In this paper, we deal with the existence and multiplicity of solutions for fractional p(x)-Kirchhoff-type problems as follows:
{M(∫Q1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy)(−Δp(x))sv(x) =λ|v(x)|r(x)−2v(x),inΩ,v=0,inRd∖Ω,
where (−△p(x))s is the fractional p(x)-Laplacian. Different from the previous ones which have recently appeared, we weaken the condition of M and obtain the existence and multiplicity of solutions via the symmetric mountain pass theorem and the theory of the fractional Sobolev space with variable exponents.
Citation: Zhiwei Hao, Huiqin Zheng. Existence and multiplicity of solutions for fractional p(x)-Kirchhoff-type problems[J]. Electronic Research Archive, 2023, 31(6): 3309-3321. doi: 10.3934/era.2023167
[1] | Tao Zhang, Tingzhi Cheng . A priori estimates of solutions to nonlinear fractional Laplacian equation. Electronic Research Archive, 2023, 31(2): 1119-1133. doi: 10.3934/era.2023056 |
[2] | Mingqi Xiang, Binlin Zhang, Die Hu . Kirchhoff-type differential inclusion problems involving the fractional Laplacian and strong damping. Electronic Research Archive, 2020, 28(2): 651-669. doi: 10.3934/era.2020034 |
[3] | Lingzheng Kong, Haibo Chen . Normalized solutions for nonlinear Kirchhoff type equations in high dimensions. Electronic Research Archive, 2022, 30(4): 1282-1295. doi: 10.3934/era.2022067 |
[4] | Mufit San, Seyma Ramazan . A study for a higher order Riemann-Liouville fractional differential equation with weakly singularity. Electronic Research Archive, 2024, 32(5): 3092-3112. doi: 10.3934/era.2024141 |
[5] | Zijian Wu, Haibo Chen . Multiple solutions for the fourth-order Kirchhoff type problems in $ \mathbb{R}^N $ involving concave-convex nonlinearities. Electronic Research Archive, 2022, 30(3): 830-849. doi: 10.3934/era.2022044 |
[6] | Yaning Li, Yuting Yang . The critical exponents for a semilinear fractional pseudo-parabolic equation with nonlinear memory in a bounded domain. Electronic Research Archive, 2023, 31(5): 2555-2567. doi: 10.3934/era.2023129 |
[7] | Huali Wang, Ping Li . Fractional integral associated with the Schrödinger operators on variable exponent space. Electronic Research Archive, 2023, 31(11): 6833-6843. doi: 10.3934/era.2023345 |
[8] | Yong Zhou, Jia Wei He, Ahmed Alsaedi, Bashir Ahmad . The well-posedness for semilinear time fractional wave equations on $ \mathbb R^N $. Electronic Research Archive, 2022, 30(8): 2981-3003. doi: 10.3934/era.2022151 |
[9] | Xing Yi, Shuhou Ye . Existence of solutions for Kirchhoff-type systems with critical Sobolev exponents in $ \mathbb{R}^3 $. Electronic Research Archive, 2023, 31(9): 5286-5312. doi: 10.3934/era.2023269 |
[10] | Yihui Xu, Benoumran Telli, Mohammed Said Souid, Sina Etemad, Jiafa Xu, Shahram Rezapour . Stability on a boundary problem with RL-Fractional derivative in the sense of Atangana-Baleanu of variable-order. Electronic Research Archive, 2024, 32(1): 134-159. doi: 10.3934/era.2024007 |
In this paper, we deal with the existence and multiplicity of solutions for fractional p(x)-Kirchhoff-type problems as follows:
{M(∫Q1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy)(−Δp(x))sv(x) =λ|v(x)|r(x)−2v(x),inΩ,v=0,inRd∖Ω,
where (−△p(x))s is the fractional p(x)-Laplacian. Different from the previous ones which have recently appeared, we weaken the condition of M and obtain the existence and multiplicity of solutions via the symmetric mountain pass theorem and the theory of the fractional Sobolev space with variable exponents.
In [1], Kirchhoff studied a stationary version of the equation
ρ0∂2v∂t2−(p1h1+E02L∫L0|∂v∂x|2dx)∂2v∂t2=0, | (1.1) |
where ρ0,p1,h1,L and E0 are constants. Such equation extends the classical D'Alembert wave equation by considering the effects of the changes in the length of the string during the vibrations. It is worthwhile to note that the Eq (1.1) received much attention only after Lions [2] put forward an abstract framework to the Eq (1.1). After this work, various equations of Kirchhoff-type have been studied extensively. For instance, many researchers have studied the Kirchhoff-type equations involving the p-Laplacian, which can be found in [3,4,5,6], p(x)-Laplacian (see, for example, [7,8,9,10,11]) and fractional p(x)-Laplacian (see [12,13,14,15]).
