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Advances in Difference Equations

, 2019:337 | Cite as

Adaptive control of Mittag-Leffler stabilization and synchronization for delayed fractional-order BAM neural networks

  • Weike Cheng
  • Ailong WuEmail author
  • Jin-E Zhang
  • Biwen Li
Open Access
Research
  • 65 Downloads

Abstract

This paper is committed to studying adaptive control design of Mittag-Leffler stabilization and synchronization for delayed fractional-order bidirectional associative memory (BAM) neural networks. Considering better dynamic property and steady state performance of the system, we adopt adaptive control approaches to stabilize and synchronize two types of delayed fractional-order BAM neural network. It is a remarkable fact, based on adaptive control scheme, the method of auxiliary functions, Mittag-Leffler stabilization and synchronization theories with respect to fractional-order systems, the adaptive controllers are very well designed in a controlled system and two coupled systems, separately. Two examples are performed to illustrate the advantage of the presented theoretic analysis and results.

Keywords

Fractional-order systems BAM neural networks Time delays Mittag-Leffler stabilization and synchronization Adaptive control design 

1 Introduction

Recently, the rapid development of fractional calculus has shown that it is an attractive hot research topic, and fractional calculus has been used successfully in different scientific and technological fields [1, 2]. For all we know, the generalized form of ordinary integer-order calculus is said to be the fractional calculus, which originated in the 17th century [3], at that time, fractional calculus could not be well studied in light of the lack of comprehensive and systematic theoretical knowledge. Along with the depth of understanding of the fractional calculus, researchers found that fractional calculus can not only provide a mathematical modeling tool, but also describe the complex dynamic behavior that ordinary integer-order calculus cannot. Namely, a fractional-order system has more efficient and accurate capabilities than conventional integer-order system and is closer to the real-world cases. In many practical dynamic processes, a fractional-order system also has the advantage of many degrees of freedom and the ability of general computation. Additionally, the infinite memory characteristics of a fractional-order system, which can include the genetic information of the past, are displayed incisively and vividly. It is precisely because of these excellent performances that the application and research of fractional-order systems in many areas has developed well [4, 5]. However, a material fact worth noting is that a fractional-order system cannot directly use the control strategies of conventional integer-order system due to the complexity and particularity of the fractional-order system. As a consequence, how to choose effective tools and reasonable schemes to control a fractional-order system is worthy of consideration.

In 1987, Kosko first put forward bidirectional associative memory (BAM) neural networks with double layers [6], which revealed the intimate connection between the neurons arranged in the U-layer and the neurons arranged in the V-layer. In general, the neurons of the U-layer are fully integrated with the neurons of the V-layer, meanwhile the neurons of the U-layer and the V-layer have no interconnection. Because of this special performance of double-layer networks, their numerous applications have shown interest and importance in the areas of artificial intelligence, combinatorial optimization, signal processing, and image processing [7, 8]. In addition, as we all know, in the process of signal transmission between neurons on double-layer networks, some hereditary characteristics are embodied in intelligent information processing of the two layers. Based on this important discovery, it is very essential and significant that BAM neural networks are incorporated into infinite memory terms. From the point of view of fractional-order neurodynamic systems, unlike the locality of integer-order derivative, fractional-order derivative with singularity and nonlocality has infinite memory and hereditary characteristics of diverse processes with potential ability. Hence, the analysis and synthesis with respect to fractional-order BAM neural networks is worth looking into.

Whether it is electronic or biological network, there exists a general phenomenon called time delay [9]. In the transmission of signals between neurons, due to the finite speed of propagation and the limited switching speed on the amplifier, it is inevitable that the problem with time delays is always encountered. Particularly, for neural networks, there are many parallel paths with different length and size of the nodes, because complex networks have the features of time and space, single and coupled networks with time delays cannot be generalized. That is, the time delays of complex networks are not the same due to different distributions of propagation delays. According to the degree of correlation between time delay and time, time delay can be divided into constant delay [10] and time-varying delay [11]. Although there exists constant delay in some networks, time delay changes with time in general. For the time-varying delayed networks, the stability of networks is not only influenced, but even the dynamic behaviors that occur in networks may be complex and difficult to handle. In other words, the existence of time delays would lead to a destruction of the networks dynamics, it can be seen that time delays have an important influence on the dynamic characteristics of networks. So compared to the networks without time delays, it is significant and necessary to introduce the phenomenon of time delays with more abundant dynamic properties into neural networks. Up to now, all kinds of literature sources on delayed neural networks have attracted a lot of experimental and theoretical attention [12, 13]. However, significant results for time-varying delayed fractional-order systems are seldom reported. Thus, it is worthy to investigate a challenging problem regarding time delays in fractional-order systems.

Stabilization and synchronization are common and typical phenomena in the real world. Over the last few decades, stabilization and synchronization problems of complex control systems made an enormous difference in the domains of physics, engineering, and science [14, 15]. Just as its name implies, the meaning of stabilization is that a controlled system is stable by applying an external force. That is, given an uncontrolled system of arbitrary states, this uncontrolled system can reach a stable state mainly because the external controller applied to the controlled system plays a significant role. Unlike the stabilization of a single network, synchronization usually occurs in two or more networks. Theoretically, in order to realize synchronization, there must be some variable coupling between the systems, and as time goes by, the trajectories of coupled systems become increasingly consistent. In short, synchronization could be construed as the tracking of target trajectory. Among numerous synchronization phenomena, drive-response synchronization is the most common type of synchronization, which is widely used in various networks [16]. To sum up, it can be said that both stabilization and synchronization are an indispensable part of system dynamics. Particularly, in fractional-order systems, some attractive results regarding stabilization and synchronization phenomena have been introduced [17, 18]. From another point of view, talking about fractional-order systems, we know that Mittag-Leffler function is one of the important functions, and related properties of Mittag-Leffler are often studied [19]. However, Mittag-Leffler stabilization and synchronization are little investigated in double-layer systems. Considering this fact, it is worthwhile studying Mittag-Leffler stabilization and synchronization that can get some results of small gains.

For control theory, it is widely known that adaptive control design has become an explored area of mathematical studies, and adaptive control is often used in many practical applications in recent years due to the fact that adaptive control itself has better stable performance and higher tracking accuracy [20]. Generally speaking, adaptive control can be regarded as a feedback control that has the ability to change its performance characteristics in response to its environment, so that the system can work in the best condition according to predefined criteria. The difference from the classic feedback control is that adaptive control is based on less prior knowledge about the model. That is to say, adaptive control needs to extract the relevant information about the model constantly in the running process of the system, then the model will be gradually improved and more closer to the real situation. As far as we know, the parameters of the traditional feedback controller are fixed, when the internal properties and external disturbances of the system change a lot, the performance of the system can be degraded and even become unstable. The emergence of adaptive control effectively solves these problems, for example, adaptive control is applied to aircraft systems with high requirements, so good performance over a wide range of the altitudes and speeds of the airplane can be maintained. With the development of adaptive control, some novel results have been shown in the relevant literature [21, 22]. It should be noted that adaptive control is much more complicated than the classic feedback control, how to achieve the ultimate purpose of optimum control effect is a challenging task. As a consequence, constructing highly-efficient, explored and analyzed adaptive control is worth thinking about.

