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Research article Special Issues

Synchronization of a class of nonlinear multiple neural networks with delays via a dynamic event-triggered impulsive control strategy

  • † The authors contributed equally to this work.
  • In this paper, the impulsive synchronization of a class of nonlinear multiple neural networks (MNNs) with multi-delays was considered under a dynamic event-based mechanism. To achieve a more comprehensive synchronization outcome and mitigate the conservativeness of impulsive control due to predetermined time sequences, we integrated a dynamic event-triggered strategy. This approach formed a novel control framework for generalized MNNs, where impulsive inputs were applied only under specific conditions governed by event-triggering rules. Towards the above objectives, the impulsive jumping system, resulting from dynamic component, and matrix measure method were invoked to directly increase the computational simplicity and extensibility of the study. As the outcome, the synchronization criteria for the MNNs could be achieved, and the exponential convergence rate is resolved by considering both the generalized comparison principle regarding impulsive systems and the variable parameter formula. Moreover, Zeno-freeness of the achieved triggering regulation is ensured. Finally, two numerical examples confirmed the validity of the designed approach.

    Citation: Chengbo Yi, Jiayi Cai, Rui Guo. Synchronization of a class of nonlinear multiple neural networks with delays via a dynamic event-triggered impulsive control strategy[J]. Electronic Research Archive, 2024, 32(7): 4581-4603. doi: 10.3934/era.2024208

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  • In this paper, the impulsive synchronization of a class of nonlinear multiple neural networks (MNNs) with multi-delays was considered under a dynamic event-based mechanism. To achieve a more comprehensive synchronization outcome and mitigate the conservativeness of impulsive control due to predetermined time sequences, we integrated a dynamic event-triggered strategy. This approach formed a novel control framework for generalized MNNs, where impulsive inputs were applied only under specific conditions governed by event-triggering rules. Towards the above objectives, the impulsive jumping system, resulting from dynamic component, and matrix measure method were invoked to directly increase the computational simplicity and extensibility of the study. As the outcome, the synchronization criteria for the MNNs could be achieved, and the exponential convergence rate is resolved by considering both the generalized comparison principle regarding impulsive systems and the variable parameter formula. Moreover, Zeno-freeness of the achieved triggering regulation is ensured. Finally, two numerical examples confirmed the validity of the designed approach.



    The growing requirements for synchronization of MNNs has inevitably raised higher precision in various areas of applications, such as biological systems, secure communications, chemical reaction, information processing, etc. (e.g., see [1,2,3,4]). Along with the outcome, the performance of network evolution and control immensely depends on the accuracy of the underlying model. However, the occurrence of time-varying delays is widely acknowledged as the major cause of chaos, oscillation, inadequate functionality, and occasional instability of complex networks. Such delays are prevalent in practical plants because of multiple factors like information transmission, controller update, communication bandwidth, and sampling. Neural networks suffering from delays, as shown by [5,6,7,8,9], could depict the practical networks more minutely and shows great superiority, leading to numerous efforts being dedicated to solving the synchronization issue of such networks [10,11,12].

    Despite the unprecedented opportunities presented by networked systems, the restrictions in network facilities and communication channels give rise to emerging challenges that coexist with the applications. The network devices in practice are constrained in processing data, particularly for battery-powered systems. Therefore, more endeavors should be focused on the design of energy-saving control strategies to avoid continuous communication and decrease the frequency of controller updates, achieving a lower communication and computation load of the proposed control strategy in actual application. Several effective strategies for conserving resources have been introduced in the existing literature so far, such as sampled-date feedback control [7,13], variable structure control [14,15] and sliding mode control [16,17,18], and so forth. However, the existing control methods often lead to a periodic transmission of packets, including some data that may be hardly necessary. Along with this consideration, alternative control strategies, such as event-triggered schemes, have been developed and garnered a wealth of research interest [18,19,20,21]. It utilizes an appropriate event generator to determine when signals should be delivered to neighboring nodes, resulting in a remarkable reduction in wastage of network resources. Specifically, sampling in event-based control only occurs as the state-dependent system error reaches a certain level. The pioneering work of Dimarogonas was based on an event-triggered control strategy that is associated with the error between the current and previous sampling instants [22]. The information of the controller is updated using the sampling data when the measurable error surpasses the allowable level. Initially, implementing the triggering conditions with static thresholds can be beneficial in minimizing communication costs since the conditions are difficult to fulfill. Nevertheless, these conditions may become easier to meet over time, resulting in frequent triggering and unnecessary updates. As a result, there is an urgent need for scholars to explore more flexible event-triggered schemes that can not only decrease communication expense and update the frequency of controller but also ensure efficient network coordination[23,24]. With the dynamic event-triggered scheme designed, fortunately, it provides us a direction to devote more effort for further optimization. Notice that only a limited number of research are available for the improved control strategy [25,26,27]. Li et al. [25] designed the synchronization controllers by incorporating a dynamic event-triggering approach involving absolute errors between system input updates, and a sufficient condition was achieved with synchronization error being exponentially ultimately bounded. In [26], a distributed dynamic event-triggered approach was initially presented utilizing an auxiliary parameter to dynamically regulate the threshold. Following this, certain criteria were developed to ensure the consensus of general linear multi-agent systems with or without a leader. The dynamic function was found to play a crucial role in regulating the triggering threshold dynamically and avoiding the Zeno behaviors in the time sequence.

