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Research article

Characterizations of matrix equalities involving the sums and products of multiple matrices and their generalized inverse

  • Received: 24 March 2023 Revised: 25 July 2023 Accepted: 09 August 2023 Published: 30 August 2023
  • It is common knowledge that matrix equalities involving ordinary algebraic operations of inverses or generalized inverses of given matrices can be constructed arbitrarily from theoretical and applied points of view because of the noncommutativity of the matrix algebra and singularity of given matrices. Two of such matrix equality examples are given by A1Bg11C1+A2Bg22C2++AkBgkkCk=D and A1Bg11A2Bg22AkBgkkAk+1=A, where A1, A2, , Ak+1, C1, C2, , Ck and A and D are given, and Bg11, Bg22, , Bgkk are generalized inverses of matrices B1, B2, , Bk. These two matrix equalities include many concrete cases for different choices of the generalized inverses, and they have been attractive research topics in the area of generalized inverse theory. As an ongoing investigation of this subject, the present author presents in this article several groups of new results and facts on constructing and characterizing the above matrix equalities for the mixed combinations of {1}- and {1,2}-generalized inverses of matrices with k=2,3 by using some elementary methods, including a series of explicit rank equalities for block matrices.

    Citation: Yongge Tian. Characterizations of matrix equalities involving the sums and products of multiple matrices and their generalized inverse[J]. Electronic Research Archive, 2023, 31(9): 5866-5893. doi: 10.3934/era.2023298

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  • It is common knowledge that matrix equalities involving ordinary algebraic operations of inverses or generalized inverses of given matrices can be constructed arbitrarily from theoretical and applied points of view because of the noncommutativity of the matrix algebra and singularity of given matrices. Two of such matrix equality examples are given by A1Bg11C1+A2Bg22C2++AkBgkkCk=D and A1Bg11A2Bg22AkBgkkAk+1=A, where A1, A2, , Ak+1, C1, C2, , Ck and A and D are given, and Bg11, Bg22, , Bgkk are generalized inverses of matrices B1, B2, , Bk. These two matrix equalities include many concrete cases for different choices of the generalized inverses, and they have been attractive research topics in the area of generalized inverse theory. As an ongoing investigation of this subject, the present author presents in this article several groups of new results and facts on constructing and characterizing the above matrix equalities for the mixed combinations of {1}- and {1,2}-generalized inverses of matrices with k=2,3 by using some elementary methods, including a series of explicit rank equalities for block matrices.



    The stability of Hopfield neural networks is a necessary prerequisite in the practical applications of signal processing [1,2], pattern recognition [3], associative memory [4], nonlinear programming [5] and optimization [6]. Accordingly, the stability of various delayed Hopfield neural networks has been received enough attention [7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33]. In particular, the neutral delays have been introduced into the model of neural networks and the stability of neutral-type neural networks has become a hot topic [18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33]. The mathematical model of neutral-type neural networks extends its application domain to a wider class of practical engineering problems, (for the detailed applications of such neural networks, the readers may refer to the references [34,35,36].)

    The model of Hopfield neural networks of neutral type considered in this paper is expressed as

    ˙xi(t)=cixi(t)+nj=1aijfj(xj(t))+nj=1bijgj(xj(tτij(t)))+nj=1eij˙xj(tξij(t))+ui,t0; (1.1)
    xi(t)=φi(t),˙xi(t)=ϕi(t),t[max{τ,ξ},0],i=1,,n,

    where ξ,τ and ci are positive numbers, φi(t) and ϕi(t) are continuous functions, ξij(t) and τij(t) are delay functions, fj() and gj() are nonlinear continuous activation functions. These functions satisfy that for every x,yR, t0 and i,j=1,,n,

    0ξij(t)ξ,0τij(t)τ,˙ξij(t)¯ξ,˙τij(t)¯τ; (1.2)
    |fi(x)fi(y)|li|xy|,|gi(x)gi(y)|mi|xy|, (1.3)

    where ¯ξ,¯τ,li and mi are some positive numbers. From [37,38], we know that x(t)=(x1(t),,xn(t))T of (1.1) is continuously differentiable.

