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Exponential Synchronization for Fractional-order Time-delayed Memristive Neural Networks Cover

Exponential Synchronization for Fractional-order Time-delayed Memristive Neural Networks

By: Ding Dawei,  Zhang Yaqin and  Wang Nian  
Open Access
|Oct 2019

Full Article

I.
INTRODUCTION

Chua already supposed the existence of memristor in 1971 [1], however, the practical device of memristor in electronics is obtained in [2] until 2008. In addition to the existing three kinds of circuit elements, memristor is regarded as the fourth basic circuit element and is defined by a nonlinear charge-flux characteristic. As everyone knows, resistors can be used to work as connection weights so that it can emulate the synapses in artificial neural networks. However, in the neural networks of biological individual, long-term memories is essential in the synapses among neurons, but for the general resistors, it is impossible to have the function of memory. Recently, due to the memory characteristics of memristor, memristor can replace the resistor to develop a new neural networks that is memristor-based neural networks (MNN) [3-6].

In recent years, more and more attentions have been put on the dynamical analysis of memristor-based neural networks, such as the investigation of stability [7-10], periodicity [11-13], system synchronization [14-22], passivity analysis [23], dissipativity [24-25] and attractivity [26]. Particularly, the stability and synchronization of MNN has been widely studied in [27-30]. In fact, synchronization means the dynamics of nodes share the common time-spatial property. Therefore we can understand an unknown dynamical system by achieving the synchronization with the well-known dynamical systems [18]. Moreover, in the transmission of digital signals, communication will become security, reliable and secrecy by achieving synchronization between the various systems. Therefore, the synchronization of MNN is still worth further research.

Moreover, the fractional-order models can better describe the memory and genetic properties of various materials and process, so the fractional-order models have received a lot of research attentions than integer-order models. In recent years, with the improvement of fractional-order differential calculus and fractional-order differential equations, it is easy to model and analyze practical problems [31, 32]. Therefore, there have been a lot of researches about the dynamical analysis and synchronization of fractional-order memristor-based neural networks (FMNN) [34-39]. Finite-time synchronization, hybrid projective synchronization and adaptive synchronization of FMNN have all been researched [34-36]. However, there are only a very few research results on exponential synchronization of FMNN. In fact, the exponential synchronization of neural networks has been widely used in the theoretical research and practical application of many scientific fields, for example, associative memory, ecological system, combinatorial optimization, military field, artificial intelligence system and so on [40-43]. So the exponential synchronization of FMNN is still worth further studying as it is a significant academic problem.

On the other hand, the stability and synchronization of FMNN without time delay have been deeply studied such as in [33]. However, in hardware implementation of neural networks, time delay is unavoidable owing to the finite switching speeds of the amplifiers. And it will cause instability, oscillation and chaos phenomena of systems. So the investigation for stability and synchronization of FMNN cannot be independent on the time delay.

Motivated by the above discussion, this paper studies the exponential synchronization of FMNN with time-varying delays. The main contributions of this paper can be listed as follow. (1) This is the first attempt to achieve exponential synchronization of FMNN with time-varying delays by employing a simple linear error feedback controller. (2) The sufficient condition for exponential synchronization of FMNN with time delays is obtained based on comparison principle instead of the traditional Lyapunov theory. (3) Some previous research results of exponential synchronization for integer-order memristor-based system are the special cases of our results. Furthermore, some numerical examples are given to demonstrate the effectiveness and correctness of the main results.

The rest of this paper is organized as follows. Preliminaries including the introduction of Caputo fractional-order derivative, model description, assumptions, definitions and lemmas are presented in Section 2. Section 3 introduces the sufficient condition for exponential synchronization of the FMNN. In Section4, the numerical simulations are presented. Section5 gives the conclusion of this paper.

II.
PRELIMINARIES

Compared to the integer-order derivatives, we know the distinct advantage of Caputo derivative is that it only requires initial conditions from the Laplace transform of fractional derivative, and it can represent well-understood features of physical situations and making it more applicable to real world problems [36]. So in the rest of this paper, we apply the Caputo fractional-order derivative for the fractional-order memristor-based neural networks (FMNN) and investigate the exponential synchronization of FMNN.

A.
The Caputo fractional-order derivative

Definition1 [32] The Caputo fractional-order derivative is defined as follows: (1)Dtqf(t)=1Γ(mq)t0tf(m)(τ)(tτ)qm+1dτ,where q is the order of fractional derivative, m is the first integer larger than q, m − 1 ≤ q < m,Γ(⋅) is the Gamma function, (2)T(x)=0tx1etdt.

