Volume 2013, Issue 1 176465
Research Article
Open Access

Reverse-Order Lower and Upper Functions for Periodic Problems of Second-Order Singular Difference Equations

Yanqiong Lu

Yanqiong Lu

Department of Mathematics, Northwest Normal University, Lanzhou 730070, China nwnu.edu.cn

Search for more papers by this author
Ruyun Ma

Corresponding Author

Ruyun Ma

Department of Mathematics, Northwest Normal University, Lanzhou 730070, China nwnu.edu.cn

Search for more papers by this author
First published: 01 October 2013
Citations: 1
Academic Editor: Irena Rachůnková

Abstract

We present sufficient conditions ensuring the lower and upper functions on the reversed-order for the periodic difference equations. This enables us to obtain the existence of positive periodic solutions of the second-order difference equation Δ2u(t − 1) = g(t)/uμ (t) − h(t)/uλ (t) + f(t),     t, where g,  h : → [0, ∞), and f : are T-periodic functions, λ,   μ > 0.

1. Introduction

The theory of nonlinear difference equations has been widely used to study discrete models appearing in many fields such as computer science, economics, neural network, ecology, and cybernetics, see for example, [1]. Recently, there are many papers to study the existence of positive periodic solutions for second-order difference equations, see [27] and their references therein. However, there are few techniques for studying the existence of positive solutions of difference equations with singularity, and thus the results in the field are very rare, see [813]. The existence of positive periodic solutions for continuous case has been studied by Torres, see [14, 15].

Let denote the integer set, for a, b with a < b, [a, b]  : = {a, a + 1, …, b}.

In 2012, Lu and Ma are concerned with the existence of positive periodic solutions of the second-order difference equation as follows:
()
where g, h : → [0, ), and f : are T-periodic functions, λ, μ > 0. Special cases of (1) are
()
()
()
In the related literature, it is said that (3) has an attractive singularity, whereas (4) has a repulsive singularity. They use the well-order lower and upper functions of (1) to show the existence of positive T-periodic solution of (1), (2), and (3), respectively, see [13].

However, the well-order lower and upper solutions lose their effects to deal with case (4). In this paper, we are devoted to constructing lower and upper functions on the reversed-order for (1) and dealing with the problems (1), (2), and (4), respectively.

The structure of the paper is as follows. Section 2 contains the tools needed in the proofs. In Section 3 we state and prove the main results and develop some corollaries for the equation with a singularity of mixed type. To illustrate the results, some examples are given.

2. Auxiliary Results

Let
()
under the norm . Then (E, ∥·∥) is a Banach space.

The proofs of our results rely on the method of upper and lower functions. The following lemmas are classical and can be found, for example, in [3]. We introduce them in a form suitable for us.

Lemma 1. Let there exist positive functions α, βE, such that

()
()
and α(t) ≤ β(t) for t ∈ [1, T] . Then there exists at least one positive T-periodic solution to (1).

A function αE (resp., βE) verifying (6) (resp, (7)) is called lower (resp, upper) function (solution) of (1). When the order between the lower and the upper functions is the inverse, an additional hypothesis is needed.

Definition 2. A function φE and φ ≥ 0 is said to verify the property (P) if the implication

()
holds.

Lemma 3. Let there exist positive functions α, βE satisfying (6), (7), and β(t) ≤ α(t), t ∈ [1, T] . Moreover, there exists φE with the property (P), such that

()
where β(t) ≤ u(t) ≤ v(t) ≤ α(t) for t ∈ [0, T + 1] . Then there exists at least one positive T-periodic solution to (1).

Proof. From the condition (9), it follows that

()
That is, the nonlinearity is increasing.

Define the operator T : EE as the unique solution of problem (1) as follows:

()
where G(t, s) is the Green’s function of
()
As φ satisfies the property (P), it follows that G(t, s) > 0. Now we divide the proof into three steps.

Step  1. We show

()
where K = {uEβuα} is a nonempty bounded closed subset in E.

In fact, for uK, set w = Tu(t). From the definitions of α, β, and K, combining with (9), we have

()
Using property (P), we get βw.

Analogously, we can prove that wα. Thus, (13) holds.

Step  2. Let u1 = Tη1, u2 = Tη2, where η1, η2K satisfy βη1η2α. Then we claim that

()
In fact, let ω = u2u1, it follows from (10) and (11) that
()

Step  3. The sequences {αn} and {βn} are obtained by recurrence:

()
From the results of Steps  1 and  2, it follows that
()
Moreover, from the definition of T, we get
()

This together with (18), we can easily get that there exists Cα depending only on α but not on t and n, such that |αn | ≤ Cα, so {αn} is bounded in E. Similarly, {βn} is bounded in E. Therefore, we can conclude that {αn} and {βn} converge uniformly to the extremal solutions u of the problem (1). Subsequently, there exists at least one positive T-periodic solutions of (1).

