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New results of exponential synchronization of complex network with timevarying delays
Advances in Difference Equations volume 2019, Article number: 10 (2019)
Abstract
In this study, we elucidated the exponential synchronization of a complex network system with timevarying delay. Then the exponential synchronization control of several types of complex network systems with timevarying delay under no requirements of delay derivable were explored. The dynamic behavior of a system node shows timevarying delays. Thus, to derive suitable conditions for the exponential synchronization of different complex network systems, we designed a linear feedback controller for linear coupling functions, using the Lyapunov stability theory, Razumikhin theorem, and Newton–Leibniz formula. The exponential damping rates for the exponential synchronization of different complex network systems were then estimated. Finally, we validated our conclusions through a numerical simulation.
1 Introduction
Many problems in nature can be descrobed by complex network models, such as the World Wide Web (WWW), food chains, traffic networks, and social networks. Thus, complex networks have attracted widespread interest.
Synchronization is an important dynamic characteristic of a complex network. Many phenomena in nature are realized by the synchronization of complex networks. For example, Strogatz discovered the synchronized contractions of cardiac muscle cells [1]. Steinmetz et al. discovered that the attention selection modes of human beings and primates are closely related with the synchronous rates of their neurons [2]. Furthermore, synchronization technologies have been widely applied in practical life. Millerioux et al. achieved chaos secure transmission from the master–slave system [3]. Kunbert et al. suggested solving problems encountered in image processing through the use of synchronously generated autowaves [4]. Synchronization control has received considerable attention in the control field, and many control technologies have been introduced into the synchronization of networks. Adaptive, pulse, intermittent, and pinning controls have been used for the synchronous control of complex networks and thereby contributed to many outstanding works [5,6,7,8].
Information transition in a network is often accompanied by time delay, which is a major cause of system instability. Therefore, studying the stability of a timedelay system has become a critical topic in control theory. Given that the timedelay system is an infinitedimensional system, studying it is difficult, and no general research method for its study is currently available. Moreover, different problems require different control technologies. This condition often results in inconsistent research conclusions [9, 10]. Nevertheless, research on methods for the synchronous control of complex networks with time delay has achieved considerable progress [11,12,13,14,15,16].
Given that time delay always changes, most studies mainly focus on the synchronization of complex network model with timevarying delay. For research on timevarying delay there are two requirements. First, timevarying delay should have boundaries [17,18,19]. Second, the derivative of a timevarying delay should satisfy only one condition. It generally requires the derivative of a timevarying delay. This derivative should be smaller than 1 [20,21,22,23,24] or should be localized in one boundary [25,26,27]. Meanwhile, the derivation of a rapidly changing timevarying delay may fail, and thus these methods are ineffective. Inspired by Ref. [9], we propose a novel method to address the problems encountered in the synchronous control of a complex network with timevarying delay. In this method, a derivable timevarying delay is unnecessary, and stability conditions for the exponential synchronization of systems are concluded by the Razumikhin theorem. This study has some innovation points:

(1)
The timevarying delay function is removed as a derivable in the study of synchronous control of common timedelay complex systems. The synchronous control problem in complex systems with timevarying delay is studied by using the Razumikhin theorem and the Newton–Leibniz formula.

(2)
Several types of complex network systems with timevarying delay are nonlinear functions and contain timevarying delays, and the conditions for exponential synchronization are obtained on the basis of the hypothesis that the nonlinear function satisfies the Lipschitz function, whether or not the coupling function between the network nodes is linear. These conditions satisfy a linear matrix inequality and are easy to determine. The upper boundary of timevarying delay can easily be calculated with the MATLAB tool box.
Notations
All the notations used in this paper are standard. For \(x \in \mathbb{R}^{n}\), let \(\Vert x \Vert \) denote the Euclidean vector norm, i.e., \(\Vert x \Vert = \sqrt{(x^{T}x)}\). For \(A \in \mathbb{R}^{N \times N}\), let \(\Vert P \Vert \) indicate the norm of P induced by the Euclidean vector norm, i.e., \(\Vert P\Vert = \sqrt{ \eta _{\max }(P^{T}P)}\), where \(\eta _{\max }(P^{T}P)\) is the maximum eigenvalue of \(P^{T}P\), I denotes the identity matrix with appropriate dimensions, \(\mathbb{R}^{m \times n}\) denotes the set of all \(m \times n\) real matrices, and \(\mathbb{R}^{n}\) is the ndimensional Euclidean space. For symmetric matrices A and B, the notation \(A > B\) (\(A \ge B\)) means that the matrix \(A  B\) is positive definite (nonnegative); \(\operatorname{diag}\{\ldots\}\) is used to denote the block diagonal matrix; the superscript “T” represents the transpose; let \(A \otimes B\) be the Kronecker product of two matrices A and B.