Particularly, when 0<q<1, (3)Dtqf(t)=1Γ(1q)t0tf'(τ)(tt0)qdτ.

B.
Model description

In this paper, referring to some relevant works on FMNN [35,36], we consider a class of FMNN with time-varying delays described by the following equation, (4)Dqxi(t)=cixi(t)+j=1naij(xj(t))fj(xj(t))+j=1nbij(xj(tτj(t)))gj(xj(tτj(t)))+Iit0,iN.aij(xj(t))=MijCi×δij,bij(xj(tτj(t)))=WijCi×δij,δij={1,ij,1,i=j,where xi(t) is the state variable of the ith neuron (the voltage of capacitor Ci), q is the order of fractional derivative, ci > 0 is the self-regulating parameters of the neurons, 0 ≤ τjτ and (τ is a constant ) represents the transmission time-varying delay. fj,gj :RR are feedback functions without and with time-varying delay. aij(xj(t)) and bij(xj(t − τj(t))) are memristive connective weights, which denote the neuron interconnection matrix and the delayed neuron interconnection matrix, respectively. Wij and Mij denote the memductances of memristors Rij and Fij respectively. And Rij represents the memristor between the feedback function fi(xi(t)) and xi(t), Fij represents the memristor between the feedback function gi(xi(tτi(t))) and xi(t). Ii represents the external input. According to the feature of memristor, we denote (5)aij(xj(t))={aij,xj(t)0,aij,xj(t)>0,bij(xj(tτj(t)))={bij,xj(tτj(t))0.bij,xj(tτj(t))>0.

C.
Assumptions, Definitions and Lemmas

In the rest of paper, we first make following assumption for system (4).

Assumption1: For jN, ∀s1, s2R, the neuron activation functions fj, gj bounded, fi(0) = gj(0) = 0 and satisfy (6)0fj(s1)fj(s2)s1s2σj,0gj(s1)gj(s2)s1s2ρj,where s1s2 and σj, ρj are nonnegative constants.

We consider system (4) as drive system and corresponding response system is given as follows:3 (7)Dqyi(t)=ciyi(t)+j=1naij(yj(t))fj(yj(t))+j=1nbij(yj(tτj(t)))gj(yj(tτj(t)))+Ii+ui,t0,iN,

Where (8)aij(yj(t))={aij,yj(t)0,aij,yj(t)>0,bij(yj(tτj(t)))={bij,yj(tτj(t))0.bij,yj(tτj(t))>0.and ui(t) is a liner error feedback control function which defined by ui(t) = ωi(yi(t) − xi(t)), where ωi, iN are constants, which denotes the control gain. Next, we define the synchronization error e(t) as e(t) = (e1(t),e2(t),….,en(t))T, where ei(t) = yi(t) − xi(t). According to the system (4) and system (7), the synchronization error system can be described as follows: (9)Dqei(t)=ciei(t)+[j=1naij(yj(t))fj(yj(t))j=1naij(xj(t))fj(xj(t))]+[j=1nbij(yj(tτj(t)))gj(yj(tτj(t)))j=1nbij(xj(tτj(t)))gj(xj(tτj(t)))]+ui(t),t0,iNwhere aij(yj(t)), bij(yj(t − τj(t))), aij(xj(t)), bij(xj(t − τj(t))) are the same as those defined above, ui(t) = ωi(yi(t) − xi(t)) = ωiei(t), where ωi, iN are constants, which denotes the control again.

According to the theories of differential inclusions and set valued maps [40], if xi(t) and yi(t) are solutions of (4) and (7) respectively, system (4) and system (7) can be written as follow: (10)Dqxi(t)cixi(t)+j=1nco[aij(xj(t))]fj(xj(t))+j=1nco[bij(xj(tτj(t)))]gj(xj(tτj(t)))+Ii,t0,iN

And

(11)Dqyi(t)ciyi(t)+j=1nco[aij(yj(t))]fj(yj(t))+j=1nco[bij(yj(tτj(t)))]gj(yj(tτj(t)))+Ii+ui,t0,iN,

Where

(12)co[aij(xj(t))]={aij,xj(t)<0,co{aij,aij},xj(t)=0aij,xj(t)>0,,co[aij(yj(t))]={aij,yj(t)<0,co{aij,aij},yj(t)=0aij,yj(t)>0,

