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R E S E A R C H

Open Access

Global robust exponential synchronization of

BAM recurrent FNNs with infinite distributed

delays and diffusion terms on time scales

Kaihong Zhao

*

*Correspondence:

[email protected] Department of Applied

Mathematics, Kunming University of Science and Technology, Kunming, Yunnan 650093, People’s Republic of China

Abstract

In this article, the global robust exponential synchronization of reaction-diffusion BAM recurrent fuzzy neural networks (FNNs) with infinite distributed delays on time scales is investigated. Applied Lyapunov functional and inequality skills, some sufficient criteria are established to guarantee the global robust exponential synchronization of reaction-diffusion BAM recurrent FNNs with infinite distributed delays on time scales. One example is given to illustrate the effectiveness of our results.

Keywords: globally robust exponential synchronization; reaction-diffusion BAM recurrent FNNs; infinite distributed delays; Lyapunov functional; time scales

1 Introduction

The study on the artificial neural networks has attracted much attention because of their potential applications such as signal processing, image processing, pattern classification, quadratic optimization, associative memory, moving object speed detection,etc. Many kinds of models of neural networks have been proposed by some famous scholars. One of these important neural network models is the bidirectional associative memory (BAM) neural network models, which were first introduced by Kosko [–]. It is a special class of recurrent neural networks that can store bipolar vector pairs. The BAM neural network is composed of neurons arranged in two layers, the X-layer and the Y-layer. The neurons in one layer are fully interconnected to the neurons in the other layer. Through iterations of forward and backward information flows between the two layers, it performs a two-way associative search for stored bipolar vector pairs and generalize the single-layer auto-associative Hebbian correlation to a two-layer pattern-matched heteroauto-associative circuits. Therefore, this class of networks possesses good application prospects in some fields such as pattern recognition, signal and image process, artificial intelligence []. In general, ar-tificial neural networks have complex dynamical behaviors such as stability, synchroniza-tion, periodic or almost periodic solutions, invariant sets and attractors, and so forth. We can refer to [–] and the references cited therein. Therefore, the analysis of dynamical behaviors for neural networks is a necessary step for practical design of neural networks. As one of the famous neural network models, it has attracted many attention in the past two decades [–] since the BAM model was proposed by Kosko. The dynamical be-haviors such as uniqueness, global asymptotic stability, exponential stability and invariant

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sets and attractors of the equilibrium point or periodic solutions were investigated for BAM neural networks with different types of time delays (see [–, ]).

Synchronization has attracted much attention after it was proposed by Carrolet al.[, ]. The principle of drive-response synchronization is this: the driver system sends a signal through a channel to the responder system, which uses this signal to synchronize itself with the driver. Namely, the response system is influenced by the behavior of the drive system, but the drive system is independent of the response one. In recent years, many results concerning a synchronization problem of time lag neural networks have been investigated in the literature [, , –, , , , ].

As is well known, both in biological and man-made neural networks, strictly speaking, diffusion effects cannot be avoided when electrons are moving in asymmetric electromag-netic fields, so we must consider that the activations vary in space as well as in time. Many researchers have studied the dynamical properties of continuous time reaction-diffusion neural networks (see, for example, [, , , , , , , , ]).

However, in mathematical modeling of real world problems, we will encounter some other inconveniences such as complexity and uncertainty or vagueness. Fuzzy theory is considered as a more suitable setting for the sake of taking vagueness into consideration. Based on traditional cellular neural networks (CNNs), T Yang and LB Yang proposed the fuzzy CNNs (FCNNs) [] which integrate fuzzy logic into the structure of traditional CNNs and maintain local connectedness among cells. Unlike previous CNNs structures, FCNNs have fuzzy logic between their template input and/or output besides the sum of product operation. FCNNs are very a useful paradigm for image processing problems, which is a cornerstone in image processing and pattern recognition. Therefore, it is nec-essary to consider both the fuzzy logic and delay effect on dynamical behaviors of neural networks. To the best of our knowledge, few authors have considered the synchronization of reaction-diffusion recurrent fuzzy neural networks with delays and Dirichlet boundary conditions on time scales which is a challenging and important problem in theory and application. Therefore, in this paper, we will investigate the global robust exponential syn-chronization of delayed reaction-diffusion BAM recurrent fuzzy neural networks (FNNs) on time scales as follows:

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

u

i (t,x) =

l

k=∂∂xk(aik

∂ui

∂xk) –biui(t,x) +

m

j=cijfj(vj(tτ,x)) +Ii

+nj=pijFj(uj(tτ,x)) +

n

j=rij

+∞

kij(s)Fj(uj(ts,x))s + nj=qijFj(uj(tτ,x)) + nj=wij

+∞

kij(s)Fj(uj(ts,x))s +nj=dijμj+

n

j=Sijμj+ nj=Tijμj,

v

j (t,x) =

l

k=

∂xk(ξjk

∂vj

∂xk) –ηjvj(t,x) +

n

i=ζjigi(ui(tτ,x)) +Jj

+mi=λjiGi(vi(tτ,x)) +

m

i=ρji

+∞

κji(s)Gi(vi(ts,x))s + mi=πjiGi(vi(tτ,x)) + mi=σji

+∞

κji(s)Gi(vi(ts,x))s

+mi=hjiνi+

m

i=Mjiνi+ mi=Njiνi,

(.)

