Volume 2014, Issue 1 791631
Research Article
Open Access

On the Oscillation of Even-Order Half-Linear Functional Difference Equations with Damping Term

Yaşar Bolat

Yaşar Bolat

Department of Mathematics, Faculty of Science and Literatures, Kastamonu University, 037100 Kastamonu, Turkey kastamonu.edu.tr

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Jehad Alzabut

Corresponding Author

Jehad Alzabut

Department of Mathematics and Physical Sciences, Prince Sultan University, P.O. Box 66833, Riyadh 11586, Saudi Arabia psu.edu.sa

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First published: 19 May 2014
Citations: 3
Academic Editor: S. R. Grace

Abstract

We investigate the oscillatory behavior of solutions of the mth order half-linear functional difference equations with damping term of the form , nn0, where m is even and Q(s) = |s|α−2s, α > 1 is a fixed real number. Our main results are obtained via employing the generalized Riccati transformation. We provide two examples to illustrate the effectiveness of the proposed results.

1. Introduction

Consider the second order half-linear difference equation:
(1)
where Δ is the forward difference operator and {pn}, {rn} are sequences of nonnegative real numbers with {pn} > 0. The study of (1) has been initiated by Rehák in [1]. It is well known that there is a close similarity between (1) and the linear second order difference equation. Indeed, if {yn} is a solution of (1), then so is {cyn} for any constant c. Thus, (1) has one half of linearity properties [2].
In the presence of damping, (1) has been extended further to the second order half-linear difference equation with damping term of the form
(2)
where {qn} is a sequence of nonnegative real numbers. It is to be noted that neither (1) nor (2) has involved a delaying term. There are numerous numbers of oscillation criteria established in the literature for the solutions of (1) and (2). Most of these results were obtained by using certain efficient tools among them we name the Riccati transformation, variational principle, and some inequality techniques; see, for instance, the monograph [3] in which many contributions have been cited therein and to the recent papers [49].
Let be defined by Q(s) = |s|α−2s; α > 1 is a fixed real number and . Consider the mth order half-linear functional difference equation with damping term of the form
(3)
where m is even number, and
  • (H1)

    with Δpn ≥ 0 for all nn0;

  • (H2)

    {qn} and with qn ≥ 0 and rn > 0;

  • (H3)

    with τn < n and lim⁡nτn = .

For close results regarding the continuous counterparts of (1), (2), and (3), the reader is suggested to consult [1014].

A primary purpose of this paper is to establish sufficient conditions that guarantee the oscillation of solutions of (3). Our main results are obtained via employing the generalized Riccati transformation. In view of (3), one can easily figure out that it is formulated in more general form so that it includes some particular cases which have been studied in the literature; see [1523] for more details. To the best of authors’ observation, however, no published result has been concerned with the investigation of oscillatory behavior of solutions of (3) or its continuous counterpart. Therefore, our paper is new and presents a new approach.

2. Main Results

We start by recalling the following standard definitions.

Definition 1. A nontrivial sequence yn is called a solution of (3) if it is defined for all nσ where , , and pnQ(Δm−1yn) is differenceable on and satisfies (3) for all .

Definition 2. A nontrivial solution yn of (3) is said to be oscillatory if the terms of the sequence yn are not eventually positive or not eventually negative. Otherwise, the solution is called nonoscillatory. A difference equation is called oscillatory if all its solutions oscillate.

To obtain our main results, we need the following essential lemmas. The first of these is the discrete analogue of the well-known Kiguradze’s lemma.

Lemma 3 (see [24].)Let yn be defined for and y(n) > 0 with Δmyn of constant sign for nn0 and not identically zero. Then, there exists an integer l, 0 ≤ lm with (m + l) odd for Δmyn ≤ 0 and (m + l) even for Δmy(n) ≥ 0 such that

  • (i)

    lm − 1 implies (−1) l+iΔiyn > 0 for all nn0, lim − 1,

  • (ii)

    l ≥ 1 implies Δiyn > 0 for all large nn0, 1 ≤ il − 1.

Lemma 4 (see [25].)Let yn be defined for nn0 and yn > 0 with Δmyn ≤ 0 for nn0 and not identically zero. Then, there exists a large integer n1n0 such that

(4)
where l is defined as in Lemma 3. Further, if yn is increasing, then
(5)

Lemma 5. Let yn satisfy conditions of Lemmas 3 and 4 and Δm−1ynΔmyn ≤ 0 for nn1n0. Further, if yn is increasing, then

(6)
where .

The proof of Lemma 5 is straightforward and it can be achieved by using the last inequality of Lemma 4.

Lemma 6. Let yn be an eventually positive solution of (3). If

(7)
then Δm−1yn > 0, Δmyn ≤ 0, and Δyn > 0 for all nn1n0.

