Research article

Exponential stability of stochastic Hopfield neural network with mixed multiple delays

  • Received: 24 December 2020 Accepted: 29 January 2021 Published: 05 February 2021
  • MSC : 34D20

  • This paper investigates the problem for exponential stability of stochastic Hopfield neural networks involving multiple discrete time-varying delays and multiple distributed time-varying delays. The exponential stability of such neural systems has not been given much attention in the past literature because this type of neural systems cannot be transformed into the vector forms and it is difficult to derive the easily verified stability conditions expressed in terms of the linear matrix inequality. Therefore, this paper tries to establish the easily verified sufficient conditions of the linear matrix inequality forms to ensure the mean-square exponential stability and the almost sure exponential stability for this type of neural systems by constructing a suitable Lyapunov-Krasovskii functional and inequality techniques. Four examples are provided to demonstrate the effectiveness of the proposed theoretical results and compare the established stability conditions to the previous results.

    Citation: Qinghua Zhou, Li Wan, Hongbo Fu, Qunjiao Zhang. Exponential stability of stochastic Hopfield neural network with mixed multiple delays[J]. AIMS Mathematics, 2021, 6(4): 4142-4155. doi: 10.3934/math.2021245

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  • This paper investigates the problem for exponential stability of stochastic Hopfield neural networks involving multiple discrete time-varying delays and multiple distributed time-varying delays. The exponential stability of such neural systems has not been given much attention in the past literature because this type of neural systems cannot be transformed into the vector forms and it is difficult to derive the easily verified stability conditions expressed in terms of the linear matrix inequality. Therefore, this paper tries to establish the easily verified sufficient conditions of the linear matrix inequality forms to ensure the mean-square exponential stability and the almost sure exponential stability for this type of neural systems by constructing a suitable Lyapunov-Krasovskii functional and inequality techniques. Four examples are provided to demonstrate the effectiveness of the proposed theoretical results and compare the established stability conditions to the previous results.



    Since Hopfield neural network was proposed in 1982, many mathematicians, physicists and computer experts have been working on the dynamic behaviors of this network and its applications in pattern recognition, associative memory and optimization [1,2,3,4]. The stability analysis of nonlinear nature of neural networks is of great interest when designing neural networks for practical applications because the existence of stable equilibrium points of such neural networks can avoid some suboptimal responses. Therefore, the stability analysis of dynamic neural system has always been a research hotspot. It is also known that it is inevitable to encounter various types of time delay which might cause great damage to the stability in the process of neural network implementation. Among the various types of time delay, time-varying delay and distributed delay are the most common. The time-varying delay must exist due to the finite switching speed of amplifiers and the distributed delay often occur beacuse a neural network usually has a spatial nature due to the presence of an amount of parallel pathways of a variety of axon sizes and lengths. Recently, some research papers have analyzed the stability of various delayed neural networks and obtained useful stability results, see, for example, [5,6,7,8,9,10,11,12,13,14,15,16,17,18,19], and references therein.

    On the other hand, it has been well recognized that stochastic perturbations are ubiquitous and inevitable in the real nervous systems [20]. Recently, some valuable stability results of stochastic delayed neural networks can be found in some famous journals related to mathematics, physics and neural network, for example, see [21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38] and references therein. It is noted that most of these literatures have studied the networks which can be expressed in the vector forms and established various stability criteria in the linear matrix inequality forms. Different from them, stochastic neural networks investigated in this paper cannot be transformed into the vector forms because of the existence of the multiple delays, which causes the difficulty of establishing the stability condition expressed in terms of the linear matrix inequality. The existence of the stochastic perturbations, the time-varying delays and the distributed delays in the stochastic neural networks further increase the difficulty. Perhaps, it is the reason that the exponential stability of such neural networks has not been given much attention in the past literature.

