• Infrared and Laser Engineering
  • Vol. 53, Issue 2, 20230441 (2024)
Pengfei Wu1、2, Chengyu Li1, Sichen Lei1、2、*, Zhenkun Tan3, and Jiao Wang4
Author Affiliations
  • 1School of Automation and Information Engineering, Xi'an University of Technology, Xi'an 710048, China
  • 2Xi'an Key Laboratory of Wireless Optical Communication and Network Research, Xi'an 710048, China
  • 3Faculty of Optoelectronic Engineering, Xi'an Technological University, Xi'an 710021, China
  • 4School of Electronic Information and Artificial Intelligence, Shaanxi University of Science and Technology, Xi'an 710021, China
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    DOI: 10.3788/IRLA20230441 Cite this Article
    Pengfei Wu, Chengyu Li, Sichen Lei, Zhenkun Tan, Jiao Wang. Propagation properties of the vortex beam in the slant path of ocean turbulence under weak wind model[J]. Infrared and Laser Engineering, 2024, 53(2): 20230441 Copy Citation Text show less
    Schematic diagram of the beam through phase screen in uplink transmission channel model of ocean turbulence
    Fig. 1. Schematic diagram of the beam through phase screen in uplink transmission channel model of ocean turbulence
    Two-dimensional diagram of random ocean turbulence. (a) Phase screen; (b) Phase structure function curves
    Fig. 2. Two-dimensional diagram of random ocean turbulence. (a) Phase screen; (b) Phase structure function curves
    Intensity profiles of collimated Gaussian vortex beam at different propagation distance in ocean turbulence of slant path
    Fig. 3. Intensity profiles of collimated Gaussian vortex beam at different propagation distance in ocean turbulence of slant path
    Phase profile of collimated Gaussian vortex beam with different topological charges as a function of propagation distance
    Fig. 4. Phase profile of collimated Gaussian vortex beam with different topological charges as a function of propagation distance
    Spot centroid distribution
    Fig. 5. Spot centroid distribution
    The beam wander σc of collimated Gaussian vortex beam. (a) the relationship between beam wander σc and propagation distance z for the values of different the topological charge l; (b) the relationship between beam wander σc and propagation distance z for the values of different the tidal velocity of depth-averaged u
    Fig. 6. The beam wander σc of collimated Gaussian vortex beam. (a) the relationship between beam wander σc and propagation distance z for the values of different the topological charge l; (b) the relationship between beam wander σc and propagation distance z for the values of different the tidal velocity of depth-averaged u
    The beam wander σc of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the wind speed W and the zenith angle ζ; (b) For the values of different the outer scale of oceanic turbulence L0
    Fig. 7. The beam wander σc of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the wind speed W and the zenith angle ζ; (b) For the values of different the outer scale of oceanic turbulence L0
    The on-axis scintillation index σI2 of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the wind speed W and the temperature-salinity distribution ratio ω. (b) For the values of different the inner scale of oceanic turbulence η and the outer scale of oceanic turbulence L0
    Fig. 8. The on-axis scintillation index σI2 of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the wind speed W and the temperature-salinity distribution ratio ω. (b) For the values of different the inner scale of oceanic turbulence η and the outer scale of oceanic turbulence L0
    The long-exposure beam radius WLE of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the topological charge l and the zenith angle ζ; (b) For the values of different the temperature-salinity distribution ratio ω and the outer scale of oceanic turbulence L0
    Fig. 9. The long-exposure beam radius WLE of the collimated Gaussian vortex beam versus the propagation distance z. (a) For the values of different the topological charge l and the zenith angle ζ; (b) For the values of different the temperature-salinity distribution ratio ω and the outer scale of oceanic turbulence L0
    The long-exposure beam radius WLE of the collimated Gaussian vortex beam versus the propagation distance z for the values of different the tidal velocity of depth-averaged u and the wind speed W
    Fig. 10. The long-exposure beam radius WLE of the collimated Gaussian vortex beam versus the propagation distance z for the values of different the tidal velocity of depth-averaged u and the wind speed W
    Pengfei Wu, Chengyu Li, Sichen Lei, Zhenkun Tan, Jiao Wang. Propagation properties of the vortex beam in the slant path of ocean turbulence under weak wind model[J]. Infrared and Laser Engineering, 2024, 53(2): 20230441
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