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R E S E A R C H

Open Access

Multiple periodic solutions for the

second-order nonlinear difference equations

Sheng Ma

1

, Zhihua Hu

1

and Qin Jiang

1*

*Correspondence: jiangqin999@126.com 1College of Mathematics and

Physics, Huanggang Normal University, Hubei, People’s Republic of China

Abstract

Multiple periodic solutions for the equation

(

pn(

xn–1)δ

)

+qnxδn=∇F(n,xn), n∈Z,

are obtained via variational method and saddle-point theorem of Brezis and Nirenberg. Our main results extend some earlier results. An example is given.

MSC: 58E50; 39A11; 39A10

Keywords: Multiple solutions; Difference equation; PS condition; Second-order; Saddle-point theorem

1 Introduction

LetZ,N. AndRbe the sets of all integers, all positive integers, and all real numbers re-spectively. SetZ[a,b] ={a,a+ 1, . . . ,b}forab,a,b∈Z.

We consider the existence of multiple solutions for the following difference equation:

pn(xn–1)δ

+qnxδn=∇F(n,xn), n∈Z. (1)

Herexn=xn+1–xn,2xn=(xn), the odd integerδ> 0 is the ratio, real sequences

{pn},{qn}and the functionF(n,x) = x

0∇F(n,s)dssatisfy

pn=pn+T> 0, qn=qn+T, F(n+T,x) =F(n,x), n∈Z,

for a fixedT∈Z.

Difference equations are widely found in mathematics itself and in its applications to combinatorial analysis, quantum physics, chemical reactions, and so on. Many authors were interested in difference equations and obtained many significant conclusions; see, for instance, the papers [1–3, 5–20]. Various methods have been used to deal with the existence of solutions to discrete problems, we refer to the fixed point theorems in cones in [12] and the variational method in [2,3,5–11,13,14,18–20]. In 2003, in [10,11] Yu and Guo made a new variational structure to handle discrete equations and obtained good conclusions on the solvability condition of a periodic solution. This new variational struc-ture represents an important advance as it allows us to prove multiplicity results as well.

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When δ = 1, equation (1) has been considered in [17] and [19]. When δ = 1 and

F(n,x) = 0, equation (1) has been also studied. For example, in [1] and [8], the authors were interested in the results on disconjugacy, disfocality, oscillation, and the asymptotic behavior. In [20] the authors were interested in the results on the existence of positive so-lutions. However, to the best of our knowledge, whenδ= 1 and∇F(n,x)= 0, besides [6] and [18], in the literature there are no results on the solvability condition of periodic solu-tions for equation (1). By employing the mountain pass lemma, in [6] the authors proved that there are at least two nontrivial periodic solutions of equation (1) under the following conditions:

(a) qn< 0,∀n∈Z[1,T].

(b) For eachn∈Z,limx→0∇F|x(|,x)= 0.

(c) There exist constantsa1> 0,a2> 0, andβ>δ+ 1such that

F(n,x)≤–a1|x|β+a2, ∀x∈R.

To get the critical points, condition (c) is essential, especially,β>δ+ 1. Later, by virtue of the saddle-point theorem, in [18] the authors obtained the periodic solution of equation (1) under condition (a) and the following assumptions:

(d) There are constantsR1> 0andα∈(1, 2)such that

α

2(δ+ 1)F(n,x)≤xF(n,x) < 0 forn∈Zand|x| ≥R1.

(e) There are constantsa3> 0,a4> 0, andγ ∈(1,α]such that

F(n,x)≤–a3|x| γ

2(δ+1)+a4,x∈R.

From condition (e) we haveβ=γ2(δ+ 1) <δ+ 1.

Hence it is natural for us to consider the caseβ=δ+ 1. In the present papere, the mo-tivation comes from the recent papers [6,7,14,18]. By virtue of the minimax methods with variational techniques, the solvability conditions on multiple periodic solutions are

proved for difference equation whenβ=δ+ 1. In particular, our results complement and

generalize the results in [6] and [18].

2 Preliminaries

To obtain multiple periodic solutions via variational techniques, we state the correspond-ing variational structure for equation (1). LetSbe the sequence

S={un}= (. . . ,un, . . . ,u–1,u0,u1, . . . ,un, . . .) ={un}+–∞∞.

Define

au+bv={aun+bvn}, ∀u,vS,a,b∈R.

This yields thatSis a vector space. For any fixedT∈N, letETbe the subspace ofSdefined

as

ET=

u={un} ∈S|un+T=un,n∈Z

(3)

Define the inner product·,·ETand norm · ETinETas follows:

u,vET=

T

i=1

uivi and uET=u=

T

j=1

u2j

1 2

u,vET.

Obviously, the spaceETis finite dimensional. Set

uδ+1= T

j=1

uδ+1j

1 δ+1

.

Sinceδ+ 1≥2, by the Hölder inequality we have

uTδ–1δ+1uδ+1T12uδ+1, uET.

On the other hand, we have

T

j=1

uδ+1j

2 δ+1

T

j=1

u2j, uET.

Obviously,

T–12uuδ+1u (2)

for alluET. Let

ϕ(x) = – 1 δ+ 1

T

n=1

pn(xn–1)δ+1+

1 δ+ 1

T

n=1

qnxδ+1nT

n=1

F(n,xn), ∀xET.