Recently, lots of researchers have been interested in the Kirchhoff-type equations involving the p-Laplacian (see [16,17]).In [5], Liu proved the existence of infinite solutions for the p-Kirchhoff-type problems via the fountain theorem. Since the infimum of its principal eigenvalue is zero, the p-Laplacian is not homogenous, and generally it does not have the alleged first eigenvalue. Hence, more and more attention has been given to partial differential equations with nonstandard growth conditions. Dai and Hao [18] investigated the existence and multiplicity of solutions to Kirchhoff-type problems associated with the p(x)-Laplacian via a direct variational approach. The p(x)-Laplacian has more complex nonlinear properties than the p-Laplacian, and we can refer to [11,19] for more details about it.
In the last few years, many researchers have tended to focus on the fractional p(x)-Kirchhoff-type problems. Kaufmann, Rossi and Vidal [20] introduced the fractional p(x)-Laplacian △p(x)v=div(|▽v|p(x)−2) (see, for example, [21,22]). In [23], the authors investigated the fractional p(x)-Laplace operator and associated fundamental properties about new fractional Sobolev spaces with variable exponents. In [14], by using dint of the variational methods, Azroul et al. investigated the existence of solutions for the Kirchhoff-type problems involving fractional p(x)-Laplacian as follows:
(PsM){M(∫Q1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy)(−Δp(x))sv(x)=λ|v(x)|r(x)−2v(x),inΩ,v=0,inRd∖Ω, |
where M∈Q1, i.e., M satisfies the following: there exist 0<a1≤a2 and β>1 such that
a1τβ−1≤M(τ)≤a2τβ−1for allτ∈Rd. |
In [24], applying the symmetric mountain pass theorem, Azroul, Benkirane and Shimi resolved the existence solutions to the following Kirchhoff-type problems involving fractional p(x,⋅)-Laplacian in Rd:
{M(∫Rd×Rd1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy)(−Δp(x,⋅))sv(x)+|v|ˉp(x)−2v=f(x,v),inRd,v∈Ws,p(x,y)(Rd), |
where M∈Q2, i.e., the continuous function M:R+0:=[0,+∞)→R+0 satisfies the following conditions:
(M1): Let ϵ0>0 and α∈(1,(p∗s)−/p+). Suppose that
kM(k)≤αˆM(k)for allk≥ϵ0, | (1.2) |
where
ˆM(k)=∫k0M(ϵ0)dϵ0 |
and (p∗s)−, p+ and p− will be introduced in Section 2.
(M2): let ϵ>0. Suppose l=l(ϵ)>0 such that
M(k)≥lfor allk≥ϵ. | (1.3) |
By comparison their definitions, we find that the condition of Q2 is weaker than Q1. Hence the spontaneous question is to show which results we can obtain if we replace M∈Q1 by M∈Q2 in [14].
Inspired by the fractional Sobolev spaces with variable exponents (for more details see [23]) and the papers referred to above, we aim to deal with the existence and multiplicity solutions to the fractional p(x)-Kirchhoff-type problem (PsM) which is introduced in [14], where
∙ M∈Q2 and λ is a positive real constant;
∙ Q:=R2d∖(Ωc×Ωc), where Ω∈Rd is a Lipschitz bounded open domain and Ωc=Rd∖Ω,d≥3;
∙ the continuous functions r:¯Ω→(1,+∞) and p:¯Q→(1,+∞) are bounded;
∙ for s∈(0,1), the operator (−Δp(x))s is the following fractional p(x)-Laplacian
(−Δp(x))sv(x)=p.v.∫Rd|v(x)−v(y)|p(x)−2(v(x)−v(y))|x−y|d+sp(x,y)dyfor allx∈Rd, |
where p.v. stands for Cauchy principle value for brevity.
We introduce our main conclusions and results as follows:
Theorem 1.1. For the continuous function r:¯Ω→(1,+∞), let
1<r−:=infx∈¯Ωr(x)≤r(x)<r+:=supx∈¯Ωr(x)<p∗s(x). | (1.4) |
Suppose that M satisfies (1.3) and r∈C+(¯Ω) such that
1<r(x)≤r+<p−for allx∈¯Ω, | (1.5) |
then problem (PsM) has a nontrivial weak solution, if there is λ1>0 such that
λ1<λ<+∞. |
Theorem 1.2. Suppose that p∈C+(¯Q) is symmetric with sp+<d and s∈(0,1). Let M∈Q2, r∈C+(¯Q) with
αp+<r−, | (1.6) |
r+<p∗s(x)for allx∈¯Ω. | (1.7) |
Then problem (PsM) has a sequence {un}n of nontrivial solutions, if there is a constant c1>0 such that
0<λ<c1. |
Remark 1.3. We discuss the p(x)-Kirchhoff-type problem (PsM) in two situations: if r satisfies (1.5), we apply the direct variational methods; we utilize the symmetric mountain pass theorem if r satisfies (1.6).
