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    Half eigenvalues and the Fucik spectrum of multi-point, boundary value problems

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    We consider the nonlinear boundary value problem consisting of the equation \tag{1} -u" = f(u) + h, \quad \text{a.e. on (βˆ’1,1)(-1,1),} where h∈L1(βˆ’1,1)h \in L^1(-1,1), together with the multi-point, Dirichlet-type boundary conditions \tag{2} u(\pm 1) = \sum^{m^\pm}_{i=1}\alpha^\pm_i u(\eta^\pm_i) where mΒ±β‰₯1m^\pm \ge 1 are integers, Ξ±Β±=(Ξ±1Β±,...,Ξ±mΒ±)∈[0,1)mΒ±\alpha^\pm = (\alpha_1^\pm, ...,\alpha_m^\pm) \in [0,1)^{m^\pm}, η±∈(βˆ’1,1)mΒ±\eta^\pm \in (-1,1)^{m^\pm}, and we suppose that βˆ‘i=1mΒ±Ξ±iΒ±<1. \sum_{i=1}^{m^\pm} \alpha_i^\pm < 1 . We also suppose that f:Rβ†’Rf : \mathbb{R} \to \mathbb{R} is continuous, and 0<f±∞:=lim⁑sβ†’Β±βˆžf(s)s<∞. 0 < f_{\pm\infty}:=\lim_{s \to \pm\infty} \frac{f(s)}{s} < \infty. We allow fβˆžβ‰ fβˆ’βˆžf_{\infty} \ne f_{-\infty} --- such a nonlinearity ff is {\em jumping}. Related to (1) is the equation \tag{3} -u" = \lambda(a u^+ - b u^-), \quad \text{on (βˆ’1,1)(-1,1),} where Ξ», a, b>0\lambda,\,a,\,b > 0, and uΒ±(x)=max⁑{Β±u(x),0}u^{\pm}(x) =\max\{\pm u(x),0\} for x∈[βˆ’1,1]x \in [-1,1]. The problem (2)-(3) is `positively-homogeneous' and jumping. Regarding a, ba,\,b as fixed, values of Ξ»=Ξ»(a,b)\lambda = \lambda(a,b) for which (2)-(3) has a non-trivial solution uu will be called {\em half-eigenvalues}, while the corresponding solutions uu will be called {\em half-eigenfunctions}. We show that a sequence of half-eigenvalues exists, the corresponding half-eigenfunctions having specified nodal properties, and we obtain certain spectral and degree theoretic properties of the set of half-eigenvalues. These properties lead to solvability and non-solvability results for the problem (1)-(2). The set of half-eigenvalues is closely related to the `Fucik spectrum' of the problem, which we briefly describe. Equivalent solvability and non-solvability results for (1)-(2) are obtained from either the half-eigenvalue or the Fucik spectrum approach

    Multiple positive solutions of a Sturm-Liouville boundary value problem with conflicting nonlinearities

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    We study the second order nonlinear differential equation \begin{equation*} u"+ \sum_{i=1}^{m} \alpha_{i} a_{i}(x)g_{i}(u) - \sum_{j=0}^{m+1} \beta_{j} b_{j}(x)k_{j}(u) = 0, \end{equation*} where Ξ±i,Ξ²j>0\alpha_{i},\beta_{j}>0, ai(x),bj(x)a_{i}(x), b_{j}(x) are non-negative Lebesgue integrable functions defined in [0,L]\mathopen{[}0,L\mathclose{]}, and the nonlinearities gi(s),kj(s)g_{i}(s), k_{j}(s) are continuous, positive and satisfy suitable growth conditions, as to cover the classical superlinear equation u"+a(x)up=0u"+a(x)u^{p}=0, with p>1p>1. When the positive parameters Ξ²j\beta_{j} are sufficiently large, we prove the existence of at least 2mβˆ’12^{m}-1 positive solutions for the Sturm-Liouville boundary value problems associated with the equation. The proof is based on the Leray-Schauder topological degree for locally compact operators on open and possibly unbounded sets. Finally, we deal with radially symmetric positive solutions for the Dirichlet problems associated with elliptic PDEs.Comment: 23 pages, 6 PNG figure
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