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Research article

Lag synchronization of complex-valued interval neural networks via distributed delayed impulsive control

  • Received: 21 October 2022 Revised: 27 November 2022 Accepted: 04 December 2022 Published: 19 December 2022
  • MSC : 34D06, 92B20, 93C27

  • This paper investigates the lag synchronization problem of complex-valued interval neural networks with both discrete and distributed time-varying delays under delayed impulsive control. A distributed delayed impulsive controller that depends on the accumulation of the states over a history time period is designed to guarantee the exponential lag synchronization between the drive and the response systems. By employing the complex Lyapunov method and a novel impulsive differential inequality technique, some delay-dependent synchronization criteria are established in terms of complex-valued linear matrix inequalities (LMIs). Finally, a numerical example is given to illustrate the effectiveness of the theoretical results.

    Citation: Zhifeng Lu, Fei Wang, Yujuan Tian, Yaping Li. Lag synchronization of complex-valued interval neural networks via distributed delayed impulsive control[J]. AIMS Mathematics, 2023, 8(3): 5502-5521. doi: 10.3934/math.2023277

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  • This paper investigates the lag synchronization problem of complex-valued interval neural networks with both discrete and distributed time-varying delays under delayed impulsive control. A distributed delayed impulsive controller that depends on the accumulation of the states over a history time period is designed to guarantee the exponential lag synchronization between the drive and the response systems. By employing the complex Lyapunov method and a novel impulsive differential inequality technique, some delay-dependent synchronization criteria are established in terms of complex-valued linear matrix inequalities (LMIs). Finally, a numerical example is given to illustrate the effectiveness of the theoretical results.



    In recent years, neural networks (NNs) have been extensively investigated due to their wide applications in many areas, such as signal processing, fault diagnosis, combinatorial optimization, pattern recognition, and so on [1,2,3]. Compared with real-valued neural networks (RVNNs), complex-valued neural networks (CVNNs) have more complex characteristics, which can simulate more practical situations and deal with some problems that RVNNs cannot solve, such as XOR problem, symmetry detection, electromagnetic wave imaging, etc. [4,5,6]. Moreover, due to the inherent information transmission between neurons and the finite switching speed of actuators in NNs, time delays are always inevitable, which may lead to undesirable dynamical behaviors and seriously affect the performance of the systems [7,8]. Consequently, the study of CVNNs with time delays has become an active research topic and some significative results have been reported in [9,10].

    Synchronization, as a significant dynamic index of NNs, has received great attention because of its potential applications. Up to now, a wide variety of synchronization phenomena have been investigated, including finite-time synchronization[11], cluster synchronization [12], projective synchronization [13], lag synchronization [14] and others. In particular, lag synchronization is characterized as the coincidence of the states of two coupled systems in which one of the systems is delayed by a given finite time, and it has been proved to be a reasonable strategy from the viewpoint of engineering applications in secure communication and parallel image processing. However, it is worth noting that the existing results on lag synchronization mainly focus on RVNNs. There are few reports on the lag synchronization problem of CVNNs. On the other hand, because of the complex topology of NNs, appropriate external controllers are needed to realize synchronization, such as feedback control [15], adaptive control [16], intermittent control [17], impulsive control [18,19], and so on. Among them, impulsive control has been widely used in control areas due to its lower control cost, higher confidentiality and stronger robustness [20]. Some interesting works on the impulsive synchronization problem of delayed CVNNs have been proposed in recent years. The global exponential synchronization of complex-valued memristor-based NNs with time-varying delays was investigated via impulsive control in [21]. Under hybrid impulsive controllers, [22] gave the results of the exponential synchronization for drive-response time-varying delayed CVNNs. In [23], some sufficient conditions were obtained for the exponential synchronization of CVNNs with time-varying delays by an impulsive controller. In fact, it is hard to require the process of sampling, processing, and transferring impulse information to achieve immediately [24,25]. Hence, delayed impulsive control is perceived as a better way to model many practical problems. In [26], authors investigated the synchronization problem of CVNNs via a delayed pinning impulsive controller. By designing a delayed impulsive control scheme, some new sufficient conditions for the exponential synchronization of complex-valued complex dynamical networks with multiple time-varying delays were obtained in [27]. However, the delayed impulsive controllers in the above mentioned literatures only considered discrete delays, not distributed ones. The distributed delayed impulsive control, as another type of delayed impulsive control, can stabilize a system based on the accumulation of the states over a history time period, which is more applicable for many industrial and biological systems such as network connection, the spread of disease and epidemic model [28,29,30]. To our best knowledge, such impulsive control has not been studied for the synchronization problem of CVNNs.

