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Multiple Solutions for Superlinear Fractional Problems via Theorems of Mixed Type

  • Vincenzo Ambrosio EMAIL logo
Published/Copyright: March 1, 2018

Abstract

In this paper, we investigate the existence of multiple solutions for the following two fractional problems:

{ ( - Δ Ω ) s u - λ u = f ( x , u ) in  Ω , u = 0 in  Ω    and    { ( - Δ N ) s u - λ u = f ( x , u ) in  Ω , u = 0 in  N Ω ,

where s(0,1), N>2s, Ω is a smooth bounded domain of N, and f:Ω¯× is a superlinear continuous function which does not satisfy the well-known Ambrosetti–Rabinowitz condition. Here (-ΔΩ)s is the spectral Laplacian and (-ΔN)s is the fractional Laplacian in N. By applying variational theorems of mixed type due to Marino and Saccon and the Linking Theorem, we prove the existence of multiple solutions for the above problems.

1 Introduction

In this paper, we focus our attention on the multiplicity of the following two fractional problems:

(1.1) { ( - Δ Ω ) s u - λ u = f ( x , u ) in  Ω , u = 0 in  Ω

and

(1.2) { ( - Δ N ) s u - λ u = f ( x , u ) in  Ω , u = 0 in  N Ω ,

where s(0,1), N>2s, λ and ΩN is a smooth bounded open set. Here (-ΔΩ)s is the spectral Laplacian which is given by

( - Δ Ω ) s u ( x ) = k = 1 + c k α k s φ k ( x ) for any  u = k = 1 + c k φ k C c ( Ω ) ,

where {φk}k denotes the orthonormal basis of L2(Ω) consisting of eigenfunctions of -Δ in Ω with homogeneous Dirichlet boundary conditions associated to the eigenvalues {αk}k, that is,

{ - Δ φ k = α k φ k in  Ω , φ k = 0 in  Ω .

The fractional Laplacian operator (-ΔN)s may be defined for any u:N belonging to the Schwarz space 𝒮(N) of rapidly decaying C functions in N by

( - Δ N ) s u ( x ) = C N , s 2 N 2 u ( x ) - u ( x + y ) - u ( x - y ) | y | N + 2 s 𝑑 y ,

where CN,s is a normalizing constant depending only on N and s; see [15, 22] for more details.

As observed in [30], these two operators are completely different. Indeed, the spectral operator (-ΔΩ)s depends on the domain Ω considered, while the integral one (-ΔN)s evaluated at some point is independent on the domain in which the equation is set. Moreover, in contrast with the setting for the fractional Laplacian, it is not true that all functions are s-harmonic with respect to the spectral fractional Laplacian, up to a small error; see [1, 16] for more details.

Recently, many papers have appeared dealing with the existence and the multiplicity of solutions to problems driven by these two operators, by applying several variational and topological techniques. In particular, a great attention has been devoted to the study of fractional problems like (1.1) and (1.2) involving superlinear nonlinearities with subcritical or critical growth; see for instance [4, 5, 6, 3, 7, 8, 9, 10, 12, 22, 26, 28, 29, 31, 34]. It is worth observing that a typical assumption to study this class of problems is to require that the nonlinearity f verifies the well-known Ambrosetti–Rabinowitz condition [2], that is, there exist μ>2 and R>0 such that

(1.3) 0 < μ F ( x , t ) t f ( x , t ) for any  x Ω , | t | > R .

This condition is quite natural and fundamental not only to guarantee that the Euler–Lagrange functional associated to the problem under consideration has a mountain pass geometry, but also to show that the Palais–Smale sequence of the Euler–Lagrange functional is bounded. We recall that (1.3) is somewhat restrictive and eliminates many nonlinearities. For instance the function

(1.4) f ( x , t ) = 2 t log ( 1 + t 4 ) + 4 t 5 t 4 + 1 with  ( x , t ) Ω ×

is superlinear at infinity but does not verify the condition (1.3).

The purpose of this paper is to investigate the multiplicity for the above two fractional problems when the parameter λ lies in a suitable neighborhood of any eigenvalue of the fractional operator under consideration, and f is superlinear and subcritical, but does not fulfill (1.3).

More precisely, along the paper we assume that f:Ω¯× is a continuous function satisfying the following conditions:

  1. there exist c1>0 and p(1,2s*-1), with 2s*=2NN-2s, such that

    | f ( x , t ) | c 1 ( 1 + | t | p ) for any  ( x , t ) Ω × ;

  2. lim | t | 0 f ( x , t ) | t | = 0 uniformly in  x Ω ;

  3. lim | t | F ( x , t ) t 2 = + uniformly in  x Ω ,

    where

    F ( x , t ) = 0 t f ( x , τ ) 𝑑 τ ;

  4. there exist β(2NpN+2s,2s*), c2>0 and T>0 such that

    f ( x , t ) t - 2 F ( x , t ) > 0 for any  x Ω , | t | > 0 ,
    f ( x , t ) t - 2 F ( x , t ) c 2 | t | β for any  x Ω , | t | T ;

  5. F ( x , t ) 0 for any (x,t)Ω×.

As a model for f we can take the function defined in (1.4).

Now we state our first main result regarding the multiplicity for problem (1.1):

Theorem 1.1.

Assume (f1)(f5). Then for any i2 there exists δi>0 such that for any λ(αis-δi,αis), problem (1.1) admits at least three nontrivial solutions.

In order to prove Theorem 1.1, we apply suitable variational methods after transforming problem (1.1) into a degenerate elliptic equation with a nonlinear Neumann boundary condition by using the extension technique [11, 12, 13, 14]. Thanks to this approach we are able to overcome the nonlocality of the operator (-ΔΩ)s and we can use some critical point results to study the extended problem. More precisely, we show that the functional associated to the extended problem respects the geometry required by the -Theorem introduced by Marino and Saccon in [19]. Roughly speaking, this theorem says that if a C1-functional I defined on a Hilbert space has a linking structure and I verifies an appropriate condition on some suitable sets (see Definition 2.7 below), then I has two nontrivial critical points which may have the same critical level. We will apply this abstract result to the functional associated to the extended problem and we will get the existence of two nontrivial solutions. Finally, exploiting an additional linking structure, we get the existence of a third nontrivial solution. We recall that in the local setting, similar arguments have been developed and applied in many situations to obtain multiplicity results for several and different problems such as elliptic problems of second and fourth order, noncooperative elliptic systems, nonlinear Schrödinger equations with indefinite linear part in N, variational inequalities; see [18, 20, 25, 32, 33]. Differently from the classic case, in the nonlocal framework, the only result comparable to Theorem 1.1 is due to Mugnai and Pagliardini [24] who obtained a multiplicity result to problem (1.1) when s=12 and f satisfies (1.3).

Our second main result concerns the multiplicity of solutions to (1.2).

Theorem 1.2.

Assume (f1)(f5). Then for any i2 there exists δi>0 such that for any λ(λi-δi,λi), problem (1.2) admits at least three nontrivial solutions. Here {λk}kN are the eigenvalues of the fractional Laplacian (-ΔRN)s with homogeneous condition in RNΩ.

The proof of the above result is obtained following the approach developed to prove Theorem 1.1. Anyway, we do not make use of any extension method and our techniques work also when we replace (-ΔN)s by the more general integro-differential operator -K defined up to a positive constant as

𝒦 u ( x ) = N ( u ( x + y ) + u ( x - y ) - 2 u ( x ) ) 𝒦 ( y ) 𝑑 y , x N ,

where 𝒦:N{0}(0,) is a measurable function such that 𝒦(-x)=𝒦(x) for all xN{0}, m𝒦L1(N) with m(x)=min{|x|2,1}, and there exists θ>0 such that 𝒦(x)θ|x|-(N+2s) for all xN{0}.

