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Research article

Finite-time anti-synchronization for delayed inertial neural networks via the fractional and polynomial controllers of time variable

  • Received: 15 January 2021 Accepted: 25 April 2021 Published: 25 May 2021
  • MSC : 34K24

  • This paper focuses on the finite-time anti-synchronization for a class of delayed master-slave inertial neural networks. By means of using the property of quadratic inequality of one variable and designing the fractional and polynomial controllers of time variable, two sufficient conditions to assure the finite-time anti-synchronization for the master-slave delayed inertial neural networks are established. Our controllers designed related to time variable t and the study method on the finite-time anti-synchronization are different from these in the existing papers.

    Citation: Ailing Li, Xinlu Ye. Finite-time anti-synchronization for delayed inertial neural networks via the fractional and polynomial controllers of time variable[J]. AIMS Mathematics, 2021, 6(8): 8173-8190. doi: 10.3934/math.2021473

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  • This paper focuses on the finite-time anti-synchronization for a class of delayed master-slave inertial neural networks. By means of using the property of quadratic inequality of one variable and designing the fractional and polynomial controllers of time variable, two sufficient conditions to assure the finite-time anti-synchronization for the master-slave delayed inertial neural networks are established. Our controllers designed related to time variable t and the study method on the finite-time anti-synchronization are different from these in the existing papers.



    As a very important neural network system, the inertial neural network model was first proposed by Babcock and Westervelt [1]. In view of its important application background in biology and engineering [2], for example, the surface layer of hair cells can be achieved in the semicircular canal of some membrane animals, which consists of an equivalent integrated circuit containing an inductor [3,4], thus, it is very crucial to add an inertial term to the nervous system. Further, the inertial term can be regarded as a powerful tool for inducing bifurcation and chaos [5,6]. Consequently, the study of dynamical behavior of the inertial delayed neural networks is very important. Recently, the dynamic behaviors of inertial neural networks have received wide attention [7,8,9,10,11,12,13,14,15,16,17].

    Synchronization of neural networks has been extensively discussed in recent years in view of their potential applications in image process, secure communication, information science and many other fields [10,12]. In practice, it also appears another prevailing phenomenon in symmetrical oscillators, anti-synchronization, which means that the state vector of synchronized systems have the same absolute values but opposite signs. It was stated that the application of anti-synchronization to lasers provides a new way to generate pulses with special forms; and its application to communication systems can strengthen the security and secrecy by the transform of the synchronization and anti-synchronization continuously in the process of digital signal transmission. As a result, the research of anti-synchronization for delayed neural networks is of very great importance in both theory and application. So far, the finite-time anti-synchronization for delayed neural networks has been investigated by some researchers [18,19,20,21,22,23,24,25,26,27]. In [18], the finite-time anti-synchronization of neural networks with time-varying delays were concerned, by combining the Holder inequality and other techniques, a sufficient condition to assure the finite-time anti-synchronization for the considered drive-response neural networks was gained. In [19], by applying integral inequality method, two criteria to ensure the finite-time anti-synchronization for the master-slave neural networks discussed in [18] were established. In [20], by mean of the inequality skills used in [18], the criteria to assure the finite-time anti-synchronization for the discussed master-slave were achieved. In [21], the master-slave finite-time anti-synchronization for memristive bidirectional associative memory neural networks (MBAMNNS) was discussed, by employing some inequality skills and constructing an appropriate Lyapunov function, some anti-synchronization criteria were derived. In [22], the finite-time anti-synchronization control of memristive neural networks with stochastic perturbations was studied by using the linear matrix inequality method. In [23], the finite-time anti-synchronization of time-varying delayed neural networks was investigated, by employing some differential inequalities and finite-time stability theory, some novel effective finite-time anti-synchronization criteria were derived based on the Lyapunov function method. In [24], the finite-time anti-synchronization of the multi-weighted coupled neural networks with and without coupling delays was analyzed, by utilizing Lyapunov functional approach and some inequality skills, several anti-synchronization criteria were put forward for the considered networks.