    In this paper, we mainly consider the mean-square stability and almost sure exponential stability for nonlinear stochastic Hopfield neural networks involving multiple discrete time-varying delays and multiple distributed time-varying delays. The main aim of this paper is to establish the stability conditions of the linear matrix inequality form for such stochastic Hopfield neural networks by constructing a suitable Lyapunov-Krasovskii functional and inequality techniques. Since the systems studied in [5,24,33] are some special cases of our proposed system, the stability conditions we established are valid for these systems while their stability conditions are invalid for our proposed system. Four examples are provided to demonstrate the effectiveness of our proposed theoretical results and compare the established stability conditions to the previous results in [5,24,33]. These examples show that the established stability conditions are easily verified by MATLAB LMI control toolbox and better than the stability conditions in [5,24,33]. Therefore, for the neural networks in [5,24,33], our results provide novel sufficient conditions which are easy to verify. Our proposed approach can be applied to study the exponential stability for other types of stochastic (or deterministic) neural networks with multiple delays.

    This paper considers the following stochastic Hopfield neural networks with the mixed multiple delays

    dxi(t)=[cixi(t)+nj=1aijfj(xj(t))+nj=1bijgj(xj(tτij(t)))+nj=1ttρij(t)dijhj(xj(s))ds]dt+nj=1σij(xj(t),xj(tτij(t)))dwj(t),i=1,,n,

    where ci is the self-feedback connection weight satisfying ci>0; aij,bij and dij present the connection weight coefficients; τij(t) and ρij(t) are multiple delays; σij(,) are the diffusion functions; fi(),gi() and hi() denote the nonlinear activation functions; w(t)=(w1(t),,wn(t))T is n-dimensional Brownian motion defined on a complete probability space (Ω,F,P) with a natural filtration {Ft}t0 generated by {w(t)}, where we associate Ω with the canonical space generated by w(t), and denote by F the associated σ-algebra generated by {w(s):0st} with the probability measure P.

    Throughout this paper, the following assumptions are required for system (2.1):

    (A1): There exist constants τ>0,ρ>0 and μ such that for t0,

    0τij(t)τ,0ρij(t)ρ,˙τij(t)μ<1.

    (A2) : The diffusion functions σij(,) satisfy σij(0,0)=0 and that there exist nonnegative constants Lij and Mij such that for all x,yR,

    |σij(x,y)|Lij|x|+Mij|y|.

    (A3):fi(),gi() and hi() satisfy fi(0)=gi(0)=hi(0)=0 and that there exist some constants αi,α+i,βi,β+i,γi and γ+i such that for all x,yR(xy),

    αifi(x)fi(y)xyα+i,βigi(x)gi(y)xyβ+i,γihi(x)hi(y)xyγ+i.

    The initial condition xi(s)=ξi(s),s[max{τ,ρ},0], and ξ={(ξ1(s),,ξ1(s))T:max{τ,ρ}s0} is C([max{τ,ρ},0];Rn)-valued function and F0-measurable Rn-valued random variable satisfying

    ||ξ||2=supmax{τ,ρ}t0Eξ(t)2<,

    where denotes the Euclidean norm and C([max{τ,ρ},0];Rn) denotes the space of all continuous Rn-valued functions defined on [max{τ,ρ},0].

    Remark 1. It is noted that assumption (A3) is less conservative than the Lipschitz conditions satisfied by fi() and gi() in [15,22,23,24,29,38] since αi,α+i,βi and β+i (αi<α+i,βi<β+i) in (A3) can be any real numbers.

    System (2.1) is a more general mathematical expression and can be described in different mathematical forms by changing the system parameters and functions. When τij(t)=ρij(t)=τj(t),fj=gj,w1(t)==wj(t)=w(t) and σij(xj(t),xj(tτij(t)))=Lijxj(t)+Mijxj(tτj(t)), system (2.1) transforms into the following equation studied in [33]:

    dxi(t)=[cixi(t)+nj=1aijfj(xj(t))+nj=1bijfj(xj(tτj(t)))+nj=1ttτj(t)dijhj(xj(s))ds]dt+nj=1[Lijxj(t)+Mijxj(tτj(t))]dw(t),i=1,,n. (2.1)

