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Research article

Synchronizations of fuzzy cellular neural networks with proportional time-delay

  • Received: 01 March 2021 Accepted: 12 July 2021 Published: 23 July 2021
  • MSC : 03E72, 34D20, 43D06, 68T07, 93D40

  • In this article, finite-time and fixed-time synchronizations (FFTS) of fuzzy cellular neural networks (FCNNs) with interaction and proportional delay terms have been investigated. The synchronizations of FCNNs are achieved with the help of p-norm based on the inequalities defined in Lemmas 2.1 and 2.2. The analysis of the method with some useful criteria is also used during the study of FFTS. Under the Lyapunov stability theory, FFTS of fuzzy-based CNNs with interaction and proportional delay terms can be achieved using controllers. Moreover, the upper bound of the settling time of FFTS is obtained. In view of settling points, the theoretical results on the considered neural network models of this article are more general as compared to the fixed time synchronization (FTS). The effectiveness and reliability of the theoretical results are shown through two numerical examples for different particular cases.

    Citation: Ankit Kumar, Subir Das, Vijay K. Yadav, Rajeev, Jinde Cao, Chuangxia Huang. Synchronizations of fuzzy cellular neural networks with proportional time-delay[J]. AIMS Mathematics, 2021, 6(10): 10620-10641. doi: 10.3934/math.2021617

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  • In this article, finite-time and fixed-time synchronizations (FFTS) of fuzzy cellular neural networks (FCNNs) with interaction and proportional delay terms have been investigated. The synchronizations of FCNNs are achieved with the help of p-norm based on the inequalities defined in Lemmas 2.1 and 2.2. The analysis of the method with some useful criteria is also used during the study of FFTS. Under the Lyapunov stability theory, FFTS of fuzzy-based CNNs with interaction and proportional delay terms can be achieved using controllers. Moreover, the upper bound of the settling time of FFTS is obtained. In view of settling points, the theoretical results on the considered neural network models of this article are more general as compared to the fixed time synchronization (FTS). The effectiveness and reliability of the theoretical results are shown through two numerical examples for different particular cases.



    The chaotic systems have become interesting topic among the researchers, scientists and engineers during last few years. In dynamical system, chaotic character is introduced by highly sensitivity to its initial conditions with variations of parameters. Chua and Yang [1] have first introduced cellular neural networks (CNNs). At that time basic CNN was structured in three types, first one is the traditional CNN [1] and it explains analogical computational network along with analog weights, states, inputs and outputs. Second one is CNN with delay term [2], which is slightly different from traditional CNN consists of delayed weights with inputs, outputs states and analogue weights and last one is the CNN in discrete-time [3] which includes analog weights, inputs, digital outputs and states. Due to immense applications in the areas of image processing, classification of patterns, quadratic optimization, associative memories, those have been broadly introduced by the researchers. Yang and Yang [4] have studied forward FCNNs, which link fuzzy logic into CNN and maintain all aspects and local connectedness among cells. So far, some different types of synchronization schemes on fuzzy neural networks and also control of the same networks have been introduced, viz., finite-time synchronization, adaptive control, lag and exponential lag synchronization, etc. [5,6,7]. Duan et al.[8] have considered discontinuous activation functions to show synchronization in finite-time of time-delayed FCNNs and Tang et al.[9] have also studied non-chattering quantized controllers for finite-time cluster synchronization of FCNNs. Abdurahman et al.[10] have shown synchronization in finite-time for FCNNs which include the time-varying delay terms, using finite-time stability theory. Mani et al.[11] have considered the adaptive control of fuzzy chaotic CNNs in fractional order and also showed its applications in image encryption. Based on the Lyapunov method and graph theory, the finite-time synchronization criteria have been obtained for FCNNs with stochastic perturbations and mixed delays by constructing appropriate state feedback controllers in [12]. The FCNN has fuzzy logic between its templates of input and output. It has potential applications in pattern recognition and image processing. Therefore, it is very important to analyze dynamical behaviors, stability analysis and synchronization of FCNNs in the aspects of theoretical and application points of view. The study of dynamical behavior of synchronization of FCNNs is also important. In the last few years, in the area of the neural network and other applied dynamical systems, many researchers have studied the stability problems [13,14,15,16,17,18,19,20].

