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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- Infrared and Laser Engineering
- Vol. 53, Issue 2, 20230441 (2024)
Fig. 1. Schematic diagram of the beam through phase screen in uplink transmission channel model of ocean turbulence
Fig. 2. Two-dimensional diagram of random ocean turbulence. (a) Phase screen; (b) Phase structure function curves
Fig. 3. Intensity profiles of collimated Gaussian vortex beam at different propagation distance in ocean turbulence of slant path
Fig. 4. Phase profile of collimated Gaussian vortex beam with different topological charges as a function of propagation distance
Fig. 5. Spot centroid distribution
Fig. 6. The beam wander σ c of collimated Gaussian vortex beam. (a) the relationship between beam wander σ c and propagation distance z for the values of different the topological charge l ; (b) the relationship between beam wander σ c and propagation distance z for the values of different the tidal velocity of depth-averaged u
Fig. 7. The beam wander σ c 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 L 0
Fig. 8. The on-axis scintillation index σ I 2 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 L 0
Fig. 9. The long-exposure beam radius W LE 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 L 0
Fig. 10. The long-exposure beam radius W LE 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
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