Abstract :
We consider the boundary value problem consisting of the pp-Laplacian equation
equation(1)
View the MathML source−ϕp(u′)′=λϕp(u),on (−1,1),
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where p>1p>1, View the MathML sourceϕp(s)≔|s|p−1sgns for s∈Rs∈R, λ∈Rλ∈R, together with the multi-point boundary conditions
equation(2)
View the MathML sourceϕp(u′(±1))=∑i=1m±αi±ϕp(u′(ηi±)),
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or
equation(3)
View the MathML sourceu(±1)=∑i=1m±αi±u(ηi±),
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or a mixed pair of these conditions (with one condition holding at each of x=−1x=−1 and x=1x=1). In (2), (3), m±⩾1m±⩾1 are integers, View the MathML sourceηi±∈(−1,1), 1⩽i⩽m±1⩽i⩽m±, and the coefficients View the MathML sourceαi± satisfy
View the MathML source∑i=1m±|αi±|<1.
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We term the conditions (2) and (3), respectively, Neumann-type and Dirichlet-type boundary conditions, since they reduce to the standard Neumann and Dirichlet boundary conditions when α±=0α±=0.
Given a suitable pair of boundary conditions, a number λλ is an eigenvalue of the corresponding boundary value problem if there exists a non-trivial solution uu (an eigenfunction). The spectrum of the problem is the set of eigenvalues. In this paper we obtain various spectral properties of these eigenvalue problems. We then use these properties to prove Rabinowitz-type, global bifurcation theorems for related bifurcation problems, and to obtain nonresonance conditions (in terms of the eigenvalues) for the solvability of related inhomogeneous problems.