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Research article

Exponential synchronization of neural networks with mixed delays under impulsive control

  • Received: 14 July 2024 Revised: 02 September 2024 Accepted: 05 September 2024 Published: 13 September 2024
  • In this paper, the exponential synchronization problem of a class of neural networks with mixed delays under impulsive control is studied. Combining the impulsive comparison principle and the concept of an average impulsive interval, two impulsive differential inequalities with mixed delays are discussed, and the sufficient conditions for the existence of exponential decay are obtained. Based on two different impulsive control strategies, and then by means of the Lyapunov function, the inequality technique, and these two new inequalities, a set of sufficient conditions are derived to ensure the synchronization of the drive and response systems. In order to prove the effectiveness of the proposed control scheme, two numerical examples are given to prove its practicability and effectiveness.

    Citation: Wanshun Zhao, Kelin Li, Yanchao Shi. Exponential synchronization of neural networks with mixed delays under impulsive control[J]. Electronic Research Archive, 2024, 32(9): 5287-5305. doi: 10.3934/era.2024244

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  • In this paper, the exponential synchronization problem of a class of neural networks with mixed delays under impulsive control is studied. Combining the impulsive comparison principle and the concept of an average impulsive interval, two impulsive differential inequalities with mixed delays are discussed, and the sufficient conditions for the existence of exponential decay are obtained. Based on two different impulsive control strategies, and then by means of the Lyapunov function, the inequality technique, and these two new inequalities, a set of sufficient conditions are derived to ensure the synchronization of the drive and response systems. In order to prove the effectiveness of the proposed control scheme, two numerical examples are given to prove its practicability and effectiveness.



    Originating from the groundbreaking M-P model devised by McCulloch and Pitts [1], neural networks (NNs) have evolved into powerful machine learning algorithms [2]. Their ubiquitous application across diverse fields stems from their remarkable aptitude for learning and discerning patterns within data. Whether in associative memory tasks that need to process a large amount of information[3], or in automatic control systems that require precise control, NNs have shown their unique advantages. Concurrently, NNs occupy an indispensable position in realms such as pattern recognition, signal processing[4,5,6], secure communication, and tackling intricate optimization challenges [7,8]. Because of its characteristics, it has attracted the attention of scholars.

    In the specific implementation, a time delay is widespread and inevitable, which is due to the limited transmission of information between systems[9,10]. On the other hand, NNs usually have spatial characteristics because numerous parallel pathways exist. The dissimilar axis-cylinder size and length, as well as the propagation velocity distribution along these pathways, brings about a propagation distribution delay[11,12]. Numerous scholars engaged in profound discourses, thereby embracing the perspective that the presence of a time delay inherently influenced the dynamic behavior exhibited by NNs, such as oscillation, divergence, or instability, and other complex dynamic behaviors [13,14]. The above phenomena is harmful to NNs and practical applications. Therefore, it is a useful theoretical research and practical application to introduce a time delay into the modeling of neural networks.

    Synchronization is a dynamic behavior of NNs, whereby two or more systems have the same behavior under coupling or external control. Synchronization is widely used in secure communication[15,16], image encryption[17,18], and image protection[19]. Many scholars studied various types of synchronizations according to various situations, see [20,21,22,23].Therefore, the study of NN synchronization has both theoretical and practical values.