Proof. The fact that yn is eventually positive solution of (3) implies yn > 0 and for all nn1n0. In view of (3), we get

(8)
which leads to
(9)
Hence,
(10)
is decreasing and Δm−1yn is eventually positive or eventually negative.

We claim that

(11)
Assume, on the contrary, that Δm−1yn < 0, nn1. Then, from (10), we obtain
(12)
where . Therefore, from (12), we have
(13)
where . It follows that
(14)
or
(15)
Consequently, we obtain
(16)
Letting n in the above inequality, one gets lim⁡nΔm−2yn = −. Hence, yn is an eventually negative function which contradicts that yn > 0. Therefore, inequality (11) holds.

From (3), we get

(17)
from which it follows that
(18)
The above inequality implies that (Δm−1yn) α−1 is nonincreasing. Therefore, we can write
(19)
Since (Δm−1yn) α−1 is nonincreasing and positive, then from the above inequality, we have
(20)
by which we have
(21)
In virtue of (21) and Lemma 3, we deduce that since m is even then l is odd. Hence Δyn > 0 for nn1n0. The proof is complete.

Theorem 7. Let condition (Λ1) hold. Further, assume that there exists a constant λ > α − 1 such that

(22)
where
(23)
and M is as in Lemma 5. Then, (3) is oscillatory.

Proof. For the sake of contradiction, assume that (1) has a nonoscillatory solution yn. Without loss of generality, we assume that yn is eventually positive (the proof is similar when yn is eventually negative). That is, yn > 0, and for all nn1n0. By Lemma 6, we have Δm−1yn > 0, Δmyn ≤ 0, and Δyn > 0 for nn1. Consider the function

(24)
Taking into account that Δyn > 0 and yn is increasing and τnk < τn, we deduce that Δmyn ≤ 0 and Δm−1yn is nonincreasing. Lemmas 3 and 4, (1), and (24) yield
(25)
Multiplying by (nk) λ and summing up from n1 to n − 1, we obtain
(26)
or
(27)
where
(28)
Let
(29)
Then, F has maximum value at . That is,
(30)
Therefore, (27) can be rewritten as
(31)
Hence, we have
(32)
which contradicts condition (Λ2). The proof is complete.

Theorem 8. Let condition (Λ1) hold. Further, assume that there exists a function such that

(33)
where M is as in Lemma 5. Then, (3) is oscillatory.

Proof. For the sake of contradiction, assume that (3) has a nonoscillatory solution yn. Without loss of generality, we assume that yn is eventually positive (the proof is similar when yn is eventually negative). That is, yn > 0, and for all nn1n0. By Lemma 6, we have Δm−1yn > 0, Δmyn ≤ 0, and Δyn > 0 for nn1. Consider the function

(34)
By utilizing the same approach as in the proof of Theorem 7, we arrive at
(35)
Summing up (35) from n1 to n − 1, we have
(36)
Letting n in the above inequality and taking the upper limit, we get a contradiction to (Λ3). The proof is complete.

Remark 9. In view of the statements of Theorems 7 and 8, one can easily deduce that condition (Λ3) is a generalization of (Λ2).

Example 10. Consider the fourth order half-linear functional difference equation with damping

(37)
where pn = n, qn = n, rn = 1/n, τn = n − 1, m = 4, and α = 3. It is easy to see that conditions (H1)(H3) are satisfied. It remains to check the validity of conditions Λ1 and Λ2.

For n ≥ 2, we have

(38)
It is clear that Γ1 → as n. Therfore, condition (Λ1) holds. For n ≥ 2 and λ = 3 > α − 1 = 2, we have
(39)
where
(40)
It is clear that Γ2 → as n. Then, condition (Λ2) holds. Thus, by the conclusion of Theorem 7, (37) is oscillatory.

Example 11. Consider the sixth order half-linear functional difference equation with damping

(41)
where pn = n, qn = n, rn = n2, τn = n − 1, m = 6, and α = 3. It is easy to see that conditions (H1)(H3) are satisfied. In Example 10, we have seen that (Λ1) is satisfied. It remains to check the validity of condition (Λ3).

For n ≥ 2 and δn = n, we have

(42)
It is clear that Γ3 → as n. Then, condition (Λ3) holds. Thus, by the conclusion of Theorem 8, (41) is oscillatory.

Remark 12. It is not possible to decide the oscillatory behavior of solutions of (37) and (41) by using any of the results reported in [12, 13]. This implies that the results of our paper extend and generalize some known theorems.

Remark 13. The main results of this paper remain valid for nondelay difference equations of the form

(43)

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgment

The authors would like to express thier sincere thanks to the referee for pointing out several suggestions and corrections that helped making the contents of this paper more accurate.

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