    When τij(t)=τj,dij=0 and σij(xj(t),xj(tτij(t)))=σij(xj(t)), system (2.1) transforms into the following equation studied in [24]

    dxi(t)=[cixi(t)+nj=1aijfj(xj(t))+nj=1bijgj(xj(tτj))]dt+nj=1σij(xj(t))dwj(t),i=1,,n,

    When fj=gj,dij=0 and σij(xj(t),xj(tτij(t)))=0, system (2.1) transforms into the following deterministic system studied in [5]:

    dxi(t)=cixi(t)+nj=1aijfj(xj(t))+nj=1bijfj(xj(tτij(t))),i=1,,n. (2.2)

    In this section, novel sufficient conditions of exponential stability of zero solution of system (2.1) are presented. Four examples are given to demonstrate the effectiveness of our theoretical results and compare the stability conditions to the previous results in [5,24,33].

    Theorem 1. Suppose that there exist some positive real numbers p1,,pn,ui1,,uin (i=1,2,3) such that

    Γ=(ΔPA+U1Σ4U2Σ6U3Σ82U1002U2+11μB202U3+ρ2D2)<0,

    where means the symmetric terms, Γ<0 means that matrix Γ is symmetric negative definite,

    Δ=2PC+PB1+PD1+Σ1+11μΣ22U1Σ32U2Σ52U3Σ7,
    A=(aij)n×n,C=diag{c1,,cn},P=diag{p1,,pn},
    U1=diag{u11,,u1n},U2=diag{u21,,u2n},U3=diag{u31,,u3n},
    B1=diag{nj=1|b1j|,,nj=1|bnj|},B2=diag{nj=1pj|bj1|,,nj=1pj|bjn|},
    D1=diag{nj=1|d1j|,,nj=1|dnj|},D2=diag{nj=1pj|dj1|,,nj=1pj|djn|},
    Σ1=2diag{nj=1pjL2j1,,nj=1pjL2jn},Σ2=2diag{nj=1pjM2j1,,nj=1pjM2jn},
    Σ3=diag{α1α+1,,αnα+n},Σ4=diag{α1+α+1,,αn+α+n},
    Σ5=diag{β1β+1,,βnβ+n},Σ6=diag{β1+β+1,,βn+β+n},
    Σ7=diag{γ1γ+1,,γnγ+n},Σ8=diag{γ1+γ+1,,γn+γ+n}.

    Then zero solution of system (2.1) is almost surely exponentially stable and exponentially stable in mean square.

    Proof. Γ<0 implies that there exists a sufficient small real number λ>0 such that

    ˉΓ=(ˉΔPA+U1Σ4U2Σ6U3Σ82U1002U2+11μeλτB202U3+ρ2eλρD2)<0,

    in which

    ˉΔ=λP2PC+PB1+PD1+Σ1+eλτ1μΣ22U1Σ32U2Σ52U3Σ7.

    Constructing the following Lyapunov-Krasovskii functional

    V(t)=eλtni=1pix2i(t)+ni=1nj=1ttτij(t)eλ(s+τ)pi|bij|g2j(xj(s))+2M2ijx2j(s)1μds+0ρtt+sni=1nj=1pi|dij|ρeλ(θ+ρ)h2j(xj(θ))dθds. (3.1)

    Applying Itˆo formula in [21] to V(t) along the trajectory of system (2.1), we obtain

    dV(t)=ˉV(t)dt+2eλtni=1pixi(t)nj=1σij(xj(t),xj(tτij(t)))dwj(t), (3.2)

    where

    ˉV(t)=λeλtni=1pix2i(t)+ni=1nj=1{eλ(t+τ)pi|bij|g2j(xj(t))+2M2ijx2j(t)1μ(1˙τij(t))eλ(tτij(t)+τ)pi|bij|g2j(xj(tτij(t)))+2M2ijx2j(tτij(t))1μ}+ni=1nj=1pi|dij|ρ{ρeλ(t+ρ)h2j(xj(t))0ρeλ(t+s+ρ)h2j(xj(t+s))ds}+2eλtni=1pixi(t){cixi(t)+nj=1aijfj(xj(t))+nj=1bijgj(xj(tτij(t)))+nj=1ttρij(t)dijhj(xj(s))ds}+eλtni=1pinj=1σ2ij(xj(t),xj(tτij(t))).

