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Dynamics of a fourthorder system of rational difference equations
Advances in Difference Equations volume 2012, Article number: 215 (2012)
Abstract
In this paper, we study the equilibrium points, local asymptotic stability of an equilibrium point, instability of equilibrium points, periodicity behavior of positive solutions, and global character of an equilibrium point of a fourthorder system of rational difference equations of the form
n=0,1,\dots , where the parameters α, β, γ, {\alpha}_{1}, {\beta}_{1}, {\gamma}_{1} and initial conditions {x}_{0}, {x}_{1}, {x}_{2}, {x}_{3}, {y}_{0}, {y}_{1}, {y}_{2}, {y}_{3} are positive real numbers. Some numerical examples are given to verify our theoretical results.
MSC:39A10, 40A05.
1 Introduction and preliminaries
The theory of discrete dynamical systems and difference equations developed greatly during the last twentyfive years of the twentieth century. Applications of difference equations also experienced enormous growth in many areas. Many applications of discrete dynamical systems and difference equations have appeared recently in the areas of biology, economics, physics, resource management, and others. The theory of difference equations occupies a central position in applicable analysis. There is no doubt that the theory of difference equations will continue to play an important role in mathematics as a whole. Nonlinear difference equations of order greater than one are of paramount importance in applications. Such equations also appear naturally as discrete analogues and as numerical solutions of differential and delay differential equations which model various diverse phenomena in biology, ecology, physiology, physics, engineering and economics. It is very interesting to investigate the behavior of solutions of a system of higherorder rational difference equations and to discuss the local asymptotic stability of their equilibrium points.
Cinar [1] investigated the periodicity of the positive solutions of the system of rational difference equations
Stević [2] studied the system of two nonlinear difference equations
where {u}_{n}, {v}_{n}, {w}_{n}, {s}_{n} are some sequences {x}_{n} or {y}_{n}.
Kurbanli [3] studied the behavior of positive solutions of the system of rational difference equations
Bajo and Liz [4] investigated the global behavior of the difference equation
for all values of real parameters a, b.
Kalabuŝić, Kulenović, and Pilav [5] investigated the global dynamics of the following systems of difference equations:
Kurbanli, Çinar, and Yalçinkaya [6] studied the behavior of positive solutions of the system of rational difference equations
Touafek and Elsayed [7] studied the periodic nature and got the form of the solutions of the following systems of rational difference equations:
Similarly, Touafek, and Elsayed [8] studied the periodicity nature of the following systems of rational difference equations:
Recently, Zhang, Yang, and Liu [9] studied the dynamics of a system of the rational thirdorder difference equation
Our aim in this paper is to investigate the dynamics of a system of fourthorder rational difference equations
n=0,1,\dots , where the parameters α, β, γ, {\alpha}_{1}, {\beta}_{1}, {\gamma}_{1} and initial conditions {x}_{0}, {x}_{1}, {x}_{2}, {x}_{3}, {y}_{0}, {y}_{1}, {y}_{2}, {y}_{3} are positive real numbers. This paper is a natural extension of [9, 10].
Let us consider an eightdimensional discrete dynamical system of the form
n=0,1,\dots , where f:{I}^{4}\times {J}^{4}\to I and g:{I}^{4}\times {J}^{4}\to J are continuously differentiable functions and I, J are some intervals of real numbers. Furthermore, a solution {\{({x}_{n},{y}_{n})\}}_{n=3}^{\mathrm{\infty}} of the system (1.2) is uniquely determined by initial conditions ({x}_{i},{y}_{i})\in I\times J for i\in \{3,2,1,0\}. Along with the system (1.2), we consider the corresponding vector map F=(f,{x}_{n},{x}_{n1},{x}_{n2},{x}_{n3},g,{y}_{n},{y}_{n1},{y}_{n2},{y}_{n3}). An equilibrium point of (1.2) is a point (\overline{x},\overline{y}) that satisfies
The point (\overline{x},\overline{y}) is also called a fixed point of the vector map F.
Definition 1.1 Let (\overline{x},\overline{y}) be an equilibrium point of the system (1.2).

