1. Introduction
The application and importance of delay difference equations with continuous time can be found in mechanical and electrical systems, as it is stated in [
1], also in modeling of distributed chaos, as it is pointed out in [
2,
3]. Analysis of oscillatory properties of solutions of delay difference equations with continuous time have been the subject of papers [
4,
5,
6,
7,
8,
9,
10,
11,
12,
13]. Literature concerned with oscillatory properties of solutions of differential and discrete difference equations can be divided into two groups: one with nonnegative or positive coefficients and the other with oscillatory coefficients. Studies on oscillatory properties of solutions of differential equations with nonnegative coefficients can be found, for example, in papers [
14,
15,
16], while with oscillating coefficients in [
17,
18]. For example, papers [
15,
19,
20,
21] and [
22,
23,
24] are devoted to discrete difference equations with positive coefficients and oscillatory coefficients, respectively. Since many papers dealing with difference equations with continuous time analyze equations with positive or nonnegative coefficients (all mentioned above), but only (to the best of our knowledge) paper [
25] considers oscillatory coefficients, our aim is to expand the set of known oscillatory conditions of solutions of delay difference equations with continuous time and oscillatory coefficients.
In this paper, we analyze the oscillatory property of the solutions of the delay difference equation
where
,
and
. For
,
is a piecewise continuous and oscillatory function, but the delay argument
is in the form
where the function
is piecewise constant. Also, the delay arguments have the following properties:
and
We present two oscillatory criteria and compare them to oscillatory conditions in [
25]. The comparison shows that there is a set of difference equations such that our new oscillatory criteria prove that their solutions oscillate, while the known criteria are not applicable to them.
A
solution of the delay difference equation (
1) is a real-valued function
x defined on the interval
, with
that satisfies Eq. (
1). If a solution of (
1) changes sign on the interval
for any
s, it is
oscillatory. Otherwise, it is
nonoscillatory. As in [
8,
26], for any bounded real-valued function
defined on the interval
there exists a unique solution
x of (
1) that satisfies the initial condition
,
, since it can be represented by
Standardly, for any
,
, and a real-valued function
f,
and
2. The New Oscillation Criteria
We define a real-valued functions
and
These functions have the following properties:
For more details and illustrations by example see [
25].
First we give the following lemma.
Lemma 1.
If there exists a sequence of disjoint intervals with properties: for every ,
and, for some ,
then there exists a sequence such that and
but
Proof. For any
, if
then
so (
15) and (
16) hold for
.
For
, (
14) gives that
that is, (
15) and (
16) hold for
. Besides that, if
then
and there exists
such that (
15) and (
16) hold.
Consequently, for every
, there exists
such that (
15) and (
16) hold. □
Now we prove an auxiliary lemma.
Lemma 2.
Let , τ, and be defined by (5), (6), and (7), respectively. Assume that the function is a nonoscillatory solution of (1). If there exists a sequence of real numbers such that
and
then
Proof. Let
and
, for
, denote the
and
, respectively. Note that properties (
10) and (
8) give that
so
.
Due to the definition of limit inferior and (
20), for arbitrary
, so for
,
Hence,
and consequently,
Since
, condition (
19) ensures that
for every
and
. Besides that, (
18), (
19), and (
23) ensure that the sequence of intervals
satisfies the conditions of Lemma 1 with
. Therefore, there exists a sequence
such that
,
By (
22),
so, using (
24), we obtain
Property (
10) secures that
.
Since
x is a nonoscillatory solution of (
1), without loss of generality, we can assume that
For every
, property (
11) ensures that, for every
,
, thus
, so (
1), (
19), and (
27) provide
i.e.,
Consequently,
Also, (
11) ensures that
for every
. Therefore, (
9) and (
28) provide that
Summing up (
1) from
to
, we obtain
Hence, by (
25),
Similarly, summing up (
1) from
to
, we obtain
Therefore, (
26) implies
Combining inequalities (
30) and (
31), we get
i.e.,
Since
,
Using that
and
, we have
Consequently,
Since (
32) holds for arbitrarily small
, it implies (
21). The proof of the lemma is complete. □
Now we are ready to formulate and prove a new criterion that provides that all solutions of the observed difference equation are oscillatory.
Theorem 1.
For , τ and defined by (5), (6), and (7) respectively, assume that there exists a sequence of real numbers such that conditions (17)-(20) are satisfied. If
then all solutions of (1) are oscillatory.
Proof. As in the proof of the previous lemma, for , and denote the intervals and , respectively.
Supposing the opposite, let the function
be a nonoscillatory solution of (
1). Without loss of generality, we can assume that
Therefore (
11), (
1), (
19), and (
34) imply
Consequently, for every
,
Since (
11) ensures that
for every
, (
9) and (
35) provide that
For any
, summing up (
1) from
to
, then using that
and applying (
19), (
36), afterwards by (
19), (
10), and (
35), we have
Dividing the obtained inequality by
, that is positive, we obtain
i.e.,
Hence,
Applying (
21) from Lemma 2, we have
which is a contradiction to condition (
33). The proof of the theorem is complete. □
Due to the following corollary, the nonnegativity of the coefficients in the definition of
and coefficients in condition (
33) combined with property (
10) yield to conclusion that for
there is no need to check the condition (
33).
Corollary 1. For , τ and defined by (5), (6), and (7) respectively, assume that there exists a sequence of real numbers such that conditions (17)-(20) are satisfied. If , then all solutions of (1) are oscillatory.
Proof. Since
, condition (
19) and definition (
20) give
For
, the inequality
holds, so (
38) ensures that condition (
33) is satisfied and, based on Theorem 1, it implies that all solutions of (
1) are oscillatory. □
Notice that the oscillatory conditions in Theorem 1 and Corollary 1 require the nonnegativity of coefficients in the disjoint intervals and do not use the intervals where the coefficients are negative. Therefore, the presented oscillatory conditions can be applied to establishing the oscillatory property of solutions of difference equations in form (
1) but with positive coefficients.
