Home Eigenvalues for a class of singular problems involving p(x)-Biharmonic operator and q(x)-Hardy potential
Article Open Access

Eigenvalues for a class of singular problems involving p(x)-Biharmonic operator and q(x)-Hardy potential

  • Abdelouahed El Khalil , Mohamed Laghzal EMAIL logo , My Driss Morchid Alaoui and Abdelfattah Touzani
Published/Copyright: November 7, 2019

Abstract

In this paper, we consider the nonlinear eigenvalue problem:

Δ(|Δu|p(x)2Δu)=λ|u|q(x)2uδ(x)2q(x)inΩ,uW02,p(x)(Ω),

where Ω is a regular bounded domain of ℝN, δ(x) = dist(x, ∂Ω) the distance function from the boundary ∂Ω, λ is a positive real number, and functions p(⋅), q(⋅) are supposed to be continuous on Ω satisfying

1<minΩ¯qmaxΩ¯q<minΩ¯pmaxΩ¯p<N2 and maxΩ¯q<p2:=Np(x)N2p(x)

for any xΩ. We prove the existence of at least one non-decreasing sequence of positive eigenvalues. Moreover, we prove that sup Λ = +∞, where Λ is the spectrum of the problem. Furthermore, we give a proof of positivity of inf Λ > 0 provided that Hardy-Rellich inequality holds.

MSC 2010: 58E05; 35J35; 35J60; 47J10

1 Introduction

During the last two decades the field of variable exponent Lebesgue spaces Lp(.) or Sobolev Wm,p(.) have received a strong deal of attention by exploiting the well-known techniques of Orlicz spaces dated back to the work of Orlicz [13] in 1931. Motivated by large applications involving partial differential equations governed by operators may vary with respect to the spacial variable x itself, this filed becomes today a research area called variable exponent analysis. This area is necessary in nonlinear electrorheological fluids and elastic mechanics. In that context, we refer the reader to Ruzicka [18], Zhikov [23] and the references therein. Our results in the present paper are partially inspired from the work of Harjulehto et al. [9] where the authors surveyed the differential equations governed by p(.)-Lapalcian with non-standard growth and compared the results on the existence and the regularity.

In particular, the equations treated here contain also Hardy potential term, which make the analysis more delicate and quite interesting. Namely, will deal with the following nonlinear eigenvalue problem involving the p(x)-Biharmonic and Hardy type potential:

Δ(|Δu|p(x)2Δu)=λ|u|q(x)2uδ(x)2q(x)inΩ,uW02,p(x)(Ω), (1.1)

where Ω is a regular bounded domain in ℝN, we denote by δ(x) := dist(x, ∂Ω) the distance from the boundary ∂Ω, λ is a positive real number playing the role of an eigenvalue, and the exponent functions p(⋅), q(⋅) are continuous on Ω¯,Δp(x)2u:=Δ(|Δu|p(x)2Δu) is the fourth order p(x)-biharmonic operator.

Recently, El Khalil et al. proved the existence of a sequence of positive eigenvalues for problem (1.1) only for the constant case q(x) = p(x) = p in [6].

As far as we are aware, nonlinear eigenvalue problems like (1.1) involving the nonhomogenous Hardy inequality in variable exponent Sobolev space have not yet been studied. That is why, at our best knowledge, the present paper is a first contribution in this direction.

In this way, inspired by the works of [12, 15, 16], we attempt to expend the results of [6] to the space of variable exponent. More precisely, we establish the existence of at least one non-decreasing sequence of nonnegative eigenvalues of this problem such that sup Λ = ∞, where Λ is the spectrum of (1.1). We prove that inf Λ > 0 when the q(.)-Hardy-Rellich inequality holds, as a characterization of the positivity of the principal eigenvalue of problem (1.1).

In this paper we assume the following conditions:

H(p, q) 1 < qq+ < pp+ < N2 and q+ < p2 (x), for any xΩ,

where

q:=minΩ¯q,q+:=maxΩ¯qandp2(x):=Np(x)N2p(x),for anyxΩ¯

The rest of this paper is structured as follows. Section 2 states some preliminary properties to establish our results presented in Section 4. Section 3 we establish and prove an axillary inequality of Hardy type in variable exponent Lebesgue spaces, and give a necessary and sufficient condition for Hardy’s inequality to be true. In Section 4 we prove the existence of at least one non-decreasing sequence of nonnegative eigenvalues to problem (1.1) under appropriate hypotheses. Section 5 discusses the positivity of the infimum of the spectrum of our eigenvalue problem.

2 Space W2,p(⋅)(Ω) and useful results

We introduce some basic properties of Lebesgue-Sobolev spaces with variable exponent Lp(⋅)(Ω) and Wm,p(⋅)(Ω). For details, we refer to the book [4] and the references therein. To handle better theses spaces we define first, for each fixed exponent function p(.), the modular functional ρp(x) defined on Lp(⋅)(Ω) by

ρp(x)(u):=Ω|u|p(x)dx.

Set

C1+(Ω):={h:hC(Ω¯)andh(x)>1,xΩ¯}

The generalized Lebesgue space is defined as

Lp()(Ω)={u:ΩR measurable and ρp(x)(u)<}.

We endow it with the Luxemburg norm

up()=inf{μ>0:ρp(x)(uμ)1}.

The following proposition assembles the most important topological features of our variable exponent space setting that we need to overcome most of difficulties related to our objectives.

Proposition 2.1

[21]. The space (Lp(.)(Ω), | ⋅|p(.)) is separable, uniformly convex, reflexive and its conjugate dual space is Lp′(⋅)(Ω) where p′(⋅) is the conjugate function of p(⋅), i.e.,

p(x)=p(x)p(x)1forallxΩ.

For uLp(⋅)(Ω) and vLp′(⋅)(Ω) we have the "equivalent" Hölder’s inequality

|Ωu(x)v(x)dx|(1p+1p)|u|p()|v|p()2|u|p()|v|p().

