arXiv subjects
Publications and source records attributed to Noemi Wolanski.
We study the large-time behavior of nonnegative solutions to a nonlocal dispersal equation in $\mathbb R^N$ with an absorption term modeled by $-u^p$, with $1 0$.
We study the large-time behavior in all $L^p$ norms and in different space-time scales of solutions to a heat equation with a Caputo $α$-time derivative posed in $\mathbb{R}^N$. The initial data are assumed to be integrable, and, when required, to be also in $L^p$. A main difficulty in the analysis comes from the singularity in space at the origin of the fundamental solution of the equation when~$N>1$. The rate of decay in $L^p$ norm in the characteristic scale, $|x|\asymp t^{α/2}$, dictated by the scaling invariance of the equation, is $t^{-\frac{αN}{2}(1-\frac1p)}$. In compact sets it is $t^{-α/2}$ for $N=1$, $t^{-α}$ for $N\ge 3$, and $t^{-α}\log t$ in the critical dimension $N=2$. In intermediate scales, going to infinity but more slowly than $t^{α/2}$, we have an intermediate decay rate. In fast scales, going to infinity faster than $t^{α/2}$, there is no universal rate, valid for all solutions, as we will show by means of some examples. Anyway, in such scales solutions decay faster than in the characteristic one. When divided by the decay rate, solutions behave for large times in the characteristic scale like $M$ times the fundamental solution, where $M$ is the integral of the initial datum. The situation is very different in compact sets, where they converge to the Newtonian potential of the initial datum if $N\ge 3$, one of the main novelties of the paper, and to a constant if $N=1,2$. In intermediate scales they approach a multiple of the fundamental solution of the Laplacian if $N\ge 3$, and a constant in low dimensions. The asymptotic behavior in scales that go to infinity faster than the characteristic one depends strongly on the behavior of the initial datum at infinity. We give results for certain initial data with specific decays.
We study an inhomogeneous minimization problems associated to the $p(x)$-Laplacian. We make a thorough analysis of the essential properties of their minimizers and we establish a relationship with a suitable free boundary problem. On the one hand, we study the problem of minimizing the functional $J(v)=\int_Ω\Big(\frac{|\nabla v|^{p(x)}}{p(x)}+λ(x)χ_{\{v>0\}}+fv\Big)\,dx$. We show that nonnegative local minimizers $u$ are solutions to the free boundary problem: $u\ge 0$ and \begin{equation} \label{fbp-px}\tag{$P(f,p,λ^*)$} \begin{cases} Δ_{p(x)}u:=\mbox{div}(|\nabla u(x)|^{p(x)-2}\nabla u)= f & \mbox{in }\{u>0\}\\ u=0,\ |\nabla u| = λ^*(x) & \mbox{on }\partial\{u>0\} \end{cases} \end{equation} with $λ^*(x)=\Big(\frac{p(x)}{p(x)-1}\,λ(x)\Big)^{1/p(x)}$ and that the free boundary is a $C^{1,α}$ surface. On the other hand, we study the problem of minimizing the functional $J_{\varepsilon}(v)= \int_Ω\Big(\frac{|\nabla v|^{p_\varepsilon(x)}}{p_\varepsilon(x)}+B_{\varepsilon}(v)+f_\varepsilon v\Big)\, dx$, where $B_\varepsilon(s)=\int _0^sβ_\varepsilon(τ) \, dτ$, $\varepsilon>0$, $β_{\varepsilon}(s)={1 \over \varepsilon} β({s \over \varepsilon})$, with $β$ a Lipschitz function satisfying $β>0$ in $(0,1)$, $β\equiv 0$ outside $(0,1)$. We prove that if $u_\varepsilon$ are nonnegative local minimizers, then any limit function $u$ ($\varepsilon\to 0$) is a solution to the free boundary problem $P(f,p,λ^*)$ with $λ^*(x)=\Big(\frac{p(x)}{p(x)-1}\,M\Big)^{1/p(x)}$, $M=\int β(s)\, ds$, $p=\lim p_\varepsilon$, $f=\lim f_\varepsilon$, and that the free boundary is a $C^{1,α}$ surface. In order to obtain our results we need to overcome deep technical difficulties and develop new strategies, not present in the previous literature for this type of problems.
