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Infinitely many sign-changing solutions for the Brézis-Nirenberg problem involving the fractional Laplacian

  • Lin Li , Jijiang Sun EMAIL logo and Stepan Tersian
Published/Copyright: October 31, 2017

Abstract

In this paper, we consider the following Brézis-Nirenberg problem involving the fractional Laplacian operator:

(Δ)su=λu+|u|2s2uinΩ,u=0onΩ,

where s ∈ (0, 1), Ω is a bounded smooth domain of ℝN (N > 6s) and 2s=2NN2s is the critical fractional Sobolev exponent. We show that, for each λ > 0, this problem has infinitely many sign-changing solutions by using a compactness result obtained in [34] and a combination of invariant sets method and Ljusternik-Schnirelman type minimax method.

1 Introduction and main results

In this paper, we consider the following nonlinear problem with the fractional Laplacian

(Δ)su=λu+|u|2s2uinΩ,u=0onΩ,(1.1)

where λ > 0, 0 < s < 1, Ω is a bounded smooth domain of ℝN and 2s=2NN2s is the critical exponent in fractional Sobolev inequalities. Here the fractional Laplacian (–Δ)s is defined as follows.

Let {φk} be an orthonormal basis of L2(Ω) with ║φkL2(Ω) = 1 forming a spectral decomposition of –Δ in Ω with zero Dirichlet boundary data and λk be the corresponding eigenvalues, i.e. –Δ φk = λkφk in Ω with φk = 0 on Ω. Let 0 < s < 1 and

H0s(Ω)=u=k=1ukφkL2(Ω):uH0s(Ω)=k=1λksuk21/2<

be the fractional Sobolev space (see [2, 37]) with inner product

(u,v)H0s(Ω)=0λksukvk=Ω(Δ)s/2u(Δ)s/2vdx.

It is not difficult to see that H0s(Ω)is a Hilbert space. For any uH0s(Ω), u=k=1ukφkwith uk=Ωuφkdx, the spectral fractional Laplacian (–Δ)s is defined by

(Δ)su=k=1λksukφk.

We say that {(φk,λks)} are the eigenfunctions and eigenvalues of (–Δ)s in Ω with zero Dirichlet boundary data. In the pioneering work [6], Brézis and Nirenberg considered the existence solutions of equation (1.1) with s = 1. They show that for λ > 0 the problem

Δu=λu+|u|22uinΩ,u>0inΩ,u=0onΩ,

where 2=2NN2, may admit non-trivial solutions under a subtle dependence on the dimension N≥ 3. After that, there are many results on this problem. See e.g. [14, 15, 1728] and the references therein. In particular, in [18], Devillanova and Solimini showed that, when N ≥ 7, problem (1.1) with s = 1 has infinitely many solutions for each λ > 0 by using the uniform bounded theorem (see Theorem 1.1 in [18]). Recently, under the same assumptions of [18], Schechter and Zou [23] proved that this problem has infinitely many sign-changing solutions by combining the estimates of Morse indices of nodal solutions with the uniform bounded theorem due to Devillanova and Solimini [18].

Nonlinear problems involving the fractional Laplacian have been extensively studied recently. Caffarelli et al. [8, 9] studied the free boundary problem for the fractional Laplacian. Silvestre [27] investigated the regularity of the obstacle problem for the fractional Laplace operator. In [10], Caffarelli and Silvestre given a new local realization of the fractional Laplacian (–Δ)s by introducing the so-called s-harmonic extension. After that, several authors, using the localization method, have extended some results of the classical elliptic problems to the fractional Laplacian, see for example [2, 5, 7, 13, 16, 31, 34, 35, 36, 24, 25, 26] and the references therein. In particular, Chang and Wang [16], using the method of invariant sets of descending flow, obtained the existence and multiplicity of nodal solutions for the elliptic equaitons involving the fractional Laplacian (–Δ)s for all s ∈ (0, 1) with subcritical nonlinearities; for the Brézis-Nirenberg type problem involving the fractional Laplacian (1.1), Tan [31] proved the existence of positive solutions with the special case s=12 and Barrios et al. [2] studied the general case with 0 < s < 1. For any λ > 0, Yan et al. [34] proved that problem (1.1) possesses infinitely many solutions by using a compactness result for the subcritical perturbed problem associated to (1.1). In [21] the authors study bifurcation and multiplicity of solutions for the fractional Laplacian with critical exponential nonlinearity using critical point theorem of Bartolo, Benci and Fortunato [3]. Multiplicity of solutions for fractional differential equations via variational method is studied in [1, 32, 37].