In this context, we take care of the well-known results on the spectrum of integro-differential operators obtained by Servadei and Valdinoci in [29, 30]. We point out that in a recent paper Molica Bisci et al. [21] proved a similar result to Theorem 1.2 when f verifies condition (1.3), obtaining a nonlocal counterpart of the multiplicity result established in [23].

The paper is organized as follows. In Section 2, we recall some useful results related to the extension method in a bounded domain and then we provide some useful lemmas which will be fundamental to apply a critical point theorem of mixed nature. In Section 3, we deal with the existence of three nontrivial weak solutions to problem (1.2).

2 Multiplicity for Problem (1.1)

2.1 Extended Problem in the Half-Cylinder

In order to study problem (1.1), we use a suitable variant of the extension technique due to Caffarelli and Silvestre [13]; see [11, 12, 14] for more details. Firstly, we collect some useful notations and basic results which will be useful along the paper.

Fix s(0,1). We say that uHs(Ω) if uL2(Ω) and it holds

[ u ] H s ( Ω ) 2 = Ω × Ω | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y < .

We define H0s(Ω) as the closure of Cc(Ω) with respect to the norm [u]Hs(Ω)2+uL2(Ω)2. The space H001/2(Ω) is the Lions–Magenes space [17] which consists of the function uH1/2(Ω) such that

Ω u 2 ( x ) dist ( x , Ω ) 𝑑 x < .

Let us introduce the Hilbert space

s ( Ω ) = { u L 2 ( Ω ) : k = 1 | c k | 2 α k s < } .

It is well known [17] that interpolation leads to

s ( Ω ) = { H s ( Ω ) if  s ( 0 , 1 2 ) , H 00 1 / 2 ( Ω ) if  s = 1 2 , H 0 s ( Ω ) if  s ( 1 2 , 1 ) .

Let us define the cylinder 𝒞=Ω×(0,+) and its lateral boundary L𝒞=Ω×[0,+). Let us denote by H0,L1(y1-2s) the space of measurable functions v:𝒞 such that vH1(Ω×(α,β)) for all 0<α<β<+, u=0 on L𝒞 and for which the following norm is finite:

u H 0 , L 1 ( y 1 - 2 s ) 2 = 𝒞 y 1 - 2 s | u | 2 𝑑 x 𝑑 y .

We recall the following trace theorem which relates H0,L1(y1-2s) to s(Ω).

Theorem 2.1 ([11, 12, 14]).

There exists a surjective continuous linear map Tr:H0,L1(y1-2s)Hs(Ω) such that, for any uH0,L1(y1-2s),

κ s Tr ( u ) s ( Ω ) 2 u H 0 , L 1 ( y 1 - 2 s ) 2 .

We also have some useful embedding results.

Theorem 2.2 ([11, 12, 14]).

Let N>2s and q[1,2s*]. Then there exists a constant C depending on N, q and the measure of Ω, such that, for all uX0,

Tr ( u ) L q ( Ω ) C u H 0 , L 1 ( y 1 - 2 s ) .

Moreover, H0,L1(y1-2s) is compactly embedded into Lq(Ω) for any q[1,2s*).

Thus, we get the following fundamental result which allows us to realize the fractional spectral Laplacian (-ΔΩ)s.

Theorem 2.3 ([11, 12, 14]).

Let uHs(Ω). Then there exists a unique vH0,L1(y1-2s) such that

{ - div ( y 1 - 2 s v ) = 0 in  𝒞 , v = 0 on  L 𝒞 , Tr ( v ) = u on  0 𝒞 .

Moreover,

v ν 1 - 2 s := - lim y 0 + y 1 - 2 s v y ( x , y ) = κ s ( - Δ Ω ) s u ( x ) in  s ( Ω ) * ,

where Hs(Ω)* is the dual of Hs(Ω). The function v is called the extension of u.

We also recall that if u=k=1ckφks(Ω), then the extension of u is given by

v ( x , y ) = k = 1 c k φ k ( x ) θ ( λ k y ) ,

where θH1(+,y1-2s) solves the problem

{ θ ′′ + 1 - 2 s y θ - θ = 0 in  + , θ ( 0 ) = 1 , - lim y 0 + y 1 - 2 s θ ( y ) = κ s .

In addition,

v H 0 , L 1 ( y 1 - 2 s ) 2 = κ s u s ( Ω ) 2 ;

see [11, 12, 14] for more details.

Remark 2.4.

In order to simplify notation, when no confusion arises, we shall denote by v the function defined in the cylinder 𝒞 as well as its trace Tr(v) on Ω×{y=0}.

Taking into account the above results, we can deduce that the study of (1.1) is equivalent to consider the following degenerate elliptic problem with nonlinear Neumann boundary condition:

(2.1) { div ( y 1 - 2 s u ) = 0 in  𝒞 , u = 0 on  L 𝒞 , u ν 1 - 2 s = κ s [ λ u + f ( x , u ) ] on  Ω × { 0 } .

For simplicity, in what follows, we will assume that κs=1.

2.2 Technical Lemmas and -Condition

For i2, let us introduce the following notations. Let Hi=span{ψ1,,ψi}, where ψk(x,y)=φk(x)θ(λky),

H i = { u H 0 , L 1 ( y 1 - 2 s ) : u , ψ j H 0 , L 1 ( y 1 - 2 s ) = 0  for all  j = 1 , , i }

and Hi0={ψi,,ψj}. We set μi=αis. Since {αk}k is increasing, a direct calculation yields the next result.

Lemma 2.5.

For any i1, the following inequalities hold:

(2.2) u H 0 , L 1 ( y 1 - 2 s ) 2 μ i u L 2 ( Ω ) 2 for any  u H i ,
(2.3) u H 0 , L 1 ( y 1 - 2 s ) 2 μ i + 1 u L 2 ( Ω ) 2 for any  u H i .

Now, we prove a very useful lemma.

Lemma 2.6.

Let K:L2(Ω)H0,L1(y1-2s) be the operator defined by setting K(u)=v, where v is the unique solution to

(2.4) { - div ( y 1 - 2 s v ) = 0 in  𝒞 , v = 0 on  L 𝒞 , v ν 1 - 2 s = u on  0 𝒞 .

Then K is compact.

Proof.

Let {un}n be a bounded sequence in L2(Ω). From the weak formulation of (2.4) and Theorem 2.2, we can see that

v n H 0 , L 1 ( y 1 - 2 s ) 2 u n L 2 ( Ω ) v n L 2 ( Ω ) C u n L 2 ( Ω ) v n H 0 , L 1 ( y 1 - 2 s ) ,

that is, {vn}n is bounded in H0,L1(y1-2s). Then, in view of Theorem 2.2, we may assume that

(2.5) { v n v in  H 0 , L 1 ( y 1 - 2 s ) , v n v in  L q ( Ω ) for all  q [ 1 , 2 s * ) .

Now, by using (2.4), we can see that, for any n,

(2.6) v n H 0 , L 1 ( y 1 - 2 s ) 2 - 𝒞 y 1 - 2 s v n v d x d y = Ω u n ( v n - v ) 𝑑 x .

Taking into account (2.5) and the fact that {un}n is bounded in L2(Ω), from (2.6) we can deduce that

v n H 0 , L 1 ( y 1 - 2 s ) v H 0 , L 1 ( y 1 - 2 s ) .