The Sobolev space with variable exponent Wm,p(⋅)(Ω) is defined as

Wm,p()(Ω)={uLp()(Ω):DαuLp()(Ω),|α|m}.

Equipped with the norm

um,p(x)=|α|m|Dαu|p(x)

Wm,p(⋅)(Ω) has the same topological features as Lp(⋅)(Ω). For more details, we refer the reader to [7, 8, 11] and [20]. We denote by W0m,p() (Ω) the closure of C0 (Ω) in Wm,p(⋅)(Ω).

We define also the functional space

L÷p()(Ω)={u:ΩR is measurable and Ω1p(x)|u(x)|p(x)dx<}

and we equip it with the norm

|u|p(.)=inf{μ>0:Ω1p(x)|u(x)μ|p(x)dx1}

so that L÷p() (Ω) is a Banach space having similar topological properties to those of variable exponent Lebesgue spaces.

Proposition 2.2

([8, Theorem 1.3]). Let un, uLp(⋅), we have

  1. |u|p(⋅) = aρp(x) (ua) = 1 for u ≠ 0 and a > 0.

  2. |u|p(⋅) < (=; > 1) ⇔ ρp(x)(u) < (=; > 1).

  3. |un| → 0 (resp → +∞) ⇔ ρp(x)(un) → 0, (resp → +∞).

  4. the following statements are equivalent.

    1. limn→+∞ |unu|p(⋅) = 0,

    2. limn→+∞ ρp(x)(unu) = 0,

    3. unu in measure in Ω and limn→+∞ ρp(x)(un) = ρp(x)(u).

Return back to our problem (1.1), solutions are considered in weak sense, namely in W02,p() (Ω) endowed with the norm

u:=inf{μ>0:ρp(x)(Δu(x)μ)1}.

Remark 2.3

According to [21] the norm ∥.∥2,p(⋅) is equivalent to the normΔ.∥p(⋅) in the space W02,p() (Ω), for the Lipschitz boundary and the exponent p(⋅) is in a class functions for which 1p() is globally log-Hölder continuous. Consequently, the norms ∥.∥2,p(⋅), ∥.∥ andΔ .∥p(⋅) are equivalent. See also [2].

Remark 2.4

In view of Proposition 2.2, for every uLp(.)(Ω), then

min{up+,up}Ω|Δu|p(x)dxmax{up+,up}. (2.1)

Theorem 2.5

([1, Theorem 3.2]). Let p, q C1+ (Ω). Assume p(x) < N2 and q(x) < p2 (x). Then there is a continuous and compact embedding of W02,p(x) (Ω) into Lq(x)(Ω).

Definition 2.6

A function u W02,p() (Ω) is said to be a weak solution of (1.1) if

Ω|Δu(x)|p(x)2Δu(x)Δv(x)dx=λΩ|u(x)|q(x)2u(x)δ(x)2q(x)v(x)dxforallvW02,p()(Ω).

We point out that in the case u is nontrivial we say that λ is an eigenvalue of (1.1) corresponding to the eigenfunction u.

We give a direct characterization of λk involving a mini-max argument over sets of genus greater than k. We set

λ1=inf{Ω1p(x)|Δu|p(x)dx, subject to Ω1q(x)|u|q(x)δ(x)2q(x)dx=1}. (2.2)

The value defined in (2.2) can be written as the Rayleigh quotient

λ1=infΩ1p(x)|Δu|p(x)dxΩ1q(x)|u|q(x)δ(x)2q(x)dx, (2.3)

where the infimum is taken over W02,p() (Ω) ∖ {0}.

3 Improved q(.)-Hardy-Rellich inequality

Famous Hardy-Rellich inequality states that for all u in the usual Hilbert space H02 (Ω),

Ω|Δu|2dxN2(N4)216Ω|u|2δ(x)4dx,N5. (3.1)

The constant N2(N4)216 is optimal, but it is never achieved in any domain Ω ∈ ℝN. This inequality was first proved by Rellich [17] in H02 (Ω) and it was extended to functions in H2(Ω) ∩ H01 (Ω) by Doled et al [5]. Davis and Hinz [3] generalized (3.1) and proved that for any p ∈ (1, N2 ),

Ω|Δu|pdx(N(p1)(N2p)p2)pΩ|u|pδ(x)2pdx, (3.2)

whenever u Cc (Ω). The inequality (3.2) was proved in [10], for all uW2,p(Ω) ∩ W01,p (Ω) for 1 < p < N2 , where p is constant. Owen [14] proved for p = 2 and Ω is bounded convex open set that

Ω|Δu|2dx916Ω|u|2δ(x)4dx,

whenever u Cc (Ω).

Lemma 3.1

Assume that H(p, q) holds. Then there exists a positive constant C such that the q(.)-Hardy-Rellich inequality

Ω1p(x)|Δu|p(x)dxCΩ1q(x)|u|q(x)δ(x)2q(x)dx (3.3)

holds for all u W02,p() (Ω) in one of the following cases:

  1. |u| ≤ δ(x)2 and |△ u| ≥ 1;

  2. |u| ≥ δ(x)2 and |△u| ≤ 1.

Proof

Let u W02,p() (Ω) such that 1 < qq+ < pp+ < N2 .

From (a) we have |△ u| ≥ 1. Thus

Ωp+p(x)|Δu|p(x)dxΩ|Δu|qdx. (3.4)

In view of (3.2), we deduce that

Ω|Δu|qdxCΩ|u|qδ(x)2qdx,

where C=(N(q1)(N2q)(q)2)q. This and (3.4) permit us to write

Ωp+p(x)|Δu|p(x)dxqCΩ1q|u|qδ(x)2qdx.

Since |u| ≤ δ(x)2, we obtain

(|u|δ(x)2)q(|u|δ(x)2)q(x).

Therefore

qCΩ1q(|u|δ(x)2)qdxqCΩ1q(x)(|u|δ(x)2)q(x)dx.