Property (P) is just an anti-maximum principle for the linear operator Lu : = Δ2u(t − 1) + φ(t)u(t) with periodic boundary conditions, and it is equivalent to have a nonnegative Green function. Reference [7] provides sufficient conditions for φ to verify property (P). In particular, we have the following lemma.

Lemma 4 (see [7].)Let us assume φE, φ≢0 and the following conditions holds:

()
Then φ verifies the property (P).

To finish this section, we give a technical bound on the amplitude of oscillation of a periodic function.

Lemma 5 ([13, Lemma  2.2]). Given vE, then

()
where
()
Moreover, (21) is fulfilled as an equality if and only if v is a constant function.

3. The Main Results

For the sake of brevity we will use the following notation throughout the paper:
()
The following theorems are the main results of the paper.

Theorem 6. Let G > 0, F < 0, let functions w, σE be such that the equalities

()
()
are fulfilled and let there exist x0 ∈ (0, +) such that
()
where
()
Moreover, define
()
and assume that φ(t) = μg(t)/β1+μ(t) verifies the property (P). Then problem (1) has at least one positive T-periodic solution.

Proof. Let β be defined by (28). Then βE and in view of (24) and (25), we have

()
Moreover, according to (26) and (27)
()
Now (29) and (30) imply
()
Consequently, β is an upper function to (1).

Further, we can choose x1 ∈ (0, x0) such that

()
and put
()
Then αE, and in view of (24) and (25) we have
()
Moreover, according to (27) and (32)
()
Now (34) and (35) imply
()
Consequently, α is a lower function to (1) and according to (30) and (35) we have
()

Furthermore, note that the function

()
is nondecreasing for yβ. Therefore we have
()
whenever β(t) ≤ u(t) ≤ v(t) for t ∈ [1, T] , hence, we get
()
Thus, the assertion follows from Lemma 3.

Remark 7. Note that for every qE such that , the periodic solution v of the equation

()
is given by the Green formula:
()
where c. Therefore, the periodic functions w and σ with properties (24) and (25) exist and, moreover, are unique up to a constant term, the value of which has no influence on the validity of the condition (26). A similar observation can be made in relation to the formulations of the theorems given below.

Theorem 8. Let μ > λ, H > 0, G > 0, F = 0, let functions w, σE be such that (24) and (25) are fulfilled and let there exist x0 ∈ (0, +) such that

()
where mw and mσ are defined by (27). Moreover, assume that φ(t) = μg(t)/β1+μ(t) verifies the property (P), where β is given by (28). Then problem (1) has at least one positive T-periodic solution.

Proof. Note that the inequality μ > λ implies

()
Therefore, analogously to the proof of Theorem 6, one can show that there exist lower and upper functions α, β satisfying (37). Consequently, the assertion follows from Lemma 3 with φ(t) = μg(t)/β1+μ(t).

Corollary 9. Let μ > λ, H > 0, G > 0, and let wE be such that (24) is fulfilled. Let

()
where mw is given by (27) and
()
Moreover, let us define
()
and assume that φ(t) = μg(t)/β1+μ(t) verifies the property (P). Then problem (2) has at least one positive solution.

Proof. Put f ≡ 0 and

()
Then the assertion follows from Theorem 8.

Corollary 10. Let G > 0, F < 0, let σE be such that (25) is fulfilled, and let

()
where mσ is defined by (27) and
()
Moreover, if
()
holds. Then problem (4) has at least one positive T-periodic solution.

Proof. Put H = 0,

()
and define a function β by (28). Let β(t) = (G/|F | ) 1/μMσ + σ(t) for t ∈ [1, T] . Then (51) guaranties that φ(t) = μg(t)/β1+μ(t) satisfies the property (P). Moreover, (51) yields (25). Therefore, the assertion follows from Theorem 6.

Corollary 11. Let G > 0, F < 0 and

()
Then problem (4) has at least one positive T-periodic solution.

Proof. According to Lemma 5,

()
Then (53) implies (51). Consequently, the assertion follows from Corollary 10.

Example 12. Let us consider the boundary value problem:

()
where T > 3 is an integer.

Obviously, (1/u)−(1/4)→+ as u → 0. Let g ≡ 1, f ≡ −1/4T, μ = 1. Then G = T, F = −1/4 and

()
Thus, from Corollary 11, problem (55) has at least one positive T-periodic solution.

Acknowledgments

The authors are very grateful to the anonymous referees for their valuable suggestions. This work was supported by the NSFC (no. 11061030, no. 11361054), Gansu provincial National Science Foundation of China (no. 1208RJZA258) and SRFDP (no. 20126203110004).

      The full text of this article hosted at iucr.org is unavailable due to technical difficulties.