    From (A1) and (A2), we derive

    ˉV(t)λeλtni=1pix2i(t)+ni=1nj=1{eλ(t+τ)pi|bij|g2j(xj(t))+2M2ijx2j(t)1μeλtpi(|bij|g2j(xj(tτij(t)))+2M2ijx2j(tτij(t)))}+ni=1nj=1pi|dij|ρ{ρeλ(t+ρ)h2j(xj(t))ttρeλ(s+ρ)h2j(xj(s))ds}+eλtni=1{2picix2i(t)+nj=12piaijxi(t)fj(xj(t))+nj=1pi|bij|(x2i(t)+g2j(xj(tτij(t))))+nj=1pi|dij|[x2i(t)+(ttρij(t)|hj(xj(s))|ds)2]+2nj=1piL2ijx2j(t)+2nj=1piM2ijx2j(tτij(t))}λeλtni=1pix2i(t)+ni=1nj=1eλ(t+τ)pi|bij|g2j(xj(t))+2M2ijx2j(t)1μ+ni=1nj=1pi|dij|ρ{ρeλ(t+ρ)h2j(xj(t))eλtttρh2j(xj(s))ds}+eλtni=1{2picix2i(t)+nj=12piaijxi(t)fj(xj(t))+nj=1pi|bij|x2i(t)+nj=1pi|dij|x2i(t)+2nj=1piL2ijx2j(t)}+eλtni=1nj=1pi|dij|ρttρh2j(xj(s))dseλt{xT(t)(λP2PC+PB1+PD1+Σ1+eλτΣ21μ)x(t)+eλτ1μgT(x(t))B2g(x(t))+2xT(t)PAf(x(t))+ρ2eλρhT(x(t))D2h(x(t))}, (3.3)

    where

    x(t)=(x1(t),,xn(t))T,f(x(t))=(f1(x1(t)),,fn(xn(t)))T,
    g(x(t))=(g1(x1(t)),,gn(xn(t)))T,h(x(t))=(h1(x1(t)),,hn(xn(t)))T.

    From (A3), we derive

    02ni=1u1i[fi(xi(t))α+ixi(t)][fi(xi(t))αixi(t)]=2ni=1u1i[f2i(xi(t))(α+i+αi)xi(t)fi(xi(t))+α+iαix2i(t)]=2fT(x(t))U1f(x(t))+2fT(x(t))U1Σ4x(t)2xT(t)U1Σ3x(t), (3.4)
    02ni=1u2i[gi(xi(t))β+ixi(t)][gi(xi(t))βixi(t)]2gT(x(t))U2g(x(t))+2gT(x(t))U2Σ6x(t)2xT(t)U2Σ5x(t) (3.5)

    and

    02ni=1u3i[hi(xi(t))γ+ixi(t)][hi(xi(t))γixi(t)]2hT(x(t))U3h(x(t))+2hT(x(t))U3Σ8x(t)2xT(t)U3Σ7x(t). (3.6)

    Inequalities (3.3)–(3.6) derive

    ˉV(t)eλtyT(t)ˉΓy(t)<0, (3.7)

    where y(t)=(xT(t),fT(x(t)),gT(x(t)),hT(x(t)))T.

    Integrating from 0 and t for (3.2) and combining with (3.7), we obtain

    V(t)=V(0)+t0ˉV(s)ds+t02eλsni=1pixi(s)nj=1σij(xj(s),xj(sτij(s)))dwj(s)<V(0)+t02eλsni=1pixi(s)nj=1σij(xj(s),xj(sτij(s)))dwj(s). (3.8)

    The nonnegative semi-martingale convergence theorem in [21] and (3.8) show that zero solution of system (2.1) is almost surely exponentially stable.