With the above discussion, we try to use adaptive control as a kind of better control scheme to explore Mittag-Leffler stabilization and synchronization on two types of delayed fractional-order BAM neural network. For purpose of the realization with Mittag-Leffler stabilization and synchronization in double-layer networks, the adaptive controllers with system and adjustable parameters are designed. Moreover, on the basis of essentially more general adaptive control conditions, the corresponding results on Mittag-Leffler stabilization and synchronization are obtained. Roughly stated, our main contributions of the paper are summed up into two points: (1) It is the first time that adaptive control design is applied to delayed fractional-order BAM neural networks. (2) Several Mittag-Leffler stabilization and synchronization criteria are first put forward in two types of delayed fractional-order BAM neural network on the basis of adaptive control scheme. There is no doubt that adaptive control strategy can be more targeted and efficient to improve the convergence character of fractional-order dynamics, and adaptive control scheme combined with Gronwall-like inequality with generalized type can be conveniently applied in a wider range of application areas. Actually, adaptive control approach only needs to set adjustable parameter values, so that it can be a powerful analysis tool for high-performance systems. Besides, adaptive control design of other fractional-order systems can be extended based on the obtained criteria. It is hoped that the theoretical analysis in this paper can provide the heuristic results regarding adaptive control scheme for fractional-order control theory.

This paper has the following four parts to constitute an overall analytical framework. In Sect. 2, the relevant preliminaries are stated from the three aspects, namely: fractional calculus, model description, definitions and properties. Several sufficient criteria are proposed to realize Mittag-Leffler stabilization and synchronization by adaptive control approaches in Sect. 3. Section 4 is utilized to give two examples to demonstrate the efficiency of our theoretic analysis. In the end, Sect. 5 summarizes the general conclusions.

2 Preliminaries

2.1 Fractional calculus

To facilitate the description of our model, two basic notions for fractional calculus are recalled.

The Caputo derivative of order \(q>0\) of a function \(\mathscr{H}(t) \in C^{n+1}([t_{0},+\infty ),\mathcal{R} )\) is characterized as
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \mathscr{H}(t)=\frac{1}{\varGamma (n-q)} \int ^{t} _{t_{0}}\frac{\mathscr{H}^{(n)}(s)}{(t-s)^{q-n+1}}\, \mathrm{d}s, \end{aligned}$$
where \(t \ge t_{0}\), n denotes a positive integer satisfying \(n-1 < q < n\), and \(\varGamma (\cdot )\) stands for the Gamma function.
Mittag-Leffler function \(E_{q}(\cdot )\) with one-parameter is given as
$$\begin{aligned} E_{q}(s)=\sum^{+\infty }_{k=0} \frac{s^{k}}{\varGamma (kq+1)}, \end{aligned}$$
where \(q>0\), s represents a complex number, and \(\varGamma (\cdot )\) stands for the Gamma function.

Remark 2.1

Fractional calculus occupies a very important position in control science and engineering. Particularly, the Caputo derivative has been the most frequently mentioned fractional-order operator for neurodynamic systems, mainly on account of the fact that the initial conditions with the Caputo derivative and the initial conditions with the integer-order derivative have much in common, and the Caputo derivative has more representations based on the descriptions of real-world situations.

Remark 2.2

It is worth noting that there are essential differences between the convergence property of traditional integer-order systems and that of fractional-order systems. For integer-order systems, we know that the exponential function can be utilized to deal with the dynamics problems. For fractional-order systems, the exponential function is no longer applicable because fractional-order systems possess abnormal and complex convergence behaviors. So the exponential function can be replaced by Mittag-Leffler function in fractional-order systems, which is a generally used function that can be widely applied to different types of factional-order system.

2.2 Model description

Throughout the paper, \(\mathcal{R}^{n}\) stands for the n-dimensional real space; given a real vector \(\alpha ={({\alpha _{1}},{\alpha _{2}} ,\ldots,{\alpha _{n}})}^{T}\in \mathcal{R}^{n}\), the norm is recorded as \(\Vert \alpha \Vert =\sum^{n}_{i=1}\vert \alpha _{i}\vert \).

