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Existence of homoclinic solutions for a fourth order differential equation with a parameter

Tiexiang Li

a

, Juntao Sun

b

, Tsung-fang Wu

c,

aDepartment of Mathematics, Southeast University, Nanjing 211189, PR China

bSchool of Science, Shandong University of Technology, Zibo 255049, PR China

cDepartment of Applied Mathematics, National University of Kaohsiung, Kaohsiung 811, Taiwan

a r t i c l e i n f o

Keywords:

Fourth order differential equations Homoclinic solutions

Mountain pass theorem Variational methods

a b s t r a c t

In this paper, we study the existence of homoclinic solutions for a class of fourth order dif- ferential equations. By using variational methods, the existence and the non-existence of nontrivial homoclinic solutions are obtained, depending on a parameter.

Ó2014 Elsevier Inc. All rights reserved.

1. Introduction

In this paper, we consider a class of fourth-order differential equations with a parameter:

uð4Þþwu00þkaðxÞufðx;uÞ ¼0; x2R; ð1:1Þ

wherewis a constant,k>0 is a parameter,f2CðRR;RÞand the functionasatisfies the following conditions:

(V1) a2CðR;RÞandaP0 onR;

(V2) there existsc>0 such that the setfa<cg:¼fx2RjaðxÞ<cgis nonempty and has finite measure;

(V3) X¼int a1ð Þ0 is nonempty andX¼a1ð Þ0 such thatXis a finite interval;

(V4) jfa<cgj<c0

S21, wherej j is the Lebesgue measure,c0is defined by(2.1)in Section2andS1is the best constant for the embedding ofH2ðRÞinL1ð Þ.R

As usual, we say that a solutionuðxÞof Eq.(1.1)is homoclinic (to 0) ifuðxÞ !0 asx! 1. In addition, ifuðxÞX0, thenuðxÞ is called a nontrivial homoclinic solution.

The above Eq. (1.1)has been put forward as mathematical model for the study of pattern formation in physics and mechanics. For example, the well-known Extended Fisher–Kolmogorov (EFK) equation proposed by Coullet et al. in 1987 [5]in study of phase transitions, and also by Dee and Van Saarlos in 1988[6], as well as the Swift–Hohenberg (SH) equation which is general model for pattern-forming process derived in[13]to describe random thermal fluctuations in the Boussin- esque equation and in the propagation of lasers in[8]. With appropriate changes of variables, stationary solutions of these equations lead to the following fourth order equation:

uð4Þþwu00uþu3¼0;

http://dx.doi.org/10.1016/j.amc.2014.11.056 0096-3003/Ó2014 Elsevier Inc. All rights reserved.

Corresponding author.

E-mail addresses:[email protected](T. Li),[email protected](J. Sun),[email protected](T.-f. Wu).

Contents lists available atScienceDirect

Applied Mathematics and Computation

j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / a m c

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wherew>0 corresponds to EFK equation andw<0 to SH equation.

The study of homoclinic and heteroclinic solutions for the fourth order differential equations has attracted a lot of atten- tion by many researchers, see[1,3,4,9–12,14,15]. These works are mainly concerned on the autonomous case, such as the following equation:

uð4Þþwu00þ

a

ubu2

c

u3¼0;

where

a

; b;

c

are nonnegative constants.

In 2001, Tersian and Chaparova[14]first considered a class of non-autonomous fourth order problems

uð4Þþwu00þaðxÞubðxÞu2cðxÞu3¼0: ð1:2Þ

Applying the mountain pass theorem, they showed that Eq.(1.2)possesses one nontrivial homoclinic solutionu2H2ðRÞ whenaðxÞ; cðxÞanddðxÞare continuous periodic functions and satisfy some other assumptions. If there is no periodicity assumption ofaðxÞ; cðxÞanddðxÞ, then the case will be more difficult. In 2009, Li[9]studied the nonperiodic case of Eq.

