Chinese Optics Letters, Volume. 23, Issue 4, 041403(2025)

280 W near-diffraction-limited picosecond amplifier system with two-segmented doped Nd:YVO4 crystals

Yiwen Jin1, Zhibin Ye2、*, Xiang Zhang3, Yang Liu1, Xiaoyan Qiu1, Yuhong Shen1, Yichao Peng1, Miao Hu4, Chong Liu1, and Dong Liu1
Author Affiliations
  • 1College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
  • 2College of Electrical and Information Engineering, Quzhou University, Quzhou 324000, China
  • 3Jiangsu Shuguang Optoelectronics Co., Ltd., Yangzhou 225009, China
  • 4College of Communication Engineering, Hangzhou Dianzi University, Hangzhou 310000, China
  • show less
    Figures & Tables(12)
    End-pumped two-segmented crystal.
    Cross-sectional temperature distributions of Nd:YVO4 with (a) 0.2 + 0.5% (atomic fraction) Nd3+-doped and (b) 0.3% (atomic fraction) Nd3+-doped on the x–z plane, and (c) the comparison of the temperature rise of the cross-section center along the z axis.
    In the case of the beam filling factor ωl/ωp = 1, the values of the 5th to 15th Zernike coefficients of the probe laser beam at the rear end of the end-pumped single-segmented and two-segmented crystals are calculated, respectively.
    Experimental setup for measuring the phase of the probe laser beam at the rear end of the crystal.
    In the cases of the single-segmented and two-segmented crystals as gain media, with the beam filling factors ωl/ωp from 0.5 to 1, the (a) spherical aberration coefficient c11 (theoretical and experimental) and (b) beam quality factor on x axis Mx2 (theoretical and experimental) are calculated and measured.
    In the cases of the single-segmented and two-segmented crystals as gain media, with the beam filling factor ωl/ωp from 0.5 to 1, (a) the spherical aberration coefficient c11 (theoretical) and (b) the beam quality factors on x axis Mx2 (theoretical and experimental) of the amplified laser at the rear end of two crystals are calculated and measured.
    In the cases of the beam filling factor ωl/ωp from 0.5 to 1 with the single-segmented and two-segmented crystals as gain media, the output power Pout is measured experimentally, and the corresponding extraction efficiency ηextr is calculated.
    In Case 1 and Case 2, the (a) output power and (b) the corresponding extraction efficiency are calculated.
    Experimental setup of high-power end-pumped multistage amplifier system.
    Output power and extraction efficiency of experimental and theoretical results of the multistage amplifier system.
    The beam quality of x and y axes is measured in the four-stage amplifier system. (a) First-stage amplifier with Pout = 63.3 W; (b) second-stage amplifier with Pout = 132.3 W; (c) third-stage amplifier with Pout = 205.2 W; and (d) fourth-stage amplifier with Pout = 280.2 W.
    • Table 1. Parameters Used in Theoretical Calculations

      View table
      View in Article

      Table 1. Parameters Used in Theoretical Calculations

      ParameterValue
      a3 mm
      b3 mm
      c12 mm
      c217 mm
      c325 mm
      ωp0.8 mm
      λp878 nm
      λl1064 nm
      T0293 K
      Kx9 W/mm·K[11,12]
      Ky9 W/mm·K[11,12]
      Kz12 W/mm·K[11,12]
      N2
      Order of G( )8
    Tools

    Get Citation

    Copy Citation Text

    Yiwen Jin, Zhibin Ye, Xiang Zhang, Yang Liu, Xiaoyan Qiu, Yuhong Shen, Yichao Peng, Miao Hu, Chong Liu, Dong Liu, "280 W near-diffraction-limited picosecond amplifier system with two-segmented doped Nd:YVO4 crystals," Chin. Opt. Lett. 23, 041403 (2025)

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Aug. 30, 2024

    Accepted: Nov. 5, 2024

    Published Online: Apr. 18, 2025

    The Author Email: Zhibin Ye (nibihzey@zju.edu.cn)

    DOI:10.3788/COL202523.041403

    CSTR:32184.14.COL202523.041403

    Topics