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Theory article

Robustness analysis of neutral fuzzy cellular neural networks with stochastic disturbances and time delays

  • Received: 16 July 2024 Revised: 08 September 2024 Accepted: 29 September 2024 Published: 17 October 2024
  • MSC : 93B35, 93D23

  • This paper discusses the robustness of neutral fuzzy cellular neural networks with stochastic disturbances and time delays. This work questions whether fuzzy cellular neural networks, which initially remains stable, can be stabilised again when the system is subjected to three simultasneous perturbations i.e., neutral items, random disturbances, and time delays. First, by using inequality techniques such as Gronwall's Lemma, the Itŏ formula, and the property of integrals, the transcendental equations that contain the contraction coefficient of the neutral terms, the intensity of the random disturbances, and the time delays are derived. Then, the upper bounds of the neutral terms, random disturbances, and time delays are estimated by solving the transcendental equations for multifactor perturbations, which ensures that the disturbed fuzzy cellular neural network can be stabilised again. Finally, the validity of the results is verified by numerical examples.

    Citation: Yunlong Ma, Tao Xie, Yijia Zhang. Robustness analysis of neutral fuzzy cellular neural networks with stochastic disturbances and time delays[J]. AIMS Mathematics, 2024, 9(10): 29556-29572. doi: 10.3934/math.20241431

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  • This paper discusses the robustness of neutral fuzzy cellular neural networks with stochastic disturbances and time delays. This work questions whether fuzzy cellular neural networks, which initially remains stable, can be stabilised again when the system is subjected to three simultasneous perturbations i.e., neutral items, random disturbances, and time delays. First, by using inequality techniques such as Gronwall's Lemma, the Itŏ formula, and the property of integrals, the transcendental equations that contain the contraction coefficient of the neutral terms, the intensity of the random disturbances, and the time delays are derived. Then, the upper bounds of the neutral terms, random disturbances, and time delays are estimated by solving the transcendental equations for multifactor perturbations, which ensures that the disturbed fuzzy cellular neural network can be stabilised again. Finally, the validity of the results is verified by numerical examples.



    In recently years, neural networks have achieved extensive and in-depth applications in many fields such as aerospace [1], biomedicine [2], and pattern recognition [3], which has inspired many scholars to explore them with great interest. With the continuous development of neural network research, many classical network types have been proposed, such as recurrent neural networks[4], Hopfield neural networks [5], cellular neural networks [6], and so on. Cellular neural networks were proposed by Chuan and Yang in 1988 [6,7], where the neural network connection method derives from neurons that are interconnected only with other neurons in a specific region. This unique connection significantly reduces the complexity of network interconnections, thus showing a great potential and value for applications in many fields such as image encryption [8], parallel signal processing [9], and so on. As an important branch of cellular neural networks, fuzzy cellular neural networks (FCNNs) were proposed by Yang and Yang in 1996 [10,11], who introduced fuzzy logic into cellular neural networks. Fuzzy logic describes and handles uncertainty or ambiguity through fuzzy sets and fuzzy rules, which makes cellular neural networks more accurate and reliable when dealing with complex information in the real world, as well as improves the robustness and fault tolerance of the system, which in turn enhances the practical application of the network [12,13].

    It is well known that stability is usually the first condition for the successful application of FCNNs. The stability of neural networks not only relies on the configuration of the parameters, but is also inevitably affected by external factors. In practical engineering applications, stochastic disturbances and time delays are common perturbation factors. If the intensity of the perturbation exceeds the perturbation limit, then it will destroy the stability of the network. In recent years, scholars have investigated the stability of FCNNs using Lyapunov's method, the Linear Matrix Inequality (LMI), and other methods, which have produced a series of remarkable research results [14,15,16,17,18,19]. For example, in the literature [14], Long et al. established a new L-operational inequality and used the properties of M-matrices, a p-order moment stability criterion for the exponential stabilisation of FCNNs, and time delays and stochastic perturbations were obtained. In the literature [15], Zhang et al. studied fractional order FCNNs with time delays and random perturbations, which produced a new stability criterion.

    However, the aforementioned literature solely discusses the stability of FCNNs. The neural network is destabilised when random disturbances and time delays are beyond the specified range. Therefore, it is a fascinating subject to discuss how much an initially stable system can withstand the intensity of perturbations and still remain stable. This type of analysis is often referred to as a robustness analysis of stability. The problem of a robustness analysis has received the attention of many scholars and many excellent outcomes have been published [4,20,21,22,23]. For example, in the literature [4], Shen et al. considered the robustness problem for the stability of recurrent neural networks that contained stochastic perturbations and time delays. In the literature [20], Zhu et al. considered the robustness of recurrent neural networks with Markov switching parameters. In the literature [21], Yang et al. explored the robustness problem of global exponential stability for nonlinear systems with time-varying delays and nonlinear stochastic perturbations. However, there is less literature on the robustness analysis of the fuzzy neural network stability, which is one of the motivations for writing this paper.

    It is worth noting that neutral neural networks belong to a particular class of neural networks whose distinguishing feature is the simultaneous existence of time delays in the system state and state derivatives. This property makes it possible to more accurately describe and portray the changes in the network state, and thus has attracted a great deal of interest from many researchers, and a series of research results were reported [24,25]. However, it is also interesting to introduce neutral terms into other neural networks and to consider their robustness. [26,27,28,29]. For example, in the literature [26], Shen et al. explored the robustness of the global exponential stability (GES) for nonlinear systems with time-varying delays and neutral terms as perturbing factors. In the literature [29], Si et al. discussed the robustness of the GES of recurrent neural networks with neutral terms and generalized piecewise constant arguments. However, the issue of the robustness of neutral FCNNs with random perturbations and time-varying delays has hardly been considered.

