High Power Laser Science and Engineering, Volume. 11, Issue 4, 04000e46(2023)

Pulse repetition-rate effect on the intensity inside a femtosecond laser filament in air

Fukang Yin1,2, Juan Long1,2, Yaoxiang Liu1、*, Yingxia Wei1, Bin Zhu3, Kainan Zhou3, Tie-Jun Wang1,2、*, Yuxin Leng1,2, and Ruxin Li1,2
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics and CAS Center for Excellence in Ultra-intense Laser Science, Chinese Academy of Sciences, Shanghai, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
  • 3Laser Fusion Research Center and Science & Technology on Plasma Physics Laboratory, China Academy of Engineering Physics, Mianyang, China
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    Figures & Tables(6)
    Maximal on-axis intensities of femtosecond laser pulses as a function of propagation distance for 100 and 1000 Hz repetition rates with different pulse energies of (a) 0.1 mJ, (b) 0.2 mJ, (c) 0.7 mJ and (d) 1.2 mJ. The geometric focus position is defined as 0 of the propagation distance and the negative values are before the focus. The inset of (a) shows the enlargement of the shadow region of (a).
    Experimental setup.
    The typical spectrum images and intensity plots captured by the ICCD mounted on the spectrometer: (a) is in non-divided imaging mode, while (b) and (c) are centered at the wavelengths of 337 and 391 nm, respectively. The laser pulse energy and repetition rate are 1.2 mJ and 1000 Hz, respectively.
    Longitudinal distribution of the nitrogen 337 and 391 nm fluorescence signal along the filaments under filament repetition rates of (a) 100 Hz and (b) 1000 Hz. The geometric focus position is defined as 0 of the propagation position and the negative values are before the focus. The laser pulse energy is 1.2 mJ for filamentation.
    The laser peak intensities with different incident laser pulse energies of (a) 0.1 mJ, (b) 0.2 mJ, (c) 0.7 mJ and (d) 1.2 mJ under different laser repetition rates (black line, 100 Hz; red line, 1 kHz), as determined by Equation (10).
    Experimentally measured average intensity of the filament as a function of (a) incident energy and (b) laser repetition rate (the incident energy is 1.2 mJ). The filament range is defined by specifying the filamentation initiation and termination when the total fluorescence intensity approaches 1/e of the maximum intensity. (c) Numerically obtained average intensity of the filamentation zone as a function of incident energy for laser repetition rates of 100 and 1000 Hz. (d) Numerically obtained average intensity of the filamentation zone as a function of laser repetition rates for incident energy of 1.2 mJ. (e) The radial distributions of the gas density hole generated by 100 and 1000 Hz repetition-rate lasers.
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    Fukang Yin, Juan Long, Yaoxiang Liu, Yingxia Wei, Bin Zhu, Kainan Zhou, Tie-Jun Wang, Yuxin Leng, Ruxin Li. Pulse repetition-rate effect on the intensity inside a femtosecond laser filament in air[J]. High Power Laser Science and Engineering, 2023, 11(4): 04000e46

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    Paper Information

    Category: Research Articles

    Received: Jan. 5, 2023

    Accepted: Mar. 24, 2023

    Published Online: Jul. 4, 2023

    The Author Email: Yaoxiang Liu (yaoxiangliu@siom.ac.cn), Tie-Jun Wang (tiejunwang@siom.ac.cn)

    DOI:10.1017/hpl.2023.31

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