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Sign-Changing Solutions of Fractional 𝑝-Laplacian Problems

  • Xiaojun Chang , Zhaohu Nie and Zhi-Qiang Wang EMAIL logo
Published/Copyright: November 16, 2018

Abstract

In this paper, we obtain the existence and multiplicity of sign-changing solutions of the fractional p-Laplacian problems by applying the method of invariant sets of descending flow and minimax theory. In addition, we prove that the problem admits at least one least energy sign-changing solution by combining the Nehari manifold method with the constrained variational method and Brouwer degree theory. Furthermore, the least energy of sign-changing solutions is shown to exceed twice that of the least energy solutions.

1 Introduction and Main Results

Recently, much attention has been focused on the study of nonlinear problems involving nonlocal operator. These types of operators arise in several areas such as phase transitions, flames propagation, chemical reaction in liquids, anomalous diffusion, conformal geometry, obstacle problem, quasi-geostrophic, population dynamics, American options in finance and crystal dislocation. We refer the reader to [3, 11, 32, 14, 15, 17, 19, 23, 43, 44] and the references therein.

In this paper we consider the following problem

(1.1) { ( - Δ ) p α u = f ( x , u ) in Ω , u = 0 in N Ω ,

where Ω𝐑N is a bounded domain with smooth boundary Ω, p(1,+), α(0,1), N>pα, f:Ω¯× is continuous and (-Δ)pα stands for the fractional p-Laplacian defined, for u sufficiently smooth, by

(1.2) ( - Δ ) α u ( x ) = c N , α PV N | u ( x ) - u ( y ) | p - 2 ( u ( x ) - u ( y ) ) | x - y | N + p α d y , x N ,

where PV is the principal value and cN,α is a normalization constant.

In the past decades, sign-changing solutions for nonlinear elliptic equations have been studied extensively, such as semilinear elliptic equations [8, 25, 28], p-Laplacian equations [5, 7], Schrödinger equations [6, 9], Schrödinger systems [26, 27] and Schrödinger–Poisson system [30]. In these papers, the main tool is the powerful method of invariant sets of descending flow for studying sign-changing solutions and, especially, the multiplicity of sign-changing solutions with high energy. Another main tool is the Nehari manifold method, which is especially effective in studying the existence of least energy sign-changing solutions. One can see [2, 10, 12, 18, 22, 29, 45, 46, 41, 38, 42] and the references therein.

In [20], we studied the sign-changing solutions of the nonlocal elliptic equations

(1.3) { ( - Δ ) α u = f ( x , u ) in Ω , u = 0 on Ω ,

where the operator (-Δ)α is defined through spectral decomposition, and it is sometimes denoted by Aα for distinction. In fact, let {φk} be an orthonormal basis of L2(Ω) with φk2=1 forming a spectral decomposition of -Δ in Ω with zero Dirichlet boundary conditions, and let λk be the corresponding eigenvalues. Let

H 0 α ( Ω ) = { u = k = 0 a k φ k L 2 ( Ω ) : u H 0 α ( Ω ) = ( k = 0 a k 2 λ k α ) 1 2 < } .

Denote by H-α(Ω) the dual space of H0α(Ω). For uH0α(Ω), u=k=0akφk with ak=Ωuφkdx, the operator Aα is defined by

A α u = k = 0 a k λ k α φ k H - α ( Ω ) .

By the arguments in [40], we can see that the operator (-Δ)pα (p=2) defined by (1.2) is different from the operator Aα in several aspects. For example, their eigenvalues and eigenfunctions are different (see also [34]). By applying the method of invariant sets of descending flow, we obtained the existence and multiplicity of sign-changing solutions with high energy and the existence of least energy sign-changing solutions in [20]. To construct the corresponding invariant sets of descending flow associated with (1.3), there the harmonic extension method introduced by Caffarelli and Silvestre [16] was applied to transform the nonlocal problem in Ω to a local problem in the half cylinder Ω×(0,+), which induces an equivalent definition of the operator Aα (see [13]). Then, by a similar variational setting in the fractional case as introduced in [39], we apply some minimax arguments to obtain the main results.

The goal of this paper is to study the sign-changing solutions of fractional p-Laplacian problem (1.1) with the operator (-Δ)pα defined through the singular integral (1.2). In contrast to [20], here we encounter some new difficulties. First, for the fractional p-Laplacian operator (-Δ)pα with p2, one cannot obtain similar equivalent definition of (-Δ)pα by the harmonic extension method, and then we cannot construct invariant sets of descending flow by transforming the nonlocal problem to local one. Second, the operator (-Δ)pα with p2 is quasi-linear, and the corresponding functional of (1.1) is defined on some Banach space, and thus the abstract critical point theorem in Hilbert space used in [20] is not applicable here. Third, we do not have the decomposition Φ(u)=Φ(u+)+Φ(u-) for u=u++u- with Φ being the corresponding functional, by which property one can get the least energy sign-changing solutions by applying the method of invariant sets of descending flow or standard Nehari manifold arguments.

To obtain the sign-changing solutions of (1.1), our strategy is to work directly on the operator (-Δ)pα in both these two cases. First, by constructing invariant sets of descending flow in some Banach space E, we will apply some abstract critical point theorems in metric space recently obtained by Liu, Liu and Wang [26] to obtain the existence and multiplicity of sign-changing solutions with high energy. Then the Nehari manifold method, combined with the constrained variational method and Brouwer degree theory, will be used to study the existence of least energy sign-changing solutions. By some careful analysis, we can see that the two methods still work on the problem (1.1). Furthermore, using the idea of [47], the energy of least energy sign-changing solutions is estimated and shown to be strictly larger than twice that of the least energy solutions. For recent studies on fractional p-Laplacian equations, one can see [4, 24, 33, 35, 36] and their references.

Our assumptions are formulated as follows:

  1. f C ( Ω ¯ × ) , lim|u|0f(x,u)|u|p-2u=0, uniformly in x;

  2. there exist constants C0>0 and q(p,pα*) with pα*=pNN-pα such that

    | f ( x , u ) | C 0 ( 1 + | u | q - 1 ) for all x Ω ¯ and all u ;

  3. there exist μ>p and M0>0 such that f(x,u)uμF(x,u)>0 for |u|M0, uniformly in x, where

    F ( x , u ) 0 u f ( x , τ ) d τ ;

  4. lim | u | + f ( x , u ) | u | p - 2 u = + , uniformly in x;

  5. f ( x , u ) | u | p - 2 u is strictly increasing on (0,+) and strictly decreasing on (-,0), uniformly in x.

We should remark that there is a typical example f(u)=|u|r-2u (p<r<pα*), which satisfies all the assumptions $f_{1}$$f_{5}$.

To describe the main results, we firstly recall some basic results on the fractional Sobolev space. For more details, one can see [1, 21]. Let α(0,1) and ΩN (N2) be a bounded domain with smooth boundary. Let ||r denote the usual Lr(Ω) norm for all r[1,+]. Set Q=2N(Ωc×Ωc) with Ωc=NΩ. Let u:N be a measurable function, and, for r(1,+), let

[ u ] α , r ( 2 N | u ( x ) - u ( y ) | r | x - y | N + α r d x d y ) 1 r

be the Gagliardo seminorm. Define the fractional Sobolev space

W α , r ( N ) { u L r ( N ) : [ u ] α , r < + } .

Then Wα,r(N) is a Banach space with respect to norm

u α , r ( | u | r r + [ u ] α , r r ) 1 r .

We will work in the closed linear subspace

E = { u W α , p ( N ) : u = 0 a.e. in N Ω } .

Then E is a uniformly convex Banach space endowed with the norm =α,p. Furthermore, the embedding ELr(Ω) is continuous for r[1,pα*] and compact for r[1,pα*). Note that, for uE and r[1,pα*],

N | u | r d x = Ω | u | r d x ,
2 N | u ( x ) - u ( y ) | r | x - y | N + r α d x d y = Q | u ( x ) - u ( y ) | r | x - y | N + r α d x d y .

Then, by the Sobolev inequality |u|pα*Cpα*[u]α,p with Cpα*>0, we can define an equivalent norm on E by

u = ( Q | u ( x ) - u ( y ) | p | x - y | N + α p d x d y ) 1 p .

Define the energy functional Φ:E by

Φ ( u ) = 1 p u p - Ω F ( x , u ) d x .

If f satisfies $f_{1}$, $f_{2}$, by standard arguments as in [37], it follows that Φ is C1 on E. Define

ζ ( u ) = Φ ( u ) , u E * , E = u p - Ω f ( x , u ) u d x for all u E ,
𝒩 { u E { 0 } : ζ ( u ) = 0 } ,

where E* is the dual space of E. In the sequel, for simplicity, we denote ,E*,E by ,. Clearly, 𝒩 contains all the nontrivial solutions of (1.1). Denote u+(x)max{u(x),0}, u-(x)min{u(x),0}. The sign-changing solutions of (1.1) stay on the following set:

= { u E : u ± 0 , Φ ( u ) , u + = Φ ( u ) , u - = 0 } .

Set mαinfuΦ(u) and cαinfu𝒩Φ(u). We can state the main results as follows:

Theorem 1.1.