subject to the following initial conditions

ui(s,x) =φi(s,x), (s,x)∈[–τ, ]T×,

(3)

and Dirichlet boundary conditions

ui(t,x) = , (t,x)∈[,∞)T×,

vj(t,x) = , (t,x)∈[,∞)T×,

(.)

wherei= , , . . . ,n;j= , , . . . ,m.T⊂Ris a time scale andT∩[, +∞)[, +∞)Tis un-bounded andT∩[–τ, ][τ, ]T=φ.τ>  is constant time delay.x= (x,x, . . . ,xl)T

⊂Rland={x= (x,x, . . . ,xl)T:|xi|<li,i= , , . . . ,l}is a bounded compact set with

smooth boundary in space Rl. u= (u

,u, . . . ,un)T∈Rn, v= (v,v, . . . ,vm)T ∈Rm.

ui(t,x) andvj(t,x) are the state of theith neurons and thejth neurons at timetand in

spacex, respectively.I= (I,I, . . . ,In)T∈RnandJ= (J,J, . . . ,Jm)T∈Rmare constant

in-put vectors. The smooth functions aik>  andξjk >  correspond to the transmission

diffusion operators along with theith neurons and thejth neurons, respectively.bi> ,

ηj> ,μj,νi,cij,pij, rij, qij, wij,dij,Sij,Tij, ζji, λji, ρji, πji,σji,hji, Mji,Mjiare constants.

biandηjdenote the rate with which theith neurons andjth neurons will reset their

po-tential to the resting state in isolation when disconnected from the network and external inputs, respectively.cij,pij,rij, qij,wij,dij,Sij,Tij, ζji,λji,ρji,πji, σji, hji,Mji,Mji denote

the connection weights.fj(·) (j= , , . . . ,m) andgi(·) (i= , , . . . ,n) denote the activation

function of the jth neurons of Y-layer on theith neurons of X-layer and theith neu-rons of X-layer on thejth neurons of Y-layer at timetand in spacex, respectively.Fj(·)

(j= , , . . . ,n) denotes the fuzzy activation function of thejth neurons on theith neu-rons inside of X-layer.Gi(·) (i= , , . . . ,m) denotes the fuzzy activation function of the

ith neurons on thejth neurons inside of Y-layer.μj(j= , , . . . ,n) denotes the bias of the

jth neurons on theith neurons inside of X-layer.νi(i= , , . . . ,m) denotes the bias of the

ith neurons on thejth neurons inside of Y-layer., denote the fuzzy AND and fuzzy OR operations, respectively. φ(t,x) = (φ(t,x),φ(t,x), . . . ,φn(t,x))T: [–τ, ]T×→Rn,

ϕ(t,x) = (ϕ(t,x),ϕ(t,x), . . . ,ϕm(t,x))T: [–τ, ]T×→Rmare rd-continuous with respect tot∈[–τ, ]Tand continuous with respect tox.

In order to investigate the global robust exponential synchronization for system (.)-(.), the quantitiesbi,aik,cij,pij,rij,qij,wij,ηj,ξjk,ζji,λji,ρji,πjiandσjimay be considered

as intervals as follows:  <bibi<∞,aikaikaik,|cij| ≤ |cij| ≤ |cij|,|pij| ≤ |pij| ≤ |pij|,

|rij| ≤ |rij| ≤ |rij|,|qij| ≤ |qij| ≤ |qij|,|wij| ≤ |wij| ≤ |wij|,  <ηjηj<∞,ξjkξjkξjk,

|ζ

ji| ≤ |ζji| ≤ |ζji|,|λji| ≤ |λji| ≤ |λji|,|ρji| ≤ |ρji| ≤ |ρji|,|πji| ≤ |πji| ≤ |πji|,|σji| ≤ |σji| ≤

|σji|.

Take the time scaleT=R(real number set), then system (.)-(.) can be changed into the following continuous case (.)-(.):

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

∂ui(t,x)

∂t =

l

k=

∂xk(aik

∂ui

∂xk) –biui(t,x) +

m

j=cijfj(vj(tτ,x)) +Ii

+nj=pijFj(uj(tτ,x)) +

n

j=rij

+∞

kij(s)Fj(uj(ts,x)) ds

+ nj=qijFj(uj(tτ,x)) + nj=wij

+∞

kij(s)Fj(uj(ts,x)) ds +nj=dijμj+

n

j=Sijμj+ nj=Tijμj,

∂vj(t,x)

∂t =

l k=

∂xk(ξjk

∂vj

∂xk) –ηjvj(t,x) +

n

i=ζjigi(ui(tτ,x)) +Jj

+mi=λjiGi(vi(tτ,x)) +

m

i=ρji

+∞

κji(s)Gi(vi(ts,x)) ds + mi=πjiGi(vi(tτ,x)) + mi=σji

+∞

κji(s)Gi(vi(ts,x)) ds +mi=hjiνi+

m

i=Mjiνi+ mi=Njiνi,

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subject to the following initial conditions

ui(s,x) =φi(s,x), (s,x)∈[–τ, ]×,

vj(s,x) =ϕj(s,x), (s,x)∈[–τ, ]×,

(.)

and Dirichlet boundary conditions

ui(t,x) = , (t,x)∈[,∞)×,

vj(t,x) = , (t,x)∈[,∞)×.

(.)

