Volume 2010, Article ID 367492,15pages doi:10.1155/2010/367492
Research Article
Global Behavior of Two Families of Nonlinear Symmetric Difference Equations
Wanping Liu,
1Xiaofan Yang,
1, 2and Luxing Yang
31College of Computer Science, Chongqing University, Chongqing 400044, China
2School of Computer and Information, Chongqing Jiaotong University, Chongqing 400074, China
3College of Mathematics and Statistics, Chongqing University, Chongqing 400044, China
Correspondence should be addressed to Wanping Liu,wanping [email protected] Received 14 May 2010; Revised 3 June 2010; Accepted 16 June 2010
Academic Editor: Josef Diblik
Copyrightq2010 Wanping Liu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We mainly investigate the global asymptotic stability and exponential convergence of positive solutions to two families of higher-order difference equations, one of which was recently studied in Stevi´c’s paper 2010. A new concise proof is given to a quite recent result by Stevi´c and analogous parallel result of the other inverse equation, which extend related results of Aloqeili 2009, Berenhaut and Stevi´c2007, and Liao et al.2009.
1. Introduction
The interest in investigating rational difference equations has a long history; for instance, see 1–24and the references cited therein. More generally, it is meaningful to study not only rational recursive equations but also those with powers of arbitrary positive degrees.
For instance, at many conferences, Stevi´c proposed to study the behavior of positive solutions of the following generic difference equationsee also25:
xnAxpn−m
xqn−k, n∈N0, 1.1
whereA, p, q >0, andk, m∈N, k /m. For some recent results in this area, see26–32and the references therein.
By a useful transformation method from 4, the authors of 3 confirmed that the unique positive equilibrium of the rational recursive equation
yn yn−kyn−m
1yn−kyn−m, n∈N0, 1.2
where 1≤k < m, is globally asymptotically stable for all solutions with positive initial values.
In the meantime, they also remarked that the global asymptotic stability for the unique equilibrium of the difference equation
yn 1yn−kyn−m
yn−kyn−m , n∈N0, 1.3
can be shown through analogous calculations. Some particular cases of1.3had already been considered in12,13.
In3were proposed the following two conjectures.
Conjecture 1.1. Suppose that 1≤k < l < mand that{yn}satisfies yn yn−kyn−lyn−myn−kyn−lyn−m
yn−kyn−lyn−kyn−myn−lyn−m1, n∈N0, 1.4 with positive initial values. Then, the sequence{yn}converges to the unique positive equilibrium point y1.
Some special cases of1.4had been studied by Li9,10with a semicycle analysis method, which is useful for lower-order difference equations but tedious and complicated to some extentsee the explanation in33. Finally,Conjecture 1.1was also confirmed in2 with the similar transformation method used in3,4. However, it is somewhat harder to prove the following conjecture in the same way.
Conjecture 1.2. Assume thatqis odd and 1≤ k1 < k2 < · · ·< kq, and defineS {1,2, . . . , q}. If {yn}satisfies
yn f1
yn−k1, yn−k2, . . . , yn−kq f2
yn−k1, yn−k2, . . . , yn−kq, n∈N0, 1.5
with y−kq, y−kq1, . . . , y−1 ∈0,∞, where
f1
x1, x2, . . . , xq
q ii1odd
{t1,t2,...,ti}⊂S t1<t2<···<ti
xt1xt2· · ·xti,
f2
x1, x2, . . . , xq
1 q−1
ii2even
{t1,t2,...,ti}⊂S t1<t2<···<ti
xt1xt2· · ·xti.
1.6
Then the sequence{yn}converges to the unique positive equilibrium pointy1.
Next, we present two definitions as defined in1.
Definition 1.3. A function ofnvariables is symmetric if it is invariant under any permutation of its variables. That is, a functionϕx1, . . . , xnis called symmetric if
ϕx1, . . . , xn ϕ
xπ1, . . . , xπn
, 1.7
whereπiis any permutation of the numbers{1,2, . . . , n}.
