Chinese Optics Letters, Volume. 22, Issue 11, 111402(2024)

Over 100 mW linearly polarized single-frequency fiber laser based on Er:YAG crystal-derived silica fiber

Xinyue Li1, Jianxiang Wen1、*, Yanhua Luo1, Wei Chen1, Fufei Pang1, Gang-Ding Peng2, and Tingyun Wang1
Author Affiliations
  • 1Key Laboratory of Specialty Fiber Optics and Optical Access Networks, Joint International Research Laboratory of Specialty Fiber Optics and Advanced Communication, School of Communication and Information Engineering, Shanghai University, Shanghai 200444, China
  • 2Photonics & Optical Communications, School of Electrical Engineering & Telecommunications, University of New South Wales, Sydney, NSW 2052, Australia
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    Figures & Tables(9)
    Properties of the EYDSF. (a) Distribution of the refractive index difference. (b) The absorption spectrum. (c) The excitation-emission spectra. (d) The fluorescence decay curves.
    Gain coefficients, unsaturated absorption, and laser output power with different pump wavelengths. (a) Gain coefficients as a function of the pump powers. (b) Unsaturated absorptions of 980 and 1480 nm pumps. (c) Output power of the DBR laser as a function of the pump power (the difference between the input pump power and the residual pump power) at different pump wavelengths without the mirror.
    Experimental setup. (a) The fiber laser system. (b) The transmission spectra of the FBG pairs. (c) Calculation of SLM conditions.
    Longitudinal modes and linewidth characteristics of the DBR fiber laser. (a) Radio frequency beating intensities of the fiber laser at different pump powers. (b) The heterodyne signal of the fiber laser with a pump power of 565 mW.
    Properties of the LP-DBR fiber laser. (a) Slope efficiency of the fiber laser with and without fiber mirror. (b) The output spectrum of the lasing under the maximum output power, and the inset is a zoomed-in view near the laser peak.
    Polarization state of the laser. (a) Output power of the different angles of the polarizer. (b) The stability of the PER at different pump powers.
    (a) Relative intensity noise (RIN) (the inset shows the laser output power dependences on time measured by an oscilloscope). (b) Laser power stability recorded within 2 h at 103 mW (the inset shows the power recorded in half an hour).
    • Table 1. Comparison of Properties for Different EYDSFs

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      Table 1. Comparison of Properties for Different EYDSFs

      SampleConcentration of Er2O3 [% (mass fration)]Gain Coefficient (dB/cm)Core Diameter (μm)NASplicing Loss (dB) @ SMF-EYDSFRef.
      EYDSF-12.961.46 @976 nm pump12.30.530.13[23]
      EYDSF-24.061.20 @976 nm pump
      EYDSF-33.491.72 @980 nm pump12.50.38[25]
      EYDSF-43.401.75 @980 nm pump12.40.370.11This work
      2.11 @1480 nm pump
    • Table 2. Performance Parameters of Linear-Cavity SFFLs Based on Different Er-Doped Fibers

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      Table 2. Performance Parameters of Linear-Cavity SFFLs Based on Different Er-Doped Fibers

      Fiber TypeGain Coefficient (dB/cm)Slope Efficiency (%)Output Power (mW)RIN (dB/Hz)Length (cm)Polarization StateRef.
      Er-doped silica fiber6.848−95400LP (15 dB)[26]
      0.92 @1530 nm15LP (20 dB)[27]
      0.5 @1530 nm2550250[28]
      Er-doped phosphate fiber3.1 @1535 nm0.852−901.8[29]
      EYDSF1.46 @1550 nm15.124.21.8[23]
      2.11 @1560 nm22.4103−1392LP (25 dB)This work
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    Xinyue Li, Jianxiang Wen, Yanhua Luo, Wei Chen, Fufei Pang, Gang-Ding Peng, Tingyun Wang, "Over 100 mW linearly polarized single-frequency fiber laser based on Er:YAG crystal-derived silica fiber," Chin. Opt. Lett. 22, 111402 (2024)

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    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Mar. 10, 2024

    Accepted: May. 29, 2024

    Published Online: Nov. 15, 2024

    The Author Email: Jianxiang Wen (wenjx@shu.edu.cn)

    DOI:10.3788/COL202422.111402

    CSTR:32184.14.COL202422.111402

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