    The stability analysis for a neural network is also employed in synchronization problems. So the synchronization problems of neural networks are often changed to a the stability problem of a error system, which is obtained from master and response systems. Synchronization of the neural networks model is addressed to the synchronization of the master-response chaotic systems having different initial values and it was first investigated by Pecora and Carroll [21]. In the literature review, it is found that a few researchers have studied stability and synchronization analyses for some different problems, viz. [22,23,24,25,26,27,28]. The synchronization problems of the neural networks mainly include finite-time, fixed-time and asymptotic synchronizations. The asymptotically synchronization is different from the FFTS because asymptotic synchronization does not give us the time interval or fixed time for synchronization while the FFTS is achieved after a fixed time or a finite-time interval between the master-response systems. The asymptotic synchronization is another area of research interest in which the synchronization error asymptotically vanishes under limiting conditions. Although it is not a realistic as machines and human beings having a limited life span. The limitations of asymptotic stabilization overcome by finite time protocol. The article [29] shows various parameters are appeared during control methods. Finite-time synchronization is studied during last few years by the researchers [30,31]. Applications in wireless sensor networks and secure communication have been studied using finite-time synchronization communication. If we compare asymptotic synchronization and finite-time synchronization, then the later can be realized at a particular moment and hence may be controlled. The fixed-time method is first studied by Polyakov [32] in which he has stabilized the systems in the finite-time considering that the settling time does not depend on initial values of the systems. This is a better method compared to other finite time methods. Some notable fixed time control works are investigated by the researchers from time to time like [33,34,35] by using neural networks as well as complex networks. The finite-time synchronization is introduced using finite-time stability analysis by Kamenkov [36]. It is seen from the definition, fixed-time stability analysis is the particular case of finite-time stability analysis and in both stability analyses, the trajectories will converge over a finite-time interval. In the finite-time stability the convergence time or settling time of the trajectories depends on the initial conditions of the model and in fixed-time stability analysis, the settling time of the trajectories has a uniform upper bound for all initial conditions within the domain which is not dependent on the initial conditions. This is the main difference between finite time and fixed time stability analyses. In these types of synchronization control problems and the estimation of time are the key features for the stability analyses. From the literature review, so many practical systems are formed such as power systems, traffic signals [37,38]. These problems are controlled using fixed-time interval. The initial conditions are rarely be given for many real practical problems. Polyakov [39] has studied the finite-time stability by using nonlinear feedback design of linear control system. In this point of view, the fixed-time synchronization (FTS) has more advantages compared to finite-time synchronization because FTS has nothing to do with initial conditions of error systems. Many synchronization problems have been done by the researchers on finite-time synchronization of FCNNs. But the study on FTS is few [40]. By designing state feedback controller and discontinuous activation function, the fixed time synchronization problem for FCNNs with time-varying delay have been discussed in [41]. Under the differential inclusion theory and discontinuous state feedback control technique, Sun and Liu [42] have investigated the fixed-time synchronization of fractional-order memristor-based FCNNs with time-varying delays by defining appropriate Laypunov functional. By constructing delay dependent controllers with or without fuzzy terms and using matrix analysis method, fixed time synchronization criteria have been discussed for delayed markovian jump FCNNs in the presence of stochastic disturbance in [43]. To study the significance of the control and synchronization in delayed FCNNs, Ding and Han [44] have studied synchronization on delayed FCNNs by using adaptive control method with unknown parameters, in which control functions are designed using Lyapunov-Lasall principle and some other synchronization conditions. The global exponential synchronization on delayed FCNNs using Lyapunov-like stability theory with some other criteria has been studied by Feng et al.[45]. From literature review it is confirmed that the researchers were only focused on synchronization problems of FCNNs with time-varying delay corresponding to finite-time problems [46,47,48,49,50,51]. The study on FTS is still in a primal stage. In the year 2015, Polyakov et al.[52] have studied the FFT stability of robust stabilization of nonlinear systems using the new nonlinear control laws and implicit lyapunov function. Wan et al.[53] have investigated the robust FTS for CGNNs by using Lyapunov stability theory, Liu and Chen [54] have also introduced the finite-time cluster and fixed-time cluster synchronizations in presence or absence of pinning control law.