A natural question is whether problem (1.1) has infinitely many sign-changing solutions for each λ > 0 and s ∈ (0, 1). To the best of our knowledge, there is no result in the literature concerning this question. In this paper, we give a positive answer to this open question. The main result of this paper is the following.

Theorem 1.1

Suppose that N > 6s and λ > 0, then problem(1.1)has infinitely many sign-changing solutions.

Remark 1.1

Denote λ1s the first eigenvalue of (–Δ)s in Ω with zero Dirichlet boundary condition. Multiplying the first eigenfunction and integrating both sides, one can easily check that if λλ1s, any nontrivial solution of (1.1) is sign-changing. Therefore, by the results of [34], to prove Theorem 1.1, it suffices to consider the case of λ(0,λ1s).

Theorem 1.1 extends the result in [23] to the fractional Laplacian. Motivated by [30] which used the more simple proof than [23] to obtain the same result, we will prove Theorem 1.1 by applying the usual Ljusternik-Schnirelman type minimax method in conjunction with invariant set method. However, due to the fact that the operator (–Δ)s is nonlocal, the techniques of constructing invariant sets of descending flow in [4, 19, 20] cannot be directly applied to problem (1.1). In order to construct invariant sets, we adopt an idea from [13, 16] to introduce an auxiliary operator Aε (see Section 3) associated to the subcritical perturbed problem (2.3). Then we can follow the same way as in [30] with the help of the compactness result (Theorem 2.1, see Section 2) due to Yan et al. [34] to obtain Theorem 1.1.

This paper is organized as follows. In Section 2, we describe a variational setting of the problem and state a compactness result due to Yan et al. [34] for the solutions of the perturbed problem (2.4). In Section 3, we introduce an auxiliary operator Aε and then construct the invariant sets, the proof of Theorem 1.1 is given at the end of this section.

2 Preliminaries and functional setting

Denote Hs(Ω) the dual space of H0s(Ω). Define the inner product in H0s(Ω) by

(u,v)H0s(Ω):=Ω(Δ)s/2u(Δ)s/2vdx.

Definition 2.1

We say that uH0s(Ω) is a weak solution of (1.1) if the identity

Ω(Δ)s/2u(Δ)s/2ϕdx=Ω(λuϕ+|u|2s2uϕ)dx

holds for every ϕH0s(Ω).

Note that the right hand side of the identity in the above definition is well defined, since ϕH0s(Ω)L2s(Ω), and for uH0s(Ω), λ u+ |u|2s2uL2NN+2s(Ω). It is standard (see e.g. [22]) to show that the weak solutions of problem (1.1) correspond to the critical points of the energy functional I: H0s(Ω) → ℝ given by

I(u)=12Ω|(Δ)s/2u|2dxλ2Ω|u|2dx12sΩ|u|2sdx,uH0s(Ω).

Clearly, IC1( H0s(Ω),ℝ).

Define R+N+1={(x,y):xRN,y>0}, the upper half space in ℝN+1. Associate to the bounded domain Ω, we consider the cylinder 𝓒 = Ω × (0, ∞) ⊂ R+N+1 and denote its lateral boundary by L𝓒 = Ω × [0, ∞).

Note that (−Δ)s is a nonlocal operator, motivated by the work of Caffarelli and Silvestre [10]. Using the so-called s-harmonic extension, several authors have considered an equivalent definition of the operator (−Δ)s defined through the spectral decomposition as above. Then the nonlocal problems can be transformed into a local problem see e.g. [2, 5, 7, 13, 16, 34, 35]. For a given uH0s(Ω), we define its s-harmonic extension w = Es(u) to 𝓒 as the solution of the problem

div(y12sw)=0in C,w=0on LC,w(x,0)=uon Ω.(2.1)

Following [10], we can define the fractional Laplacian operator by the Dirichlet to Neumann map as follows.

Definition 2.2

For any uH0s(Ω), the fractional Laplacian (−Δ)s acting on u is defined by

(Δ)su(x):=1kslimy0+y12swyw(x,y),xΩ,

where w = Es(u) and ks=212sΓ(1s)Γ(s) is a normalization constant.

Define H0,Ls(𝓒) as the closure of C0(𝓒) under the norm

wH0,Ls(C)=ksCy12s|w|2dxdy1/2.