(1.2)and obtained the existence of nontrivial homoclinic solution by establishing a compactness lemma and using the mountain pass theorem. Furthermore, the author also studied a class of the nonhomogeneous fourth order equations with the general nonlinear termf:

uð4Þþwu00þaðxÞu¼fðx;uÞ þhðxÞ;

and obtained the existence of homoclinic solution whenfsatisfied the well-known (AR) condition. Very recently, Sun and Wu[12]considered a class of fourth order differential equations with a perturbation:

uð4Þþwu00þaðxÞu¼fðx;uÞ þkhðxÞjujp2u; ð1:3Þ

wherek>0 is a parameter, 16p<2 andh2L2p2ðRÞ. By using variational methods, the existence result of two homoclinic solutions for Eq.(2.6)is obtained if the parameterkis small enough. In all these papers, in order to obtain an important inequality, the following condition

(A) there exists a constanta1>0 such that

0<a16aðxÞ ! þ1; asjxj ! þ1; ð1:4Þ

andw2 ffiffiffiffiffi a1

p ;

is required. However, if there exists the functionasatisfyinga¼0 in some finite intervalTofR, then the conditionðAÞdoes not hold.

Inspired by the above facts, the aim of this paper is to consider this case. We shall establish the existence result of non- trivial homoclinic solutions for Eq.(1.1)when the nonlinear termfsatisfies the asymptotically linear condition. Moreover, the non-existence of nontrivial homoclinic solutions will be discussed.

Before stating our result we need to introduce some notations.

Notation 1.1. Throughout this paper, we denote byj jr theLr-norm, 26r61 andh¼maxfh;0g. Also if we take a subsequence of a sequencefungwe shall denote it againfung.

Now we state our main result.

Theorem 1.1. Assume that the conditions (V1)–(V4) hold and w<2. In addition, we assume that the function f satisfy the following conditions:

(D1) f x;ð sÞis a continuous function onRRsuch that fðx;sÞ 0for all s<0and x2R. Moreover, there exists p2L1ðR;RþÞ with pj j1<H20such that

lim

s!0þ

f x;ð sÞ

s ¼pðxÞuniformly inx2R and

f x;ð sÞ

s PpðxÞfor alls>0 andx2R;

whereH0c0c0S

2 1jfa<cgj

ð Þ

S21jfa<cgj ; (D2) there exist r>1and q2L1X;Rþ

withjqj1>0such that lims!1

f x;ð sÞ

sr ¼0 uniformly inx2RnX and

lims!1

f x;ð sÞ

s ¼qðxÞuniformly inx2X;

(3)

(D3) there exist two constantsh;d0satisfyingh>2and06d0<ðh22hÞH0such that Fðx;sÞ 1

hfðx;sÞs6d0s2for alls>0 andx2R;

(D4)

l

:¼inf R

Xu00ðxÞ2wu0ðxÞ2

dxju2H2ðXÞ \H10ðXÞ;R

XqðxÞu2dx¼1

n o

<1.

Then there existsK0>0such that for everyk>K0, Eq. (1.1) has at least one homoclinic solution.

Remark 1.1. By[14, Lemma 8]and Sobolev embedded theorem, it is not difficult to claim that

l

>0, which is achieved by some/12H2ðXÞ \H10ðXÞwithR

Xq/21dx¼1; seeAppendix A Now, we consider the following the minimum problem:

l

0¼inf Z

R

u00ðxÞ2þu0ðxÞ2þuðxÞ2

dxju2H2ðRÞ;

Z

R

qðxÞu2dx¼1

: ð1:5Þ

Then we have the following result.

Theorem 1.2. Suppose that the conditions (V1)–(V4) and (D1)–(D2) hold. If

l

0> 1

c0S21jfa<cgj and s#f x;sðs Þ is non-decreasing function for any fixed x2R, then for anykP1c, Eq.(1.1)does not admit any nontrivial homoclinic solution.

