A Final Result on the Oscillation of Solutions of the Linear Discrete Delayed Equation with a Positive Coefficient
J. Baštinec,1L. Berezansky,2J. Diblík,1,3 and Z. Šmarda1
1Department of Mathematics, Faculty of Electrical Engineering and Communication, Brno University of Technology, 61600 Brno, Czech Republic
2Department of Mathematics, Ben-Gurion University of the Negev, 84105 Beer-Sheva, Israel
3Department of Mathematics and Descriptive Geometry, Faculty of Civil Engineering, Brno University of Technology, 602 00 Brno, Czech Republic
Academic Editor: Yuri V. Rogovchenko
Received15 Jan 2011
Accepted06 Jun 2011
Published05 Sep 2011
A linear th-order discrete delayed equation where a positive sequence is considered for . This equation is known to have a positive solution if the sequence satisfies an inequality. Our aim is to show that, in the case of the opposite inequality for , all solutions of the equation considered are oscillating for .
The existence of positive solutions of difference equations is often encountered when analysing mathematical models describing various processes. This is a motivation for an intensive study of the conditions for the existence of positive solutions of discrete or continuous equations. Such analysis is related to investigating the case of all solutions being oscillating (for investigation in both directions, we refer, e.g., to [1–30] and to the references therein). The existence of monotonous and nontrivial solutions of nonlinear difference equations (the first one implies the existence of solutions of the same sign) also has attracted some attention recently (see, e.g., several, mostly asymptotic methods in [31–42] and the related references therein). In this paper, sharp conditions are derived for all the solutions being oscillating for a class of linear -order delayed discrete equations.
We consider the delayed -order linear discrete equation
where , is fixed, , , . In what follows, we will also use the sets and for , . A solution of (1.1) is positive (negative) on if () for every . A solution of (1.1) is oscillating on if it is not positive or negative on for an arbitrary .
Definition 1.1. Let us define the expression , , by , , where and , , , and (instead of , , we will only write and ).
In  difference equation (1.1) is considered and the following result on the existence of a positive solution is proved.
Theorem 1.2 (see ). Let be a fixed integer, let be sufficiently large and
for every . Then there exists a positive integer and a solution , of equation (1.1) such that
holds for every .
Our goal is to answer the open question whether all solutions of (1.1) are oscillating if inequality (1.2) is replaced with the opposite inequality
assuming , and is sufficiently large. Below we prove that if (1.4) holds and , then all solutions of (1.1) are oscillatory. This means that the result given by Theorem 1.2 is a final in a sense. This is discussed in Section 4. Moreover, in Section 3, we show that all solutions of (1.1) will be oscillating if (1.4) holds only on an infinite sequence of subintervals of .
Because of its simple form, equation (1.1) (as well as its continuous analogue) attracts permanent attention of investigators. Therefore, in Section 4 we also discuss some of the known results.
The proof of our main result will use the next consequence of one of Domshlak’s results [13, Theorem 4, page 66].
Lemma 1.3. Let and be fixed natural numbers such that . Let be a bounded sequence of real numbers and be a positive number such that there exists a number satisfying
Then, if for and
for , any solution of (1.1) has at least one change of sign on .
Throughout the paper, symbols “” and “” (for ) will denote the well-known Landau order symbols.
2. Main Result
In this section, we give sufficient conditions for all solutions of (1.1) to be oscillatory as . It will be necessary to develop asymptotic decompositions of some auxiliary expressions. As the computations needed are rather cumbersome, some auxiliary computations are collected in the appendix to be utilized in the proof of the main result (Theorem 2.1) below.
Theorem 2.1. Let be sufficiently large, and . Assuming that the function satisfies inequality (1.4) for every , all solutions of (1.1) are oscillating as .