Definition 1.4. Thekth elementary symmetric functionσkof variablesx1, . . . , xn, wherek ∈ {1,2, . . . , n}is defined by
σkx1, . . . , xn
i1<i2<···<ik
xi1xi2· · ·xik, 1.8
where the sum is taken over allCnk choices of the indicesi1, . . . , ik from the set of integers {1,2, . . . , n}.
Obviously, the functions f1, f2 defined by1.6and 1.7are symmetric and can be rewritten as
f1
x1, x2, . . . , xq
q ii1odd
σi, f2
x1, x2, . . . , xq
1 q−1
ii2even
σi. 1.9
In this paper, we give a new proof of a quite recent result by Stevi´c in34where he, among others, studied the stability of one of the following two difference equations, which are dual:
yn f2 yn−kr
1, yrn−k
2, . . . , yn−kr q f1
yn−kr
1, yrn−k
2, . . . , yn−kr q, n∈N0, 1.10
yn f1
yn−kr
1, yrn−k
2, . . . , yn−kr q f2
yn−kr
1, yrn−k
2, . . . , yn−kr q, n∈N0, 1.11
where 3≤q∈Nis odd,r ∈0,1and 1≤k1< k2<· · ·< kq.
Apparently, Equation1.11is the generic form of1.2,1.4, and1.5.
In6,18the authors proved that the main results in some of papers9–12are direct consequences of a result confirmed by Kruse and Nesemann35. For example, in6was showed that the main result in13is also a consequence of Corollary 3 in35. On basis of these works, in 2008, Aloqeili1confirmedConjecture 1.2in the same way.
Later, Liao et al.14 provedConjecture 1.2 by using a new approach. They used a sort of “frame sequences” methodthe notion suggested by Stevi´c, which has been widely used in5,7,18,36–41. Through careful analysis, we find that the method used in14can be further simplified and applied in proving Stevi´c’s result in a more concise and interesting way. Namely, we give a new proof of the following result, which generalizes related results in1,2,9,10,14.
Theorem 1.5. Assume thaty−kq, y−kq1, . . . , y−1∈0,∞, r ∈0,1,3≤q∈Nis odd and positive integersk1, k2, . . . , kqare satisfying 1≤k1< k2<· · ·< kq. Then
1the unique positive equilibrium pointy1 of 1.10is globally asymptotically stable;
2the unique positive equilibrium pointy1 of 1.11is globally asymptotically stable.
2. Auxiliary Results and Notation
In this section, we will introduce some useful notation and lemmas. Consider the following notationfor similar ones see14, which play an important role in the paper:
α
x1, x2, . . . , xq 1
2 q
i1
xir1
− q
i1
xir−1 ,
β
x1, x2, . . . , xq 1
2 q
i1
xir1
q i1
xir−1 .
2.1
Employingαandβ, define a mappingΦ1:Rq → Ras follows:
Φ1
x1, x2, . . . , xq α
x1, . . . , xq β
x1, . . . , xq q
i1
xri 1
−q i1
xri −1 q
i1
xri 1 q
i1
xri −1. 2.2
Then1.10can be rewritten as
yn q
i1
yrn−ki1
−q i1
yn−kr i−1 q
i1
yrn−ki1 q
i1
yn−kr i−1, n∈N0, 2.3
or
yn Φ1
yn−k1, yn−k2, . . . , yn−kq
, n∈N0, 2.4
with 3≤q∈Nbeing odd, andr∈R.
By the notation defined by2.1, define the other functionΦ2:Rq → Rsuch that:
Φ2
x1, x2, . . . , xq β
x1, . . . , xq α
x1, . . . , xq q
i1
xri 1 q
i1
xri −1 q
i1
xri 1
−q i1
xri −1. 2.5
Then1.11can be rewritten as
yn q
i1
yrn−ki1 q
i1
yn−kr i−1 q
i1
yrn−ki1
−q i1
yn−kr i−1, n∈N0, 2.6
or
yn Φ2
yn−k1, yn−k2, . . . , yn−kq
, n∈N0, 2.7
with 3≤q∈Nbeing odd, andr∈R.
