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Infinitely many periodic solutions for ordinary p(t)-Laplacian differential systems

  • In this paper, we consider the existence of infinitely many periodic solutions for some ordinary p(t)-Laplacian differential systems by minimax methods in critical point theory.

    Citation: Chungen Liu, Yuyou Zhong. Infinitely many periodic solutions for ordinary p(t)-Laplacian differential systems[J]. Electronic Research Archive, 2022, 30(5): 1653-1667. doi: 10.3934/era.2022083

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  • In this paper, we consider the existence of infinitely many periodic solutions for some ordinary p(t)-Laplacian differential systems by minimax methods in critical point theory.



    Consider periodic solution of the ordinary p(t)-Laplacian differential system

    {ddt(|˙u(t)|p(t)2˙u(t))+F(t,u(t))=0,uRN,u(0)u(T)=˙u(0)˙u(T)=0, (1.1)

    where T>0, p(t)>1 is a T-periodic continuous function, F(t,x) is T-periodic in t for any xRN. Here we always assume that F(t,x) satisfies the following condition.

    (A) F(t,x) is measurable in t for any xRN and continuously differentiable in x for a.e. t[0,T], and there exist two functions aC(R+;R+),bL1([0,T];R+) such that

    |F(t,x)|a(|x|)b(t),|F(t,x)|a(|x|)b(t),xRNanda.e.t[0,T],

    where F(t,x) denotes the gradient of F(t,x) in x.

    In the sequel of this paper, we set p:=min0tTp(t), p+:=max0tTp(t) and q>1 such that 1p+1q=1.

    We define the generalized Lebesgue space as

    Lp(t)T=Lp(t)(ST;RN):={uL1(ST;RN):T0|u|p(t)dt<},ST=R/TZ

    with the norm

    uLp(t)=inf{λ>0:T0|uλ|p(t)dt1}.

    Lp(t)T is a kind of generalized Orlicz space. We also define the generalized Sobolev space by

    W1,p(t)T=W1,p(t)(ST;RN):={uLp(t)(ST;RN):˙uLp(t)(ST;RN)}

    with the norm

    uW1,p(t)T=u=uLp(t)+˙uLp(t).

    W1,p(t)T is a kind of generalized Orlicz-Sobolev space. In our case with the condition p(t)>1, the two spaces Lp(t)T and W1,p(t)T are both reflective Banach spaces with the norms defined above. It is known that there is a compact embedding W1,p(t)TC([0,T];RN). One can refer [1] for details.

    The corresponding functional φ of (1.1) on W1,p(t)T is given by

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt,uW1,p(t)T. (1.2)

    Wang and Yuan in [2] verified that the functional φ denoted in (1.2) is continuously differentiable, i.e., there holds

    φ(u),v=T0[(|˙u(t)|p(t)2˙u(t),˙v(t))(F(t,u(t)),v(t))]dt

    for any u,vW1,p(t)T. So the critical points of φ correspond to the solutions of problem (1.1). Then Zhang et al. in [3] proved that the functional φ defined in (1.2) is weakly lower semicontinuous on W1,p(t)T.

    When p(t)=2, problem (1.1) reduces to the following Hamiltonian system

    {¨u(t)+F(t,u(t))=0a.e.t[0,T],u(0)u(T)=˙u(0)˙u(T)=0, (1.3)

    which has been extensively investigated in many literatures (see, e.g., [4,5,6,7,8] and the references therein). Particularly, under the following conditions:

    (M1) there exists gL1([0,T];R+) such that |F(t,x)|g(t) for xRN and a.e. t[0,T],

    (M2) T0F(t,x)dt± as |x|+,

    Mawhin and Willem in [6] established the existence of solutions for problem (1.3).

    When N=1, T=2π, Habets, Manasevich and Zanolin in [4] established the existence of two sequences of different periodic solutions for problem (1.3) when the potential F(t,x) satisfies the following oscillating conditions:

    lim supa±2π0F(t,a)dt=+,lim infb±2π0F(t,b)dt=.

