On the higher order rational recursive sequence xn=Axn-k+Bxn-3k

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Abstract

The main purpose of the current paper is to prove that every positive solution of the delay difference equationxn=Axn-k+Bxn-3k,where A, B  (0, ∞), the initial conditions x−3k+1, x−3k+2, …, x0  (0, ∞) and k  {1, 2, 3, …}, converges eventually to a period-k solution. We also give the results of computational examples to support our theoretical discussion.

Section snippets

Preliminaries

Consider the recursive sequencexn=Axn-k+Bxn-3k,n=1,2,,where A, B  (0, ∞), k  {1, 2, 3, …}, and the initial conditions x−3k+1, x−3k+2, …, x0, are arbitrary positive real numbers. We investigate the periodic character of the positive solution of Eq. (1) and we shall show that the sequence {xn} converges eventually to a period-k solution. This confirms Conjecture 4.8.1 in [10], [11] given by Ladas and his co-workers for the above mentioned particular case.

Basically, we generalize some of the results due to

Local stability of Eq. (3)

In this section, we discuss locally asymptotically stable of Eq. (3).

Letf(x,y)=C+xy,assume thatpp(y¯,y¯)=f(y¯,y¯)x=1y¯=1C+1andqq(y¯,y¯)=f(y¯,y¯)y=-1y¯=-1C+1,denote the partial derivates of f(x, y) evaluated at the equilibrium point y¯ of Eq. (3). Then the equationzn=pzn-k+qzn-2k=1C+1zn-k-1C+1zn-2kis called the Linearized equation associated with Eq. (3) about the equilibrium point y¯. Its characteristic equation isλ2k-1C+1λk+1C+1=0.By substituting θ = λk, it turns to the following equation:θ2

Analysis of semi-cycle and global stability of Eq. (3)

In this section, first we investigate the semi-cycle of Eq. (3). Next we consider the global behavior of solutions of it and we prove that the equilibrium y¯ is globally asymptotically stable for all C > 0.

Definition 3

Let {yn}n=-2k+1 be a positive solution of Eq. (3). A positive semi-cycle of {yn}n=-2k+1 consists of a “string” of terms {yl, yl+1 …, ym}, all greater than or equal to the equilibrium y¯, with l  −2k + 1 and m  ∞ and such thateitherl=-2k+1,orl>-2k+1,andyl-1<y¯,andeitherm=,orm<,andym+1<y¯.

Definition 4

Let {yn}n=-

The periodic behavior of the solution of Eq. (1)

Here we show that the equilibrium of the solution of Eq. (1) is periodic with period k.

From Eq. (1), we obtainx2n=Ax2n-k+Bx2n-3k,andx2n-k=Ax2n-2k+Bx2n-4k.So it follows thatx2n=AAx2n-2k+Bx2n-4k+BAx2n-4k+Bx2n-6k.The following statements outline properties of the Eq. (1). Their proofs are based on Eq. (14).

Lemma 2

Let {xn} be a positive solution of Eq. (1). Then the following statements hold.

  • (i)

    For N > 0, letmN=Min{x2N-4k,x2N-2k,x2N},andMN=Max{x2N-4k,x2N-2k,x2N}.ThenmNx2N+2lkMNforl1.

  • (ii)

    There exist positive

Numerical discussion

In this section, we present two test examples to support our theoretical discussion.

Example 1

Assume that Eq. (1) hold, k = 2 and A = B = 1. So the equation reduces to the following:xn=1xn-2+1xn-6.Using the change of variableyn=xnxn-2,the corresponding equation will be as follows:yn=1+yn-2yn-4.In this part, to illustrate the result of this paper a numerical example is given, which was carried out using Maple 7. We assume A = B = 1 and the initial points x−5, x−4, …, x0 in the following table.

nxnnxnnxnnxn
−53.0520

Conclusion

The results of this paper are generalizations of those of DeVault [2]. This solves the conjecture of Ladas and his co-workers [5], [6] for some special cases. However, the general case is still open. By a change of variable, we deduce a new difference equation which involves some interesting results in its own right. For instance, it has a unique positive equilibrium which is oscillatory and globally attractive. This was used to show that every positive solution of Eq. (1) converges to a

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  • Cited by (4)

    1

    Department of Mathematics and Statistics, University of Laval, Quebec, Canada.

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