    The mathematical expression of system (1.1) includes some models studied in existing references. For example, when τij(t)=τj(t) and ξij(t)=ξj(t), system (1.1) transforms into the following vector-matrix form studied [18,20]:

    ˙x(t)=Cx(t)+Af(x(t))+Bg(x(tτ(t)))+E˙x(tξ(t))+u,t0, (1.4)

    whereA=(aij)n×n,B=(bij)n×n,C=diag(c1,,cn),u=(u1,,un)T,

    x(t)=(x1(t),,xn(t))T,˙x(tξ(t))=(˙x1(tξ1(t)),,˙xn(tξn(t)))T,
    f(x(t))=(f1(x1(t)),,fn(xn(t)))T,g(x(tτ(t)))=(g1(x1(tτ1(t))),,gn(xn(tτn(t))))T.

    When τij(t)=τij,fj=gj and ξij(t)=ξij (or ξj), system (1.1) transforms into the following system studied in [30]:

    ˙xi(t)=cixi(t)+nj=1aijfj(xj(t))+nj=1bijfj(xj(tτij))+nj=1eij˙xj(tξij)+ui, (1.5)

    or the following system studied in [29]:

    ˙xi(t)=cixi(t)+nj=1aijfj(xj(t))+nj=1bijfj(xj(tτij))+nj=1eij˙xj(tξj)+ui. (1.6)

    Different from the systems studied in [18,19,20,21,22,23,24,25,26,27,28], system (1.1) cannot be expressed in the vector-matrix form due to the existence of multiple delays τij(t) and ξij(t). Therefore, it is impossible to obtain the stability conditions of the linear matrix inequality form for the system with multiple delays [29,31]. In this case, it is necessary to develop new mathematical techniques and find more suitable Lyapunov-Krasovskii functional for the stability analysis of system (1.1).

    On the other hand, the results of [18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33] have only provided the sufficient conditions of global asymptotic stability and have not considered the exponential stability. Actually, in the stability analysis of neural networks, exponential stability is a better property than asymptotic stability since it can converge to the equilibrium point faster and provides information about the decay rate of the networks. Moreover, the exponential stability property can ensure that whatever transformation occurs, the network stability of fast storage activity mode remains unchanged by self-organization [39]. Therefore, the exponential stability analysis of neural networks with multiple time-varying delays is worth investigating.

    In addition, based on our careful review of recently almost all the existing stability results for system (1.1), we have realized that the research on the exponential stability of system (1.1) has not received enough attention. These facts have been the main motivations of the current paper to focus on the exponential stability of system (1.1).

    The primary contributions and innovations of this work are summarized as follows: (1) novel sufficient conditions of exponential stability are established for Hopfield neural networks of neutral type with multiple time-varying delays; (2) a modified and suitable Lyapunov-Krasovskii functional is provided to study the exponential stability; (3) novel sufficient conditions of global asymptotical stability are provided for the systems studied in the existing references; (4) compared with the existing results, the established conditions are less conservative.

    From [18,20], we know that system (1.1) has at least one equilibrium point x=(x1,,xn)T under the conditions (1.2) and (1.3). By employing the formula yi(t)=xi(t)xi(i=1,,n), system (1.1) can be transformed into the following equivalent system

    ˙yi(t)=ciyi(t)+nj=1aij˜fj(yj(t))+nj=1bij˜gj(yj(tτij(t)))+nj=1eij˙yj(tξij(t)), (2.1)

    where

    ˜fj(yj(t))=fj(yj(t)+xj)fj(xj),˜gj(yj(tτij(t)))=gj(yj(tτij(t))+xj)gj(xj).

    Similarly, system (1.5) can be transformed into the following equivalent system

    ˙yi(t)=ciyi(t)+nj=1aij˜fj(yj(t))+nj=1bij˜fj(yj(tτij))+nj=1eij˙yj(tξij). (2.2)

    It is obvious that if the origin of system (2.1) is exponentially stable, then the equilibrium point of system (1.1) is also exponentially stable. Meanwhile, the origin of system (2.1) and the equilibrium point of system (1.1) are also globally asymptotically stable. Now, we state the main stability result for system (2.1).

