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On a class of second-order nonlinear difference equation
Advances in Difference Equations volume 2011, Article number: 46 (2011)
Abstract
In this paper, we consider the rule of trajectory structure for a kind of second-order rational difference equation. With the change of the initial values, we find the successive lengths of positive and negative semicycles for oscillatory solutions of this equation, and the positive equilibrium point 1 of this equation is proved to be globally asymptotically stable.
Mathematics Subject Classification (2000)
39A10
1 Introduction and preliminaries
Motivated by those work [1–17], especially [10], we consider in this paper the following second-order rational difference equation
the initial values x -1, x 0 ∈ (0, +∞), a ∈ (0, +∞) and k, l ∈ (-∞, +∞).
Mainly, by analyzing the rule for the length of semicycle to occur successively, we describe clearly out the rule for the trajectory structure of its solutions and further derive the global asymptotic stability of positive equilibrium of Equation (1.1).
It is easy to see that the positive equilibrium of Equation (1.1) satisfies
From this, we see that Equation (1.1) possesses a positive equilibrium . In this paper, our work is only limited to positive equilibrium .
Here, for readers' convenience, we give some corresponding definitions.
Definition 1.1. A positive semicycle of a solution of Equation (1.1) consists of a string of terms {x r , x r+1, ..., x m }, all greater than or equal to the equilibrium , with r ≥ -1 and m ≤ ∞ such that
and
A negative semicycle of a solution of Equation (1.1) consists of a string of terms {x r , x r+1, ..., x m }, all less than the equilibrium , with r ≥ -1 and m ≤ ∞ such that
and
The length of a semicycle is the number of the total terms contained in it.
Definition 1.2. A solution of Equation (1.1) is said to be eventually positive if x n is eventually greater than . A solution of Equation (1.1) is said to be eventually negative if x n is eventually smaller than .
Definition 1.3. We can divide the solutions of Equation (1.1) into two kinds of types: trivial ones and nontrivial ones. A solution of Equation (1.1) is said to be eventually trivial if x n is eventually equal to ; otherwise, the solution is said to be nontrivial.
If the solution is a nontrivial solution, then we can further divide the solution into two cases: non-oscillatory solution and oscillatory solution. A nontrivial solution of Equation (1.1) is regarded as non-oscillatory solution if x n is eventually positive or negative; otherwise, the nontrivial solution is oscillatory.
2 Trajectory structure rule
The solutions of Equation (1.1) include trivial ones, non-oscillatory ones and oscillatory ones, and their trajectory structure rule of the solutions is as follows.
2.1 Nontrivial solution
Theorem 2.1. A positive solution of Equation (1.1) is eventually trivial if and only if
Proof. Sufficiency. Assume that Equation (2.1) holds. Then according to Equation (1.1), we know that the following conclusions are true:
-
(i)
If x -1 = 1, then x n = 1 for n ≥ 1.
-
(ii)
If x 0 = 1, then x n = 1 for n ≥ 1.
Necessity. Conversely, assume that
Then, we can show x n ≠1 for any n ≥ 1. For the sake of contradiction, assume that for some N ≥ 1,
Clearly,
From this, we can know that
which implies x N-1= 1, or x N-2= 1. This contradicts with Equation (2.3).
Remark 2.2. Theorem 2.1 actually demonstrates that a positive solution of Equation (1.1) is eventually nontrivial if (x -1 - 1)(x 0 - 1) ≠0. So, if a solution is a nontrivial one, then x n ≠1 for any n ≥ -1.
2.2 Non-oscillatory solution
Lemma 2.3. Let be a positive solution of Equation (1.1) which is not eventually equal to 1, then the following conclusion is true:
-
(A)
If kl < 0, then (x n+1- 1)(x n - 1)(x n-1- 1) < 0, for n ≥ 0;
-
(B)
If kl > 0, then (x n+1- 1)(x n - 1)(x n-1- 1) > 0, for n ≥ 0;
Proof. First, we consider (A). According to Equation (1.1), we have that
Considering kl < 0,
Noting that kl < 0, that is k ∈ (-∞, 0) and l ∈ (0, +∞), or k ∈ (0, +∞ -∞, 0), and l ∈ (-∞, 0), one has , , or , . From those, one can get the result easily.
The proof of (B) is similar to (A).
Theorem 2.4. Let kl < 0, there exist non-oscillatory solutions of Equation (1.1) with x -1, x 0 ∈ (0, 1), which must be eventually negative. There do not exist eventually positive non-oscillatory solutions of Equation (1.1).
Proof. Consider a solution of Equation (1.1) with
We then know from Lemma 2.3 (A) that 0 < x n < 1 for n ∈ N, where N ∈ 1, 2, 3, .... So, this solution is just a non-oscillatory solution and furthermore eventually negative.
Suppose that there exists eventually positive non-oscillatory of Equation (1.1). Then, there exists a positive integer N such that x n > 1 for n ≥ N. Thereout, for n ≥ N + 1,
This contradicts Lemma 2.3. So, there do not exist eventually positive non-oscillatory of Equation (1.1), as desired.
From Lemma 2.3 (B), we can get the result as follows, also.