(i)
An equilibrium point (\overline{x},\overline{y}) is said to be stable if for every \epsilon >0, there exists \delta >0 such that for every initial condition ({x}_{i},{y}_{i}), i\in \{3,2,1,0\} if \parallel {\sum}_{i=3}^{0}({x}_{i},{y}_{i})(\overline{x},\overline{y})\parallel <\delta implies \parallel ({x}_{n},{y}_{n})(\overline{x},\overline{y})\parallel <\epsilon for all n>0, where \parallel \cdot \parallel is the usual Euclidean norm in {\mathbb{R}}^{2}.

(ii)
An equilibrium point (\overline{x},\overline{y}) is said to be unstable if it is not stable.

(iii)
An equilibrium point (\overline{x},\overline{y}) is said to be asymptotically stable if there exists \eta >0 such that \parallel {\sum}_{i=3}^{0}({x}_{i},{y}_{i})(\overline{x},\overline{y})\parallel <\eta and ({x}_{n},{y}_{n})\to (\overline{x},\overline{y}) as n\to \mathrm{\infty}.

(iv)
An equilibrium point (\overline{x},\overline{y}) is called a global attractor if ({x}_{n},{y}_{n})\to (\overline{x},\overline{y}) as n\to \mathrm{\infty}.

(v)
An equilibrium point (\overline{x},\overline{y}) is called an asymptotic global attractor if it is a global attractor and stable.
Definition 1.2 Let (\overline{x},\overline{y}) be an equilibrium point of the map
where f and g are continuously differentiable functions at (\overline{x},\overline{y}). The linearized system of (1.2) about the equilibrium point (\overline{x},\overline{y}) is
where
and {F}_{J} is a Jacobian matrix of the system (1.2) about the equilibrium point (\overline{x},\overline{y}).
To construct the corresponding linearized form of the system (1.1), we consider the following transformation:
where f=\frac{\alpha {x}_{n3}}{\beta +\gamma {y}_{n}{y}_{n1}{y}_{n2}{y}_{n3}}, g=\frac{{\alpha}_{1}{y}_{n3}}{{\beta}_{1}+{\gamma}_{1}{x}_{n}{x}_{n1}{x}_{n2}{x}_{n3}}, {f}_{1}={x}_{n}, {f}_{2}={x}_{n1}, {f}_{3}={x}_{n2}, {f}_{4}={x}_{n3}, {g}_{1}={y}_{n}, {g}_{2}={y}_{n1}, {g}_{3}={y}_{n2} and {g}_{4}={y}_{n3}. The Jacobian matrix about the fixed point (\overline{x},\overline{y}) under the transformation (1.3) is given by
where A=\frac{\alpha}{\beta +\gamma {\overline{y}}^{4}}, B=\frac{\alpha \gamma \overline{x}{\overline{y}}^{3}}{{(\beta +\gamma {\overline{y}}^{4})}^{2}}, C=\frac{{\alpha}_{1}{\gamma}_{1}\overline{y}{\overline{x}}^{3}}{{({\beta}_{1}+{\gamma}_{1}{\overline{x}}^{4})}^{2}} and D=\frac{{\alpha}_{1}}{{\beta}_{1}+{\gamma}_{1}{\overline{x}}^{4}}.
Theorem 1.3 For the system {X}_{n+1}=F({X}_{n}), n=0,1,\dots , of difference equations such that \overline{X} is a fixed point of F. If all eigenvalues of the Jacobian matrix {J}_{F} about \overline{X} lie inside the open unit disk \lambda <1, then \overline{X} is locally asymptotically stable. If one of them has a modulus greater than one, then \overline{X} is unstable.
Theorem 1.4 (RouthHurwitz criterion)
For real numbers {a}_{1},{a}_{2},\dots ,{a}_{n}, let
Consider the polynomial equation
We define the n matrices as follows:
where (l,m) element in the matrix {H}_{j}, for 0<2lm<k is
The following statements are true:

(i)
A necessary and sufficient condition for all of the roots of (1.5) to have a negative real part is det({H}_{j})>0 for j=1,2,\dots ,n.