    When the nonlinearity F(t,x) is sublinear, i.e., there exist f,gL1([0,T];R+) and α[0,1) such that

    |F(t,x)|f(t)|x|α+g(t),xRNanda.e.t[0,T],

    and F(t,x) satisfies oscillating conditions, i.e., there holds

    lim supr+infxRN,|x|=r|x|2αT0F(t,x)dt=+,lim infR+supxRN,|x|=R|x|2αT0F(t,x)dt=,

    Zhang and Tang in [8] obtained the existence of two sequences of different periodic solutions for problem (1.3).

    When p(t)=p is a constant for general p>1, problem (1.1) reduces to the following ordinary p-Laplacian problem

    {ddt(|˙u(t)|p2˙u(t))+F(t,u(t))=0,a.e.t[0,T],u(0)u(T)=˙u(0)˙u(T)=0. (1.4)

    In recent years, the existence results for problem (1.4) was considered via the variational methods (see, e.g., [9,10,11] and references therein). Specially, L¨u, O'Regan and Agarwal in [10] generalized the results of [4] to the p-Laplacian problem (1.4) and established the existence of two sequences of different periodic solutions for problem (1.4). Li, Agarwal and Tang in [9] also established the existence of two sequences of different periodic solutions for problem (1.4) for the case with the potential F(t,x) possessing the mixed nonlinearity, that is, F(t,x)=F1(t,x)+F2(t,x) with F1(t,x) being (λ,μ)-subconvex in x, i.e., function F1(t,):RNR satisfies

    F1(t,λ(x+y))μ(F1(t,x)+F1(t,y)) (1.5)

    for some λ,μ>0 and each x,yRN (see [7] for details) and F2(t,x) being p-sublinear, namely, there exist f,gL1([0,T];R+) and α[0,p1) such that

    |F2(t,x)|f(t)|x|α+g(t),xRNanda.e.t[0,T].

    Then they also considered the other case with the nonlinearity F(t,x) being p-linear, i.e., there exist f,gL1([0,T];R+) such that

    |F(t,x)|f(t)|x|p1+g(t),xRNanda.e.t[0,T].

    Many scholars are interested in the nonlinear problems including the p(t)-Laplacian problem, this kind of problems can be used to model the dynamical phenomena arising from the field of elastic mechanics. One can refer [12,13] and the references therein for more application of the p(t)-Laplacian problem to various practical issues. The p(t)-Laplacian problem has more complicated nonlinearity than that of the p-Laplacian problem, for example, the second order differential operator is not homogeneous, this may causes some troubles such as some classical theories and methods, for instance, the Sobolev spaces theory are not applicable.

    In recent years, the study of variational problems and elliptic partial differential equations with nonstandard growth conditions has been an interesting topic (see, e.g., [13,14] and references therein). In 2001, Fan et al. in [14,15] established some basic theory of space Lp(x)(Ω) and Wk,p(x)(Ω). In 2003, Fan et al. in [1] first studied the ordinary p(t)-Laplacian problem (1.1). Subsequently, Wang and Ruan in [2] established the existence and multiplicity of periodic solutions for the ordinary p(t)-Laplacian problem (1.1) under the generalized Ambrosetti-Rabinowitz conditions. Recently, many scholars considered the existence of periodic solutions of the ordinary p(t)-Laplacian problem (1.1). Some existence theorems of the ordinary p(t)-Laplacian problem (1.1) are established by using the least action principle and minimax methods in critical point theory (see, e.g., [1,3,16] and the references therein).

    In this paper, motivated by the results of [4,5,8,9,10], we first aim to consider the ordinary p(t)-Laplacian problem (1.1) with a mixed nonlinearity, that is, F(t,x)=F1(t,x)+F2(t,x) with F1(t,x) being (λ,μ)-subconvex and F2(t,x) being p-sublinear. Then we consider the other case with the nonlinearity F(t,x) being p-linear. Following the idea of paper [8,9], we obtain the existence of two sequences of different periodic solutions for problem (1.1). The main results of this paper are stated as follows.

