Abstract
This work provides new adequate conditions for difference equations with forcing, positive and negative terms to have non-oscillatory solutions. A few mathematical inequalities and the properties of discrete fractional calculus serve as the fundamental foundation to our approach. To help establish the main results, an analogous representation for the main equation, called a Volterra-type summation equation, is constructed. Two numerical examples are provided to demonstrate the validity of the theoretical findings; no earlier publications have been able to comment on their solutions’ non-oscillatory behavior.
Keywords:
non-oscillatory solutions; asymptotic behavior; caputo nabla fractional difference; nabla fractional difference equations MSC:
34K11; 34N05
1. Introduction
Fractional order differential equations (FDEs) are generalized, non-integer order differential equations that can be obtained in time and space with a power law memory kernel of the nonlocal relationships; they offer an effective means of describing the memory of various substances and the characteristics of inheritance. The authors, who have shown a great deal of interest in studying the qualitative characteristics of the solution of FDEs, such as existence, uniqueness, oscillation, stability, and control, have provided details of significant findings in this area; see some of the illustrious monographs [1,2,3] and recent papers [4,5,6,7,8,9,10]. In particular, the oscillation of solutions was a subject that was taken into account for FDEs; the review paper in [11] is available to readers.
In recent years, academics have started to pay significant attention to discrete fractional calculus. The arbitrary order difference and summation features have considerably demonstrated their utility and validity due to their long memory nature and their flexible capability in carrying out mathematical computations [12]. As a result, numerous studies that investigate the qualitative traits of fractional difference equation solutions have been published, including their oscillation properties [13,14,15,16].
Let for any . Research on the oscillation of solutions of nabla fractional difference equations was started by Alzabut et al. [15] with the following problems:
and
where and such that ; , and .
Then, Abdalla et al. [13,14] continued to study the oscillation of solutions of different types of mixed nonlinear nabla fractional difference equations:
and
where b, , ; , , ⋯, and are the ratios of odd natural numbers with .
In this vein, Alzabut et al. [16] derived the conditions for the oscillation of solutions of a forced and damped nabla fractional difference equation:
where ; ; p, and .
Motivated by the above studies, which concentrated on oscillation discussion, and for the sake of giving an affirmative response about the behavior of non-oscillatory solutions, in this work, we consider the higher-order forced nabla fractional difference equation with positive and negative terms of the following form:
where
where , is the ratio of two odd natural numbers, , and denotes the xth Caputo nabla fractional difference of z. Throughout this work, we need the following conditions in the sequel.
- (i)
- , , and , are real valued continuous functions;
- (ii)
- There exist two continuous functions and , and positive real numbers and , where such thatfor and .
Unlike most existing results, which often discuss the oscillation of solutions, the asymptotic behavior of the Equation (6)’s non-oscillatory solutions is examined in this study. Our method is essentially based on some mathematical inequalities and the properties of discrete fractional calculus. A Volterra-type summation equation is built as an analogous representation for Equation (6) to aid in establishing the key conclusions. In order to demonstrate the validity of the theoretical findings, we offer numerical examples.
2. Essential Preliminaries
The results in this section are adopted from the two main monographs [12,17].
Definition 1
(See [12]). For and such that , we define the generalized rising function by
Furthermore, if and such that , then .
Definition 2
(See [12]). Let κ be a real valued function defined on . The first nabla difference of κ is given by
Definition 3
(See [12]). Let κ be a real valued function defined on and . The xth nabla fractional sum of κ based at χ is given by
where, by convention, .
Definition 4
(See [3]). Let and κ be a real valued function defined on . The xth Caputo nabla fractional difference of κ based at χ is given by
Theorem 1.
The initial value problem
has the unique solution
where and .
Lemma 1.
The following properties hold well.
- 1.
- If , then ;
- 2.
- ;
- 3.
- If and , then
Lemma 2.
Under the assumption that b, x and p are positive constants with and , we obtain
where
Lemma 3.
If R and S are nonnegative, , and , then
where equality holds if and only if .
We denote
and
3. Main Results
In this section, we provide sufficient conditions for which any non-oscillatory solution of (6) satisfies
Theorem 2.
Proof.