3. Examples and Comparisons
The following examples illustrate the presented conditions for oscillatory solutions of the observed difference equation. For first two examples, the oscillatory conditions from Theorem 1 are satisfied, but the oscillatory conditions from Corollary 1 and oscillatory conditions from [
25] are not fulfilled. The last example shows the application of oscillatory conditions from Corollary 1 on delay difference equation with unbounded delays. Moreover, oscillatory conditions from [
25] are not satisfied for that example either.
Theorem 2 ([
25, Theorem 2.2]).
For the functions τ and defined by (6) and (7) respectively, assume that there exists a sequence of real numbers such that condition (17) holds and the intervals of the sequence are nonempty, disjoint, and contained in . If, in addition,
and
then all solutions of (1) are oscillatory.
Theorem 3 ([
25, , Theorem 2.3]).
For the functions τ and defined by (6) and (7) respectively, assume that there exists a sequence of real numbers such that condition (17) holds and the intervals of the sequence are nonempty, disjoint, and contained in . If, moreover,
and there exists a real number such that
then all solutions of (1) are oscillatory.
Example 1.
Consider the difference equation
where functions and are periodic, with the basic period 10, such that
Here, and , thus and . Therefore, and . For the sequence of real numbers such that ,
so, for every ,
It means that conditions (17), (18), and (19) are satisfied with
Due to and
condition (33) is also fulfilled, thus all conditions of Theorem 1 are satisfied, and therefore all solutions of equation (43) are oscillatory.
The graphs of the functions and , the intervals , and relevant points from conditions (20) and (33) are presented at Figure 1. Figure 2 shows the graphs of some solutions of Eq. (43).
Conditions of Theorem 3 cannot be fulfilled since the length of intervals of condition (41) are expanding as j increases, but the functions and are nonnegative only on the interval with length 7. Therefore, the oscillatory conditions of Theorem 3 cannot be satisfied.
The oscillatory conditions of Theorem 2 also cannot be satisfied. Namely, for any sequence of real numbers such that condition (39) is fulfilled,
Besides that, and are for with , so . Therefore,
Consequently, condition (40) cannot be fulfilled.
Example 2.
Conditions of Theorem 1 are satisfied for equation
with
and
so all solutions of equation (44) are oscillatory.
Namely, and , thus and . Therefore, and . For every ,
For the sequence of real numbers such that ,
so, for ,
Hence, conditions (17), (18), and (19) are satisfied and
Since and
also condition (33) holds, so all conditions of Theorem 1 are fulfilled.
The graphs of the functions and , the intervals , and relevant points from conditions (20) and (33) are presented at Figure 3. Figure 4 shows the graphs of some solutions of Eq. (44).
Now, we show that the oscillatory conditions of Theorem 2 cannot be fulfilled. For any sequence of real numbers such that condition (39) holds,
so . Therefore, using that the functions and are nonincreasing on ,
Consequently, condition (40) cannot be satisfied.
At the end, we show that the oscillatory conditions of Theorem 3 cannot be fulfilled. For any sequence of real numbers such that condition (41) holds,
so . Hence,
Using that the functions and are nonincreasing on and the fact that for ,
Consequently, condition (42) cannot be fulfilled.
Example 3.
Consider the difference equation
with
and
where denotes the integer part.
Delay functions, and , are unbounded, but satisfy conditions (3) and (4). and , thus, for the sequence of real numbers such that ,
Therefore,
so conditions (17), (18), and (19) are satisfied. Besides,
implying that
Hence,
Consequently, conditions of Corollary 1 are satisfied, so all solutions of Eq. (45) are oscillatory.
The graphs of the functions and , the intervals , and relevant points from condition (20) are presented at Figure 5. Figure 6 shows the graphs of some solutions of Eq. (45).
The oscillatory conditions of Theorem 2 cannot be satisfied since for any sequence of real numbers such that condition (39) is fulfilled, for some , so
Hence,
Using that ,
and therefore
Since the intervals of sequence are disjoint, implies that , so inequality (46) gives
Consequently, condition (40) cannot be fulfilled.
Conditions of Theorem 3 also cannot be fulfilled since there is no sequence of real numbers such that condition (41) is satisfied. Namely, by condition (41), there is a sequence of real numbers such that
for some . The length of interval are expanding as n increases and the length of interval is . Even for ,
so the length of interval is . Since for every , the condition (47) cannot be fulfilled for any integer and . Hence, the oscillatory conditions of Theorem 3 cannot be satisfied.
4. Conclusions
Our study of the oscillatory properties of the solutions of the first-order difference equations with continuous time, piecewise linear delay functions, and oscillatory coefficients has led us to the new condition that ensures the oscillatory solutions. By the proposed results, the oscillatory property of all solutions of the considered difference equation is ensured by sufficiently positive coefficients of the equation in the sense that the sum of the values of the coefficients defined by
in (
20) is in the interval
. For
, the oscillatory property of all solutions is ensured when condition (
33) is fulfilled.
We have shown, through examples, that there are difference equations for which the previously known oscillatory conditions for the same type of difference equations are not applicable, but the proposed criteria are satisfied. Therefore, we have extended the set of difference equations with oscillatory coefficients for which conditions verifying their oscillatory properties exist.
Author Contributions
Conceptualization, G.E.C. and H.P.; methodology, H.P. and A.R.; investigation, H.P. and A.R.; writing—original draft preparation, A.R.; writing—review and editing, G.E.C., H.P. and A.R. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Conflicts of Interest
The authors declare no conflicts of interest.
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