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Electronic Journal of Qualitative Theory of Differential Equations 2009, No.40, 1-13;http://www.math.u-szeged.hu/ejqtde/

Positive solutions for a multi-point eigenvalue problem involving the one dimensional

p-Laplacian ∗†

Youyu Wang1 Weigao Ge2 Sui Sun Cheng3

1. Department of Mathematics, Tianjin University of Finance and Economics, Tianjin 300222, P. R. China

2. Department of Mathematics, Beijing Institute of Technology, Beijing 100081, P. R. China

3. Department of Mathematics, Tsing Hua University, Hsinchu, Taiwan 30043.

AbstractA multi-point boundary value problem involving the one dimensionalp-Laplacian and depending on a parameter is studied in this paper and existence of positive solutions is established by means of a fixed point theorem for operators defined on Banach spaces with cones.

KeywordsPositive solutions; Boundary value problems; One-dimensionalp-Laplacian

1. Introduction

In this paper we study the existence of positive solutions to the boundary value problem (BVP) for the one-dimensionalp-Laplacian

p(u0))0+λq(t)f(t, u) = 0, t∈(0,1), (1.1) u0(0) =

n−2X

i=1

αiu0i), u(1) =

n−2X

i=1

βiu(ξi), (1.2)

whereφp(s) =|s|p−2s,p >1,ξi∈(0,1) with 0< ξ1< ξ2<· · ·< ξn−2<1 andαi, βi, f satisfy (H1i, βi∈[0,∞) satisfy 0<

n−2P

i=1

αi<1, and

n−2P

i=1

βi<1;

(H2)f ∈C([0,1]×[0,∞),[0,∞));

This work is sponsored by the National Natural Science Foundation of China (No. 10671012).

2000 Mathematics Subject Classification 34B10, 34B15

Email: wangyouyu@163.com

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(H3) q(t)∈C(0,1)∩L1[0,1] withq >0 on (0,1). The numberλ is regarded as a parameter and is to be determined among positive numbers.

The study of multipoint boundary value problems for linear second-order ordinary differential equations was initiated by Il’in and Moiseev [1,2]. Since then there has been much current attention focused on the study of nonlinear multipoint boundary value problems, see [3,4,5,7]. The meth- ods include the Leray-Schauder continuation theorem, nonlinear alternatives of Leray-Schauder, coincidence degree theory, and fixed point theorem in cones. For example,

In [6], R. Ma and N. Castaneda studied the following BVP







x00(t) +a(t)f(x(t)) = 0, 0≤t≤1, x0(0) =

m−2P

i=1

αix0i), x(1) =

m−2P

i=1

βix(ξi), where 0< ξ1<· · ·< ξm−2 <1,αi, βi ≥0 with 0<Pm

i=1αi <1 andPm

i=1βi<1. They showed the existence of at least one positive solution iff is either superlinear or sublinear by applying the fixed point theorem in cones.

The authors in [7] considered the multi-point BVP for one dimensionalp-Laplacian (φp(u0))0+f(t, u) = 0, t∈(0,1),

φp(u0(0)) =

n−2X

i=1

αiφp(u0i)), u(1) =

n−2X

i=1

βiu(ξi).

Using a fixed point theorem in a cone, we provided sufficient conditions for the existence of multiple positive solutions to the above BVP.

In paper [8], we investigated the following more general multi-point BVPs (φp(u0))0+q(t)f(t, u, u0) = 0, t∈(0,1),

u(0) =

n−2X

i=1

αiu(ξi), u0(1) =

n−2X

i=1

βiu0i),

u0(0) =

n−2X

i=1

αiu0i), u(1) =

n−2X

i=1

βiu(ξi).

The main tool is a fixed point theorem due to Avery and Peterson[9], we provided sufficient conditions for the existence of multiple positive solutions.

In view of the common concern about multi-point boundary value problems as exhibited in [6,7,8] and their references, it is of interests to continue the investigation and study the problem (1.1) and (1.2).

