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Open Mathematics

formerly Central European Journal of Mathematics

Editor-in-Chief: Gianazza, Ugo / Vespri, Vincenzo


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Volume 16, Issue 1

Issues

Volume 13 (2015)

Nontrivial periodic solutions to delay difference equations via Morse theory

Yuhua Long
  • School of Mathematics and Information Science, Guangzhou University, Guangzhou 510006, China
  • Key Laboratory of Mathematics and Interdisciplinary Sciences of Guangdong, Higher Education Institute, Guangzhou University, Guangzhou 510006, China
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  • Other articles by this author:
  • De Gruyter OnlineGoogle Scholar
/ Haiping Shi
  • Modern Business and Management Department, Guangdong Construction Polytechnic, Guangzhou 510440, China
  • School of Mathematics and Statistics, Central South University, Changsha, 410083, China
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/ Xiaoqing Deng
Published Online: 2018-08-08 | DOI: https://doi.org/10.1515/math-2018-0077

Abstract

In this paper some sufficient conditions are obtained to guarantee the existence of nontrivial 4T + 2 periodic solutions of asymptotically linear delay difference equations. The approach used is based on Morse theory.

Keywords: Nontrivial periodic solution; Delay difference equation; Morse theory

MSC 2010: 39A11

1 Introduction

In the present paper we are concerned with the existence of periodic solutions to the system of delay difference equations

Δx(t)=f(x(tT)),(1)

where xRn, Δ x(t) = x(t + 1) − x(t), fC(Rn, Rn) and T is a given positive integer.

In general, (1) may be regarded as a discrete analog of the following differential equation

dxdt=f(x(tr)).(2)

So far, there have been various approaches developed to the existence of the periodic solutions for delay differential equations since the first study [7] in 1962. As to (2), when n = 1, [8] introduced the Yorke-Kaplan’s technique in 1974 to study the existence problem of periodic solutions of

dxdt=f(x(t1)).(3)

They obtained that (3) had 4 periodic solutions under assumptions

  1. fC(R, R) is odd;

  2. xf(x) > 0.

In 2005, by the critical point theory and pseudo-index, Guo and Yu [6] obtained multiplicity results for 4r periodic solutions of (2) when xRn, fC(Rn, R). To our best knowledge, it is the first time that the existence of periodic solutions to systems of delay differential equations is dealt with by using variational method. In addition to that, there are many excellent works dealing with (2) by variational method, for example [13,14,15] and references therein.

It is known that the discrete analogs of differential equations represent the discrete counterpart of corresponding differential equations, and are usually studied in connection with numerical analysis. They occur widely in numerous settings and forms, both in mathematics itself and in its applications to computing, statistics, electrical circuit analysis, biology, dynamical systems, economics and other fields, monograph [1] gives some examples. As to (3), the discrete analog is

Δx(t)=f(x(t1)).(4)

Usually, we try to look for 4 periodic nontrivial solutions which satisfy x(t − 2) = −x(t) of (4) under assumptions (i) and (ii). However, the answer is negative because (4) has no nontrivial 4 periodic solution at all. In [5], authors give an example

Δx(t)=x3(t1)(5)

and prove that (5) has no nontrivial 4 periodic solution. By the example, we find that there may be many differences between solutions of differential equations and solutions of corresponding difference equations. Given another more classical example, solutions of classical logistic model are simple, whereas its discrete analog difference model has chaotic solutions.

Guo [4, 5] who studied delay difference equations by critical point theory [6, 16,17,18,19,20]. Critical point

On the other hand, since [12] studied (1) when n = 1 for the first time, there have been few authors besides Guo [4, 5] who studied delay difference equations by critical point theory [6, 16,17,18,19,20]. Critical point theory is a powerful tool to establish sufficient conditions on the existence of periodic solutions of difference equations. Based on above reasons, our purpose in this paper is to consider the existence of periodic solutions to problem (1). By using Morse theory, we get some existence results on the system (1). To the best of our knowledge, it is the first time that the existence of periodic solutions to systems of delay difference equations is dealt with using Morse theory.

