• Infrared and Laser Engineering
  • Vol. 50, Issue 9, 20210242 (2021)
Xueting Liu1、2、3, Yanwang Zhai1、2、3, Shiyao Fu1、2、3, and Chunqing Gao1、2、3
Author Affiliations
  • 1School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
  • 2Key Laboratory of Information Photonics Technology, Ministry of Industry and Information Technology, Beijing 100081, China
  • 3Key Laboratory of Photoelectronic Imaging Technology and System Ministry of Education,Beijing 100081, China
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    DOI: 10.3788/IRLA20210242 Cite this Article
    Xueting Liu, Yanwang Zhai, Shiyao Fu, Chunqing Gao. Selection of full Poincaré beams with higher robustness in turbulent atmosphere (Invited)[J]. Infrared and Laser Engineering, 2021, 50(9): 20210242 Copy Citation Text show less
    2nd order FPBs (m=2, n=0) with C-point polarization on HyOPS
    Fig. 1. 2nd order FPBs (m=2, n=0) with C-point polarization on HyOPS
    Polarization and intensity of beams in (a) low-order correspondence and (b) high-order correspondence. ID: intensity distribution; RCP: right-handed circular polarization; LCP: left-handed circular polarization
    Fig. 2. Polarization and intensity of beams in (a) low-order correspondence and (b) high-order correspondence. ID: intensity distribution; RCP: right-handed circular polarization; LCP: left-handed circular polarization
    NCC of 2nd and 4th order FPBs at different propagation distances and turbulence intensities
    Fig. 3. NCC of 2nd and 4th order FPBs at different propagation distances and turbulence intensities
    OAM components and mode purity of (a) the 2nd order FPB and (b) the 4th order FPB under different turbulence intensities at 3 km
    Fig. 4. OAM components and mode purity of (a) the 2nd order FPB and (b) the 4th order FPB under different turbulence intensities at 3 km
    Comparison on NCC between (a) class 1 and (b) class 2 under different distances and turbulence intensities
    Fig. 5. Comparison on NCC between (a) class 1 and (b) class 2 under different distances and turbulence intensities
    Comparison on MP between class 1 and class 2 under different turbulence intensities at 3 km
    Fig. 6. Comparison on MP between class 1 and class 2 under different turbulence intensities at 3 km
    (a) NCC and (b) MP between 2nd order FPB and 1st order CVB with 2θ change (2σ=0, r0 = 0.125 m)
    Fig. 7. (a) NCC and (b) MP between 2nd order FPB and 1st order CVB with 2θ change (2σ=0, r0 = 0.125 m)
    The first three rows: NCC and MP performance of class 1 and class 2 when changing coordinates along a latitude line with 2θ=0 under (a), (d) weak turbulence (r0=0.5 m); (b), (e) moderate turbulence (r0=0.125 m) and (c), (g) strong turbulence (r0=0.056 m) respectively. The last three rows: the dominated longitude and latitude regions of (g), (h), (i) 2nd FPBs and (j), (k), (l) 4th FPBs on HyOPS under weak, moderate and strong turbulence
    Fig. 8. The first three rows: NCC and MP performance of class 1 and class 2 when changing coordinates along a latitude line with 2θ=0 under (a), (d) weak turbulence (r0=0.5 m); (b), (e) moderate turbulence (r0=0.125 m) and (c), (g) strong turbulence (r0=0.056 m) respectively. The last three rows: the dominated longitude and latitude regions of (g), (h), (i) 2nd FPBs and (j), (k), (l) 4th FPBs on HyOPS under weak, moderate and strong turbulence
    [in Chinese]
    Fig. 8. [in Chinese]
    Light intensity distributions of 2nd order FPB in radial direction with 2σ change(without AT)
    Fig. 9. Light intensity distributions of 2nd order FPB in radial direction with 2σ change(without AT)
    Xueting Liu, Yanwang Zhai, Shiyao Fu, Chunqing Gao. Selection of full Poincaré beams with higher robustness in turbulent atmosphere (Invited)[J]. Infrared and Laser Engineering, 2021, 50(9): 20210242
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