• Photonics Research
  • Vol. 7, Issue 3, 283 (2019)
Chenxi Dou1, Wen Wen2,3, Junli Wang1,*, Mengyuan Ma1..., Liming Xie2,3, Ching-Hwa Ho4 and Zhiyi Wei5|Show fewer author(s)
Author Affiliations
  • 1School of Physics and Optoelectronics Engineering, Xidian University, Xi’an 710071, China
  • 2CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Graduate Institute of Applied Science and Technology, Taiwan University of Science and Technology, Taipei 106, China
  • 5Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
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    DOI: 10.1364/PRJ.7.000283 Cite this Article Set citation alerts
    Chenxi Dou, Wen Wen, Junli Wang, Mengyuan Ma, Liming Xie, Ching-Hwa Ho, Zhiyi Wei, "Ternary ReS2(1-x)Se2x alloy saturable absorber for passively Q-switched and mode-locked erbium-doped all-fiber lasers," Photonics Res. 7, 283 (2019) Copy Citation Text show less
    (a) SEM image, EDS elemental mapping and spectrum of Re, S, and Se. (b) AFM topography, (c) height diagram of a ReS1.02Se0.98 flake on a SiO2/Si substrate. (d) HRTEM image, (e) XPS profiles, and (f) Raman spectra of a ReS1.02Se0.98 flake.
    Fig. 1. (a) SEM image, EDS elemental mapping and spectrum of Re, S, and Se. (b) AFM topography, (c) height diagram of a ReS1.02Se0.98 flake on a SiO2/Si substrate. (d) HRTEM image, (e) XPS profiles, and (f) Raman spectra of a ReS1.02Se0.98 flake.
    Nonlinear absorption of a ReS1.02Se0.98 SA.
    Fig. 2. Nonlinear absorption of a ReS1.02Se0.98 SA.
    Schematic of the all-fiber Q-switched EDF laser cavity.
    Fig. 3. Schematic of the all-fiber Q-switched EDF laser cavity.
    (a) Pulse trains of Q-switching operation at pump power of 600 mW; inset: the corresponding pulse width. (b) RF spectrum (measured with 100 Hz RBW) of Q-switching operation with a ReS1.02Se0.98 SA at a center frequency of 128 kHz.
    Fig. 4. (a) Pulse trains of Q-switching operation at pump power of 600 mW; inset: the corresponding pulse width. (b) RF spectrum (measured with 100 Hz RBW) of Q-switching operation with a ReS1.02Se0.98 SA at a center frequency of 128 kHz.
    (a) Pulse duration and repetition rate versus incident pump power of the Q-switched mechanism. (b) Output average power and pulse energy versus incident pump power of Q-switched operation. (c) The wavelength spectrum of the Q-switched EDF laser at the pump power of 300 mW.
    Fig. 5. (a) Pulse duration and repetition rate versus incident pump power of the Q-switched mechanism. (b) Output average power and pulse energy versus incident pump power of Q-switched operation. (c) The wavelength spectrum of the Q-switched EDF laser at the pump power of 300 mW.
    Diagram of the mode-locked fiber laser setup with a ReS1.02Se0.98 SA.
    Fig. 6. Diagram of the mode-locked fiber laser setup with a ReS1.02Se0.98 SA.
    (a) Pulse trains of mode-locking operation at pump power of 530 mW; inset: oscilloscope trace. (b) RF spectra (measured with 100 Hz RBW) of mode-locking operation with a ReS1.02Se0.98 SA at the pump power of 530 mW. (c) Optical spectrum with the bandwidth of 4.85 nm. (d) Autocorrelation trace for output pulse with a pulse duration of 888 fs with sech2 fit.
    Fig. 7. (a) Pulse trains of mode-locking operation at pump power of 530 mW; inset: oscilloscope trace. (b) RF spectra (measured with 100 Hz RBW) of mode-locking operation with a ReS1.02Se0.98 SA at the pump power of 530 mW. (c) Optical spectrum with the bandwidth of 4.85 nm. (d) Autocorrelation trace for output pulse with a pulse duration of 888 fs with sech2 fit.
    Chenxi Dou, Wen Wen, Junli Wang, Mengyuan Ma, Liming Xie, Ching-Hwa Ho, Zhiyi Wei, "Ternary ReS2(1-x)Se2x alloy saturable absorber for passively Q-switched and mode-locked erbium-doped all-fiber lasers," Photonics Res. 7, 283 (2019)
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