168 4 Introduction to Minimax Methods
The requirement that f be C
1
can be weakened, and we use it only to avoid some
technicalities (for example we could take f bounded and satisfying (f
6
)). If we
define
˜
f : ×R →R as
˜
f(x,t)=λt +f(t)+h(x),
we see that
lim
t→±∞
˜
f(t,x)
t
=λ
almost everywhere in . Thus
˜
f grows linearly in t at infinity, and this characterizes
(4.18) as an asymptotically linear problem.
Once H
1
0
() is equipped with the usual norm defined by (4.14), the weak so-
lutions of (4.18) are the critical points of the functional J : H
1
0
() → R defined
by
J(u)=
1
2
u
2
−
λ
2
u
2
dx −
F(u)dx −
hu dx,
where of course F(t) =
t
0
f(s)ds.Dueto(f
10
), repeating the arguments of
Lemma 4.4.5, the functional J is readily seen to be in C
1,1
(H
1
0
()), and we will
not discuss this point anymore.
Let 0 <λ
1
<λ
2
≤···be the usual sequence of the eigenvalues of the operator
− +q(x). The solvability of Problem (4.18) strongly depends on the location of
λ with respect to the eigenvalues λ
k
.
Definition 4.4.10 If λ =λ
k
for every k, Problem (4.18) is said to be nonresonant. If
λ = λ
k
for some k, the problem is said to be resonant or at resonance with the k-th
eigenvalue.
Resonant problems are much more difficult to solve, and it may happen that they
do not have any solution at all, even in the linear case (compare with Theorem 1.7.8).
So, to illustrate the method we first consider a nonresonant problem.
Theorem 4.4.11 Assume that (h
1
), (h
2
) and (f
10
) hold. If λ = λ
k
for every k, then
Problem (4.18) has at least one solution.
If λ<λ
1
, the functional J is coercive and can be shown to have a global min-
imum, with the methods of Sect. 2.1. The interesting case is thus λ>λ
1
, and we
define n ∈N to be the number such that
λ
n
<λ<λ
n+1
. (4.19)
In this case we are going to show that the functional J satisfies the assumptions of
the Saddle Point Theorem. As usual we split the problem in two parts: compactness
and geometric assumptions.
In what follows, we always take for granted the assumptions of Theorem 4.4.11
and (4.19).