Volume 2013, Issue 1 503659
Research Article
Open Access

Projective Lag Synchronization of Delayed Neural Networks Using Intermittent Linear State Feedback

Junjian Huang

Junjian Huang

College of Computer Science, Chongqing University, Chongqing 400030, China cqu.edu.cn

Department of Computer Science, Chongqing University of Education, Chongqing 400067, China cqu.edu.cn

Search for more papers by this author
Chuandong Li

Corresponding Author

Chuandong Li

College of Computer Science, Chongqing University, Chongqing 400030, China cqu.edu.cn

School of Electronics and Information Engineering, Southwest University, Chongqing 400715, China southwest.edu

Search for more papers by this author
Tingwen Huang

Tingwen Huang

Texas A&M University at Qatar, P.O. Box 23874, Doha, Qatar qatar.tamu.edu

Search for more papers by this author
Huaqing Li

Huaqing Li

College of Computer Science, Chongqing University, Chongqing 400030, China cqu.edu.cn

Search for more papers by this author
Mei Peng

Mei Peng

College of Mathematical and Computer Science, Yangtze Normal University, Chongqing 400084, China yznu.cn

Search for more papers by this author
First published: 18 November 2013
Citations: 3
Academic Editor: Jinde Cao

Abstract

The problem of projective lag synchronization of coupled neural networks with time delay is investigated. By means of the Lyapunov stability theory, an intermittent controller is designed for achieving projective lag synchronization between two delayed neural networks systems. Numerical simulations on coupled Lu neural systems illustrate the effectiveness of the results.

1. Introduction

In the past few years, synchronization of neural networks has been extensively investigated due to their successful application in many areas, such as communication, modeling brain activity, signal processing, and combinatorial optimization. There are several different synchronization schemes including complete, lag, projective, generalized, phase, and anticipated synchronization [19]. In projective synchronization, the master-slave systems can be synchronized up to a scaling factor. Due to the potential applications in secure communication, projective synchronization has attracted increasing attention [1013]. In [10], the authors study the projective synchronization for different chaotic delayed neural networks via sliding mode control approach. Function projective synchronization of two-cell Quantum-CNN chaotic oscillators using adaptive method is investigated in [11]. It is worth noting that the propagation delay may exist in remote communication systems. However, to the best of the authors’ knowledge, few results (if any) for the projective lag synchronization of neural networks with time delay have been reported in the literature.

In this paper, we will deal with the analysis issue for projective lag synchronization of neural networks with time delay by intermittent control approach. Recently, we have employed this method to stabilize and synchronize chaotic systems [1416]. In this paper, by using Lyapunov stability theory and intermittent control technique, the intermittent controllers and corresponding parameter update rules are designed to obtain projective lag synchronization of neural networks. The rest of the paper is organized as follows. In Section 2, we formulate the problem of projective lag synchronization of coupled neural networks. In Section 3, a general scheme for the projective lag synchronization is presented. Numerical simulations are given in Section 4. Finally, conclusions are given in Section 5.

2. Problem Formulation and Preliminaries

In this paper, we consider the chaotic cellular neural networks described by
()
or, in a compact form,
()
where x(t) = [x1(t), x2(t), …, xn(t)] ∈ Rn denotes the state vector, C, A, and BRm×m are constant matrices, τ is the time delay, and f, g : RmRm are nonlinear functions satisfying the Lipschitz condition, namely; there exist positive constants Lf, Lg such that, for all x, yRn,
()
Consider the corresponding slave system given in the following form:
()
where y(t) ∈ Rn denotes the state vector, C, A, and BRn×n are constant matrices, and u(t) denotes the intermittent feedback control defined as follows:
()
where k denotes the control strength, 0 < σ < 1 denotes the switching rate, T denotes the control period, and H(t) and K(t) are the active control functions.
Let θ be the transmittal delay. Defining the projective lag synchronization error between systems (2) and (4) as e(t) = y(t) − αx(tθ), where α denotes projective scaling factor, we have the following error dynamical system:
()
Under the control of the form (5), the system (6) can be rewritten as
()

Definition 1. The master system (2) and the slave system (4) are said to be projective lag synchronization if there exist a compact set α, σ and delay time θ such that, for any initial values φ(t0), ψ(t0) ∈ Ω, t0 ∈ [−τ, 0], the error system is exponentially stable; that is,

()

3. Main Results

This section addresses the projective lag synchronization problem of coupled neural networks.

Theorem 2. Suppose that there exist constants α, the coupling strength k, time delay θ, and the functions H(t), K(t) such that

  • (i)

    C + CT − 2kI + g1I ≤ 0;

  • (ii)

    C + CTg2I ≤ 0;

  • (iii)

    H(t) = −Af(y(t)) − Bg(y(tτ)) + αAf(x(tθ)) + αBg(x(tτθ));

  • (iv)

    K(t) = −k(y(t) − αx(tθ));

  • (v)

    g1σ − (1 − σ)g2 > 0.