In this paper we study a one phase free boundary problem for the p(x)-Laplacian with non-zero right hand side. We prove that the free boundary of a weak solution is a C^1 surface in a neighborhood of every free boundary point. We also obtain further regularity results on the free boundary, under further regularity assumptions on the data. We apply these results to limit functions of an inhomogeneous singular perturbation problem for the p(x)-Laplacian that we studied in Lederman, C., & Wolanski, N. An inhomogeneous singular perturbation problem for the p(x)-Laplacian, Non- linear Anal. 138 (2016), 300-325.
In this paper we study a nonlocal diffusion problem on a manifold. These kind of equations can model diffusions when there are long range effects and have been widely studied in Euclidean space. We first prove existence and uniqueness of solutions and a comparison principle. Then, for a convenient rescaling we prove that the operator under consideration converges to a multiple of the usual Heat-Beltrami operator on the manifold. Next, we look at the long time behavior on compact manifolds by studying the spectral properties of the operator. Finally, for the model case of hyperbolic space we study the long time asymptotics and find a different and interesting behavior.
In this paper we study the following singular perturbation problem for the $p_\varepsilon(x)$-Laplacian: \[ Δ_{p_\varepsilon(x)}u^\varepsilon:=\mbox{div}(|\nabla u^\varepsilon(x)|^{p_\varepsilon(x)-2}\nabla u^\varepsilon)=β_{\varepsilon}(u^\varepsilon)+f_\varepsilon, \quad u^\varepsilon\geq 0, \] where $\varepsilon>0$, $β_{\varepsilon}(s)={1 \over \varepsilon} β({s \over \varepsilon})$, with $β$ a Lipschitz function satisfying $β>0$ in $(0,1)$, $β\equiv 0$ outside $(0,1)$ and $\int β(s)\, ds=M$. The functions $u^\varepsilon$, $f_\varepsilon$ and $p_\varepsilon$ are uniformly bounded. We prove uniform Lipschitz regularity, we pass to the limit $(\varepsilon\to 0)$ and we show that, under suitable assumptions, limit functions are weak solutions to the free boundary problem: $u\ge0$ and \[ \begin{cases} Δ_{p(x)}u= f & \mbox{in }\{u>0\}\\ u=0,\ |\nabla u| = λ^*(x) & \mbox{on }\partial\{u>0\} \end{cases} \] with $λ^*(x)=\Big(\frac{p(x)}{p(x)-1}\,M\Big)^{1/p(x)}$, $p=\lim p_\varepsilon$ and $f=\lim f_\varepsilon$. In \cite{LW4} we prove that the free boundary of a weak solution is a $C^{1,α}$ surface near flat free boundary points. This result applies, in particular, to the limit functions studied in this paper.