    In addition, it is pertinent to note that the convergence rate of systems can be affected when their state undergoes changes instantaneously at some impulsive moments, resulting in decelerated, accelerated, or non-convergence scenarios. Therefore, investigating the impact of impulsive control upon the synchronization or stability of controlled systems is of great necessity. Numerous studies have concentrated on impulsive control via a time-triggered mechanism for neural networks. However, since the impulsive controller should be designed with fixed impulsive instants, its operating time cannot be altered [28,29,30,31]. This may cause constant changes in the actuator state, leading to performance degradation and wastage of resources. To optimize performance, the control instants can be computed by dynamically event-triggered conditions. The combined approach, which inherits the advantages of both single control strategies, also compensates for the drawbacks of event-triggered control by significantly reducing control expense and the resource usage of transmitted information. That is to say, the two approaches complement each other. Therefore, some results about impulsive control based on event-triggered schemes have been proposed recently [32,33,34,35]. As an example, Lu and Li [33] examined the consensus of a simple linearity system employing a distributed event-triggered impulsive (ETI) control scheme, in which impulse is implemented in a distributed framework according to the local information. In [34], Chen et al. designed the event-triggering impulsive control scheme, where impulsive instants and event-triggered sequences are separated and independent, and the synchronization of MNNs was discussed based on this.

    However, either those studies are based only on some simple systems that the delays, nonlinear terms, and characterizing the dynamical behavior are neglected, or the proposed controlling mechanism remains to be improved. All these matters above notwithstanding, the ETI control of complex systems subject to multi-delays is not yet considered and remains challenging, and a more generalized and utility-controlling theoretical method needs to be given.

    Thus, the innovations and contributions of this paper can be summarized as:

    1) Compared with the event-triggered control based on mathematical induction applying only to single delay linear system [33], the novel mechanism, introducing the impulsive-jumping system to improve the traditional comparison principle for the impulsive scheme, can solve the event-triggered control problem of system with multi-delays and nonlinear terms for the more practical situation.

    2) In comparison with the static event-triggered control in [32], the dynamic one benefiting from the import of dynamic function η(t) takes advantage of the resource-efficiency of the networks while guaranteeing the synchronization. Furthermore, the constraint resulting from the upper bound T requirement for consecutive impulse intervals can be optimized by the proposed event-triggering regulation.

    3) Different from the event-triggered control based on Lyapunov function [34,36,37], the designed event-triggered control in terms of observation error and synchronization error shows superior feasibility, which makes the algorithms easy to implement during the realization of synchronization.

    4) The p-norm and matrix measure approach is employed to handle the Lyapunov function rather than using cumbersome linear matrix inequalities, leading to the reduction of computational complexity and less conservativeness in the results.

    The remainder of this paper is structured as follows: Section 2 introduces the network model and basic knowledge. The main outcomes are demonstrated in Section 3. Section 4 extends the application to memristive neural networks and Section 5 presents the numerical simulations. Finally, the conclusion is made in Section 6.

    Notations: R is the set of real number and Rp×p denotes the p-dimensional Euclidean space. For a vector or a matrix, the symbol q(q=1,2,) stands for its q- norm. Let diag{ξ1,,ξp} represent the diagonal matrix with diagonal elements ξ1 to ξp. The transpose of matrix Q is given as QT and the identity matrix in Rp×p is denoted as Ip. For a given function f:RR, f(t+)=limh0+f(t+h) (or f(t)=limh0f(t+h)) indicates the upper-left Dini derivative Df(t)=limh0supf(t+h)f(t)h (or the upper-right Dini derivative D+f(t)=limh0+supf(t+h)f(t)h).

    Consider an array of coupled neural networks with nonlinear coupling and multi-delays, of which the i th neural network model can be represented as

    ˙ξi(t)=Dξi(t)+Af(t)+Bf(ξi(tτ1(t)))+c1Nj=1h1ijΓ1g1(ξj(t))+c2Nj=1h2ijΓ2g2(ξj(tτ2(t)))+J+ui(t),i=1,2,,N, (2.1)

    with u=1,2,,N. ξi(t)=(ξi1(t),ξi2(t),,ξin(t))TRn represents the state variable of the i neural network; D=diag{d1,d2,,dn}>0 refers to the rate at which the cell returns to its resting state potential when separated from other cells and inputs; A and B respectively stand for the connection weighting matrix with and without delay; f:R+×Rn×RnRn denotes the activation function referring to a continuous vector-valued function; c1 and c2 are positive constants to describe the coupling strengths; The current-state and time-delay inner coupling matrices are denoted by positive defined matrices Γ1 and Γ2, respectively; τs(t),s=1,2 represent the time-varying delays with 0τs(t)ˉτ. H1=[h1ij]N×N and H2=[h2ij]N×N are the current-state and time-delay coupling matrices, respectively, which are defined as follows: hsij>0, for s=1,2, if the ith node is capable of receiving the signal from the jth node, otherwise hsij=0. Moreover, the diagonal entries are redefined as hsii=Nj=1hsij. J=(J1,J2,,Jn) is an external input constant vector. In particular, ui(t) denotes an appropriate controller.

