We consider the nonlinear boundary value problem consisting of the equation (1) − u ″ = f ( u ) + h , a.e. on ( − 1 , 1 ) , where h ∈ L 1 ( − 1 , 1 ) , together with the multi-point, Dirichlet-type boundary conditions (2) u ( ± 1 ) = ∑ i = 1 m ± α i ± u ( η i ± ) , where m ± ⩾ 1 are integers, α ± = ( α 1 ± , … , α m ± ) ∈ [ 0 , 1 ) m ± , η ± ∈ ( − 1 , 1 ) m ± , and we suppose that ∑ i = 1 m ± α i ± < 1 . We also suppose that f : R → R is continuous, and 0 < f ± ∞ : = lim s → ± ∞ f ( s ) s < ∞ (we assume that these limits exist). We allow f ∞ ≠ f − ∞ — such a nonlinearity f is said to be jumping . Related to (1) is the equation (3) − u ″ = λ ( a u + − b u − ) , on ( − 1 , 1 ) , where λ , a , b > 0 , and u ± ( x ) = max { ± u ( x ) , 0 } for x ∈ [ − 1 , 1 ] . The problem (2) , (3) is ‘positively-homogeneous’ and jumping. Regarding a , b as fixed, values of λ = λ ( a , b ) for which (2) , (3) has a non-trivial solution u will be called half-eigenvalues , while the corresponding solutions u will be called 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 ‘Fučík 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 Fučík spectrum approach.
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