    Designing a suitable controller to achieve synchronization is a challenge. Based on the time interval operation, the intermittent controller automatically switches the working / resting state of the equipment, optimizes energy consumption, and reduces costs. Because of its energy saving effect and practicability, it has attracted wide attention and application, see[24,25,26,27,28]. Impulse control turns a continuous system into a discontinuous one at the impulse moment. Both pulse control and intermittent control exert infleunces at the corresponding time. However, compared with intermittent control, pulse control is a time rather than a time period, which helps reduce the cost of control. Therefore, impulsive control is widely used in synchronization problems. In [29], the exponential synchronization problem of delayed coupled NNs was studied by means of a Razumikhin-type inequality. In [30], the exponential synchronization problem of stochastic coupled NNs was studied by using the stochastic impulsive differential inequality. In [31], the quasi-synchronization of NNs was studied using the Lyapunov function and the impulsive comparison principle. In [32], the quasi-synchronization problem of directed coupled heterogeneous NNs was studied using the extended pulse comparison principle and the saturated nonlinear dead-zone function. In [33], the μ-synchronization of coupled NNs was studied by constructing a new impulsive differential inequality. In [34], the quasi-synchronization problem of the quasi-synchronization of multi-layer delayed NNs was studied using the Lyapunov function and the pulse comparison principle. In [35], the synchronization problem of nonlinear, delayed, semi-Markov, jump NNs was studied using the stochastic Lyapunov function and the Razumikhin technique. In [36], the synchronization problem of coupled delayed inertial NNs was studied using the improved pulse comparison principle. In [37], the synchronization problem of hybrid coupled NNs was studied using delay impulsive differential inequalities. For example, in the above cited literature, the main proof of [33] and [36] is to transform the original problem into an impulsive differential inequality by means of the Lyapunov function. The forms of the two are similar. [33] proved the impulsive differential inequality first, while [36] was based on the improved impulsive comparison principle. Inspired by this, we can first discuss the transformed impulsive differential inequalities. This is the source of the idea of the impulsive inequality in this paper.

    The main results of this paper focus on the following aspects:

    (ⅰ) Two delay impulsive differential inequalities are given; and

    (ⅱ) The exponential synchronization problem of two different impulsive control strategies is considered.

    The subsequent sections of this paper are organized in the following manner: Section 2 presents an overview of the model and introduces the prerequisite knowledge; Section 3 delves into the presentation of sufficient conditions to achieve exponential synchronization in impulsive neural networks that incorporate mixed delays; in Section 4, two numerical examples are provided to demonstrate the practical efficacy of the proposed approach; and finally, Section 5 concludes the paper with a summary of the key findings.

    Hereof, unless otherwise elucidated, we will use the following notation. We define R as the set of real numbers, N as the set of positive integers, and Rn as the set of n-dimensional real vectors equipped with the Euclidean norm ||||. Additionally, we let Rm×n represent the set of m×n real matrices. The n×n unit matrix is represented by E. When A and B are regular intersection matrices, the notationA>B (respectively, A<B) indicates that AB is a positive definite (respectively, a negative definite). The transpose and the inverse of matrix A are denoted by AT and A1, respectively. The maximal and minimal eigenvalues of symmetric A are λmax(A) and λmin(A). The function σ() denotes the spectral radius of a matrix. For any interval JR, PC = {ψ:JRn that are continuous everywhere except at a finite number of points t, where ψ(t+),ψ(t) exist and ψ(t+)=ψ(t)}. For ς(t)PC([τ,0],Rn), define ||ς(t)||=ςT(t)ς(t).

    The driving system considered in this paper is a NN with mixed delays, which is defined as follows:

    {dx(t)dt=˜Dx(t)+˜Af(x(t))+˜Bf(x(tτ(t)))+˜Ctthf(x(s))ds+˜I(t),x(t)=˜ϕ(t), ϱ<t<0, (2.1)

    where the neuron state vector x=(x1,x2,,xn)T and matrices ˜D>0, ˜A, ˜B, ˜C represent the diagonal matrix, connection weight matrix, delayed weight matrix, and distributively delayed connection weight matrix of the neural network, respectively. The activation function is f()=(f1(),f2(),,fn())T. Time-varying delays τ(t) satisfy 0τ(t)τ. The distributed-delay is h, and ϱ=max{τ,h}. ˜ϕ(t)PC([ϱ,0],Rn). with components ˜ϕi(t),i=1,2,,n.

    The response system is as follows:

    {dy(t)dt=˜Dy(t)+˜Af(y(t))+˜Bf(y(tτ(t)))+˜Ctthf(y(s))ds+˜I(t)+˜u(t),y(t)=˜φ(t), ϱ<t<0, (2.2)

    where ˜φ(t)=(˜φ1(t),˜φ2(t),,˜φn(t))T, has components ˜φi(t) that belong to PC([ϱ,0],Rn).