Denote by trΩ the trace operator on Ω × {0} for functions in H0,Ls(𝓒):

trΩw=w(,0),forwH0,Ls(C).

Then for any wH0,Ls(C), the following trace inequality holds

|trΩwH0s(Ω)wH0,Ls(C).

Moreover, we have the following result (see [2, 16]).

Lemma 2.1

[Lemma 2.3, [16]).

  1. Es(⋅) is an isometry betweenH0s(Ω) andH0,Ls(𝓒), that is

    uH0s(Ω)=Es(u)H0,Ls(C);
  2. For anywH0,Ls(𝓒), there exists a constant C independent of w such that

    trΩwLr(Ω)CwH0,Ls(C)

    holds for all r ∈ [2, 2s]. Moreover, H0,Ls(𝓒) is compactly embedded into Lr(Ω) for every r ∈ [2, 2s).

Set

νsw(x):=1kslimy0+y12swyw(x,y).

With the above extension, from [10], we can transform the nonlocal problem (1.1) into the following local problem

div(y12sw)=0inC,w=0onLC,νsw=λw(x,0)+|w(x,0)|2s2w(x,0)onΩ.(2.2)

A weak solution to this problem is a function wH0,Ls(𝓒) such that

ksCy12s(w,ψ)dxdy=Ω(λw(x,0)+|w(x,0)|2sw(x,0))trΩψdx,

for all ψH0,Ls(𝓒). Then, critical points of the functional

J(w)=ks2Cy12s|w|2dxdyλ2Ω|w(x,0)|2dx12sΩ|w(x,0)|2sdx,

defined on H0,Ls(𝓒) correspond to the solutions of (2.2). For any weak solution wH0,Ls(𝓒) to (2.2), the function u = trΩwH0s(Ω) is a weak solution of problem (1.1) and is a critical point of I. The converse is also true. Therefore, these two formulations are equivalent, and we will use both formulations in the sequel.

Given ε > 0 small enough, associated to problems (1.1) and (2.2), we consider the following subcritical perturbed nonlocal problem:

(Δ)su=λu+|u|2s2εuin Ω,u=0on Ω,(2.3)

and the local problem

div(y12sw)=0in C,w=0on LC,νsw=λw(x,0)+|w(x,0)|2s2εw(x,0)on Ω.(2.4)

The functional Iε: H0s(Ω) → ℝ corresponding to (2.3) is defined as follows

Iε(u)=12Ω|(Δ)s/2u|2dxλ2Ω|u|2dx12sεΩ|u|2sεdx,uH0s(Ω).

It is easy to check that IεC1( H0s(Ω),ℝ).

Now we state the following compactness result due to Yan et al. [34], which plays an important role in our proof.

Theorem 2.1

([34], Theorem 1.1). SupposeN > 6s and λ > 0. Assume that wn (n = 1,2,⋅s) is a nontrivial solution of (2.4) withε = εn > 0, and {wn}n ∈ℕsatisfieswn∥ ≤ C for some positive constant independent of n. Then {wn}n ∈ℕpossesses a subsequence which converges strongly inH0,Ls(Ω) as n → ∞.

3 Proof of the main result

In this section, we will prove Theorem 1.1.

3.1 Some technical lemmas

Let

0<λ1s<λ2sλ3sλms

be the eigenvalues of ((−Δ)s, H0s(Ω)) introduced in Section 1 and φm be the eigenfunction corresponding to λms. Denote

Em:=span{φ1,φ2,,φm}.

Fix ζ ∈ (2, 2s). In the following, we will always assume that

λ(0,λ1s)andε(0,2sζ).

In order to construct the minimax values for the perturbed functional Iε, the following three technical lemmas are needed.

Lemma 3.1

For any ε ∈ (0, 2s-ζ), the functionalIεsatisfies the Palais-Smale ((PS) for short) condition.

Proof

Suppose {un} ⊂ H0s(Ω) is a (PS) sequence for Iε, i.e.,

Iε(un)cRandIε(un)0asn.

We have

c+o(1)(1+unH0s(Ω))=Iε(un)12sIε(un),unHs(Ω),H0s(Ω)=1212s(unH0s(Ω)2λun22)1212sλ1sλλ1sunH0s(Ω)2,

which implies that {un} is bounded sequence in H0s(Ω). Hence, there exists u0H0s(Ω) such that

unu0 in H0s(Ω).