2 Preliminaries
We consider a general timevarying delay complex dynamic network consisting of N dynamic nodes with linear couplings, which is described by
\(x_{i} = (x_{i1}(t),x_{i2}(t),\ldots,x_{in}(t))^{T} \in \mathbb{R}^{n}\) is the state vector of the ith leader, \(f:\mathbb{R}^{n} \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) is a continuously differential nonlinear vector function, \(c_{1} > 0\) and \(c_{2} > 0\) are the nondelay and timevarying delay coupling strengths, \(\varGamma _{1} = \operatorname{diag}(\gamma _{1}^{1},\gamma _{1}^{2},\ldots,\gamma _{1}^{n})\) and \(\varGamma _{2} = \operatorname{diag}( \gamma _{2}^{1},\gamma _{2}^{2},\ldots,\gamma _{2}^{n})\) are positive definite diagonal matrices, which represent the inner connection matrices between each pair of nodes; Meanwhile, \(A = (a_{ij}) \in \mathbb{R}^{N \times N}\), \(B = (b_{ij}) \in \mathbb{R}^{N \times N}\) are the nondelay and timevarying delay weight matrices. The entries are defined as follows: if is a link is present from the node i to the node j (\({i \ne j}\)), then \(a_{ij} \ne 0\), \(b_{ij} \ne 0\); otherwise \(a_{ij} = 0\), \(b_{ij} = 0\), and the diagonal elements of matrices A and B are defined as \(a_{ii} =  \sum_{j = 1,j \ne i}^{N} a_{ij}\), \(b_{ii} =  \sum_{j = 1,j \ne i}^{N} b_{ij}\). Given that the networks in this paper are direct, \(a_{ij} \ne a_{ji}\) and \(b_{ij} \ne b_{ji}\) (\(i,j = 1,2,\ldots,N\)). The coupling timevarying delay \(\tau (t)\) is a bound function and a positive constant τ satisfying \(0 \le \tau (t) \le \tau \), \(\forall t > 0\), \(u_{i} \in \mathbb{R}^{N \times N}\) is the control input of node i. In this paper, we aim to design a suitable controller
where \(k_{i}\) is the gain of the ith node.
Let \(\tilde{f}(x(t),x(t  \tau (t))) = f(x(t),x(t  \tau (t)))  f(s(t),s(t  \tau (t)))\), and \(K = \operatorname{diag}(k_{1},k_{2},\ldots,k_{n})\).
We use the Newton–Leibniz formula
Equation (1) is converted to
The set \(s = \{ x_{1}^{T}(t),x_{2}^{T}(t),\ldots,x_{n}^{T}(t) \in \mathbb{R}^{n}\vert {x}_{i}(t) = s(t),i \in \mathbb{N}\}\) is defined as synchronization manifold, where \(s(t) \in \mathbb{R}^{n}\) satisfies
The synchronization error vector is defined as
Through Eqs. (4) and (5), we can obtain the following error system:
To achieve the synchronization of system (1), we add controller (2) to the error system and we have
Therefore, if the error system (6) is exponentially stable, then the complex network (1) is exponentially synchronized.
The following assumptions and lemmas are needed for the derivation of our main results.
Definition 1
(see [9])
The complex network system is exponentially synchronized when positive numbers ξ, α are present, so every error vector \(e(t,\phi )\) of the system satisfies
Lemma 1
(Cauchy inequality [9])
For any vector \(x,y \in \mathbb{R}^{n}\) and positive definite matrix \(W \in \mathbb{R}^{N \times N}\), the following matrix inequality holds:
Lemma 2
(Razumikhin stability theorem [28])
Assume that \(\upsilon ,u,\omega :\mathbb{R}^{ +} \to \mathbb{R}^{ +} \) are nondecreasing, and \(u(v)\), \(\upsilon (v)\) are positive for \(v \ge 0\), \(\upsilon (0) = u(0) = 0\), and \(q > 1\). If a function \(V(t,e): \mathbb{R}^{ +} \times \mathbb{R}^{ +} \to \mathbb{R}^{ +} \) exists, so

(i)
\(u( \Vert e \Vert ) \le V(t,e) \le \upsilon ( \Vert e \Vert )\), \(t \in \mathbb{R}^{ +}\), \(e \in \mathbb{R}^{n}\),

(ii)
\(\dot{V}(t,e(t)) \le  \omega ( \Vert e \Vert )\), if \(V(t + v,e(t + v)) \le qV(t,e(t))\), \(\forall v \in [  \tau ,0]\), \(t \ge 0\),
then the error system is asymptotically stable.