Therefore

Ωp+p(x)|Δu|p(x)dxqCΩ1q(x)(|u|δ(x)2)q(x)dx.

That is

Ω1p(x)|Δu|p(x)dxqp+CΩ1q(x)|u|q(x)δ(x)2q(x)dx.

Hence we conclude that

Ω1p(x)|Δu|p(x)dxC1Ω1q(x)|u|q(x)δ(x)2q(x)dx,

where C1=qp+C.

From (b) w have |△ u| ≤ 1. Thus in this case

Ωp+p(x)|Δu|p(x)dxΩ|Δu|p+dx. (3.5)

Using again (3.2), we have

Ω|Δu|p+dxC+Ω|u|p+δ(x)2p+dx,

where C+=(N(p+1)(N2p+)(p+)2)p+. This and (3.5) give

Ωp+p(x)|Δu|p(x)dxqC+Ω1q|u|p+δ(x)2p+dx.

Since |u| ≥ δ(x)2, we get

(|u|δ(x)2)p+(|u|δ(x)2)q(x).

Thus

qC+Ω1q(|u|δ(x)2)p+dxqC+Ω1q(x)(|u|δ(x)2)q(x)dx.

Therefore

Ωp+p(x)|Δu|p(x)dxqC+Ω1q(x)(|u|δ(x)2)q(x)dx.

Then

Ω1p(x)|Δu|p(x)dxqp+C+Ω1q(x)|u|q(x)δ(x)2q(x)dx.

Hence we deduce that

Ω1p(x)|Δu|p(x)dxC2Ω1q(x)|u|q(x)δ(x)2q(x)dx,

where C2=qp+C+. The result follows. □

Remark 3.2

In view of (3.3), λ1 > 0 if and only if the q(.)-Hardy-Rellich inequality holds in Ω. Moreover, λ1 is exactly the best constant in the inequality (3.3). This makes our problem (1.1) naturally well defined.

Definition 3.3

Let X be a real reflexive Banach space and let X* stand for its dual with respect to the pairing 〈⋅, ⋅〉. We shall deal with mappings T acting from X into X*. The strong convergence in X (and in X*) is denoted byand the weak convergence by ⇀. T is said to belong to the class (S+) if for any sequence un in X converging weakly to uX and limsupn→+∞Tun, unu〉 ≤ 0, un converges strongly to u in X. We write T ∈ (S+).

Define Φ(u), φ(u) : W02,p() (Ω) → ℝ by

Φ(u)=Ω1p(x)|Δu|p(x)dxandφ(u)=Ω1q(x)|u|q(x)δ(x)2q(x)dx,

and set 𝓗 = {u W02,p() (Ω); φ(u) = 1}.

Lemma 3.4

We have the following statements:

  1. Φ and φ are even, and of class C1 on W02,p() (Ω).

  2. 𝓗 is a closed C1-manifold.

Proof

It is clear that φ and Φ are even and of class C1 on W02,p() (Ω) and 𝓗 = φ−1 {1}. In view of (3.3) 𝓗 is closed. The derivative operator φ′ satisfies φ′(u) ≠ 0 ∀ u ∈ 𝓗 (i.e., φ′(u) is onto for all u ∈ 𝓗). Hence φ is a submersion, which proves that 𝓗 is a C1-manifold. □

The operator T := Φ′: W02,p() (Ω) → W−2,p′(⋅)(Ω) defined as

T(u),v=Ω|Δu|p(x)2ΔuΔvdx for any u,vW02,p()(Ω)

satisfies the assertions of the following lemma.

Lemma 3.5

The following statements hold:

  1. T is continuous, bounded and strictly monotone.

  2. T is of (S+) type.

  3. T is a homeomorphism.

Proof

  1. Since T is the Fréchet derivative of Φ, it follows that T is continuous and bounded.

    Using the following elementary inequalities, which hold for any three real x, y and γ.

    |xy|γ2γ(|x|γ2x|y|γ2y)(xy)if γ2,|xy|21(γ1)(|x|+|y|)2γ(|x|γ2x|y|γ2y)(xy)if 1<γ<2,

    we obtain for all u, v W02,p() (Ω) such that uv,

    T(u)T(v),uv>0,

    which means that T is strictly monotone.

  2. Let (un)n be a sequence of W02,p() (Ω) such that

    unu weakly in W02,p()(Ω) and lim supn+T(un),unu0.

    In view of the monotonicity of T, we have

    T(un)T(u),unu0, (3.6)

    and since unu weakly in W02,p() (Ω), it follows that

    lim supn+T(un)T(u),unu=0. (3.7)

    Thanks to the above inequalities,

    {xΩ:p(x)2}|ΔunΔu|p(x)dx2(p2)ΩA(un,u)dx,{xΩ:1<p(x)<2}|ΔunΔu|p(x)dx(p+1)Ω(A(un,u))p(x)2(B(un,u))(2p(x))p(x)2dx,

    where

    A(un,u)=(|Δun|p(x)2Δun|Δu|p(x)2Δu)(ΔunΔu),B(un,u)=(|Δun|+|Δu|)2p(x).ΩA(un,u)dx=T(un)T(u),unu,

    we can consider

    0ΩA(un,u)dx<1

    and we distinguish two cases.

    First, if ∫Ω A(un, u) dx = 0, then A(un, u) = 0, since A(un, u) ≥ 0 a.e. in Ω.

    Second, if 0 < ∫Ω A(un, u) dx < 1, then

    tp(x):=({xΩ:1<p(x)<2}A(un,u)dx)1

    is positive and by applying Young’s inequality we deduce that

    {xΩ:1<p(x)<2}[t(A(un,u))p(x)2](B(un,u))(2p(x))p(x)2dx{xΩ:1<p(x)<2}A(un,u)(t)2p(x)+(B(un,u))p(x)dx.

