中国物理B ›› 2023, Vol. 32 ›› Issue (10): 105201-105201.doi: 10.1088/1674-1056/acb0bf

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Transmission effects of high energy nanosecond lasers in laser-induced air plasma under different pressures

Wei-Min Hu(胡蔚敏)1,2,3, Kai-Xin Yin(尹凯欣)1,2,†, Xiao-Jun Wang(王小军)1,2, Jing Yang(杨晶)1,2, Ke Liu(刘可)1,2, Qin-Jun Peng(彭钦军)1,2, and Zu-Yan Xu(许祖彦)1,2   

  1. 1 Key Laboratory of Solid State Lasers, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China;
    2 Institute of Optical Physics and Engineering Technology, Qilu Zhongke, Jinan 250000, China;
    3 University of Chinese Academy of Sciences, Beijing 100049, China
  • 收稿日期:2022-11-23 修回日期:2023-01-04 接受日期:2023-01-06 出版日期:2023-09-21 发布日期:2023-09-27
  • 通讯作者: Kai-Xin Yin E-mail:yinkx@mail.ipc.ac.cn
  • 基金资助:
    Project supported by the Science and Technology Innovation Foundation of the Chinese Academy of Sciences (Grant No. CXJJ-20S020).

Transmission effects of high energy nanosecond lasers in laser-induced air plasma under different pressures

Wei-Min Hu(胡蔚敏)1,2,3, Kai-Xin Yin(尹凯欣)1,2,†, Xiao-Jun Wang(王小军)1,2, Jing Yang(杨晶)1,2, Ke Liu(刘可)1,2, Qin-Jun Peng(彭钦军)1,2, and Zu-Yan Xu(许祖彦)1,2   

  1. 1 Key Laboratory of Solid State Lasers, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China;
    2 Institute of Optical Physics and Engineering Technology, Qilu Zhongke, Jinan 250000, China;
    3 University of Chinese Academy of Sciences, Beijing 100049, China
  • Received:2022-11-23 Revised:2023-01-04 Accepted:2023-01-06 Online:2023-09-21 Published:2023-09-27
  • Contact: Kai-Xin Yin E-mail:yinkx@mail.ipc.ac.cn
  • Supported by:
    Project supported by the Science and Technology Innovation Foundation of the Chinese Academy of Sciences (Grant No. CXJJ-20S020).

摘要: When a high energy nanosecond (ns) laser induces breakdown in the air, the plasma density generated in the rarefied atmosphere is much smaller than that at normal pressure. It is associated with a relatively lower absorption coefficient and reduces energy loss of the laser beam at low pressure. In this paper, the general transmission characterizations of a Joule level 10 ns 1064 nm focused laser beam are investigated both theoretically and experimentally under different pressures. The evolution of the electron density ($n_{\rm e}$), the changes in electron temperature ($T_{\rm e}$) and the variation of laser intensity ($I$) are employed for numerical analyses in the simulation model. For experiments, four optical image transfer systems with focal length ($f$) of 200 mm are placed in a chamber and employed to focus the laser beam and produce plasmas at the focus. The results suggest that the transmittance increases obviously with the decreasing pressure and the plasma channels on the transmission path can be observed by the self-illumination. The simulation results agree well with the experimental data. The numerical model presents that the maximum $n_{\rm e}$ at the focus can reach 10$^{19}$ cm$^{-3}$, which is far below the critical density ($n_{\rm c}$). As a result, the laser beam is not completely shielded by the plasmas.

关键词: laser-induced plasma, high energy, nanosecond laser pulse, rarefied atmosphere

Abstract: When a high energy nanosecond (ns) laser induces breakdown in the air, the plasma density generated in the rarefied atmosphere is much smaller than that at normal pressure. It is associated with a relatively lower absorption coefficient and reduces energy loss of the laser beam at low pressure. In this paper, the general transmission characterizations of a Joule level 10 ns 1064 nm focused laser beam are investigated both theoretically and experimentally under different pressures. The evolution of the electron density ($n_{\rm e}$), the changes in electron temperature ($T_{\rm e}$) and the variation of laser intensity ($I$) are employed for numerical analyses in the simulation model. For experiments, four optical image transfer systems with focal length ($f$) of 200 mm are placed in a chamber and employed to focus the laser beam and produce plasmas at the focus. The results suggest that the transmittance increases obviously with the decreasing pressure and the plasma channels on the transmission path can be observed by the self-illumination. The simulation results agree well with the experimental data. The numerical model presents that the maximum $n_{\rm e}$ at the focus can reach 10$^{19}$ cm$^{-3}$, which is far below the critical density ($n_{\rm c}$). As a result, the laser beam is not completely shielded by the plasmas.

Key words: laser-induced plasma, high energy, nanosecond laser pulse, rarefied atmosphere

中图分类号:  (Laser light absorption in plasmas (collisional, parametric, etc.))

  • 52.38.Dx
42.25.Bs (Wave propagation, transmission and absorption) 52.38.-r (Laser-plasma interactions) 52.80.Mg (Arcs; sparks; lightning; atmospheric electricity)