(ii)
A necessary and sufficient condition for the existence of a root of (1.5) with a positive real part is det({H}_{j})<0 for some j\in \{1,2,\dots ,n\}.
2 Main results
Let (\overline{x},\overline{y}) be an equilibrium point of the system (1.1), then for \alpha >\beta and {\alpha}_{1}>{\beta}_{1}, the system (1.1) has the following five equilibrium points:
where A={(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}} and B={(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}}.
Theorem 2.1 Let ({x}_{n},{y}_{n}) be a positive solution of the system (1.1), then for every m\ge 0, the following results hold:
Proof The results are obviously true for m=0. Suppose that results are true for m=k\ge 1, i.e.,
Now, for m=k+1 using (1.1), one has
□
Theorem 2.2 For the equilibrium point {P}_{0}=(0,0) of Equation (1.1), the following results hold:

(i)
Let \alpha <\beta and {\alpha}_{1}<{\beta}_{1}, then the equilibrium point {P}_{0}=(0,0) of the system (1.1) is locally asymptotically stable.

(ii)
If \alpha >\beta or {\alpha}_{1}>{\beta}_{1}, then the equilibrium point {P}_{0}=(0,0) of the system (1.1) is unstable.
Proof (i) The linearized system of (1.1) about the equilibrium point (0,0) is given by
where
and
The characteristic polynomial of {F}_{J}(0,0) is given by
The roots of P(\lambda ) are \lambda =\pm \frac{\alpha}{\beta}, \lambda =\pm \frac{{\alpha}_{1}}{{\beta}_{1}}, \lambda =\pm \iota \frac{\alpha}{\beta}, \lambda =\pm \iota \frac{{\alpha}_{1}}{{\beta}_{1}}. Since all eigenvalues of the Jacobian matrix {F}_{J}(0,0) about (0,0) lie in an open unit dick \lambda <1, the equilibrium point (0,0) is locally asymptotically stable.

(ii)
It is easy to see that if \alpha >\beta or {\alpha}_{1}>{\beta}_{1}, then there exists at least one root λ of Equation (2.1) such that \lambda >1. Hence, by Theorem 1.3 if \alpha >\beta or {\alpha}_{1}>{\beta}_{1}, then (0,0) is unstable. □
Theorem 2.3 If \alpha >\beta and {\alpha}_{1}>{\beta}_{1}, then a positive equilibrium point {P}_{1}=({(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}},{(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}}) of Equation (1.1) is unstable.
Proof The linearized system of (1.1) about the equilibrium point {P}_{1} is given by
where
and
where
and
The characteristic polynomial of {F}_{J}({P}_{1}) is given by
The roots of the characteristic polynomial P(\lambda ) given in Equation (2.2) are given by
It is sufficient to prove that any one of these roots has absolute value greater than one. For this, consider
Hence, by Theorem 1.3 if \alpha >\beta and {\alpha}_{1}>{\beta}_{1}, then {P}_{1} is unstable. □
Theorem 2.4 If \alpha >\beta and {\alpha}_{1}>{\beta}_{1}, then the equilibrium points {P}_{2}, {P}_{3}, {P}_{4} of Equation (1.1) are unstable.
Proof The proof is similar to Theorem 2.3, so it is omitted. □
The following theorem is similar to Theorem 3.4 of [9].
Theorem 2.5 Let \alpha >\beta and {\alpha}_{1}>{\beta}_{1}, and let ({x}_{n},{y}_{n}) be a solution of the system (1.1). Then, for k=3,2,1,0, the following statements are true:

(i)
If ({x}_{k},{y}_{k})\in (0,{(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}})\times ({(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}},\mathrm{\infty}), then ({x}_{n},{y}_{n})\in (0,{(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}})\times ({(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}},\mathrm{\infty}).