Suppose that $f_{1}$$f_{3}$ hold. Then problem (1.1) admits a sign-changing solution. Furthermore, if f is odd in u, then problem (1.1) admits infinitely many sign-changing solutions.

Theorem 1.2.

Suppose that fC1(Ω¯×R,R) and $f_{1}$, $f_{2}$, $f_{4}$, $f_{5}$ hold. Then problem (1.1) admits one sign-changing solution u*E such that Φ(u*)=mα. Moreover, mα>2cα.

The paper is organized as follows: In Section 2, we present some useful notations and give some preliminary results. In Section 3, some suitable settings for applying the method of invariant sets of descending flow are introduced. By constructing invariant sets of some descending flow associated with problem (1.1), we apply the abstract theorems in Section 2 to give the proof of Theorem 1.1. In Section 4, we combine the Nehari manifold method with the constraint variational method and Brouwer degree theory to prove Theorem 1.2. Throughout the paper, we always denote by C1,C2, positive constants (possibly different in different places). The distance in E with respect to the norm is denoted by dist(,).

2 Preliminaries

We first recall two abstract critical point theorems in metric space on studying sign-changing solutions [26]. Let X be a complete metric space, ΦC1(X,), let P1,P2X be open sets, M=P1P2, Σ=P1P2 and W=P1P2. For a,b,c, we define

Φ c = { u X : Φ ( u ) c } ,
Φ - 1 ( [ a , b ] ) = { u X : a Φ ( u ) b } ,
K = { u X : Φ ( u ) = 0 } ,
K c = { u X : Φ ( u ) = c , Φ ( u ) = 0 } ,
K ( [ a , b ] ) = { u X : Φ ( u ) [ a , b ] , Φ ( u ) = 0 } .

Definition 2.1 (see [26]).

{ P 1 , P 2 } is called an admissible family of invariant sets with respect to Φ at level c provided the following deformation property holds: If KcW=, then there exists ϵ0>0 such that, for ϵ(0,ϵ0), there exists a continuous map σ:XX satisfying

  1. σ ( P 1 ¯ ) P 1 ¯ , σ(P2¯)P2¯,

  2. σ | Φ c - ϵ = id ,

  3. σ ( Φ c + ϵ W ) Φ c - ϵ .

Theorem 2.2 (see [26]).

Let ΦC1(X,R) and P1,P2 be open subsets of X. Assume that {P1,P2} is an admissible family of invariant sets with respect to Φ at level cc*infuΣΦ(u) and there exists a continuous map φ0:ΔX such that

  1. φ 0 ( 1 Δ ) P 1 , φ0(2Δ)P2,

  2. φ 0 ( 0 Δ ) M = ,

  3. sup u φ 0 ( 0 Δ ) Φ ( u ) < c * ,

where

Δ = { ( t 1 , t 2 ) 2 : t 1 , t 2 0 , t 1 + t 2 1 } ,
0 Δ = { ( t 1 , t 2 ) 2 : t 1 , t 2 0 , t 1 + t 2 = 1 } ,
1 Δ = { 0 } × [ 0 , 1 ] , 2 Δ = [ 0 , 1 ] × { 0 } .

Define

c 0 = inf φ Γ sup u φ ( Δ ) W Φ ( u ) ,

where Γ{φC(Δ,X):φ(1Δ)P1,φ(2Δ)P2,φ|0Δ=φ0|0Δ}. Then c0c* and Kc0W.

Assume that G:XX is an isometric involution, i.e., G2=id. A subset FX is said to be symmetric if GuF for all uF. Denote by Σ the family of closed symmetric subsets of X which do not contain 0. For FΣ, the genus γ(F) of F is defined as the smallest integer n for which there exists an odd and continuous map h:Fn{0}, γ(F)=+ if no such map exists, and γ()=0.

Definition 2.3 (see [26]).

We say that {P1,P2} is a G-admissible family of invariant sets with respect to Φ at level c provided the following deformation property holds: There exists ϵ0>0 and a symmetric open neighborhood Nc of KcW with γ(Nc¯)<+ (Nc= if KcW=) such that, for ϵ(0,ϵ0), there exists a continuous map σ:XX satisfying

  1. σ ( P 1 ¯ ) P 1 ¯ , σ(P2¯)P2¯,

  2. σ G = G σ ,

  3. σ | Φ c - 2 ϵ = id ,

  4. σ ( Φ c + ϵ ( N c W ) ) Φ c - ϵ .

Let Bn{xn:|x|1}.

Theorem 2.4 (see [26]).

Assume that ΦC1(X,R) is a G-invariant functional, P1,P2 are open subsets of X, FG{uX:Gu=u}. Assume that {P1,P2} is a G-admissible family of invariant sets with respect to Φ at level cc*infuΣΦ(u). Suppose that there exists a continuous map φn:BnX such that

  1. φ n ( 0 ) M , φ n ( - t ) = G φ n ( t ) for all t B n ,

  2. φ n ( B n ) M = ,

  3. c 0 sup u F G φ n ( B n ) Φ ( u ) < c * inf u Σ Φ ( u ) .

For jN, define

c j = inf B Γ j sup u B W Φ ( u ) ,

where Γj{B:B=φ(BnY) for some φGn, nj, and open YBn such that -Y=Y and γ(Y¯)n-j} and Gn{φ:φC(Bn,X),φ(-t)=Gφ(t) for tBn, φ(0)M and φ|Bn=φn|Bn}. Then, for j2, cjc* and KcjW. Furthermore, cj+ as j+.

The following lemma will be useful in both of the proofs of Theorem 1.1 and 1.2.

Lemma 2.5 (see [5]).

For p(2,+), there exist positive constants d1,d2 such that, for all ξ,ηRN,

( | ξ | p - 2 ξ - | η | p - 2 η ) ( ξ - η ) d 1 | ξ - η | p ,
| | ξ | p - 2 ξ - | η | p - 2 η | d 2 ( | ξ | + | η | ) p - 2 | ξ - η | .

For p(1,2], there exist positive constants d3,d4 such that, for all ξ,ηRN,

( | ξ | p - 2 ξ - | η | p - 2 η ) ( ξ - η ) d 3 | ξ - η | 2 ( | ξ | + | η | ) 2 - p ,
| | ξ | p - 2 ξ - | η | p - 2 η | d 4 | ξ - η | p - 1 .

3 Proof of Theorem 1.1

By $f_{1}$$f_{3}$, we can easily get that there exists β>0 such that

f ( x , u ) u + β | u | p > 0 for all x Ω ¯ and all u 0 .

Define uβ=(up+β|u|pp)1p for uE. Clearly, β is an equivalent norm to in E. The distance in E with respect to the norm β is denoted by distβ(,). In the sequel of this section, we will use both these two norms for simplicity.

Denote g(x,u)=f(x,u)+β|u|p-2u. To use the method of invariant sets of descending flow, we will define the auxiliary operator A as follows: For uE, let w=A(u) be the unique solution of the problem

{ ( - Δ ) p α w + β | w | p - 2 w = g ( x , u ) in Ω , w = 0 in N Ω ,

which can be written in the weak form

(3.1) Q | w ( x ) - w ( y ) | p - 2 ( w ( x ) - w ( y ) ) ( φ ( x ) - φ ( y ) ) | x - y | N + p α d x d y + β Ω | w | p - 2 w φ d x = Ω g ( x , u ) φ d x for all φ E .

Then we have the following lemma:

Lemma 3.1.

The operator A is well-defined, continuous and compact.

Proof.

Firstly, we prove that A is well-defined. For given uE, consider the minimization problem

m = inf w E J 1 ( w ) ,

where J1(w)1pwβp-Ωg(x,u)wdx,wE. Clearly, J1 is C1, coercive, bounded from below and weakly lower semicontinuous, which implies that there exists w*E to be a minimizer of J1. Furthermore, we can see that J1 admits a unique minimizer. In fact, if we assume that w1,w2E are two different minimizers of J1, then, together with Lemma 2.5 and (3.1), defining w~i(x,y)=wi(x)-wi(y),i=1,2, we can get, for p>2,

0 = Q | w ~ 1 ( x , y ) | p - 2 w ~ 1 ( x , y ) ( w ~ 1 ( x , y ) - w ~ 2 ( x , y ) ) | x - y | N + p α d x d y - Q | w ~ 2 ( x , y ) | p - 2 w ~ 2 ( x , y ) ( w ~ 1 ( x , y ) - w ~ 2 ( x , y ) ) | x - y | N + p α d x d y + β Ω ( | w 1 | p - 2 w 1 - | w 2 | p - 2 w 2 ) ( w 1 - w 2 ) d x C 1 w 1 - w 2 β p

for some C1>0. On the other hand, for p(1,2], using Lemma 2.5 and (3.1) again, it follows that

0 = Q | w ~ 1 ( x , y ) | p - 2 w ~ 1 ( x , y ) ( w ~ 1 ( x , y ) - w ~ 2 ( x , y ) ) | x - y | N + p α d x d y - Q | w ~ 2 ( x , y ) | p - 2 w ~ 2 ( x , y ) ( w ~ 1 ( x , y ) - w ~ 2 ( x , y ) ) | x - y | N + p α d x d y
+ β Ω ( | w 1 | p - 2 w 1 - | w 2 | p - 2 w 2 ) ( w 1 - w 2 ) d x
d 3 ( Q | w ~ 1 ( x , y ) - w ~ 2 ( x , y ) | 2 ( | w ~ 1 ( x , y ) | + | w ~ 2 ( x , y ) | ) p - 2 | x - y | N + p α d x d y + β Ω | w 1 - w 2 | 2 ( | w 1 | + | w 2 | ) p - 2 d x )
C 2 [ ( Q | w ~ 1 ( x , y ) - w ~ 2 ( x , y ) | p | x - y | N + p α ) 2 p ( Q ( | w ~ 1 ( x , y ) | + | w ~ 2 ( x , y ) | ) p | x - y | N + p α d x d y ) p - 2 p
    + β ( Ω | w 1 - w 2 | p d x ) 2 p ( Ω ( | w 1 | + | w 2 | ) p d x ) p - 2 p ]
= C 2 [ w 1 - w 2 2 ( Q ( | w ~ 1 ( x , y ) | + | w ~ 2 ( x , y ) | ) p | x - y | N + p α d x d y ) p - 2 p + β | w 1 - w 2 | p 2 ( Ω ( | w 1 | + | w 2 | ) p d x ) p - 2 p ]

for some C2>0, which implies that w1-w2β=0 and thus w1w2. Hence, both of these two cases imply that w1w2.

