High Power Laser Science and Engineering, Volume. 11, Issue 2, 02000e22(2023)

1.2 kW all-fiber narrow-linewidth picosecond MOPA system

Jiexi Zuo1,2,3,4, Haijuan Yu1,2,3,4, Shuzhen Zou1,4, Zhiyong Dong1,4, Chaojian He1,4, Shuang Xu1,2,3,4, Chaoyu Ning1,2,3,4, Xuechun Chen1,2,3,4, Xinyao Li1,2,3,4, and Xuechun Lin1,2,3,4、*
Author Affiliations
  • 1Laboratory of All-Solid-State Light Sources, Institute of Semiconductors, Chinese Academy of Sciences, Beijing, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
  • 3College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing, China
  • 4Beijing Engineering Technology Research Center of All-Solid-State Lasers Advanced Manufacturing, Beijing, China
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    Figures & Tables(5)
    The general layout of the MOPA system: SESAM, semiconductor saturable absorber mirror; LD, laser diode at 976 nm; WDM, 980/1060 wavelength division multiplexer; YSF, ytterbium-doped single-mode fiber; FBG, fiber Bragg grating; ISO, isolator; BP, bandpass filter; LMA, large mode-field area; CPS, cladding pump stripper; XLMA, extra-large mode area; DM, dichroic mirror.
    Measurement results of the seed: (a) spectral width in the logarithmic scale (with a resolution of 0.02 nm); (inset) snapshot of pulse train; (b) trace of intensity autocorrelation; (c) spectrum of pre-amplified signal: after and (inset) before the BPF2.
    (a) Experimentally observed spectral evolution with different pumping currents; (b) typical spectral evolution of an unchirped pulse under SPM; (c) signal bandwidth of seed and after amplification; (d) autocorrelation trace of the ultimate pulse.
    (a) Raman content versus pump current of the first booster amplifier; (inset) global spectrum under 6 A pump measured at ISO4; (b) output power versus pump of the second booster amplifier; (c) spectrum at 1220 W output measured at the end of the XLMA.
    Output stability of the system. (a) With a full collimated beam captured by a charge-coupled device (CCD); (inset) sampling spot selected by pinhole; (b) Fourier transform of the temporal trace; (c) power stability within 1 hour.
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    Jiexi Zuo, Haijuan Yu, Shuzhen Zou, Zhiyong Dong, Chaojian He, Shuang Xu, Chaoyu Ning, Xuechun Chen, Xinyao Li, Xuechun Lin. 1.2 kW all-fiber narrow-linewidth picosecond MOPA system[J]. High Power Laser Science and Engineering, 2023, 11(2): 02000e22

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    Paper Information

    Category: Research Articles

    Received: Jan. 28, 2023

    Accepted: Mar. 7, 2023

    Posted: Mar. 10, 2023

    Published Online: Apr. 23, 2023

    The Author Email: Xuechun Lin (xclin@semi.ac.cn)

    DOI:10.1017/hpl.2023.26

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