(ii)
If ({x}_{k},{y}_{k})\in ({(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}},\mathrm{\infty})\times (0,{(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}}), then ({x}_{n},{y}_{n})\in ({(\frac{{\alpha}_{1}{\beta}_{1}}{{\gamma}_{1}})}^{\frac{1}{4}},\mathrm{\infty})\times (0,{(\frac{\alpha \beta}{\gamma})}^{\frac{1}{4}}).
Theorem 2.6 The system (1.1) has no prime periodtwo solutions.
Proof Assume that ({p}_{1},{q}_{1}),({p}_{2},{q}_{2}),({p}_{1},{q}_{1}),\dots is a prime periodtwo solution of Equation (1.1) such that {p}_{i},{q}_{i}\ne 0 and {p}_{i}\ne {q}_{i} for i=1,2. Then, from the system (1.1), one has
and
From (2.3) and (2.4), one has {p}_{i},{q}_{i}=0 for i=1,2. Which is a contradiction. Hence, the system (1.1) has no prime periodtwo solutions. □
Theorem 2.7 Let \alpha <\beta and {\alpha}_{1}<{\beta}_{1}, then the equilibrium point {P}_{0}=(0,0) of Equation (1.1) is globally asymptotically stable.
Proof For \alpha <\beta and {\alpha}_{1}<{\beta}_{1}, from Theorem 2.2, (0,0) is locally asymptotically stable. From Theorem 2.1, it is easy to see that every positive solution ({x}_{n},{y}_{n}) is bounded, i.e., 0\le {x}_{n}\le \mu and 0\le {y}_{n}\le \nu for all n=0,1,2,\dots , where \mu =max\{{x}_{3},{x}_{2},{x}_{1},{x}_{0}\} and \nu =max\{{y}_{3},{y}_{2},{y}_{1},{y}_{0}\}. Now, it is sufficient to prove that ({x}_{n},{y}_{n}) is decreasing. From the system (1.1), one has
This implies that {x}_{4n+1}<{x}_{4n3} and {x}_{4n+5}<{x}_{4n+1}. Hence, the subsequences \{{x}_{4n+1}\}, \{{x}_{4n+2}\}, \{{x}_{4n+3}\}, \{{x}_{4n+4}\} are decreasing, i.e., the sequence \{{x}_{n}\} is decreasing. Similarly, one has
This implies that {y}_{4n+1}<{y}_{4n3} and {y}_{4n+5}<{y}_{4n+1}. Hence, the subsequences \{{y}_{4n+1}\}, \{{y}_{4n+2}\}, \{{y}_{4n+3}\}, \{{y}_{4n+4}\} are decreasing, i.e., the sequence \{{y}_{n}\} is decreasing. Hence, {lim}_{n\to \mathrm{\infty}}{x}_{n}={lim}_{n\to \mathrm{\infty}}{y}_{n}=0. □
Theorem 2.8 Let \alpha >\beta and {\alpha}_{1}>{\beta}_{1}. Then, for a solution ({x}_{n},{y}_{n}) of the system (1.1), the following statements are true:

(i)
If {x}_{n}\to 0, then {y}_{n}\to \mathrm{\infty}.