    To achieve the article's objective, the error e(t)=y(t)x(t) is defined.

    Combining networks (2.1) and (2.2), the error system is formulated as follows:

    {de(t)dt=˜De(t)+˜Ag(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds+˜u(t),e(t)=˜ψ(t), ϱ<t<0, (2.3)

    where g(e(t))=f(y(t))f(x(t)), ˜ψ(t)=˜φ(t)˜ϕ(t).

    The impulsive control protocol has been designed in the following manner:

    ˜u(t)=˜K1e(t)+˜K2g(e(t))μk=1˜Rke(t)δ(ttk), (2.4)

    where the gain matrices are represented by ˜K1 and ˜K2 in this context. ˜Rk>0 is the control gain. The fixed impulsive moments tk (for kN) form a strictly increasing sequence that satisfy 0=t0<t1<t2<,tk<  with the property that the sequence diverges to infinity, (i.e., limttk=+). The Dirac impulsive function is denoted by δ().

    Remark 2.1. In [38], the controller only considered the feedback of the activation function in t and tτ(t). In [34], the controller was composed of the linear term of the error function and the dirac impulsive function. In [35], the controller was only composed of the dirac impulsive function. The controller in this paper considers the non-delay term of the error function and the dirac impulsive function.

    By combining Eqs (2.3) and (2.4), we obtain a rephrased version of the error system:

    {de(t)dt=(˜D˜K1)e(t)+(˜A+˜K2)g(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds, ttk,:=ˆDe(t)+ˆAg(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds, ttk,Δe(tk)=e(t+k)e(tk)=μ˜Rke(tk), t=tk,e(t)=˜ψ(t), ϱ<t<0. (2.5)

    Definition 2.1. [38] The systems (2.1) and (2.2) were deemed to be exponentially synchronized if there existed positive constants λ and M1, such that for every t>0, the norm of the error function ||e(t)|| between the two systems satisfied the inequality ||e(t)||supτs0||φ(s)ϕ(s)||Meλt. Here, λ serves as the convergence rate (or degree), which characterizes the exponential decline in the synchronization error as time progresses.

    Definition 2.2. [31] The average impulsive interval of the impulsive sequence ζ={t1,t2,,tk,} was equal to Ta, if there existed the positive integer N0 and the positive scalar Ta such that for all 0tT, the number of impulsive times Nζ(T,t) of the sequence ζ within the time interval (t,T) satisfied the following inequality:

    TtTaN0Nζ(T,t)TtTa+N0, 0tT.

    Here, Nζ(T,t) represents the count of impulsive instants which belong to the sequence ζ that strictly occur between the times t and T.

    Lemma 2.1. [31] Let τ1(t) and τ2(t) be functions which satisfy 0τ1(t),τ2(t)τ for all t. Consider the function G(t,u,ˉu1):R+×R×RR, which is nondecreasing in its third argument ˉu1 for fixed values of t and u. Additionally, let Ik(u):RR be a function that is nondecreasing in u. If there exists a positive constant α>0 such that

    {D+u(t)G(t,u(t),u(tτ1(t)))+αttτ2(t)u(s)ds, ttk,u(tk)Ik(u(tk), kN, (2.6)
    {D+v(t)>G(t,v(t),v(tτ1(t)))+αttτ2(t)v(s)ds, ttk,v(tk)Ik(v(tk), kN, (2.7)

    then u(t)v(t) holds for τt0, and under the assumption that certain properties related to the right upper derivativeD+u(t) hold, it can be shown that u(t)v(t) also holds for all t>0.

    Lemma 2.2. [32] Given any real, symmetric, and positive definite matrix M of an appropriate dimension, a positive scalar η>0, and a vector function ω():[a,b]Rn such that the relevant integrals are well-defined, the following inequality holds:

    [baω(s)ds]TM[baω(s)ds](ba)baωT(s)Mω(s)ds.