    Theorem 1.1 Assume that F(t,x)=F1(t,x)+F2(t,x) where F1(t,x) and F2(t,x) satisfy condition (A) and the following conditions.

    (H1) F1(t,) is (λ,μ)-subconvex defined in (1.5) with λ>12 and 12μ<(2λ)p for a.e. t[0,T], and there exist α[0,p1),f,gL1([0,T];R+) such that

    |F2(t,x)|f(t)|x|α+g(t),forxRNanda.e.t[0,T].

    (H2) There exists a positive sequence {Rn} with limn+Rn=+, such that

    limn+infxRN,|x|=RnT0F(t,x)dt=+

    and there exists a positive sequence {rm} with limm+rm=+, such that

    limm+supxRN,|x|=rm1rqαm(μT0F1(t,xλ)dt+T0F2(t,x)dt)=.

    Then problem (1.1) possesses two sequences of solutions {u±n} with φ(u±n)± as n+.

    Remark 1.2 Theorem 1.1 above generalizes Theorem 1.1 of [10], Theorem 1.1 of [8], Theorem 1 of [5] and Theorem 1.1 of [9]. There are functions F(t,x) satisfying the conditions in Theorem 1.1 but not satisfying the conditions in [5,8,9,10]. For example, for p(t)=4+cosωt with ω=2πT, we take

    F1(t,x)=5+sin|x|6,F2(t,x)=|x|7/4sin(ln(|x|2+1))+(e(t),x),

    where eL1([0,T];RN) and T0e(t)dt=0. Then F(t,x)=F1(t,x)+F2(t,x) is such a function.

    Theorem 1.3 Assume that F(t,x) satisfies condition (A) and the following conditions.

    (H3) There exist f,gL1([0,T];R+) with fL1<α(p) such that

    |F(t,x)|f(t)|x|p1+g(t),xRNanda.e.t[0,T],

    where α(p) is a positive constant depending on the function p(t), and so on the constants p±.

    (H4) There exists a positive sequence {Rn} with limn+Rn=+, such that

    limn+infxRN,|x|=RnT0F(t,x)dt=+

    and there exists a positive sequence {rm} with limm+rm=+, such that

    limm+supxRN,|x|=rm1rpmT0F(t,x)dt<β(p),

    where β(p) is a positive constant depending on the function p(t), and so on the constants p±. Then problem (1.1) possesses two sequences of solutions {u±n} such that φ(u±n)± as n+.

    Remark 1.4 In the process of the proof of Theorem 1.3, the constants α(p) and β(p) will be defined clearly (see (3.20) and (3.26)). Theorem 1.3 above generalizes Theorem 1.3 of [9] since here the range of the function p(t) is wider than theirs. There exist functions satisfying the conditions of Theorem 1.3. For example, for p(t)=54+18cosωt, one can take

    F(t,x)=1T|x|178sin(716ln(|x|2+1)).

    Then F(t,x) satisfies the conditions of Theorem 1.3 with p=98,p+=118,q=9,θp=1,f(t)=3T.

    For the convenience of readers, we first introduce two important properties of the variable exponent Lebesgue-Sobolev spaces Lp(t) and W1,p(t)T.

    We define

    ˜W1,p(t)T={uW1,p(t)T:T0u(s)ds=0}.

    For uW1,p(t)T, let

    ˉu=1TT0u(s)ds,

    then ˜u(t)=u(t)ˉu˜W1,p(t)T. So we get

    W1,p(t)T=RN˜W1,p(t)T.

    Lemma 2.1 [16] For all u˜W1,p(t)T, there exist constants C0, C0 such that

    uC0˙uLp(t),u2C0[(T0|˙u(t)|p(t)dt)1p+T1p],

    where C0, C0>0.

    Lemma 2.2 [1] Let u=ˉu+˜uW1,p(t)T with ˉuRN and ˜u˜W1,p(t)T, then the norm ˙˜uLp(t) is an equivalent norm on ˜W1,p(t)T and |ˉu|+˙uLp(t) is an equivalent norm on W1,p(t)T. Therefore, for uW1,p(t)T,

    u+|ˉu|+T0|˙u(t)|p(t)dt+.