Take the time scaleT=Z(integer number set), then system (.)-(.) can be changed into the following discrete case (.)-(.):

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

tui(t,x) =

l k=

∂xk(aik

∂ui

∂xk) –biui(t,x) +

m

j=cijfj(vj(tτ,x)) +Ii

+nj=pijFj(uj(tτ,x)) +

n

j=rij

s=kij(s)Fj(uj(ts,x))

+ nj=qijFj(uj(tτ,x)) + nj=wij

s=kij(s)Fj(uj(ts,x))

+nj=dijμj+

n

j=Sijμj+ nj=Tijμj,

tvj(t,x) =

l k=

∂xk(ξjk

∂vj

∂xk) –ηjvj(t,x) +

n

i=ζjigi(ui(tτ,x)) +Jj

+mi=λjiGi(vi(tτ,x)) +

m

i=ρji

s=κji(s)Gi(vi(ts,x))

+ mi=πjiGi(vi(tτ,x)) + mi=σji

s=κji(s)Gi(vi(ts,x))

+mi=hjiνi+

m

i=Mjiνi+ mi=Njiνi,

(.)

subject to the following initial conditions

ui(s,x) =φi(s,x), (s,x)∈ {–τ, –τ+ , . . . , –, –, } ×,

vj(s,x) =ϕj(s,x), (s,x)∈ {–τ, –τ+ , . . . , –, –, } ×,

(.)

and Dirichlet boundary conditions

ui(t,x) = , (t,x)∈Z+×,

vj(t,x) = , (t,x)∈Z+×,

(.)

where t∈Z, τ is a positive integer, Z+={, , , . . .}, tui(t,x)ui(t+ ,x) –ui(t,x),

tvj(t,x)vj(t+ ,x) –vj(t,x).

If we chooseT=R, thenσ(t) =t,μ(t) = . In this case, system (.)-(.) is the contin-uous reaction-diffusion BAM recurrent FNNs (.)-(.). IfT=Z, thenμ(t) = , system (.)-(.) is the discrete difference reaction-diffusion BAM recurrent FNNs (.)-(.). In this paper, we study the global robust exponential synchronization of reaction-diffusion BAM recurrent FNNs (.)-(.), which unify both the continuous case and the discrete difference case. What is more, system (.)-(.) is a good model for handling many prob-lems such as predator-prey forecast or optimizing of goods output.

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2 Preliminaries

In this section, we first recall some basic definitions and lemmas on time scales which are used in what follows.

LetTbe a nonempty closed subset (time scale) ofR. The forward and backward jump operatorsρ,σ:T→Tand the graininessμ:→R+are defined, respectively, by

σ(t) =inf{s∈T:s>t},

ρ(t) =sup{s∈T:s<t},

μ(t) =σ(t) –t.

A pointt∈Tis called left-dense ift>infTandρ(t) =t, left-scattered ifρ(t) <t, right-dense ift<supTandσ(t) =t, and right-scattered ifσ(t) >t. IfThas a left-scattered maxi-mumm, thenTk=T\ {m}, otherwiseTk=T. IfThas a right-scattered minimumm, then

Tk=T\ {m}, otherwiseTk=T.

Definition .([]) A functionf:T→Ris called regulated provided its right-hand side limits exist (finite) at all right-hand side points inTand its left-hand side limits exist (finite) at all left-hand side points inT.

Definition .([]) A functionf :T→Ris called rd-continuous provided it is con-tinuous at right-dense point in Tand its left-hand side limits exist (finite) at left-dense points inT. The set of rd-continuous functionf :T→Rwill be denoted byCrd=Crd(T) =

Crd(T,R).

Definition .([]) Assumef:T→Randt∈Tk. Then we definef(t) to be the number

(if it exists) with the property that given any>  there exists a neighborhoodUoft(i.e.,

U= (t,t+)∩Tfor some> ) such that (t)–f(s)–f(t)σ(t) –s<σ(t) –s

for allsU. We callf(t) the delta (or Hilger) derivative off att. The set of functions f :T→Rthat is a differentiable and whose derivative is rd-continuous is denoted byC

rd=

Crd(T) =Crd(R,T).

Iff is continuous, thenf is rd-continuous. Iff is rd-continuous, thenf is regulated. Iff

is delta differentiable att, thenf is continuous att.

Lemma .([]) Let f be regulated,then there exists a function F which is delta differen-tiable with region of differentiation D such that F(t) =f(t)for all tD.

Definition .([]) Assume thatf :T→Ris a regulated function. Any functionFas in Lemma . is called a-antiderivative off. We define the indefinite integral of a regulated functionf by

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whereCis an arbitrary constant andFis a-antiderivative off. We define the Cauchy integral byabf(s)s=F(b) –F(a) for alla,b∈T.

A functionF:T→Ris called an antiderivative off :T→RprovidedF(t) =f(t) for

allt∈Tk.

Lemma .([]) If a,b∈T,α,β∈Rand f,gC(T,R),then

(i) ab[αf(t) +βg(t)]t=αabf(t)t+βabg(t)t, (ii) iff(t)≥for allatb,thenabf(t)t≥,

(iii) if|f(t)| ≤g(t)on[a,b){t∈T:atb},then|abf(t)t| ≤abg(t)t.

A functionp:T→Ris called regressive if  +μ(t)p(t)=  for allt∈Tk. The set of all

regressive and rd-continuous functionsf :T→Rwill be denoted byR=R(T) =R(T,R). We define the setR+of all positively regressive elements ofRbyR+=R+(T,R) ={p

R:  +μ(t)p(t) >  for allt∈T}. Ifpis a regressive function, then the generalized expo-nential functionep(t,s) is defined byep(t,s) =exp{

t

sξμ(τ)(p(τ))τ}for alls,t∈T, with the

cylinder transformation

ξh(z) =

Log (+hz)

h , ifh= ,

z, ifh= .