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Motivated by the works of [7] and [8], the aim of this paper is to show the existence of positive solutionsu to BVP(1.1) and (1.2). For this purpose, we consider the Banach space E =C[0,1]

with the maximum norm kxk= max

0≤t≤1|x(t)|. By a positive solution of (1.1) and (1.2), we means a function u∈ C1[0,1],(φp(u0))0(t)∈ C(0,1)∩L[0,1] which is positive on [0,1] and satisfies the differential equation (1.1) and the boundary conditions (1.2).

Our main results will depend on the following Guo-Krasnoselskii fixed-point theorem . Theorem A[10][11].LetE be a Banach space and letK⊂Ebe a cone inE. Assume Ω1,Ω2

are open subsets ofE with 0∈Ω1,Ω1⊂Ω2, and let

T :K∩(Ω2\Ω1)→K

be a completely continuous operator such that either

(i)kT xk ≤ kxk, x∈K∩∂Ω1 andkT xk ≥ kxk, x∈K∩∂Ω2, or (ii)kT xk ≥ kxk, x∈K∩∂Ω1 andkT xk ≤ kxk, x∈K∩∂Ω2. ThenT has a fixed point inK∩(Ω2\Ω1).

In section 3, we shall present some sufficient conditions withλbelonging to an open interval to ensure the existence of positive solutions to problems (1.1) and (1.2). To the author’s knowledge, no one has studied the existence of positive solutions for problems (1.1) and (1.2) using the Guo- Krasnoselskii fixed-point theorem.

2. The preliminary lemmas

Let

C+[0,1] ={ω∈C[0,1] :ω(t)≥0, t∈[0,1]}.

Lemma 2.1Let (H1)−(H3) hold. Then forx∈C+[0,1], the problem

p(u0))0+λq(t)f(t, x(t)) = 0, t∈(0,1), (2.1)

u0(0) =

n−2X

i=1

αiu0i), u(1) =

n−2X

i=1

βiu(ξi), (2.2)

has a unique solution

u(t) =Bx− Z 1

t

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds, (2.3)

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whereAx, Bxsatisfy

φ−1p (Ax) =

n−2X

i=1

αiφ−1p Ax−λ Z ξi

0

q(s)f(s, x(s))ds

!

, (2.4)

Bx=− 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds.

Lemma 2.2 Supposeβi, ri≥0 (i= 1,2,· · ·, n−2) andPn−2

i=1 βi<1, denoter= min

1≤i≤n−2ri, R= max

1≤i≤n−2ri, then there exists a unique x∈

 φ−1p Pn−2 i=1 βi

1−φ−1p Pn−2

i=1 βi

r,

φ−1p Pn−2 i=1 βi

1−φ−1p Pn−2

i=1 βi

R

such that

φp(x) =

n−2X

i=1

βiφp(x+ri).

Proof. Define

H(x) =φp(x)−

n−2X

i=1

βiφp(x+ri).

Then,H(x)∈C((−∞,+∞), R).

Let

x=

φ−1p Pn−2 i=1 βi

1−φ−1p Pn−2

i=1 βi

·r, x=

φ−1p Pn−2 i=1 βi

1−φ−1p Pn−2

i=1 βi

·R, then we have

H(x) = φp(x)−

n−2X

i=1

βiφp(x+ri)

≤ φp(x)−

n−2X

i=1

βiφp(x+r)

= φp(x)−φp

"

φ−1p

n−2X

i=1

βi

! (x+r)

#

= φp(x)−φp(x) = 0, and

H(x) = φp(x)−

n−2X

i=1

βiφp(x+ri)

≥ φp(x)−

n−2X

i=1

βiφp(x+R)

= φp(x)−φp

"

φ−1p

n−2X

i=1

βi

!

(x+R)

#

= φp(x)−φp(x) = 0.

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The zero point theorem guarantees that there exists anx0∈[x, x] such thatH(x0) = 0.

