• Chinese Optics Letters
  • Vol. 22, Issue 4, 040603 (2024)
Wenyu Du1, Sen Gao2, Xiaojuan Zhang1, Siqi Li1, Yan Kuai1, Zhiqiang Wang1, Zhigang Cao1, Feng Xu1, Yu Liu1, Lin Xu1, Junxi Zhang2, Kang Xie3, Benli Yu1, and Zhijia Hu1、*
Author Affiliations
  • 1Information Materials and Intelligent Sensing Laboratory of Anhui Province, Key Laboratory of Opto-Electronic Information Acquisition and Manipulation of Ministry of Education, School of Physics and Opto-electronics Engineering, Anhui University, Hefei 230601, China
  • 2School of Instrument Science and Opto-electronics Engineering, Laboratory of Optical Fibers and Micro-nano Photonics, Hefei University of Technology, Hefei 230009, China
  • 3School of Opto-electronic Engineering, Zaozhuang University, Zaozhuang 277160, China
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    DOI: 10.3788/COL202422.040603 Cite this Article Set citation alerts
    Wenyu Du, Sen Gao, Xiaojuan Zhang, Siqi Li, Yan Kuai, Zhiqiang Wang, Zhigang Cao, Feng Xu, Yu Liu, Lin Xu, Junxi Zhang, Kang Xie, Benli Yu, Zhijia Hu. Picosecond gain-switched polymer fiber random lasers[J]. Chinese Optics Letters, 2024, 22(4): 040603 Copy Citation Text show less
    Optical micrographs of three types of disordered POF cross sections, corresponding to (a) POPOF, (b) FePOF, and (c) AuPOF; (d) experimental setup for testing RL emission.
    Fig. 1. Optical micrographs of three types of disordered POF cross sections, corresponding to (a) POPOF, (b) FePOF, and (c) AuPOF; (d) experimental setup for testing RL emission.
    RL emission property of three POFs. The emission spectrum variations with pump energy of POPOF, FePOF, and AuPOF are shown in (a), (c), and (e), respectively. The variations of integral intensity with pump energy of POPOF, FePOF, and AuPOF are shown in (b), (d), and (f), respectively.
    Fig. 2. RL emission property of three POFs. The emission spectrum variations with pump energy of POPOF, FePOF, and AuPOF are shown in (a), (c), and (e), respectively. The variations of integral intensity with pump energy of POPOF, FePOF, and AuPOF are shown in (b), (d), and (f), respectively.
    RL pulse characteristic of polymer fibers. The normalized time distributions for POPOF, FePOF, and AuPOF are shown in (a), (c), and (e), respectively. The emission pulse widths of POPOF, FePOF, and AuPOF are shown in (b), (d), and (f), respectively. The red dotted line represents the threshold for the random lasing emission spectrum.
    Fig. 3. RL pulse characteristic of polymer fibers. The normalized time distributions for POPOF, FePOF, and AuPOF are shown in (a), (c), and (e), respectively. The emission pulse widths of POPOF, FePOF, and AuPOF are shown in (b), (d), and (f), respectively. The red dotted line represents the threshold for the random lasing emission spectrum.
    (a) Simulation of gain and RL pulse compression. The red line is the gain curve of the RLs. The blue line is the pump laser pulse. The green line is the fluorescence pulse below the threshold. The black line is the RL pulse. (b) Simulation of pulse width variation when pump energy is below and above the threshold.
    Fig. 4. (a) Simulation of gain and RL pulse compression. The red line is the gain curve of the RLs. The blue line is the pump laser pulse. The green line is the fluorescence pulse below the threshold. The black line is the RL pulse. (b) Simulation of pulse width variation when pump energy is below and above the threshold.
    (a) Normalized periodic distribution of short pulse RLs within 1 s. Inset, an enlarged view of an RL pulse. (b) Simultaneous acquisition of pump laser and RL pulses.
    Fig. 5. (a) Normalized periodic distribution of short pulse RLs within 1 s. Inset, an enlarged view of an RL pulse. (b) Simultaneous acquisition of pump laser and RL pulses.
    (a) Linewidth of the three POFs at 35,000 pumps; (b) the pulse width of RLs varies with the angle θ.
    Fig. 6. (a) Linewidth of the three POFs at 35,000 pumps; (b) the pulse width of RLs varies with the angle θ.
     Size of Doped NPs (nm)Core Size (µm)Cladding Size (µm)
    POPOF20026.7696.4
    FePOF10 nm Fe3O4@5 nm SiO259.5637.2
    AuPOF2968.4639.5
    Table 1. Parameters of POFs
    POFPump Energy (µJ)Fall Time (ns)Pulse Width (ns)
    POPOF2319.96.4
    3811.62.4
    502.30.6
    FePOF3720.45.8
    408.61.5
    452.10.7
    AuPOF6518.46.6
    8012.82.4
    903.40.7
    Table 2. Single Exponential Decay Fitting of Temporal Properties
    Wenyu Du, Sen Gao, Xiaojuan Zhang, Siqi Li, Yan Kuai, Zhiqiang Wang, Zhigang Cao, Feng Xu, Yu Liu, Lin Xu, Junxi Zhang, Kang Xie, Benli Yu, Zhijia Hu. Picosecond gain-switched polymer fiber random lasers[J]. Chinese Optics Letters, 2024, 22(4): 040603
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