    The desired trajectory s(t) is given as follows:

    ˙s(t)=Ds(t)+Af(s(t))+Bf(s(tτ1(t)))+J. (2.2)

    Then, the synchronization error is further represented by ϵi(t)=ξi(t)s(t) with initial condition ϵi(t)=ϕi(t)φi(t)C([ˉτ,0],Rn). Thus, we are situated to explore the stability of the ith error systems:

    ˙ϵi(t)=Dϵi(t)+A˜f(ϵi(t))+B˜f(ϵi(tτ1(t)))+c1Nj=1h1ijΓ1˜g1(ϵj(t))+c2Nj=1h2ijΓ2˜g2(ϵj(tτ2(t)))+ui(t), (2.3)

    in which t0,i=1,2,,N, ˜f(ϵi(t))=f(ξi(t))f(s(t)), ˜f(ϵi(tτ1(t)))=f(ξi(tτ1(t)))f(s(tτ1(t))), ˜g1(ϵj(t))=g1(ξj(t))g1(s(t)), and ˜g2(ϵj(tτ2(t)))=g2(ξj(tτ2(t)))g2(s(tτ2(t))). The event-based impulsive controller ui(t) for delayed neural networks (2.1) is designed as

    ui(t)=Kiϵi(tk1)+k=1[μkϵi(t)ϵi(t)]δ(ttk),kN, (2.4)

    where t0=0 is the initial instant and {t1,t2,} denotes the sequence of impulsive instants, which will be decided by developed event generator later; KiRn×n is the state feedback gain matrix, and δ() denotes the Dirac delta function. Note that the impulsive mechanism demands the control strength μk(0,1) which will be determined later.

    Remark 1. Noticing that the novel controller (2.4) consists impulsive term k=1[μkϵi(t)ϵi(t)]δ(ttk) and event-triggered state feedback term Kiϵi(tk1), the specific event-triggered condition will be employed to generate the impulsive instants for avoiding the unnecessary energy cost resulting from the preset of time series, and it determines the updating of state feedback controlling term. Previous studies on impulsive control [10,29,38,39] have shown that a sufficiently high impulse frequency is required to achieve a desired convergence rate, in which case the unreasonable controlling time may result in unnecessary resource waste and poor performance. Obviously, in contrast with the traditional impulsive controllers or event-triggered controllers, in practical applications, the novel control mechanism not only makes up the above deficiency but also gives an instantaneous impulsive jump to further enhance the transient performance of the proposed controller.

    Supposing ϵi(t) is right-continuous, we have ϵi(tk)=ϵi(t+k) at t=tk, which further means the error system' solutions exhibit jump discontinuities at t=tk in the presence of impulsive scheme. In particular, the desired trajectory (2.2) is transmitted as a system input to system (2.1), causing an instantaneous change of corresponding state variable at t=tk. As a result, we obtain the following ETI error system with state feedback control input:

    {˙ϵi(t)=Dϵi(t)+A˜f(ϵi(t))+B˜f(ϵi(tτ1(t)))+c1Nj=1h1ijΓ1˜g1(ϵj(t))+c2Nj=1h2ijΓ2˜g2(ϵj(tτ2(t)))Kiϵi(tk1),t[tk1,tk),ϵi(t+k)=μkϵi(tk),kN.

    Letting ˜D=IND, ˜A=INA, ˜B=INB, ˜H1=(H1Γ1), ˜H2=(H2Γ2), K=diag{K1,K2,,KN}>0, ϵ(t)=(ϵ1(t),ϵ2(t),,ϵN(t))T, ˜g1(ϵ(t))=(˜g1(ϵ1(t)), ˜g2(ϵ2(t)), , ˜g1(ϵN(t)))T, and ˜g2(ϵ(tτ2(t)))=(˜g2(ϵ1(tτ2(t))), ˜g2(ϵ2(tτ2(t))), , g2(ϵN(tτ2(t))))T, the compact form of error systems can be expressed as

    {˙ϵ(t)=˜Dϵ(t)+˜A˜f(ϵ(t))+˜B˜f(ϵ(tτ1(t)))+c1˜H1˜g1(ϵ(t))+c2˜H2˜g2(ϵ(tτ2(t)))Kϵ(tk1),t[tk1,tk),ϵ(t+k)=μkϵ(tk),kN. (2.5)

    Remark 2. In this research, the goal is to devise the ETI control for solving the synchronization for general network systems with multi-delays. Toward this objective, several problems must be taken into account during the investigation. First, how to develop a control framework that combines the existing achievements on event-triggered control [20,40] and impulsive control [28,29,39] while retaining the main advantages of each strategy. Second, due to the unpredictability of controlling instants, the extraordinary assumption of the impulsive interval is no longer valid, and it becomes impossible and unreasonable to verify the theorem conditions in terms of the generated infinite controlling time. Third, for the distributed event-triggered strategy proposed in [41,42], every node is being updated based on the local information. Nevertheless, the ETI, with distributed form [33], may result in unsuitable impulses and raise great challenges for deriving the correlation between V(tk) and V(t+k). Instead, in accordance with the impulsive scheme, the centralized event-triggered scheme[37,43] should be a superior alternative to the candidate for synthesizing the innovative approach. Besides, the distributed one can be reviewed in future studies.

    Definition 1. [44] The matrix measure of a real square matrix Z=(zij)N×N is defined as

    mp(Z)=limh0+IN+hZp1h, (2.6)

    where p=1,2,.

    Given a constant matrix Z, recall the matrix norms by Z1=maxjNi=1|zij|, Z2=λmax(ZTZ), Z=maxjNj=1. Then, the corresponding matrix measures are derived as: m1(Z)=maxj{zij+ni=1,ij|zij|}, m2(Z)=(12λmax(ZT+Z)), m=maxi{zii+nj=1,ij|zij|}.