Lemma 3
(Schur complement [29])
The matrix \left[\begin{array}{cc}{S}_{11}& {S}_{12}\\ {S}_{21}& {S}_{22}\end{array}\right]<0, where \(S_{11} = S_{11}^{T}\), \(S_{12} = S_{21}^{T}\) is equivalent to any one of the following conditions:

(1)
\(S_{22} < 0\), \(S_{11}  S_{12}S_{22}^{  1}S_{12}^{T} < 0\);

(2)
\(S_{11} < 0\), \(S_{22}  S_{12}^{T}S_{11}^{  1}S_{12} < 0\).
Assumption 1
(see [30])
For the vector function \(f(x(t),x(t  \tau (t)))\), suppose that the uniform Lipschitz condition holds and \(L_{1}\) and \(L_{2}\) are positive numbers such that
In particular, we have
where \(i = 1,2,\ldots,N\).
Remark 1
In some studies on complex network synchronization problems, the effects of time delay were not considered. For example JinLiang Wang discussed the output synchronization and \(H_{\infty } \) output synchronization of multiweighted complex network in [31] but did not consider the network model with time delay. Moreover, many studies on complex network often require derivable or bounded time delay [20,21,22,23,24,25,26,27]. In the proposed model, the requirements for time delay (\(\tau (t)\)) are reduced, and the time delay does not need to be differentiated.
Remark 2
At present, there are many research results on the synchronous control of linearly coupled complex network models [31,32,33], but their research methods are different from ours.
3 Main result
3.1 Synchronization control of a general complex dynamical network with dynamic behavior including timevarying delays and linear timevarying coupling delay consisting of N identical nodes with linear couplings
Theorem 1
The complex network system (1) is exponentially synchronized if positive numbers β, δ, λ, \(L_{1}\), \(L_{2}\) and a positive matrix P are present and the following inequality equation holds:
where \(\gamma _{1} = [4\lambda ^{  1} + 4\lambda ^{  1}\tau + 2K](P + \beta I) + \delta I\).
Moreover, the error vector \(e(t,\phi )\) satisfies the condition
Here \(p = \Vert P \Vert \).
Proof
Consider the following Lyapunov function:
where P is a positive symmetric matrix. It is easy to see that
For the chosen number \(\lambda > 0\), we have
We get the following inequality:
Therefore, the following estimates hold by applying Lemma 2 with \(W = I\), and by taking \(q \to 1^{ +} \):
In a similar way
According to the above proof, we get
Assume \(\dot{V} \le  \delta e^{T}e\), where \(\forall \delta > 0\), it means \(\dot{V} < 0\), therefore
According to Lemma 3, it is equivalent to the following matrix inequalities:
Here \(\gamma _{1} = [4\lambda ^{  1} + 4\lambda ^{  1}\tau + 2K](P + \beta I) + \delta I\) and
This, by the Razumikhin stability theorem and Lemma 2, implies the asymptotic stability of the error system (6). To find the exponential factor of the solution, integrating both sides of the inequality, due to (16), \(\dot{V}(t,e(t)) \le 0\) and using the condition (8), we have
such that
Hence
Here \(p = \Vert P \Vert \), this completes the proof of Theorem 1. □
Remark 3
Although many studies on the synchronous control of complex network systems with timevarying delay have generated many and variable conclusions, the studies, especially those regarding the synchronization stability of systems, all used the same two requirements on timevarying delay. First, a timevarying delay should have boundaries; that is, \(0 \le \tau (t) \le \tau \), \(\forall t > 0\). Second, the timevarying delay should be derivable and smaller than 1; that is, \(0 \le \dot{\tau } (t) \le 1\), \(\forall t > 0\). For example [22, 25], the timevarying delay may not be derivable. In fact, the timevarying delay is not derivable when it changes quickly in a time period. In this study, only the first requirement of timevarying delay is needed. The second requirement can be solved by the Newton–Leibniz formula. The stability conditions of the exponential synchronization of the system are obtained through the Razumikhin theorem. Therefore, this theorem relieves the requirements to the system in contrast to the theorems used in other studies [20,21,22,23,24,25,26,27].
Remark 4
In [34, 35], the synchronization (or stability) of similar models, which all require a derivable timevarying delay, is investigated. Similarly, this requirement is unnecessary in Corollary 2.