We denote by R, Z the sets of real numbers and integers, respectively. Rn is the real space with dimension n, and [a, b] stands for the discrete interval {a, a + 1, ⋯, b} if ab and a, bZ.

Throughout this paper we assume that the following (f1)-(f3) are satisfied.

  • (f1)

    fC1(Rn, Rn) is odd, i.e., for any xRn, f(−x) = −f(x).

  • (f2)

    There exists a continuously differentiable function F, such that the gradient of F is f, i.e., for any xRn, ∇xF(x) = f(x) and F(0) = 0.

  • (f3)

    There exist real symmetric n × n matrices A and B such that

f(x)=Ax+o(|x|)as|x|,(6)

f(x)=Bx+o(|x|)as|x|0,(7)

that is, (1) is asymptotically linear at both infinity and origin.

Denote G (x) = F(x)− 12 (Ax, x) and G0 (x) = F(x)− 12 (Bx, x) respectively, we need further assumptions, which will be employed to determine the critical groups at infinity and at origin respectively.

(f+)(G(x),x)c1|x|s+1,|G(x)|c2|x|s for xRn with |x| ≥ R, where constants R, c1, c2 > 0 and 0 < s < 1.

(f)(G(x),x)0|(G(x),x)|c1|x|s+1 and G (x)| ≤ c2 |x|s for xRn with |x| ≥ R, where constants R, c1, c2 > 0 and 0 < s < 1.

(f0+) G0 (x) ≥ 0 for xRn with |x| ≤ ϱ, where ϱ > 0 is a constant.

(f0) G0 (x) ≤ 0 for xRn with |x| ≤ ϱ, where ϱ > 0 is a constant.

Remark 1.1

It is easy to see that (f+)and(f) imply (6) in (f3).

Similarly to the argument in [6], for given n × n real symmetric matrices A, B and integer k ∈ [0, T], we set

Nk={the number of negative eigenvalues ofA+2(1)ksin(2k+1)π4T+2I},Nk¯={the number of nonpositive eigenvalues ofA+2(1)ksin(2k+1)π4T+2I},

and

ν(A,B)=k=0T[Nk(A)Nk(B)],ν1(A,B)=k=0T[Nk¯(A)Nk(B)],ν2(A,B)=k=0T[Nk¯(A)Nk¯(B)],

where I is the n × n identity matrix.

Now let us state our main results.

Theorem 1.2

Suppose (f1)-(f3) hold and that f is C1-differentiable near the origin 0Rn. If ν1 (B, B) = 0, then (1) has a nontrivial 4T + 2 periodic solution x which satisfies x(t + 2T + 1) = −x(t) provided one of the following conditions holds:

  1. (f+) and ν (A, B) ≠ 0;

  2. (f) and ν1 (A, B) ≠ 0.

Theorem 1.3

Suppose (f1)-(f3) hold and that f is C1-differentiable near the origin 0Rn. If ν1 (B, B) > 0, then (1) has a nontrivial 4T + 2 periodic solution x which satisfies x(t + 2T + 1) = −x(t) provided one of the following conditions holds:

  1. (f+),(f0+) and ν (B, A) ≠ 0;

  2. (f+),(f0) and ν1 (B, A) ≠ 0;

  3. (f),(f0+) and ν1 (A, B) ≠ 0;

  4. (f),(f0) and ν2 (A, B) ≠ 0.

This paper is divided into four parts. In Section 2, we establish the variational framework associated with (1) and transfer the problem on the existence of periodic solutions of (1) into the existence of critical points of the corresponding functional defined on a suitable Hilbert space. In Section 3, we summarize some basic knowledge on Morse theory which will be used to prove our main results. Also some preliminary results are obtained in this section. The detailed proofs of main results are presented in Section 4.

2 Variational structure

In this section we establish a variational structure which enables us to reduce the existence of 4T + 2 nontrivial periodic solutions of (1) to the existence of critical points of corresponding functional defined on some appropriate function space.