The remainder of this paper is organized as follows. In Section2, some preliminary results are presented. In Section 3, we give the proofs of our main results.

2. Variational setting and preliminaries

In this section, we give the variational setting for Eq.(1.1). We need the following result.

Lemma 2.1 [14, Lemma 8]. Assume that w<2. Then there exists a constant c0>0such that Z

R

u00ðxÞ2wu0ðxÞ2þuðxÞ2

h i

dxPc0kuk2H2 for allu2H2ðRÞ; ð2:1Þ

wherekukH2¼ R

Rhu00ðxÞ2þu0ðxÞ2þuðxÞ2i

dx1=2

is the norm of Sobolev space H2ðRÞ.

Let

X¼ fu2H2ðRÞj Z

R

u00ðxÞ2wu0ðxÞ2þaðxÞuðxÞ2

h i

dx<þ1g

be equipped with the inner product and norm u;

v

ð Þ ¼ Z

R

u00ðxÞ

v

00ðxÞ wu0ðxÞ

v

0ðxÞ þaðxÞuðxÞ

v

ðxÞ

½ dx

and corresponding normk ku 2¼ðu;uÞ. Fork>0, we also need the following inner product and norm ðu;

v

Þk¼

Z

R

u00ðxÞ

v

00ðxÞ wu0ðxÞ

v

0ðxÞ þkaðxÞuðxÞ

v

ðxÞ

½ dx

and corresponding normk ku 2k¼ ðu;uÞk. It is clear thatk ku 6k ku kforkP1. SetXk¼ðX;k ku kÞ. From the conditions (V1)–(V4), (2.1)and the Sobolev inequality, we have

c0

Z

R

u00ðxÞ2þu0ðxÞ2þuðxÞ2

h i

dx6 Z

R

u00ðxÞ2wu0ðxÞ2þuðxÞ2

h i

dx

¼ Z

R

u00ðxÞ2wu0ðxÞ2

h i

dxþ Z

a<c

f g

uðxÞ2dxþ Z

aPc

f g

uðxÞ2dx 6

Z

R

u00ðxÞ2wu0ðxÞ2

h i

dxþk ku 21jfa<cgj þ1 kc

Z

R

kaðxÞjuðxÞj2dx 6

Z

R

u00ðxÞ2wu0ðxÞ2

h i

dxþ1 kc

Z

R

kaðxÞuðxÞ2dx þS21jfa<cgj

Z

R

u00ðxÞ2þu0ðxÞ2þuðxÞ2

h i

dx:

(4)

Thus, Z

R

u00ðxÞ2þu0ðxÞ2þuðxÞ2

h i

dx6 1

c0S21jfa<cgj Z

R

u00ðxÞ2wu0ðxÞ2

h i

dxþ1 kc

Z

R

kaðxÞuðxÞ2dx

6 1

c0S21jfa<cgj Z

R

u00ðxÞ2wu0ðxÞ2þkaðxÞuðxÞ2

h i

dx

¼ 1

c0S21jfa<cgjk ku 2k for allkP1

c; ð2:2Þ

which implies that the imbeddingXk,!H2ð ÞR is continuous for allkP1c, here the setfaPcg:¼fx2RjaðxÞPcg. Further- more, usingLemma 2.1again, one has

Z

R

uðxÞ2dx¼ Z

a<c

f g

uðxÞ2dxþ Z

faPcg

uðxÞ2dx6k ku 21jfa<cgj þ1 kc

Z

R

kaðxÞuðxÞ2dx 6S21jfa<cgj

Z

R

u00ðxÞ2þu0ðxÞ2þuðxÞ2

h i

dxþ1 kc

Z

R

kaðxÞuðxÞ2dx

6S21jfa<cgj c0

Z

R

u00ðxÞ2wu0ðxÞ2þuðxÞ2

h i

dxþ1 kc

Z

R

kaðxÞuðxÞ2dx;

