• Laser & Optoelectronics Progress
  • Vol. 60, Issue 1, 0119001 (2023)
Xiangshuai Guo, Shangqi Kuang*, and Yuling Feng**
Author Affiliations
  • School of Physics, Changchun University of Science and Technology, Changchun 130022, Jilin , China
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    DOI: 10.3788/LOP212600 Cite this Article Set citation alerts
    Xiangshuai Guo, Shangqi Kuang, Yuling Feng. Comparison of Calculation Methods for Chaotic Laser in Semiconductor Laser System[J]. Laser & Optoelectronics Progress, 2023, 60(1): 0119001 Copy Citation Text show less
    Schematic diagram of optical feedback semiconductor laser system
    Fig. 1. Schematic diagram of optical feedback semiconductor laser system
    Schematic diagram of optical injection-optical feedback semiconductor laser system
    Fig. 2. Schematic diagram of optical injection-optical feedback semiconductor laser system
    Maximum Lyapunov exponent as a function of feedback strength of optical feedback semiconductor laser system
    Fig. 3. Maximum Lyapunov exponent as a function of feedback strength of optical feedback semiconductor laser system
    Attractors of laser intensity in phase space for various linewidth enhancement factor α. Simulation method of photoelectric field amplitude-phase decomposition for system when (a) α=3 and (c) α=8;simulation method of photoelectric field real-imaginary part solution for system when (b) α=3 and (d) α=8. Two-dimensional phase space consists of laser intensity It=E2t and carrier density Nt
    Fig. 4. Attractors of laser intensity in phase space for various linewidth enhancement factor α. Simulation method of photoelectric field amplitude-phase decomposition for system when (a) α=3 and (c) α=8;simulation method of photoelectric field real-imaginary part solution for system when (b) α=3 and (d) α=8. Two-dimensional phase space consists of laser intensity It=E2t and carrier density Nt
    Maximum Lyapunov exponent as a function of feedback strength with optical injection-optical feedback semiconductor laser system
    Fig. 5. Maximum Lyapunov exponent as a function of feedback strength with optical injection-optical feedback semiconductor laser system
    Attractors of laser intensity in space for various linewidth enhancement factor α. Simulation method of photoelectric field amplitude-phase decomposition for system when (a) α=3 and (c) α=8;simulation method of photoelectric field real-imaginary part solution for system when (b) α=3 and (d) α=8. Two-dimensional phase space consists of laser intensity It=E2t and carrier density Nt
    Fig. 6. Attractors of laser intensity in space for various linewidth enhancement factor α. Simulation method of photoelectric field amplitude-phase decomposition for system when (a) α=3 and (c) α=8;simulation method of photoelectric field real-imaginary part solution for system when (b) α=3 and (d) α=8. Two-dimensional phase space consists of laser intensity It=E2t and carrier density Nt
    Feedback term of semiconductor laser system with optical injection-optical feedback using different decomposition calculation methods. (a) Amplitude-phase decomposition calculation method; (b) real-imaginary part solution calculation method
    Fig. 7. Feedback term of semiconductor laser system with optical injection-optical feedback using different decomposition calculation methods. (a) Amplitude-phase decomposition calculation method; (b) real-imaginary part solution calculation method
    Phase feedback terms at different feedback intensities of amplitude-phase simulation method in optical injection-optical feedback semiconductor laser system. (a) κ=3.106 ns-1; (b) κ=4.659 ns-1; (c) κ=6.212 ns-1
    Fig. 8. Phase feedback terms at different feedback intensities of amplitude-phase simulation method in optical injection-optical feedback semiconductor laser system. (a) κ=3.106 ns-1; (b) κ=4.659 ns-1; (c) κ=6.212 ns-1
    Phase feedback items at different linewidth enhancement factors of amplitude-phase simulation method in optical injection-optical feedback system. (a) α=3; (b) α=5; (c) α=8
    Fig. 9. Phase feedback items at different linewidth enhancement factors of amplitude-phase simulation method in optical injection-optical feedback system. (a) α=3; (b) α=5; (c) α=8
    SymbolParameterValue
    GNGain coefficient8.40×10-13 m3·s-1
    NCarrier density at transparency1.40×10-24 m-3
    εGain saturation coefficient2.5×10-23
    τpPhoton lifetime1.927×10-12 s
    τsCarrier lifetime2.04×10-9 s
    τinRound-trip time in internal cavity8.0×10-12 s
    r2Reflectivity of laser facet0.556
    αLine width enhancement factor3.0
    λOptical wavelength of laser1.537×10-6 m
    cSpeed of light2.998×108 m·s-1
    τ

    Round-trip time of light in external cavity

    (feedback delay time)for response laser

    1.501×10-9 s
    κFeedback strength1.553×10-9 s
    JInjection current1.098×1033 m-3·s-1
    Table 1. Parameters of semiconductor laser system
    Xiangshuai Guo, Shangqi Kuang, Yuling Feng. Comparison of Calculation Methods for Chaotic Laser in Semiconductor Laser System[J]. Laser & Optoelectronics Progress, 2023, 60(1): 0119001
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