
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)dt−brxr(t)+Fr(x′(t),x(t)),r=1,2,⋯,ˆn, | (2.1) |
where
Fr(x′(t),x(t))=ˆn∑j=1crjfj(xj(t))+ˆn∑j=1drjfj(xj(qt))+ˆn∑j=1frjfj(x′j(qt))+ˆIr, |
x(t)=(x1(t),x2(t),⋯,xˆn(t))T∈Rˆn,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=t−τ(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=maxt∈R{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)dt−brur(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)dt−brwr(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))=ˆn∑j=1crj[fj(uj(t))+fj(xj(t))]+ˆn∑j=1drj[fj(uj(qt))+fj(xj(qt))]+ˆn∑j=1frj[fj(u′j(qt))+fj(x′j(qt))]. |
Assumption 1. The activation function fj is odd, and there exists a constant Lj≥0 such that
|fj(w)−fj(z)|≤Lj|w−z|,j=1,2,⋯,ˆn,w,z∈R. |
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,
limt→ˉT|ur(t)+xr(t)|=0,|ur(t)+xr(t)|=0,t≥ˉT. |
Lemma 2.1. [quadratic inequality of one variable] If a<0,b2<4ac, then ax2+bx+c<0,x∈R.
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)=−[w′r(t)]−1[ξ1w2r(t)+β0+c0+2c1t+3c2t2+4c3t3+⋯+(ˆk+1)cˆktˆk],w′r(t)≠0, | (3.1) |
and
vr(t)=sign[w′r(t)][b(t+a)2+β1+β2w2r(t)+β3[w′r(t)]2−β4−β5], | (3.2) |
where sign[w′r(t)]={1,w′r(t)>0,−1,w′r(t)<0,0,w′r(t)=0,a>0,b<0,β1<0,ξ1>0,β2<0,β3<0,β4>0,β5>0,ˆk is a positive integer, t≥0,β0>0,c1>0,c2>0,⋯,cˆk>0 with c0−ˆI2r<0,β4>ˆIr,β5>ˆIr,b<−aM(0),M(0)=ˆn∑r=1(|wr(0)|+|w′r(0)|)+11−τˆn∑r=1ˆn∑j=1Lj(|drj|∫0−τ(0)|w′j(s)|ds+|frj|∫0−τ(0)|w′j(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>0.5ˆn∑j=1(|crj|+|drj|1−τ)Lr |
(m2) There exists a constant γr>0 such that
(γr−br)2<4[1−ar+0.5ˆn∑j=1(|crj|+|drj|1−τ)Lj+ˆn∑j=1|frj|Lj1−τ][0.5ˆn∑j=1(|crj|+|drj|1−τ)Lr−ξ1], |
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 w′r(t)≠0,r=1,2,⋯,ˆn. If w′r(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)=12ˆn∑r=1[dwr(t)dt]2+12ˆn∑r=1γrw2r(t), |
K2(t)=11−τˆn∑r=1ˆn∑j=1∫tt−τ(t)|frj|Lj|w′j(s)|ds+11−τˆn∑r=1ˆn∑j=1∫tt−τ(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:
K′1(t)=ˆn∑r=1(w′r(t)w″r(t)+γrwr(t)w′r(t))=ˆn∑r=1{w′r(t)(−arw′r(t)+(γr−br)wr(t)+ˆn∑j=1crj[fj(uj(t))+fj(xj(t))]+ˆn∑j=1drj×[fj(uj(qt))+fj(xj(qt))]+ˆn∑j=1frj[fj(u′j(qt))+fj(x′j(qt))]+2ˆIr+vr(t))}≤ˆn∑r=1{w′r(t)(−arw′r(t)+(γr−br)wr(t)+ˆn∑j=1|crj||fj(uj(t))+fj(−[−xj(t)])|+ˆn∑j=1|drj|×|fj(uj(qt))+fj(−[−xj(qt)])|+ˆn∑j=1|frj||fj(u′j(qt))+fj(−[−x′j(qt)])|+2ˆIr+vr(t))}≤ˆn∑r=1{w′r(t)(−arw′r(t)+(γr−br)wr(t)+ˆn∑j=1|crj|Lj|wj(t)|+ˆn∑j=1|drj||wj(qt)|Lj+ˆn∑j=1|frj||w′j(qt)|Lj+2ˆIr)−[ξ1w2r(t)+β0+c0+2c1t+3c2t2+⋯+(ˆk+1)cˆktˆk]. | (3.3) |
