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Volume 2011, Article ID 308362,11pages doi:10.1155/2011/308362

Research Article

Solvability of a Class of Generalized Neumann Boundary Value Problems for

Second-Order Nonlinear Difference Equations

Jianye Xia

1

and Yuji Liu

2

1Department of Applied Mathematics, Guangdong University of Finance, Guangzhou 510000, China

2Department of Mathematics, Guangdong University of Business Studies, Guangzhou 510000, China

Correspondence should be addressed to Jianye Xia,jianye [email protected] Received 18 April 2011; Accepted 17 June 2011

Academic Editor: Hassan A. El-Morshedy

Copyrightq2011 J. Xia and Y. Liu. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

This paper is motivated by Rachnkovab and Tisdell2006and Anderson et al.2007. New suf- ficient conditions for the existence of at least one solution of the generalized Neumann boundary value problems for second order nonlinear difference equations∇Δxk fk, xk, xk1, k∈1, n−1,x0 ax1,xn bxn−1, are established.

1. Introduction

Recently, there have been many papers discussed the solvability of two-point or multipoint boundary value problems for second-order or higher-order difference equations, we refer the readers to the text books1,2 and papers3–8 and the references therein.

In a recent paper3 , Anderson et al. studied the following problem:

∇Δyk f

k, yk,Δyk

, k1, . . . , n−1,

Δy0 Δyn 0, 1.1

(2)

where

Δyk

⎧⎨

yk1−yk, fork0, . . . , n−1,

0, forkn,

∇Δyk

⎧⎨

yk1−2yk yk−1, fork1, . . . , n−1,

0, fork0 orn.

1.2

The following result was proved.

Theorem ART

Suppose thatfis continuous and there exist constantsα≤0,K≥0 such that f

t, p, q

pα 2pf

t, p, q

q2 K, t, p, q

∈ {1, . . . , n−1} ×R2.

Then BVP1.1has at least one solution.

The methods in3 involved new inequalities on the right-hand side of the difference equation and Schaefer’s Theorem in the finite-dimensional space setting.

In7 , the following discrete boundary value problemBVPinvolving second order difference equations and two-point boundary conditions

∇Δyk

h2 f

tk, yk,Δyk

h

, k1, . . . , n−1, y00, yn0,

1.3

was studied, wheren ≥ 2 an integer,f is continuous, scalar-valued function, the step size ish N/nwith N a positive constant, the grid points aretk kh for k 0, . . . , n. The differences are given by

Δyk

⎧⎨

yk1yk, k0, . . . , n−1,

0, kn,

∇Δyk

⎧⎨

yk1−2ykyk−1, k1, . . . , n−1,

0, k0 orkn.

1.4

The following two results were proved in7 .

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Theorem RT

Letf be continuous on0, N ×R2andα, β, and,Kbe nonnegative constants. If there exist c, d∈0,1such that

ft, u, vα|u|cβ|v|dK, t, u, v∈0, N ×R2, 1.5

then the discrete BVP1.3has at least one solution.

Theorem RT

Letfbe continuous on0, N ×R2andα, β, andKnonnegative constants. If

ft, u, vα|u|β|v|K, t, u, v∈0, N ×R2, 1.6 αN2

8 βN

2 <1, 1.7

then the discrete BVP1.3has at least one solution.

In paper8 , Cabada and Otero-Espinar studied the existence of solutions of a class of nonlinear second-order difference problem with Neumann boundary conditions by using upper and lower solution methods. Assuming the existence of a pair of ordered lower and upper solutionsγandβ, they obtained optimal existence results for the caseγβand even forγβ.