Letp,q:T→Rbe two regressive functions, we define

pq=p+q+μpq,

p= – p

 +μp,

pq=pp(q).

IfpR+, thenp∈R+.

The generalized exponential function has the following properties.

Lemma .([]) Assume that p,q:T→Rare two regressive functions,then

(i) ep(σ(t),s) = ( +μ(t)p(t))ep(t,s);

(ii) /ep(t,s) =ep(t,s);

(iii) ep(t,s) = /ep(s,t) =ep(s,t);

(iv) ep(t,s)ep(s,r) =ep(t,r);

(v) [ep(t,s)]=p(t)ep(t,s);

(vi) [ep(c,·)]= –p[ep(c,·)]σ for allc∈T;

(vii) (d/dz)[ez(t,s)] = [

t

s /( +μ(τ)z)τ]ez(t,s).

Lemma .([]) Assume that f,g:T→Rare delta differentiable at t∈Tk.Then

(fg)(t) =f(t)g(t) +fσ(t)g(t) =g(t)f(t) +gσ(t)f(t).

Lemma .([]) For each t∈T,let N be a neighborhood of t.Then,for VCrd(T,R+),

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that

u(t)

(t)–V(t) –μ(t)f(t)<D+V(t) + for each sN,s>t,

whereμ(t) =σ(t) –s.If t is right-scattered and V(t)is continuous at t,this reduces to D+V(t) = V(σ(t))–V(t)

σ(t)–t .

Next, we introduce the Banach space which is suitable for system (.)-(.).

Let={x= (x,x, . . . ,xl)T:|xi|<li,i= , , . . . ,l}be an open bounded domain inRlwith

smooth boundary. LetCrd(T×,Rn+m) be the set consisting of all the vector function

y(t,x) = (y(t,x),y(t,x), . . . ,yn+m(t,x))T which is rd-continuous with respect tot∈Tand

continuous with respect tox. For everyt∈Tandx, we define the setCTt ={y(t,·) :

yC(,Rn+m)}. ThenCt

Tis a Banach space with the normy(t,·)= (in=+myi(t,·))/, whereyi(t,·)= (

|yi(t,x)|

dx)/. LetC

rd([–τ, ]T×,Rn+m) consist of all functions

f(t,x) which map [–τ, ]T× into Rn+m andf(t,x) is rd-continuous with respect to

t∈[–τ, ]T and continuous with respect tox. For everyt∈[–τ, ]Tandx, we define the setCt[–τ,]T={u(t,·) :uC(,Rn+m)}. ThenCt

[–τ,]Tis a Banach space equipped

with the normψ= ( n+m

i= φi)/, whereψ(t,x) = (ψ(t,x),ψ(t,x), . . . ,ψn+m(t,x))T

Ct

[–τ,]T,ψi(t,·)= (

|ψi(·,x)|

τdx)/,|ψi(·,x)|τ =sups∈[–τ,]T|ψi(s,x)|.

In order to achieve the global robust exponential synchronization, the following system (.)-(.) is the controlled slave system corresponding to the master system (.)-(.):

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

˜ u

i (t,x) =

l k=

∂xk(aik

∂˜ui

∂xk) –biu˜i(t,x) +

m

j=cijfj(v˜j(tτ,x)) +Ii

+nj=pijFj(u˜j(tτ,x)) +

n

j=rij

+∞

kij(s)Fj(u˜j(ts,x))s

+ nj=qijFj(u˜j(tτ,x)) + nj=wij

+∞

kij(s)Fj(u˜j(ts,x))s +nj=dijμj+

n

j=Sijμj+ nj=Tijμj+miEi(t,x),

˜ v

j (t,x) =

l

k=

∂xk(ξjk

∂˜vj

∂xk) –ηjv˜j(t,x) +

n

i=ζjigi(u˜i(tτ,x)) +Jj

+mi=λjiGi(v˜i(tτ,x)) +

m

i=ρji

+∞

κji(s)Gi(v˜i(ts,x))s + mi=πjiGi(v˜i(tτ,x)) + mi=σji

+∞

κji(s)Gi(v˜i(ts,x))s

+mi=hjiνi+

m

i=Mjiνi+ mi=Njiνi+mn+jEn+j(t,x),

(.)

subject to the following initial conditions

˜

ui(s,x) =φ˜i(s,x), (s,x)∈[–τ, ]T×,

˜

vj(s,x) =ϕ˜j(s,x), (s,x)∈[–τ, ]T×, (.)

and Dirichlet boundary conditions

˜

ui(t,x) = , (t,x)∈[,∞)T×,

˜

vj(t,x) = , (t,x)∈[,∞)T×,

(.)

where Ei(t,x) = u˜i(t,x) –ui(t,x) (i = , , . . . ,n) and En+j(t,x) =v˜n+j(t,x) –vn+j(t,x) (j=

, , . . . ,m) are error functions.mk>  (k= , , . . . ,n+m) is a constant error weighting

co-efficient.u˜(t,x) = (u˜(t,x),u˜(t,x), . . . ,u˜n(t,x))TCrd(T×,Rn),v˜(t,x) = (v˜(t,x),˜v(t,x), . . . ,v˜m(t,x))TCrd(T×,Rm),φ˜(t,x) = (φ˜(t,x),φ˜(t,x), . . . ,φ˜n(t,x))TC([–τ, ]×,Rn),