At the same time, one has
K′2(t)=11−τˆn∑r=1ˆn∑j=1|frj|Lj[|w′j(t)|−(1−τ′(t))|w′j(t−τ(t))|]+11−τˆn∑r=1ˆn∑j=1|drj|×Lj[|wj(t)|−(1−τ′(t))|wj(t−τ(t))|]≤11−τˆn∑r=1ˆn∑j=1|frj|Lj[|w′j(t)|−(1−τ)|w′j(t−τ(t))|]+11−τˆn∑r=1ˆn∑j=1|drj|×Lj[|wj(t)|−(1−τ)|wj(t−τ(t))|]. | (3.4) |
Based on (3.3) and (3.4), one obtain
K′(t)≤ˆn∑r=1{w′r(t)(−arw′r(t)+(γr−br)wr(t)+ˆn∑j=1(|crj|+|drj|1−τ)Lj|wj(t)|+ˆn∑j=1|frj|1−τ×|w′j(t)|Lj+2ˆIr)−[ξ1w2r(t)+β0+c0+2c1t+3c2t2+⋯+cˆktˆk]}, |
from which, by means of using ab≤0.5(a2+b2), it follows that
K′(t)≤ˆn∑r=1{[0.5ˆn∑j=1(|crj|+|drj|1−τ)Lr−ξ1]w2r(t)+(γr−br)w′r(t)wr(t)+[1−ar+0.5× |
ˆn∑j=1(|crj|+|drj|1−τ)Lj+ˆn∑j=1|frj|Lj1−τ][w′r(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
[0.5ˆn∑j=1(|crj|+|drj|1−τ)Lr−ξ1]w2r(t)+(γr−br)w′r(t)wr(t)+[1−ar+0.5׈n∑j=1(|crj|+|drj|1−τ)Lj+ˆn∑j=1|frj|Lj1−τ][w′r(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],t≥0. |
Then
F(0)=c0−ˆI2r<0,limt→∞F(t)=+∞>0. |
So there exists a point t1>0 such that F(t1)=0. Letting
−ˆI2r+[c0+c1t+c2t2+⋯+cˆntˆn]=(t−t1)[bˆn−1tˆn−1+bˆn−2tˆn−2+⋯+b1t+b0], | (3.9) |
one has
{bˆn−1=cˆn,bˆn−2−t1bˆn−1=cˆn−1,bˆn−3−t1bˆn−2=cˆn−2,⋯⋯⋯⋯⋯⋯⋯,b1−b2t1=c2,b0−b1t1=c1,−t1b0=c0−ˆI2r. |
As a result
{bˆn−1=cˆn>0,bˆn−2=cˆn−1+t1bˆn−1>0,bˆn−3=cˆn−2+t1bˆn−2>0,⋯⋯⋯⋯⋯⋯b1=c2+t1b2>0,b0=c1+b1t1>0,c0−ˆI2r=−t1b0<0. | (3.10) |
Since bi>0,i=0,1,⋯,bˆn−1, by (3.9) and (3.10), it follows that the equation
−ˆI2r+[c0+c1t+c2t2+⋯+cˆntˆn]=0, |
namely the equation
(t−t1)[bˆn−1tˆn−1+bˆn−2tˆn−2+⋯+b1t+b0]=0 |
has only positive real root t=t1 and when t≥t1
−ˆI2r+[c0+c1t+c2t2+⋯+cˆntˆn]=(t−t1)[bˆn−1tˆn−1+bˆn−2tˆn−2+⋯+b1t+b0]>0. |
That is when t≥t1
−ˆkt{−ˆI2r+[c0+c1t+c2t2+⋯+cˆntˆn]=−(t−t1)[bˆn−1tˆn−1+bˆn−2tˆn−2+⋯+b1t+b0]}<0. | (3.11) |
Because when t≥t2=K(0)ˆkβ0
K(0)−ˆkβ0t<0, | (3.12) |
Then letting t∗=max{t1,t2}, it follows that when t≥t∗, the following two inequalities hold:
−ˆkt{−ˆI2r+[c0+c1t+c2t2+⋯+cˆntˆn]=(t−t1)[bˆn−1tˆn−1+bˆn−2tˆn−2+⋯+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 t≥t∗
0≤K(t)≤0. |
Consequently, limt→t∗K1(t)=0,K1(t)=0,t≥t∗.