    Now, by the fact that 2p(x)<2, we have

    {xΩ:1<p(x)<2}A(un,u)(t)2p(x)+(B(un,u))p(x)dx{xΩ:1<p(x)<2}A(un,u)t2+(B(un,u))p(x)dx1+{xΩ:1<p(x)<2}(B(un,u))p(x)dx.

    Hence

    {xΩ:1<p(x)<2}|ΔunΔu|p(x)dx({xΩ:1<p(x)<2}A(un,u)dx)12(1+Ω(B(un,u))p(x)dx).

    Since ∫Ω(B(un, u))p(x) dx is bounded, we have

    {xΩ:1<p(x)<2}|ΔunΔu|p(x)dx0 as n.
  3. Note that the strict monotonicity of T implies that T is into an operator.

Moreover, T is a coercive operator. Indeed, from (2.1) and since p − 1 > 0, for each u W02,p() (Ω) such that ∥ u ∥ ≥ 1, we have

T(u),uu=Φ(u)uup1 as u.

Finally, thanks to the Minty-Browder Theorem [22], the operator T is surjective and admits an inverse mapping.

To complete the proof of (3), it suffices then to show the continuity of T−1. Indeed, let (fn)n be a sequence of W−2,p′(⋅)(Ω) such that fnf in W−2,p′(⋅)(Ω). Let un and u in W02,p() (Ω) such that

T1(fn)=un and T1(f)=u.

By the coercivity of T, we deduce that the sequence (un)n is bounded in the reflexive space W02,p() (Ω). For a subsequence, if necessary, we have unû in W02,p() (Ω) for a some û. Then

limn+T(un)T(u),unu^=limn+fnf,unu^=0.

It follows by the assertion (2) and the continuity of T that

unu^ in W02,p(x)(Ω) and T(un)T(u^)=T(u) in W2,p(x)(Ω).

Further, since T is an into operator, we conclude that uû. □

We shall use The following results to prove our theorem related to the existence.

Lemma 3.6

We have the following statements:

  1. φis completely continuous.

  2. The functional Φ satisfies the Palais-Smale condition on 𝓗, i.e., for {un} ⊂ 𝓗, if {Φ(un)}n is bounded and

    αn=Φ(un)βnφ(un)0asn+, (3.8)

    where

    βn=Φ(un),unφ(un),un,

    then {un}n≥1 has a convergent subsequence in W02,p() (Ω).

Proof

  1. First let us prove that φ′ is well defined. Let u, v W02,p() (Ω). We have

    φ(u),v=Ω|u|q(x)2uδ(x)2q(x)vdx.

    Thus

    |φ(u),v|xΩ:δ(x)>1|u|q(x)1δ(x)2q(x)vdx+xΩ:δ(x)1|u|q(x)1δ(x)2q(x)vdx.

    Therefore

    |φ(u),v|xΩ:δ(x)>1|u|q(x)1vdx+xΩ:δ(x)11δ(x)2|u|q(x)1δ(x)2(q(x)1)vdx.

    By applying Hölder’s inequality, we obtain

    |φ(u),v|2(|u|r(x)q(x)1|v|q(x)+uδ(x)2r(x)q(x)1vδ(x)2q(x)).

    where r(x)=q(x)q(x)1.

    This and (3.3) yield

    |φ(u),v|2(|u|r(x)q(x)1|v|q(x)+1C2|Δu|r(x)q(x)1|Δv|q(x)).

    Then

    |φ(u),v|2(k1uq(x)1v+k2C2uq(x)1v),

    where k1 is a constant given by the embedding of W02,p() (Ω) in Lq(⋅)(Ω) and k2 is given by the equivalence of the norm |Δ.|p(⋅) and ∥.∥. Hence

    φ(u)2k1+k2C2uq(x)1,

    where ∥⋅∥ is the dual norm associated with ∥.∥.

    For the complete continuity of φ′, we argue as follow. Let (un)n W02,p() (Ω) be a bounded sequence and unu (weakly) in W02,p() (Ω). Due to the q(⋅)-Hardy inequality (3.3) unu in Lq()(Ω;1q()) and due to the fact that the embedding W02,p() (Ω) ↪ Lq(⋅)(Ω) is compact, un converges strongly to u in Lq(⋅)(Ω). Consequently, there exists a positive function gLq(⋅)(Ω) such that

    ug a.e. in Ω.

    Since gLq(⋅)–1(Ω), it follows from the Dominated Convergence Theorem that

    unq(x)2unuq(x)2u in Lq()(Ω).

    That is,

    φ(un)φ(u) in Lq()(Ω).

    Recall that the embedding

    Lq()(Ω)W2,p()(Ω)

    is compact. Thus

    φ(un)φ(u) in W2,p()(Ω).

    This proves the assertion (i).

  2. By the definition of Φ we have that ρp(x)(Δun) is bounded in ℝ. Thus, without loss of generality, we can assume that un converges weakly in W02,p() (Ω) for some functions u W02,p() (Ω) and ρp(x)(Δun) → . For the rest we distinguish two cases. If = 0, then un converges strongly to 0 in W02,p() (Ω). Otherwise, let us prove that

    lim supnΔp()2un,unu0.

    Indeed, notice that

    Δp()2un,unu=ρp(x)(Δun)Δp()2un,u.

    Applying αn of (3.8) to u, we deduce that

    θn=Δp()2un,uβnφ(un),u0 as n.

    Therefore

    Δp()2un,unu=ρp(x)(Δun)θn(Φ(un),unφ(un),un)φ(un),u.

    That is,

    Δp()2un,unu=ρp(x)(Δun)φ(un),un(φ(un),unφ(un),u)θn.

    On the other hand, from Lemma 3.6, φ′ is completely continuous. Thus

    φ(un)φ(u)andφ(un),unφ(u),u.

    Then

    |φ(un),unφ(un),u||φ(un),unφ(u),u|+|φ(un),uφ(u),u|.