    Based on the above analysis, the authors have motivated to study FFTS of FCNNs with interaction and proportional delay terms. In real-time, the interactions [55,56] of two networks are diverted through the nonlinear signals, mutual connections, or by the hub nodes. The proportional delay [57,58,59] has wide existence in the real-world such as routing decision and web quality of service [60]. The dynamical nature of the neural networks include proportional delays term have been introduced by the researchers and most of the works concerning synchronizations of neural networks include proportional delays term are asymptotic. This implies synchronization of neural networks is achieved when time becomes large. In this article a drive has been taken to study FFTS in which the error model of networks will be convergent in an estimated time domain. The main contributions of this article are summarized as:

    (1) Almost all works in references [61,62] are related to study on FNNs assuming that the continuous activation functions are time varying-delays or smooth, and Lipschitz continuous. In this article, the main focus is given on the study of synchronization of FCNNs with continuous activation function having interaction and proportional delay terms.

    (2) Simple controller is designed for FFTS of considered FCNN models by using some new algebraic criteria and some sufficient conditions which confirm that the both master and response systems can be synchronized in finite and fixed time, and also it gives a range of domain of time for FFTS.

    (3) In this article, the settling time can easily be estimated. The settling time of the fixed-time synchronization is bounded for any initial states. Furthermore, as compared to the classical results, our proposed estimation bound of the settling time is more effective and accurate.

    (4) Two examples are considered to show the effectiveness, reliability and the accuracy of the proposed numerical scheme of FFTS.

    The organization of the article is as follows. Some preliminaries in which system description, some definitions, lemmas, assumptions, and problem formulation are introduced in section 2. Two control laws for the FFTS are designed in the section 3. Two examples have been taken to validate, the reliability, effectiveness and efficiency of the results given in section 4. The overall conclusions of the article are discussed in the section 5.

    Notations

    In this section the symbols and are used to denote the fuzzy OR operation and fuzzy AND operation respectively. p is used for positive integer, ||.|| denotes the vector norm and ||.||p is the representation of p-norm. C([τ,0],Rn) is taken in Banach space, where τ stands for delay term in time. fj(.) and hj(.) are taken as activation function and interaction function between two neurons, respectively.

    Suppose p1 be a positive integer and Rn is the real column vectors of n-dimensional space and z=(z1,z2,...,zn)T, then ||z|| represents vector norm and is defined as

    ||z||=(ni=1|zi|p)1p.

    Lemma 2.1. [10] Assume z and w are two state variables, then we have following inequalities as

    |nj=1αijfj(zj)nj=1αijfj(wj)|nj=1|αij||fj(zj)fj(wj)|,|nj=1βijfj(zj)nj=1βijfj(wj)|nj=1|βij||fj(zj)fj(wj)|,i=1,2,...,n.

    Lemma 2.2. Suppose 0<s<1 and c,dR, then the following condition

    (|c|+|d|)s|c|s+|d|s

    is satisfied.

    Lemma 2.3. Consider nN and 0<i<j, i,jR, then the following condition holds

    |c1|i+|c2|i+...+|cn|i(|cj1|+|cj2|+...+|cjn|)ij.

    Let us consider n-dimensional FCNNs with interaction and proportional delay terms as drive system given by

    ˙zi(t)=cizi(t)+nj=1aijfj(zj(t))+nj=1bijfj(zj(rt))+nj=1qijvj+nj=1Tijvj+nj=1αijfj(zj(rt))+nj=1βijfj(zj(rt))+nj=1Sijvj+ϵnj=1dijhj(wj(t))+Ii, (2.1)

    with initial conditions zi(s)=ψi(s),s[τ,0], where iI{1,2,...,n}, zi(t) represents the i-th unit state variable at time t. aij and bij represent the elements of feedback templates, ci denotes the passive decay rate of the ith unit state, qij is taken for the feed-forward template and αij and βij respectively represent fuzzy feedback templates of MIN and MAX, Tij and Sij respectively denote fuzzy feed-forward templates of MIN and MAX. vi and Ii represent input of neuron and bias of neuron at i-th iteration respectively. The proportional delay term is r(0,1) and rt=t(1r)t, with τ(t)=(1r)t is a continuous time varying function which satisfies (1r)t+ as t+. dij, ¯dij denote the interaction structures. fj and hj are the activation and interaction functions between the networks, respectively, ϵ is outer interaction strength. Here ψ(s)=(ψ1(s),ψ2(s),...,ψn(s))TC([τ,0],Rn) represents the Banach space of all continous functions with p-norm defined as

    ||ψ||p=[sups[τ,0]ni=1|ψi(s)|p]1p,

    where p>0 is an even integer.

