Research Article
Intensity Distribution of Partially Coherent Array Finite Airy Beams Propagating in Atmospheric Turbulence
Figure 4
Influence of Cn2 on PCAFAB evolution characteristics; other parameters are the same as those in Figure 1(b), and the blue arrow head denotes each beamlet’s acceleration direction: (a) Cn2 = 10−13m−2/3, (z) = 50m; (b) Cn2 = 10−13m−2/3, (z) = 100m; (c) Cn2 = 10−13m−2/3, (z) = 500m; (d) Cn2 = 5 × 10−12m−2/3, (z) = 1000m; (e) zoom in on Figure 4(d) in the first quadrant; (f) Cn2 = 10−11m−2/3, (z) = 500m; (g) Cn2 = 10−9m−2/3, (z) = 100m; (h) Cn2 = 10−9m−2/3, (z) = 250m; (i) Cn2 = 10−8m−2/3, (z) = 50m; (j) Cn2 = 10−8m−2/3, (z) = 100m.
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