Proof. As emphasized above, in the proof, we will use Lemma 1.3. We define
where is sufficiently large, and is a fixed integer. Although the idea of the proof is simple, it is very technical and we will refer to notations and auxiliary computations contained in the appendix. We will develop an asymptotic decomposition of the right-hand side of inequality (1.7) with the function defined by (2.1). We show that this will lead to the desired inequality (1.4). We set
where and are defined by (A.4) and (A.5). Moreover, can be expressed as
Recalling the asymptotic decomposition of when : , we get (since , , , and , )
as . Then, it is easy to see that, by (A.13), we have , for every and
Moreover, for , we will get an asymptotic decomposition as . Using formulas (A.13), (A.57), and (A.60), we get
Since , , , we can decompose the denominator of the second fraction as the sum of the terms of a geometric sequence. Keeping only terms with the order of accuracy necessary for further analysis (i.e. with order ), we get
We perform an auxiliary computation in ,
Thus, we have
Finalizing our decompositions, we see that
It is easy to see that inequality (1.7) becomes
and will be valid if (see (1.4))
for . If , where is sufficiently large, (2.13) holds for with sufficiently small because . Consequently, (2.11) is satisfied and the assumption (1.7) of Lemma 1.3 holds for . Let in Lemma 1.3 be fixed, be so large (and so small if necessary) that inequalities (1.5) hold. Such choice is always possible since the series is divergent. Then Lemma 1.3 holds and any solution of (1.1) has at least one change of sign on . Obviously, inequalities (1.5) can be satisfied for another pair of , say with and sufficiently large and, by Lemma 1.3, any solution of (1.1) has at least one change of sign on . Continuing this process, we will get a sequence of pairs with such that any solution of (1.1) has at least one change of sign on . This concludes the proof.
3. A Generalization
The coefficient in Theorem 2.1 is supposed to be positive on . For all sufficiently large , the expression , as can easily be seen from (2.10), is positive. Then, as follows from Lemma 1.3, any solution of (1.1) has at least one change of sign on if is nonnegative on and satisfies inequality (1.4) on .
Owing to this remark, Theorem 2.1 can be generalized because (and the following argumentation was used at the end of the proof of Theorem 2.1) all solutions of (1.1) will be oscillating as if a sequence of numbers , , , exists such that (i.e., the sets , are disjoint and ), and, for every pair , all assumptions of Lemma 1.3 are satisfied (because of the specification of function by (2.1), inequalities (1.6) are obviously satisfied). This means that, on the set
function can assume even negative values, and, moreover, there is no restriction on the behavior of for . This leads to the following generalization of Theorem 2.1 with a proof similar to that of Theorem 2.1 and, therefore, omitted.
Theorem 3.1. Let be sufficiently large, , be a positive number, and . Let there exists a sequence on integers , , , , sufficiently large and such that, for function (defined by (2.1)) and for each pair , , there exists a number such that
for , and (1.4) holds for , then all solutions of (1.1) are oscillating as .
4. Comparisons, Concluding Remarks, and Open Problems
Equation (1.1) with was considered in , where a particular case of Theorem 2.1 is proved. In , a hypothesis is formulated together with the proof of Theorem 1.2 (Conjecture 1) about the oscillation of all solutions of (1.1) almost coinciding with the formulation of Theorem 2.1. For its simple form, (1.1) is often used for testing new results and is very frequently investigated.
Theorems 1.2 and 2.1 obviously generalize several classical results. We mention at least some of the simplest ones (see, e.g., [16, Theorem 7.7] or [19, Theorem ]),
Theorem 4.1. Let = const. Then every solution of (1.1) oscillates if and only if
Or the following result holds as well (see, e.g., [16, Theorem 7.6]) [18, 19]).
Theorem 4.2. Let and
Then (1.1) has a nonoscillatory solution.
In  a problem on oscillation of all solutions of equation
is considered where , , and . Since in (4.3) delay is variable, we can formulate
Open Problem 1. It is an interesting open question whether Theorems 1.2 and 2.1 can be extended to linear difference equations with a variable delay argument of the form, for example,
where . For some of the related results for the differential equation
see the results in [3, 12] that are described below.
Open Problem 2. It is well known [19, 22] that the following condition is also sufficient for the oscillation of all solutions of (4.5) with :
The right-hand side of (4.6) is a critical value for this criterion since this number cannot be replaced with a smaller one. In  equation (1.1) is considered as well. The authors prove that all solutions oscillate if , and
An open problem is to obtain conditions similar to Theorem 2.1 for this kind of oscillation criteria. Some results on this problem for delay differential equations were also obtained in paper .
In  the authors establish an equivalence between the oscillation of (1.1) and the equation
under the critical state
Then they obtain some sharp oscillation and nonoscillation criteria for (1.1). One of the results obtained there is the following.
Theorem 4.3. Assume that, for sufficiently large , inequality (4.11) holds. Then the following statements are valid. (i)If
then every solution of (1.1) is oscillatory. (ii)If, on the other hand,
then (1.1) has a nonoscillatory solution.
Regarding our results, it is easy to see that statement (i) is a particular case of Theorem 2.1 while statement (ii) is a particular case of Theorem 1.2.
In , the authors investigate (1.1) for and prove that (1.1) is oscillatory if
Comparing (4.14) with Theorem 2.1, we can see that (4.14) gives not sharp sufficient condition. Set, for example, , and
and the series in the left-hand side of (4.14) converges since
But, by Theorem 2.1 all solutions of (1.1) are oscillating as . Nevertheless (4.14) is not a consequence of Theorem 2.1.
