Chengjun GUO(郭承軍)
School of Applied Mathematics,Guangdong University of Technology,Guangzhou 510006,China
Donal O'REGAN
School of Mathematics,Statistics and Applied Mathematics,National University of Ireland,Galway,Ireland
Nonlinear Analysis and Applied Mathematics(NAAM)-Research Group,Department of Mathematics,King Abdulaziz University,Jeddah,Saudi Arabia
Yuantong XU(徐遠通)
Department of Mathematics,Sun Yat-sen University,Guangzhou 510275,China
Ravi P.AGARWAL
Department of Mathematics,Texas A and M University-Kingsville,Texas 78363,USA Nonlinear Analysis and Applied Mathematics(NAAM)-Research Group,Department of Mathematics,King Abdulaziz University,Jeddah,Saudi Arabia
EXISTENCE OF HOMOCLINIC ORBITS FOR A CLASS OF FIRST-ORDER DIFFERENTIAL DIFFERENCE EQUATIONS?
Chengjun GUO(郭承軍)
School of Applied Mathematics,Guangdong University of Technology,Guangzhou 510006,China
E-mail:guochj817@163.com
Donal O'REGAN
School of Mathematics,Statistics and Applied Mathematics,National University of Ireland,Galway,Ireland
Nonlinear Analysis and Applied Mathematics(NAAM)-Research Group,Department of Mathematics,King Abdulaziz University,Jeddah,Saudi Arabia
E-mail:donal.oregan@nuigalway.ie
Yuantong XU(徐遠通)
Department of Mathematics,Sun Yat-sen University,Guangzhou 510275,China
E-mail:xyt@mail.sysu.edu.cn
Ravi P.AGARWAL
Department of Mathematics,Texas A and M University-Kingsville,Texas 78363,USA Nonlinear Analysis and Applied Mathematics(NAAM)-Research Group,Department of Mathematics,King Abdulaziz University,Jeddah,Saudi Arabia
E-mail:agarwal@tamuk.edu
In this article we consider via critical point theory the existence of homoclinic orbits of the first-order differential difference equation
homoclinic solutions;differential difference equation;critical point theory 2010 MR Subject Classification 34K13;34K18;58E50
In this article we study the existence of homoclinic solutions of the differential difference equation
This is the so-called mixed functional differential equation involving both advance and retardation terms and they arise for example in optimal control problems with delays.The Euler equation corresponding to the action functional often involves both advanced and delayed terms,see[12].Mixed functional differential equation were studied in Rustichini[16,17]and in Wu and Zou[20].
In this article motivated by the work of Rabinowitz[13]we establish the existence of homoclinic orbits to(DE)using a variational approach.For the existence of homoclinic orbits for second order differential equations we refer the reader to[2-4,7-9,11,13,15]and for first order to[1,5,10,18,21-23].
Throughout this article,we always assume the following:
(F) there exists a continuously differentiable τ-periodic function F(t,v1,v2)∈C(R× Rn×Rn,R)with respect to t,such that
where z belongs to the Hilbert space of 2kτ-periodic functions.
A solution z(t)of(DE)is said to be homoclinic(to 0)if z(t)→0 as t→±∞.In addition,if z(t)/≡0 then z(t)is called a nontrivial homoclinic solution.
Finally we state a result which will be used in the proof of our main results.
Lemma 1.1[14]Let E be a real Hilbert space with E=E(1)⊕E(2)and E(1)=(E(2))⊥. Suppose I∈C1(E,R)satisfies the(PS)condition,and
(C1)I(u)=12(Lu,u)+b(u),where Lu=L1P1u+L2P2u,Li:E(i)-→E(i)is bounded and selfadjoint,Piis the projector of E onto E(i),i=1,2,
(C2)b′is compact,and
(C3) there exists a subspace~E?E and sets S?E,Q? ~E and constants~α>ω such that
(i) S?E(1)and I|S≥~α,
(ii)Q is bounded and I|?Q≤ω,
(iii) S and?Q link.
Then I possesses a critical value c≥~α given by
where
(Γ1)g(0,u)=u,
(Γ2)g(t,u)=u for u∈?Q,and
(Γ3)g(t,u)=eθ(t,u)Lu+χ(t,u),where θ(t,u)∈C([0,1]×E,R)and χ is compact.