If there exist two constantsx1, x2∈[x, x] satisfyingH(x1) =H(x2) = 0, then Case 1. x1= 0.

i.e., H(0) = 0,

n−2P

i=1

βiφp(ri) = 0. So, βiφp(ri) = 0, (i = 1,2,· · ·, n−2), then, riφ−1pi) = 0, (i= 1,2,· · ·, n−2).Therefore,

H(x) = φp(x)−

n−2X

i=1

βiφp(x+ri)

= φp(x)−

n−2X

i=1

φp φ−1pi)x+φ−1pi)ri

= φp(x)−

n−2X

i=1

βiφp(x) = 1−

n−2X

i=1

βi

! φp(x).

Obviously, there exists a uniquex= 0 satisfyingH(x) = 0.So,x1=x2= 0.

Case 2. x16= 0.

(i) Ifx1∈(−∞,0), then

H(x1) = φp(x1)−

n−2X

i=1

βiφp(x1+ri)

≤ φp(x1)−

n−2X

i=1

βiφp(x1)

= 1−

n−2X

i=1

βi

!

φp(x1)<0.

So, when,x1∈(−∞,0), H(x1)6= 0.

(ii) Ifx1∈(0,+∞), then

H(x1) = φp(x1)−

n−2X

i=1

βiφp(x1+ri)

= φp(x1)

"

1−

n−2X

i=1

βiφp

1 + ri

x1

#

= φp(x1)He(x1), where

He(x) = 1−

n−2X

i=1

βiφp

1 + ri

x

.

As H(x1) = 0 and x1 6= 0, so there must existi0 ∈ {1,2,· · ·, n−2}, such that βi0φp(ri0) >0.

Thus, we getHe(x) is strictly increasing on (0,+∞).

IfH(x1) =H(x2) = 0, thenHe(x1) =H(xe 2) = 0. So,x1=x2 sinceH(x) is strictly increasinge on (0,+∞).

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Therefore,H(x) = 0 has a unique solution on (0,+∞). Combining case 1, case 2, we obtain H(x) = 0 has a unique solution on (−∞,+∞) andx∈[x, x].

Lemma 2.3 Let k =

φpPn−2 i=1 αi

1−φpPn−2

i=1 αi

, then there exists a unique real number Ax that

satisfies (2.4). Furthermore,Axis contained in the interval

−λk Z 1

0

q(s)f(s, x(s))ds,0

. Proof The equation is equivalent to

φ−1p (−Ax) =

n−2X

i=1

αiφ−1p −Ax+λ Z ξi

0

q(s)f(s, x(s))ds

! .

By Lemma 2.2, we can easily obtain

−Ax

"

λk Z ξ1

0

q(s)f(s, x(s))ds, λk Z ξn2

0

q(s)f(s, x(s))ds

#

0, λk Z 1

0

q(s)f(s, x(s))ds

.

So the conclusion is obvious.

Lemma 2.4 Let (H1)−(H3) hold. If x∈ C+[0,1] andλ > 0, then the unique solution of problem (2.1)-(2.2) satisfiesu(t)≥0 fort∈[0,1].

Proof: According to Lemmas 2.1 and 2.3, we first have

u(1) = Bx

= − 1

1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

= 1

1−n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ 1

1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ 0, and

u(0) = Bx− Z 1

0

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

= u(1) + Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ u(1) + Z 1

0

φ−1p

λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ 0.

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Ift∈(0,1), we have

u(t) = Bx− Z 1

t

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

= u(1) + Z 1

t

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ u(1) + Z 1

t

φ−1p

λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ 0.

Sou(t)≥0, t∈[0,1].

Lemma 2.5 Let (H1)−(H3) hold. If x∈ C+[0,1] andλ > 0, then the unique solution of problem (2.1)-(2.2) satisfies

t∈[0,1]min u(t)≥γkuk, where

γ= Pn−2

i=1 βi(1−ξi) 1−Pn−2

i=1 βiξi

. Proof: Clearlyu0(t) =φ−1p

Ax−λRt

0q(s)f(s, x(s))ds

=−φ−1p

−Ax+λRt

0q(s)f(s, x(s))ds

≤ 0. This implies that

kuk=u(0) and min

t∈[0,1]u(t) =u(1).