    As we know, since NNs have many parallel pathways with different axon sizes and lengths, delays may be distributed during a certain time period [31,32,33]. Therefore, besides discrete delays, distributed delays should be also incorporated in the models. In addition, model errors and parameter fluctuations are unavoidable in the modeling process of CVNNs, which will lead to poor performance and asynchronization of the systems [34]. It is very significant to study interval NNs whose parameters values are unknown but bounded in given compact sets [35,36]. However, there are very few developed achievements on the synchronization problem of complex-valued interval NNs with mixed delays, especially with distributed delayed impulsive control, which motivates our present study. Moreover, to deal with complex variables in CVNNs, the method of separating real-imaginary parts was extensively used in most of the existing literatures. Nevertheless, an explicit separation of complex-valued activation functions of CVNNs into their real and imaginary parts is needed when applying this kind of method, which may cause the theoretical results to be more conservative and disheveled. Therefore, how to take the model as a whole to develop theoretical results in complex domain for the synchronization of CVNNs with mixed delays and uncertain parameters is a very interesting and challenging work.

    Based on the above discussions, this paper aims to investigate the exponential lag synchronization for complex-valued interval neural networks with both discrete and distributed delays via delayed impulsive control. The main contributions in our work can be summarized as follows: (ⅰ) The model of CVNNs under discussion is quite comprehensive, which takes mixed time-delays and uncertain parameters into simultaneous consideration. (ⅱ) To realize lag synchronization of the drive and the response systems, a distributed delayed impulsive controller that depends on the accumulation of the states over a history time period is designed. (ⅲ) A novel impulsive differential inequality is employed to deal with the mathematical difficulty caused by mixed time-delays and distributed delayed impulses, which makes our results less conservative than the existing ones. (ⅳ) Instead of the separation approach, a uniform research framework in complex domain is developed and some synchronization criteria are derived in the form of complex-valued LMIs, which are easily checked by using the Matlab LMI toolbox. The rest of this paper is organized as follows. Model description and preliminaries are introduced in Section 2. The main results are obtained in Section 3. Section 4 provides an example to verify the validity of the derived results. The summary of this paper is given in Section 5.

    Notations. Let C, Cn and Cn×n be the set of complex numbers, n-dimensional complex space and n×n-dimensional complex space, respectively. Correspondingly, let R, Rn, Rn×n and Rn2×n2 denote the set of real numbers, n-dimensional real space, n×n-dimensional real space and n2×n2-dimensional real space, respectively. The set of positive integers is denoted by Z+. For a matrix A, A>0 (A<0, A0, A0) denotes that A is a positive definite (negative definite, positive semi-definite, negative semi-definite) matrix, λmax(A) (λmin(A)) stands for the maximum (minimum) eigenvalue of matrix A, A1 represents the inverse of A and A means the conjugate transpose of A. Unless otherwise specified, I is the identity matrix with appropriate dimensions. The maximum value of α and β is defined as αβ. Let i be the imaginary, i.e., i=1. Re(x) and Im(x) denote the real part and the imaginary part of a number xC. For x, yC, xy means that Re(x)Re(y) and Im(x)Im(y). x=xx, where x is the conjugate transpose of x. ¯x represents the conjugate of x. For any JR and SCk(1kn,kZ+), set PC(J,S)={φ:JS is continuous everywhere except at a finite number of points t, at which φ(t+),φ(t) exist and φ(t)=φ(t+)}. φρ=supt[ρ,0]φ(t). is the conjugate transpose of a suitable block in a Hermitian matrix and Λ={1,2,,n},nZ+ is an index set.