    In order to study the exponential synchronization of NNs with mixed discrete delays and finite distributed delays, the following impulsive differential inequalities which involve discrete delays and finite distributed delays are first established.

    Lemma 2.3. Let u(t)PC([ϱ,+),R) with u(t)0; for the impulsive sequence ζ={t1,t2,,tk,}, consider the following differential inequalities:

    {D+u(t)αu(t)+θ1u(tτ(t))+θ2tthv(s)ds, ttk,u(tk)βu(tk), kN,u(s)=φ(s)0,s[ϱ,0], (2.8)

    where α>0, θ1>0, θ2>0,0τ(t)τ, for tR, 0<β<1 for kN, ϱ=max{τ,h}. If α+lnβTa+θ1βN0+θ2hβN0<0, then λ>0 with the following property:

    u(t)βN0supϱs0||φ(s)||2eλ0t,t0,

    where λ0 satisfies λ0+α+lnβTa+θ1eλ0τβN0+eλ0h1λ0θ2βN0=0.

    Proof. The following comparison system is considered:

    {˙˜u(t)=α˜u(t)+θ1˜u(tτ(t))+θ2tth˜u(s)ds+ε, ttk,˜u(tk)=β˜u(tk), kN,˜u(s)=φ(s)+ε, ϱs0. (2.9)

    For any ε>0, ˜u(t) denotes the unique solution. According to Lemma 2.1, we have the inequality ˜u(t)u(t)0 holding for ϱs0. Consequently, it follows that ˜u(t)u(t) also holds for t0. Leveraging the formula for the variation of parameters, we can describe ˜u(t) as follows:

    ˜u(t)=W(t,0)˜u(0)+t0W(t,s)[θ1˜u(sτ(s))+θ2tth˜u(r)dr+ε]ds. (2.10)

    The function W(t,s) defined for allt,s0, serves as the Cauchy matrix for the subsequent linear impulsive system:

    {˙˜u(t)=α˜u(t), ttk,˜u(tk)=β˜u(tk), kN. (2.11)

    Definition 2.2 states that it can acquire the following:

    W(t,s)eα(ts)Πs<tk<tβ=eα(ts)βNζ(s,t)eα(ts)βtsTaN0=βN0e(α+lnβTa)(ts). (2.12)

    Let q=βN0supϱs0||φ(s)||2. The result of substituting (2.12) into (2.10) is as follows:

    ˜u(t)qe(α+lnβTa)t+t0βN0e(α+lnβTa)(ts)[θ1˜u(sτ(s))+θ2ssh˜u(r)dr+ε]ds, (2.13)

    Denote G(λ)=λ+α+lnβTa+θ1eλτβN0+eλh1λθ2βN0. Then, we have the following:

    G(0+)=α+lnβTa+θ1βN0+limλ0+(eλh1λθ2βN0)=α+lnβTa+θ1βN0+θ2hβN0<0.

    For any λ(0,+), it is evident that G(+)>0 and G(λ)>0. As a result, the equation G(λ)=0 admits a unique positive solution, denoted by λ0, where λ0>0.

    Since ε>0,λ0>0,α+lnβTa+θ1βN0+θ2hβN0<0 and 0<β<1, we have the following:

    ˜u(s)<q<qeλ0s+εσ0,ϱs0, (2.14)

    where ϖ=(α+lnβTa+θ1βN0+θ2hβN0)βN0.