˜

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From (.)-(.) and (.)-(.), we obtain the error system (.)-(.) as follows: ⎧

⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

E

i (t,x) =

l

k=∂∂xk(aik

∂Ei

∂xk) + (mibi)Ei(t,x) +mj=cij[fj(v˜j(tτ,x)) –fj(vj(tτ,x))]

+nj=pij[Fj(u˜j(tτ,x)) –Fj(uj(tτ,x))]

+nj=rij

+∞

kij(s)[Fj(u˜j(ts,x)) –Fj(uj(ts,x))]s

+ nj=qij[Fj(u˜j(tτ,x)) –Fj(uj(tτ,x))]

+ nj=wij

+∞

kij(s)[Fj(u˜j(ts,x)) –Fj(uj(ts,x))]s,

E

n+j(t,x) =

l

k=∂∂xk(ξjk

∂En+j

∂xk ) + (mn+jηj)En+j(t,x) +ni=ζji[gi(u˜i(tτ,x)) –gi(ui(tτ,x))]

+mi=λji[Gi(v˜i(tτ,x)) –Gi(vi(tτ,x))]

+mi=ρji

+∞

κji(s)[Gi(v˜i(ts,x)) –Gi(vi(ts,x))]s

+ mi=πji[Givi(tτ,x)) –Gi(vi(tτ,x))]

+ mi=σji

+∞

κji(s)[Gi(v˜i(ts,x)) –Gi(vi(ts,x))]s,

(.)

subject to the following initial conditions

Ei(s,x) =φ˜i(s,x) –φi(s,x), (s,x)∈[–τ, ]T×,

En+j(s,x) =ϕ˜j(s,x) –ϕj(s,x), (s,x)∈[–τ, ]T×,

(.)

and Dirichlet boundary conditions

Ei(t,x) = , (t,x)∈[,∞)T×,

En+j(t,x) = , (t,x)∈[,∞)T×.

(.)

The following definition is significant to study the global robust exponential synchro-nization of coupled neural networks (.)-(.) and (.)-(.).

Definition . Let y(t,x) = (u(t,x),u(t,x), . . . ,un(t,x),v(t,x),v(t,x), . . . ,vm(t,x))T

Rn+m andy˜(t,x) = (u˜

(t,x),u˜(t,x), . . . ,u˜n(t,x),v˜(t,x),v˜(t,x), . . . ,v˜m(t,x))T∈Rn+m be the

solution vectors of system (.)-(.) and its controlled slave system (.)-(.), respec-tively.E(t,x) = (E(t,x),E(t,x), . . . ,En+m(t,x))T∈Rn+mis the error vector. Then the

cou-pled systems (.)-(.) and (.)-(.) are said to be globally exponentially synchronized if there exists a controlled input vectorz(t,x) = (mE(t,x),mE(t,x), . . . ,mn+mEn+m(t,x))T

and a positive constantαR+andM≥ such that E(t,·)=y˜(t,·) –y(t,·)≤Meα(t, ), t∈[,∞)T,

whereαis called the degree of exponential synchronization on time scales.

3 Main results

In this section, we will consider the global robust exponential synchronization of coupled systems (.)-(.) and (.)-(.). At first, we need to introduce some useful lemmas.

Lemma . ([]) Let be a cube |xi|<li (i= , , . . . ,l) and assume that h(x) is a

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h(x)|∂= .Then

Throughout this paper, we always assume that:

(H) The neurons activationfj,Fi,giandGjare Lipschitz continuous, that is, there exist

positive constantsαj,βi,γiandδjsuch that|fj(ξ) –fj(η)| ≤αj|ξη|,|Fi(ξ) –Fi(η)| ≤βi|ξ

η|,|gi(ξ) –gi(η)| ≤γi|ξη|,|Gj(ξ) –Gj(η)| ≤δj|ξη|for anyξ,η∈R,i= , , . . . ,n;j=

, , . . . ,m.

(H) The delay kernelskij,κji: [, +∞)T→[, +∞) (i= , , . . . ,n;j= , , . . . ,m) are

real-valued non-negative rd-continuous functions and satisfy the following conditions:

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(H) The following conditions are always satisfied:

globally robustly exponentially synchronous with the master system(.)-(.).

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+ 

(12)

and

By applying Lemma ., (.)-(.), conditions (H)-(H) and the Hölder inequality, and noting the robustness of parameter intervals, we get

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+ Similar to the arguments of (.), we obtain

En+j(t,·)

If the first inequality of condition (H) holds, there exists one positive numberς>  (may be sufficiently small) such that

Now we consider the functions

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whereθ(zi) =

Similar to the above arguments of (.)-(.), we can always choose  <<  such that for

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+

m

=

δj

|ρj|+|σj|

+∞

κj(s)e⊕(s, )s+

n

i=

αj|cij|e⊕(τ, )

+

max{e⊕(σ(t), ),e(θ()–)μ(t)R(t)Ei(t,·)

(t, )}θ()μ(t)R(t)

e⊕(σ(t), ) ≤. (.)

