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Chinese Optics Letters, Volume. 14, Issue 7, 071404(2016)

MoS2 saturable absorber for single frequency oscillation of highly Yb-doped fiber laser

Baole Lu1,2,3、*, Limei Yuan1,2,3, Xinyuan Qi4, Lei Hou1,2,3, Bo Sun1,2,3, Pan Fu1,2,3, and Jintao Bai1,2,3,4
Author Affiliations
  • 1National Key Laboratory of Photoelectric Technology and Functional Materials (Culture Base), Institute of Photonics and Photonics-Technology, Northwest University, Xi’an 710069, China
  • 2Shaanxi Engineering Technology Research Center for Solid State Lasers and Application, Xi’an 710069, China
  • 3Institute of Photonics and Photonics-Technology, Provincial Key Laboratory of Photoelectronic Technology, Northwest University, Xi’an 710069, China
  • 4School of Physics, Northwest University, Xi’an 710069, China
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    (a) Raman spectrum of the MoS2 film. (b) The transmission spectrum of the MoS2 film.

    Fig. 1. (a) Raman spectrum of the MoS2 film. (b) The transmission spectrum of the MoS2 film.

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    Experimental setup of the SF fiber laser based on the LMF. WDM: wavelength division multiplexer.

    Fig. 2. Experimental setup of the SF fiber laser based on the LMF. WDM: wavelength division multiplexer.

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    Longitudinal mode oscillations over one FSR scanned by an F–P interferometer. (a) Multi-longitudinal mode oscillation without PC. (b) Longitudinal mode oscillation with PC1 and PC3. (c) Single longitudinal mode oscillation with PC2. (d) Multi-longitudinal mode oscillation without the MoS2 film.

    Fig. 3. Longitudinal mode oscillations over one FSR scanned by an F–P interferometer. (a) Multi-longitudinal mode oscillation without PC. (b) Longitudinal mode oscillation with PC1 and PC3. (c) Single longitudinal mode oscillation with PC2. (d) Multi-longitudinal mode oscillation without the MoS2 film.

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    (a) Emission spectrum of the SF laser with the MoS2. (b) The output power versus pump power of the SF laser. (c) The power and wavelength stabilities of the fiber laser for 1 h.

    Fig. 4. (a) Emission spectrum of the SF laser with the MoS2. (b) The output power versus pump power of the SF laser. (c) The power and wavelength stabilities of the fiber laser for 1 h.

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    Line shape of the heterodyne signal measured with a 30 km fiber delay.

    Fig. 5. Line shape of the heterodyne signal measured with a 30 km fiber delay.

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    Baole Lu, Limei Yuan, Xinyuan Qi, Lei Hou, Bo Sun, Pan Fu, Jintao Bai. MoS2 saturable absorber for single frequency oscillation of highly Yb-doped fiber laser[J]. Chinese Optics Letters, 2016, 14(7): 071404

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    Paper Information

    Category: Lasers and Laser Optics

    Received: Mar. 28, 2016

    Accepted: May. 16, 2016

    Published Online: Aug. 3, 2018

    The Author Email: Baole Lu (lubaole1123@163.com)

    DOI:10.3788/COL201614.071404

    Topics

    laser devices and laser physics
    Lasers and Laser Optics
    Laser physics
    laser manufacturing
    Instrumentation, Measurement and Metrology