Since H0,L1(y1-2s) is a Hilbert space, we can conclude the proof. ∎

In order to deduce a multiplicity result for (2.1), we need to recall the -Theorem due to Marino and Saccon [19]. We begin with the following definition.

Definition 2.7.

Let X be a Hilbert space, IC1(X,) and M a closed subspace of X, a,b{-,+}. We say that the condition ()(I,M,a,b) holds if there is γ>0 such that

inf { P M I ( u ) : a I ( u ) b , dist ( u , M ) < γ } > 0 ,

where PM:XM is the orthogonal projection of X onto M.

Therefore, if the above condition holds, then I|M has no critical points u such that aI(u)b, with some uniformity.

Theorem 2.8 ([19]).

Let X be a Hilbert space and Xi, i=1,2,3, three subspaces of X such that X=X1X2X3 and dim(Xi)<+ with i=1,2. Let us denote by Pi the orthogonal projection of X onto Xi, IC1,1(X,R). Let R,R,R′′,ϱ>0 such that R<ϱ<R′′. Define

Γ = { u X 1 X 2 : R u R ′′ , P 1 u R } , T = X 1 X 2 Γ ,
S 23 ( ϱ ) = { u X 2 X 3 : u = ϱ } , B 23 ( ϱ ) = { u X 2 X 3 : u ϱ } .

Especially, if R=0, T may be defined as follows:

T = { u X 1 : u R } { u X 1 X 2 : P 2 u = R ′′ , P 1 u R }
{ u X 1 X 2 : P 2 u R ′′ , P 1 u = R } .

Assume that

a = sup I ( T ) < inf I ( S 23 ( ϱ ) ) = a ′′ .

Let a and b such that a<a<a′′ and b>supI(Γ). Assume that ()(I,X1X3,a,b) holds and that the (PS)c condition holds at any c[a,b]. Then I has at least two critical points in I-1([a,b]). Moreover, if

inf I ( B 23 ( ϱ ) ) > a 1 > -

and the (PS)c condition holds at any c[a1,b], then I has another critical level in [a1,a].

Now, we introduce the energy functional Iλ:H0,L1(y1-2s) associated to (2.1), that is,

I ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x

defined for any uH0,L1(y1-2s). From the assumptions on f, it is clear that the functional Iλ is well-defined, IλC1(H0,L1(y1-2s),) and its derivative is given by

I λ ( u ) , v = 𝒞 y 1 - 2 s u v d x d y - λ Ω u v 𝑑 x - Ω f ( x , u ) v 𝑑 x for any  v H 0 , L 1 ( y 1 - 2 s ) .

Since we aim to show that Iλ verifies the assumptions of Theorem 2.8, we need to prove some useful lemmas which allow us to verify that there exist 0<a<b such that the condition ()(Iλ,Hi-1Hi,a,b) holds.

Lemma 2.9.

Assume that (f1) and (f4) hold. Then, for any δ(0,min{μi+1-μi,μi-μi-1}) there exists ε0>0 such that for any λ[μi-δ,μi+δ] the unique critical point u of Iλ constrained on Hi-1Hi such that Iλ(u)[-ε0,ε0] is the trivial one.

Proof.

Suppose by contradiction that there exist δ0, λn[μi-δ0,μi+δ0] and {un}nHi-1Hi{0} such that, for any vHi-1Hi we get

(2.7) I λ n ( u n ) = 1 2 𝒞 y 1 - 2 s | u n | 2 𝑑 x 𝑑 y - λ n 2 Ω | u n | 2 𝑑 x - Ω F ( x , u n ) 𝑑 x 0 ,
(2.8) I λ n ( u n ) , v = 𝒞 y 1 - 2 s u n v d x d y - λ n Ω u n v 𝑑 x - Ω f ( x , u n ) v 𝑑 x = 0 .

Up to a subsequence, we may assume that λnλ[μi-δ0,μi+δ0] as n. Let us define

A n := { x Ω : | u n ( x ) | T } .

Then, by assumption (f4) we deduce

(2.9) 2 I λ n ( u n ) - I λ n ( u n ) , u n = Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x c 2 A n | u n | β 𝑑 x .

By using (2.7) and (2.8) with v=un, from inequality (2.9) we get

(2.10) A n | u n | β 𝑑 x 0 as  n .

Now, let us observe that

(2.11) Ω | u n | β 𝑑 x = A n | u n | β 𝑑 x + Ω A n | u n | β 𝑑 x A n | u n | β 𝑑 x + | Ω | T β .

Set un=vn+wnHi-1Hi. Then, by using (2.2), (2.3), the fact that

u n H 0 , L 1 ( y 1 - 2 s ) 2 = v n H 0 , L 1 ( y 1 - 2 s ) 2 + w n H 0 , L 1 ( y 1 - 2 s ) 2 ,

and (2.8), we have

Ω f ( x , u n ) ( w n - v n ) 𝑑 x = w n H 0 , L 1 ( y 1 - 2 s ) 2 - λ n Ω | w n | 2 𝑑 x - v n H 0 , L 1 ( y 1 - 2 s ) 2 + λ n Ω | v n | 2 𝑑 x
μ i + 1 - λ n μ i + 1 w n H 0 , L 1 ( y 1 - 2 s ) 2 - μ i - 1 - λ n μ i - 1 v n H 0 , L 1 ( y 1 - 2 s ) 2
(2.12) c 3 u n H 0 , L 1 ( y 1 - 2 s ) 2 ,

where c3=min{μi+1-λnμi+1,λn-μi-1μi-1}.

From Theorem 2.2 and by applying Hölder’s inequality, we can infer that

Ω f ( x , u n ) ( w n - v n ) 𝑑 x ( Ω | f ( x , u n ) | p + 1 p 𝑑 x ) p p + 1 ( Ω | w n - v n | p + 1 𝑑 x ) 1 p + 1
(2.13) 2 C u n H 0 , L 1 ( y 1 - 2 s ) ( Ω | f ( x , u n ) | p + 1 p 𝑑 x ) p p + 1 .

Taking into account (2.12) and (2.13), and recalling that un0, we have

(2.14) u n H 0 , L 1 ( y 1 - 2 s ) c 4 ( Ω | f ( x , u n ) | p + 1 p 𝑑 x ) p p + 1

for some positive constant c4.

Now, by using (f1), Theorem 2.2, (2.11) and Hölder’s inequality, we can deduce that

| Ω f ( x , u n ) ( v n - w n ) 𝑑 x | Ω | f ( x , u n ) | | v n - w n | 𝑑 x
c 1 Ω ( | v n - w n | + | u n | p | v n - w n | ) 𝑑 x
c 1 v n - w n L 1 ( Ω ) + c 1 ( Ω | u n | β 𝑑 x ) p β ( Ω | v n - w n | β β - p 𝑑 x ) β - p β
c 1 C v n - w n H 0 , L 1 ( y 1 - 2 s ) ( 1 + ( A n | u n | β 𝑑 x + | Ω | T β ) p β )
(2.15) c 1 C u n H 0 , L 1 ( y 1 - 2 s ) ( 1 + ( A n | u n | β + | Ω | T β ) p β ) .

Therefore, putting together (2.10), (2.12) and (2.15), we deduce that {un}n is bounded in H0,L1(y1-2s). Hence, in view of Theorem 2.2, we may assume that, up to a subsequence, there are a sequence {un}n and a function uH0,L1(y1-2s) such that

(2.16) { u n u in  H 0 , L 1 ( y 1 - 2 s ) , u n u in  L r ( Ω ) for all  r [ 1 , 2 s * ) , u n ( x ) u ( x ) a.e.  x Ω .

