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钛宝石激光器9.5 fs脉冲输出中的啁啾镜色散补偿
引用本文:王胭脂,邵建达,董洪成,晋云霞,贺洪波,易葵,范正修,宋有建,胡明列,柴路,王清月. 钛宝石激光器9.5 fs脉冲输出中的啁啾镜色散补偿[J]. 物理学报, 2011, 60(1): 18101-018101
作者姓名:王胭脂  邵建达  董洪成  晋云霞  贺洪波  易葵  范正修  宋有建  胡明列  柴路  王清月
作者单位:(1)天津大学精密仪器与光电子工程学院超快激光研究室,光电信息技术科学教育部重点实验室,天津大学,天津 300072; (2)中国科学院上海光学精密机械研究所,中国科学院强激光材料重点实验室,上海 201800; (3)中国科学院上海光学精密机械研究所,中国科学院强激光材料重点实验室,上海 201800;中国科学院研究生院,北京 100049
基金项目:国家重点基础研究发展计划(批准号:2006CB806002)资助的课题.
摘    要:根据钛宝石激光器的要求,实验设计了中心波长800 nm带宽200 nm的啁啾镜,在700—900 nm波长范围内提供约-60 fs2群延迟色散(group delay dispersion,GDD).采用双射频离子束溅射方法进行制备,用实验室搭建的白光干涉仪进行色散性能测试,从测试结果可以看出,制备的啁啾镜的性能和设计值符合得比较好.制备得到的非成对啁啾镜在钛宝石激光谐振腔中进行色散补偿,锁模后分别获得了12 fs和9.5 fs的激光脉冲输出.这是目前报道的使用国产啁啾镜获得的最短的关键词:啁啾镜群延迟色散色散补偿钛宝石激光器

关 键 词:啁啾镜  群延迟色散  色散补偿  钛宝石激光器
收稿时间:2010-01-13

Generation of 9.5 fs pulse by use of chirped mirrors in Ti: sapphire laser cavity
Wang Yan-Zhi,Shao Jian-Da,Dong Hong-Cheng,Jin Yun-Xia,He Hong-Bo,Yi Kui,Fan Zheng-Xiu,Song You-Jian,Hu Ming-Lie,Chai Lu,Wang Qing-Yue. Generation of 9.5 fs pulse by use of chirped mirrors in Ti: sapphire laser cavity[J]. Acta Physica Sinica, 2011, 60(1): 18101-018101
Authors:Wang Yan-Zhi  Shao Jian-Da  Dong Hong-Cheng  Jin Yun-Xia  He Hong-Bo  Yi Kui  Fan Zheng-Xiu  Song You-Jian  Hu Ming-Lie  Chai Lu  Wang Qing-Yue
Affiliation:Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Graduate School of the Chinese Academy of Sciences, Beijing 100049, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Graduate School of the Chinese Academy of Sciences, Beijing 100049, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics,The Chinese Academy of Sciences, Shanghai 201800, China;Ultrafast Laser Laboratory, College of Precision Instruments and Opto-electronics Engineering, Key Laboratory ofOpto-electronic Information Science and Technology of Ministry of Education, Tianjin University, Tianjin 300072, China;Ultrafast Laser Laboratory, College of Precision Instruments and Opto-electronics Engineering, Key Laboratory ofOpto-electronic Information Science and Technology of Ministry of Education, Tianjin University, Tianjin 300072, China;Ultrafast Laser Laboratory, College of Precision Instruments and Opto-electronics Engineering, Key Laboratory ofOpto-electronic Information Science and Technology of Ministry of Education, Tianjin University, Tianjin 300072, China;Ultrafast Laser Laboratory, College of Precision Instruments and Opto-electronics Engineering, Key Laboratory ofOpto-electronic Information Science and Technology of Ministry of Education, Tianjin University, Tianjin 300072, China
Abstract:According to the requirement of Ti: sapphire laser, the optimized chirped mirrors(CM) are designed to provide group delay dispersion (GDD) of around -60 fs2 with bandwidth 200 nm at a center wavelength of 800 nm. The CMs are manufactured by time controlled ion beam sputtering.The GDD is determined by using a home-built white light interferometer. The measurement results show that the manufactured CM can meat our requirement. By balancing the intra-cavity dispersion with our manufactured chirped mirrors, 12 fs and 9.5 fs pulses have been obtained respecitively.
Keywords:chirped mirrors  group delay dispersion  dispersion compression  Ti:sapphire laser
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