• High Power Laser Science and Engineering
  • Vol. 7, Issue 2, 02000e27 (2019)
Rongtao Su1,2,3, Pengfei Ma1,2,3, Pu Zhou1,2,3,†,*..., Zilun Chen1,2,3, Xiaolin Wang1,2,3, Yanxing Ma1,2,3, Jian Wu1,2,3 and Xiaojun Xu1,2,3|Show fewer author(s)
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2State Key Laboratory of Pulsed Power Laser Technology, Changsha 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha 410073, China
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    DOI: 10.1017/hpl.2019.13 Cite this Article Set citation alerts
    Rongtao Su, Pengfei Ma, Pu Zhou, Zilun Chen, Xiaolin Wang, Yanxing Ma, Jian Wu, Xiaojun Xu, "High-peak-power temporally shaped nanosecond fiber laser immune to SPM-induced spectral broadening," High Power Laser Sci. Eng. 7, 02000e27 (2019) Copy Citation Text show less
    Calculated pulse shapes and the corresponding spectra. (a) Gaussian-shape pulse and the corresponding (b), (c) spectra; (d) sawtooth-shape pulse and the corresponding (e), (f) spectra; (g) square-shape pulse and the corresponding (h), (i) spectra; (j) distorted-square-shape pulse and the corresponding (k), (l) spectra.
    Fig. 1. Calculated pulse shapes and the corresponding spectra. (a) Gaussian-shape pulse and the corresponding (b), (c) spectra; (d) sawtooth-shape pulse and the corresponding (e), (f) spectra; (g) square-shape pulse and the corresponding (h), (i) spectra; (j) distorted-square-shape pulse and the corresponding (k), (l) spectra.
    Experimental setup for spectral measurement of Gaussian-like and square-like pulses. EOIM, electro-optic intensity modulator; AFG, arbitrary function generator; SWG, square wave generator; SMF-PA, single-mode-fiber-based preamplifier; LD, laser diode; WDM, wavelength division multiplexer; PM YDF, polarization-maintained Yb-doped fiber; BPF, band pass filter; ISO: isolator; FPI, Fabry–Perot interferometer.
    Fig. 2. Experimental setup for spectral measurement of Gaussian-like and square-like pulses. EOIM, electro-optic intensity modulator; AFG, arbitrary function generator; SWG, square wave generator; SMF-PA, single-mode-fiber-based preamplifier; LD, laser diode; WDM, wavelength division multiplexer; PM YDF, polarization-maintained Yb-doped fiber; BPF, band pass filter; ISO: isolator; FPI, Fabry–Perot interferometer.
    Measured pulse shapes and the corresponding spectra. (a) Gaussian-like pulse and corresponding spectra at the (b) input and (c) output of the GDF; (d) square-like pulse and corresponding spectra at the (e) input and (f) output of the GDF.
    Fig. 3. Measured pulse shapes and the corresponding spectra. (a) Gaussian-like pulse and corresponding spectra at the (b) input and (c) output of the GDF; (d) square-like pulse and corresponding spectra at the (e) input and (f) output of the GDF.
    Experimental setup of the LMA fiber amplifier. LD, laser diode; FPI, Fabry–Perot interferometer; P1, P2, power meter; PM YDF, polarization-maintained Yb-doped fiber; CLS, cladding laser stripper; CO, collimator.
    Fig. 4. Experimental setup of the LMA fiber amplifier. LD, laser diode; FPI, Fabry–Perot interferometer; P1, P2, power meter; PM YDF, polarization-maintained Yb-doped fiber; CLS, cladding laser stripper; CO, collimator.
    Average backward propagating power of the Gaussian-like pulses as a function of the forward propagating output power.
    Fig. 5. Average backward propagating power of the Gaussian-like pulses as a function of the forward propagating output power.
    Measured pulse shape and the corresponding spectra of the Gaussian-like pulse. (a) Output pulse shape; (b) spectrum of the pulsed seed; (c) spectrum of the output pulses.
    Fig. 6. Measured pulse shape and the corresponding spectra of the Gaussian-like pulse. (a) Output pulse shape; (b) spectrum of the pulsed seed; (c) spectrum of the output pulses.
    Average backward propagating power of square-like pulses as functions of the (a) average forward propagating output and (b) peak power.
    Fig. 7. Average backward propagating power of square-like pulses as functions of the (a) average forward propagating output and (b) peak power.
    Measured pulse shapes and the corresponding spectra of square-like pulses. (a) 8 ns pulse and (b), (c) corresponding spectra; (d) 7 ns pulse and (e), (f) corresponding spectra; (g) 6 ns pulse and (h), (i) corresponding spectra; (j) 5 ns pulse and (k), (l) corresponding spectra.
    Fig. 8. Measured pulse shapes and the corresponding spectra of square-like pulses. (a) 8 ns pulse and (b), (c) corresponding spectra; (d) 7 ns pulse and (e), (f) corresponding spectra; (g) 6 ns pulse and (h), (i) corresponding spectra; (j) 5 ns pulse and (k), (l) corresponding spectra.
    Measured (a) spectra and (b) PER in the main amplifier for 5 ns pulses.
    Fig. 9. Measured (a) spectra and (b) PER in the main amplifier for 5 ns pulses.
    Pulse width (ns) 8 7 6 5
    Maximum average power (W) 2.57 2.83 3.13 3.72
    Maximum peak power (kW) 4.02 5.06 6.52 9.30
    Measured linewidth (MHz)129.5137.6156.2200.1
    Table 1. Maximum output power and the corresponding linewidth in the main amplifier.
    Rongtao Su, Pengfei Ma, Pu Zhou, Zilun Chen, Xiaolin Wang, Yanxing Ma, Jian Wu, Xiaojun Xu, "High-peak-power temporally shaped nanosecond fiber laser immune to SPM-induced spectral broadening," High Power Laser Sci. Eng. 7, 02000e27 (2019)
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