Theorem 2.5. Let kl > 0, there exist non-oscillatory solutions of Equation (1.1) with x -1, x 0 ∈ (1, +∞), which must be eventually positive. There do not exist eventually negative non-oscillatory solutions of Equation (1.1).
2.3 Oscillatory solution
Theorem 2.6. Let kl < 0, and be a strictly oscillatory of Equation (1.1), then the rule for the lengths of positive and negative semicycles of this solution to occur successively is ..., 2+, 1-, 2+, 1-, ....
Proof. By Lemma 2.3, one can see that the length of a negative semicycle is at most 3, and a positive semicycle is at most 2. On the basis of the strictly oscillatory character of the solution, we see that, for some integer p ≥ 0, one of the following 32 cases must occur:
case 1: x p < 1, x p+1< 1;
case 2: x p > 1, x p+1< 1;
case 3: x p < 1, x p+1> 1;
case 4: x p > 1, x p+1> 1.
case 1 cannot occur. Otherwise, the solution is a non-oscillatory solution of Equation (1.1).
If Case 2 occurs, it follows from Lemma 2.3 that x p+2> 1, x p+3> 1, x p+4< 1, x p+5> 1, x p+6> 1, x p+7< 1, x p+8> 1, x p+9> 1, x p+10< 1, ....
This means that rule for the lengths of positive and negative semicycles of the solution of Equation (1.1) to occur successively is ..., 2+, 1-, 2+, 1-, .... The proof for other cases, except Case 1, is completely similar to that of Case 2. So, the proof for this theorem is complete.
Theorem 2.7. Let kl > 0, and be a strictly oscillatory of Equation (1.1), then the rule for the lengths of positive and negative semicycles of this solution to occur successively is ..., 1+, 2-, 1+, 2-, ....
The proof of theorem (2.7) is similar to that of theorem (2.6).
3 Local asymptotic stability and global asymptotic stability
Before stating the oscillation and non-oscillation of solutions, we need the following key lemmas. For any integer a, denote N a = {a, a + 1, ...,}.
3.1 Four Lemmas
Lemma 3.1. Let k ∈ (0, 1], and be a positive solution of Equation (1.1) which is not eventually equal to 1, then the following conclusions are valid:
(a) (x n+1- x n )(x n - 1) < 0, for n ≥ 0;
(b) (x n+1- x n-1)(x n-1- 1) < 0, for n ≥ 0.
Proof. First, we consider (a). From Equation (1.1), we obtain
From k ∈ (0, 1] and not eventually equal to 1, one can see that
This teaches us that (x n+1- x n )(1 - x n ) > 0, n = 0, 1, .... That is to say, (x n+1- x n )(x n - 1) < 0, n = 0, 1, .... So, the proof of (a) is complete.
Second, one investigates (b). From Equation (1.1), one has
From Equation (1.1), one gets
According to k ∈ (0, 1] and not eventually equal to 1, one arrives at
From Equations (3.2) and (3.3), we know . So, we can get immediately
From Equation (1.1), one can have
According to k ∈ (0, 1] and not eventually equal to 1, one arrives at
From Equations (3.5), (3.6), we can obtain that , i.e.,
By virtue of Equations (3.1), (3.4), (3.7), we see that (b) is true.
The proof for Lemma (3.1) is complete.
Lemma 3.2. Let be a positive solution of Equation (1) which is not eventually equal to 1, then (x n+1- x n-2)(x n-2- 1) < 0, for n ≥ 1.
Proof. By virtue of Equation (1.1), one gets
By virtue of Equation (1.1), one obtains that
According to k ∈ (0, 1] and not eventually equal to 1, we get
So,
That is
By virtue of Equation (1.1), we can know
Utilizing (3.11),(3.12), adding , when k ∈ (0, 1], we know the following is true
So,
Similar to (3.13), we know this is true
So,
From (3.8),(3.13)and (3.14), one obtains that the following is true
This shows Lemma (3.2) is true.
Lemma 3.3. Let x -1, x 0 ∈ (0, 1), then the following conclusions are true:
-
(a)
If l > 0 and -1 < k < 0 or l < 0 and 0 < k <1, then (x n+1- x n ) < 0, for n ≥ 0;
-
(b)
If k > 0 and -1 < l < 0 or k < 0 and 0 < l < 1, then (x n+1- x n-1) < 0, for n ≥ 0.
The proof of lemma (3.3) can be completed by Equation (1.1), theorem 2.4 and properties of power function easily.
Lemma 3.4. Let x -1, x 0 ∈ (1, ∞), then the following conclusions are true:
(a) If l > 0 and 0 < k < 1 or l < 0 and -1 < k < 0, then (x n+1- x n ) < 0, for n ≥ 0;
(b) If k > 0 and 0 < l < 1 or k < 0 and -1 < l < 0, then (x n+1- x n-1) < 0, for n ≥ 0.
The proof of lemma (3.4) can be completed by Equation (1.1), theorem 2.5 and properties of power function easily.
First, we consider the local asymptotic stability for unique positive equilibrium point of Equation (1.1). We have the following results.