    It follows that

    |φ(un),unφ(un),u||φ(un),unφ(u),u|+φ(un)φ(u)u.

    This implies that

    φ(un),unφ(un),u0 as n. (3.9)

    Combining with the above equalities, we obtain

    lim supn+Δp()2un,unuφ(u),ulim supn(φ(un),unφ(un),u).

    We deduce

    lim supnΔp()2un,unu0. (3.10)

    On the other hand,

    Φ(un),unu=Δp()2un,unu.

    According to (3.10), we conclude that

    lim supnΦ(un),unu0. (3.11)

    In view of Lemma 3.5, unu strongly in W02,p() (Ω). This achieves the proof of Lemma 3.6. □

4 Existence of infinitely many eigenvalue sequences

Set

Γj=KH:K is symmetric, compact and γ(K)j,

where γ(K) = j is the Krasnoselskii genus of the set K, i.e., the smallest integer j, such that there exists an odd continuous map from K to ℝj ∖ {0}.

Now, let us establish some useful properties of the Krasnoselskii genus proved by Szulkin [19].

Lemma 4.1

Let X be a real Banach space and A, B be symmetric subsets of X ∖ {0} which are closed in X. Then

  1. If there exists an odd continuous mapping f : AB, then γ(A) ≤ γ(B).

  2. If AB, then γ(A) ≤ γ(B).

  3. γ(AB) ≤ γ(A) + γ(B).

  4. If γ(B) < +∞, then γ(AB) ≥ γ(A) – γ(B).

  5. If A is compact, then γ(A) < +∞ and there exists a neighborhood N of A, N is a symmetric subset of X ∖ {0}, closed in X such that γ(N) = γ(A).

  6. If N is a symmetric and bounded neighborhood of the origin ink and if A is homeomorphic to the boundary of N by an odd homeomorphism, then γ(A) = k.

  7. If X0 is a subspace of X of codimension k and if γ(A) > k then AX0ϕ.

We now state our first main theorem of this paper using the Ljusternik-Schnirelmann theory.

Theorem 4.2

For any integer j ∈ ℕ,

λj=infKΓjmaxuKΦ(u)

is a critical value of Φ restricted on 𝓗. More precisely, there exists ujK such that

λj=Φ(uj)=supuKΦ(u),

and uj is a solution of (2.6) associated to the positive eigenvalue λj. Moreover,

λj,asj.

Proof

We only need to prove that for any j ∈ ℕ, Γj ≠ ∅ and the last assertion. Indeed, let j ∈ ℕ be given and let x1Ω and r1 > 0 be small enough such that B(x1, r1)Ω and meas(B(x1, r1)) < meas(Ω)2 . First, we take u1 C0 (Ω) with supp(u1) = B(x1, r1). Put B1 := ΩB(x1, r1), then meas(B1) > meas(Ω)2 . Let x2B1 and r2 > 0 such that B(x2, r2)B1 and meas(B(x1, r1)) < meas(B1)2 .

Next, we take u2 C0 (Ω) with supp(u2) = B(x2, r2).

Continuing the process described above we can construct by recurrence a sequence of functions u1, u2, …., uj C0 (Ω) such that supp(ui) ∩ supp(uj) = ∅ if ij and meas(supp(ui)) > 0 for i ∈ {1, 2, …, j}.

Let Ej = Span{u1, u2, …, uj} be the vector subspace of C0 (Ω) Spanned by {u1, u2, …, uj}. Then, dim Ej = j and note that the map

w|w|:={α>0:Ω|w(x)α|p(x)dx},

defines a norm on Ej. Putting Sj := {Ej : |v| = 1} the unit sphere of Ej. Let us introduce the functional g : ℝ+ × Ej ⟶ ℝ by g(s, u) = φ(su). It is clear that g (0, u) = 0 and g(s, u) is non decreasing with respect to s. More, for s > 1 we have

g(s,u)sqφ(u),

and so lims→+∞ g(s, u) = +∞. Therefore, for every uSj fixed, there is a unique value s = s(u) > 0 such that g (s(u), u) = 1.

On the other hand, since

gs(s(u),u)=Ω(s(u))q(x)1|u|q(x)δ2q(x)dxqs(u)g(s(u),u)=qs(u)>0.

The implicit function theorem implies that the map us(u) is continuous and even by uniqueness.

Now, take the compact Kj := 𝓗 ∩ Ej. Since the map h : SjKj defined by h(u) = s(u).u is continuous and odd, it follows by the property of genus that γ(Kj) ≥ j. This completes the proof of first part of the theorem.

Now, we claim that

λj as j.

Since W02,p() (Ω) is separable, there exists (ek,en)k,n a bi-orthogonal system such that ek W02,p() (Ω) and en W–2,p′(⋅)(Ω), the (ek)k are linearly dense in W02,p() (Ω) and the (en)n are total for the dual W–2,p′(⋅)(Ω)). For k ∈ ℕ, set

Fk=span{e1,,ek}andFk=span{ek+1,ek+2,}.

By (g) of Lemma 4.1, we have for any KΓk, K Fk1 ≠ ∅. Thus

tk=infKΓksupuKFk1Φ(u) as k.

Indeed, if not, for large k there exists uk Fk1 with ∥ukp(⋅) = 1 such that tkΦ(uk) ≤ M for some M > 0 independent of k. Thus ∥Δukp(⋅)M. This implies that (uk)k is bounded in W02,p() (Ω). For a subsequence of {uk} if necessary, we can assume that {uk} converges weakly in W02,p() (Ω) and strongly in Lp(⋅)(Ω). By our choice of Fk1 , we have uk ⇀ 0 weakly in W02,p() (Ω) because 〈 en , ek〉 = 0, for any k > n. This contradicts the fact that ∥ukp(⋅) = 1 for all k. Since λktk, the claim is proved. □

5 The infimum of the eigenvalues

Now, we give the following lemma which will be used in Theorem 5.2 which is the second main result of this paper.