    In this paper, we consider the following complex-valued interval neural networks :

    {˙x(t)=Cx(t)+Af(x(t))+Bf(x(tτ(t)))+Dttβ(t)f(x(s))ds+J(t),t>0,x(t)=ϕ(t),t[ρ1,0], (2.1)

    where x(t)=(x1(t),,xn(t))TCn is the state vector of the complex-valued interval neural networks; f(x())=(f1(x1()),,fn(xn()))TCn is the neuron activation function; C=diag{c1,c2,,cn}Rn×n denotes the self-feedback connection weight matrix with cj>0,jΛ; A, B and DCn×n are the connection weight matrices; J(t)Cn is an external input vector; τ(t) is discrete delay and β(t) is distributed delay satisfying 0τ(t)τ and 0β(t)β, where τ and β are constants; ϕ()PC([ρ1,0],Cn) is the initial condition for ρ1=τβ.

    Throughout this paper, we make the following assumptions.

    Assumption 1. For all u, vC, there exists a positive diagonal matrix L=diag{L1,L2,,Ln}, LjR, jΛ, such that

    fj(u)fj(v)∥≤Ljuv.

    Assumption 2. Matrices C, A, B and D in the model (2.1) are bounded in the following intervals

    CCI,AAI,BBI,DDI,

    where

    CI=[ˇC,ˆC]={diag(cj)|0<ˇcjcjˆcj;jΛ},AI=[ˇA,ˆA]={(apq)n×n|ˇapqapqˆapq;p,qΛ},BI=[ˇB,ˆB]={(bpq)n×n|ˇbpqbpqˆbpq;p,qΛ},DI=[ˇD,ˆD]={(dpq)n×n|ˇdpqdpqˆdpq;p,qΛ},

    with ˇC=diag(ˇc1,,ˇcn), ˆC=diag(ˆc1,,ˆcn), ˇA=(ˇapq)n×n, ˆA=(ˆapq)n×n, ˇB=(ˇbpq)n×n, ˆB=(ˆbpq)n×n, ˇD=(ˇdpq)n×n and ˆD=(ˆdpq)n×n.

    We refer to system (2.1) as the drive system, and the corresponding response system is characterized by

    {˙y(t)=Cy(t)+Af(y(t))+Bf(y(tτ(t)))+Dttβ(t)f(y(s))ds+u(t)+J(t),t>α,y(t)=φα(t),t[ρ1,0], (2.2)

    where φα(t)=φ(α+t), t[ρ1,0], φα(t)PC([ρ1,0],Cn), where α>0 is response time delay between the drive system (2.1) and the response system (2.2), and u(t) is the control input that needs to be designed.

    To achieve lag synchronization between the drive system (2.1) and the response system (2.2), a class of distributed delayed impulsive controller can be given as follows

    u(t)=n=1(Kttrke(s)dse(t))δ(ttk),kZ+, (2.3)

    where rk are the distributed delays satisfying 0rkr with r is a constant; e(t)=y(t)x(tα) is the lag synchronization error for α<ρ and ρ=τβr; δ() is the Dirac delta function; KCn×n is a gain matrix to be designed. Then, one can obtain the following error system

    {˙e(t)=Ce(t)+Ah(e(t))+Bh(e(tτ(t)))+Dttβ(t)h(e(s))ds,t>α,e(t)=Kttrke(s)ds,t=tk,e(t)=φα(t)ϕ(t),t[ρ,0], (2.4)

    where h(e(t))=f(y(t))f(x(tα)), h(e(tτ(t)))=f(y(tτ(t)))f(x(tατ(t))).

    Furthermore, let

    L{diag(δ11,,δ1n,,δn1,,δnn)Rn2×n2;|δpq|1,p,qΛ},
    C0=ˆC+ˇC2,A0=ˆA+ˇA2,B0=ˆB+ˇB2,D0=ˆD+ˇD2,
    HC=ˆCˇC2=diag(γ1,,γn),HA=ˆAˇA2=(αpq)n×n,HB=ˆBˇB2=(βpq)n×n,HD=ˆDˇD2=(ηpq)n×n,

    where C0, A0, B0 and D0 are reference matrices of interval matrices C, A, B and D, respectively. Define

