Chinese Optics Letters, Volume. 23, Issue 6, 061402(2025)

0.275 THz high-power ultrahigh-repetition-rate pulses in a dissipative fiber ring cavity by ultrafast ignition On the Cover

Jingmin Liu, Xu Chen, Junjie Jiang, Wenlin Luan, and Xia Yu*
Author Affiliations
  • School of Instrumentation and Optoelectronic Engineering, Beihang University, Beijing 100191, China
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    Figures & Tables(10)
    Principle of the ultrafast pulse-stimulated UHRP. T0, period of the seed pulse; F, repetition rate of the seed pulse; Fs, repetition rate of the UHRP; FF and T, repetition rate and period of the dissipative cavity.
    Experimental setup of the UHRP fiber ring cavity. DCF, dispersion-compensating fiber; EYDFA, erbium-ytterbium co-doped amplifier; OC, output coupler; FROG, frequency-resolved optical gating; OSA, optical spectrum analyzer.
    Characteristics of the seed pulse and MZI filter. (a) Spectra of the ultrafast pulse at Point A; (b) FROG trace of the seed pulse (inset, autocorrelation trace); (c) transmission curve and (d) FROG trace of the pulse at Point B.
    Ultrafast pulse-stimulated UHRPs. (a) The spectra at different seed pulse powers; (b) the spectrum of the UHRP when the ultrafast seed pulse is switched off (see the Visualization 1); (c) the recording of UHRP spectra every 5 min, with corresponding parts (d) detailing the FROG and the autocorrelation trace, respectively.
    Diagram of the ultrafast pulse-stimulated UHRP. (a) Spectra when the seed pulses are ON (in blue) and OFF (in red), respectively; (b) presentation of the corresponding temporal characterization through FROG trace analysis.
    Simulation model of the ultrafast pulse-stimulated UHRP fiber laser. SMF, single-mode fiber; OC, optical coupler.
    Spectra and temporal pulses at different cavity locations: (a) and (b) seed pulses; (c) and (d) pulses after the comb filter.
    Characteristics of the pulse evolution: (a) UHRP spectrum; (b) pulse evolution in the frequency domain; (c) pulse evolution in the time domain (Insets illustrate three steps from the split state to the UHRP state); (d) energy evolution (The inset shows energy oscillation).
    Relationship of the rates between MZI spacing and the cavity fundamental rate.
    • Table 1. Comparison of Different Schemes of UHRP Fiber Lasers

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      Table 1. Comparison of Different Schemes of UHRP Fiber Lasers

      FilterDispersionRate (GHz)Pump (mW)Output (mW)
      High-nonlinear
      Raman fiber laser[27,28]negative160926
      High-nonlinear
      Fabry–Perot filter[29]6402.5
      MZI
      (Dual pump)[30]negative100080050
      High-nonlinear microring[16]negative20015.4
      High-nonlinear microfiber[26]negative144.33906.21
      Fiber loop[31]negative0.99204.5
      High-nonlinear microfiber[32]negative106.7200
      Fiber loop[33]normal280200050
      This studynormal275500
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    Jingmin Liu, Xu Chen, Junjie Jiang, Wenlin Luan, Xia Yu, "0.275 THz high-power ultrahigh-repetition-rate pulses in a dissipative fiber ring cavity by ultrafast ignition," Chin. Opt. Lett. 23, 061402 (2025)

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    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Oct. 22, 2024

    Accepted: Dec. 9, 2024

    Published Online: May. 19, 2025

    The Author Email: Xia Yu (xiayu@buaa.edu.cn)

    DOI:10.3788/COL202523.061402

    CSTR:32184.14.COL202523.061402

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