Segmentation of Stochastic Images using ... - Jacobs University
Segmentation of Stochastic Images using ... - Jacobs University
Segmentation of Stochastic Images using ... - Jacobs University
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
2.3 Mumford-Shah and Ambrosio-Tortorelli <strong>Segmentation</strong><br />
Theorem 2.1. Define Ẽ AT : L 1 (D) × L 1 (D) → IR + by<br />
{<br />
EAT (u,φ) if (u,φ) ∈ H<br />
Ẽ AT (u,φ) :=<br />
1 (D) × H 1 (D),0 ≤ φ ≤ 1<br />
+∞ otherwise<br />
(2.21)<br />
and G : L 1 (D) × L 1 (D) → IR + by<br />
{<br />
EMS (u) if u ∈ GSBV(D) and φ = 1 almost everywhere<br />
G(u,φ) =<br />
+∞ otherwise.<br />
(2.22)<br />
If k ε = o(ε), then Ẽ AT Γ-converges to G(u,φ) for ε → 0.<br />
The convergence <strong>of</strong> the Ambrosio-Tortorelli energy towards the Mumford-Shah energy enables us<br />
to use the coupled pair <strong>of</strong> PDEs obtained as Euler-Lagrange equations <strong>of</strong> the Ambrosio-Tortorelli<br />
energy and to solve this with very small ε. The result is a phase field that is close to the characteristic<br />
function <strong>of</strong> the edge set <strong>of</strong> the Mumford-Shah functional.<br />
2.3.3 Edge Continuity and Edge Consistency<br />
The classical Mumford-Shah model and the Ambrosio-Tortorelli approximation lack a step linking<br />
edges. This step is necessary to enforce the detection <strong>of</strong> closed contours in the images. Otherwise,<br />
the appearance <strong>of</strong> partially detected, breaking up contours is possible, see Fig. 2.5. For example,<br />
Erdem et al. [49] introduced such a step for the Ambrosio-Tortorelli model. The idea is to use a<br />
modified diffusion coefficient in the image equation. This modified coefficient does not depend on<br />
the phase field exclusively, but contains information about the continuity and directional consistency<br />
<strong>of</strong> the detected edges. To be more precise, Erdem et al. [49] proposed to use the equation<br />
−∇ · (µ((cφ) 2 + k ε )∇u ) + u = u 0 , (2.23)<br />
instead <strong>of</strong> the first equation <strong>of</strong> (2.18). The additional factor c is the product <strong>of</strong> the two factors from<br />
the directional consistency c dc and the edge continuity c h , i.e.<br />
c = c dc · c h . (2.24)<br />
If c < 1, the diffusivity decreases, allowing to form new edges in the image, whereas c > 1 leads to<br />
an increased diffusivity, allowing to smooth away unwanted edges.<br />
Directional Consistency<br />
The directional consistency tries to judge the quality <strong>of</strong> the detected edges based on information<br />
from surrounding pixels. The idea is that an edge is reliable if the gradients <strong>of</strong> the image for pixels<br />
in directions perpendicular to the edge are in parallel. For inaccurately detected edges, e.g. due to<br />
noise, these gradients are typically not aligned. To do so, Erdem et al. [49] introduced<br />
(c dc ) i = ζ dc<br />
i<br />
+ 1 − ζ i<br />
dc<br />
(2.25)<br />
φ i<br />
for all pixels i ∈ I , where ζi<br />
dc measures the alignment <strong>of</strong> the gradients. This factor increases the<br />
diffusion, if the image gradients around the detected edge are not aligned. As the feedback measure<br />
for the alignment <strong>of</strong> the gradients they proposed to use<br />
( ( ))<br />
1<br />
ζi<br />
dc = exp ε dc |η s | ∑ ∇v<br />
j∈η s i · ∇v j − 1 , (2.26)<br />
15