    Θ1=[γ1ϵ1,,0,0,γ2ϵ2,,0,,0,,γnϵn]n×n2,Θ2=[α11ϵ1,,α1nϵ1,,αn1ϵn,,αnnϵn]n×n2,Θ3=[β11ϵ1,,β1nϵ1,,βn1ϵn,,βnnϵn]n×n2,Θ4=[η11ϵ1,,η1nϵ1,,ηn1ϵn,,ηnnϵn]n×n2,Φ1=[γ1ϵ1,,0,0,γ2ϵ2,,0,,0,,γnϵn]Tn2×n,Φ2=[¯α11ϵ1,,¯α1nϵn,,¯αn1ϵ1,,¯αnnϵn]n2×n,Φ3=[¯β11ϵ1,,¯β1nϵn,,¯βn1ϵ1,,¯βnnϵn]n2×n,Φ4=[¯η11ϵ1,,¯η1nϵn,,¯ηn1ϵ1,,¯ηnnϵn]n2×n,

    where ϵjRn,jΛ represents the jth unit column vector. Then the system (2.4) can be rewritten as

    {˙e(t)=[C0+Θ1Δ1Φ1]e(t)+[A0+Θ2Δ2Φ2]h(e(t))+[B0+Θ3Δ3Φ3]h(e(tτ(t)))+[D0+Θ4Δ4Φ4]ttβ(t)h(e(s))ds,t>0,e(t)=Kttrke(s)ds,t=tk,e(t)=φα(t)ϕ(t),t[ρ,0],

    which is equivalent to

    {˙e(t)=C0e(t)+A0h(e(t))+B0h(e(tτ(t)))+D0ttβ(t)h(e(s))ds+ΘΨe(t),ttk,e(t)=Kttrke(s)ds,t=tk,e(t)=φα(t)ϕ(t),t[ρ,0], (2.5)

    where Θ=[Θ1,Θ2,Θ3,Θ4]n×4n2, ΔjL, j=1, 2, 3, 4,

    Ψe(t)=(Δ1Φ10000Δ2Φ20000Δ3Φ30000Δ4Φ4)4n2×4n×(e(t)h(e(t))h(e(tτ(t)))ttβ(t)h(e(s))ds)4n×1.

    Remark 1. The robust stability of complex-valued interval neural networks has been studied in [9], where the interval parameters are processed by dividing them into real and imaginary parts. Here, without the separation method, we directly use matrix transformations in the complex field to deal with the interval parameter uncertainties.

    Based on the above analysis and description, the following definitions and lemmas are needed.

    Definition 1 ([37]). If sequence {tk, kZ+} satisfies

    0t0<t1<<tkwithtk+ask+,

    then A0={tk} is called impulse time sequence. Furthermore, for any constant ζ>0, define Aζ as the set of impulse time sequences in A0 such that tktk1ζ, kZ+.

    Definition 2 ([38]). The drive-response system (2.1) and (2.2) are said to be exponentially lag synchronized under the impulse set Aζ, if there exist constants M1 and ε>0 such that

    y(t)x(tα)Mφαϕρexp(ε(tα)),tα,

    where φα,ϕPC([ρ,0],Cn), and ε is called the degree of exponential lag synchronization.

    Lemma 1 ([39]). Consider the following impulsive differential inequality,

    {D+g(t)σ1g(t)+σ2ˉg(t),ttk,g(t)μkttrkg(s)ds,t=tk, (2.6)

    where D+ is the right-upper Dini derivative, gPC(R,R+), ˉg(t)=sups[tρ,t]g(s). If there exist constants σ1R, σ2>0, μk>0, kZ+, ζ>0 and δ>1, such that the following conditions hold:

    σ1+σ2δ<lnδζ, (2.7)
    infkZ+{ln(μkrkδ)rk}=η>0, (2.8)

    then the solution of the inequality (2.6) over the set Aζ satisfies

    g(t)δˉg(0)exp(λt),t0,

    where λ(0,η) is a positive constant satisfying θ(λ)>0 for θ(λ)=lnδζσ1σ2δexp(ρλ)λ.

    Lemma 2 ([40]). For any positive definite Hermitian matrix ECn×n, any function u(s):[a,b]Cn with scalars a<b such that the integrals concerned are well defined, then

    (bau(s)ds)Ebau(s)ds(ba)bau(s)Eu(s)ds.