First of all, we recall some notations and preliminary results. Let

S={x={x(t)}tZ|x=(,x(t),,x(1),x(0),x(1),,x(t),),x(t)Rn},

where n is a given positive integer. For some given integer T > 0, E is defined as a subspace of S by

E={x={x(t)}S|x(t+2T+1)=x(t),tZ}

and equipped with the inner product as

<x,y>=t=12T+1(x(t),y(t)),x,yE,

then the induced norm is

x=t=12T+1|x(t)|21/2,xE,

where ( ⋅, ⋅) and |⋅| denote the inner product and norm in Rn. It follows that (E, < ⋅, ⋅ >) is a Hilbert space, which can be identified with R(2T+1)n.

Define a functional J : ER by

J(x)=t=12T+1x(t+T)x(t)t=12T+1F(x(t))xE,(8)

then JC1(E, R) and if xE is a critical point of J, i.e. J′(x) = 0, if and only if

J(x)xl(t)=0

holds for all t ∈ [1, 2T + 1], l ∈ [1, n]. By the same way of [5], we have xE and x is a critical point of J when it is a periodic solution of

x(t+T)+x(tT)f(x(t))=0.(9)

Together with xE, x(tT) = −x(t + T + 1), (9) changes into

Δx(t+T)=f(x(t)).

Since f is odd, we can show that the critical points of J in E are the 4T + 2 periodic solutions of (1). For details, the reader is referred to [12].

We define an operator L: EE as

(Lx)(t)=x(t+T)+x(tT),t=1,2,.(10)

It is easy to check that L is a bounded linear operator on E. For any x, yE, by the periodicity of x, y, we have

<Lx,y>=t=12T+1(x(t+T)+x(tT),y(t))=t=12T+1(x(t+T),y(t))+t=12T+1(x(tT),y(t))=t=12T+1(x(t),y(tT))+t=12T+1(x(t),y(t+T))=t=12T+1(x(t),y(t+T)+y(tT))=<x,Ly>.

It follows that L is self-adjoint.

Define a map

Φ(x)=t=12T+1F(x(t)),xE,(11)

then ΦC1(E, R) and J can be rewritten as

J(x)=12<Lx,x>+Φ(x),xE.(12)

Consider the eigenvalue problem of

x(t+T)+x(tT)=λx(t),x(t+2T+1)=x(t).(13)

By direct computation, we get

λk=2(1)kcosTk2T+1π,k=0,1,,T,

are eigenvalues of (13). It is obvious that 0 ∉ σ (L), where σ (L) is the spectrum of L. Furthermore, when k = T, λT = 2 ⋅ (−1)T is an n-multiple eigenvalue of (13) and the corresponding eigenvector is

ηT=(1,1,1,1,,1,1)T;

when 0 ≤ kT − 1, λk = 2 ⋅ (−1)k cos Tk2T+1π is a 2n-multiple eigenvalue of (13) and the corresponding eigenvectors are

ηk(c)=(cos12T+1tπ,cos32T+1tπ,,cos2k+12T+1tπ),ηk(s)=(sin12T+1tπ,sin32T+1tπ,,sin2k+12T+1tπ).

Then for any xE, x can be expressed as

x(t)=aTηT+k=0T1(akηk(c)+bkηk(s))=k=0T(akcos2k+12T+1tπ+bksin2k+12T+1tπ),(14)

where ak, bk (0 ≤ kT) are constant vectors.

For later use, we need the following lemma.

Lemma 2.1

For any x(j) > 0, y(j) > 0, j ∈ [1, k], kZ,

j=1kx(j)y(j)j=1kxr(j)1rj=1kys(j)1s,

where r > 1, s > 1 and 1r+1s=1.

For any r > 1, by Lemma 2.1, we can define another norm on E as

xr=t=12T+1|x(t)|r1/r,xE.

Obviously, ∥x∥ = ∥x2 and there exist constants c4c3 > 0 such that

c3xrxc4xr,xE.(15)

3 Some preparatory results

In order to obtain critical points of functional J via Morse theory, we will state some basic facts and some preparatory results which will be used in proofs of our main results.

First, let us recall the definition of Palais-Smale condition.

