• Chinese Optics Letters
  • Vol. 21, Issue 5, 053401 (2023)
Dongdi Zhao, Yongpeng Zhao*, Huaiyu Cui, Bo An, Lei Li, and Yunsong Bai
Author Affiliations
  • National Key Laboratory of Science and Technology on Tunable Laser, Harbin Institute of Technology, Harbin 150080, China
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    DOI: 10.3788/COL202321.053401 Cite this Article Set citation alerts
    Dongdi Zhao, Yongpeng Zhao, Huaiyu Cui, Bo An, Lei Li, Yunsong Bai. Effect of delay time between pre-pulse and main pulse on single-pass and double-pass amplification of 46.9 nm laser[J]. Chinese Optics Letters, 2023, 21(5): 053401 Copy Citation Text show less
    Laser spatial distributions corresponding to delay times between pre-pulse and main pulse of (a) 10 µs, (b) 60 µs, and (c) 75 µs.
    Fig. 1. Laser spatial distributions corresponding to delay times between pre-pulse and main pulse of (a) 10 µs, (b) 60 µs, and (c) 75 µs.
    The laser pulse signals corresponding to different delay times.
    Fig. 2. The laser pulse signals corresponding to different delay times.
    The double-pass amplified laser spots and their intensity distributions.
    Fig. 3. The double-pass amplified laser spots and their intensity distributions.
    The double-pass amplified laser pulse signals corresponding to different delay times.
    Fig. 4. The double-pass amplified laser pulse signals corresponding to different delay times.
    The radial distributions of (a) the electron density and (b) the gain coefficient corresponding to different delay times.
    Fig. 5. The radial distributions of (a) the electron density and (b) the gain coefficient corresponding to different delay times.
    The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 10 µs.
    Fig. 6. The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 10 µs.
    The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 60 µs.
    Fig. 7. The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 60 µs.
    The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 75 µs.
    Fig. 8. The simulation spot and the intensity distribution in the vertical direction of (a), (b) the single-pass amplified laser and (c), (d) the double-pass amplified laser at 75 µs.
    Delay Time (µs)Single-pass Amplified Laser Energy (µJ)Double-pass Amplified Laser Energy (µJ)Magnification in the Laser EnergyLaser Pulse Width of the Single-pass Amplification (ns)Laser Pulse Width of the Double-pass Amplification (ns)Increase in the Laser Pulse Width (ns)
    102905601.931.21.80.6
    602408903.711.12.00.9
    752605101.961.21.70.5
    Table 1. The Double-pass Amplification Compared with the Single-pass Amplification Corresponding to Different Delay Times
    Dongdi Zhao, Yongpeng Zhao, Huaiyu Cui, Bo An, Lei Li, Yunsong Bai. Effect of delay time between pre-pulse and main pulse on single-pass and double-pass amplification of 46.9 nm laser[J]. Chinese Optics Letters, 2023, 21(5): 053401
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