Boundary Value Problems
VolumeΒ 2009Β (2009), Article IDΒ 820237, 32 pages
doi:10.1155/2009/820237
Research Article

Constant Sign and Nodal Solutions for Problems with the 𝑝 -Laplacian and a Nonsmooth Potential Using Variational Techniques

1Department of Mathematical Sciences, Florida Institute of Technology, Melbourne, FL 32901-6975, USA
2Department of Mathematics, Hellenic Army Academy, Vari, 16673 Athens, Greece
3Department of Mathematics, National University of Ireland, Galway, Ireland
4Department of Mathematics, National Technical University, Zografou Campus, 15780 Athens, Greece

Received 10 December 2008; Revised 21 January 2009; Accepted 23 January 2009

Academic Editor: Juan J.Β Nieto

Copyright Β© 2009 Ravi P. Agarwal et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

We consider a nonlinear elliptic equation driven by the 𝑝 -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 𝑝 -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 𝑝 -Laplacian and having a nonsmooth potential (hemivariational inequalities). So let 𝑍 βŠ† ℝ β„• be a bounded domain with a 𝐢 2 -boundary πœ• 𝑍 . The problem under consideration is the following:

Here image/svg+xml𝑗(𝑧,π‘₯) is measurable function on 𝑍 Γ— ℝ , which in the π‘₯ ∈ ℝ variable is locally Lipschitz and πœ• 𝑗 ( 𝑧 , π‘₯ ) stands for the generalized subdifferential of π‘₯ β†’ 𝑗 ( 𝑧 , π‘₯ ) 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 𝑝 -Laplacian and with a 𝐢 1 -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 πœ† ∈ ℝ . The question of existence of nodal solutions was first addressed within the framework of semilinear problems (i.e., 𝑝 = 2 ). 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 𝐢 1 0 ( 𝑍 ) . Recently these methods were extended to “smooth” problems driven by the 𝑝 -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 𝑝 -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 𝑝 -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 𝑝 -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 𝑋 be a Banach space and let 𝑋 βˆ— be its topological dual. By ⟨ β‹… , β‹… ⟩ we denote the duality brackets for the pair ( 𝑋 , 𝑋 βˆ— ) . Given a locally Lipschitz function πœ‘ ∢ 𝑋 β†’ ℝ , the generalized directional derivative πœ‘ 0 ( π‘₯ ; β„Ž ) of πœ‘ at π‘₯ ∈ 𝑋 in the direction β„Ž ∈ 𝑋 is defined as follows:

The function β„Ž β†’ πœ‘ 0 ( π‘₯ ; β„Ž ) is sublinear continuous and so it is the support function of a nonempty, convex, and 𝑀 βˆ— -compact set πœ• πœ‘ ( π‘₯ ) βŠ† 𝑋 βˆ— defined by

The multifunction π‘₯ β†’ πœ• πœ‘ ( π‘₯ ) is called the “generalized gradient" (or generalized subdifferential) of πœ‘ . If πœ‘ ∢ 𝑋 β†’ ℝ is also convex, then πœ• πœ‘ ( π‘₯ ) coincides with the subdifferential in the sense of convex analysis πœ• 𝑐 πœ‘ ( π‘₯ ) , defined by

Moreover if πœ‘ ∈ 𝐢 1 ( 𝑋 ) , then πœ‘ is locally Lipschitz and πœ• πœ‘ ( π‘₯ ) = { πœ‘ ξ…ž ( π‘₯ ) } .

We say that π‘₯ ∈ 𝑋 is a critical point of the locally Lipschitz function πœ‘ ∢ 𝑋 β†’ ℝ , if 0 ∈ πœ• πœ‘ ( π‘₯ ) . It is easy to see that if π‘₯ ∈ 𝑋 is a local extremum of πœ‘ (i.e., a local minimum or a local maximum of πœ‘ ), then π‘₯ ∈ 𝑋 is a critical point of πœ‘ .

A locally Lipschitz function πœ‘ ∢ 𝑋 β†’ ℝ satisfies the Palais-Smale condition at level 𝑐 ∈ ℝ ( 𝑃 𝑆 𝑐 -condition for short), if every sequence { π‘₯ 𝑛 } 𝑛 β‰₯ 1 βŠ† 𝑋 such that πœ‘ ( π‘₯ 𝑛 ) β†’ 𝑐 and π‘š ( π‘₯ 𝑛 ) = i n f { β€– π‘₯ βˆ— β€– ∢ π‘₯ βˆ— ∈ πœ• πœ‘ ( π‘₯ 𝑛 ) } β†’ 0 as 𝑛 β†’ ∞ has a strongly convergent subsequence. We say that πœ‘ satisfies the 𝑃 𝑆 -condition, if it satisfies the 𝑃 𝑆 𝑐 -condition for every 𝑐 ∈ ℝ .