By Lemma 2.1, we have

unu0 in Lr(Ω) with r[2,2s)

and

un(x)u0(x) for a.e. xΩ.

It follows that

o(1)=Iε(un),unu0Hs(Ω),H0s(Ω)=Ω(Δ)s/2un(Δ)s/2(unu0)dx+Ω(λ+|un|2s2ε)un(unu0)dx=unu0H0s(Ω)2+o(1),asn,

which implies that

unu0 in H0s(Ω)

and the proof is completed.□

Lemma 3.2

Suppose m ≥ 1. Then there exists R = R(Em) > 0, such that for allε ∈ (0, 2sζ),

supBRcEmIε<0,

whereBRc:=H0s(Ω)BRandBR={uH0s(Ω):uH0s(Ω)R}.

Proof

Define an auxiliary functional I* : H0s (Ω) → ℝ given by

I(u)=12Ω|(Δ)s/2u|2λu2dx12sΩ|u|ζdx.(3.1)

Noting that

12s(|u|ζ1)12sε|u|2sε,

it is easy to check that

Iε(u)I(u)+|Ω|2s,

holds for any ε ∈ (0, 2sζ). Since any norm in finite dimensional space is equivalent,

limuH0s(Ω),uEmI(u)=

for any fixed m ≥ 1. Thus the result follows.□

Lemma 3.3

For anyε ∈ (0, 2sζ), there existρε > 0 andαε > 0 such that

infBρεIεαε,

whereBρε={uH0s(Ω):uH0s(Ω)ρε}.

Proof

For uH0s(Ω), by Lemma 2.1, there exists C(ε) > 0 such that

Iε(u)=12uH0s(Ω)2λ2u2212sεu2sε2sελ1sλ2λ1suH0s(Ω)2C(ε)2sεuH0s(Ω)2sε.

Noting that 2 < 2sε, we conclude that there exist ρε > 0 and αε > 0 such that

infBρεIεαε,

as required.□

3.2 Properties of the operator Aε

In order to introduce an auxiliary operator Aε, which will be used to construct invariants set, we first define the inverse of the operator (−Δ)s (see [16], Section 4).

Definition 3.1

Given gHs(Ω), define the operator Ts : Hs(Ω) → H0s(Ω), by Ts(g)= trΩw, where wH0,Ls(C) solves

div(y12sw)=0in C,w=0on LC,νsw=g(x)on Ω.(3.2)

As in [16] (see also [7]), the above definition is well defined and

Ts(Δ)s=idH0s(Ω),(Δ)sTs=idHs(Ω),

which implies Ts is the inverse of the operator (−Δ)s. Denote Ts by (−Δ)s. Clearly,

(Δ)s=((Δ)s)1.

Moreover, by Proposition 4.2 in [16], the operator (−Δ)s is a self-adjoint and positive compact operator.

Now we define the operator Aε : H0s(Ω)H0s(Ω) by

Aε(u)=(Δ)s[λu+|u|2s2εu]

for uH0s(Ω). Then the gradient of Iε has the form

Iε(u)=uAε(u).

Indeed, we have

Iε(u),φHs(Ω),H0s(Ω)=Ω(Δ)s/2u(Δ)s/2φdxΩ(λu+|u|2s2εu)φdx=Ω(Δ)s/2u(Δ)s/2φdxΩ(Δ)sAε(u)φdx=Ω(Δ)s/2u(Δ)s/2φdxΩ(Δ)s/2Aε(u)(Δ)s/2φdx=uAε(u),φH0s(Ω),u,φH0s(Ω).

Note that the set of fixed points of Aε is the same as the set of critical points of Iε, which is Kε:={uH0s(Ω):Iε(u)=0}.

3.3 Invariant subsets of descending flow

It is easy to check that Iε is locally Lipschitz continuous. We consider the negative gradient flow φε of Iε defined by

ddtφε(t,u)=Iε(φε(t,u))for t0,φε(0,u)=u.

Here and in the sequel, define the convex cones

P+={uH0s(Ω):u0}andP={uH0s(Ω):u0}.

For ϑ > 0, we denote

Pϑ+={uH0s(Ω):dist(u,P+)<ϑ}

and

Pϑ={uH0s(Ω):dist(u,P)<ϑ},

where dist(u, P±) = infvP±uvH0s(Ω). Obviously, Pϑ=Pϑ+. Let

W=Pϑ+Pϑ.

