Assistant Professor
Universidad de Talca
I'm from Chile. I have a B.Sc. in Engineering Mathematics and a Mathematical Engineering professional degree (which is kind of equivalent to a Ms.Sc. in Mathematics) from the Departamento de Ingeniería Matemática at the Universidad de Chile, where I worked under the supervision of Juan Dávila on a singular perturbation problem. The thesis (in spanish) and the article that I wrote about the subject can be found in my publication list. I completed my Ph.D. in Mathematics studies at the Mathematics Department from Rutgers University with Haim Brezis as my advisor. My thesis is the compilation of the research I did while at Rutgers about singular Sturm-Liouville equations. You can find the thesis and the respective papers in my publication list.
Currently I am an Assistant Professor at the Instituto de Matemáticas from the Universidad de Talca where I teach both undergraduate and graduate courses. My current research interests are degenerate/singular elliptic equations together with some aspects related to weighted Sobolev spaces, you can see more details by clicking the Research and Publications links from the side panel.
Universidad de Talca
Universidad de Talca
Universidad de Talca
Ph.D. in Mathematics
Rutgers University
Mathematical Engineering
Universidad de Chile
Bachelor of Sciences in Engineering Mathematics
Universidad de Chile
In the past years I have been studying singular (degenerate) second order elliptic operators such as the singular Sturm-Liouville operator Lαu(t):=−(t2αu′(t))′ where α>0, or the degenerate elliptic operator Lαu(x):=−div(xA∇u(x)) where A∈RN is a given vector and xA=|x1|a1⋅…|xN|aN. In such studies the construction of suitable weighted Sobolev spaces and the study of their properties were quite significant and opened a very interesting line of research. In particular, it was established the validity of the following Hardy-Sobolev inequalities (∫RN|xBu(x)|p∗dx)1p∗≤C(∫RN|xA∇u(x)|pdx)1p for suitable p≥1, A,B∈RN and p∗=NpN−p(1+b−a), where a=a1+…+aN and b=b1+…+bN. This work leads to several interesting open problems, some of which are the purpose of this research project.
One of the natural topics of interest that arise when one has proved such an inequality is the existence of extremals and the value of the best possible constant C>0. Namely, for a given open set Ω⊆RN, we would like to investigate the existence of a function uA,B,p=up and the value of the constant SA,B,p>0 such that SpA,B,p(Ω)=inf here D^1_{A,p}(\Omega) denotes the completion of C^\infty_0(\Omega) under the norm \Vert u\Vert^p=\int_{\Omega}\left|x^A\nabla u(x)\right|^p dx. The main difficulty in this problem arises when one notices that p^* is critical from the viewpoint of the embedding of the weighted Sobolev space into the weighted L^q space. More precisely, if \Omega is bounded and contains the origin then the space D^1_{A,p}(\Omega) is embedded into the respective weighted space L^q(\Omega, x^{Bp^*}) for 1\leq q\leq p^*, but the embedding is compact if and only if q<{p^*}. This lack of compactness prevents us from using the classical minimization strategy to obtain extremals for S_{A,B,p}(\Omega), thus making this a problem worth addressing.
The other problem we plan to attack in this research project concerns the the asymptotic behavior of minimizer sequences for the problem S^p_{A,p}=\inf\left\{\int_{\Omega}\left|\nabla u(x)\right|^2x^A dx:u\in D^1_{A,2}(\Omega),~\int_{\Omega} \left|u(x)\right|^{p}x^A dx=1\right\} where p\nearrow 2^*. More precisely, since the embedding from D^1_{A,2}(\Omega) to L^p(\Omega,x^Adx) is compact for q<{2^*} we can assert the existence of a function u_{A,p}=u_p\in D^1_{A,2}(\Omega) such that \int_{\Omega} \left|u(x)\right|^{p}x^A dx=1 and \int_{\Omega}\left|\nabla u_p(x)\right|^2x^A dx=S^2_{A,p}+o(1) as p\nearrow 2^*. The idea is to obtain a generalization of the known results about the classical Sobolev inequality (A=0). For example, we would like to know if u_p develops blow up points as p\nearrow 2^*, and if this is the case, we would also like to discover the location of such blow up points and the respective limiting profile of suitable normalized minimizers.