The following topological notion is crucial in the minimax characterization of the critical values of a locally Lipschitz functional πœ‘ ∢ 𝑋 β†’ ℝ . Definition 2.1. Let π‘Œ be a Hausdorff topological space and 𝐸 0 , 𝐸 , and 𝐷 are nonempty closed subsets of π‘Œ with 𝐸 0 βŠ† 𝐸 . We say that the pair { 𝐸 0 , 𝐸 } is linking with 𝐷 in π‘Œ if and only if
(a) 𝐸 0 ∩ 𝐷 = βˆ… ;(b)for any 𝛾 ∈ 𝐢 ( 𝐸 , π‘Œ ) such that 𝛾 | 𝐸 0 = 𝑖 𝑑 | 𝐸 0 , we have 𝛾 ( 𝐸 ) ∩ 𝐷 β‰  βˆ… .

Using this notion, we have the following general minimax principle for the critical values of a locally Lipschitz function πœ‘ ∢ 𝑋 β†’ ℝ . Theorem 2.2. If 𝑋 is a reflexive Banach space, 𝐸 0 , 𝐸 , and 𝐷 are nonempty closed subsets of 𝑋 such that { 𝐸 0 , 𝐸 } is linking with 𝐷 in 𝑋 , πœ‘ ∢ 𝑋 β†’ ℝ is locally Lipschitz, image/svg+xmlsup 𝐸 0 πœ‘<inf 𝐷 πœ‘,Ξ“={π›ΎβˆˆπΆ(𝐸,𝑋)βˆΆπ›Ύ| 𝐸 0 =𝑖𝑑| 𝐸 0 }, image/svg+xml𝑐=inf π›ΎβˆˆΞ“ sup π‘£βˆˆπΈ πœ‘(𝛾(𝑣)), and image/svg+xmlπœ‘ satisfies the image/svg+xml𝑃𝑆 𝑐 -condition, then image/svg+xml𝑐β‰₯inf 𝐷 πœ‘ and image/svg+xml𝑐 is a critical value of image/svg+xmlπœ‘. 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 image/svg+xmlπ‘Œ is a subset of the Banach space image/svg+xml𝑋, a “deformation of image/svg+xmlπ‘Œ ” is a continuous map image/svg+xmlβ„ŽβˆΆ[0,1]Γ—π‘Œβ†’π‘Œ such that image/svg+xmlβ„Ž(0,β‹…)=𝑖𝑑 π‘Œ . If image/svg+xmlπ‘‰βŠ†π‘Œ , then we can say that 𝑉 is a “weak deformation retract of π‘Œ ”, if there exists a deformation β„Ž ∢ [ 0 , 1 ] Γ— π‘Œ β†’ π‘Œ such that β„Ž ( 1 , π‘Œ ) βŠ† 𝑉 and β„Ž ( 𝑑 , β‹… ) βŠ† 𝑉 for all 𝑑 ∈ [ 0 , 1 ] .

Given a locally Lipschitz function πœ‘ ∢ 𝑋 β†’ ℝ and 𝑐 ∈ ℝ , 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 𝑋 is a Banach space, πœ‘ ∢ 𝑋 β†’ ℝ is locally Lipschitz and satisfies the 𝑃 𝑆 -condition, π‘Ž ∈ ℝ , 𝑏 ∈ ℝ βˆͺ { + ∞ } , πœ‘ has no critical points in πœ‘ βˆ’ 1 ( π‘Ž , 𝑏 ) , and 𝐾 π‘Ž is discrete nonempty, then there exists a deformation β„Ž ∢ [ 0 , 1 ] Γ— 0 πœ‘ 𝑏 β†’ 0 πœ‘ 𝑏 such that
(a) β„Ž ( 𝑑 , β‹… ) | 𝐾 π‘Ž = 𝑖 𝑑 for all 𝑑 ∈ [ 0 , 1 ] ; (b) β„Ž ( 1 , 0 πœ‘ 𝑏 ) βŠ† 0 πœ‘ π‘Ž βˆͺ 𝐾 π‘Ž ; (c) πœ‘ ( β„Ž ( 𝑑 , π‘₯ ) ) ≀ πœ‘ ( π‘₯ ) for all 𝑑 ∈ [ 0 , 1 ] and all π‘₯ ∈ 0 πœ‘ 𝑏 .

In particular the set 0 πœ‘ π‘Ž βˆͺ 𝐾 π‘Ž is a weak deformation retract of 0 πœ‘ 𝑏 .

Next let us recall some basic facts about the spectrum of the negative 𝑝 -Laplacian with Dirichlet boundary conditions. So let 𝑍 βŠ† ℝ β„• be a bounded domain with a 𝐢 2 -boundary πœ• 𝑍 and π‘š ∈ 𝐿 ∞ ( 𝑍 ) + , π‘š β‰  0 . We consider the following nonlinear weighted (with weight π‘š ) eigenvalue problem:

The least number Μ‚ πœ† ∈ ℝ for which problem (2.5) has a nontrivial solution is the first eigenvalue of ( βˆ’ Ξ” 𝑝 , π‘Š 0 1 , 𝑝 ( 𝑍 ) , π‘š ) and it is denoted by Μ‚ πœ† 1 ( π‘š ) . The first eigenvalue Μ‚ πœ† 1 ( π‘š ) is strictly positive (i.e., Μ‚ πœ† 1 ( π‘š ) > 0 ); 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 Μ‚ πœ† 1 ( π‘š ) , namely, (see also Cuccu et al. [22]).