We focus on the following delayed fractional-order BAM neural networks of the form
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t}x_{i}(t)=- \beta _{i}x_{i}(t)+\sum_{j=1}^{m}a_{ij}f _{j}\bigl(y_{j}(t)\bigr) +\sum _{j=1}^{m}b_{ij}f_{j} \bigl(y_{j}\bigl(t-\sigma _{j}(t)\bigr)\bigr)+p _{i}(t), \\ {}^{C}_{t_{0}}D^{q}_{t}y_{j}(t)=- \gamma _{j}y_{j}(t)+\sum_{i=1}^{n}c _{ji}g_{i}\bigl(x_{i}(t)\bigr) +\sum _{i=1}^{n}d_{ji}g_{i} \bigl(x_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr)+r _{j}(t), \end{gathered} \end{aligned}$$
(1)
where \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), \(0< q<1\), \(x_{i}(t)\) and \(y_{j}(t)\) mean the state variables, \(\beta _{i}>0\) and \(\gamma _{j}>0\) represent the self-inhibition, \(a_{ij}\), \(b_{ij}\), \(c_{ji}\) and \(d_{ji}\) stand for the synaptic strengths, \(p_{i}(t)\) and \(r_{j}(t)\) denote the external inputs, the time delays \(\sigma _{j}(t)\) and \(\theta _{i}(t)\) are continuous and bounded on \([0,+\infty )\), the output functions \(f_{j}(\cdot )\), \(g_{i}(\cdot )\) satisfy \(f_{j}(0)=0\), \(g_{i}(0)=0\) and \(\forall v,\bar{v}\in \mathcal{R}\),
$$\begin{aligned} & \bigl\vert f_{j}(v)-f_{j}(\bar{v}) \bigr\vert \le k_{j} \vert v-\bar{v} \vert , \end{aligned}$$
(2)
$$\begin{aligned} & \bigl\vert g_{i}(v)-g_{i}(\bar{v}) \bigr\vert \le h_{i} \vert v-\bar{v} \vert , \end{aligned}$$
(3)
in which \(k_{j}>0\), \(h_{i}>0\) (\(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\)).
The initial conditions regarding system (1) are described by
$$\begin{aligned} x_{i}(t_{0}+s)=\psi _{i}(s),\quad\quad y_{j}(t_{0}+s)=\varphi _{j}(s),\quad s\in [-\tau ,0], \end{aligned}$$
(4)
for \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), where \(\tau = \max_{1\le i\le n, 1\le j\le m}\{\sigma _{j}(t), \theta _{i}(t)\}\), real-valued functions \(\psi _{i}(s)\) and \(\varphi _{j}(s)\) defined on \([-\tau ,0]\) are continuous, and the corresponding norms are expressed as
$$\begin{aligned} \Vert \psi \Vert =\sum_{i=1}^{n} \sup_{s\in [-\tau ,0]}\bigl\{ \bigl\vert \psi _{i}(s) \bigr\vert \bigr\} , \quad\quad \Vert \varphi \Vert =\sum _{j=1}^{m}\sup_{s\in [-\tau ,0]}\bigl\{ \bigl\vert \varphi _{j}(s) \bigr\vert \bigr\} . \end{aligned}$$
(5)
For Mittag-Leffler synchronization, we focus on another type of system (1) as the drive system governed by
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t}x_{i}(t)=- \beta _{i}x_{i}(t)+\sum_{j=1}^{m}a_{ij}f _{j}\bigl(y_{j}(t)\bigr) +\sum _{j=1}^{m}b_{ij}f_{j} \bigl(y_{j}\bigl(t-\sigma _{j}(t)\bigr)\bigr), \\ {}^{C}_{t_{0}}D^{q}_{t}y_{j}(t)=- \gamma _{j}y_{j}(t)+\sum_{i=1}^{n}c _{ji}g_{i}\bigl(x_{i}(t)\bigr) +\sum _{i=1}^{n}d_{ji}g_{i} \bigl(x_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr), \end{gathered} \end{aligned}$$
(6)
in which \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), where the initial conditions of system (6) are the same as described for system (1).
We aim to design the following associated response system:
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t} \tilde{x}_{i}(t)=-\beta _{i}\tilde{x}_{i}(t)+ \sum_{j=1}^{m}a_{ij}f_{j} \bigl(\tilde{y}_{j}(t)\bigr) +\sum_{j=1}^{m}b_{ij}f _{j}\bigl(\tilde{y}_{j}\bigl(t-\sigma _{j}(t)\bigr)\bigr)+p_{i}(t), \\ {}^{C}_{t_{0}}D^{q}_{t} \tilde{y}_{j}(t)=-\gamma _{j}\tilde{y}_{j}(t)+ \sum_{i=1}^{n}c_{ji}g_{i} \bigl(\tilde{x}_{i}(t)\bigr) +\sum_{i=1}^{n}d_{ji}g _{i}\bigl(\tilde{x}_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr)+r_{j}(t), \end{gathered} \end{aligned}$$
(7)
in which \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), and \(p_{i}(t)\), \(r_{j}(t)\) signify the control inputs that need to be constructed appropriately.
The initial conditions for system (7) are given by
$$\begin{aligned} \tilde{x}_{i}(t_{0}+s)=\tilde{\psi }_{i}(s),\quad\quad \tilde{y}_{j}(t_{0}+s)= \tilde{\varphi }_{j}(s),\quad s\in [-\tau ,0], \end{aligned}$$
(8)
for \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), where \(\tau = \max_{1\le i\le n, 1\le j\le m}\{\sigma _{j}(t), \theta _{i}(t)\}\), real-valued functions \(\tilde{\psi }_{i}(s)\) and \(\tilde{\varphi } _{j}(s)\) defined on \([-\tau ,0]\) are continuous, and the corresponding norms are expressed as
$$\begin{aligned} \Vert \tilde{\psi } \Vert =\sum _{i=1}^{n}\sup_{s\in [-\tau ,0]}\bigl\{ \bigl\vert \tilde{\psi }_{i}(s) \bigr\vert \bigr\} ,\quad\quad \Vert \tilde{\varphi } \Vert =\sum_{j=1}^{m} \sup_{s\in [-\tau ,0]}\bigl\{ \bigl\vert \tilde{\varphi }_{j}(s) \bigr\vert \bigr\} . \end{aligned}$$
(9)
Let \(z_{i}(t)=\tilde{x}_{i}(t)-x_{i}(t)\) for \(i=1,2,\ldots,n\) and \(\tilde{z}_{j}(t)=\tilde{y}_{j}(t)-y_{j}(t)\) for \(j=1,2,\ldots,m\), then the error system between (6) and (7) is obtained by
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t}z_{i}(t)=- \beta _{i}z_{i}(t)+\sum_{j=1}^{m}a_{ij}f _{j}\bigl(\tilde{z}_{j}(t)\bigr) +\sum _{j=1}^{m}b_{ij}f_{j} \bigl(\tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr) \bigr)+p_{i}(t), \\ {}^{C}_{t_{0}}D^{q}_{t} \tilde{z}_{j}(t)=-\gamma _{j}\tilde{z}_{j}(t)+ \sum_{i=1}^{n}c_{ji}g_{i} \bigl(z_{i}(t)\bigr) +\sum_{i=1}^{n}d_{ji}g_{i} \bigl(z_{i}\bigl(t- \theta _{i}(t)\bigr) \bigr)+r_{j}(t), \end{gathered} \end{aligned}$$
(10)
where \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), \(f_{j}( \tilde{z}_{j}(t))=f_{j}(\tilde{y}_{j}(t))-f_{j}(y_{j}(t))\), \(g_{i}(z_{i}(t))=g_{i}(\tilde{x}_{i}(t))-g_{i}(x_{i}(t))\), and \(p_{i}(t)\), \(r_{j}(t)\) signify the control inputs that need to be constructed appropriately.
Naturally, the initial conditions for system (10) can be stated by
$$\begin{aligned} &z_{i}(t_{0}+s)=\tilde{\psi }_{i}(s)-\psi _{i}(s),\quad\quad \tilde{z}_{j}(t _{0}+s)=\tilde{\varphi }_{j}(s)-\varphi _{j}(s),\quad s\in [-\tau ,0], \end{aligned}$$
(11)
for \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), where \(\tau = \max_{1\le i\le n, 1\le j\le m}\{\sigma _{j}(t), \theta _{i}(t)\}\), real-valued functions \(\tilde{\psi }_{i}(s)-\psi _{i}(s)\) and \(\tilde{\varphi }_{j}(s)-\varphi _{j}(s)\) defined on \([-\tau ,0]\) are continuous, and the corresponding norms are expressed as
$$\begin{aligned} \begin{gathered} \Vert \tilde{\psi }-\psi \Vert =\sum_{i=1}^{n}\sup_{s\in [-\tau ,0]} \bigl\{ \bigl\vert \tilde{\psi }_{i}(s)-\psi _{i}(s) \bigr\vert \bigr\} , \\ \Vert \tilde{\varphi }-\varphi \Vert =\sum_{j=1}^{m} \sup_{s\in [-\tau ,0]}\bigl\{ \bigl\vert \tilde{\varphi }_{j}(s)-\varphi _{j}(s) \bigr\vert \bigr\} . \end{gathered} \end{aligned}$$
(12)

Remark 2.3

In the process of our model description, we adopt drive–response systems (6) and (7) to realize Mittag-Leffler synchronization. The drive system (6) can be called a master system, which is uncontrolled due to lack of control inputs. The response system (7) is also said to be a slave system, which possesses control inputs. In theory, after a long enough period of time, the error system (10) can realize Mittag-Leffler stability based on some appropriate feedback control design, so the coupled systems (6) and (7) are referred to be Mittag-Leffler synchronized.

2.3 Definitions and properties

In this subsection, in order to better analyze the problems of Mittag-Leffler dynamics, some important definitions about Mittag-Leffler dynamics and several relevant lemmas are provided, which are utilized for our theoretical results later.

Definition 2.1

For any \(\eta >0\), if there exist \(T>0\), \(\mathscr{M}(\eta )>0\) and \(\delta >0\) satisfying for any \(t\ge t_{0}+T\),
$$\begin{aligned} \bigl\Vert x(t) \bigr\Vert + \bigl\Vert y(t) \bigr\Vert \le \mathscr{M}( \eta )E_{q}\bigl(-\delta (t-t_{0})^{q}\bigr), \end{aligned}$$
when \(\Vert \psi \Vert +\Vert \varphi \Vert \le \eta \), then the zero solution of system (1) is called Mittag-Leffler stabilizable, where \(p_{i}(t)=0\), \(r_{j}(t)=0\) (\(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\)).

Remark 2.4

What needs to be pointed out is that the original reference in Definition 2.1 is from the definition of Mittag-Leffler synchronization for fractional-order single-layer networks, which has been given in [2, Definition 4.2]. In view of the structural property of double-layer networks and the connection between stability and synchronization, it is not a difficult to see that the definition of Mittag-Leffler dynamics on single-layer networks is extended to double-layer networks, so there is no doubt that Definition 2.1 can be obtained.

Remark 2.5

From Definition 2.1, we can learn that the sum of two final values will converge to zero after a fixed amount of time, that is, the system can realize ultimate Mittag-Leffler stability as time t goes to infinity. In addition, δ is also said to be the degree of Mittag-Leffler stability.