The article is organized as follows.In Section 2,we establish a variational structure for(DE)with periodic boundary value conditions.In Section 3 using the linking theorem we show that(DE)has a homoclinic solution.In Section 4 we prove a second existence result for(DE)under the Ambrosetti-Rabinowitz growth condition.
Let A=d/dt+B(t)be the self-adjoint operator acting on L2(R,R2n)with the domainthen E is a Hilbert space with inner product
As in[11],a homoclinic solution of(DE)will be obtained as a limit,as k→±∞,of a certain sequence of functions zk∈Ek.We consider a sequence of systems of differential equations
where for each k∈N,zk,a 2kτ-periodic solution of(DEk)(which will be obtained via the linking theorem).
We define
and
Then,Ik∈C1(Ek,R)and it is easy to check that for any z,y∈Ek,
By the periodicity of z(t)and F(t,z(t),z(t-τ))with respect to t,we obtain
Thus
Therefore,the corresponding Euler equation of the functional Ikis the following equation
Moreover,under assumption(F),it is clear that critical points of Ikare classical 2kτ-periodic solutions of(DEk).
We have from(2.2)that A has a sequence of eigenvalues
and
Hence,there exist an orthogonal decomposition Ek=E0k⊕E-k⊕E+kwith dim(E0k)<∞.
We now assume that the following are satisfied:
(V1)F(t,v1,v2)≥0,for all(t,v1,v2)∈R×Rn×Rn;
(V2) F(t,v1,v2)=o(|v|2)as|v|-→0 uniformly in t,here
(V4) there exist constantsand ψ(t),?(t)∈L1(R,R+)such that for(t,v1,v2)∈R×Rn×Rn,
and
Now,we state our first existence result.
Theorem 3.1 Let(F)and(V1)-(V4)be satisfied.Then(DE)possesses a nontrivial homoclinic solution such that z(t)→0 as t→±∞.
In order to prove Theorem 3.1,the following result in[14,Proposition 6.6]will be used.
Proposition 3.2 There is a positive constant cθsuch that for each k∈N and z∈Ekthe following inequality holds:
where θ∈[1,+∞).For notational purposes let c2λ=?.
Lemma 3.3 Under the conditions of Theorem 3.1,Iksatisfies the(PS)condition.
Proof Assume that{zkn}n∈Nin Ekis a sequence such that{Ik(zkn)}n∈Nis bounded and I′k(zkn)→0 as n→+∞.Then there exists a constant d1>0 such that
We first prove that{zkn}n∈Nis bounded.Let zkn=z0kn+z+kn+z-kn∈E0k⊕E+k⊕E-k. We have from(2.3),(2.5)and(3.1)of(V4)that
where for each k∈N,ψk:R→RNis a 2kτ-periodic extension of the restriction of ψ(t)to the interval[-kτ,kτ]and
This implies that there exists a constant M0>0 with
By(3.7)and(3.8),there exists a constantsuch that
If 0<|zkn|<1 for zkn∈Ek,we have from(3.2)of(V4)and the periodicity of zkn(t)with respect to t that
where for each k∈N,?k:R→Rnis a 2kτ-periodic extension of the restriction of ? to the interval[-kτ,kτ].
Using(3.2)of(V4),(3.4)and(3.10)-(3.11)we have(here1α+1σ=1)
and
Combining(3.7)with(3.12)-(3.14)yields that
From(3.9)and(3.15),there exists a positive constant~D1>0 such that
This implies that
It is easy to check that Φ→0 as n→+∞.Moreover,an easy computation shows that
This implies that‖zkn-z‖Ek→0.
Lemma 3.4 Under the conditions of Theorem 3.1,then for every k∈N the system(DEk)possesses a 2kτ-periodic solution.
Proof The proof will be divided into three steps.
