A. Obaton, J. Bernard, C. Parent, G. L. Flem, C. Labbé, P. Le Boulanger, G. Boulton
{"title":"Synthesis and Spectroscopic Investigation of Yb/sup 3+/-Er/sup 3+/-Codoped LaLiP/sub 4/O/sub 12/ Glasses Relevant for Laser Applications","authors":"A. Obaton, J. Bernard, C. Parent, G. L. Flem, C. Labbé, P. Le Boulanger, G. Boulton","doi":"10.1109/CLEOE.1998.719180","DOIUrl":null,"url":null,"abstract":"We are involved in Yb'*-E?sodoped phosphate glass research for eye-de laser source near 1535 nm, wavelength corresponding to the 'Ilt7+'l13~ E? transition [I]. Undoped and doped glasses of the composition Laz03-Li20-P20,, with L ~ L ~ P , O I ~ fonnulq have been synthesised. Absorption tiom the 'Ii5? E+and 'F,,? Yb\" ground states have been investigated. Under pumping Yb'' ions at 975 q we have studied both E? ion emission spectra and excited state dynamics ~ f ' l ~ ~ , ~ and *Ilm E? ion levels. The emission cross-mtion of the 'Im+'Its> transition at 1535 mn is high. A comparison with the 'Ill?+'Lz excited state absorption @SA) band shows that there is no overlap between them. This mthat this ESA will not perturb the emission around 1535 mn. The ludd-Ofell intensiry parameters R, (1 = 2, 4, 6) for E? ions have been calculated in order to duermine the radiative lifetimes, the branching ratios of the transitions and the oscillator strength ofthe excited state absorption %2-+'h Similar results for n, have been found previously P I The hieh Iiequency Raman peak shape, localised around 1200 cm\", is well defined and then, this enables U% to conclude that such glass is more ordered than ofher glasses. In addition, the thermal conductivity is high for a phosphate glass. In order to characterise the laser performances of this new glarq we are planning to measure gain parmeters.","PeriodicalId":404067,"journal":{"name":"CLEO/Europe Conference on Lasers and Electro-Optics","volume":"122 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"CLEO/Europe Conference on Lasers and Electro-Optics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE.1998.719180","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
We are involved in Yb'*-E?sodoped phosphate glass research for eye-de laser source near 1535 nm, wavelength corresponding to the 'Ilt7+'l13~ E? transition [I]. Undoped and doped glasses of the composition Laz03-Li20-P20,, with L ~ L ~ P , O I ~ fonnulq have been synthesised. Absorption tiom the 'Ii5? E+and 'F,,? Yb" ground states have been investigated. Under pumping Yb'' ions at 975 q we have studied both E? ion emission spectra and excited state dynamics ~ f ' l ~ ~ , ~ and *Ilm E? ion levels. The emission cross-mtion of the 'Im+'Its> transition at 1535 mn is high. A comparison with the 'Ill?+'Lz excited state absorption @SA) band shows that there is no overlap between them. This mthat this ESA will not perturb the emission around 1535 mn. The ludd-Ofell intensiry parameters R, (1 = 2, 4, 6) for E? ions have been calculated in order to duermine the radiative lifetimes, the branching ratios of the transitions and the oscillator strength ofthe excited state absorption %2-+'h Similar results for n, have been found previously P I The hieh Iiequency Raman peak shape, localised around 1200 cm", is well defined and then, this enables U% to conclude that such glass is more ordered than ofher glasses. In addition, the thermal conductivity is high for a phosphate glass. In order to characterise the laser performances of this new glarq we are planning to measure gain parmeters.