• High Power Laser and Particle Beams
  • Vol. 33, Issue 11, 111006 (2021)
Yu Huang1, Pei Zhou1、2, Yigong Yang1, Nianqiang Li1、2、*, and Xiaofeng Li1、2、*
Author Affiliations
  • 1School of Optoelectronic Science and Engineering, Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China
  • 2Key Laboratory of Advanced Optical Manufacturing Technologies of Jiangsu Province, Key Laboratory of Modern Optical Technologies of Education Ministry of China, Soochow University, Suzhou 215006, China
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    DOI: 10.11884/HPLPB202133.210323 Cite this Article
    Yu Huang, Pei Zhou, Yigong Yang, Nianqiang Li, Xiaofeng Li. Progress in research of dynamic properties and applications of spin-lasers[J]. High Power Laser and Particle Beams, 2021, 33(11): 111006 Copy Citation Text show less
    Intensity time sequence of the spin-VCSEL
    Fig. 1. Intensity time sequence of the spin-VCSEL
    The real parts of the critical eigenvalues λ for the in-phase (solid line) and out of phase (dashed line) solution as a function of P, where η=1.8
    Fig. 2. The real parts of the critical eigenvalues λ for the in-phase (solid line) and out of phase (dashed line) solution as a function of P, where η=1.8
    Bifurcation diagram of the RCP intensity
    Fig. 3. Bifurcation diagram of the RCP intensity
    Bifurcation diagrams (κ=230 ns−1, γa=0, γp=8.8π ns−1, γs=30 ns−1, γ=0.68 ns−1, α=4, P=−0.1[39])
    Fig. 4. Bifurcation diagrams (κ=230 ns−1, γa=0, γp=8.8π ns−1, γs=30 ns−1, γ=0.68 ns−1, α=4, P=−0.1[39])
    Schematics of spin polarization modulation
    Fig. 5. Schematics of spin polarization modulation
    Simulated intensity modulation and polarization modulation (κ=325 ns−1, γa=0, γs=450 ns−1, γ=1 ns−1, α=5, P=0 [22])
    Fig. 6. Simulated intensity modulation and polarization modulation (κ=325 ns−1, γa=0, γs=450 ns−1, γ=1 ns−1, α=5, P=0 [22])
    Polarization modulation response at various polarization ellipticity (κ=325 ns−1, γa=0, γs=450 ns−1, γ=1 ns−1, α=5, η=5.4[22])
    Fig. 7. Polarization modulation response at various polarization ellipticity (κ=325 ns−1, γa=0, γs=450 ns−1, γ=1 ns−1, α=5, η=5.4[22])
    Schematic model of spin-injected birefringent VCSEL toward analog radio-over-fiber systems [62]
    Fig. 8. Schematic model of spin-injected birefringent VCSEL toward analog radio-over-fiber systems [62]
    Schematic of reservoir computing based on a spin-VCSEL with delayed feedback
    Fig. 9. Schematic of reservoir computing based on a spin-VCSEL with delayed feedback
    Schematic of the proposed photonic microwave generation system and optical spectra and radio-frequency spectra
    Fig. 10. Schematic of the proposed photonic microwave generation system and optical spectra and radio-frequency spectra
    Cross-correlation between the master laser and slave laser
    Fig. 11. Cross-correlation between the master laser and slave laser
    Modulated pump magnitude and polarization of the master spin-VCSEL (PM,S=−0.1)
    Fig. 12. Modulated pump magnitude and polarization of the master spin-VCSEL (PM,S=−0.1)
    Key distribution based on spin-VCSELs
    Fig. 13. Key distribution based on spin-VCSELs
    Yu Huang, Pei Zhou, Yigong Yang, Nianqiang Li, Xiaofeng Li. Progress in research of dynamic properties and applications of spin-lasers[J]. High Power Laser and Particle Beams, 2021, 33(11): 111006
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