Definition 2.2

If the controlled system of (1) realizes Mittag-Leffler stability based on some appropriate feedback control design, then system (1) is called Mittag-Leffler stabilizable.

Definition 2.3

If the error dynamics system (10) realizes Mittag-Leffler stability, then the drive system (6) and the response system (7) are called Mittag-Leffler synchronizable.

Remark 2.6

It is easy to see that the definitions with respect to Mittag-Leffler stabilization and synchronization are based on the stability definition of Mittag-Leffler. And it is also important to notice that Mittag-Leffler dynamics involves asymptotic behavior due to the properties of Mittag-Leffler function, namely, Mittag-Leffler stability means asymptotic stability, the same goes for Mittag-Leffler stabilization and Mittag-Leffler synchronization.

Lemma 2.1

([1])

Let\(0< q<1\)be given. If\(\mathscr{H}(t)\in {C}^{1}[t_{0},+\infty )\), then
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl\vert \mathscr{H}(t) \bigr\vert \le \operatorname{sgn}\bigl(\mathscr{H}(t)\bigr) {}^{C}_{t_{0}}D^{q}_{t} \mathscr{H}(t), \end{aligned}$$
for\(t\ge t_{0}\), where
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl\vert \mathscr{H}(t) \bigr\vert =\frac{1}{\varGamma (1-q)} \int _{t _{0}}^{t} \frac{\frac{\mathrm{d}}{\mathrm{d}s} \vert \mathscr{H}(s) \vert }{(t-s)^{q}} \, \mathrm{d}s. \end{aligned}$$

Remark 2.7

Taking into account the complexity of Caputo derivative of the absolute value function in fractional calculus, Lemma 2.1 gives the connection between the Caputo derivative of function \(\vert \mathscr{H}(t)\vert \) and Caputo derivative of function \(\mathscr{H}(t)\), which provides a convenient approach for fractional calculation.

Lemma 2.2

([2])

If\(\mathscr{W}(t)\)and\(\mathscr{U}(t)\)are two continuous nonnegative functions satisfying
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t}\bigl( \mathscr{W}(t)+\mathscr{U}(t)\bigr)\le -\delta \mathscr{W}(t), \end{aligned}$$
where\(0< q<1\), \(\delta >0\), then there exists a constant\(T>0\)such that
$$\begin{aligned} \mathscr{W}(t)\le \bigl(\mathscr{W}(t_{0})+\mathscr{U}(t_{0})+ \ell \bigr)E_{q}\bigl(- \delta (t-t_{0})^{q} \bigr), \end{aligned}$$
for any positive constant, where\(t\ge t_{0}+T\).

Remark 2.8

In order to ensure that Mittag-Leffler stabilization and synchronization can be realized, Lemma 2.2 offers the convergence property regarding Gronwall-like inequality of generalized type, which can deal with the problems of convergence very well in many types of fractional-order systems, and it can be utilized to establish a criterion with respect to fractional-order dynamics. Moreover, more relevant details about Lemma 2.2 can be found in [2, Lemma 4.3].

3 Main results

After a detailed introduction and explanation, in this section, we present adaptive control strategies, which can be used to realize Mittag-Leffler stabilization and synchronization in the corresponding systems.

For the sake of narrative, the adaptive control schemes are first used to deal with Mittag-Leffler stabilization and synchronization problems in double-layer networks, and then the theoretical results are reviewed and analyzed.

3.1 Mittag-Leffler stabilization

Theorem 3.1

Suppose positive constants\(\mu _{i}\), \(\breve{\mu }_{i}\), \(\xi _{j}\), \(\breve{\xi }_{j}\)are arbitrary. If system (1) is controlled based on the following adaptive control scheme:
$$ \textstyle\begin{cases} p_{i}(t)=-w_{i}(t)x_{i}(t-\theta _{i}(t))-\breve{w}_{i}(t)x_{i}(t), \\ r_{j}(t)=-u_{j}(t)y_{j}(t-\sigma _{j}(t))-\breve{u}_{j}(t)y_{j}(t), \\ {}^{C}_{t_{0}}D^{q}_{t}w_{i}(t)=\mu _{i} \vert x_{i}(t-\theta _{i}(t)) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}u_{j}(t)=\xi _{j} \vert y_{j}(t-\sigma _{j}(t)) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}\breve{w}_{i}(t)=\breve{\mu }_{i} \vert x_{i}(t) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}\breve{u}_{j}(t)=\breve{\xi }_{j} \vert y_{j}(t) \vert , \end{cases} $$
(13)
in which\(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), then Mittag-Leffler stabilization can be realized for system (1).