    Based on the above discussions and analyses, the main problem investigated for this paper is the robustness of the GES for neutral FCNNs with time delays and stochastic perturbations. The major contents and contributions of this paper include the following:

    (i) By using some inequality techniques such as the Gronwall lemma, the Itŏ formula, and the Cauchy inequality, multivariate implicit transcendental equations which incorporate random perturbations, time delays, and contraction coefficients of the neutral terms are obtained. From this, an upper bound on the effect of these perturbations on the stability of the fuzzy system is estimated, which ensures that the initially stable fuzzy system can remain globally exponentially stable when subjected to perturbations.

    (ii) Compared with the literature, which is known to contain two kinds of perturbation factors, this paper considers the robustness analysis of the GES of FCNNs with three kinds of perturbation factors: neutral terms, random perturbations and time delays. It not only enriches the theoretical study of FCNNs, but also provides theoretical support for fuzzy system stability analyses and designs.

    (iii) Compared with the existing literature [4,28,30], the system in this paper contains fuzzy logic, neutral terms, time delays, and random disturbances. Therefore, when solving the transcendental equation, there are more disturbances to be considered, which increases the difficulty of solving and makes the system more applicable.

    The rest of the paper is organised as follows: Section 2 provides a model of a neutral FCNN with random disturbances and time delays, as well as the relevant definitions and lemmas to be used in the proof; Section 3 derives the theoretical results for an initially stable fuzzy system that remains GES in spite of multifactorial disturbances; and Section 4 provides some numerical examples to verify the validity of the results.

    Notations : Denote R=(,+), R+=[0,+), N={1,2,}, and Rm denotes the space which consists of all m-dimensional vectors. For a vectors η=(η1,η2,,ηm)T, we denote η=mi=1|ηi|, iN, where ηiR. (Ω,F,{Ft}t0,P) is a complete filtered probability space, where {Ft}t0 is a right-continuous filter and satisfies the usual condition that the space contains all P-null sets. B(t) is a scalar brownian motion defined at (Ω,F,{Ft}t0,P). E represents an operator that computes the mathematical expectation of a given probability measure P. Fuzzy AND and fuzzy OR operations are denoted by and , respectively.

    Consider the following mathematical model of FCNNs:

    {dˉPi(t)=[aiˉPi(t)+mj=1bijgj(ˉPj(t))+mj=1cijgj(ˉPj(t))+mj=1dijgj(ˉPj(t))+mj=1eijgj(ˉPj(t))]dt,ˉPi(t0)=ψ(0), (2.1)

    where i,jN, and ˉPi(t) denotes the state of the i th neuron at time t. dij and eij are elements of the fuzzy feedback MIN template and the fuzzy feed-forward MAX template, respectively. gj() is the activation function. ˉPi(t0)R is the initial value of FCNNs (2.1).

    Assume P is the equilibrium point of FCNNs (2.1), where P={P1,,Pm}T; then, let P(t)=ˉP(t)P(t) and fj(Pj(t))=gj(Pj(t)+Pj)g(P), Pi(t0)=φ(0)=ψi(0)ψ. Then, FCNNs (2.1) can be written in the following form:

    {dPi(t)=[aiPi(t)+mj=1bijfj(Pj(t))+mj=1cijfj(Pj(t))+mj=1dijfj(Pj(t))+mj=1eijfj(Pj(t))]dt,Pi(t0)=φ(0). (2.2)

    Next, consider the FCNNs model with neutral terms, random perturbations, and time delays:

    {d[Qi(t)Gi(Qi(tτ(t)))]=[aiQi(t)+mj=1bijfj(Qj(t))+mj=1cijfj(Qj(tτ(t)))                             +mj=1dijfj(Qj(t)τ(t))+mj=1eijfj(Qj(tτ(t)))]dt+mj=1σijQj(t)dB(t),Qi(t)=ϕ(tt0)([τ,0],Rm),t0ˉτtt0, (2.3)

    where i,jN, Qi(t) is the state of the i neuron at time t, and G:RmRm is the weight matrix of neutral term. τ(t) is a delay that satisfies τ(t): [t0,+) [0,ˉτ], τ(t)ζ<1, ϕ={ϕi(s):ˉτs0}([ˉτ,0],Rm). B(t) is a scalar brownian motion defined in the probability space (Ω,F,{Ft}t0,P). σ=(σij)m×m is a matrix of diffusion coefficients.

    For the purpose of the proof of this paper, some assumptions and definitions to be used are given below.

    Assumption A1. Assume the activation functions fj(), satisfies the following inequality:

    |fj(Uj(t))fj(Vj(t))|Lj|Uj(t)Vj(t)|,     fj(0)0     j=1,2,,

    where Lj(0,1) are known constants.

    Lemma 1. [15] If A1 holds, then the solution P(t)=(P1(t),,Pm(t))T of FCNNs (2.2) satisfies the initial unique condition.

    Assumption A2. [28] There exists the Lipschitz coefficient κi(0,1), im, such that |Gi(Ui(t))Gi(Vi(t))|κi|Ui(t)Vi(t)| holds for any variable component Ui,Vi. Therefore, let κ=maxim{κi}, where the above formula can be expressed as follows:

    Gi(U(t))Gi(V(t))κU(t)V(t).