    To the best of our knowledge, up to now, the finite-time anti-synchronization (or finite-time synchronization) has been extensively studied mainly by applying the following four classes of study approaches: (1) Some finite-time stability theorems were used to study the finite-time anti-synchronization (or finite-time synchronization)[23,28,29]; (2) Algebraic inequality approaches were used to investigate finite-time the anti-synchronization (or finite-time synchronization)[17,18,21,24]; (3) Linear matrix inequality approaches were applied to studying the finite-time anti-synchronization (or finite-time synchronization)[22]; (4) Integral inequality approaches were used to investigate the finite-time anti-synchronization (or finite-time synchronization)[19,25,26,27]. On the other hand, up to until, in almost papers which studied the synchronization, the controllers designed only have been independent of the time variable t, a.e, the designed controllers are only the functions of the error variables ei(t).

    Inspired by the above analysis, we will attempt to study the finite-time anti-synchronization of the master-slave delayed inertial neural networks by employing the quadratic inequality of one variable under the fractional and polynomial controllers of time variable t. By applying the quadratic inequality of one variable (see Lemma 2.1), the differential inequalities (3.7) and (3.20) (see (3.7) and (3.20) In the proofs of Theorem 3.1 and Theorem 3.2) are obtained. Then integrating two differential inequalities give two sufficient conditions on the finite-time anti-synchronization for the master-slave neural networks. Our results of the finite-time anti-synchronization are more concise and easily verified than these obtained in the existing papers [18,19,20,21,22,23,24,25,26,27,28,29]. Designing the the fractional and polynomial controllers of time variable t, our results obtained are more objective and practical than these obtained in [18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33] on the finite-time anti-synchronization of the master-slave systems. The main contributions of this paper are the following aspects: (1) For the first place, by using the behavior of quadratic inequality of one variable, more concise and easily verified criteria of the finite-time anti-synchronization for the delayed master-slave neural networks are put forward; (2) By using the fractional and polynomial controllers of time variable, the more objective and practical criteria of finite-time anti-synchronization for the master-slave neural networks are given.

    Consider the following delayed inertial neural networks:

    d2xr(t)dt2=ardxr(t)dtbrxr(t)+Fr(x(t),x(t)),r=1,2,,ˆn, (2.1)

    where

    Fr(x(t),x(t))=ˆnj=1crjfj(xj(t))+ˆnj=1drjfj(xj(qt))+ˆnj=1frjfj(xj(qt))+ˆIr,

    x(t)=(x1(t),x2(t),,xˆn(t))TRˆn,xr(t) represents the states of the rth neuron at time t; the second derivatives are called inertial terms of system (2.1); ar>0,br>0 they denote the rates with which the ith neuron will reset its potential to the resting state in isolation when disconnected from the network and external inputs; crj,drj,frj are constants, denoting the connection weights; ˆIr denotes external inputs of the rth neurons, fj is the activation function; qt=tτ(t),τ(t)0,τ(t)τ<1.

    The initial conditions of system (2.1) are

    xr(s)=ϕxr(s),dxr(s)dt=ψxr(s),s[α,0],

    where ϕxr(s),ψxr(s) are real-valued bounded continuous functions on [α,0],α=maxtR{τ(t)}.

    If we refer to system (2.1) as the master system, then the slave system is expressed as follows:

    d2ur(t)dt2=ardur(t)dtbrur(t)+Fr(u(t),u(t))+^Ir+vr(t),r=1,2,,ˆn,

    where vr(t) is the controller to design later.

    The initial conditions of system (2.2) are

    ur(s)=ϕur(s),dur(s)dt=ψur(s),s[α,0],

    where ϕur(s),ψur(s) are real-valued continuous functions on [α,0].

