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Research article Special Issues

A new class of multiple nonlocal problems with two parameters and variable-order fractional p()-Laplacian

  • In the present manuscript, we focus on a novel tri-nonlocal Kirchhoff problem, which involves the p(x)-fractional Laplacian equations of variable order. The problem is stated as follows:

    {M(σp(x,y)(u))(Δ)s()p()u(x)=λ|u|q(x)2u(Ω1q(x)|u|q(x)dx)k1+β|u|r(x)2u(Ω1r(x)|u|r(x)dx)k2in Ω, u=0on Ω,

    where the nonlocal term is defined as

    σp(x,y)(u)=Ω×Ω1p(x,y)|u(x)u(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy.

    Here, ΩRN represents a bounded smooth domain with at least N2. The function M(s) is given by M(s)=absγ, where a0, b>0, and γ>0. The parameters k1, k2, λ and β are real parameters, while the variables p(x), s(), q(x), and r(x) are continuous and can change with respect to x. To tackle this problem, we employ some new methods and variational approaches along with two specific methods, namely the Fountain theorem and the symmetric Mountain Pass theorem. By utilizing these techniques, we establish the existence and multiplicity of solutions for this problem separately in two distinct cases: when a>0 and when a=0. To the best of our knowledge, these results are the first contributions to research on the variable-order p(x)-fractional Laplacian operator.

    Citation: Mohamed Karim Hamdani, Lamine Mbarki, Mostafa Allaoui. A new class of multiple nonlocal problems with two parameters and variable-order fractional p()-Laplacian[J]. Communications in Analysis and Mechanics, 2023, 15(3): 551-574. doi: 10.3934/cam.2023027

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  • In the present manuscript, we focus on a novel tri-nonlocal Kirchhoff problem, which involves the p(x)-fractional Laplacian equations of variable order. The problem is stated as follows:

    {M(σp(x,y)(u))(Δ)s()p()u(x)=λ|u|q(x)2u(Ω1q(x)|u|q(x)dx)k1+β|u|r(x)2u(Ω1r(x)|u|r(x)dx)k2in Ω, u=0on Ω,

    where the nonlocal term is defined as

    σp(x,y)(u)=Ω×Ω1p(x,y)|u(x)u(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy.

    Here, ΩRN represents a bounded smooth domain with at least N2. The function M(s) is given by M(s)=absγ, where a0, b>0, and γ>0. The parameters k1, k2, λ and β are real parameters, while the variables p(x), s(), q(x), and r(x) are continuous and can change with respect to x. To tackle this problem, we employ some new methods and variational approaches along with two specific methods, namely the Fountain theorem and the symmetric Mountain Pass theorem. By utilizing these techniques, we establish the existence and multiplicity of solutions for this problem separately in two distinct cases: when a>0 and when a=0. To the best of our knowledge, these results are the first contributions to research on the variable-order p(x)-fractional Laplacian operator.



    Given that N2 and ΩRN is a smooth bounded domain. The goal of this paper is to investigate the existence and multiplicity of solutions for variable order p(x)-Kirchhoff tri-nonlocal fractional equations.

    {M(σp(x,y)(u))(Δ)s()p()u(x)=λ|u|q(x)2u(Ω1q(x)|u|q(x)dx)k1+β|u|r(x)2u(Ω1r(x)|u|r(x)dx)k2in Ω,u=0on Ω, (1.1)

    where

    σp(x,y)(u)=Ω×Ω1p(x,y)|u(x)u(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy,

    where N>s(x,y)p(x,y) for all (x,y)¯ΩׯΩ, λ,β are two real parameters, k1,k2>0, M(x)=abxγ, a0, b,γ>0 and q, r are continuous real functions on ˉΩ.

    The operator defined as (Δ)s()p() is referred to as the p(x)-fractional Laplacian with variable order, and it is defined as follows:

    (Δ)s()p()u(x):=P.V.Ω1p(x,y)|u(x)u(y)|p(x,y)2(u(x)u(y))|xy|N+s(x,y)p(x,y)dy;

    for any uC0(RN), where the notation P.V. means the Cauchy principal value.

