• High Power Laser Science and Engineering
  • Vol. 6, Issue 2, 02000e15 (2018)
Wenfa Huang1、2、*, Jiangfeng Wang1、2, Xinghua Lu1、2, Tingrui Huang1、2, Jiangtao Guo1、2, Wei Fan1、2, and Xuechun Li1、2
Author Affiliations
  • 1Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2National Laboratory on High Power Laser and Physics, Shanghai 201800, China
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    DOI: 10.1017/hpl.2018.7 Cite this Article Set citation alerts
    Wenfa Huang, Jiangfeng Wang, Xinghua Lu, Tingrui Huang, Jiangtao Guo, Wei Fan, Xuechun Li. LD-pumped gas-cooled multislab Nd:glass laser amplification to joule level[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e15 Copy Citation Text show less
    Layout of the LD-pumped gas-cooled multislab Nd:glass amplifier. LD1–LD2: laser diode arrays; L1–L6: lenses; MON: monitor; 10X: expander; SA: serrated aperture; PBS: polarization beam splitter; FR: Faraday rotator; M1–M4: 1053-nm HR mirrors; DM5–DM6: dichroic mirrors.
    Fig. 1. Layout of the LD-pumped gas-cooled multislab Nd:glass amplifier. LD1–LD2: laser diode arrays; L1–L6: lenses; MON: monitor; 10X: expander; SA: serrated aperture; PBS: polarization beam splitter; FR: Faraday rotator; M1–M4: 1053-nm HR mirrors; DM5–DM6: dichroic mirrors.
    Schematic overview of the amplifier head.
    Fig. 2. Schematic overview of the amplifier head.
    Sketch overview of the fringe mirror.
    Fig. 3. Sketch overview of the fringe mirror.
    Pump light distribution: (a) experimental result; (b) theoretical prediction.
    Fig. 4. Pump light distribution: (a) experimental result; (b) theoretical prediction.
    Pump profiles at different positions.
    Fig. 5. Pump profiles at different positions.
    Gain distribution over the cross section of the four slabs.
    Fig. 6. Gain distribution over the cross section of the four slabs.
    Single-pass, thermally induced transmitted wavefront distortion through the amplifier: (a) theoretical prediction; (b) experimental result.
    Fig. 7. Single-pass, thermally induced transmitted wavefront distortion through the amplifier: (a) theoretical prediction; (b) experimental result.
    2D-Legendre polynomial analysis of the measured single-pass transmission wavefronts.
    Fig. 8. 2D-Legendre polynomial analysis of the measured single-pass transmission wavefronts.
    Wavefront aberration profile with the defocus term removed.
    Fig. 9. Wavefront aberration profile with the defocus term removed.
    Predicted and measured output energy of the amplifier as a function of the number of passes at different repetition rates for a pump pulse energy of 7.3 J. The inset shows the near-field profile of the output for a repetition rate of 0.2 Hz at a 0.5 J operation.
    Fig. 10. Predicted and measured output energy of the amplifier as a function of the number of passes at different repetition rates for a pump pulse energy of 7.3 J. The inset shows the near-field profile of the output for a repetition rate of 0.2 Hz at a 0.5 J operation.
    Output energy stability at 0.2 Hz.
    Fig. 11. Output energy stability at 0.2 Hz.
    PerformanceValue
    Refractive index 1.542
    Fluorescence lifetime 360
    Temp. coeff. refractive index () ()8.7
    Thermal expansion coeff. () ()82
    Thermal conductivity () 0.83
    Density ()2.76
    Elastic modulus ()58
    Poisson’s ratio0.232
    Table 1. Optical and thermal properties of Nd:glass slabs (NAP2).
    Wenfa Huang, Jiangfeng Wang, Xinghua Lu, Tingrui Huang, Jiangtao Guo, Wei Fan, Xuechun Li. LD-pumped gas-cooled multislab Nd:glass laser amplification to joule level[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e15
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