We carry on an asymptotic analysis for a class of non-convex integral functionals with a singular perturbation by derivatives of order k≥ 2. In the case $k=2$ these functional have been already proved to converge to a free-discontinuity functional whose jump part energy density is a constant m₂ times the square root of the jump size by Alicandro et al.~and by Bouchitt\'e et al. We show that the k-th order perturbation gives a constant, mₖ, times the k-th root of the jump size as the jump part energy density. The constant mₖ is characterized by an optimal-profile problem with zero derivatives up to order $k-1$ at the boundary. Contrary to the case $k=2$, the set of points where these boundary conditions hold are not naturally selected from the energy, and the main technical part of the paper is the analysis of the properties of such sets, carried on by a combined use of interpolation inequalities and energy estimates. The result is proven for truncated quadratic energy densities and in the one-dimensional case, from which the general higher-dimensional case can be obtained by slicing techniques and a wide class of non-convex energies can be studied as an envelope of the particular ones. Finally, we remark that an approximation of the Mumford-Shah functional can be obtained by letting k→+∞.
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Margherita Solci (2024) studied this question.
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