    Theorem 1. Suppose that there exist some positive numbers γ,p1,p2,,pn such that γ<1,max{ˉξ,ˉτ}<1γ,

    γpicinj=1pj(li|aji|γ+mi|bji|)>0,piγnj=1pj|eji|>0,i=1,2,,n.

    Then the origin of system (2.1) is exponentially stable.

    Proof. Let

    h1(z)=1eξz¯ξeξzγ,h2(z)=1eτz¯τγ,
    h3(z)=γpicizpiγznj=1pj|eji|nj=1pj(li|aji|γ+mi|bji|eτz).

    Then, ˙hi(z)<0,hi(+)<0,i=1,2,3, and

    h1(0)=1¯ξγ>0,h2(0)=1¯τγ>0,
    h3(0)=γpicinj=1pj(li|aji|γ+mi|bji|)>0.

    Therefore, there exist some positive numbers λ1,λ2 and λ3 such that h1(λ1)=h2(λ2)=h3(λ3)=0, which implies that there must exist a positive number λ(0,min{λ1,λ2,λ3}) such that

    1eλξ¯ξeλξγ>0,1eλτ¯τγ>0, (2.3)
    γpiciλpiγλnj=1pj|eji|nj=1pj(li|aji|γ+mi|bji|eλτ)>0. (2.4)

    We construct the following Lyapunov-Krasovskii functional [40]

    V(t)=eλ(t+ξ)ni=1[piγnj=1pj|eji|sgn(yi(t))sgn(˙yi(t))]|yi(t)|+ni=1nj=1pi|eij|ttξij(t)eλ(s+ξ)|˙yj(s)|ds+eλξni=1nj=1pi|bij|mjttτij(t)eλ(s+τ)|yj(s)|ds, (2.5)

    and derive

    min1in{piγnj=1pj|eji|}eλ(t+ξ)y(t)1eλ(t+ξ)ni=1[piγnj=1pj|eji|]|yi(t)|eλ(t+ξ)ni=1[piγnj=1pj|eji|sgn(yi(t))sgn(˙yi(t))]|yi(t)|V(t), (2.6)
    V(0)=eλξni=1[piγnj=1pj|eji|sgn(yi(0))sgn(˙yi(0))]|yi(0)|+eλξni=1nj=1pi|eij|0ξij(0)eλs|˙yj(s)|ds+eλ(ξ+τ)ni=1nj=1pi|bij|mj0τij(0)eλs|yj(s)|dseλξmax1in{piγ+nj=1pj|eji|}y(0)1+eλξni=1nj=1pi|eij|0ξ|˙yj(s)|ds+eλ(ξ+τ)ni=1nj=1pi|bij|mj0τ|yj(s)|ds. (2.7)

    Taking the right upper Dini derivative of the first term and the time derivatives of the all other terms in the Lyapunov-Krasovskii functional V(t) along the trajectories of system (2.1), we derive

    ˙V(t)=λeλ(t+ξ)ni=1[piγnj=1pj|eji|sgn(yi(t))sgn(˙yi(t))]|yi(t)|+eλtni=1eλξ[piγnj=1pj|eji|sgn(yi(t))sgn(˙yi(t))]sgn(yi(t))˙yi(t)+eλ(t+ξ)ni=1nj=1pi|eij||˙yj(t)|ni=1nj=1(1˙ξij(t))eλ(tξij(t)+ξ)pi|eij||˙yj(tξij(t))|+eλξni=1nj=1pi|bij|mj(eλ(t+τ)|yj(t)|(1˙τij(t))eλ(tτij(t)+τ)|yj(tτij(t))|)λeλ(t+ξ)ni=1(piγ+nj=1pj|eji|)|yi(t)|+eλtni=1{eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|}+ni=1nj=1(˙ξij(t)eλ(tξij(t)+ξ)eλ(tξij(t)+ξ))pi|eij||˙yj(tξij(t))|+eλξni=1nj=1pi|bij|mj(eλ(t+τ)|yj(t)|+[˙τij(t)eλ(tτij(t)+τ)eλ(tτij(t)+τ)]|yj(tτij(t))|)λeλ(t+ξ)ni=1(piγ+nj=1pj|eji|)|yi(t)|+eλtni=1{eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|}+ni=1nj=1(ˉξeλ(t+ξ)eλt)pi|eij||˙yj(tξij(t))|+eλξni=1nj=1pi|bij|mj(eλ(t+τ)|yj(t)|+(ˉτeλ(t+τ)eλt)|yj(tτij(t))|)=λeλ(t+ξ)ni=1(piγ+nj=1pj|eji|)|yi(t)|+eλtni=1{eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|}+eλt(¯ξeλξ1)ni=1nj=1pi|eij||˙yj(tξij(t))|+eλξni=1nj=1pi|bij|mj(eλ(t+τ)|yj(t)|+(¯τeλτ1)eλt|yj(tτij(t))|). (2.8)