And

(13)co[bij(xj(tτ(j)))]={bij,xj(tτ(j))<0,co{bij,bij},xj(tτ(j))=0,bij,xj(tτ(j))>0,co[bij(yj(tτ(j)))]={bij,yj(tτ(j))<0,co{bij,bij},yj(tτ(j))=0,bij,yj(tτ(j))>0,

where co{u, v} denotes the closure of convex hull generated by real numbers u and v or real matrices u and v. Then the synchronization error system can be described as follows: (14)Dqei(t)ciei(t)+{j=1nco[aij(yj(t))]fj(yj(t))j=1nco[aij(xj(t))]fj(xj(t))}+{j=1nco[bij(yj(tτj(t)))]gj(yj(tτj(t)))j=1nco[bij(xj(tτj(t)))]gj(xj(tτj(t)))}+ωiei,t0,iN.

Definition2 [8] For ∀t ≥ 0, the exponential synchronization of system (4) and system (7) can be transformed to the exponential stability of the error system (9) (error approaches to zero). The error system (9) is said to be exponentially stable, if there exist constant Qi > 0, Pi > 0, such that the solution e(t) = (e1(t),e2(t),…,en(t))T of error system (9) with initial condition e(s) = ϕ(s) ∈ ([t0τ, t0],Rn) satisfies |ei(t)|Qimax1in{supt0τst0|ϕi(s)|}exp{Pi(tt0)},tt0>0,i = 1,2,…,n, where Pi is called the estimated rate of exponential convergence.

Lemma1 [14] Under the assumption1, the following estimation can be obtained:

(i) co[aij(yj(t))]fj(yj(t)) − co[aij(xj(t))]fj(xj(t)) ≤ AijFj(ej(t)),

(ii) co[bij(yj(t − τj(t)))]gj(yj(t − τj(t))) − co[bij(xj(t − τj(t)))]gj(xj(t − τj(t))) ≤ BijGj(ej(t − τj(t))),

where Aij=max{|aij|,|aij|},Bij=max{|bij|,|bij|},i,jN,Fj(ej(t))=fj(yj(t))fj(xj(t)),Gj(ej(tτj(t)))=gj(yj(tτj(t)))gj(xj(tτj(t))),jN.

Proof: If yi(t) = 0, xi(t) = 0, iN we can easily have part(i) hold. From (9) and (10), we can get

  • (1)

    For yi(t) < 0, xi(t) < 0, then co[aij(yj(t))]fj(yj(t))co[aij(xj(t))]fj(xj(t))=aijfj(yj(t))aijfj(xj(t)=aijFj(ej(t))AijFj(ej(t)).

  • (2)

    For yi(t) > 0, xi(t) > 0, then co[aij(yj(t))]fj(yj(t))co[aij(xj(t))]fj(xj(t))=aijfj(yj(t))aijfj(xj(t)=aijFj(ej(t))AijFj(ej(t)).

  • (3)

    For xi(t) < 0 < yi(t) or yi(t) < 0 < xi(t), then co[aij(yj(t))]fj(yj(t))co[aij(xj(t))]fj(xj(t))=aijfj(yj(t))f(0))+aij(f(0)fj(xj(t)))Aij(fj(yj(t))f(0))+Aij(f(0)fj(xj(t)))=Aij(fj(yj(t))fj(xj(t)))=AijFj(ej(t)).

Then complete the proof of part (i). In the similar way, part(ii) can be easily hold.

III.
MAIN RESULTS

We present the exponential stability results for the synchronization error system of FMNN when the error system (9) is exponentially stable, the system (4) and system (7) will achieve the exponential synchronization.

tt0>0,i{1,2,,n}

Theorem1 If there exist positive constant ε,η1,η2,…,ηn such that for any (15)(ci+ωi+ε)ηi+j=1nAijσjηj+j=1nBijρjηjexp{ετj(t)}<0,then the error system (9) is globally exponentially stable.

Proof: Consider Wi(t) = |ei(t)|/ηi,i = 1,2,…,n, according to the error system (9) or (14) and lemma1, we can get the following inequality (16)Dqei(t)ciei(t)+j=1nAijFj(ej(t))+j=1nBijGj(ej(tτj(t)))+ωiei(t)=(ci+ωi)ei(t)+j=1nAijFj(ej(t))+j=1nBijGj(ej(tτj(t))).

