Chinese Journal of Lasers, Volume. 50, Issue 11, 1101017(2023)

Theoretical Research on Output Characteristics of High‐Pressure Isotope CO2 Picosecond Pulse Laser Amplification

Jinghan Ye1,2, Ziren Zhu1,2, Jinzhou Bai1,2, Yu Liu1,2, Rongqing Tan1, Yijun Zheng1、*, and Xinjun Su3
Author Affiliations
  • 1Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100094, China
  • 2School of Electronic, Electrical and Communication Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Science and Technology on Particle Transport and Separation Laboratory, Tianjin 300180, China
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    Figures & Tables(8)
    Laser transitions of CO2 isotopes at bands 0001-1000 and 0001-0200
    Output characteristics under different atom ratios, where the left images show the input and output pulse waveforms and the right images show the output spectra and amplifier gain spectra. (a)(b) 13C and 18O account for 0%, respectively; (c)(d) 13C and 18O account for 25%, respectively; (e)(f) 13C and 18O account for 50%, respectively; (g)(h) 13C and 18O account for 75%, respectively; (i)(j) 13C and 18O account for 100%, respectively
    Output characteristics in four bands with 18O accounting for 50%, where the left images are the input/output pulse waveforms and the right images are the output spectra and amplifier gain spectra. (a)(b) 10.532 μm; (c)(d) 10.247 μm; (e)(f) 9.411 μm; (g)(h) 9.222 μm
    Output characteristics under the conditions of different pressures and CO2 isotopes (12C16O2 and the gas with six CO2 isotopes with 13C and 18O accounting for 50%, respectively) at 5, 8 and 10 bar, where the left images are the input/output pulse waveforms and the right images are the output spectra and amplifier gain spectra. (a)(b) At 5 bar, the proportions of 13C and 18O are 0%, respectively; (c)(d) at 5 bar, the proportions of 13C and 18O are 50%, respectively; (e)(f) at 8 bar, the proportions of 13C and 18O are 0%, respectively; (g)(h) at 8 bar, the proportions of 13C and 18O are 50%, respectively; (i)(j) at 10 bar, the proportions of 13C and 18O are 0%, respectively; (k)(l) at 10 bar, the proportions of 13C and 18O are 50%, respectively
    Gain near 10.591 μm at 10 bar and gain contribution of each isotope
    Amplifier gain spectra at 8.8-11.7 μm band. (a) 13C accounts for 0% and 18O accounts for 50%; (b) 13C accounts for 100% and 18O accounts for 50%; (c) 13C accounts for 50% and 18O accounts for 50%
    Output characteristics at 9 and 10 μm band under different CO2 isotopes (three isotopes of 12C, three isotopes of 13C and all six isotopes), where the left images are the input/output pulse waveforms and the right images are the input/output spectra and amplifier gain spectra. (a)(b) 9.330 μm, 13C accounts for 0% and 18O accounts for 50%; (c)(d) 9.442 μm, 13C accounts for 50% and 18O accounts for 50%; (e)(f) 10.869 μm, 13C accounts for 100% and 18O accounts for 50%; (g)(h) 10.767 μm, 13C accounts for 50% and 18O accounts for 50%
    • Table 1. Parameters of incident Gaussian pulse and amplifier configuration

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      Table 1. Parameters of incident Gaussian pulse and amplifier configuration

      IndexContent
      Pulse energy /J0.01
      Pulse width(FWHM)/ps5
      Central wavelength /μm10.591
      Band width(FWHM)/THz0.088
      Beam radius(HWHM)/cm0.25
      Gain volume /(cm×cm×cm)2×2×100
      Electrode length /m1.0
      Peak voltage /kV100
      Volume ratio of CO2,N2,and He1∶1∶8
      Gas pressure /bar5
      Temperature /K300
      Entrance and exit windows materialNaCl
      Attenuation0.96
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    Jinghan Ye, Ziren Zhu, Jinzhou Bai, Yu Liu, Rongqing Tan, Yijun Zheng, Xinjun Su. Theoretical Research on Output Characteristics of High‐Pressure Isotope CO2 Picosecond Pulse Laser Amplification[J]. Chinese Journal of Lasers, 2023, 50(11): 1101017

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    Paper Information

    Category: laser devices and laser physics

    Received: Dec. 22, 2022

    Accepted: Mar. 13, 2023

    Published Online: May. 19, 2023

    The Author Email: Zheng Yijun (yjzheng@mail.ie.ac.cn)

    DOI:10.3788/CJL221558

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