    As the problem (1.1) involves integrals over the domain Ω, it deviates from being a pointwise identity. Consequently, it is commonly referred to as a tri-nonlocal problem due to the presence of the following integrals.

    σp(x,y)(u) and Ω1s(x)|u|s(x)dx,for s={q,r}.

    In recent years, the wide class of problems involving nonlocal operators have been an increasing attention and have acquired relevance due to their occurrence in pure and applied mathematical point view, for instance, finance, the thin obstacle problem, biology, probability, optimization and others.

    In the current work, our attention will be focused on a very interesting nonlocal operator known as the fractional p(x)-Laplacian with variable order. This type of operator represents an extension and a combination of many other operators. Indeed, the nonlocal fractional p-Laplacian, which has been extensively studied in the literature, is defined as

    (Δ)spu(x)=2limε0+RNBε(0)|u(x)u(y)|p2(u(x)u(y))|xy|N+spdy,xRN.

    During this time, problems involving variable exponents have attracted many researchers [1,2,3]. These types of problems primarily arise from the p(x)-Laplace operator div(|u|p(x)2u), which serves as a natural extension of the classical p-Laplace operator div(|u|p2u) when p is a positive constant. However, these operators possess a more intricate structure due to their lack of homogeneity. Hence, problems involving p(x)-Laplacian become more tricky. Moreover, concerning the nonlocal problem involving the p(x)-Laplacian, we can refer to [4,5,6,7,8,9,10,11,12,13] and the references therein. For instance, in [9], the authors focused their study on a specific fourth-order bi-nonlocal elliptic equation of Kirchhoff type with Navier boundary conditions, which is expressed as:

    {M(Ω1p(x)|Δu|p(x)dx)Δ2p(x)u(x)=λ|u|q(x)2u(Ω1q(x)|u|q(x)dx)rin Ω,Δu=u=0on Ω,

    By using a variational method and critical point theory, the authors obtained a nontrivial weak solution. Consequently, the idea to replace the fractional p-Laplacian by its variable version was initiated. For this purpose, Kaufmann et al. [14] introduced the fractional p(x)-Laplacian (Δ)sp() as follows:

    (Δ)spu(x)=limε0+RNBε(0)|u(x)u(y)|p(x,y)2(u(x)u(y))|xy|N+sp(x,y)dy,xRN.

    To address such problems, the authors considered the fractional Sobolev space with variable exponents, variational methods, existence. Simultaneously, many works involving the variable-order fractional Laplacian (see [15]) have emerged, defined as follows:

    (Δ)s()u(x)=limε0+RNBε(0)|u(x)u(y)||xy|N+2s(x,y)dy,xRN.

    Furthermore, the combination of these operators leads to the emergence of the so-called fractional p(x)-Laplacian with variable order. This class of operators has captured the attention of numerous researchers [15,16,17,18,19,20], who have investigated various aspects, including the existence, multiplicity, and qualitative properties of the solutions. Additionally, there are several works focusing on the nonlocal fractional p(x)-Laplacian with variable order [15,16,17,19,21,22] and their references therein. For instance, in [19], the authors studied the existence and multiplicity of solutions for the following fractional p()-Kirchhoff type problem with a variable order s():

    {M(R2N1p(x,y)|v(x)v(y)|p(x,y)|xy|N+p(x,y)s(x,y)dxdy)(Δ)s()p()v(x)+|v(x)|¯p(x)2v(x)=μg(x,v)in RN,vWs(),p()(RN), (1.2)

    where (x,y)RN×RN satisfies the condition N>p(x,y)s(x,y), s():R2N(0,1) and p():R2N(1,), and ¯p(x)=p(x,x) for xRN, M is a continuous Kirchhoff-type function, g(x,v) is a Carathéodory function and μ>0 is a parameter. The authors obtained at least two distinct solutions for the above problem by applying the generalized abstract critical point theorem. In addition, under weaker conditions, they also proved the existence of one solution and infinitely many solutions using the mountain pass lemma and fountain theorem, respectively.