Evaluating the fractional order derivative of Wi(t) along the trajectory of error system, then (17)DqWi(t)(ci+ωi)|ei(t)|/ηi+1/ηi[j=1nAijσj|ej(t)|+j=1nBijρj|ej(tτj(t))|]=(ci+ωi)Wi(t)+1/ηi[j=1nAijσjηjWj(t)+j=1nBijρjηjWj(tτj(t)))].

Define W˜i(t)=Wi(t)W¯(t0)exp{ε(tt0)},tt0>0,i=1,2,,n, where W¯(t0)=max1in{supt0τst0|ei(s)|/ηi}.

We will prove that W˜i(t)0,i=1,2,,n, for any tt0>0. Otherwise, since W˜i(t)0,i=1,2,,nfor t ∈ [t0τ, t0], there must exist t1t0 and some ς such that DqW˜ς(t1)0and W˜ς(t1)=0. Then (18)DqW˜ς(t1)(cς+ως)Wς(t1)+1/ης[j=1nAςjσjηjWj(t1)+j=1nBςjρjηjWj(tτj(t1))]+εW¯(t0)exp{ε(t1t0)}=(cς+ως)W¯(t0)exp{ε(t1t0)}+1/ης[j=1nAςjσjηjW¯(t0)exp{ε(t1t0)}+j=1nBςjρjηjW¯(t0)exp{ε(t1τj(t1)t0)}]+εW¯(t0)exp{ε(t1t0)}=(cς+ως+ε)W¯(t0)exp{ε(t1t0)}+1/ης[j=1nAςjσjηjW¯(t0)exp{ε(t1t0)}+j=1nBςjρjηjW¯(t0)exp{ε(t1τj(t1)t0)}]=(cς+ως+ε)W¯(t0)exp{ε(t1t0)}+1/ης[j=1nAςjσjηjW¯(t0)+j=1nBςjρjηjW¯(t0)exp{ετj(t1)}]exp{ε(t1t0)}.

Moreover, from inequality(15), we have (cς+ως+ε)+1/ηi[j=1nAijσjηj+j=1nBijσjηjexp{ετj(t)}]<0,tt0>0,i=1,2,,n,

Therefore (19)(ci+ωi+ε)W¯(t0)exp{ε(t1t0)}+1/ηi[j=1nAijσjηj+j=1nBijρjηjexp{ετj(t)}]W¯(t0)exp{ε(t1t0)}<0,tt0>0,i=1,2,,n,so it is easy to find that DqW˜ς(t1)<0, which contradicts DqW˜ς(t1)0. That shows W˜i(t)=Wi(t)W¯(t0)exp{ε(tt0)}0,tt0>0,i=1,2,,n. Thus |ei(t)|/ηimax1in{supt0τst0|ei(s)|/ηi}exp{ε(tt0)},tt0>0,i=1,2,,n.

It shows (20)|ei(t)|ηimax1in{supt0τst0|ei(s)|/ηi}exp{ε(tt0)},tt0>0,i=1,2,,n.

This completes the proof.

IV.
NUMERICAL RESULTS

In this section, we will give two numerical examples to demonstrate our analysis on exponential synchronization of FMNN.

Example1 Consider two-dimension fractional-order memristor-based neural networks (21){Dqx1(t)=c1x1(t)+a11(x1(t))f1(x1(t))+a12(x2(t))f2(x2(t))+b11(x1(tτ1(t)))g1(x1(tτ1(t)))+b12(x2(tτ2(t)))g2(x2(tτ2(t)))+I1Dqx2(t)=c2x2(t)+a21(x1(t))f1(x1(t))+a22(x2(t))f2(x2(t))+b21(x1(tτ1(t)))g1(x1(tτ1(t)))+b22(x2(tτ2(t)))g2(x2(tτ2(t)))+I2where c1 = c2 = 1, a11(x1(t)) = 1, a22(x2(t)) = 1.8, a12(x2(t))={12,x2(t)0,14,x2(t)>0,a21(x1(t))={0.1,x1(t)0,0.05,x1(t)>0,b11(x1(tτ1(t)))={1.2,x1(tτ1(t))0,1.5,x1(tτ1(t))>0,b12(x2(tτ2(t)))={0.8,x2(tτ2(t))0,1.0,x2(tτ2(t))>0,b21(x1(tτ1(t)))={0.05,x1(tτ1(t))0,0.1,x1(tτ1(t))>0,b22(x2(tτ2(t)))={1.6,x2(tτ2(t))0,1.4,x2(tτ2(t))>0,where τj(t) = et/1 + et, I = (I1,I2)T = (0,0)T, q = 0.92 and take the activation function as fi(xi) = sin(xi), gi(xi) = 0.5(|xi + 1| − |xi − 1|), i, j = 1,2. The model (21) has chaotic attractors with initial values x(0) = (0.45,0.65)T which can be seen in Figure1.

