• Laser & Optoelectronics Progress
  • Vol. 58, Issue 19, 1906004 (2021)
Hao Wen, Yang Cao*, Xiaofeng Peng, and Yuchao Dang
Author Affiliations
  • School of Electrical and Electronic Engineering, Chongqing University of Technology, Chongqing 400054, China
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    DOI: 10.3788/LOP202158.1906004 Cite this Article Set citation alerts
    Hao Wen, Yang Cao, Xiaofeng Peng, Yuchao Dang. MIMO Polarization-Coding Method in Free Space Optical Communication[J]. Laser & Optoelectronics Progress, 2021, 58(19): 1906004 Copy Citation Text show less
    Transmission model of the space-time polarization-coding
    Fig. 1. Transmission model of the space-time polarization-coding
    Relative characteristics of the polarized sub-channels
    Fig. 2. Relative characteristics of the polarized sub-channels
    Flow chart of the partial order construction
    Fig. 3. Flow chart of the partial order construction
    BER of different polarization code construction schemes. (a) σL2=0.16; (b) σL2=2.2
    Fig. 4. BER of different polarization code construction schemes. (a) σL2=0.16; (b) σL2=2.2
    BER of SISO and MIMO under different turbulence intensities. (a) σL2= 0.16 (SISO); (b) σL2= 2.2 (SISO); (c) σL2= 0.16 (MIMO); (d) σL2= 2.2 (MIMO)
    Fig. 5. BER of SISO and MIMO under different turbulence intensities. (a) σL2= 0.16 (SISO); (b) σL2= 2.2 (SISO); (c) σL2= 0.16 (MIMO); (d) σL2= 2.2 (MIMO)
    MIMO-polar performance under different code lengths and code rates. (a) σL2=0.16, N=512; (b) σL2=0.16, N=1024; (c) σL2=2.2, N=512; (d) σL2=2.2, N=1024
    Fig. 6. MIMO-polar performance under different code lengths and code rates. (a) σL2=0.16, N=512; (b) σL2=0.16, N=1024; (c) σL2=2.2, N=512; (d) σL2=2.2, N=1024
    Wavelength /nm1550
    Modulation4-PPM
    Transmission distance /km2
    σL20.16,2.2
    Extinction ratio /dB20
    Table 1. Parameters in the simulation experiment
    Hao Wen, Yang Cao, Xiaofeng Peng, Yuchao Dang. MIMO Polarization-Coding Method in Free Space Optical Communication[J]. Laser & Optoelectronics Progress, 2021, 58(19): 1906004
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