A. Azouz, N. Stelmakh, P. Langlois, J. Lourtioz, P. Gavrilovic
{"title":"Nonlinear chirp compensation in high-power (>100 W) broad spectrum (/spl sim/20 nm) pulses from mode-locked AlGaAs lasers","authors":"A. Azouz, N. Stelmakh, P. Langlois, J. Lourtioz, P. Gavrilovic","doi":"10.1109/ISLC.1994.519349","DOIUrl":null,"url":null,"abstract":"In this paper, we show that very broad pulse spectra (20 nm) can be effectively obtained by active/hybrid mode-locking of long-stripe (1 mm) high-power AlGaAs laser diodes, the spectral widths corresponding in principle to sub-100 fs pulses in the transform-limit situation. A novel technique is presented in order to analyze chirp non-linearities (i.e, high-order dispersion effects) in the laser pulses. Second- and third-order dispersion compensation is realized with an external compressor, leading to 160 fs pulses after compression with peak powers in excess of 100 W.","PeriodicalId":356540,"journal":{"name":"Proceedings of IEEE 14th International Semiconductor Laser Conference","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of IEEE 14th International Semiconductor Laser Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISLC.1994.519349","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
In this paper, we show that very broad pulse spectra (20 nm) can be effectively obtained by active/hybrid mode-locking of long-stripe (1 mm) high-power AlGaAs laser diodes, the spectral widths corresponding in principle to sub-100 fs pulses in the transform-limit situation. A novel technique is presented in order to analyze chirp non-linearities (i.e, high-order dispersion effects) in the laser pulses. Second- and third-order dispersion compensation is realized with an external compressor, leading to 160 fs pulses after compression with peak powers in excess of 100 W.