By applying (2.7), (2.8) and Fatou’s lemma, we get

0 = lim n 2 I λ n ( u n ) - I λ n ( u n ) , u n
= lim n Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x
Ω lim inf n ( f ( x , u n ) u n - 2 F ( x , u n ) ) d x
= Ω ( f ( x , u ) u - 2 F ( x , u ) ) 𝑑 x

which, combined with assumptions (f2) and (f4), gives u=0.

Now, we distinguish two cases. Let us assume that un0 as n in H0,L1(y1-2s). From (f1) and (f2) we know that for any ε>0 there exists cε>0 such that

(2.17) | f ( x , t ) | ε | t | + c ε | t | p for any  ( x , t ) Ω × .

By using (2.14), (2.17) and Theorem 2.2, we have

1 lim n c 4 ( Ω | f ( x , u n ) | p + 1 p 𝑑 x ) p p + 1 u n H 0 , L 1 ( y 1 - 2 s ) = 0 .

On the other hand, if there exists α>0 such that unH0,L1(y1-2s)α for n large enough, then from (2.14), (2.16), (f2), the Dominated Convergence Theorem and u=0, we get

0 < α lim n c 4 ( Ω | f ( x , u n ) | p + 1 p 𝑑 x ) p p + 1 = 0 ,

which is a contradiction. This ends the proof of the lemma. ∎

Lemma 2.10.

Assume that (f1) and (f4) hold, λ(μi-1,μi+1) and {un}nNH0,L1(y1-2s) such that Iλ(un) is bounded, Pun0 and QIλ(un)0 as n+. Then {un}nN is bounded in H0,L1(y1-2s).

Proof.

Assume by contradiction that, up to a subsequence, unH0,L1(y1-2s) as n.

Note that un=Pun+Qun, Pun0 in H0,L1(y1-2s) and QIλ(un)0, where Iλ(un)=vn is such that

I λ ( u n ) , z = 𝒞 y 1 - 2 s v n z d x d y

for any zH0,L1(y1-2s). So we get

v n = u n - K ( λ u n + f ( x , u n ) ) ,

where K is defined as in Lemma 2.6. Now, we recall that un=Pun+Qun and Pun0 in H0,L1(y1-2s). Then, by exploiting assumption (f1), Hölder’s inequality and the fact that all norms in Hi0 are equivalent, we can see that

| Ω f ( x , u n ) P u n 𝑑 x | Ω | f ( x , u n ) | | P u n | 𝑑 x
c 1 ( Ω | P u n | 𝑑 x + Ω | P u n | | u n | p 𝑑 x )
c 1 P u n L 1 ( Ω ) + c 1 ( Ω | u n | β 𝑑 x ) p β ( Ω | P u n | β β - p 𝑑 x ) β - p β
(2.18) c 5 P u n L ( Ω ) ( 1 + u n L β ( Ω ) p ) ,

with c5>0. Now, from assumption (f4) and (2.18), we can deduce that

2 I λ ( u n ) - Q I λ ( u n ) , u n
= Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x + P u n H 0 , L 1 ( y 1 - 2 s ) 2 - λ Ω | P u n | 2 𝑑 x - Ω f ( x , u n ) P u n 𝑑 x
(2.19) c 2 u n L β ( Ω ) β + P u n H 0 , L 1 ( y 1 - 2 s ) 2 - λ P u n L 2 ( Ω ) 2 - c 5 P u n L ( Ω ) ( 1 + u n L β ( Ω ) p ) .

Here we used that for every zH0,L1(y1-2s), Pz is smooth and Pun=Pun due to uspan{ψi,,ψj} and PzQz, so we have

𝒞 y 1 - 2 s ( P ( u n - K ( λ u n + g ( x , u n ) ) ) ) u n d x d y
= P u n H 0 , L 1 ( y 1 - 2 s ) 2 - λ Ω | P u n | 2 𝑑 x - Ω f ( x , u n ) P u n 𝑑 x .

Since 1<p<β, dimHi0<+ and PunL(Ω)0 as n, from (2.19) we can infer that

(2.20) u n L β ( Ω ) p u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n .

Set Qun=vn+wnHi-1Hi. By using (f1), Theorem 2.2, (2.2) and Hölder’s inequality, we have

Q I λ ( u n ) , - v n = λ v n L 2 ( Ω ) 2 - v n H 0 , L 1 ( y 1 - 2 s ) 2 + Ω f ( x , u n ) v n 𝑑 x
λ - μ i - 1 μ i - 1 v n 2 - Ω | f ( x , u n ) | | v n | 𝑑 x
λ - μ i - 1 μ i - 1 v n H 0 , L 1 ( y 1 - 2 s ) 2 - c 1 Ω ( | u n | p | v n | + | v n | ) 𝑑 x
λ - μ i - 1 μ i - 1 v n H 0 , L 1 ( y 1 - 2 s ) 2 - c 1 ( Ω | u n | β 𝑑 x ) p β ( Ω | v n | β β - p 𝑑 x ) β - p β - c 1 v n L 1 ( Ω )
λ - μ i - 1 μ i - 1 v n H 0 , L 1 ( y 1 - 2 s ) 2 - c 1 C v n H 0 , L 1 ( y 1 - 2 s ) ( 1 + u n L β ( Ω ) p ) .

Therefore, (2.20) and Hölder’s inequality imply that

(2.21) v n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n .

In a similar fashion, we can infer that

(2.22) w n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n .

We can also show that

(2.23) P u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n .

Indeed, if (2.23) does not hold, then

P u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) ( 0 , + )

and we can see that

0 P u n H 0 , L 1 ( y 1 - 2 s ) = P u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) ( + ) = + ,

which is impossible. Putting together (2.21), (2.22) and (2.23), we deduce that

1 = u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) v n H 0 , L 1 ( y 1 - 2 s ) + P u n H 0 , L 1 ( y 1 - 2 s ) + w n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n ,

which is a contradiction. Thus {un}n is bounded in H0,L1(y1-2s). ∎

Lemma 2.11.

Assume (f1) and (f4). Then, for any δ(0,min{μi+1-μi,μi-μi-1}) there exists ε0>0 such that for any λ[μi-δ,μi+δ] and for any ε1,ε2(0,ε0) with ε1<ε2, the condition ()(Iλ,Hi-1Hi,ε1,ε2) holds.

Proof.

Suppose by contradiction that there exists a positive constant δ0 such that for all ε0>0 there are λ[μi-δ0,μi+δ0] and ε1,ε2(0,ε0) with ε1<ε2 such that the condition ()(Iλ,Hi-1Hi,ε1,ε2) does not hold.

Take ε0>0 as given by Lemma 2.9 and assume the existence of a sequence {un}nH0,L1(y1-2s) such that dist(un,Hi-1Hi)0, Iλ(un)(ε1,ε2) and QIλ(Un)0. By Lemma 2.10 we deduce that {un}n is bounded. Thus, by applying Theorem 2.2, there are a subsequence (still denoted by un) and uH0,L1(y1-2s) such that unu in H0,L1(y1-2s) and unu in Lq(Ω) for any q[1,2s*). Taking into account assumption (f1), QIλ(un)0, Pun0, and Lemma 2.6, we can see that

Q I λ ( u n ) = u n - P u n - K ( λ u n + f ( x , u n ) )

yields unu in H0,L1(y1-2s) and u is a critical point of Iλ constrained on Hi-1Hi. Hence, in view of Lemma 2.9, we can infer that u=0. Since 0<ε1Iλ(u), we obtain a contradiction. ∎

Let us introduce the following notations: for fixed i,k and R,ϱ>0, let

B i ( R ) = { u H i : u H 0 , L 1 ( y 1 - 2 s ) R } ,
T i - 1 , i ( R ) = { u H i - 1 : u H 0 , L 1 ( y 1 - 2 s ) R } { u H i : u H 0 , L 1 ( y 1 - 2 s ) = R } ,
S k + ( ϱ ) = { u H k : u H 0 , L 1 ( y 1 - 2 s ) = ϱ } ,
B k + ( ϱ ) = { u H k : u H 0 , L 1 ( y 1 - 2 s ) ϱ } .

