151 research outputs found

    Positive solutions to indefinite Neumann problems when the weight has positive average

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    We deal with positive solutions for the Neumann boundary value problem associated with the scalar second order ODE u"+q(t)g(u)=0,t[0,T], u" + q(t)g(u) = 0, \quad t \in [0, T], where g:[0,+[Rg: [0, +\infty[\, \to \mathbb{R} is positive on ]0,+[\,]0, +\infty[\, and q(t)q(t) is an indefinite weight. Complementary to previous investigations in the case 0Tq(t)<0\int_0^T q(t) < 0, we provide existence results for a suitable class of weights having (small) positive mean, when g(x)<0g'(x) < 0 at infinity. Our proof relies on a shooting argument for a suitable equivalent planar system of the type x=y,y=h(x)y2+q(t), x' = y, \qquad y' = h(x)y^2 + q(t), with h(x)h(x) a continuous function defined on the whole real line.Comment: 17 pages, 3 figure

    Scattering parabolic solutions for the spatial N-centre problem

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    For the NN-centre problem in the three dimensional space, x¨=i=1Nmi(xci)xciα+2,xR3{c1,,cN}, \ddot x = -\sum_{i=1}^{N} \frac{m_i \,(x-c_i)}{\vert x - c_i \vert^{\alpha+2}}, \qquad x \in \mathbb{R}^3 \setminus \{c_1,\ldots,c_N\}, where N2N \geq 2, mi>0m_i > 0 and α[1,2)\alpha \in [1,2), we prove the existence of entire parabolic trajectories having prescribed asymptotic directions. The proof relies on a variational argument of min-max type. Morse index estimates and regularization techniques are used in order to rule out the possible occurrence of collisions

    A priori bounds and multiplicity of positive solutions for pp-Laplacian Neumann problems with sub-critical growth

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    Let 1<p<+1<p<+\infty and let ΩRN\Omega\subset\mathbb R^N be either a ball or an annulus. We continue the analysis started in [Boscaggin, Colasuonno, Noris, ESAIM Control Optim. Calc. Var. (2017)], concerning quasilinear Neumann problems of the type -\Delta_p u = f(u), \quad u>0 \mbox{ in } \Omega, \quad \partial_\nu u = 0 \mbox{ on } \partial\Omega. We suppose that f(0)=f(1)=0f(0)=f(1)=0 and that ff is negative between the two zeros and positive after. In case Ω\Omega is a ball, we also require that ff grows less than the Sobolev-critical power at infinity. We prove a priori bounds of radial solutions, focusing in particular on solutions which start above 1. As an application, we use the shooting technique to get existence, multiplicity and oscillatory behavior (around 1) of non-constant radial solutions.Comment: 26 pages, 3 figure

    Asymptotic and chaotic solutions of a singularly perturbed Nagumo-type equation

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    We deal with the singularly perturbed Nagumo-type equation ϵ2u+u(1u)(ua(s))=0, \epsilon^2 u'' + u(1-u)(u-a(s)) = 0, where ϵ>0\epsilon > 0 is a real parameter and a:RRa: \mathbb{R} \to \mathbb{R} is a piecewise constant function satisfying 0<a(s)<10 < a(s) < 1 for all ss. We prove the existence of chaotic, homoclinic and heteroclinic solutions, when ϵ\epsilon is small enough. We use a dynamical systems approach, based on the Stretching Along Paths method and on the Conley-Wazewski's method

    Pairs of positive periodic solutions of nonlinear ODEs with indefinite weight: a topological degree approach for the super-sublinear case

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    We study the periodic and the Neumann boundary value problems associated with the second order nonlinear differential equation \begin{equation*} u'' + c u' + \lambda a(t) g(u) = 0, \end{equation*} where g ⁣:[0,+[[0,+[g \colon \mathopen{[}0,+\infty\mathclose{[}\to \mathopen{[}0,+\infty\mathclose{[} is a sublinear function at infinity having superlinear growth at zero. We prove the existence of two positive solutions when 0Ta(t) ⁣dt<0\int_{0}^{T} a(t) \!dt < 0 and λ>0\lambda > 0 is sufficiently large. Our approach is based on Mawhin's coincidence degree theory and index computations.Comment: 26 page
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