Discrete Dynamics in Nature and Society

Volume 2014 (2014), Article ID 408972, 14 pages

http://dx.doi.org/10.1155/2014/408972

## Synchronization of Fractional-Order Hyperchaotic Systems via Fractional-Order Controllers

^{1}School of Science, Sichuan University of Science and Engineering, Zigong 643000, China^{2}Sichuan Province University Key Laboratory of Bridge Non-destruction Detecting and Engineering Computing, Zigong 643000, China

Received 18 November 2013; Revised 27 February 2014; Accepted 5 March 2014; Published 1 April 2014

Academic Editor: Beatrice Paternoster

Copyright © 2014 Tianzeng Li 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.

#### Abstract

In this paper, the synchronization of fractional-order chaotic systems is studied and a new fractional-order controller for hyperchaos synchronization is presented based on the Lyapunov stability theory. The proposed synchronized method can be applied to an arbitrary four-dimensional fractional hyperchaotic system. And we give the optimal value of control parameters to achieve synchronization of fractional hyperchaotic system. This approach is universal, simple, and theoretically rigorous. Numerical simulations of several fractional-order hyperchaotic systems demonstrate the universality and the effectiveness of the proposed method.

#### 1. Introduction

Fractional calculus is a 300-year-old mathematical topic. Although it has a long history, it has not been used in physics and engineering for many years. However, during the last twenty years or so, fractional calculus starts to attract increasing attentions of physicists and engineers from an application point of view [1, 2]. It was found that many systems in interdisciplinary fields could be elegantly described with the help of fractional derivatives. Many systems are known to display fractional-order dynamics, such as viscoelastic systems [3], dielectric polarization [4], electrode-electrolyte polarization [5], electromagnetic waves [6], quantitative finance [7], and quantum evolution of complex systems [8].

It is well known that chaos cannot occur in autonomous continuous-time systems of integer-order less than three according to the Poincarè-Bendixon theorem [9, 10]. A famous example of a continuous-time three-order system which exhibits chaos is the Lorenz system [11]. The order of this system can be defined as the sum of the orders of all involved derivatives. However, in autonomous fractional-order systems, it is not the case. For example, it has been shown that the fractional order Chua's circuit with an appropriate cubic nonlinearity and with order as low as 2.7 can produce a chaotic attractor [12]. In [13], chaos and hyperchaos in fractional-order Rössler equations are discussed, in which it is shown that chaos can exist in the fractional-order Rössler equation with order as low as 2.4, and hyperchaos can also exist in the fractional-order Rössler hyperchaotic system with order as low as 3.8. Also in [14, 15], chaotic behaviors in the fractional-order Chen system are studied and the lowest order to have chaos in this fractional order Chen system is shown to be 2.1 and 2.92, respectively.

In recent years, hyperchaotic system is also considered with quickly increasing interest [16, 17]. Hyperchaotic system is usually defined as a chaotic system with more than one positive Lyapunov exponent, which implies that its dynamics are extended in several different directions simultaneously. It has more complex dynamical behaviors than chaotic system. Typical examples are fractional-order hyperchaotic Chen's system [18], hyperchaotic Lorenz system [19, 20], and hyperchaotic Rössler system [21–23]. As we known, hyperchaos synchronization is very important, but it is also very difficult. However, there are only a few synchronization methods, such as feedback controller [20, 24] and nonlinear controller [25]. Most of the above synchronization methods concentrate on certain fractional systems, and there are few general methods that can be applied to control arbitrary fractional-order hyperchaotic systems.

On the other hand, the fractional-order control, which is a generalization of the traditional integer-order control, is becoming a matter of concern because of its flexibility and integrity [26–29]. The TID controller [27], the controller [28], and the CRONE controller [29] are the well-known fractional-order controllers. In these papers, it is verified that fractional-order controller is implemented more easily and more efficiently compared to the traditional controller.