Lemma 2.1. Ifr∈0,1, then both2.4and2.7have the unique positive equilibrium pointy1.
Proof. Suppose thatλ1>0 is an equilibrium of2.4, then
λ1 Φ1λ1, . . . , λ1
λr11q− λr1−1q
λr11q
λr1−1q, 2.8
which implies
1−λ1 λr11q
λ11 λr1−1q
. 2.9
Obviouslyλ11, due to the different signs of both sides of the last equality for the caseλ1/1.
Likewise, letλ2>0 be an equilibrium of2.7; then
λ2 Φ2λ2, . . . , λ2
λr21q
λr2−1q λr21q
−
λr2−1q, 2.10
which indicates
λ2−1
λr21q λ21
λr2−1q. 2.11
Assume thatλ2/1. Ifλ2>1, then by the monotonicity of the maphx x1/x−1,x >1 we have that
λ21
λ2−1 ≤ λr21 λr2−1 <
λr21 λr2−1
q
, 2.12
which contradicts 2.11.Similarly, if 0 < λ2 < 1, then by the monotonicity of the function
lx 1x/1−x,x∈0,1,we have that
1λ2
1−λ2 ≤ 1λr2 1−λr2 <
1λr2 1−λr2
q
, 2.13
which also contradicts2.11. Thusλ21.
The proof is complete.
Lemma 2.2. (1) LetΦ1 be defined by2.2; thenΦ1 is monotonically increasing inxj if and only ifq
i1,i /jxi−1< 0,and monotonically decreasing inxjif and only ifq
i1,i /jxi−1 > 0,for j1,2, . . . , q.
(2) Let Φ2 be defined by 2.5, then Φ2 is monotonically decreasing in xj if and only if q
i1,i /jxi−1 < 0,and monotonically increasing in xj if and only ifq
i1,i /jxi−1 > 0,for j1,2, . . . , q.
Proof. The results follow directly from the facts below:
∂Φ1
∂xj −rxr−1j q i1,i /j
x2ri −1 β
x1, x2, . . . , xq2
⎧⎪
⎪⎪
⎪⎪
⎨
⎪⎪
⎪⎪
⎪⎩
<0, q i1,i /j
xi−1>0,
>0, q i1,i /j
xi−1<0,
j ∈
1, . . . , q ,
∂Φ2
∂xj rxjr−1q i1,i /j
x2ri −1 α
x1, x2, . . . , xq2
⎧⎪
⎪⎪
⎪⎪
⎨
⎪⎪
⎪⎪
⎪⎩
>0, q i1,i /j
xi−1>0,
<0, q i1,i /j
xi−1<0, j∈
1, . . . , q .
2.14
Remark 2.3. The second statementi.e.,2inLemma 2.2can also be found in Stevi´c’s paper 34 see Lemma 1 and Corollary 1.
Forr∈R,3≤q∈Nodd, define a mapΨ:R → Rsuch that
Ψx 1xrq−1−xrq
1xrq 1−xrq, 2.15
which has the following simple property:
Ψ 1
x
1
Ψx, x∈R. 2.16
Lemma 2.4. Suppose that 0 < ξ <1,and letΓ Ψξ,Φ ∈ {Φ1,Φ2}.Ifx1, x2, . . . , xq ∈ξ,1/ξ, then
Γ≤Φ
x1, x2, . . . , xq
≤ 1
Γ. 2.17 Proof. Since Φx1, x2, . . . , xq is symmetric in x1, x2, . . . , xq, without loss of generality, we suppose thatξ ≤ x1 ≤ x2 ≤ · · · ≤ xq ≤ 1/ξ.If there existsj ∈ {1, . . . , q}such thatxj 1, then by2.2and2.5we can easily get thatΦx1, x2, . . . , xq 1. Thus, assumexj/1 for all j∈ {1, . . . , q}.
