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R E S E A R C H

Open Access

Eigenvalue of boundary value problem for

nonlinear singular third-order

q

-difference

equations

Changlong Yu

*

and Jufang Wang

*Correspondence: changlongyu@126.com College of Sciences, Hebei University of Science and Technology, Shijiazhuang, Hebei 050018, P.R. China

Abstract

In this paper, we establish the existence of positive solutions of a boundary value problem for nonlinear singular third-orderq-difference equations

D3

qu(t) +

λ

a(t)f(u(t)) = 0,tIq,u(0) = 0,Dqu(0) = 0,

α

Dqu(1) +

β

D2qu(1) = 0, by using

Krasnoselskii’s fixed-point theorem on a cone, where

λ

is a positive parameter. Finally, we give an example to demonstrate the use of the main result of this paper. The conclusions in this paper essentially extend and improve known results.

Keywords: q-difference equations; positive solutions; singular boundary value problem; Krasnoselskii’s fixed-point theorem

1 Introduction

Theq-difference equations initiated in the beginning of the th century [–], is a very interesting field in difference equations. In the last few decades, it has evolved into a mul-tidisciplinary subject and plays an important role in several fields of physics, such as cos-mic strings and black holes [], conformal quantum mechanics [], and nuclear and high-energy physics []. For some recent work onq-difference equations, we refer the reader to [–]. However, the theory of boundary value problems (BVPs) for nonlinearq-difference equations is still in an early stage and many aspects of this theory need to be explored. To the best of our knowledge, for the BVPs of nonlinear third-orderq-difference equations, a few works were done, see [, ] and the references therein.

Recently, in [], El-Shahed has studied the existence of positive solutions for the fol-lowing nonlinear singular third-order BVP:

u(t) +λa(t)f(u(t)) = , ≤t≤,

u() =u() = , αu() +βu() = ,

by Krasnoselskii’s fixed-point theorem on a cone.

More recently, in [] Ahmad has studied the existence of positive solutions for the fol-lowing nonlinear BVP of third-orderq-difference equations:

D

qu(t) =f(t,u(t)), ≤t≤,

u() = , Dqu() = , u() = ,

by Leray-Schauder degree theory and some standard fixed-point theorems.

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Motivated by the work above, in this paper, we will study the following BVP of nonlinear singular third-orderq-difference equations:

D

qu(t) +λa(t)f(u(t)) = , tIq,

u() = , Dqu() = , αDqu() +βDqu() = ,

(.)

whereλ>  is a positive parameter,a: (, )→[,∞) is continuous and  <a(t)dqt< ∞,f is a continuous function,Iq={qn:nN} ∪ {, },q∈(, ) is a fixed constant, and

α,β≥,α+β> .

Obviously, whenq→–, BVP (.) reduces to the standard BVP in []. Throughout this paper, we always suppose the following conditions to hold:

(C) fC([, ], [, +∞));

(C) α,β≥,α+β> and αα+ββq.

2 Preliminary results

In this section, firstly, let us recall some basic concepts ofq-calculus [, ].

Definition . For  <q< , we define theq-derivative of a real-value functionf as

Dqf(t) =

f(t) –f(qt)

( –q)t , tIq–{}, Dqf() =tlim→Dqf(t).

Note thatlimqDqf(t) =f(t).

Definition . The higher-orderq-derivatives are defined inductively as

Dqf(t) =f(t), Dnqf(t) =DqDnq–f(t), nN.

For example,Dq(tk) = [k]qtk–, wherekis a positive integer and the bracket [k]q= (qk– )/(q– ). In particular,Dq(t) = ( +q)t.

Definition . Theq-integral of a functionf defined in the interval [a,b] is given by

x

a

f(t)dqt:=

n=

x( –q)qnfxqnafaqn, x∈[a,b],

and fora= , we denote

Iqf(x) = x

f(t)dqt=

n=

x( –q)qnfxqn,

then b

a

f(t)dqt= b

f(t)dqta

f(t)dqt.

Similarly, we have

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Observe that

DqIqf(x) =f(x),

and iff is continuous atx= , thenIqDqf(x) =f(x) –f().

Inq-calculus, the product rule and integration by parts formula are

Dq(gh)(t) =Dqg(t)h(t) +g(qt)Dqh(t), (.) x

f(t)Dqg(t)dqt=

f(t)g(t)xx

Dqf(t)g(qt)dqt. (.)

Remark . In the limitq→–, the above results correspond to their counterparts in

standard calculus.

Definition . LetEbe a real Banach space. A nonempty closed convex setPEis called a cone if it satisfies the following two conditions:

(i) xP,λ≥impliesλxP; (ii) xP,xPimpliesx= .