Let us consider a continuous variant of (1.1): a delayed differential linear equation of the form
where is a constant delay and (or ), . This equation, too, for its simple form, is often used for testing new results and is very frequently investigated. It is, for example, well known that a scalar linear equation with delay
has a nonoscillatory solution as . This means that there exists an eventually positive solution. The coefficient is called critical with the following meaning: for any , all solutions of the equation
are oscillatory while, for , there exists an eventually positive solution. In , the third author considered (4.18), where is a continuous function, and is sufficiently large. For the critical case, he obtained the following result (being a continuous variant of Theorems 1.2 and 2.1).
Theorem 4.4. (a) Let an integer exist such that if where
Then there exists an eventually positive solution of (4.18). (b) Let an integer and , exist such that
if . Then all solutions of (4.18) oscillate.
Further results on the critical case for (4.18) can be found in [1, 11, 14, 17, 24].
In , Theorem 7 was generalized for equations with a variable delay
where and are continuous functions. The main results of this paper include the following.
Theorem 4.5 (see ). Let if . Let an integer exist such that for , where
then there exists an eventually positive solution of (4.23) for .
Finally, the last results were generalized in . We reproduce some of the results given there.
Theorem 4.6. (A) Let , for , and let condition (a) of Theorem 4.4 holds. Then (4.23) has a nonoscillatory solution. (B) Let for , and let condition (b) of Theorem 4.4 holds. Then all solutions of (4.23) oscillate.
For every integer , and , we define
Theorem 4.7. Let for sufficiently large and : a.e., be a locally integrable function,
and let there exists such that , . (a)If there exists a such that
and, for a fixed integer ,
then there exists an eventually positive solution of (4.23). (b)If there exists a such that
and, for a fixed integer and , ,
if , then all solutions of (4.23) oscillate.
A. Auxiliary Computations
This part includes auxiliary results with several technical lemmas proved. Part of them is related to the asymptotic decomposition of certain functions and the rest deals with computing the sums of some algebraic expressions. The computations are referred to in the proof of the main result (Theorem 2.1) in Section 2.
First we define auxiliary functions (recalling also the definition of function given by (2.1)):
where is sufficiently large and . Moreover, we set (for admissible values of arguments)
A.1. Asymptotic Decomposition of Iterative Logarithms
In the proof of the main result, we use auxiliary results giving asymptotic decompositions of iterative logarithms. The following lemma is proved in .
Lemma A.1. For fixed and a fixed integer , the asymptotic representation
holds for .
A.2. Formulas for and for
Lemma A.2. The following formulas hold:
Proof. It is easy to see that
A.3. Formula for the Sum of the Terms of an Arithmetical Sequence
Denote by the terms of an arithmetical sequence of th order (th differences are constant),, the first differences (, ,…), , the second differences (,…), and so forth. Then the following result holds (see, e.g., ).
Lemma A.3. For the sum of terms of an arithmetical sequence of th order, the following formula holds
A.4. Asymptotic Decomposition of
Lemma A.4. For fixed and , the asymptotic representation
holds for .
Proof. The function is defined by (2.1). We develop the asymptotic decomposition of when is sufficiently large and . Applying Lemma A.1 (for , and ), we get
Finally, gathering the same functional terms and omitting the terms having a higher order of accuracy than is necessary, we obtain the asymptotic decomposition (A.13).
A.5. Formula for
Lemma A.5. For fixed , the formula
holds for all sufficiently large .
Proof. It is easy to see that
A.6. Asymptotic Decomposition of
Lemma A.6. For fixed and , the asymptotic representation
holds for .
Proof. It is easy to deduce from formula (A.13) with that
A.7. Asymptotic Decomposition of
Lemma A.7. For fixed and , the asymptotic representation
holds for .
Lemma A.9. For the above sum, the following formula holds:
Proof. Using formula (A.9), we get
We compute the sum in the square brackets. We use formula (A.12). In our case,
the second differences are constant, and
Then the sum in the square brackets equals
and formula (A.24) is proved.
A.10. Formula for
Lemma A.10. For the above product, the following formula holds:
Proof. We have
Then, using formulas (A.22), and (A.24), we get
A.11. Formula for
Lemma A.11. For the above sum, the following formula holds:
Proof. Using formulas (A.9), (A.10), and (A.22), we get
A.12. Formula for
Lemma A.12. For the above sum, the following formula holds: