• Acta Physica Sinica
  • Vol. 68, Issue 2, 025201-1 (2019)
Tao Liu1, Yong-Peng Zhao2、*, Huai-Yu Cui2, and Xiao-Lin Liu1
Author Affiliations
  • 1College of Electronic Information and Automation, Civil Aviation University of China, Tianjin 300300, China
  • 2National Key Laboratory of Science and Technology on Tunable Laser, Harbin Institute of Technology, Harbin 150080, China
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    DOI: 10.7498/aps.68.20181617 Cite this Article
    Tao Liu, Yong-Peng Zhao, Huai-Yu Cui, Xiao-Lin Liu. Characteristics of gain in Ne-like Ar 69.8 nm laser pumped by capillary discharge based on double-pass amplification[J]. Acta Physica Sinica, 2019, 68(2): 025201-1 Copy Citation Text show less
    Schematic diagram of position of mirror in double-pass amplification.双程放大实验反射镜位置示意图
    Fig. 1. Schematic diagram of position of mirror in double-pass amplification.双程放大实验反射镜位置示意图
    The pulse waveform of single-pass amplification and double-pass amplification output: (a) Single-pass amplification output; (b) double-pass amplification output.单程放大和双程放大输出脉冲波形 (a)单程放大输出; (b)双程放大输出
    Fig. 2. The pulse waveform of single-pass amplification and double-pass amplification output: (a) Single-pass amplification output; (b) double-pass amplification output.单程放大和双程放大输出脉冲波形 (a)单程放大输出; (b)双程放大输出
    CCD image in capillary radius: (a) Intensity image of single-pass amplification; (b) intensity image of double-pass amplification.毛细管径向上CCD图像 (a)单程放大强度图像; (b)双程放大强度图像
    Fig. 3. CCD image in capillary radius: (a) Intensity image of single-pass amplification; (b) intensity image of double-pass amplification.毛细管径向上CCD图像 (a)单程放大强度图像; (b)双程放大强度图像
    Laser divergence angle in capillary radius: (a) Divergence angle of the single-pass amplification; (b) divergence angle of the double-pass amplification.毛细管径向上激光束散角 (a) 单程放大的束散角; (b) 双程放大的束散角
    Fig. 4. Laser divergence angle in capillary radius: (a) Divergence angle of the single-pass amplification; (b) divergence angle of the double-pass amplification.毛细管径向上激光束散角 (a) 单程放大的束散角; (b) 双程放大的束散角
    Gain coefficient as a function of time for 69.8 nm laser.69.8 nm激光的增益系数随时间的变化
    Fig. 5. Gain coefficient as a function of time for 69.8 nm laser.69.8 nm激光的增益系数随时间的变化
    Gain coefficient as a function of angle in the spatial distribution for 69.8 nm laser peak.69.8 nm激光峰值处的增益系数在空间上的分布情况
    Fig. 6. Gain coefficient as a function of angle in the spatial distribution for 69.8 nm laser peak.69.8 nm激光峰值处的增益系数在空间上的分布情况
    尖峰位置/mrad−1.41−0.92−0.4900.250.681.23
    单程放大强度/arb.units23454525670815712996470767017
    双程放大强度/arb.units55844567625612851205548035077244720
    增长倍数23.812.58.43.35.57.26.4
    Table 1.

    The peak position laser intensity of single-pass amplification and double-pass amplification.

    单程放大与双程放大尖峰位置处激光强度

    Tao Liu, Yong-Peng Zhao, Huai-Yu Cui, Xiao-Lin Liu. Characteristics of gain in Ne-like Ar 69.8 nm laser pumped by capillary discharge based on double-pass amplification[J]. Acta Physica Sinica, 2019, 68(2): 025201-1
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