Lemma 5.1

λ1 = 0 → R(u) = 0, where

R(u)=Rp()(u)=infuW02,p()(Ω),u0Ω|Δu|p(x)dxΩ|u|q(x)δ(x)2q(x)dx.

Proof

It is clear that we have the bounds

qp+R(u)λ1p+qR(u),

then from this it follows that λ1 = 0 → R(u) = 0. □

Theorem 5.2

If there are an open subset UΩ and a point x0Ω such that p(x0) < (or >) p(x) for all x U, then λ1 = 0.

Proof

We only deal with the case that p(x0) < p(x). The proof of the case that p(x0) > p(x) is similar. Denote for OΩ and δ > 0, B(O; δ) = {x ∈ ℝN : dist (x; O) < δ}. Without loss of generality, we may assume that UΩ, then there is ε0 > 0 such that

p(x0)<p(x)4ε0for allxU,

and there is ε1 > 0 such that

p(x0)<p(x)2ε0for allxB(U,ε1), (5.1)

where B(∂U, ε1) = {x : ∃y∂U such that |xy | < ε1} ⊂ Ω, and there is ε2 > 0 such that B(x0, ε2) ⊂ UB(∂U, ε1), and

|p(x0)p(x)|<ε0for allxB(x0,ε2). (5.2)

We can find a function u0 C0 (Ω) such that |Δ(u0(x))| ≤ C, 0 ≤ u0 ≤ 1 and

u0(x)=1ifxUB(U,ε1),0ifxUB(U,ε1).

Then, for t > 0 small enough such that

Ω|tu0|p(x)δ(x)2p(x)dxΩ|tu0|q(x)δ(x)2q(x)dx<1.

Thus

R(tu0)=Ω|Δ(tu0(x))|p(x)dxΩ|tu0|q(x)δ(x)2q(x)dx=(Ω|Δ(tu0(x))|p(x)dxΩ|tu0|p(x)δ(x)2p(x)dx)(Ω|tu0|p(x)δ(x)2p(x)dxΩ|tu0|q(x)δ(x)2q(x)dx)B(x0,ε2)|Δ(tu0(x))|p(x)dxB(x0,ε2)|tu0|p(x)δ(x)2p(x)dxC1C2tp(ξ1)p(ξ2),

where C1 = ∫B(∂U,ε1)|Δu0(x)|p(x) dx and C2=B(x0,ε2)|u0|p(x)δ(x)2p(x)dx are positive constants independent of t with ξ1B(∂U, ε1) and ξ2B(x0, ε2).

Using (5.1) and (5.2), we get |p(ξ1) – p(ξ2)| > ε0. Therefore,

R(tu0)C1C2tε0 for all t(0;1).

When t → 0+, we obtain R(u) = 0, because limt0+C1C2tε0=0 and in view of Lemma 5.1, we deduce λ1 = 0. This completes the proof. □

Corollary 5.3

If Ω satisfies the q(.)-Hardy-Rellich inequality, then we have the following statements:

  1. λ1=infΩ1p(x)|Δu|p(x)dx,whereuW02,p()(Ω)andΩ1q(x)|u|q(x)δ(x)2q(x)dx=1;

  2. 0 < λ1λ2 ≤ … ≤ λn → +∞;

  3. λ1 = inf Λ (i.e., λ1 is the smallest eigenvalue in the spectrum of (1.1))).

Proof

  1. For u ∈ 𝓗, set K1 = {u, –u}. It is clear that γ(K1) = 1, Φ is even and

    Φ(u)=maxK1ΦinfKΓ1maxuKΦ(u).

    Thus

    infuHΦ(u)infKΓ1maxuKΦ(u)=λ1.

    On the other hand, for all KΓ1 and uK, we have

    supuKΦΦ(u)infuHΦ(u).

    It follows that

    infKΓ1maxKΦ=λ1infuHΦ(u).

    Then

    λ1=inf{Ω1p(x)|Δu|p(x)dx, where uW02,p()(Ω) and Ω1q(x)|u|q(x)δ(x)2q(x)dx=1}.
  2. For all ij, we have ΓiΓj and in view of the definition of λi, i ∈ ℕ, we get λiλj. As regards λn → ∞, it has been proved in Theorem 4.2.

  3. Let λΛ. Thus there exists uλ an eigenfunction of λ such that

    Ω1q(x)|uλ|q(x)δ(x)2q(x)dx=1.

    Therefore

    Δp(x)2uλ=λ|uλ|q(x)2uλδ(x)2q(x) inΩ.

    Then

    Ω1p(x)|Δuλ|p(x)dx=λΩ1q(x)|uλ|q(x)2q(x)2q(x)dx.

    In view of the characterization of λ1 in (2.2), we conclude that

    λ=Ω1p(x)|Δuλ|p(x)dxΩ1q(x)|uλ|q(x)2q(x)2q(x)dx=Ω1p(x)|Δuλ|p(x)dxλ1.

    This implies that λ1 = inf Λ. □

References

[1] A. Ayoujil, A., EI Amrouss, On the spectrum of a fourth order elliptic equation with variable exponent, Nonlinear Anal. Theory Methods. 71(2009), 4916-4926.10.1016/j.na.2009.03.074Search in Google Scholar

[2] F. Colasuonno and P. Pucci, Multiplicity of solutions for p(x)-polyharmonic elliptic Kirchhoff equations, Nonlinear Anal. 74 (2011), no. 17, 5962–5974.10.1016/j.na.2011.05.073Search in Google Scholar

[3] E. B. Davies and A. M. Hinz, Explicit constants for Rellich inequalities in Lp(Ω), Math. Z. 227 (1998), no. 3, 511–523.10.1007/PL00004389Search in Google Scholar

[4] L. Diening, P. Harjulehto, P. Hästö and M. Růžička, Lebesgue and Sobolev Spaces with Variable Exponents, Lecture Notes in Mathematics, 2017. Springer, Heidelberg, 2011.10.1007/978-3-642-18363-8Search in Google Scholar