The paper is organized as follows: we introduce the fractional Sobolev spaces with variable exponents and some necessary properties of variable Lebesgue spaces in Section 2. In the end, Section 3 gives the proofs of Theorems 1.1 and 1.2.
In this section, we present some useful properties of the fractional Sobolev spaces with variable exponents and the generalized Lebesgue spaces. We can refer to [17,18,20,25,26] and the references therein for more details.
We always suppose that Ω is a Lipschitz bounded open domain in Rd and ¯Ω is a closure of Ω. Consider a continuous function r:¯Ω→(1,+∞) and set
C+(¯Ω)={r∈(¯Ω)c:r(x)>1for allx∈¯Ω}. |
For a measurable function v and any r∈C+(¯Ω), the modular functional ρr(x)(v) is defined by
ρr(x)(v)=∫Ω|v(x)|r(x)dx |
The variable Lebesgue space is defined as
Lr(x):=Lr(x)(Ω)={v:ρr(x)(λv)<+∞} |
equipped with the norm
‖v‖Lr(x)=inf{λ>0:ρr(x)(f/λ)≤1}. |
Suppose r∈C+(¯Ω) such that 1r(x)+1r′(x)=1, where r′(x) is the conjugate exponent of r(x). Then the Hölder inequality is as follows:
Lemma 2.1 ([20]). Let v∈Lr(x) and u∈Lr′(x). There exists a positive constant c such that
|∫Ωv(x)u(x)dx|≤c‖v‖Lr(x)‖u‖Lr′(x). |
Proposition 2.2 ([27]). Let v∈Lr(x). The following properties hold:
(i) ‖v‖Lr(x)=1 (resp.>1,<1)⇔ρr(x)(v)=1 (resp.>1,<1);
(ii) ‖v‖Lr(x)<1⇒‖v‖r+Lr(x)≤ρr(x)(v)≤‖v‖r−Lr(x);
(iii) ‖v‖Lr(x)>1⇒‖v‖r−Lr(x)≤ρr(x)(v)≤‖v‖r+Lr(x);
(iv)limk→+∞‖vk−v‖Lr(x)=0⇔limk→+∞ρr(x)(vk−v)=0.
We show the following proposition, which is from Theorems 1.6 and 1.10 in [26].
Proposition 2.3. Suppose 1<r−≤r(x)≤r+<∞; then, (Lr(x),‖⋅‖Lr(x)) is a reflexive uniformly convex and separable Banach space.
Let the continuous function p:¯Q→(1,+∞) be bounded. We set
1<p−:=inf(x,y)∈¯Qp(x,y)≤p(x,y)≤p+:=sup(x,y)∈¯Qp(x,y) | (2.1) |
and p is symmetric, if p(x,y) satisfies the following
p(x,y)=p(y,x)for all(x,y)∈¯Q. | (2.2) |
We assume that
ˉp(x):=p(x,x)for allx=y. |
Throughout this paper, s∈(0,1) and the fractional Sobolev space with variable exponents is defined in [14] given by
S={v:Rd→R measurable such that v|Ω∈Lˉp(x) with∫Q|v(x)−v(y)|p(x,y)λp(x,y)|x−y|d+sp(x,y)dxdy<+∞ for some λ>0}. |
The norm of S is as follows
‖v‖S=‖v‖Lˉp(x)+[v]S, |
where [v]S is defined by
[v]S=[v]s,p(x,y)(Q)=inf{λ>0:∫Q|v(x)−v(y)|p(x,y)λp(x,y)|x−y|d+sp(x,y)dxdy≤1}. |
Also, (S,‖⋅‖S) is a separable reflexive Banach space which is introduced in [14].
Now, we denote the linear subspace of S given by
S0={v∈S:v=0a.e.inRd∖Ω}; |
the modular norm is as follows
‖v‖S0:=[v]S=inf{λ>0:∫Q|v(x)−v(y)|p(x,y)λp(x,y)|x−y|d+sp(x,y)dxdy≤1}. |
We know that (S0,‖⋅‖S0) is a separable, reflexive and uniformly convex Banach space (see Lemma 2.3 in [14]).