We consider system (21) as the drive system and corresponding response system is defined as Eq.(7). And for the controller ui(t) = ωi(yi(t) − xi(t)), the parameter ωi is chosen as ω1 = −9.5, ω2 = −10.5. From Theorem1, when we take ε = 0.7, τj(t) = 1, η1 = η2 = ρ1 = ρ2 = σ1= σ2 = 0.1, we can easily know (ci+ωi+ε)ηi+j=1nAijσjηj+j=1nBijρjηjexp{ετj(t)}<0ω1 = −9.5, ω2 = −10.5, we can get is true when ω1 < −1.703, ω2 < −0.232. So when (c1+ω1+ε)η1+A11σ1η1+A12σ2η2+B11ρ1η1exp{ετ1(t)}+B12ρ2η2exp{ετ2(t)}=0.798<0,(c2+ω2+ε)η2+A21σ1η1+A22σ2η2+B21ρ1η1exp{ετ1(t)}+B22ρ2η2exp{ετ2(t)}=1.027<0.

It satisfies the condition of Theorem 1, then the exponential synchronization of drive-response system is achieved.

When the response system with this controller, we get state trajectories of variable x1(t), y1(t) and x2(t), y2(t) are depicted in Figure2a and 2b. Moreover, Figure3a and 3b depict the synchronization error curves e1(t), e2(t) between the drive system and response system. These numerical simulations show the state trajectories of variable x1(t), y1(t) and x2(t), y2(t) are synchronous and synchronization error e1(t), e2(t) are converge to zero. These prove the correctness of the Theorem1.

Figure 1.

The chaotic attractors of fractional-order memristor-based neural networks(18)

Figure 2.

Exponential synchronization of state variable with cntroller (a: x1(t),y1(t),b : x2(t),y2(t))

Figure 3.

Synchronization error between the drive and response system (a : e1(t),b : e2(t))

Example2 Consider three-dimension fractional-order memristor-based neural networks (22){Dqx1(t)=c1x1(t)+a11(x1(t))f1(x1(t))+a12(x2(t))f2(x2(t))+a13(x3(t))f3(x3(t))+b11(x1(tτ1(t)))g1(x1(tτ1(t)))+b12(x2(tτ2(t)))g2(x2(tτ2(t)))+b13(x3(tτ3(t)))g3(x3(tτ3(t)))+I1Dqx2(t)=c2x2(t)+a21(x1(t))f1(x1(t))+a22(x2(t))f2(x2(t))+a23(x3(t))f3(x3(t))+b21(x1(tτ1(t)))g1(x1(tτ1(t)))+b22(x2(tτ2(t)))g2(x2(tτ2(t)))+b23(x3(tτ3(t)))g3(x3(tτ3(t)))+I2Dqx3(t)=c3x3(t)+a31(x1(t))f1(x1(t))+a32(x2(t))f2(x2(t))+a33(x3(t))f3(x3(t))+b31(x1(tτ1(t)))g1(x1(tτ1(t)))+b32(x2(tτ2(t)))g2(x2(tτ2(t)))+b33(x3(tτ3(t)))g3(x3(tτ3(t)))+I3where c1 = c2 = c3 = 1, a11(x1(t))={1,x1(t)0,1x1(t)>0,a21(x1(t))={1,x1(t)0,1x1(t)>0,a31(x1(t))={1,x1(t)0,1x1(t)>0,a12(x2(t))={1,x2(t)0,1x2(t)>0,a22(x2(t))={1,x2(t)0,1x2(t)>0,a32(x2(t))={1,x2(t)0,1x2(t)>0,a13(x3(t))={1,x3(t)0,1x3(t)>0,a23(x3(t))={1,x3(t)0,1x3(t)>0,a33(x3(t))={1,x3(t)0,1x3(t)>0,b11(x1(tτ1(t)))={1,x1(tτ1(t))0,1x1(tτ1(t))>0,b12(x2(tτ2(t)))={1,x2(tτ2(t))0,1x2(tτ2(t))>0,b21(x1(tτ1(t)))={1,x1(tτ1(t))0,1x1(tτ1(t))>0,b22(x2(tτ2(t)))={1,x2(tτ2(t))0,1x2(tτ2(t))>0,b31(x2(tτ2(t)))={1,x2(tτ2(t))0,1x2(tτ2(t))>0,b32(x2(tτ2(t)))={1,x2(tτ2(t))0,1x2(tτ2(t))>0,b13(x3(tτ3(t)))={1,x3(tτ3(t))0,1x3(tτ3(t))>0,b23(x3(tτ3(t)))={1,x3(tτ3(t))0,1x3(tτ3(t))>0,b33(x3(tτ3(t)))={1,x3(tτ3(t))0,1x3(tτ3(t))>0.