this implies that Z

R

uðxÞ2dx6 1 c0S21jfa<cgj

S21jfa<cgj c0

Z

R

u00ðxÞ2wu0ðxÞ2

h i

dxþ1 kc

Z

R

kaðxÞuðxÞ2dx

" #

6

max S21jfca<cgj

0 ;kc1

n o

c0S21jfa<cgj Z

R

u00ðxÞ2wu0ðxÞ2þkaðxÞuðxÞ2

h i

dx¼ S21jfa<cgj

c0c0S21jfa<cgjk ku 2k

¼H10 k ku 2k; for allkP c0

cS21jfa<cgjP1

c: ð2:3Þ

Thus, by(2.2) and (2.3), for anyr2ð2;1ÞandkP c0

cS21jfa<cgj, one has Z

R

uðxÞ

j jrdx6k ku r21 Z

R

uðxÞ2dx6Sr21 1

c0S21jfa<cgjk ku 2k

!r22

S21jfa<cgj c0S21jfa<cgjk ku 2k

¼ 1

a<c

f g

j jr22

S21jfa<cgj c0S21jfa<cgj

!2r

k ku rk¼ 1 a<c

f g

j jr22H20rk ku

r

k: ð2:4Þ

Now we begin describing the variational formulation of Eq.(1.1). Consider the functionalJ:Xk!Rdefined by JðuÞ ¼1

2k ku 2k Z

R

Fðx;uÞdx; ð2:5Þ

whereFis the primitive Fðx;uÞ ¼

Z u 0

fðx;sÞds:

Sincefis continuous, we deduce thatJis of classC1and its derivative is given by hJ0ðuÞ;

u

i ¼

Z

R

u00ðxÞ

v

00ðxÞ wu0ðxÞ

v

0ðxÞ þkaðxÞuðxÞ

v

ðxÞ

½ dx

Z

R

fðx;uðxÞÞ

u

ðxÞdx;

for allu;

u

2Xk. Then, we can infer thatu2Xkis a critical point ofJif and only if it is a homoclinic solution of Eq.(1.1).

Furthermore, we have the following result.

Lemma 2.2. Suppose that the conditions (D1) and (D3) hold. Let u0 be a nontrivial homoclinic solution of Eq.(1.1), we have J uð 0Þ>0.

Proof. Sinceu0is a nontrivial homoclinic solution of Eq.(1.1), u0

k k2k¼ Z

R

f x;ð u0Þu0dx: ð2:6Þ

By the conditions (D1) and (D3), the Hö lder inequality,(2.3) and (2.6), we have

(5)

J uð Þ ¼0 1 2k ku0 2k

Z

R

F x;ð u0ÞdxP1

2k ku0 2kd0

Z

R

u0ðxÞ2dx1 h Z

R

f x;ð u0Þu0dxP h2 2h d0

H0

u0

k k2k>0;

whereH01SS221jfb<cgj

1jfb<cgj >0 as in the condition (D1). This completes the proof. h

Next, we give a useful theorem. It is the variant version of the mountain pass theorem, which allows us to find a so-called Cerami typeðPSÞsequence.

Theorem 2.1 ([7], Mountain Pass Theorem). Let E be a real Banach space with its dual space E, and suppose that I2C1ðE;RÞ satisfies

maxfIð0Þ;IðeÞg6

l

<

g

6 inf

kuk¼qIðuÞ;

for some

l

<

g

;

q

>0and e2E withkek>

q

. Let^cP

g

be characterized by

^c¼inf

c2Cmax

06s61

c

ð

s

ÞÞ;

where C¼ f

c

2Cð½0;1 ;EÞ:

c

ð0Þ ¼0;

c

ð1Þ ¼eg is the set of continuous paths joining 0 and e, then there exists a sequence fung E such that

IðunÞ !^cP

g

and ð1þ kunkÞkI0ðunÞkE!0; asn! 1:

3. Proofs of Theorems1.1 and 1.2

In what follows, we give the following two lemmas which ensure that the functionalJhas the mountain pass geometry, which will be used in the proof ofTheorem 1.1.