Let X be a real Banach space, IC(X, R). I is a continuously Fréchet differentiable functional defined on X. I is said to satisfy Palais-Smale condition (P.S. for short), if any sequence {x(t)} ⊂ X for which {I (x)} is bounded and I′(x) → 0 (t → ∞) possesses a convergent subsequence in X.

Write κ = {xE|J′(x) = 0}. As in [2] and [9], we will work on the following framework under which the qth critical group of J at infinity Cq(J, ∞) can be described precisely, here qZ.

(A)J(x) = 12 < Lx, x > + Φ (x), where L: EE is a self-adjoint operator such that 0 is isolated in the spectrum of L. The map ΦC1(E, R) satisfies Φ′(x) = o(∥x∥) as ∥x∥ → ∞. Φ and Φ′ map bounded sets into bounded sets. J(κ) is bounded from below and J satisfies (PS)c for c ≪ 0.

Let (A) hold. Set V = Ker(L) and W = V. One can split W as W+W such that L|W+ is positive definite and L|W is negative definite. Denote by μ = dim W, ν = dim V, the Morse index and the nullity of J at infinity, respectively.

In order to compute the critical group of J at infinity we need the following angle condition at infinity which was built by Bratsch and Li [2]. Here the given angle condition have been made some improvement on [2]. We refer to [3] and [11].

Proposition 3.1

Let J satisfy (A). Then:

  1. Cq(J, ∞) ≅ δq,μZ provided J satisfies the angle condition at infinity:

    (AC+) There exist M > 0, α ∈ (0,1) such that < J′(x), v > ≥ 0 for any

    x=v+wE=VW,withxM,wαx.

  2. Cq(J, ∞) ≅ δq,μ+νZ provided J satisfies the angle condition at infinity:

    (AC) There exist M > 0, α ∈ (0,1) such that < J′(x), v > ≤ 0 for any

    x=v+wE=VW,withxM,wαx.

When Hilbert space E=E0+E0. One can split E0asW0W00 such that L|W00 is zero and L|W0 is negative definite. Denote by μ0=dimW0,ν0=dimW00, the Morse index and the nullity of J at 0 respectively. Su [10] gives the following proposition which can be used to compute the critical group of J at origin.

Proposition 3.2

Let JC2 (E, R) satisfy P.S. and k = dimE0. If J has a local linking at 0 corresponding to the spilt E=E0+E0, i.e. there exists ρ > 0 small enough such that

J(x)J(0),xE;J(x)>J(0),xE+,0<xρ.

Then

Cq(J,0)δq,kZ,k=μ0ork=μ0+ν0.

Recall that, in our setting,

J(x)=12<Lx,x>+Φ(x),xE.

Denote

G(x)=F(x)12(Ax,x)andΦ(x)=t=12T+1G(x(t)),G0(x)=F(x)12(Bx,x)andΦ0(x)=t=12T+1G0(x(t)).

Let LA, LB be bounded linear operators from E to E defined by the following forms

(LAx)(t)=x(t+T)+x(tT)Ax(t),(16)

(LBx)(t)=x(t+T)+x(tT)Bx(t),(17)

then J can be reformulated by

J(x)=12<LAx,x>+Φ(x),(18)

J(x)=12<LBx,x>+Φ0(x).(19)

For an n × n symmetric matrix DRn × n, we define linear operator D : EE by extending the bilinear forms

<Dx,y>=t=12T+1(Dx(t),y(t)),x,yE.

Clearly, D is a bounded linear self-adjoint operator. Moreover, we can easily verify that D is compact on E because E is a finite dimensional Hilbert space. Now, we can draw a conclusion that LA = LA and LB = LB are bounded linear self-adjoint operators. Furthermore, ϕ = ϕA and ϕ0 = ϕB are compact, where ϕ* = Φ and * = 0, ∞.

Lemma 3.3

Assume that f satisfies (f1)-(f3). Then Φ (0) = 0 and

limx+ϕ(x)x=0.(20)

Proof

Φ (0) = 0 follows by the definition of Φ and (f1), (f2). By (f3), (i), for any ε > 0, there exists a constant C > 0 such that

|f(x)Ax|<ε|x|+C.(21)

Note that

<ϕ(x),h>=<(ϕA)(x),h>=t=12T+1f(x(t))Ax(t),h(t),x,hE.

