• High Power Laser Science and Engineering
  • Vol. 6, Issue 4, 04000e57 (2018)
Pengfei Ma1、2, Hu Xiao1、2, Daren Meng1, Wei Liu1, Rumao Tao1、2, Jinyong Leng1、2, Yanxing Ma1、2, Rongtao Su1、2, Pu Zhou1、2、†, and Zejin Liu1、2
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies , National University of Defense Technology , Changsha 410073 , China
  • 2Hunan Provincial Collaborative Innovation Center of High Power Fiber Laser , National University of Defense Technology , Changsha 410073 , China
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    DOI: 10.1017/hpl.2018.51 Cite this Article Set citation alerts
    Pengfei Ma, Hu Xiao, Daren Meng, Wei Liu, Rumao Tao, Jinyong Leng, Yanxing Ma, Rongtao Su, Pu Zhou, Zejin Liu. High power all-fiberized and narrow-bandwidth MOPA system by tandem pumping strategy for thermally induced mode instability suppression[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e57 Copy Citation Text show less
    Experimental setup of high power tandem-pumped, narrow-bandwidth and all-fiberized fiber amplifier.
    Fig. 1. Experimental setup of high power tandem-pumped, narrow-bandwidth and all-fiberized fiber amplifier.
    (a) The measured spectral distribution of the phase modulated laser; (b) the trend of backward power ratio ($R_{bs}$) along with power scaling.
    Fig. 2. (a) The measured spectral distribution of the phase modulated laser; (b) the trend of backward power ratio ( $R_{bs}$ ) along with power scaling.
    (a) The change of$R_{bs}$along with output power; (b) the spectral bandwidth as a function of output power (inset: the frequency offset distributions at different output powers).
    Fig. 3. (a) The change of $R_{bs}$ along with output power; (b) the spectral bandwidth as a function of output power (inset: the frequency offset distributions at different output powers).
    (a) The power scaling process of the MOPA system along with increase of pump power; (b) the increase of$R_{bs}$(%) as a function of the output power.
    Fig. 4. (a) The power scaling process of the MOPA system along with increase of pump power; (b) the increase of $R_{bs}$ (%) as a function of the output power.
    (a) The change of spectral bandwidth with the output power (inset: the frequency offset at several different output powers); (b) the spectrum from 1000 to 1200 nm at 3940 W.
    Fig. 5. (a) The change of spectral bandwidth with the output power (inset: the frequency offset at several different output powers); (b) the spectrum from 1000 to 1200 nm at 3940 W.
    (a) The normalized intensity signals collected by PD; (b) the corresponding Fourier spectral distributions; (c) the measured$M^{2}$factor along with power enhancement; (d) the typical far-field beam profiles at different output powers.
    Fig. 6. (a) The normalized intensity signals collected by PD; (b) the corresponding Fourier spectral distributions; (c) the measured $M^{2}$ factor along with power enhancement; (d) the typical far-field beam profiles at different output powers.
    Pengfei Ma, Hu Xiao, Daren Meng, Wei Liu, Rumao Tao, Jinyong Leng, Yanxing Ma, Rongtao Su, Pu Zhou, Zejin Liu. High power all-fiberized and narrow-bandwidth MOPA system by tandem pumping strategy for thermally induced mode instability suppression[J]. High Power Laser Science and Engineering, 2018, 6(4): 04000e57
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