ThenϕC1(E

T,R), and we have the partial derivative

∂ϕ ∂xn

=pn(xn–1)δ

+qnxδn–∇F(n,xn), n∈Z[1,T],

viax0=xT,x1=xT+1. ThusxETsatisfiesϕ(x) = 0 if and only ifxsatisfies equation (1)

for anyn∈Z[1,T]. To seek theT-periodic solutions for equation (1) is to find the critical points of functionalϕsincexn=xT+nand∇F(n+T,x) =∇F(n,x).

Set theT×Tmatrix

P=

⎡ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣

2 –1 0 · · · 0 –1 –1 2 –1 · · · 0 0

0 –1 2 · · · 0 0

· · · ·

0 0 0 · · · 2 –1 –1 0 0 · · · –1 2

⎤ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦

.

From the matrix theory we know that

λk= 2

1 –cos2

T

(4)

are the eigenvalues ofPandλ0= 0,λ1> 0,λ2> 0, . . . ,λT–1> 0. Thus we have

λmin=min{λ1,λ2, . . . ,λT–1}=λ1= 2

1 –cos2π

T

.

Let

W=kerP={xET|Px= 0}.

Then

W=xET|x={c},c∈R

.

Set V =W⊥. Clearly, ET =VW. For convenience, we identify xET with x=

(x1,x2, . . . ,xT)T.

3 Main results and proofs

Set

pmin= min

n∈Z[1,T]pn> 0, qmin=n∈minZ[1,T]qn, qmax=n∈maxZ[1,T]qn.

We study equation (1) under the following conditions:

(F1) qmax–qmin<pminλ

δ+1 2 1 Tδ+11 .

(F2) There exist constantsρ0> 0and

a1∈

qmax–qmin

pminλ

δ+1 2 1

1 δ+1

, 1

T

such that

qmax–pminλ

δ+1 2 1 aδ+11

δ+ 1 |x|

δ+1F(n,x) qmin δ+ 1|x|

δ+1

for alln∈Zand|x| ≤ρ0.

(F3) lim sup|x|→∞F|(n,x)

x|δ+1< –δ+1A , whereA=maxn∈Z[1,T][2δ+1(pn+pn+1) –qn].

(F4) There are constantsρ1> 0anda2∈(0,T1)such that

pminλ

δ+1 2 1 aδ+12

δ+ 1 |x|

δ+1F(n,x)0

for alln∈Zand|x| ≤ρ1.

(F5) lim sup|x|→∞F|(n,x)

x|δ+1< –δ+1B , whereB=maxn∈Z[1,T][2δ+1(pn+pn+1)].

Now we state our main results.

Theorem 3.1 Under hypotheses(F1), (F2),and(F3),equation(1)has at least two nontriv-ial T -periodic solutions.

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Corollary 3.2 Under hypotheses(F4)and(F5),equation(1)has at least two nontrivial T -periodic solutions.

Remark3.3 Theorem3.1generalizes Theorem 3.2 in [6]. On the one hand, the sequence

{qn}can be sign-changing. However,{qn}is negative in Theorem 3.2 of [6]. On the other

hand, conditions (F2) and (F3) in our Theorem 3.1are weaker than the corresponding

conditions in Theorem 3.2. There are functionsFsatisfying Theorem3.1but not fulfilling Theorem 3.2 in [6] and Theorem 1.3 in [18]. For example, set

sponding condition of Theorem 3.2 of [6]. A simple computation yields

lim

SoFsatisfies (F2). Further, we have

lim

|x|→∞sup

F(n,x)

|x|δ+1 = –∞,

which implies that such a functionFsatisfies condition (F3) of Theorem3.1but does not satisfy the corresponding condition of Theorem 3.2 in [6] and the corresponding condition of Theorem 1.3 in [18]. Moreover, our conclusion complements the results of Theorem 3.2 in [6] and Theorem 1.3 in [18].

The proof of Theorem3.1uses the following saddle-point theorem of Brezis and

(6)

Lemma 3.4([4]) Let X be a Banach space with X=X1+X2,wheredimX2<∞,and let

ϕbe a C1function on X withϕ(0) = 0satisfying the PS condition.Suppose that,for some

δ0> 0,

(I1) ϕ(v)≥0,forvX1withvδ0,and

(I2) ϕ(v)≤0,forvX2withvδ0.

Ifϕis bounded from below andinfXϕ< 0,thenϕhas at least two nonzero critical points.

Proof of Theorem3.1 Set

W=X1, V=X2.

First, we claim thatϕsatisfies the PS condition. Now let{x(k)}be a sequence forϕsuch that{ϕ(x(k))}is bounded andϕ(x(k))→0 ask→ ∞. Then we need to verify that there is a convergent subsequence of{x(k)}. SinceE

Tis finite dimensional, we only need to prove

that{x(k)}is bounded.

dimensional spaceET, such a bounded consequence{x(k)}has a convergent subsequence.

Henceϕsatisfies the PS condition.

(7)

For allxET, by the Hölder inequality we have

Then a simple computation yields

T

Thus condition (I2) of Lemma3.4is verified. Moreover, we have

inf ET

ϕ(x)≤0. (8)

Next, we consider two cases.

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This means that allxVwithxρare solutions of equation (1). Hence the proof of

Theorem3.1is finished.

The proof of Corollary3.2is omitted since it is similar to that of Theorem3.1.

Acknowledgements

The authors sincerely thank the reviewers for their valuable suggestions and useful comments that have led to the present improved version.

Funding

The work is supported by the Science Foundation of Education Department for Hubei Provincial, China (No. D20172905).

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

SM chose the problem and drafted the manuscript with ZHH. QJ conceived the solution method. All authors read and approved the final manuscript.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 14 November 2017 Accepted: 17 July 2018

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