As a special case, for the system (17), we consider the following Lyapunov function:
According to the proof of Theorem 1, it is easy to get the following conclusion. We have the following corollary.
Corollary 1
The complex network system (1) is exponentially synchronized if positive numbers β, δ, λ, \(L_{1}\), \(L_{2}\), and a positive matrix P exist such that the following inequality equation holds:
where \(\gamma _{2} = [4\lambda ^{  1} + 4\lambda ^{  1}\tau + 2K]P + \delta I\).
Moreover, the error vector \(e(t,\phi )\) satisfies the condition
Here \(p = \Vert P \Vert \).
Remark 5
In Corollary 1, \(\beta e^{T}e\) is removed from the Lyapunov function by proving Theorem 1, which simplifies the judgment on synchronization stability and requires fewer parameters. However, this approach increases the difficulty of selecting the parameter λ.
3.2 The synchronization control of complex dynamical network with timevarying coupling delay consisting of N identical nodes with linear couplings
In this section, we consider a general complex dynamical network consisting of dynamical nodes with linear couplings, which is described by
\(x_{i} = (x_{i1}(t),x_{i2}(t),\ldots,x_{in}(t))^{T} \in \mathbb{R}^{n}\) is the state vector of the ith leader, \(f:\mathbb{R}^{n} \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) is a continuously differential nonlinear vector function, \(c_{1} > 0\) and \(c_{2} > 0\) are the nondelay and timevarying delay coupling strengths, \(\varGamma _{1} = \operatorname{diag}(\gamma _{1}^{1},\gamma _{1}^{2},\ldots,\gamma _{1}^{n})\) and \(\varGamma _{2} = \operatorname{diag}( \gamma _{2}^{1},\gamma _{2}^{2},\ldots,\gamma _{2}^{n})\) are positive definite diagonal matrices, which represent the inner connection matrices between each pair of nodes; \(A = (a_{ij}) \in \mathbb{R}^{N \times N}\), \(B = (b_{ij}) \in \mathbb{R}^{N \times N}\) are the nondelay and timevarying delay weight matrices. The entries are defined as follows: if is a link is present from the node i to the node j (\(i \ne j\)), then \(a_{ij} \ne 0\), \(b_{ij} \ne 0\); otherwise \(a_{ij} = 0\), \(b_{ij} = 0\), and the diagonal elements of matrices A and B are defined as \(a_{ii} =  \sum_{j = 1,j \ne i}^{N} a_{ij}\), \(b_{ii} =  \sum_{j = 1,j \ne i}^{N} b_{ij}\). Given that the networks in this paper are direct, \(a_{ij} \ne a_{ji}\) and \(b_{ij} \ne b_{ji}\) (\(i,j = 1,2,\ldots,N\)). The coupling timevarying delay \(\tau (t)\) is a bound function and a positive constant τ satisfying \(0 \le \tau (t) \le \tau \), \(\forall t > 0\), \(u_{i} \in \mathbb{R}^{N \times N}\) is the control input of node i. In this paper, we aim to design a suitable controller,
where \(k_{i}\) is the gain of the ith node.
We use the Newton–Leibniz formula
We convert Eq. (21) to
The set \(s = \{ x_{1}^{T}(t),x_{2}^{T}(t),\ldots,x_{n}^{T}(t) \in \mathbb{R}^{n}\vert {x}_{i}(t) = s(t),i \in \mathbb{N}\}\) is defined as a synchronization manifold, where \(s(t) \in \mathbb{R}^{n}\) satisfies
Let \(\tilde{f}(x) = f(x)  f(s(t))\), \(K = \operatorname{diag}(k_{1},k_{2},\ldots,k_{N})\).
Define the synchronization error vector as
Through (22) and (23), in order to achieve the synchronization of system (20), we add controller (21) to the error system, we can get the following equation:
where \(e_{i}(t) = (e_{i1}(t),e_{i2}(t),\ldots,e_{in}(t))^{T} \in \mathbb{R}^{n}\), \(e(t) = (e_{1}(t),e_{2}(t),\ldots,e_{n}(t))^{T} \in \mathbb{R}^{n}\).
Therefore, if the error system (24) is exponentially stable, the complex network system (20) is exponentially synchronized.
Theorem 2
The complex network system (18) is exponentially synchronized if positive numbers β, δ, λ, \(L_{1}\), and a positive matrix P exist such that the following inequality equation holds:
where \(\gamma _{3} = L_{1}^{2}I + (1 + 4\tau )\lambda ^{  1}(P + \beta I) + \delta I + 2K(P + \beta I)\).