    Assumption 1. The function f(), ˜g1(), and ˜g2() are Lipschitz continuous, i.e., there exist constants L1,L2,L3>0, such that

    f(u)f(v)pL1uvp,˜g1(u)˜g1(v)pL2uvp,˜g2(u)˜g2(v)pL3uvp,

    for all u,vR, and p=1,2,.

    Lemma 1. [28] Let 0τi(t)τ,F(t,u,u1,,um):R+×m+1R××RR be nondecreasing in ui for each fixed (t,u,u1,,ui1,ui+1,,um),i=1,2,,m, and Ik(u):RR be nondecreasing in u. Suppose that u(t),v(t)PC([τ,+),R) satisfy

    {D+u(t)F(t,u(t),u(tτ1(t)),,u(tτm(t))),ttk,t0,u(t+k)Ik(u(tk)),kN,

    and

    {D+v(t)>F(t,v(t),v(tτ1(t)),,v(tτm(t))),ttk,t0v(t+k)Ik(v(tk)),kN.

    Then u(t)v(t) for τt<0 implies u(t)v(t) for t0. where D+u(t)=¯limh0+u(t+h)u(t)h.

    Recalling the theory of differential equations, W(t,s)=s<tk<tμketsf(u)du is denoted as the Cauchy matrix of linear equations:

    {˙v(t)=f(t)v(t),tt0,v(t+k)=μkv(tk),kZ+. (2.7)

    Then, the following useful lemma is presented.

    Remark 3. For Cauchy matrix W(t,s)=s<tk<tμketsf(u)du, in analyzing impulsive systems, it is often necessary to solve differential or difference equations with impulsive effects. The Cauchy matrix is frequently used to solve these equations, especially in pulse systems with periodic or quasi-periodic characteristics. The Cauchy matrix provides an effective tool in the convolution operations within pulse systems, aiding in the analysis of the response of the system to impulsive inputs.

    Lemma 2. Let {tk} be a sequence satisfying 0t0<t1<t2< and limttk=. The function v()PC1(R+,R) is right continuous in each tk. Suppose that the following inequalities hold

    {˙v(t)f(t)v(t)+g(t),tt0,v(t+k)μkv(tk)+ck,kZ+, (2.8)

    where f(),g()C(R+,R),μk0 and ck are constants. Then, we have

    v(t)v(t0)W(t,t0)+tt0W(t,s)g(s)ds+t0tk<tW(t,tk)μk,tt0. (2.9)

    Proof. Letting t[t0,t1), according to (2.8), one gets

    (v(t)ett0f(u)du)g(t)ett0f(u)du.

    Taking integral from t0 to t, it has

    v(t)v(t0)ett0f(u)du+tt0g(s)etsf(u)duds,t0t<t1,

    therefore, (2.9) holds over the time interval t[t0,t1]. Assume that there exists a n>1, when t[t0,tn], the Eq (2.9) is satisfied. Then, it can be verified for t[tn,tn+1) that

    v(t)v(t+n)ettnf(u)du+ttng(s)etsf(u)duds,

    recalling the inequalities (2.8), it gets

    v(t+n)μnv(tn)+cn,

    then

    v(t)(μnv(tn)+cn)ettnf(u)du+ttng(s)etsf(u)duds.

    By applying mathematical induction, we have

    v(t)μnettnf(u)du[v(t0)t0<tk<tnμketnt0f(v)dv+t0<tk<tn(tk<tj<tnμjetntkf(u)du)ck+tnt0(s<tk<tnμketnsf(u)dug(s))ds]+cnettnf(u)du+ttng(s)etsf(u)duds. (2.10)

    By means of certain algebraic manipulations, it can be verified that (2.10) is the (2.9) for t[t0,tn+1]. Hence, the proof is complete.

    Remark 4. Lemma 2 proposes the form of a generalized impulsive system with ck0. Obviously, it is able to characterize more complicated impulsive mechanisms than classical homogeneous impulses with ck=0 [28,39,43], which is much less conservative than many other reported impulsive strategy results involved. In this paper, the generalization impulsive system is first introduced to address the synchronization problem of complex networks, which may greatly expand the application of the impulsive control method such that more intricate impulsive mechanisms can be employed in future works.

    In this section, the ETI control schemes will be constructed to study the synchronization of general delayed MNNs with time-varying delays for the first time.

    Define the measurement error of the error system as

    ˆϵi(t)=ϵi(tk1)ϵi(t),t[tk1,tk),

    and ˆϵ(t)=(ˆϵ1(t),ˆϵ2(t),,ˆϵN(t))T.

    Based on Assumption 2, the following dynamic variable η(t) is proposed to satisfy the differential equation as follows:

    ˙η(t)=βη(t)ε(Kpˆϵ(t)pσϵ(t)p), (3.1)

    with η(0)>0,β>0, and appropriate parameters ε[0,1], σ[0,1] guaranteeing ˙η(t)<0. These dynamic variables are associated with the triggering laws, which will be developed in Theorem 1.

    Given θ and T are positive constants, the triggering time sequence is determined by

    tk=inf{t>tk1:ttk1>Torˆϵ(t)p1θ(Kp+σ)η(t)+σKp+σϵ(tk1)p}. (3.2)

    Remark 5. The internal dynamic variable η(t) in (3.2) is involved, of which the updating law involves the measurement error, negative self-feedback, and state error. Different from the static event-triggered scheme, the adoption of η(t) in (3.2) is a vital element to adjust the triggering level adaptively. If η(t) is devised to be zero, the event-triggered condition degenerates into the static one, which is a special case for (3.2). Moreover, it is not hard to prove that the triggering interval of two consecutive instants is lengthened due to the injection of η(t). Moreover, it results in the lessening of triggering frequency.

