We consider the p-Laplacian boundary value problemc 00 u(0) = c 01 u (0), c 10 u(1) = c 11 u (1),where p > 1 is a fixed number, φ p (s) = |s| p−2 s, s ∈ R, and for each j = 0, 1, |c j 0 | + |c j 1 | > 0. The function f : [0, 1] × R 2 → R is a Carathéodory function satisfying, for (x, s, t) ∈ [0, 1] × R 2 ,where ψ ± , Ψ ± ∈ L 1 (0, 1), and E has the form E(x, s, t) = ζ(x)e(|s| + |t|), with ζ ∈ L 1 (0, 1), ζ 0, e 0 and lim r→∞ e(r)r 1−p = 0. This condition allows the nonlinearity in (1) to behave differently as u → ±∞. Such a nonlinearity is often termed jumping.together with (2), where a, b ∈ L 1 (0, 1), λ ∈ R, and u ± (x) = max{±u(x), 0} for x ∈ [0, 1]. This problem is 'positively-homogeneous' and jumping. Values of λ for which (2), (3) has a nontrivial solution u will be called half-eigenvalues, while the corresponding solutions u will be called halfeigenfunctions.We show that a sequence of half-eigenvalues exists, the corresponding half-eigenfunctions having certain nodal properties, and we obtain certain spectral and degree theoretic properties of the set of half-eigenvalues. These properties lead to existence and nonexistence results for the problem (1), (2). We also consider a related bifurcation problem, and obtain a global bifurcation result similar to the well-known Rabinowitz global bifurcation theorem. This then leads to a multiplicity result for (1), (2).When the functions a and b are constant the set of half-eigenvalues is closely related to the 'Fučík spectrum' of the problem, and equivalent solvability results are obtained using the two approaches. However, when a and b are not constant the half-eigenvalue approach yields stronger results.