Then we have the followingq1 cases to consider:
1 ξ≤x1≤ · · · ≤xq−1≤xq<1< 1 ξ; 2 ξ≤x1≤ · · · ≤xq−1<1< xq ≤ 1
ξ; 3 ξ≤x1≤ · · ·<1< xq−1≤xq ≤ 1
ξ; ...
q
ξ≤x1<1<· · · ≤xq−1≤xq ≤ 1 ξ; q1
ξ <1< x1≤ · · · ≤xq−1≤xq ≤ 1 ξ.
2.18
ByLemma 2.2, for the above cases, we have that
1 1<Φ1
x1, . . . , xq−1, xq
≤ 1 Γ; 2 Γ≤Φ1
x1, . . . , xq−1, xq
<1;
3 1<Φ1
x1, . . . , xq−1, xq
≤ 1 Γ; ...
q
1<Φ1
x1, . . . , xq−1, xq
≤ 1 Γ; q1
Γ≤Φ1
x1, . . . , xq−1, xq
<1.
2.19
Obviously,Γ≤Φ1x1, x2, . . . , xq≤1/Γfollows directly from the above inequalities.
The proof of the caseΦ Φ2is analogous and hence omitted.
Lemma 2.5. Suppose that 0< r ≤1, ξ∈0,1is fixed and letΓ Ψξ.Then we have
Γ> ξ. 2.20
Proof. By the monotonicity of the functionhx 1x/1−x, x∈0,1,we have that 1ξ
1−ξ ≤ 1ξr 1−ξr <
1ξr 1−ξr
q
, 2.21
which implies
1−ξ1ξrq>1ξ1−ξrq. 2.22 Therefore,1ξrq−1−ξrq/1ξrq 1−ξrq> ξ, that is,Γ> ξ.
The proof is complete.
The following corollary follows directly fromLemma 2.4andLemma 2.5.
Corollary 2.6. Assume that 0 < ξ < 1.If any positive solution yn∞n−kq to2.4or2.7has the initial values
y−kq, y−kq1, . . . , y−1∈
ξ,1 ξ
, 2.23
then we haveyn∈ξ,1/ξ,forn∈N0.
Define two sequencesξi∞i0 andηi∞i0 as follows:
ξi1 Ψξi, ηi1 Ψ ηi
, i∈N0, 2.24
with initial valuesξ0, η0>0.
Lemma 2.7. For the sequencesξi∞i0 andηi∞i0 defined by2.24, if 0< ξ0 <1,andξ0η01, then
ilim→ ∞ξi lim
i→ ∞ηi1. 2.25
Proof. Inductively, we can simply obtain that 0 < ξi <1 < ηi < ∞, i∈N0.Through simple calculations, by2.16, we have that
ξiηi≡1, ∀i∈N0. 2.26
Therefore byLemma 2.4andLemma 2.5, we get that
0< ξi≤ξi1<1< ηi1 ≤ηi, i∈N0, 2.27
which implies that the sequencesξi∞i0 andηi∞i0 converge to some limitsdenoted byξ∗ andη∗, resp., that is,
ξ∗ lim
i→∞ξi∈ξ0,1, η∗ lim
i→∞ηi∈ 1, η0
. 2.28
By taking limits on both sides of the first identity of2.24, we get
ξ∗
1 ξ∗rq
−
1−ξ∗rq 1 ξ∗rq
1−ξ∗rq, 2.29
which implies
1−ξ∗
1 ξ∗rq
1ξ∗1−ξ∗rq. 2.30
Suppose thatξ∗/1; then by the monotonicity of the functionfx 1x/1−x,x∈0,1, we have that
1ξ∗
1−ξ∗ ≤ 1 ξ∗r 1−ξ∗r <
1 ξ∗r 1−ξ∗r
q
, 2.31
which contradicts2.29. Hence, we have thatξ∗ 1 and then obviously it follows by2.26 and2.28thatξ∗η∗1.