Moreover, the error vector \(e(t,\phi )\) satisfies the condition
Here \(p = \Vert P \Vert \).
Proof
We consider the following Lyapunov function:
Here P is a positive symmetric matrix. It is easy to see that
The time derivative of \(V(t,x)\) along the trajectory of the system (22) is given by
For the chosen number \(\lambda > 0\), we have
Therefore, the following estimates hold by applying Lemma 1 with \(W = I\):
In the light of the Razumikhin theorem, we assume that for any real number \(q > 1\)
and taking \(q \to 1^{ +} \) leads to
In a similar way
Therefore
Assume \(\dot{V} \le  \delta e^{T}e\), where \(\forall \delta > 0\), which means \(\dot{V} < 0\), therefore
According to Lemma 3, we could have transformed (36) into (37), it is equivalent to the following matrix inequalities:
where \(\gamma _{3} = L_{1}^{2}I + \lambda ^{  1}(1 + 4\tau )(P + \beta I) + \delta I + 2K(P + \beta I)\).
Also
This, by the Razumikhin stability theorem and Lemma 2, implies the asymptotic stability of the error system (24). To find the exponential factor of the solution, integrating both sides of the inequality, due to (39), \(\dot{V}(t,e(t)) \le 0\) and using the condition (26), we have
and hence
Here \(p = \Vert P \Vert \), this completes the proof of Theorem 2. □
Remark 6
Many researchers who studied the synchronous control of complex network with timevarying delay hypothesized that dynamic behaviors include nonlinear function. Some of them did not consider time delay in nonlinear dynamic behaviors [36] and some did [37]. Notably, the timevarying delay of systems (time delay in dynamic behavior and node coupling) was considered derivable in previous studies. This condition is eliminated in our Theorem 2, which relieves the requirements on time delay and thereby reduces the conservation of conclusions.
We turn to system (18). We consider the following Lyapunov function:
According to Theorem 2, it is easy to get the following conclusion. We have the following corollary.
Corollary 2
The complex network system (18) is exponentially synchronized when positive numbers δ, λ, \(L_{1}\) and a positive matrix P are present and the following inequality equation holds:
where \(\gamma _{4} = L_{1}^{2}I + \lambda ^{  1}(1 + 4\tau )P + \delta I + 2KP\).
Moreover, the error vector \(e(t,\phi )\) satisfies the condition
Here \(p = \Vert P \Vert \).
3.3 Numerical simulation
In this section, the exponential synchronization conditions obtained in this paper are illustrated with an example.
Consider a general complex dynamical network consisting of dynamical nodes with linear couplings system in Theorem 2. We have
and consider a complex network system with 10 nodes, each of which is a threedimensional linear system. Here
According to the LMI toolbox in Matlab, the parameters K and P can be obtained, and the initial conditions of the system are given, \(t_{0} = 0\), and the initial state \(x(0) = [2.62342,  5.74317,\ldots,2.62342,  2.74317,1.89187]^{T}\) is given at random. Figures 1, 2, and 3 are for the node 1, 2, 3 status curves without controller and Figs. 4, 5, and 6 are for the node 1, 2, 3 status curves with controller.
As can be seen from the figure, after a period of time, the system state is synchronous, and the feasibility and effectiveness of the control method are demonstrated.
4 Conclusions and discussions
This work focuses on the problem of exponential synchronization in complex network systems with timevarying delay. In the light of the Razumikhin stability theorem combined with the Newton–Leibniz formula, we deduced an exponential synchronization condition, without considering the differentiability of the timedelay function. Finally, a numerical simulation is given to show its effectiveness. The following will be considered in our future work: how to achieve synchronization through a network that is less strict and sufficient, and how to extend existing methods to the problem of finitetime synchronization or fixedtime synchronization. This is the goal we will consider and study in the future.
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Acknowledgements
The authors would like to thank X. Zou for her great help in many aspects.
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The datasets used or analyzed during the current study are available from the corresponding author on request.
Funding
This work was jointly supported by the National Natural Science Foundation of China (Grant No. 11372107), the Natural Science Foundation of Hunan Province (Grant No. 2017JJ5011) and the Natural Science Foundation of Hunan Province (Grant No. 2017JJ4004).
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Luo, Y., Ling, Z., Cheng, Z. et al. New results of exponential synchronization of complex network with timevarying delays. Adv Differ Equ 2019, 10 (2019). https://doi.org/10.1186/s1366201919471
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DOI: https://doi.org/10.1186/s1366201919471
Keywords
 Exponential synchronization
 Complex network
 Timevarying delay
 Razumikhin theorem