Take the Lyapunov functionalV(t) as follows:

V(t) =Vt,E(t)=V(t) +V(t), (.)

where

V(t) =

n

i=

e⊕(t, )Ei(t,·)

+e(θ()–)μ(t)Q(t)Ei(t,·)(t, )

+

m

j=

αj|cij|

t tτ

e⊕σ(s+τ), En+j(s,·)s

+

n

ν=

βν

|piν|+|q|

t tτ

e

σ(s+τ), (s,·)s

+

n

ν=

βν

|r|+|wiν|

+∞

kiν(s)

t

ts

e⊕σ(s+r), (r,·)r

s

,

V(t) =

m

j=

e⊕(t, )En+j(t,·)+e(θ()–)μ(t)R(t)En+j(t,·)(t, )

+

n

i=

γi|ζji|

t tτ

e

σ(s+τ), Ei(s,·)

 s

+

m

=

δ

|λj|+|πj| t tτ

e⊕σ(s+τ), En+(s,·)

 s

+

m

=

δ

|ρj|+|σj|

+∞

κj(s)

t

ts

e⊕σ(s+r), En+(r,·)

 r

s

.

Calculating D+V

 (t) along (.) associated with (.) and noting that (d/dz)[ez(t,s)] =

[st/( +μ(τ)z)τ]ez(t,s) >  if and only ifzR+(that is,ez(t,s) is increasing with respect

tozif and only ifzR+), we have

D+V(t) =

n

i=

()e⊕(t, )Ei(t,·)+eσ(t), Ei(t,·)

+θ() – μ(t)Q(t)Ei(t,·)

e(θ()–)μ(t)Q(t)Ei(t,·)(t, ) +

m

j=

αj|cij|e⊕

σ(t+τ), En+j(t,·)

 

m

j=

αj|cij|e⊕

σ(t), En+j(tτ,·)

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(17)

×maxe

By applying (.), we can similarly calculateD+V

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+

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+

which implies that

E(t,·)≤Me(t, ). (.)

Obviously,M> . According to Definition ., we conclude that the controlled slave sys-tem (.)-(.) is globally robustly exponentially synchronous with the master syssys-tem

(.)-(.) on the time scale [, +∞)T. The proof is complete.

When the time scaleT=RandT=Z, we will obtain the following two important corol-laries.

Corollary . Assume that the following(H)-(H)hold.Then the master system(.) -(.)and its controlled slave system are globally robustly exponentially synchronous.

(H) The neurons activationfj,Fi,giandGjare Lipschitz continuous, that is, there exist

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η|,|gi(ξ) –gi(η)| ≤γi|ξη|,|Gj(ξ) –Gj(η)| ≤δj|ξη|for anyξ,η∈R,i= , , . . . ,n;j=

, , . . . ,m.

(H) The delay kernelskij,κji: [, +∞)→[, +∞) (i= , , . . . ,n;j= , , . . . ,m) are

real-valued non-negative continuous functions and satisfy the following conditions:

kij(s) ds= ,

skij(s) ds<∞,

κji(s) ds= ,

sκji(s) ds<∞

and there exist constantsω> ,ω>  such that

kij(s)esωds<∞,

κji(s)esωds<∞.

(H) The following conditions are always satisfied:

l

k= aik

lk + (mibi) +

m

j=

αj|cij|+ n

ν=

βν

|piν|+|qiν|+|riν|+|wiν|

+

n

ν=

βi

|pνi|+|qνi|

eτ+

n

ν=

βi

|rνi|+|wνi|

+∞

kνi(s)esds

+

m

j=

γi|ζji|eτ < , i= , , . . . ,n;

l

k= ξ

jk

l

k

+ (mn+jηj) + n

i=

γi|ζji|+ m

=

δ

|λj|+|πj|+|ρj|+|σj|

+

m

=

δj

|λj|+|πj|

eτ+

m

=

δj

|ρj|+|σj|

+∞

κj(s)esds

+

n

i=

αj|cij|eτ< , j= , , . . . ,m.

Corollary . Assume that the following(H)-(H)hold. Then the master system(.) -(.)and its controlled slave system are globally robustly exponentially synchronous.

(H) The neurons activationfj,Fi,giandGjare Lipschitz continuous, that is, there exist

positive constantsαj,βi,γiandδjsuch that|fj(ξ) –fj(η)| ≤αj|ξη|,|Fi(ξ) –Fi(η)| ≤βi|ξ

η|,|gi(ξ) –gi(η)| ≤γi|ξη|,|Gj(ξ) –Gj(η)| ≤δj|ξη|for anyξ,η∈R,i= , , . . . ,n;j=

, , . . . ,m.

(H) The delay kernelskij,κji:Z+→[, +∞) (i= , , . . . ,n;j= , , . . . ,m) are real-valued

non-negative rd-continuous functions and satisfy the following conditions:

s=

kij(s) = ,

s=

skij(s) <∞,

s=

κji(s) = ,

s=

sκji(s) <∞,

and there exist constantsω> ,ω>  such that

s=

kij(s)( +ω)s<∞,

s=

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(H) The following conditions are always satisfied:

4 Illustrative example

Consider the following reaction-diffusion BAM recurrent FNNs on time scales:

subject to the following initial conditions

ui(s,x) =φi(s,x), (s,x)∈[–τ, ]T×,

vj(s,x) =ϕj(s,x), (s,x)∈[–τ, ]T×, (.)

and Dirichlet boundary conditions

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+ 

j=

γ|ζj|τ≈–. < ,

– 

k= ξ

k

l

k

+ (m–η) + 

i=

γi|ζi|+

=

δ

|λ|+|π|+|ρ|+|σ|

+ 

=

δ

|λ|+|π|

τ +

=

δ

|ρ|+|σ| +∞

s=

κ(s)s

+ 

i=

α|ci|τ≈–. < ,

– 

k= ξ

k

lk + (m–η) + 

i=

γi|ζi|+

=

δ

|λ|+|π|+|ρ|+|σ|

+ 

=

δ

|λ|+|π|

τ+ 

=

δ

|ρ|+|σ| +∞

s=

κ(s)s

+ 

i=

α|ci|τ≈–. < .

