• Laser & Optoelectronics Progress
  • Vol. 60, Issue 7, 0726001 (2023)
Dong Ye*, Zongchen Li, Yi Zhang, Junyao Li, and Yining Ma
Author Affiliations
  • Department of Criminal Science and Technology, Jiangsu Police Institute, Nanjing 210031, Jiangsu, China
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    DOI: 10.3788/LOP213008 Cite this Article Set citation alerts
    Dong Ye, Zongchen Li, Yi Zhang, Junyao Li, Yining Ma. Simulated Generation of Perfect Polarization Singularity Light Fields[J]. Laser & Optoelectronics Progress, 2023, 60(7): 0726001 Copy Citation Text show less
    Electric field distributions of LGB(a)-(d) and PLGB (e)-(h). (a) p=0,l=0; (b) p=0,l=-1; (c) p=0,l=-2; (d) p=2,l=-2; (e) p=0,l=0; (f) p=0,l=-1; (g) p=0,l=-2; (h) p=2,l=-2
    Fig. 1. Electric field distributions of LGB(a)-(d) and PLGB (e)-(h). (a) p=0,l=0; (b) p=0,l=-1; (c) p=0,l=-2; (d) p=2,l=-2; (e) p=0,l=0; (f) p=0,l=-1; (g) p=0,l=-2; (h) p=2,l=-2
    Polarization singular light fields generated by the same beam type. (a), (b) are the Lemon structure and Star structure polarization singular light fields based on PLGB, respectively; (c), (d) are the Lemon structure and Star structure polarization singular light fields based on LGB, respectively
    Fig. 2. Polarization singular light fields generated by the same beam type. (a), (b) are the Lemon structure and Star structure polarization singular light fields based on PLGB, respectively; (c), (d) are the Lemon structure and Star structure polarization singular light fields based on LGB, respectively
    Polarization singular light fields with different topological charges. (a), (b) are the V-points with topological charges of +1 and -1 based on PLGB, respectively; (c), (d) are the V-points with topological charges of +1 and -1 based on LGB, respectively
    Fig. 3. Polarization singular light fields with different topological charges. (a), (b) are the V-points with topological charges of +1 and -1 based on PLGB, respectively; (c), (d) are the V-points with topological charges of +1 and -1 based on LGB, respectively
    Polarization state distributions of polarized singular light fields with topological charge being +1/2 or -1/2 on the initial plane. (a) Lemon structure of left-handed polarization; (b) Star structure of right-handed polarization; (c) Star structure with both left-handed and right-handed polarizations; (d) Lemon structure with both left-handed and right-handed polarizations
    Fig. 4. Polarization state distributions of polarized singular light fields with topological charge being +1/2 or -1/2 on the initial plane. (a) Lemon structure of left-handed polarization; (b) Star structure of right-handed polarization; (c) Star structure with both left-handed and right-handed polarizations; (d) Lemon structure with both left-handed and right-handed polarizations
    Polarization state distributions of polarized singular light fields with topological charge being +1 or -1 on the initial plane. (a) EL is LGB with p=0, l=1 and ER is PLGB with p=0, l=-1; (b) EL is PLGB with p=0, l=-1 and ER is LGB with p=0, l=1
    Fig. 5. Polarization state distributions of polarized singular light fields with topological charge being +1 or -1 on the initial plane. (a) EL is LGB with p=0, l=1 and ER is PLGB with p=0, l=-1; (b) EL is PLGB with p=0, l=-1 and ER is LGB with p=0, l=1
    Stokes phase and ellipticity of the quasi high-order polarization singularity light field. (a) Stokes phase field; (b) distribution of ellipticity
    Fig. 6. Stokes phase and ellipticity of the quasi high-order polarization singularity light field. (a) Stokes phase field; (b) distribution of ellipticity
    High-order polarization singularity light field when EL is the PLGB with p=0, l=0, and ER is the PLGB with p=0, l=-2. (a) Polarization states of the light field; (b) Stokes phase field of the light field; (c) ellipticity of the light field
    Fig. 7. High-order polarization singularity light field when EL is the PLGB with p=0, l=0, and ER is the PLGB with p=0, l=-2. (a) Polarization states of the light field; (b) Stokes phase field of the light field; (c) ellipticity of the light field
    Polarization states of perfect polarization singularities at different distances during free propagation(the upper row is C-points and the down row is V-points). (a) Propagation distance z = 100 mm; (b) propagation distance z = 300 mm; (c) propagation distance z = 1000 mm
    Fig. 8. Polarization states of perfect polarization singularities at different distances during free propagation(the upper row is C-points and the down row is V-points). (a) Propagation distance z = 100 mm; (b) propagation distance z = 300 mm; (c) propagation distance z = 1000 mm
    Dong Ye, Zongchen Li, Yi Zhang, Junyao Li, Yining Ma. Simulated Generation of Perfect Polarization Singularity Light Fields[J]. Laser & Optoelectronics Progress, 2023, 60(7): 0726001
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