    Next we give two important properties of minimax methods as follows.

    Lemma 2.3[6] Let K be a compact metric space, X a Banach space and K0K is a closed subset, χC(K0;X). We define a complete metric space M as

    M={γC(K;X):γ(s)=χ(s),sK0}

    with the usual norm and metric. Let φC1(X;R) and

    c=infγMmaxsKφ(γ(s)),c1=maxχ(K0)φ.

    If c>c1, then for each ε>0 and each γM such that

    maxsKφ(γ(s))c+ε,

    there exists vX such that

    cεφ(v)maxsKφ(γ(s)),dist(v,γ(K))ε1/2,|φ(v)|ε1/2.

    Corollary 2.4[6] Under the conditions of Lemma 2.3, for each sequence (γk) in M such that

    maxKφ(γk)c,

    there exists a sequence (vk) in X such that

    φ(vk)c,dist(vk,γk(K))0,|φ(vk)|0ask+.

    Proof of Theorem 1.1. The proof is divided into four steps.

    Step 1. We demonstrate that φ(u)+ as u for u˜W1,p(t)T.

    Let β=log2λ(2μ), then one gets 0β<p. For |x|>1, there exists a positive integer n such that

    n1<log2λ|x|n.

    Therefore one has |x|β>(2λ)(n1)β=(2μ)n1 and |x|(2λ)n. Combining the conditions (A) and (H1), one obtains

    F1(t,x)2μF1(t,x2λ)(2μ)nF1(t,x(2λ)n)2μ|x|βa0b(t)

    for any |x|>1 and a.e. t[0,T], where a0=max0s1a(s). Therefore one gets

    F1(t,x)(2μ|x|β+1)a0b(t) (3.1)

    for any |x|>1 and a.e. t[0,T]. In the sequel, we denote by C a suitable positive constant which may take different value in various estimations.

    Combining Lemma 2.1, (H1) and (3.1), for the functional φ defined in (1.2), we obtain

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt1p+T0|˙u(t)|p(t)dtT0F1(t,u(t))dtT0F2(t,u(t))dt1p+T0|˙u(t)|p(t)dtT0(2μ|u(t)|β+1)a0b(t)dt1α+1T0f(t)|u(t)|α+1dtT0g(t)|u(t)|dt1p+T0|˙u(t)|p(t)dt2μa0uβT0b(t)dtT0a0b(t)dtuα+1fL1α+1ugL11p+T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)βpC(T0|˙u(t)|p(t)dt)α+1pC(T0|˙u(t)|p(t)dt)1pC (3.2)

    for any u˜W1,p(t)T. From Lemma 2.2, estimate (3.2) implies that

    φ(u)+asu+foru˜W1,p(t)T.

    Step 2. We verify that for the positive sequence {rm} defined in (H2), there holds

    limm+infuWrmφ(u)=+, (3.3)

    where Wrm={uRN||u|=rm}˜W1,p(t)T.

    By Lemma 2.1, (H1) and Young inequality, we obtain

    |T0(F2(t,u(t))F2(t,ˉu))dt|=|T010(F2(t,ˉu+s˜u(t)),˜u(t))dsdt|T010f(t)|ˉu+s˜u(t)|α|˜u(t)|dsdt+T010g(t)|˜u(t)|dsdt2p1(|ˉu|α+˜uα)˜uT0f(t)dt+˜uT0g(t)dt=((p2p+)1/p˜u2C0)((p2p+)1/p2pC0T0f(t)dt)|ˉu|α+2p1˜uα+1T0f(t)dt+˜uT0g(t)dt12p+T0|˙u(t)|p(t)dt+C|ˉu|qα+C(T0|˙u(t)|p(t)dt)α+1p+C(T0|˙u(t)|p(t)dt)1p+C (3.4)

    for any uW1,p(t)T, where C0 is the constant defined in Lemma 2.1.