    Now, we consider the following assumptions as (H1) real constants L_i, N_i and positive real numbers ¯Li, ¯Ni such that

    L_ifi(z1)fi(z2)z1z2¯Li,z1,z2R,z1z2andiI,N_ihi(z1)hi(z2)z1z2¯Ni,z1,z2R,z1z2andiI.

    (H2) The neuron activation function fi and interaction function hi are bounded then Li>0 and Ni>0 for each i, such that

    |fi(z)|Li,zR,|hi(z)|Ni,zR.

    Let the response system is

    ˙wi(t)=ciwi(t)+nj=1aijfj(wj(t))+nj=1bijfj(wj(rt))+nj=1qijvj+nj=1Tijvj+nj=1αijfj(wj(rt))+nj=1βijfj(wj(rt))+nj=1Sijvj+ϵnj=1ˉdijhj(zj(t))+Ii+ui(t),iI, (2.2)

    where wi(s)=ξi(s),s[τ,0],ξi(s)C([τ,0],R) is the initial conditions and ui(t) is the coupling control.

    Let us consider zi(t),wi(t) are state variables of the systems (2.1) and (2.2), and ψi,ξi are initial conditions respectively. Assuming that ei(t)=wi(t)zi(t), iI and fj(ej(t))=fj(wj(t))fj(zj(t)), we get the error system as

    ˙ei(t)=ciei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+ϵnj=1ˉdijhj(zj(t))ϵnj=1dijhj(wj(t))+ui(t),t0. (2.3)

    Definition 2.1. [10] The systems (2.1) and (2.2) are synchronized in a finite time after appropriate design of the controller ui(t), if a constant T>0 s.t.

    limtT|zi(t)wi(t)|=0

    and |zi(t)wi(t)|=0fort>T,iI.

    Definition 2.2. [63] The considered system (2.1) achieves FTS with response system (2.2) if a settling time function T(e0(θ)) and a fixed time Tmax such that

    limtT(e0(θ))||e(t)||=0,e(t)=0,foralltT(e0(θ)),T(e0(θ))Tmax,foralle0(θ)Cn[τ,0],

    where ||.|| represents the Euclidean norm.

    Definition 2.3. [64] If f(t) is differentiable on R, then the upper Dini derivative of |f(t)| is given by D+(|f(t)|) = ˙(f(t))sgn(f(t)) for f(t)0.

    Lemma 2.4. [10] Suppose V1(t) is a continuous and positive-definite function, then it satisfies

    D+V1(t)βVμ1(t),tt0,V1(t0)0,

    where 0μ<1,β0 are constants.

    Then, for given t0, the following inequalities hold for V1(t).

    V1μ1(t)V1μ1(t0)β(1μ)(tt0),t0tT

    and

    V1(t)0,tT,

    with T is given by

    T=t0+V1μ1(t0)β(1μ).

    Remark. In the view of Lemma 2.4, the system (2.3) is fixed-time stable at origin and the settling time is obtained as

    T(e(t0))Tmax=(1β)(11μ).

    Suppose that the activation functions fi are bounded, then we define the control law in the following form as

    ui(t)=ηiei(t)σisgn(ei(t))ksgn(ei(t))|ei(t)|θ,iI, (3.1)

    where ei(t)=zi(t)wi(t), with ηi,k are the parameters.

    Theorem 3.1. Assuming H1 and H2 are satisfied, then the drive system (2.1) will be finite-time synchronized with response system (2.2) with the help of controller (3.1) if the conditions ηici+λi+wi+vi and ρiσi0 are satisfied,

    where wi=1pnj=1,jip1i=1|aij|pγlijLpδlijj+1pnj=1,ji|aji|pγpijLpδpiji

    and vi=ϵpnj=1,jip1i=1|dij|pγlijNpδlijj+ϵpnj=1,ji|dji|pγpijNpδpiji.

