Applied Mathematics and Computation 109 (2000) 301±306 www.elsevier.nl/locate/amc
A note on the periodic cycle of Xn2
1 Xn1=
Xn H.M. El-Owaidy, M.M. El-A®®
*
Mathematics Department, Faculty of Science Al-Azhar University, Nasr City, Cairo 11884, Egypt
Abstract n xn The behaviour of solutions of the dierence equation xn1 anxb ; n 0; 1; . . . ; nÿ1 are investigated, where the sequences an and bn are periodic. Ó 2000 Elsevier Science Inc. All rights reserved.
AMS classi®cation: 39A10; 39A99; 34C99 Keywords: Dierence equations; Oscillatory solutions
1. Introduction Kocic [1] has studied the behaviour of solutions of the dierence equation xn1
1 xn xnÿ1 xnÿk2 ; xnÿk1
n 0; 1; 2; . . . ;
1:1
where k is a nonnegative integer and xÿk ; . . . ; x0 are arbitrary positive numbers. The special cases of Eq. (1.1) for k 0; 1 and 2 are:
*
xn1
1 ; xn
xn1
1 xn ; xnÿ1
n 0; 1; . . . ; n 0; 1; . . . ;
Corresponding author.
0096-3003/00/$ - see front matter Ó 2000 Elsevier Science Inc. All rights reserved. PII: S 0 0 9 6 - 3 0 0 3 ( 9 9 ) 0 0 0 3 1 - 4
1:2
1:3
302
H.M. El-Owaidy, M.M. El-A®® / Appl. Math. Comput. 109 (2000) 301±306
xn1
1 xn xnÿ1 ; xnÿ2
n 0; 1; . . . ;
1:4
respectively. They have the property that every solution of each equation is periodic with period 2, 5 and 8, respectively, that is, for k 0, 1 and 2 the positive solutions of Eq. (1.1) are all periodic with period (3k + 2). The 5-cycle Eq. (1.3) was discovered by Lyness [2,3], while he was working on a problem in number theory. This equation has also applications in geometry [4]. In this paper we shall investigate the behaviour of the dierence equation an bn x n ; n 0; 1; . . . ; xnÿ1 where an and bn are periodic. xn1
1:5
De®nition 1. A sequence fxn g is said to oscillate about zero or simply to oscillate if the terms xn are neither eventually all positive nor eventually all negative. Otherwise the sequence is called nonoscillatory. De®nition 2. A sequence fxn g is called strictly oscillatory if for every n0 P 0, there exists n1 ; n2 P n0 such that xn1 xn2 < 0. De®nition 3. A sequence fxn g is said to oscillate about x if the sequence xn ÿ x oscillates, and it is called strictly oscillatory about x if the sequence xn ÿ x is strictly oscillatory. De®nition 4. A positive semicycle of fxn g of Eq. (1.5) consists of `string' of terms fxl ; xl1 ; . . . ; xm g all greater than or equal to x, with l P ÿ 1 and m < 1 and such that either
l ÿ1 or l > ÿ1 and xlÿ1 < x
either
m 1 or m < 1 and xm1 < x:
and
De®nition 5. A negative semicycle of fxn g of Eq. (1.5) consists of `string' of terms fxl ; xl1 ; . . . ; xm g all less than x, with l P ÿ 1 and m < 1 and such that either
l ÿ1 or l > ÿ1 and xlÿ1 P x
either
m 1 or m < 1 and xm1 P x:
and The ®rst semicycle of a solution of Eq. (1.5) starts with the term xÿ1 and is positive if xÿ1 P x and negative if xÿ1 < x.
H.M. El-Owaidy, M.M. El-A®® / Appl. Math. Comput. 109 (2000) 301±306
303
A solution may have a ®nite number of semicycles or in®nitely many semicycles. De®nition 6. A sequence fxn g is said to be periodic with period p if xnp xn
for
n 0; 1; . . .
1:6
De®nition 7. A sequence fxn g is said to be periodic with prime period p, or with minimal period p, if it is periodic with period p, where p is the least positive integer for which (1.6) holds. De®nition 8. A dierence equation is called a p-cycle, if every solution of it is periodic with period p. Consider the dierence equation xn1
a xn xnÿk2 ; xnÿk1
n 0; 1; . . . ;
1:7
where a 2 0; 1 and
k 2 f1; 2; . . .g:
1:8
The following theorems show that the solution of Eq. (1.7) is bounded from below and from above by positive constants. Theorem A [1]. Assume that (1.8) holds and that xÿk1 ; . . . ; x0 are arbitrary positive numbers then the soultion fxn g of equation (3.1) is such that " # kÿ1 k ÿ1 Y X 1 xn
k1j 1 constant; n 0; 1; . . .