Furthermore, it is easy to see thatu0(t2)≤u0(t1) for anyt1, t2∈[0,1] witht1≤t2. Henceu0(t) is a decreasing function on [0,1]. This means that the graph of u0(t) is concave down on (0,1). For eachi∈ {1,2,· · ·, n−2} we have

u(ξi)−u(1) 1−ξi

≥ u(0)−u(1)

1 ,

i.e.,

u(ξi)−ξiu(1)≥(1−ξi)u(0) so that

n−2X

i=1

βiu(ξi)−

n−2X

i=1

βiξiu(1)≥

n−2X

i=1

βi(1−ξi)u(0)

and, by means of the boundary conditionu(1) =

n−2P

i=1

βiu(ξi), we have

u(1)≥ Pn−2

i=1 βi(1−ξi) 1−Pn−2

i=1 βiξi

u(0).

This completes the proof.

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Now we define

K={ω|ω∈C+[0,1], min

0≤t≤1ω(t)≥γkωk},

whereγ is defined in Lemma 2.5. For anyλ >0,define operatorTλ:C+[0,1]→Kby

(Tλx)(t) = − 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

− Z 1

t

φ−1p

Ax−λ Z s

0

q(τ)f(τ, x(τ))dτ

ds. (2.5)

By Lemmas 2.1 and 2.3, we knowTλxis well defined. Furthermore, we have the following result.

Lemma 2.6[Lemma 2.4, 7] T:K→K is completely continuous.

Let

minf:= lim

x→∞inf min

t∈[0,1]

f(t, x)

φp(x), maxf0:= lim

x→0+sup max

t∈[0,1]

f(t, x) φp(x), minf0:= lim

x→0+inf min

t∈[0,1]

f(t, x)

φp(x), maxf:= lim

x→∞sup max

t∈[0,1]

f(t, x) φp(x). 3. Main results

We now give our results on the existence of positive solutions of BVP(1.1) and (1.2).

Theorem 3.1Let (H1)−(H3) hold and minf>0,maxf0<∞. If 1

γp−1minf·Np−1 < λ < 1

(k+ 1) maxf0·Mp−1. (3.1) where

M = 1−Pn−2 i=1 βiξi

1−Pn−2 i=1 βi

·φ−1p Z 1

0

q(s)ds

,

N = 1

1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p Z s

0

q(τ)dτ

ds+ Z 1

0

φ−1p Z s

0

q(τ)dτ

ds,

then the problem (1.1)(1.2) has at least one positive solution.

Proof. Define the operatorTλ as (2.5). Under the condition (3.1), there exists anε >0 such that

1

γp−1(minf−ε)·Np−1 ≤λ≤ 1

(k+ 1)(maxf0+ε)·Mp−1. (3.2) (i). Since maxf0<∞, there exists anH1>0 such that forx: 0≤x≤H1,

f(t, x)≤(maxf0+ε)φp(x). (3.3)

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Let Ω1={x∈E:kxk< H1}, then forx∈K∩∂Ω1, we have

−Ax+λ Z s

0

q(s)f(s, x(s))ds ≤ λk Z 1

0

q(s)f(s, x(s))ds+λ Z s

0

q(s)f(s, x(s))ds

≤ λ(k+ 1) Z 1

0

q(s)f(s, x(s))ds

≤ λ(k+ 1)(maxf0+ε) Z 1

0

q(s)φp(x(s))ds

≤ λ(k+ 1)(maxf0+ε)φp(kxk) Z 1

0

q(s)ds.

So,

φ−1p

−Ax+λ Z s

0

q(s)f(s, x(s))ds

≤[λ(k+ 1)(maxf0+ε)]q−1φ−1p Z 1

0

q(s)ds

kxk.

Therefore,

kTλxk= (Tλx)(0) = 1 1−n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

+ Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≤ 1−Pn−2 i=1 βiξi

1−Pn−2 i=1 βi

[λ(k+ 1)(maxf0+ε)]q−1φ−1p Z 1

0

q(s)ds

kxk

= M[λ(k+ 1)(maxf0+ε)]q−1kxk

≤ kxk.

ThuskTλxk ≤ kxk.