During the course of my Ph.D. studies, I developed a theory about the singular second order Sturm-Liouville operator L_\alpha u(x)=-(x^{2\alpha}u'(t))' on the interval (0,1), where \alpha>0 is a real parameter. One of the main reasons I studied this operator is that it serves as a toy model to more general degenerate elliptic operators, and results obtained in this simpler setup might shed some light into the study of more general cases.
In joints works with H. Wang we used tools from functional analysis to prove existence and regularity, uniqueness of solutions, as-well as spectral properties of the equation L_\alpha u+u=f. The core idea behind this study was to look for solutions in appropriate weighted Sobolev spaces (which had to be constructed for the occasion). Later, I studied the semi-linear eigenvalue problem L_\alpha u=\lambda u+|u|^{p-1}u, where \lambda and p>1 are real parameters. In those works, I performed a bifurcation analysis for L_\alpha, determining the relationship between the parameters \alpha,~\lambda and p and the existence/non-existence of a branch of positive solutions emanating form the first eigenvalue \lambda_1 of L_\alpha.
The main goal of this work will be to continue the research about the operator L_\alpha by answering some of the open problems that arose in the works cited before.
In terms of the semi-linear eigenvalue problem L_\alpha u=\lambda u+|u|^{p-1}u the open problems I plan to attack can be divided into two cases with respect to the parameter \alpha: 0 < \alpha<1 and \alpha\geq 1. In the case where 0<\alpha<1 there are a few open questions, specially when the parameter p is large: in a previous article we showed that positive solutions only exist in a range \hat\lambda<\lambda<\lambda_1 for some \hat\lambda>0, however we still do not have a precise description of the optimal \hat\lambda, and how the branch of positive solutions behave near that \hat\lambda. When \alpha\geq 1, we know that all solutions satisfying u(1)=0 must have infinite sing changes in the interval (0,1), however, we would like to know how fast the sing changes occur as we approach x=0; also, the existence of bounded solutions in this case remain an open question.
On the other hand, the operator L_\alpha u(x)=-(x^{2\alpha}u'(x))' can be generalized into two different directions:
We establish point-wise asymptotic estimates at infinity for solutions to the doubly weighted quasi-linear equation \left\lbrace \begin{aligned} -\mathrm{div}(w_1|\nabla u|^{p-2}\nabla u)&=w_2|u|^{q-2}u&&\text{in }\Omega,\\ u\in D^{1,p,w_1}&(\Omega) \end{aligned} \right. where w_1 and w_2 are compatible weights and q>p>1 is a critical exponent q>p>1 in the sense of Sobolev.
In this article we obtain point-wise asymptotic estimates for solutions to \left\lbrace \begin{aligned} -\mathrm{div}\,(w|\nabla u|^{p-2}\nabla u)&=w|u|^{q-2}u&&\text{in }\Omega,\\ u\in D^{1,p}&(\Omega;wdx) \end{aligned} \right. for a critical exponent q>p in the sense of Sobolev. To do so, we firstly study the quasi-linear equation \left\lbrace \begin{aligned} \mathrm{div}\, \mathcal A(x,u,\nabla u)&=\mathcal B(x,u,\nabla u)&&\text{in }\Omega,\\ u\in H^{1,p}_{loc}&(\Omega;wdx) \end{aligned} \right. where \mathcal A and \mathcal B are functions satisfying \mathcal A(x,u,\nabla u)\sim w(|\nabla u|^{p-2}\nabla u+|u|^{p-2}u) and \mathcal B(x,u,\nabla u)\sim w(|\nabla u|^{p-1}+|u|^{p-1}) for p>1 and a p-admissible weight function w. We fill a gap in the literature and we establish interior regularity results of weak solutions to this kind of quasi-linear equations.
In this paper we consider the following Sturm-Liouville equation \begin{equation*} \left\lbrace \begin{aligned} -(x^{2\alpha}u'(x))'+u(x)&=f(x) && \text{ on } (0,1],\\ u(1)&= 0, && \end{aligned} \right. \end{equation*} where \alpha<1 is a nonzero real number and f belongs to L^p(0,1) for p\geq 1. We analyze the existence and regularity of solutions to the equation under suitable weighted Dirichlet boundary condition at the origin.