The proof is complete.
3. Stability
In this section, we give a new, concise and clear proof of Stevi´c’sTheorem 1.5, by the lemmas inSection 2.
Proof ofTheorem 1.5. EmployingLemma 2.2, the linearized equations of2.4and2.7about the equilibriumy1 are both
zn0·zn−k10·zn−k2· · ·0·zn−kq ≡0, n∈N0. 3.1
Then by the Linearized Stability Theorem,y1 is locally stable.
Thus it suffices to confirm thaty1 is also a global attractor for all positive solutions of2.4and2.7.
Letyn∞n−kqbe a positive solution to2.4or2.7with initial values
y−kq, y−kq1, . . . , y−1 ∈0,∞. 3.2
We need to prove that limn→ ∞yn1.
Apparently, there existsξ0∈0,1such that yi∈
ξ0, η0
, i−kq,−kq1, . . . ,−1, 3.3
whereη01/ξ0.EmployingCorollary 2.6, we have yn∈
ξ0, η0
, n−kq,−kq1, . . . . 3.4
Let sequences ξi∞i0 and ηi∞i0 be defined by2.24. Let Φ ∈ {Φ1,Φ2}; then in light of Lemma 2.4,3.4, and2.26, we get
Ψξ0≤Φ
yn−k1, yn−k2, . . . , yn−kq
≤ 1
Ψξ0 Ψ η0
, n∈N0. 3.5
That is,
yn∈ ξ1, η1
, n∈N0. 3.6
In view of3.6,2.26andLemma 2.4, we have that Ψξ1≤Φ
yn−k1, yn−k2, . . . , yn−kq
≤ 1
Ψξ1 Ψ η1
, n≥kq. 3.7
That is,
yn∈ ξ2, η2
, n≥kq. 3.8
Reasoning inductively, we can get yn∈
ξi1, ηi1
, n≥ikq, i∈N0. 3.9
ByLemma 2.7and3.9, we obtain 1 lim
i→ ∞ξi1≤ lim
n→ ∞yn≤ lim
i→ ∞ηi11,
3.10
which implies
nlim→ ∞yn1. 3.11
The proof is complete.
4. Exponential Convergence
In this section, we will prove that all positive solutions to2.4and2.7with 0 < r ≤ 1 are exponentially convergent, by using an approach from paper42.
Theorem 4.1. Ifr∈0,1,then every positive solution to2.4and2.7exponentially converges to 1.
Proof. Letyn∞n−kqbe a positive solution to2.4or2.7; then byTheorem 1.5, there exists a sufficiently large natural numberNsuch that for arbitrary fixedε >0 we have|yn−1|< εfor alln≥N.
DenoteTn|yn−1|, n≥ −kq; thenTn< εfor alln≥N.
(1). For2.4.
Let 0< ε≤1−r
1/q; then by2.4, we have
Tnyn−1 2q
j1yn−kr j−1 q
j1
yn−kr j1 q
j1
yrn−kj−1
≤ 2q
j1yrn−kj−1 2q
j1yn−kr j ≤ q
j1yrn−kj−1 q1−εr
≤ q
j1
yn−kr j−1≤ q
j1
yn−kj−1
q j1
Tn−kj ≤εq−1Tn−kq, n≥Nkq.
4.1
(2). For2.7.
Let 0< ε <1 be fixed; then by2.7, we get
Tnyn−1 2q
j1yn−kr j−1 q
j1
yn−kr j1
−q j1
yrn−kj−1
≤ q
j1
yn−kr j−1≤ q
j1
yn−kj−1
q j1
Tn−kj ≤εq−1Tn−kq, n≥Nrq.
