18.01.2013 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

3.7 Summary<br />

3.7.1 <strong>Reconstruction</strong> Summary<br />

Here we summarize the state <strong>of</strong> the art in EIT difference imaging <strong>for</strong> clinical applications<br />

such as pulmonary imaging. The framework is the non-linear optimization problem, equation<br />

3.7, which is reproduced below:<br />

ˆx = arg min<br />

x<br />

�<br />

�Hx − z� 2 + λ 2 �Rx� 2�<br />

(3.24)<br />

This is solved using the MAP regularized framework <strong>of</strong> equation 3.22 again repeated below:<br />

ˆx = (H T WH + λ 2 R T R) −1 H T Wz = B(λ)z (3.25)<br />

where z = v2 − v1. The framework has several explicit parameters that must be selected<br />

by the user:<br />

1. The regularization hyperparameter, λ, is the subject <strong>of</strong> chapter 4.<br />

2. The norm <strong>of</strong> the prior, �Rx� 2 , has historically been the ℓ 2 norm. The ℓ 1 norm has<br />

been used <strong>for</strong> “blocky” reconstructions. An algorithm <strong>for</strong> solving the ℓ 1 norm is<br />

evaluated in chapter 7.<br />

3. The prior matrix, R, has many possibilities as discussed in this chapter.<br />

4. The data weighting matrix W has the ability to consider noise and erroneous electrode<br />

data. However with equal noise variance on each measurement channel and with good<br />

electrodes (no accounting <strong>for</strong> erroneous electrodes), W becomes a scaled version <strong>of</strong><br />

the identity matrix.<br />

In addition to these explicit parameters there are several implied parameters that con<strong>for</strong>m<br />

to some assumptions:<br />

1. The initial conductivity, σ0, is typically assumed to be homogenous.<br />

2. The conductivity used to calculate the Jacobian, σ ∗ , is typically assumed to be homogenous.<br />

3. FEM modeling issues including degree <strong>of</strong> the shape functions (linear, quadratic),<br />

isotropy <strong>of</strong> element conductivity, and mesh parameters such as number and degree<br />

(triangle, quadrilateral) <strong>of</strong> elements, geometry, shape <strong>of</strong> the reconstructed mesh dimension<br />

(2 or 3).<br />

4. Electrode types, locations and size.<br />

5. Current injection and measurement patterns.<br />

None <strong>of</strong> these parameters appear explicitly in equations 3.24 or 3.25 but are important<br />

parts <strong>of</strong> the problem. There is much work describing variations <strong>of</strong> the framework in terms<br />

<strong>of</strong> explicit and implied parameters, however, there is little quantitative in<strong>for</strong>mation on how<br />

they compare and how important any one <strong>of</strong> them is.<br />

45

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!