By Lemma 2.1, we get

|<ϕ(x),h>|t=12T+1f(x(t))Ax(t)h(t)t=12T+1ε|x(t)||h(t)|+C|h(t)|εxh+2T+1Ch,

this yields

ϕ(x)εx+2T+1C,

so

limx+supϕ(x)xε.

By the arbitrariness of ε, we show that limx+ϕ(x)x=0.

Lemma 3.4

Let D be the self-adjoint operator defined by an n × n symmetric matrix D and m+(LD), m0(LD) and m(LD) denote the dimension of the subspaces of E where LD is positive definite, zero and negative definite respectively. Then

m(LD)=k=0TNk(D),m0(LD)=k=0T[Nk¯(D)Nk(D)],m+(LD)=(2T+1)nm(LD)m0(LD).

Proof

Consider the operator LD = LD, which is defined by

(LD)x(t)=x(t+T)+x(tT)Dx(t),xE.

Together with (14) and x(tT) = –x(tT + 2T + 1) = –x(t + T + 1), we get

LDx(t)=x(t+T)+x(tT)Dx(t)=x(t+T)x(t+T+1)Dx(t)=k=0T[akcos2k+12T+1(t+T)π+bksin2k+12T+1(t+T)πakcos2k+12T+1(t+T+1)πbksin2k+12T+1(t+T+1)πDakcos2k+12T+1tπDbksin2k+12T+1tπ]=k=0T[(2(1)ksin(2k+1)π4T+2ID)akcos2k+12T+1tπ+(2(1)ksin(2k+1)π4T+2ID)aksin2k+12T+1tπ].

Consider the eigenvalue problem of operator LD. Let

LDx(t)=λx(t),

where λ is a constant. Then for any k ∈ [0, T], we have

[2(1)ksin(2k+1)π4T+2ID]ak=λak

and

[2(1)ksin(2k+1)π4T+2ID]bk=λbk.

This implies that λ is an eigenvalue of operator LD if and only if it is an eigenvalue of 2 ⋅ (–1)k ⋅sin (2k+1)π4T+2ID for some k ∈ [0, T]. It follows that the conclusions hold. □

4 Proofs of main results

With above preparations, we shall prove our main results in this section. In order to give proofs of our theorems, we need following lemmas.

Lemma 4.1

Assume that f satisfies (f1)-(f3) and (f±). Then J(x) satisfies P.S. condition.

Proof

Denote the smallest eigenvalue of LA is λmin. Since LA = LA is compact perturbation of L and 0 ∉ σ(L), we find 0 ∉ σ(LA), that is, λmin > 0. Then for any xE, we have

|<LAx,x>|λminx.(22)

Let {x(k)} ⊂ E be a PS sequence in E, i.e., there is a constant M1 > 0 such that |J(x(k))| ≤ M1 holds for any kN and J′(x(k)) → 0 as k → ∞. Since E is a finite dimensional Hilbert space, here we only need to prove {x(k)} is bounded in E.

Since J′(x(k)) → 0 as k → ∞, without generality, we can let |J′(x(k))| ≤ 1 when k is large enough. Write x(k) = u(k) + v(k), where u(k)Y, v(k)Z. Here Y, Z are subspaces of E where LA is positive and negative definite respectively. For sufficiently large k, making use of (21) and (22), we have

x(k)=u(k)v(k)|J(x(k)),u(k)v(k)|=|<LAx(k)ϕ(x(k)),u(k)v(k)>||<LAx(k),u(k)v(k)>|t=12T+1|(fA)x(k)(t),u(k)(t)v(k)(t)|λminx(k)u(k)v(k)t=12T+1|ε|x(k)(t)|+C,u(k)(t)v(k)(t)|λminx(k)2εx(k)t=12T+1|u(k)(t)v(k)(t)|Ct=12T+1|u(k)(t)v(k)(t)|λminx(k)22T+1εx(k)22T+1Cx(k).(23)

For λmin > 0, we can choose a sufficiently small ε > 0 such that λmin > 2T+1ε. Then from (23) we get {x(k)} is bounded. □

In order to prove our main results by Proposition 3.1, we are in the position to give the verification of these angle conditions at infinity.