    It is noted that for yi(t)0,

    eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|=eλξpiγsgn(yi(t))˙yi(t)=eλξ{γpisgn(yi(t))ciyi(t)+γpisgn(yi(t))nj=1aij˜fj(yj(t))+γpisgn(yi(t))nj=1bij˜gj(yj(tτij(t)))+γpisgn(yi(t))nj=1eij˙yj(tξij(t))}eλξ{γpisgn(yi(t))ciyi(t)+|γpisgn(yi(t))nj=1aij˜fj(yj(t))|+|γpisgn(yi(t))nj=1bij˜gj(yj(tτij(t)))|+|γpisgn(yi(t))nj=1eij˙yj(tξij(t))|}eλξ{γpici|yi(t)|+γpinj=1|aij|lj|yj(t)|+γpinj=1|bij|mj|yj(tτij(t))|}+eλξγpinj=1|eij||˙yj(tξij(t))|,

    and for yi(t)=0,

    eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|=eλξnj=1pj|eji||˙yi(t)|=eλξ{nj=1pj|eji|sgn(˙yi(t))ciyi(t)+nj=1pj|eji|sgn(˙yi(t))nj=1aij˜fj(yj(t))+nj=1pj|eji|sgn(˙yi(t))nj=1bij˜gj(yj(tτij(t)))+nj=1pj|eji|sgn(˙yi(t))nj=1eij˙yj(tξij(t))}eλξ{γpici|yi(t)|+|nj=1pj|eji|sgn(˙yi(t))nj=1aij˜fj(yj(t))|+|nj=1pj|eji|sgn(˙yi(t))nj=1bij˜gj(yj(tτij(t)))|+|nj=1pj|eji|sgn(˙yi(t))nj=1eij˙yj(tξij(t))|}eλξ{γpici|yi(t)|+nj=1pj|eji|nj=1|aij|lj|yj(t)|+nj=1pj|eji|nj=1|bij|mj|yj(tτij(t))|}+eλξnj=1pj|eji|nj=1|eij||˙yj(tξij(t))|eλξ{γpici|yi(t)|+γpinj=1|aij|lj|yj(t)|+γpinj=1|bij|mj|yj(tτij(t))|}+eλξγpinj=1|eij||˙yj(tξij(t))|,

    where we use nj=1pj|eji|<piγ, and nj=1pj|eji|sgn(˙yi(t))ciyi(t)=γpici|yi(t)|=0 when yi(t)=0.

    Therefore, for every yi(t)R, we have

    eλξpiγsgn(yi(t))˙yi(t)eλξnj=1pj|eji|(sgn(yi(t)))2|˙yi(t)|+eλξnj=1pj|eji||˙yi(t)|eλξ{γpici|yi(t)|+γpinj=1|aij|lj|yj(t)|+γpinj=1|bij|mj|yj(tτij(t))|}+eλξγpinj=1|eij||˙yj(tξij(t))|. (2.9)

    Then, from (2.3), (2.4), (2.8) and (2.9), we have

    ˙V(t)λeλ(t+ξ)ni=1(piγ+nj=1pj|eji|)|yi(t)|+eλtni=1{eλξ(γpici|yi(t)|+γpinj=1|aij|lj|yj(t)|+γpinj=1|bij|mj|yj(tτij(t))|)+(eλξγ+eλξ¯ξ1)pinj=1|eij||˙yj(tξij(t))|}+eλξni=1nj=1pi|bij|mj(eλ(t+τ)|yj(t)|+(¯τeλτ1)eλt|yj(tτij(t))|)=eλ(t+ξ)ni=1(γpiciλpiγλnj=1pj|eji|nj=1pj(li|aji|γ+mi|bji|eλτ))|yi(t)|eλt(1eλξ¯ξeλξγ)ni=1nj=1pi|eij||˙yj(tξij(t))|(1eλτ¯τγ)eλ(t+ξ)ni=1nj=1pi|bij|mj|yj(tτij(t))|0. (2.10)

