We consider a nonlinear elliptic equation driven by the -Laplacian with a nonsmooth potential (hemivariational inequality) and Dirichlet boundary
condition. Using a variational approach based on nonsmooth critical point
theory together with the method of upper and lower solutions, we prove the
existence of at least three nontrivial smooth solutions: one positive, the second
negative, and the third sign changing (nodal solution). Our hypotheses on
the nonsmooth potential incorporate in our framework of analysis the so-called
asymptotically -linear problems.
1. Introduction
The aim of this
work is to prove the existence of multiple solutions of constant sign and of
nodal solutions (sign changing solutions) for nonlinear elliptic equations
driven by the -Laplacian and having a nonsmooth potential
(hemivariational inequalities). So let be a bounded domain with a -boundary The problem under consideration is the
following:
Here is measurable function on ,
which in the variable is locally Lipschitz and stands for the generalized subdifferential of in the sense of Clarke [1]. Problem (1.1) is a
hemivariational inequality. Hemivariational inequalities are a new type of
variational expressions, which arise in applications if one considers more
realistic mechanical laws of multivalued and nonmonotone nature. Then the
corresponding energy (Euler) functional is nonsmooth and nonconvex. Various
engineering applications of hemivariational inequalities can be found in the
book of Naniewicz-Panagiotopoulos [2].
Multiple solutions of constant sign for problems
monitored by the -Laplacian and with a -potential were obtained by Ambrosetti et al. [3], García Azorero-Peral Alonso [4], and García
Azorero et al. [5]. In all these works, the authors consider nonlinear
eigenvalue problems and prove the existence of positive and negative solutions
for certain values of the parameter The question of existence of nodal solutions
was first addressed within the framework of semilinear problems (i.e., ). We mention the works of Dancer-Du [6] and Zhang-Li [7], which contain two
different approaches to the problem. In Dancer-Du [6], the authors use a
combination of the variational method (critical point theory) with the method
of upper and lower solutions. In contrast Zhang-Li [7] use invariance properties
of the negative gradient flow of the corresponding equation in Recently these methods were extended to
“smooth” problems driven by the -Laplacian differential operator. Carl-Perera
[8] extended the work
of Dancer-Du [6], by
assuming the existence of upper and lower solutions for the problem. Zhang-Li
[9] and Zhang et al.
[10] extended the
semilinear work of [7], by carefully constructing a pseudogradient vector
field whose descent flow exhibits the necessary invariance properties. These
works were extended recently by Filippakis-Papageorgiou [11]. Recently the approach based on the invariance
properties of descent flow was used by Zhang-Perera [12] to produce nodal solutions
for certain Kirchhoff type equations. Other recent works dealing with -Laplacian equations are those by Ahmad-Nieto
[13] (monotone
iterative technique), Kim et al. [14] (radial solutions), Lin et al. (singular odes)
[15], and Väth
[16] (degree theoretic
approach).
In this paper using techniques from nonsmooth critical
point theory in conjunction with the method of upper and lower solutions, we
are able to extend the works of Dancer-Du [6] and Carl-Perera [8] to hemivariational inequalities. Helpful in this
respect is the nonsmooth second deformation lemma of Corvellec [17]. Recently, sign-changing
solutions for problems with discontinuous nonlinearities were obtained by
Averna et al. [18], but in contrast to our work they deal with -superlinear problems.
2. Mathematical Background
In our analysis of problem (1.1), we use the nonsmooth
critical point theory which is based on the subdifferential theory for locally
Lipschitz functions and some basic facts about the spectrum of the negative -Laplacian with Dirichlet boundary conditions.
For easy reference, we recall some definitions and results from these areas,
which will be used in the sequel.
We start with the subdifferential theory for locally
Lipschitz functions and the corresponding nonsmooth critical point theory.
Details can be found in the books of Gasiński-Papageorgiou [19] and
Motreanu-Panagiotopoulos [20]. So let be a Banach space and let be its topological dual. By we denote the duality brackets for the pair .
Given a locally Lipschitz function the generalized directional derivative of at in the direction is defined as follows:
The function is sublinear continuous and so it is the
support function of a nonempty, convex, and -compact set defined by
The multifunction is called the “generalized gradient" (or
generalized subdifferential) of If is also convex, then coincides with the subdifferential in the
sense of convex analysis defined by
Moreover if then is locally Lipschitz and
We say that is a critical point of the locally Lipschitz
function if It is easy to see that if is a local extremum of (i.e., a local minimum or a local maximum of ), then is a critical point of .