    Next, we prove that

    ˜u(t)qeλ0t+εϖ,t>0. (2.15)

    There exists a t>0 such that, if (2.15) is false, then

    ˜u(t)>qeλ0t+εϖ (2.16)

    and

    ˜u(t)qeλ0t+εϖ, t<t. (2.17)

    Combine (2.15) with (2.17), we have the following:

    ˜u(t)qe(α+lnβTa)t+t0βN0e(α+lnβTa)(ts)θ1(qeλ0(sτ(s))+εϖ)ds+t0βN0e(α+lnβTa)(ts)θ2ssh(qeλ0r+εϖ)drds+εt0βN0e(α+lnβTa)(ts)dsqe(α+lnβTa)t+t0βN0e(α+lnβTa)(ts)θ1(qeλ0(sτ)+εϖ)ds+t0βN0e(α+lnβTa)(ts)θ2ssh(qeλ0r+εϖ)drds+εt0βN0e(α+lnβTa)(ts)dsqe(α+lnβTa)t+βN0e(α+lnβTa)tt0e(λ0+α+lnβTa)sqθ1eλ0τds+εϖt0βN0e(α+lnβTa)(ts)θ1ds+βN0e(α+lnβTa)tt0e(λ0+α+lnβTa)sqθ2eλ0h1λ0ds+εϖt0βN0e(α+lnβTa)(ts)θ2hds+εt0βN0e(α+lnβTa)(ts)dsqe(α+lnβTa)t+qe(α+lnβTa)tt0e(λ0+α+lnβTa)s(λ0αlnβTa)ds+ε(θ1+θ2h+ϖ)ϖt0βN0e(α+lnβTa)(ts)dsqe(α+lnβTa)t+qeλ0tqe(α+lnβTa)t+ε(α+lnβTa)βN0ϖβN0(α+lnβTa)(1e(α+lnβTa)t)qeλ0t+εϖ, (2.18)

    which contracts with (2.16). Therefore, (2.15) holds true.

    Let ε0; then

    u(t)˜u(t)qeλ0t=βN0supϱs0||φ(s)||2eλ0t, t0. (2.19)

    This completes the proof.

    Lemma 2.4. Let u(t)PC([ϱ,+),R) with u(t)0; for the impulsive sequence ζ={t1,t2,,tk,}, consider the following differential inequalities:

    {D+u(t)αu(t)+θ1u(tτ(t))+θ2tthv(s)ds, ttk,u(tk)βu(tk), kN,u(s)=φ(s)0,s[ϱ,0], (2.20)

    where α<0, θ1>0, θ2>0,0τ(t)τ, for tR, β1 for kN, ϱ=max{τ,h}. If α+lnβTa+θ1βN0+θ2hβN0<0, then λ>0 with the following property:

    u(t)βN0supϱs0||φ(s)||2eλ0t,t0,

    where λ0 satisfies λ0+α+lnβTa+θ1eλ0τβN0+eλ0h1λ0θ2βN0=0.

    Proof. The proof process follows a similar approach to that of Lemma 2.4, specifically involving the Cauchy matrix as follows:

    W(t,s)eα(ts)Πs<tk<tβ=eα(ts)βNζ(s,t)eα(ts)βtsTa+N0=βN0e(α+lnβTa)(ts). (2.21)

    This completes the proof.

    Remark 2.2. In [33], our focus was on the impulsive differential inequality that incorporated multiple discrete delays. Subsequently, in [37], we delved into the delayed impulsive differential inequality characterized by finite distributed delays. Furthermore, in [39], we explored the scenario where the integral term within the impulsive inequality assumed the form of a kernel function. However, this paper presents a comprehensive study of the impulsive differential inequality that encompasses both discrete delays and finite distributed delays, with no imposed constraints on the intensity of the impulse.

    The following presumptions are made throughout this paper:

    (A1) For every u1,u2R,u1u2, where Fj, j=1,2,,n are real positive constants, the activation functions fj(), where j ranges from 1 to n, are bounded functions that satisfy a specific Lipschitz condition:

    |fj(u1)fj(u2)|Fj|u1u2|; and

    (A2) β=σ((Eμ˜Rk)T(Eμ˜Rk)).

    Within this section, we explore the attainment of exponential synchronization between systems (2.1) and (2.2) through the construction of an appropriate Lyapunov functional.

    |gi(ei(t))|Fi(ei(t)), which indicates that gi() in system (2.5) is constrained from (A1). Thus, for any positive diagonal matrices A, the function g(e(t)) satisfies the following inequality:

    gT(e(t))Ag(e(t))eT(t)FTAFe(t), (3.1)

    where F=diag{F1,F2,,Fn}.

