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Solvability for second-order nonlocal boundary value problems with a p-Laplacian at resonance on a half-line

Abstract

This paper investigates the solvability of the second-order boundary value problems with the one-dimensional pp-Laplacian at resonance on a half-line {(c(t)ϕp(x(t)))=f(t,x(t),x(t)),    0<t<,x(0)=i=1nμix(ξi),  limt+c(t)ϕp(x(t))=0\left\{\begin{array}{llll} (c(t)\phi_{p}(x'(t)))'=f(t,x(t),x'(t)),~~~~0<t<\infty,\\ x(0)=\sum\limits_{i=1}^{n}\mu_ix(\xi_{i}), ~~\lim\limits_{t\rightarrow +\infty}c(t)\phi_{p}(x'(t))=0 \end{array}\right. and {(c(t)ϕp(x(t)))+g(t)h(t,x(t),x(t))=0,    0<t<,x(0)=0g(s)x(s)ds,  limt+c(t)ϕp(x(t))=0\left\{\begin{array}{llll} (c(t)\phi_{p}(x'(t)))'+g(t)h(t,x(t),x'(t))=0,~~~~0<t<\infty,\\ x(0)=\int_{0}^{\infty}g(s)x(s)ds,~~\lim\limits_{t\rightarrow +\infty}c(t)\phi_{p}(x'(t))=0 \end{array}\right. with multi-point and integral boundary conditions, respectively, where ϕp(s)=sp2s\phi_{p}(s)=|s|^{p-2}s, p>1p>1. The arguments are based upon an extension of Mawhin's continuation theorem due to Ge. And examples are given to illustrate our results

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