Therefore, in this paper, we present a new fractional-order controller to synchronize the arbitrary 4D fractional-order hyperchaotic systems. The control approach which is based on the Lyapunov stability theory has the following three advantages. It is so general that it can be applied to almost all four-dimensional (4D) hyperchaotic systems. It can synchronize the systems very fast with little control cost and no changes on the parameters of the original systems. It is very simple, easily realized experimentally, and more suitable for engineering applications. Numerical simulation results of synchronization of the fractional-order hyperchaotic Chen system, the fractional-order hyperchaotic Lorenz system, and the fractional-order hyperchaotic Lü system demonstrate the effectiveness and the validity of the proposed method.

#### 2. Fractional Derivatives and Fractional Dynamic Systems

The fractional calculus plays an important role in modern science. In this paper, we mainly use the Caputo fractional operators [1, 26]. The Caputo definition of the fractional derivative, which is called smooth fractional derivative, is described as where is the lowest integer which is not less than , and is the Gamma function: When we numerically solve the fractional differential equations, we also adopt the improved version of Adams-Bashforth-Moulton algorithm [26, 30] which is proposed based on the predictor-correctors scheme. To explain the method, we consider the following differential equation: The differential equation (3) is equivalent to Volterra integral equation in the following: Now, set , . The integral equation can be discretized as follows: where The error of this approximation is described as follows: where .

In this paper, we mainly consider the order . There are some general properties of the fractional-order derivative which are described as follows [1, 26].

*Property 1. *Caputo fractional derivative is a linear operator; that is,
where , are real constants.

*Property 2. *Caputo fractional derivative satisfies additive index law (semigroup property); that is,
holds under some reasonable constraints on the function .

*Property 3. *For the fractional-order nonlinear system , satisfies the Lipschiz condition with respect to ; that is,
where is 1-norm and is a positive constant. Especially, if at . It follows that

In the following, we mainly consider a four-dimensional fractional-order nonlinear system: where is the fractional order of derivatives, is the system state variable, is the initial value, and denotes the Caputo fractional-order derivative operator [26]. The equilibrium points of system (14) are calculated via solving . Then we have the following conclusion for the stability of these equilibrium points.

Theorem 1 (see [26]). *The equilibrium points of system (14) are globally asymptotically stable if all the eigenvalues of the Jacobian matrix , evaluated at , satisfy the condition
*

*3. Synchronization of the Fractional-Order Hyperchaotic Systems*

*For the 4D fractional-order nonlinear system (14), we assume that
where is a bounded matrix with its elements depending on and . We consider the system (14) as a drive system, then the response system is given by
Adding a control function to the system (17), the controlled response system is
Let synchronization error , the error system from (14) and (18) is obtained as follows:
The control function is usually defined as
where is the control parameter matrix which is always diagonal and is defined as
with being a nonnegative diagonal matrix.*

*According to the Property 2 and formula (21), we have . In the same way, according to Properties 1 and 3 of the Caputo fractional derivative operator, there is a positive number , such that . Let be the positive minimum value of , then , and if , then .*

*Then we can easily obtain that the systems (14) and (18) are synchronized if and only if the error system (19) is asymptotically stable at the origin point.*

*Theorem 2. The fractional-order controller can make the error system (19) asymptotically stable at the origin point; that is, systems (14) and (18) are globally asymptotically synchronized if the control parameters and satisfy the following conditions:*

*Proof. *Since system (14) is fractional-order hyperchaotic system and is a bounded matrix, there is a nonnegative constants such that . We introduce a Lyapunov function

Differentiating with respect to , we have
The conclusion would be obtained, if the control parameters and satisfy the following conditions:

After calculation, the above conditions are equivalent to

Hence, we have . Obviously, if and only if (or ). Then set is the largest invariant set for the system. According to the LaSalle invariance principle, the fractional-order controller can make the error system (19) be asymptotically stable at origin point, that is, systems (14) and (18) are globally asymptotically synchronized.

Consider a three-dimensional fractional-order nonlinear system
where is the fractional order of derivative, is the system state variable, is the initial value, and denotes the Caputo fractional-order derivative operator. We consider the system (30) as a drive system, then the response system is given by
Let synchronization error , the error system from (30) and (31) is obtained by the same way:
where the control function is usually given as (20). Then we can get the conclusion.

