High Power Laser and Particle Beams, Volume. 35, Issue 11, 111001(2023)

Recent progress of temporal coherent combination of chirped pulses in fiber lasers

Bida Liu, Zhimeng Huang*, Fan Zhang, Handing Xia, Dandan Zhou, Jianbin Li, Junwen Zheng, Rui Zhang, Ping Li, Zhitao Peng, Qihua Zhu, and Dongxia Hu
Author Affiliations
  • Laser Fusion Research Center, CAEP, Mianyang 621900, China
  • show less
    Figures & Tables(23)
    Schematic of principle and experiment of DPA[67]
    Principle of EDPA system[47]
    Schematic illustration of the EDPA setup used for the combination of four temporally separated pulses[47]
    Experimental results of temporal combination system of 128 pulse replicas based on EDPA setup[59]
    Experimental results of spatiotemporal combination system based on EDPA set up[65]
    Experimental results of spatiotemporal combination system with a pulse energy of 32 mJ based on EDPA setup[66]
    Stack and dump enhancement cavity[49]
    Schematic of a chopper-wheel[49]
    Set up of SnD enhancement cavity and its experimental results[60]
    Coherent pulse stacking in a traveling-wave Gires-Tournois interferometer[48]
    Cascaded GTI cavities[48]
    Coherent pulse stacking of 27 pulses in a 4+1 GTI resonator sequence[62]
    Coherent pulse stacking of 81 pulses in a 4+4 GTI resonator sequence[63]
    Simulation and experimental result of coherent pulse dtacking of 81 pulses in a 4+4 GTI resonator sequence[63]
    Experimental result of efficient coherent pulse stacking of 81 pulses in a 4+4 GTI resonator sequence[70]
    Principle of coherent pulse stacking based on deep recurrent neural network[72]
    Experimental results of the coherent pulse stacking based on deep recurrent neural network[72]
    Principle of temporal coherent combination in DPA based on RL controller[73]
    Principle of temporal coherent combination in DPA based on SAC-SPGDM and the procedure of algorithm[74]
    Comparison of control algorithms in DL-CPS[74]
    Simulations illustrating the tolerances of the coherent pulse stacking parameters for 4+4 GTIs. Achievable pre-pulse contrast degrades in the presence of cavity phase errors, pulse phase errors, or pulse intensity errors[70]
    • Table 1. Representative results of DPA of ultra-short pulsed lasers

      View table
      View in Article

      Table 1. Representative results of DPA of ultra-short pulsed lasers

      yearinstitutiontechnical solutionresults
      2017Friedrich-Schiller-Universität, Jena, Germany EDPA, free space delay linesN=4, tp=190 ps, fRR=135 kHz, J=3.4 μJ, η=82.7%; N=8, tp=190 ps, fRR=1075 kHz, η=76.8%[47]
      2019Friedrich-Schiller-Universität, Jena, Germany EDPA+active CBC, free space delay lines N×M=8×12, tp=235 fs, Pave=674 W, fRR=25 kHz, J= 23 mJ, ηcomb = 71%, ηtemp=85%, ηsys=56%[65]
      2020Peking University, ChinaEDPA, free space delay linesN=128, fRR=200 kHz, η=35%[59]
      2023Friedrich-Schiller-Universität, Jena, Germany EDPA+active CBC, free space delay lines N×M=8×16, tp=158 fs, Pave=703 W, fRR=20 kHz, J= 32 mJ, ηcomb = 86%, ηtemp=90%,ηsys=77%[66]
    • Table 2. Representative results of CPS of ultra-short pulsed lasers

      View table
      View in Article

      Table 2. Representative results of CPS of ultra-short pulsed lasers

      yearinstitutiontechnical solutionresults
      2015University of Michigan, USAGires-Tournois interferometersN=5, tp=700 fs, fRR=10 kHz, J=μJ level, η= 97.4%[48]
      2016University of Michigan, USA4+1 Gires-Tournois interferometersN=27, tp=330 fs, η=50%[62]
      2017University of Michigan, USA4+4 Gires-Tournois interferometersN=81, tp=300 fs, fRR=1 kHz, J=multi-mJ, η=35%[63]
      2018Tsinghua University2+1 Gires-Tournois interferometersN=15, tp=10 ps, fRR=98 kHz, η= 76%[69]
      2021University of Michigan, USA4+4 Gires-Tournois interferometersN=81, tp=1 ns, J=4μJ, η=70.5%[70]
    Tools

    Get Citation

    Copy Citation Text

    Bida Liu, Zhimeng Huang, Fan Zhang, Handing Xia, Dandan Zhou, Jianbin Li, Junwen Zheng, Rui Zhang, Ping Li, Zhitao Peng, Qihua Zhu, Dongxia Hu. Recent progress of temporal coherent combination of chirped pulses in fiber lasers[J]. High Power Laser and Particle Beams, 2023, 35(11): 111001

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category:

    Received: Sep. 11, 2023

    Accepted: Oct. 26, 2023

    Published Online: Dec. 26, 2023

    The Author Email: Huang Zhimeng (huangzhimeng@caep.cn)

    DOI:10.11884/HPLPB202335.230308

    Topics