Namely, limt→t∗|ur(t)+xr(t)|=0,|ur(t)+xr(t)|=0,t≥t∗. 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)
(1−ar+ˆn∑j=1|frj|1−τLj)2<4β3(|ˆIr|−β5) |
(l2)
[br+ˆn∑j=1Lr(|cjr|+|djr|1−τ)]2<4β2(|ˆIr|−β4), |
where, the finite-time T∗=β1a+√β21a2+4β1b−2β1.
Proof. Introduce a Lyapunov functional as follows:
M(t)=M1(t)+M2(t), |
where
M1(t)=ˆn∑r=1[|wr(t)|+|w′r(t)|], |
M2(t)=11−τˆn∑r=1ˆn∑j=1Lj(|drj|∫tt−τ(t)|wj(s)|ds+|frj|∫tt−τ(t)|w′j(s)|ds). |
Calculating the derivatives of M1(t) along the solution of system (2.3), one has based on the Assumption 1:
M′1(t)=ˆn∑r=1(sign[w′r(t)]w″r(t)+sign[wr(t)]w′r(t))=ˆn∑r=1{sign[w′r(t)](−arw′r(t)−brwr(t)+ˆn∑j=1crj[fj(uj(t))+fj(xj(t))]+ˆn∑j=1drj×[fj(uj(qt))+fj(xj(qt))]+ˆn∑j=1frj[fj(u′j(qt))+fj(x′j(qt))]+2ˆIr+vr(t))+sign[wr(t)]×w′r(t)}≤ˆn∑r=1{(1−ar)|w′r(t)|+br|wr(t)|+ˆn∑j=1|crj||fj(uj(t))+fj(−[−xj(t)])|+ˆn∑j=1|drj|×|fj(uj(qt))+fj(−[−xj(qt)])|+ˆn∑j=1|frj||fj(u′j(qt))+fj(−[−x′j(qt)])|+2|ˆIr|−β1+b−a(t+a)2+β2w2r(t)+β3[w′r(t)]2}≤ˆn∑r=1{(1−ar)|w′r(t)|+br|wr(t)|+ˆn∑j=1|crj|Lj|wj(t)|+ˆn∑j=1|drj||wj(qt)|Lj+ˆn∑j=1|frj|×|w′j(qt)|Lj+2|ˆIr|−β1+b−a(t+a)2+β2w2r(t)+β3[w′r(t)]2−β4−β5]. | (3.15) |
On the other hand, we have
M′2(t)=11−τˆn∑r=1ˆn∑j=1Lj(|drj||wj(t)|−(1−τ′(t))|drj||wj(qt)|+|frj||w′j(t)|−(1−τ′(t))×|frj||w′j(qt)|)≤11−τˆn∑r=1ˆn∑j=1Lj(|drj||wj(t)|−(1−τ)|drj||wj(qt)|+|frj||w′j(t)|−(1−τ)|frj|×|w′j(qt)|). | (3.16) |
In view of (3.15) and (3.16), one has
M′(t)≤ˆn∑r=1{(1−ar)|w′r(t)|+br|wr(t)|+ˆn∑j=1Lj[|crj|+|drj|1−τ]|wj(t)|+ˆn∑j=1|frj|1−τLj|w′j(t)|+2|ˆIr|−β1+b−a(t+a)2+β2w2r(t)+β3[w′r(t)]2−β4−β5} |
=ˆn∑r=1{β2|wr(t)|2+[br+ˆn∑j=1Lr(|cjr|+|djr|1−τ)]|wr(t)|+(|ˆIr|−β4)+β3|w′r(t)|2+(1−ar+ˆn∑j=1|frj|1−τLj)|w′r(t)|+(|ˆIr|−β5)−β1+b−a(t+a)2} | (3.17) |
In view of (l1) and (l2), according Lemma 2.1, one has
β2|wr(t)|2+[br+ˆn∑j=1Lr(|cjr|+|djr|1−τ)]|wr(t)|+(|ˆIr|−β4)<0 | (3.18) |
and
β3|w′r(t)|2+(1−ar+ˆn∑j=1|frj|1−τLj)|w′r(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+b∫t0ds(s+a)2=M(0)+β1t−bt+a+ba≤β1t−bt+a. | (3.21) |
Letting β1t−bt+a≤0, then −β1t2−β1t+b>0. Consequently
t≥T∗=β1a+√β21a2+4β1b−2β1. |