Lemma 3.1. Suppose that the conditions (V1)–(V4) and (D1)–(D2) hold. Then for everykP c0

cS21jfa<cgjthere exist two positive constants

q

;

g

such that JðuÞjkuk

k¼qP

g

>0.

Proof. For any

>0, it follows from the conditions (D1) and (D2) that there existC>0 andr>2 such that Fðx;sÞ6j jp1þ

2 s2þC

r jsjr; for alls2R: ð3:1Þ

So that, fromLemma 2.1, (3.1)and the Sobolev inequality, we have for allu2Xk, Z

R

Fðx;uÞdx6j jp1þ

2 Z

R

u2dxþC r

Z

R

jujrdx6j jp1þ

2H0

u k k2kþC

r

cr202 a<c

f g

j jr22Hr20k ku

r k;

which implies that JðuÞ ¼1

2k ku 2k Z

R

Fðx;uÞdxP1

2k ku 2kj jp1þ

2H0

u k k2kC

r

cr202 a<c

f g

j jr22H20rk ku

r k

¼k ku 2k 1

2 1j jp1þ

H0

Ccr202 r ajf <cgjr22Hr20k ku

r2 k

" #

: ð3:2Þ

Take

¼H20j jp1. It follows from(3.2)that there exist

q

;

g

>0 such thatJðuÞjkuk

k¼qP

g

. h

Lemma 3.2. Suppose that the conditions (V1)–(V4), (D2) and (D4) hold. Let

q

>0be as inLemma3.1. Then there exists e2Xk

withkekk>

q

such that JðeÞ<0for allkP c0

cS21jfa<cgj.

Proof. By the conditionðD4ÞandRemark 1.1, we can choose a nonnegative function/12H2ð Þ \X H10ð ÞX with Z

X

qðxÞ/21ðxÞdx¼1 such that Z

X

/001ðxÞ2w/01ðxÞ2

h i

dx¼

l

<1:

Therefore, by the condition (D2) and Fatou’s lemma, we have

t!þ1lim Jðt/1Þ

t2 ¼1

2k/1k2klim

t!þ1

Z

R

Fðx;t/1Þ

t2/21 /21dx¼1 2 Z

X

/001ðxÞ2w/01ðxÞ2

h i

dx lim

t!þ1

Z

X

Fðx;t/1Þ t2/21 /21dx 61

2

l

1 2 Z

R

qðxÞ/21ðxÞdx¼1

l

1Þ<0:

(6)

So, ifJðt/1Þ ! 1ast! þ1, then there existse2Xkwithkekk>

q

such thatJðeÞ<0. h Next, we define

a

¼inf

c2Ck max

06t61

c

ðtÞÞ and

a

0ð Þ ¼X inf

c2Ckð ÞT max

06t61JjH2ð Þ\HX 1

0ð ÞXð

c

ðtÞÞ;

whereJjH2ð Þ\HX 10ð ÞX is a restriction ofJonH2ð Þ \X H10ð Þ,X C¼ f

c

2Cð½0;1 ;XkÞ:

c

ð0Þ ¼0;

c

ð1Þ ¼eg and

Cð Þ ¼ fT

c

2Cð½0;1 ;H2ð Þ \X H10ð ÞÞX :

c

ð0Þ ¼0;

c

ð1Þ ¼eg:

Note that JjH2ð Þ\HX 1

0ð ÞXð Þ ¼u 1 2 Z

R

u00ðxÞ2wu0ðxÞ2

h i

dx Z

R

Fðx;uÞdx;

foru2H2ð Þ \X H10ð ÞX and

a

0ð ÞX independent ofk. Moreover, if the conditions (D1)–(D4) hold, then by the proofs ofLemmas 2.1 and 3.1, we can conclude that JjH2ð Þ\HX 10ð ÞX satisfies the mountain pass hypothesis as in Theorem 2.1. Since