[5] J. W. Dold, V. A. Galaktionov, A. A. Lacey and J. L. Vázquez, Rate of approach to a singular steady state in quasilinear reaction-diffusion equations, Ann. Scuola Norm. Sup. Pisa Cl. Sci. (4) 26 (1998), no. 4, 663–687.Search in Google Scholar

[6] A. El khalil, M. D. Morchid Alaoui and A. Touzani, On the spectrum of the p-biharmonic operator involving p-Hardy’s inequality, Appl. Math. (Warsaw) 41 (2014), no. 2-3, 239–246.10.4064/am41-2-11Search in Google Scholar

[7] X. L. Fan and X. Fan, A Knobloch-type result for p(t)-Laplacian systems, J. Math. Anal. Appl. 282 (2003), no. 2, 453–464.10.1016/S0022-247X(02)00376-1Search in Google Scholar

[8] X. L. Fan and D. Zhao, On the spaces Lp(x)(Ω) and Wm,p(x)(Ω), J. Math. Anal. Appl. 263 (2001), no. 2, 424–446.10.1006/jmaa.2000.7617Search in Google Scholar

[9] P. Harjulehto, P. Hästö, V. Lê, Út and M. Nuortio, Overview of differential equations with non-standard growth, Nonlinear Anal. 72 (2010), no. 12, 4551–4574.10.1016/j.na.2010.02.033Search in Google Scholar

[10] É. Mitidieri, A simple approach to Hardy inequalities (in Russian), translated from Mat. Zametki 67 (2000), no. 4, 563–572; Math. Notes 67 (2000), no. 3-4, 479–486.Search in Google Scholar

[11] M. Mihǎilescu, Existence and multiplicity of solutions for a Neumann problem involving the p(x)-Laplace operator, Nonlinear Anal. 67 (2007), no. 5, 1419–1425.10.1016/j.na.2006.07.027Search in Google Scholar

[12] M. Mihǎilescu, V. Rǎdulescu; A multiplicity result for a nonlinear degenerate problem arising in the theory of electrorheological fluids, Proc. R. Soc, A 462 (2006) 2073, 2625–2641.10.1098/rspa.2005.1633Search in Google Scholar

[13] W. Orlicz, b̈er konjugierte exponentenfolgen, Studia Mathematica 3, (1931), 200-211.10.4064/sm-3-1-200-211Search in Google Scholar

[14] M. P. Owen, The Hardy–Rellich inequality for polyharmonic operators, Proc. Roy. Soc. Edinburgh Sect. A 129 (1999), no. 4, 825–839.10.1017/S0308210500013160Search in Google Scholar

[15] V. Rǎdulescu; Nonlinear elliptic equations with variable exponent, Old and new, Nonlinear Anal.121 (2015), 336–369.10.1016/j.na.2014.11.007Search in Google Scholar

[16] V. Rǎdulescu, D.D. Repov’s; Partial Differential Equations with Variable Equations, Variational Methods and Qualitative Analysis, Monographs and Research Notes in Mathematics, CRC Press, Boca Raton, FL, 2015.Search in Google Scholar

[17] F. Rellich, in: Proceedings of the International Congress of Mathematicians, 1954, Amsterdam, vol. III, pp. 243–250. Erven P. Noordhoff N.V., Groningen; North-Holland Publishing Co., Amsterdam, 1956.Search in Google Scholar

[18] M. Růžička, Electrorheological Fluids: Modeling and Mathematical Theory, Lecture Notes in Mathematics, 1748. Springer-Verlag, Berlin, 2000.10.1007/BFb0104029Search in Google Scholar

[19] A. Szulkin, Ljusternik-Schnirelmann theory on C1-manifolds, Ann. Inst. H. Poincaré Anal. Non Linéaire 5 (1988), no. 2, 119–139.10.1016/s0294-1449(16)30348-1Search in Google Scholar

[20] J. H. Yao, Solutions for Neumann boundary value problems involving p(x)-Laplace operators, Nonlinear Anal. 68 (2008), no. 5, 1271–1283.10.1016/j.na.2006.12.020Search in Google Scholar

[21] A. Zang and Y. Fu, Interpolation inequalities for derivatives in variable exponent Lebesgue-Sobolev spaces, Nonlinear Anal. 69 (2008), no. 10, 3629–3636.10.1016/j.na.2007.10.001Search in Google Scholar

[22] E. Zeidler, Nonlinear Functional Analysis and Its Applications. II/B. Nonlinear monotone operators, Translated from the German by the author and Leo F. Boron, Springer-Verlag, New York, 1990.Search in Google Scholar

[23] V. V. Zhikov, Averaging of functionals of the calculus of variations and elasticity theory (in Russian), Izv. Akad. Nauk SSSR Ser. Mat. 50 (1986), no. 4, 675–710.Search in Google Scholar

