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On the Fredholm Alternative for the p-Laplacian in One Dimension
Authors:Manasevich  Raul F; TakaC  Peter
Institution:Centro de Modelamiento Matemático and Departamento de Ingenieria Matemática FCFM, Universidad de Chile, Casilla 170, Correo 3, Santiago, Chile manasevi{at}dim.uchile.cl
Fachbereich Mathematik, Universität Rostock D-18055 Rostock, Germany peter.takac{at}mathematik.uni-rostock.de
Abstract:We investigate the existence of a weak solution u to the quasilineartwo-point boundary value problem Formula We assume that 1 < p < {infty} p ¬ = 2, 0 < a < {infty}, andthat f isin L1(0,a) is a given function. The number {lambda}k stands forthe k-th eigenvalue of the one-dimensional p-Laplacian. Letisinp {pi}p x/a) denote the eigenfunction associated with {lambda}1; then isinp(k{pi}p x/a) is the eigenfunction associated with {lambda}k. We show the existenceof solutions to (P) in the following cases. (i) When k=1 and f satisfies the orthogonality condition Formula the set of solutions is bounded. (ii) If k=1 and ft isin L1(0,a) is a continuous family parametrizedby t isin 0,1], with Formula then there exists some t* isin 0,1] such that (P) has a solutionfor f = ft*. Moreover, an appropriate choice of t* yields asolution u with an arbitrarily large L1(0,a)-norm which meansthat such f cannot be orthogonal to isinp{pi}p x/a. (iii) When k ≥ 2 and f satisfies a set of orthogonality conditionsto isinp(k {pi}p x/a) Formula on the subintervals Formula, again, the set of solutions is bounded. Formula is a continuous family satisfying either Formula or another related condition, then there exists some t* isin 0,1]such that (P) has a solution for f = ft*. Prüfer's transformation plays the key role in our proofs.2000 Mathematical Subject Classification: primary 34B16, 47J10;secondary 34L40, 47H30.
Keywords:non-linear eigenvalue problem  Fredholm alternative  quasilinear two-point Dirichlet problem  one-dimensional p-Laplacian  Prü  fer's transformation
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