    Proof. Let the Lyapunov functional is

    V1(t)=ni=1|ei(t)|p (3.2)

    In view of (2.3), calculating the upper right-hand Dini derivative of Eq (3.2), we have

    D+V1(t)=ni=1psgn(ei(t))|ei(t)|p1˙ei(t)=ni=1psgn(ei(t))|ei(t)|p1[ciei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+ϵnj=1ˉdijhj(zj(t))ϵnj=1dijhj(wj(t))+ui(t)]=ni=1psgn(ei(t))|ei(t)|p1[ciei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+ϵnj=1ˉdijhj(zj(t))ϵnj=1dijhj(wj(t))ηi(ei(t))σisgn(ei(t))ksgn(ei(t))|ei(t)|θ]. (3.3)

    From H1,H2 and Lemma 2.1, we obtain

    L_j|ej(t)||fj(ej(t))|¯Lj|ej(t)|Lj|ej(t)|N_j|ej(t)||hj(ej(t))|¯Nj|ej(t)|Nj|ej(t)||nj=1αijfj(ej(rt))|nj=1|αij||fj(ej(rt))|nj=1|αij|Mj|nj=1βijfj(ej(rt))|nj=1|βij||fj(ej(rt))|nj=1|βij|Mj, (3.4)

    where Lj = max{|L_j|,|¯Lj|}, Nj = max{|N_j|,|¯Nj|}, then from Eqs (3.3) and (3.4), we get

    D+V1(t)=ni=1psgn(ei(t))|ei(t)|p1[(ci+ηi)ei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+nj=1ϵdij(hj(zj(t))hj(wj(t)))σisign(ei(t))ksgn(ei(t))|ei(t)|θ]ni=1p(ci+ηiλi)|ei(t)|p+ni=1nj=1,jip|aij|Lj|ei(t)|p1|ej(t)|+ni=1nj=1pμij|ei(t)|p1Mj+ni=1nj=1,jipϵ|dij|Nj|ei(t)|p1|ej(t)|ni=1pσi|ei(t)|p1ni=1pk|ei(t)|(p1+θ), (3.5)

    where λi is given by

    λi={aii¯Li,ifaii0,aiiLi_,ifaii<0

    and μij=|bij|+|αij|+|βij| and q=p+θ1>0. Assume that γlij,δlij0 are real numbers and satisfy pl=1γlij=1,pl=1δlij=1. Then applying the condition pc1c2...cpcp1+cp2+...+cpp, where ci>0 for i=1,2,...,p, we get

    nj=1,jip|aij|Lj|ei(t)|p1|ej(t)|=nj=1,jip[p1l=1(|aij|γlijLδlijj|ei(t)|)](|aij|γpijLδpijj|ej(t)|)nj=1,jip1l=1|aij|pγlijLpδlijj|ei(t)|p+nj=1,ji|aij|pγpijLpδpijj|ej(t)|p, (3.6)

    with

    wi=1pnj=1,jip1l=1|aij|pγlijLpδlijj+1pnj=1,ji|aji|pγpijLpδpjii.

    Similarly,

    nj=1,jip|dij|Nj|ei(t)|p1|ej(t)|nj=1,jip1l=1|dij|pγlijNpδlijj|ei(t)|p+nj=1,ji|dij|pγpijNpδpijj|ej(t)|p, (3.7)

    with

    vi=ϵpnj=1,jip1l=1|dij|pγlijNpδlijj+ϵpnj=1,ji|dji|pγpijNpδpjii,

    ρi=nj=1μijMj,iI.

    Using Eqs (3.6) and (3.7) in Eq (3.5), we get

    D+V1(t)ni=1p(ciλi+ηiwivi)|ei(t)|p+ni=1p(ρiσi)|ei(t)|p1ni=1pk|ei(t)|(p1+θ).

    Choosing ηi such that ηici+λi+wi+vi and (ρiσi)0, we get using Lemma 2.3,

    D+V1(t)pkni=1|ei(t)|(p+θ1)pk(ni=1|ei(t)|p)qp=pkVqp1(t),

    Hence from Lemma 2.4, the systems (2.1) and (2.2) will be synchronized in the finite-time T1=V1θp1(0)k(1θ). Also the control law (3.1) and the system (2.3) will converge to zero within time T1.