    Moreover, (3.1) and (3.8) deduce

    eλtmin1in{pi}Ex(t)2EV(t)<EV(0)E{max1in{pi}x(0)2+ni=1nj=10τeλ(s+τ)pi|bij|β2j+2M2ij1μx2j(s)ds+0ρ0sni=1nj=1pi|dij|ρeλ(θ+ρ)γ2jx2j(θ)dθds}{max1in{pi}+eλττ1μmax1in{nj=1pj(|bji|β2i+2M2ji)}+eλρρ3max1in{nj=1pj|dji|γ2i}}ξ2,

    where βi=max{|βi|,|β+i|},γi=max{|γi|,|γ+i|}, which shows that zero solution of system (2.1) is exponentially stable in mean square.

    Remark 2. Generally speaking, it is difficult to establish the stability conditions of the linear matrix inequality forms for the system which cannot be transformed into vector-matrix form. For system (2.1), Theorem 1 gives the stability conditions of the linear matrix inequality forms. Unsurprisingly, it is difficult to write an executable Matlab program to solve the matrices P, U1,U2 and U3 by Matlab LMI Control Toolbox because the matrices B2,D2,Σ1 and Σ2 involve the elements p1,,pn of matrix P.

    In what follows, we express a special case of Theorem 1 for p1==pn=p, which provides a easily verified sufficient criterion by Matlab LMI Control Toolbox.

    Theorem 2. Suppose that there exist positive constants p,ui1,,uin(i=1,2,3) such that

    Γ=(ΔpA+U1Σ4U2Σ6U3Σ82U1002U2+11μB202U3+ρ2D2)<0,

    where ,A,C,B1,D1,U1,U2,U3, and Σi(i=3,4,5,6,7,8) are defined as in Theorem 1,

    Δ=2pC+pB1+pD1+Σ1+11μΣ22U1Σ32U2Σ52U3Σ7,
    B2=pdiag{nj=1|bj1|,,nj=1|bjn|},D2=pdiag{nj=1|dj1|,,nj=1|djn|},
    Σ1=2pdiag{nj=1L2j1,,nj=1L2jn},Σ2=2pdiag{nj=1M2j1,,nj=1M2jn}.

    Then zero solution of system (2.1) is almost surely exponentially stable and exponentially stable in mean square.

    For the systems (2.2)–(2.4), Theorem 2 gives the following results.

    Corollary 1. Suppose that there exist positive constants p,ui1,,uin(i=1,2,3) such that

    Γ=(ΔpA+U1Σ4U2Σ4U3Σ82U1002U2+11μB202U3+τ2D2)<0,

    where Δ=2pC+pB1+pD1+Σ1+11μΣ22U1Σ32U2Σ32U3Σ7, other symbols are the same as Theorem 2. Then, zero solution of system (2.2) is almost surely exponentially stable and exponentially stable in mean square.

    Corollary 2. Suppose that there exist positive constants p,ui1,,uin(i=1,2,3) such that

    Γ=(ΔpA+U1Σ4U2Σ62U102U2+B2)<0,

    where Δ=2pC+pB1+Σ12U1Σ32U2Σ5, other symbols are the same as Theorem 2. Then, zero solution of system (2.3) is almost surely exponentially stable and exponentially stable in mean square.

    Corollary 3. Suppose that there exist positive constants p,ui1,,uin(i=1,2,3) such that

    Γ=(ΔpA+U1Σ4U2Σ42U102U2+11μB2)<0,

    where Δ=2pC+pB12U1Σ32U2Σ3, other symbols are the same as Theorem 2. Then, zero solution of system (2.4) is globally exponentially stable.

    Remark 3. Since the networks studied in [5,24,33] are some special cases of system (2.1), their stability conditions are invalid for system (2.1). On the contrary, our stability conditions are valid for the systems in [5,24,33]. In particular, the deterministic system (2.4) in [5] is a special case of stochastic system (2.1), which leads to that it is easy to transform Theorem 2 into Corollary 3. That is, Theorem 2 for system (2.1) includes Corollary 3 for corresponding system (2.4), which shows the stability result of stochastic system is more general than that of corresponding deterministic system.