    Remark 6. In almost all impulsive schemes, the average impulsive interval T is introduced as a definition or assumption for the preset impulsive instants such that the synchronization of the complex system can be ensured. However, for event-triggered control, the triggering times are generated by the designed condition, it is unreasonable to propose the criteria involves the controlling instant tk owing to the uncertainty, infinity, and unpredictability of event-triggering instants. The incorporation of impulsive control and event-triggering schemes inevitably possesses additional limitations. Fortunately, benefiting from the event-triggered machine, it can provide great flexibility during the construction of an appropriate triggering strategy such that some specific objectives can be achieved. For example, in [37], the triggering condition provided the upper bound of the involved time-vary delay during the controlling. Consequently, as for the unpredictable impulsive instants, the former average impulsive interval may be weakened into the triggering condition characterized as the constant T here.

    In what follows, the criteria of the delayed MNNs under the dynamic ETI strategy are formulated and the elimination of the Zeno phenomenon is discussed as well.

    Theorem 1. Suppose that Assumption 1 holds. Then, the delayed neural networks are synchronized via the controller (2.4) with dynamic event-triggered conditions (3.2) if there exist constants γ1,γ2,ω>0 such that

    (Λ+ln˜μT)+γ1+γ2<0, (3.3)

    where the control gains satisfy

    (1eωT)+eωTμk<μk+1, (3.4)

    where Λ=max{(mp(K)+Lp˜Ap+cH˜Dp),1εθβ}, ˜μ=maxk{μk}, γ1=L1Bp,γ2=L3c2˜H2p, ω(Λ+ln˜μT), and λ>0 is a unique positive solution for λ+(Λ+ln˜μT)+(γ1+γ2)eλˉτ=0.

    Proof. In accordance with the triggering condition, one has

    ˆϵ(t)p1θ(Kp+σ)η(t)+σKp+σϵ(tk1)p,t[tk1,tk). (3.5)

    Moreover, recalling the Eq (3.1), we have ˙η(t)βη(t)εθη(t). Thus

    η(t)η(0)e(β+εθ)t>0. (3.6)

    Design the Lyapunov functional as follows:

    ˜V(t)=V(t)+η(t), (3.7)

    where V(t)=ϵ(t)p, p=1,2,. Computing the upper Dini derivative of (3.7) for [tk1,tk) along the trajectory of error system (2.5) and control input (2.4), there exists

    D+˜V(t)=limh0+ϵ(t+h)pϵ(t)ph+˙η(t)=limh0+ϵ(t)+h˙ϵ(t)+o(h)pϵ(t)ph+˙η(t)=limh0+1h{ϵ(t)+h(˜Dϵ(t)+˜A˜f(ϵ(t))+˜B˜f(ϵ(tτ1(t)))+c1˜H1˜g1(ϵ(t))+c2˜H2˜g2(ϵ(tτ2(t)))Kϵ(tk1))+o(h)pϵ(t)p}+˙η(t)limh0+InhKp1hϵ(t)p+˜Apf(ϵ(t))p+˜Bpf(ϵ(tτ1(t)))p+˜Dpϵ(t)p+c1˜H1p˜g1(ϵ(t))p+c2˜H2p˜g2(ϵ(tτ2(t)))p+Kpˆϵ(t)p+˙η(t)(mp(K)+L1˜AP+˜Dp+c1L2˜H1p)ϵ(t)p+L1Bpϵ(tτ1(t))p+L3c2˜H2pϵ(tτ2(t))p+Kpˆϵ(t)pβη(t)+ε(σϵ(t)pKpˆϵ(t)p)(mp(K)+L1˜AP+˜Dp+c1L2˜H1p)ϵ(t)p+(1εθβ)η(t)+L1Bpϵ(tτ1(t))p+L3c2˜H2pϵ(tτ2(t))pΛ˜V(t)+γ1˜V(tτ1(t))+γ2˜V(tτ2(t)), (3.8)

    where Λ=max{(mp(K)+L1˜AP+˜Dp+c1L2˜H1p),1εθβ}, and γ1=L1Bp,γ2=L3c2˜H2p.

    Hereafter, we are devoted to developing the correlation between V(t+k) and V(tk) which allows the outcomes to match the framework in Lemma 2. If t=tk, there exists

    ˜V(t+k)=V(t+k)+η(t+k)=μkV(tk)+η(tk)=μk˜V(tk)+(1μk)η(tk). (3.9)

    Denoting ck=(1μk)η(tk), κ>0, v(t) is a unique solution of the novel impulsive system

    {˙v(t)=Λv(t)+γ1v(tτ1(t))+γ2v(tτ2(t))+κ,ttk,v(tk)=μkv(tk)+ck,t=tk,v(s)=ϵ(s)p,τs0.

    From Lemma 1, one gets v(t)˜V(t)0, t0. Applying the result of Lemma 2, it can be obtained that

    v(t)=W(t,0)v(0)+t0W(t,s)[γ1v(sτ1(s))+γ2v(sτ2(s))+κ]ds+t0tk<tW(t,tk)ck, (3.10)

    in which W(t,s) (t,s0) refer to the Cauchy matrix of the corresponding linear impulsive system.

    In light of the formulation of the Cauchy matrix, we have the below inequality:

    W(t,s)=s<tk<tˉμetsΛdveΛ(ts)ˉμtsT=e(Λ+lnˉμT)(ts).