Lemma 2.12.

Assume (f1)(f3) and (f5). Then, for any λ(μi-1,μi+1), there are R>ϱ>0 such that

0 = sup I λ ( T i - 1 , i ( R ) ) < inf I λ ( S i - 1 + ( ϱ ) ) .

Proof.

By using (2.2) and assumption (f5), for any uHi-1 and λ(μi-1,μi) we have

(2.24) I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x μ i - 1 - λ 2 μ i - 1 u H 0 , L 1 ( y 1 - 2 s ) 2 0 .

Taking into account assumption (f3) and the continuity of F, for any c6>0 there is M1>0 such that

(2.25) F ( x , t ) c 6 2 t 2 - M 1 for all  ( x , t ) Ω × .

By using (2.2) and (2.25), for any uHi and λ(μi-1,μi) we have

I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x
μ i - λ 2 μ i u H 0 , L 1 ( y 1 - 2 s ) 2 - c 6 2 u L 2 ( Ω ) 2 + M 1 | Ω |
(2.26) μ i - λ - c 6 2 μ i u H 0 , L 1 ( y 1 - 2 s ) 2 + M 1 | Ω | .

Taking c6=2(μi-λ), from (2.26) we deduce that

(2.27) I λ ( u ) - as  u H 0 , L 1 ( y 1 - 2 s ) .

Now, we note that (f1) and (f2) imply that for any ε>0 there is Cε>0 such that

F ( x , t ) ε 2 t 2 + C ε | t | p + 1 for all  ( x , t ) Ω × ,

which gives

(2.28) | Ω F ( x , u ) 𝑑 x | ε 2 u L 2 ( Ω ) 2 + C ε u L p + 1 ( Ω ) p + 1 for all  u H 0 , L 1 ( y 1 - 2 s ) .

Thus, from (2.28), we can see that, for any uHi-1,

I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(2.29) μ i - λ - ε 2 μ i u H 0 , L 1 ( y 1 - 2 s ) 2 - C C ε u H 0 , L 1 ( y 1 - 2 s ) p + 1 .

Take ε=(μi-λ)/2>0. Recalling that λ(μi-1,μi) and p+1>2, from (2.24), (2.27) and (2.29), we can find R>ϱ>0 such that

sup I λ ( T i - 1 , i ( R ) ) < inf I λ ( S i - 1 + ( ϱ ) ) .

Lemma 2.13.

Assume that (f5) holds. Then, for R>0 in Lemma 2.12 and for any ε>0 there exists δi>0 such that for any λ(μi-δi,μi) it holds

sup I λ ( B i ( R ) ) < ε .

Proof.

By using (2.2), assumption (f5) and λ<μi, we deduce that, for any uHi,

I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x μ i - λ 2 μ i u H 0 , L 1 ( y 1 - 2 s ) 2 .

Take δi=μiε/R2. Then we deduce that

sup I λ ( B i ( R ) ) μ i - λ 2 μ i R 2 = ( μ i - λ ) ε 2 δ i < ε .

Lemma 2.14.

Assume that (f1) and (f4) hold. Then Iλ verifies the Palais–Smale condition.

Proof.

Let {un}n be a Palais–Smale sequence of Iλ. Taking into account (f1), we have only to show that {un}n is bounded. From the arguments in Lemma 2.10, it is enough to prove that

(2.30) P u n H 0 , L 1 ( y 1 - 2 s ) u n H 0 , L 1 ( y 1 - 2 s ) 0 as  n + .

In view of (f4), we know that there exist c7,c8>0 such that

f ( x , t ) t - 2 F ( x , t ) c 7 | t | - c 8 for any  ( x , t ) Ω × .

Then, by using the above inequality, the equivalence of the norms on the finite-dimensional space, and Theorem 2.2, we get

2 I λ ( u n ) - I λ ( u n ) , u n = Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x
Ω ( c 7 | u n | - c 8 ) 𝑑 x
Ω ( c 7 | P u n | - c 7 | v n | - c 7 | w n | - c 8 ) 𝑑 x
c 9 P u n L 1 ( Ω ) - c 10 ( v n H 0 , L 1 ( y 1 - 2 s ) + w n H 0 , L 1 ( y 1 - 2 s ) + 1 )
(2.31) c 9 P u n H 0 , L 1 ( y 1 - 2 s ) - c 10 ( v n H 0 , L 1 ( y 1 - 2 s ) + w n H 0 , L 1 ( y 1 - 2 s ) + 1 ) .

Putting together (2.21), (2.22) and (2.31), we can deduce that (2.30) holds. ∎

Now we are in the position to give the proof of the main result of this section.

Proof of Theorem 1.1.

Firstly, we prove the existence of two critical points. Taking into account Lemmas 2.11, 2.12 and 2.13, we can take a(0,infIλ(Si-1+(ϱ))) and b>supIλ(Bi(R)) such that 0<a<b<ε0. Then the condition ()(Iλ,Hi-1Hi,a,b) is satisfied. By applying Lemma 2.14 and Theorem 2.8, we can deduce that there exist two critical points u1,u2H0,L1(y1-2s) such that Iλ(ui)[a,b] for i=1,2. Now, we prove the existence of a third critical point by invoking the Linking Theorem [27]. Taking into account [27, Theorem 5.3] and Lemma 3.8, it is enough to prove that there are δi′′>0 and R1>ϱ1>0 such that for any λ(μi-δi′′,μi) we get

(2.32) sup I λ ( T i , i + 1 ( R 1 ) ) < inf I λ ( S + ( ϱ 1 ) ) .

Let us note that (2.3), (2.28) and Theorem 2.2 yield

I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(2.33) μ i + 1 - λ - ε 2 μ i + 1 u H 0 , L 1 ( y 1 - 2 s ) 2 - C C ε u H 0 , L 1 ( y 1 - 2 s ) p + 1 for any  u H i .

Take ε=(μi+1-λ)/2. Then, recalling that p>1, in view of (2.33), we can find ϱ1>0 and α>0 such that

(2.34) inf I λ ( S i + ( ϱ 1 ) ) α > 0 .

Now, by using (2.2) and (f5), we deduce that

I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(2.35) μ i - λ 2 μ i u H 0 , L 1 ( y 1 - 2 s ) 2 for any  u H i .

Hence, by using (2.35), we can see that there exist δi′′>0 and R1>0 such that for any λ(μi-δi′′,μi) we get

(2.36) I λ ( u ) < α for any  u H 0 , L 1 ( y 1 - 2 s ) R 1 .

On the other hand, by using (2.2) and (f5), we can see that for any uHi+1 and λ(μi-δi′′,μi), we have

(2.37) I λ ( u ) = 1 2 u H 0 , L 1 ( y 1 - 2 s ) 2 - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x μ i + 1 - λ 2 μ i + 1 u H 0 , L 1 ( y 1 - 2 s ) 2 .

