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Articles

Quasi-optimal Tikhonov penalization and parameterization coarseness in space-dependent function estimation

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Pages 465-481 | Received 04 Jul 2014, Accepted 28 Apr 2015, Published online: 01 Jun 2015

Figures & data

Figure 1. Distance from the solution to the target E(ϑ) as a function of the Tikhonov parameter ϑ, for three control space dimensions Ξ equal to 7, 15 and 20. It is seen that ϑ=argminE(ϑ) is independent of Ξ. The quasi-optimal Tikhonov parameter found according to the discrepancy principle has also been added.

Figure 1. Distance from the solution to the target E(ϑ) as a function of the Tikhonov parameter ϑ, for three control space dimensions Ξ equal to 7, 15 and 20. It is seen that ϑ∗=argminE(ϑ) is independent of Ξ. The quasi-optimal Tikhonov parameter found according to the discrepancy principle has also been added.

Table 1. Value of the Tikhonov parameter ϑdp solution of (Equation6) for different discretizations and different noise magnitudes.

Figure 2. Reconstructions φϑ(x2) for Ξ=15 (top), Ξ=10 (middle) and Ξ=7 (bottom) for under-regularization (ϑ=10-15), over-regularization (ϑ=1) and appropriate regularization (ϑ=510-10ϑ). Note that points for Ξ=15 and Ξ=10 (over-parameterization) with ϑ=10-15 (under-regularization) are not presented because of divergence. The noise variance ϵl2=0.001 was used after generating the synthetic data.

Figure 2. Reconstructions φϑ(x2) for Ξ=15 (top), Ξ=10 (middle) and Ξ=7 (bottom) for under-regularization (ϑ=10-15), over-regularization (ϑ=1) and appropriate regularization (ϑ=510-10≈ϑ∗). Note that points for Ξ=15 and Ξ=10 (over-parameterization) with ϑ=10-15 (under-regularization) are not presented because of divergence. The noise variance ϵl2=0.001 was used after generating the synthetic data.

Figure 3. Test medium geometry representation. Eight sources are located on the boundary. For each source (which constitutes a test), the emerging radiation is measured on all sensors.

Figure 3. Test medium geometry representation. Eight sources are located on the boundary. For each source (which constitutes a test), the emerging radiation is measured on all sensors.

Table 2. Dimensions of finite element spaces for φ, φ˘ and α.

Table 3. CPU time comparisons for the generation of the error curves E(ϑ).

Figure 4. Distance from the solution to the target E(ϑ) as a function of the Tikhonov parameter ϑ, for κap,σap=0.08,20cm-1 and three control space dimensions Ξα equal to 384, 1382 and 2924. It is seen that ϑ=argminE(ϑ) is quasi-independent of Ξ.

Figure 4. Distance from the solution to the target E(ϑ) as a function of the Tikhonov parameter ϑ, for κap,σap=0.08,20cm-1 and three control space dimensions Ξα equal to 384, 1382 and 2924. It is seen that ϑ∗=argminE(ϑ) is quasi-independent of Ξ.

Figure 5. Reconstruction of κ (left) and σ (right) with ϑ=0.2, κap,σap=0.08,20cm-1 and Ξα=2924. It should be noted the divergence for the reduced diffusion coefficient.

Figure 5. Reconstruction of κ (left) and σ (right) with ϑ=0.2, κap,σap=0.08,20cm-1 and Ξα=2924. It should be noted the divergence for the reduced diffusion coefficient.

Figure 6. Reconstruction of κ (left) and σ (right) with ϑ=0.4, κap,σap=0.08,20cm-1 and Ξα=2924.

Figure 6. Reconstruction of κ (left) and σ (right) with ϑ=0.4, κap,σap=0.08,20cm-1 and Ξα=2924.

Figure 7. Reconstruction of κ (left) and σ (right) with ϑ=1.4, κap,σap=0.088,24cm-1 and Ξα=2924.

Figure 7. Reconstruction of κ (left) and σ (right) with ϑ=1.4, κap,σap=0.088,24cm-1 and Ξα=2924.

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