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Articles

Numerical method for inverse scattering in two-layered background in near-field optics

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Pages 130-154 | Received 23 Apr 2013, Accepted 26 Jan 2014, Published online: 28 Feb 2014

Figures & data

Figure 1. The geometry of the model problem. The scatterer q(x) is in a compact support in D, the measurements are taken on Γ and Ω is a compact set containing D and Γ.

Figure 1. The geometry of the model problem. The scatterer q(x) is in a compact support in D, the measurements are taken on Γ and Ω is a compact set containing D and Γ.

Figure 2. Direct discretization method and Tikhonov regularization of problem (Equation4.1).

Figure 2. Direct discretization method and Tikhonov regularization of problem (Equation4.14.1 g(t)=∫01e-tsf(s)ds,t∈[0,1],4.1 ).

Figure 3. Moment method and moment method with truncated SVD for problem (Equation4.1).

Figure 3. Moment method and moment method with truncated SVD for problem (Equation4.14.1 g(t)=∫01e-tsf(s)ds,t∈[0,1],4.1 ).

Figure 4. Computing model.

Figure 4. Computing model.

Figure 5. 2c=λ/2, b=λ/2, σ=0, Λ=10-8.

Figure 5. 2c=λ/2, b=λ/2, σ=0, Λ=10-8.

Figure 6. 2c=λ/2, b=λ/2, σ=0, Λ=10-6.

Figure 6. 2c=λ/2, b=λ/2, σ=0, Λ=10-6.

Figure 7. 2c=λ/2, b=λ/2, σ=10-6, Λ=10-6.

Figure 7. 2c=λ/2, b=λ/2, σ=10-6, Λ=10-6.

Figure 8. 2c=λ/2, b=λ/2, σ=10-6, Λ=10-3.

Figure 8. 2c=λ/2, b=λ/2, σ=10-6, Λ=10-3.

Figure 9. 2c=λ/2, b=λ/2, σ=10-3, Λ=10-6.

Figure 9. 2c=λ/2, b=λ/2, σ=10-3, Λ=10-6.

Figure 10. 2c=λ/2, b=λ/2, σ=10-3, Λ=10-3.

Figure 10. 2c=λ/2, b=λ/2, σ=10-3, Λ=10-3.

Figure 11. 2c=λ/2, b=λ, σ=0, Λ=10-6.

Figure 11. 2c=λ/2, b=λ, σ=0, Λ=10-6.

Figure 12. 2c=λ/2, b=λ, σ=10-6, Λ=10-6.

Figure 12. 2c=λ/2, b=λ, σ=10-6, Λ=10-6.

Figure 13. 2c=λ/2, b=λ, σ=10-3, Λ=10-3.

Figure 13. 2c=λ/2, b=λ, σ=10-3, Λ=10-3.

Figure 14. 2c=λ/4, b=λ/2, σ=0, Λ=10-6.

Figure 14. 2c=λ/4, b=λ/2, σ=0, Λ=10-6.

Figure 15. 2c=λ/4, b=λ/2, σ=10-3, Λ=10-3.

Figure 15. 2c=λ/4, b=λ/2, σ=10-3, Λ=10-3.

Figure 16. 2c=λ/4, b=λ, σ=0, Λ=10-6.

Figure 16. 2c=λ/4, b=λ, σ=0, Λ=10-6.

Figure 17. 2c=λ/4, b=λ, σ=10-3, Λ=10-3.

Figure 17. 2c=λ/4, b=λ, σ=10-3, Λ=10-3.

Figure 18. 2c=λ/8, b=λ/2, σ=0, Λ=10-6.

Figure 18. 2c=λ/8, b=λ/2, σ=0, Λ=10-6.

Figure 19. 2c=λ/8, b=λ, σ=0, Λ=10-6.

Figure 19. 2c=λ/8, b=λ, σ=0, Λ=10-6.

Figure 20. n0=1.5,2c=λ/8, b=λ/2, σ=0, Λ=10-6.

Figure 20. n0=1.5,2c=λ/8, b=λ/2, σ=0, Λ=10-6.

Figure 21. n0=1.5,2c=λ/8, b=λ, σ=0, Λ=10-6.

Figure 21. n0=1.5,2c=λ/8, b=λ, σ=0, Λ=10-6.

Figure 22. θ[-π/2,-θcr][θcr,π/2],2c=λ/8, σ=0, Λ=10-6.

Figure 22. θ∈[-π/2,-θcr]∪[θcr,π/2],2c=λ/8, σ=0, Λ=10-6.

Figure 23. θ[-θcr,θcr], 2c=λ/8, σ=0, Λ=10-6.

Figure 23. θ∈[-θcr,θcr], 2c=λ/8, σ=0, Λ=10-6.

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