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, 2τ
],u(0) –u(2
τ
) =u˙(0) –u˙(2τ
) = 0,where
τ
> 0 is a given constant,r∈Ris 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(t–τ) +∇F(t,u(t–τ)) = , a.e.t∈[, τ],
u() –u(τ) =u˙() –u˙(τ) = , (.) whereτ > is a given constant, r∈Ris a parameter.F: [, τ]×RN →Rsatisfies the
following assumptions:
(A)F(t,x) is measurable with respect tot, for allx∈RN, continuously differentiable inx, for a.e.t∈[, τ], and there exista∈C(R+; R+) andb∈L([, τ]; R+) such that
F(t,x),∇F(t,x)≤a|x|b(t)
for allx∈RNand 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
[], 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) +rλu(t–π) +λ∇F(λt,u(t–π)) = , a.e.t∈[, π],
u() –u(π) =u˙() –u˙(π) = , (.) by making the change of variablet→πτt=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-periodicC∞ vector-valued
func-tions with dimension N. For anyu∈C∞(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=
where a,aj,bj∈RN. 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) ={u∈L(S, RN) :u< +∞}with the inner product
u,v=
π
u(t),v(t)+u˙(t),v˙(t)dt
for anyu,v∈H(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 operatorsLandLfromH(S, RN) intoH∗(S, RN) as follows: for any
u∈H(S, RN), which are given by
(Lu)(v) =
π
˙
u(t+π),v˙(t)dt,
(Lu)(v) = –rλ
π
u(t),v(t)dt,
for allv∈H∗(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,v∈H(S, RN), wherei= or . It is easy
to check thatLandLare 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–rλ 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
whereH=KerLis finite dimensional, andH+,H–areL-invariant subspaces such that
for someσ> ,
Lu,u ≥σu (.)
for allu∈H+,
Lu,u ≤–σu (.)
for allu∈H–.
Remark . By [], we can choose the properrto make that the set{j≥|(–)jjj+–rλ =
} =∅, which meansH=∅, wherej∈Z.
Lemma .[] There exists C> such that
uLp≤Cu, u∞≤Cu, (.)
for p= +α, ,u∞=maxt∈[,π]|u(t)|,∀u∈H(S, RN).
Now consider the functionalϕdefined onH(S, RN) given by
ϕ(u) =
Lu,u–λ
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,v–λ π
∇Fλt,u(t),v(t)dt (.)
for all v∈H(S, RN).
Lemma . [] A critical point u∈H(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=X⊕X. Consider two
sequences of subspaces:
Xj⊂Xj⊂ · · · ⊂Xj
such thatXj= n∈NX
j
n,j= , . For every multi-indexα= (α,α)∈N, we denote byXα
Definition .[] A sequence{αn} ⊂Nis said to be admissible if, for everyα∈Nthere
ism∈Nsuch thatn≥m⇒αn>α.
Definition .[] Letf ∈C(X,R). Then the functionf satisfies the (PS)∗ condition if
every sequence{uαn}such that{αn}is admissible and
uαn∈Xαn, sup n
f(uαn) <∞, fαn(uαn)→
contains a subsequence which converges to a critical point off, wherefα=f|Xα.
Definition .[] LetXbe a Banach space with a direct sum decompositionX=X⊕X.
The functionf ∈C(X,R) has a local linking at , with respect to (X,X), if, for somer> ,
f(x)≥, ∀x∈X,x ≤r,
f(x)≤, ∀x∈X,x ≤r.
Theorem A[] Suppose that f ∈C(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 everym∈N,f(x)→–∞asx → ∞onX
m⊕X.
Then f has at least one nonzero critical point.
3 Proofs of theorems
In this section,cistand for different positive constants fori∈Z+, Z+is the set of all positive
integers. Let
X=X⊕X, (.)
whereX=H+,X=H–⊕H.
Lemma . Under assumption(H), (H)-(H),the functionalϕsatisfies the(PS)∗ condi-tion.
Proof Let{uαn}be a sequence such that{αn}is admissible and
uαn∈Xαn, 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+v–n+vnandv=v++v–+v, then
vn v, vn→v inX, vn→v inC
In view of (H), we have
F(t,x)≤c
|x|+α+|x|, ∀x∈RN 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, ∀x∈RN 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,un ≤c+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)= ,
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| dt≥ E lim
|un|→∞
infF(λt,un) |un| |
v|
dt> . (.)
By the boundedness ofϕ(un) and (.), we have ϕ(un)
un
=Lun,un un
–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+u–n+unandu=u++u–+u, then
u±n u±, un→u inX, u±n →u± inCS, RN.
In view of (.) andu–
n→u–inC(S, RN), it is easy to verify π
∇F(λt,un) –∇F(λt,u),u–n–u–
dt→, asn→ ∞.
Note that
ϕ(un) –ϕ(u),u–n–u–
→, asn→ ∞.
Thus,
–ϕ(un) –ϕ(u),u–n–u–
= –Lu–n–w–,u–n–u–+λ π
∇F(λt,un) –∇F(λt,u),u–n–u–
dt
≥σu–n–u–+λ π
∇F(λt,un) –∇F(λt,u),u–n–u–
dt.