    Definition 1. The state of FCNNs (2.2) is GES, if there exist λ>0 and θ>0 such that

    P(t;t0,φ(0))λφ(0)exp(θ(tt0)),tt0.

    Definition 2. [14] FCNNs (2.3) is said to be mean square globally exponentially stable (MSGES), if tR+, ϕ(0)Rm, exist ˉλ>0 and ˉθ>0 such that

    EQ(t;t0,ϕ)2ˉλϕ2exp(ˉθ(tt0)),tt0,

    where the Lyapunov exponent lim supt1tlnEQ(t;t0,ϕ)2<0. And Q(t;t0,ϕ) is the state of FCNNs (2.3). FCNNs (2.3) is said to be almost surely globally exponentially stable (ASGES), if tR+, ϕ(0)Rm, and the Lyapunov exponent almost surely lim supt1tlnQ(t;t0,ϕ)<0.

    Remark 1. From the above definitions, it is clear that the ASGES of FCNNs (2.3) implies the MSGES of FCNNs (2.3) [31], but not vice versa. Therefore, let Assumption A1 hold. The MSGES of FCNNs (2.3) implies the ASGES of FCNNs (2.3).

    Lemma 2.[11] For FCNNs (2.3),

    |mj=1dijfj(Uj(t))mj=1dijfj(Vj(t))|mj=1lj|dij||Uj(t)Vj(t)|,|mj=1eijfj(Uj(t))mj=1eijfj(Vj(t))|mj=1lj|eij||Uj(t)Vj(t)|.

    Lemma 3.[31] Let f:Rm×R×[a,b]Rm×m, such that the following inequality holds

    E|baf(t)dB(t)|2=Eba|f(t)|2dt.

    Theorem 1. If Assumptions A1 and A2, Lemmas 2 and 3 hold, and stystem FCNNs (2.2) is GES, then FCNNs (2.3) is MSGES and ASGES. If κ<min{˜κ,(exp(2ΔM1)12[1+24m22Δ2((1ζ)1+(12ζ)1)])12}, then |σ|<ˉσ and ˉτ<min{Δ/2,˘τ}, where ˜κ, ˉσ, ˘τ are the solutions of following three transcendental equations:

    2λ2exp(2θΔ)+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)=1, (3.1)

    and

    2λ2exp(2θΔ)+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)=1, (3.2)

    and

    2λ2exp(2θ(Δτ))+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)=1, (3.3)

    where

    Δ>2ln(2λ2)/2θ,  m1=max1im{|ai|+|Li|mj=1|bji|},   m2=max1im{|Li|mj=1|cji|+|li|mj=1|dji|+|li|mj=1|eji|},σ=max1immj=1|σji|,   M1=12Δ(m1+m2)2,   M2=6κ2[1+24Δ2m22(11ζ+112ζ)],    M3=12κ2,M1=12Δ(m1+m2)2+6σ2,    M2=6˜κ2[1+24Δ2m22(11ζ+112ζ)],    M3=12˜κ2+3σ2λ2/θ,M1=6{2Δ(m1+m2)2+ˉσ2(1+12Δm22˘τ)+24Δm22˘τ2(m21+m22(1ζ)1)},M3=3{4˜κ2+8m22Δ˘τ[1+1+3˜κ2+3m22˘τ21ζ+6˜κ212ζ]+24m22Δ˘τ2[m21+m22(1ζ)1]λ2/θ+ˉσ2(1+12Δm22˘τ)λ2/θ}.

    Proof. From the fuzzy systems (2.2) and (2.3),

    Pi(t)Qi(t)+Gi(Qi(tτ(t)))Gi(Qi(t0τ(t0)))  =tt0{ai(Pi(s)Qi(s))+mj=1bij(fj(Pj(s))fj(Qj(s))  +mj=1cij(fj(Pj(s))fj(Qj(sτ(s))))+mj=1dij(fj(Pj(s))fj(Qj(sτ(s))))  +mj=1eij(fj(Pj(s))fj(Qj(sτ(s))))}dstt0mj=1σijQj(s)dB(s). (3.4)

    Let

    m1=max1im{|ai|+|Li|mj=1|bji|},  m2=max1im{|Li|mj=1|cji|+|li|mj=1|dji|+|li|mj=1|eji|},  σ=max1immj=1|σji|.

    Based on A1, A2, and Lemma 2, when t0tt0+2Δ, we have the following:

    P(t)Q(t)=mi=1|Pi(t)Qi(t)|  G(Q(tτ(t)))G(Q(t0τ(t0)))+mi=1{tt0|ai||Pi(s)Qi(s)|    +|Li|mj=1|bji||Pi(s)Qi(s)|+|Li|mj=1|cji||Pi(s)Qi(sτ(s))|    +|li|mj=1|dji||Pi(s)Qi(sτ(s))|+|li|mj=1|eji||Pi(s)Qi(sτ(s))|}ds    +tt0mi=1mj=1|σji||Qi(s)|dB(s)  κQ(tτ(t))Q(t0τ(t0))+tt0(m1+m2)P(s)Q(s)ds    +tt0m2Q(s)Q(sτ(s))ds+tt0σQ(s)dB(s). (3.5)