    Let wr(t)=ur(t)+xr(t). Then we can get the following error system of (2.1) and (2.2) for r=1,2,,ˆn:

    d2wr(t)dt2=ardwr(t)dtbrwr(t)+Fr(u(t),u(t))+Fr(x(t),x(t))+2ˆIr+vr(t), (2.2)

    where

    Fr(u(t),u(t))+Fr(x(t),x(t))=ˆnj=1crj[fj(uj(t))+fj(xj(t))]+ˆnj=1drj[fj(uj(qt))+fj(xj(qt))]+ˆnj=1frj[fj(uj(qt))+fj(xj(qt))].

    Assumption 1. The activation function fj is odd, and there exists a constant Lj0 such that

    |fj(w)fj(z)|Lj|wz|,j=1,2,,ˆn,w,zR.

    Definition 2.1. Master system (2.1) and slave system (2.2) are said to achieve the finite-time anti-synchronization, if there exists a constant ˉT>0, which depends on the initial conditions of the system (2.1) and system (2.2), such that for r=1,2,,ˆn,

    limtˉT|ur(t)+xr(t)|=0,|ur(t)+xr(t)|=0,tˉT.

    Lemma 2.1. [quadratic inequality of one variable] If a<0,b2<4ac, then ax2+bx+c<0,xR.

    Proof. The inequality is well known and its proof is omitted.

    In this section, two novel sufficient conditions on the finite-time anti-synchronization for drive-response delayed inertial neural networks (2.1) and (2.2) are derived by applying quadratic inequality of one variable under the fractional and polynomial controllers.

    The controllers in system (2.3) are designed as follows :

    vr(t)=[wr(t)]1[ξ1w2r(t)+β0+c0+2c1t+3c2t2+4c3t3++(ˆk+1)cˆktˆk],wr(t)0, (3.1)

    and

    vr(t)=sign[wr(t)][b(t+a)2+β1+β2w2r(t)+β3[wr(t)]2β4β5], (3.2)

    where sign[wr(t)]={1,wr(t)>0,1,wr(t)<0,0,wr(t)=0,a>0,b<0,β1<0,ξ1>0,β2<0,β3<0,β4>0,β5>0,ˆk is a positive integer, t0,β0>0,c1>0,c2>0,,cˆk>0 with c0ˆI2r<0,β4>ˆIr,β5>ˆIr,b<aM(0),M(0)=ˆnr=1(|wr(0)|+|wr(0)|)+11τˆnr=1ˆnj=1Lj(|drj|0τ(0)|wj(s)|ds+|frj|0τ(0)|wj(s)|ds).

    Theorem 3.1. Under Assumption 1, the master system (2.1) and slave system (2.2) can gain the finite-time anti-synchronization under the controller (3.1) when the following conditions are satisfied for r=1,2,,ˆn:

    (m1)

    ξ1>0.5ˆnj=1(|crj|+|drj|1τ)Lr

    (m2) There exists a constant γr>0 such that

    (γrbr)2<4[1ar+0.5ˆnj=1(|crj|+|drj|1τ)Lj+ˆnj=1|frj|Lj1τ][0.5ˆnj=1(|crj|+|drj|1τ)Lrξ1],

    where, the finite-time t=max{t1,t2},t2=K(0)ˆkβ0,t1 is the only positive real root of the equation ˆI2r+c0+c1t+c2t2++cˆntˆn=0.

    Proof. Without loss of generalization, we assume that wr(t)0,r=1,2,,ˆn. If wr(t)=0, then wr(t) = constant. In the case, by letting ϕur(s)+ϕxr(s)=0,s[α,0], where ϕxr(s) and ϕur(s) are respectively the initial conditions of the solution xr(s) of system (2.1) and the solution ur(s) of system (2.2), the proof of Theorem 3.1 can be finished.

