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We present two results characterizing minimizers of the Chan-Esedoglu L1TV functional $F(u) equiv int | abla u | dx + lambda int |u - f| dx $; $u,f:Bbb{R}^n to Bbb{R}$. If we restrict to $u = chi_{Sigma}$ and $f = chi_{Omega}$, $Sigma, Omega in Bbb{R}^n$, the $L^1$TV functional reduces to $E(Sigma) = Per(Sigma) + lambda |Sigmavartriangle Omega |$. We show that there is a minimizer $Sigma$ such that its boundary $partialSigma$ lies between the union of all balls of radius $frac{n}{lambda}$ contained in $Omega$ and the corresponding union of $frac{n}{lambda}$-balls in $Omega^c$. We also show that if a ball of radius $frac{n}{lambda} + epsilon$ is almost contained in $Omega$, a slightly smaller concentric ball can be added to $Sigma$ to get another minimizer. Finally, we comment on recent results Allard has obtained on $L^1$TV minimizers and how these relate to our results.
We show that generic Holder continuous functions are $rho$-irregular. The property of $rho$-irregularity has been first introduced by Catellier and Gubinelli (Stoc. Proc. Appl. 126, 2016) and plays a key role in the study of well-posedness for some c
We consider Cheeger-like shape optimization problems of the form $$minbig{|Omega|^alpha J(Omega) : Omegasubset Dbig}$$ where $D$ is a given bounded domain and $alpha$ is above the natural scaling. We show the existence of a solution and analyze as $J
We prove the $C^{1}$ regularity for a class of abnormal length-minimizers in rank $2$ sub-Riemannian structures. As a consequence of our result, all length-minimizers for rank $2$ sub-Riemannian structures of step up to $4$ are of class $C^{1}$.
We derive moment estimates and a strong limit theorem for space inverses of stochastic flows generated by jump SDEs with adapted coefficients in weighted Holder norms using the Sobolev embedding theorem and the change of variable formula. As an appli
We present and study novel optimal control problems motivated by the search for photovoltaic materials with high power-conversion efficiency. The material must perform the first step: convert light (photons) into electronic excitations. We formulate