  We consider the nonlinear eigenvalue problem $[D(u(t))u(t)']' + \lambda
g(u(t)) = 0$, $u(t) > 0$, $t \in I := (0,1)$, $u(0) = u(1) = 0$, which comes
from the porous media type equation. Here, $D(u) = pu^{2n} + \sin u$ ($n \in
\mathbb{N}$, $p > 0$: given constants), $g(u) = u$ or $g(u) = u + \sin u$.
$\lambda > 0$ is a bifurcation parameter which is a continuous function of
$\alpha = \Vert u_\lambda\Vert_\infty$ of the solution $u_\lambda$
corresponding to $\lambda$, and is expressed as $\lambda = \lambda(\alpha)$.
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 $\lambda(\alpha)$. 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 $\lambda(\alpha)$.