Step 1 Assume that 0<‖z‖Ek≤1 for z∈E(1)k=E+k.From(3.1)of(V4),(3.4)and the periodicity of z(t)with respect to t,we have
Note from(3.3)of(V4)that ξ-2a2?λ>0.Set
Let Bρdenote the open ball in Ekwith radius ρ about 0 and let?Bρdenote its boundary.Let Sk=?Bρ∩E+k.If z∈Skthen(note||z||Ek≤1 from(3.3)of(V4))and so(3.19)gives
Then(C3)(i)of Lemma 1.1 holds.
Step 2 Let e∈E+kwith‖e‖Ek=1 and~Ek=E-k⊕span{e}.Now,let
For z∈Θk,we write z=z-+z+.
I) If‖z-‖Ek>κ‖z+‖Ek,then for any γ>0,we have from(V1)that
Let?k={z∈Θk:‖z-‖Ek≤κ‖z+‖Ek}.
II) If‖z-‖Ek≤κ‖z+‖Ek,we have
i.e.,
The argument in[6]guarantees that there exists ε1k>0 such that,?z∈?k,
From(3.25),we have for z=z-+z+∈?kthat
Therefore,we have
Step 3 (C3)(iii)(i.e.,Sklinks?Qk)holds from the definition of Skand Qkand(see[14],page 32).Thus,(C3)(iii)holds.
Note that(C1)and(C2)of Lemma 1.1 are true.Now from Lemma 1.1,Ikpossesses a critical value ckgiven by
where Υksatisfies(Γ1)-(Γ3).Hence,for every k∈N,there is z?k∈Eksuch that
The function z?kis a desired classical 2kτ-periodic solution of(DEk).Becauseis a nontrivial solution.
Proof The first step in the proof is to show that the sequences{ck}k∈Nand{‖z?k‖Ek}k∈Nare bounded.There exists︿z?1∈E1with︿z?1(±τ)=0 such that
For every k∈N,let
We have from(F),(3.1)of(V4)and(3.32)that
This implies that
An argument similar to that in(3.7)-(3.17)guarantees that there exists a constant~M?1>0 such that
We now show that for a large enough k,
If not(note(2.1)and(3.35)),by passing a subsequence,without the loss of generality,for each k∈N,there exist z?k,?kandsuch that(?denotes large enough)and](η is a constant and M?k→∞as k→∞).
Hence,we have from(F),(DEk),(3.2)and(3.3)of(V4),(3.33)-(3.34)and the periodicity of z?k(t)with respect to t that
This shows that(3.36)holds.
It remains now to show that{z?k}k∈Nis equicontinuous.
From(DEk)and(3.36),there exists a constant~M?3>0 independent of k such that
which implies that
Let k∈N and t,t0∈R,then
Because{z?k}k∈Nis bounded in L∞2kτ(R,R2n)and equicontinuous,we obtain that the sequence{z?k}k∈Nconverges to a certain z?0∈Cloc(R,R2n)by using the Arzel`a-Ascoli theorem. □
Lemma 3.6 The function z?0determined by Lemma 3.5 is the desired homoclinic solution of(DE).
Proof The proof will be divided into three steps.
Step 1 We prove that z?0(t)→0,as t→±∞.
Note we have
Clearly,by(2.1)and(3.35),for every j∈N there exists nj∈N such that for all k≥njwe have
and now,letting j→+∞,we have
and so
Then(3.40)shows that our claim holds.
Step 2 We show that z?0/≡0.
Now,up to a subsequence,we have either
or there exist α?>0 such that
In the first case we shall say that z?0is vanishing,in the second we shall say that z?0is nonvanishing.
By assumptions(F)and(3.2)of(V4),for any ε>0 there exists Cε>0 such that
Hence,from(3.43)and the periodicity of z?
nk(t),there exists a constant~γ>0 such that
Arguing indirectly,we suppose thatis vanishing.We have from(3.41)and(3.44)that
and
Note that dim(E0k)<+∞,so there exist two positive constants,andsuch that
We have from(3.41)and(3.48)that
Now,(3.49)implies that there exists a positive constant bε(0<bε≤ξ4)such that
Hence,we have from(3.46)-(3.47)and(3.50)that
On the other hand,we have from (3.41),(3.45)and(3.49)thatandas k→ ∞.This means thatas k→ ∞,which leads to a contradiction.Hence,is nonvanishing,so(3.42)holds,and this shows that our claim holds.