    Furthermore, by Lemma 3,

    EP(t)Q(t)23κ2EQ(tτ(t))Q(t0τ(t0))2+3E{tt0(m1+m2)P(s)Q(s)+m2Q(s)Q(sτ(s))ds}2+3Ett0σ2Q(s)2ds3κ2EQ(tτ(t))Q(t0τ(t0))2+6[2Δ(m1+m2)2+σ2]tt0EP(s)Q(s)2ds+12Δm22tt0EQ(s)Q(sτ(s))2ds+6σ2tt0EP(s)2ds. (3.6)

    For the first term in (3.6), when t0tt0+2Δ,

    3κ2EQ(tτ(t))Q(t0τ(t0))26κ2EQ(tτ(t))2+6κ2EQ(t0τ(t0))26κ2supt0ˉτst0ˉτ+2ΔEQ(s)2+6κ2supt0ˉτst0+ˉτEQ(s)212κ2supt0ˉτst0+ˉτEQ(s)2+6κ2supt0+ˉτst0ˉτ+2ΔEQ(s)2. (3.7)

    For the time delays term contained in (3.6), when t0tt0+ˉτ, we can obtain the following:

    tt0EQ(s)Q(sτ(s))2ds  t0+ˉτt02EQ(s)2ds+t0+ˉτt02EQ(sτ(s))2ds  2[τ+τ(1ζ)1]supt0ˉτst0+ˉτEQ(s)2. (3.8)

    When t0+ˉτtt0+2Δ, we can obtain the following:

    tt0+ˉτEQ(s)Q(sτ(s))2dstt0+ˉτ3κ2EQ(sτ(s))Q(s2τ(s))2ds  +tt0+ˉτ3E(ssˉτm1Q(u)+m2Q(uτ(u))du)2ds+tt0+ˉτ3Essˉτσ2Q(u)2duds3κ2tt0+ˉτEQ(sτ(s))Q(s2τ(s))2ds+3(2ˉτm21+σ2)tt0+ˉτssˉτEQ(u)2duds  +6ˉτm22tt0+ˉτssˉτEQ(uτ(u))2duds. (3.9)

    Noting that 2ˉτΔ, for the first term in (3.9), when t0+ˉτtt0+2ˉτ, we have the following:

    3κ2tt0+ˉτEQ(sτ(s))Q(s2τ(s))2ds 6κ2tt0ˉτEQ(sτ(s))2ds+6κ2tt0ˉτEQ(s2τ(s))2ds 6κ2(1ζ)1t0ˉτt0EQ(u)2du+6κ2(12ζ)1t2τt0ˉτEQ(u)2du 6κ2(1ζ)1t0ˉτt0EQ(s)2ds+6κ2(12ζ)1t0t0ˉτEQ(u)2du   +6κ2(12ζ)1tˉτt0EQ(u)2du 6κ2ˉτ(12ζ)1supt0ˉτst0EQ(s)2+6κ2(11ζ+112ζ)tˉτt0EQ(s)2ds 6κ2ˉτ(12ζ)1supt0ˉτst0EQ(s)2+6κ2(11ζ+112ζ)t0+ˉτt0EQ(s)2ds   +6κ2(11ζ+112ζ)t0ˉτ+2Δt0+ˉτEQ(s)2ds6κ2ˉτ(12ζ)1supt0ˉτst0EQ(s)2+6κ2ˉτ(11ζ+112ζ)supt0st0+ˉτEQ(s)2   +6κ2(2Δ2ˉτ)(11ζ+112ζ)supt0+ˉτst0ˉτ+2ΔEQ(s)26κ2ˉτ(11ζ+212ζ)supt0ˉτst0+ˉτEQ(s)2+12κ2Δ(11ζ+112ζ)supt0+ˉτst0ˉτ+2ΔEQ(s)2. (3.10)

    For the second term in (3.9), exchanging the order of integrations,

    3(2ˉτm21+σ2)tt0+ˉτssˉτEQ(u)2duds=3(2ˉτm21+σ2)tt0dumin(u+ˉτ,t)max(t0+ˉτ,u)EQ(u)2ds3ˉτ(2ˉτm21+σ2)tt0EQ(u)2du. (3.11)

    Similarly, for the third term in (3.9),

    6ˉτm22tt0+ˉτssˉτEQ(uτ(u))2duds=6ˉτm22tt0dumin(u+ˉτ,t)max(t0+ˉτ,u)EQ(uτ(u))2ds 6ˉτ2m22tt0EQ(uτ(u))2du 6ˉτ2m22(1ζ)1tt0ˉτEQ(v)2dv 6ˉτ2m22(1ζ)1t0t0ˉτEQ(v)2dv+6ˉτ2m22(1ζ)1tt0EQ(v)2dv 6ˉτ3m22(1ζ)1supt0ˉτst0EQ(s)2+6ˉτ2m22(1ζ)1tt0EQ(s)2ds. (3.12)

    Therefore, from (3.8)–(3.12), when t0tt0+2Δ, we have the following:

    tt0EQ(s)Q(sτ(s))2ds2[ˉτ+ˉτ(1ζ)1]supt0ˉτst0+ˉτEQ(s)2+6k2ˉτ(11ζ+212ζ)supt0ˉτst0+ˉτEQ(s)2   +12k2Δ(11ζ+112ζ)supt0+ˉτst0ˉτ+2ΔEQ(s)2+3ˉτ(2ˉτm21+σ2)tt0EQ(s)2ds   +6ˉτ3m22(1ζ)1supt0ˉτst0EQ(s)2+6ˉτ2m22(1ζ)1tt0EQ(s)2ds3ˉτ[2ˉτm21+σ2+2ˉτm22(1ζ)1]tt0EQ(s)2ds   +12k2Δ(11ζ+112ζ)supt0+ˉτst0ˉτ+2ΔEQ(s)2   +2ˉτ[1+1+3k2+3ˉτ2m221ζ+6k212ζ]supt0ˉτst0+ˉτEQ(s)2. (3.13)