    Introduce a Lyapunov functional as follows:

    K(t)=K1(t)+K2(t),

    where

    K1(t)=12ˆnr=1[dwr(t)dt]2+12ˆnr=1γrw2r(t),
    K2(t)=11τˆnr=1ˆnj=1ttτ(t)|frj|Lj|wj(s)|ds+11τˆnr=1ˆnj=1ttτ(t)|drj|Lj|wj(s)|ds.

    Calculating the derivatives of K1(t) along the solution of system (2.3), one has based on the Assumption 1 as follows:

    K1(t)=ˆnr=1(wr(t)wr(t)+γrwr(t)wr(t))=ˆnr=1{wr(t)(arwr(t)+(γrbr)wr(t)+ˆnj=1crj[fj(uj(t))+fj(xj(t))]+ˆnj=1drj×[fj(uj(qt))+fj(xj(qt))]+ˆnj=1frj[fj(uj(qt))+fj(xj(qt))]+2ˆIr+vr(t))}ˆnr=1{wr(t)(arwr(t)+(γrbr)wr(t)+ˆnj=1|crj||fj(uj(t))+fj([xj(t)])|+ˆnj=1|drj|×|fj(uj(qt))+fj([xj(qt)])|+ˆnj=1|frj||fj(uj(qt))+fj([xj(qt)])|+2ˆIr+vr(t))}ˆnr=1{wr(t)(arwr(t)+(γrbr)wr(t)+ˆnj=1|crj|Lj|wj(t)|+ˆnj=1|drj||wj(qt)|Lj+ˆnj=1|frj||wj(qt)|Lj+2ˆIr)[ξ1w2r(t)+β0+c0+2c1t+3c2t2++(ˆk+1)cˆktˆk]. (3.3)

    At the same time, one has

    K2(t)=11τˆnr=1ˆnj=1|frj|Lj[|wj(t)|(1τ(t))|wj(tτ(t))|]+11τˆnr=1ˆnj=1|drj|×Lj[|wj(t)|(1τ(t))|wj(tτ(t))|]11τˆnr=1ˆnj=1|frj|Lj[|wj(t)|(1τ)|wj(tτ(t))|]+11τˆnr=1ˆnj=1|drj|×Lj[|wj(t)|(1τ)|wj(tτ(t))|]. (3.4)

    Based on (3.3) and (3.4), one obtain

    K(t)ˆnr=1{wr(t)(arwr(t)+(γrbr)wr(t)+ˆnj=1(|crj|+|drj|1τ)Lj|wj(t)|+ˆnj=1|frj|1τ×|wj(t)|Lj+2ˆIr)[ξ1w2r(t)+β0+c0+2c1t+3c2t2++cˆktˆk]},

    from which, by means of using ab0.5(a2+b2), it follows that

    K(t)ˆnr=1{[0.5ˆnj=1(|crj|+|drj|1τ)Lrξ1]w2r(t)+(γrbr)wr(t)wr(t)+[1ar+0.5×
    ˆnj=1(|crj|+|drj|1τ)Lj+ˆnj=1|frj|Lj1τ][wr(t)]2}+ˆn(ˆI2r[β0+c0+2c1t+3c2t2++(ˆk+1)cˆktˆk]). (3.5)

    According to Lemma 2.1, in view of (m1) and (m2), one has

    [0.5ˆnj=1(|crj|+|drj|1τ)Lrξ1]w2r(t)+(γrbr)wr(t)wr(t)+[1ar+0.5׈nj=1(|crj|+|drj|1τ)Lj+ˆnj=1|frj|Lj1τ][wr(t)]2<0. (3.6)

    Substituting (3.6) into (3.5) yields

    K(t)ˆk(ˆI2r[c0+2c1t+3c2t2++(ˆk+1)cˆktˆk])ˆkβ0. (3.7)

    Integrating (3.7) over [0,t] yields

    K(t)K(0)ˆkβ0t+ˆkt[ˆI2r[c0+c1t+c2t2++cˆktˆk]. (3.8)

    Let

    F(t)=ˆI2r+[c0+c1t+c2t2++cˆntˆn],t0.