    Motivated by the aforementioned works, the present work aims to study the problem (1.1) mentioned above. The main difficulties and innovations lie in the form of the new Kirchhoff functions M(s)=absγ, derived from the negative Young's modulus when the atoms are spread apart rather than compressed together, resulting in negative deformation. In the case a=0, to overcome this challenge, inspired by [23], our main approach is based on the notion of the first eigenvalue associated with our operator.

    The specificity of this tool is that, in the literature, we only find the recent paper [23], in which the authors introduce the s(,)-fractional Musielak-Sobolev spaces Ws(x,y)Lφ(x,y)(Ω). By employing Ekeland's variational principle, the authors establish the existence of a positive value λ>0 such that for any λ within the interval (0,λ), it serves as an eigenvalue for the following problem:

    (Pa){(Δ)s(x,.)a(x,.)u=λ|u|q(x)2uin Ω,u=0in RNΩ,

    where Ω is a bounded open subset of RN with a C0,1-regularity and a bounded boundary conditions. It is noteworthy that this operator represents a generalization of (Δ)s()p() (whenever we take a(x,.)=tp(x,.)2). Thus, this characterization is applicable in our case.

    Throughout this work, the functions s() and p() satisfy the following conditions:

    (H1): s(x,y) is a symmetric function, i.e., s(x,y)=s(y,x), and we have

    0<s:=inf(x,y)¯ΩׯΩs(x,y)s+:=sup(x,y)¯ΩׯΩs(x,y)<1.

    (H2): p(x,y) is a symmetric function, i.e., p(x,y)=p(y,x), and we have

    1<p:=inf(x,y)¯ΩׯΩp(x,y)p+:=sup(x,y)¯ΩׯΩp(x,y)<.

    For any xΩ, we denote

    ¯p(x):=p(x,x),¯s(x):=s(x,x).

    Moreover, it is also assumed that the function p() satisfies the following condition:

    min{p(γ+1),q(k1+1),r(k2+1)}>p+. (1.3)

    Now, we are ready to state our main results.

    Theorem 1.1. Let a>0. Assume that (H1)(H2) and (1.3) are satisfied. Then, for all λ>0 and β>0, the problem (1.1) possesses a nontrivial weak solution in X.

    Theorem 1.2. Let a>0. Assume that (H1)(H2) and (1.3) are satisfied. Then, for all λ>0 and β>0, the problem (1.1) admits an unbounded sequence of solutions in X.

    Moreover, we also obtain the following existence results for problem (1.1) in the case a=0.

    Theorem 1.3. Let a=0, λ1 be the first eigenvalue associated with our operator (For more comprehensive details and references, we recommend referring to [23]), and

    {λ=βλ1(x)(q)k1+1(k1+1)4C(r+)k2+1(k2+1)ρq(k1+1)r+(k2+1),ifλ>0,β<0,β=λλ1(x)(r)k2+1(k2+1)4C(q+)k1+1(k1+1)ρr(k2+1)q+(k1+1),ifλ<0,β>0.

    If the following conditions are satisfied:

    λ<0,β(0,β) and r+(k2+1)<min{(γ+1)p,q(k1+1)},λ(0,λ),β<0 and q+(k1+1)<min{(γ+1)p,r(k2+1)},λ<0,β<0 and r+(k2+1)<q(k1+1)<(γ+1)p, (1.4)

    then problem (1.1) has infinitely many solutions in X.

    However, as far as our knowledge extends, there are no existing results regarding the existence and multiplicity of solutions for problem (1.1) involving the new tri-nonlocal Kirchhoff function and the p(x)-fractional Laplacian operator with variable order.

    The structure of this paper is as follows: In the second section, an abstract framework is presented, where we provide a review of some preliminary results that will be utilized throughout the subsequent sections. The third section is specifically focused on presenting the Palais-Smale condition separately for the cases of a>0 and a=0. The subsequent sections are dedicated to proving the main results of this study.

    In this section, we provide a brief review of the definition and key results concerning Lebesgue spaces with variable exponents and generalized Sobolev spaces. For a more comprehensive understanding, interested readers are referred to [1,2,24] and the references therein.