    Remark 4. Although Theorem 5 in [33] gives the sufficient conditions of the linear matrix inequality forms, the stability conditions of Corollary 1 are more easy to verify. Example 2 demonstrates that the validity of Corollary 1 and the stability conditions of Corollary 1 are better than those of Theorem 5 in [33].

    Remark 5. Theorem 3.1 in [24] gives the sufficient conditions of the algebraic forms by using Lyapunov function eλt|x(t)|2. This Lyapunov function cannot be applied to study the system with time-varying delays. Example 3 demonstrates that the validity of Corollary 2 and the invalidity of Theorem 3.1 in [24], which shows that the stability conditions of Corollary 2 are better.

    Remark 6. In [5], Theorem 2.4 provides the stability condition of the spectral radius form which requires that the absolute values of all eigenvalues of matrix are less than 1. Example 4 demonstrates that the validity of Corollary 3 and the invalidity of Theorem 2.4 in [5], which shows that the stability conditions of Corollary 3 are better.

    Example 1. Consider system (2.1) with the following parameters and functions:

    A=(aij)4×4=(1111111111111111),B=(bij)4×4=(1111111111111111),
    D=(dij)4×4=(1111111111111111),C=(6000060000500006),

    fi(x)=0.5tanh(x),gi(x)=0.4tanh(x),hi(x)=0.3tanh(x), Lij=Mij=0.1,τij(t)=0.2sint, ρij(t)=0.5cost,i=j;τij(t)=0.2cost, ρij(t)=0.5sint,ij,i,j=1,2,3,4.

    Then we calculate that Σ3=Σ5=Σ7=0,B1=D1=4I,B2=D2=4pI,Σ1=Σ2=0.08pI,Σ4=0.5I,Σ6=0.4I,Σ8=0.3I,μ=0.2,ρ=0.5, where I denotes identity matrix.

    By using Matlab LMI Control Toolbox, we calculate P=0.1668I,U1=diag{0.5170, 0.5170,0.5777,0.5777},U2=0.8794I and U3=0.6455I satisfy the condition of Theorem 2, which demonstrates the effectiveness of our theoretical result.

    Example 2. Consider system (2.2) with the following parameters and functions:

    D=(dij)4×4=(1111111111111111),C=(6000060000500006),

    fi(x)=gi(x)=0.5tanh(x),hi(x)=0.3tanh(x),Lij=Mij=0.1,τj(t)=0.2sint,i,j=1,2,3,4, the matrices A and B are the same as in Example 1.

    Then we calculate that Σ3=Σ5=Σ7=0,B1=D1=4I,B2=D2=4pI,Σ1=Σ2=0.08pI,Σ4=Σ6=0.5I,Σ8=0.3I,μ=τ=0.2. By using Matlab LMI Control Toolbox, we know Corollary 1 holds when P=0.5791I,U1=diag{2.6460,2.4054,1.5394,3.2237}, U2=diag{2.8763,2.8877,2.8635,2.8751} and U3=diag{1.6561,1.6904,1.3281,1.8608}.

    On the other hand, Theorem 5 in [33] shows that zero solution of system (2.2) is almost surely exponentially stable and exponentially stable in mean square provided that there exist some matrices P>0,Ui=diag{ui1,,uin}0(i=1,2,3) and positive constants γ1,γ2,λ such that λ1τγ12(0,1) and

    Σ=(Δ10PA+U1L2PBU3M2Δ20U2L20Δ300Δ40Δ5)<0,

    where σ1=(Lij)n×n,σ2=(Mij)n×n,L1=Σ3,L2=Σ4,M1=Σ7,M2=Σ8,

    Δ1=(γ1+2λ)P2PC+2σT1Pσ1+U1(λI2L1)+U3(λI2M1),
    Δ2=2σT2Pσ2+U2(λI2L1),Δ3=(2λ2)U1,
    Δ4=(2λ2)U2,Δ5=(2λ2)U3+γ2DTPD.