Let y be a non-oscillatory solution of (6), say for for some . Take . Letting , it follows from (6) and that, for ,
Applying Lemma 3 to with
we obtain
Substituting (18) into (17) and applying Lemma 1, for , we obtain
In view of (14) and (15), we see from (19) that, for ,
where is defined by
By the integer order variation of constants formula, it follows from (20) that
where
Note that (21) holds for . Hence, (21) holds for all and for all . Next, we proceed to estimate (21) as
implying that
where
Applying Lemmas 1 and 2, and Holder’s inequality to the sum on the far right in (22), we have
where
Using (23) in (22), we obtain from (22) that
where
with
We rewrite (24) as
Noting that , , and are all increasing, summing (25) from to yields that
holds for with . Thus,
where
Applying one of the elementary inequalities
with y, , to (26) gives
where and are defined by
and
Recalling the definition of , from (28), we have that
holds for , where
Applying the inequality (27) to (31) gives that
holds for , where
Denoting the left-hand side of (32) by , (32) yields that
holds for , and this can be rewritten as
which holds for , where
Using (13) and Gronwall’s inequality, we have the conclusion to the theorem. The proof for an eventually negative solution is similar. So, we omit it here. Thus, the theorem is proved. □
Next, we consider and we provide sufficient conditions for which any non-oscillatory solution of (6) is bounded.
Theorem 3.
Proof.
Let y be a non-oscillatory solution of (6), say for for some . Proceeding as in the proof of Theorem 2, we obtain (25) when . Since is increasing, summing (25) from to yields
Using the definition of , we obtain
for , where
and
Using the inequality (27) to (37), we have
for , where
Now, using (36) and Gronwall’s inequality, we have the conclusion to the theorem. The proof for an eventually negative solution is similar. So, we omit it here. The theorem is proved. □
4. Examples
We conclude this paper with the following examples to illustrate our main results.
Example 1.
Consider the equation
Here, we have , , , , , , , , and
Clearly, condition holds. Let and . Clearly, . Additionally, we have , and
implying that (13) holds. Considering and = with , , we see that holds. To check (14), we assume
that is,
Similarly, it is easy to verify that (15) holds. Therefore, all conditions of Theorem 2 are satisfied. Thus, every non-oscillatory solution of (6) satisfies
Example 2.
Consider the equation
Here, we have , , , , , , and . Hence, condition holds. Assuming , , and , we find
Therefore, (35) holds. Now, if we take , then we have , and
that is, (36) holds. Again, if
with , , then it is easy to verify that condition holds. To check that (14) holds, we assume
that is,
Similarly, it is easy to verify that (15) holds. Therefore, all conditions of Theorem 3 are satisfied. Thus, every non-oscillatory solution of (41) is bounded.
5. Concluding Remarks
Unlike most existing results in the literature that have been dedicated to oscillation criteria, we introduced a number of additional necessary conditions for non-oscillatory solutions to forced nabla difference equations with positive and negative terms. The main equation is of a general nature, and it covers many particular cases. By creating an equivalent representation of the primary equation in the form of a summation equation similar to Volterra and using some mathematical inequalities, the results are stated and proved. Some earlier findings in the literature were enhanced by the results. In fact, we give two brand-new cases, the non-oscillatory behavior of whose solutions has never been discussed in earlier studies. The existing methodology can be used in the future to produce comparable outcomes for higher order dynamic equations with forcing, positive and negative terms.
Author Contributions
Conceptualization, J.A., S.R.G., J.M.J., S.S.S. and B.A.; methodology, J.A., S.R.G., J.M.J., S.S.S. and B.A.; validation, J.A., S.R.G., J.M.J., S.S.S. and B.A.; formal analysis, J.A., S.R.G., J.M.J. and S.S.S.; investigation, J.A., S.R.G., J.M.J. and S.S.S.; resources, J.A., S.R.G., J.M.J. and S.S.S.; data curation, J.A., S.R.G., J.M.J. and S.S.S.; writing—original draft preparation, J.A., S.R.G., J.M.J. and S.S.S.; writing—review and editing, J.A., S.R.G., J.M.J., S.S.S. and B.A.; visualization, J.A., S.R.G., J.M.J. and S.S.S.; project administration, J.A. and B.A.; funding acquisition, J.A. and B.A. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
Not applicable.
Acknowledgments
The authors would like to thank the editor and the three anonymous reviewers for their constructive comments and suggestions, which helped us to improve themanuscript considerably. J. Alzabut and B. Abdalla express their gratitude to Prince Sultan University for their unwavering support. J. Alzabut also thanks OSTIM Technical University for helping him finish this paper.
Conflicts of Interest
The authors declare no conflict of interest.
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