    For this purpose, let us define

    C+(Ω):={h:hC(¯Ω) and h(x)>1 for all x¯Ω}.

    For p()C+(Ω), the variable exponent Lebesgue space Lp()(Ω) is defined by

    Lp()(Ω):={u:ΩR measurable and Ω|u(x)|p(x)dx<}.

    This space is endowed with the so-called Luxemburg norm given by

    uLp(x)(Ω)=|u|p():=inf{δ>0:Ω|u(x)δ|p(x)dx1}

    and (Lp()(Ω),|u|p()) becomes a Banach space, and we call it a variable exponent Lebesgue space.

    Now, in order to claim the (PS) condition cited in Section 3, we state the following lemma for the variable exponent Lebesgue spaces (see [3, Lemma A.1])

    Lemma 2.1. Assume that h1L(Ω) such that h10 and h10 a.e. in Ω. Let h2:ΩR be a measurable function such that h1h21 a.e. in Ω. Then for any uLh1()h2()(Ω),

    |u|h1()h2()uh1h1()h2()+uh+1h1()h2().

    The generalized Sobolev space, denoted by Wk,p()(Ω), is defined as follows

    Wk,p()(Ω)={uLp()(Ω)|DαuLp()(Ω),|α|k}

    where

    Dαu=|α|xα11xαNNu

    with α=(α1,,αN) is a multi-index and |α|=Ni=1αi. The space Wk,p()(Ω), equipped with the norm

    uk,p():=|α|k|Dαu|p(),

    is a uniformly convex, separable, and reflexive Banach space.

    In the present part, we recall some properties of the fractional Sobolev spaces with variable exponents which will be useful in the rest of the paper. For more details, we can refer to [14,21,22,25,26].

    In the present part, we give the variational setting of problem (1.1) and state important results to be used later. We set Q:=R2N(CΩRN×CΩRN) and define the fractional Sobolev space with variable exponent as

    X=Ws(x,y),¯p(x),p(x,y)(Ω):={u:RNR:u|ΩL¯p(x)(Ω),Q|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy<, for some η>0}.

    The space X is equipped with the norm

    uX:=uL¯p(x)(Ω)+[u]X;

    where [u]X is the seminorm defined as follows

    [u]X=inf{η>0:Q|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy<1}.

    Then (X,X) is a separable reflexive Banach space.

    Now, define the subspace X0 of X as

    X0=:={uX:u=0 a.e. in Ωc}.

    We define the norm on X0 as follows

    uX0:=inf{η>0:Q|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy<1}.

    Remark 2.1. For uX0, we obtain

    Q|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy=RN×RN|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy.

    Thus, we have

    uX0:=inf{η>0:RN×RN|u(x)u(y)|p(x,y)ηp(x,y)|xy|N+s(x,y)p(x,y)dxdy<1}.

    Now we state the following continuous and compact embedding result for the space X0. The proof follows from [27, Theorem 2.2, Remark 2.2].

    Theorem 2.1. Let Ω be a smooth bounded domain in RN, s(,)(0,1) and p(,) satisfy (H1) and (H2) with s+p+<N. Then, for any rC+(¯Ω) such that 1<r(x)<ps(x) for all x¯Ω, there exits a constant C=C(N,s,p,r,Ω)>0 such that for every uX0,

    uLr(x)(Ω)CuX0.

    Moreover, this embedding is compact.

    Definition 2.1. For uX0, we define the modular ρX0:X0R as

    ρX0(u):=RN×RN|u(x)u(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy. (2.1)

    The interplay between the norm in X0 and the modular function ρX0 can be studied in the following lemma.

    Lemma 2.2. Let uX0 and ρX0 be defined as in (2.1). Then we have the following results:

    (i) uX0<1 (=1;>1) if and only if ρX0(u)<1(=1;>1).

    (ii) If uX0>1, then upX0ρX0(u)up+X0.

    (iii) If uX0<1, then up+X0ρX0(u)upX0.

