High Power Laser Science and Engineering, Volume. 11, Issue 5, 05000e58(2023)

Generation of a curved plasma channel from a discharged capillary for intense laser guiding

Jian-Long Li1, Bo-Yuan Li2, Xin-Zhe Zhu1, Ze-Wu Bi1, Xin-Hui Wen1, Lin Lu1, Xiao-Hui Yuan1,3, Feng Liu1,3、*, and Min Chen1,3
Author Affiliations
  • 1Key Laboratory for Laser Plasmas (Ministry of Education), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
  • 2Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, China
  • 3Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai, China
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    Figures & Tables(9)
    Design of the curved capillary: (a) schematic view of the curved plasma channel on a sapphire substrate; (b) typical cross-section of the laser etched channel on the substrate.
    Schematic diagram of a plasma channel generated by high-voltage discharging of a gas-filled capillary.
    Scheme for plasma density measurement inside the capillary: (a) diagram of the optical fiber detector for spectrum collection; (b) normalized discharge current waveform and collection gate (labeled by the dashed box); (c) typical spectrum detected by a CCD; (d) typical calculated density distribution along the capillary.
    Effects of different gas-filling modes on the plasma density distribution: (a) single-side gas-filling; (b) two-side gas-filling.
    Plasma density distribution along the laser propagation direction in the curved capillary with different back pressures: (a) single-side gas-filling mode; (b) two-side gas-filling mode. The discharge voltage is 22 kV.
    Effects of the discharge voltage on the longitudinal plasma density distribution: (a) single-side gas-filling mode; (b) two-side gas-filling mode. Here the back pressure is fixed to be 15 psig for all cases.
    Measurement of the radial plasma density distribution: (a), (b) raw spectral images when the gas back pressure is 15 and 30 psig, respectively; (c) effects of back pressure on the radial plasma density distribution, where the marked results are measured and the curves are fitted; (d) dependence of the channel radius (r0) on the discharge voltage. The discharge voltage for (a), (b) and (c) is 22 kV.
    Temporal evolution of a plasma channel: (a) normalized discharge current in the capillary; (b) evolution of r0 and n0 when the back pressure is 25 psig and the discharge voltage is 26 kV.
    (a) Focused laser spot at the entrance of the curved capillary in a vacuum. (b) Laser spot at the exit of the curved capillary without discharging. (c) Guided laser spot at the exit of the curved capillary with discharging.
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    Jian-Long Li, Bo-Yuan Li, Xin-Zhe Zhu, Ze-Wu Bi, Xin-Hui Wen, Lin Lu, Xiao-Hui Yuan, Feng Liu, Min Chen. Generation of a curved plasma channel from a discharged capillary for intense laser guiding[J]. High Power Laser Science and Engineering, 2023, 11(5): 05000e58

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    Paper Information

    Category: Research Articles

    Received: Jan. 10, 2023

    Accepted: May. 8, 2023

    Published Online: Sep. 6, 2023

    The Author Email: Feng Liu (liuf001@sjtu.edu.cn)

    DOI:10.1017/hpl.2023.40

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