We denote the modular ρp(x,y):S0→R by
ρp(x,y)(v)=∫Q|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy, |
where
‖v‖ρp(x,y)(v)=inf{λ>0:ρp(x,y)(v/λ)≤1}=[v]S. |
Similarly to Proposition 2.1, ρp(x,y) has the following property:
Lemma 2.4 ([13]). Let p satisfy (2.1) and s∈(0,1). Suppose v∈S0; we can obtain
(i) ‖v‖S0≤1⇒‖v‖p+S0≤ρp(x,y)(v)≤‖v‖p−S0;
(ii) ‖v‖S0≥1⇒‖v‖p−S0≤ρp(x,y)(v)≤‖v‖p+S0.
We will introduce a continuous compact embedding theorem as follows.
Theorem 2.5 ([13]). Let s∈(0,1) and p satisfy (2.1) and (2.2) with sp+<d. If r satisfies (1.4), i.e.,
1<r−≤r(x)<p∗s(x):=dˉp(x)d−sˉp(x)for allx∈¯Ω. |
Then we have
‖v‖Lr(x)≤c‖v‖Sfor anyv∈S, |
where c is a positive constant depending on p, s, r, d and Ω. In other words, the embedding S↪Lr(x) is continuous and this embedding is compact.
Remark 2.6. (i) Theorem 2.5 still holds if we replace S by S0.
(ii) Since 1<r−≤r(x)<p∗s(x), then according to Theorem 2.5, we can get that ‖⋅‖S0 and ‖⋅‖S are equivalent on S0.
We need to introduce the functional L:S0→S∗0 defined by
⟨L(v),φ⟩=∫Q|v(x)−v(y)|p(x,y)−2(v(x)−v(y))(φ(x)−φ(y))|x−y|d+sp(x,y)dxdy |
for all φ∈S0, where S∗0 is the dual space of S0.
Lemma 2.7 ([23]). Suppose that p satisfies (2.1), (2.2) and s∈(0,1). Then the following results hold:
(i) L is a bounded and strictly monotone operator;
(ii) L is a homeomorphism;
(iii) L is a mapping of type (S+), i.e., vn→v in S0, if vn⇀v in S0 and L
lim supn→+∞⟨L(vn)−L(v),vn−v⟩≤0. |
Definition 3.1. We say that v∈S0 is a weak solution of problem (PsM), if
M(σp(x,y)(v))∫Q|v(x)−v(y)|p(x,y)−2(v(x)−v(y))(φ(x)−φ(y))|x−y|d+sp(x,y)dxdy−λ∫Ω|v(x)|r(x)−2v(x)φ(x)dx=0 |
for all φ∈S0, where
σp(x,y)(v)=∫Q1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy. |
For the purpose of formulating the variational method of problem (PsM), we present the functional Iλ:S0→R given by
Iλ(v)=ˆM(∫Q1p(x,y)|v(x)−v(y)|p(x,y)|x−y|d+sp(x,y)dxdy)−λ∫Ω1r(x)|v(x)|r(x)dx=ˆM(σp(x,y)(v))−λ∫Ω1r(x)|v(x)|r(x)dx. |
It is not tough to demonstrate that Iλ∈C1(S0,R) and Iλ is well defined. Moreover, for all v,φ∈S0, the Gateaux derivative of Iλ is introduced by
⟨I′λ(v),φ⟩=M(σp(x,y))(v)∫Q∣v(x)−v(y)∣p(x,y)−2(v(x)−v(y))(φ(x)−φ(y))|x−y|d+sp(x,y)dxdy−λ∫Ω|v(x)|r(x)−2v(x)φ(x)dx=0. |
Thus, the weak solutions of (PsM) correspond to the critical points of Iλ.
To prove Theorem 1.1, we need to introduce the next result:
Lemma 3.2. For λ∈R, the functional Iλ is coercive on S0.
Proof. We assume ‖v‖S0>1. By (M2) we obtain that
Iλ(v)≥lσp(x,y)(v)−λr−ρp(x,y)(v). |
According to Remark 2.6 (i), we have
Iλ(v)≥lp+‖v‖p−S0−λcr−r−min{‖v‖r−S0,‖v‖r+S0}, |
where c is a positive constant depending on d,s,p,r and Ω. It follows from (1.5) that
Iλ(v)→∞,as‖v‖S0→∞. |
Next, we prove Theorem 1.1.
Proof of Theorem 1.1: According to Lemma 3.2, we know that Iλ is coercive on S0. Moreover, Iλ is weakly lower semi-continuous on S0. Applying Theorem 1.2 in [28], we find that there exists ˉv1∈S0 which is a global minimizer of Iλ; thus, the problem (PsM) has a weak solution.