4.2
From this inequality and Lemma 1 in43 see also Corollary 1 therein, the result directly follows.
5. Other Simple Results
In this section, we will present some elementary results of2.3and2.6withr >1.
Proposition 5.1. Ifr >1, then there is no positive solutionyn∞n−kqto2.3such that limn→ ∞yn
∞.
Proof. Supposeyn∞n−kqis a positive solution to2.3such that
nlim→ ∞yn ∞. 5.1
Then for some fixedM >1, there existsN∈Nsuch that
∀n≥N, yn> M. 5.2
Employing2.3and5.2, we can simply get that
yNkq q
j1
yrNkq−kj1
−q j1
yNkr q−kj−1 q
j1
yNkr q−kj1 q
j1
yrNkq−kj−1 <1 5.3
which contradicts5.2. The proof is complete.
Proposition 5.2. We have the following simple statements:
1if r > 1, then 2.6 has nonoscillatory positive solutions with all initial values yi ≥ 1,
−kq≤i≤ −1,or 0< yi<1,−kq ≤i≤ −1;
2letH {yi | yi/1,−kq ≤ i ≤ −1}and denote byHthe cardinality of the setH. If H< q, then for any positive solutionyn∞n−kqto2.3or2.6, we getyn ≡1,for all n≥0.
6. Conclusions
In the following, leta∗max{a,1/a}for anya∈Ras defined in20and firstly we present 20, Theorem 1.
Theorem 6.1see20. Letf, g satisfy the following two conditions:
H1 fu1, u2, . . . , uk∗fu∗1, u∗2, . . . , u∗kandgu1, . . . , ul∗gu∗1, . . . , u∗l; H2fu∗1, u∗2, . . . , u∗k≤u∗1.
Thenx1 is the unique positive equilibrium for equation (1) which is globally asymptotically stable.
The Equation (1) mentioned in Theorem 6.1 is the following difference equation:
xn1 fxn−r1, . . . , xn−rkgxn−m1, . . . , xn−ml 1
fxn−r1, . . . , xn−rk gxn−m1, . . . , xn−ml , n∈N, 6.1
wheref∈CRk, Randg ∈CRl, Rwithk, l∈ {1,2, . . .},0≤r1<· · ·< rk, and 0≤m1<· · ·<
ml, and the initial values are positive real numbers.
Remark 6.2. Equation1.10is a special case of equation1in20.
Proof. Letk≥3, f1u uru >0,r∈R,and define a recursive equation
fj
u1, u2, . . . , uj
fj−1
u1, u2, . . . , uj−1 urj1 fj−1
u1, u2, . . . , uj−1
urj , 6.2
for all 2≤j ≤q.Then the following difference equation:
ynfq
yn−r1, . . . , yn−rq
, n∈N0, 6.3
where 1 ≤ r1 < r2 < · · · < rq and the initial valuesy−rq, y−rq1, . . . , y−1 ∈ 0,∞, is the very Equation1.10in this paper.
Remark 6.3. Letfu ur,r ∈0,1, andgu1, u2, . . . , uk fku1, u2, . . . , uk. Then through simple calculations, we have
H1 fu∗fu∗andgu1, u2, . . . , uk∗gu∗1, u∗2, . . . , u∗k; H2 H2fu∗≤u∗.
Thus the conditionsH1and H2of20, Theorem 1hold. By20, Theorem 1, we know that the unique positive equilibrium y 1 of1.10 also6.3is globally asymptotically stable.
Remark 6.4. Although the stability of1.10can be also obtained as a corollary from Theorem 1 of the paper by Sun and Xi20, the method of proof ofTheorem 1.5in this paper is distinct.
Acknowledgments
The authors are grateful to the referees for their huge number of valuable suggestions, which considerably improved the presentation of this paper. This work was financially supported by National Natural Science Foundation of Chinano. 10771227.
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