    Note. If p=2,γlij=δlij=12 for l=1,2, then

    ¯wi=nj=1,ji(|aij|Lj+|aji|Li)2, ¯ρi=nj=1Mj(|bij|+|αij|+|βij|),i I.

    Let us define controller as

    ui(t)=sgn(ei(t))(σiηiei(t)k|ei(t)|θ), (3.8)

    where σi,ηi, i=1,2,...n. and k are parameters.

    Theorem 3.2. If we consider H1 and H2 hold, then systems (2.1) and (2.2) will be synchronized in the fixed time with the help of controller (3.8).

    The settling time Tmax is estimated as

    Tmax=(1pk)(ppq).

    Proof. Assume that Lyapunov function as

    V1(e(t))=ni=1|ei(t)|p

    In view of (2.3), calculating the upper right-hand Dini derivative of V1(t), we get

    D+V1(t)=ni=1psgn(ei(t))|ei(t)|p1˙ei(t)=ni=1psgn(ei(t))|ei(t)|p1[ciei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+ϵnj=1ˉdijhj(zj(t))ϵnj=1dijhj(wj(t))+ui(t)]=ni=1psgn(ei(t))|ei(t)|p1[ciei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+ϵnj=1ˉdijhj(zj(t))ϵnj=1dijhj(wj(t))+sgn(ei(t))(σiηi(ei(t))ksgn(ei(t))|ei(t)|θ)]. (3.9)

    Using Lemma 2.1 and Assumptions H1 and H2, we obtain

    L_j|ej(t)||fj(ej(t))|¯Lj|ej(t)|Lj|ej(t)|,N_j|ej(t)||hj(ej(t))|¯Nj|ej(t)|Nj|ej(t)|,|nj=1αijfj(ej(rt))|nj=1|αij||fj(ej(rt))|nj=1|αij|Mj,|nj=1βijfj(ej(rt))|nj=1|βij||fj(ej(rt))|nj=1|βij|Mj, (3.10)

    where Lj = max{|L_j|,|¯Lj|}, Nj = max{|N_j|,|¯Nj|}.

    Thus from Eqs (3.9) and (3.10), we get

    D+V1(t)=ni=1psgn(ei(t))|ei(t)|p1[(ci+ηi)ei(t)+nj=1aijfj(ej(t))+nj=1bijfj(ej(rt))+nj=1αijfj(ej(rt))+nj=1βijfj(ej(rt))+nj=1ϵdij(hj(zj(t))hj(wj(t)))+σisgn(ei(t))ksgn(ei(t))|ei(t)|θ]ni=1p(ci+ηiλi)|ei(t)|p+ni=1nj=1,jip|aij|Lj|ei(t)|p1|ej(t)|+ni=1nj=1pμij|ei(t)|p1Mj+ni=1nj=1,jipϵ|dij|Nj|ei(t)|p1|ej(t)|ni=1pσi|ei(t)|p1ni=1pk|ei(t)|(p1+θ).

    Similarly, by Theorem 3.1, we obtain

    D+V1(t)ni=1p(ciλi+ηiwivi)|ei(t)|p+ni=1p(ρiσi)|ei(t)|p1ni=1pk|ei(t)|(p1+θ)

    Choosing ηi and σi such that ηici+λi+wi+vi and ρiσi0 and using Lemma 2.3, we get

    D+V1(t)pkni=1|ei(t)|(p+θ1)pk(ni=1|ei(t)|p)qp=pkVqp1(t),

    where q=p+θ1, From the Lemma 2.4, we say that error system (2.3) is fixed-time stabled at origin. Then fixed-time synchronization is achieved between the considered systems (2.1) and (2.2).

    By Lemma 2.4, we can estimate the settling time as

    T(e(t0))Tmax=(1pk)(ppq).

    Remark. Since the controllers (3.1) and (3.8) contain the discontinuous sgn function, as a hard switcher, it may be caused to undesirable chattering. In order to avoid the chattering, the sgn function is replaced by a continuous tanh function to remove discontinuity. For examples, the control laws (3.1) and (3.8) can be modified as follows

    ui(t)=ηiei(t)σitanh(ξiei(t))ktanh(κiei(t))|ei(t)|θ,
    ui(t)=tanh(ξiei(t))(σiηiei(t)k|ei(t)|θ),

    where ξi,κi>0 and iI.