    Theorem 3.1. Assume that the assumptions (A1) and (A2) are satisfied. Then, systems (2.1) and (2.2) are exponentially synchronized if there exist real constants α>0, θ1>0, θ2>0, along with an n×nmatrix P>0, four diagonal positive definite n×nmatrix Σi>0,i=1,2,3, and an M such that the subsequent conditions are fulfilled:

    Case Ⅰ: The impulsive strength is within the range 0<β<1:

    (a1)

    Ξ=[ξ11000FTΣ2Fθ1P000Σ31hM]<0,

    where ξ11=PˆDˆDTP+PˆAΣ11ˆATP+FTΣ1F+P˜BΣ12˜BTP+P˜CΣ13˜CTPαP.

    (b1)

    FTMFθ2P<0, and

    (c1)

    α+lnβTa+θ1βN0+θ2hβN0<0.

    Case Ⅱ: The impulsive strength is within the range β1:

    The three real constants in the theorem satisfy the relation α<0, θ1>0, θ2>0, conditions (a2) and (b2) are identical to conditions (a1) and (b1) respectively, as defined in Case Ⅰ, and

    (c2)

    α+lnβTa+(θ1+θ2h)βN0<0.

    Proof. We build the subsequent Lyapunov function as follows:

    V(t)=eT(t)Pe(t), (3.2)

    where P is strictly positive definite matrix.

    ˙V(t)=2eT(t)P˙e(t)=2eT(t)P{ˆDe(t)+ˆAg(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds}=2eT(t)PˆDe(t)+2eT(t)PˆAg(e(t))+2eT(t)P˜Bg(e(tτ(t)))+2eT(t)P˜Ctthg(e(s))dseT(t)(PˆDˆDTP)e(t)+eT(t)PˆAΣ11ˆATPe(t)+gT(e(t))Σ1g(e(t))+eT(t)P˜BΣ12˜BTPe(t)+gT(e(tτ(t)))Σ2g(e(tτ(t)))+eT(t)P˜CΣ13˜CTPe(t)+[tthg(e(s))ds]TΣ3tthg(e(s))dseT(t)(PˆDˆDTP)e(t)+eT(t)PˆAΣ11ˆATPe(t)+eT(t)FTΣ1Fe(t)+eT(t)P˜BΣ12˜BTPe(t)+eT(tτ(t))FTΣ2Fe(tτ(t))+eT(t)P˜CΣ13˜CTPe(t)+[tthg(e(s))ds]TΣ3tthg(e(s))ds=eT(t)(PˆDˆDTP+PˆAΣ11ˆATP+FTΣ1F+P˜BΣ12˜BTP+P˜CΣ13˜CTP)e(t)+eT(tτ(t))FTΣ2Fe(tτ(t))+[tthg(e(s))ds]TΣ3tthg(e(s))ds. (3.3)

    According to Eqs (a1)–(c1), the following inequality is valid for all ttk, where kN.

    ˙V(t)αeT(t)Pe(t)+θ1eT(tτ(t))Pe(tτ(t))+θ2ttheT(s)Pe(t)dsαV(t)+θ1V(tτ(t))+θ2tthV(s)ds. (3.4)

    Otherwise,

    V(tk)=eT(tk)Pe(tk)=eT(tk)(Eμ˜Rk)TP(Eμ˜Rk)e(tk)σ((Eμ˜Rk)T(Eμ˜Rk))eT(tk)Pe(tk)βV(tk) (3.5)

    holds for kN.

    By integrating the conditions (a1)–(c1) with Lemma 2.3, we derive the subsequent conclusion:

    λmin(P)||eT(t)e(t)||V(t)βN0supϱs0||˜φ(s)˜ϕ(s)||2eλ0t,t0, (3.6)

    quasi,

    ||e(t)||βN0λmin(P)supϱs0||˜φ(s)˜ϕ(s)||eλ02t,t0. (3.7)

    Systems (2.1) and (2.2) exhibit an exponential synchronization, which conforms to the criteria specified in Definition 2.1.