    Finally, (2.6), (2.7) and (2.10) imply that there must exist a number δ>1 such that

    y(t)1δeλt(φ1+ϕ1),t0,

    where

    φ1=supt[max{τ,ξ},0]φ(t)1,ϕ1=supt[max{τ,ξ},0]ϕ(t)1.

    Generally speaking, it is not easy to find the values of the positive constants p1,,pn. Therefore, it is necessary to give a result without involving the constants p1,,pn. The following result is a special case of Theorem 1 for p1==pn, which is easier to validate.

    Theorem 2. Suppose that there exists a positive number γ such that

    max{ˉξ,ˉτ}<1γ,nj=1|eji|<γ<1,γcinj=1(li|aji|γ+mi|bji|)>0,i=1,2,,n.

    Then the equilibrium point of system (1.1) is globally asymptotically stable, even exponentially stable.

    Remark 1. Theorem 1 and Theorem 2 give novel sufficient conditions of global asymptotical stability for the systems studied in [18,20,29,30] since these systems are some special cases of system (1.1).

    For system (1.5) or (1.6), Theorem 1 and Theorem 2 give the following results.

    Corollary 1. Suppose that there exist some positive numbers γ,p1,p2,,pn such that γ<1,

    γpicinj=1pjli(|aji|γ+|bji|)>0,piγnj=1pj|eji|>0,i=1,2,,n.

    Then the equilibrium point of system (1.5) (or (1.6)) is globally asymptotically stable, even exponentially stable.

    Corollary 2. Suppose that there exists a positive number γ such that γ<1,

    γcinj=1li(|aji|γ+|bji|)>0,γnj=1|eji|>0,i=1,2,,n.

    Then the equilibrium point of system (1.5) (or (1.6)) is globally asymptotically stable, even exponentially stable.

    Remark 2. It is noted that γpicinj=1pjli(|aji|γ+|bji|)>0 and 0<γ<1 can deduce that picinj=1pjli(|aji|+|bji|)>0. Therefore, the conditions of Corollary 2 are less conservative than those of the result in [29].

    Remark 3. For system (1.5), the conditions of Theorem 1 in [30] are as follows:

    αi=c2il2inj=1|nk=1akiakj|l2inj=1nk=1(|aji||bjk|+|bji||ajk|+|bji||bjk|)l2inj=1nk=1cj|ejk|(|aji|+|bji|)nj=1nk=1cj|eji|(|ajk|+|bjk|)nj=1c2i|eij|nj=1c2j|eji|>0,

    and 1nj=1|eji|>0,i=1,,n. Example 2 demonstrates the above conditions are not satisfied while the conditions of Corollary 1 and Corollary 2 can be satisfied.

    Remark 4. Global asymptotical stability of a more general class of multiple delayed neutral type neural network model has been studied in [31,32]. The results of [31,32] can be particularized for system (2.2) as follows:

    i) The sufficient conditions of global asymptotical stability are given in [31]:

    σi=2cinj=1(lj|aij|+li|aji|)nj=1(lj|bij|+li|bji|)nj=1(|eij|+|eji|)nj=1nk=1(li|aki||ekj|+li|bki||ekj|)nj=1nk=1(lk|ajk||eji|+lk|bjk||eji|)>0,

    and 1nj=1|eji|>0,i=1,,n.

    ii) The sufficient conditions of global asymptotical stability are given in [32]:

    ϵi=c2inj=1|nk=1akiakj|nj=1nk=1(|aji||bjk|+|aji||ejk|+|bji||ajk|+|bji||ejk|+|bji||bjk|)>0,
    εij=1nnk=1(|eji||ejk|+|ajk||eji|+|bjk||eji|)>0,i,j=1,,n.

