate glass matrix allows one to suppress PD almost completely (the grey loss due to PD is 10–100 times smaller in comparison with that in the aluminosilicate fiber) [1], but a typical Δn in such fibers is about 0.005–0.015.\",\"PeriodicalId\":6331,\"journal\":{\"name\":\"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)\",\"volume\":\"76 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2011-05-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"25\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEOE.2011.5943202\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE.2011.5943202","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Large-mode area (LMA) Yb-doped fibers are routinely used in high-power CW and pulsed fiber lasers and amplifiers. Solubility of Yb3+ ions in pure silica glass is rather small; therefore co-doping with Al2O3 is required to suppress clustering. Single-mode operation in LMA fibers (core diameter ∼ 20 µm) is possible, when the refractive index difference between the core and the cladding (Δn) is about 0.002 or less. Both Al2O3 and Yb2O3 have a relatively high molar refractivity (∼0.0025/mol.% and 0.001/wt.%, respectively), and therefore only a small Al2O3 concentration can be incorporated into a highly Yb-doped LMA fiber. Clustering of Yb3+ ions results in photodarkening (PD) - degradation of the laser properties with time due to a grey loss increase. Utilization of the phosphorosilicate glass matrix allows one to suppress PD almost completely (the grey loss due to PD is 10–100 times smaller in comparison with that in the aluminosilicate fiber) [1], but a typical Δn in such fibers is about 0.005–0.015.