    Let q=supˉτs0{ϵ(s)p}. From (3.10), it gets

    v(t)qe(Λ+lnˉμT)t+t0e(Λ+lnˉμT)(ts)[γ1v(sτ1(s))+γ2v(sτ2(t))+κ]ds+t0tk<te(Λ+lnˉμT)(ttk)ck. (3.11)

    Let h(λ)=λ+(Λ+ln˜μT)+(γ1+γ2)eλˉτ. Utilizing the condition in Theorem 1, we have

    h(0+)=(Λ+ln˜μT)+γ1+γ2<0. (3.12)

    Obviously, we have h(+)>0 and h(λ)=1+ˉτ(γ1+γ2)eλˉτ>0. Therefore, there is a only positive solution λ>0 of the equation h(λ)=0.

    Thereafter, we will prove that the following inequality is satisfied for t0

    v(t)<qeλt+t0tk<teλt+ωtkck+κ(Λ+ln˜μT)γ1γ2, (3.13)

    where (Λ+ln˜μT)ω.

    If it does not hold, a positive constant t can be found with

    v(t)qeλt+t0tk<teλt+ωtkck+κ(Λ+ln˜μT)γ1γ2. (3.14)
    v(t)<qeλt+t0tk<teλt+ωtkck+κ(Λ+ln˜μT)γ1γ2,t<t. (3.15)

    From (3.11) and (3.15), it holds that

    v(t)qe(Λ+ln˜μT)t+t0e(Λ+ln˜μT)(ts)[γ1v(sτ1(s))+γ2v(sτ2(s))+κ]ds+t0tk<te(Λ+ln˜μT)(ttk)ck<qe(Λ+ln˜μT)t+e(Λ+ln˜μT)tt0e(λ+(Λ+ln˜μT))s(γ1+γ2)[qeλˉτ+t0tk<teλ(sˉτ)+ωtkck]ds+κ(Λ+ln˜μT)γ1γ2t0e(Λ+ln˜μT)(ts)(γ1+γ2)ds+κt0e(Λ+ln˜μT)(ts)ds+t0tk<te(Λ+ln˜μT)(ttk)ckqe(Λ+ln˜μT)t+qe(Λ+ln˜μT)tt0e(λ+(Λ+ln˜μT))s[(λ+(Λ+ln˜μT))]ds+t0tk<teλt+ωtkckt0tk<te(Λ+ln˜μT)t+ωtkck+t0tk<te(Λ+ln˜μT)(ttk)ck+κ(Λ+ln˜μT)(Λ+ln˜μT)γ1γ2t0e(Λ+ln˜μT)(ts)ds<qeλt+t0tk<teλt+ωtkck+κ(Λ+ln˜μT)γ1γ2,

    which results in a contradiction with (3.14). Thus, the inequality (3.13) is satisfied. Letting κ0, it holds for t0 that

    e(t)p˜V(t)v(t)qeλt+t0tk<teλt+ωtkck,t0,

    which indicates

    e(t)psupˉτs0ϵ(s)peλt+t0tk<teλt+ωtkck.

    Recalling the differential Eq (3.1), it has

    η(t)=eβt(η(0)+t0eβs(ε(Kpˆϵ(s)pσϵ(s)p))ds).

    Noticing the noincreasing of dynamic function η(), the impulsive gain μk+1 for the event-triggered instant t=tk+1 can be designed such that

    (1μk+1)η(tk+1)(1μk)η(tk)<eωT<1,

    then, we can have

    (1eωT)+eωTμk<μk+1. (3.16)

    Finally, for the constant M>0, one has

    e(t)p(supˉτs0ϵ(s)p+M)eλt. (3.17)

    The theorem is proved.

    Remark 7. Note from the condition (3.4) that the sequential impulsive gain μk+1 is closely related to the system parameter term Λ, former impulsive strength μk and the length of T. Obviously, each impulsive instant gives us a guideline for balancing the selection of impulsive gain μk to obtain a suitable hybrid impulsive controller. Just event-triggering rules may not guarantee the realization of synchronization for underlying networks, some restricted conditions should be additionally put forward for certain objectives. For example, as a compromise, there exists a constant ρ2 which satisfies ρ2supkN{tktk1} for triggering instants in [32], and the authors choose a suitable parameter β such that maxk{eln(βγ)+λ(tk+1tk)}<α<1 in [36].

    Remark 8. Different from previous works, the existence of dynamic function η(t) greatly improves the challenges of the considered problem, which not only induces the constants ck, in each impulsive instants, turning the traditional impulsive system into impulsive jumping systems but also should promise the monotone decreasing of dynamic triggering function that ˙η<0 at the same time.

    The following theorem will demonstrate that the proposed control scheme gets rid of the Zeno-phenomenon, which means tk+1tk>0 can be guaranteed with a lower bound of interval times.

    Theorem 2. Supposed that criteria (3.3) and (3.4) hold, then the time interval Tk exists and satisfies the following

    tk=tk+1tkσ>0. (3.18)

    That is to say, the Zeno phenomenon of the proposed control scheme is excluded.

    Proof. According to (3.17), we have for t[tk1,tk) that

    ϵ(tk1)p(supˉτs0ϵ(s)p+M)eλtk1,ϵ(tτ1(t))p=ϵ(t)p+ξ1(t)(supˉτs0ϵ(s)p+M)eλtk1,

    where ξ(t)0 is associated with τ(t).