    It is clear that the above stability condition is more difficult to verify than that of Corollary 1. Moreover, when we choose λ=γ1=γ2=0.5, we can not find the suitable matrices P,U1,U2 and U3 satisfying the condition of Theorem 5 in [33] by using Matlab LMI Control Toolbox. Therefore, Theorem 5 in [33] is invalid for the system (2.2) in Example 2.

    Example 3. Consider system (2.3) with C=diag{3.5,5,5,5},fi(x)=0.5tanh(x),gi(x) =0.4tanh(x),Lij=0.1,τj=0.2,i,j=1,2,3,4, the matrices A and B are the same as in Example 1.

    Then we calculate that Σi=0(i=2,3,5,7,8),B1=4I,B2=4pI,Σ1=0.08pI,Σ4=0.5I,Σ6=0.4I,τ=0.2,μ=0. By using Matlab LMI Control Toolbox, we know that Corollary 2 holds when P=0.1817I,U1=diag{0.6431,0.6431,0.7092,0.7092} and U2=0.9723I.

    On the other hand, Theorem 3.1 in [24] shows that the following inequalities

    2ci+nj=1|aij|αj+nj=1|bij|βj+nj=1|aji|αi+nj=1|bji|βi+nj=1L2ji<0(i=1,,n)

    are the sufficient conditions of almost sure exponential stability and mean square exponential stability of system (2.3), where αi and βi correspond to max{|αi|,|α+i|} and max{|βi|,|β+i|} in this paper, respectively.

    Then, we calculate that for i=1,2,3,4,αi=0.5,βi=0.4 and

    2ci+4j=1|aij|αj+4j=1|bij|βj+4j=1|aji|αi+4j=1|bji|βi+4j=1L2ji={0.24,i=1;2.76,i=2,3,4.

    Therefore, Theorem 3.1 in [24] is invalid for the system (2.3) in Example 3.

    Example 4. Consider system (2.4) with C=4I,fi(x)=0.5tanh(x),τij(t)=0.2sint,i=j;τij(t)=0.2cost,ij,i,j=1,2,3,4, the matrices A and B are the same as in Example 1.

    Then we calculate that Σi=0(i=1,2,3,5,7,8),B1=4I,B2=4pI,Σ1=0.08pI,Σ4=0.5I,Σ6=0.4I,τ=μ=0.2. By using Matlab LMI Control Toolbox, we know the matrices P=0.1679I,U1=diag{0.5707,0.5707,0.6318,0.6318} and U2=0.9065I satisfy the condition of Corollary 3.

    On the other hand, Theorem 2.4 in [5] shows that if ρ(K)<1, then zero solution of system (2.4) is globally exponentially stable, where ρ(K) denotes spectral radius of matrix K=(kij)n×n, kij=c1i(|aij|+|bij|)αj,αj corresponds to max{|αj|,|α+j|} in this paper.

    Then, we calculate that for i=1,2,3,4,αi=0.5 and ρ(K)=1, where

    K=(kij)4×4=(0.250.250.250.250.250.250.250.250.250.250.250.250.250.250.250.25).

    Therefore, the condition of Theorem 2.4 in [5] is not satisfied for the system (2.4) in Example 4.

    This paper has investigated the problem for exponential stability of stochastic Hopfield neural networks involving multiple discrete time-varying delays and multiple distributed time-varying delays. The exponential stability of such neural systems has not been given much attention because it is difficult to derive the easily verified stability conditions of the linear matrix inequality forms for this type of neural systems that cannot be transformed into the vector forms. This paper has established the easily verified sufficient conditions of the linear matrix inequality forms to ensure the mean-square exponential stability and the almost sure exponential stability by constructing a suitable Lyapunov-Krasovskii functional and inequality techniques. Four examples demonstrate the effectiveness of the proposed theoretical results and show that the established stability conditions are better than the conditions of the previous stability results.

    The authors would like to thank the editor and the reviewers for their detailed comments and valuable suggestions. This work was supported by the National Natural Science Foundation of China (No: 11971367, 11826209, 11501499, 61573011 and 11271295), the Natural Science Foundation of Guangdong Province (2018A030313536).

    All authors declare no conflicts of interest in this paper.



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