Proof

Under the controller (13), the controlled system (1) is rewritten as
$$\begin{aligned} \begin{gathered} \begin{aligned} {}^{C}_{t_{0}}D^{q}_{t}x_{i}(t) &=-\beta _{i}x_{i}(t)+\sum _{j=1}^{m}a_{ij}f _{j} \bigl(y_{j}(t)\bigr) +\sum_{j=1}^{m}b_{ij}f_{j} \bigl(y_{j}\bigl(t-\sigma _{j}(t)\bigr)\bigr) \\ &\quad {} -w_{i}(t)x_{i}\bigl(t-\theta _{i}(t)\bigr)-\breve{w}_{i}(t)x_{i}(t), \end{aligned} \\ \begin{aligned} {}^{C}_{t_{0}}D^{q}_{t}y_{j}(t) &=-\gamma _{j}y_{j}(t)+\sum _{i=1}^{n}c _{ji}g_{i} \bigl(x_{i}(t)\bigr) +\sum_{i=1}^{n}d_{ji}g_{i} \bigl(x_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr) \\ &\quad {} -u_{j}(t)y_{j}\bigl(t-\sigma _{j}(t)\bigr)-\breve{u}_{j}(t)y_{j}(t), \end{aligned}\end{gathered} \end{aligned}$$
(14)
where \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\).
We construct an auxiliary function
$$\begin{aligned} W(t)=\sum_{i=1}^{n} \bigl\vert x_{i}(t) \bigr\vert +\sum _{j=1}^{m} \bigl\vert y_{j}(t) \bigr\vert . \end{aligned}$$
(15)
Through Lemma 2.1, by (14) we can derive
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} W(t) &\le \sum_{i=1}^{n} \operatorname{sgn} \bigl(x_{i}(t)\bigr){}^{C} _{t_{0}}D^{q}_{t} x_{i}(t)+\sum_{j=1}^{m} \operatorname{sgn}\bigl(y_{j}(t)\bigr){}^{C} _{t_{0}}D^{q}_{t} y_{j}(t) \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert x_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert a_{ij} \vert \bigl\vert f _{j}\bigl(y_{j}(t)\bigr) \bigr\vert + \sum_{j=1}^{m} \vert b_{ij} \vert \bigl\vert f_{j}\bigl(y_{j} \bigl(t-\sigma _{j}(t)\bigr)\bigr) \bigr\vert \\ &\quad {} -w_{i}(t) \bigl\vert x_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert -\breve{w}_{i}(t) \bigl\vert x_{i}(t) \bigr\vert \Biggr]+\sum _{j=1}^{m} \Biggl[-\gamma _{j} \bigl\vert y_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert c_{ji} \vert \bigl\vert g_{i}\bigl(x_{i}(t) \bigr) \bigr\vert +\sum_{i=1}^{n} \vert d_{ji} \vert \bigl\vert g _{i} \bigl(x_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr) \bigr\vert \\ &\quad {} -u_{j}(t) \bigl\vert y_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -\breve{u}_{j}(t) \bigl\vert y_{j}(t) \bigr\vert \Biggr] \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert x_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert a_{ij} \vert k _{j} \bigl\vert y_{j}(t) \bigr\vert +\sum _{j=1}^{m} \vert b_{ij} \vert k_{j} \bigl\vert y_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert \\ &\quad {} -w_{i}(t) \bigl\vert x_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert -\breve{w}_{i}(t) \bigl\vert x_{i}(t) \bigr\vert \Biggr]+\sum _{j=1}^{m} \Biggl[-\gamma _{j} \bigl\vert y_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert c_{ji} \vert h_{i} \bigl\vert x_{i}(t) \bigr\vert +\sum_{i=1}^{n} \vert d_{ji} \vert h _{i} \bigl\vert x_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert \\ &\quad {} -u_{j}(t) \bigl\vert y_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -\breve{u}_{j}(t) \bigl\vert y_{j}(t) \bigr\vert \Biggr] \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert x_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert c_{ji} \vert h _{i} \bigl\vert x_{i}(t) \bigr\vert - \breve{w}_{i}(t) \bigl\vert x_{i}(t) \bigr\vert \\ &\quad {} +\sum_{j=1}^{m} \vert d_{ji} \vert h_{i} \bigl\vert x_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert -w_{i}(t) \bigl\vert x _{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert \Biggr] \\ &\quad {} +\sum_{j=1}^{m} \Biggl[- \gamma _{j} \bigl\vert y_{j}(t) \bigr\vert +\sum _{i=1}^{n} \vert a _{ij} \vert k_{j} \bigl\vert y_{j}(t) \bigr\vert - \breve{u}_{j}(t) \bigl\vert y_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert b_{ij} \vert k_{j} \bigl\vert y_{j} \bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -u_{j}(t) \bigl\vert y _{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert \Biggr]. \end{aligned}$$
(16)
In the following, consider another auxiliary function
$$\begin{aligned} U(t) &=\sum_{i=1}^{n} \biggl[ \frac{1}{2\mu _{i}}\bigl(w_{i}(t)-w_{i}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\mu }_{i}} \bigl(\breve{w}_{i}(t)- \breve{w}_{i} ^{\vartriangle }\bigr)^{2} \biggr] \\ &\quad {} +\sum_{j=1}^{m} \biggl[ \frac{1}{2\xi _{j}}\bigl(u_{j}(t)-u_{j}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\xi }_{j}} \bigl(\breve{u}_{j}(t)- \breve{u}_{j} ^{\vartriangle }\bigr)^{2} \biggr]. \end{aligned}$$
(17)
By (16) and (17), it holds
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl(W(t)+U(t)\bigr) &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert x _{i}(t) \bigr\vert +\sum_{j=1}^{m} \vert c_{ji} \vert h_{i} \bigl\vert x_{i}(t) \bigr\vert -\breve{w}_{i}^{\vartriangle } \bigl\vert x_{i}(t) \bigr\vert \\ &\quad {} +\sum_{j=1}^{m} \vert d_{ji} \vert h_{i} \bigl\vert x_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert -w_{i}^{ \vartriangle } \bigl\vert x_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert \Biggr] \\ &\quad {} +\sum_{j=1}^{m} \Biggl[- \gamma _{j} \bigl\vert y_{j}(t) \bigr\vert +\sum _{i=1}^{n} \vert a _{ij} \vert k_{j} \bigl\vert y_{j}(t) \bigr\vert - \breve{u}_{j}^{\vartriangle } \bigl\vert y_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert b_{ij} \vert k_{j} \bigl\vert y_{j} \bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -u_{j}^{ \vartriangle } \bigl\vert y_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert \Biggr]. \end{aligned}$$
(18)
Selecting \(\breve{w}_{i}^{\vartriangle }\), \(w_{i}^{\vartriangle }\), \(\breve{u}_{j}^{\vartriangle }\) and \(u_{j}^{\vartriangle }\) large enough to satisfy
$$ \textstyle\begin{cases} \breve{w}_{i}^{\vartriangle }\ge -\beta _{i}+\sum_{j=1}^{m} \vert c_{ji} \vert h _{i}+\delta _{1}, \\ \breve{u}_{j}^{\vartriangle }\ge -\gamma _{j}+\sum_{i=1}^{n} \vert a_{ij} \vert k _{j}+\delta _{2}, \\ w_{i}^{\vartriangle }\ge \sum_{j=1}^{m} \vert d_{ji} \vert h_{i}, \\ u_{j}^{\vartriangle }\ge \sum_{i=1}^{n} \vert b_{ij} \vert k_{j}, \end{cases} $$
(19)
where \(\delta _{1}\) and \(\delta _{2}\) are positive constants, we get
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl(W(t)+U(t)\bigr) &\le -\delta W(t), \end{aligned}$$
(20)
where \(\delta =\min \{\delta _{1},\delta _{2}\}\).
According to Lemma 2.2, it follows from (20) that for any positive constant there exists \(T\ge 0\) such that
$$\begin{aligned} \bigl\Vert x(t) \bigr\Vert + \bigl\Vert y(t) \bigr\Vert &\le \bigl(W(t_{0})+U(t_{0})+\ell \bigr)E_{q} \bigl(-\delta (t-t_{0})^{q}\bigr) \\ &\le M(\eta )E_{q}\bigl(-\delta (t-t_{0})^{q} \bigr), \end{aligned}$$
for any \(t\ge t_{0}+T\), when \(\Vert \psi \Vert +\Vert \varphi \Vert \le \eta \), where
$$\begin{aligned} M(\eta ) &=\eta +\ell +\sum_{i=1}^{n} \biggl[\frac{1}{2\mu _{i}}\bigl(w_{i}(t _{0})-w_{i}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\mu }_{i}} \bigl( \breve{w}_{i}(t_{0})- \breve{w}_{i}^{\vartriangle }\bigr)^{2} \biggr] \\ &\quad {} +\sum_{j=1}^{m} \biggl[ \frac{1}{2\xi _{j}}\bigl(u_{j}(t_{0})-u_{j}^{ \vartriangle } \bigr)^{2}+\frac{1}{2\breve{\xi }_{j}} \bigl(\breve{u}_{j}(t_{0})- \breve{u}_{j}^{\vartriangle }\bigr)^{2} \biggr]. \end{aligned}$$

Hence, under the adaptive controller (13), it can be claimed that system (1) realizes Mittag-Leffler stabilization. □

3.2 Mittag-Leffler synchronization

Theorem 3.2

Suppose positive constants\(\mu _{i}\), \(\breve{\mu }_{i}\), \(\xi _{j}\), \(\breve{\xi }_{j}\)are arbitrary. If the response system (7) is controlled based on the following adaptive control scheme:
$$ \textstyle\begin{cases} p_{i}(t)=-w_{i}(t)z_{i}(t-\theta _{i}(t))-\breve{w}_{i}(t)z_{i}(t), \\ r_{j}(t)=-u_{j}(t)\tilde{z}_{j}(t-\sigma _{j}(t))-\breve{u}_{j}(t) \tilde{z}_{j}(t), \\ {}^{C}_{t_{0}}D^{q}_{t}w_{i}(t)=\mu _{i} \vert z_{i}(t-\theta _{i}(t)) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}u_{j}(t)=\xi _{j} \vert \tilde{z}_{j}(t-\sigma _{j}(t)) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}\breve{w}_{i}(t)=\breve{\mu }_{i} \vert z_{i}(t) \vert , \\ {}^{C}_{t_{0}}D^{q}_{t}\breve{u}_{j}(t)=\breve{\xi }_{j} \vert \tilde{z}_{j}(t) \vert , \end{cases} $$
(21)
in which\(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\), then Mittag-Leffler synchronization can be realized for the drive system (6) and response system (7).