Now, we claim that the weak solution ˉv1 is nontrivial for all λ large enough. Indeed, let δ0>1 and |Ω1|>0, where Ω1 is an open subset of Ω. Suppose η0∈C∞0(¯Ω) such that η0(x) satisfies
{η0(x)=δ0for allx∈¯Ω1,0≤η0(x)≤δ0for allx∈Ω∖Ω1. |
Then we have that
Iλ(η0)=ˆM(σp(x,y)(η0))−λ∫Ω1r(x)|η0(x)|r(x)dx≤c3−λr+∫Ω|η0(x)|r(x)dx≤c3−λr+δr−0|Ω1|, |
where c3 is a constant. Therefore, we get
Iλ(η0)<0for allλ∈(λ1,+∞), |
if the nonnegative λ1 is large enough. The proof is now complete.
We say that Iλ satisfies (Ce)c-condition for any c∈R if every sequence {vn} such that
Iλ(vn)→c,‖I′λ(vn)‖S∗0(1+‖vn‖S0)→0 |
has a strongly convergent subsequence in S0. In order to prove Theorem 1.2, we need the symmetric mountain pass theorem as follows.
Theorem 3.3 ([29,30]). For the infinite dimensional Banach space S, we define
S=2⨁j=1Sj, |
where S2 is finite dimensional. Suppose I∈C1(S,R), if I satisfies the following
(1) I(0)=0,I(−v)=I(v) for all v∈S;
(2) for all c>0, I satisfies (Ce)c-condition;
(3) suppose constants ρ,a are positive, and we have I|∂Bρ∩Z≥a;
(4) for each finite dimensional subspace ˜S⊂S, we obtain I(v)≤0 on ˜S∖Br, if r=r(˜S) is a positive constant.
Then I possesses an unbounded sequence of critical values.
The following result shows that the functional Iλ satisfies the geometrical condition of the mountain pass.
Lemma 3.4. Let c1>0 and v∈S0 with ‖v‖S0=ρ>0. Then for each λ∈(0,c1), we can choose a>0 such that Iλ|∂Bρ∩Z≥a.
Proof. Suppose v∈S0 and ρ∈(0,1) such that ‖u‖S0=ρ. It follows from Theorem 2.5, (M1), (1.6) and (1.7) that
Iλ(v)=ˆM(σp(x,y)(v))−λ∫Ω1r(x)|v(x)|r(x)dx≥ˆM(1)(σp(x,y)(v))α−λr−∫Ω|v(x)|r(x)dx≥ˆM(1)(p+)α(ρp(x,y)(v))α−λr−ρr(x)(v)≥ˆM(1)(p+)α‖v‖αp+S0−λr−‖v‖r+Lr(x)≥ˆM(1)(p+)α‖v‖αp+S0−λcr+r−‖v‖r+S0≥ραp+(ˆM(1)(p+)α−λcr+r−ρr+−αp+). |
Thus, choosing ρ even smaller, we have
Iλ(v)>0, |
since αp+<r−<r+.
Lemma 3.5. For each finite dimensional subspace ˜S⊂S0, v∈˜S and λ∈R, there exists r=r(˜S)>0 such that
Iλ(v)≤0, |
where ‖v‖S0≥r.
Proof. Suppose ϕ∈C∞0(Ω) with ϕ>0. According to (M1), one must have
ˆM(k)≤ˆM(1)kα for all k≥1. | (3.1) |
Therefore, by (3.1), we have
Iλ(tϕ)=ˆM(σp(x,y)(tϕ))−λ∫Ω1r(x)|tϕ|r(x)dx≤ˆM(1)tαp+(σp(x,y)(ϕ))α−λr+∫Ω|tϕ|r(x)dx≤ˆM(1)(p−)αtαp+(ρp(x,y)(ϕ))α−tr−λr+∫Ω|ϕ|r(x)dx. |
It follows from (1.6) that
limt→∞Iλ(tϕ)=−∞. |
Thus, there exists a large t>1 such that
Iλ(v)≤0. |
The statement holds.
Lemma 3.6. The functional Iλ satisfies condition (Ce)c in S0.