Thus, conditions (H)-(H) are satisfied. It follows from Theorem . that the master sys-tem (.)-(.) and its controlled slave syssys-tem are globally robustly exponentially synchro-nized.

Competing interests

The author declares to have no competing interests.

Author’s contributions

The author read and approved the final manuscript.

Acknowledgements

The author would like to thank the anonymous referees for their useful and valuable suggestions. This work is supported by the National Natural Sciences Foundation of Peoples Republic of China under Grant (No. 11161025; No. 11326101), Yunnan Province natural scientific research fund project (No. 2011FZ058).

Received: 3 September 2014 Accepted: 28 November 2014 Published:16 Dec 2014

References

1. Kosko, B: Adaptive bidirectional associative memories. Appl. Opt.26(23), 4947-4960 (1987) 2. Kosko, B: Bidirectional associative memories. IEEE Trans. Syst. Man Cybern.18(1), 49-60 (1988)

3. Kosko, B: Neural Networks and Fuzzy Systems: A Dynamical Systems Approach to Machine Intelligence. Prentice Hall, New York (1992)

4. Mathai, G, Upadhyaya, BR: Performance analysis and application of the bidirectional associative memory to industrial spectral signatures. Neural Netw.1, 33-37 (1989)

5. Yu, WW, Cao, JD: Adaptive synchronization and lag synchronization of uncertain dynamical system with time delay based on parameter identification. Physica A375, 467-482 (2007)

6. Tang, Y, Fang, JA: Robust synchronization in an array of fuzzy delayed cellular neural networks with stochastic ally hybrid coupling. Neurocomputing72, 3253-3262 (2009)

7. Yuan, K, Cao, JD: Exponential stability and periodic solutions of fuzzy cellular neural networks with time-varying delays. Neurocomputing69, 1619-1627 (2006)

8. Wang, K, Teng, ZD, Jiang, HJ: Adaptive synchronization in an array of linearly coupled neural networks with reaction-diffusion terms and time delays. Commun. Nonlinear Sci. Numer. Simul.17, 3866-3875 (2012)

9. Sheng, L, Yang, HZ: Exponential synchronization of a class of neural networks with mixed time-varying delays and impulsive effects. Neurocomputing71, 3666-3674 (2008)

10. Yan, P, Lv, T: Exponential synchronization of fuzzy cellular neural networks with mixed delays and general boundary conditions. Commun. Nonlinear Sci. Numer. Simul.17, 1003-1011 (2012)

11. Gan, QT: Exponential synchronization of stochastic Cohen-Grossberg neural networks with mixed time-varying delays and reaction-diffusion via periodically intermittent control. Neural Netw.31, 12-21 (2012)

(24)

13. Luo, M, Xu, J: Suppression of collective synchronization in a system of neural groups with washout-filter-aided feedback. Neural Netw.24, 538-543 (2011)

14. Yang, XS, Huang, CX, Zhu, QX: Synchronization of switched neural networks with mixed delays via impulsive control. Chaos Solitons Fractals44, 817-826 (2011)

15. Li, T, Fei, SM, Zhu, Q, Cong, S: Exponential synchronization of chaotic neural networks with mixed delays. Neurocomputing71, 3005-3019 (2008)

16. Du, BZ, James, L: Stability analysis of static recurrent neural networks using delay-partitioning and projection. Neural Netw.22, 343-347 (2009)

17. Liu, PC, Yi, FQ, Guo, Q, Yang, J, Wu, W: Analysis on global exponential robust stability of reaction-diffusion neural networks with S-type distributed delays. Physica D237, 475-485 (2008)

18. Li, YK, Zhao, KH: Robust stability of delayed reaction-diffusion recurrent neural networks with Dirichlet boundary conditions on time scales. Neurocomputing74, 1632-1637 (2011)

19. Gilli, M: Stability of cellular neural networks with nonpositive templates and nonmonotonic output functions. IEEE Trans. Circuits Syst. I41, 518-528 (1994)

20. Gopalsamy, K, He, XZ: Stability in asymmetric Hopfield nets with transmission delays. Physica D76, 344-358 (1994) 21. Zeng, Z, Wang, J: Improved conditions for global exponential stability of recurrent neural networks with time-varying

delays. Chaos Solitons Fractals23(3), 623-635 (2006)

22. Shao, YF: Exponential stability of periodic neural networks with impulsive effects and time-varying delays. Appl. Math. Comput.217, 6893-6899 (2011)

23. Yang, T, Yang, LB: The global stability of fuzzy cellular neural networks. IEEE Trans. Circuits Syst. I43, 880-883 (1996) 24. Zhao, KH, Li, YK: Existence and global exponential stability of equilibrium solution to reaction-diffusion recurrent

neural networks on time scales. Discrete Dyn. Nat. Soc.2010, Article ID 624619 (2010)

25. Li, YK, Zhao, KH, Ye, Y: Stability of reaction-diffusion recurrent neural networks with distributed delays and Neumann boundary conditions on time scales. Neural Process. Lett.36, 217-234 (2012)

