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A discrete second-order Hamiltonian system with asymptotically linear conditions

  • This paper deals with a non-autonomous discrete second-order Hamiltonian system under asymptotically linear conditions. The existence of a periodic solution is obtained via the saddle point theorem.

    Citation: Xiaoxing Chen, Chungen Liu, Jiabin Zuo. A discrete second-order Hamiltonian system with asymptotically linear conditions[J]. Electronic Research Archive, 2023, 31(9): 5151-5160. doi: 10.3934/era.2023263

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  • This paper deals with a non-autonomous discrete second-order Hamiltonian system under asymptotically linear conditions. The existence of a periodic solution is obtained via the saddle point theorem.



    We are interested in the following discrete second-order Hamiltonian system (SOHS in short):

    Δ2u(n1)=F(n,u(n)),nZ, (1.1)

    where u(n)RN, Δ2u(n)=Δ(Δu(n)), Δu(n)=u(n+1)u(n), and F(n,x) is continuously differentiable about the first variable. F(n+T,x)=F(n,x),(n,x)Z×RN, with the positive integer T2.

    The study of nonlinear Hamiltonian systems (HS) is one of the important research directions in mathematics, and it is related to many mathematical physics fields. Many scholars are committed to studying the continuous HS and have obtained a lot of results on nonlinear HS in studies of past decades via different critical point theories (see [1,2] and references therein). The critical point theories also have important applications in nonlocal elliptic problems [3].

    Guo and Yu [4,5,6] first studied the discrete SOHS by using variational method and aroused much research enthusiasm in this topic. Specially, in [4] the authors obtained the existence of periodic solutions with the help of the saddle point theorem with F(n,x) satisfying superlinear conditions at the origin and infinity.

    In [7] Tang and Zhang investigated a discrete SOHS under sublinear conditions. Wang, Zhang and Chen [8] introduced a control function h(s) and discussed a class of non-autonomous SOHS via the least action principle.

    Tang and Xiao [9] obtained the existence of a nontrivial homoclinic solution for continuous HS via the mountain pass theorem. Tang and Xue [10] investigated the multiplicity of periodic solutions for a discrete SOHS under superquadratic conditions via the operator theory. Gradually, more and more scholars have devoted themselves to studying the non-autonomous SOHS under quadratic conditions. Some solvable results have been for the non-autonomous SOHS by the minimax methods, such as in the papers[11,12,13]. Among them, [11,13] considered the cases with subquadratic conditions, while in [12], it was treated with superquadratic conditions. However, Xie, Li and Luo in [14] studied a continuous SOHS with the help of the linking theorem.

    Zhao, Yang and Chen considered an asymptotically linear case for the SOHS in [15], that is, F(t,x)=W(t,x)K(t,x), where W satisfies the asymptotically linear condition at infinity, and K satisfies the coupling condition. Chen, Guo and Liu [16] demonstrated continuous HS with asymptotically linear terms, which further extended the previous results under coupling conditions.

    HS with asymptotically linear terms have been extensively studied in the continuous case, e.g., [17,18,19], whereas few results have been obtained in the discrete case. Inspired by the above literature, we will discuss a non-autonomous SOHS with asymptotically linear terms in discrete cases. The difference with [16] is that we construct a new workspace to estimate the minimax level associated with the energy functional.

    We first write the nonlinear term F(n,x) in (1.1) in the form F(n,x)=G(n,x)+H(n,x) with the following conditions:

    (G1): for any (n,x)Z[1,T]×RN, there exist b>0 and g1(n)R satisfying

    G(n,x)b|x|2+g1(n);

    (G2): for any nZ[1,T], there exists K1>0 such that

    (G(n,x),x)2G(n,x),|x|K1;

    (H1): for any (n,x)Z[1,T]×RN, there exist g2(n)R and

    d(0,bT2+b+3T21)

    such that

    H(n,x)d|x|2+g2(n);

    (H2): (H(n,x),x)2H(n,x)+ uniformly for nZ[1,T], when |x|+;

    (W1): for all nZ[1,T], there exists K2>0, such that

    max|x|=aG(n,x)<min|x|=aH(n,x),aK2;

    (W2): for any nZ[1,T], there exists a constant K3>0, such that

    {F(n,x)0for all|x|K3,Tn=1F(n,x)>Tn=1[g2(n)g1(n)]for all|x|>K3.

    Theorem 1.1. If (G1),(G2),(H1),(H2),(W1) and (W2) hold, then system (1.1) has a nontrivial T-periodic solution.