*Corollary 3. The fractional-order controller can control the error system (32) responses to the asymptotically stable at the origin point, that is, systems (30) and (31) are globally asymptotically synchronized, if the control parameters and satisfy the following conditions:*

*4. Simulation and Analysis*

*4. Simulation and Analysis**In this section, three 4D fractional-order hyperchaotic systems are used as examples to illustrate how to use the results obtained in this paper to analyze the synchronization of fractional-order hyperchaotic systems.*

*4.1. Synchronization of the Fractional-Order Chen Hyperchaotic System*

*4.1. Synchronization of the Fractional-Order Chen Hyperchaotic System**In 2005, Li et al. [18] proposed a new hyperchaotic chen system form Chen system, which is described as
where . When , , , , and , the system (35) is hyperchaotic [18]. Then we consider the fractional version of this system which is given by
where is the fractional order. When , , , , and , according to the numerical simulations, the lowest order of this system to generate hyperchaos is 0.946. If we select the order and initial value , the system exhibits hyperchaotic behavior, as shown in Figure 1.*

*We consider the system (36) as a drive system, then the controlled response system is
where is control parameter and . According to systems (36) and (37), the error system is obtained as follows:
When the control parameters and satisfy the conditions of Theorem 2, the system (38) can be stabilized to the original point; that is, the synchronization of systems (36) and (37) are achieved.*

*In order to implement this controller easily, we select the parameters , , and initial values , , ; the numerical results, illustrated in Figure 2, show that the error system is driven to original point very fast; that is, the system (36) and (37) are synchronized. From Figure 2, we can obtain that two systems are synchronized about at 0.1 s, so the fractional-order controller can synchronize the hyperchaotic Chen systems very effectively.*

*To get an optimal value of the parameters which make two hyperchaotic systems synchronize, we continuously increase the parameters , form 1 to 4650, in step 1. By the numerical simulations with same initial values, we find the following conclusion.(i)When , two systems cannot achieve synchronization.(ii)When , two systems achieve synchronization, but the synchronization times are more than 1 s.(iii)When , two systems achieve synchronization very fast and the synchronization times are less than 1 s, which are shown in Figure 3(a).(iv)When , two systems cannot achieve synchronization.*

*In Figures 3(b)–3(d), the time evolutions of the error functions between systems (36) and (37) are given with , respectively. Furthermore, we find that the optimal value of is about 750. And the more the parameters are close to 750, the shorter the time will be required for synchronization of the drive system and response system, the better the effect of synchronization will be.*

*4.2. Synchronization of the Fractional-Order Hyperchaotic Lorenz System*

*4.2. Synchronization of the Fractional-Order Hyperchaotic Lorenz System**Lorenz system can be described as follows [26]:
When , , and , this system exhibits a chaotic behavior. X. Y. Wang and M. J. Wang [19] add a nonlinear controller to the first equation of Lorenz system, and let , then a new system is obtained as follows:
When , , , and , the system exhibits a hyperchaotic behavior. Wang and Song [20] consider the 4D fractional-order Lorenz system which can be described as
When we select the parameters as , , , , and , the system (41) is hyperchaotic [20]. Now, we select the order and initial value , the system exhibits hyperchaotic behavior, as shown in Figure 4.*

*We consider the system (41) as a drive system, then the controlled response system is given by
where is control parameter and . According to system (41) and (42), the error system is obtained as follows:
When the control parameters and satisfy the conditions of Theorem 2, the system (43) can be stabilized to the original point; that is, synchronization of systems (41) and (42) is achieved.*

*In order to implement this controller easily, we also select the parameters , and initial values , , ; the numerical results, illustrated in Figure 5, show that the error system (43) is driven to original point; that is, the systems (41) and (42) are synchronized. From Figure 5, two systems are synchronized about at 0.05 s, which demonstrates that the fractional-order controller can synchronize the Lorenz system very effectively and fast.*

*To get an optimal value of the parameters which make the two hyperchaotic systems synchronize, we continuously increase the parameters , form 1 to 2000, in step 1. By the numerical simulations with same initial values, we find the following conclusion.(i)When , two systems cannot achieve synchronization.(ii)When , two systems achieve synchronization, but the synchronization times are more than 1 s.(iii)When , two systems achieve synchronization very fast and the synchronization times are less than 1 s, which are shown in Figure 6(a).(iv)When , two systems cannot achieve synchronization.*