    Hence from (H1), (3.1) and (3.4), for the functional φ defined in (1.2), we have

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt1p+T0|˙u(t)|p(t)dtT0F1(t,u(t))dtT0F2(t,u(t))dt1p+T0|˙u(t)|p(t)dtμT0F1(t,ˉuλ)dtμT0F1(t,˜u(t)λ)dtT0(F2(t,u(t))F2(t,ˉu))dtT0F2(t,ˉu)dt12p+T0|˙u(t)|p(t)dtμT0F1(t,ˉuλ)dtμ(2μλβ˜uβ+1)T0a0b(t)dtC|ˉu|qαT0F2(t,ˉu)dtC(T0|˙u(t)|p(t)dt)α+1pC(T0|˙u(t)|p(t)dt)1pC12p+T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)α+1pC(T0|˙u(t)|p(t)dt)1pC(T0|˙u(t)|p(t)dt)βp|ˉu|qα(1|ˉu|qα(μT0F1(t,ˉuλ)dt+T0F2(t,ˉu)dt+C))C. (3.5)

    One can check that

    B=inf˜u˜W1,p(t)T(12p+T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)α+1pC(T0|˙u(t)|p(t)dt)1pC(T0|˙u(t)|p(t)dt)βp)>

    and

    infuWrmφ(u)BCsupˉuRN,|ˉu|=rm|rm|qα(1|rm|qα(μT0F1(t,ˉuλ)dt+T0F2(t,ˉu)dt)).

    Thus the above inequality and (H2) imply (3.3).

    Step 3. Prove (ⅰ) of Theorem 1.1. For the positive sequence {Rn} defined in the condition (H2), we define

    Γn={γC(BRn;W1,p(t)T)|γ|BRn=id|BRn}

    and

    cn=infγΓnmaxxBRnφ(γ(x)), (3.6)

    where

    Bδ={xRN||x|δ}.

    One can verify that γ(BRn)˜W1,p(t)T (for more details see [10]).

    From Step 1, we know that φ is coercive on ˜W1,p(t)T. Since W1,p(t)T is a reflective Banach space, hence there is a constant M such that

    maxxBRnφ(γ(x))infu˜W1,p(t)Tφ(u)=M. (3.7)

    Combining (3.6) and (3.7), one obtains that cnM.

    As in (3.3), we can easily verify that

    limn+supuRN,|u|=Rnφ(u)=. (3.8)

    From (3.8), for large enough n, we obtain

    cn>supuRN,|u|=Rnφ(u).

    Now in Lemma 2.3 and Corollary 2.4, we take the compact set K=BRn and K0=BRn, then for any sequence {γk}Γn such that

    maxxBRnφ(γk(x))cn, (3.9)

    there exists a sequence {vk}W1,p(t)T satisfying

    φ(vk)cn,dist(vk,γk(BRn))0,|φ(vk)|0,ask. (3.10)

    Combining (3.6), (3.9) and (3.10), for k large enough, we have

    cnmaxxBRnφ(γk(x))cn+1 (3.11)

    Define π:W1,p(t)TRN as

    π(u)=1TT0u(t)dt,foruW1,p(t)T.

    For fixed n, we obtain

    |π(γk(BRn))|Kn.

    for some positive constant Kn, here |S|:=supxSx for a set SRN.

    We now take ωkγk(BRn) such that

    vkωk1. (3.12)

    We write ωk=ˉωk+˜ωk with ˉωkRN and ˜ωk˜W1,p(t)T. So there holds |ˉωk|Kn, which implies that

    μT0F1(t,ˉωkλ)dt+T0F2(t,ˉωk)dt

    is bounded. Combining (H1), (3.1), (3.4), (3.11) and Lemma 2.1, we obtain

    cn+1φ(ωk)=T0|˙ωk(t)|p(t)p(t)dtT0F(t,ωk(t))dt1p+T0|˙ωk(t)|p(t)dtT0F1(t,ωk(t))dtT0F2(t,ωk(t))dt1p+T0|˙ωk(t)|p(t)dtμT0F1(t,ˉωkλ)dtμT0F1(t,˜ωk(t)λ)dtT0(F2(t,ωk(t))F2(t,ˉωk))dtT0F2(t,ˉωk)dt12p+T0|˙ωk(t)|p(t)dtμT0F1(t,ˉωkλ)dtμ(2μλβ˜ωkβ+1)T0a0b(t)dtCT0F2(t,ˉωk)dtC|ˉωk|qαC(T0|˙ωk(t)|p(t)dt)α+1pC(T0|˙ωk(t)|p(t)dt)1p12p+T0|˙ωk(t)|p(t)dtC(T0|˙ωk(t)|p(t)dt)α+1pC(T0|˙ωk(t)|p(t)dt)1pC(T0|˙ωk(t)|p(t)dt)βpC. (3.13)

