• Photonics Research
  • Vol. 6, Issue 10, C44 (2018)
X. Zhu1、†, S. Chen2、†, M. Zhang1、*, L. Chen2、3、5, Q. Wu1, J. Zhao4, Q. Jiang1, Z. Zheng1, and H. Zhang2
Author Affiliations
  • 1School of Electronic and Information Engineering, Beihang University, Beijing 100191, China
  • 2Department of Optoelectronics Engineering, Shenzhen University, Shenzhen 518060, China
  • 3College of Health Science and Environmental Engineering, Shenzhen Technology University, Shenzhen 518118, China
  • 4College of Materials Science and Engineering, Shenzhen University, Shenzhen 518060, China
  • 5e-mail: l.chen10@alumni.imperial.ac.uk
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    DOI: 10.1364/PRJ.6.000C44 Cite this Article Set citation alerts
    X. Zhu, S. Chen, M. Zhang, L. Chen, Q. Wu, J. Zhao, Q. Jiang, Z. Zheng, H. Zhang. TiS2-based saturable absorber for ultrafast fiber lasers[J]. Photonics Research, 2018, 6(10): C44 Copy Citation Text show less
    Characterization of the few-layer TiS2 nanosheets: (a) TEM image of the TiS2 nanosheets; (b) corresponding Raman spectrum of few-layer TiS2 nanosheets; (c) AFM image of few-layer TiS2 nanosheets; (d) height profile of the section marked in (c).
    Fig. 1. Characterization of the few-layer TiS2 nanosheets: (a) TEM image of the TiS2 nanosheets; (b) corresponding Raman spectrum of few-layer TiS2 nanosheets; (c) AFM image of few-layer TiS2 nanosheets; (d) height profile of the section marked in (c).
    (a) Diagram of fabricating the microfiber-based TiS2 using an optical deposition method; (b) saturable absorption property of the SA device.
    Fig. 2. (a) Diagram of fabricating the microfiber-based TiS2 using an optical deposition method; (b) saturable absorption property of the SA device.
    (a) Configuration of the Er-doped fiber laser for mode-locking operation; (b) output pulse train; (c) optical spectrum; (d) radio frequency spectra, where fs=22.7 MHz and the higher harmonics on a span of 500 MHz; (e) the intensity autocorrelation profile of the generated pulses.
    Fig. 3. (a) Configuration of the Er-doped fiber laser for mode-locking operation; (b) output pulse train; (c) optical spectrum; (d) radio frequency spectra, where fs=22.7  MHz and the higher harmonics on a span of 500 MHz; (e) the intensity autocorrelation profile of the generated pulses.
    (a) Polarization-resolved spectra of the solitons, with a green line and a red line representing the vertical axis and the horizontal axis, respectively; (b) the total and polarization-resolved soliton pulse trains.
    Fig. 4. (a) Polarization-resolved spectra of the solitons, with a green line and a red line representing the vertical axis and the horizontal axis, respectively; (b) the total and polarization-resolved soliton pulse trains.
    Typical output characteristics of the Q-switched pulses at a pump power of 27.5 mW: (a) optical spectrum; (b) single pulse profile, with a 4.49 μs FWHM pulse width; and (c) radio frequency spectrum of fundamental frequency on a 10 kHz span, where f1=33.387 kHz. (d) Variation of the pulse duration and repetition rate with pump power for the Q-switched Er-doped fiber laser using the few-layer TiS2 SA.
    Fig. 5. Typical output characteristics of the Q-switched pulses at a pump power of 27.5 mW: (a) optical spectrum; (b) single pulse profile, with a 4.49 μs FWHM pulse width; and (c) radio frequency spectrum of fundamental frequency on a 10 kHz span, where f1=33.387  kHz. (d) Variation of the pulse duration and repetition rate with pump power for the Q-switched Er-doped fiber laser using the few-layer TiS2 SA.
    X. Zhu, S. Chen, M. Zhang, L. Chen, Q. Wu, J. Zhao, Q. Jiang, Z. Zheng, H. Zhang. TiS2-based saturable absorber for ultrafast fiber lasers[J]. Photonics Research, 2018, 6(10): C44
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