    In a similar fashion, utilizing the constraints (a2)–(c2) in conjunction with Lemma 2.4, we can ascertain that systems (2.1) and (2.2) exhibit an exponential synchronization.

    The proof is completed.

    Replace the impulse control mentioned in Eq (2.4) with the following impulsive control

    ˜u(t)=˜Le(t)μk=1˜Rke(t)δ(ttk), (3.8)

    where the notation L=diag(l1,l2,,ln), li>0 designates the feedback control gain matrix. The impulsive gain is μ. The control gain is Rk>0.

    Remark 3.1. This kind of controller is widely used, which can be seen in [34], and the secondary controller can be used to expand the existing conclusions.

    Consider the error function e(t)=y(t)x(t), which quantifies the deviation between the outputs of networks (2.1) and (2.2). When these networks are interconnected, and the error dynamics are governed by Eq (3.8), the resulting error system is derived as outlined below:

    {de(t)dt=˜De(t)+˜Ag(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds˜Le(t), ttk,:=ˆDe(t)+˜Ag(e(t))+˜Bg(e(tτ(t)))+˜Ctthg(e(s))ds, ttk,Δe(tk)=e(t+k)e(tk)=μ˜Rke(tk), t=tk,e(t)=˜ψ(t), ϱ<t<0. (3.9)

    By repeating the previous proof process, we can obtain the following theorem:

    Theorem 3.2. Assume that the assumptions (A1) and (A2) are satisfied. Then, systems (2.1) and (2.2) are exponentially synchronized if exist real constants α>0, θ1>0, θ2>0, an n×nmatrix P>0, three diagonal positive definite n×nmatrix Σi>0,i=1,2,3, and an M such that the subsequent conditions are fulfilled:

    Case Ⅰ: The impulsive strength is within the range 0<β<1:

    (a1)

    ˆΞ=[ˆξ11000FTΣ2Fθ1P000Σ31hM]<0,

    where ˆξ11=PˆDˆDTP+P˜AΣ11˜ATP+FTΣ1F+P˜BΣ12˜BTP+P˜CΣ13˜CTPαP. (b1)

    FTMFθ2P<0, and

    (c1)

    α+lnβTa+θ1+θ2hβN0<0.

    Case Ⅱ: The impulsive strength is within the range β1:

    The three real constants in the theorem satisfy the relation α<0, θ1>0, θ2>0, conditions (a2) and (b2) are same as the conditions (a1) and (b1) in Case Ⅰ, and

    (c2)

    α+lnβTa+(θ1+θ2h)βN0<0.

    Proof. If we assume that V(t)=eT(t)Pe(t), and P is a positive integer martix, then we may show a method analogous to Theorem 3.1. The proof is completed.

    Example 4.1. Consider the following model:

    {dei(t)dt=diei(t)+2j=1aijgj(ej(t))+2j=1bijgj(ej(tτ(t))+2j=1cijtt0.9fj(ej(s))ds+k1iei(t)+k2igi(ei(t),ttk,t0ei(tk)=ei(t+k)ei(tk)=μRke(tk),t=tk, (4.1)

    where the coefficients and functions are taken as follows:

    D=[7.5006], A=[60.153.26], B=[2.40.120.262.2],
    C=[2.5002], K1=[1.5003.3], K2=[2.1002.2].
    g1(x)=g2(x)=tanh(x),  τ(t)=0.8.

    In order to see the effect of control more clearly, we first consider the situation without control, see Figure 1.

    Figure 1.  The state trajectory of the system (4.1) without control.

    Case(1). Let μ=0.9, P=E, Rk=E, tk=tk1+0.02k,kN, and β=0.01. It is easy to calculate that ϱ=0.9, Fi=1,i=1,,n, Ta=0.02,N0=1. By employing the MATLAB toolbox, we are capable of obtaining the subsequent details:

    α=150, θ1=θ2=0.1,
    Σ1=[50000300], Σ2=Σ3=[0.09000.09].