    Substituting (3.7) and (3.13) into (3.6), we further conclude the following:

    EP(t)Q(t)212κ2supt0ˉτst0+ˉτEQ(s)2+6κ2supt0+ˉτst0ˉτ+2ΔEQ(s)2    +6[2Δ(m1+m2)2+σ2]tt0EP(s)Q(s)2ds+6σ2tt0EP(s)ds    +36Δm22ˉτ[2ˉτm21+σ2+2ˉτm22(1ζ)1]tt0EQ(s)2ds    +144m22Δ2κ2(11ζ+112ζ)supt0+ˉτst0ˉτ+2ΔEQ(s)2    +24m22Δˉτ[1+1+3κ2+3m22ˉτ21ζ+6κ212ζ]supt0ˉτst0+ˉτEQ(s)26{2Δ(m1+m2)2+σ2(1+12Δm22ˉτ)+24Δm22ˉτ2(m21+m22(1ζ)1)}tt0EP(s)Q(s)2ds    +6κ2[1+24Δ2m22(11ζ+112ζ)]supt0+ˉτst0ˉτ+2ΔEQ(s)2    +3{4κ2+8m22Δˉτ[1+1+3κ2+3m22ˉτ21ζ+6κ212ζ]+24m22Δˉτ2[m21+m22(1ζ)1]λ2/θ       +σ2(1+12Δm22ˉτ)λ2/θ}supt0ˉτst0+ˉτEQ(s)2=M1tt0EP(s)Q(s)2ds+M2supt0+ˉτst0ˉτ+2ΔEQ(s)2+M3supt0ˉτst0+ˉτEQ(s)2M1tt0EP(s)Q(s)2ds+2M2supt0ˉτ+Δst0ˉτ+2ΔEP(s)Q(s)2     +[M3+M2(1+2λ2exp(2θ(Δˉτ)))]supt0ˉτst0ˉτ+ΔEQ(s)2=M1tt0Ey(s)x(s)2ds+2M2ˉM+[M3+M2(1+2λ2exp(2θ(Δˉτ)))]˜M, (3.14)

    where

    M1=6{2Δ(m1+m2)2+σ2(1+12Δm22ˉτ)+24Δm22ˉτ2(m21+m22(1ζ)1)},M2=6κ2[1+24Δ2m22(11ζ+112ζ)],M3=3{4κ2+8m22Δˉτ[1+1+3κ2+3m22ˉτ21ζ+6κ212ζ]+24m22Δˉτ2[m21+m22(1ζ)1]λ2/θ+σ2(1+12Δm22τ)λ2/θ},ˉM=supt0ˉτ+Δst0ˉτ+2ΔEP(s)Q(s)2,   ˜M=supt0ˉτst0ˉτ+ΔEQ(s)2.

    Noting that 2ˉτΔ, by the Gronwall inequality, for t0tt0+2Δ, we can obtain the following:

    EP(t)Q(t)2{2M2ˉM+[M3+M2(1+2λ2exp(2θ(Δˉτ)))]˜M}exp(2ΔM1). (3.15)

    Therefore,

    ˉM=supt0ˉτ+Δst0ˉτ+2ΔEP(s)Q(s)2supt0st0+2ΔEP(s)Q(s)2{2M2ˉM+[M3+M2(1+2λ2exp(2θ(Δˉτ)))]˜M}exp(2ΔM1). (3.16)

    Noting that κ<(exp(2ΔM1)12[1+24m22Δ2((1ζ)1+(12ζ)1)])12, thus ˉM[M3+M2(1+2λ2exp(2θ(Δˉτ)))]˜Mexp(2ΔM1)12M2exp(2ΔM1).

    Therefore, owing to system (2.2) being GES, when t0ˉτ+Δtt0ˉτ+2Δ, we have the following:

    EQ(t)22EP(t)2+2EP(t)Q(t)22λ2exp(2θ(Δˉτ))supt0ˉτst0ˉτ+ΔEQ(s)2+2[M3+M2(1+2λ2exp(2θ(Δˉτ)))]˜Mexp(2ΔM1)12M2exp(2ΔM1){2λ2exp(2θ(Δˉτ))+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)}˜M:=(M(κ,σ,ˉτ))˜M, (3.17)

    where, M(κ,σ,τ)=2λ2exp(2θ(Δˉτ))+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)1. If κ=0,σ=0,ˉτ=0, then we have M(0,0,0)=2λ2exp(2θΔ)1<0, and Δ>ln(2λ2)/(2θ). Therefore, if σ=0,τ=0, then

    M(κ,0,0)=2λ2exp(2θΔ)+2(M2+M3)exp(2ΔM1)12M2exp(2ΔM1)1,

    where M1=12Δ(m1+m2)2,  M2=6κ2[1+24Δ2m22(11ζ+112ζ)],  M3=12κ2.