    Lemma 3 ([26]). For any vector x, yCn and positive definite Hermitian matrix RCn×n, it holds that

    xy+yxxRx+yR1y.

    In this section, with the help of the Lyapunov method and the delayed impulsive differential inequality technique, we get some criteria of exponential lag synchronization of complex-valued interval neural networks by designing the distributed delayed impulsive controller.

    Theorem 1. Under Assumption 1 and Assumption 2, if there exist constants σ1R, σ2>0, ζ>0, δ>1, 0<μ<1 and positive definite Hermitian matrix P, positive diagonal matrices QjRn×n (j=1,2,3), QjRn2×n2 (j=4,5,6,7), matrix ZCn×n such that (2.7) and the following inequalities hold

    (Ω11PA0PB0PD0PΘQ1000Q200Q30(Q40000Q50000Q60000Q7))0, (3.1)
    (PδrZP)<0, (3.2)
    L(Q2Φ3Q6Φ3)Lμσ2P, (3.3)
    β2L(Q3Φ4Q7Φ4)L(1μ)σ2P, (3.4)

    where Ω11=PC0C0Pσ1P+LQ1L+Φ1Q4Φ1+LΦ2Q5Φ2L, then the drive system (2.1) and the response system (2.2) are exponentially lag synchronized over the set A(ζ) with control gain

    K=P1Z.

    Proof. Choose the Lyapunov function

    V(t)=e(t)Pe(t). (3.5)

    Taking the derivative of V(t) along the trajectory of the system (2.5) on t[tk1,tk), kZ+, we have

    D+V(t)=˙e(t)Pe(t)+e(t)P˙e(t)=e(t)(PC0+C0P)e(t)+e(t)PA0h(e(t))+h(e(t))A0Pe(t)+e(t)PB0h(e(tτ(t)))+h(e(tτ(t)))B0Pe(t)+e(t)PD0ttβ(t)h(e(s))ds+ttβ(t)h(e(s))dsD0Pe(t)+e(t)PΘΨe(t)+Ψe(t)ΘPe(t)

    By Lemma 3 and Assumption 1,

    D+V(t)e(t)(PC0+C0P)e(t)+e(t)PA0Q11A0Pe(t)+h(e(t))Q1h(e(t))+e(t)PB0Q12B0Pe(t)+h(e(tτ(t)))Q2h(e(tτ(t)))+e(t)PD0Q13D0Pe(t)+ttβ(t)h(e(s))dsQ3ttβ(t)h(e(s))ds+e(t)PΘΨe(t)+Ψe(t)ΘPe(t)e(t)(PC0+C0P)e(t)+e(t)PA0Q11A0Pe(t)+e(t)LQ1Le(t)+e(t)PB0Q12B0Pe(t)+e(tτ(t))LQ2Le(tτ(t))+e(t)PD0Q13D0Pe(t)+ttβ(t)h(e(s))dsQ3ttβ(t)h(e(s))ds+e(t)PΘΨe(t)+Ψe(t)ΘPe(t). (3.6)

    Applying Lemma 3 again to the last term of inequality (3.6), it can be seen that

    e(t)PΘΨe(t)+Ψe(t)ΘPe(t)e(t)PΘ(Q140000Q150000Q160000Q17)ΘPe(t)+Ψe(t)(Q40000Q50000Q60000Q7)Ψe(t) (3.7)

    Moreover, according to the definition of Ψe(t), we can derive that

    Ψe(t)(Q40000Q50000Q60000Q7)Ψe(t)=(e(t)h(e(t))h(e(tτ(t)))ttβ(t)h(e(s))ds)×(Φ1Δ1Q4Δ1Φ10000Φ2Δ2Q5Δ2Φ20000Φ3Δ3Q6Δ3Φ30000Φ4Δ4Q7Δ4Φ4)×(e(t)h(e(t))h(e(tτ(t)))ttβ(t)h(e(s))ds)e(t)Φ1Q4Φ1e(t)+h(e(t))Φ2Q5Φ2h(e(t))+h(e(tτ(t)))Φ3Q6Φ3h(e(tτ(t)))+(ttβ(t)h(e(s))ds)Φ4Q7Φ4(ttβ(t)h(e(s))ds)e(t)Φ1Q4Φ1e(t)+e(t)LΦ2Q5Φ2Le(t)+e(tτ(t))LΦ3Q6Φ3Le(tτ(t))+(ttβ(t)h(e(s))ds)Φ4Q7Φ4(ttβ(t)h(e(s))ds). (3.8)