*In Figures 6(b)–6(d), the time evolutions of the error functions between systems (41) and (42) are given with , respectively. Furthermore, we find that the optimal value of is about 750. And the more the parameters are close to 750, the shorter the time will be required for synchronization of the drive system and response system, the better the effect of synchronization will be.*

*4.3. Synchronization of the Fractional-Order Hyperchaotic Lü System*

*4.3. Synchronization of the Fractional-Order Hyperchaotic Lü System**In 2006, Chen et al. [31] construct a new hyperchaotic system based on Lü system by using a state feedback controller. It is given by
where are the constants of Lü system and is a control parameter. When , , , and , system (44) has a hyperchaotic attractor [31]. Then we consider the fractional version of this system which is given by
If we select the order , and initial value , the system exhibits hyperchaotic behavior, as shown in Figure 7.*

*We consider the system (45) as a drive system, then the controlled response system is
where is control parameter and . According to systems (45) and (46), the error system is obtained as follows:
When the control parameters and satisfy the conditions of Theorem 2, the system (47) can be stabilized to the original point; that is, the synchronization of systems (45) and (46) is achieved.*

*In order to implement this controller easily, we also select the parameters , and initial values , , ; the numerical results, illustrated in Figure 8, show that the error system (47) is driven to original point; that is, the systems (45) and (46) are synchronized. From the Figure 8, we can obtain that two systems are synchronized about at 0.1 s, so the fractional-order controller can synchronize the Lü's system very effectively and fast.*

*To get an optimal value of the parameters to make the two hyperchaotic systems synchronize, we continuously increase the parameters , form 1 to 4500, in step 1. By the numerical simulations with same initial values, we find the following conclusion.(i)When , two systems cannot achieve synchronization.(ii)When , two systems achieve synchronization, but the synchronization times are more than 0.1 s.(iii)When , two systems achieve synchronization very fast and the synchronization times are less than 0.1 s, which are shown in Figure 9(a).(iv)When , two systems cannot achieve synchronization.*

*In Figures 9(b)–9(d), the time evolutions of the error functions between systems (45) and (46) are given with , respectively. Furthermore, we find that the optimal value of is about 2000. And the more the parameters are close to 2000, the shorter the time will be required for synchronization of the drive system and response system, the better the effect of synchronization will be.*

*4.4. Fractional-Order Control in the Presence of Measurement Noise*

*4.4. Fractional-Order Control in the Presence of Measurement Noise**Further, in order to study the control performance of the proposed fractional-order controller in the presence of measurement noise, we add the white noise with variance into the first formula of the controlled fractional-order hyperchaotic Chen system and Lorenz system. The control results of without and with noise are given in Figures 10(a)–10(d), which show that the method can effectively filter out the out-of-band noise and thus reduce the noise effect on the control. This also shows the superiority of the proposed fractional-order controller.*

*5. Conclusion*

*5. Conclusion**In conclusion, we proposed a fractional-order controller and presented a synchronization law for the 4D fractional-order hyperchaotic systems. According to the Lyapunov stability theorem of the fractional systems, the proposed method achieved to synchronize arbitrary 4D fractional-order hyperchaotic systems. Our proposed controller is very simple and could be easily realized experimentally. Furthermore, the present method is universal, that is, for almost all 4D fractional-order systems, and the controllers obtained are similar in form. Numerical simulation results of synchronization of the fractional-order hyperchaotic Chen system, the fractional-order hyperchaotic Lorenz system, and the fractional-order hyperchaotic Lü system demonstrate the effectiveness and the validity of the proposed method. And we give the optimal value of the parameters by numerical simulation. Furthermore, we have implemented and verified our method for other fractional-order hyperchaotic systems [21, 32, 33], namely, the generalized Henon-Heiles system [32], the Rössler system [21], the hyperchaotic Chua system [33], and so forth. The numerical simulation results indicated that the controller can make the fractional-order hyperchaotic systems synchronize very effectively and fast, and it provides a theoretical basis for the applications of synchronization in fractional hyperchaotic systems. In the future work, we will discuss the synchronization of hyperchaotic systems which have the different structure.*