    As 0<κ<(exp(2ΔM1)12[1+24m22Δ2((1ζ)1+(12ζ)1)])12 and dM(k,0,0)dk>0, then M(κ,0,0) is strictly increasing with respect to κ. When κ(exp(2ΔM1)12[1+24m22Δ2((1ζ)1+(12ζ)1)])12, M(κ,0,0)+. Therefore, by the existence theorem for roots, it is known that there exists ˜κ such that M(˜κ,0,0)=0. Using the above method, we can get M(κ,σ,0)=0 and M(κ,σ,ˉτ)=0.

    We can choose ω=ln(M(κ,σ,ˉτ)+1)/Δ, where ω>0, Δ>ln(2λ2)/(2θ). For t0+Δtt0+2Δ, we can obtain the following:

    EQ(t)2exp(ωΔ)Eϕ(t0)2.

    Therefore, for any positvite integer m=1,2,, when tt0+(m1)Δ,

    Q(t;t0,ϕ(t0))=Q(t;t0+(m1)Δ,Q(t0+(m1)Δ;t0,ϕ(t0))).

    Thus, for tt0+mΔ,

    EQ(t)2=EQ(t;t0+(p1)Δ,Q(t0+(p1)Δ;t0,ϕ(t0)))2exp(ωΔ)EQ(t;t0+(p1)Δ;t0,ϕ(t0)))2=exp(ωΔ)EQ(t;t0+(p2)Δ,Q(t0+(p2)Δ;t0,ϕ(t0))2      exp(pωΔ)Eϕ(t0)2.

    Therefore, when t>t0+Δ, we have EQ(t)2exp(ω(tt0))exp(ωΔ)Eϕ(t0)2. Obviously, the above formula also holds when t0tt0+Δ. Therefore, FCNNs (2.3) is ASGES.

    Remark 2. Theorem 1 displays that when system (2.2) is GES, the perturbed system (2.3) can be MSGES; it is also ASGES if the bounds on the neutral terms, the stochastic disturbances, and the time delays are less than the upper bound of the estimation.

    Example 1. We consider the following FCNNs model:

    {d[Q1(t)ksinQ1(tτ(t))]=[a1Q1(t)+2j=1b1jfj(Qj(t))+2j=1c1jfj(Qj(tτ(t)))+2j=1d1jfj(Qj(t)τ(t))+2j=1e1jfj(Qj(tτ(t)))]dt+2j=1σ1jQj(t)dB(t),d[Q2(t)ksinQ2(tτ(t))]=[a2Q2(t)+2j=1b2jfj(Qj(t))+2j=1c2jfj(Qj(tτ(t)))+2j=1d2jfj(Qj(t)τ(t))+2j=1e2jfj(Qj(tτ(t)))]dt+2j=1σ2jQj(t)dB(t), (4.1)

    where, a=(aij)2×2=[1001],    b=(bij)2×2=[0.020.010.010.02],

    c=(cij)2×2=[0.010.020.020.01],   d=(dij)2×2=[0.020.010.010.02],   and   e=(eij)2×2=[0.010.020.020.01].

    Without any disturbance, (4.1) becomes the following:

    {dQ1(t)=[a1Q1(t)+2j=1b1jfj(Qj(t))+2j=1c1jfj(Qj(t))+2j=1d1jfj(Qj(t))+2j=1e1jfj(Qj(t)]dt,dQ2(t)=[a2Q2(t)+2j=1b2jfj(Qj(t))+2j=1c2jfj(Qj(t))+2j=1d2jfj(Qj(t))+2j=1e2jfj(Qj(t))]dt. (4.2)

    Based on the principle of comparison, FCNNs (4.2) is GES when λ=1,θ=1.6. When we select Δ=0.3 and fj()=tanh(), then |fj(u)fj(v)||uv| holds, so L and l are set as 1. Therefore, if we let ζ=0, we can obtain m1=1.03 and m2=0.09. From Theorem 1, the following three equations can be obtained:

    2exp(0.96)+37.3992κ2exp(2.7095)113.3992κ2exp(2.7095)=1,

    and

    2exp(0.96)+(37.3992˜κ2+3.75σ2)exp(2.7095+6σ2)113.3992˜κ2exp(2.7095+6σ2)=1,

    and

    2exp(0.96+3.2ˉτ)+2(24.499˜k2+1.875ˉσ2+3ˉτ(0.0388+0.1746˜κ2+0.128ˉσ2+0.0389ˉτ+0.0005ˉτ2))exp(3.6(0.7526+1.0292ˉσ2ˉτ+0.0623ˉτ2))/124.8398˜κ2exp(3.6(0.7526+1.0292ˉσ2ˉτ+0.0623ˉτ2))=1.

    Thus, we can obtain ˜κ=0.0175, ˉσ=0.0639, and ˉτ=0.0261. From Theorem 1, the perturbed FCNNs (4.1) is said to be MSGES if the coefficient of neutrality κ, the random interferences σ, and the time delays τ(t) are lower than the thresholds we deduced above, where, κ˜κ, σˉσ and τ(t)min{ˉτ,Δ/2}.

    Remark 3. Figure 1 illustrates the state of FCNNs (4.1) at different initial values, where κ=0.015, σ=0.06, and τ=0.025. Since the neutrality coefficients, stochastic disturbance intensities, and time delays are all less than the derived bounds, the FCNNs (4.1) can be regarded as MSGES and ASGES.

    Figure 1.  States of (4.1) with k=0.015,σ=0.06,τ(t)=0.025.