    Therefore one can check that {˜ωk} and {ωk} is bounded from Lemma 2.2 and (3.13). By (3.12), we obtain that {vk} is bounded. By a standard argument, one can easy to verify that {vk} possesses a convergent subsequence. It is still denoted by {vk}. One can refer [2] for more details about the proof of (PS) condition.

    Let

    u+n=limk+vk.

    Then from (3.10), we obtain

    φ(u+n)=limk+φ(vk)=cn,φ(u+n)=limk+φ(vk)=0.

    This means u+n is a solution of problem (1.1) with φ(u+n)=cn.

    For all γΓn, by definition, there holds γ(BRn)Wrm. Then we get

    maxxBRnφ(γ(x))infuWrmφ(u). (3.14)

    Now combining (3.3), (3.6) and (3.14), we obtain

    limn+cn=+.

    Hence there exists a sequence of periodic solutions {u+n} which are minimax-type critical points of the functional φ and φ(u+n)+ as n+. So (ⅰ) of Theorem 1.1 is proved.

    Step 4. Prove (ⅱ) of Theorem 1.1. For the sequence {rn} defined in condition (H2) and as the same from (3.3), we define Pn as

    Pn={uW1,p(t)T|u=ˉu+˜u,ˉuRN,|ˉu|rn,˜u˜W1,p(t)T}.

    For uPn, it is easy to see that

    μT0F1(t,ˉuλ)dt+T0F2(t,ˉu)dt

    is bounded.

    Combining (H1), (3.1) and (3.4), for uPn, by the same process as in (3.13), we get

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt12p+T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)α+1pC(T0|˙u(t)|p(t)dt)1pC(T0|˙u(t)|p(t)dt)βpC. (3.15)

    Thus the functional φ is bounded below in Pn.

    Set

    ρn=infuPnφ(u) (3.16)

    and let {uk} be a sequence on Pn such that

    φ(uk)ρnask.

    We write

    uk=ˉuk+˜uk,ˉukRN,|ˉuk|rn,˜uk˜W1,p(t)T.

    From (3.15) and (3.16), it is easy to see that {uk} is bounded sequence in W1,p(t)T. Then {uk} possesses a subsequence, which is still denoted by {uk} such that

    ukuninW1,p(t)T.

    As Pn is a closed convex subset of W1,p(t)T, one has unPn.

    Since the functional φ is weakly lower semicontinuous, we obtain

    ρn=limkφ(uk)φ(un).

    Therefore we get

    ρn=φ(un). (3.17)

    From (3.3), for large n, we get that un{ˉu+˜u,ˉuRN,|ˉu|=rn}, and hence unIntPn={uW1,p(t)T|u=ˉu+˜u,|ˉu|<rn}. Thus combining (3.16) and (3.17), one obtains

    φ(un)=0

    and un is a solution of problem (1.1).

    Since rn+ as n+, we can choose the sequence {Rn} in the condition (H2) and as the same in (3.8) satisfying 0<Rn<rn. By (3.16), we obtain

    φ(un)supxRN,|x|=Rnφ(x). (3.18)

    From (3.8) and (3.18), we have

    φ(un)asn.

    So (ⅱ) of Theorem 1.1 is true. The proof of Theorem 1.1 is complete.

    Proof of Theorem 1.3. The proof is divided into two steps.

    Step 1. We show that φ(u)+ as u for u˜W1,p(t)T.