Secondly, we prove that A is continuous. Let {un}E such that unuE strongly in E. Clearly, {un} is uniformly bounded in E. Then unu strongly in Lr(Ω) for r[1,pα*), un(x)u(x) for a.e. xΩ. Denote w=A(u), wn=A(un). By (3.1),

w n β p = Ω g ( x , u n ) w n d x .

In view of $f_{1}$$f_{3}$, we can see that {wn} is uniformly bounded in E, i.e., wnβM1 for all n and some M1>0. When p>2, using Lemma 2.5, the Hölder inequality, (3.1) and defining w~n(x,y)=wn(x)-wn(y), w~(x,y)=w(x)-w(y), we obtain

w n - w β p C 3 [ Q | w ~ n ( x , y ) | p - 2 w ~ n ( x , y ) ( w ~ n ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
    - Q | w ~ ( x , y ) | p - 2 w ~ ( x , y ) ( w ~ n ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
    + β Ω ( | w n | p - 2 w n - | w | p - 2 w ) ( w n - w ) d x ]
= C 3 Ω ( g ( x , u n ) - g ( x , u ) ) ( w n - w ) d x
= C 3 I 1

for some C3>0, where I1Ω(g(x,un)-g(x,u))(wn-w)dx. When p(1,2], we get from Lemma 2.5 again that

I 1 = Q | w ~ n ( x , y ) | p - 2 w ~ n ( x , y ) ( w ~ n ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y - Q | w ~ ( x , y ) | p - 2 w ~ ( x , y ) ( w ~ n ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
+ β Ω ( | w n | p - 2 w n - | w | p - 2 w ) ( w n - w ) d x
d 3 ( Q | w ~ n ( x , y ) - w ~ ( x , y ) | 2 ( | w ~ n ( x , y ) | + | w ~ ( x , y ) | ) p - 2 | x - y | N + p α d x d y + β Ω | w n - w | 2 ( | w n | + | w | ) p - 2 d x )
C 4 [ ( Q | w ~ n ( x , y ) - w ~ ( x , y ) | p | x - y | N + p α ) 2 p ( Q ( | w ~ n ( x , y ) | + | w ~ ( x , y ) | ) p | x - y | N + p α d x d y ) p - 2 p
    + β ( Ω | w n - w | p d x ) 2 p ( Ω ( | w n | + | w | ) p d x ) p - 2 p ]
= C 4 [ w n - w 2 ( Q ( | w ~ n ( x , y ) | + | w ~ ( x , y ) | ) p | x - y | N + p α d x d y ) p - 2 p + β | w n - w | p 2 ( Ω ( | w n | + | w | ) p d x ) p - 2 p ]

for some C4>0. Take Rr. Define χC0() such that χ(t)=1 for |t|R, χ(t)=0 for |t|R+1 and 0χ(t)1 for all t. Set

ϕ g , 1 ( t ) χ ( t ) g ( x , t ) , ϕ g , 2 ( t ) ( 1 - χ ( t ) ) g ( x , t ) .

By $f_{1}$, $f_{2}$, there exists C5>0 such that

| ϕ g , 1 ( t ) | C 5 | t | p - 1 , | ϕ g , 2 ( t ) | C 5 | t | q - 1 for all t .

Then, by the Hölder and Sobolev inequalities, we get

I 1 C 6 [ | ϕ g , 1 ( u n ) - ϕ g , 1 ( u ) | p p - 1 + | ϕ g , 2 ( u n ) - ϕ g , 2 ( u ) | q q - 1 ] w n - w β

for some C6>0. Hence, in both of there two cases we can apply the dominated convergence theorem to obtain that wn-w0 as n+.

Now we prove that A is compact. Assume that {un}E is uniformly bounded. Let wn=A(un). By (3.1) and similar arguments as above, it follows that wnβM2 for some M2>0 independent of n. Thus, there exist subsequences of {wn} and {un}, which are still denoted by {wn} and {un} for simplicity, such that wnw¯E, unu¯E weakly in E. Then wnw¯, unu¯ strongly in Lr(Ω) for r[1,pα*), wn(x)w¯(x), un(x)u¯(x) for a.e. xΩ. By similar arguments as above, we can get that wn-w¯β0 as n+. This completes the proof. ∎

Lemma 3.2.

For p>2, there exists a constant ρ1>0 such that

Φ ( u ) , u - A ( u ) ρ 1 u - A ( u ) p .

For p(1,2], there exists a constant ρ2>0 such that

(3.2) Φ ( u ) , u - A ( u ) ρ 2 u - A ( u ) 2 ( u + A ( u ) ) 2 - p .

Proof.

Let uE and w=A(u). Define u~(x,y)=u(x)-u(y) and w~(x,y)=w(x)-w(y). Then, for p>2, by Lemma 2.5, it follows that

Φ ( u ) , u - A ( u ) = Q | u ~ ( x , y ) | p - 2 u ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y - Ω f ( x , u ) ( u - w ) d x
= Q | u ~ ( x , y ) | p - 2 u ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
- Q | w ~ ( x , y ) | p - 2 w ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
+ β Ω ( | u | p - 2 u - | w | p - 2 w ) ( u - w ) d x
ρ 1 [ Q | u ~ ( x , y ) - w ~ ( x , y ) | p | x - y | N + p α d x d y + β Ω | u - w | p d x ]
ρ 1 u - A ( u ) p ,

for some ρ1>0. For p(1,2], by Lemma 2.5 again, it follows that

Φ ( u ) , u - A ( u ) = Q | u ~ ( x , y ) | p - 2 u ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y - Ω f ( x , u ) ( u - w ) d x
= Q | u ~ ( x , y ) | p - 2 u ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
- Q | w ~ ( x , y ) | p - 2 w ~ ( x , y ) ( u ~ ( x , y ) - w ~ ( x , y ) ) | x - y | N + p α d x d y
+ β Ω ( | u | p - 2 u - | w | p - 2 w ) ( u - w ) d x
d 3 [ Q | u ~ ( x , y ) - w ~ ( x , y ) | 2 ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p - 2 | x - y | N + p α d x d y
    + β Ω | u - w | 2 ( | u | + | w | ) p - 2 d x ] ,

where d3 is taken as in Lemma 2.5. Note that, by the Hölder inequality we get

Q | u ~ ( x , y ) - w ~ ( x , y ) | p | x - y | N + p α d x d y = Q | u ~ ( x , y ) - w ~ ( x , y ) | p ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p ( p - 2 ) 2 ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p ( 2 - p ) 2 | x - y | N + p α d x d y
( Q | u ~ ( x , y ) - w ~ ( x , y ) | 2 ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p - 2 | x - y | N + p α d x d y ) p 2
( Q ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p | x - y | N + p α d x d y ) 2 - p 2
C 1 ( Q | u ~ ( x , y ) - w ~ ( x , y ) | 2 ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p - 2 | x - y | N + p α d x d y ) p 2 ( u + w ) p ( 2 - p ) 2

for some C1>0, which implies that

u - w 2 C 1 2 p Q | u ~ ( x , y ) - w ~ ( x , y ) | 2 ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p - 2 | x - y | N + p α d x d y ( u + w ) 2 - p .

Thus, we can see that there exists ρ2>0 such that (3.2) holds.∎

Lemma 3.3.

For p>2, there exists a constant ρ3>0 such that

(3.3) Φ ( u ) E * ρ 3 u - A ( u ) ( u + A ( u ) ) p - 2 .

For p(1,2], there exists a constant ρ4>0 such that

(3.4) Φ ( u ) E * ρ 4 u - A ( u ) p - 1 .

Proof.