In this article we use a weighted version of Poincaré's inequality to study density and extension properties of weighted Sobolev spaces over some open set \Omega\subseteq\mathbb{R}^N. Additionally, we study the specific case of monomial weights w(x_1,\ldots,x_N)=\prod_{i=1}^N|x_i|^{a_i},\ a_i\geq 0, showing the validity of a weighted Poincaré inequality together with some embedding properties of the associated weighed Sobolev spaces.
In this article we study the existence and non-existence of extremals for the following family of Hardy-Sobolev inequalities \left({\int_{(\mathbb R_+)^k\times{\mathbb R}^{N-k}}|x^B u|^{q}}\right)^{\frac{1}{q}}\leq C\left({\int_{(\mathbb R_+)^k\times\mathbb R^{N-k}}|x^A \nabla u|^{p}}\right)^{\frac{1}{p}}, which holds for suitable values of A,~B\in\mathbb R^N, q>p>1. Here the quantity x^A (respectively x^B) denotes the monomial weight defined as x^A=|x_1|^{a_1}\cdot\ldots\cdot |x_k|^{a_k}\quad \text{(respectively } x^B=|x_1|^{b_1}\cdot\ldots\cdot |x_k|^{b_k}\text{)}.
In this paper we study the essential spectrum of the operator L_Au(x)=-(A(x)u'(x))'+u(x) where A(x) is a positive absolutely continuous function on (0,1) that resembles x^{2\alpha} for some \alpha\geq 1. We prove that the essential spectrum of L_A coincides with the essential spectrum of the operator L_\alpha u(x):=-(x^{2\alpha}u'(x))'+u(x).
In this work we study the uniqueness of solutions to the following singular non-linear Sturm-Liouville equation \left\lbrace\begin{aligned} -(x^{2\alpha}u')'&=\lambda u + u^p &\hbox{in } (0,1),\\ u&>0 &\hbox{in } (0,1),\\ u(1)&=0, \end{aligned}\right. where 0<\alpha<1, p>1 and \lambda\in\mathbb R are parameters.
We show that when 0<\alpha\leq \frac12 and p>1, and when \frac12<\alpha<1 and 1 < p \leq\frac{3-2\alpha}{2\alpha-1} uniqueness of solutions is guaranteed to hold when one imposes some appropriate behavior at the origin.
We give an elementary proof of a family of Hardy-Sobolev-type inequalities with monomial weights. As a corollary, we obtain a weighted trace inequality related to the fractional Laplacian.
In this work we study the asymptotic behavior of the L^\infty norm of the least energy solution u_p of the following semi-linear Neumman problem \left\lbrace\begin{aligned} \Delta u = u&,\; u>0 &&\text{in }\Omega,\\ \frac{\partial u}{\partial \nu} &=u^p &&\text{on }\partial\Omega,\\ \end{aligned}\right. where \Omega is a smooth bounded domain in \mathbb R^2. Our main result shows that the L^\infty norm of u_p remains bounded, and bounded away from zero as p goes to infinity, more precisely, we prove that \lim\limits_{p\to\infty}\Vert u\Vert_{L^\infty(\partial\Omega)}=\sqrt e.
Please check the addendum where an additional remark has been included in page 8.
We study the semi-linear Sturm-Liouville equation \left\lbrace\begin{aligned} -(x^{2\alpha}u')'&=\lambda u + |u|^{p-1}u &\hbox{in } (0,1),\\ u(1)&=0, \end{aligned}\right. where \alpha\geq 1, p>1, and \lambda are real parameters. We prove that all non-trivial solutions are oscillatory and unbounded as x approaches 0. Moreover, there exist \gamma>0 and \delta>0 such that any solution u(x) resembles x^{-\gamma}\eta(x^{-\delta}) near the origin, where \eta is a non-trivial periodic solution to the Emden-Fowler equation \delta^2\eta''+|\eta|^{p-1}\eta=0 in [0,\infty).
In this paper we study existence of positive solutions to the following singular non-linear Sturm-Liouville equation \left\lbrace\begin{aligned} -(x^{2\alpha}u')'&=\lambda u + u^p \hbox{ in } (0,1),\\ u(1)&=0,\\ \end{aligned}\right. where \alpha>0, p>1 and \lambda are real constants.
