9 research outputs found

    Proofs of Urysohn's Lemma and the Tietze Extension Theorem via the Cantor function

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    Urysohn's Lemma is a crucial property of normal spaces that deals with separation of closed sets by continuous functions. It is also a fundamental ingredient in proving the Tietze Extension Theorem, another property of normal spaces that deals with the existence of extensions of continuous functions. Using the Cantor function, we give alternative proofs for Urysohn's Lemma and the Tietze Extension Theorem.Comment: A slightly modified version has been accepted for publication in the Bulletin of the Australian Mathematical Societ

    Examples of sharp asymptotic profiles of singular solutions to an elliptic equation with a sign-changing non-linearity

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    The first two authors [Proc. Lond. Math. Soc. (3) {\bf 114}(1):1--34, 2017] classified the behaviour near zero for all positive solutions of the perturbed elliptic equation with a critical Hardy--Sobolev growth Δu=xsu2(s)1μuq in B{0},-\Delta u=|x|^{-s} u^{2^\star(s)-1} -\mu u^q \hbox{ in }B\setminus\{0\}, where BB denotes the open unit ball centred at 00 in Rn\mathbb{R}^n for n3n\geq 3, s(0,2)s\in (0,2), 2(s):=2(ns)/(n2)2^\star(s):=2(n-s)/(n-2), μ>0\mu>0 and q>1q>1. For q(1,21)q\in (1,2^\star-1) with 2=2n/(n2)2^\star=2n/(n-2), it was shown in the op. cit. that the positive solutions with a non-removable singularity at 00 could exhibit up to three different singular profiles, although their existence was left open. In the present paper, we settle this question for all three singular profiles in the maximal possible range. As an important novelty for μ>0\mu>0, we prove that for every q(2(s)1,21)q\in (2^\star(s) -1,2^\star-1) there exist infinitely many positive solutions satisfying xs/(q2(s)+1)u(x)μ1/(q2(s)+1)|x|^{s/(q-2^\star(s)+1)}u(x)\to \mu^{-1/(q-2^\star(s)+1)} as x0|x|\to 0, using a dynamical system approach. Moreover, we show that there exists a positive singular solution with lim infx0x(n2)/2u(x)=0\liminf_{|x|\to 0} |x|^{(n-2)/2} u(x)=0 and lim supx0x(n2)/2u(x)(0,)\limsup_{|x|\to 0} |x|^{(n-2)/2} u(x)\in (0,\infty) if (and only if) q(22,21)q\in (2^\star-2,2^\star-1).Comment: Mathematische Annalen, to appea

    Sharp asymptotic profiles for singular solutions to an elliptic equation with a sign-changing nonlinearity

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    Given B1(0)B_1(0) the unit ball of Rn\mathbb{R}^n (n3n\geq 3), we study smooth positive singular solutions uC2(B1(0){0})u\in C^2(B_1(0)\setminus \{0\}) to Δu=u2(s)1xsμuq-\Delta u=\frac{u^{2^\star(s)-1}}{|x|^s}-\mu u^q. Here 0<s<20< s<2, 2(s):=2(ns)/(n2)2^\star(s):=2(n-s)/(n-2) is critical for Sobolev embeddings, q>1q>1 and μ>0\mu> 0. When μ=0\mu=0 and s=0s=0, the profile at the singularity 00 was fully described by Caffarelli-Gidas-Spruck. We prove that when μ>0\mu>0 and s>0s>0, besides this profile, two new profiles might occur. We provide a full description of all the singular profiles. Special attention is accorded to solutions such that lim infx0xn22u(x)=0\liminf_{x\to 0}|x|^{\frac{n-2}{2}}u(x)=0 and lim supx0xn22u(x)(0,+)\limsup_{x\to 0}|x|^{\frac{n-2}{2}}u(x)\in (0,+\infty). The particular case q=(n+2)/(n2)q=(n+2)/(n-2) requires a separate analysis which we also perform

    Singular anisotropic elliptic equations with gradient-dependent lower order terms

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    We prove the existence of a solution to a singular anisotropic elliptic equation in a bounded open subset Ω\Omega of RN\mathbb R^N with N2N\ge 2, subject to a homogeneous boundary condition: \begin{equation} \label{eq0} \left\{ \begin{array}{ll} \mathcal A u+ \Phi(u,\nabla u)=\Psi(u,\nabla u)+ \mathfrak{B} u \quad& \mbox{in } \Omega,\\ u=0 & \mbox{on } \partial\Omega. \end{array} \right. \end{equation} Here Au=j=1Njupj2ju \mathcal A u=-\sum_{j=1}^N |\partial_j u|^{p_j-2}\partial_j u is the anisotropic p\overrightarrow{p}-Laplace operator, while B\mathfrak B is an operator from W01,p(Ω)W_0^{1,\overrightarrow{p}}(\Omega) into W1,p(Ω)W^{-1,\overrightarrow{p}'}(\Omega) satisfying suitable, but general, structural assumptions. Φ\Phi and Ψ\Psi are gradient-dependent nonlinearities whose models are the following: \begin{equation*} \label{phi}\Phi(u,\nabla u):=\left(\sum_{j=1}^N \mathfrak{a}_j |\partial_j u|^{p_j}+1\right)|u|^{m-2}u, \quad \Psi(u,\nabla u):=\frac{1}{u}\sum_{j=1}^N |u|^{\theta_j} |\partial_j u|^{q_j}. \end{equation*} We suppose throughout that, for every 1jN1\leq j\leq N, \begin{equation*}\label{ass} \mathfrak{a}_j\geq 0, \quad \theta_j>0, \quad 0\leq q_j<p_j, \quad 1<p_j,m\quad \mbox{and}\quad p<N, \end{equation*} and we distinguish two cases: 1) for every 1jN1\leq j\leq N, we have θj1\theta_j\geq 1; 2) there exists 1jN1\leq j\leq N such that θj<1\theta_j<1. In this last situation, we look for non-negative solutions of \eqref{eq0}
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