The minimum in (2.6) is attained on the corresponding one-dimensional eigenspace. In what follows by 𝑒 1 ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) we denote the normalized eigenfunction. Note that | 𝑒 1 | also realizes the minimum in (2.6). Hence we may assume that 𝑒 1 ( 𝑧 ) β‰₯ 0 a.e. on 𝑍 . Moreover, from nonlinear regularity theory (see, e.g., Gasiński-Papageorgiou [21, page 738]), we have 𝑒 1 ∈ 𝐢 1 0 ( 𝑍 ) = { π‘₯ ∈ 𝐢 1 ( 𝑍 ) ∢ π‘₯ ( 𝑧 ) = 0 f o r a l l 𝑧 ∈ πœ• 𝑍 } . The Banach space 𝐢 1 0 ( 𝑍 ) is an ordered Banach space with order cone given by

We know that i n t 𝐢 1 0 ( 𝑍 ) + β‰  βˆ… and in fact

By virtue of the strong maximum principle of Vázquez [23], we have 𝑒 1 ∈ i n t 𝐢 1 0 ( 𝑍 ) + .

Using the Lusternik-Schnirelmann theory, in addition to Μ‚ πœ† 1 ( π‘š ) > 0 , we obtain a whole strictly increasing sequence { Μ‚ πœ† π‘˜ ( π‘š ) } π‘˜ β‰₯ 1 βŠ† ℝ + of eigenvalues of (2.5), such that Μ‚ πœ† π‘˜ ( π‘š ) β†’ + ∞ as π‘˜ β†’ ∞ . These are the so-called “variational eigenvalues” of ( βˆ’ Ξ” 𝑝 , π‘Š 0 1 , 𝑝 ( 𝑍 ) , π‘š ). When 𝑝 = 2 (linear case), then these are all the eigenvalues. For 𝑝 β‰  2 (nonlinear case), we do not know if this is true. Nevertheless exploiting the fact that Μ‚ πœ† 1 ( π‘š ) > 0 is isolated, we can define

Because the set of eigenvalues of (2.5) is closed, we see that Μ‚ πœ† βˆ— 2 ( π‘š ) is an eigenvalue of ( βˆ’ Ξ” 𝑝 , π‘Š 0 1 , 𝑝 ( 𝑍 ) , π‘š ) . In fact we have Μ‚ πœ† βˆ— 2 Μ‚ πœ† ( π‘š ) = 2 ( π‘š ) ; that is, the second eigenvalue and the second variational eigenvalue of ( βˆ’ Ξ” 𝑝 , π‘Š 0 1 , 𝑝 ( 𝑍 ) , π‘š ) coincide. Then for Μ‚ πœ† 2 ( π‘š ) we have a variational expression provided by the Lusternik-Schnirelmann theory. The eigenvalues Μ‚ πœ† 1 ( π‘š ) and Μ‚ πœ† 2 ( π‘š ) exhibit some monotonicity properties with respect to the weight function π‘š ∈ 𝐿 ∞ ( 𝑍 ) + . More precisely, we have the following.

(a)If π‘š ( 𝑧 ) ≀ π‘š ξ…ž ( 𝑧 ) a.e. on 𝑍 with strict inequality on a set of positive measure, then Μ‚ πœ† 1 ( π‘š ξ…ž Μ‚ πœ† ) < 1 ( π‘š ) (this is immediate from (2.6).(b) If π‘š ( 𝑧 ) < π‘š ξ…ž ( 𝑧 ) a.e. on 𝑍 , then Μ‚ πœ† 2 ( π‘š ξ…ž Μ‚ πœ† ) < 2 ( π‘š ) (see Anane-Tsouli [24]).

If π‘š ≑ 1 , then we write Μ‚ πœ† 1 ( π‘š ) = πœ† 1 and Μ‚ πœ† 2 ( π‘š ) = πœ† 2 . For πœ† 2 > 0 , there is an alternative variational characterization, due to Cuesta et al. [25]; namely, if πœ• 𝐡 𝐿 𝑝 1 ( 𝑍 ) = { π‘₯ ∈ 𝐿 𝑝 ( 𝑍 ) ∢ β€– π‘₯ β€– 𝑝 = 1 } , 𝑆 = π‘Š 0 1 , 𝑝 ( 𝑍 ) ∩ πœ• 𝐡 𝐿 𝑝 1 ( 𝑍 ) , and Ξ“ 0 = { 𝛾 0 ∈ 𝐢 ( [ βˆ’ 1 , 1 ] , 𝑆 ) ∢ 𝛾 0 ( βˆ’ 1 ) = βˆ’ 𝑒 1 , 𝛾 0 ( 1 ) = 𝑒 1 } , then

Finally we recall the notions of upper and of lower solutions for problem (1.1).

