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R E S E A R C H

Open Access

Periodic solutions for a class of second

order delay differential systems

Qiong Meng

*

and Juntang Ding

*Correspondence:

[email protected] School of Mathematical Science, Shanxi University, Taiyuan, Shanxi 030006, P.R. China

Abstract

Consider the periodic boundary value problem

¨

u(t) +ru(t

τ

) +∇F(t,u(t

τ

)) = 0, a.e.t∈[0, 2

τ

],

u(0) –u(2

τ

) =u˙(0) –u˙(2

τ

) = 0,

where

τ

> 0 is a given constant,rRis a parameter. Periodic solutions are obtained by using linking theorems.

MSC: 34K13; 34K18; 58E50

Keywords: periodic boundary value problem; delay differential systems; linking theorems

1 Introduction

Consider the periodic boundary value problem

¨

u(t) +ru(tτ) +∇F(t,u(tτ)) = , a.e.t∈[, τ],

u() –u(τ) =u˙() –u˙(τ) = , (.) whereτ >  is a given constant, rRis a parameter.F: [, τRN Rsatisfies the

following assumptions:

(A)F(t,x) is measurable with respect tot, for allxRN, continuously differentiable inx, for a.e.t∈[, τ], and there existaC(R+; R+) andbL([, τ]; R+) such that

F(t,x),∇F(t,x)≤a|x|b(t)

for allxRNand a.e.t[, τ].

Variational methods are very powerful techniques in nonlinear analysis and are exten-sively used in many disciplines of pure and applied mathematics, including ordinary and partial differential equations, mathematical physics, and geometrical analysis. The exis-tence and multiplicity of solutions for Hamilton systems and Schrödinger equations have been studied extensively via critical point theory; see [–].

In the past several years, some results on the existence of periodic solutions for the func-tional differential equation by the critical point theory have been obtained (see [–]). In

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[], the authors obtained the multiplicity results for periodic solutions to (.) by using critical point theory. Our proof method in this paper is different from the literature [].

Motivated by the above observation, in this paper, we study the existence of periodic solutions to the system (.). The following theorems are the main results of our paper.

(H) There exists a constantR> such that

(i) F(t,x)≥,∀|x| ≤R,t∈[, τ]; or

(ii) F(t,x)≤,∀|x| ≤R,t∈[, τ].

(H) lim|x|→∞infF|(xt|,x) > uniformly fort∈[, τ].

(H) lim|x|→|∇F|x(t|,x)|= uniformly fort∈[, τ].

(H) There existα> anda> such that

F(t,x)≤a|x|α+ , (t,x)[, τ]×RN.

(H) There existμ> , <β< ,R> , and a functionb(t)∈L([, τ]; R+)such that

μF(t,x)≤∇F(t,x),x+b(t)|x|β, ∀|x| ≥R,t∈[, τ].

(H) There existβ>α≥andb> ,R> such that

F(t,x),x– F(t,x)≥b|x|β, ∀|x| ≥R,t[, τ].

Theorem . Assume that(H)-(H)hold,ifis an eigenvalue of L(L is defined in Sec-tion),BVP(.)has at least one nontrivial solution.

Theorem . Assume that(H)-(H)and(H)hold,ifis an eigenvalue of L(L is defined in Section),BVP(.)has at least one nontrivial solution.

Remark . The condition (H) and the condition (H) are appeared, respectively, in [] and [].

2 Preliminaries

In order to seek τ-periodic orbits of (.), let us transform (.) to

¨

u(t) +u(tπ) +λF(λt,u(tπ)) = , a.e.t[, π],

u() –u(π) =u˙() –u˙(π) = , (.) by making the change of variabletπτt=λ–t, which implies that a π-periodic solution of (.) corresponds to a τ-periodic solution of (.). Hence we will only look for the π -periodic solutions of (.) in the sequel.

LetL(S, RN) be the space of square integrable π-periodic vector-valued functions

with dimension N, andC∞(S, RN) be the space of π-periodicCvector-valued

func-tions with dimension N. For anyuC∞(S, RN), it has the following Fourier expansion in the sense that it is convergent in the spaceL(S, RN):

u(t) =√a π +

π

+∞

j=

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where a,aj,bjRN. Let H(S, RN) be the closure ofC∞(S, RN) with respect to the

Hilbert norm

u=

|a|+

+∞

j=

 +j|aj|+|bj| /

.

