High Power Laser Science and Engineering, Volume. 9, Issue 3, 03000e41(2021)

A 3.5-kW near-single-mode oscillating–amplifying integrated fiber laser

Lingfa Zeng1, Xiaolin Wang1,2,3、*, Baolai Yang1,2,3, Hanwei Zhang1,2,3, and Xiaojun Xu1,2,3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha410073, China
  • 2State Key Laboratory of Pulsed Power Laser Technology, Changsha410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha410073, China
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    Figures & Tables(7)
    Schematic diagram of the three structures of fiber lasers: (a) fiber laser oscillator based on the FP-fiber cavity; (b) fiber laser amplifier based on the MOPA structure; (c) OAIFL.
    Schematic of the bidirectionally pumped OAIFL: (a) experimental structure; (b) schematic diagram of the fiber groove.
    Experimental results of co-pumping: (a) variation curves of the output laser power and the O–O efficiency with the pump power; (b) signal of the PD at the maximum output power and their FFT results (inset); (c) result of the beam quality M2 factor at the power of 1537 W (inset: the beam profile); (d) spectra at different output powers.
    Experimental results of bidirectional pumping: (a) variation curves of the output laser power and the O–O efficiency with the pump power; (b) signal of the PD at the highest output power and their FFT results (inset); (c) spectra at different output powers; (d) measured 3-dB bandwidth at the different output powers.
    Experimental results of bidirectional pumping after shortening the active fiber of the amplifying section: (a) spectral comparison before and after the shortening of the fiber; (b) result of the beam quality M2 factor at the power of 3517 W. Inset: a beam profile of the output laser.
    • Table 1. The main experimental parameters and results before and after the shortening of the active fiber in the amplifying section.

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      Table 1. The main experimental parameters and results before and after the shortening of the active fiber in the amplifying section.

      Length of DCYDF1 (m)Length of DCYDF2 (m)Output power (W)EfficiencySRS intensity (dB)
      8.022.0312487.5%29.92
      8.017.6311587.2%34.72
      8.017.6351787.0%23.61
    • Table 2. Comparison of the main parameters and results of the existing OAIFL.

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      Table 2. Comparison of the main parameters and results of the existing OAIFL.

      Core/cladding
      diameter of theFiber length of
      oscillatingthe oscillating
      (amplifying) section(amplifying)OutputExperimental
      (μm)section (m)power (W)M2EfficiencypurposeReference
      20/400 (20/400)1.5 (22.5)15701.3671.4%Increase the TMI threshold of the fiber oscillator[21]
      20/400 (25/400)10.0 (14.5)21901.4678.3%Narrow-linewidth laser[24]
      20/400 (20/400)2.0 (15.0)20311.4083.6%Verification of anti-back-reflected light ability[22]
      10/130 (20/130)1.3 (1.3)3001.1979.3%1018-nm fiber laser[23]
      22/400 (22/400)8.0 (17.6)35171.2387.0%High-power, high-beam-quality laserThis work
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    Lingfa Zeng, Xiaolin Wang, Baolai Yang, Hanwei Zhang, Xiaojun Xu. A 3.5-kW near-single-mode oscillating–amplifying integrated fiber laser[J]. High Power Laser Science and Engineering, 2021, 9(3): 03000e41

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    Paper Information

    Category: Research Articles

    Received: Apr. 1, 2021

    Accepted: May. 24, 2021

    Published Online: Jul. 27, 2021

    The Author Email: Xiaolin Wang (chinaphotonics@163.com), Xiaojun Xu (xuxiaojun@nudt.edu.cn)

    DOI:10.1017/hpl.2021.31

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