A locally Lipschitz function satisfies the Palais-Smale condition at level (-condition for short), if every sequence such that and as has a strongly convergent subsequence. We say
that satisfies the -condition, if it satisfies the -condition for every
The following topological notion is crucial in the
minimax characterization of the critical values of a locally Lipschitz
functional Definition 2.1. Let be a Hausdorff topological space and and are nonempty closed subsets of with We say that the pair is linking with in if and only if
(a);(b)for any such that we have
Using this notion, we have the following general
minimax principle for the critical values of a locally Lipschitz function Theorem 2.2. If is a reflexive Banach space, , ,
and are nonempty closed subsets of such that is linking with in is locally Lipschitz, and satisfies the -condition, then and is a critical value of Remark 2.3. From this general minimax
principle, by appropriate choices of the linking sets, one can produce
nonsmooth versions of the mountain pass theorem, of the saddle point theorem,
and of the generalized mountain pass theorem.Definition 2.4. If is a subset of the Banach space a “deformation of ” is a continuous map such that . If ,
then we can say that is a “weak deformation retract of ”, if there exists a deformation such that and for all .
Given a locally Lipschitz function and we define
The next theorem is a partial extension to a nonsmooth
setting of the so-called “second deformation theorem” (see, e.g.,
Gasiński-Papageorgiou [21, page 628]) and it is due to Corvellec [17]. In fact the result of
Corvellec is formulated in the more general context of metric spaces, for
continuous functions using the so-called weak slope. For our purposes, it
suffices to use a particular form of the result which we state next.
Theorem 2.5. If is a Banach space, is locally Lipschitz and satisfies the -condition, has no critical points in and is discrete nonempty, then there exists a
deformation such that
(a) for all (b) (c) for all and all
In particular the set is a weak deformation retract of .
Next let us recall some basic facts about the spectrum
of the negative -Laplacian with Dirichlet boundary conditions.
So let be a bounded domain with a -boundary and . We consider the following nonlinear weighted
(with weight ) eigenvalue problem:
The least number for which problem (2.5) has a nontrivial solution
is the first eigenvalue of and it is denoted by . The first eigenvalue is strictly positive (i.e., ); it is isolated and it is simple (i.e., the
associated eigenspace is one dimensional). Moreover, using the Rayleigh
quotient we have a variational characterization of , namely, (see also Cuccu et al. [22]).
The minimum in (2.6)
is attained on the corresponding
one-dimensional eigenspace. In what follows by we denote the normalized eigenfunction. Note
that also realizes the minimum in (2.6). Hence we
may assume that a.e. on Moreover, from nonlinear regularity theory
(see, e.g., Gasiński-Papageorgiou [21, page 738]), we have The Banach space is an ordered Banach space with order cone
given by
We know that and in fact
By virtue of the strong maximum principle of Vázquez
[23], we have
Using the Lusternik-Schnirelmann theory, in addition
to we obtain a whole strictly increasing sequence of eigenvalues of (2.5), such that as These are the so-called “variational
eigenvalues” of ( ). When (linear case), then these are all the
eigenvalues. For (nonlinear case), we do not know if this is
true. Nevertheless exploiting the fact that is isolated, we can define
Because the set of eigenvalues of (2.5) is closed, we
see that is an eigenvalue of ( In fact we have that is, the second eigenvalue and the second
variational eigenvalue of coincide. Then for we have a variational expression provided by
the Lusternik-Schnirelmann theory. The eigenvalues and exhibit some monotonicity properties with
respect to the weight function More precisely, we have the following.
(a)If a.e. on with strict inequality on a set of positive
measure, then (this is immediate from (2.6).(b) If a.e. on then (see Anane-Tsouli [24]).
If then we write and For there is an alternative variational
characterization, due to Cuesta et al. [25]; namely, if ,
and then
Finally we recall the notions of upper and of lower
solutions for problem (1.1).
(a)A function with is an “upper solution” for problem
(1.1), if for all a.e. on and for some a.e. on for some .(b) A function with is a “lower solution” for problem (1.1),
iffor all a.e. on and for some a.e. on for some .
3. Solutions of Constant Sign
In this section, we produce two nontrivial solutions
of (1.1) which have constant sign. The first is positive and the second is
negative. To do this, we will need the following hypotheses on the nonsmooth
potential .
