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The jump set under geometric regularisation. Part 2: Higher-order approaches

Published 9 Jul 2014 in math.FA and cs.CV | (1407.2334v1)

Abstract: In Part 1, we developed a new technique based on Lipschitz pushforwards for proving the jump set containment property H<sup>m−1(Ju</sup>∖Jf)=0\mathcal{H}<sup>{m-1}(J_u</sup> \setminus J_f)=0 of solutions uu to total variation denoising. We demonstrated that the technique also applies to Huber-regularised TV. Now, in this Part 2, we extend the technique to higher-order regularisers. We are not quite able to prove the property for total generalised variation (TGV) based on the symmetrised gradient for the second-order term. We show that the property holds under three conditions: First, the solution uu is locally bounded. Second, the second-order variable is of locally bounded variation, $w \in \mbox{BV}_\mbox{loc}(\Omega; \mathbb{R}<sup>m)$, instead of just bounded deformation, $w \in \mbox{BD}(\Omega)$. Third, ww does not jump on JuJ_u parallel to it. The second condition can be achieved for non-symmetric TGV. Both the second and third condition can be achieved if we change the Radon (or L<sup>1L<sup>1) norm of the symmetrised gradient EwEw into an L<sup>pL<sup>p norm, $p&gt;1$, in which case Korn's inequality holds. We also consider the application of the technique to infimal convolution TV, and study the limiting behaviour of the singular part of DuD u, as the second parameter of $\mbox{TGV}<sup>2$ goes to zero. Unsurprisingly, it vanishes, but in numerical discretisations the situation looks quite different. Finally, our work additionally includes a result on TGV-strict approximation in $\mbox{BV}(\Omega)$.

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