More specifically,H(S, RN) ={uL(S, RN) :u< +∞}with the inner product

u,v=

π

u(t),v(t)+u˙(t),v˙(t)dt

for anyu,vH(S, RN), where (·,·) denotes the usual inner product in RN. The norm on

H(S, RN) is defined by

u=

π

u(t)+u˙(t)dt

/

. (.)

It is well known thatH(S, RN) is compactly embedded inC(S, RN) (see Proposition .

of []). Define two operatorsLandLfromH(S, RN) intoH∗(S, RN) as follows: for any

uH(S, RN), which are given by

(Lu)(v) =

π

˙

u(t+π),v˙(t)dt,

(Lu)(v) = –

π

u(t),v(t)dt,

for allvH∗(S, RN), whereu˙(t) andH(S, RN) denote the weak derivative ofuand the

dual space ofH(S, RN), respectively. By the Riesz representation theorem, we can

iden-tifyH∗(S, RN) withH(S, RN). Thus,L

iucan also be viewed as an element belonging to

H(S, RN) such thatL

iu,v= (Liu)(v) for allu,vH(S, RN), wherei=  or . It is easy

to check thatLandLare bounded linear operators onH(S, RN). Note thatH(S, RN)

is compactly embedded inC(S, RN), thusL

is compact onH(S, RN).

Lemma .[] The operator L:=L+L,that is,

Lu,v= (Lu)(v) =

π

˙

u(t+π),v˙(t)dt π

u(t),v(t)dt

is self-adjoint on H(S, RN).The operators L

and Lare also self-adjoint on H(S, RN).

Lemma .[] The essential spectrum of Lon H(S, RN)is just{–, }.

In view of the above facts,  is not in the essential spectrum ofLas it is a compact perturbation of the self-adjoint operatorL. This implies that  is at most an eigenvalue

of finite multiplicity ofL.

Remark . H(S, RN) has an orthogonal decomposition

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whereH=KerLis finite dimensional, andH+,HareL-invariant subspaces such that

for someσ> ,

Lu,uσu (.)

for alluH+,

Lu,u ≤–σu (.)

for alluH.

Remark . By [], we can choose the properrto make that the set{j≥|(–)jjj+ =

} =∅, which meansH=, wherejZ.

Lemma .[] There exists C> such that

uLpCu, u∞≤Cu, (.)

for p=  +α, ,u∞=maxt∈[,π]|u(t)|,∀uH(S, RN).

Now consider the functionalϕdefined onH(S, RN) given by

ϕ(u) = 

Lu,uλ

π

Fλt,u(t)dt. (.)

SinceFsatisfies the assumption (A), a standard argument shows the following.

Lemma .[] The functionalϕis continuously differentiable on H(S, RN)andϕ is

defined by

ϕ(u),v=Lu,vλ π

Fλt,u(t),v(t)dt (.)

for all vH(S, RN).

Lemma . [] A critical point uH(S, RN)of functional ϕ is equivalent to a π

-periodic solution of system(.).

In this paper, we will use the following local linking Theorem A to prove our theorems. The following concepts appeared in [, , ].

LetX be a real Banach space with direct decompositionX=XX. Consider two

sequences of subspaces:

XjXj⊂ · · · ⊂Xj

such thatXj= nNX

j

n,j= , . For every multi-indexα= (α,α)∈N, we denote by

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Definition .[] A sequence{αn} ⊂Nis said to be admissible if, for everyαNthere

ismNsuch thatnmαn>α.

Definition .[] LetfC(X,R). Then the functionf satisfies the (PS)condition if

every sequence{uαn}such that{αn}is admissible and

uαnXαn, sup n

f(uαn) <∞, fαn(uαn)→

contains a subsequence which converges to a critical point off, where=f|.

Definition .[] LetXbe a Banach space with a direct sum decompositionX=XX.

The functionfC(X,R) has a local linking at , with respect to (X,X), if, for somer> ,

f(x)≥, ∀xX,xr,

f(x)≤, ∀xX,xr.

Theorem A[] Suppose that fC(X, R)satisfies the following assumptions:

(f) f has a local linking atandX={}; (f) f satisfies(PS)∗condition;

(f) f maps bounded sets into bounded sets;

(f) for everymN,f(x)→–∞asx → ∞onX

mX.

Then f has at least one nonzero critical point.

3 Proofs of theorems

In this section,cistand for different positive constants foriZ+, Z+is the set of all positive

integers. Let

X=X⊕X, (.)

whereX=H+,X=HH.

