期刊文献+

高功率全光纤啁啾脉冲放大激光系统 被引量:5

High power all-fiber chirped pulse amplification laser system
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摘要 采用基于非线性偏振旋转原理的光纤被动锁模激光器作为主振荡器。输出信号脉冲的重复频率为30MHz,脉冲半高全宽为265fs。信号脉冲通过全光纤啁啾脉冲激光放大系统展宽至100ps后,经过1级芯径10μm的光纤预放大器和1级芯径50μm的光纤功率放大器将脉冲平均功率放大至10W,斜率效率41.5%。输出脉冲经光栅压缩器将脉宽压缩至594fs。 The passive mode-locked fiber laser based on the nonlinear polarization rotation principle is applied as the master oscillator.The repetition rate and pulse width of the pulse are 30 MHz and 265 fs,respectively.After stretching the pulse width to 100 ps via the chirped fiber Bragg grating,the signal is amplified by one stage of 10μm-core-diameter fiber pre-amplifier and one stage of 50μm-core-diameter fiber power amplifier.The output average power is 10 W with a slope efficiency of 41.5%.And the pulse is compressed to 594 fs via a bulk grating compressor.
出处 《强激光与粒子束》 EI CAS CSCD 北大核心 2014年第9期84-87,共4页 High Power Laser and Particle Beams
基金 中国工程物理研究院高能激光科学与技术重点实验室项目(HEL2013-02)
关键词 非线性偏振旋转 啁啾脉冲放大 B积分 nonlinear polarization rotation chirped pulse amplification B integral
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参考文献10

  • 1张红,杨春平,李伟,董海燕,杨超,王琦,肖小果.高功率全光纤激光器特性[J].强激光与粒子束,2012,24(6):1287-1289. 被引量:13
  • 2王雄,周朴,王小林,陶汝茂,司磊.全光纤主动锁模2μm掺铥脉冲激光器[J].强激光与粒子束,2013,25(10):2477-2478. 被引量:5
  • 3Eidam T,HanfS,SeiseE,etal.FemtosecondfiberCPAsystememitting830Waverageoutputpower[J].OptLett,2010,35(2):94-96.
  • 4FernándezAD,VerhoefAJ,JespersenK,etal.High-fidelity165fs5-μJpulsesfromanintegratedytterbiumfibersystem[C]//2011ConferenceonLasersandElectro-Optics(CLEO).2011:1-2.
  • 5LimpertJ,RoserF,SchimpfDN,etal.Highrepetitionrategigawattpeakpowerfiberlasersystems:challenges,design,andexperiment[J].IEEEJSelTopQuantElectron,2009,15(1):159-169.
  • 6马再如,朱启华,冯国英,陈建国.啁啾光脉冲的自相位调制效应对压缩光脉冲的影响[J].强激光与粒子束,2005,17(3):391-394. 被引量:8
  • 7RuehlA,KuhnV,WandtD,etal.Normaldispersionerbium-dopedfiberlaserwithpulseenergiesabove10nJ[J].OptExpress,2008,16(5):3130-3135.
  • 8AguergarayC,BroderickNGR,ErkintaloM,etal.Mode-lockedfemtosecondall-normalall-PMYb-dopedfiberlaserusinganonlinearamplifyingloopmirror[J].OptExpress,2012,20(10):10545-10551.
  • 9LiJing,LinHonghuan,JingFeng,etal.Intermodalinterferenceinducedsignificantfrequencymodulationtoamplitudemodulationconversioninabroadbandlarge-mode-areafiberlaser[J].OptLett,2011,36(7):1053-1055.
  • 10黄志华,林宏奂,王建军,李超,许党朋,张锐,张永亮,田小程.基于光子晶体光纤的全光纤脉冲放大器[J].强激光与粒子束,2014,26(2):3-7. 被引量:7

二级参考文献27

  • 1沈宇震,王清月,邢歧荣,石季英.啁啾脉冲激光放大中的自相位调制效应[J].物理学报,1996,45(2):214-221. 被引量:11
  • 2Simmons W W, Hunt J T. Light propagation through large laser systems[J]. IEEE J of Quantum Electronics, 1981, 17(9) :1727-1744.
  • 3Maine P, Strickland D,Bado P, et al. Generation of ultrahigh peak power pulses by chirped pulse amplification[J]. IEEE J of Quantum Electronics, 1988,24(2) : 398-403.
  • 4Chuang Y H. Propagation of light pulses in a chirped-pulse-amplification laser[J]. IEEE J of Quantum Electronics, 1993,29( 1):270-280.
  • 5Chuang Y H,Peatross J, Meyerhofer D D. Modelling the pedestal in a chirped-pulse-amplification laser[A]. Proc of SPIE[C]. 1991,1413:32-40.
  • 6Fan D Y, Zhao X M. Development and future of inertial confinement fusion laser system[R]. Annual Reports of Inertial Confinement Fusion,2000.11-12.
  • 7Perry M D, Ditmtre T, Stuart B C. Self-phase modulation in chirped-pulse amplification [J]. Optics Letteres, 1994,19(24) : 2149-2151.
  • 8AgrawalGP 贾东方 余震虹.非线性光纤光学原理及应用[M].北京:电子工业出版社,2003..
  • 9Wang Q, Geng J, Jiang Z, et al. Mode-locked Tm Ho Co doped fiber laser at 2.06μm[J]. IEEE Photon Technol Lett, 2011, 23(11) : 682- 684.
  • 10Wang Q, Geng J, Luo T, et al. Mode-locked 2 μm laser with highly thulium-doped silicate fiber[J]. Opt Lett, 2009, 34(23): 3616-3618.

共引文献29

同被引文献28

  • 1Kim K J, Shvyd'ko Y, Reiche S. A proposal for an X-ray free-electron laser oscillator with an energy recovery linac[J]. Physical Review Letters, 2008, 100: 244802.
  • 2Honda Y. Development of a photo-injector laser system for KEK ERL test accelerator[C]//Proc of IPAC. 2012: 1530-1532.
  • 3Zhao Z, Bartnik A, Wise F, et al. High-power fiber lasers for photocathode electron injectors[J]. Physical Review Special Topics-Accelae- rtor and Beams, 2014, 17: 053501.
  • 4Zhang S. Drive laser systems for electron accelerators and free-electron-lasers based on photocathode-injector energy-recovery-linac[C]// Proe of ERL. 2009: WGl10.
  • 5Ito I, Kawasaki T, Nakamura N, et al. Development of an Yb-dnped {iber laser system for an ERL photocathode[C]//Proc of IPAC. 2010: 2141-2143.
  • 6Gavrila M. Atomic stabilization in superintense laser fields[J]. Journal of Physics B ~ Atomic, Molecular and Optical Physics, 2002, 35 (18) : R147-R193.
  • 7de Boer M P, Hoogenraad J H, Vrijen R B, et al. Adiabatic stabilization against photoionization: an experimental study[J]. Physics Review A, 1994, 50(5): 4085-4098.
  • 8Birkeland T, Nepstad R, Forre M. Stabilization of helium in intense XUV laser fieldsEJ]. Physical Review Letters, 2010, 104: 1630112.
  • 9Henneberger W C. Perturbation method for atoms in intense light beams[J]. Physical Review Letters, 1968, 21(12) : 838-841.
  • 10Gavrila M. Atoms in intense laser fields[M]. New York: Academic Press, 1992:435-475.

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