Elsevier

Physics Letters A

Volume 375, Issue 24, 13 June 2011, Pages 2322-2326
Physics Letters A

Finite-time synchronization for a class of chaotic and hyperchaotic systems via adaptive feedback controller

https://doi.org/10.1016/j.physleta.2011.04.041Get rights and content

Abstract

This Letter investigates chaos synchronization of chaotic and hyperchaotic systems. Based on finite-time stability theory, a simple adaptive control method for realizing chaos synchronization in a finite time is proposed. In comparison with previous methods, the present method is not only simple, but could also be easily utilized in application. Numerical simulations are given to illustrate the effectiveness and validity of the proposed approach.

Highlights

► Optimizing the synchronization time is essential for chaotic synchronization application. ► This is particularly important in communication system for recovering encoded message/data. ► This Letter proposes an adaptive control method for realizing finite-time chaos synchronization. ► The method gives simple control inputs that guarantee finite-time synchronization. ► It could be exploited for experimental realization of finite-time synchronization.

Introduction

The phenomenon of synchronization has been known since the 17th century through the work of Christian Huygens. However, its importance, particularly for chaotic systems was not fully realized until Pecora and Carroll [1] in 1990 presented their seminal work on chaos synchronization. Since then, increased interest has been devoted to the study of varieties of synchronization phenomena in many chaotic systems. Some recent advances in different kinds of chaotic synchronization and reviews of relevant experimental applications of various techniques can be found in [2], [3]. Many significant real applications have been found in different areas including secure communication, chaos generators design, chemical reactions, biological systems, information science, to mention but a few [4], [5], [6], [7], [8], [9].

In principle, synchronization between two chaotic systems (with state space x(t) and y(t)) is directly equivalent to the asymptotic stabilization of the error state (i.e. |y(t)x(t)|0 as t). Based on the above rule, a large number of chaos synchronization schemes are aimed at achieving synchronization asymptotically. From a practical point of view, optimizing the synchronization time is more important than achieving asymptotic synchronization. This implies the optimality in settling time [11]. In secure communication and data encryption systems for instance, the range of time during which chaotic systems are out-of-synchrony is equivalent to the range of time in which the encoded message/data cannot be recovered or sent; due to the fact that the first bits of standardized bit strings always contain signalization data, namely the “identity card” of the message. Therefore, minimizing the synchronization time is essential for achieving fast communication synchrony; and this could be done by means of finite-time control—a very promising technique that has demonstrated better robustness and disturbance rejection properties [10], [11], [12].

Some authors have investigated chaos synchronization based on finite-time [13], [14], [15], [16], [17], [18]. However, the works reported in Refs. [14], [16], [17], were more specific to some systems; while the proposed methods in Ref. [16], [17] are such that control inputs must be applied to all the state space dynamics. This introduces undue complication into the control inputs—making them too complex compared to systems being controlled. These approaches are usually difficult to implement in experiments when possible. Recent research results have shown that the unified chaotic system can indeed be stabilized using a single variable feedback [25], [26]. This technique is very promising, not only for stabilization but also for synchronization [19], [20], [21]. In fact, the problem of controller complexity has recently become a crucial issue in control theory research [22], [23], [24], [25], [26] because simple control inputs, for example, simple limiters are easy-to-implement and effective for stabilizing irregular fluctuations [22], [23].

Moreover, the works in Refs. [14], [16], [17] were limited to lower dimensional chaotic systems. Considering finite-time synchronization for higher dimensional chaotic systems (hyperchaotic systems) is very relevant since they are potential models for secure communications. To our knowledge, there are no results in this direction. In this Letter, we propose a more general control scheme based on the finite-time stability theory for realizing chaos synchronization in a finite time. Recently, we have employed this method to achieve finite-time stabilization of three-dimensional chaotic systems [27]. In Ref. [27], we proposed a theorem for finite-time stabilization and used several examples to show that stabilization can indeed be achieved in finite-time with single control input. In the present Letter, we develop on our previous technique [27] in relation to master–slave synchronization scheme in other to achieve finite-time chaos synchronization. We would show that this approach is also effective for synchronizing a large class of chaotic as well as hyperchaotic systems. In Section 2, we give some preliminary definitions. Section 3 contains the main results; while in Section 4, some examples are used for illustrations. Our conclusions are given in Section 5.

Section snippets

Preliminary definition and lemma

Finite-time synchronization of chaotic systems means that the state of the master system can converge to the state of the slave system after a finite time. The precise definition of finite-time synchronization and a lemma are given below. For details see [16], [17]. Here, we extend the definition and lemma in our previous paper [27] to a master–slave configuration of coupled chaotic systems.

Definition 1

Consider the following chaotic system [27]x˙=f(x), where f(x)=(f1(x),f2(x),,fn(x))T:RnRn; x=(x1,x2,,xn)

Main results

In this section, we make use of the same assumption as in our previous paper to develop the proposed finite-time synchronization scheme (see Ref. [27]).

Assumption 1

There exists a nonsingular coordinate transformation z=Te, such that system (3) can be rewritten asw˙1=G1(x,w1,w2),w˙2=G2(x,w1,w2), where w1=(e1,e2,,el)TRl and w2=(el+1,el+2,,en)TRnl. The vector function G2(x,w1,w2) is a smooth function in the neighborhood of w1=0, and the subsystem w˙2=G2(x,0,w2) is uniformly exponentially stable about the

Applications

We have tested the applicability of our proposed approach to a large number of chaotic and hyperchaotic systems. In this section, we choose two examples—a chaotic and hyperchaotic system, respectively for the purpose of illustration and brevity.

Conclusion

Summarily, optimizing the synchronization time is essential for real-time data applications. This is currently a challenging task in control theory applications. To tackle this problem with the simplest control input, we have investigated the synchronization of chaotic and hyperchaotic systems based on finite-time stability theory, and proposed a simple adaptive control method for chaos synchronization within a finite time. For three-dimensional chaotic systems in particular, a single control

Acknowledgements

U.E.V. has been supported by the British Academy, the Royal Academy of Engineering and the Royal Society of London, through the Newton International Fellowships. We acknowledge the reviewers constructive comments.

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    Permanent address: Department of Physics, Faculty of Science, Olabisi Onabanjo University, P.M.B. 2002, Ago-Iwoye, Nigeria.

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