We study the long time behavior of bounded, integrable solutions to a nonlocal diffusion equation, $\partial _t u=J*u-u$, where $J$ is a smooth, radially symmetric kernel with support $B_d(0)\subset\mathbb{R}^2$. The problem is set in an exterior two-dimensional domain which excludes a hole $\mathcal{H}$, and with zero Dirichlet data on $\mathcal{H}$. In the far field scale, $ξ_1\le |x|t^{-1/2}\le ξ_2$ with $ξ_1,ξ_2>0$, the scaled function $\log t\, u(x,t)$ behaves as a multiple of the fundamental solution for the local heat equation with a certain diffusivity determined by $J$. The proportionality constant, which characterizes the first non-trivial term in the asymptotic behavior of the mass, is given by means of the asymptotic \lq logarithmic momentum' of the solution, $\lim_{t\to\infty}\int_{\mathbb{R}^2}u(x,t)\log|x|\,dx$. This asymptotic quantity can be easily computed in terms of the initial data. In the near field scale, $|x|\le t^{1/2}h(t)$ with $\lim_{t\to\infty} h(t)=0$, the scaled function $t(\log t)^2u(x,t)/\log |x|$ converges to a multiple of $ϕ(x)/\log |x|$, where $ϕ$ is the unique stationary solution of the problem that behaves as $\log|x|$ when $|x|\to\infty$. The proportionality constant is obtained through a matching procedure with the far field limit. Finally, in the very far field, $|x|\ge t^{1/2} g(t)$ with $g(t)\to\infty$, the solution is proved to be of order $o((t\log t)^{-1})$.
We study the long time behavior of solutions to the nonlocal diffusion equation $\partial_t u=J*u-u$ in an exterior one-dimensional domain, with zero Dirichlet data on the complement. In the far field scale, $ξ_1\le|x|t^{-1/2}\leξ_2$, $ξ_1,ξ_2>0$, this behavior is given by a multiple of the dipole solution for the local heat equation with a diffusivity determined by $J$. However, the proportionality constant is not the same on $\mathbb{R}_+$ and $\mathbb{R}_-$: it is given by the asymptotic first momentum of the solution on the corresponding half line, which can be computed in terms of the initial data. In the near field scale, $|x|\le t^{1/2}h(t)$, $\lim_{t\to\infty}h(t)=0$, the solution scaled by a factor $t^{3/2}/(|x|+1)$ converges to a stationary solution of the problem that behaves as $b^\pm{x}$ as $x\to\pm\infty$. The constants $b^\pm$ are obtained through a matching procedure with the far field limit. In the very far field, $|x|{\ge}t^{1/2} g(t)$, $g(t)\to\infty$, the solution has order $o(t^{-1})$.
We study the large time behavior of solutions to a non-local diffusion equation, $u_t=J*u-u$ with $J$ smooth, radially symmetric and compactly supported, posed in $\mathbb{R}_+$ with zero Dirichlet boundary conditions. In sets of the form $x\ge ξt^{1/2}$, $ξ>0$, the outer region, the asymptotic behavior is given by a multiple of the dipole solution for the local heat equation, and the solution is $O(t^{-1})$. The proportionality constant is determined from a conservation law, related to the asymptotic first momentum. On compact sets, the inner region, after scaling the solution by a factor $t^{3/2}$, it converges to a multiple of the unique stationary solution of the problem that behaves as $x$ at infinity. The precise proportionality factor is obtained through a matching procedure with the outer behavior. Since the outer and the inner region do not overlap, the matching is quite involved. It has to be done for the scaled function $t^{3/2}u(x,t)/x$, which takes into account that different scales lead to different decay rates.
In this paper we study the asymptotic behavior as time goes to infinity of the solution to a nonlocal diffusion equation with absorption modeled by a powerlike reaction $-u^p$, $p>1$ and set in $\R^N$. We consider a bounded, nonnegative initial datum $u_0$ that behaves like a negative power at infinity. That is, $|x|^αu_0(x)\to A>0$ as $|x|\to\infty$ with $0<α\le N$. We prove that, in the supercritical case $p>1+2/α$, the solution behaves asymptotically as that of the heat equation --with diffusivity $\a$ related to the nonlocal operator-- with the same initial datum.