Theorem .(Krasnoselskii) [] Let E be a Banach space and let KE be a cone in E. As-sume thatandare open subsets of E with∈and⊂.Let T:K∩(\)→ K be a completely continuous operator.In addition,suppose either

(H) Tuu,∀uKandTuu,∀uKor (H) Tuu,∀uKandTuu,∀uK

holds.Then T has a fixed point in K∩(\).

Lemma . Let yC[, ],then the BVP

Dqu(t) +y(t) = , tIq,

u() = , Dqu() = , αDqu() +βDqu() = ,

(.)

has a unique solution

u(t) = 

G(t,s;q)y(s)dqs,

where

G(t,s;q) =  ( +q)(α+β)

αt( –qs) +βt– (tqs)(tqs)(α+β), st,

αt( –qs) +βt, ts.

Proof Integrate theq-difference equation from  tot, we get

Dqu(t) = – t

y(s)dqs+a. (.)

Integrate (.) from  tot, and change the order of integration, we have

Dqu(t) = – t

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Integrating (.) from  tot, and changing the order of integration, we obtain

This completes the proof.

Remark . Forq→, equation (.) takes the form

which is the solution of a classical third-order ordinary differential equationu(t)+y(t) =  and the associated form of Green’s function for the classical case is

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Ifts, then

The proof is complete.

We consider the Banach space Cq =C(Iq,R) equipped with standard norm u =

We adopt the following assumption:

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Next, forn≥, we define the operatorTn:PPby

Obviously,Tnis completely continuous onPfor anyn≥ by an application of the Ascoli-Arzelá theorem. Denote BK ={uP:uK}. ThenTn converges uniformly toT as

Tnconverges uniformly toT asn→ ∞, and thereforeT is completely continuous also.

This completes the proof.

3 Main results

In this section, we will apply Krasnoselskii’s fixed-point theorem to the eigenvalue problem (.). First, we define some important constants:

Aq=

The main result of this paper is the following.

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From the definition off∞, we see that there exist anl>  andl>l, such thatf(u)≥

(f∞ε)uforu>l. Letl>l, ifuPwithu=lwe have

Tu=Tu() =λ

G(,s;q)a(s)fu(s)dqs

λ

G(,s;q)a(s)g(s)fu(s)dqsλ(f∞–ε)uAq.

Chooseε>  sufficiently small such thatλ(f∞–ε)Aq≥. Then we haveTuu. Let

={uCq|u<l}, then⊂andTuuforuP.

Condition (H) of Krasnoselskii’s fixed-point theorem is satisfied. Hence, by

Theo-rem ., the result of TheoTheo-rem . holds. This completes the proof of TheoTheo-rem ..

Theorem . Suppose that(C), (C)and(C)hold and Aqf>BqF∞.Then for eachλ∈ ( 

Aqf, 

BqF∞),BVP(.)has at least one positive solution.

Proof It is similar to the proof of Theorem ..

Theorem . Suppose that(C), (C)and(C)hold andλBqf(u) <u for u∈(, +∞).Then

BVP(.)has no positive solution.

Proof Assume to the contrary thatuis a positive solution of BVP (.). Then

u() =λ

G(,s;q)a(s)fu(s)dqs< 

Bq

G(,s;q)a(s)u(s)dqs

u()

Bq

G(,s;q)a(s)dqs=u().

This is a contradiction and completes the proof.

Theorem . Suppose that(C), (C)and(C)hold andλAqf(u) >u for u∈(, +∞).Then

BVP(.)has no positive solution.

Proof It is similar to the proof of Theorem ..

4 Example

Consider the following BVP: ⎧

⎨ ⎩

D  

u(t) +λt–u+u

u+ ( +sinu) = , tIq, u() = , D

u() = , Du() + D

 

u() = . (.)

Then F= , f = ,F∞ = , f∞ = , and uf(u)≤u. By direct calculations,

we obtain Aq = . and Bq = .. From Theorem . we see that if λ ∈ (., .) then the problem (.) has a positive solution. From Theorem . we see that ifλ< . then the problem (.) has no positive solution. By Theorem . we see that ifλ> . then the problem (.) has no positive solution.

Competing interests

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Authors’ contributions

Each of the authors, CY and JW contributed to each part of this work equally and read and approved the final version of the manuscript.

Acknowledgements

This work was supported by the Natural Science Foundation of China (10901045), (11201112) and (61304106), the Natural Science Foundation of Hebei Province (A2013208147) and (A2011208012).

Received: 4 October 2013 Accepted: 26 December 2013 Published:16 Jan 2014

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4. Adams, CR: On the linear ordinaryq-difference equation. Ann. Math.30, 195-205 (1928) 5. Strominger, A: Information in black hole radiation. Phys. Rev. Lett.71, 3743-3746 (1993) 6. Youm, D:q-Deformed conformal quantum mechanics. Phys. Rev. D62, 095009 (2000)

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Cite this article as:Yu and Wang:Eigenvalue of boundary value problem for nonlinear singular third-order

References

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