Lemma . Under assumption(H), (H)-(H),the functionalϕsatisfies the(PS)∗ condi-tion.

Proof Let{uαn}be a sequence such that{αn}is admissible and

uαnXαn, sup n

ϕ(uαn) <∞, ϕαn(uαn)→.

For the sake of notational simplicity, setun=uαn.

Claim.{un}is bounded inX.

If not, passing to a subsequence if necessary, we assume thatun → ∞asn→ ∞. Set

vn=uunn, then{vn}is bounded inX. Hence, there exists a subsequence, still denoted by {vn}. Writevn=v+n+vn+vnandv=v++v–+v, then

vn v, vnv inX, vnv inC

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In view of (H), we have

F(t,x)≤c

|x|+α+|x|, ∀xRN andt∈[, τ]. (.)

For|x| ≤Randt∈[, τ], one has

F(t,x)≤c

|x|+α+|x|≤c

R+α+|R|:=A,

together with (H), one has

μF(t,x)≤∇F(t,x),x+b(t)|x|β+μA, ∀xRN andt∈[, τ]. (.)

Hence, by (.) and (.), we have

μ

 – 

Lun,un=μϕ(un) –

ϕ(un),un

+λ π

μF(λt,un) –

F(λt,un),un

dt

c+cun+λ π

b(t)|un|β+μA

dt

c+cun+cunβ+c.

This implies that

Lun,unc+cun+cunβ (.)

sinceμ> . Together with (.), we have

Lvn,vn=

Lun,un un →

, asn→ ∞,

since  <β< . Hence,

Lv,v= .

That means that

Lv+,v++Lv–,v–= .

By using (.) and (.), we discuss two cases:

Ifv+= , we havev–= , then we obtainv=v=vn= .

Ifv+ = , we havev= , then we obtainv = .

So we getv(t)≡ fort∈[, π]. Set

E=

t∈[, π] :v(t)= ,

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From (H), we get

lim

|un|→∞ inf

π

F(λt,un)dt

un

≥ π

 [lim|un|→∞infF(λt,un)]dt un

E

lim

|un|→∞

infF(λt,un) |un| |

vn| dtE lim

|un|→∞

infF(λt,un) |un| |

v|

dt> . (.)

By the boundedness ofϕ(un) and (.), we have ϕ(un)

un

=Lun,unun

λ

π

F(λt,un)dt

un

c+cun+cunβ

un

λ

π

F(λt,un)dt

un

,

which together with  <β<  implies that

lim

|un|→∞ inf

π

F(λt,un)dt

un

= .

This contradicts (.). Therefore,{un}is bounded inX.

Claim.{un}possesses a strong convergent subsequence inX.

Writeun=u+n+un+unandu=u++u–+u, then

u±n u±, unu inX, u±nu± inCS, RN.

In view of (.) andu

nu–inC(S, RN), it is easy to verify π

F(λt,un) –∇F(λt,u),unu

dt→, asn→ ∞.

Note that

ϕ(un) –ϕ(u),unu

→, asn→ ∞.

Thus,

ϕ(un) –ϕ(u),unu

= –Lunw–,unu–+λ π

F(λt,un) –∇F(λt,u),unu

dt

σunu–+λ π

F(λt,un) –∇F(λt,u),unu

dt.

This yieldsu

nu–inX. Similarly,u+nu+inX. HenceunuinX. Hence,{un}

pos-sesses a strong convergent subsequence inX. The proof of Lemma . is complete.

Lemma . Under assumption(H), (H),and(H),the functionalϕsatisfies the(PS)∗

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Proof Let{uαn}be a sequence such that{αn}is admissible and

uαnXαn, sup n

ϕ(uαn) <∞, ϕαn(uαn)→.

For the sake of notational simplicity, setun=uαn.

Claim.{un}is bounded inX.

If not, passing to a subsequence if necessary, we assume thatun → ∞asn→ ∞. In

view of (H), there existsc>  such that

F(t,x),x– F(t,x)≥b|x|βc, ∀(t,x)∈[, τRN. (.)

Hence, we have

ϕ(un) –

ϕ(un),un

=λ π

F(λt,un),un

– F(λt,un)

dt

λ π

b|un|βc

dt

= π

|un|βdt– πcλ.

This implies that

T

 |un| βdt

un

, asn→ ∞. (.)