    The next lemma can easily be obtained using the properties of the modular function ρX0 from Lemma 2.2.

    Proposition 2.1. ([19,28]). Let u,umX0, mN. Then the following two statements are equivalent:

    (i) limmumuX0=0,

    (ii) limmρX0(umu)=0.

    Lemma 2.3 ([27, Lemma 2.3]). (X0,X0) is a separable, reflexive and uniformly convex Banach space.

    In this part, we will use as the space of work, the space X0, and by simplicity we will denote this as X instead of X0 in the rest of this paper.

    Considering the variational structure of (1.1), we look for critical points of the corresponding Euler-Lagrange functional Iλ,β:XR, which is defined as follows:

    Iλ,β(u)=aσp(x,y)(u)bγ+1(σp(x,y)(u))γ+1λk1+1(Ω1q(x)|u|q(x)dx)k1+1βk2+1(Ω1r(x)|u|r(x)dx)k2+1, (3.1)

    for all uX. It is important to note that Iλ,β is a C1(X,R) functional, and its derivative can be computed as follows:

    Iλ,β(u),ϕ=[ab(σp(x,y)(u))γ]Ω×Ω|u(x)u(y)|p(x,y)2(u(x)u(y))(ϕ(x)ϕ(y))|xy|N+p(x,y)s(x,y)dxdyλ(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uϕdxβ(Ω1r(x)|u|r(x)dx)k2Ω|u|r(x)2uϕdx, (3.2)

    for any vX. Consequently, critical points of Iλ,β correspond to weak solutions of (1.1).

    Lemma 3.1. Assuming that (1.3) is valid, then the functional Iλ,β satisfies the Palais-Smale condition at level c, where c(0,aγ+1γb1γ+b1γγ).

    Proof. Let un be a (PS)c sequence of Iλ,β with c(0,aγ+1γb1γ+b1γγ). This implies that the following conditions hold:

    Iλ,β(un)c,Iλ,β(un)0 in X,n, (3.3)

    where X denotes the dual space of X.

    Step 1. We aim to prove that the sequence un is bounded in X. By assuming the contrary, i.e., supposing that un is unbounded in X, so up to a subsequence, we may assume that unX as n. we have

    p+c+1+unXp+Iλ,β(un)Iλ,β(un),un=p+(aσp(x,y)(un)bγ+1(σp(x,y)(un))γ+1λk1+1(Ω1q(x)|un|q(x)dx)k1+1βk2+1(Ω1r(x)|un|r(x)dx)k2+1)([ab(σp(x,y)(un))γ]Ω×Ω|un(x)un(y)|p(x,y)|xy|N+p(x,y)s(x,y)dxdyλ(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)dxβ(Ω1r(x)|un|r(x)dx)k2Ω|un|r(x)dx)b(p+)γ(1p+(γ+1)(p))(Ω×Ω|un(x)un(y)|p(x,y)|xy|N+p(x,y)s(x,y)dxdy)γ+1+λ(q+)k1(1p+(k1+1)(q))(Ω|un|q(x)dx)k1+1+β(r+)k2(1p+(k2+1)(r))(Ω|un|r(x)dx)k2+1. (3.4)

    From (1.3) and the fact that γ>0 and ki>0 for i=1,2, it follows that

    {1p+(γ+1)(p)>0,1p+(k1+1)(q)>0,1p+(k2+1)(r)>0. (3.5)

    We deduce from (3.4) and (3.5), that

    p+c+1+unXb(p+)γ(1p+(γ+1)(p))(Ω×Ω|un(x)un(y)|p(x,y)|xy|N+p(x,y)s(x,y)dxdy)γ+1.

    If the sequence (un) is unbounded in X, we can assume, by passing to a subsequence if necessary, that unX>1. Considering the previous inequalities, we have the following:

    p+c+1+unXb(p+)γ(1p+(γ+1)(p))un(γ+1)pX,

    which is absurd since (γ+1)p>1. Thus, {un} must be bounded in X, and the first assertion is proven.

