Chinese Journal of Lasers, Volume. 50, Issue 11, 1101017(2023)
Theoretical Research on Output Characteristics of High‐Pressure Isotope CO2 Picosecond Pulse Laser Amplification
Fig. 2. 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
Fig. 3. 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
Fig. 4. 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
Fig. 6. 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%
Fig. 7. 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%
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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
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)