• High Power Laser Science and Engineering
  • Vol. 9, Issue 3, 03000e46 (2021)
Dongyu Yan, Bowen Liu*, Defeng Zou, Jie Guo, Yuxi Chu, Youjian Song, and Minglie Hu
Author Affiliations
  • Ultrafast Laser Laboratory, School of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Optoelectronic Information Technology (Ministry of Education), Tianjin University, Tianjin300072, China
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    DOI: 10.1017/hpl.2021.34 Cite this Article Set citation alerts
    Dongyu Yan, Bowen Liu, Defeng Zou, Jie Guo, Yuxi Chu, Youjian Song, Minglie Hu. Spectral filtering effect on multi-pulsing induced by chirped fiber Bragg grating in dispersion-managed mode-locked Yb-doped fiber lasers[J]. High Power Laser Science and Engineering, 2021, 9(3): 03000e46 Copy Citation Text show less
    Experimental setup of the passively mode-locked all-PM fiber laser. LD, laser diode; WDM, wavelength division multiplexer; CFBG, chirped fiber Bragg grating; YDF, Yb-doped fiber; SMF, single-mode fiber; SESAM, semiconductor saturable absorber mirror; HWP, half-wave plate; PBS, polarization beam splitter; ISO, isolator.
    Fig. 1. Experimental setup of the passively mode-locked all-PM fiber laser. LD, laser diode; WDM, wavelength division multiplexer; CFBG, chirped fiber Bragg grating; YDF, Yb-doped fiber; SMF, single-mode fiber; SESAM, semiconductor saturable absorber mirror; HWP, half-wave plate; PBS, polarization beam splitter; ISO, isolator.
    Spectral width at 10 dB (red solid squares) and dechirped pulse width at 3 dB (blue open circles) of the output pulses versus the NCD at a pump power of (a) 80 mW, (b) 90 mW, (c) 100 mW, (d) 110 mW, (e) 120 mW, and (f) 130 mW (gray area: multi-pulsing region).
    Fig. 2. Spectral width at 10 dB (red solid squares) and dechirped pulse width at 3 dB (blue open circles) of the output pulses versus the NCD at a pump power of (a) 80 mW, (b) 90 mW, (c) 100 mW, (d) 110 mW, (e) 120 mW, and (f) 130 mW (gray area: multi-pulsing region).
    (a) Spectrum and autocorrelation trace of soliton molecules at 80 mW pump power. (b) Spectra of single soliton states for two critical NCD values at 80 mW pump power (gray area: CFBG reflection spectrum).
    Fig. 3. (a) Spectrum and autocorrelation trace of soliton molecules at 80 mW pump power. (b) Spectra of single soliton states for two critical NCD values at 80 mW pump power (gray area: CFBG reflection spectrum).
    Autocorrelation traces of dechirped output pulses (blue solid lines) and Gaussian fitting curves (red dashed lines) at a pump power of (a) 80 mW, (b) 100 mW, and (c) 130 mW. Insets: corresponding spectra of output pulses.
    Fig. 4. Autocorrelation traces of dechirped output pulses (blue solid lines) and Gaussian fitting curves (red dashed lines) at a pump power of (a) 80 mW, (b) 100 mW, and (c) 130 mW. Insets: corresponding spectra of output pulses.
    (a) Schematic of the numerical simulation model. Evolution of spectral width (red solid line) and temporal width (blue dotted line) when the NCD is for (b) βnet = −1.1 × 10−3 ps2 and (c) βnet = +1.5 × 10−2 ps2. YDF, Yb-doped fiber; SMF, single-mode fiber; SESAM, semiconductor saturable absorber mirror; DCF, dispersion compensating fiber; OC, optical coupler.
    Fig. 5. (a) Schematic of the numerical simulation model. Evolution of spectral width (red solid line) and temporal width (blue dotted line) when the NCD is for (b) βnet = −1.1 × 10−3 ps2 and (c) βnet = +1.5 × 10−2 ps2. YDF, Yb-doped fiber; SMF, single-mode fiber; SESAM, semiconductor saturable absorber mirror; DCF, dispersion compensating fiber; OC, optical coupler.
    (a) FWHM spectral width of output pulses as a function of NCD and Esat. Linear scale: 4 nm 20 nm (white area: multi-pulsing region). (b) FWHM spectral width of pulses at point D as a function of filter bandwidth and Esat. Linear scale: 8 nm 16 nm (white area: multi-pulsing region). (c) FWHM spectral width of pulses at the OC (red open squares) and at point D (red open-triangles) at critical pump power and corresponding Esat (blue solid circles).
    Fig. 6. (a) FWHM spectral width of output pulses as a function of NCD and Esat. Linear scale: 4 nm 20 nm (white area: multi-pulsing region). (b) FWHM spectral width of pulses at point D as a function of filter bandwidth and Esat. Linear scale: 8 nm 16 nm (white area: multi-pulsing region). (c) FWHM spectral width of pulses at the OC (red open squares) and at point D (red open-triangles) at critical pump power and corresponding Esat (blue solid circles).
    Net dispersionSpectral widthPulse widthPulse energyAverage powerReference
    0.016 ps212.3 nm213 fs160 pJ4 mW[22]
    0.02 ps210.4 nm162 fs27 pJ0.5 mW[28]
    −1.96 ps20.7 nm2.7 ps130 pJ2.5 mW[29]
    −1.7 ps20.65 nm3.6 ps22 pJ1 mW[30]
    −0.004 ps217 nm139 fs140 pJ6 mW[13]
    −0.0167 ps219.4 nm108 fs420 pJ21 mWThis work
    Table 1. Overview of key parameters of mode-locked YDF lasers using a CFBG for dispersion management.
    Dongyu Yan, Bowen Liu, Defeng Zou, Jie Guo, Yuxi Chu, Youjian Song, Minglie Hu. Spectral filtering effect on multi-pulsing induced by chirped fiber Bragg grating in dispersion-managed mode-locked Yb-doped fiber lasers[J]. High Power Laser Science and Engineering, 2021, 9(3): 03000e46
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