    It follows from (3.6)-(3.8) that

    D+V(t)e(t){PC0C0Pσ1P+LQ1L+Φ1Q4Φ1+LΦ2Q5Φ2L+PA0Q11A0P+PB0Q12B0P+PD0Q13D0P+PΘ(Q140000Q150000Q160000Q17)ΘP}e(t)+e(tτ(t))[LQ2L+LΦ3Q6Φ3L]e(tτ(t))+σ1e(t)Pe(t)+(ttβ(t)h(e(s))ds)(Φ4Q7Φ4+Q3)(ttβ(t)h(e(s))ds). (3.9)

    Next, we deal with the last two terms of the above inequality. From (3.3), we have

    e(tτ(t))[LQ2L+LΦ3Q6Φ3L]e(tτ(t))μσ2e(tτ(t))Pe(tτ(t))μσ2sups[tρ,t]e(s)Pe(s). (3.10)

    Based on Lemma 2, Assumption 1 and (3.4), we get

    (ttβ(t)h(e(s))ds)(Φ4Q7Φ4+Q3)(ttβ(t)h(e(s))ds)β(t)ttβ(t)h(e(s))(Φ4Q7Φ4+Q3)h(e(s))dsβ(t)ttβ(t)e(s)L(Φ4Q7Φ4+Q3)Le(s)dsβ2sups[tρ,t]e(s)[LQ3L+LΦ4Q7Φ4L]e(s)(1μ)σ2sups[tρ,t]e(s)Pe(s). (3.11)

    Applying the Schur complement lemma to (3.1), together with (3.9) (3.11), we can obtain

    D+V(t)σ1V(t)+σ2ˉV(t).

    On the other hand, at t=tk, kZ+, we have

    V(tk)=e(tk)Pe(tk)=(tktkrke(s)ds)KPK(tktkrke(s)ds)rktktkrke(s)KPKe(s)ds. (3.12)

    Meanwhile, it follows from (3.2) that there exists a constant ˜δ>δ such that P˜δ+r2KPK0. Then,

    KPKPr2˜δPr2k˜δ.

    It can be obtained that

    V(tk)μktktkrke(s)Pe(s)ds=μktktkrkV(s)ds,

    where μk=1rk˜δ. Noting that μkrkδ=δ˜δ<1, we have

    infkZ+{ln(μkrkδ)rk}=ln˜δδr>0.

    Therefore, the conditions of Lemma 1 are satisfied and we get

    V(t)δ¯V(0)exp(λt)<δλmax(P)φαϕ2ρexp(λ(tα)),tα,

    where λ(0,ln˜δδr). From (3.5), one can derive that

    V(t)λmin(P)e(t)2=λmin(P)y(t)x(tα)2,tα.

    Hence,

    y(t)x(tα)Mφαϕρexp(λ2(tα)),tα,

    where M=(δλmax(P)λmin(P))12. This means that the drive system (2.1) is exponentially lag synchronized with the response system (2.2) over the set A(ζ), which completes the proof.

    Remark 2. Recently, there have been a lot of interesting works on the impulsive control synchronization of CVNNs [21,22,23,26]. However, these results are concerned with either delay-independent impulsive control or delayed impulsive control involving discrete delays. In this paper, the distributed delayed impulsive control is proposed to synchronize the driver and response systems. It is an important type of delayed impulsive control that can be employed to stabilize a system based on the accumulation of the states over a history time period, not just the states at certain history instant. This feature enables the distributed delayed impulsive control to be more applicable for many industrial and biological systems such as network connection [28], the spread of disease [29] and epidemic model [30].

    Remark 3. It should be mentioned that three types of delays τ(t), β(t) and rk are involved in the closed-loop systems (2.5), which brings certain difficulties to the research. In Theorem 1, a novel impulsive differential inequality combined with Lyapunov function is adopted to overcome these difficulties. The obtained results require neither the differentiability of time-varying delays nor the restriction on the relationship between delays τ(t), β(t) and rk, which makes our results posses better applications.