Thus when t≥β1a+√β21a2+4β1b−2β1, we have by (3.21)
0≤M(t)≤0. |
Namely,
limt→T∗|ur(t)+xr(t)|=0,|ur(t)−xr(t)|=0,t≥T∗. |
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 γr−br(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 w′i(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 x′r(t)=yr(t),ur(t)=zr(t), then the delayed inertial neural networks (2.1) and (2.2) reduce to respectively the master system
{x′r(t)=yr(t)y′r(t)=−aryr(t)−brxr(t)+2∑j=1[crjfj(xj(t))+drjfj(xj(t−τ(t)))+frjfj(yj(t−τ(t)))+ˆIr] | (4.1) |
and the slave system
{u′r(t)=zr(t)z′r(t)=−arzr(t)−brur(t)+2∑j=1[crjfj(uj(t))+drjfj(uj(t−τ(t)))+frjfj(zj(t−τ(t)))+vr(t)+ˆIr], | (4.2) |
Example 1. Consider the neural networks (4.1) and (4.2) with following controllers:
vr(t)=−[w′r(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 c0−ˆI2r<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>0.5ˆn∑j=1(|c1j|+|d1j|1−τ)L1=1, |
10=ξ1>0.5ˆn∑j=1(|c2j|+|d2j|1−τ)L2=0.9667, |
0.01=(γ1−b1)2<4[1−a1+0.5ˆn∑j=1(|c1j|+|d1j|1−τ)Lj+ˆn∑j=1|f1j|Lj1−τ]×[0.5ˆn∑j=1(|c1j|+|d1j|1−τ)L1−ξ1]=798. |
0.04=(γ2−b2)2<4[1−a2+0.5ˆn∑j=1(|c2j|+|d2j|1−τ)Lj+ˆn∑j=1|f2j|Lj1−τ]×[0.5ˆn∑j=1(|c2j|+|d2j|1−τ)L2−ξ1]=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 1–3.
Example 2. Consider the master system (4.1) and the slave system (4.2) with controllers (3.2) as follows :
vr(t)=sign[w′r(t)][b(t+a)2+β1+β2w2r(t)+β3[w′r(t)]2−β4−β5], | (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=(1−a1+ˆn∑j=1|f1j|1−τLj)2<4β3(ˆI1−β5)=208 |
0.0100=(1−a2+ˆn∑j=1|f2j|1−τLj)2<4β3(ˆI2−β5)=192 |
0.5776=[b1+ˆn∑j=1L1(|cj1|+|dj1|1−τ)]2<4β2(|ˆI1|−β4)=160 |
0.7744=[b2+ˆn∑j=1L2(|cj2|+|dj2|1−τ)]2<4β2(|ˆI2|−β4)=140. |
Let w1(s)=u1(s)+x1(s)=s−1+2s+1=3s,w2(s)=u2(s)+x2(s)=2s−3+s+3=3s,w′j(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)=ˆn∑r=1(|wr(0)|+|w′r(0)|)+11−τˆn∑r=1ˆn∑j=1Lj(|drj|∫0−τ(0)|w′j(s)|ds+|frj|∫0−τ(0)|w′j(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 4–6.
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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