*Conflict of Interests*

*Conflict of Interests**The authors declare that there is no conflict of interests regarding the publication of this paper.*

*Acknowledgments*

*Acknowledgments**This work is supported by Artificial Intelligence Key Laboratory of Sichuan Province 2014RYJ05, The Opening Project of Sichuan Province University Key Laboratory of Bridge Non-Destruction Detecting and Engineering Computing 2013QYJ01, and Found of Sichuan University of Science and Engineering Grant nos. 2012PY17, 2012KY06.*

*References*

*References*

- I. Podlubny,
*Fractional Differential Equations*, vol. 198, Academic Press, San Diego, Calif, USA, 1999. View at MathSciNet - R. Hilfer,
*Applications of Fractional Calculus in Physics*, World Scientific, River Edge, NJ, USA, 2001. View at MathSciNet - R. L. Bagley and R. A. Calico, “Fractional order state equations for the control of viscoelastically damped structures,”
*Journal of Guidance, Control, and Dynamics*, vol. 14, no. 2, pp. 304–311, 1991. View at Google Scholar · View at Scopus - H. H. Sun, A. A. Abdelwahab, and B. Onaral, “Linear approximation of transfer function with a pole of fractional power,”
*IEEE Transactions on Automatic Control*, vol. 29, no. 5, pp. 441–444, 1984. View at Google Scholar · View at Scopus - M. Ichise, Y. Nagayanagi, and T. Kojima, “An analog simulation of non-integer, order transfer functions for analysis of electrode ppocesses,”
*Journal of Electroanalytical Chemistry*, vol. 33, no. 2, pp. 253–265, 1971. View at Google Scholar · View at Scopus - O. Heaviside,
*Electromagnetic Theory*, Chelsea, New York, NY, USA, 1971. - N. Laskin, “Fractional market dynamics,”
*Physica A*, vol. 287, no. 3-4, pp. 482–492, 2000. View at Publisher · View at Google Scholar · View at MathSciNet - D. Kusnezov, A. Bulgac, and G. D. Dang, “Quantum Lévy Processes and Fractional Kinetics,”
*Physical Review Letters*, vol. 82, no. 6, pp. 1136–1139, 1999. View at Google Scholar · View at Scopus - H. G. Schuster,
*Deterministic Chaos: An Introduction*, Physik-Verlag, Weinheim, Germany, 2nd edition, 1988. View at MathSciNet - M. W. Hirsch and S. Smale,
*Differential Equations, Dynamical Systems, and Linear Algebra*, Academic Press, New York, NY, USA, 1974. View at MathSciNet - E. N. Lorenz, “Deterministic nonperiodic flow,”
*Journal of the Atmospheric Sciences*, vol. 20, pp. 130–141, 1963. View at Google Scholar - C. G. Li and G. Chen, “Chaos and hyperchaos in the fractional-order Rössler equations,”
*Physica A*, vol. 341, no. 1–4, pp. 55–61, 2004. View at Publisher · View at Google Scholar · View at MathSciNet - C. G. Li and G. Chen, “Chaos in the fractional order Chen system and its control,”
*Chaos Solitons & Fractals*, vol. 22, pp. 549–554, 2004. View at Google Scholar - C. P. Li and G. J. Peng, “Chaos in Chen's system with a fractional order,”
*Chaos, Solitons & Fractals*, vol. 22, no. 2, pp. 443–450, 2004. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - B. Cannas and S. Cincotti, “Hyperchaotic behaviour of two bi-directionally coupled Chua's circuits,”
*International Journal of Circuit Theory and Applications*, vol. 30, no. 6, pp. 625–637, 2002. View at Publisher · View at Google Scholar · View at Scopus - G. Grassi and S. Mascolo, “A systematic procedure for synchronizing hyperchaos via observer design,”
*Journal of Circuits, Systems and Computers*, vol. 11, no. 1, pp. 1–16, 2002. View at Google Scholar · View at Scopus - J. Y. Hsieh, C. C. Hwang, A. P. Wang, and W. J. Li, “Controlling hyperchaos of the Rössler system,”