    Example 3 demonstrates the above conditions are not satisfied while the conditions of Corollary 1 and Corollary 2 can be satisfied.

    Example 1. Consider system (1.1) with the following conditions:

    A=(1111111111111111),B=(1111111111111111),E=(0.10.10.10.10.10.10.10.10.10.10.10.10.10.10.10.1),

    c1=c2=c3=9,c4=8,fi(x)=tanh(x),gi(x)=0.5tanh(x),ξii(t)=0.1sint+0.1,τii(t)=0.1cost+0.1;ξij(t)=0.1cost+0.1,τij(t)=0.1sint+0.1,ij;i,j=1,2,3,4.

    We calculate ˉξ=ˉτ=0.1,li=1,mi=0.5,4j=1|eji|=0.4 and

    ciγ4j=1(li|aji|γ+mi|bji|)={5γ2,i=1,2,3;4γ2,i=4.

    It is clear that when γ(0.5,0.9), Theorem 2 holds.

    Now we choose γ=0.424 and require that

    γpici4j=1pj(li|aji|γ+mi|bji|)=0.01,i=1,2,3,4.

    Then, we calculate p1=p2=p3=2.2222,p4=2.5000, and

    piγ4j=1pj|eji|=0.424pi0.14j=1pj={0.025552,i=1,2,3;0.14334,i=4.

    Thus, all conditions of Theorem 1 are satisfied.

    If we choose γ=0.423 and still require that

    γpici4j=1pj(li|aji|γ+mi|bji|)=0.01,i=1,2,3,4.

    Then pi<0,i=1,2,3,4. Therefore, when γ[0.424,0.9), the system (1.1) in this example is globally asymptotically stable, even exponentially stable.

    Example 2. Consider system (1.5) with the conditions: c1=c2=c3=9,c4=8.5,fi(x)=tanh(x),ξii=0.2,τii=0.1;ξij=0.3,τij=0.4,ij;i,j=1,2,3,4, the matrices A,B,E are the same as in Example 1.

    Then, we calculate li=1,4j=1|eji|=0.4 and

    ciγ4j=1li(|aji|γ+|bji|)={5γ4,i=1,2,3;4.5γ4,i=4.

    It is clear that when γ(8/9,1), Corollary 2 holds.

    Now we choose γ=0.85 and require that

    γpici4j=1pjli(|aji|γ+|bji|)=0.01,i=1,2,3,4.

    Then, we calculate p1=p2=p3=0.0708,p4=0.0750, and

    piγ4j=1pj|eji|=0.85pi0.14j=1pj={0.03144,i=1,2,3;0.03501,i=4.

    Thus, all conditions of Corollary 1 are satisfied.

    On the other hand, we calculate

    α1=814j=1|4k=1ak1akj|3×4×435.5×4×0.235.5×4×0.281×0.4315.25×0.1<0,

    which shows the conditions of Theorem 1 in [30] are not satisfied. Therefore, Theorem 1 in [30] is invalid for the system (1.5) in this example.

    Example 3. Consider system (2.2) with all parameters and functions are the same as in Example 2. Then, we calculate li=1,4j=1|eji|=0.4,

    εij=140.21×4=0.59<0,
    σ1=2×92×42×40.2×40.2×420.2×42=5.2<0.

    Therefore, the sufficient conditions of the results in [31,32] are not satisfied. Meanwhile, all conditions of Corollary 1 and Corollary 2 are staisfied for system (2.2) since system (1.5) is equivalent to system (2.2).

    This paper has investigated the exponential stability of neutral-type Hopfield neural networks involving multiple time-varying delays. Different from some existing results, linear matrix inequality approach cannot be used to determine the stability conditions of such networks since the networks studied here can not be expressed in vector-matrix form. By using a modified and suitable Lyapunov-Krasovskii functional and inequality techniques, novel algebraic conditions are established to ensure the exponential stability and the global asymptotic stability of neutral-type Hopfield neural networks involving multiple time-varying delays. Compared with some references, the networks studied here is more general and the established conditions are less conservative. Three examples are given to demonstrate the effectiveness of the theoretical results and compare the established stability conditions to the previous 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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