Th`ese Marouan BOUALI - Sites personnels de TELECOM ParisTech
Th`ese Marouan BOUALI - Sites personnels de TELECOM ParisTech
Th`ese Marouan BOUALI - Sites personnels de TELECOM ParisTech
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98 4. A Variational approach for the <strong>de</strong>striping issue<br />
Figure 4.10 – (Left) Noisy image from Terra MODIS band 30 (Center) Destriped<br />
with histogram matching (IMAPP) showing residual stripes (Right) Destriped with the<br />
UVDM illustrating complete removal of striping without any bluring or ringing artifacts<br />
Figure 4.11 – (Left) Noisy image from Terra MODIS band 33 (Center) Destriped<br />
with histogram matching (IMAPP) showing residual stripes in spite of noisy <strong>de</strong>tectors<br />
being replaced with neighbors (Right) Image <strong>de</strong>striped with the UVDM showing efficient<br />
removal of radom striping without bluring or ringing artifacts<br />
these requirements dictates minimum distortion in the <strong>de</strong>striped image. The ID in<strong>de</strong>x in<br />
clearly <strong>de</strong>pen<strong>de</strong>nt on the choice of the lagrange multiplier λ. The coefficient λ regulates<br />
the smoothness of the solution and its impact on the restored image can be interpreted as<br />
follows : A large value of λ may result in an oversmoothed solution, visually similar to what<br />
could be achieved with a low-pass filter, or a hard thresholding of wavelet coefficients in<br />
the lower scales. On the other hand, if λ is too small, the result might still contain noise. In<br />
fact, if we consi<strong>de</strong>rer the ROF mo<strong>de</strong>l, its minimizer converges to the original noisy image<br />
f when λ → 0. In the case of the UVDM, when λ → 0, the solution converges to that of<br />
the following optimization problem :<br />
√<br />
∫ (∂(u ) − Is ) 2<br />
E ɛ (u) =<br />
+ ɛ<br />
∂x<br />
2 (4.95)<br />
Ω