Acta Optica Sinica, Volume. 38, Issue 6, 0601004(2018)
Propagation Properties of Gaussian Array Beams Transmitted in Oceanic Turbulence Simulated by Phase Screen Method
Fig. 2. Schematic of different beam arrangements. (a) 3×3 beam array with rectangle distribution; (b) 7 beam array with radial distribution; (c) single Gaussian beam
Fig. 3. Average radii of beams under different turbulence conditions. (a) Z=10 m, ε=10-6 m2·s-3, ω=-2,η=0.001 m, λ=532 nm; (b) Z=10 m, ε=10-6 m2·s-3, χT=10-6 K2·s-1, η=0.001 m, λ=532 nm; (c) ε=10-6 m2·s-3, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm; (d) Z=10 m, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm
Fig. 5. Standard deviation of spot centroid wander. (a) Z=10 m, ε=10-6 m2·s-3, ω=-2, η=0.001 m, λ=532 nm; (b) Z=10 m, ε=10-6 m2·s-3, χT=10-6 K2·s-1, η=0.001 m, λ=532 nm; (c) ε=10-6 m2·s-3, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm; (d) Z=10 m, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm
Fig. 6. Numerical simulation of on-axis scintillation index of beam array. (a) Z=10 m, ε=10-6 m2·s-3, ω=-2, η=0.001 m, λ=532 nm; (b) Z=10 m, ε=10-6 m2·s-3, χT=10-6 K2·s-1, η=0.001 m, λ=532 nm; (c) ε=10-6 m2·s-3, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm; (d) Z=10 m, χT=10-6 K2·s-1, ω=-2, η=0.001 m, λ=532 nm
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Chaojun Niu, Fang Lu, Xiang'e Han. Propagation Properties of Gaussian Array Beams Transmitted in Oceanic Turbulence Simulated by Phase Screen Method[J]. Acta Optica Sinica, 2018, 38(6): 0601004
Category: Atmospheric Optics and Oceanic Optics
Received: Dec. 12, 2017
Accepted: --
Published Online: Jul. 9, 2018
The Author Email: Han Xiang'e (xehan@mail.xid)