This yieldsu–
n→u–inX. Similarly,u+n→u+inX. Henceun→uinX. 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)∗
Proof Let{uαn}be a sequence such that{αn}is admissible and
uαn∈Xαn, 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|β–c, ∀(t,x)∈[, τ]×RN. (.)
Hence, we have
ϕ(un) –
ϕ(un),un
=λ π
∇F(λt,un),un
– F(λt,un)
dt
≥λ π
b|un|β–c
dt
=bλ π
|un|βdt– πcλ.
This implies that
T
|un| βdt
un →
, asn→ ∞. (.)
Letun=u+n+u–n+un∈H+⊕H–⊕H. By (H), we have
ϕ(un),u+n
=Lu+n,u+n–λ π
∇F(λt,un),u+n
dt
≥σu+n–aλ π
|un|αun++u+ndt
≥σu+n–aλ(π)β–βα
π
|un|α×
β αdt
α
β
u+n∞– πaλu+n∞
≥σu+n–aλ(π)β–βαCu
nαLβu+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
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
n–bu+n–bu–n–c
dt
≥cun–cun+–cu–n–c.
So we get
un
un
→, asn→ ∞. (.)
Hence by (.)-(.), one has
=un
un≤ u
n+u+n+u–n
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],x∈RN. (.)
Hence, foru∈X, we have
ϕ(u)≥
Lu,u–λ
π
ε|u|+c|u|+α
dt≥σ
u
–ελCu–c
λCu+α.
Takingε=σ/(λC) and noting thatα> in (H), we can find a constantρ> such
that
On the other hand, letu=u+u–∈Xsatisfyingu ≤ρ
=R/(C) and let
=
t∈[, π]|u–≤R/
, =
t∈[, π]|u–>R/
. Then we have
u≤u
∞≤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≤–σ u
–+ (C)+αc u–
+α
.
Consequently,
ϕ(u)≤, ∀u∈Xwithu ≤ρ,
whereρ<ρis small enough.
() We claim that for everym∈N,ϕ(u)→–∞asu → ∞onX
m⊕X.
SinceXm andHare finite dimensional, we can chooseσm> ,Cm> such that
u ≤CmuL, for allu∈Xm⊕H.
By (H), there existsc> such that
F(t,x)≥σm
Cm|
x|–c, ∀t∈[, τ],∀x∈RN.
So foru∈X
m⊕X, ϕ(u) =
Lu+,u++
Lu–,u––λ π
Fλt,u(t)dt
≤σm
u
+–σ
u
––σm
Cm π
u(t)dt+c
= σm u
+
–σ u
–
–σm
Cm
u+L+u–L+uL
+c
≤–σm u
+
–σ u
–
–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
References
1. Ding, Y: Variational Methods for Strongly Indefinite Problems. World Scientific, Singapore (2007)
2. Guo, Y: Nontrivial periodic solutions for asymptotically linear Hamiltonian systems with resonance. J. Differ. Equ.175, 71-87 (2001)
3. Su, JB: Nontrivial periodic solutions for the asymptotically linear Hamiltonian systems with resonance at infinity. J. Differ. Equ.145, 252-273 (1998)
4. Li, SJ, Willem, M: Applications of local linking to critical point theory. J. Math. Anal. Appl.189, 6-32 (1995) 5. Mawhin, J, Willem, M: Critical Point Theory and Hamiltonian Systems. Springer, New York (1989)
6. Rabinowitz, PH: Minimax Methods in Critical Point Theory with Applications to Differential Equations. CBMS Reg. Conf. Ser. Math., vol. 65. Am. Math. Soc., Providence (1986)
7. Zhang, Q, Tang, XH: New existence of periodic solutions for second order non-autonomous Hamiltonian systems. J. Math. Anal. Appl.369, 357-367 (2010)
8. He, X, Wu, X: Periodic solutions for a class of nonautonomous second order Hamiltonian systems. J. Math. Anal. Appl. 341, 1354-1364 (2008)
9. Fei, G: Multiple periodic solutions of differential delay equations via Hamiltonian systems (I). Nonlinear Anal.65, 25-39 (2006)
11. Guo, Z, Yu, J: Multiplicity results for periodic solutions to delay differential equations via critical point theory. J. Differ. Equ.218, 15-35 (2005)
12. Li, J, He, X: Multiple periodic solutions of differential delay equations created by asymptotically linear Hamiltonian systems. Nonlinear Anal.31(1/2), 45-54 (1998)
13. Wu, K, Wu, X: Existence of periodic solutions for a class of first order delay differential equations dealing with vectors. Nonlinear Anal.72, 4518-4529 (2010)
14. Wu, K, Wu, X: Multiplicity results of periodic solutions for systems of first order delay differential equation. Appl. Math. Comput.218, 1765-1773 (2011)
15. Wu, K: Multiplicity results of periodic solutions for a class of first order delay differential equations. J. Math. Anal. Appl. 390, 427-438 (2012)
16. Wu, K, Wu, X, Zhou, F: Multiplicity results of periodic solutions for a class of second order delay differential equations. Nonlinear Anal.75, 5836-5844 (2012)
17. Zhang, X, Meng, Q: Nontrivial periodic solutions for delay differential systems via Morse theory. Nonlinear Anal.74, 1960-1968 (2011)