Projective synchronization of different chaotic time-delayed neural networks based on integral sliding mode controller
Introduction
Chaos appears in time evolutions of some kinds of nonlinear equations. Chaotic systems intrinsically defy synchronization due to the evolution of a chaotic system sensitive dependence on its initial condition. However, since the pioneer work that Pecora and Carroll introduced a method to realize the synchronization of two identical chaotic systems with different initial conditions [1], many attentions have been attracted on the chaos synchronization over the past decades. The increasing interest in researching the synchronization characteristics of chaotic systems stems from its potential applications in cryptography, secure communication, optimization of nonlinear systems performance, modeling brain activity, and chemical reaction [2], [3], [4], [5], [6], [7]. The phenomena of chaos synchronization in coupled nonlinear systems are being extensively studied in the context of laser dynamics, electronics circuits, chemical and biological systems [8].
Recently, the study of dynamical properties of neural networks appears more and more [9], [10], [11], [12] due to their extensive applications in differential fields such as signal and image processing, combinatorial optimization, pattern recognition and etc. In the electronic implementation of a neural network, time delay will occur in the interaction between the neurons inevitably, and will affect the dynamic behavior of the neural network model. In some particular cases, chaotic and hyperchaotic attractors may be generated by the introduction of delays into neural networks [13], [14], [15]. Therefore, some time-delayed neural networks could be as a model when we study the chaos synchronization.
In practice, the chaotic systems are inevitably subject to some environmental changes, which may render their parameters to be variant. Furthermore, from the point of view of engineering, it is very difficult to keep the two chaotic systems to be identical all the time [16]. It is thus of great significance to study the synchronization problem of nonidentical chaotic neural networks. Obviously, if the neural networks considered are distinct and with time delay, it becomes more complex and challenging. Not any two different chaotic systems can be synchronized. The synchronization can occur only when the response system attractor possesses the same topological characteristic as the drive system in essence, such as Lyapunov exponents and fractal dimensions [17].
Over the past few years, following complete synchronization, several new types of synchronization have been found in interesting chaotic systems, such as anticipatory synchronization [18], lag synchronization [19], phase synchronization [20], antiphase synchronization [21], generalized synchronization [22], and etc. Among all kinds of chaos synchronization, projective synchronization, characterized by a scaling factor that two systems synchronize proportionally, is one of most interesting problems. Projective synchronization is interesting because of its proportionality between the synchronized dynamical states. In application to secure communication, this feature can be used to M-nary digital communication for achieving fast communication [23].
In 1998, projective synchronization phenomenon was first reported and discovered by Gonzalez-Miranda [24]. She observed that when chaotic systems exhibit invariance properties under a special type of continuous transformation, amplification and displacement of the attractor occurs. This degree of amplification or displacement obtained is smoothly dependent on the initial condition. By this definition, complete synchronization is not a special case of projective synchronization. In 1999, Mainieri and Rehacek called this type of synchronization projective synchronization [25], and declared that the two identical systems could be synchronized up to a scaling factor α. Subsequently, some researchers extended the concept of projective synchronization and termed it as generalized projective synchronization [26], [27]. Dibakar Ghosh in Ref. [23] presented a point of view that projective synchronization is not in the category of generalized synchronization because the response system of projective synchronization is not asymptotically stable.
In the past 15 years, many techniques for chaos synchronization have been developed. These include periodic parametric perturbation [28], drive-response synchronization [29], adaptive control [30], sliding mode (or variable structure) control [31], [32], [33], backstepping control [34], fuzzy control [35], impulsive control [36], and many others. The sliding mode control theory introduced by Utkin [37] in 1977 provides an efficient way to the robust control problem. Its main advantages are fast response, good transient performance and robustness to variations of system parameters.
In this paper, an integral sliding mode control approach will be developed to address the projective synchronization problem of different chaotic time-delayed neural networks. It overcomes some limitations of the previous work where projective synchronization has been investigated only in chaotic systems without time delay [25], [26], [27], [33], [34] or in delayed chaotic systems always with identical structure and same parameters [38], [39]. Firstly, an integral sliding surface is properly constructed and an integral sliding mode controller is designed to guarantee the reachability of the specified sliding surface. Then, by employing the L–K function and LMI technique, the delay-dependent condition is derived under which the resulting error system is globally asymptotically stable in the specified switching surface. Generally speaking, delay-dependent conditions are less conservative than the delay-independent ones, especially when the size of delay is small. Moreover, in engineering practice, information on the delay range is generally available [40]. The main contributions of this study are to propose an integral sliding mode controller to deal with the projective synchronization of different drive-response systems with delay, obtain a delay-dependent LMI criterion for the stability of error system by constructing an appropriate Lyapunov–Krasovskii function, verify the conservativeness of the maximum time-delay value solved by L–K method and LMI technique [40], [41], [42], [43] and show the variation of convergence velocity of the error dynamical system with the gain matrix in the simulation. Notation Throughout the paper, for any real symmetric matrices A and B, the notation A ⩾ B or A > B means that matrix A − B is positive semi-definite or positive definite, and A ⩾ 0 or A > 0 means that matrix A is positive semi-definite or positive definite. AT and A−1 represent the transpose and the inverse of matrixA respectively.
Section snippets
Problem description and preliminaries
A class of delayed chaotic neural networks is described by the following time-delay differential equations:where n ⩾ 2 denotes the number of neurons in the network, xi(t) denotes the state variable associated with the ith neuron, τ ⩾ 0 denotes the transmission time delay, ci > 0 denotes the self connection of neurons, aij indicates the strength of the neuron interconnections within the network, bij indicates the strength of the neuron
Sliding surface and equivalent control law design
It can be seen clearly from (8) that the dynamic behavior of the error system depends on the chaotic states x(t) and x(t − τ) of the drive system (2) because of the difference between the drive and response systems and the existence of scaling factor α in projective synchronization. Therefore, projective synchronization between different chaotic neural networks (2), (4) cannot be achieved only by utilizing output feedback control. An integral sliding mode control approach will be proposed to
Numerical simulations
Assume that the following delayed chaotic Hopfield neural networks [13] is the drive system:where gj(xj(t)) = tanh (xj(t)), j = 1, 2, and the following delayed chaotic cellular neural networks [14] is the response system:where fj(zj(t)) = 0.5(∣zj(t) + 1∣ − ∣zj(t) − 1∣), j = 1, 2.
For numerical simulation, we choose the fourth-order Runge–Kutta method to solve the
Conclusions
In the fields of secure communication, projective synchronization can be used to extend binary digital to M-nary digital communication for achieving fast communication, so the research on projective synchronization has important theoretical significance and improved value. Furthermore, projective synchronization has been applied in the research of secure communication due to the unpredictability of the scaling factors. In this paper, the projective synchronization problem has been studied for
Acknowledgements
This research is supported by the NNSF of China under Grant No. 10532050, the National Outstanding Young Funds of China under Grant No. 10625211 and the Program of Shanghai Subject Chief Scientist No. 08XD14044.
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2021, European Journal of ControlCitation Excerpt :As a result, one can get desired benefits such as robustness, tracking ability and insensitivity to external disturbance. In comparison with the existing works of [19,23,46,53], the fixed-time sliding mode control approach (SMC) of this letter is superior to them from the following aspects: 1) Based on the idea given in [46], the constructed integral sliding mode surface is extended. 2) The fixed-time synchronization between drive-response systems (1) and (2) is assured under the fixed-time SMC, but the synchronization in fixed-time cannot be obtained by these SMC in [19,23,46,53].
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2020, ISA Transactions