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2025-11-04 12:43:23 -06:00
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content/CSE5519/CSE5519_E1.md
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@@ -469,7 +469,7 @@ $$
Then we use $\mathcal{L}_{ds}$ to enforce the smoothness of the disparity map.
$$
\mathcal{L}_{ds}=\sum_{p\in I^l}\left|\partial_x d^l_p\right|e^{-\left|\partial_x d^l_p\right|}+\left|\partial_y d^l_p\right|e^{-\left|\partial_y d^l_p\right|}=\sum_{p_t}|\nabla D(p_t)|\cdot \left(e^{-|\nabla I(p_t)|}\right)^T\tag{2}
\mathcal{L}_{ds}=\sum_{p\in I^l}\left|\partial_x d^l_p\right|e^{-\left|\partial_x d^l_p\right|}+\left|\partial_y d^l_p\right|e^{-\left|\partial_y d^l_p\right|}=\sum_{p_t}|\nabla D(p_t)|\cdot \left(e^{-|\nabla I(p_t)|}\right)^\top\tag{2}
$$
Replacing $\hat{I}^{rig}_s$ with $\hat{I}^{full}_s$, in (1) and (2), we get the $\mathcal{L}_{fw}$ and $\mathcal{L}_{fs}$ for the non-rigid motion localizer.