    Combining Lemma 2.1 and (H3), we obtain

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt1p+T0|˙u(t)|p(t)dt1pT0f(t)|u(t)|pdtT0g(t)|u(t)|dt1p+T0|˙u(t)|p(t)dtfL1pupugL1(1p+(2C0)ppfL1)T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)1pC, (3.19)

    for any u˜W1,p(t)T, where C0 is the positive constant defined in Lemma 2.1. We now define the constant α(p) in Theorem 1.3 as

    α(p)=p2p+θp(2C0)p, (3.20)

    where θp is a positive constant defined by θp=1 for p(1,2], and θp=2p2 for p>2. Now if fL1<α(p), in view of Lemma 2.2, the estimate (3.19) implies that

    φ(u)+asu+foru˜W1,p(t)T.

    Step 2. We verify that for the positive sequence {rm} defined in condition (H4), there holds

    limm+infuWrmφ(u)=+, (3.21)

    where Wrm={uRN||u|=rm}˜W1,p(t)T.

    For uW1,p(t)T with u=ˉu+˜u where |ˉu|=rm and ˜u˜W1,p(t)T. Here we recall that rm is defined in condition (H4), namely we have

    limm+supxRN,|x|=rm1|rm|pT0F(t,x)dt<β(p). (3.22)

    Combining (H3), we obtain

    |T0(F(t,u(t))F(t,ˉu))dt|=|T010(F(t,ˉu+s˜u(t)),˜u(t))dsdt|T010f(t)|ˉu+s˜u(t)|p1|˜u(t)|dsdt+T010g(t)|˜u(t)|dsdtθp(|ˉu|p1˜u+1p˜up)fL1+˜ugL12θppfL1˜up+α(p)θpq|ˉu|p+C˜u, (3.23)

    for any uW1,p(t)T, where 1p+1q=1. Where in (3.23), in the second estimate, we have used the inequality (a+b)cac+bc for a,b0, c(0,1], (a+b)c2c1(ac+bc) for a,b0, c(1,+), and in the last estimate, we have used the Young inequality abapp+bqq, a,b0. In the Lemma 2.1 of [11], we know that for a fixed ρ>1 and any ε>0, there is a number B(ε)>0 such that

    (a+b)ρ(1+ε)aρ+B(ε)bρ,a,b>0.

    Now we take ε>0 such that α(p)(1+ε)fL1+ε, and ρ=p, from Lemma 2.1, there holds

    fL1˜up(α(p)ε)(2C0)pT0|˙˜u|p(t)dt+C.

    Thus we get

    |T0(F(t,u(t))F(t,ˉu))dt|2θp(2C0)p(α(p)ε)pT0|˙˜u|p(t)dt+θpα(p)q|ˉu|p+C(T0|˙˜u|p(t)dt)1p+C. (3.24)

    Therefore, from (H3) and (3.24), we have

    φ(u)=T0|˙u(t)|p(t)p(t)dtT0F(t,u(t))dt1p+T0|˙u(t)|p(t)dtT0(F(t,u(t))F(t,ˉu))dtT0F(t,ˉu)dt(1p+2θp(2C0)p(α(p)ε)p)T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)1p|ˉu|p(1|ˉu|pT0F(t,ˉu)dt+θpα(p)q)C (3.25)

    for all uW1,p(t)T. From (3.20), we can check that

    1p+2θp(2C0)p(α(p)ε)p>0.

    Hence we obtain

    D=inf˜u˜W1,p(t)T(1p+2θp(2C0)p(α(p)ε)p)T0|˙u(t)|p(t)dtC(T0|˙u(t)|p(t)dt)1p)>.

    Now define the constant β(p) in Theorem 1.3 as

    β(p)=p2p+q(2C0)p. (3.26)

    Therefore combining the above expression and (3.22), we obtain (3.21).

    The remainder is similar to that as in the proof of Theorem 1.1, we omit the detail here.

    The first author is Partially supported by the NSF of China (11790271, 12171108), Guangdong Basic and Applied basic Research Foundation(2020A1515011019), Innovation and Development Project of Guangzhou University.

    All authors declare no conflicts of interest in this paper.



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