    Then, the system after the controller is made by MATLAB (Figure 2).

    Figure 2.  The state trajectory of the system (4.1) with control (0.9E).

    Case(2). Let μ=2.1, P=E, Rk=E, tk=tk1+0.5k,kN, and β=1.21. It is easy to calculate that ϱ=0.9, Fi=1,i=1,,n, Ta=0.5,N0=1. By employing the MATLAB toolbox, we are capable of obtaining the subsequent details:

    α=6, θ1=θ2=2,
    Σ1=[5000200], Σ2=Σ3=[1.9001.9]

    Then, the system after the controller is made by MATLAB (Figure 3).

    Figure 3.  The state trajectory of the system (4.1) with control (2.1E).

    Example 4.2. Consider the following model:

    {dei(t)dt=diei(t)+2j=1aijgj(ej(t))+2j=1bijgj(ej(tτ(t))+2j=1cijtt0.9fj(ej(s))dsliei(t),ttk,t0ei(tk)=ei(t+k)ei(tk)=μRke(tk),t=tk,kN, (4.2)

    where the coefficients and functions are defined as follows:

    D=[2.5002], A=[20.151.23.5], B=[1.70.120.261],
    C=[2.5002], L=[4.5005],
    g1(x)=g2(x)=12(|x+1||x1|),  τ(t)=0.8.

    In order to see the effect of control more clearly, we first consider the situation without control, see Figure 4.

    Figure 4.  The state trajectory of the system (4.2) without control.

    Case(1). Let μ=0.9, P=E, Rk=E, tk=tk1+0.04k,kN, and β=0.01. It is easy to calculate that ϱ=0.9, Fi=1,i=1,,n, Ta=0.04,N0=1. By employing the MATLAB toolbox, we are capable of obtaining the subsequent details:

    α=95, θ1=θ2=0.1,
    Σ1=[10010], Σ2=Σ3=[0.09000.09].

    Then, the system after the controller is made by MATLAB (Figure 5).

    Figure 5.  The state trajectory of the system (5.2) with control (0.9E).

    Case(2). Let μ=2.1, P=E, Rk=E, tk=tk1+0.5k,kN, and β=1.21. It is easy to calculate that ϱ=0.9, Fi=1,i=1,,n, Ta=0.5,N0=1. By employing the MATLAB toolbox, we are capable of obtaining the subsequent details:

    α=6, θ1=θ2=2,
    Σ1=[5000200], Σ2=Σ3=[1.9001.9].

    Then, the system after the controller is made by MATLAB (Figure 6).

    Figure 6.  The state trajectory of the system (4.2) with control (2.1E).

    This paper delved into the exponential synchronization challenge posed by NNs that incorporated time-varying delays alongside finite distributed delays. To tackle this, a hybrid impulsive controller was devised. Initially, two impulsive differential inequalities were rigorously proven. Subsequently, in the course of proving the main theorem, the original synchronization problem was strategically reframed into a category of impulsive differential inequalities through the application of an apt Lyapunov function. This transformation facilitated the derivation of sufficient corresponding conditions that leveraged lemmas. Ultimately, the validity and efficacy of the obtained conclusions were showcased through two illustrative numerical examples which focused on error analysis.

    The attained conclusions affirmed the system's attainment of objectives, yet post-achievement, the control process persisted in the resource exhaustion. Consequently, contemplating a novel impulsive control strategy is advisable to halt the control upon the goal fulfillment. Furthermore, the model overlooked network couplings, which hindered its applicability to broader contexts.

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

    This work was supported by the National Natural Science Foundation of China under Grant 61573010, the Opening Project of Sichuan Province University Key Laboratory of Bridge Non-Destruction Detecting and Engineering Computing under Grant 2021QYJ06.

    The authors declare there is no conflicts of interest.



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