Author Affiliations
Department of Physics, School of Science and Technology, Nazarbayev University, 53 Qabanbay Batyr Ave, Astana KZ-010000, Kazakhstanshow less
Fig. 1. Schematic of the regarded configuration. The aggregate field of an active laser array is perturbed by a passive cylindrical obstacle.
Fig. 2. Percent error of the obstacle-free optimal solution as functions of: (a) radius of the obstacle b/λ0 (ϵ=2) and (b) relative permittivity of the obstacle ϵ (b=λ0/4) for several vertical positions yb. Plot parameters: G˜(φ)=e−γ(φ−ϑ)2, ϑ=90°, γ=10, k0L=0.1, M=80, U=12, xb=0.
Fig. 3. Percent error of the obstacle-free optimal solution as a function of the horizontal position of the obstacle xb/D=xb/(ML) for several (a) radii b/λ0 (ϵ=2) and (b) permittivities ϵ (b=λ0/4). Plot parameters: yb=2λ0, and the remaining ones the same as in Fig. 2.
Fig. 4. Percent error of the obstacle-free optimal solution in contour plot of the permittivity ϵ and the electrical radius of the cylinder b/λ0 for (a) centered obstacle (xb=0) and (b) off-centered obstacle (xb=ML=D=4λ0/π). Plot parameters: yb=2λ0 and the remaining ones the same as in Fig. 2.
Fig. 5. Ideal target
G˜(φ) and the optimal actual pattern
G(φ) (both real and imaginary parts) as functions of azimuthal angle
φ for the obstacle-free solution of Ref. [
5] with (a)
b=λ0/8, (b)
b=λ0/4, (c)
b=λ0/2, and (d) for the solution of Section
2 of this study and the worst case
b=λ0/2. Plot parameters:
ϵ=2,
xb=0,
yb=2λ0, and the remaining ones the same as in Fig.
2.
Fig. 6. (a) Percent error of optimal solution without and with the obstacle as a function of the optical distance between two neighboring lasers k0L. (b) Ideal target G˜(φ) and the optimal actual pattern G(φ) (both real and imaginary parts) as functions of azimuthal angle φ for k0L=2.4. The configuration of Fig. 5(c) is considered.
Fig. 7. Ideal target
G˜(φ) and the optimal actual pattern
G(φ) (both real and imaginary parts) as functions of azimuthal angle
φ for the obstacle-free solution of Ref. [
5] with (a)
ϵ=1.5, (b)
ϵ=2, (c)
ϵ=2.5, and (d) for the solution of Section
2 of this study and the worst case
ϵ=2.5. Plot parameters:
G˜(φ)=e−βφ[1+A cos(αφ)],
A=0.7,
α=13.5,
β=0.2,
k0L=1,
M=50,
U=12,
b=λ0/4,
xb=0,
yb=2λ0.
Fig. 8. Block diagram for the introduced processes and presented concepts of the study at hand. A greedy inverse search by trial and error for the actual obstacle; as long as the error is non-negligible, a new trial object is considered.