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Th`ese Marouan BOUALI - Sites personnels de TELECOM ParisTech

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87<br />

The minimization of (4.60) is obtained with the Euler-Lagrange equation :<br />

( ) ∇u<br />

2λ △ −1 (f − u) =div<br />

|∇u|<br />

which takes a pratical form after application of the Laplacian operator :<br />

( ( )) ∇u<br />

2λ(f − u) =△ div<br />

|∇u|<br />

(4.61)<br />

(4.62)<br />

Equation (4.62) can be solved using a fixed step gradient <strong>de</strong>scent. The estimation of u at<br />

iteration n + 1 is given by :<br />

( ( ))) ∇u<br />

u n+1 = u n − ∆ t<br />

(2λ(f − u n n<br />

) −△ div<br />

|∇u n |<br />

(4.63)<br />

u 0 = f<br />

It is interesting to point out that Osher-Solé-Vese mo<strong>de</strong>l is very similar to the particular<br />

case of Vese-Osher mo<strong>de</strong>l where p = 2 and λ = ∞. In fact, the space G p (Ω) coinci<strong>de</strong>s<br />

with the Sobolev space W −1,p (Ω) which is the dual of W 1,p′<br />

0 (Ω) where p and p ′ satisfie the<br />

relationship 1 p + 1 p<br />

= 1. If p = 2, then the texture component v lies in G ′ 2 (Ω) = W −1,2 (Ω) =<br />

H −1 (Ω). The <strong>de</strong>composition mo<strong>de</strong>l of Vese and Osher can then be written as :<br />

inf |u| BV (Ω) + λ‖f − (u + v)‖ 2 L 2 (Ω) + µ ‖v‖ H −1 (Ω) (4.64)<br />

(u,v)∈BV (Ω)×H −1 (Ω)<br />

4.3.4 Other u + v mo<strong>de</strong>ls<br />

More image <strong>de</strong>composition mo<strong>de</strong>ls were introduced following [Vese and Osher, 2002]<br />

and [Osher et al., 2002]. In [Aujol et al., 2005], the following energy is consi<strong>de</strong>red :<br />

(<br />

)<br />

TV(u)+λ‖f − (u + v)‖ 2 L 2 (Ω)<br />

(4.65)<br />

inf<br />

(u,v)∈BV (Ω)×G µ(Ω)<br />

where the space G µ is <strong>de</strong>fined as :<br />

G µ = {v ∈ G(Ω)/‖v‖ G ≤ µ)} (4.66)<br />

The minimization of (4.66) is obtained with the projection algorithm of Chambolle.<br />

[Daubechies and Teschke, 2005] introduced an image <strong>de</strong>composition mo<strong>de</strong>l based on a<br />

wavelet framework as :<br />

inf<br />

(u,v)∈B 1 1 (L1 (Ω))×H −1 (Ω)<br />

(<br />

)<br />

2α|u| B 1<br />

1 (L 1 (Ω)) + ‖f − (u + v)‖2 L 2 (Ω) + ‖‖2 H −1 (Ω)<br />

(4.67)<br />

The space BV (Ω) used in most image <strong>de</strong>composition mo<strong>de</strong>ls is replaced by a space suited<br />

for wavelet coefficients, namely the Besov space B 1 1 (Ω).

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