Lemma 4.2

Let f satisfy (f1)-(f3) and the functional J(x) be defined by (12), we have the following conclusion: if (f+) (or (f)) holds, then J satisfies the angle condition (SAC)(or(SAC+)) at infinity; i.e., there exist M > 0, α ∈ (0, 1) such that

<J(x),vv><0,(or<J(x),vv>>0)

for any x = v + wE = VW with |x| ≥ M, |w| ≤ α |x|, where V = Ker(LA) and W = V.

Proof

Set

Ω(M,ε)={x=v+wE=VW|xM,wεx},(24)

where M > 0 and ε ∈ (0, 1) will be chosen below. For any xΩ(M, ε), we have

v1ε2x,wε1ε2v.(25)

We only prove the case that the functional J(x) satisfies the angle condition (SAC) under condition (f+), the other case is similar and here the proof is omitted.

t=12T+1(G(x(t)),v(t))=t=12T+1(G(x(t)),x(t)w(t))=t=12T+1(G(x(t)),x(t))t=12T+1(G(x(t)),w(t))t=12T+1c1|x|1+st=12T+1|G(x(t)||w(t)|c1x1+s1+sc2t=12T+1|x(t)|s|w(t)|c1x1+s1+sc2(2T+1)1s2xswc1x1+s1+sc2(2T+1)1s2ε1ε2vxs.

From (15), for any xE, there exist constants 0 < r1r2 such that

r1x1+s1+sx1+sr2x1+s1+s,

then

t=12T+1(G(x(t)),v(t))c1r2x1+sc2(2T+1)1s2ε1ε2vxs.

Let |v| ≤ 1, we have

t=12T+1(G(x(t)),v(t))c1r2x1+svc2(2T+1)1s2ε1ε2vxs,

it follows

t=12T+1G(x(t)),v(t)vc1r2xc2(2T+1)1s2ε1ε2xs.

Denote β=c2(2T+1)1s2εr2c11ε2,thent=12T+1G(x(t)),v(t)v>0 is true when ∥v∥ ≤ 1 and ∥x∥ > β hold. From (25), we get xv1ε211ε2, then we can choose suitable c1, c2 and r2 such that ε=c1c2(2T+1)1s2r2(0,1) and M[c2r2ε(2T+1)1s2c11ε2,11ε2] it is clear that M > 0. Now fixing M > 0, 0 < ε < 1, we get

t=12T+1G(x(t)),v(t)v>0(26)

for any x = v + wΩ(M, ε) with ∥x∥ ≥ M and ∥w∥ ≤ εx∥. Since for any xE,

J(x)=12<Lx,x>t=12T+1F(x(t))=12<(L+A)x,x>t=12T+1G(x(t)),

we have

<J(x),vv>=t=12T+1G(x(t)),v(t)v.

By the above argument we get easily that J satisfies the angle condition (SAC) at infinity if we take α = ε ∈ (0, 1). □

Denote W00=Ker(LB),W0=(W00),thenW0=W0+W0,andW0± is an invariant subspace according to operator LB, where LB is positive definite and negative definite, respectively. Therefore, E can be expressed as

E=W00W0+W0.(27)

What’s more, there exists a constant δ > 0 such that

<LBx,x>≥δx2,xW0+,<LBx,x>≤δx2,xW0,<LBx,x>=0,xW00.(28)

To compute the critical group of J at origin, we are in position to prove that J has a local linking at origin.

Lemma 4.3

Let f satisfy (f1)-(f3) and (f0±), then J has a local linking at 0 corresponding to the spilt E = W0+E0,whereE0=W0W00 (according to condition (f0+))orE0=W0 (according to condition (f0)).

Proof

By (27), given xE, we can write x = u + v + w, where uW0+,vW0andwW00.

