• High Power Laser Science and Engineering
  • Vol. 6, Issue 2, 02000e18 (2018)
Wei Chen1, Bowen Liu1, Youjian Song1, Lu Chai1, Qianjin Cui2, Qingjing Liu2, Chingyue Wang1, and Minglie Hu1、*
Author Affiliations
  • 1Ultrafast Laser Laboratory, Key Laboratory of Opto-Electronic Information Technology, Ministry of Education, School of Precision Instrument and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, China
  • 2Laize Photonics Co., Ltd, Beijing 101399, China
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    DOI: 10.1017/hpl.2018.20 Cite this Article Set citation alerts
    Wei Chen, Bowen Liu, Youjian Song, Lu Chai, Qianjin Cui, Qingjing Liu, Chingyue Wang, Minglie Hu. High pulse energy fiber/solid-slab hybrid picosecond pulse system for material processing on polycrystalline diamonds[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e18 Copy Citation Text show less
    Setup of the all PM fiber mode-locked laser. ISO: isolator, WDM: wavelength division multiplexer, SESAM: semiconductor saturable absorber mirror, FBG: fiber Bragg grating, PD: photonics detector, SG: signal generator, AOM: acoustic optical modulator, RF signal: radio frequency signal.
    Fig. 1. Setup of the all PM fiber mode-locked laser. ISO: isolator, WDM: wavelength division multiplexer, SESAM: semiconductor saturable absorber mirror, FBG: fiber Bragg grating, PD: photonics detector, SG: signal generator, AOM: acoustic optical modulator, RF signal: radio frequency signal.
    Configuration of the ultraviolet picosecond pulse laser system.
    Fig. 2. Configuration of the ultraviolet picosecond pulse laser system.
    Output characteristics of the all PM fiber pulse seed source. (a) Spectrum profiles, the inset shows the long term stability of the seed pulses (in the 10% output port) in 2 h. (b) Autocorrelation trace and its Gaussian fitting.
    Fig. 3. Output characteristics of the all PM fiber pulse seed source. (a) Spectrum profiles, the inset shows the long term stability of the seed pulses (in the 10% output port) in 2 h. (b) Autocorrelation trace and its Gaussian fitting.
    Output characteristics of the all slab amplifier. (a) Measured (dots) and calculated (line) output power of the slab amplifier. (b) Long term stability of the slab amplifier in 2 h. (c) Beam radius and profile. (d) Autocorrelation trace and its Gaussian fitting.
    Fig. 4. Output characteristics of the all slab amplifier. (a) Measured (dots) and calculated (line) output power of the slab amplifier. (b) Long term stability of the slab amplifier in 2 h. (c) Beam radius and profile. (d) Autocorrelation trace and its Gaussian fitting.
    SEM images of laser-cut grooves on the diamond surface by 355 nm picosecond pulses with (a) at the repetition rate of 500 kHz (the corresponding pulse energy is ) and (b) at the repetition rate of 10 MHz (the corresponding pulse energy is ), respectively.
    Fig. 5. SEM images of laser-cut grooves on the diamond surface by 355 nm picosecond pulses with (a) at the repetition rate of 500 kHz (the corresponding pulse energy is ) and (b) at the repetition rate of 10 MHz (the corresponding pulse energy is ), respectively.
    Wei Chen, Bowen Liu, Youjian Song, Lu Chai, Qianjin Cui, Qingjing Liu, Chingyue Wang, Minglie Hu. High pulse energy fiber/solid-slab hybrid picosecond pulse system for material processing on polycrystalline diamonds[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e18
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