    In this section two numerical examples are considered to demonstrate the effectiveness and efficiency of our proposed synchronization scheme.

    Example 4.1. Suppose that following FCNN with interaction and proportional delay terms as drive system. Then for n = 2,

    ˙zi(t)=cizi(t)+2j=1aijfj(zj(t))+2j=1bijfj(zj(rt))+2j=1αijfj(zj(rt))+2j=1βijfj(zj(rt))+ϵ2j=1dijhj(wj(t))+Ii,i=1,2, (4.1)

    where fj(xj)=tanh(xj) and hj(xj)=sin(xj). ci,aij,bij,αij,βij and dij are the parameters of the system which are taken as c1=1.5,c2=0.5,a11=1.4,a12=0.8,a21=1.8,a22=2,b11=1,b12=0.2,b21=0.5,b22=0.5,α11=1.2,α12=0.2,α21=1.8,α22=0.4,β11=0.4,β12=1.2,β21=1.5,β22=0.2,d11=0.5,d12=0,d21=0,d22=0.5,r=0.7,τ(t)=0.3exp(t) and I1=0,I2=0, ϵ=0.5.

    The 3-D plot of the trajectories z1(t) and z2(t) with time t of the system (4.1) is depicted through Figure 1 with initial values as z1(s)=0.50,z2(s)=0.75,w1(s)=0.25,w2(s)=0.25 for s[0.3,1].

    Figure 1.  Plots of the state trajectories z1(t) and z2(t) vs. t for Example 4.1.

    The corresponding response system is taken as

    ˙wi(t)=ciwi(t)+nj=1aijfj(wj(t))+nj=1bijfj(wj(rt))+nj=1αijfj(wj(rt))+nj=1βijfj(wj(rt))+ϵnj=1ˉdijhj(zj(t))+Ii+ui(t), (4.2)

    where ci,aij,bij,dij,αij,βij,fj,hj,r and Ii are similar to the system (4.2), and ui(t) is the controller which is given as

    ui(t)=ηiei(t)σitanh(ei(t))ktanh(ei(t))|ei(t)|θ, (4.3)

    where ei(t)=wi(t)zi(t).

    For L_i=0,¯Li=Mi=1, Ni=1, i=1,2, the assumptions (H1) and (H2) hold. After choosing the values p=2, θ=0.6 and k = 3, we have L1=L2=1,λ1=1.4,λ2=2,¯w1=¯w2=1.30,¯ρ1=4.2,¯ρ2=4.9,¯v1=¯v1=0. Considering η1=1.50, η2=3, σ1=4.2, σ2=4.9, all the conditions of Theorem 3.1 hold. Therefore, in view of the Theorem 3.1, the considered systems (4.1) and (4.2) will be synchronized in a finite time with the help of the defined controllers given in Eq (4.3). Figures 2 and 3 show the synchronizations between the systems (4.1) and (4.2). The synchronizations of errors between systems (4.1) and (4.2) are depicted through Figure 4 for the earlier considered initial values.

    Figure 2.  Plots of the state trajectories z1(t) and w1(t) vs. t, of master system (4.1) and response system (4.2) for Example 4.1.
    Figure 3.  Plots of the state trajectories z2(t) and w2(t) vs. t, of master system (4.1) and response system (4.2) for Example 4.1.
    Figure 4.  Plots of errors e1(t) and e1(t) of the systems (4.1) and (4.2) for Example 4.1.

    Example 4.2. Let us consider following FCNN with interaction and proportional delay terms for fixed time synchronization as a drive system as

    ˙zi(t)=cizi(t)+2j=1aijfj(zj(t))+2j=1bijfj(zj(rt))+2j=1αijfj(zj(rt))+2j=1βijfj(zj(rt))+ϵ2j=1dijhj(wj(t))+Ii, (4.4)

    where hj(xj)=sin(xj) and fi(x)=(|x+1||x1|)/2,i=1,2. Now the values of the parameters of the system (4.4) are taken as c1=1.2,c2=1,a12=0.5,a11=1.5,a21=1.8,a22=2.1,b12=0.2,b11=1,b21=0.5,b22=0.5,α12=0.1,α11=1.5,α22=0.4,α21=0.5,β11=0.5,β12=1.1,β21=1.5,β22=0.1,d12=0,d11=0.4,d22=0.4,d21=0,r=0.2,τ(t)=0.8exp(t) and I1=0.1,I2=0.2,ϵ=0.5.