First, we prove it under the condition (f0+).

Making use of (f3) (ii) and (28), there exists a constant ρ ∈ (0, ϱ] such that

|G0(x)|δ3|x|2,|x|ρ.(29)

On one side, by (19), (28) and (29), we have

J(x)δ2x2δ3x2>0.(30)

On the other side, since |x| ≤ ρϱ, when xW0W00 and ∥x∥ ≤ ρ, write x = v + w where vW0andwW00 we get

J(x)12δv2t=12T+1G0(x(t))0.(31)

Together with (30), (31) and J(0) = 0, we complete the proof that J has a local linking at 0 under the condition (f0+).

Following, we consider the second case with the condition (f0+). Similarly, we have

J(x)δ2x2+δ3x20,asxW0,xρ.(32)

and

J(x)12δu2t=12T+1G0(x(t)),asxW0+W00,0<xρ.(33)

If u ≠ 0, then (33) means J(x) > 0. If u = 0, i.e. xW00 ∖ {0} and ∥x∥ ≤ ρ, then

J(x)=t=12T+1G0(x(t))0.(34)

In fact we can prove that J(x) > 0. Since if J(x) = 0 in (34) is true, (1) has infinite solutions. That is, J has a local linking at 0 under the condition (f0+). This completes the proof. □

Proof of Theorem 1.2

We will only present the proof for case (i) and the proof for case (ii) is similar.

By Lemma 3.3, we know that Φ is C1, Φ(0) = 0 and

Φ(x)=ϕ(x)=o(x),asx,xE.

Combining with Lemma 4.1, we have that J satisfies (A). It follows by Lemma 3.4, Proposition 3.1 and Lemma 4.2 that

Cq(J,)δq,μZ,(35)

where μ = m(LA).

Since the injection of E into E, with its norm ∥⋅∥, is continuous and f is C1 differentiable near 0Rn, we know that J is C2 differentiable near the origin 0 ∈ E. Further, we have

J(0)=LB.

Since ν1(B, B) = 0 implies that for every k ∈ [0, T], k(B)–Nk(B) = 0, we see that 0 in E is a non-degenerate critical point of J. Thus, for every k ∈ [0, T], we have

Cq(J,0)δq,μ0Z,(36)

where μ0 = m(LB). By the condition ν(A, B) ≠ 0, we see that

m(LA)m(LB).

Thus μμ0. It follows from (35) and (36) that J has different critical groups at infinity and at origin respectively, which implies that J has at least one nontrivial critical point x ≠ 0, i.e., (1) has a nontrivial 4T + 2 periodic solution x(t) which satisfies x(t + 2T + 1) = –x(t). □

Proof of Theorem 1.3

Similarly to the proof of Theorem 1.2, we can get (35). By Proposition 3.2, Lemmas 4.1 and 4.1, we have

Cq(J,0)δq,μ0Z.

Note that ν(A, B) ≠ 0 implies μμ0 for every k ∈ [0, T], we get

Cq(J,0)Cq(J,),

which implies that J has at least one nontrivial critical point x ≠ 0. The proof is complete. □

Acknowledgement

The authors would like to thank the referees and the editors for their careful reading and making some valuable comments and suggestions on the manuscript. This work was carried out while visiting Central South University. The author Haiping Shi wishes to thank Professor Xianhua Tang for his invitation.

References

  • [1]

    Agarwal R.P., Difference Equations and Inequalities: Theory, Methods and Applications, Marcel Dekker, New York, 1992. Google Scholar

  • [2]

    Bartsch T., Li S.J., Critical point theory for asyptotically quadratic functionals and applications to problem with resonance, Nonlinear Anal., 1997, 28, 419-441. CrossrefGoogle Scholar

  • [3]

    Chang K.C., Morse theory on Banach space and its applications to partial differential equations, Chin. Ann. Math. Ser. B, 1983, 4, 381-399. Google Scholar

  • [4]

    Guo L.F., Guo Z.M., Periodic solutions to first order superlinear delay difference equation, J. Guangzhou University, 2014, 13, 19-23. Google Scholar

  • [5]

