2.3 Superlinear Problems and Constrained Minimization 55
orthogonally as H
1
0
() = X
1
⊕X
2
, according to convexity and concavity proper-
ties of the functional I ; then, writing the generic element of H
1
0
() as u +v, with
u ∈X
1
and v ∈X
2
, we have found a critical level s for I as
s = max
u∈X
1
min
v∈X
2
I(u+v).
This is a first example of a procedure that we will generalize in Chap. 4.
Remark 2.2.14 It is important to notice that many steps of the proof of the theo-
rem work because of convexity (or concavity) properties of the functional I. These
properties hold because of the rather strong assumption (h
7
), that rules the behavior
of the nonlinearity f on the entire real line. For example, if f is differentiable and
we require that it satisfies (2.7)for|t| large only, then the convexity properties of I
fail, and we cannot prove Theorem 2.2.3. This does not mean that we cannot find a
solution to the problem, but certainly we cannot repeat the above proof. These cases
will be dealt with in later chapters with stronger methods.
Remark 2.2.15 In assumption (h
7
) one cannot allow α =λ
ν
or β =λ
ν+1
. For exam-
ple, as we have already pointed out, the linear equation −u = λ
ν
u +h in H
1
0
()
does not admit a solution for every h ∈L
2
().
Remark 2.2.16 As a final remark we point out that if h = 0 in Theorem 2.2.3, then
the problem admits only the trivial solution when f(0) = 0. Indeed in this case
u =0 is a critical point of I , and, by uniqueness, it is its only critical point.
2.3 Superlinear Problems and Constrained Minimization
Up to now we have only treated problems where the nonlinear term f has an at
most linear growth. In case the nonlinearity grows faster than linearly, one speaks
of superlinear problems. For these types of problems the techniques used so far
do not work anymore; for example the functionals associated to these problems are
generally unbounded from below and they present a lack of convexity or concavity
properties that makes the arguments of the previous sections useless.
Actually for rather general f and h only partial results are known, though a quite
rich theory has been developed. We begin to present here some of the simplest cases,
in which h is identically zero and f is a power. Further results will be presented in
later sections.
We take throughout this section a real number p such that
2 <p<2
∗
=
2N
N −2
,
and we search a function u that satisfies the superlinear and subcritical problem
−u +q(x)u =|u|
p−2
u in ,
u =0on∂.
(2.18)