3.2 Local asymptotic stability
Theorem 3.5. The positive equilibrium point of Equation (1.1) is locally asymptotically stable.
Proof. The linearized equation of Equation (1.1) about the positive equilibrium point is
and so it is clear from the paper [[2], Remark 1.3.7] that the positive equilibrium point of Equation (1.1) is locally asymptotically stable. The proof is complete.
We are now in a position to study the global asymptotically stability of positive equilibrium point .
3.3 Global asymptotic stability of oscillatory solution
Theorem 3.6. The positive equilibrium point of Equation (1.1) is globally asymptotically stable when k ∈ (0, 1] and l ∈ (0, +∞).
Proof We must prove that the positive equilibrium point of Equation (1.1) is both locally asymptotically stable and globally attractive. Theorem 3.5 has shown the local asymptotic stability of . Hence, it remains to verify that every positive solution of Equation (1.1) converges to as n → ∞. Namely, we want to prove
Consider now {x n } to be non-oscillatory about the positive equilibrium point of Equation (1.1). By virtue of Lemma 3.1(a), it follows that the solution is monotonic and bounded. So, lim n→∞ x n exists and is finite. Taking limits on both sides of Equation (1.1), one can easily see that (3.15) holds.
Now let {x n } be strictly oscillatory about the positive equilibrium point of Equation (1.1). By virtue of Theorem 2.6, one understands that the rule for the lengths of positive and negative semicycles occurring successively is ..., 2+, 1-, 2+, 1-, 2+, 1-, .... For simplicity, for some nonnegative integer p, we denote by {x p , x p+1}+ the terms of a positive semicycle of length two, followed by {x p+2}-, a negative semicycle with semicycle length one, then a positive semicycle of length two and a negative semicycle of length one, and so on. Namely, the rule for the lengths of positive and negative semicycles to occur successively can be periodically expressed as follows:
Lemma (3.1) (a), (b) and Lemma (3.2) teaches us that the following results are true:
-
(A)
x p+3n > x p+3n+1> x p+3n+3> x p+3n+4, n = 0, 1, 2, ....
-
(B)
x p+3n+2< x p+3n+5< x p+3n+8, n = 0, 1, 2, ....
So, from (A) one can see that is decreasing with lower bound 1. So, the limit S = lim n→∞ x p+3n exists and is finite.
Furthermore, From (A) one can further obtain
Similarly, by (B) one can see that is increasing with upper bound 1. So, the limit T = lim n→∞ x p+3n+2exists and is finite.
Now, it suffices to prove S = T = 1.
Noting that
Taking limits on both sides of the Equations (3.16) and (3.17), respectively, we get
From this one can see S = 1. Again, by Equation (3.18), we have T = 1, too. These show that (3.15) is true. The proof for Theorem 3.6 is complete.
Theorem 3.7. The positive equilibrium point of Equation (1.1) is globally asymptotically stable when k ∈ (0, 1] and l ∈ (-∞, 0).
The proof of theorem 3.7 is similar to that of theorem 3.6 by virtue of theorem 3.5, theorem 2.7, Lemma (3.1), Lemma (3.2) and Equation (1.1).
3.4 Global asymptotic stability of non-oscillatory solution
Theorem 3.8. The positive equilibrium point of Equation (1.1) is globally asymptotically stable when x -1, x 0 ∈ (0, 1) and one of the following conditions is satisfied:
-
(a)
-1 < k < 0 and l > 0;
-
(b)
0 < k < 1 and l < 0;
-
(c)
> 0 and -1 < l < 0;
-
(d)
< 0 and 0 < l < 1.
The proof of theorem 3.8 is similar to that of theorem 3.6 by virtue of theorem 2.4, theorem 3.5, Lemma (3.3) and Equation (1.1).
Theorem 3.9. The positive equilibrium point of Equation (1.1) is globally asymptotically stable when x -1, x 0 ∈ (1, +∞) and one of the following conditions is satisfied:
-
(a)
-1 < k < 0 and l < 0;
-
(b)
0 < k < 1 and l > 0;
-
(c)
< 0 and -1 < l < 0;
-
(d)
> 0 and 0 < l < 1.
The proof of theorem 3.9 is similar to that of theorem 3.6 by virtue of theorem 2.5, theorem 3.5, Lemma (3.4) and Equation (1.1).
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6 Acknowledgements
The authors would like to thank the referees for giving useful suggestions and comments for the improvement of this paper. This research is supported by Social Science Foundation of Hunan Province of China (Grant no. 2010YBB287), Science and Research Program of Science and Technology Department of Hunan Province (Grant no.2010FJ3163, 2011ZK3066).
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4 Competing interests
The authors declare that they have no competing interests.
5 Authors' contributions
All authors carried out the proof. All authors conceived of the study and participated in its design and coordination. All authors read and approved the final manuscript.
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Dongsheng, L., Shuliang, Z. & Maoxin, L. On a class of second-order nonlinear difference equation. Adv Differ Equ 2011, 46 (2011). https://doi.org/10.1186/1687-1847-2011-46
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DOI: https://doi.org/10.1186/1687-1847-2011-46