High Power Laser Science and Engineering, Volume. 12, Issue 1, 010000e9(2024)

Theoretical analysis of frequency modulation-to-amplitude modulation on the final optics and target of the SG II-Up laser facility

Yujia Zhang1,2, Wei Fan1,2、*, Jiangfeng Wang1,2, Xiaochao Wang1,2, Xinghua Lu1, Dajie Huang1, Shouying Xu1,2, Yanli Zhang1, Mingying Sun1,2, Zhaoyang Jiao1, Shenlei Zhou1,2, and Xiuqing Jiang1
Author Affiliations
  • 1Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
  • show less
    Figures & Tables(17)
    Schematic layout of the SG II-Up laser facility and the key unit that causes FM-to-AM conversion. DFB fiber laser, distributed feedback fiber laser; AOM, acoustic-optical modulator; YDFA, ytterbium-doped fiber amplifier; BS, beam splitter; APC, automatic polarization controller; 2-stage-PM, two-stage phase modulator; AFG, arbitrary function generator; AWG, arbitrary waveform generator; EOM, electro-optical modulator; SYNC, synchronization controller; EAMP, electric amplifier; ATD, adjustable time delay; CSF, cavity spatial filter; TSF, transmission spatial filter; AMP, amplifier; FCC, frequency conversion crystal; WFL, wedge focusing lens; BSG, beam sampling grating.
    Beam smoothing technology for a single laser beam.
    (a) The 3 GHz sinusoidal phase modulation spectrum; (b) the 3 + 20 GHz sinusoidal phase modulation spectrum.
    AM spectrum of several transfer functions: (a) pure phase transfer function; (b) symmetric exponential amplitude transfer function; (c) asymmetric exponential amplitude transfer function; (d) linear amplitude transfer function.
    Analysis diagram of FM-to-AM influencing factors of the high-power laser facility.
    Schematic diagram of dispersion compensation for the parallel grating pair.
    Temporal modulation (a) before and (b) after GVD compensation for 0.3 nm @ 3 GHz + 20 GHz phase modulation.
    Principle of pinhole aperture selection.
    Configuration of the final optics components of the SG II-Up facility.
    When the FM-to-AM is 5% @ 3 GHz, 0.15 nm after the main amplifier, the FM-to-AM on the subsequent optical components and the target surface: (a) last transmission reflector surface; (b) incident surface of the WFL; (c) BSG; (d) target.
    Time-domain modulation (measured by an Agilent DSO93004L with 30 GHz and an EOT ET-3600 with 22 GHz) at different wavelengths for the High Energy Integrated Laser Beam of the SG II-Up facility: (a) wavelength at 1052.5 nm (4.3%); (b) wavelength at 1053 nm (4.9%).
    Phase modulation with 3 GHz + 20 GHz: (a) after the main amplifier (); (b) incident surface of the WFL; (c) BSG; (d) target.
    (a) Temporal modulation before (blue) and after (red) the WFL; (b) AM spectral transfer function.
    • Table 1. Spatial filters parameters and FM-to-AM caused by the pinhole.

      View table
      View in Article

      Table 1. Spatial filters parameters and FM-to-AM caused by the pinhole.

      Spatial filteraInput lens focal length (mm)Incident beam aperture (mm)Pinhole aperture ( $\unicode{x3bc} {\mathrm{rad}}$ )FM-to-AM modulation
      TSF-122,500310±101.90.093%
      TSF-222,500310±203.80.043%
      CSF-111,883310±203.80.087%
      CSF-211,117290±217.90.080%
      CSF-311,883310±203.80.087%
      CSF-411,117290±217.90.080%
      Total——————0.2%
    • Table 2. FM-to-AM conversion of laser free transmission to the surface of each transmission mirror and the incident surface of the final optics.

      View table
      View in Article

      Table 2. FM-to-AM conversion of laser free transmission to the surface of each transmission mirror and the incident surface of the final optics.

      Spacing (mm)Modulation
      After main amplifier5%
      WPa5004.996%
      TM18970.15.020%
      TM22683.85.028%
      TM310,216.35.056%
      TM45103.45.070%
      TM56450.25.088%
      TM616085.092%
      CPP2783.55.100%
      Vacuum window105.100%
      FCC605.100%
      WFL612.515.088%
      BSG306.915.089%
      Target2005.613.710%
    • Table 3. Proportion of each frequency modulation component before and after focusing.

      View table
      View in Article

      Table 3. Proportion of each frequency modulation component before and after focusing.

      Spectral component3 GHz6 GHz17 GHz20 GHz23 GHz40 GHz
      Before focusing0.68%0.78%3.09%9.14%3.11%3.17%
      After focusing0.64%0.60%0.80%1.70%0.23%0.27%
      Transmission rate0.970.650.220.200.060.075
    • Table 4. FM-to-AM conversion of laser free transmission to the surface of each transmission mirror and the incident surface of the final optics.

      View table
      View in Article

      Table 4. FM-to-AM conversion of laser free transmission to the surface of each transmission mirror and the incident surface of the final optics.

      Spacing (mm)Modulation
      After main amplifier~5%
      WPa5005.000%
      TM18970.15.353%
      TM22683.85.459%
      TM310,216.35.862%
      TM45103.46.063%
      TM56450.26.317%
      TM616086.381%
      CPP2783.56.490%
      Vacuum window106.491%
      FCC606.493%
      WFL612.518.979%
      BSG306.918.989%
      Target2005.64.921%
    Tools

    Get Citation

    Copy Citation Text

    Yujia Zhang, Wei Fan, Jiangfeng Wang, Xiaochao Wang, Xinghua Lu, Dajie Huang, Shouying Xu, Yanli Zhang, Mingying Sun, Zhaoyang Jiao, Shenlei Zhou, Xiuqing Jiang. Theoretical analysis of frequency modulation-to-amplitude modulation on the final optics and target of the SG II-Up laser facility[J]. High Power Laser Science and Engineering, 2024, 12(1): 010000e9

    Download Citation

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

    Category: Research Articles

    Received: Aug. 11, 2023

    Accepted: Nov. 10, 2023

    Published Online: Feb. 19, 2024

    The Author Email: Wei Fan (fanweil@siom.ac.cn)

    DOI:10.1017/hpl.2023.89

    Topics