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Image Reconstruction for 3D Lung Imaging - Department of Systems ...

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Iteration 1<br />

(a)<br />

Iteration 4<br />

(d)<br />

Iteration 7<br />

(g)<br />

Iteration 2<br />

(b)<br />

Iteration 5<br />

(e)<br />

Iteration 8<br />

(h)<br />

TV<br />

L2<br />

phantom<br />

Iteration 3<br />

(c)<br />

Iteration 6<br />

(f)<br />

Iteration 9<br />

Figure 7.6: Pr<strong>of</strong>ile plots <strong>of</strong> the originating contrast, TV, and ℓ 2 reconstructions. No Noise<br />

added. Pr<strong>of</strong>iles are vertical slices through the middle <strong>of</strong> the reconstructed image.<br />

7.4.5 Parameters<br />

The PD-IPM method has two tuneable parameters β and λ. The value <strong>of</strong> β has a large<br />

effect on convergence. Too large a value <strong>of</strong> β (greater than 10 −6 ) prevented convergence<br />

to the desired “blocky” solution; the solution stabilized but showed smoothed features that<br />

were not consistent with the edges obtained with smaller values <strong>of</strong> β. Ultimately it was<br />

determined that the quickest convergence occurred when β was initialized to a small value<br />

(we used 10 −12 ) and left unchanged. This was the method used in the results shown in this<br />

paper.<br />

With an iterative algorithm multiple values <strong>of</strong> the regularization hyperparameter, λ,<br />

could be used <strong>for</strong> each iteration. In this work, <strong>for</strong> the TV algorithm, a different value was<br />

used <strong>for</strong> λ0, in the initialization step (7.40) and <strong>for</strong> λi in the iterative steps (7.38). λ0<br />

was selected using the BestRes method described in [52]. BestRes is an algorithm <strong>for</strong> objectively<br />

calculating the hyperparameter <strong>for</strong> linearized one-step EIT image reconstruction<br />

algorithms. This method suggests selecting a hyperparameter that results in a reconstruction<br />

that has maximum resolution <strong>for</strong> an impulse contrast. Although TV is not intended<br />

<strong>for</strong> use in imaging impulse type contrasts the first step <strong>of</strong> the algorithm requires solution<br />

<strong>of</strong> the quadratic problem. In previous work the BestRes algorithm has provided λ values<br />

based on an impulse contrast that has generalized well to non-impulse contrasts. See, <strong>for</strong><br />

108<br />

(i)

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