: is a function such that a.e. on a.e. on ,
and(i)for
every , is measurable;(ii)for
almost all , is locally Lipschitz;(iii)for
almost all all ,
and all we have(iv)there
exists satisfying a.e. on with strict inequality on a set of positive
measure, such that uniformly for almost all and all (v)there
exist satisfying a.e. on where the first inequality is strict on a set
of positive measure, such that uniformly for almost all and all (vi)for
almost all all ,
and all we have (sign condition).Remark 3.1. Hypotheses (iv) and (v) are nonuniform nonresonance conditions at zero
and at ,
respectively. Moreover, as we move from to the “slopes” cross the first eigenvalue So our framework incorporates the so-called
asymptotically -linear equations. For ,
since the appearance of the pioneering work of Amann-Zehnder [26], these problems have
attracted a lot of interest.
The next lemma is an easy consequence of the strict
positivity of and of the hypotheses on (see (iv). We omit the proof.Lemma 3.2. If satisfies a.e. on with strict inequality on a set of positive
measure, then there exists such that
Given and ,
we consider the following nonlinear Dirichlet problem:
In the next proposition, we establish the solvability
of (3.5).Proposition 3.3. If satisfies a.e. on with strict inequality on a set of positive
measure, then for all small problem (3.5) admits a solution Proof. In what
follows by we denote the duality brackets for the pair ). We introduce the nonlinear operator defined by
It is straightforward to check that is strictly monotone and demicontinuous, hence
maximal monotone too. Also let be the nonlinear, bounded, continuous map
defined by
Because of the compact embedding of into , viewed as a map from into is completely continuous. Therefore is pseudomonotone from into Also for every we have
Therefore, if then by virtue of Poincare's inequality is coercive. But a pseudomonotone coercive
operator is surjective. Hence we can find that such that
Thus is a solution of (3.5). We take duality
brackets of (3.9) with the test function We obtain
But recall that So it follows that hence that is, Since from (3.10) it follows that and (nonlinear regularity theory). In addition,
from (3.10), we see that
In fact the solution of (3.5) is an upper solution for problem
(1.1).Proposition 3.4. If hypotheses (i)→(iv) hold and is small, then the solution of problem (3.5) obtained in Proposition 3.3
is a strict upper solution of problem (1.1) (strict means that is an upper solution of (1.1) which is not a
solution).Proof. Because
of hypotheses (iv), given we can find such that for almost all all ,
and all we have
Also due to hypothesis (iii), we can find such that for almost all all ,
and all we have
Therefore it follows that for almost all all ,
and all we have
So for and as above, we consider problem (3.5). From
Proposition 3.3, we have a solution Then due to (3.15), for all with a.e. on we have
Since a.e. on is a lower solution for problem (1.1).
We introduce the set
and the truncation function defined by
Then we set and we consider the locally Lipschitz
functional defined by
We will show that we can find a nontrivial solution of
(1.1) in which is a local minimizer of and of To do this we will need the following simple
result about ordered Banach spaces.Lemma 3.5. If is an ordered Banach space, is the order cone of ,
and then for every we can find such that Proof. Since we can find such that
Let (if then clearly the lemma holds for all ). We have the following:
So, if then
Using this lemma, we can prove the following
result.Proposition 3.6. If hypotheses hold, then there exists which is a local minimizer of and of Proof. From
(3.15), we know that given we can find such that
Because of hypotheses (i), (ii), for almost all is almost everywhere differentiable on (Rademacher's theorem) and at every point of
differentiability we have
Integrating this inequality and since for almost all we obtain
Then for every we have
Choosing because from (3.25) and Poincare's inequality, we infer
that is coercive. Also it is easy to see that is weakly lower semicontinuous on Hence by virtue of the theorem of Weierstrass,
we can find such that
First we show that To this end, note that hypothesis (v) implies that given we can find such that
As before, integrating (3.27), we
obtain
We know that (see Proposition 3.3). So using Lemma 3.5, we
can find small such that
Then, because of (3.28), we have
Let Using the hypothesis on (see (v) and the fact that for all we see that So, if we choose we have
Note that for small, Hence
Given any we define Then is Lipschitz continuous, hence differentiable
almost everywhere and for all From Chang [27, page 106], we know that we can find a.e. on such that
For any and we define
Clearly We use this