    Then

    F(0)=c0ˆI2r<0,limtF(t)=+>0.

    So there exists a point t1>0 such that F(t1)=0. Letting

    ˆI2r+[c0+c1t+c2t2++cˆntˆn]=(tt1)[bˆn1tˆn1+bˆn2tˆn2++b1t+b0], (3.9)

    one has

    {bˆn1=cˆn,bˆn2t1bˆn1=cˆn1,bˆn3t1bˆn2=cˆn2,,b1b2t1=c2,b0b1t1=c1,t1b0=c0ˆI2r.

    As a result

    {bˆn1=cˆn>0,bˆn2=cˆn1+t1bˆn1>0,bˆn3=cˆn2+t1bˆn2>0,b1=c2+t1b2>0,b0=c1+b1t1>0,c0ˆI2r=t1b0<0. (3.10)

    Since bi>0,i=0,1,,bˆn1, by (3.9) and (3.10), it follows that the equation

    ˆI2r+[c0+c1t+c2t2++cˆntˆn]=0,

    namely the equation

    (tt1)[bˆn1tˆn1+bˆn2tˆn2++b1t+b0]=0

    has only positive real root t=t1 and when tt1

    ˆI2r+[c0+c1t+c2t2++cˆntˆn]=(tt1)[bˆn1tˆn1+bˆn2tˆn2++b1t+b0]>0.

    That is when tt1

    ˆkt{ˆI2r+[c0+c1t+c2t2++cˆntˆn]=(tt1)[bˆn1tˆn1+bˆn2tˆn2++b1t+b0]}<0. (3.11)

    Because when tt2=K(0)ˆkβ0

    K(0)ˆkβ0t<0, (3.12)

    Then letting t=max{t1,t2}, it follows that when tt, the following two inequalities hold:

    ˆkt{ˆI2r+[c0+c1t+c2t2++cˆntˆn]=(tt1)[bˆn1tˆn1+bˆn2tˆn2++b1t+b0]}<0 (3.13)

    and

    K(0)ˆkβ0t<0. (3.14)

    Substituting (3.13) into (3.14) into (3.8), it follows that when tt

    0K(t)0.

    Consequently, limttK1(t)=0,K1(t)=0,tt.

    Namely, limtt|ur(t)+xr(t)|=0,|ur(t)+xr(t)|=0,tt. This finishes the proof of Theorem 3.1.

    Theorem 3.2. Assume that Assumption 1 holds. Then the master system (2.1) and the slave system (2.2) can reach the finite-time anti-synchronization under the controller (3.2) when the following inequalities hold:

    (l1)

    (1ar+ˆnj=1|frj|1τLj)2<4β3(|ˆIr|β5)

    (l2)

    [br+ˆnj=1Lr(|cjr|+|djr|1τ)]2<4β2(|ˆIr|β4),

    where, the finite-time T=β1a+β21a2+4β1b2β1.

    Proof. Introduce a Lyapunov functional as follows:

    M(t)=M1(t)+M2(t),

    where

    M1(t)=ˆnr=1[|wr(t)|+|wr(t)|],
    M2(t)=11τˆnr=1ˆnj=1Lj(|drj|ttτ(t)|wj(s)|ds+|frj|ttτ(t)|wj(s)|ds).

