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Original Articles

On the Laplacian operation with applications in magnetic resonance electrical impedance imaging

&
Pages 251-268 | Received 27 Aug 2011, Accepted 19 Apr 2012, Published online: 20 Jun 2012

Figures & data

Figure 1. The approximation to α* by above iterative algorithm.

Figure 1. The approximation to α* by above iterative algorithm.

Figure 2. The relative errors RE of the regularizing solution uα,δ for different noise level δ when α = αH, αG and αM, respectively (left), the RE for α = αG and different δ when q = 1, 0.6, 0.2 and 0, respectively (right).

Figure 2. The relative errors RE of the regularizing solution uα,δ for different noise level δ when α = αH, αG and αM, respectively (left), the RE for α = αG and different δ when q = 1, 0.6, 0.2 and 0, respectively (right).

Figure 3. Exact solution u = Δf and the regularizing solutions uα,δ for δ = 0.005, 0.01 and 0.05 when α = αH.

Figure 3. Exact solution u = Δf and the regularizing solutions uα,δ for δ = 0.005, 0.01 and 0.05 when α = αH.

Table 1. The values of α*, αH and the iteration number it for solving the generalized discrepancy principle.

Table 2. The values of αH, αM, αG and the relative errors RE of the corresponding regularizing solution uα,δ.

Figure 4. The functions f and u = Δf.

Figure 4. The functions f and u = Δf.

Figure 5. The regularizing solutions uα,δ for different noise level δ.

Figure 5. The regularizing solutions uα,δ for different noise level δ.

Figure 6. The picture with grey level f.

Figure 6. The picture with grey level f.

Figure 7. The exact magnetic flux and .

Figure 7. The exact magnetic flux and .

Figure 8. The reconstructive results of σn when noise level δ = 3%.

Figure 8. The reconstructive results of σn when noise level δ = 3%.

Table 3. The relative error E(n) of the iterative sequence σn for different noise level δ and iteration number n.

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