    Guo Z.M., Guo L.F., The existence of periodic solutions to higher-order dimensional sublinear delay difference equation, J. Guangzhou University, 2014, 13, 7-12. Google Scholar

  • [6]

    Guo Z.M., Yu J.S., Multiplicity results for periodic solutions to delay differential equations via critical point theory, J. Differential Equations, 2005, 218, 15-35. CrossrefGoogle Scholar

  • [7]

    Jones G.S., The existence of periodic solutions of f′(x) = -af(x-1)[1+f(x)], J. Math. Anal. Appl., 1962, 5, 435-450. Web of ScienceCrossrefGoogle Scholar

  • [8]

    Kaplan J.L., Yorke J.A., Ordinary differential equations which yield periodic solution of delay equations, J. Math. Anal. Appl., 1974, 48, 317-324. CrossrefGoogle Scholar

  • [9]

    Su J.B., Nontrivial periodic solutions for the asymptotically linear Hamiltonian systems with resonance at infinity, J. Differential Equations, 1998, 145, 252-273. CrossrefGoogle Scholar

  • [10]

    Su J.B., Multiplicity results for asymptotically linear elliptic problems at resonance, J. Math. Anal. Appl., 2003, 278, 397-408. CrossrefGoogle Scholar

  • [11]

    Wang Z.Q., Multiple solutions for indefinite functionals and applications to asymptotically linear problems, Acta Math. Sinica, 1989, 5, 101-113. CrossrefGoogle Scholar

  • [12]

    Xing Q.P., Wang Q.R., Guo Z.M., Existence of periodic solutions to nonlinear diffference equations with delay, Acta Anal. Func. Appl., 2012, 14, 61-70. Google Scholar

  • [13]

    Yu J.S., Xiao H.F., Multiple periodic solutions with minimal period 4 of the delay differential equation (t) = –f(t, x(t–1)), J. Differential Equations, 2013, 254, 2158-2172. CrossrefWeb of ScienceGoogle Scholar

  • [14]

    Yu J.S., A note on periodic solutions of the the delay differential equation (t) = –f(t, x(t–1)), Proc. Amer. Math. Soc., 2013, 14, 1281-1288. Google Scholar

  • [15]

    Zhang X.S., Meng Q., Nontrivial periodic solutions for delay differential systems via Morse theory, Nonlinear Anal., 2011, 74, 1960-1968. Web of ScienceCrossrefGoogle Scholar

  • [16]

    Zhou Z., Ma D.F., Multiplicity results of breathers for the discrete nonlinear Schrödinger equations with unbounded potentials, Sci. China Math., 2015, 58(4), 781-790. CrossrefGoogle Scholar

  • [17]

    Zhou Z., Su M.T., Boundary value problems for 2n-order ϕc-Laplacian difference equations containing both advance and retardation, Appl. Math. Lett., 2015, 41, 7-11. CrossrefWeb of ScienceGoogle Scholar

  • [18]

    Zhou Z., Yu J.S., Homoclinic solutions in periodic nonlinear difference equations with superlinear nonlinearity, Acta Math. Sin. (Engl. Ser.), 2013, 29(9), 1809-1822. CrossrefGoogle Scholar

  • [19]

    Zhou Z., Yu J.S., On the existence of homoclinic solutions of a class of discrete nonlinear periodic systems, J. Differential Equations, 2010, 249(5), 1199-1212. Web of ScienceCrossrefGoogle Scholar

  • [20]

    Zhou Z., Yu J.S., Chen Y.M., Homoclinic solutions in periodic difference equations with saturable nonlinearity, Sci. China Math., 2011, 54(1), 83-93. CrossrefWeb of ScienceGoogle Scholar

About the article

Received: 2018-04-03

Accepted: 2018-06-12

Published Online: 2018-08-08


Citation Information: Open Mathematics, Volume 16, Issue 1, Pages 885–896, ISSN (Online) 2391-5455, DOI: https://doi.org/10.1515/math-2018-0077.

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© 2018 Long et al, published by De Gruyter. This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License. BY-NC-ND 4.0

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