H2ð Þ \X H10ð ÞX

Xkfor allk>0, we have 0<

g

6

a

6

a

0ð ÞX for allkP 1

cS21jfa<cgj. TakeD0>

a

0ð Þ. Thus,T 0<

g

6

a

k6

a

0ð ÞX <D0for allkP 1

cS21jfa<cgj: ð3:3Þ

FromLemmas 2.1 and 3.1andTheorem 2.1, we obtain that for eachkP 1

cS21jfa<cgj, there existsfung Xksuch that JðunÞ !

a

>0 and ð1þ kunkkÞkJ0ðunÞkX1

k !0; asn! 1; ð3:4Þ

where 0<

g

6

a

6

a

0ð ÞX <D0. Furthermore, we have the following results.

Lemma 3.3.Suppose that the conditions (V1)–(V4) and (D1)–(D3) hold. Then fungdefined by(3.4)is bounded in Xk for all kP 1

cS21jfb<cgj.

Proof. Fornlarge enough, byðD3Þ, the Hölder inequality and Lemmas2.1 and 3.1, one has

a

þ1PJ uð Þ n 1

hhJ0ðunÞ;uni ¼ 1 21

h

kunk2k Z

R

Fðx;unÞ 1 hfðx;unÞ

dxPh2

2h kunk2kd0

Z

R

u2ndx

P h2 2h d0

H0

kunk2k;

which implies thatfungis bounded inXk. h

Proposition 3.4. Suppose that the conditions (V1)–(V4) and (D1)–(D4) hold. Let D0>0 be as in (3.3). Then there exists K¼KðD0ÞP 1

cS21jfb<cgjsuch that J satisfies theðCÞa–condition in Xkfor all

a

<D0andk>K.

Proof. Letfungbe aðCÞa–sequence with

a

<D0. ByLemma 3.3, there exist a subsequencefungandu0inXksuch that un*u0weakly inXk;

un!u0strongly inLrlocð Þ;R for 26r<1: ð3:5Þ

Now we prove thatun!u0strongly inXk. Let

v

n¼unu0. Then by the conditions (D1)–(D4) and Brezis–Lieb Lemma[2], we have

Jð

v

nÞ ¼J uð Þ n J uð Þ þ0 oð Þ1 andJ0ð

v

nÞ ¼oð Þ:1

It follows from (V2) and(3.5)that Z

R

v

2nðxÞdx¼ Z

aPc

f g

v

2nðxÞdxþ Z

a<c

f g

v

2nðxÞdx6 1 kc

Z

aPc

f g

kaðxÞ

v

2nðxÞdxþoð Þ1 6 1

kck

v

nk2kþoð Þ:1 ð3:6Þ

(7)

Then, by the Sobolev inequality and(2.2), we have Z

R

v

nðxÞ

j jrdx6j

v

njr21 Z

R

v

nðxÞ2dx6Sr21

kc k

v

nkr2H2k

v

nk2kþoð Þ1 6Sr21 kc

1 c0S21jfa<cgj

!r22

v

n

k krkþoð Þ1: ð3:7Þ

By the conditions (D1)–(D3) and Brezis–Lieb Lemma[2], we have Jð

v

nÞ ¼J uð Þ n J uð Þ þ0 oð Þ1 andJ0ð

v

nÞ ¼oð Þ1:

