• High Power Laser Science and Engineering
  • Vol. 11, Issue 1, 010000e2 (2023)
Meizhi Sun1、2, Jun Kang1, Xiao Liang1, Haidong Zhu1、2, Qingwei Yang1, Qi Gao1, Ailin Guo1, Ping Zhu1、2, Panzheng Zhang1、2, Linjun Li1、2, Lijuan Qiu1、2, Zhantao Lu1、2, Sheng Wang3, Xiaoniu Tu3、*, Xinglong Xie1、2、*, and Jianqiang Zhu1、2、*
Author Affiliations
  • 1Key Laboratory on 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
  • 3Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
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    DOI: 10.1017/hpl.2023.7 Cite this Article Set citation alerts
    Meizhi Sun, Jun Kang, Xiao Liang, Haidong Zhu, Qingwei Yang, Qi Gao, Ailin Guo, Ping Zhu, Panzheng Zhang, Linjun Li, Lijuan Qiu, Zhantao Lu, Sheng Wang, Xiaoniu Tu, Xinglong Xie, Jianqiang Zhu. Demonstration of a petawatt-scale optical parametric chirped pulse amplifier based on yttrium calcium oxyborate[J]. High Power Laser Science and Engineering, 2023, 11(1): 010000e2 Copy Citation Text show less
    Schematic of the experiment. SHG, second harmonic generation; AO, adaptive optics; OAP, off-axis parabolic mirror.
    Fig. 1. Schematic of the experiment. SHG, second harmonic generation; AO, adaptive optics; OAP, off-axis parabolic mirror.
    Normalized waveforms of the incidence signal (blue), amplified signal (red) and incidence pump (green) for OPCPA-II.
    Fig. 2. Normalized waveforms of the incidence signal (blue), amplified signal (red) and incidence pump (green) for OPCPA-II.
    Normalized spectra of the incidence (blue) and amplified (red) signal, compared with the theoretical gain of YCOB-based OPCPA-II (green).
    Fig. 3. Normalized spectra of the incidence (blue) and amplified (red) signal, compared with the theoretical gain of YCOB-based OPCPA-II (green).
    The reflection (a) and transmission (b) properties of YCOB crystal measured by a ZYGO interferometer.
    Fig. 4. The reflection (a) and transmission (b) properties of YCOB crystal measured by a ZYGO interferometer.
    (a) Amplified signal energy achieved by numerical simulation (red solid line) and measured in the experiment (red circles); (b) conversion efficiency obtained by numerical simulation (blue solid line) and experimental measurement (blue circles).
    Fig. 5. (a) Amplified signal energy achieved by numerical simulation (red solid line) and measured in the experiment (red circles); (b) conversion efficiency obtained by numerical simulation (blue solid line) and experimental measurement (blue circles).
    OPCPA conversion efficiency versus the deviation from the optimal phase-matching angle, when the non-collinear angle was set at 2.74°.
    Fig. 6. OPCPA conversion efficiency versus the deviation from the optimal phase-matching angle, when the non-collinear angle was set at 2.74°.
    Near fields of the amplified signal in OPCPA-II based on YCOB (a) and LBO (b) crystals.
    Fig. 7. Near fields of the amplified signal in OPCPA-II based on YCOB (a) and LBO (b) crystals.
    The dynamic wavefront aberrations measured by a Hartmann sensor in the adaptive optics assembly for OPCPA–II with YCOB crystal (a) and LBO crystal (b).
    Fig. 8. The dynamic wavefront aberrations measured by a Hartmann sensor in the adaptive optics assembly for OPCPA–II with YCOB crystal (a) and LBO crystal (b).
    The autocorrelation (AC) trace of a signal pulse after the master compressor.
    Fig. 9. The autocorrelation (AC) trace of a signal pulse after the master compressor.
    Meizhi Sun, Jun Kang, Xiao Liang, Haidong Zhu, Qingwei Yang, Qi Gao, Ailin Guo, Ping Zhu, Panzheng Zhang, Linjun Li, Lijuan Qiu, Zhantao Lu, Sheng Wang, Xiaoniu Tu, Xinglong Xie, Jianqiang Zhu. Demonstration of a petawatt-scale optical parametric chirped pulse amplifier based on yttrium calcium oxyborate[J]. High Power Laser Science and Engineering, 2023, 11(1): 010000e2
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