High Power Laser Science and Engineering, Volume. 11, Issue 6, 06000e88(2023)

Experimental investigation of the stimulated Raman scattering effect in high-power nanosecond superfluorescent fiber source

Chaoyu Ning1,2,3,4, Shuzhen Zou1,4, Haijuan Yu1,2,3,4, Jiexi Zuo1,2,3,4, Xuechun Chen1,2,3,4, Shuang Xu1,2,3,4, Shifei Han1,2,3,4, Xinyao Li1,2,3,4, Wenjuan Wu1,2,3,4, Chaojian He1,4, 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(9)
    The experimental setup of the ns-SFS seed.
    The output characteristics of the ns-SFS seed. The output spectra of the unfiltered ns-SFS (a) and the filtered ns-SFSs (b). (c) The pulse profiles. (d) The fluctuations at the pulse peak of the ns-SFS seed.
    The experimental setup of the ns-SFS amplifier.
    The output spectra (a) and the pulse profiles (b) of the ns-SFS signals at an output power of approximately 18 W.
    (a) The output power and (b) pulse width of amplified ns-SFS signals as a function of pumping power, (c) the pulse profiles and (d) the details of the pulse peak of amplified ns-SFS signals at a pump power of 370 W.
    The SRS of the amplified ns-SFS with various linewidths. (a) The first-order SRS power ratio of seven ns-SFS amplifiers under different pump powers. (b) The output spectra of the ns-SFS amplifiers with a pump power of 370 W. (c) The experimental and fitted output spectra in the case of an 8 nm ns-SFS at a pump power of 370 W in a linear scale; inset, the corresponding spectra in a logarithmic coordinate. (d) The first-order SRS power ratio and the second-order SRS power ratio versus the ns-SFS seed’s FWHM linewidth at a pump power of 370 W.
    The dependence of the ASE power ratio and spectral broadening factor on the FWHM linewidth of the ns-SFS seed at a pump power of 370 W.
    Output performance of the 2 nm ns-SFS amplifier. (a) Output average power (black line) and pulse width (red line) versus pump power. (b) Pulse profiles at different output powers. (c) Output spectra dependence on the operation power. (d) Beam quality at the maximum output power of 602 W.
    • Table 1. Output power of the ns-SFS seed versus the FWHM linewidth.

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      Table 1. Output power of the ns-SFS seed versus the FWHM linewidth.

      SeedOutputSeedOutput
      linewidth (nm)power (mW)linewidth (nm)power (mW)
      Unfiltered ns-SFS445.0222.4
      8133.1111.5
      536.60.55.7
      330.80.253.0
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    Chaoyu Ning, Shuzhen Zou, Haijuan Yu, Jiexi Zuo, Xuechun Chen, Shuang Xu, Shifei Han, Xinyao Li, Wenjuan Wu, Chaojian He, Xuechun Lin. Experimental investigation of the stimulated Raman scattering effect in high-power nanosecond superfluorescent fiber source[J]. High Power Laser Science and Engineering, 2023, 11(6): 06000e88

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    Paper Information

    Category: Research Articles

    Received: May. 11, 2023

    Accepted: Aug. 22, 2023

    Published Online: Dec. 7, 2023

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

    DOI:10.1017/hpl.2023.72

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