Consequently, this together with the condition (D3),Lemma 2.2 and (2.3), we obtain D0>

a

J uð Þ0 PJð

v

nÞ 1

h J0ð

v

nÞ;

v

n

þoð Þ1 P h2 2h d0

H0

v

n

k k2kþoð Þ;1

which implies that

v

n

k k2k6 2hH0D0

H0ðh2Þ 2hd0

þoð Þ:1 Moreover, by(2.4), one has

Z

R

v

nðxÞ

j jrdx6 cr202 a<c

f g

j jr22Hr20k

v

nkrk6 1 a<c

f g

j jr22

2hH0D0

H0ðh2Þ 2hd0

2r

þoð Þ1: ð3:8Þ

Since J0ð

v

nÞ;

v

n

¼oð Þ1 and Z

R

f x;ð

v

nÞ

v

ndx6jpþj1þ

Z

R

v

nðxÞ2dxþC Z

R

v

nðxÞ

j jrdx; ð3:9Þ

it follows from(3.6) and (3.8) and (3.9)that oð Þ ¼1 k

v

nk2k

Z

R

fðx;

v

nÞ

v

ndxPk

v

nk2kjpþj1þ

Z

R

v

2nðxÞdxC Z

R

v

nðxÞ j jrdx

Pk

v

nk2kjpþj1þ

kc k

v

nk2kC Z

RN

v

n

j jrdx

ðr2Þ=r Z

RN

v

n

j jrdx

2=r

Pk

v

nk2k 1jpþj1þ

kc 2hH0D0

H0ðh2Þ 2hd0

ð Þjfa<cgjr2r

!r22

Sr21 kc

1 c0S21jfa<cgj

!r22

2 4

3 5 8 2=r

><

>:

9>

=

>;: Thus, there existsK¼KðD0ÞPmax 1c;cS2 1

1jfa<cgj

n o

such that

v

n!0 strongly inXkfork>K. This completes the proof.

h

Now we give the proof ofTheorem 1.1: ByProposition 3.4and 0<

g

6

a

6

a

0ð ÞX for allkP 1

cS21jfa<cgj, for eachD0>

a

0ð ÞX there exists

KPmax 1

c; 1

cS21jfa<cgj

( )

>0

such that for everyk>KandðCÞa–sequencefungforJonXkthere exist a subsequencefunganduk2Xksuch thatun!uk

strongly inXk. Moreover,J uð Þ ¼k

a

andukis a nontrivial homoclinic solution of Eq.(1.1).

Now we give the proof ofTheorem 1.2:Letu02H2ð ÞR be a nontrivial homoclinic solution of Eq.(1.1). Then by(2.2), for kP1cwe have

Z

R

u000ðxÞ2wu00ðxÞ2þkaðxÞuðxÞ20

h i

dx¼ Z

R

fðx;u0Þu0dx6 Z

R

qu20dx6 1

l

0k ku0

2 H2

6 1

l

0c0S21jfa<cgj Z

R

u000ðxÞ2wu00ðxÞ2þkaðxÞuðxÞ20

h i

dx

<

Z

R

u000ðxÞ2wu00ðxÞ2þkaðxÞuðxÞ20

h i

dx;

which is a contradiction.

Acknowledgment

T. Li was supported by the NSFC (Grand No. 11471074, No. 91330109) and the Fundamental Research Funds for the Central Universities. J. Sun was supported by the NSFC (Grant No. 11201270, No. 11271372), Shandong Natural Science

(8)

Foundation (Grant No. ZR2012AQ010), and Young Teacher Support Program of Shandong University of Technology. T. F. Wu was supported by the National Science Council, Taiwan.

Appendix A

Consider the minimum problem

l

¼inf Z

X

u00ðxÞ2wu0ðxÞ2

h i

dxju2H2ðXÞ \H10ðXÞ; Z

X

qu2dx¼1

: ð4:1Þ

Then we have the following result.

Lemma 4.1.There exist a constant c1>0and/12H2ðXÞ \H10ðXÞwithR

Xq/21dx¼1such that

l

¼ Z

X

/001ðxÞ2w/01ðxÞ2

h i

dxPc1;

i.e., the minimum problem(4.1)is achieved.