We prove that when 0<\alpha\leq\frac12 and p>1 or when \frac12<\alpha<1 and 1 < p\leq \frac{3-2\alpha}{2\alpha-1}, there exists a branch of continuous positive solutions bifurcating to the left of the first eigenvalue of the operator \mathcal L_\alpha u=-(x^{2\alpha}u')' under the boundary condition \lim\limits_{x\to0}x^{2\alpha}u'(x)=0. The projection of this branch onto its \lambda component is unbounded in two cases: when 0<\alpha\leq\frac12 and p>1, and when \frac12<\alpha<1 and p<\frac{3-2\alpha}{2\alpha-1}. On the other hand, when \frac12<\alpha<1 and p\geq\frac{3-2\alpha}{2\alpha-1}, the projection of the branch has a positive lower bound below which no positive solution exists.
When 0<\alpha<\frac12 and p>1, we show that a second branch of continuous positive solution can be found to the left of the first eigenvalue of the operator \mathcal L_\alpha under the boundary condition \lim\limits_{x\to 0}u(x)=0.
Finally, when \alpha\geq1, the operator \mathcal L_\alpha has no eigenvalues under its canonical boundary condition at the origin, and we prove that in fact there are no positive solutions to the equation, regardless of \lambda\in \mathbb R and p>1.
We consider functions u\in W^{m,1}_0(\Omega), where \Omega\subset \mathbb R^N is a smooth bounded domain, and m\geq 2 is an integer. For all j\geq 0, 1\leq k\leq m-1, such that 1\leq j+k\leq m, we prove that \frac{\partial^ju(x)}{d(x)^{m-j-k}}\in W^{k,1}_0(\Omega) with \left\Vert\partial^k\left(\frac{\partial^ju(x)}{d(x)^{m-j-k}}\right)\right\Vert_{L^1(\Omega)}\leq C\left\Vert u\right\Vert_{W^{m,1}(\Omega)}, where d is a smooth positive function which coincides with \mathrm{dist}(x,\partial\Omega) near \partial\Omega, and \partial^l denotes any partial differential operator of order l.
Given \alpha>0 and f\in L^2(0,1), consider the following singular Sturm-Liouville equation, \left\lbrace\begin{aligned} -(x^{2\alpha}u'(x))'+u(x)&=f(x) \hbox{ a.e. on } (0,1),\\ u(1)&=0. \end{aligned}\right. We prove existence of solutions under (weighted) non-homogeneous boundary conditions at the origin.
We consider functions u\in W^{2,1}_0(\Omega), where \Omega\subset \mathbb R^N is a smooth bounded domain. We prove that \frac{u(x)}{d(x)}\in W^{1,1}_0(\Omega) with \left\Vert \nabla\left(\frac{u(x)}{d(x)}\right)\right\Vert_{L^1(\Omega)}\leq C\left\Vert u\right\Vert_{W^{2,1}(\Omega)}, where d is a smooth positive function which coincides with \mathrm{dist}(x,\partial\Omega) near \partial\Omega and C is a constant depending only on \Omega.
Given \alpha>0 and f\in L^2(0,1), we are interested in the equation \begin{equation*} \left\lbrace\begin{aligned} -(x^{2\alpha}u'(x))'+u(x)&=f(x) \hbox{ on } (0,1],\\ u(1)&=0. \end{aligned}\right. \end{equation*} We prescribe appropriate (weighted) homogeneous boundary conditions at the origin and prove the existence and uniqueness of H^2_{loc}(0,1] solutions. We study the regularity at the origin of such solutions. We perform a spectral analysis of the differential operator \mathcal{L}u:=-(x^{2\alpha}u')'+u under those appropriate homogenous boundary conditions.
In this paper, we consider functions u\in W^{m,1}(0,1) where m\geq 2 and u(0)=Du(0)=\ldots=D^{m-1}u(0)=0. Although it is not true in general that \frac{D^ju(x)}{x^{m-j}}\in L^1(0,1) for j\in\{0,1,\ldots,m-1\}, we prove that \frac{D^ju(x)}{x^{m-j-k}}\in W^{k,1}(0,1) if k\geq 1 and 1\leq j+k\leq m, with j,k integers. Furthermore, we have the following Hardy type inequality, \left\Vert D^k\left(\frac{D^ju(x)}{x^{m-j-k}}\right)\right\Vert_{L^1(0,1)}\leq \frac {(k-1)!}{(m-j-1)!}\left\Vert D^mu\right\Vert_{L^1(0,1)}, where the constant is optimal.
