We consider the nonlinear eigenvalue problem [D(u(t))u(t) ′ ] ′ + λg(u(t)) = 0, u(t) > 0, t ∈ I := (0, 1), u(0) = u(1) = 0, which comes from the porous media type equation. Here, D(u) = pu 2n + sin u (n ∈ N, p > 0: given constants), g(u) = u or g(u) = u + sin u. λ > 0 is a bifurcation parameter which is a continuous function of α = u λ ∞ of the solution u λ corresponding to λ, and is expressed as λ = λ(α). Since our equation contains oscillatory term in diffusion term, it seems significant to study how this oscillatory term gives effect to the structure of bifurcation curves λ(α). We prove that the simplest case D(u) = u 2n + sin u and g(u) = u gives us the most significant phenomena to the global behavior of λ(α).