    Remark 4. By the separation approach, the impulsive control synchronization problem for CVNNs has been discussed in [10,21,22,41]. However, this kind of approach is invalid when the activation functions cannot be divided into their real parts and imaginary parts in an analytical form. Here, instead of the separation approach, we retain the complex nature of NNs and explore the synchronization criteria by utilizing the Lyapunov function in the complex field. Only the Lipschitz condition on the activation functions is assumed, which broadens the applications of our results.

    Remark 5. In [10,26,41,42], the synchronization of delayed CVNNs have been investigated via impulsive control. While in this paper, using a different impulsive control scheme, we extend the previous results from the following aspects: Firstly, the mixed time-delays in the models and the distributed delays in the impulsive controller are considered simultaneously in our work. Secondly, by introducing a novel differential inequality with the distributed delayed impulsive effects, the synchronization conditions are obtained in terms of complex-valued LMIs, which are less conservative than the existing ones. Finally, to govern more general real-world applications, the influence of interval parameter uncertainties and the lag effects of signal transmission during synchronization are also considered in our models.

    Remark 6. It can be observed from Theorem 1 that the size of delays rk may affect the convergence rate of synchronization. As the delays rk increase, the convergence speed of synchronization will become slower.

    If the system considered only contains discrete time-delays, i.e. D=0 in the system (2.1), we have the following corollary.

    Corollary 1. Under Assumption 1 and Assumption 2, if there exist constants σ1R, σ2>0, ζ>0, δ>1, 0<μ<1 and positive definite Hermitian matrix P, positive diagonal matrices QjRn×n (j=1,2), QjRn2×n2 (j=4,5,6), matrix ZCn×n such that (2.7), (3.2), (3.3) and the following inequalities hold

    (Ω11PA0PB0PΘQ100Q20(Q4000Q5000Q6))0,

    then the drive system (2.1) and the response system (2.2) are exponentially lag synchronized over the set A(ζ) with control gain

    K=P1Z.

    In particular, if C, A, B and D are known constant matrices in the system (2.1), then we can get the following corollary based on Theorem 1.

    Corollary 2. Under Assumption 1, if there exist constants σ1R, σ2>0, ζ>0, δ>1, 0<μ<1, and positive definite Hermitian matrix P, positive diagonal matrices QjRn×n (j=1,2,3), matrix ZCn×n such that (2.7) and the following inequalities hold

    (Ω11PAPBPDQ100Q20Q3)0,
    (PδrZP)<0,
    LQ2Lμσ2P,
    β2LQ3L(1μ)σ2P,

    where Ω11=PCCPσ1P+LQ1L, then the drive system (2.1) and the response system (2.2) are exponentially lag synchronized over the set A(ζ) with control gain

    K=P1Z.

    In this section, a numerical example is given to verify the effectiveness of our main results.

    Consider the complex-valued interval networks (2.1) with the following parameters:

    C([1,1.2]00[0.8,1.2]),
    A([0.90.01i,1.1+i][0.20.01i,0.01i][65.2i,40.03i][30.03i,3.2+2.1i]),
    B([1.20.01i,1.5+1.3i][0.20.1i,0.04i][0.20.1i,0.04i][4.23.8i,3.3+0.14i]),
    D([0.50.45i,0.4+0.17i][10.5i,0.1i][43i,2+1.3i][3.53.41i,3.3+0.22i]),

    and the initial conditions ϕ1(t)=1+i, ϕ2(t)=1i, t[0.4,0]. Select the activation functions f1(s)=f2(s)=tanh(Re(s))+itanh(Im(s)), time-delays τ(t)=0.390.01sin(t), β(t)=0.38+0.01cos(t) and the external input J=(0,0)T. The initial conditions in the response system (2.2) are chosen as φα1(t)=1.51.5i, φα2(t)=2+2i, t[0.4,0]. Then it is easy to obtain that L=I2×2,