    Define the Hilbert space

    HT={{u(n)}:u(n)RN,u(n+T)=u(n),nZ}

    with its inner product

    u,v=Tn=1[(Δu(n),Δv(n))+(u(n),v(n))],u,vHT,

    and the corresponding norm

    u=(Tn=1[|Δu(n)|2+|u(n)|2])12,uHT.

    The corresponding functional of the equation is

    φ(u)=12Tn=1|Δu(n)|2+Tn=1G(n,u(n))Tn=1H(n,u(n)),uHT, (2.1)

    which is continuously differentiable. So,

    φ(u),v=Tn=1(Δu(n),Δv(n))+Tn=1(G(n,u(n)),v(n))Tn=1(H(n,u(n)),v(n)),u,vHT. (2.2)

    Clearly, the critical point of functional (2.1) is the T-periodic solution of problem (1.1).

    Proposition 2.1. [16] Suppose that H(n,x) satisfies (H2), G(n,x) satisfies (G2), for any nZ[1,T]. Then, there is a sufficiently large M>0, such that

    H(n,x)|x|2M2min|x|=MH(n,x),|x|M, (2.3)
    G(n,x)|x|2M2max|x|=MG(n,x),|x|M. (2.4)

    Recall that (PS) condition in [8], a sequence {up}HT has a convergent sequence when φ(up) is bounded, and φ(up)0,p+. Similarly, we can see (C) condition in [16], if φ(up) is bounded, and φ(up)(1+up)0,p+, then the sequence {up}HT has a convergent sequence.

    Lemma 2.2. If G satisfies (G1) and (G2), H satisfies (H1) and (H2), then the functional φ fulfills the (C) condition.

    Proof. Assume that {up}HT is a (C) sequence, i.e.,

    suppN{|φ(up)|}<+,(1+up)φ(up)0,p+.

    In addition, there exists M1>0 sufficiently large, such that

    |φ(up)|M1,(1+up)φ(up)M1,p+.

    We claim that {up} is bounded. Conversely, we obtain upk+, as k+. We replace {upk} with {up}.

    Let sp=up/up, and obviously, we know that sp=1. There exists sHT, such that sps in HT.

    As

    spssps0,sspsps0,

    we have s=sp=1. Therefore, s0.

    As s0, we set

    L={nZ[1,T]:|s(n)|>0}.

    From the previously described results, we obtain

    |up(n)|=up|sp(n)|+,p+. (2.5)

    When pN,λ>max{K1,M}, set

    M2=TmaxnZ[1,T]max|x|λ{2|G(n,x)|+|G(n,x)||x|,2|H(n,x)|+|H(n,x)||x|},

    by (G2), we have

    Tn=1[2G(n,up(n))(G(n,up(n)),up(n))]{nZ[1,T]:|up(n)|λ}[2G(n,up(n))(G(n,up(n)),up(n))]M2. (2.6)

    We set

    Lc=Z[1,T]L.

    By (H2), we obtain

    Lc[(H(n,up(n)),up(n))2H(n,up(n))]Lc{nZ[1,T]:|up(n)|λ}[(H(n,up(n)),up(n))2H(n,up(n))]+Lc{nZ[1,T]:|up(n)|>λ}[(H(n,up(n)),up(n))2H(n,up(n))]Lc{nZ[1,T]:|up(n)|λ}[(H(n,up(n)),up(n))2H(n,up(n))]M2. (2.7)

    Combining (H2) with (2.5), we obtain

    L[(H(n,up(n)),up(n))2H(n,up(n))]+,p+. (2.8)

    As |φ(up)|M1, one has

    φ(up),upφ(up)upφ(up)(1+up)M1. (2.9)

    Therefore, we have

    2φ(up)φ(up),up3M1. (2.10)

    Combining (2.1) and (2.2), we have

    2φ(up)φ(up),up=Tn=1[(H(n,up(n)),up(n))2H(n,up(n))]+Tn=1[2G(n,up(n))(G(n,up(n)),up(n))]. (2.11)

    To be convenient, we denote

    Tn=1[(H(n,up(n)),up(n))2H(n,up(n))]

    by I1 and

    Tn=1[2G(n,up(n))(G(n,up(n)),up(n))]

    by I2. By (2.6), (2.7) and (2.8), we see that

    I1+I2=L[(H(n,up(n)),up(n))2H(n,up(n))]+Lc[(H(n,up(n)),up(n))2H(n,up(n))]+Tn=1[2G(n,up(n))(G(n,up(n)),up(n))]L[(H(n,up(n)),up(n))2H(n,up(n))]2M2+,p+. (2.12)

    By (2.10)-(2.12), we have

    3M1+,

    which contradicts the boundedness of M1.

    Therefore {up} is bounded in HT, and then we have upu in HT, which demonstrates that φ fulfills (C) condition.