    Calculating the derivatives of M1(t) along the solution of system (2.3), one has based on the Assumption 1:

    M1(t)=ˆnr=1(sign[wr(t)]wr(t)+sign[wr(t)]wr(t))=ˆnr=1{sign[wr(t)](arwr(t)brwr(t)+ˆnj=1crj[fj(uj(t))+fj(xj(t))]+ˆnj=1drj×[fj(uj(qt))+fj(xj(qt))]+ˆnj=1frj[fj(uj(qt))+fj(xj(qt))]+2ˆIr+vr(t))+sign[wr(t)]×wr(t)}ˆnr=1{(1ar)|wr(t)|+br|wr(t)|+ˆnj=1|crj||fj(uj(t))+fj([xj(t)])|+ˆnj=1|drj|×|fj(uj(qt))+fj([xj(qt)])|+ˆnj=1|frj||fj(uj(qt))+fj([xj(qt)])|+2|ˆIr|β1+ba(t+a)2+β2w2r(t)+β3[wr(t)]2}ˆnr=1{(1ar)|wr(t)|+br|wr(t)|+ˆnj=1|crj|Lj|wj(t)|+ˆnj=1|drj||wj(qt)|Lj+ˆnj=1|frj|×|wj(qt)|Lj+2|ˆIr|β1+ba(t+a)2+β2w2r(t)+β3[wr(t)]2β4β5]. (3.15)

    On the other hand, we have

    M2(t)=11τˆnr=1ˆnj=1Lj(|drj||wj(t)|(1τ(t))|drj||wj(qt)|+|frj||wj(t)|(1τ(t))×|frj||wj(qt)|)11τˆnr=1ˆnj=1Lj(|drj||wj(t)|(1τ)|drj||wj(qt)|+|frj||wj(t)|(1τ)|frj|×|wj(qt)|). (3.16)

    In view of (3.15) and (3.16), one has

    M(t)ˆnr=1{(1ar)|wr(t)|+br|wr(t)|+ˆnj=1Lj[|crj|+|drj|1τ]|wj(t)|+ˆnj=1|frj|1τLj|wj(t)|+2|ˆIr|β1+ba(t+a)2+β2w2r(t)+β3[wr(t)]2β4β5}
    =ˆnr=1{β2|wr(t)|2+[br+ˆnj=1Lr(|cjr|+|djr|1τ)]|wr(t)|+(|ˆIr|β4)+β3|wr(t)|2+(1ar+ˆnj=1|frj|1τLj)|wr(t)|+(|ˆIr|β5)β1+ba(t+a)2} (3.17)

    In view of (l1) and (l2), according Lemma 2.1, one has

    β2|wr(t)|2+[br+ˆnj=1Lr(|cjr|+|djr|1τ)]|wr(t)|+(|ˆIr|β4)<0 (3.18)

    and

    β3|wr(t)|2+(1ar+ˆnj=1|frj|1τLj)|wr(t)|+(|ˆIr|β5)<0. (3.19)

    Substituting (3.18) and (3.19) into (3.17) yields

    M(t)β1+b(t+a)2. (3.20)

    Integrating (3.20) over [0,t] yields

    M(t)M(0)+β1t+bt0ds(s+a)2=M(0)+β1tbt+a+baβ1tbt+a. (3.21)

    Letting β1tbt+a0, then β1t2β1t+b>0. Consequently

    tT=β1a+β21a2+4β1b2β1.

    Thus when tβ1a+β21a2+4β1b2β1, we have by (3.21)

    0M(t)0.

    Namely,

    limtT|ur(t)+xr(t)|=0,|ur(t)xr(t)|=0,tT.

    The proof of Theorem 3.2 is finished.

    Remark 1. In [19,20,21,23,24,25], the integral inequality is used to study the finite-time synchronization (anti-synchronization), in [29], the finite-time stability theory is used to study the finite-time synchronization, but in our paper, without applying above study approaches, the quadratic inequality of one variable is used to study the finite-time anti-synchronization for the master inertial neural networks and the slave inertial neural networks. Hence, our approach of finite-time synchronization for master-slave neural networks is different from these in the existing papers.

    Remark 2. In our paper, by designing different controllers from those in existing papers [16,17,19,20,21,23,24,25,28,29,30,31], namely, by designing the polynomial and fractional controllers, two novel criteria ensuring the finite-time anti-synchronization for the master system (2.1) and the slave system (2.2) are established. Hence, our results on the finite-time synchronization for the master-slave neural networks are novel.

