• High Power Laser Science and Engineering
  • Vol. 11, Issue 6, 06000e81 (2023)
Shuailin Liu1,2,3, Bin Zhang1,2,3,*, Yuanzhuang Bu1,2,3, Desheng Zhao1,2,3..., Xiran Zhu1,2,3, Linyong Yang1,2,3 and Jing Hou1,2,3,*|Show fewer author(s)
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha, China
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    DOI: 10.1017/hpl.2023.62 Cite this Article Set citation alerts
    Shuailin Liu, Bin Zhang, Yuanzhuang Bu, Desheng Zhao, Xiran Zhu, Linyong Yang, Jing Hou, "High-energy and high-peak-power GHz burst-mode all-fiber laser with a uniform envelope and tunable intra-burst pulses," High Power Laser Sci. Eng. 11, 06000e81 (2023) Copy Citation Text show less
    (a) Schematic diagram of the laser system. LD, laser diode; IBP, isolator/bandpass filter hybrid; SM, single mode; YDF, Yb3+-doped fiber; AOM, acousto-optic modulator; ISO, isolator. (b) Time sequence of seed and pump pulses.
    Fig. 1. (a) Schematic diagram of the laser system. LD, laser diode; IBP, isolator/bandpass filter hybrid; SM, single mode; YDF, Yb3+-doped fiber; AOM, acousto-optic modulator; ISO, isolator. (b) Time sequence of seed and pump pulses.
    Evolution of the pulse shape during the secondary pre-compensation process. (a) The signal waveform for the seed driver and the pulse train of the seed. (b) The signal waveform from the AWG and the burst-mode pulse waveform after AOM modulation.
    Fig. 2. Evolution of the pulse shape during the secondary pre-compensation process. (a) The signal waveform for the seed driver and the pulse train of the seed. (b) The signal waveform from the AWG and the burst-mode pulse waveform after AOM modulation.
    Performance of the output burst-mode laser. (a) Variation of pulse energy with different pump energies of the main amplifier. (b) Temporal shape of the pulse with different pulse energies. (c) Comparison of the intra-burst pulse in detail between the seed and output. (d) Spectrum evolution of the seed and main amplifier.
    Fig. 3. Performance of the output burst-mode laser. (a) Variation of pulse energy with different pump energies of the main amplifier. (b) Temporal shape of the pulse with different pulse energies. (c) Comparison of the intra-burst pulse in detail between the seed and output. (d) Spectrum evolution of the seed and main amplifier.
    The envelope uniformity factors with different input energies as a function of main amplifier pump energy. Inset: diagram of the calculation region of the envelope uniformity factor.
    Fig. 4. The envelope uniformity factors with different input energies as a function of main amplifier pump energy. Inset: diagram of the calculation region of the envelope uniformity factor.
    RF spectrum of different frequencies ranging from 0.5 to 10 GHz.
    Fig. 5. RF spectrum of different frequencies ranging from 0.5 to 10 GHz.
    Performance of the output under different intra-burst duty cycles at the same pump energy (42.3 mJ) when the intra-burst repetition rate is fixed at 1 GHz. (a) The energy and peak power. (b) The waveform details of the intra-burst pulse. (c) The spectra in the 300 nm scanning range.
    Fig. 6. Performance of the output under different intra-burst duty cycles at the same pump energy (42.3 mJ) when the intra-burst repetition rate is fixed at 1 GHz. (a) The energy and peak power. (b) The waveform details of the intra-burst pulse. (c) The spectra in the 300 nm scanning range.
    The long-term stability of energy, measured at an output energy of 13.3 mJ (50 ns, 1 GHz).
    Fig. 7. The long-term stability of energy, measured at an output energy of 13.3 mJ (50 ns, 1 GHz).
    Shuailin Liu, Bin Zhang, Yuanzhuang Bu, Desheng Zhao, Xiran Zhu, Linyong Yang, Jing Hou, "High-energy and high-peak-power GHz burst-mode all-fiber laser with a uniform envelope and tunable intra-burst pulses," High Power Laser Sci. Eng. 11, 06000e81 (2023)
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