    Set

    ˉu=1TTn=1u(n),˜u(n)=uˉuforalluHT.

    Let

    ˜HT={uHTˉu=0},

    and therefore

    HT=˜HTRN.

    Just as in [7], we have

    ˜u2T216TTn=1|Δu(n)|2. (3.1)

    Next, we will prove Theorem 1.1 in two steps.

    Step 1 Set W=XY as H=VX in [16, Lemma 4], where X=RN and Y=˜HT. As is discussed in [16], (PS) condition can be replaced by (C) condition, and [16, Lemma 4] holds under (C) condition. Now, we will prove that (i) holds in [16, Lemma 4]. By (W1) and Proposition 2.1, let m0RN, and |m0|=1. If zmax{M,K2}, we obtain

    φ(zm0)=Tn=1[G(n,zm0)H(n,zm0)]z2M2Tn=1[max|m|=MG(n,m)min|m|=MH(n,m)]z2TM2maxnZ[1,T][max|m|=MG(n,m)min|m|=MH(n,m)],z+. (3.2)

    There exist r>0 large enough and a constant

    α:=Tn=1[g1(n)g2(n)]1,

    such that

    φ|Br(0)Xα.

    Step 2 We will show that (ii) holds in [16, Lemma 4]. By (G1),(H1), and (3.1), for all u˜HT, we get

    φ(u)=12Tn=1|Δ(n)|2+Tn=1[G(n,u(n))H(n,u(n))]12Tn=1|Δu(n)|2(b+d)Tn=1|u(n)|2+Tn=1[g1(n)g2(n)](12(b+d)(T21)6)Tn=1|Δu(n)|2+Tn=1[g1(n)g2(n)]Tn=1[g1(n)g2(n)]. (3.3)

    Let constant

    β=Tn=1[g1(n)g2(n)],

    and then φ|Yβ. From [16, Lemma 4], we know that φ has a critical value

    cβ.

    Therefore, there is a uHT such that

    Tn=1(Δu(n),Δl(n))(F(n,u(n)),l(n))=0,l(n)HT.

    Finally, we can get our conclusion according to (W2).

    We provide an example to demonstrate the rationality of Theorem 1.1.

    Example 1 Suppose T=2 and set

    G,H:Z[1,T]×RNR

    with

    G(n,x)=cos2πn6(D(n)x,x),

    where

    D(n)=diag((1)2,(1)3,...,(1)1+n).

    Let

    H(n,x)=1+cos2πn5|x|2(11ln(e10+|x|2)),

    where nZ[1,T] and xRN.

    First of all, set

    g1(n)0,b=16.

    Then, we have

    cos2πn6(D(n)x,x)16|x|2,

    and

    (G(n,x),x)=2cos2πn6ni=1(1)1+iX2i2cos2πn6ni=1(1)1+iX2i=2G(n,x).

    Then, G satisfies (G1) and (G2) conditions.

    In the same way, let

    g2(n)0,d=12(0,56).

    Then, we obtain

    1+cos2πn5|x|2(11ln(e10+|x|2))12|x|2,

    and

    (H(n,x),x)2H(n,x)=2(1+cos2πn)|x|25(11ln(e10+|x|2))+2(1+cos2πn)|x|45(1(e10+|x|2)ln2(e10+|x|2))2(1+cos2πn)5|x|2(11ln(e10+|x|2))=2(1+cos2πn)|x|45(e10+|x|2)ln2(e10+|x|2)+.

    Obviously, H(n,x) satisfies (H1) and(H2) conditions. Also,

    max|x|=aG(n,x)16a2<min|x|=aH(n,x)

    for any aR and nZ[1,T], so that (W1) holds. In addition,

    F(n,x)=G(n,x)+H(n,x)16a2+H(n,x)>0.

    Therefore,

    Tn=1F(n,x)>Tn=1[g2(n)g1(n)],

    which means that (W2) holds.

    According to Theorem 1.1, we can get the existence of a nontrivial 2-periodic solution for system (1.1).

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

    Chungen Liu is supported by the National Natural Science Foundation of China (Grant No.11790271, 12171108), Guangdong Basic and Applied basic Research Foundation (Grant No. 2020A1515011019), Innovation and development project of Guangzhou University. Jiabin Zuo is supported by the Guangdong Basic and Applied Basic Research Foundation (2022A1515110907) and the Project funded by China Postdoctoral Science Foundation (2023M730767).

    The authors declare there is no conflict of interest.



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  • This article has been cited by:

    1. Huiting He, Chungen Liu, Jiabin Zuo, Periodic solutions of a class of non-autonomous second-order discrete Hamiltonian systems, 2024, 9, 2473-6988, 3303, 10.3934/math.2024161
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