    Step 2. Now, we aim to demonstrate that the sequence {un} has a convergent subsequence in X. According to Theorem 2.1, the embedding XLτ(x)(Ω) is compact, where 1τ(x)<ps(x). Since X is a reflexive Banach space, passing, if necessary, to a subsequence, there exists uX satisfying:

    unu in X,unu in Lτ(x)(Ω),un(x)u(x), a.e. in Ω. (3.6)

    From (3.2), we find that

    Iλ,β(u),unu=[ab(σp(x,y)(un))γ]Ω×Ω|un(x)un(y)|p(x,y)2(un(x)un(y))((un(x)u(x))(un(y)u(y)))|xy|N+p(x,y)s(x,y)dxdyλ(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2un(unu)dxβ(Ω1r(x)|un|r(x)dx)k2Ω|un|r(x)2un(unu)dx. (3.7)

    Furthermore, utilizing Hölder's inequality and (3.6), we can estimate:

    |Ω|un|q(x)2un(unu)dx|Ω|un|q(x)1|unu|dxC||un|q(x)1|q(x)q(x)1|unu|q(x)Cmax{unq+1X,unq1X}|unu|q(x). (3.8)

    Therefore, thanks to the convergence result (3.6), we can deduce that

    |unu|q(x)0 as n. (3.9)

    By combining the boundedness of {un} in X with the estimates (3.8) and (3.9), we can conclude that

    limnΩ|un|q(x)2un(unu)dx=0.

    As {un} is bounded in X, there exist positive constants c1 and c2 such that

    c1Ω1q(x)|un|q(x)dxc2. (3.10)

    So, we have

    (Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2un(unu)dx0. (3.11)

    Similarly, we obtain

    limn(Ω1r(x)|un|r(x)dx)k2Ω|un|r(x)2un(unu)dx=0. (3.12)

    By (3.3), we have

    Iλ,β(u),unu0.

    Which means, based on equations (3.11) and (3.12), that

    [ab(σp(x,y)(un))γ]Ω×Ω|un(x)un(y)|p(x,y)2(un(x)un(y))((un(x)u(x))(un(y)u(y)))|xy|N+p(x,y)s(x,y)dxdy0. (3.13)

    Since {un} is bounded in X, passing to a subsequence, if necessary, we may assume that when n

    σp(x,y)(un)=Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdyt00.

    Considering two cases: t0=0 and t0>0. Now, proceed with a case analysis. First, if t0=0, then the sequence {un} converges strongly to u=0 in X, and the proof is concluded. However, if t0>0, we will further examine the two sub-cases below:

    Subcase 1. If t0(ab)1γ then ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ0 is false, and there is no subsequence of {ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ0} that converges to zero. Thus, we can find a positive value δ>0 such that

    |ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ|>δ>0,

    for sufficiently large n. As a result, we can conclude that the set

    {ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ0} is bounded. (3.14)

    Subcase 2. If t0=(ab)1γ, then

    ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ0.

    We define

    φ(u)=λk1+1(Ω1q(x)|u|q(x)dx)k1+1+βk2+1(Ω1r(x)|u|r(x)dx)k2+1,for alluX.

    Then

    φ(u),v=λ(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uvdx+β(Ω1r(x)|u|r(x)dx)k2Ω|u|r(x)2uvdx,for allvX.

    It follows that

    φ(un)φ(u),v=λ[(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2unvdx(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uvdx]+β[(Ω1r(x)|un|r(x)dx)k2Ω|un|r(x)2unvdx(Ω1r(x)|u|r(x)dx)k2Ω|u|r(x)2uvdx].

    To complete our proof we require the following lemma.

    Lemma 3.2. Suppose we have sequences un and u belonging to X such that (3.6) is satisfied. Then, passing to a subsequence, if necessary, the following properties hold:

    (i) limn[(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2unvdx(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uvdx]=0;

    (ii) limn[(Ω1r(x)|un|r(x)dx)k2Ω|un|r(x)2unvdx(Ω1r(x)|u|r(x)dx)k2Ω|u|r(x)2uvdx]=0;

    (iii) φ(un)φ(u),v0,vX.