Proof. For all c∈R, suppose a sequence {vn}⊂S0 such that
Iλ(vn) →n→+∞c2, |
I′λ(vn) →n→+∞0. | (3.2) |
First, we claim that {vn}⊂S0 is bounded. Arguing by contrary, passing eventually to a subsequence, still denote by vn, we assume that limn→+∞‖vn‖S0=+∞. Hence, for all n, we can consider that ‖vn‖S0>1. According to (3.2), Lemma 2.4, (M1) and (M2), we get that
1+c2+‖vn‖S0≥Iλ(vn)−1αp+⟨I′λ(vn),vn⟩=ˆM(σp(x,y)(vn))−λ∫Ωλr(x)|vn(x)|r(x)dx−1αp+M(σp(x,y)(vn))∫Q∣vn(x)−vn(y)∣p(x,y)∣x−y∣d+sp(x,y)dxdy+λαp+∫Ω|vn(x)|r(x)dx≥ˆM(σp(x,y)(vn))−1αp+M(σp(x,y)(vn))∫Q∣vn(x)−vn(y)∣p(x,y)∣x−y∣d+sp(x,y)dxdy−λr−∫Ω|vn(x)|r(x)dx+λαp+∫Ω|vn(x)|r(x)dx≥lσp(x,y)(vn)−1p+ˆM(1)(σp(x,y)(vn))α−1ρp(x,y)(vn)−(λr−−λαp+)ρr(x)(vn)≥lp+ρp(x,y)(vn)−ˆM(1)p+(p−)α−1(ρp(x,y)(vn))α−(λr−−λαp+)min{‖vn‖r+Lr(x),‖vn‖r−Lr(x)}≥lp+‖vn‖p−S0−ˆM(1)(p−)α‖vn‖αp+S0−(λcr−r−−λcr−αp+)min{‖vn‖r+S0,‖vn‖r−S0}, |
when n is large enough. Dividing the above inequality by ‖vn‖S0. According to αp+<r−<r+, we have −(λr−−λαp+)>0. By passing to the limit as n→+∞, we can get a contradiction.
Since S0 is reflexive, then we can assume that vn⇀ˉv in S0. It follows from (3.2) that
limn→+∞⟨I′λ(vn),vn−ˉv⟩=0, |
that is
M(σp(x,y))(vn)∫Q|vn(x)−vn(y)|p(x,y)−2(vn(x)−vn(y))((vn(x)−vn(y))−(ˉv(x)−ˉv(y)))|x−y|d+sp(x,y)dxdy−λ∫Ω|vn(x)|r(x)−2vn(x)(vn(x)−ˉv(x))dx=0. | (3.3) |
Moreover, due to r(x)<p∗s(x) for all x∈¯Ω and Remark 2.6 (i), we can conclude that vn→ˉv in Lr(x). Hence according to Lemma 2.1 and the proof of Theorem 3.1 in [14], we have that
limn→+∞∫Ω|vn|r(x)−2vn(vn−ˉv)dx=0. | (3.4) |
Since {vn} is bounded in S0, if necessary, we can suppose that
σp(x,y)(vn) →n→+∞t2≥0. |
If t2=0, then {vn}→ˉv=0 in S0 and the proof is complete. If t2>0, according to the continuous function M, we have
M(σp(x,y)(vn))→n→+∞M(t2)≥0. |
Thus, for n large enough and M∈Q2, we get that
0<l<M(σp(x,y)(vn))<c3. | (3.5) |
Combining (3.3)–(3.5), we deduce that
limn→+∞∫Ω|vn(x)−vn(y)|p(x,y)−2(vn(x)−vn(y))((vn(x)−vn(y))−(ˉv(x)−ˉv(y)))|x−y|d+sp(x,y)dxdy=0. | (3.6) |
Using (3.6), Lemma 2.7 (iii) and vn⇀ˉv in S0, we obtain that
{limn→+∞⟨L(vn),vn−ˉv⟩≤0vn⇀ˉv in S0L is a mapping of type (S+)⇒ vn→ˉv in S0. |
Moreover, according to (3.2), we have
limn→+∞Iλ(vn)=Iλ(ˉv)=c2andI′λ(ˉv)=0. |
This completes the proof of Lemma 3.6.
Proof of Theorem 1.2: Clearly, Iλ(0)=0 and Iλ(−v)=Iλ(v). According to Theorem 3.3 and Lemmas 3.4–3.6, we deduce that Theorem 1.2 holds.
This project was supported by the Hunan Provincial Natural Science Foundation (Nos. 2022JJ40145 and 2022JJ40146).
The authors declare that there is no conflict of interest.
