• Photonics Research
  • Vol. 9, Issue 5, 649 (2021)
Ying Wan1, Jianxiang Wen1、*, Chen Jiang1, Fengzai Tang2、4, Jing Wen3, Sujuan Huang1, Fufei Pang1, and Tingyun Wang1、5
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
  • 2WMG, University of Warwick, Coventry CV4 7AL, UK
  • 3Optoelectronics Research Centre, University of Southampton, Southampton SO17 1BJ, UK
  • 4e-mail: fengzai.Tang@warwick.ac.uk
  • 5e-mail: tywang@shu.edu.cn
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    DOI: 10.1364/PRJ.419178 Cite this Article Set citation alerts
    Ying Wan, Jianxiang Wen, Chen Jiang, Fengzai Tang, Jing Wen, Sujuan Huang, Fufei Pang, Tingyun Wang. Over 255 mW single-frequency fiber laser with high slope efficiency and power stability based on an ultrashort Yb-doped crystal-derived silica fiber[J]. Photonics Research, 2021, 9(5): 649 Copy Citation Text show less
    (a) Schematic diagram of YCDSF fabrication using the preform with a YAG crystal core and a silica cladding, where the insets are the optical images of the (1) side view and (2) cross-sectional view of the YCDSF; (b) XRD analysis of the YAG crystal rod and the fiber cores.
    Fig. 1. (a) Schematic diagram of YCDSF fabrication using the preform with a YAG crystal core and a silica cladding, where the insets are the optical images of the (1) side view and (2) cross-sectional view of the YCDSF; (b) XRD analysis of the YAG crystal rod and the fiber cores.
    (a) Absorption and emission cross sections of the YCDSF; (b) gain cross section of the YCDSF.
    Fig. 2. (a) Absorption and emission cross sections of the YCDSF; (b) gain cross section of the YCDSF.
    Setup of the DBR SFFL based on a 0.7 cm long YCDSF and the laser measurement system (WDM, wavelength-division multiplexer; ISO, isolator; LR-FBG, low-reflectivity fiber Bragg grating; HR-FBG, high-reflectivity fiber Bragg grating; TC, temperature controller; VOA, variable optical attenuator; OSA, optical spectrum analyzer; PM, power meter; ESA, electric spectrum analyzer; PD, photodetector).
    Fig. 3. Setup of the DBR SFFL based on a 0.7 cm long YCDSF and the laser measurement system (WDM, wavelength-division multiplexer; ISO, isolator; LR-FBG, low-reflectivity fiber Bragg grating; HR-FBG, high-reflectivity fiber Bragg grating; TC, temperature controller; VOA, variable optical attenuator; OSA, optical spectrum analyzer; PM, power meter; ESA, electric spectrum analyzer; PD, photodetector).
    (a) Calculated effective length of the HR-FBG and LR-FBG with respect to reflectivity; (b) calculated longitudinal mode spacing as a function of YCDSF length.
    Fig. 4. (a) Calculated effective length of the HR-FBG and LR-FBG with respect to reflectivity; (b) calculated longitudinal mode spacing as a function of YCDSF length.
    Radio-frequency beating spectra of the built fiber laser with a 0.7 cm long YCDSF at different pump powers, measured by a delayed self-heterodyne measurement system.
    Fig. 5. Radio-frequency beating spectra of the built fiber laser with a 0.7 cm long YCDSF at different pump powers, measured by a delayed self-heterodyne measurement system.
    (a) Output power of the SFFL as a function of pump power, and the inset shows a magnified view of the graph at a pump power range of 0 to 70 mW; (b) output spectrum of the single-frequency fiber laser under the maximum output power, and the inset is an enlarged view at the wavelengths of 1028–1031 nm.
    Fig. 6. (a) Output power of the SFFL as a function of pump power, and the inset shows a magnified view of the graph at a pump power range of 0 to 70 mW; (b) output spectrum of the single-frequency fiber laser under the maximum output power, and the inset is an enlarged view at the wavelengths of 1028–1031 nm.
    (a) Laser stability record within 13 h at 210.5 mW; (b) beam quality of the fiber laser and its two-dimensional beam profile.
    Fig. 7. (a) Laser stability record within 13 h at 210.5 mW; (b) beam quality of the fiber laser and its two-dimensional beam profile.
    Measured (a) relative intensity noise (RIN), (b) heterodyne signal, and (c) linewidth of the SFFL versus the pump power.
    Fig. 8. Measured (a) relative intensity noise (RIN), (b) heterodyne signal, and (c) linewidth of the SFFL versus the pump power.
    Fiber TypeYb-Doped Phosphate Glass FibersYb-Doped Silica Fiber (Fibercore, DF1100)Yb-Doped Silica FiberYCDSF-1YCDSF
    Yb concentration (%, mass fraction)18.3015.20<1.00<1.00/4.805.66
    Gain coefficient (dB/cm)/5.7 at 1064 nm///1.7 at 1064 nm4.4 at 1030 nm
    Gain fiber length (cm)1.80.81.11.91.51.40.7
    Slope efficiency (%)38.675.427.028.0/18.534.9
    Maximum output power (mW)100.0210.7160.0126.235.0110.0258.0
    Threshold power (mW)405051.710/25
    OSNR (dB)6165//658079
    Power stability<0.10% at 8.0 h at 17 mW0.50% at 1.0 h at 34 mW1.30% at 1.0 h at 80 mW0.54% at 0.5 h at 67 mW<0.90% at 2.0 h0.51% at 1.0 h at 110 mW<0.85% at 13.0 h at 210 mW
    Refs.[34][35][36][37][38][13]This work
    Table 1. Summary of the All-Fiber DBR SFFLs Based on Different Gain Fibers
    Ying Wan, Jianxiang Wen, Chen Jiang, Fengzai Tang, Jing Wen, Sujuan Huang, Fufei Pang, Tingyun Wang. Over 255 mW single-frequency fiber laser with high slope efficiency and power stability based on an ultrashort Yb-doped crystal-derived silica fiber[J]. Photonics Research, 2021, 9(5): 649
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