    Remark 4. Figures show that the cases one of the neutrality coefficient, stochastic disturbance intensity, and time delay exceeds the bounds, respectively. In Figure 2, the neutrality coefficient κ=0.03 exceeds the given bounds, thus making it unstable. In Figure 3, the stochastic disturbance intensity σ=0.15 clearly exceeds the given bounds; therefore, it is also unstable. In Figure 4, the time delay τ(t)=0.04, clearly exceeds the threshold; therefore, it is not stable. The parameters of Figures 14 are listed in Table 1.

    Figure 2.  States of (4.1) with k=0.05,σ=0.06,τ(t)=0.025.
    Figure 3.  States of (4.1) with k=0.015,σ=0.15,τ(t)=0.025.
    Figure 4.  States of (4.1) with k=0.015,σ=0.06,τ(t)=0.04.
    Table 1.  Parameters of Figures 14.
    κ σ τ(t)
    Figure 1 0.015 0.06 0.025
    Figure 2 0.05 0.06 0.025
    Figure 3 0.015 0.15 0.025
    Figure 4 0.015 0.06 0.04

     | Show Table
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    In this paper, we explored the problem of the robustness analysis of the global exponential stability of FCNNs with the combined interference of three factors, namely neutral items, stochastic disturbances, and time delays. By constructing and solving the transcendental equations relevant to neutral items, random disturbances, and time delays, the upper bound thresholds for each of these disturbances were determined. These thresholds ensure that the initially stable fuzzy system continues to be stable when the perturbation intensity to which the perturbed system is subjected does not exceed these limits. Finally, we used a simulation example to verify the correctness of the derived results, thus enriching the theoretical research system of the FCNNs stabilization problem under multi-factor perturbations. In the future, we will further discuss the effects of other factors on fuzzy neural networks with neutral terms.

    Yunlong Ma: Conceptualization, methodology, software, validation, formal analysis, writing—original draft preparation; Tao Xie: Conceptualization, methodology, validation, writing—review and editing, project administration; Yijia Zhang: Conceptualization, software, formal analysis, investigation. All authors have read and agreed to the published version of the manuscript.

    The authors declare that there are no conflicts of interest regarding the publication of this paper.