Proof

By the controller (21), the error system (10) is rewritten as
$$\begin{aligned} \begin{gathered}\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t}z_{i}(t) &=-\beta _{i}z_{i}(t)+\sum _{j=1}^{m}a_{ij}f _{j} \bigl(\tilde{z}_{j}(t)\bigr) +\sum_{j=1}^{m}b_{ij}f_{j} \bigl(\tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr)\bigr) \\ &\quad {} -w_{i}(t)z_{i}\bigl(t-\theta _{i}(t)\bigr)-\breve{w}_{i}(t)z_{i}(t), \end{aligned} \\ \begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \tilde{z}_{j}(t) &=-\gamma _{j}\tilde{z}_{j}(t)+ \sum_{i=1}^{n}c_{ji}g_{i} \bigl(z_{i}(t)\bigr) +\sum_{i=1}^{n}d_{ji}g_{i} \bigl(z_{i}\bigl(t- \theta _{i}(t)\bigr)\bigr) \\ &\quad {} -u_{j}(t)\tilde{z}_{j}\bigl(t-\sigma _{j}(t)\bigr)-\breve{u}_{j}(t) \tilde{z}_{j}(t), \end{aligned} \end{gathered} \end{aligned}$$
(22)
where \(t\ge t_{0}\), \(i=1,2,\ldots,n\), \(j=1,2,\ldots,m\).
We design an auxiliary function
$$\begin{aligned} W(t)=\sum_{i=1}^{n} \bigl\vert z_{i}(t) \bigr\vert +\sum _{j=1}^{m} \bigl\vert \tilde{z}_{j}(t) \bigr\vert . \end{aligned}$$
(23)
Through Lemma 2.1, by (23) we can derive
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} W(t) &\le \sum_{i=1}^{n} \operatorname{sgn} \bigl(z_{i}(t)\bigr){}^{C} _{t_{0}}D^{q}_{t} z_{i}(t)+\sum_{j=1}^{m} \operatorname{sgn}\bigl(\tilde{z}_{j}(t)\bigr){}^{C} _{t_{0}}D^{q}_{t} \tilde{z}_{j}(t) \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert z_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert a_{ij} \vert \bigl\vert f _{j}\bigl(\tilde{z}_{j}(t)\bigr) \bigr\vert +\sum_{j=1}^{m} \vert b_{ij} \vert \bigl\vert f_{j}\bigl( \tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr)\bigr) \bigr\vert \\ &\quad {} -w_{i}(t) \bigl\vert z_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert -\breve{w}_{i}(t) \bigl\vert z_{i}(t) \bigr\vert \Biggr]+\sum _{j=1}^{m} \Biggl[-\gamma _{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert c_{ji} \vert \bigl\vert g_{i}\bigl(z_{i}(t) \bigr) \bigr\vert +\sum_{i=1}^{n} \vert d_{ji} \vert \bigl\vert g _{i} \bigl(z_{i}\bigl(t-\theta _{i}(t)\bigr)\bigr) \bigr\vert \\ &\quad {} -u_{j}(t) \bigl\vert \tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr) \bigr\vert -\breve{u}_{j}(t) \bigl\vert \tilde{z}_{j}(t) \bigr\vert \Biggr] \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert z_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert a_{ij} \vert k _{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert +\sum _{j=1}^{m} \vert b_{ij} \vert k_{j} \bigl\vert \tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr) \bigr\vert \\ &\quad {} -w_{i}(t) \bigl\vert z_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert -\breve{w}_{i}(t) \bigl\vert z_{i}(t) \bigr\vert \Biggr]+\sum _{j=1}^{m} \Biggl[-\gamma _{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert c_{ji} \vert h_{i} \bigl\vert z_{i}(t) \bigr\vert +\sum_{i=1}^{n} \vert d_{ji} \vert h _{i} \bigl\vert z_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert \\ &\quad {} -u_{j}(t) \bigl\vert \tilde{z}_{j}\bigl(t- \sigma _{j}(t)\bigr) \bigr\vert -\breve{u}_{j}(t) \bigl\vert \tilde{z}_{j}(t) \bigr\vert \Biggr] \\ &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert z_{i}(t) \bigr\vert +\sum _{j=1}^{m} \vert c_{ji} \vert h _{i} \bigl\vert z_{i}(t) \bigr\vert - \breve{w}_{i}(t) \bigl\vert z_{i}(t) \bigr\vert \\ &\quad {} +\sum_{j=1}^{m} \vert d_{ji} \vert h_{i} \bigl\vert z_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert -w_{i}(t) \bigl\vert z _{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert \Biggr] \\ &\quad {} +\sum_{j=1}^{m} \Biggl[- \gamma _{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert + \sum_{i=1} ^{n} \vert a_{ij} \vert k_{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert -\breve{u}_{j}(t) \bigl\vert \tilde{z}_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert b_{ij} \vert k_{j} \bigl\vert \tilde{z}_{j} \bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -u _{j}(t) \bigl\vert \tilde{z}_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert \Biggr]. \end{aligned}$$
(24)
In the following, consider another auxiliary function
$$\begin{aligned} U(t) &=\sum_{i=1}^{n} \biggl[ \frac{1}{2\mu _{i}}\bigl(w_{i}(t)-w_{i}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\mu }_{i}} \bigl(\breve{w}_{i}(t)- \breve{w}_{i} ^{\vartriangle }\bigr)^{2} \biggr] \\ &\quad {} +\sum_{j=1}^{m} \biggl[ \frac{1}{2\xi _{j}}\bigl(u_{j}(t)-u_{j}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\xi }_{j}} \bigl(\breve{u}_{j}(t)- \breve{u}_{j} ^{\vartriangle }\bigr)^{2} \biggr]. \end{aligned}$$
(25)
By (24) and (25), it holds
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl(W(t)+U(t)\bigr) &\le \sum_{i=1}^{n} \Biggl[-\beta _{i} \bigl\vert z _{i}(t) \bigr\vert +\sum_{j=1}^{m} \vert c_{ji} \vert h_{i} \bigl\vert z_{i}(t) \bigr\vert -\breve{w}_{i}^{\vartriangle } \bigl\vert z_{i}(t) \bigr\vert \\ &\quad {} +\sum_{j=1}^{m} \vert d_{ji} \vert h_{i} \bigl\vert z_{i} \bigl(t-\theta _{i}(t)\bigr) \bigr\vert -w_{i}^{ \vartriangle } \bigl\vert z_{i}\bigl(t-\theta _{i}(t)\bigr) \bigr\vert \Biggr] \\ &\quad {} +\sum_{j=1}^{m} \Biggl[- \gamma _{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert + \sum_{i=1} ^{n} \vert a_{ij} \vert k_{j} \bigl\vert \tilde{z}_{j}(t) \bigr\vert -\breve{u}_{j}^{\vartriangle } \bigl\vert \tilde{z}_{j}(t) \bigr\vert \\ &\quad {} +\sum_{i=1}^{n} \vert b_{ij} \vert k_{j} \bigl\vert \tilde{z}_{j} \bigl(t-\sigma _{j}(t)\bigr) \bigr\vert -u _{j}^{\vartriangle } \bigl\vert \tilde{z}_{j}\bigl(t-\sigma _{j}(t)\bigr) \bigr\vert \Biggr]. \end{aligned}$$
(26)
Selecting \(\breve{w}_{i}^{\vartriangle }\), \(w_{i}^{\vartriangle }\), \(\breve{u}_{j}^{\vartriangle }\) and \(u_{j}^{\vartriangle }\) large enough to satisfy
$$\begin{aligned}& \textstyle\begin{cases} \breve{w}_{i}^{\vartriangle }\ge -\beta _{i}+\sum_{j=1}^{m} \vert c_{ji} \vert h _{i}+\delta _{1}, \\ \breve{u}_{j}^{\vartriangle }\ge -\gamma _{j}+\sum_{i=1}^{n} \vert a_{ij} \vert k _{j}+\delta _{2}, \\ w_{i}^{\vartriangle }\ge \sum_{j=1}^{m} \vert d_{ji} \vert h_{i}, \\ u_{j}^{\vartriangle }\ge \sum_{i=1}^{n} \vert b_{ij} \vert k_{j}, \end{cases}\displaystyle \end{aligned}$$
(27)
where \(\delta _{1}\) and \(\delta _{2}\) are positive constants, we get
$$\begin{aligned} {}^{C}_{t_{0}}D^{q}_{t} \bigl(W(t)+U(t)\bigr) &\le -\delta W(t), \end{aligned}$$
(28)
where \(\delta =\min \{\delta _{1},\delta _{2}\}\).
According to Lemma 2.2, it follows from (28) that for any positive constant there exists \(T\ge 0\) such that
$$\begin{aligned} \bigl\Vert z(t) \bigr\Vert + \bigl\Vert \tilde{z}(t) \bigr\Vert &\le \bigl(W(t_{0})+U(t_{0})+\ell \bigr)E_{q} \bigl(-\delta (t-t_{0})^{q}\bigr) \\ &\le M(\eta )E_{q}\bigl(-\delta (t-t_{0})^{q} \bigr), \end{aligned}$$
for any \(t\ge t_{0}+T\), when \(\Vert \tilde{\psi }-\psi \Vert +\Vert \tilde{\varphi }-\varphi \Vert \le \eta \), where
$$\begin{aligned} M(\eta ) &=\eta +\ell +\sum_{i=1}^{n} \biggl[\frac{1}{2\mu _{i}}\bigl(w_{i}(t _{0})-w_{i}^{\vartriangle } \bigr)^{2}+\frac{1}{2\breve{\mu }_{i}} \bigl( \breve{w}_{i}(t_{0})- \breve{w}_{i}^{\vartriangle }\bigr)^{2} \biggr] \\ &\quad {} +\sum_{j=1}^{m} \biggl[ \frac{1}{2\xi _{j}}\bigl(u_{j}(t_{0})-u_{j}^{ \vartriangle } \bigr)^{2}+\frac{1}{2\breve{\xi }_{j}} \bigl(\breve{u}_{j}(t_{0})- \breve{u}_{j}^{\vartriangle }\bigr)^{2} \biggr]. \end{aligned}$$