    Remark 3. It is true that the controller (3.1) contain many parameters (ˆk+2 parameters), but (3.1) is only designed in theory. In practice, when we take ˆk=2, then the controller (3.1) only contain 5 parameters. By designing these 5 parameters, we can establish the sufficient condition of the finite-time anti-synchronization for system (2.1) and system (2.2) by putting more large ξ1 and more small γrbr(see (m1) and (m2) in Theorem 3.1).

    Remark 4. In many papers which studied the stability and synchronization of inertial neural networks, the results were obtained on the stability and synchronization for discussed inertial neural networks by transforming the discussed inertial neural networks described with a second order differential equations into the new system described with first order differential equations. Thus to show the stability or synchronization, a Lyapunov functional of wi(t) has to be constructed. In this paper, since without transforming the discussed inertial neural networks described with a second order differential equations into the new system described with first order differential equations, to finish showing the finite-time anti-synchronization, a Lyapunov functional of wi(t) and wi(t) is constructed in each Theorem. By constructing such Lyapunov functionals, without transforming processing and complicated computation, the more concise and easily verified criteria on the finite-time anti-synchronization are acquired.

    Letting xr(t)=yr(t),ur(t)=zr(t), then the delayed inertial neural networks (2.1) and (2.2) reduce to respectively the master system

    {xr(t)=yr(t)yr(t)=aryr(t)brxr(t)+2j=1[crjfj(xj(t))+drjfj(xj(tτ(t)))+frjfj(yj(tτ(t)))+ˆIr] (4.1)

    and the slave system

    {ur(t)=zr(t)zr(t)=arzr(t)brur(t)+2j=1[crjfj(uj(t))+drjfj(uj(tτ(t)))+frjfj(zj(tτ(t)))+vr(t)+ˆIr], (4.2)

    Example 1. Consider the neural networks (4.1) and (4.2) with following controllers:

    vr(t)=[wr(t)]1[ξ1w2r(t)+β0+c0+2c1t+3c2t2+4c3t3++(ˆk+1)cˆktˆk] (4.3)

    where r=2,β0=1.5,ξ1=10,a1=25,a2=30,b1=2.1,b2=0.8,γ1=2,γ2=1,c0=1,c1=0.5,c2=0.3,c3=0.1,c4=0.2,c5=1,c6=0.35,c7=0.4,c8=0.2,c9=0.25,c10=0.15,ˆk=10,ˆI1=7,ˆI2=5, with c0ˆI2r<0,τ(t)=0.2t+1,τ=0.4,0.2=τ(t)<τ<1,fr(x)=0.2x,

    (c11c12c21c22)=(2312),(d11d12d21d22)=(1231),(f11f12f21f22)=(4123).

    Therefore L1=L2=0.2,

    10=ξ1>0.5ˆnj=1(|c1j|+|d1j|1τ)L1=1,
    10=ξ1>0.5ˆnj=1(|c2j|+|d2j|1τ)L2=0.9667,
    0.01=(γ1b1)2<4[1a1+0.5ˆnj=1(|c1j|+|d1j|1τ)Lj+ˆnj=1|f1j|Lj1τ]×[0.5ˆnj=1(|c1j|+|d1j|1τ)L1ξ1]=798.
    0.04=(γ2b2)2<4[1a2+0.5ˆnj=1(|c2j|+|d2j|1τ)Lj+ˆnj=1|f2j|Lj1τ]×[0.5ˆnj=1(|c2j|+|d2j|1τ)L2ξ1]=982.8267.

    The all conditions are satisfied. Based on Theorem 3.1, the system (4.1) and system (4.2) are finite-time anti-synchronization. In the existing papers, the controllers designed are not related to the time variable t, hence, the result in the example cannot verified with these theorems in the existing papers [18,19,20,21,22,23,24,25,26,27,28,29].