(a)A function π‘₯ ∈ π‘Š 1 , 𝑝 ( 𝑍 ) with π‘₯ | πœ• 𝑍 β‰₯ 0 is an “upper solution” for problem (1.1), if for all πœ“ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) , πœ“ ( 𝑧 ) β‰₯ 0 a.e. on 𝑍 and for some 𝑒 ∈ 𝐿 πœ‚ ( 𝑍 ) , 𝑒 ( 𝑧 ) ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ( 𝑧 ) ) a.e. on 𝑍 for some 1 < πœ‚ < 𝑝 βˆ— = 𝑁 𝑝 / ( 𝑁 βˆ’ 𝑝 ) i f 𝑁 > 𝑝 , + ∞ i f 𝑁 ≀ 𝑝 .(b) A function π‘₯ ∈ π‘Š 1 , 𝑝 ( 𝑍 ) with π‘₯ | πœ• 𝑍 ≀ 0 is a “lower solution” for problem (1.1), iffor all πœ“ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) , πœ“ ( 𝑧 ) β‰₯ 0 a.e. on 𝑍 and for some 𝑒 ∈ 𝐿 πœ‚ ( 𝑍 ) , 𝑒 ( 𝑧 ) ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ( 𝑧 ) ) a.e. on 𝑍 for some 1 < πœ‚ < 𝑝 βˆ— .

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 𝑗 ( 𝑧 , π‘₯ ) .

𝐻 ( 𝑗 ) 1 : 𝑗 ∢ 𝑍 Γ— ℝ β†’ ℝ is a function such that 𝑗 ( 𝑧 , 0 ) = 0 a.e. on 𝑍 , πœ• 𝑗 ( 𝑧 , 0 ) = { 0 } a.e. on 𝑍 , and(i)for every π‘₯ ∈ ℝ , 𝑧 β†’ 𝑗 ( 𝑧 , π‘₯ ) is measurable;(ii)for almost all 𝑧 ∈ 𝑍 , π‘₯ β†’ 𝑗 ( 𝑧 , π‘₯ ) is locally Lipschitz;(iii)for almost all 𝑧 ∈ 𝑍 , all π‘₯ ∈ ℝ , and all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) , we have(iv)there exists πœƒ ∈ 𝐿 ∞ ( 𝑍 ) + satisfying πœƒ ( 𝑧 ) ≀ πœ† 1 a.e. on 𝑍 with strict inequality on a set of positive measure, such that uniformly for almost all 𝑧 ∈ 𝑍 and all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) ; (v)there exist πœ‚ , Μ‚ πœ‚ ∈ 𝐿 ∞ ( 𝑍 ) + satisfying πœ† 1 ≀ πœ‚ ( 𝑧 ) ≀ Μ‚ πœ‚ ( 𝑧 ) a.e. on 𝑍 , where the first inequality is strict on a set of positive measure, such that uniformly for almost all 𝑧 ∈ 𝑍 and all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) ; (vi)for almost all 𝑧 ∈ 𝑍 , all π‘₯ ∈ ℝ , and all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) , we have 𝑒 π‘₯ β‰₯ 0 (sign condition).Remark 3.1. Hypotheses 𝐻 ( 𝑗 ) 1 (iv) and (v) are nonuniform nonresonance conditions at zero and at Β± ∞ , respectively. Moreover, as we move from 0 to Β± ∞ , the “slopes” 𝑒 / | π‘₯ | 𝑝 βˆ’ 2 π‘₯ . 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) cross the first eigenvalue πœ† 1 > 0 . So our framework incorporates the so-called asymptotically 𝑝 -linear equations. For 𝑝 = 2 , 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 𝑒 1 ∈ 𝐢 1 0 ( 𝑍 ) and of the hypotheses on πœƒ ∈ 𝐿 ∞ ( 𝑍 ) + (see 𝐻 ( 𝑗 ) (iv). We omit the proof.Lemma 3.2. If πœƒ ∈ 𝐿 ∞ ( 𝑍 ) + satisfies πœƒ ( 𝑧 ) ≀ πœ† 1 a.e. on 𝑍 with strict inequality on a set of positive measure, then there exists πœ‰ 0 > 0 such that

Given πœ€ > 0 and 𝛾 πœ€ ∈ 𝐿 ∞ ( 𝑍 ) + , 𝛾 πœ€ β‰  0 , we consider the following nonlinear Dirichlet problem:

