Chinese Journal of Lasers, Volume. 52, Issue 18, 1803009(2025)

Research Progress on Frequency Conversion Technology for Laser Fusion Drivers (Invited)

Song Zhou1,2, Xiangxu Chai1,2, Xiangbing Wang1,2, Fang Wang1, Bin Feng1, Wei Zhou1, Qihua Zhu1,2, Dongxia Hu1, and Ping Li1,2、*
Author Affiliations
  • 1Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, Sichuan , China
  • 2State Key Laboratory of Crystal Materials, Jinan 250100, Shandong , China
  • show less
    Figures & Tables(14)
    Schematic diagram of the Nova laser facility's third-harmonic generation system[6]
    Nova laser facility. (a) Schematic diagram of “Type-II/Type-II” third-harmonic generation phase-matching design in the Nova laser facility[7]; (b) third-harmonic generation conversion efficiency of the Nova laser facility[6]
    Beamlet laser facility. (a) Schematic diagram of “Type-I/Type-II” phase-matching design in the Beamlet laser facility[10]; (b) third-harmonic generation conversion efficiency of the Beamlet laser facility[9]
    Comparison between experimental and numerical simulation results of high-efficiency third-harmonic generation on China’s high-power laser facilities (solid line: numerical simulation curve, dashed line: fitted curve according to experimental results)
    Temperature uniformity test results of large-aperture DKDP crystal. (a) Test device; (b) test results
    Comparison between experimental and numerical simulation results of third-harmonic generation conversion efficiency
    Fourth-harmonic generation with focusing beams[38]. (a) Schematic diagram of fourth-harmonic generation with focusing beams using non-critical phase-matching technique (SHG: second-harmonic generation crystal, FL: focusing lens, FHG: fourth-harmonic generation crystal, DS: debris shield); (b) fourth-harmonic generation experimental results
    Second-harmonic generation experimental results of three nonlinear crystals[54]. (a) DKDP; (b) YCOB; (c) LBO
    Schematic layout of the conversion experiment at Bivoj/DiPOLE[65]
    Beam profile of different moments at the third-harmonic frequency under operating conditions of 50 J/10 Hz[65]. (a) In the beginning of the experiment; (b) after temperature stabilization for 90 min
    Optimization results. (a) Temperature map of LBO crystal under high-power operation; (b) experimental results of non-critical phase-matching second-harmonic generation
    • Table 1. Performance specifications of third-harmonic generation crystals in large-scale laser facilities

      View table

      Table 1. Performance specifications of third-harmonic generation crystals in large-scale laser facilities

      NOVABeamletNIF
      D-crystalKDP(3×3 array)KDPKDP
      T-crystalKDP(3×3 array)KDPKDP
      Size /(cm×cm)27×2737×3742×42
      Roughness<5 nm RMS<5 nm RMS<1.5 nm RMS
      Roughness PSD2<15ν-1.55, 2.5‒0.12 mm
      Scratch/Dig60/2060/2040/15
      Transmitted wavefront@633 nm<0.25 λ<0.25 λ5 nm Rq, >33 mm
      PSD1<15ν-1.55, 33‒2.5 mm
      Transmitted wavefront gradient<0.25 λ<0.25 λ11 nm/cm RMS, >33 mm
      Orientation<30 μrad<15 μrad<20 μrad
      Wedge /(′)<2<12±1
      Surface flatness /μm663.16
    • Table 2. Evaluation of third-harmonic generation phase-matching accuracy

      View table

      Table 2. Evaluation of third-harmonic generation phase-matching accuracy

      Control factorControl accuracyEquivalent detune angle (Δθ@THG)
      Optical axis uniformity≤0.6×10-6~15 μrad
      Deuterium content uniformity±0.05%~10 μrad
      Reflective surface form errorPV≤5λ~5 μrad
      Beam pointing±5 μrad~5 μrad
      Temperature measurement±0.1 ℃~5 μrad
      Total~40 μrad
    • Table 3. Key parameters of DKDP, YCOB and LBO crystals for second harmonic generation[54]

      View table

      Table 3. Key parameters of DKDP, YCOB and LBO crystals for second harmonic generation[54]

      DKDP (98%)YCOB (XZ)LBO (XY)
      Interaction typeType-I(e+e-o)
      Crystal cut angles /(°)θ=36.9, φ=0θ=150.9, φ=0θ=90.0, φ=13.2
      deff (pm/V)0.4-0.950.83
      Walk off angle /mrad2.71.87.8
      Angle acceptance bandwidth /(mrad·cm)1.350.824.05
      Temperature acceptance bandwidth /(K·cm)12.71064.2
      1 µm absorption coefficient /cm⁻¹0.00150.00150.001
      Thermal conductivity /(Wm/K)1.352.33.5
      Damage threshold at 1064 nm /(GW/cm²)8.4 (1.3 ns pulse)2.4 (10 ns pulse)18.9 (10 ns pulse, 10 Hz)
      Aperture /(mm×mm)80×8030×3030 diameter
      Length of crystal /mm501515
      Coating

      Soft gel AR@515 and

      1030 nm

      E-Beam AR@515 nm

      and 1030 nm

      IAD AR@532 nm

      and 1064 nm

      Calculated efficiency 18 mm diameter beam /%708160
      Calculated efficiency 10 mm diameter beam /%9586
      Biaxial / UniaxialUniaxialBiaxialBiaxial
    Tools

    Get Citation

    Copy Citation Text

    Song Zhou, Xiangxu Chai, Xiangbing Wang, Fang Wang, Bin Feng, Wei Zhou, Qihua Zhu, Dongxia Hu, Ping Li. Research Progress on Frequency Conversion Technology for Laser Fusion Drivers (Invited)[J]. Chinese Journal of Lasers, 2025, 52(18): 1803009

    Download Citation

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

    Category: Materials

    Received: Jun. 16, 2025

    Accepted: Jul. 21, 2025

    Published Online: Sep. 17, 2025

    The Author Email: Ping Li (liping1984@caep.cn)

    DOI:10.3788/CJL250957

    CSTR:32183.14.CJL250957

    Topics