    [1] W. E. Faller, S. J. Schreck, Neural networks: Applications and opportunities in aeronautics, Prog. Aerosp. Sci., 32 (1996), 433–456. https://doi.org/10.1016/0376-0421(95)00011-9 doi: 10.1016/0376-0421(95)00011-9
    [2] T. Chen, Fuzzy neural network applications in medicine, In: Proceedings of 1995 IEEE International Conference on Fuzzy Systems, 2 (1995), 627–634. https://doi.org/10.1109/FUZZY.1995.409750
    [3] A. Kumar, P. Mohanty, Autoassociative memory and pattern recognition in micromechanical oscillator network, Sci. Rep., 7 (2017), 411. https://doi.org/10.1038/s41598-017-00442-y doi: 10.1038/s41598-017-00442-y
    [4] Y. Shen, J. Wang, Robustness analysis of global exponential stability of recurrent neural networks in the presence of time delays and random disturbances, IEEE T. Neur. Net. Lear., 23 (2011), 87–96. https://doi.org/10.1109/TNNLS.2011.2178326 doi: 10.1109/TNNLS.2011.2178326
    [5] L. García, P. M. Talaván, J. Yáñez, The 2-opt behavior of the Hopfield Network applied to the TSP, Oper. Res., 22 (2020), 1127–1155. https://doi.org/10.1007/s12351-020-00585-3 doi: 10.1007/s12351-020-00585-3
    [6] L. O. Chua, L. Yang, Cellular neural networks: Theory, IEEE T. Circuits Syst., 35 (1988), 1257–1272. http://dx.doi.org/10.1109/31.7600 doi: 10.1109/31.7600
    [7] L. O. Chua, L. Yang, Cellular neural networks: Applications, IEEE T. Circuits Syst., 35 (1988), 1273–1290. http://dx.doi.org/10.1109/31.7601 doi: 10.1109/31.7601
    [8] L. Wang, T. Dong, M. Ge, Finite-time synchronization of memristor chaotic systems and its application in image encryption, Appl. Math. Comput., 347 (2019), 293–305. https://doi.org/10.1016/j.amc.2018.11.017 doi: 10.1016/j.amc.2018.11.017
    [9] R. Matei, New model and applications of cellular neural networks in image processing, 2009. https://doi.org/10.5772/8223
    [10] T. Yang, L. Yang, C. Wu, L. O. Chua, Fuzzy cellular neural networks: Theory, In: 1996 Fourth IEEE International Workshop on Cellular Neural Networks and their Applications Proceedings (CNNA-96), 1996,181–186. http://dx.doi.org/10.1109/cnna.1996.566545
    [11] T. Yang, L. Yang, The global stability of fuzzy cellular neural network, IEEE T. Circuits-I, 43 (1996), 880–883. http://dx.doi.org/10.1109/81.538999 doi: 10.1109/81.538999
    [12] P. Mani, R. Rajan, L. Shanmugam, Y. H. Joo, Adaptive control for fractional order induced chaotic fuzzy cellular neural networks and its application to image encryption, Inform. Sciences, 491 (2019), 74–89. https://doi.org/10.1016/j.ins.2019.04.007 doi: 10.1016/j.ins.2019.04.007
    [13] K. Ratnavelu, M. Kalpana, P. Balasubramaniam, K. Wong, P. Raveendran, Image encryption method based on chaotic fuzzy cellular neural networks, Signal Process., 140 (2017), 87–96. https://doi.org/10.1016/j.sigpro.2017.05.002 doi: 10.1016/j.sigpro.2017.05.002
    [14] S. Long, D. Xu, Stability analysis of stochastic fuzzy cellular neural networks with time-varying delays, Neurocomputing, 74 (2011), 2385–2391. https://doi.org/10.1016/j.neucom.2011.03.017 doi: 10.1016/j.neucom.2011.03.017
    [15] Q. Zhang, H. Yang, Z. Xin, Uniform stability of stochastic fractional-order fuzzy cellular neural networks with delay, Int. J. Knowl.-Based In., 21 (2017), 1–14. https://doi.org/10.3233/KES-160336 doi: 10.3233/KES-160336
    [16] L. Chen, H. Zhao, Stability analysis of stochastic fuzzy cellular neural networks with delays, Neurocomputing, 72 (2008), 436–444. https://doi.org/10.1016/j.neucom.2007.12.005 doi: 10.1016/j.neucom.2007.12.005
    [17] X. Yao, X. Liu, S. Zhong, Exponential stability and synchronization of memristor-based fractional-order fuzzy cellular neural networks with multiple delays, Neurocomputing, 419 (2021), 239–250. https://doi.org/10.1016/j.neucom.2020.08.057 doi: 10.1016/j.neucom.2020.08.057
    [18] F. Du, J. Lu, Finite-time stability of fractional-order fuzzy cellular neural networks with time delays, Fuzzy Set. Syst., 438 (2021), 107–120. https://doi.org/10.1016/j.fss.2021.08.01 doi: 10.1016/j.fss.2021.08.01
    [19] R. Tang, X. Yang, P. Shi, Z. Xiang, L. Qing, Finite-time stabilization of uncertain delayed T–S fuzzy systems via intermittent control, IEEE T. Fuzzy Syst., 32 (2024), 116–125. https://doi.org/10.1109/TFUZZ.2023.3292233 doi: 10.1109/TFUZZ.2023.3292233
    [20] S. Zhu, Y. Shen, Robustness analysis of global exponential stability of neural networks with Markovian switching in the presence of time-varying delays or noises, Neural Comput. Appl., 23 (2013), 1563–1571. https://doi.org/10.1007/s00521-012-1105-0 doi: 10.1007/s00521-012-1105-0
    [21] Q. Yang, S. Zhu, W. Luo, Noise expresses exponential decay for globally exponentially stable nonlinear time delay systems, J. Franklin I., 353 (2016), 2074–2086. https://doi.org/10.1016/j.jfranklin.2016.03.013 doi: 10.1016/j.jfranklin.2016.03.013
    [22] Y. Shen, J. Wang, Robustness of global exponential stability of nonlinear systems with random disturbances and time delays, IEEE T. Syst. Man Cy.-S., 46 (2015), 1157–1166. https://doi.org/10.1109/TSMC.2015.2497208 doi: 10.1109/TSMC.2015.2497208
    [23] F. Jiang, H. Yang, Y. Shen, On the robustness of global exponential stability for hybrid neural networks with noise and delay perturbations, Neural Comput. Appl., 24 (2014), 1497–1504. https://doi.org/10.1007/s00521-013-1374-2 doi: 10.1007/s00521-013-1374-2
    [24] Y. Zou, E. Tian, H. Chen, Finite-time synchronization of neutral-type coupled systems via event-triggered control with controller failure, IEEE T. Control Netw., 11 (2024), 1214–1224. https://doi.org/10.1109/TCNS.2023.3336594 doi: 10.1109/TCNS.2023.3336594
    [25] Z. Zhou, Z. Zhang, M. Chen, Finite-time synchronization for fuzzy delayed neutral-type inertial BAM neural networks via the figure analysis approach, Int. J. Fuzzy Syst., 24 (2022), 1–18. https://doi.org/10.1007/s40815-021-01132-8 doi: 10.1007/s40815-021-01132-8
    [26] Y. Shen, J. Wang, Robustness analysis of global exponential stability of non-linear systems with time delays and neutral terms, IET Control Theory A., 7 (2013), 1127–1232. https://doi.org/10.1049/iet-cta.2012.0781 doi: 10.1049/iet-cta.2012.0781
    [27] W. Si, S. Gao, H. Dong, Ternary implicit criterion for robust exponential stability of perturbed stochastic BAM systems, IEEE T. Circuits II, 70 (2023), 3119–3123. https://doi.org/10.1109/TCSII.2023.3249181 doi: 10.1109/TCSII.2023.3249181
    [28] W. Si, S. Gao, W. Tian, Robust global exponential stability of fuzzy neural networks with bis-disturbances, 2023 China Automation Congress (CAC), 2023, 9103–9107. https://doi.org/10.1109/CAC59555.2023.10452099
    [29] W. Si, T. Xie, B. Li, Exploration on robustness of exponentially global stability of recurrent neural networks with neutral terms and generalized piecewise constant arguments, Discrete Dyn. Nat. Soc., 2021 (2021), 9941881. https://doi.org/10.1155/2021/9941881 doi: 10.1155/2021/9941881
    [30] W. Fang, T. Xie, B. Li, Robustness analysis of fuzzy cellular neural network with deviating argument and stochastic disturbances, IEEE Access, 11 (2023), 3717–3728. https://doi.org/10.1109/ACCESS.2023.3233946 doi: 10.1109/ACCESS.2023.3233946
    [31] X. Mao, Stochastic differential equations and applications, 2Eds., UK: Woodhead Publishing, 2008.
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