In the next proposition, we establish the solvability of (3.5).Proposition 3.3. If πœƒ ∈ 𝐿 ∞ ( 𝑍 ) + satisfies πœƒ ≀ πœ† 1 a.e. on 𝑍 with strict inequality on a set of positive measure, then for all πœ€ > 0 small problem (3.5) admits a solution π‘₯ ∈ i n t 𝐢 1 0 ( 𝑍 ) + . Proof. In what follows by ⟨ β‹… , β‹… ⟩ we denote the duality brackets for the pair ( π‘Š βˆ’ 1 , 𝑝 β€² ( 𝑍 ) , π‘Š 0 1 , 𝑝 ( 𝑍 ) ) ( 1 / 𝑝 + 1 / 𝑝 ξ…ž = 1 ). We introduce the nonlinear operator 𝐴 ∢ π‘Š 0 1 , 𝑝 ( 𝑍 ) β†’ π‘Š βˆ’ 1 , 𝑝 β€² ( 𝑍 ) defined by
It is straightforward to check that 𝐴 is strictly monotone and demicontinuous, hence maximal monotone too. Also let 𝑁 πœ€ ∢ 𝐿 𝑝 ( 𝑍 ) β†’ 𝐿 𝑝 β€² ( 𝑍 ) be the nonlinear, bounded, continuous map defined by
Because of the compact embedding of π‘Š 0 1 , 𝑝 ( 𝑍 ) into 𝐿 𝑝 ( 𝑍 ) , 𝑁 πœ€ viewed as a map from π‘Š 0 1 , 𝑝 ( 𝑍 ) into 𝐿 𝑝 β€² ( 𝑍 ) is completely continuous. Therefore π‘₯ β†’ 𝐺 πœ€ ( π‘₯ ) = 𝐴 ( π‘₯ ) βˆ’ 𝑁 πœ€ ( π‘₯ ) is pseudomonotone from π‘Š 0 1 , 𝑝 ( 𝑍 ) into π‘Š βˆ’ 1 , 𝑝 β€² ( 𝑍 ) . Also for every π‘₯ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) , we have
Therefore, if πœ€ < πœ† 1 πœ‰ 0 , then by virtue of Poincare's inequality 𝐺 πœ€ ( β‹… ) is coercive. But a pseudomonotone coercive operator is surjective. Hence we can find that π‘₯ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) such that
Thus βˆ’ π‘₯ βˆ’ = βˆ’ m a x { βˆ’ π‘₯ , 0 } ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) . is a solution of (3.5). We take duality brackets of (3.9) with the test function β€– 𝐷 π‘₯ βˆ’ β€– 𝑝 𝑝 βˆ’ ξ€œ 𝑍 πœƒ ( 𝑧 ) | π‘₯ βˆ’ ( 𝑧 ) | 𝑝 𝑑 𝑧 ≀ πœ€ β€– π‘₯ βˆ’ β€– 𝑝 𝑝 ξ€· s i n c e 𝛾 πœ€ ξ€Έ , β‰₯ 0 ⟹ πœ‰ 0 β€– 𝐷 π‘₯ βˆ’ β€– 𝑝 𝑝 ≀ πœ€ πœ† 1 β€– 𝐷 π‘₯ βˆ’ β€– 𝑝 𝑝 ( s e e L e m m a 3 . 2 a n d ( 2 . 6 ) ) . ( 3 . 1 1 ) We obtain
But recall that β€– 𝐷 π‘₯ βˆ’ β€– 𝑝 = 0 , So it follows that π‘₯ βˆ’ = 0 ; hence π‘₯ β‰₯ 0 . that is, 𝛾 πœ€ β‰  0 , Since π‘₯ β‰  0 from (3.10) it follows that π‘₯ ∈ 𝐢 1 0 ( 𝑍 ) and d i v ξ€· β€– 𝐷 π‘₯ ( 𝑧 ) β€– 𝑝 βˆ’ 2 𝐷 ξ€Έ π‘₯ ( 𝑧 ) ≀ 0 a . e . o n ⟹ 𝑍 , π‘₯ ∈ i n t 𝐢 1 0 ( 𝑍 ) + ( s e e V Γ‘ z q u e z [ 2 3 ] ) . ( 3 . 1 2 ) (nonlinear regularity theory). In addition, from (3.10), we see that

In fact the solution 𝐻 ( 𝑗 ) 1 of (3.5) is an upper solution for problem (1.1).Proposition 3.4. If hypotheses πœ€ > 0 (i)→(iv) hold and π‘₯ ∈ 𝑖 𝑛 𝑑 𝐢 1 0 ( 𝑍 ) + is small, then the solution π‘₯ of problem (3.5) obtained in Proposition 3.3 is a strict upper solution of problem (1.1) (strict means that 𝐻 ( 𝑗 ) 1 is an upper solution of (1.1) which is not a solution).Proof. Because of hypotheses πœ€ > 0 , (iv), given 𝑀 1 = 𝑀 1 ( πœ€ ) > 0 we can find 𝑧 ∈ 𝑍 , such that for almost all π‘₯ β‰₯ 𝑀 1 all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) , , and all 𝑒 ≀ ( πœƒ ( 𝑧 ) + πœ€ ) π‘₯ 𝑝 βˆ’ 1 . ( 3 . 1 3 ) we have
Also due to hypothesis 𝛾 πœ€ ∈ 𝐿 ∞ ( 𝑍 ) + , 𝛾 πœ€ β‰  0 (iii), we can find 𝑧 ∈ 𝑍 , such that for almost all π‘₯ ∈ [ 0 , 𝑀 1 ] all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) , , and all 𝑒 < 𝛾 πœ€ ( 𝑧 ) . ( 3 . 1 4 ) we have
Therefore it follows that for almost all π‘₯ β‰₯ 0 all 𝑒 ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ) , , and all 𝑒 < ( πœƒ ( 𝑧 ) + πœ€ ) π‘₯ 𝑝 βˆ’ 1 + 𝛾 πœ€ ( 𝑧 ) . ( 3 . 1 5 ) we have
So for 𝛾 πœ€ and π‘₯ ∈ i n t 𝐢 1 0 ( 𝑍 ) + . as above, we consider problem (3.5). From Proposition 3.3, we have a solution 𝑒 ∈ 𝐿 𝑝 β€² ( 𝑍 ) + Then due to (3.15), for all 𝑒 ( 𝑧 ) ∈ πœ• 𝑗 ( 𝑧 , π‘₯ ( 𝑧 ) ) with 𝑍 , a.e. on 𝑒 ( 𝑧 ) < ( πœƒ ( 𝑧 ) + πœ€ ) π‘₯ ( 𝑧 ) 𝑝 βˆ’ 1 + 𝛾 πœ€ ( 𝑧 ) a . e . o n ⟹ 𝑍 , π‘₯ ∈ i n t 𝐢 1 0 ( 𝑍 ) + i s a s t r i c t u p p e r s o l u t i o n f o r p r o b l e m ( 1 . 1 ) . ( 3 . 1 6 ) we have