Then, the projective lag synchronization error system (7) is globally exponentially stable, that is; the projective lag synchronization between the master system (2) and the slave system (4) under intermittent control (5) is achieved.

Proof. Consider the following Lyapunov function:

()

When nTt < nT + σT, the derivative of (9) with respect to time t along the trajectories of the first subsystem of the system (7) is calculated and estimated as follows:

()
Similarly, when nT + σTt < (n + 1)T, one obtains
()
Therefore,
()
Then, one observes that
()
By (12) and (13), we can obtain the following.

(1) For 0 ≤ t < σT,

()

(2) For σTt < T,

()

(3) For Tt < T + σT,

()

(4) For T + σTt < 2T,

()
By induction, we have the following.

(5) For nTt < nT + σT,

()
Note that (tσT)/Tn < t/T; in this case, we can obtain
()

(6) For nT + σTt < (n + 1)T

()
Note that t/Tn + 1 < (t + TσT)/T; in this case, we can obtain
()
Therefore, for any t ≥ 0,
()

This implies that the projective lag synchronization error system (7) is globally exponentially stable, and the following estimate holds:

()

This implies that the projective lag synchronization between the master system (2) and slave system (4) is achieved.

Let and , where , . If we replace the first condition in Theorem 2 with , , then Theorem 2 also can hold. In addition, one can obtain the following corollary from Theorem 2.

Corollary 3. Suppose that there exist positive scalars k and σ satisfying 0 < σ < 1 such that

()
where and . Then, the system (7) is exponentially stable, and the projective lag synchronization between the master system (2) and the slave system (4) under intermittent control (5) is achieved.

Remark 4. If α = 1, it is clear that the lag synchronization between the system (2) and system (4) will occur.

Remark 5. It is clear that when the time delay vanishes, that is, θ = 0, we have e(t) = y(t) − αx(t), which implies that the projective synchronization between master system (2) without delay and system (4) without delay will occur.

Remark 6. From Corollary 3, one observes that the control strength k can be estimated as follows:

()

Note that C are determined only by the system itself, and σ is control parameter. Then, we can estimate the feasible region D of control parameters (k, σ) as follows:

()

4. Numerical Example

In this section, Lu neural oscillator [17] is presented as an example to verify the effectiveness of Theorem 2. The programs DDE23 in MATLAB are used to solve numerically the delay differential equations.

Example 1. Consider the Lu neural oscillator [17]

()
where
()
and f(x(t)) = g(x(t)) = tanh(x(t)).

This model was investigated by Lu in [17] where it was shown to be chaotic, as shown in Figure 1. The corresponding slave system is given by

()

From Theorem 2, the controller can be obtained as follows:

()
So, when nTt < nT + σT, we have
()
When nT + σTt < (n + 1)T, we have
()

Noting that λmax (C + CT) = 2, the feasible region of control parameters (k, σ) is D = {(k, σ)∣k < k* = −1/σ,  0 < σ < 1}, as shown in Figure 2. For numerical simulation, we select α = 2, θ = 0.01, σ = 0.1, and k = 10 and plot the norm of projective lag synchronization errors curve, as shown in Figure 3. As the time t goes to infinity, the projective lag synchronization error system is stable. Hence, the projective lag synchronization between system (27) and system (29) is achieved.

Details are in the caption following the image
The chaotic attractor of the Lu oscillator described by (7) with initial value x1(θ) = 0.2, x2(θ) = −0.5, for θ ∈ [−1,   0].
Details are in the caption following the image
The relationship between k and σ.
Details are in the caption following the image
The norm of synchronization error curve with α = 2, θ = 0.01, σ = 0.1 and k = 10.

5. Conclusions

This paper addressed projective lag synchronization of coupled neural networks with time delay. Based on Lyapunov stability theory and adaptive control techniques, several criteria for projective lag synchronization of identical neural networks with time delay have been established. With the proposed method, the simulations of projective lag between coupled Lu systems have showed the effectiveness of theoretical result.

Acknowledgments

This publication was made possible by NPRP Grant no. NPRP 4-1162-1-181 from the Qatar National Research Fund (a member of Qatar Foundation). The statements made herein are solely the responsibility of the authors. This work was also supported by Natural Science Foundation of China (Grant no. 61374078), the Scientific and Technological Research Program of Chongqing Municipal Education Commission (Grant no. KJ121505), the Natural Science Foundation Project of Chongqing CSTC (Grant no. cstc2011jjA40005).

      The full text of this article hosted at iucr.org is unavailable due to technical difficulties.