EXISTENCE OF HOMOCLINIC SOLUTIONS TO NONAUTONOMOUS SECOND-ORDER p-LAPLACIAN SYSTEM WITH A COERCIVE POTENTIAL∗†

2015-05-04 04:58YunXin
Annals of Applied Mathematics 2015年3期

Yun Xin

(CollegeofComputerScienceandTechnology,HenanPolytechnicUniversity, Jiaozuo454000,Henan,E-mail:xy_1982@126.com)

Zhibo Cheng

(SchoolofMathematicsandInformationScience, HenanPolytechnicUniversity,Jiaozuo454000,Henan)

EXISTENCE OF HOMOCLINIC SOLUTIONS TO NONAUTONOMOUS SECOND-ORDER p-LAPLACIAN SYSTEM WITH A COERCIVE POTENTIAL∗†

Yun Xin

(CollegeofComputerScienceandTechnology,HenanPolytechnicUniversity, Jiaozuo454000,Henan,E-mail:xy_1982@126.com)

Zhibo Cheng

(SchoolofMathematicsandInformationScience, HenanPolytechnicUniversity,Jiaozuo454000,Henan)

In this paper,we investigate a non-autonomous second-orderp-Laplacian system. Based on critical point theory,we discuss the existence of homoclinic orbits of the system.

homoclinic solutions;p-Laplacian;coercive potential

2000MathematicsSubjectClassification34C37;58E05;70H05

1 Introduction

In this paper,we consider the existence of homoclinic orbits to the non-autonomous second-orderp-Lapcian system

wherep>1,t∈R,u∈RnandF:R×Rn→R andf:R→Rn.

As it is well known,a solutionu(t)to(1.1)is homoclinic(to 0)ifu(t)→0 and˙u(t)→0 as|t|→∞.In addition,ifu/≡0,thenuis called a nontrivial homoclinic solution.

The existence of homoclinic orbits is one of the most important problems in the theory of Hamiltonian systems.Recently the existence and multiplicity of homoclinic orbits to Hamiltonian systems have been studied extensively via critical point theory,such as[1-12]and the references therein.In particular,the second-order systems were considered in [2-5,8-10,12].

Whenp=2,(1.1)reduces to the following second-order Hamiltonian system

In[3],Izydorek and Janczewka proved the following theorem.

Theorem1.1[3]AssumethatandFandfsatisfythefollowingconditions:

(A1)F∈C1(R×Rn,R)isT-periodicwithrespecttot,T>0;

(A2)thereisaconstantb>0suchthatforall(t,x)∈R×Rn,

Thensystem(1.2)possessesahomoclinicsolution

In[9],Tang and Xiao further investigated the existence of homoclinic solutions to(1.1). And the following theorem was obtained.

Theorem1.2[9]AssumethatFsatisfies(A1)andthefollowingconditions:

(B2)Thereareconstantsb>0andµ>1suchthatforall(t,x)∈[0,T]×Rn,

Then(1.1)possessesahomoclinicsolution.

Clearly,either assumption(A2)in Theorem 1.1 or assumption(B2)in Theorem 1.2 implies that the coercive condition

holds,which is crucial for obtaining the existence of homoclinic solution to(1.2)and(1.1) in[3,9],respectively.In this paper,we continuously investigate the existence of homoclinic solutions to(1.1),and our result generalizes the above results.

Our goal in this paper is to use the following more general conditions instead of(B2), such asFcan change sign when|x|is small enough.

(C2)There are constantsb>0,ν>1 andµ>νsuch that for all

Next,we present our main result.

Theorem1.3AssumethatFandfsatisfyassumptionsThen system(1.1)possessesahomoclinicsolution

In order to receive a homoclinic solution to(1.1),similarly to[3],we consider a sequence of diff erential system:

wherefk:R→Rnis a 2kT-periodic extension offin the interval

ε0∈(0,min{1,T})is a constant independent ofk.We will prove the existence of one homoclinic solution to(1.1)similar to that of the limit of the 2kT-periodic solutions to(1.3) in[3].However,some technical details in this paper are diff erent form that in[3].

2 Proof of Theorem 1.3

For eachk∈N,letdenote the Hilbert space of 2kT-periodic functions on R with values in Rnunder the norm

Then we can easily check thatis a weakly lower semi-continuous and

for allu,v∈Ek.Furthermore,it is well known that the critical points ofIkinEkare classical 2kT-periodic solutions to(1.3).

Based the follows lemmas,Theorem 1.3 obviously holds.

Lemma2.1[9]Leta>0andu∈W1,p(R,Rn).Thenforeveryt∈R,thefollowing inequalityholds:

Lemma2.2[9]Letu∈Ek.Thenthefollowinginequalityholds:

Lemma2.3AssumethatFandfsatisfy(A1),(C2)and(B3).Thenforeveryk∈N, system(1.3)possessesa2kT-periodicsolutionuk∈Eksuchthat

where

Set

Then by Sobolev’s inequality,we have

In view of(2.9),it is easy to verify,for eachk∈N,that the following conditions are equivalent:

Hence,form(2.8),we obtain

Now by Theorem 1.1 and Corollary 1.1 in[13],we conclude that for everyk∈N there exists auk∈Eksuch that

Since

This completes the proof.

Lemma2.4Letuk∈Ekbeasolutiontosystem(1.3)whichsatisfies(2.5)fork∈N. ThenthereexistsapositiveconstantCindependentofksuchthat

ProofBy(2.5),we can see that

which implies that there is anM1>0 independent ofksuch that

From(2.5)and(2.11),we obtain

It follows from(2.4),(2.11)and(2.12)that

which shows that(2.10)holds.The proof is complete.

From(2.10),(2.13),(A1)and(B3),we obtain

which implies that

Consequently,

We claim thatis also equicontinuous.If not,then there exist anε0>0,two sequencesand a sequenceof integers such that

Combining(2.16)with(2.17),we have

On the other hand,from(2.14)and(2.16),we have

Lemma2.6LetbedeterminedbyLemma2.5.Thenu0isasolutionto(1.1)suchthatu0(t)→0and˙u0→0ast→±∞.

ProofStep 1We will show thatu0(t)satisfi es(1.1).By Lemmas 2.3 and 2.5,we have

Takea,b∈R such thata<b.There exists aj0∈N such that for allj>j0

Integrating(2.20)fromatot∈[a,b],we have

Note that Lemma 2.5 shows thatukj→u0uniformly on[a,b]anduniformly on [a,b]asj→∞.Letj→∞in(2.21),then we get

Sinceaandbare arbitrary,(2.22)shows thatu0(t)is a solution to(1.1).

Obviously,for everyi∈N,there exists aj1∈N such that for allj>j1we have

by(2.11)and(2.12).Lettingj→+∞,we get

next lettingi→+∞,we have

so

By(2.3),we obtain

Combining(2.24)and(2.25),we receive,as

Step 3Finally,we will show that

From(2.10)and Lemma 2.5,we have

which together with(1.1),(A1)and(B3)imply that

and

It follows that

which contradicts(2.23),so(2.26)holds.The proof is complete.

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(editedbyLiangweiHuang)

∗This research was supported by NNSF of China Project(No.11326124)and Education Department of Henan Province Project(No.14A110002).

†Manuscript received January 21,2015