Let uE and w=A(u). Define u~(x,y)=u(x)-u(y) and w~(x,y)=w(x)-w(y). Then, for any φE, defining φ~(x,y)=φ(x)-φ(y), by the Hölder inequality we get,

Φ ( u ) , φ = Q | u ~ ( x , y ) | p - 2 u ~ ( x , y ) φ ~ ( x , y ) | x - y | N + p α d x d y - Ω f ( x , u ) φ d x
= Q ( | u ~ ( x , y ) | p - 2 u ~ ( x , y ) - | w ~ ( x , y ) | p - 2 w ~ ( x , y ) ) φ ~ ( x , y ) | x - y | N + p α d x d y
+ β Ω ( | u | p - 2 u - | w | p - 2 w ) φ d x
( Q | | u ~ ( x , y ) | p - 2 u ~ ( x , y ) - | w ~ ( x , y ) | p - 2 w ~ ( x , y ) | p p - 1 | x - y | N + p α d x d y ) p - 1 p ( Q | φ ~ ( x , y ) | p | x - y | N + p α d x d y ) 1 p
+ β ( Ω | | u | p - 2 u - | w | p - 2 w | p p - 1 d x ) p - 1 p ( Ω | φ | p d x ) 1 p ,

which implies that

(3.5) Φ ( u ) E * ( Q | | u ~ ( x , y ) | p - 2 u ~ ( x , y ) - | w ~ ( x , y ) | p - 2 w ~ ( x , y ) | p p - 1 | x - y | N + p α d x d y ) p - 1 p + β ( Ω | | u | p - 2 u - | w | p - 2 w | p p - 1 d x ) p - 1 p .

When p>2, by Lemma 2.5 and the Sobolev inequality, it follows that

Φ ( u ) E * C 1 [ ( Q ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p ( p - 2 ) p - 1 | u ~ ( x , y ) - w ~ ( x , y ) | p p - 1 | x - y | N + p α d x d y ) p - 1 p
    + β ( Ω ( | u | + | w | ) p ( p - 2 ) p - 1 | u - w | p p - 1 d x ) p - 1 p ]
C 1 [ ( Q ( | u ~ ( x , y ) | + | w ~ ( x , y ) | ) p | x - y | N + p α d x d y ) p - 2 p ( Q | u ~ ( x , y ) - w ~ ( x , y ) | p | x - y | N + p α d x d y ) 1 p
    + β ( Ω ( | u | + | w | ) p d x ) p - 2 p ( Ω | u - w | p d x ) 1 p ]
C 2 ( u + w ) p - 2 u - w

for some C1,C2>0. Hence, (3.3) holds. When p(1,2], by (3.5), Lemma 2.5 and the Sobolev inequality again, we get

Φ ( u ) E * C 3 [ ( Q | u ~ ( x , y ) - w ~ ( x , y ) | p | x - y | N + p α d x d y ) p - 1 p + β ( Ω | u - w | p d x ) p - 1 p ]
C 4 u - w p - 1

for some C3,C4>0, which implies that (3.4) holds. ∎

By standard arguments as in [5, Lemma 5.2], we have

Lemma 3.4.

For p>1, there exists a constant ρ5>0 such that

u + A ( u ) ρ 5 ( 1 + u - A ( u ) )

if Φ(u)c for some cR.

Lemma 3.5.

For a<b and a>0, there exists b>0 such that

u - A ( u ) b

if uΦ-1[a,b] and Φ(un)E*a.

Proof.

We assume by contradiction that there exists a sequence {un}E satisfying {un}Φ-1[a,b] and Φ(un)E*a such that un-A(un)0. When p>2, by Lemma 3.3 and Lemma 3.4, it follows that

Φ ( u n ) E * ρ 3 u n - A ( u n ) ( u n + A ( u n ) ) p - 2
ρ 3 ρ 5 p - 2 u n - A ( u n ) ( 1 + u n - A ( u n ) ) p - 2 ,

which implies that Φ(un)E*0, which is a contradiction. Here ρ3 and ρ5 are taken as in Lemma 3.3 and Lemma 3.4, respectively. When p(1,2], by Lemma 3.3, we can get a contradiction again. Hence, the conclusions follow. ∎

In the following, we introduce some notations. Define

P { u E : u 0 } , P - { u E : u 0 } .

For ϵ>0, define

P ϵ { u E : dist ( u , P ) < ϵ } , P ϵ - { u E : dist ( u , P - ) < ϵ } .

Lemma 3.6.

Under the assumptions of Theorem 1.1, there exists an ϵ0>0 small enough such that, for all ϵ(0,ϵ0),

(3.6) dist β ( A ( u ) , P - ) < θ 0 ϵ for all u P ϵ - ,
dist β ( A ( u ) , P ) < θ 0 ϵ for all u P ϵ

for some θ0(0,1).

Proof.

We just prove the case (3.6). The other case can be obtained similarly. For uPϵ-, denote w=A(u). By $f_{1}$, $f_{2}$, for any δ>0, there exists Cδ>0 such that

(3.7) | f ( x , τ ) | δ | τ | p - 1 + C δ | τ | q - 1 for all x Ω ¯ and all τ .

Taking w+ as test function in (3.1), by (3.7), it follows that

Q | w ( x ) - w ( y ) | p - 2 ( w ( x ) - w ( y ) ) ( w + ( x ) - w + ( y ) ) | x - y | N + p α d x d y + β Ω | w + | p d x
= Ω g ( x , u ) w + d x
Ω ( f ( x , u + ) + β | u + | p - 2 u + ) w + d x
Ω ( δ | u + | p - 1 + C δ | u + | q - 1 ) w + d x
( δ + β ) | u + | p p - 1 | w + | p + C δ | u + | q q - 1 | w + | q
δ + β ( λ 1 + β ) 1 p | u + | p p - 1 w + β + C δ C 1 | u + | q q - 1 w + β

for some C1>0, where λ1 is the first eigenvalue of ((-Δ)ps,E). On the other hand,

Q | w ( x ) - w ( y ) | p - 2 ( w ( x ) - w ( y ) ) ( w + ( x ) - w + ( y ) ) | x - y | N + p α d x d y
= Ω + Ω + | w + ( x ) - w + ( y ) | p | x - y | N + p α d x d y
    + Ω + Ω - | w + ( x ) - w - ( y ) | p - 2 ( w + ( x ) - w - ( y ) ) w + ( x ) | x - y | N + p α d x d y + Ω + Ω c | w + ( x ) | p | x - y | N + p α d x d y
    + Ω - Ω + | w - ( x ) - w + ( y ) | p - 2 ( w - ( x ) - w + ( y ) ) ( - w + ( y ) ) | x - y | N + p α d x d y + Ω c Ω + | w + ( y ) | p | x - y | N + p α d x d y
Q | w + ( x ) - w + ( y ) | p | x - y | N + p α d x d y .

Then, taking δ(0,λ11+2(λ1+β)), we get

( dist β ( w , P - ) ) p - 1 w + β p - 1 ( 1 - 2 δ ) dist β ( u , P - ) p - 1 + C δ C 1 dist β ( u , P - ) q - 1 .

Take ϵ0(0,(δCδC1)1q-p). If distβ(u,P-)<ϵϵ0, then

dist β ( w , P - ) ( 1 - δ ) dist β ( u , P - ) < ( 1 - δ ) ϵ .

Denote θ0=1-δ. Then w=A(u)Pθ0ϵ-. Thus, if uPϵ- with ϵ(0,ϵ0) is a nontrivial solution of problem (1.1), then u=A(u) and uP-. This completes the proof. ∎

Similar to [7, Lemma 2.1], we have the following results.

Lemma 3.7.

There exists a locally Lipschitz continuous operator B:E0EKE with the following properties:

  1. There exists ϵ 1 > 0 small enough such that, for ϵ ( 0 , ϵ 1 ) and some θ 1 ( 0 , 1 ) ,

    dist β ( B ( u ) , P - ) < θ 1 ϵ for all u P ϵ - ,
    dist β ( B ( u ) , P ) < θ 1 ϵ for all u P ϵ .

  2. For all u E 0 ,

    1 2 u - B ( u ) u - A ( u ) 2 u - B ( u ) .

  3. For all u E 0 ,

    Φ ( u ) , u - B ( u ) { ρ 1 2 u - A ( u ) p 𝑖𝑓 p > 2 , ρ 2 2 u - A ( u ) 2 ( u + A ( u ) ) 2 - p 𝑖𝑓 p ( 1 , 2 ] .

    Here ρ 1 , ρ 2 are taken as in Lemma 3.2.

  4. If f is odd, then B is odd.

By standard arguments, we get the following lemma:

Lemma 3.8.

Assume that $f_{1}$$f_{3}$ hold. Then the functional Φ satisfies the (PS)c condition for any cR.

Lemma 3.9.

If KcW=, then there exists ϵ0>0 such that, for 0<ϵ<ϵ<ϵ0, there exists a continuous map σ:EE such that

  1. σ ( 0 , u ) = u for all u E ,

  2. σ ( t , u ) = u for all t [ 0 , 1 ] , u Φ - 1 [ c - ϵ , c + ϵ ] ,

  3. σ ( 1 , Φ c + ϵ W ) Φ c - ϵ ,

  4. σ ( t , P - ¯ ) P - ¯ and σ ( t , P ¯ ) P ¯ for t [ 0 , 1 ] .

Proof.

Denote Nδ={uE:dist(u,Kc)<δ}. Take δ>0 small enough such that NδW. By Lemma 3.8, there exist ϵ0,a1>0 such that, for uΦ-1([c-ϵ0,c+ϵ0])Nδ2,

(3.8) Φ ( u ) E * a 1 .