Since 𝑍 , π‘₯ ≑ 0 a.e. on 𝐢 = { π‘₯ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) ∢ 0 ≀ π‘₯ ( 𝑧 ) ≀ π‘₯ ( 𝑧 ) a . e . o n 𝑍 } ( 3 . 1 7 ) is a lower solution for problem (1.1).

We introduce the set

and the truncation function 𝜏 + ξƒ― 0 ( π‘₯ ) = i f π‘₯ π‘₯ ≀ 0 , i f π‘₯ > 0 . ( 3 . 1 8 ) defined by

Then we set πœ‘ + ∢ π‘Š 0 1 , 𝑝 ( 𝑍 ) β†’ ℝ and we consider the locally Lipschitz functional πœ‘ + 1 ( π‘₯ ) = 𝑝 β€– 𝐷 π‘₯ β€– 𝑝 𝑝 βˆ’ ξ€œ 𝑍 𝑗 + ( 𝑧 , π‘₯ ( 𝑧 ) ) 𝑑 𝑧 βˆ€ π‘₯ ∈ π‘Š 0 1 , 𝑝 ( 𝑍 ) . ( 3 . 1 9 ) defined by

We will show that we can find a nontrivial solution of (1.1) in πœ‘ + which is a local minimizer of πœ‘ . and of 𝑋 To do this we will need the following simple result about ordered Banach spaces.Lemma 3.5. If 𝐾 is an ordered Banach space, 𝑋 , i n t 𝐾 β‰  βˆ… is the order cone of π‘₯ 0 ∈ i n t 𝐾 , , and 𝑦 ∈ 𝑋 , then for every 𝑑 = 𝑑 ( 𝑦 ) > 0 we can find 𝑑 π‘₯ 0 βˆ’ 𝑦 ∈ i n t 𝐾 . such that π‘₯ 0 ∈ i n t 𝐾 , Proof. Since 𝛿 > 0 we can find 𝐡 𝛿 ( π‘₯ 0 ξ€½ ) = π‘₯ ∈ 𝑋 ∢ β€– π‘₯ βˆ’ π‘₯ 0 ξ€Ύ βŠ† β€– ≀ 𝛿 i n t 𝐾 . ( 3 . 2 0 ) such that
Let 𝑦 = 0 , (if 𝑑 > 0 then clearly the lemma holds for all π‘₯ 0 𝑦 βˆ’ 𝛿 ∈ β€– 𝑦 β€– i n t ⟹ 𝐾 , β€– 𝑦 β€– 𝛿 π‘₯ 0 βˆ’ 𝑦 ∈ i n t 𝐾 . ( 3 . 2 1 ) ). We have the following:
So, if 𝑑 π‘₯ 0 βˆ’ 𝑦 ∈ i n t 𝐾 . then 𝐻 ( 𝑗 ) 1

