• 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
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
  • show less
    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[J]. Photonics Research, 2019, 7(3): 283 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[J]. Photonics Research, 2019, 7(3): 283
    Download Citation