Then, W is an open and symmetric subset of H0s(Ω) and Q := H0s(Ω)\ W contains only sign-changing functions. By similar arguments as in [16] (see also [13]) and [19], we have the following result which shows that for ϑ small, Pϑ± is an invariant set and all sign-changing solutions to (2.3) are contained in Q.

Lemma 3.4

There exists ϑ0 > 0 such that for any ϑ ∈ (0, ϑ0], there holds

Aε(Pϑ±)Pϑ±,

and

φε(t,u)Pϑ±for all t>0 and uPϑ±¯.

Moreover, every nontrivial solutionsuPϑ+anduPϑof (2.3) are positive and negative, respectively.

Remark 3.1

Note that there exists a constant C > 0 independent of p ∈ [2, 2*] such that ∥upCu2* for all p ∈ [2, 2*], as in the proof of Lemma 5.2 in [16], one can show that there exists ϑ0 > 0 such that for any ϑ ∈ (0, ϑ0], there holds Aε(Pϑ±)Pϑ± for all ε > 0 small enough.

In the following, we may choose an ϑ > 0 small enough such that Pϑ± is an invariant set. In order to construct nodal solution by using the combination of invariant sets method and minimax method, we need a deformation lemma in the presence of invariant sets. Since Iε satisfies the (PS) condition, using similar arguments to Lemma 5.1 in [20], we have the following result.

Lemma 3.5

DefineKε,c1:=Kε,cW,Kε,c2:=Kε,cQ,where 𝓚ε,c := {uH0s(Ω):Iε(u)=c,Iε(u)=0}.Letϱ > 0 be such that(Kε,c1)ϱWwhere(Kε,c1)ϱ:={uH0s(Ω): dist(u,Kε,c1)<ϱ}.Then there exists anδ0 > 0 such that for any 0 < δ < δ0, there existsηC([0, 1] × H0s(Ω),H0s(Ω))satisfying:

  1. η(t, u) = u for t = 0 oruIε1([cδ0,c+δ0])(Kε,c2)ϱ.

  2. η(1,Iεc+δW(Kε,c2)3ϱ)IεcδWandη(1,Iεc+δW)IεcδWifKε,c2=.HereIεd={uH0s(Ω):Iε(u)d}for any d ∈ ℝ.

  3. η(t, ⋅) is odd and a homeomorphism ofH0s(Ω) for t ∈ [0, 1].

  4. Iε(η(⋅, u)) is non-increasing.

  5. η(t, W) ⊂ W for any t ∈ [0, 1].

3.4 Existence of infinitely many sign-changing solutions

Now we prove the existence of infinitely many sign-changing solutions to problem (1.1).

Proof of Theorem 1.1

Here and in the sequel, we fix λ ∈ (0, λ1s). As in [30], we divide the proof into three steps.

Step 1. For any ε ∈ (0, 2*ζ) small, we define the minimax value cε,k for the perturbed functional Iε(u) with k = 2, 3, ⋯. Set

Gm:={hC(BREm,H0s(Ω)):h is odd and h=id on BREm},

where R > 0 is given by Lemma 3.2. Note that idGm, thus Gm ≠ ∅. For k ≥ 2, we define

Γk:={h(BREmY):hGm,mk,Y=Y is open and γ(Y)mk},

where γ(K) is the Krasnoselskii genus of the symmetric closed se K, i.e. the smallest integer n such that there exists and odd continuous map σ : KSn−1. From [22], Γk possess the following properties:

  1. Γk≠ ∅ and Γk+1⊂ Γk for all k ≥ 2.

  2. If ϕC(H0s(Ω),H0s(Ω)) is odd and ϕ = id on 𝓑REm, then ϕ(A) ∈ Γk if A ∈ Γk for all k ≥ 2.

  3. If A ∈ Γk, Z = −Z is open and γ(Z) ≤ s < k and ks ≥ 2, then A \ Z ∈ Γks.

Now, for k = 2, 3, ⋯, we can define the minimax value cε, k given by

cε,k:=infAΓksupuAQIε(u).

We need to show that cε, k (k ≥ 2) are well defined (that is for any A ∈ Γk, AQ ≠ ∅) and cε, kαε > 0, where αε is given by Lemma 3.3.

Consider the attracting domain of 0 in H0s (Ω):

D:={uH0s(Ω):φε(t,u)0, as t}.

Note that 𝓓 is open, since 0 is a local minimum of Iε and by the continuous dependence of ODE on initial data. Moreover, ∂𝓓 is an invariant set and

Pϑ+¯Pϑ¯D.