Hence, under the adaptive controller (21), it can be claimed that the drive system (6) and response system (7) realize Mittag-Leffler synchronization. □

Remark 3.1

As we have seen, the auxiliary functions (15), (17), (23), and (25) are actually Lyapunov-like functions. Taking auxiliary functions (15) and (23) for example, this form of auxiliary functions are chosen because they make full use of the properties of two variables in BAM networks, so it is natural to go back to the considered systems (1) and (10). Additionally, the construction of auxiliary functions (17) and (25) is very ingenious, it is easy to find that “2” in the denominator and “2” in the index just cancel each other out when taking the derivatives of auxiliary functions (17) and (25), the results are not affected and the calculation is much simper.

Remark 3.2

In the course of our derivation, a Caputo fractional-order derivative can be calculated in two ways for the auxiliary function \(W(t)\) in (15). The first method is to use the definition of Caputo fractional-order derivative directly, and then Lemma 2.1 is utilized to simplify results. The second method is that auxiliary function \(W(t)\) can be treated as two functions, and then Lemma 2.1 is utilized for each function. No matter which approach, the Caputo fractional-order derivative of \(W(t)\) can be shown to satisfy \({}^{C}_{t_{0}}D^{q}_{t} W(t)\le \sum_{i=1}^{n} \operatorname{sgn}(x_{i}(t)){}^{C} _{t_{0}}D^{q}_{t} x_{i}(t)+\sum_{j=1}^{m} \operatorname{sgn}(y_{j}(t)){}^{C} _{t_{0}}D^{q}_{t} y_{j}(t)\). Similarly, these two methods are used to calculate the Caputo fractional-order derivative for the auxiliary function \(W(t)\) in (23).

Remark 3.3

As introduced in Theorems 3.1 and 3.2, it is shown that there are similarities and differences in the analysis of Mittag-Leffler stabilization and synchronization. For the method of auxiliary functions, we can find that the auxiliary functions constructed with respect to Mittag-Leffler stabilization or synchronization are similar. In addition, for Mittag-Leffler stabilization, system (1) itself is controlled based on a suitable adaptive controller, and the realization of stabilization for system (1) implies that system (14) must realize Mittag-Leffler stability. For Mittag-Leffler synchronization, the response system (7) is controlled based on a suitable adaptive controller, and the realization of synchronization for the drive–response systems (6) and (7) implies that the error system (22) must realize Mittag-Leffler stability.

Remark 3.4

It is clear that the adaptive control schemes are very effective for dealing with Mittag-Leffler dynamics problems of fractional-order systems in Theorems 3.1 and 3.2. There is no doubt that the key-point of the proposed control method is the application of a family of fractional-order nonlinear systems. Through the transformation of auxiliary functions, the function terms of the adaptive control design are eliminated, and then the results of Mittag-Leffler dynamics can be obtained by using Lemma 2.2. In fact, Lemma 2.2 becomes the principal ingredient in the proof process which brings together the adaptive control and Mittag-Leffler dynamics. That is, if there exists a lemma which can find a bridge between the adaptive control and other dynamics in fractional-order systems, then the results regarding other dynamics can be derived. It follows that the main idea of the designed adaptive control can be used widely due to the flexibility. Hence, there is generality in this adaptive control approach for fractional-order systems.

Remark 3.5

What is noteworthy is that the change of adaptive control gains \(\mu _{i}\), \(\breve{\mu }_{i}\), \(\xi _{j}\), \(\breve{\xi } _{j}\) will affect the change of control inputs under adaptive control strategies (13) and (21), and meanwhile, the stabilization and synchronization speeds will also change accordingly. Hence, when adaptive control strategy is utilized for fractional-order dynamics, the adaptive control gains \(\mu _{i}\), \(\breve{\mu }_{i}\), \(\xi _{j}\), \(\breve{\xi }_{j}\) can be selected according to the requirements of designer, such as appropriate control inputs and fast convergence speed.

Remark 3.6

In the contemporary literature, from the perspective of the control design, there are many new results about the network control systems; for example, see [23, 24]. However, in fractional-order systems, the adaptive control strategy based on double-layer networks has not been studied, yet; so Theorems 3.1 and 3.2 are new. Comparing with similar findings in [2], the obtained results in this paper generalize the cases on single-layer networks and add a meaningful criterion regarding Mittag-Leffler stabilization, which reveals the differences and connections between Mittag-Leffler stabilization and synchronization and has certain representativeness.