    C0=(1.1001), A0=(1+0.495i0.152.615i3.1+1.035i),
    B0=(1.35+0.645i0.10.03i0.10.03i3.751.83i), D0=(0.450.14i0.50.2i30.85i3.41.595i),
    Θ1=(0.10000000.2),
    Θ2=(0.5544+0.4554i0.3166+0.0158i00001.3733+0.9412i0.7647+0.6963i),
    Θ3=(0.6411+0.5109i0.3332+0.105i00000.3332+0.105i1.1115+0.8862i),
    Θ4=(0.4266+0.3633i0.7359+0.2038i00001.2983+0.828i0.9792+0.9268i),
    Φ1=(0.10000000.2)T,
    Φ2=(0.55440.4554i01.37330.9412i000.31660.0158i00.76470.6963i),
    Φ3=(0.64110.5109i00.33320.105i000.33320.105i01.11150.8862i),
    Φ4=(0.42660.3633i01.29830.828i000.73590.2038i00.97920.9268i).

    We consider the control input u(t) with distributed delay rk=0.4 and impulsive interval tk+1tk=0.03, kZ+. Choose σ1=70.3, σ2=92, δ=2.65, μ=0.8, β=0.39, ρ=0.4 and α=0.2. Based on Theorem 1 and Matlab LMI toolbox, the following feasible solutions can be obtained

    P=(0.0557000.0535), Q1=(1.0153001.0153),
    Q2=(1.1931001.1931), Q3=(1.0285001.0285),
    Q4=(1.080200001.080200001.080200001.0802),
    Q5=(0.816700000.816700000.816700000.8167),
    Q6=(1.03100001.03100001.03100001.031),
    Q7=(1.015700001.015700001.015700001.0157),
    Z=(0.01670.0006i0.00130.0053i0.00730.0028i0.02140.0059i).

    Then impulsive control gain matrix K is designed as follows

    K=P1Z=(0.3+0.01i0.13+0.05i0.025+0.1i0.4+0.11i).

    Take C=C0, A=A0, B=B0, D=D0. When the control input u(t)=0, we can see that the drive system (2.1) and the response system (2.2) cannot achieve exponential lag synchronization from Figure 1, Figure 3 and Figure 5. Under the distributed delayed impulsive control, when α=0.2, the state trajectories of the real parts and the imaginary parts of vectors x and y are illustrated separately in Figure 2 and Figure 4, while the state trajectories of the error system (2.5) is shown in Figure 6. According to the above simulation results, it can be clearly seen that the drive system (2.1) and the response system (2.2) can be exponentially lag synchronized by an appropriate delayed impulsive controller over the set Aξ (ξ=0.03).

    Figure 1.  State trajectories of real parts of the drive system (2.1) and the response system (2.2) without impulsive control.
    Figure 2.  State trajectories of real parts of the drive system (2.1) and the response system (2.2) with impulsive control (α=0.2).
    Figure 3.  State trajectories of imaginary parts of the drive system (2.1) and the response system (2.2) without impulsive control.
    Figure 4.  State trajectories of imaginary parts of the drive system (2.1) and the response system (2.2) with impulsive control (α=0.2).
    Figure 5.  State trajectories of real parts and imaginary parts of the error system (2.5) without impulsive control.
    Figure 6.  State trajectories of real parts and imaginary parts of the error system (2.5) with impulsive control (α=0.2).

    In this paper, the exponential lag synchronization of complex-valued interval neural networks has been investigated under distributed delayed impulsive control. Both discrete and distributed time-varying delays were considered in the model, which is more general than the previous works. A new impulsive differential inequality was applied to resolve the difficulties caused by the mixed time-delays and distributed delayed impulse effects. Instead of the separation approach, some synchronization criteria were derived based on the complex Lyapunov method, where only the Lipschitz condition on the activation functions need to be assumed. All the synchronization criteria were formulated in the form of complex-valued LMIs, which were easily checked by using the Matlab LMI toolbox. Finally, a numerical example was given to illustrate the validity of the proposed results. In the future, we will consider finite-time synchronization problem of complex-valued interval neural networks via delayed impulsive control.

    This work is supported by National Natural Science Foundation of China (62173215), Major Basic Research Program of the Natural Science Foundation of Shandong Province in China (ZR2021ZD04, ZR2020ZD24) and National Natural Science Foundation of China (11501333).

    The authors declare no conflict of interest.



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