By Lemma 3.5 and Lemma 3.7, there exists b1>0 such that

(3.9) u - B ( u ) 1 2 u - A ( u ) b 1 for all u Φ - 1 ( [ c - ϵ 0 , c + ϵ 0 ] ) N δ 2 .

Without loss of generality, we may take ϵ0<ρ0δ4, where ρ0=min{T1,T2} with

T 1 ρ 1 2 p b 1 p - 1 8 , T 2 ρ 2 b 1 2 ρ 5 2 - p ( 1 + 2 2 - p b 1 2 - p ) .

Define

κ 1 ( u ) = { 0 , u N δ 4 , 1 , u E N δ 2 ,
κ 2 ( u ) = { 0 , u E Φ - 1 ( [ c - ϵ , c + ϵ ] ) , 1 , u Φ - 1 ( [ c - ϵ , c + ϵ ] ) ,

where 0<ϵ<ϵ<ϵ0. Clearly, κ1,κ2 are locally Lipschitz continuous functions. Define

V ( u ) = - u + B ( u ) u - B ( u ) for all u E 0 .

Consider the initial value problem

(3.10) { d φ d t = κ 1 ( φ ) κ 2 ( φ ) V ( φ ) , φ ( 0 ) = u ,

where uE0. By the theory of ordinary differential equations in Banach spaces, problem (3.10) has a unique solution, denoted by φ(t,u), with maximal interval of existence [0,+). Define σ(t,u)=φ(2ϵρ0t,u). It is easily seen that (i) and (ii) hold. We just need to prove (iii) and (iv).

For (iii), take uΦc+ϵW. Then uNδ. We assume by contradiction that

Φ ( φ ( t , u ) ) c - ϵ

for t[0,2ϵρ0]. Clearly, κ2(φ(t,u))=1 for all t[0,2ϵρ0]. Note that, for t[0,2ϵρ0],

φ ( t , u ) - u 0 t d φ d s d s t 2 ϵ ρ 0 < δ 2 ,

it follows that φ(t,u)ENδ2 for t[0,2ϵρ0]. Then κ1(φ(t,u))=1.

For p>2, using Lemma 3.7 (iii), Lemma 3.3, (3.8) and (3.9), we get

Φ ( φ ( 2 ϵ ρ 0 , u ) ) = Φ ( u ) + 0 2 ϵ ρ 0 Φ ( φ ( τ , u ) ) , V ( φ ( τ , u ) ) d τ
= Φ ( u ) - 0 2 ϵ ρ 0 Φ ( φ ( τ , u ) ) , φ ( τ , u ) - B ( φ ( τ , u ) ) φ ( τ , u ) - B ( φ ( τ , u ) ) d τ
Φ ( u ) - ρ 1 4 0 2 ϵ ρ 0 φ ( τ , u ) - A ( φ ( τ , u ) ) p - 1 d τ
Φ ( u ) - T 1 2 ϵ ρ 0
c + ϵ - 2 ϵ < c - ϵ ,

which produces a contradiction. For p(1,2], by Lemma 3.5, Lemma 3.7 (iii), Lemma 3.3, (3.8) and (3.9), we obtain

Φ ( φ ( 2 ϵ ρ 0 , u ) ) = Φ ( u ) + 0 2 ϵ ρ 0 Φ ( φ ( τ , u ) ) , V ( φ ( τ , u ) ) d τ
= Φ ( u ) - 0 2 ϵ ρ 0 Φ ( φ ( τ , u ) ) , φ ( τ , u ) - B ( φ ( τ , u ) ) φ ( τ , u ) - B ( φ ( τ , u ) ) d τ
Φ ( u ) - ρ 2 4 0 2 ϵ ρ 0 φ ( τ , u ) - A ( φ ( τ , u ) ) ( φ ( τ , u ) + A ( φ ( τ , u ) ) ) 2 - p d τ
Φ ( u ) - ρ 2 4 ρ 5 2 - p 0 2 ϵ ρ 0 φ ( τ , u ) - A ( φ ( τ , u ) ) ( 1 + φ ( τ , u ) - A ( φ ( τ , u ) ) ) 2 - p d τ
Φ ( u ) - ρ 2 4 ρ 5 2 - p 0 2 ϵ ρ 0 φ ( τ , u ) - A ( φ ( τ , u ) ) 1 + φ ( τ , u ) - A ( φ ( τ , u ) ) 2 - p d τ
c + ϵ - T 2 2 ϵ ρ 0 < c - ϵ ,

which is a contradiction. Here we have used that the function h(x)x1+xr with r[0,1) is strictly increasing in x0.

For (iv), note that φ(t,u)=u+tddtφ(0,u)+o(t) as t0, by the convexity of P± and Lemma 3.7 (i), we can get the conclusion by standard arguments. ∎

Lemma 3.10.

For a given symmetric neighborhood NE of Kc*, there exists ϵ0>0(0<ϵ<ϵ<ϵ0) such that there exists an odd and continuous map σ:EE such that

  1. σ ( 0 , u ) = u for all u E ,

  2. σ ( t , u ) = u for all t [ 0 , 1 ] , u Φ - 1 [ c - ϵ , c + ϵ ] ,

  3. σ ( 1 , Φ c + ϵ N ) Φ c - ϵ ,

  4. σ ( t , P - ¯ ) P - ¯ and σ ( t , P ¯ ) P ¯ for t [ 0 , 1 ] .

Proof of Theorem 1.1.

The proof is split into two parts.

Existence. It suffices to verify the assumptions of Theorem 2.2. By $f_{1}$$f_{3}$ and the Sobolev inequalities, for any ϵ>0, there exists Cϵ>0 such that

Φ ( u ) 1 p u p - ϵ Ω | u | p d x - C ϵ Ω | u | q d x ( 1 p - ϵ C 1 ) u p - C ϵ C 2 u q

for some C1,C2>0. Since q>p, we can see that there exists ϵ0>0 small enough such that if ϵ(0,ϵ0], then

(3.11) Φ ( u ) δ for all u E with u = ϵ

for some δδ(ϵ)>0, and Φ(u)0 for all uE with uϵ0. Thus,

(3.12) inf u P ¯ ϵ + P ¯ ϵ - Φ ( u ) = 0 for all ϵ ( 0 , ϵ 0 ] ,

which implies that 0 is the unique critical point of Φ in P¯ϵ+P¯ϵ-.

Take v1,v2C0(N){0} such that

supp ( v 1 ) supp ( v 2 ) = and v 1 0 , v 2 0 .

Let φ0(t,s)=R(tv1+sv2) for (t,s)Δ, where R+. Clearly, for (t,s)Δ,

φ 0 ( 0 , s ) = R s v 2 P ϵ + , φ 0 ( t , 0 ) = R t v 1 P ϵ - .

By $f_{1}$$f_{3}$, there exist C3,C4>0 such that F(x,t)C3|t|μ-C4 holds uniformly for xΩ¯. Then, for any u=R(tv1+(1-t)v2)φ0(0Δ), we have

Φ ( u ) = 1 p u p - Ω F ( x , u ) d x
1 p u p - C 3 Ω | u | μ d x + C 4 | Ω |
= R p [ 1 p t v 1 + ( 1 - t ) v 2 p - C 3 supp ( v 1 ) supp ( v 2 ) | t v 1 ( x ) + ( 1 - t ) v 2 ( x ) | μ d x ] + C 4 | Ω |
= R p [ 1 p t v 1 + ( 1 - t ) v 2 p - C 3 ( t μ supp ( v 1 ) | v 1 ( x ) | μ d x + ( 1 - t ) μ supp ( v 2 ) | v 2 ( x ) | μ d x ) ] + C 4 | Ω | .

It is easily seen that Φ(R(tv1+(1-t)v2))- as R-. Hence, defining the map φ0 for R>0 large enough and letting M=Pϵ+Pϵ-, we get supuφ0(0Δ)Φ(u)<0 and φ0(0Δ)M=. Thus, together with (3.11) and (3.12), by Theorem 2.2, it follows that the functional Φ has at least one critical point u*KcW, i.e., u* is a sign-changing solution of (1.1).

Multiplicity. By Theorem 2.4, we just need to construct φn. For any n, take {vi}1nC0{0} such that supp(vi)supp(vj)= for ij. Define φn(t)=Rni=1ntivi for t(t1,t2,,tn)Bn, where Rn>0. Clearly, φnC(Bn,E). Furthermore, we can easily get φn(0)=0Pϵ+Pϵ- and φn(-t)=-φn(t) for all tBn. By similar arguments as above, we can see that there exists Rn>0 large enough such that

sup u φ n ( B n ) Φ ( u ) < 0 < inf u P ϵ + P ϵ - Φ ( u ) .

Then, by defining Tj for j as in Theorem 2.4, we can apply Theorem 2.4 to see that

c j inf B Γ j sup u B W Φ ( u )

is a critical value of Φ for all j2 and there exist {uj}j2EW such that Φ(uj)=cj+ as j+. ∎

4 Least Energy Sign-Changing Solutions

In this section, we will combine the Nehari manifold method with the constraint variational method and Brouwer degree theory to study the existence of least energy sign-changing solutions of problem (1.1). We will prove that problem (1.1) admits least energy solutions and least energy sign-changing solutions, and the energy of least energy sign-changing solutions exceeds twice that of the least energy solutions.