    Taking derivation of ˆϵ(t) for [tk1,tk),kN, yields

    D+ϵ(t)˙ϵ(t)=˜Dϵ(t)+˜A˜f(ϵ(t))+˜B˜f(ϵ(tτ1(t)))+c1˜H1˜g1(ϵ(t))+c2˜H2˜g2(ϵ(tτ2(t)))Kϵ(tk1)(˜D+c1L2˜H1)ϵ(t)+L1˜Aϵ(t)+L1˜Bϵ(tτ1(t))+c2L3˜H2ϵ(tτ2(t))+Kϵ(tk1)(cH˜D+Lf˜A+Lf˜B)^ϵ(t)+(cH˜D+Lf˜A+Lf˜B+K)ϵ(tk1)+Lf˜Bξ(t)=Υ^ϵ(t)+˜C(t),

    where Υ=cH˜D+Lf˜A+Lf˜B, ˜C(t)=(cH˜D+Lf˜A+Lf˜B+K)ϵ(tk1)+Lf˜Bξ(t).

    Therefore, we can solve the equality with the initial condition ˆϵ(tk)=0 for t[tk1,tk) as follows:

    ˆϵ(t)˜C(t)Υ[eΥ(ttk1)1].

    By virtue of the dynamic triggering condition, when t=tk we have

    1θ(Kp+σ)η(t)+σKp+σϵ(tk1)˜C(t)Υ[eΥ(tktk1)1],

    which means that

    tk=tktk11Υln[1+Υ(η(t)+θσϵ(tk1))θ(K+σ)˜C(t)].

    Thus ˜C(t)(supˉτs0ϵ(s)p+M)(cH˜D+Lf˜A+Lf˜B+K+Lf˜B)=˜C. It follows that

    tk1Υln[1+Υ(η(t)+θσϵ(tk1))θ(K+σ)˜C].

    Hence, for t[tk1,tk),kN,

    tk1Υln[1+Υ(η(tk)+θσϵ(tk1))θ(K+σ)˜C]>0.

    Thus, the lower bound of inter-execution time exists and satisfies Tk=tktk1σ>0. The completes the proof.

    Remark 9. It can be found that according to property of dynamic function η(t), only when the synchronization comes true with error state ϵ(t)=0, ϵ(tk1)=0 and the dynamic function decreasing to η(t)=0, the Zeno phenomenon can emerge. That is to say, the Zeno-behavior is ruled out for error system (2.5).

    The proposed control scheme is capable of improving the traditional impulsive. When the interval T refers to the average impulsive interval T, with event-triggered strategy removing, it is easy to obtain the following result.

    Corollary 1. Suppose that the Assumption 1 holds. Then, the delayed MNNs are synchronized via the controller (2.4) with the dynamic event-triggering rule (3.2), if

    (Λ+ln˜μT)+γ1+γ2<0, (3.19)

    and selecting

    (Λ+ln˜μT)<ω<λ,

    where Λ=mp(K)+Lp˜Ap+cH˜Dp, ˜μ=maxk{μk}, γ1=L1Bp,γ2=L3c2˜H2p and λ>0 is a unique positive solution of λ+(Λ+ln˜μT)+(γ1+γ2)eλˉτ=0.

    Remark 10. If the dynamic event-triggered mechanism is separated, the investigation becomes the traditional impulsive synchronization problem. The corollary not only contains some correlational previous problems as a special case but also, with the introduction of p-norm, the simpler and easier verifiable criterion is achieved compared with some former achievement [28,39].

    In this section, we present two numerical simulations to illustrate the efficiency of the theoretical results obtained in this paper.

    Example 1. The effectiveness of Theorem 1 is verified in this section. To illustrate the efficiency of the proposed theoretical results, the following cellular neural network is considered the leader

    [˙s1(t)˙s2(t)]=[1001][s1(t)s2(t)]+[1+π/4200.11+π/4][f1(s1(t))f2(s2(t))]+[2π13400.10.12π1340][f1(s1(tτ1(t)))f2(s2(tτ1(t)))]

    where fi(si)=(|si+1||si1|)/2, i=1,2. It is clearly that Π=diag{1,1} [39]. Then, to validate the feasibility of Theorem 1, we consider a networked multi-agent system of six agents, and the coupled cellular neural network satisfies (2) with

    D=[1001],A=[1+π/4200.11+π/4],B=[2π13400.10.12π1340].

    It is obviously the Lipschitz condition in Assumption 1 is computed as L=0.6I3. Assume that Γ1=Γ2=Γ3=diag{1,1} and τ1(t)=τ2(t)=0.1etet+1. The current-state coupling and time-delay can be respectively chosen as

    H1=(210100011000103101000210000011100003),H2=(1000100021100002001101200000011001001).

    Without the lost of general, the nonlinear coupling function g1(x)=g2(x)=0.32x0.295(|x+1||x1|), coupling strength c1=c2=0.5, and the state feedback control gain matrix K=10diag{1,1}. Considering the 2-norm of the vector or matrix in the simulations, therefore, we have mp(K)=10. Noticing that the upper impulsive bound T, γ1=1.539L1 and γ2=1.5432L3 can be calculated to satisfy the condition (13) in Theorem 1. By solving the inequality, we can set the controlling interval T=20 and maximum impulsive gain ˜μ=0.943. Therefore, conditions (13) and (14) can be satisfied. To clearly demonstrate the complexity of our algorithm, the method of choosing the parameters in the controller can refer to Algorithm 1.