(ii). Next, since minf>0, there exists anH2>0 such that forx > H2,

f(t, x)≥(minf−ε)φp(x). (3.4)

TakeH2= max{H2,2H1}and Ω2={x∈E:kxk< H2}. Then forx∈K∩∂Ω2, we have

−Ax+λ Z s

0

q(τ)f(s, x(τ))dτ ≥ λ Z s

0

q(τ)f(τ, x(τ))dτ

≥ λ(minf−ε) Z s

0

q(τ)φp(x(τ))dτ

≥ λφp(γ)(minf−ε)φp(kxk) Z s

0

q(τ)dτ.

So,

φ−1p

−Ax+λ Z s

0

q(s)f(s, x(s))ds

≥[λ(minf−ε)]q−1φ−1p Z s

0

q(τ)dτ

γkxk.

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Therefore,

kTλxk= (Tλx)(0) = 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

+ Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ [λ(minf−ε)]q−1γkxk 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p Z s

0

q(τ)dτ

ds

+ [λ(minf−ε)]q−1γkxk Z 1

0

φ−1p Z s

0

q(τ)dτ

ds

= N[λ(minf−ε)]q−1γkxk

≥ kxk.

SokTλxk ≥ kxk.

Therefore, by the first part of Theorem A,Tλ has a fixed pointx ∈K∩(Ω2\Ω1) such that H1≤ kxk ≤H2. It is easily checked thatx(t) is a positive solution of problems (1.1) and (1.2).

The proof is complete.

Theorem 3.2. Let (H1)−(H3) hold and minf0>0,maxf<∞. If 1

γp−1minf0·Np−1 < λ < 1

(k+ 1) maxf·Mp−1. (3.5) then the problem (1.1)(1.2) has at least one positive solution.

Proof. Under the condition (3.5), there exists anε >0 such that 1

γp−1(minf0−ε)·Np−1 ≤λ≤ 1

(k+ 1)(maxf+ε)·Mp−1. (3.6) (i). Since minf0>0, there exists anH1>0 such that forx: 0≤x≤H1,

f(t, x)≥(minf0−ε)φp(x). (3.7)

Let Ω1={x∈E:kxk< H1}, then forx∈K∩∂Ω1, we have

−Ax+λ Z s

0

q(τ)f(s, x(τ))dτ ≥ λ Z s

0

q(τ)f(τ, x(τ))dτ

≥ λ(minf0−ε) Z s

0

q(τ)φp(x(τ))dτ

≥ λφp(γ)(minf0−ε)φp(kxk) Z s

0

q(τ)dτ.

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So,

φ−1p

−Ax+λ Z s

0

q(s)f(s, x(s))ds

≥[λ(minf0−ε)]q−1φ−1p Z s

0

q(τ)dτ

γkxk.

Therefore,

kTλxk= (Tλx)(0) = 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

+ Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≥ [λ(minf0−ε)]q−1γkxk 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p Z s

0

q(τ)dτ

ds

+ [λ(minf0−ε)]q−1γkxk Z 1

0

φ−1p Z s

0

q(τ)dτ

ds

= N[λ(minf0−ε)]q−1γkxk

≥ kxk.

SokTλxk ≥ kxk.

(ii). Since maxf<∞, there exists anH2>0 such that forx > H2,

f(t, x)≤(maxf+ε)φp(x). (3.8)

There are two cases : Case 1,f is bounded, and Case 2,f is unbounded.

Case 1. Suppose that f is bounded, i.e., there exists N > 0 such thatf(t, x)≤ φp(N) for t∈[0,1] and 0≤x <∞. Define

H2= max (

2H1,1−Pn−2 i=1 βiξi

1−Pn−2 i=1 βi

[λ(k+ 1)]q−1φ−1p Z 1

0

q(s)ds

N )

,

and Ω2={x∈E:kxk< H2}. Then forx∈K∩∂Ω2, we have

−Ax+λ Z s

0

q(s)f(s, x(s))ds ≤ λk Z 1

0

q(s)f(s, x(s))ds+λ Z s

0

q(s)f(s, x(s))ds

≤ λ(k+ 1) Z 1

0

q(s)f(s, x(s))ds

≤ λ(k+ 1)φp(N) Z 1

0

q(s)ds.