Using this lemma, we can prove the following result.Proposition 3.6. If hypotheses π‘₯ 0 ∈ 𝐢 hold, then there exists πœ‘ + which is a local minimizer of πœ‘ . and of πœ€ > 0 , Proof. From (3.15), we know that given 𝛾 πœ€ ∈ 𝐿 ∞ ( 𝑍 ) + , 𝛾 πœ€ β‰  0 we can find 𝑒 < ( πœƒ ( 𝑧 ) + πœ€ ) π‘₯ 𝑝 βˆ’ 1 + 𝛾 πœ€ ( 𝑧 ) f o r a . a . 𝑧 ∈ 𝑍 , a l l π‘₯ β‰₯ 0 , a n d a l l 𝑒 ∈ πœ• 𝑗 + ( 𝑧 , π‘₯ ) = πœ• 𝑗 ( 𝑧 , π‘₯ ) . ( 3 . 2 2 ) such that
Because of hypotheses 𝑧 ∈ 𝑍 , π‘₯ β†’ 𝑗 + ( 𝑧 , π‘₯ ) (i), (ii), for almost all ℝ is almost everywhere differentiable on 𝑑 𝑗 𝑑 π‘₯ + ( 𝑧 , π‘₯ ) ∈ πœ• 𝑗 + ⟹ 𝑑 ( 𝑧 , π‘₯ ) , 𝑗 𝑑 π‘₯ + ( 𝑧 , π‘₯ ) < ( πœƒ ( 𝑧 ) + πœ€ ) π‘₯ 𝑝 βˆ’ 1 + 𝛾 πœ€ ( 𝑧 ) f o r a . a . 𝑧 ∈ 𝑍 , a l l π‘₯ β‰₯ 0 ( s e e ( 3 . 2 2 ) ) . ( 3 . 2 3 ) (Rademacher's theorem) and at every point of differentiability we have
Integrating this inequality and since 𝑧 ∈ 𝑍 , for almost all 𝑗 + 1 ( 𝑧 , π‘₯ ) < 𝑝 ( πœƒ ( 𝑧 ) + πœ€ ) | π‘₯ | 𝑝 + 𝛾 πœ€ ( 𝑧 ) | π‘₯ | f o r a . a . 𝑧 ∈ 𝑍 , a l l π‘₯ ∈ ℝ . ( 3 . 2 4 ) we obtain
Then for every πœ‘ + 1 ( π‘₯ ) = 𝑝 β€– 𝐷 π‘₯ β€– 𝑝 𝑝 βˆ’ ξ€œ 𝑍 𝑗 + > 1 ( 𝑧 , π‘₯ ( 𝑧 ) ) 𝑑 𝑧 𝑝 β€– 𝐷 π‘₯ β€– 𝑝 𝑝 βˆ’ 1 𝑝 ξ€œ 𝑍 πœƒ ( 𝑧 ) | π‘₯ ( 𝑧 ) | 𝑝 πœ€ 𝑑 𝑧 βˆ’ 𝑝 β€– π‘₯ β€– 𝑝 𝑝 βˆ’ 𝑐 1 β€– 𝐷 π‘₯ β€– 𝑝 f o r s o m e 𝑐 1 > 0 ( s e e β‰₯ 1 ( 3 . 2 4 ) ) 𝑝 ξ‚€ πœ‰ 0 βˆ’ πœ€ πœ† 1  β€– 𝐷 π‘₯ β€– 𝑝 𝑝 βˆ’ 𝑐 1 β€– 𝐷 π‘₯ β€– 𝑝 ( s e e L e m m a 3 . 2 ) . ( 3 . 2 5 ) we have
Choosing 𝑝 > 1 , because πœ‘ + from (3.25) and Poincare's inequality, we infer that πœ‘ + is coercive. Also it is easy to see that π‘Š 0 1 , 𝑝 ( 𝑍 ) . is weakly lower semicontinuous on π‘₯ 0 ∈ 𝐢 Hence by virtue of the theorem of Weierstrass, we can find πœ‘ + ( π‘₯ 0 ) = i n f 𝐢 πœ‘ + . ( 3 . 2 6 ) such that
First we show that 𝐻 ( 𝑗 ) 1 To this end, note that hypothesis πœ€ > 0 , (v) implies that given 𝛿 = 𝛿 ( πœ€ ) > 0 we can find 𝑒 β‰₯ ( πœ‚ ( 𝑧 ) βˆ’ πœ€ ) π‘₯ 𝑝 βˆ’ 1 f o r a . a . 𝑧 ∈ 𝑍 , a l l π‘₯ ∈ [ 0 , 𝛿 ] a n d a l l 𝑒 ∈ πœ• 𝑗 + ( 𝑧 , π‘₯ ) = πœ• 𝑗 ( 𝑧 , π‘₯ ) . ( 3 . 2 7 ) such that
As before, integrating (3.27), we obtain
We know that πœ‡ > 0 (see Proposition 3.3). So using Lemma 3.5, we can find πœ‡ 𝑒 1 ( 𝑧 ) ≀ m i n { π‘₯ ( 𝑧 ) , 𝛿 } βˆ€ 𝑧 ∈ 𝑍 . ( 3 . 2 9 ) small such that
Then, because of (3.28), we have