Proof. For anyu2H2ðXÞ \H10ðXÞwithR

Xqu2dx¼1, byLemma 2.1and Sobolev embedded theorem, we have Z

X

u00ðxÞ2wu0ðxÞ2

h i

dx¼ Z

R

u00ðxÞ2wu0ðxÞ2þaðxÞuðxÞ2

h i

dxPc0kuk2H2Pc0S22 Z

X

u2dxPc0S22 jqj1>0:

Therefore,

l

Pcjqj0S22

1>0. Letfung H2ðXÞ \H10ðXÞbe a minimizing sequence of(4.1). Clearly,R

Xqu2ndx¼1 andfungis bounded. Then by the compact imbedding theorem, there exist a subsequence fung and /12H2ðXÞ \H10ðXÞsuch that un*/1weakly inH2ðXÞ \H10ðXÞandun!/1strongly inL2ðRÞ. So it is easy to verify thatR

Xqu2ndx!R

Xq/21dxasn! 1 andR

Xq/21dx¼1. Therefore,

l

6Z

X

/001ðxÞ2w/01ðxÞ2

h i

dx6lim inf

n!1

Z

X

u00nðxÞ2wu0nðxÞ2

h i

dx¼

l

; which implies thatR

Xh/001ðxÞ2w/01ðxÞ2i

dx¼

l

. This completes the proof. h

References

[1]C.J. Amick, J.F. Toland, Homoclinic orbits in the dynamic phase space analogy of an elastic strut, Eur. J. Appl. Math. 3 (1991) 97–114.

[2]H. Brezis, E.H. Lieb, A relation between pointwise convergence of functions and convergence functionals, Proc. Am. Math. Soc. 8 (1983) 486–490.

[3]B. Buffoni, Periodic and homoclinic orbits for Lorentz–Lagrangian systems via variational method, Nonlinear Anal. 26 (1996) 443–462.

[4]Y. Chen, P. Mckenna, Travelling waves in a nonlinearly suspended beam: theoretical results and numerical observations, J. Diff. Equ. 136 (1997) 325–

355.

[5]P. Coullet, C. Elphick, D. Repaux, Nature of spatial chaos, Phys. Rev. Lett. 58 (1987) 431–434.

[6]G.T. Dee, W. van Saarloos, Bistable systems with propagating fronts leading to pattern formation, Phys. Rev. Lett. 60 (1988) 2641–2644.

[7]I. Ekeland, Convexity Methods in Hamiltonian Mechanics, Springer, 1990.

[8]J. Lega, J. Moloney, A. Newell, Swift–Hohenberg for lasers, Phys. Rev. Lett. 73 (1994) 2978–2981.

[9]C. Li, Remarks on homoclinic solutions for semilinear fourth-order ordinary differential equations without periodicity, Appl. Math. J. Chin. Univ. 24 (2009) 49–55.

[10]L.A. Peletier, W.C. Troy, Spatial Patterns: Higher Order Models in Physics and Mechanics, Birkhauser, Boston, 2001.

[11]D. Smets, J.B. van den Berg, Homoclinic solutions for Swift–Hohenberg and suspension bridge type equations, J. Diff. Equ. 184 (2002) 78–96.

[12]J. Sun, T.F. Wu, Two homoclinic solutions for a nonperiodic fourth order differential equation with a perturbation, J. Math. Anal. Appl. 413 (2014) 622–

632.

[13]J.B. Swift, P.C. Hohenberg, Hydrodynamic fluctuations at the convective instability, Phys. Rev. A 15 (1977) 319–328.

[14]S. Tersian, J. Chaparova, Periodic and homoclinic solutions of extended Fisher–Kolmogorov equations, J. Math. Anal. Appl. 260 (2001) 490–506.

[15]Y.L. Yeun, Heteroclinic solutions for the extended Fisher–Kolmogorov equations, J. Math. Anal. Appl. 407 (2013) 119–129.

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