1:9 a xn
k1j j0 j0 We note that, for a 1 and k 2, the invariance (1.9) appears in [3]. For a 1 and k > 2, (1.5) is due to [5]. Theorem A shows also, the solution xn is such that m 6 xn 6 M, where m and M are positive numbers. Theorem B [1]. Assume that a; b0 ; . . . ; bkÿ1 2
0; 1 with a
kÿ1 X
bi > 0
and
k 2 f1; 2; . . .g
i0
then every nontrivial solution of the equation, xn1
a b0 xn bkÿ1 xnÿk1 ; xnÿk
n 0; 1; . . .
1:10
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H.M. El-Owaidy, M.M. El-A®® / Appl. Math. Comput. 109 (2000) 301±306
is strictly oscillatory about the positive equilibrium x of this equation. Furthermore, every semicycle of a nontrivial solution contains no more than (2k + 1) terms. For the dierence equation a bxn ; n 0; 1; . . .
1:11 xnÿ1 when a 0 and b 2
0; 1, every solution of Eq. (1.11) is periodic with period six. When a 2
0; 1 and b 0, every solution of Eq. (1.11) is periodic with period four. if a; b 2
0; 1, by change of variables, xn byn reduces Eq. (1.11) to xn1
a xn ; xnÿ1 where a a=b2 . xn1
n 0; 1; . . .
1:12
Theorem C [1]. If a; b 2
0; 1, then every positive solution of Eq. (1.11) is bounded away from zero and in®nity by positive constants, and every nontrivial solution of this equation is strictly oscillatory about the positive equilibrium x of Eq. (1.11). Furthermore, every semicycle of nontrivial solution contains at most three terms. Theorem D [1]. If a; b 2
0; 1, then the following statements about the positive solutions of Eq. (1.11) are true: (a) The absolute extreme in a semicycle occurs in the ®rst or in the second term. (b) Every nontrivial semicycle, after the ®rst one, contains at least two and at most three terms. Theorem E [1]. Assume that a P 0 and let fxn g be a positive solution of Eq. (1.12) then for n 0; 1; . . . ; the following statments are true:
1 , (i) yn5 ÿ yn
1 ÿ a
1=yn2 ÿ yn3 (ii) yn6 ÿ yn a
1
1=yn3
1=yn4 ÿ
1=yn2 : This theorem shows that, the solutions of Eq. (1.12) are periodic with period ®ve i a 1, and are periodic with period six i a 0. 2. Main result In this section we investigate the behaviour of solutions of the dierence equation xn1
an bn x n ; xnÿ1
n 0; 1; . . .
2:1
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305
with 1 X 1 < 1; b n0 n
2:2
where fan g and fbn g are periodic sequences, Lemma 2.1. If the sequence fbn g satis®es bn1 bnÿ1 1; n 0; 1; . . . ; then fbn g is periodic with period four. Proof. Since bn1 bnÿ1 1, then bn1
1 bnÿ1
and also bn2
1 bn
and
bn3
1 bn1
which gives bn4
1 1 bn bn2 1=bn
and hence fbn g is periodic with period four. Theorem 2.1. If the sequence fbn g is periodic with period four and fan g is periodic with period one, then all results in Theorems D and E are true for the solution of Eq. (2.1). Proof. Since fan g is periodic with period one, then an1 an , which has a solution an constant, say a. The change of variables xn bn yn reduces Eq. (2.1) to yn1 bn1 bnÿ1
a yn : ynÿ1
2:3
Since fbn g is periodic with period four, then by using Lemma 2.1, Eq. (2.3) takes the form yn1
a yn ynÿ1
2:4
which has the same form of Eq. (1.12) and has the same results of Theorems D and E.
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References [1] V.L. Kocic, G. Ladas, I.W. Rodrigues, On rational recursive sequences, J. Math. Anal. Appl. 173 (1993) 127±157. [2] R.C. Lyness, Note 1581, Math. Gaz 26 (1942) 62. [3] R.C. Lyness, Note 1847, Math. Gaz 29 (1945) 231. [4] J. Leech, The rational cubiod revisited, Amer. Math. Monthly 84 (1977) 518±533. [5] Y. Jianslle, H. Xuli, Private communication.