• Infrared and Laser Engineering
  • Vol. 52, Issue 5, 20220745 (2023)
Hang Ren1, Tianshu Wang1, Lei Du1, Xin Li1..., Lin Xiao1 and Jianhong Zhou2,*|Show fewer author(s)
Author Affiliations
  • 1Institute of Space Optoelectronic Technology, School of Optoelectronic Engineering, Changchun University of Science and Technology, Changchun 130022, China
  • 2Department of Optical Engineering, School of Optoelectronic Engineering, Changchun University of Science and Technology, Changchun 130022, China
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    DOI: 10.3788/IRLA20220745 Cite this Article
    Hang Ren, Tianshu Wang, Lei Du, Xin Li, Lin Xiao, Jianhong Zhou. Flat supercontinuum generation via wave-free breaking pulse in the optical fiber[J]. Infrared and Laser Engineering, 2023, 52(5): 20220745 Copy Citation Text show less
    Schematic diagram of passive mode-locked laser. WDM: wavelength division multiplexer; EDF: erbium-doped fiber; OC: 10∶90 optical coupler; PC1 and PC2: polarization controller; PD-ISO: polarization dependent isolator; SMF: single-mode fiber; DCF: dispersion compensation fiber; EDFA: erbium-doped fiber amplifier; HNLF: high nonlinear fiber; OSA: optical spectrum analyzer; OSC: oscilloscope
    Fig. 1. Schematic diagram of passive mode-locked laser. WDM: wavelength division multiplexer; EDF: erbium-doped fiber; OC: 10∶90 optical coupler; PC1 and PC2: polarization controller; PD-ISO: polarization dependent isolator; SMF: single-mode fiber; DCF: dispersion compensation fiber; EDFA: erbium-doped fiber amplifier; HNLF: high nonlinear fiber; OSA: optical spectrum analyzer; OSC: oscilloscope
    (a) Structure diagram of tapered optical fiber; (b) Physical drawing of tapered HNLF
    Fig. 2. (a) Structure diagram of tapered optical fiber; (b) Physical drawing of tapered HNLF
    Mode-locked laser operates in the normal dispersion region. (a) Optical spectrum; (b) Time-domain diagram; (c) RF spectrum, insert (range of RF spectrum in 300 MHz); (d) Autocorrelation trace of pulse (black point), Sech2 fit (red curve)
    Fig. 3. Mode-locked laser operates in the normal dispersion region. (a) Optical spectrum; (b) Time-domain diagram; (c) RF spectrum, insert (range of RF spectrum in 300 MHz); (d) Autocorrelation trace of pulse (black point), Sech2 fit (red curve)
    (a) Time-domain diagram; (b) Autocorrelation trace of dissipative soliton in 11 m single-mode fiber
    Fig. 4. (a) Time-domain diagram; (b) Autocorrelation trace of dissipative soliton in 11 m single-mode fiber
    (a) Evolution of DS spectrum; (b) Time-domain diagram; (c) RF spectrum, insert (0-300 MHz span range of PF spectrum); (d) Autocorrelation trace of evolution pulse (black), Gaussian fit (red)
    Fig. 5. (a) Evolution of DS spectrum; (b) Time-domain diagram; (c) RF spectrum, insert (0-300 MHz span range of PF spectrum); (d) Autocorrelation trace of evolution pulse (black), Gaussian fit (red)
    (a) Evolution of optical spectrum with pump power; (b) Autocorrelation trace at the pump power of 1 W; (c) Comparison of pump1 power vs output power between DS and wave-free breaking pulse; (d) Comparing between maximum lock-mode pump power, optical conversion efficiency, pulse width, pulse energy, peak power for DS and wave-free breaking pulse
    Fig. 6. (a) Evolution of optical spectrum with pump power; (b) Autocorrelation trace at the pump power of 1 W; (c) Comparison of pump1 power vs output power between DS and wave-free breaking pulse; (d) Comparing between maximum lock-mode pump power, optical conversion efficiency, pulse width, pulse energy, peak power for DS and wave-free breaking pulse
    Evolution of supercontinuum with the increasing of pump power. (a) Supercontinuum generated by dissipative soliton; (b) Supercontinuum generated by wave-free breaking pulse
    Fig. 7. Evolution of supercontinuum with the increasing of pump power. (a) Supercontinuum generated by dissipative soliton; (b) Supercontinuum generated by wave-free breaking pulse
    Hang Ren, Tianshu Wang, Lei Du, Xin Li, Lin Xiao, Jianhong Zhou. Flat supercontinuum generation via wave-free breaking pulse in the optical fiber[J]. Infrared and Laser Engineering, 2023, 52(5): 20220745
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