In this paper, we study the following boundary value problem for second-order nonlinear difference equation

∇Δxk fk, xk, xk1, k∈1, n−1 ,

x0 ax1, xn bxn−1, 1.8

wherea, bR,n≥2 is an integer, andfis continuous, scalar-valued function. We note that whenab1, BVP1.8becomes the following BVP:

∇Δxk fk, xk, xk1, t∈1, T −1 ,

Δx0 0 Δxn−1, 1.9

which is called Neumann boundary value problem of difference equation and is a special case of BVP1.1. Whenab0, BVP1.8is changed to

∇Δxk fk, xk, xk1, t∈1, T −1 ,

x0 0xn, 1.10

which is the so-called Dirichlet problem for discrete difference equations and is a special case of BVP1.3.

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The purpose of this paper is to improve the assumptions∗,1.5, and 1.6 in the results in paper3,5,7–9 , by using Mawhin’s continuation theorem of coincidence degree, to establish sufficient conditions for the existence of at least one solution of BVP1.8. It is interesting that we allowfto be sublinear, at most linear or superlinear.

This paper is organized as follows. In Section 2, we make the main results, and in Section 3, we give some examples, which cannot be solved by theorems in5,7,9 , to illustrate the main results presented inSection 3.

2. Main Results

To get the existence results for solutions of BVP1.8, we need the following fixed point theorems.

LetX and Y be Banach spaces, L :DLXY a Fredholm operator of index zero, andP :XX,Q :YY projectors such that ImP KerL, KerQ ImL, X KerL⊕ KerP, Y ImL⊕ ImQ. It follows thatL|DL∩KerP :DL∩KerP → ImLis invertible;

we denote the inverse of that map byKp.

IfΩis an open bounded subset ofX,DL∩Ω/∅, the mapN:XY will be called L-compact onΩifQNΩis bounded andKpI−QN:Ω → Xis compact.

Lemma 2.1see9 . LetL be a Fredholm operator of index zero, and letN beL-compact on Ω.

Assume that the following conditions are satisfied:

iLx /λNxfor everyx, λ∈DL\KerL∂Ω ×0,1;

iiNx /∈ImLfor everyx∈KerL∂Ω;

iiideg∧QN|KerL,Ω∩KerL,0/0, where∧: KerLY/ImLis the isomorphism.

Then the equationLxNxhas at least one solution inDL∩Ω.

Lemma 2.2see9 . LetX andY be Banach spaces. SupposeL:DLXY is a Fredholm operator of index zero with KerL {0},N:XY isL-compact on any open bounded subset of X. If 0 ∈Ω ⊂ Xis an open bounded subset andLx /λNxfor allxDL∂Ωand λ∈ 0,1 , then there is at least onex∈Ωso thatLxNx.

LetXRn1, Y Rn−1be endowed with the norms

x max

n∈0,n |xn|, y max

k∈1,n−1 yk 2.1

forxXandyY, respectively. It is easy to see thatXandY are Banach spaces. ChooseDL {x∈ X :x0 ax1, xn bxn−1}. LetL :XY, Lxk ∇Δxk, x∈DL, and N:XY byNxk fk, xk, xk1.

Consider the following problem:

∇Δxk 0, x0 ax1, xn bxn−1. 2.2

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It is easy to see that problem2.2has a unique solutionxk 0 if and only if

1−an−1b−n /a1b. 2.3 If2.3holds, we call BVP1.8at nonresonance case. If1−an−1b−n a1b, then problem2.2has infinite nontrivial solutions. At this case, we call BVP1.8at resonance case.

In this paper, we establish sufficient conditions for the existence of solutions of BVP1.8at nonresonance case, that is,1−an−1b−n /a1b, and at resonance case, a b 1. It is similar to get existence results for the existence of solutions at resonance case when 1−an−1b−n a1banda /1, b /1.

Lemma 2.3. Supposeab1. Then the following results are valid.

iKerL{x c, . . . , c∈X:cR}.

iiImL{y∈Y :n−1

i1 yi 0}.

iiiLis a Fredholm operator of index zero.

ivThere are projectorsP :XXandQ : YY such that KerL ImP, KerQ ImL. Furthermore, letΩ⊂Xbe an open bounded subset withΩ∩DL/∅; thenNisL-compact on Ω.

vxDLis a solution ofLx Nxwhich implies thatxis a solution of BVP1.8.