    Algorithm 1 Dynamic event-triggered impulsive control implementation
    Require: Give the initial values ξi(t), s(t), η(t) for all i=1,2,,N, t0=0, k=0. Set t, sampling time h, and simulation time T;
     1: Chose the parameters β, ε, σ, θ, T, control feedback parameters K, μk;
    Ensure:
     2: if Assumption 1 holds simultaneously, then
     3:        go to Line 7
     4: else
     5:        go to Line 1
     6: end if
     7: for 0<t<T do
     8:        if t=0; then
     9:                Compute the value of Λ=max{(mp(K)+Lp˜Ap+cH˜Dp),1εθβ}, ˜μ=maxk{μk}, γ1=L1Bp,γ2=L3c2˜H2p, ω(Λ+ln˜μT), and λ>0 is a unique positive solution for λ+(Λ+ln˜μT)+(γ1+γ2)eλˉτ=0, and control input ui(t) in (2.4) using the initial value ϵi(t);
     10:        else
     11:                if event-triggered condition (3.2) holds; then
     12:                    k=k+1;
     13:                    tk=t;
     14:                else
     15:                    tk keeps its value of k-triggering;
     16:                end if
     17:                Compute the impulsive gain μk in (2.4);
     18:                Compute the control input in (2.4);
     19:        end if
     20:        t=t+h;
     21: end for

    Next, we will show the dynamic state-triggering rule (3.2) revolution with θ=10,σ=1 and dynamic function ηi(0)=10. The dynamic ETI instants are given in Figure 1(a) and static ETI one [33,37,43] in Figure 1(b), in which the value equal to 1.5 refers to the triggering generated from the upper triggering bound T in blue and 1 resulting from the error triggering condition in pale green. Obviously, compared with the static triggering condition with the same parameters as the dynamic one, it is shown that the dynamic one can significantly decrease the triggering number, especially behind t=2. Figure 2(a) shows the state trajectories of the leader and the following coupled neural networks. With the event-based impulsive controller is replaced by

    ui(t)=Kϵi(tk1)+k=1[μϵi(t)ϵi(t)]δ(ttk),kN, (4.1)
    Figure 1.  Triggering time sequences of Example 1 with 6 coupled neural networks.
    Figure 2.  State Trajectories of Example 1 with 6 coupled neural networks.

    the error system of (2.5) under the designed control is shown in Figure 2(b). Obviously, the exponential synchronization of the coupled neural networks and the state leader is achieved with multi-delays and nonlinear terms.

    Example 2. To demonstrate the effectiveness of the dynamic EIC method in practical applications. Consider the Chua's circuits model, of which the dynamic is described by

    {˙s1(t)=a(s2(t)G(s1(t))),˙s2(t)=s1(t)s2(t)+s3(t),˙s3(t)=bs2(t), (4.2)

    where G(s1(t))=0.32x0.295(|s1(t)+1||s1(t)1|),a=10,b=14.87. Without loss of generality, we consider the system (4.2) as the leader of the networked system. Therefore, we can obtain the system parameters in the following

    A=(0.32aa01110b0),B=(a00000000).

    The nonlinear function f(s1(t))=0.295(|s1(t)+1||s1(t)1|). Thus the Lipschitz condition in Assumption 1 can be calculated as L=0.6I3. To verify the feasibility of Theorem 1, we consider a networked system of six agents, where the dynamic of each agent is depicted by the Chua's circuits (4.2), the coupling delay τ0=0.2, coupling strength d=0.5, and the coupling matrix can be chosen as

    H=(110000011000001100000110000011100001).

    Basing simulation of example 1 and taking the same parameters of controller and event-triggered method, some similar results can be obtained. Obviously, the exponential synchronization of Chua's circuits model is achieved under the event-triggered impulsive control, and the state trajectories of the leader and following agents are shown in Figure 3(a). In addition, the event-triggered impulsive instants and traditional impulsive instants are given in Figure 3(b). It should be noted that if impulsive instants are set before, some impulsive instants are unnecessary, and the instants sequence has to be unrelenting owing to the unknown terminal time.

    Figure 3.  The simulations of Example 2 with Chua's circuits model.

    Basing the traditional impulsive control theory, this paper combines the dynamic event-triggered rule to further improve control performance and reduce impulse consumption, of which the impulsive instants are generated according to the predesigned event-triggering condition. Moreover, the synchronization problem of coupled neural networks with nonlinear and multi-delays is investigated to enhance the applicability and universality of the outcome. By achieving the solution and impulsive jumping system and introducing measure measure method, the dynamic event-based impulsive mechanism is successfully constructed and applied to receive some sufficient conditions of the considered synchronization problem, and the Zeno behavior has been excluded in the proposed strategy. Finally, two numerical simulations are conducted to verify the correctness of the proposed algorithm. Although our network model can describe certain real-world phenomena, it still has some limitations. It should be noted that state-dependent networks, of which the communication structure varies related to the state of nodes, can better characterize the practice network. We will extend the proposed dynamic ETI scheme to the synchronization problem of state-dependent networks in our future work.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This research was supported by the High-Level Talent Initiation Project of Shenzhen Polytechnic University (6024330003K); in part by the 2024 Guizhou University of Finance and Economics student-funded scientific research project under Grant 2024ZXSY206; in part by the project of Young Scientific and Technical Talents Development of Education Department of Guizhou Province under Grant [2024]80.

    The authors declare there are no conflicts of interest.



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