And τj(t) = et/1 + et, I = (I1,I2,I3)T = (0,0,0)Tq = 0.92 and take the activation function as fi(xi) = gi(xi) = tanh(xi),i = 1,2,3. We consider system(22) as the drive system and the corresponding response system is defined in Eq.(7). And for the controller ui(t) = ωi(yi(t) − xi(t)), ωi is chosen as ω1 = −9.5, ω2 = −10.5, ω3 = −11. From Theorem1, we take ε = 0.7, τj(t) = 1 and choose η1 = η2 = 0.1 ρ1 = ρ2 = σ1 = σ2 = 0.1. According to Aij=max{|aij|,|aij|},Bij=max{|bij|,|bij|}i,j = 1,2,3 Aij = Bij = 1, we can easily know (ci+ωi+ε)ηi+j=1nAijσjηj+j=1nBijρjηjexp{ετj(t)}<0is true when ωi < −0.604. So when ω1 = −9.5, ω2 = −10.5, ω3 = −11 we can get (c1+ω1+ε)η1+A11σ1η1+A12σ2η2+A13σ3η3+(B11ρ1η1+B12ρ2η2+B13ρ3η3)exp{ετj(t)}=0.89<0,(c2+ω2+ε)η2+A21σ1η1+A22σ2η2+A23σ3η3+(B21ρ1η1+B22ρ2η2+B23ρ3η3)exp{ετj(t)}=0.99<0,(c3+ω3+ε)η1+A31σ1η1+A32σ2η2+A33σ3η3+(B31ρ1η1+B32ρ2η2+B33ρ3η3)exp{ετj(t)}=1.04<0.

It suggests the condition of Theorem 1 is satisfied, then drive-response system achieves the synchronization.

When the response system with this controller, we get state trajectories of variable x1(t), y1(t) and x2(t), y2(t) and x3(t), y3(t) are depicted in Figure 4a,4b,4c. Moreover, Figure 5a,5b,5c depict the synchronization error curves e1(t), e2(t), e3(t) between the drive system and response system. It’s easy to see that the state trajectories of variable x1(t), y1(t), x2(t), y2(t), and x3(t), y3(t) are synchronous and synchronization error e1(t), e2(t), e3(t) are converge to zero. So the Theorem1 is proved to be correct.

In addition, we choose ω1 = −9.5, ω2 = −10.5, ω3 = −11, according to the Theorem1, it needs the following inequalities to hold: {τ<1εln(1173103ε)τ<1εln(1123103ε)τ<1εln(1023103ε)

So, we just need τ<1εln(1023103ε)holds. We have the exponential convergence rate 0 < ε < 1, figure 6 depicts the relation of time-varying delay τ and exponential convergence rate ε.

Figure 4.

Synchronization of state variable with controller (a:x1(t),y1(t),b:x2(t),y2(t),c:x3(t),y3(t))

Figure 5.

Synchronization error between the drive and response system (a:e1(t),b:e2(t),c:e3(t))

Figure 6.

The relation of time-varying delay τ and exponential convergence rate ε.

V.
CONCLUSION

This paper achieves the exponential synchronization of a class of FMNN with time-varying delays by using linear error feedback controller. Based on comparison principle, the new theorem is derived to guarantee the exponential synchronization between the drive system and response system. The methods proposed for synchronization is effective and it is easy to achieve than other complex control methods. Moreover, it can be extended to investigate other dynamical behaviors of fractional-order memristive neural networks, such as realizing the lag synchronization or anti-synchronizaton of this system based on the suitable controller. These issues will be the topic of future research. Finally, numerical examples are given to illustrate the effectiveness of the proposed theory.

Language: English
Page range: 1 - 15
Published on: Oct 1, 2019
Published by: Xi’an Technological University
In partnership with: Paradigm Publishing Services
Publication frequency: 4 issues per year

© 2019 Ding Dawei, Zhang Yaqin, Wang Nian, published by Xi’an Technological University
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.