The projectorsP :XX andQ :YY, the isomorphism∧ : KerLY/ImL, and the generalized inverseKp: ImLDL∩ImPare as follows:

P xn x1,

Qyn 1

n−1

n−1

i1

yi,

∧c c, Kpyn k

s1

s i1

yi.

2.4

Lemma 2.4. Suppose1−an−1b−n /a1b. Then the following results are valid.

ixDLis a solution ofLx Nxwhich implies thatxis a solution of BVP1.8.

ii KerL{0}.

iiiLis a Fredholm operator of index zero,NisL-compact on each open bounded subset ofX.

Suppose

Athere exist numbersβ >0,θ≥1, nonnegative sequencespn, qn, rn, functions gn, x, y,hn, x, ysuch thatfn, x, y gn, x, y hn, x, yand

g n, x, y

xβ|x|θ1, h

n, x, ypn|x|θqnyθrn, 2.5

for alln∈ {1, . . . , n−1}, x, y∈R2;

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Bthere exists a constantM >0 so that

c n−1

i1

fn, c, c

>0 2.6

for all|c|> Mor

c n−1

i1

fn, c, c

<0 2.7

for all|c|> M.

Theorem L

Supposea2≤1, b2≤1, and thatAandBhold. Then BVP1.8has at least one solution if pqmax

|b|θ1,1

< β. 2.8

Proof. To applyLemma 2.1, we considerLxλNxforλ∈0,1 . Step 1. LetΩ1{x∈X:LxλNx, λ∈0,1 }. Forx∈Ω1, we have

xk1−2xk xk−1 λfk, xk, xk1, k∈1, n−1 , x0 ax1,

xn bxn−1.

2.9

So

xk1−2xk xk−1 xk λfk, xk, xk1xk, k∈1, n−1 . 2.10

It is easy to see that

2

n−1

n1

xk1−2xk xk−1 xk

n−1

n1

−xk1 22xkxk1−xk 2−xk−1 22xk−1xk−xk 2

xk1 2−2xk 2 xk−1 2 n−1

n1

−xk1−xk 2−xk−1−xk 2 xk1 2−2xk 2 xk−1 2

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n−1

n1

−xk1−xk 2−xk−1−xk 2

xn 2−xn−1 2−x1 2 x0 2

n−1

n1

−xk1−xk 2−xk−1−xk 2

b2−1

xn−1 2 a2−1

x1 2 .

2.11

Sincea2≤1, b2≤1, we get

n−1

n1

xk1−2xk xk−1 xk≤0. 2.12

So, we get

λ n−1 n1

fk, xk, xk1xk≤0. 2.13

Then

n−1

n1

gk, xk, xk1 hk, xk, xk1

xk≤0. 2.14

It follows that

β

n−1

k1

|xk|θ1≤ −n−1

n1

hk, xk, xk1xk

n−1

n1

pk|xk|θ1qk|xk1|θ|xk|rk|xk|

pn−1

n1

|xk|θ1qn−1

k1

|xk1|θ|xk|n−1

k1

rk|xk|.

2.15

Forxi≥0, yi≥0, Holder’s inequality implies s

i1

xiyis

i1

xpi

1/p s

i1

yiq 1/q

, 1 p 1

q 1, q >0, p >0. 2.16

(8)

It follows that

β

n−1

k1

|xk|θ1

pn−1

n1

|xk|θ1qn−1

k1

|xk1|θ1

θ/θ1n−1

k1

|xk|θ1

1/θ1

rn−1

k1

|xk|

rn−1θ/θ1 n−1

k1

|xk|θ1

1/θ1

pn−1

n1

|xk|θ1 q

|b|θ1|x1|θ1n−2

k1

|xk1|θ1

θ/θ1n−1

k1

|xk|θ1

1/θ1

rn−1θ/θ1 n−1

k1

|xk|θ1

1/θ1

pn−1

n1

|xk|θ1 qmax

|b|θ1,1n−1

k1

|xk|θ1

θ/θ1n−1

k1

|xk|θ1

1/θ1

rn−1θ/θ1 n−1

k1

|xk|θ1

1/θ1

pn−1

n1

|xk|θ1 qmax

|b|θ1,1n−1

k1

|xk|θ1.