    Letting x1(0)=1.12,x2(0)=2.1,y1(0)=50,y2(0)=50,u1(0)=1,u2(0)=2,z1(0)=45,z2(0)=45, then the finite-time anti-synchronization diagrams can be seen in Figures 13.

    Figure 1.  Curves of the xr(t), yr(t).
    Figure 2.  Curves of the ur(t), zr(t).
    Figure 3.  Curves of the wr(t), er(t).

    Example 2. Consider the master system (4.1) and the slave system (4.2) with controllers (3.2) as follows :

    vr(t)=sign[wr(t)][b(t+a)2+β1+β2w2r(t)+β3[wr(t)]2β4β5], (4.4)

    where r=2,β1=2,β2=10,β3=8,β4=5,β5=7.5,a1=1,a2=1.2,b1=0.2,b2=0.3,a=1,b=30,ˆI1=1,ˆI2=1.5, with 5=β4>ˆIr,7.5=β5>ˆIr,τ(t)=0.3t,τ=0.5,0.3=τ(t)<τ<1,fr(x)=0.1x.

    (c11c12c21c22)=(0.30.10.20.4),(d11d12d21d22)=(0.20.30.10.1),(f11f12f21f22)=(0.40.20.30.2).

    Therefore L1=L2=0.1,

    0.0144=(1a1+ˆnj=1|f1j|1τLj)2<4β3(ˆI1β5)=208
    0.0100=(1a2+ˆnj=1|f2j|1τLj)2<4β3(ˆI2β5)=192
    0.5776=[b1+ˆnj=1L1(|cj1|+|dj1|1τ)]2<4β2(|ˆI1|β4)=160
    0.7744=[b2+ˆnj=1L2(|cj2|+|dj2|1τ)]2<4β2(|ˆI2|β4)=140.

    Let w1(s)=u1(s)+x1(s)=s1+2s+1=3s,w2(s)=u2(s)+x2(s)=2s3+s+3=3s,wj(s)=(3s)=3,wj(0)=0,x1(0)=1,x2(0)=3,y1(0)=1,y2(0)=2,u1(0)=1,u2(0)=3,z1(0)=1,z2(0)=1.

    Then

    M(0)=ˆnr=1(|wr(0)|+|wr(0)|)+11τˆnr=1ˆnj=1Lj(|drj|0τ(0)|wj(s)|ds+|frj|0τ(0)|wj(s)|ds)=6,

    so 30=b<aM(0)=6. By Theorem 3.2, the system (4.1) and system (4.2) are finite-time anti-synchronization. Since the controllers of time variable t are designed, while in the existing papers [17,23,24,25,26,27], the controllers related to the time variable t were not designed, thus the results in the example cannot be verified with the theorems in [19,25,26,27,28,29].

    The finite-time anti-synchronization diagrams can be seen in Figures 46.

    Figure 4.  Curves of the xr(t), yr(t).
    Figure 5.  Curves of the ur(t), zr(t).
    Figure 6.  Curves of the wr(t), er(t).

    This paper discusses the finite-time anti-synchronization for the master-slave delayed inertial neural networks. Without making the variable transformation, the inertial system was analyzed directly. By making use of the quadratic inequality of one variable under the fractional and polynomial controllers, two novel sufficient conditions are obtained to ensure the finite-time anti-synchronization between the master system and the slave system. Applying the quadratic inequality of one variable and the fractional and polynomial controllers of the time variable t, our results obtained are more concise and easily verified and more objective and practical than these in the existing papers [16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31]. Our future works are using the more quadratic inequality to discuss the finite-time anti-synchronization for the master-slave delayed inertial neural networks, there are many problems in this field that deserve further study.

    We are thankful to the reviewers for their constructive comments which help us to improve the manuscript. The work was supported by Basic research expenses for provincial colleges and universities under grant number JYT2020030.

    The authors declare that there is no conflict of interests regarding the publication of this paper.



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