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Juan Carlos Chata Ortiz

Publications and source records attributed to Juan Carlos Chata Ortiz.

2 recordsLinked to original sources

Gradient constraints, Born-Infeld, and maximal surfaces via superposition of infinitely many $p$-Laplacians

We study the Dirichlet problem for an infinite series of $p$-Laplacians, $$-\sum_{p=2}^{\infty}a_{p}Δ_{p}u=f \ \text{ in } Ω, \qquad u=g \ \text{ on } \partialΩ,$$ where $\{a_{p}\}$ is a sequence of nonnegative numbers whose power series has radius of convergence $σ\in(0,\infty]$. The operator is formally $-\operatorname{div}( {A}(|\nabla u|)\nabla u)$ with $ {A}$ singular at $|\nabla u|=σ$; model cases are the mean curvature operator in Minkowski space and the Born-Infeld operator of nonlinear electrostatics. The radius of convergence forces the gradient constraint $\|\nabla u\|_\infty\leσ$, so the natural variational problem is constrained. A unique minimizer of the associated energy always exists (for boundary data compatible with the constraint) and always solves a variational inequality, and we identify the saturation flux $Λ:=\sum_{p\ge2}a_pσ^{p-1}$ as the quantity governing solvability of the equation: if $Λ<\infty$ a weak solution exists only if $|\int_E f|\leΛP(E)$ for every set of finite perimeter $E\SubsetΩ$, so for $f\equivλ$ no solution exists once $λ>Λh(Ω)$, $h(Ω)$ the Cheeger constant of $Ω$. The threshold is sharp on balls, where the minimizer has a saturation region $\{|\nabla u|=σ\}$ of positive measure. When $Λ=\infty$, as for Born-Infeld type operators, no such obstruction is present, and the minimizer solves the equation whenever a Lipschitz bound below $σ$ is available; for $f\equiv0$ we obtain such a bound, uniform in the truncations of the series, under a bounded slope condition on the boundary datum. As applications we obtain an isoperimetric bound on the charge densities supported by a nonlinear electrostatics with saturating displacement, and a quantitative convergence rate for the weak field expansion of the Born-Infeld model.

math.AP↗

Sharp existence and non-existence for singular $1$-Laplace equations with Hardy potentials

In this paper, we investigate the singular Dirichlet problem \begin{equation}\label{abs1} \left\{ \begin{array}{rclr} -Δ_1u &=&\dfracλ{|x|}\hbox{Sgn}\,(u)+\dfrac{f}{u^γ}&\quad\mbox{in}\; Ω,\\[1ex] u &=&0& \quad\mbox{on}\; \partialΩ, \end{array} \right. \end{equation} where $Δ_1u=\hbox{div}\left(\frac{Du}{|Du|}\right)$ denotes the $1$-Laplacian operator, the parameters are $λ\in {R}$ and $γ>0$, and $f$ is a non-negative function belonging to the Lorentz space $L^{N,\infty}(Ω)$. Our main goal is to establish the existence of non-trivial solutions under the sharp restriction $λ 0$. We also show that these solutions are globally bounded and that, on the contrary, no solution exists as soon as $λ\geq N-1$ and $f$ is positive. These results are achieved by rigorously analyzing the asymptotic behavior, as $p\to 1^+$, of the solutions to the approximating $p$-Laplace problems \begin{equation} \left\{ \begin{array}{rclc} -Δ_pu&=&\dfracλ{|x|^p}|u|^{p-2}u+\dfrac{f}{u^γ}&\quad\mbox{ in }\; Ω,\\[1ex] u&=&0&\quad\mbox{ on }\; \partialΩ. \end{array} \right. \end{equation} Finally, we provide a family of explicit examples designed to illustrate the sharp optimality of our main assumptions.

math.AP↗