2.17

It follows from2.8that there exists a constantM1>0 such that

n−1

k1

|xk|θ1M1. 2.18

Hence|xk| ≤M1/n−11/θ1for allk∈ {1, . . . , n−1}. Hence||x|| ≤M1/n−11/θ1. SoΩ1is bounded.

Step 2. Prove that the setΩ2{x∈ KerL:Nx∈ ImL}is bounded.

For x ∈ KerL, we havexk c fork ∈ 0, n . Thus we have Nxk fk, c, c.

Nx, y∈ ImLimplies that

n−1

k1

fn, c, c 0. 2.19

It follows from conditionBthat|c| ≤M. ThusΩ2is bounded.

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Step 3. Prove the setΩ3{x∈ KerL:±λ∧x 1−λQNx 0, ∃λ∈0,1 }is bounded.

If the first inequality ofBholds, let

Ω3{x∈KerL:λ∧x 1−λQNx 0, ∃λ∈0,1 }. 2.20

We will prove thatΩ3 is bounded. Forxk cfork ∈ 0, n such thatx ∈ Ω3, and λ∈0,1 , we have

−1−λn−1

k1

fn, c, c λcn−1. 2.21

Ifλ1, thenc0. Ifλ /1, then

0>−1−λcn−1

k1

fn, c, c λc2T ≥0, 2.22

a contradiction.

If the second inequality ofBholds, let

Ω3{x∈KerL:−λ∧x 1−λQNx 0, ∃λ∈0,1 }. 2.23

Similarly, we can get a contradiction. SoΩ3is bounded.

Step 4. Obtain open bounded setΩsuchi,ii, andiiiofLemma 2.1.

In the following, we will show that all conditions ofLemma 2.1are satisfied. SetΩan open bounded subset ofXsuch thatΩ⊃3

i1Ωi. We know thatLis a Fredholm operator of index zero andNisL-compact onΩ. By the definition ofΩ, we haveΩ⊃Ω1andΩ⊃Ω2, thus Lx/λNxforx∈DL\KerL∂Ωandλ∈0,1;Nx/ImLforx∈ KerL∂Ω.

In fact, letHx, λ ±λ∧x 1−λQNx. According the definition ofΩ, we know Ω⊃Ω3, thusHx, λ/0 forx∂Ω∩KerL, thus by homotopy property of degree,

degQN|KerL,Ω∩KerL,0 degH·,0,Ω∩KerL,0 degH·,1,Ω∩KerL,0 deg±∧,Ω∩KerL,0/0.

2.24

Thus byLemma 2.1,Lx Nxhas at least one solution inDL∩Ω, which is a solution of BVP1.8. The proof is completed.

Theorem L

Supposea2≤1, b2≤1,1−an−1b−n /a1b, and thatAholds. Then BVP1.8has at least one solution if2.8holds.

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Proof. To applyLemma 2.2, we consider Lx λNxforλ ∈ 0,1 . LetΩ1 {x ∈ X : Lx λNx, λ ∈ 0,1 }. Forx ∈ Ω1, we get 2.9and 2.10. using the methods in the proof of Theorem LX1, we get thatΩ1 is bounded. LetΩbe a nonempty open bounded subset ofX such thatΩ⊃Ω1centered at zero. It is easy to see thatLis a Fredholm operator of index zero andNis L-compact onΩ. One can see thatLx /λNxfor allxDL∂Ωand λ∈ 0,1 . Thus, fromLemma 2.2,LxNxhas at least one solutionxDL∩Ω, soxis a solution of BVP1.8. The proof is complete.