[1] | G. Kirchhoff, Mechanik, Teubner, Leipzig, 1883. |
[2] |
J. L. Lions, On some questions in boundary value problems of mathematical physics, North-Holland Math. Stud., 30 (1978), 284–346. https://doi.org/10.1016/S0304-0208(08)70870-3 doi: 10.1016/S0304-0208(08)70870-3
![]() |
[3] |
F. Fang, S. Liu, Nontrivial solutions of superlinear p-Laplacian equations, J. Math. Anal. Appl., 351 (2009), 138–146. https://doi.org/10.1016/j.jmaa.2008.09.064 doi: 10.1016/j.jmaa.2008.09.064
![]() |
[4] |
Y. Guo, J. Nie, Existence and multiplicity of nontrivial solutions for p-Laplacian Schrödinger-Kirchhoff-type equations, J. Math. Anal. Appl., 428 (2015), 1054–1069. https://doi.org/10.1016/j.jmaa.2015.03.064 doi: 10.1016/j.jmaa.2015.03.064
![]() |
[5] |
D. Liu, On a p-Kirchhoff equation via fountain theorem and dual fountain theorem, Nonlinear Anal., 72 (2010), 302–308. https://doi.org/10.1016/j.na.2009.06.052 doi: 10.1016/j.na.2009.06.052
![]() |
[6] |
L. Wang, K. Xie, B. Zhang, Existence and multiplicity of solutions for critical Kirchhoff-type p-Laplacian problems, J. Math. Anal. Appl., 458 (2018), 361–378. https://doi.org/10.1016/j.jmaa.2017.09.008 doi: 10.1016/j.jmaa.2017.09.008
![]() |
[7] |
F. Cammaroto, L. Vilasi, Multiple solutions for a Kirchhoff-type problem involving the p(x)-Laplacian operator, Nonlinear Anal., 74 (2011), 1841–1852. https://doi.org/10.1016/j.na.2010.10.057 doi: 10.1016/j.na.2010.10.057
![]() |
[8] |
G. Dai, D. Liu, Infinitely many positive solutions for a p(x)-Kirchhoff-type equation, J. Math. Anal. Appl., 359 (2009), 704–710. https://doi.org/10.1016/j.jmaa.2009.06.012 doi: 10.1016/j.jmaa.2009.06.012
![]() |
[9] |
G. Dai, R. Ma, Solutions for a p(x)-Kirchhoff type equation with Neumann boundary data, Nonlinear Anal. Real World Appl., 12 (2011), 2666–2680. https://doi.org/10.1016/j.nonrwa.2011.03.013 doi: 10.1016/j.nonrwa.2011.03.013
![]() |
[10] |
A. Zang, p(x)-Laplacian equations satisfying Cerami condition, J. Math. Anal. Appl., 337 (2008), 547–555. https://doi.org/10.1016/j.jmaa.2007.04.007 doi: 10.1016/j.jmaa.2007.04.007
![]() |
[11] |
Q. Zhang, C. Zhao, Existence of strong solutions of a p(x)-Laplacian Dirichlet problem without the Ambrosetti-Rabinowitz condition, Comput. Math. Appl., 69 (2015), 1–12. https://doi.org/10.1016/j.camwa.2014.10.022 doi: 10.1016/j.camwa.2014.10.022
![]() |
[12] | E. Azroul, A. Benkirane, M. Shimi, An introduction to generalized fractional Sobolev space with variable exponent, arXiv preprint, 2019, arXiv: 1901.05687. https://doi.org/10.48550/arXiv.1901.05687 |
[13] |
E. Azroul, A. Benkirane, M. Shimi, Eigenvalue problems involving the fractional p(x)-Laplacian operator, Adv. Oper. Theory, 4 (2019), 539–555. https://doi.org/10.15352/aot.1809-1420 doi: 10.15352/aot.1809-1420
![]() |
[14] |
E. Azroul, A. Benkirane, M. Shimi, M. Srati, On a class of fractional p(x)-Kirchhoff type problems, Appl. Anal., 100 (2021), 383–402. https://doi.org/10.1080/00036811.2019.1603372 doi: 10.1080/00036811.2019.1603372
![]() |
[15] |
A. Bahrouni, Comparison and sub-supersolution principles for the fractional p(x)-Laplacian, J. Math. Anal. Appl., 458 (2018), 1363–1372. https://doi.org/10.1016/j.jmaa.2017.10.025 doi: 10.1016/j.jmaa.2017.10.025
![]() |
[16] |
F. J. S. A. Corrêa, G. M. Figueiredo, On an elliptic equation of p-Kirchhoff type via variational methods, Bull. Aust. Math. Soc., 74 (2006), 263–277. https://doi.org/10.1017/S000497270003570X doi: 10.1017/S000497270003570X
![]() |
[17] |