    Proof. By (3.6), we have unu in Lp(x)(Ω) which implies that

    |un|p(x)2un|u|p(x)2u in Lp(x)p(x)1(Ω). (3.15)

    From (3.10) we deduce that

    ck11(Ω1q(x)|un|q(x)dx)k1,(Ω1q(x)|u|q(x)dx)k1ck12. (3.16)

    Due to Hölder's inequality, we have

    |(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2unvdx(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uvdx|=|(Ω1q(x)|un|q(x)dx)k1Ω|un|q(x)2unvdx+(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2u(v)dx|ck12|Ω(|un|q(x)2un|u|q(x)2u)vdx|ck12||un|q(x)2un|u|q(x)2u|q(x)q(x)1|v|q(x)Cck12||un|q(x)2un|u|q(x)2u|q(x)q(x)1vX0.

    By making a minor adjustment to the aforementioned proof, we can also establish assertion (ii), but we will omit the specific details. As a result, by combining parts (i) and (ii), we can conclude assertion (iii).

    Consequently, φ(un)φ(u)X0 and φ(un)φ(u).

    We are now able to conclude the proof of Subcase 2. Utilizing Lemma 3.2 and taking into account the fact that Iλ,β(u),v=[ab(σp(x,y)(u))γ]Ω×Ω|u(x)u(y)|p(x,y)2(u(x)u(y))(v(x)v(y))|xy|N+p(x,y)s(x,y)dxdyφ(u),v, Iλ,β((un),v0 and ab(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ0, then we can infer that φ(un)0(n), i.e.,

    φ(u),v=λ(Ω1q(x)|u|q(x)dx)k1Ω|u|q(x)2uvdx+β(Ω1r(x)|u|r(x)dx)k2Ω|u|r(x)2uvdx,for allvX,

    and therefore

    λ(Ω1q(x)|u|q(x)dx)k1|u(x)|q(x)2u(x)+β(Ω1r(x)|u|r(x)dx)k2|u(x)|r(x)2u(x)=0 for a.e.xΩ.

    By invoking the fundamental lemma of the variational method (see [29]), we can conclude that u=0. Hence,

    φ(un)=λk1+1(Ω1q(x)|un|q(x)dx)k1+1+βk2+1(Ω1r(x)|un|r(x)dx)k2+1λk1+1(Ω1q(x)|u|q(x)dx)k1+1+βk2+1(Ω1r(x)|u|r(x)dx)k2+1=0.

    Hence, we can deduce that

    Iλ,β(un)=aΩ×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdybγ+1(Ω×Ω1p(x,y)|un(x)un(y)|p(x,y)|xy|N+s(x,y)p(x,y)dxdy)γ+1λk1+1(Ω1q(x)|u|q(x)dx)k1+1βk2+1(Ω1r(x)|u|r(x)dx)k2+1γaγ+1γ(γ+1)b1γ.

    Therefore, we have reached a contradiction since .

    Then is not true. Similarly to Subcase 1, we can argue as follows:

    So, combining the two cases discussed above, we can conclude that:

    Therefore, by invoking the condition and Proposition 2.1, we conclude that as , which implies that satisfies the condition. Hence, the proof is now complete.

    Lemma 3.3. Assuming that (1.4) is valid, the functional satisfies the Palais-Smale condition at all levels .

    Proof. Let be a sequence of , that is

    (3.17)

    where is the dual space of .

    Step 1. We will prove that is bounded in . Let us assume by contradiction that is unbounded in . Without loss of generality, we can assume that for all . Take

    then, we have

    (3.18)

    For simplicity, denote

    (3.19)

    Using (3.18) and (3.19), we can write

    (3.20)

    It follows from (1.4) and (3.20) that is bounded in .

    Step 2. We will now demonstrate that the sequence possesses a convergent subsequence in the space . According to Theorem 2.1, the embedding is compact where . Since is a reflexive Banach space, passing, if necessary, to a subsequence, there exists such that

    (3.21)

    From (3.2), we find that

    (3.22)

    So, we have

    (3.23)

    Similarly, we obtain

    (3.24)

    By (3.17), we have

    So, based on the expressions (3.23) and (3.24), we can conclude that (3.22) leads to the following implications:

    (3.25)

    Since is bounded in and , we have

    Therefore, we can conclude from the two aforementioned cases that

    Therefore, by utilizing the condition and Proposition 2.1, we can deduce that as , indicating that satisfies the condition. This concludes the proof.