Putting together (2.34), (2.36) and (2.37), we can infer that (2.32) is verified. By applying the Linking Theorem, we can deduce that there exists a critical point u3H0,L1(y1-2s) of Iλ such that Iλ(u)infIλ(Si+(ϱ1)). Choosing δi=min{δi,δi′′}, where δi is given in Lemma 2.13, we can conclude that Theorem 1.1 holds. ∎

3 Multiple Solutions for Problem (1.2)

This section is devoted to the proof of Theorem 1.2. Since many calculations are adaptations to the ones presented in the previous section, we will emphasize only the differences between the “spectral” and the “integral” case. Firstly, we collect some notations and results which we will use in the sequel. For more details we refer the interested reader to [22, 28, 29, 30].

Let us define

𝕏 0 = { u H s ( N ) : u = 0  a.e. in  N Ω }

endowed wit the norm

u 𝕏 0 2 = 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y .

Then, 𝕏0 is a Hilbert space, and the following useful embedding result holds.

Theorem 3.1 ([28]).

𝕏 0 is compactly embedded into Lq(RN) for any q[1,2s*).

Let us denote by {ek,λk}k the eigenvalues and corresponding eigenfunctions of the fractional Laplacian operator (-ΔN)s with homogeneous boundary condition in NΩ, that is,

{ ( - Δ N ) s e k = λ k e k in  Ω , e k = 0 in  N Ω .

We recall that λ1 is simple, 0<λ1<λ2λkλk+1, λk+ and ek are Hölder continuous up to the boundary (differently from the ones of (-ΔΩ)s that are as smooth up the boundary as the boundary allows).

As in Section 2, for any i2, we denote by P:𝕏0Hi0 and Q:𝕏0Hi-1Hi the orthogonal projections, where Hi0=span{ei,,ej}. The next lemma is proved in [29].

Lemma 3.2 ([29]).

The following inequalities hold:

(3.1) 2 N | u ( x ) - u ( y ) | 2 d x | x - y | N + 2 s 𝑑 x 𝑑 y λ j Ω | u | 2 𝑑 x for all  u H j ,
(3.2) 2 N | u ( x ) - u ( y ) | 2 d x | x - y | N + 2 s 𝑑 x 𝑑 y λ j + 1 Ω | u | 2 𝑑 x for all  u H j .

We say that a function u𝕏0 is a weak solution to (1.2) if it satisfies the identity

2 N ( u ( x ) - u ( y ) ) | x - y | N + 2 s ( v ( x ) - v ( y ) ) 𝑑 x 𝑑 y = λ Ω u v 𝑑 x + Ω f ( x , u ) v 𝑑 x

for any v𝕏0. For this reason, we will look for critical points of the Euler–Lagrange functional Iλ:𝕏0 defined by

I λ ( u ) = 1 2 u 𝕏 0 2 - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x .

Since we will proceed as in Section 2, we prove some technical lemmas which will be fundamental to deduce Theorem 1.2. With suitable modifications, it is easy to see that the next lemma can be proved following the lines of the proof of Lemma 2.9.

Lemma 3.3.

Assume that (f1) and (f4) hold. Then, for any δ(0,min{λi+1-λi,λi-λi-1}) there exists ε0>0 such that for any λ[λi-δ,λi+δ] the unique critical point u of Iλ constrained on Hi-1Hi such that Iλ(u)[-ε0,ε0] is the trivial one.

Lemma 3.4.

Assume that (f1) and (f4) hold, λ(λi-1,λi+1) and {un}nNX0 such that Iλ(un) is bounded, Pun0 and QIλ(un)0 as n+. Then {un}nN is bounded in X0.

Proof.

Suppose by contradiction that, up to a subsequence, un𝕏0 as n.

Set un=Pun+Qun. By using (f1), Hölder’s inequality and the fact that all norms in Hi0 are equivalent, we get

| Ω f ( x , u n ) P u n 𝑑 x | Ω | f ( x , u n ) | | P u n | 𝑑 x
c 1 ( Ω | P u n | 𝑑 x + Ω | P u n | | u n | p 𝑑 x )
c 1 P u n L 1 ( Ω ) + c 1 ( Ω | u n | β 𝑑 x ) p β ( Ω | P u n | β β - p 𝑑 x ) β - p β
(3.3) c 5 P u n L ( Ω ) ( 1 + u n L β ( Ω ) p ) ,

with c5>0. Now, we observe that

Q I λ ( u n ) , u n = I λ ( u n ) , u n - P I λ ( u n ) , u n
= u n 𝕏 0 2 - λ u n L 2 ( Ω ) 2 - Ω f ( x , u n ) u n 𝑑 x - P ( u n - ( - ( - Δ ) s ) - 1 ( λ u n + f ( x , u n ) ) ) , u n .

Since Pu,v𝕏0=u,Pv𝕏0 for any u,v𝕏0, we can see that

P ( u n - ( - ( - Δ ) s ) - 1 ( λ u n + f ( x , u n ) ) ) , u n = P u n 𝕏 0 2 - λ P u n , ( - ( - Δ ) s ) - 1 u n - P u n , ( - ( - Δ ) s ) - 1 f ( x , u n )
= P u n 𝕏 0 2 - λ P u n L 2 ( Ω ) 2 - Ω f ( x , u n ) P u n 𝑑 x .

Thus (f4) and (3.3) give

2 I λ ( u n ) - Q I λ ( u n ) , u n = Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x + P u n 𝕏 0 2 - λ P u n L 2 ( Ω ) 2 - Ω f ( x , u n ) P u n 𝑑 x
(3.4) c 2 u n L β ( Ω ) β + P u n 𝕏 0 2 - λ P u n L 2 ( Ω ) 2 - c 5 P u n L ( Ω ) ( 1 + u n L β ( Ω ) p ) .

Since 1<p<β, dimHi0<+ and PunL(Ω)0 as n, from (3.4) we can deduce that

u n L β ( Ω ) p u n 𝕏 0 0 as  n .

Set Qun=vn+wnHi-1Hi. By using (f1), Theorem 3.1, (3.1) and Hölder’s inequality, we have

Q I λ ( u n ) , - v n = λ v n L 2 ( Ω ) 2 - v n 𝕏 0 2 + Ω f ( x , u n ) v n 𝑑 x
λ - λ i - 1 λ i - 1 v n 𝕏 0 2 - Ω | f ( x , u n ) | | v n | 𝑑 x
λ - λ i - 1 λ i - 1 v n 𝕏 0 2 - c 1 Ω ( | u n | p | v n | + | v n | ) 𝑑 x
λ - λ i - 1 λ i - 1 v n 𝕏 0 2 - c 1 ( Ω | u n | β 𝑑 x ) p β ( Ω | v n | β β - p 𝑑 x ) β - p β - c 1 v n L 1 ( Ω )
λ - λ i - 1 λ i - 1 v n 𝕏 0 2 - c 1 C v n 𝕏 0 ( 1 + u n L β ( Ω ) p ) .

Arguing as in the proof of Lemma 2.10, we can see that

(3.5) v n 𝕏 0 u n 𝕏 0 0 , w n 𝕏 0 u n 𝕏 0 0 as  n ,

and

(3.6) P u n 𝕏 0 u n 𝕏 0 0 as  n .

Putting together (3.5) and (3.6), we can see that

1 = u n 𝕏 0 u n 𝕏 0 v n 𝕏 0 + P u n 𝕏 0 + w n 𝕏 0 u n 𝕏 0 0 as  n ,

which is impossible. ∎

Lemma 3.5.

Assume (f1) and (f4). Then, for any δ(0,min{λi+1-λi,λi-λi-1}) there exists ε0>0 such that for any λ[λi-δ,λi+δ] and for any ε1,ε2(0,ε0) with ε1<ε2, the condition ()(Iλ,Hi-1Hi,ε1,ε2) holds.