Step 3 We show that z?0(t)is a nontrivial homoclinic solution of(DE).
According to Step 3,z?0(t)/≡0,so it suffices to prove for any ?∈C∞0(R,Rn),
By Step 1,we can choose k0such that supp??[-kiτ,kiτ]for all ki≥k0,and we have for ki≥k0,
By(3.40)and(3.52),letting ki→ ∞ we obtain(3.51),which shows z?0(t)is a nontrivial homoclinic solution of(DE).
Proof of Theorem 3.1 The result follows from Lemma 3.6.
In this section we prove that(DE)has a nonconstant homoclinic solution under the Ambrosetti-Rabinowitz growth condition.
Now,we make the following assumptions:
(H0) 0/∈σ(A),where A=d/dt+B(t)and σ(A)is the spectrum of A;
(H1) there is a constantμ>2 such that for every t∈R and(v1,v2)∈Rn×Rn{(0,0)}and F(t,v1,v2)=0 if and only if v1=v2=0;
(H2)there is a constant~D>0 such that for|z(t)|≥1
where z belongs to the Hilbert space of 2kτ-periodic functions.
Set m?:=inf{F(t,v1,v2):t∈[0,τ],v21+v22=1}.
Our second existence result is the following theorem.
Theorem 4.1 Under assumptions(F)and(H0)-(H2),the system(DE)possesses a nontrivial homoclinic solution solution such that z(t)→0 as t→±∞.
In order to prove Theorem 4.1,the following result in[11]will be used.
Proposition 4.2 For every t∈[0,τ]the following inequalities hold:
Lemma 4.3 Under the conditions of Theorem 4.1,Iksatisfies the(PS)condition.
Proof Assume that{zkn}n∈Nin Ekis a sequence such that{Ik(zkn)}n∈Nis bounded and I′k(zkn)→0 as n→+∞.Then,there exists a constant D1>0 such that
We first prove that{zkn}n∈Nis bounded.From (H0),we have that Ekhas the direct sum decomposition Ek=E+k⊕E-k.Let zkn=z+kn+z-kn∈E+k⊕E-k.
From(F),(H1)-(H2),(2.3),(2.5),(4.1),(4.2),the periodicity of zkn(t)and F(t,zkn(t),zkn(t-τ))with respect to t,we obtain
From(4.3),we have
Also we have from(H1)and(4.3)that
From(H2)and the periodicity of zkn(t)with respect to t this implies that
We now show that for a large enough n,
If not,by passing to a subsequence,without loss of generality,for each n∈N,there exist zn,?nandsuch that[-kτ,kτ](is a constant and).
Hence,we have from(F),(H2),(4.4)and(4.6)that
However,we have Λn→0 andas n→∞,which leads to a contradiction.Hence(4.7)holds.
We have from(4.6)and(4.7)that
and
From(4.9)and(4.10),we have
This implies that{‖xn‖Ek}n∈Nis bounded.An argument similar to that in Lemma 3.3 yields‖zkn-z‖Ek→0. □
Lemma 4.4 Under the conditions of Theorem 4.1,then for every k∈N the system(DEk)possesses a 2kτ-periodic solution.
Proof As in Step 1 of Lemma 3.4,choose p>2,by(H1),and for any︿ε>0,there exists︿M(︿ε)>0 such that
An argument similar to that in Lemma 3.5 yields the following lemma.
Lemma 4.5 Let{z?k}k∈Nbe the sequence given by Lemma 4.4.There exists a z?0such that z?k→z?0in Cloc(R,Rn)as k→+∞.
Lemma 4.6 The function z?0determined by Lemma 4.5 is the desired homoclinic solution of(DE).
Proof Our argument is a straightforward modification of that in Lemma 3.6 and we just only show step 2.By assumptions(F)and(H1),choose q>1,and for any ε>0 there exists Cε>0 such that
Hence,from(3.4)and(4.14)and the periodicity ofthere exists a constant~γ>0 such that
Arguing indirectly,we suppose thatis vanishing.We have from(3.41)and(4.15)that
and
Hence,we have from(4.17)and(4.18)that
Also,we have from(3.41),(4,15)and(4.16)thatandas k→∞.This means thatas k→∞,which leads to a contradiction.Henceis nonvanishing,so(3.42)holds,and this shows that our claim holds.