To obtain least energy sign-changing solutions, we will prove the existence of critical points of Φ on , where is defined in Section 1.

Lemma 4.1.

Under the assumptions of Theorem 1.2, there exist μ1,μ2>0 such that

  1. u ± μ 1 for all u ,

  2. Ω | u ± | q d x μ 2 for all u .

Proof.

For u, we have Φ(u),u±=0. Clearly,

Ω f ( x , u ) u + d x = Ω f ( x , u + ) u + d x .

By a simple computation as in Lemma 3.6, it follows that

Φ ( u ) , u + = Φ ( u + ) , u + + 2 C 1 + ( u ) ,

where

C 1 + ( u ) Ω + Ω - | u + ( x ) - u - ( y ) | p - 1 u + ( x ) | x - y | N + p α d x d y - Ω + Ω - | u + ( x ) | p | x - y | N + p α d x d y .

Clearly, C1+(u)>0. Hence, Φ(u+),u+<0, which implies that

u + p < Ω f ( x , u + ) u + d x .

Similarly, we get

u - p < Ω f ( x , u - ) u - d x .

By $f_{1}$, $f_{2}$, for any ϵ>0, there exists Cϵ>0,

(4.1) f ( x , τ ) τ ϵ | τ | p + C ϵ | τ | q for all x Ω ¯ and all τ .

Then, by the Sobolev inequalities, it follows that there exists C1>0 such that

u ± p ϵ C 1 u ± p + C ϵ C 1 u ± q .

Since q(p,pα*), letting ϵ=12C1, it is easily seen that (i) holds. Furthermore, by (4.1) again, we have

μ 1 p u ± p ϵ C 1 u ± p + C ϵ | u ± | q q .

For ϵ=12C1, we can obtain that

| u ± | q q μ 1 p 2 C ϵ μ 2 .

Lemma 4.2.

Assume that fC1(Ω¯×R) and (f1),(f2),(f4),(f5) hold. Then, for any uE{0}, there exists a unique τ0R+ such that τ0uN. Moreover, for any uN, we have

(4.2) Φ ( u ) = max t [ 0 , ) Φ ( t u ) .

Proof.

(i) Given uE{0}, define h(t)=Φ(tu) for all t0, i.e.,

h ( t ) = t p p u p - Ω F ( x , t u ) d x .

Clearly, h(0)=0. In addition,

h ( t ) = Φ ( t u ) , u = t p - 1 u p - Ω f ( x , t u ) u d x ,

which implies that h(τ0)=0 for some τ0>0 if and only if

τ 0 p u p = Ω f ( x , τ 0 u ) τ 0 u d x ,

i.e., τ0u𝒩. By (f1),(f2),(f4), there exists δ>0 such that h(t)>0 if t(0,δ) and h(t)<0 if t(1δ,+). Since h(0)=0, we can see that h has a maximum at some point τ0>0. Hence, h(τ0)=0 and τ0u𝒩. Moreover, by $f_{5}$, h(t)tp-1 is strictly increasing with respect to t on (0,), and hence τ0 is unique.

When u𝒩, we have τ0=1, and h(t) is increasing on (0,1) and decreasing on (1,). Hence,

h ( 1 ) = max t Θ h ( t ) = max t [ 0 , ) h ( t ) ,

i.e., (4.2) holds. ∎

Now, we show that cα can be achieved.

Lemma 4.3.

There exists u~E such that cα can be achieved at u~.

Proof.

By the arguments as in the proof of Theorem 1.1, it follows that Φ has a strict local minimum at 0 and limt+Φ(tu)=- for all uE{0} . Moreover, by Lemma 4.2, for any uE{0}, there exists a unique τu>0 such that Φ(τuu)=maxt>0Φ(tu)>0. Let

c = inf u E { 0 } max t > 0 Φ ( t u ) .

Take a minimizing sequence {un}E of c such that Φ(un)=maxt>0Φ(tun)c. We claim that {un} is uniformly bounded. In fact, if not, we may assume that un. Set zn=unun. Then zn=1, and passing to a subsequence if necessary, there exists z0E such that znz0 in E, znz0 in Lr(Ω) for all r[1,pα*), zn(x)z0(x) for a.e. xΩ. We claim that z00. If not, denoting Ω1={xΩ:z0(x)0}, by $f_{4}$ and the Fatou lemma, we get

1 p - c + o ( 1 ) u n p = 1 p - Φ ( u n ) u n p = Ω F ( x , u n ) u n p z n p d x Ω 1 F ( x , u n ) u n p z n p d x + ,

which gives a contradiction. Hence, z00.

On the other hand, by $f_{1}$ and $f_{2}$, it follows that ΩF(x,u)dx is weakly continuous on E. Then, by Lemma 4.2, it follows that

c + o ( 1 ) = Φ ( u n ) Φ ( R z n ) = 1 p R p - Ω F ( x , R z n ) d x = 1 p R p + o ( 1 ) for all R > 0 .

Hence, we can get a contradiction by taking R>0 large enough. Thus, by standard arguments (one can see [29]), we can see that there exists u~𝒩 such that Φ(u~)=cα. ∎

In the following, we will show that mα can also be achieved.

Lemma 4.4.

If uE with u±0, then there exists a unique pair (tu,su) of positive numbers such that

t u u + + s u u - .

Proof.

For t,s>0, let

g 1 ( t , s ) Φ ( t u + + s u - ) , t u +
= Ω + Ω + | t u + ( x ) - t u + ( y ) | p | x - y | N + p α d x d y + Ω + Ω c | t u + ( x ) | p | x - y | N + p α d x d y + Ω c Ω + | t u + ( y ) | p | x - y | N + p α d x d y
+ Ω + Ω - | t u + ( x ) - s u - ( y ) | p - 1 t u + ( x ) | x - y | N + p α d x d y + Ω - Ω + | s u - ( x ) - t u + ( y ) | p - 1 t u + ( y ) | x - y | N + p α d x d y
- Ω f ( x , t u + ) t u + d x

and

g 2 ( t , s ) Φ ( t u + + s u - ) , s u -
= Ω + Ω - | t u + ( x ) - s u - ( y ) | p - 1 ( - s u - ( y ) ) | x - y | N + p α d x d y + Ω - Ω + | s u - ( x ) - t u + ( y ) | p - 1 ( - s u - ( x ) ) | x - y | N + p α d x d y
+ Ω - Ω - | s u - ( x ) - s u - ( y ) | p | x - y | N + p α d x d y + Ω - Ω c | s u - ( x ) | p | x - y | N + p α d x d y + Ω c Ω - | - s u - ( y ) | p | x - y | N + p α d x d y
- Ω f ( x , s u - ) s u - d x .

By $f_{4}$, for any C1>0, there exists C2>0 such that

(4.3) f ( x , τ ) τ C 1 | τ | p - C 2 for all x Ω ¯ and all τ .

Then, by q(p,pα*), (4.1), (4.3) and Lemma 4.1, we can see that there exist r1>0 small enough and R1>0 large enough such that

(4.4) g 1 ( t , t ) > 0 , g 2 ( t , t ) > 0 , for all t ( 0 , r 1 ) ,
g 1 ( t , t ) < 0 , g 2 ( t , t ) < 0 , for all t ( R 1 , + ) .

Thus, note that g1(t,s) is increasing in s on (0,+) for fixed t>0 and g2(t,s) is increasing in t on (0,+) for fixed s>0. Using (4.4), there exist r>0, R>0 with r<R such that

g 1 ( r , s ) > 0 , g 1 ( R , s ) < 0 for all s ( r , R ] ,
g 2 ( t , r ) > 0 , g 2 ( t , R ) < 0 for all t ( r , R ] .

Now, applying the Miranda theorem [31], there exist some tu,su[r,R] such that g1(tu,su)=g2(tu,su)=0, which implies that tuu++suu-.

In what follows, we prove the uniqueness of the pair (tu,su). Let (t1,s1) and (t2,s2) be the two different positive number pairs such that tiu++siu-, i=1,2. Firstly, we consider the case that u. Then, without loss of generality, we may take (t1,s1)=(1,1) and assume that t2s2. For uE, define

A + ( u ) Ω + Ω + | u + ( x ) - u + ( y ) | p | x - y | N + p α d x d y + Ω + Ω c | u + ( x ) | p | x - y | N + p α d x d y + Ω c Ω + | u + ( y ) | p | x - y | N + p α d x d y + Ω + Ω - | u + ( x ) - u - ( y ) | p - 1 u + ( x ) | x - y | N + p α d x d y + Ω - Ω + | u - ( x ) - u + ( y ) | p - 1 u + ( y ) | x - y | N + p α d x d y ,
A - ( u ) Ω - Ω - | u - ( x ) - u - ( y ) | p | x - y | N + p α d x d y + Ω - Ω c | u - ( x ) | p | x - y | N + p α d x d y + Ω c Ω - | - u - ( y ) | p | x - y | N + p α d x d y + Ω + Ω - | u + ( x ) - u - ( y ) | p - 1 ( - u - ( y ) ) | x - y | N + p α d x d y + Ω - Ω + | u - ( x ) - u + ( y ) | p - 1 ( - u - ( x ) ) | x - y | N + p α d x d y .