Proof.

The proof follows the lines of the proof of Lemma 2.11 replacing Lemma 2.9, Lemma 2.10 and Theorem 2.2 by Lemma 3.3, Lemma 3.4, and Theorem 3.1, respectively. Moreover, in this case, to prove that un converges strongly in 𝕏0, we use that fact that K=(-(-ΔN)s)-1:Lq(Ω)𝕏0 is compact, with q[1,2s*); see [21, Section 2.4]. ∎

Now, we define the following sets: for fixed i,k and R,ϱ>0, let

B i ( R ) = { u H i : u 𝕏 0 R } ,
T i - 1 , i ( R ) = { u H i - 1 : u 𝕏 0 R } { u H i : u 𝕏 0 = R } ,
S k + ( ϱ ) = { u H k : u 𝕏 0 = ϱ } ,
B k + ( ϱ ) = { u H k : u 𝕏 0 ϱ } .

Lemma 3.6.

Assume that (f1)(f3) and (f5) hold. Then, for any λ(λi-1,λi+1), there are R>ϱ>0 such that

0 = sup I λ ( T i - 1 , i ( R ) ) < inf I λ ( S i - 1 + ( ϱ ) ) .

Proof.

By using (3.1) and assumption (f5), for any uHi-1 and λ(λi-1,λi) we have

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(3.7) λ i - 1 - λ 2 λ i - 1 u 𝕏 0 2 0 .

Recalling (f3) and (3.1), for any uHi and λ(λi-1,λi) we get

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x
λ i - λ 2 λ i u 𝕏 0 2 - c 6 2 u L 2 ( Ω ) 2 + M 1 | Ω |
(3.8) λ i - λ - c 6 2 λ i u 𝕏 0 2 + M 1 | Ω | .

Taking c6=2(λi-λ), from (3.8) we deduce that

(3.9) I λ ( u ) - as  u 𝕏 0 .

By exploiting (f1) and (f2), we can see that, for any uHi-1,

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω | u | 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(3.10) λ i - λ - ε 2 λ i u 𝕏 0 2 - C C ε u 𝕏 0 p + 1 .

Choosing ε=(λi-λ)/2>0, and by using λ(λi-1,λi), p+1>2, (3.7), (3.9) and (3.10), we can deduce that there exist R>ϱ>0 such that

sup I λ ( T i - 1 , i ( R ) ) < inf I λ ( S i - 1 + ( ϱ ) ) .

The next result can be obtained following the proof of Lemma 2.13.

Lemma 3.7.

Assume that (f5) holds. Then, for R>0 in Lemma 3.6 and for any ε>0 there exists δi>0 such that for any λ(λi-δi,λi) it holds

sup I λ ( B i ( R ) ) < ε .

Lemma 3.8.

Assume that (f1) and (f4) hold. Then Iλ verifies the Palais–Smale condition.

Proof.

Let {un}n be a Palais–Smale sequence of Iλ. We have only to show that

(3.11) P u n 𝕏 0 u n 𝕏 0 0 as  n + .

By using (f4) and the equivalence of the norms on the finite-dimensional space, we get

2 I λ ( u n ) - I λ ( u n ) , u n = Ω ( f ( x , u n ) u n - 2 F ( x , u n ) ) 𝑑 x
Ω ( c 7 | u n | - c 8 ) 𝑑 x
Ω ( c 7 | P u n | - c 7 | v n | - c 7 | w n | - c 8 ) 𝑑 x
(3.12) c 9 P u n 𝕏 0 - c 10 ( v n 𝕏 0 + w n 𝕏 0 + 1 ) .

Putting together (3.5) and (3.12), we can deduce that (3.11) holds. ∎

Proof of Theorem 1.2.

In view of Lemmas 3.5, 3.6 and 3.7, we can take

a ( 0 , inf I λ ( S i - 1 + ( ϱ ) ) ) and b > sup I λ ( B i ( R ) )

such that 0<a<b<ε0. Thus the condition ()(Iλ,Hi-1Hi,a,b) holds. By using Lemma 3.8 and Theorem 2.8, we can find two critical points u1,u2𝕏0 such that Iλ(ui)[a,b] for i=1,2. The existence of a third critical point will be obtained by applying the Linking Theorem. We prove that there are δi′′>0 and R1>ϱ1>0 such that, for any λ(λi-δi′′,λi),

(3.13) sup I λ ( T i , i + 1 ( R 1 ) ) < inf I λ ( S + ( ϱ 1 ) ) .

By using (3.2), (f1), and (f2), we get

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(3.14) λ i + 1 - λ - ε 2 λ i + 1 u 𝕏 0 2 - C C ε u 𝕏 0 p + 1 for any  u H i .

Then, taking ε=(λi+1-λ)/2, and recalling that p>1, from (3.14) it follows that there are ϱ1>0 and α>0 such that

(3.15) inf I λ ( S i + ( ϱ 1 ) ) α > 0 .

On the other hand, by using (3.1) and (f5), we deduce that

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(3.16) λ i - λ 2 λ i u 𝕏 0 2 for any  u H i .

Therefore (3.16) implies that there exist δi′′>0 and R1>0 such that for any λ(λi-δi′′,λi) we get

(3.17) I λ ( u ) < α for any  u 𝕏 0 R 1 .

Thus by using (3.1) and (f5), we can see that for any uHi+1 and λ(λi-δi′′,λi), we have

I λ ( u ) = 1 2 2 N | u ( x ) - u ( y ) | 2 | x - y | N + 2 s 𝑑 x 𝑑 y - λ 2 Ω u 2 𝑑 x - Ω F ( x , u ) 𝑑 x
(3.18) λ i + 1 - λ 2 λ i + 1 u 𝕏 0 2 .

Putting together (3.15), (3.17) and (3.18), we can deduce that (3.13) is verified. By applying the Linking Theorem, we can find a third critical point u3𝕏0 of Iλ such that Iλ(u)infIλ(Si+(ϱ1)). Choosing δi=min{δi,δi′′}, where δi is given in Lemma 3.7, we can conclude that Theorem 1.2 holds. ∎


Communicated by Enrico Valdinoci


Funding statement: This research was carried out under the auspices of the INDAM-Gnampa Project 2017 titled Teoria e modelli per problemi non locali.

Acknowledgements

The author warmly thanks the anonymous referee for her/his useful and nice comments on the paper.

References

[1] N. Abatangelo and E. Valdinoci, Getting acquainted with the fractional Laplacian, preprint (2017), https://arxiv.org/abs/1710.11567. 10.1007/978-3-030-18921-1_1Search in Google Scholar

[2] A. Ambrosetti and P. H. Rabinowitz, Dual variational methods in critical point theory and applications, J. Funct. Anal. 14 (1973), 349–381. 10.1016/0022-1236(73)90051-7Search in Google Scholar

[3] V. Ambrosio, An Ambrosetti–Prodi type-result for fractional spectral problems, preprint (2017), https://arxiv.org/abs/1712.10295. 10.1002/mana.201800416Search in Google Scholar

[4] V. Ambrosio, Nontrivial solutions for a fractional p-Laplacian problem via Rabier theorem, Complex Var. Elliptic Equ. 62 (2017), no. 6, 838–847. 10.1080/17476933.2016.1245725Search in Google Scholar

[5] V. Ambrosio, Periodic solutions for a superlinear fractional problem without the Ambrosetti–Rabinowitz condition, Discrete Contin. Dyn. Syst. 37 (2017), no. 5, 2265–2284. 10.3934/dcds.2017099Search in Google Scholar