26. Zhao, KH, Wang, LWJ, Liu, JQ: Global robust attractive and invariant sets of fuzzy neural networks with delays and impulses. J. Appl. Math.2013, Article ID 935491 (2013)

27. Zhao, KH: Globally exponential synchronization of diffusion recurrent FNNs with time-delays and impulses on time scales. WSEAS Trans. Math.13, 224-235 (2014)

28. Zhang, JY, Yang, YR: Global stability analysis of bidirectional associative memory neural networks with time delay. Int. J. Circuit Theory Appl.29(2), 185-196 (2001)

29. Zhao, H: Global stability of bidirectional associative memory neural networks with distributed delays. Phys. Lett. A

297, 182-190 (2002)

30. Liu, B, Huang, L: Global exponential stability of BAM neural networks with recent-history distributed delays and impulse. Neurocomputing69(16-18), 2090-2096 (2006)

31. Song, QK, Cao, JD: Global exponential stability of bidirectional associative memory neural networks with distributed delays. J. Comput. Appl. Math.202, 266-279 (2007)

32. Song, QK, Cao, JD: Global exponential stability and existence of periodic solutions in BAM networks with delays and reaction-diffusion terms. Chaos Solitons Fractals23(2), 421-430 (2005)

33. Cao, JD, Wang, L: Exponential stability and periodic oscillatory solution in BAM networks with delays. IEEE Trans. Neural Netw.13(2), 457-463 (2002)

34. Wu, XL, Zhang, JH, Guan, XP, Meng, H: Delay-dependent asymptotic stability of BAM neural networks with time delay. Kybernetes39(8), 1313-1321 (2010)

35. Zhu, QX, Li, XD, Yang, XS: Exponential stability for stochastic reaction-diffusion BAM neural networks with time-varying and distributed delays. Appl. Math. Comput.217, 6078-6091 (2011)

36. Ge, JH, Xu, J: Synchronization and synchronized periodic solution in a simplified five-neuron BAM neural network with delays. Neurocomputing74, 993-999 (2011)

37. Zhang, ZQ, Yang, Y, Huang, YS: Global exponential stability of interval general BAM neural networks with reaction-diffusion terms and multiple time-varying delays. Neural Netw.24, 457-465 (2011)

38. Ding, W, Wang, LS: 2NAlmost periodic attractors for Cohen-Grossberg-type BAM neural networks with variable

coefficients and distributed delays. J. Math. Anal. Appl.373, 322-342 (2011)

39. Li, YK, Chen, XR, Zhao, L: Stability and existence of periodic solutions to delayed Cohen-Grossberg BAM neural networks with impulses on time scales. Neurocomputing72, 1621-1630 (2009)

40. Li, YK, Gao, S: Global exponential stability for impulsive BAM neural networks with distributed delays on time scales. Neural Process. Lett.31(1), 65-91 (2010)

41. Li, YK: Global exponential stability of BAM neural networks with delays and impulses. Chaos Solitons Fractals24(1), 279-285 (2005)

42. Cao, JD, Wan, Y: Matrix measure strategies for stability and synchronization of inertial BAM neural network with time delays. Neural Netw.53, 165-172 (2014)

43. Du, YH, Zhong, SM, Zhou, N: Global asymptotic stability of Markovian jumping stochastic Cohen-Grossberg BAM neural networks with discrete and distributed time-varying delays. Appl. Math. Comput.243, 624-636 (2014) 44. Jian, JG, Wang, BX: Stability analysis in Lagrange sense for a class of BAM neural networks of neutral type with

multiple time-varying delays. Neurocomputing (2015). doi:10.1016/j.neucom.2014.07.041

45. Berezansky, L, Braverman, E, Idels, L: New global exponential stability criteria for nonlinear delay differential systems with applications to BAM neural networks. Appl. Math. Comput.243, 899-910 (2014)

46. Li, YK, Yang, L, Wu, WQ: Anti-periodic solution for impulsive BAM neural networks with time-varying leakage delays on time scales. Neurocomputing (2015). doi:10.1016/j.neucom.2014.08.020

47. Zhang, AC, Qiu, JL, She, JH: Existence and global exponential stability of periodic solution for high-order discrete-time BAM neural networks. Neural Netw.50, 98-109 (2014)

48. Quan, ZY, Huang, LH, Yu, SH, Zhang, ZQ: Novel LMI-based condition on global asymptotic stability for BAM neural networks with reaction-diffusion terms and distributed delays. Neurocomputing136, 213-223 (2014)

49. Carroll, TL, Pecora, LM: Cascading synchronized chaotic systems. Phys. D, Nonlinear Phenom.67(1-3), 126-140 (1993) 50. Carroll, TL, Heagy, J, Pecora, LM: Synchronization and desynchronization in pulse coupled relaxation oscillators. Phys.

(25)

51. Bohner, M, Peterson, A: Dynamic Equation on Time Scales: An Introduction with Applications. Birkäuser, Boston (2001)

52. Lakshmikantham, V, Vatsala, AS: Hybrid system on time scales. J. Comput. Appl. Math.141, 227-235 (2002) 53. Lu, JG: Global exponential stability and periodicity of reaction-diffusion delayed recurrent neural networks with

Dirichlet boundary conditions. Chaos Solitons Fractals35(1), 116-125 (2008)

10.1186/1687-1847-2014-317

References

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