    In this part, we will prove Theorem 1.1 by applying the mountain pass theorem, see [29].

    Lemma 4.1. Assume that (1.3) holds. Then there exist and such that , for any with .

    Proof. Let with . From (3.3), Lemma 2.2 and Sobolev immersions, we get

    Hence, based the fact that and satisfies condition (1.3), we infer the result.

    Lemma 4.2. Assume that the conditions , , (1.3) hold. Then there exists with (where is given by Lemma 4.1) such that .

    Proof. Let . According the condition (1.3), for large enough, we have

    If condition (1.3) holds, then as . So, for some large enough, we deduce that and . Choosing , the proof of Lemma 4.2 is completed.

    Proof of Theorem 1.1.

    It follows from Lemmas 3.3, 4.1, 4.2 and the fact that , satisfies all conditions of the mountain pass theorem [29]. Thus, problem (1.1) admits a nontrivial weak solution.

    Since is a reflexive and separable Banach space, there exist and such that where means the Kronecker symbol.

    We denote

    Now, we consider and denote

    Theorem 5.1 (Fountain Theorem, see [29]). Let be a Banach space with the norm and let be a sequence of subspace with for each . In addition, set

    For each even functional and for each , we suppose that there exists such that

    (1) ,

    (2) , ,

    (3) The functional satisfies the condition for every .

    Then admits an unbounded sequence of critical values.

    To prove our result, we will use the Fountain theorem 5.1. So, this proof is divided in several lemmas given as follows

    Lemma 5.1. (see [26]) If satisfying and let denote by

    Then

    Lemma 5.2. The functional verifies the following property , where the space is given in Theorem 5.1.

    Proof. Let Since , then or all norms are equivalent in the finite dimensional space. With such that , we have

    Hence, using the embeddings and (see Theorem 2.1) and based the inequality (1.3), we infer that

    Lemma 5.3. The functional verifies the following property , , where the space is given in Theorem 5.1.

    Proof. Let with . So, we have

    So, we obtain

    where,

    and

    Hence, we have

    So, based the fact that and , we can deduce that for sufficiently large, we have and . Thus, we have , since we have taken

    Proof of Theorem 1.2 We have that belongs to , even functional and verifies the Palais-smale condition. Moreover, we have

    and

    for Then, by using the Fountain theorem, we deduce that admits an unbounded sequence of critical points.

    To prove Theorem 1.3, we shall use the following symmetric mountain pass theorem in [30]:

    Theorem 5.2. ([30]). Let be a real infinite dimensional Banach space and satisfying the Palais-Smale condition. Suppose , where is finite dimensional, and assume the following conditions:

    1. is even and ;

    2. there exist and such that for any with ;

    3. for any finite dimensional subspace there is such that for , ;

    then, possesses an unbounded sequence of critical values.

    Lemma 5.4. Assume that (1.4) holds. Then there exist and such that , for any with .

    Proof. Let with . Following, let denote by the eigenvalue related to our operator. By using the Sobolev immersions, we get

    Thus,

    Choosing

    we deduce, for any with , that

    (5.1)

    Now, we put

    We can conclude that for any (respectively ), there exists such that for any with

    We have completed the proof of Lemma 5.4.

    Lemma 5.5. Assume that (1.4) holds. Then for every finite dimensional subspace , there exists such that , for all , with .

    Proof. Let , for all , with , then, we have

    Therefore, as a consequence, all norms on the finite-dimensional space are equivalent, implying the existence of a positive constant such that

    Therefore, we obtain

    Then, it is deduced from (1.4) that . Hence, the proof of Lemma 5.5 is complete.

    Hamdani was supported by the Tunisian Military Research Center for Science and Technology Laboratory LR19DN01.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors declare there is no conflict of interest.



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