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Sirgue, Laurent, 2003. Inversion de la forme d'onde dans le ...

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2.2. INVERSION OF LINEAR PROBLEMS 19<br />

Equation (2.18) shows that the SVD allows the reduction of the forward operator G to its<br />

efficient state of information. The forward prob<strong>le</strong>m may use the portion of the mo<strong>de</strong>l space<br />

constrained to V p to mo<strong>de</strong>l the data contained in U p only. The other portion of the data U o<br />

cannot be mo<strong>de</strong><strong>le</strong>d.<br />

Solution estimate of the inverse prob<strong>le</strong>m<br />

We have seen that the SVD allows the diagnosis of the forward prob<strong>le</strong>m by i<strong>de</strong>ntifying the<br />

portion of the data and mo<strong>de</strong>l spaces U p , V p . The SVD technique may also be used to estimate<br />

a solution of the inverse prob<strong>le</strong>m. By reformu<strong>la</strong>ting the state of information with the perspective<br />

of inversion, the sub-space<br />

• V p is constrained by U p only<br />

• V 0 is un<strong>de</strong>termined<br />

• U 0 is use<strong>le</strong>ss<br />

Since V p can only be <strong>de</strong>termined using the information contained in U p only, we <strong>de</strong>fine the<br />

generalised inverse G † as<br />

G † = V p Λ −1<br />

p Ut p . (2.19)<br />

The generalised inverse G † is an estimate of the inverse matrix G −1 (which may not exist, see<br />

tab<strong>le</strong> 2.1). The estimate of the inverse prob<strong>le</strong>m solution m † is then <strong>de</strong>fined as<br />

m † = G † d. (2.20)<br />

In or<strong>de</strong>r to evaluate how well the mo<strong>de</strong>l is resolved, equation (2.4) may be inclu<strong>de</strong>d into equation<br />

(2.20) yielding<br />

m † = G † Gm<br />

= R m m (2.21)<br />

where R m = G † G is the mo<strong>de</strong>l resolution matrix. We can also measure how well the estimated<br />

solution exp<strong>la</strong>ined the data by <strong>de</strong>fining d † , the data predicted by the generalised inverse solution<br />

d † = Gm †<br />

= GG † d<br />

= R d d (2.22)

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