2.4 A Perturbed Problem 63
By construction, s =0 is a minimum point for γ . Therefore
0 =γ
(0) =I
(t (0)u)[t
(0)u +t(0)v]=t
(0)I
(u)u +I
(u)v =I
(u)v.
For the last equality we have used the fact that I
(u)u =0 because u ∈N.Wehave
obtained I
(u)v =0 for all v ∈H
1
0
(), proving that u is a solution of (2.18).
Remark 2.3.13 The last part of the proof shows that a minimum of I constrained
on the Nehari manifold N is actually a free critical point of I , on the whole space
H
1
0
(). This remarkable fact is expressed by saying that the Nehari manifold is a
natural constraint for I.
2.4 A Perturbed Problem
As we have anticipated the method of minimization on the Nehari manifold can be
extended to cover more general problems than that of the preceding section.
We begin with an existence result for a perturbed problem, in the sense that we
consider a power nonlinearity plus afixedfunctionh ∈L
2
(). The result contained
in this section is quite delicate, and can be omitted upon first reading.
We are going to prove that under suitable assumptions, and particularly if h is
small, the problem admits two solutions. Let us make this more precise.
We consider, for h ∈L
2
() and p ∈(2, 2
∗
), the Dirichlet problem
−u +q(x)u =|u|
p−2
u +h(x) in ,
u =0on∂.
(2.25)
Or aim is to show that if |h|
2
is sufficiently small, then (2.25) admits at least two non-
trivial solutions. This is not really surprising since the unperturbed problem (h ≡0)
also admits two solutions: the one found with Theorem 2.3.1 and the trivial solution
u ≡ 0. If h does not vanish identically, the trivial solution is replaced by a “true”
nonzero solution. Thus one can think that for h small the two solutions are “pertur-
bations” of the two solutions already present in the autonomous case.
We add that the solution corresponding in this scheme to the trivial solution of
the unperturbed case can be found very easily, while most of the work must be
devoted to the search of the analogue of the solution found in Theorem 2.3.1 by
minimization on the Nehari manifold.
The functional associated to (2.25)is
J(u)=
1
2
u
2
−
1
p
|u|
p
dx −
hu dx =
1
2
u
2
−
1
p
|u|
p
p
−
hu dx,
which is of course differentiable on H
1
0
(). The main result is the following.
Theorem 2.4.1 Let p ∈(2, 2
∗
) and assume that (h
1
) holds. Then there exists ε
∗
> 0
such that for every h ∈ L
2
(), with |h|
2
≤ ε
∗
, Problem (2.25) admits at least two
solutions.