Then, by Φ(u),u+=0=Φ(u),u-, we get

(4.5) A + ( u ) = Ω f ( x , u + ) u + d x ,
(4.6) A - ( u ) = Ω f ( x , u - ) u - d x .

Using Φ(t2u++s2u-),t2u+=0=Φ(t2u++s2u-),s2u-, we get

(4.7) t 2 p ( A + ( u ) + B 1 + ( u ) + B 2 + ( u ) ) = Ω f ( x , t 2 u + ) t 2 u + d x ,
(4.8) s 2 p ( A - ( u ) + B 1 - ( u ) + B 2 - ( u ) ) = Ω f ( x , s 2 u - ) s 2 u - d x ,

where

B 1 + ( u ) Ω + Ω - | u + ( x ) - s 2 t 2 u - ( y ) | p - 1 u + ( x ) | x - y | N + p α d x d y - Ω + Ω - | u + ( x ) - u - ( y ) | p - 1 u + ( x ) | x - y | N + p α d x d y ,
B 2 + ( u ) Ω - Ω + | s 2 t 2 u - ( x ) - u + ( y ) | p - 1 u + ( y ) | x - y | N + p α d x d y - Ω - Ω + | u - ( x ) - u + ( y ) | p - 1 u + ( y ) | x - y | N + p α d x d y ,
B 1 - ( u ) Ω + Ω - | t 2 s 2 u + ( x ) - u - ( y ) | p - 1 ( - u - ( y ) ) | x - y | N + p α d x d y - Ω + Ω - | u + ( x ) - u - ( y ) | p - 1 ( - u - ( y ) ) | x - y | N + p α d x d y ,
B 2 - ( u ) Ω - Ω + | u - ( x ) - t 2 s 2 u + ( y ) | p - 1 ( - u - ( x ) ) | x - y | N + p α d x d y - Ω - Ω + | u - ( x ) - u + ( y ) | p - 1 ( - u - ( x ) ) | x - y | N + p α d x d y .

Since t2s2, it is easily seen that B1+(u),B2+(u)0. Then, by (4.5) and (4.7), it follows that

0 Ω [ f ( x , t 2 u + ) | t 2 u + | p - 2 t 2 u + - f ( x , u + ) | u + | p - 2 u + ] | u + | p d x ,

which, together with $f_{5}$, implies that t21. On the other hand, B1-(u),B2-(u)0. Then, by (4.6) and (4.8), it follows that

0 Ω [ f ( x , s 2 u - ) | s 2 u - | p - 2 s 2 u - - f ( x , u - ) | u - | p - 2 u - ] | u - | p d x ,

which, together with $f_{5}$, implies that s21. Hence, t2=s2=1.

Secondly, for the case that u, letting v1=t1u++s1u- and v2=t2u++s2u-, by similar arguments as above, we can obtain that t2t1=s2s1=1. Hence, (t1,s1)=(t2,s2). This completes the proof. ∎

By Lemma 4.4, it is easily seen that . Hence, we can consider the minimization problem

m α inf u Φ ( u ) .

Lemma 4.5.

Under the assumptions of Theorem 1.2, mα can be achieved.

Proof.

Let {un} be a minimizing sequence such that Φ(un)mα as n+. By similar arguments as in Lemma 4.3, we can see that {un} is uniformly bounded in E. Then there exists u*E such that

(4.9) u n ± ( u * ) ± in E ,
(4.10) u n ± ( u * ) ± in L r ( Ω ) for r [ 1 , p α * ) ,
(4.11) u n ( x ) u * ( x ) a.e. x Ω .

By Lemma 4.1, we get (u*)±0. Furthermore, by $f_{1}$, $f_{2}$, we can apply the compact embedding of ELr(Ω) for r[1,pα*) and some standard arguments [48] to get that

(4.12) lim n + Ω f ( x , u n ± ) u n ± d x = Ω f ( x , ( u * ) ± ) ( u * ) ± d x ,
(4.13) lim n + Ω F ( x , u n ± ) d x = Ω F ( x , ( u * ) ± ) d x .

In view of Lemma 4.4, there exist t*,s*>0 such that t*(u*)++s*(u*)-, which implies that

(4.14) ( t * ) p [ A + ( u * ) + B 1 + ( u * ) + B 2 + ( u * ) ] = Ω f ( x , t * ( u * ) + ) t * ( u * ) + d x ,
(4.15) ( s * ) p [ A - ( u * ) + B 1 - ( u * ) + B 2 - ( u * ) ] = Ω f ( x , s * ( u * ) - ) s * ( u * ) - d x .

In what follows we will show that t*,s*1. Since {un}, we have Φ(un),un±=0, i.e.,

A ± ( u n ) = Ω f ( x , u n ± ) u n ± d x .

Using (4.9)–(4.14) and the Fatou lemma, we get

(4.16) A ± ( u * ) Ω f ( x , ( u * ) ± ) ( u * ) ± d x .

Without loss of generality, we may assume that t*s*. Since B1-(u*),B2-(u*)0, together with (4.15) and (4.16), we obtain

(4.17) 0 Ω [ f ( x , ( u * ) - ) | ( u * ) - | p - 2 ( u * ) - - f ( x , s * ( u * ) - ) | s * ( u * ) - | p - 2 s * ( u * ) - ] | ( u * ) - | p d x .

If s*>1, we can get a contradiction from (4.17). Hence, 0<t*s*1.

By $f_{5}$, we can see that (x,τ)f(x,τ)τ-pF(x,τ)0 is increasing with respect to τ on (0,+) and decreasing on (-,0). Then, by the Fatou lemma, it follows that

m α Φ ( t * ( u * ) + + s * ( u * ) - )
= Φ ( t * ( u * ) + + s * ( u * ) - ) - 1 p Φ ( t * ( u * ) + + s * ( u * ) - ) , t * ( u * ) + + s * ( u * ) -
= 1 p Ω ( x , t * ( u * ) + + s * ( u * ) - ) d x
= 1 p [ Ω + ( x , t * ( u * ) + ) d x + Ω - ( x , s * ( u * ) - ) d x ]
1 p [ Ω + ( x , ( u * ) + ) d x + Ω - ( x , ( u * ) - ) d x ]
lim inf n + 1 p Ω ( x , u n ) d x
= lim n + [ Φ ( u n ) - 1 p Φ ( u n ) , u n ]
= m α .

Thus, t*=s*=1 and Φ(u*)=mα. ∎

For any uE with u±0, define Iu:[0,+)×[0,+) by

I u ( t , s ) Φ ( t u + + s u - ) for all t , s 0 .

Lemma 4.6.

If uM, then we have

Φ ( u ) > Φ ( t u + + s u - ) for all s , t 0 such that ( t , s ) ( 1 , 1 ) .

Proof.

By $f_{4}$, we have

lim | ( t , s ) | + I u ( t , s ) = - ,

which implies that Iu admits a global maximum at some (t0,s0)[0,+)×[0,+). We claim that t0>0, s0>0. We will show this fact by proving that the following three cases cannot happen:

  1. t 0 = s 0 = 0 ,

  2. t 0 > 0 , s0=0,

  3. t 0 = 0 , s0>0.

In fact, if s0=0, then Φ(t0u+)Φ(tu+) for all t>0. Hence, Φ(t0u+),t0u+=0, i.e.,

(4.18) t 0 p u + p = Ω f ( x , t 0 u + ) t 0 u + d x .

In view of u, we can see that Φ(u+),u+<0, which implies that

u + p < Ω f ( x , u + ) u + d x .

Then, together with (4.18), we get

0 < Ω [ f ( x , u + ) | u + | p - 2 u + - f ( x , t 0 u + ) | t 0 u + | p - 2 t 0 u + ] | u + | p d x .

Hence, we can obtain that t01 by using $f_{5}$. Since (x,τ)0 for all xΩ¯ and all τ, and (x,τ) is increasing with respect to τ on (0,+) and decreasing on (-,0), we have

I u ( t 0 , 0 ) = Φ ( t 0 u + )
= Φ ( t 0 u + ) - 1 p Φ ( t 0 u + ) , t 0 u +
= 1 p Ω ( x , t 0 u + ) d x
1 p Ω + ( x , u + ) d x
< 1 p [ Ω + ( x , u + ) d x + Ω - ( x , u - ) d x ]
= Φ ( u ) - 1 p Φ ( u ) , u
= Φ ( u ) = I u ( 1 , 1 ) .

This is a contradiction. Thus, s0>0. By similar arguments, we can show that t0>0. By Lemma 4.4, we can see that (1,1) is the unique critical point of Iu in (0,+)×(0,+). Hence, we have, if t0,s0(0,1] with (t0,s0)(1,1), then

I u ( t 0 , s 0 ) < I u ( 1 , 1 ) .

This completes the proof. ∎

Lemma 4.7.

If Φ(u*)=mα for some u*M, then Φ(u*)=0, i.e., u* is a critical point of Φ.

Proof.