[6] V. Ambrosio, On the existence of periodic solutions for a fractional Schrödinger equation, Proc. Amer. Math. Soc. (2018), 10.1090/proc/13630. 10.1090/proc/13630Search in Google Scholar

[7] V. Ambrosio, Periodic solutions for critical fractional problems, Calc. Var. Partial Differential Equations 57 (2018), no. 2, 57:45. 10.1007/s00526-018-1317-ySearch in Google Scholar

[8] G. Autuori, A. Fiscella and P. Pucci, Stationary Kirchhoff problems involving a fractional elliptic operator and a critical nonlinearity, Nonlinear Anal. 125 (2015), 699–714. 10.1016/j.na.2015.06.014Search in Google Scholar

[9] B. Barrios, E. Colorado, A. de Pablo and U. Sánchez, On some critical problems for the fractional Laplacian operator, J. Differential Equations 252 (2012), no. 11, 6133–6162. 10.1016/j.jde.2012.02.023Search in Google Scholar

[10] Z. Binlin, G. Molica Bisci and R. Servadei, Superlinear nonlocal fractional problems with infinitely many solutions, Nonlinearity 28 (2015), no. 7, 2247–2264. 10.1088/0951-7715/28/7/2247Search in Google Scholar

[11] C. Brändle, E. Colorado, A. de Pablo and U. Sánchez, A concave-convex elliptic problem involving the fractional Laplacian, Proc. Roy. Soc. Edinburgh Sect. A 143 (2013), no. 1, 39–71. 10.1017/S0308210511000175Search in Google Scholar

[12] X. Cabré and J. Tan, Positive solutions of nonlinear problems involving the square root of the Laplacian, Adv. Math. 224 (2010), no. 5, 2052–2093. 10.1016/j.aim.2010.01.025Search in Google Scholar

[13] L. Caffarelli and L. Silvestre, An extension problem related to the fractional Laplacian, Comm. Partial Differential Equations 32 (2007), no. 7–9, 1245–1260. 10.1080/03605300600987306Search in Google Scholar

[14] A. Capella, J. Dávila, L. Dupaigne and Y. Sire, Regularity of radial extremal solutions for some non-local semilinear equations, Comm. Partial Differential Equations 36 (2011), no. 8, 1353–1384. 10.1080/03605302.2011.562954Search in Google Scholar

[15] E. Di Nezza, G. Palatucci and E. Valdinoci, Hitchhiker’s guide to the fractional Sobolev spaces, Bull. Sci. Math. 136 (2012), no. 5, 521–573. 10.1016/j.bulsci.2011.12.004Search in Google Scholar

[16] S. Dipierro, O. Savin and E. Valdinoci, All functions are locally s-harmonic up to a small error, J. Eur. Math. Soc. (JEMS) 19 (2017), no. 4, 957–966. 10.4171/JEMS/684Search in Google Scholar

[17] J.-L. Lions and E. Magenes, Problèmes aux limites non homogènes et applications. Vol. 1, Trav. Rech. Math. 17, Dunod, Paris, 1968. Search in Google Scholar

[18] P. Magrone, D. Mugnai and R. Servadei, Multiplicity of solutions for semilinear variational inequalities via linking and -theorems, J. Differential Equations 228 (2006), no. 1, 191–225. 10.1016/j.jde.2005.10.010Search in Google Scholar

[19] A. Marino and C. Saccon, Some variational theorems of mixed type and elliptic problems with jumping nonlinearities. Dedicated to Ennio De Giorgi, Ann. Sc. Norm. Super. Pisa Cl. Sci. (4) 25 (1997), no. 3–4, 631–665. Search in Google Scholar

[20] A. Marino and C. Saccon, Nabla theorems and multiple solutions for some noncooperative elliptic systems, Topol. Methods Nonlinear Anal. 17 (2001), no. 2, 213–237. 10.12775/TMNA.2001.014Search in Google Scholar

[21] G. Molica Bisci, D. Mugnai and R. Servadei, On multiple solutions for nonlocal fractional problems via -theorems, Differential Integral Equations 30 (2017), no. 9–10, 641–666. 10.57262/die/1495850422Search in Google Scholar

[22] G. Molica Bisci, V. D. Radulescu and R. Servadei, Variational Methods for Nonlocal Fractional Problems, Encyclopedia Math. Appl. 162, Cambridge University Press, Cambridge, 2016. 10.1017/CBO9781316282397Search in Google Scholar

[23] D. Mugnai, Multiplicity of critical points in presence of a linking: Application to a superlinear boundary value problem, NoDEA Nonlinear Differential Equations Appl. 11 (2004), no. 3, 379–391. 10.1007/s00030-004-2016-2Search in Google Scholar

[24] D. Mugnai and D. Pagliardini, Existence and multiplicity results for the fractional Laplacian in bounded domains, Adv. Calc. Var. 10 (2017), no. 2, 111–124. 10.1515/acv-2015-0032Search in Google Scholar

[25] Z.-Q. Ou and C. Li, Existence of three nontrivial solutions for a class of superlinear elliptic equations, J. Math. Anal. Appl. 390 (2012), no. 1, 418–426. 10.1016/j.jmaa.2012.01.056Search in Google Scholar

[26] G. Palatucci, A. Pisante and Y. Sire, Subcritical approximation of a Yamabe-type nonlocal equation: A gamma-convergence approach, Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) 14 (2015), no. 3, 819–840. 10.2422/2036-2145.201302_006Search in Google Scholar

[27] P. H. Rabinowitz, Minimax Methods in Critical Point Theory with Applications to Differential Equations, CBMS Reg. Conf. Ser. Math. 65, American Mathematical Society, Providence, 1986. 10.1090/cbms/065Search in Google Scholar

[28] R. Servadei and E. Valdinoci, Mountain pass solutions for non-local elliptic operators, J. Math. Anal. Appl. 389 (2012), no. 2, 887–898. 10.1016/j.jmaa.2011.12.032Search in Google Scholar

[29] R. Servadei and E. Valdinoci, Variational methods for non-local operators of elliptic type, Discrete Contin. Dyn. Syst. 33 (2013), no. 5, 2105–2137. 10.3934/dcds.2013.33.2105Search in Google Scholar

[30] R. Servadei and E. Valdinoci, On the spectrum of two different fractional operators, Proc. Roy. Soc. Edinburgh Sect. A 144 (2014), no. 4, 831–855. 10.1017/S0308210512001783Search in Google Scholar

[31] R. Servadei and E. Valdinoci, The Brezis–Nirenberg result for the fractional Laplacian, Trans. Amer. Math. Soc. 367 (2015), no. 1, 67–102. 10.1090/S0002-9947-2014-05884-4Search in Google Scholar

[32] F. Wang, Multiple solutions for some nonlinear Schrödinger equations with indefinite linear part, J. Math. Anal. Appl. 331 (2007), no. 2, 1001–1022. 10.1016/j.jmaa.2006.09.047Search in Google Scholar

[33] W. Wang, A. Zang and P. Zhao, Multiplicity of solutions for a class of fourth elliptic equations, Nonlinear Anal. 70 (2009), no. 12, 4377–4385. 10.1016/j.na.2008.10.020Search in Google Scholar

[34] S. Yan, J. Yang and X. Yu, Equations involving fractional Laplacian operator: Compactness and application, J. Funct. Anal. 269 (2015), no. 1, 47–79. 10.1016/j.jfa.2015.04.012Search in Google Scholar

Received: 2018-02-09
Revised: 2018-02-16
Accepted: 2018-02-17
Published Online: 2018-03-01
Published in Print: 2018-11-01

© 2018 Walter de Gruyter GmbH, Berlin/Boston

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

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