Proof of Theorem 4.1 The result follows from Lemma 4.6.
[1]Coti Zelati V,Ekeland I,S′es′e E.A variational approach to homoclinic orbits in Hamiltonian systems.Math Ann,1990,228:133-160
[2]Coti Zelati V,Rabinowitz P H.Homoclinic orbits for second order Hamiltonian systems possessing superquadratic potentials.J Amer Math Soc,1991,4:693-727
[3]Ding Y H.Existence and multiplicity results for homoclinic solutions to a class of Hamiltonian systems. Nonlinear Anal,1995,25:1095-1113
[4]Ding Y H,Girardi M.Periodic and homoclinic solutions to a class of Hamiltonian systems with the potentials changing sign.Dynam Systems Appl,1993,2(1):131-145
[5]Ding Y H,Jeanjean L.Homoclinic orbits for a nonperiodic Hamiltonian system.J Diff Eqns,2007,237: 473-490
[6]Fei G H.On periodic solutions of superquadratic Hamiltonian systems.Elec J Diff Equ,2002,2002(8): 1-12
[7]Guo C J,O'Regan D,Agarwal R.Homoclinic orbits for singular second-order neutral differential equation. J Math Anal Appl,2010,366:550-560
[8]Guo C J,O'Regan D,Agarwal R.Existence of subharmonic solutions and homoclinic orbits for a class of high-order differential equations.Appl Anal,2011,9(7):1169-1183
[9]Guo C J,O'Regan D,Agarwal R.Existence and multiplicity of homoclinic orbits of a second-order differential difference equation via variational methods.Scientific Publications of the State University of Novi Pazarser A:Appl Math Inform and Mech,2012,4(1):1-15
[10]Hofer H,Wysocki K.First order elliptic systems and the existence of homoclinic orbits in Hamiltonian systems.Math Ann,1990,228:483-503
[11]Izydorek M,Janczewska J.Homoclinic solutions for a class of the second order Hamiltonian systems.J Diff Eqns,2005,219:375-389
[12]Pontryagin L S,Gamkreledze R V,Mischenko E F.The Mathematical Theory of Optimal Processes.New York:Interscience,1962
[13]Rabinowitz P H.Homoclinic orbits for a class of Hamiltonian systems.Proc Roy Soc Edinburgh,1990,114A:33-38
[14]Rabinowitz P H.Minimax Methods in Critical Point Theory with Applications to Differential Equations. Providence,RI:Amer Math Soc,1986
[15]Rabinowitz P H,Tanaka K.Some results on connecting orbits for a class of Hamiltonian systems.Math Z,1991,206:472-499
[16]Rustichini A.Functional differential equations of mixed type:the linear autonomous case.J Dynam Diff Eqns,1989,1:121-143
[17]Rustichini A.Hopf bifurcation for functional differential equations of mixed type.J Dynam Diff Eqns,1989,1:145-177
[18]S′es′e E.Existence of infinitely many homoclinic orbits in Hamiltonian systems.Math Z,1993,209:561-590
[19]Stuart C A.Bifurcation into spectral gaps.Bull Belg Math Soc,Supplement,1995
[20]Wu J H,Zou X F.Asymptotic and periodic boundary value problems of of mixed FDEs and wave solutions lattice differential equations.J Diff Eqns,1997,21:315-357
[21]Szulkin A,Zou W M.Homoclinic orbits for asymptotically linear Hamiltonian systems.J Funct Anal,2001,187:25-41
[22]Xu X J.Sub-harmonics of first order Hamiltonian systems and their asymptotic behaviors.Discrete Contin Dyn Syst Ser B,2003,3(4):643-654
[23]Xu X J.Homoclinic orbits for first order Hamiltonian systems with convex potentials.Adv Nonlinear Studi,2006,6:399-410
?Received January 13,2014;revised October 29,2014.This project is supported by National Natural Science Foundation of China(51275094),by High-Level Personnel Project of Guangdong Province(2014011)and by China Postdoctoral Science Foundation(20110490893).
Acta Mathematica Scientia(English Series)2015年5期