We consider the elliptic equation -\Delta u+u=0 in a bounded, smooth domain \Omega in \mathbb R^2, subject to the nonlinear Neumann boundary condition \frac{\partial u}{\partial \nu}=u^p. Here p>1 is a large parameter. We prove that given any integer m\ge 1 there exist at least two families of solutions u_p developing exactly m peaks \xi_i \in \partial\Omega, in the sense that pu^p\rightharpoonup 2e\pi\sum\limits_{i=1}^{m}\delta_{\xi_i}, as p\rightarrow\infty.
The main body of this dissertation can be divided into two separate topics. The first topic deals with a Hardy type inequality for functions belonging to the Sobolev space W^{m,1}_0(\Omega), where m\geq 2 and \Omega is a smooth bounded domain in \mathbb R^N, N\geq 1. We show that for such functions u\in W^{m,1}_0(\Omega), one has \left\Vert\partial^k\left(\frac{\partial^ju(x)}{d(x)^{m-j-k}}\right)\right\Vert_{L^1(\Omega)}\leq C\Vert u\Vert_{W^{m,1}(\Omega)}, where j,k are non-negative integers such that 1 \leq k \leq m-1 and 1\leq j+k\leq m, and d(x) is a smooth positive function which coincides with \mathrm{dist}(x,\partial\Omega) near \partial\Omega.
The second topic deals with the study of the singular Sturm-Liouville operator \mathcal L_\alpha u:=-(x^{2\alpha}u')', where \alpha>0. We develop a linear theory for such operator by introducing suitable weighted Sobolev spaces and prove existence and uniqueness for equations of the form \mathcal L_\alpha u+u=f\in L^2 under both homogeneous and non-homogeneous boundary data at the origin. In addition, the spectrum of the operator \mathcal L_\alpha is fully described.
Finally, we prove existence, non-existence and uniqueness results for positive solutions of the non-linear singular Sturm-Liouville equation \mathcal L_\alpha u=\lambda u+u^p,\ u(1)=0, where \alpha>0, p>1 and \lambda\in\mathbb R are parameters.
En este trabajo de título se presenta un estudio de la ecuación \begin{aligned} -\Delta u + u &= 0 &\text{en }\Omega\\ \frac{\partial u}{\partial \nu} &= u^p &\text{en }\partial\Omega, \end{aligned} donde \Omega es un dominio en el plano de frontera suave y p es un parámetro que tiende a infinito. Tal estudio tiene como objetivo final probar la existencia de una familia de soluciones que presenten concentración en puntos de la frontera de \Omega.
Para obtener tal resultado, se ha procedido siguiendo un esquema de reducción finito-dimensional, lo que consiste, en términos generales, en buscar una solución de la forma U+\phi, donde U es una función escogida adecuadamente y \phi es un término de ajuste, cuya existencia está ligada a un problema en dimensión finita. El marco analítico funcional planteado, presenta grandes similitudes con trabajos anteriores, en particular, con el utilizado por Esposito, Musso y Pistoia en un problema interior análogo al que aquí se estudia.
La primera parte de esta memoria trata con la elección de una buena aproximación inicial, la función U, de modo que se tenga el comportamiento asintótico esperado, y que el error obtenido sea lo suficientemente pequeño. El trabajo continúa al reescribir la ecuación original, para obtener una ecuación no-lineal en términos de \phi. Para estudiar dicha ecuación, primero se realiza un completo análisis de la invertibilidad de un problema lineal asociado. En segundo lugar, se analiza la existencia en una ecuación no-lineal auxiliar vía un esquema de punto fijo, entregando, además, las condiciones necesarias de regularidad sobre la solución para reducir el problema de existencia de soluciones del problema original, al de encontrar puntos críticos de una función finito-dimensional. Finalmente, demostramos que dicha función finito-dimensional admite al menos dos puntos críticos y que tales puntos críticos resultan ser los puntos en donde se produce concentración.
Finalmente, se formulan algunas interrogantes respecto a posibles mejoras en el resultado obtenido. Así también, siguiendo lo realizado por Adimurthi y Grossi, como lo desarrollado en trabajos de Ren y Wei respecto al problema interior asociado, se conjeturan ciertos resultados que se podrían obtener respecto al comportamiento asintótico de la solución de mínima energía de este problema.
Here you can find some teaching material (lecture notes, exercises, past exams) from the courses I have taught. Most of the material is in spanish.
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