*International Journal of Control*, vol. 72, no. 10, pp. 882–886, 1999. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - Y. Li, W. K. S. Tang, and G. R. Chen, “Generating hyperchaos via state feedback control,”
*International Journal of Bifurcation and Chaos in Applied Sciences and Engineering*, vol. 15, no. 10, pp. 3367–3375, 2005. View at Publisher · View at Google Scholar · View at Scopus - X. Y. Wang and M. J. Wang, “A hyperchaos generated from Lorenz system,”
*Physica A*, vol. 387, no. 14, pp. 3751–3758, 2008. View at Publisher · View at Google Scholar · View at MathSciNet - X. Y. Wang and J. M. Song, “Synchronization of the fractional order hyperchaos Lorenz systems with activation feedback control,”
*Communications in Nonlinear Science and Numerical Simulation*, vol. 14, no. 8, pp. 3351–3357, 2009. View at Publisher · View at Google Scholar · View at Scopus - O. E. Rössler, “An equation for hyperchaos,”
*Physics Letters*, vol. 71, no. 2-3, pp. 155–157, 1979. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - S. Yanchuk and T. Kapitaniak, “Chaos-hyperchaos transition in coupled Rössler systems,”
*Physics Letters A*, vol. 290, no. 3-4, pp. 139–144, 2001. View at Publisher · View at Google Scholar · View at Scopus - S. Yanchuk, Y. Maistrenko, and E. Mosekilde, “Loss of synchronization in coupled Rössler systems,”
*Physica D: Nonlinear Phenomena*, vol. 154, no. 1-2, pp. 26–42, 2001. View at Publisher · View at Google Scholar · View at MathSciNet - C. X. Zhu, “Controlling hyperchaos in hyperchaotic Lorenz system using feedback controllers,”
*Applied Mathematics and Computation*, vol. 216, no. 10, pp. 3126–3132, 2010. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - S. Zheng, G. G. Dong, and Q. S. Bi, “A new hyperchaotic system and its synchronization,”
*Applied Mathematics and Computation*, vol. 215, no. 9, pp. 3192–3200, 2010. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - I. Petras,
*Fractional-Order Nonlinear Systems: Modeling, Analysis and Simulation*, Higher Education Press, Beijing, China, 2011. - B. J. Lurie, Three-parameter tunable Tilt-Integral-Derivative (TID) controller, U.S. Patent. 5, 371, 670, pp. 54–66, 1994.
- I. Podlubny, “Fractional-order systems and $P{I}^{\lambda}{D}^{\mu}$-controllers,”
*Institute of Electrical and Electronics Engineers. Transactions on Automatic Control*, vol. 44, no. 1, pp. 208–214, 1999. View at Publisher · View at Google Scholar · View at MathSciNet - A. Oustaloup, J. Sabatier, and P. Lanusse, “From fractal robustness to the CRONE control,”
*Fractional Calculus & Applied Analysis*, vol. 2, no. 1, pp. 1–29, 1999. View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - M. S. Tavazoei and M. Haeri, “A necessary condition for double scroll attractor existence in fractional-order systems,”
*Physics Letters A*, vol. 367, no. 1-2, pp. 102–113, 2007. View at Publisher · View at Google Scholar · View at Scopus - A. M. Chen, J. A. Lu, J. H. Lü, and S. M. Yu, “Generating hyperchaotic Lü attractor via state feedback control,”
*Physica A*, vol. 364, pp. 103–110, 2006. View at Publisher · View at Google Scholar · View at Scopus - X. Wu, Z. H. Guan, and Z. P. Wu, “Adaptive synchronization between two different hyperchaotic systems,”
*Nonlinear Analysis: Theory, Methods & Applications*, vol. 68, no. 5, pp. 1346–1351, 2008. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet - T. Kapitaniak and L. O. Chua, “Hyperchaotic attractors of unidirectionally-coupled Chua's circuits,”
*International Journal of Bifurcation and Chaos in Applied Sciences and Engineering*, vol. 4, no. 2, pp. 477–482, 1994. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at MathSciNet

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