In particular, there holds

Iε(u)>0 for every uPϑ+¯Pϑ¯{0}

by the similar arguments to Lemma 3.4 in [4]. Now we claim that for any A ∈ Γk with k ≥ 2, it holds

AQD.(3.3)

Set

A=h(BREmY)

with γ(Y) ≤ mk and k ≥ 2. Define

O:={uBREm:h(u)D}.

Obviously, 𝓞 is a bounded open symmetric set with 0 ∈ 𝓞 and 𝓞 ⊂ 𝓑REm. Thus, by the Borsuk-Ulam theorem that γ(∂𝓞) = m and by the continuity of h, h(∂𝓞) ⊂ ∂𝓓. As a consequence,

h(OY)AD,

and therefore

γ(AD)γ(h(OY))γ(OY)γ(O)γ(Y)k,

by the “monotone, sub-additive and supervariant” property of the genus (cf. Proposition 5.4 in [29]). Since Pϑ+PϑD=, one has

γ(WD)1.

Thus for k ≥ 2, we conclude that

γ(AQD)γ(AD)γ(WD)k11,

which proves (3.3). Therefore, it follows from (3.3) that AQ ≠ ∅. Moreover, we have

cε,2αε>0,

because ∂𝓑ρε ⊂ 𝓓 and supAQIε ≥ inf∂𝓓Iε ≥ inf∂𝓑ρεIεαε > 0 by Lemma 3.3.

Hence, cε, k are well defined for all k ≥ 2 and 0 < αεcε, 2cε, 3 ≤ ⋯.

Now, we claim

Kε,cε,kQ,(3.4)

which implies that there exists a sign-changing critical point uε, k such that

Iε(uε,k)=cε,k,

and cε, k → ∞, as k → ∞. It can be done, using deformation Lemma 3.5 following the same arguments as in the proof of Step 1 in [30].

Step 2. We show that for any fixed k2,uε,kH0s(Ω) is uniformly bounded with respect to ε, and then uε, k converges strongly to uk in H0s (Ω) as ε → 0.

In fact, using the same Γk above, we can also define the minimax value for the auxiliary functional I* (see (3.1) by

βk:=infAΓksupuAI(u),k=2,3,.

Here, choosing R > 0 sufficiently large if necessary, we point out that Lemma 3.2 also holds for I*. Then from a ℤ2 version of the Mountain Pass Theorem (see Theorem 9.12 in [22]), for each k ≥ 2, βk > 0 is well defined and

βk,ask.

Since

Iε(u)I(u)+|Ω|2s

holds for any ε(0,2sζ), by the definition of cε, k and βk, we have

cε,kβk+|Ω|2s.

Therefore, for fixed k ≥ 2, cε, k is uniformly bounded for ε ∈ (0, 2sζ), i.e., there exists C = C(βk, Ω) > 0 independent on ε, such that cε, kC uniformly for ε. Since uε, k is a nodal solution of (2.3) and Iε(uε, k) = cε, k, one concludes that

λ1sλλ1sΩ|(Δ)s/2uε,k|2dxΩ|uε,k|2sεdx=2(2sε)2sε2cε,kC,(3.5)

which implies that uε,kH0s(Ω)C uniformly with respect to ε. Denote

wε,k=Es(uε,k).

Then, wε, k is a solution of (2.4) satisfying wε,kH0,Ls(C)C uniformly with respect to ε. So we can apply Theorem 2.1 and obtain a subsequence {wεn,k}n∈ℕ, such that

wεn,kwk strongly in H0,Ls(C)

for some wkH0,Ls(C). We set

uk=trΩwk.

Then,

uεn,kuk strongly in H0s(Ω)

by the trace inequality and also cεn,kck. Thus uk is a solution of (1.1) and I(uk) = ck. Moreover, since uεn,k is sign-changing, similar to Step 1, by Lemma 2.1, we can show that uk is still sign-changing.

Step 3. We are in a position to prove that the functional has infinitely many sign-changing critical points. Recalling that ck is non-decreasing with respect to k, we distinguish two cases:

Case I: There exist 2 ≤ k1 < ⋯ < ki < ⋯, satisfying ck1 < ⋯ < cki < ⋯.

Case II: There is a positive integer l such that ck = c for all kl.

