Abstract

We will consider oscillation criteria for the second order difference equation with forced term (). We establish sufficient conditions which guarantee that every solution is oscillatory or eventually positive solutions converge to zero.


In the last thirty years, there has been an increasing interest in the study of oscillation and asymptotic behavior of solutions of second order difference equations (see [111]). In [1], Arul and Thandapani considered the equation and gave some sufficient conditions for the existence of positive solutions. In [3], Saker considered the equation and gave some sufficient conditions which guarantee that every solution is oscillatory. Following this trend, we are concerned with oscillation criteria of solutions for a second order difference equation with forced term where is a positive sequence, is a nonnegative sequence and not identically zero for all large , is a real sequence, is a real number, and , are nonnegative integers, .

A solution of (3) is said to be eventually positive if for all large and eventually negative if for all large . Equation (3) is said to be oscillatory if it is neither eventually positive nor eventually negative.

In order to obtain our conclusions, we first give two lemmas.

Lemma 0.1. If difference inequality is oscillation, then difference equation is oscillation.

Otherwise, if (5) has eventually positive solution, then (4) has eventually positive solution; this is contradictory.

Lemma 0.2. Suppose that is an eventually positive solution of (3), , and(i), (ii), (iii). Set . Then and

Proof. Suppose that is an eventually positive solution of (3), then there exists , such that , , and for , then for . By summing up (3) from to , we obtain From (6), we know that , where α is a positive limited number or . Thus , β is a limited number or .
If ( is a constant), then there exist , for , so that which is contrary to .
If , then there exist , for ; hence, therefore, ; thus, there exist , , and () for . By summing up (3) from to, we obtain As , the right-hand side of (9) is bounded, but the left-hand side of (9) tends to ; this is contradictory.
Then ; thus . This completes the proof.

By means of Lemma 0.2, we obtain the following.

Theorem 0.3. If conditions (i), (ii), and (iii) hold and is an eventually positive solution of (3), then .

Proof. Making use of (6) and the conclusion of Lemma 0.2, we know so . If not, suppose that , then there exist ,  for . Now substitute for in (6), we obtain a contrary. This completes the proof.

Theorem 0.4. If conditions (i), (ii), and (iii) hold, let and if is oscillation, then (3) is oscillation.

Proof. Suppose that is an eventually positive solution of (3), then there exist , , , and for . From (6), we have Letting and making use of Lemma 0.2, we get or By summing up (14) from to , we obtain In view of Theorem 0.3, we know that , then there exists a sequence , such that , , and ; by means of (15), we have so This shows that is nonoscillatory, which is a contradiction. This completes the proof.

The oscillation of is only the sufficient condition for the oscillation of (3). The following examples will illustrate this point.

Example 0.5. Consider the difference equation Here, is nonoscillatory, and the other conditions (i), (ii), and (iii) are satisfied. Equation (18) has the nonoscillatory solution .

Example 0.6. Consider the difference equation Here, is oscillatory, and the conditions (i), (ii), and (iii) are satisfied. Equation (19) is oscillation.

Example 0.7. Consider the difference equation Here, is nonoscillatory, and the other conditions (i), (ii), (iii) are satisfied. But (20) has the oscillatory solution .

Remarks:
(1)When , Theorems 0.3 and 0.4 still hold.(2)As , Lemma 0.2, Theorems 0.3, and 0.4 still hold. In Theorem 0.4, It has been discussed that . We have the following conclusion as . Set If is an eventually positive solution of (3), then there exist , for . Thus, Therefore, we obtain the following

Theorem 0.8. As , if difference inequality (4) is oscillation, then difference equation (3) is oscillation.

Acknowledgments

This work is supported by the National Natural Science Foundation of China (Grant no. 60771026), the Program for international cooperation of Shan’xi Province (Grant no. 2010081005), and the Natural Science Foundation of Shan’xi Province (Grant no. 2010011007).