3. An Example

In this section, we present an example to illustrate the main results inSection 2.

Example 3.1. Consider the following problem:

xk1−2xk xk−1 βxk 2m1pkxk 2m1qkxk1 2m1rk, k∈1, n−1 , x0 ax1,

xn bxn−1,

3.1

wheren≥2, m≥1 are integers andβ >0,pn, qn, rnare sequences. Corresponding to the assumptions of Theorem L1, we set

f k, x, y

βx2m1pkx2m1qky2m1rk, g

k, x, y

βx2m1, h

k, x, y

pkx2m1qky2m1rk,

3.2

andθ2m1. It is easy to see thatAholds, and

fn, c, c c2m1βpkc2m1qkc2m1rk 3.3

implies that there isM >0 such thatcn−1

i1c2m1βpkc2m1qkc2m1rk >0 for all n∈1, n−1 and|c|> M.

It follows from Theorem L2 that3.1has at least one solution ifa2 ≤1, b2 ≤ 1, 1− an−1b−n /a1band||p||||q||max{|b|θ1,1}< β. BVP3.1has at least one solution ifab1 and||p||||q||max{|b|θ1,1}< β.

Remark 3.2. It is easy to see that BVP3.1whenab0 cannot be solved by using theorems obtained in paper7 . BVP3.1whenab1 cannot be solved by the results obtained in paper3 .

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Acknowledgments

This paper is supported by Natural Science Foundation of Hunan province, China no.

06JJ5008and Natural Science Foundation of Guangdong provinceno. 7004569.

References

1 R. P. Agarwal, Focal Boundary Value Problems for Differential and Difference Equations, vol. 436 of Mathematics and Its Applications, Kluwer Academic Publishers, Dordrecht, The Netherlands, 1998.

2 R. P. Agarwal, D. O’Regan, and P. J. Y. Wong, Positive Solutions of Differential, Difference and Integral Equations, Kluwer Academic Publishers, Dordrecht, The Netherlands, 1999.

3 D. R. Anderson, I. Rach ˚unkova, and C. C. Tisdell, “Solvability of discrete Neumann boundary value problems,” Journal of Mathematical Analysis and Applications, vol. 331, no. 1, pp. 736–741, 2007.

4 A. Bensedik and M. Bouchekif, “Symmetry and uniqueness of positive solutions for a Neumann boundary value problem,” Applied Mathematics Letters, vol. 20, no. 4, pp. 419–426, 2007.

5 J.-P. Sun, W.-T. Li, and S. S. Cheng, “Three positive solutions for second-order Neumann boundary value problems,” Applied Mathematics Letters, vol. 17, no. 9, pp. 1079–1084, 2004.

6 A. Cabada and V. Otero-Espinar, “Existence and comparison results for difference φ-Laplacian boundary value problems with lower and upper solutions in reverse order,” Journal of Mathematical Analysis and Applications, vol. 267, no. 2, pp. 501–521, 2002.

7 I. Rach ˚unkova and C. C. Tisdell, “Existence of non-spurious solutions to discrete boundary value problems,” The Australian Journal of Mathematical Analysis and Applications, vol. 3, no. 2, pp. 1–9, 2006.

8 A. Cabada and V. Otero-Espinar, “Fixed sign solutions of second-order difference equations with Neumann boundary conditions,” Computers & Mathematics with Applications, vol. 45, no. 6–9, pp. 1125–

1136, 2003.

9 R. E. Gaines and J. L. Mawhin, Coincidence Degree, and Nonlinear Differential Equations, vol. 568 of Lecture Notes in Mathematics, Springer, Berlin, Germany, 1977.

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