On the Oscillation of Even-Order Half-Linear Functional Difference Equations with Damping Term
Abstract
We investigate the oscillatory behavior of solutions of the mth order half-linear functional difference equations with damping term of the form , n ≥ n0, 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
- (H1)
with Δpn ≥ 0 for all n ≥ n0;
- (H2)
{qn} and with qn ≥ 0 and rn > 0;
- (H3)
with τn < n and limn→∞τn = ∞.
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 [15–23] 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 n ≥ σ 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 n ≥ n0 and not identically zero. Then, there exists an integer l, 0 ≤ l ≤ m with (m + l) odd for Δmyn ≤ 0 and (m + l) even for Δmy(n) ≥ 0 such that
- (i)
l ≤ m − 1 implies (−1) l+iΔiyn > 0 for all n ≥ n0, l ≤ i ≤ m − 1,
- (ii)
l ≥ 1 implies Δiyn > 0 for all large n ≥ n0, 1 ≤ i ≤ l − 1.
Lemma 4 (see [25].)Let yn be defined for n ≥ n0 and yn > 0 with Δmyn ≤ 0 for n ≥ n0 and not identically zero. Then, there exists a large integer n1 ≥ n0 such that
Lemma 5. Let yn satisfy conditions of Lemmas 3 and 4 and Δm−1ynΔmyn ≤ 0 for n ≥ n1 ≥ n0. Further, if yn is increasing, then
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
Proof. The fact that yn is eventually positive solution of (3) implies yn > 0 and for all n ≥ n1 ≥ n0. In view of (3), we get
We claim that
From (3), we get
Theorem 7. Let condition (Λ1) hold. Further, assume that there exists a constant λ > α − 1 such that
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 n ≥ n1 ≥ n0. By Lemma 6, we have Δm−1yn > 0, Δmyn ≤ 0, and Δyn > 0 for n ≥ n1. Consider the function
Theorem 8. Let condition (Λ1) hold. Further, assume that there exists a function such that
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 n ≥ n1 ≥ n0. By Lemma 6, we have Δm−1yn > 0, Δmyn ≤ 0, and Δyn > 0 for n ≥ n1. Consider the function
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
For n ≥ 2, we have
Example 11. Consider the sixth order half-linear functional difference equation with damping
For n ≥ 2 and δn = n, we have
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
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.