(ii)
If {y}_{n}\to 0, then {x}_{n}\to \mathrm{\infty}.
3 Examples
In order to verify our theoretical results and to support our theoretical discussions, we consider several interesting numerical examples in this section. These examples represent different types of qualitative behavior of solutions to the system of nonlinear difference equations (1.1). All plots in this section are drawn with mathematica.
Example Consider the system (1.1) with initial conditions {x}_{3}=1.1, {x}_{2}=2.6, {x}_{1}=1.6, {x}_{0}=1.7, {y}_{3}=1.5, {y}_{2}=1.3, {y}_{1}=2.5, {y}_{0}=0.5. Moreover, choosing the parameters \alpha =0.01, \beta =0.011, \gamma =50, {\alpha}_{1}=0.03, {\beta}_{1}=0.031, {\gamma}_{1}=70, the system (1.1) can be written as follows:
n=0,1,\dots , and with initial conditions {x}_{3}=1.1, {x}_{2}=2.6, {x}_{1}=1.6, {x}_{0}=1.7, {y}_{3}=1.5, {y}_{2}=1.3, {y}_{1}=2.5, {y}_{0}=0.5. The plot of the system (3.1) is shown in Figure 1 and its global attractor is shown in Figure 2.
Example Consider the system (1.1) with initial conditions {x}_{3}=2.1, {x}_{2}=2.6, {x}_{1}=0.6, {x}_{0}=1.4, {y}_{3}=1.5, {y}_{2}=1.6, {y}_{1}=2.7, {y}_{0}=0.45. Moreover, choosing the parameters \alpha =12, \beta =12.5, \gamma =90, {\alpha}_{1}=15, {\beta}_{1}=15.5, {\gamma}_{1}=75, the system (1.1) can be written as follows:
n=0,1,\dots , and with initial conditions {x}_{3}=2.1, {x}_{2}=2.6, {x}_{1}=0.6, {x}_{0}=1.4, {y}_{3}=1.5, {y}_{2}=1.6, {y}_{1}=2.7, {y}_{0}=0.45. The plot of the system (3.2) is shown in Figure 3 and its global attractor is shown in Figure 4.
Example Consider the system (1.1) with initial conditions {x}_{3}=9.2, {x}_{2}=1.8, {x}_{1}=0.76, {x}_{0}=1.1, {y}_{3}=1.1, {y}_{2}=1.2, {y}_{1}=8.1, {y}_{0}=0.52. Moreover, choosing the parameters \alpha =200, \beta =225, \gamma =1000, {\alpha}_{1}=150, {\beta}_{1}=160, {\gamma}_{1}=700, the system (1.1) can be written as follows:
n=0,1,\dots , and with initial conditions {x}_{3}=9.2, {x}_{2}=1.8, {x}_{1}=0.76, {x}_{0}=1.1, {y}_{3}=1.1, {y}_{2}=1.2, {y}_{1}=8.1, {y}_{0}=0.52. The plot of the system (3.3) is shown in Figure 5 and its global attractor is shown in Figure 6.
Example Consider the system (1.1) with initial conditions {x}_{3}=1.3, {x}_{2}=1.8, {x}_{1}=2.6, {x}_{0}=2.1, {y}_{3}=0.01, {y}_{2}=1.2, {y}_{1}=2.8, {y}_{0}=1.5. Moreover, choosing the parameters \alpha =12, \beta =10.5, \gamma =15, {\alpha}_{1}=14, {\beta}_{1}=13, {\gamma}_{1}=0.2, the system (1.1) can be written as follows:
n=0,1,\dots , with initial conditions {x}_{3}=1.3, {x}_{2}=1.8, {x}_{1}=2.6, {x}_{0}=2.1, {y}_{3}=0.01, {y}_{2}=1.2, {y}_{1}=2.8, {y}_{0}=1.5. The plot of the system (3.4) is shown in Figure 7.
4 Conclusion
This work is a natural extension of [9, 10]. In the paper, we investigated some dynamics of an eightdimensional discrete system. The system has five equilibrium points all of which except (0,0) are unstable. The linearization method is used to show that the equilibrium point (0,0) is locally asymptotically stable. We prove that the system has no prime periodtwo solutions. The main objective of dynamical systems theory is to predict the global behavior of a system based on the knowledge of its present state. An approach to this problem consists of determining the possible global behaviors of the system and determining which initial conditions lead to these longterm behaviors. In case of higherorder dynamical systems, it is crucial to discuss global behavior of the system. Some powerful tools such as semiconjugacy and weak contraction cannot be used to analyze global behavior of the system (1.1). In the paper, we prove the global asymptotic stability of the equilibrium point (0,0) by using simple techniques. Some numerical examples are provided to support our theoretical results. These examples are experimental verifications of theoretical discussions.
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Acknowledgements
Authors would like to thank the referees for their comments and suggestions on the manuscript. This work was supported by the Higher Education Commission of Pakistan.
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QD and MNQ carried out the theoretical proof and drafted the manuscript. AQK participated in the design and coordination. All authors read and approved the final manuscript.
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Din, Q., Qureshi, M. & Khan, A.Q. Dynamics of a fourthorder system of rational difference equations. Adv Differ Equ 2012, 215 (2012). https://doi.org/10.1186/168718472012215
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DOI: https://doi.org/10.1186/168718472012215