Letun=u+n+un+unH+⊕H–⊕H. By (H), we have

ϕ(un),u+n

=Lu+n,u+nλ π

F(λt,un),u+n

dt

σu+n– π

|un|αun++u+ndt

σu+n–(π)ββα

π

|un|α×

β αdt

α

β

u+n– πaλu+n

σu+n–(π)ββαCu

Lβu+n– πaλCu+n

for alln, where we use the Hölder inequality and (.). We have

u+

n un

, asn→ ∞. (.)

Similarly foru

n, we also get u

n un

, asn→ ∞. (.)

Again, by (H), we have

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sinceβ>α≥. Since dimH<,

ϕ(un) –

ϕ(un),un

=λ π

F(λt,un),un

– F(λt,un)

dt

λ π

b|un|–c

dt

λ π

bu

nbu+nbunc

dt

cuncun+–cunc.

So we get

un

un

→, asn→ ∞. (.)

Hence by (.)-(.), one has

 =un

unu

n+u+n+un

un

, asn→ ∞,

a contradiction. Therefore,{un}is bounded inX.

Using similar arguments to the proof of Claim  in Lemma .,{un}possesses a strong

convergent subsequence inX. The proof of Lemma . is complete.

Lemma . Under assumption(H)-(H),the functionϕsatisfies the conditions(f), (f),

and(f)of TheoremA.

Proof We only consider the case (i) in (H). The other case is similar. () We claim thatϕhas a local linking at  with respect to (X,X). By (H), for anyε> , there existsδ>  such that

F(t,x)≤ε|x|, ∀t∈[, τ],|x| ≤δ. (.)

By (.) and (.), there existsc>  such that

F(t,x)≤ε|x|+c|x|+α, ∀t∈[, τ],xRN. (.)

Hence, foruX, we have

ϕ(u)≥ 

Lu,uλ

π

ε|u|+c|u|+α

dtσ

u

ελCuc

λCu+α.

Takingε=σ/(λC) and noting thatα>  in (H), we can find a constantρ>  such

that

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On the other hand, letu=u+uXsatisfyinguρ

=R/(C) and let

=

t∈[, π]|u–≤R/

, =

t∈[, π]|u–>R/

. Then we have

uu

∞≤Cu≤R/

for allt∈[, π]. Consequently,

|u| ≤u+u–≤R, for allt.

Hence, from (H)(i), we obtain

F(t,u)dt≥.

On the one hand, one obtains

|u| ≤u+u–≤R/ +u–≤u–, for allt.

It follows from (.) that

F(λt,u)≤ε|u|+c|u|+α≤εu– 

+ +αcu– +α

, for allt, which implies that

F(λt,u)dt≤ε

u–dx+ +αc

u–+αdt

≤ε π

u–dx+ +αc

π

u–+αdt

≤εCu–+ (C)+αcu– +α

. Settingε=σ/(C), we have

ϕ(u)≤–σ

u–,u––λ π

F(λt,u)dt≤–σu

–+ (C)+αcu

+α

.

Consequently,

ϕ(u)≤, ∀uXwithuρ,

whereρ<ρis small enough.

() We claim that for everymN,ϕ(u)→–∞asu → ∞onX

mX.

SinceXm andHare finite dimensional, we can chooseσm> ,Cm>  such that

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uCmuL, for alluXmH.

By (H), there existsc>  such that

F(t,x)≥σm

Cm|

x|–c, ∀t∈[, τ],∀xRN.

So foruX

mX, ϕ(u) = 

Lu+,u++ 

Lu–,u––λ π

Fλt,u(t)dt

σm

u

+σ

u

–σm

Cm π

u(t)dt+c

= σmu

+

σu

–

σm

Cm

u+L+uL+uL

+c

≤–σmu

+

σu

–

σmu+c→–∞,

foru → ∞.

() By (.), we see thatϕmaps bounded sets into bounded sets.

The proof of Lemma . is complete.

Proof of Theorem. By Lemmas . and ., all conditions of Theorem A are satisfied. Thus, problem (.) has at least one nonzero critical point.

Proof of Theorem. By Lemmas . and ., all conditions of Theorem A are satisfied. Thus, problem (.) has at least one nonzero critical point.

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

The authors read and approved the final manuscript.

Acknowledgements

The authors would like to express their sincere thanks to the referees for their helpful comments. Supported by the Natural Science Foundation of Shanxi Province (No. 2012011004-1) of China and by the National Natural Science Foundation of China (No. 61473180).

Received: 28 August 2015 Accepted: 25 January 2016

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