Obviously, in Case I, problem (1.1) has infinitely many sign-changing solutions such that I(ui) = cki, thus we are done. So we assume in the sequel that Case II holds. From now on, we suppose that there exists a δ > 0, such that I(u) has no sign-changing critical point u with

I(u)[cδ,c)(c,c+δ].

Otherwise, the result follows.

We claim that

γ(Kc2)2,

where 𝓚c := {uH0s (Ω) : I(u) = c, I′(u) = 0} and Kc2 = 𝓚cQ. If it is true, I(u) has infinitely many sign-changing critical points and thus we are done. Here we borrow some ideas used in [11]. Arguing by contradiction, suppose that

γ(Kc2)=1

(note that Kc2 ≠ ∅). Moreover, we assume Kc2 contains only finitely many critical points, otherwise the proof is completed. As a consequence, Kc2 is compact. Clearly, 0 ∉ Kc2. Thus there exists a open neighborhood N in H0s (Ω) with Kc2N such that γ(N) = γ( Kc2).

Define

Uε:=Iε1([cδ,c+δ])N.

Now we claim that for ε > 0 small, Iε has no sign-changing critical point in Uε. Indeed, if not, we suppose that there exist εn → 0 and unUεn satisfying Iεn(un)=0,withun±0,andunN. Obviously,

Iεn(un)[cδ,c+δ].

Then, similar to (3.5), one can obtain that unH0s(Ω)C uniformly with respect to n. Set

wn=Es(un).

By Lemma 2.1wn is a solution of (2.4) satisfying wnH0,Ls(C)C uniformly with respect to n. Therefore, by Theorem 2.1, we obtain, up to a subsequence, that

wnw strongly in H0,Ls(C)

for some wH0,Ls (𝓒). We set

u=trΩw.

Clearly, unu strongly in H0s (Ω). Thus

I(u)=0,I(u)[cδ,c+δ] and uKc2.

But u is still sign-changing, a contradiction.

From the above observation, one can easily show that for any ε > 0 small, there exists a constant αε > 0 such that

Iε(u)αε,for uIε1([cδ,c+δ])NW.

Then, as in [11], standard techniques show that for ε > 0 small enough, there exists an odd homeomorphism ηC( H0s(Ω), H0s(Ω)) such that η(u) = u for uIεc2δ and

η(Iεc+δWN)IεcδW.(3.6)

See for example the proof of Theorem A.4 in [22] and also Lemma 5.1 in [20].

Now fix k > l. Since cε, k, cε,k+1c as ε → 0, we can find an ε > 0 small, such that

cε,k,cε,k+1(cδ4,c+δ4).

By the definition of cε,k+1, we can find a set A ∈ Γk+1, A = h(𝓑REmY), where hGm, mk + 1, γ(Y)≤ m − (k + 1), such that

Iε(u)cε,k+1+δ4<c+δ2,

for any uAQ, which implies, AIεc+δ2W Then by (3.6), we have

η(AN)Iεcδ2W.(3.7)

Let Y~ = Yh−1(N). Then Y~ is symmetric and open, and

γ(Y~)γ(Y)+γ(h1(N))m(k+1)+1=mk.

Therefore one can obtain that A^:=η(h(BREmY~))Γk by (2) and (3) above. Consequently, by (3.7),

cε,ksupA^QIεsupη(AN)QIεcδ2,

which contradicts to

cε,k>cδ4.

Hence the proof is completed and the functional I has infinitely many sign-changing critical points.  □


Dedicated to Professor Virginia Kiryakova on the occasion of her 65th birthday and the 20th anniversary of FCAA


Acknowledgements

L. Li is supported by Research Fund of National Natural Science Foundation of China (No. 11601046), Chongqing Science and Technology Commission (No. cstc2016jcyjA0310), Chongqing Municipal Education Commission (No. KJ1600603), Chongqing Technology and Business University (No. 2015-56-09, 1552007) and Program for University Innovation Team of Chongqing (No. CXTDX201601026).

J. Sun is supported by Research Fund of National Natural Science Foundation of China (No. 11501280) and Natural Science Foundation of Jiangxi Province (No. 20151BAB211001).

The work of S. Tersian is in the frames of the bilateral research project between Bulgarian and Serbian Academies of Sciences, “Analytical and numerical methods for differential and integral equations and mathematical models of arbitrary (fractional or high) order”.

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Received: 2017-02-27
Published Online: 2017-10-31
Published in Print: 2017-10-26

© 2017 Diogenes Co., Sofia

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