红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2014年
9期
2849-2853
,共5页
匡鸿深%赵方舟%高静%葛廷武%王智勇
劻鴻深%趙方舟%高靜%葛廷武%王智勇
광홍심%조방주%고정%갈정무%왕지용
光纤激光器%自相位调制%SESAM锁模%MOPA结构
光纖激光器%自相位調製%SESAM鎖模%MOPA結構
광섬격광기%자상위조제%SESAM쇄모%MOPA결구
fiber laser%self-phase modulation%SESAM mode-locked%MOPA structure
利用主振荡功率放大(MOPA)结构高功率皮秒脉冲全光纤激光器,对高功率皮秒脉冲放大器中自相位调制(SPM)效应进行了实验研究。激光器种子源是自行搭建的半导体可饱和吸收镜(SESAM)被动锁模光纤激光器。为了抑制非线性效应,使用一个自制重频倍增器把种子脉冲的重频增加到328 MHz后再放大。放大器部分采用三级放大结构,最终获得了中心波长为1066.5 nm,3 dB光谱线宽约为2.5 nm,平均功率为91 W的稳定皮秒脉冲激光输出。实验对光脉冲在放大的过程中自相位调制引起的光谱变化进行了研究。对激光器输出光谱的分析表明,随着功率的增大,高功率光纤激光器中自相位调制效应受到入射脉冲的初始啁啾和脉冲形状的影响程度也随着变大,与此同时还受到自陡峭效应的影响。
利用主振盪功率放大(MOPA)結構高功率皮秒脈遲全光纖激光器,對高功率皮秒脈遲放大器中自相位調製(SPM)效應進行瞭實驗研究。激光器種子源是自行搭建的半導體可飽和吸收鏡(SESAM)被動鎖模光纖激光器。為瞭抑製非線性效應,使用一箇自製重頻倍增器把種子脈遲的重頻增加到328 MHz後再放大。放大器部分採用三級放大結構,最終穫得瞭中心波長為1066.5 nm,3 dB光譜線寬約為2.5 nm,平均功率為91 W的穩定皮秒脈遲激光輸齣。實驗對光脈遲在放大的過程中自相位調製引起的光譜變化進行瞭研究。對激光器輸齣光譜的分析錶明,隨著功率的增大,高功率光纖激光器中自相位調製效應受到入射脈遲的初始啁啾和脈遲形狀的影響程度也隨著變大,與此同時還受到自陡峭效應的影響。
이용주진탕공솔방대(MOPA)결구고공솔피초맥충전광섬격광기,대고공솔피초맥충방대기중자상위조제(SPM)효응진행료실험연구。격광기충자원시자행탑건적반도체가포화흡수경(SESAM)피동쇄모광섬격광기。위료억제비선성효응,사용일개자제중빈배증기파충자맥충적중빈증가도328 MHz후재방대。방대기부분채용삼급방대결구,최종획득료중심파장위1066.5 nm,3 dB광보선관약위2.5 nm,평균공솔위91 W적은정피초맥충격광수출。실험대광맥충재방대적과정중자상위조제인기적광보변화진행료연구。대격광기수출광보적분석표명,수착공솔적증대,고공솔광섬격광기중자상위조제효응수도입사맥충적초시조추화맥충형상적영향정도야수착변대,여차동시환수도자두초효응적영향。
An experimental research on self-phase modulation (SPM) of high power picosecond pulse amplifier was conducted by high-power all-fiber picosecond pulse fiber laser with an MOPA configuration. The seed source is a self-built fiber laser passively mode-locked by semiconductor saturable absorber mirror (SESAM). To avoid nonlinear effect, the repetition rate of the seed pulse should be increased to 328 MHz through a self-made repetition multiplier before amplification. The amplifier employed a three-level amplifying structure and finally received a stable picosecond pulse laser output with a center wavelength of 1 066.5 nm, a 3 dB spectrum width of 2.5 nm, and an average power of 91 W. In the experiment, there was research on change of spectrum caused by SPM in the process of amplification. An analysis of the output spectrum of the laser demonstrates that with the increase of power, the influence of the initial chirp and the shape of the pulse on the SPM effect of high power fiber laser becomes deepens. In the mean time, it is also influenced by self-steepening effect.