So,

φ−1p

−Ax+λ Z s

0

q(s)f(s, x(s))ds

≤[λ(k+ 1)]q−1φ−1p Z 1

0

q(s)ds

N.

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Therefore,

kTλxk= (Tλx)(0) = 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

+ Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≤ 1−Pn−2 i=1 βiξi

1−Pn−2 i=1 βi

[λ(k+ 1)]q−1φ−1p Z 1

0

q(s)ds

N

≤ H2=kxk.

Case 2. We choose H2 > max{2H1, H2} such that f(t, x) ≤ f(t, H2) for t ∈ [0,1] and 0< x < H2. Let Ω2={x∈E:kxk< H2}. Then forx∈K∩∂Ω2, we have

−Ax+λ Z s

0

q(s)f(s, x(s))ds ≤ λk Z 1

0

q(s)f(s, x(s))ds+λ Z s

0

q(s)f(s, x(s))ds

≤ λ(k+ 1) Z 1

0

q(s)f(s, x(s))ds

≤ λ(k+ 1) Z 1

0

q(s)f(s, H2)ds

≤ λ(k+ 1)(maxf+ε)φp(H2) Z 1

0

q(s)ds.

So,

φ−1p

−Ax+λ Z s

0

q(s)f(s, x(s))ds

≤[λ(k+ 1)(maxf+ε)]q−1φ−1p Z 1

0

q(s)ds

H2.

Therefore,

kTλxk= (Tλx)(0) = 1 1−

n−2P

i=1

βi n−2X

i=1

βi

Z 1 ξi

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

+ Z 1

0

φ−1p

−Ax+λ Z s

0

q(τ)f(τ, x(τ))dτ

ds

≤ 1−Pn−2 i=1 βiξi

1−Pn−2 i=1 βi

[λ(k+ 1)(maxf+ε)]q−1φ−1p Z 1

0

q(s)ds

H2

= M[λ(k+ 1)(maxf+ε)]q−1H2

≤ H2=kxk.

Therefore, by the second part of Theorem A,Tλhas a fixed pointx∈K∩(Ω2\Ω1) such that H1≤ kxk ≤H2. It is easily checked thatx(t) is a positive solution of problems (1.1) and (1.2).

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REFERENCES

1. V. A. Il’in, E. I. Moiseev, Nonlocal boundary value problem of the first kind for a Sturm-Liouville operator in its differential and finite difference aspects, Differential Equations, 23 (1987) 803-810.

2. V. A. Il’in, E. I. Moiseev, Nonlocal boundary value problem of the second kind for a Sturm-Liouville operator, Differential Equations, 23 (1987) 979-987.

3. W. Feng, On an m-point boundary value problem, Nonlinear Anal. 30 (1997) 5369-5374.

4. W. Feng, J. R. L. Webb, Solvability of m-point boundary value problem with nonlinear growth, J.

Math. Anal. Appl. 212 (1997) 467-480.

5. C. P. Gupta, A generalized multi-point boundary value problem for second order ordinary differential equations, Appl. Math. Comput. 89 (1998) 133-146.

6. R. Ma and N. Castaneda, Existence of solutions of nonlinear m-point boundary-value problems, J.

Math. Anal. Appl. 256 (2001) 556-567.

7. Y. Wang and C. Hou, Existence of multiple positive solutions for one dimensionalp-Laplacian, J.

Math. Anal. Appl. 315 (2006) 144-153.

8. Y. Wang and W. Ge, Multiple positive solutions for multi-point boundary value problem with one dimensionalp-Laplacian, J. Math. Anal. Appl. 327 (2007) 1381-1395.

9. R. I. Avery, A. C. Peterson, Three positive fixed points of nonlinear operators on ordered Banach spaces, Comput. Math. Appl. 42 (2001) 313-322.

10. D. Guo and V. Lakshmikantham, Nonlinear Problems in Abstract Cones, Academic Press, New York, (1988).

11. M.A. Krasnosel’skii, Positive Solutions of Operator Equations, Noordhoff, Gronignen, (1964).

(Received February 14, 2009)

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