Received: 2019-03-22
Accepted: 2019-07-26
Published Online: 2019-11-07

© 2019 A. El Khalil et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

Articles in the same Issue

  1. Frontmatter
  2. On the moving plane method for boundary blow-up solutions to semilinear elliptic equations
  3. Regularity of solutions of the parabolic normalized p-Laplace equation
  4. Cahn–Hilliard equation on the boundary with bulk condition of Allen–Cahn type
  5. Blow-up solutions for fully nonlinear equations: Existence, asymptotic estimates and uniqueness
  6. Radon measure-valued solutions of first order scalar conservation laws
  7. Ground state solutions for a semilinear elliptic problem with critical-subcritical growth
  8. Generalized solutions of variational problems and applications
  9. Existence and non-existence results for Kirchhoff-type problems with convolution nonlinearity
  10. Nonlinear Sherman-type inequalities
  11. Global regularity for systems with p-structure depending on the symmetric gradient
  12. Homogenization of a net of periodic critically scaled boundary obstacles related to reverse osmosis “nano-composite” membranes
  13. Noncoercive resonant (p,2)-equations with concave terms
  14. Evolutionary quasi-variational and variational inequalities with constraints on the derivatives
  15. Sharp estimates on the first Dirichlet eigenvalue of nonlinear elliptic operators via maximum principle
  16. Localization and multiplicity in the homogenization of nonlinear problems
  17. Remarks on a nonlinear nonlocal operator in Orlicz spaces
  18. A Picone identity for variable exponent operators and applications
  19. On the weakly degenerate Allen-Cahn equation
  20. Continuity results for parametric nonlinear singular Dirichlet problems
  21. Construction of type I blowup solutions for a higher order semilinear parabolic equation
  22. Singularly perturbed Choquard equations with nonlinearity satisfying Berestycki-Lions assumptions
  23. Comparison results for nonlinear divergence structure elliptic PDE’s
  24. Constant sign and nodal solutions for parametric (p, 2)-equations
  25. Monotonicity formulas for coupled elliptic gradient systems with applications
  26. Berestycki-Lions conditions on ground state solutions for a Nonlinear Schrödinger equation with variable potentials
  27. A class of semipositone p-Laplacian problems with a critical growth reaction term
  28. The role of superlinear damping in the construction of solutions to drift-diffusion problems with initial data in L1
  29. Reconstruction of Tesla micro-valve using topological sensitivity analysis
  30. Lewy-Stampacchia’s inequality for a pseudomonotone parabolic problem
  31. Global well-posedness of nonlinear wave equation with weak and strong damping terms and logarithmic source term
  32. Regularity Criteria for Navier-Stokes Equations with Slip Boundary Conditions on Non-flat Boundaries via Two Velocity Components
  33. Homoclinics for singular strong force Lagrangian systems
  34. A constructive method for convex solutions of a class of nonlinear Black-Scholes equations
  35. On a class of nonlocal nonlinear Schrödinger equations with potential well
  36. Superlinear Schrödinger–Kirchhoff type problems involving the fractional p–Laplacian and critical exponent
  37. Regularity for minimizers for functionals of double phase with variable exponents
  38. Boundary blow-up solutions to the Monge-Ampère equation: Sharp conditions and asymptotic behavior
  39. Homogenisation with error estimates of attractors for damped semi-linear anisotropic wave equations
  40. A-priori bounds for quasilinear problems in critical dimension
  41. Critical growth elliptic problems involving Hardy-Littlewood-Sobolev critical exponent in non-contractible domains
  42. On the Sobolev space of functions with derivative of logarithmic order
  43. On a logarithmic Hartree equation
  44. Critical elliptic systems involving multiple strongly–coupled Hardy–type terms
  45. Sharp conditions of global existence for nonlinear Schrödinger equation with a harmonic potential
  46. Existence for (p, q) critical systems in the Heisenberg group
  47. Periodic traveling fronts for partially degenerate reaction-diffusion systems with bistable and time-periodic nonlinearity
  48. Some hemivariational inequalities in the Euclidean space
  49. Existence of standing waves for quasi-linear Schrödinger equations on Tn
  50. Periodic solutions for second order differential equations with indefinite singularities
  51. On the Hölder continuity for a class of vectorial problems
  52. Bifurcations of nontrivial solutions of a cubic Helmholtz system
  53. On the exact multiplicity of stable ground states of non-Lipschitz semilinear elliptic equations for some classes of starshaped sets
  54. Sign-changing multi-bump solutions for the Chern-Simons-Schrödinger equations in ℝ2
  55. Positive solutions for diffusive Logistic equation with refuge
  56. Null controllability for a degenerate population model in divergence form via Carleman estimates
  57. Eigenvalues for a class of singular problems involving p(x)-Biharmonic operator and q(x)-Hardy potential
  58. On the convergence analysis of a time dependent elliptic equation with discontinuous coefficients
  59. Multiplicity and concentration results for magnetic relativistic Schrödinger equations
  60. Solvability of an infinite system of nonlinear integral equations of Volterra-Hammerstein type
  61. The superposition operator in the space of functions continuous and converging at infinity on the real half-axis
  62. Estimates by gap potentials of free homotopy decompositions of critical Sobolev maps
  63. Pseudo almost periodic solutions for a class of differential equation with delays depending on state
  64. Normalized multi-bump solutions for saturable Schrödinger equations
  65. Some inequalities and superposition operator in the space of regulated functions
  66. Area Integral Characterization of Hardy space H1L related to Degenerate Schrödinger Operators
  67. Bifurcation of time-periodic solutions for the incompressible flow of nematic liquid crystals in three dimension
  68. Morrey estimates for a class of elliptic equations with drift term
  69. A singularity as a break point for the multiplicity of solutions to quasilinear elliptic problems
  70. Global and non global solutions for a class of coupled parabolic systems
  71. On the analysis of a geometrically selective turbulence model
  72. Multiplicity of positive solutions for quasilinear elliptic equations involving critical nonlinearity
  73. Lack of smoothing for bounded solutions of a semilinear parabolic equation
  74. Gradient estimates for the fundamental solution of Lévy type operator
  75. π/4-tangentiality of solutions for one-dimensional Minkowski-curvature problems
  76. On the existence and multiplicity of solutions to fractional Lane-Emden elliptic systems involving measures
  77. Anisotropic problems with unbalanced growth
  78. On a fractional thin film equation
  79. Minimum action solutions of nonhomogeneous Schrödinger equations
  80. Global existence and blow-up of weak solutions for a class of fractional p-Laplacian evolution equations
  81. Optimal rearrangement problem and normalized obstacle problem in the fractional setting
  82. A few problems connected with invariant measures of Markov maps - verification of some claims and opinions that circulate in the literature
Downloaded on 31.10.2025 from https://www.degruyterbrill.com/document/doi/10.1515/anona-2020-0042/html?lang=en
Scroll to top button