    Figure 5 depicts the 3-D plot of the trajectories z1(t) and z2(t) at time t of the system (4.4) with initial values as z1(s)=0.15,z2(s)=0.45,w1(s)=0.25,w2(s)=0.35 for s[0.5,1].

    Figure 5.  Plots of the state trajectories z1(t) and z2(t) vs. t for Example 4.2.

    The corresponding response system is considered as

    ˙wi(t)=ciwi(t)+nj=1aijfj(wj(t))+nj=1bijfj(wj(rt))+nj=1αijfj(wj(rt))+nj=1βijfj(wj(rt))+ϵnj=1ˉdijhj(zj(t))+Ii+ui(t), (4.5)

    where ci,aij,bij,dij,αij,βij,fj,hj,r and Ii are the same parameters as considered in system (4.4), and ui(t) is the controller designed as

    ui(t)=tanh(ei(t))(σiηiei(t)k|ei(t)|θ), (4.6)

    where ei(t)=wi(t)zi(t).

    For L_i=0,¯Li=Mi=1, Ni=1, i=1,2, Assumptions (H1) and (H2) hold. Choosing the values p=2, θ=0.3 and k = 3, we have L1=L2=1,λ1=1.5,λ2=2.1,ˉw=ˉw=1.15,¯ρ1=4.4,¯ρ2=4.6,¯v1=¯v1=0. After considering η1=1.60,η2=2.50,σ1=4.4,σ2=4.6, all conditions of Theorem 1 hold. So in view of the Theorem 1, the systems (4.4) and (4.5) will be synchronized with the help of the controllers (4.6). Figures 6 and 7 show the fixed time synchronizations between systems (4.4) and (4.5). The synchronizations of the errors between systems (4.4) and (4.5) are shown through Figure 8.

    Figure 6.  Plots of the state trajectories z1(t) and w1(t) vs. t of master system (4.4) and response system (4.5) for Example 4.2.
    Figure 7.  Plots of the state trajectories z2(t) and w2(t) vs. t, of master system (4.4) and response system (4.5) for Example 4.2.
    Figure 8.  Plots of errors e1(t) and e1(t) of the systems (4.4) and (4.5) for Example 4.2.

    Here the settling time is Tmax=0.4761. In order to show the estimation bound of the settling time in more effective and more accurate ways a comparison is executed with the results given in [42].

    As far as we know, there is no research on the finite and fixed-time synchronization for FCNNs model with interaction and proportional delays. Here it is mentioned that interaction functions are bounded and delays are proportional, which are more general than the bounded delays. Here, some special types of controller are taken to achieve finite and fixed-time synchronizations. The method used in this article provides a useful approach to study the problems on the finite and fixed time synchronizations of other fuzzy neural networks with interaction term and proportional delays.

    In the present endeavor, finite and fixed-time synchronizations (FFTS) of FCNNs are discussed under the impact of proportional delays and interaction terms. Based on Lyapunov stability technique, finite-time and fixed-time convergence theory and some other criteria along with Lyapunov functional, the FFTS is achieved. The controllers have been designed in a simple way to achieve the said synchronizations for FCNNs. In the case of finite-time synchronization of FCNNs, the upper bound of the settling time can be estimated which depends on initial conditions, whereas in FTS of FCNNs, the settling time does not depend on initial conditions. Two numerical examples are taken to verify the correctness of the mathematical results. Consequently, the obtained results on FCNN models with interaction and proportional delay terms are first of its kind and also convenient as compared to the previous available results of the FTS obtained by [8,9,10,31,34,35,61,63]. Our future work will be focused on quasi-synchronization problem of FCNNs with interaction terms. Also the FFTS of impulsive FCNNs with mixed delay and interaction terms will be considered in near future.

    The authors are extending their heartfell thanks to the revered reviewers for their valuable comments towards upgradation of the article. The second author S.Das acknowledges the project grant provided by the SERB, Government of India under the MATRICS scheme (File no: MTR/2020/000053).

    The authors declare that they have no conflict of interest.



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