Let πœ‚ Using the hypothesis on 𝐻 ( 𝑗 ) 1 (see 𝑒 1 ( 𝑧 ) > 0 (v) and the fact that 𝑧 ∈ 𝑍 , for all 𝜎 < 0 . we see that πœ€ < βˆ’ 𝜎 / β€– 𝑒 1 β€– 𝑝 𝑝 , So, if we choose πœ‘ + ξ€· πœ‡ 𝑒 1 ξ€Έ < 0 βˆ€ πœ‡ > 0 s m a l l . ( 3 . 3 1 ) we have
Note that for πœ‡ 𝑒 1 ∈ 𝐢 . small, πœ‘ + ξ€· π‘₯ 0 ξ€Έ = i n f 𝐢 πœ‘ + ≀ πœ‘ + ξ€· πœ‡ 𝑒 1 ξ€Έ < 0 = πœ‘ + ( 0 ) ( s e e ( 3 . 3 1 ) ) , ⟹ π‘₯ 0 β‰  0 , π‘₯ 0 ∈ 𝐢 . ( 3 . 3 2 ) Hence
Given any π‘˜ 0 ( 𝑑 ) = πœ‘ + ( 𝑑 𝑦 + ( 1 βˆ’ 𝑑 ) π‘₯ 0 ) , 𝑑 ∈ [ 0 , 1 ] . we define π‘˜ Then π‘˜ 0 ( 0 ) ≀ π‘˜ 0 ( 𝑑 ) is Lipschitz continuous, hence differentiable almost everywhere and 𝑑 ∈ [ 0 , 1 ] . for all 𝑒 ∈ 𝐿 𝑝 β€² ( 𝑍 ) , 𝑒 ( 𝑧 ) ∈ πœ• 𝑗 + ( 𝑧 , π‘₯ 0 ( 𝑧 ) ) = πœ• 𝑗 ( 𝑧 , π‘₯ 0 ( 𝑧 ) ) From Chang [27, page 106], we know that we can find 𝑍 , a.e. on ξ€· π‘₯ 0 ≀ ⟨ 𝐴 0 ξ€Έ , 𝑦 βˆ’ π‘₯ 0 ξ€œ ⟩ βˆ’ 𝑍 ξ€· 𝑒 ( 𝑧 ) 𝑦 βˆ’ π‘₯ 0 ξ€Έ ( 𝑧 ) 𝑑 𝑧 , βˆ€ 𝑦 ∈ 𝐢 . ( 3 . 3 3 ) such that
For any πœ€ > 0 , and ⎧ βŽͺ ⎨ βŽͺ ⎩ 0 𝑦 ( 𝑧 ) = i f ξ€½ π‘₯ 𝑧 ∈ 0 ξ€Ύ , π‘₯ + πœ€ 𝑣 ≀ 0 0 ( 𝑧 ) + πœ€ 𝑣 ( 𝑧 ) i f ξ€½ 𝑧 ∈ 0 < π‘₯ 0 + πœ€ 𝑣 < π‘₯ ξ€Ύ , π‘₯ ( 𝑧 ) i f ξ€½ 𝑧 ∈ π‘₯ ≀ π‘₯ 0 ξ€Ύ . + πœ€ 𝑣 ( 3 . 3 4 ) we define
Clearly 𝑦 ∈ 𝐢 We use this ξ€œ 0 ≀ πœ€ { 0 < π‘₯ 0 + πœ€ 𝑣 < π‘₯ } β€– 𝐷 π‘₯ 0 β€– 𝑝 βˆ’ 2 ( 𝐷 π‘₯ 0 , 𝐷 𝑣 ) ℝ β„• ξ€œ 𝑑 𝑧 βˆ’ { 0 < π‘₯ 0 + πœ€ 𝑣 < π‘₯ } βˆ’ ξ€œ 𝑒 ( πœ€ 𝑣 ) 𝑑 𝑧 { π‘₯ 0 + πœ€ 𝑣 ≀ 0 } β€– 𝐷 π‘₯ 0 β€– 𝑝 ξ€œ 𝑑 𝑧 + { π‘₯ 0 + πœ€ 𝑣 ≀ 0 } 𝑒 π‘₯ 0 + ξ€œ 𝑑 𝑧 { π‘₯ 0 + πœ€ 𝑣 β‰₯ π‘₯ } β€– 𝐷 π‘₯ 0 β€– 𝑝 βˆ’ 2 ( 𝐷 π‘₯ 0 , 𝐷 ( π‘₯ βˆ’ π‘₯ 0 ) ) ℝ β„• ξ€œ 𝑑 𝑧 βˆ’ { π‘₯ 0 + πœ€ 𝑣 β‰₯ π‘₯ } 𝑒 ( π‘₯ βˆ’ π‘₯ 0 ξ€œ ) 𝑑 𝑧 = πœ€ 𝑍 β€– 𝐷 π‘₯ 0 β€– 𝑝 βˆ’ 2 ( 𝐷 π‘₯ 0 , 𝐷 𝑣 ) ℝ β„• ξ€œ 𝑑 𝑧 βˆ’ πœ€ 𝑍 βˆ’ ξ€œ 𝑒 𝑣 𝑑 𝑧 { π‘₯ 0 + πœ€ 𝑣 β‰₯ π‘₯ } β€– 𝐷 π‘₯ β€– 𝑝 βˆ’ 2 ( 𝐷 π‘₯ , 𝐷 ( π‘₯ 0 + πœ€ 𝑣 βˆ’ π‘₯ ) ℝ β„• ξ€œ 𝑑 𝑧 + { π‘₯ 0 + πœ€ 𝑣 β‰₯ π‘₯ } 𝑒 ( π‘₯ 0 + πœ€ 𝑣 βˆ’ ξ€· π‘₯ ) 𝑑 𝑧 𝑒 ∈ 𝐿 𝑝 β€² ( 𝑍 ) , 𝑒 ( 𝑧 ) ∈ πœ• 𝑗 + ( 𝑧 , π‘₯ ( 𝑧 ) ) a . e . a n d c l e a r l y f r o m t h e d e fi n i t i o n o f 𝑒 , w e c a n a l w a y s a s s u m e 𝑒 = 𝑒 a . e . o n ξ€½ π‘₯ = π‘₯ 0 + ξ€œ ξ€Ύ ξ€Έ { π‘₯ 0 + πœ€ 𝑣 ≀ 0 } 𝑒 ξ€· π‘₯ 0 ξ€Έ ξ€œ + πœ€ 𝑣 𝑑 𝑧 + { π‘₯ 0 + πœ€ 𝑣 β‰₯ π‘₯ } ( ξ€· 𝑒 βˆ’ 𝑒 ) π‘₯ βˆ’ π‘₯ 0 ξ€Έ βˆ’ ξ€œ βˆ’ πœ€ 𝑣 𝑑 𝑧 { π‘₯ 0 + πœ€ 𝑣 ≀ 0 } β€– β€– 𝐷 π‘₯ 0