We assume by contradiction that Φ(u*)0. Then there exist ρ1,μ1>0 such that

Φ ( u ) ρ 1 for all B 3 μ 1 ( u * ) ,

where B3μ1(u*){uE:u-u*3μ1}. Since u* implies that (u*)±0, we can take μ1>0 small enough such that u±0 for all uB3μ1(u*). Let D(1-δ1,1+δ1)×(1-δ1,1+δ1) with δ1(0,12) small enough such that t(u*)++s(u*)-B3μ1(u*) for all (t,s)D¯. By Lemma 4.6, we get

m ~ α max ( t , s ) D Φ ( t ( u * ) + + s ( u * ) - ) < m α .

Let ϵ1min{mα-m~α2,ρ1μ18}. By similar arguments as in Lemma 3.9, it follows that there exists a continuous map η:×EE such that

  1. η ( 1 , u ) = u if uΦ-1[mα-2ϵ1,mα+2ϵ1]B2μ1(u*),

  2. η ( 1 , Φ m α + ϵ 1 B μ 1 ( u * ) ) Φ m α - ϵ 1 ,

  3. Φ ( η ( 1 , u ) ) Φ ( u ) for all uE.

Define σ(t,s)η(1,t(u*)++s(u*)-) for all (t,s)D¯. By (ii), (iii) and Lemma 4.6, we can see that

(4.19) max ( t , s ) D ¯ Φ ( η ( 1 , t ( u * ) + + s ( u * ) - ) ) < m α ,

which implies that {σ(t,s)}(t,s)D¯=.

In the following, we will produce a contradiction by proving that {σ(t,s)}(t,s)D¯. For (t,s)D¯, define

J 1 ( t , s ) ( Φ ( t ( u * ) + + s ( u * ) - ) , ( u * ) + , Φ ( t ( u * ) + + s ( u * ) - ) , ( u * ) - ) ,
J 2 ( t , s ) ( 1 t Φ ( σ ( t , s ) ) , σ + ( t , s ) , 1 s Φ ( σ ( t , s ) ) , σ - ( t , s ) ) .

Since fC1, the functional J1 is C1. By Φ(u*),(u*)+=0=Φ(u*),(u*)-, we get

Q | u * ( x ) - u * ( y ) | p - 2 ( u * ( x ) - u * ( y ) ) ( ( u * ) + ( x ) - ( u * ) + ( y ) ) | x - y | N + p α d x d y = Ω f ( x , ( u * ) + ) ( u * ) + d x ,
Q | u * ( x ) - u * ( y ) | p - 2 ( u * ( x ) - u * ( y ) ) ( ( u * ) - ( x ) - ( u * ) - ( y ) ) | x - y | N + p α d x d y = Ω f ( x , ( u * ) - ) ( u * ) - d x .

By $f_{5}$, we can see that τ(x,τ)τ=fτ(x,τ)τ2-(p-1)f(x,τ)τ>0 for all τ{0}. Denote

a 1 = Q | u * ( x ) - u * ( y ) | p - 2 | ( u * ) + ( x ) - ( u * ) + ( y ) | 2 | x - y | N + p α d x d y ,
a 2 = Ω f u ( x , ( u * ) + ) | ( u * ) + | 2 d x , a 3 = Ω f ( x , ( u * ) + ) ( u * ) + d x ,
b 1 = Q | u * ( x ) - u * ( y ) | p - 2 | ( u * ) - ( x ) - ( u * ) - ( y ) | 2 | x - y | N + p α d x d y ,
b 2 = Ω f u ( x , ( u * ) - ) | ( u * ) - | 2 d x , b 3 = Ω f ( x , ( u * ) - ) ( u * ) - d x ,
c 1 = Q | u * ( x ) - u * ( y ) | p - 2 ( ( u * ) - ( x ) - ( u * ) - ( y ) ) ( ( u * ) + ( x ) - ( u * ) + ( y ) ) | x - y | N + p α d x d y ,
c 2 = Q | u * ( x ) - u * ( y ) | p - 2 ( ( u * ) + ( x ) - ( u * ) + ( y ) ) ( ( u * ) - ( x ) - ( u * ) - ( y ) ) | x - y | N + p α d x d y .

Clearly, we have

a 1 > 0 , a 2 > ( p - 1 ) a 3 > 0 , b 1 > 0 , b 2 > ( p - 1 ) b 3 > 0 ,
c 1 = Q | u * ( x ) - u * ( y ) | p - 2 ( - ( u * ) - ( x ) ( u * ) + ( y ) - ( u * ) - ( y ) ( u * ) + ( x ) ) | x - y | N + p α d x d y = c 2 > 0 ,
a 1 + c 1 = a 3 , b 1 + c 2 = b 3 .

Then we obtain

det ( J 1 ( 1 , 1 ) ) = Φ ′′ ( u * ) ( u * ) + , ( u * ) + Φ ′′ ( u * ) ( u * ) - , ( u * ) - - Φ ′′ ( u * ) ( u * ) + , ( u * ) - Φ ′′ ( u * ) ( u * ) - , ( u * ) + = [ ( p - 1 ) a 1 - a 2 ] [ ( p - 1 ) b 1 - b 2 ] - ( p - 1 ) 2 c 1 c 2 > ( p - 1 ) 2 c 1 c 2 - ( p - 1 ) 2 c 1 c 2 = 0 .

By the Brouwer degree theory, we get deg(J1,D,0)=1. In view of (4.19), it follows that

σ ( t , s ) = t ( u * ) + + s ( u * ) - for all ( t , s ) D .

Then

deg ( J 2 , D , 0 ) = deg ( J 1 , D , 0 ) = 1 ,

which implies that J2(t0,s0)=0 for some (t0,s0)D. Using (i) and (ii), we obtain that

u 0 σ ( t 0 , s 0 ) = η ( 1 , t 0 ( u * ) + + s 0 ( u * ) - ) B 3 μ 1 ( u * ) .

Hence, we can see that Φ(u0),u0+=0=Φ(u0),u0- with u0±0, i.e., u0{η(t,s)}(t,s)D¯, which produces a contradiction. Thus, u* is a critical point of Φ and a least energy sign-changing solution of problem (1.1). ∎

Lemma 4.8.

For any uM, there exist t~u,s~u(0,1] such that t~uu+,s~uu-N.

Proof.

We just prove t~u(0,1]. The other case can be obtained by similar arguments. Since u, we have Φ(u),u+=0, which implies that

(4.20) u + p < A + ( u ) = Ω f ( x , u + ) u + d x .

On the other hand, by Lemma 4.2, there exists t~u>0 such that t~uu+𝒩, which implies that

Φ ( t ~ u u + ) , t ~ u u + = 0 ,

i.e.,

(4.21) t ~ u p u + p = Ω f ( x , t ~ u u + ) t ~ u u + d x .

Then, together with (4.20) and (4.21), we get

0 < Ω [ f ( x , u + ) | u + | p - 2 u + - f ( x , t ~ u u + ) | t ~ u u + | p - 2 t ~ u u + ] | u + | p d x .

Hence, we can obtain that t~u1 by using $f_{5}$. ∎

By Lemma 4.5 and Lemma 4.7, we can see that the functional Φ admits at least one least energy sign-changing critical point u* on . In what follows, we estimate the energy of u*. Using the fact that (x,τ) is increasing with respect to τ on (0,+) and decreasing on (-,0), we get by Lemma 4.8 that

m α = Φ ( u * )
= Φ ( u * ) - 1 p Φ ( u * ) , u *
= 1 p Ω ( x , u * ) d x
= 1 p [ Ω + ( x , ( u * ) + ) d x + Ω - ( x , ( u * ) - ) d x ]
> 1 p [ Ω + ( x , t ~ u * ( u * ) + ) d x + Ω - ( x , s ~ u * ( u * ) - ) d x ]
= [ Φ ( t ~ u * ( u * ) + ) - 1 p Φ ( t ~ u * ( u * ) + ) , t ~ u * ( u * ) + ] + [ Φ ( s ~ u * ( u * ) - ) - 1 p Φ ( s ~ u * ( u * ) - ) , s ~ u * ( u * ) - ]
= Φ ( t ~ u * ( u * ) + ) + Φ ( s ~ u * ( u * ) - ) 2 c α .


Communicated by Enrico Valdinoci


Award Identifier / Grant number: 201606625030

Award Identifier / Grant number: 11471067

Award Identifier / Grant number: 2412017BJ001

Funding source: Simons Foundation

Award Identifier / Grant number: 430297

Award Identifier / Grant number: 11771324

Funding statement: The first author is partially supported by NSFC Grant (No. 11471067), the Science and Technology Research Project of the Education Department of Jilin Province and the Fundamental Research Funds for the Central Universities (No. 2412017BJ001). The second author is supported by the Simons Foundation through Grant (No. 430297). The third author is supported by NSFC Grant (No. 11771324).

Acknowledgements

The authors thank the anonymous referee for his or her careful reading of our manuscript and valuable suggestions. This work was done when X. J. Chang visited the Department of Mathematics and Statistics, Utah State University during the academic year 2016–2017 under the support of China Scholarship Council (201606625030), and he would like to thank the Department for their support and kind hospitality.

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Received: 2018-08-17
Revised: 2018-09-14
Accepted: 2018-09-15
Published Online: 2018-11-16
Published in Print: 2019-02-01

© 2018 Walter de Gruyter GmbH, Berlin/Boston

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

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