We study the large time behavior of nonnegative solutions of the Cauchy problem $u_t=\int J(x-y)(u(y,t)-u(x,t))\,dy-u^p$, $u(x,0)=u_0(x)\in L^\infty$, where $|x|^αu_0(x)\to A>0$ as $|x|\to\infty$. One of our main goals is the study of the critical case $p=1+2/α$ for $0<α<N$, left open in previous articles, for which we prove that $t^{α/2}|u(x,t)-U(x,t)|\to 0$ where $U$ is the solution of the heat equation with absorption with initial datum $U(x,0)=C_{A,N}|x|^{-α}$. Our proof, involving sequences of rescalings of the solution, allows us to establish also the large time behavior of solutions having more general nonintegrable initial data $u_0$ in the supercritical case and also in the critical case ($p=1+2/N$) for bounded and integrable $u_0$.
We consider the optimization problem of minimizing $\int_Ω|\nabla u|^{p(x)}+ λχ_{\{u>0\}} dx$ in the class of functions $W^{1,p(\cdot)}(Ω)$ with $u-ϕ_0\in W_0^{1,p(\cdot)}(Ω)$, for a given $ϕ_0\geq 0$ and bounded. $W^{1,p(\cdot)}(Ω)$ is the class of weakly differentiable functions with $\int_Ω|\nabla u|^{p(x)} dx<\infty$. We prove that every solution $u$ is locally Lipschitz continuous, that it is a solution to a free boundary problem and that the free boundary, $Ω\cap\partial\{u>0\}$, is a regular surface.
In this paper we study the following problem. For any $\ep>0$, take $u^{\ep}$ a solution of, $$ Łu^{\ep}:= {div}\Big(\di\frac {g(|\nabla \uep|)}{|\nabla \uep|}\nabla \uep\Big)=β_{\ep}(u^{\ep}),\quad u^{\ep}\geq 0. $$ A solution to $(P_{\ep})$ is a function $u^{\ep}\in W^{1,G}(Ω)\cap L^{\infty}(Ω)$ such that $$ \int_Ω g(|\nabla u^{\ep}|) \frac{\nabla u^{\ep}}{|\nabla u^{\ep}|} \nabla ϕdx =-\int_Ω ϕβ_{\ep}(u^{\ep}) dx $$ for every $ϕ\in C_0^{\infty}(Ω)$. Here $β_{\ep}(s)= \frac{1}{\ep} β(\frac{s}{\ep}), $ with $β\in {Lip}(\R)$, $β>0$ in $(0,1)$ and $β=0$ otherwise. We are interested in the limiting problem, when $\ep\to 0$. As in previous work with $Ł=Δ$ or $Ł=Δ_p$ we prove, under appropriate assumptions, that any limiting function is a weak solution to a free boundary problem. Moreover, for nondegenerate limits we prove that the reduced free boundary is a $C^{1,α}$ surface. This result is new even for $Δ_p$. Throughout the paper we assume that $g$ satisfies the conditions introduced by G. Lieberman in \cite{Li1}
We consider the optimization problem of minimizing $\int_ΩG(|\nabla u|)+λχ_{\{u>0\}} dx$ in the class of functions $W^{1,G}(Ω)$ with $u-ϕ_0\in W_0^{1,G}(Ω)$, for a given $ϕ_0\geq 0$ and bounded. $W^{1,G}(Ω)$ is the class of weakly differentiable functions with $\int_ΩG(|\nabla u|) dx<\infty$. The conditions on the function G allow for a different behavior at 0 and at $\infty$. We prove that every solution u is locally Lipschitz continuous, that they are solution to a free boundary problem and that the free boundary, $\partial\{u>0\}\cap Ω$, is a regular surface. Also, we introduce the notion of weak solution to the free boundary problem solved by the minimizers and prove the Lipschitz regularity of the weak solutions and the $C^{1,α}$ regularity of their free boundaries near ``flat'' free boundary points.
We consider the optimization problem of minimizing $\int_Ω|\nabla u|^p dx$ with a constrain on the volume of $\{u>0\}$. We consider a penalization problem, and we prove that for small values of the penalization parameter, the constrained volume is attained. In this way we prove that every solution $u$ is locally Lipschitz continuous and that the free boundary, $\partial\{u>0\}\cap Ω$, is smooth.