F. J. S. A. Corrêa, G. M. Figueiredo, On a p-Kirchhoff equation via Krasnoselskii's genus, Appl. Math. Lett., 22 (2009), 819–822. https://doi.org/10.1016/j.aml.2008.06.042 doi: 10.1016/j.aml.2008.06.042
![]() |
[18] |
G. Dai, R. Hao, Existence of solutions for a p(x)-Kirchhoff-type equation, J. Math. Anal. Appl., 359 (2009), 275–284. https://doi.org/10.1016/j.jmaa.2009.05.031 doi: 10.1016/j.jmaa.2009.05.031
![]() |
[19] | L. Diening, P. Harjulehto, P. Hästö, M. Ruzicka, Lebesgue and Sobolev Spaces with Variable Exponents, Springer, 2011. https://doi.org/10.1007/978-3-642-18363-8 |
[20] |
U. Kaufmann, J. D. Rossi, R. Vidal, Fractional Sobolev spaces with variable exponents and fractional p(x)-Laplacians, Electron. J. Qual. Theory Differ. Equations, 76 (2017), 1–10. https://doi.org/10.14232/ejqtde.2017.1.76 doi: 10.14232/ejqtde.2017.1.76
![]() |
[21] |
E. Azroul, A. Benkirane, M. Shimi, General fractional Sobolev space with variable exponent and applications to nonlocal problems, Adv. Oper. Theory, 5 (2020), 1512–1540. https://doi.org/10.1007/s43036-020-00062-w doi: 10.1007/s43036-020-00062-w
![]() |
[22] |
J. Zhang, D. Yang, Y. Wu, Existence results for a Kirchhoff-type equation involving fractional p(x)-Laplacian, AIMS Math., 6 (2021), 8390–8404. https://doi.org/10.3934/math.2021486 doi: 10.3934/math.2021486
![]() |
[23] |
A. Bahrouni, V. Rǎdulescu, On a new fractional Sobolev space and applications to nonlocal variational problems with variable exponent, Discrete Contin. Dyn. Syst. Ser. S, 11 (2018), 379–389. https://doi.org/10.3934/dcdss.2018021 doi: 10.3934/dcdss.2018021
![]() |
[24] |
E. Azroul, A. Benkirane, M. Shimi, Existence and multiplicity of solutions for fractional p(x,⋅)-Kirchhoff-type problems in RN, Appl. Anal., 100 (2021), 2029–2048. https://doi.org/10.1080/00036811.2019.1673373 doi: 10.1080/00036811.2019.1673373
![]() |
[25] |
E. Di Nezza, G. Palatucci, E. Valdinoci, Hitchhiker's guide to the fractional Sobolev spaces, Bull. Sci. Math., 136 (2012), 521–573. https://doi.org/10.1016/j.bulsci.2011.12.004 doi: 10.1016/j.bulsci.2011.12.004
![]() |
[26] |
X. Fan, D. Zhao, On the spaces Lp(x)(Ω) and Wm,p(x)(Ω), J. Math. Anal. Appl., 263 (2001), 424–446. https://doi.org/10.1006/jmaa.2000.7617 doi: 10.1006/jmaa.2000.7617
![]() |
[27] |
G. Dai, J. Wei, Infinitely many non-negative solutions for a p(x)-Kirchhoff-type problem with Dirichlet boundary condition, Nonlinear Anal., 73 (2010), 3420–3430. https://doi.org/10.1016/j.na.2010.07.029 doi: 10.1016/j.na.2010.07.029
![]() |
[28] | M. Struwe, Variational Methods: Applications to Nonlinear Partial Differential Equations and Hamiltonian Systems, Springer, 1996. https://doi.org/10.1007/978-3-540-74013-1 |
[29] |
R. Kajikiya, A critical point theorem related to the symmetric mountain pass lemma and its applications to elliptic equations, J. Funct. Anal., 225 (2005), 352–370. https://doi.org/10.1016/j.jfa.2005.04.005 doi: 10.1016/j.jfa.2005.04.005
![]() |
[30] |
X. H. Tang, Infinitely many solutions for semilinear Schrödinger equations with sign-changing potential and nonlinearity, J. Math. Anal. Appl., 401 (2013), 407–415. https://doi.org/10.1016/j.jmaa.2012.12.035 doi: 10.1016/j.jmaa.2012.12.035
![]() |
1. | Lili Wan, Solutions for fractional $p(x,\cdot )$-Kirchhoff-type equations in $\mathbb{R}^{N}$, 2024, 2024, 1029-242X, 10.1186/s13660-024-03204-3 | |
2. | Limin Guo, Cheng Li, Jingbo Zhao, Existence of Monotone Positive Solutions for Caputo–Hadamard Nonlinear Fractional Differential Equation with Infinite-Point Boundary Value Conditions, 2023, 15, 2073-8994, 970, 10.3390/sym15050970 |