Remark 3.7

Looking through the whole process of analysis, there is no doubt that the prominent role of design schemes with respect to adaptive controllers cannot be ignored. Besides, according to the characteristics of adjustable parameters, adaptive control is more advantageous for complex systems, such as the controlled system with unknown features or large disturbances. Namely, it is an interesting issue that adaptive control is applied to more systems in future studies.

4 Illustrative examples

In this section, for the purpose of substantiating the validity of the above theoretical criteria, two numerical examples are put forward through computer simulation.

Example 4.1

We focus on a class of delayed fractional-order BAM neural networks
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t}x(t)=-0.11x(t)+0.15f \bigl(y(t)\bigr) +0.12f\bigl(y\bigl(t-\sigma (t)\bigr)\bigr)+p(t), \\ {}^{C}_{t_{0}}D^{q}_{t}y(t)=-0.13y(t)-0.14g \bigl(x(t)\bigr) -0.16g\bigl(x\bigl(t-\theta (t)\bigr)\bigr)+r(t), \end{gathered} \end{aligned}$$
(29)
where \(t\ge 0\), \(q=0.96\), \(f(\cdot )=g(\cdot )= \tanh (\cdot )\), \(\sigma (t)=1\), \(\theta (t)=0.9\), then \(\tau =1\).
Under system (29) without adaptive controller, the time response curves of system (29) are depicted in Fig. 1, which shows that state trajectories cannot convergence to the origin.
Figure 1

Time response curves of system (29) without adaptive controller

Taking \(\mu =0.01\), \(\breve{\mu }=0.01\), \(\xi =0.01\), \(\breve{\xi }=0.01\) and setting initial values as \(w(0)=0.1\), \(\breve{w}(0)=0.1\), \(u(0)=0.25\), \(\breve{u}(0)=0.05\), the time evolution of stabilization curves of system (29) with initial conditions \(x(s)=1\), \(y(s)=-2\) for \(s\in [-1,0]\) is portrayed in Fig. 2. The adaptive control gains \(w(t)\), \(\breve{w}(t)\), \(u(t)\), \(\breve{u}(t)\) are described in Figs. 3 and 4, respectively.
Figure 2

Time evolution of stabilization curves of x and y

Figure 3

Time evolution of the adaptive control gains \(w(t)\), \(\breve{w}(t)\)

Figure 4

Time evolution of the adaptive control gains \(u(t)\), \(\breve{u}(t)\)

Example 4.2

We focus on the following type of delayed fractional-order BAM neural network as a drive system:
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t}x(t)=-1.2x(t)+1.8f \bigl(y(t)\bigr) +1.3f\bigl(y\bigl(t-\sigma (t)\bigr)\bigr), \\ {}^{C}_{t_{0}}D^{q}_{t}y(t)=-1.4y(t)-1.6g \bigl(x(t)\bigr) -1.1g\bigl(x\bigl(t-\theta (t)\bigr)\bigr), \end{gathered} \end{aligned}$$
(30)
where \(t\ge 0\), \(q=0.96\), \(f(\cdot )=g(\cdot )=\sin (\cdot )\), \(\sigma (t)=1\), \(\theta (t)=0.9\), then \(\tau =1\).
The computer simulation of system (30) starting from initial conditions \(x(s)=4\), \(y(s)=-5\) for \(s\in [-1,0]\) is depicted in Fig. 5, which displays a chaotic attractor in system (30).
Figure 5

Chaotic attractor of system (30)

The associated response system is designed by
$$\begin{aligned} \begin{gathered} {}^{C}_{t_{0}}D^{q}_{t} \tilde{x}(t)=-1.2\tilde{x}(t)+1.8f\bigl(\tilde{y}(t)\bigr) +1.3f\bigl(\tilde{y} \bigl(t-\sigma (t)\bigr)\bigr)+p(t), \\ {}^{C}_{t_{0}}D^{q}_{t} \tilde{y}(t)=-1.4\tilde{y}(t)-1.6g\bigl(\tilde{x}(t)\bigr) -1.1g\bigl(\tilde{x} \bigl(t-\theta (t)\bigr)\bigr)+r(t), \end{gathered} \end{aligned}$$
(31)
where \(t\ge 0\), \(q=0.96\), \(f(\cdot )=g(\cdot )=\sin (\cdot )\), \(\sigma (t)=1\), \(\theta (t)=0.9\), and \(\tau =1\).
Taking \(\mu =0.01\), \(\breve{\mu }=0.01\), \(\xi =0.01\), \(\breve{\xi }=0.01\) and setting initial values as \(w(0)=0.05\), \(\breve{w}(0)=0.2\), \(u(0)=0.25\), \(\breve{u}(0)=0.2\), Figs. 69 portray the time evolution regarding adaptive synchronization curves and adaptive synchronization errors of systems (30) and (31) starting from initial values \(x(s)=2\), \(y(s)=3\), \(\tilde{x}(s)=-2\), \(\tilde{y}(s)=-3\) for \(s\in [-1,0]\), respectively. Figures 10 and 11 depict the adaptive control gains \(w(t)\), \(\breve{w}(t)\), \(u(t)\), \(\breve{u}(t)\), respectively.
Figure 6

Time evolution of synchronization curves of x and

Figure 7

Time evolution of synchronization curves of y and

Figure 8

Time evolution of synchronization error of z

Figure 9

Time evolution of synchronization error of 

Figure 10

Time evolution of the adaptive control gains \(w(t)\), \(\breve{w}(t)\)

Figure 11

Time evolution of the adaptive control gains \(u(t)\), \(\breve{u}(t)\)

Remark 4.1

Comparing with the numerical simulation results of Mittag-Leffler stabilization and synchronization, the object of stabilization and the object of synchronization that converge to the origin are different. For Mittag-Leffler stabilization, the curves of two states x and y converge to the origin, while for Mittag-Leffler synchronization, the curves of two errors z and converge to the origin. Additionally, Figs. 3, 4, 10, and 11 show that the adaptive controllers are very well designed.

5 Conclusion

The research of dynamic behavior of fractional-order systems by various control schemes has attracted extensive attention, nevertheless, the analysis and design of a kind of double-layer network by adaptive control approach has seldom been studied. In this paper, for a class of delayed fractional-order BAM neural networks, we use adaptive control strategy to exploit Mittag-Leffler stabilization and synchronization. Our main results of the paper are that adaptive controllers with adjustable parameters are constructed to stabilize and synchronize two types of delayed double-layer network. Based on the adaptive control design, the method of auxiliary functions and Mittag-Leffler dynamics theory of fractional-order systems, several sufficient criteria guaranteeing the realization of Mittag-Leffler stabilization in a controlled system and the realization of Mittag-Leffler synchronization in two coupled systems are shown. Moreover, the corresponding numerical simulations show the validity of the proposed results.

It should be noted that the adaptive controllers only contain some adjustable parameters and a little priori information about system itself. As the future work, much room for improvement remains based on adaptive control strategy, the corresponding adaptive controllers can be designed appropriately according to the requirements of different fractional-order systems. Indeed, those issues may be considerable research topics in the future.

Notes

Authors’ contributions

All authors contributed equally to this work. All authors read and approved the final manuscript.

Funding

This work was supported in part by the Natural Science Foundation of China under Grant 61773152, in part by the Natural Science Foundation of Hubei Province of China under Grant 2018CFB532.

Competing interests

The authors declare that they have no competing interests.

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Authors and Affiliations

  1. 1.College of Applied MathematicsHubei Normal UniversityHuangshiChina
  2. 2.College of Mathematics and StatisticsHubei Normal UniversityHuangshiChina

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