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Research article Special Issues

Event-triggered fixed/preassigned time stabilization of state-dependent switching neural networks with mixed time delays

  • Received: 14 January 2024 Revised: 23 February 2024 Accepted: 28 February 2024 Published: 06 March 2024
  • MSC : 34H15, 34K34

  • This study employed an event-triggered control (ETC) strategy to investigate the problems of fixed-time stabilization (FTS) and preassigned-time stabilization (PTS) for state-dependent switching neural networks (SDSNNs) that involved mixed time delays. To enhance the network's generalization capability and accelerate convergence stabilization, a more intricate weight-switching mechanism was introduced, then to mitigate transmission energy consumption, this paper proposed a tailored event-triggering rule that triggered the ETC solely at predetermined time points. This rule ensured the stability of the system while effectively reducing energy consumption. Using the Lyapunov stability theory and various inequality techniques, this paper presented new results for FTS and PTS of SDSNNs. The validity of these findings was supported by conducting data simulations in two illustrative examples.

    Citation: Jiashu Gao, Jing Han, Guodong Zhang. Event-triggered fixed/preassigned time stabilization of state-dependent switching neural networks with mixed time delays[J]. AIMS Mathematics, 2024, 9(4): 9211-9231. doi: 10.3934/math.2024449

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  • This study employed an event-triggered control (ETC) strategy to investigate the problems of fixed-time stabilization (FTS) and preassigned-time stabilization (PTS) for state-dependent switching neural networks (SDSNNs) that involved mixed time delays. To enhance the network's generalization capability and accelerate convergence stabilization, a more intricate weight-switching mechanism was introduced, then to mitigate transmission energy consumption, this paper proposed a tailored event-triggering rule that triggered the ETC solely at predetermined time points. This rule ensured the stability of the system while effectively reducing energy consumption. Using the Lyapunov stability theory and various inequality techniques, this paper presented new results for FTS and PTS of SDSNNs. The validity of these findings was supported by conducting data simulations in two illustrative examples.



    Based on research in modern neuroscience [1], neural networks have gained attention due to their ability to simulate the structural characteristics of the human brain. After being activated by external stimuli, the synaptic connection weights of neurons can be adjusted to facilitate information transmission between neurons; therefore, a large number of circuit components are constructed to support this transmission. When facing practical applications that require processing large-scale datasets, the complex computations and the transmission of a vast amount of data result in catastrophic power consumption and storage usage.

    Memristors [2,3], due to their non-volatility and the ability to continuously change their resistance states, can effectively exhibit the plasticity of neural synapses. They are gradually replacing traditional resistors in the design of artificial neural networks and have been widely applied in simulating the human brain [4]. In the research, memristors are utilized as state switching elements to achieve internal state switching in neural networks by adjusting the resistance values of memristors. As a result, the state-dependent switching neural networks (SDSNNs) were constructed [5]. A state switching system is typically composed of transition rules between several discrete states through which the system's behavior and evolution are described. In neural networks, this switching mode exhibits significant advantages in processing dynamic data and reducing the high power consumption and storage caused by signal transmission. Consequently, they have found widespread applications in diverse fields, including speech recognition [6], intelligent control [7], and fault diagnosis [8].

    Undoubtedly, the significance of stability in nonlinear systems [9,10,11,12,13] is widely recognized. Compared to the conventional notion of asymptotic stability, finite-time stability possesses superior performance advantages, which has attracted extensive research attention from many researchers. The relevant finite-time stability results of SDSNNs have been presented in [14,15,16]. However, due to the dependency of finite-time stability on initial conditions, the precise acquisition of initial conditions remains a major challenge in practical applications. Therefore, considering this limitation, we introduce the concept of fixed-time stability (FTS) to address this issue [17].

    In FTS, the settling-time is dictated by designing the control strategy and parameters, and is independent of the initial conditions. The system must converge to a stable state within a fixed time. Under its own strict and robust stability requirements, FTS has significant application value for control problems that demand high precision and response speed, such as aerospace engineering, robot control, and intelligent transportation. The research on FTS has attracted increasing attention and has become a vital research area in contemporary control theory and applications [18,19,20,21,22].

    Nonetheless, FTS sets time as a parameter or hyperparameter in the model, which restricts its capability to flexibly learn the relationship between time and other features. To address this limitation, our study proposes the concept of preassigned-time stabilization (PTS), whereby time is considered an input feature alongside other features provided to the neural network model; thus, time is no longer considered as a static, immutable parameter but rather as a dynamic factor that allows for future data prediction. PTS necessitates swift convergence the system to a stable state within a predefined time, indicating that the control system can achieve fast stabilization at any moment and exhibits stronger robustness against external disturbances and parameter fluctuations; therefore, PTS offers more stringent performance guarantees. PTS has been employed in numerous studies on stabilization and synchronization, showcasing encouraging outcomes [23,24]. When confronted with requirements for real-time performance and safety, PTS can present an effective method and guide principles for devising more efficient, rapid, and precise control systems.

    Traditional control methods rely on continuous control inputs to ensure system performance, which requires a significant amount of communication resources to transmit control signals. In contrast, event-triggered control (ETC) only triggers sampling and control actions when specific events occur by monitoring changes in system states or errors. By designing event-triggering rules appropriately, it is possible to flexibly meet the practical control requirements.

    With the increasing attention to ETC, numerous researchers have made significant achievements around event triggering strategies [5,20,21,25,26,27,28,29]. Among these studies, event-triggering strategies have been successfully applied to neural networks with state switches in [5,21,25,26,27,28,29]. In 2022, Li et al. [30] introduced a more concise lemma for demonstrating the FTS of systems. In 2022, Li et al. [24] examined the fixed and preassigned-time stabilization of SDSNNs incorporating time delays. In 2023, Zhang [20] developed a novel and effective ETC technique for achieving fixed-time synchronization and stabilization. Based on the above discussions, the objective of this paper is to tackle the fixed/preassigned-time stabilization problem of neural networks with mixed delays in state switches through ETC. The innovations of this paper are summarized as follows:

    1) Differing from the models in [23,28,29] that employ simple switch of connection weights, the model proposed in this paper adopts a more complex switching mechanism in the form of differentiable switches. Results obtained under this switching mode are more generalizable and enable the network to exhibit superior performance when handling unknown data.

    2) Despite the extensive results presented in [5,14,15,18,19,20,25,31] on the traditional asymptotic stability, finite-time or fixed-time stabilization of switched systems, there has been no such study for the model in this paper. This paper discusses fixed/preassigned-time stabilization, filling this research gap and enriching the results for achieving stabilization, thereby enhancing the efficiency and precision of the system.

    3) Compared to [32], which only employs mixed delays, this paper proposes an ETC strategy based on mixed delays. This strategy eliminates the need for the system to remain in a control state at all times, thus effectively saving communication resources. The proposed control strategy is more widely applicable and can be easily extended to higher-order, complex-valued, and quaternion-valued domains.

    The remaining parts have the following structures: Section 2 covers the preliminaries. In Section 3, the main results of this paper about FTS and PTS are disclosed. Simulations and comparisons are displayed in Section 4. Finally, some conclusions are given in Section 5.

    Notation: In this paper, the solutions of all systems are considered in Filippov's sense [33]. co[δ,δ] denotes the convex hull of {δ,δ}.

    ¯ȷs=max{ȷs,ȷs},ȷ_s=min{ȷs,ȷs},¯asz=max{asz,asz},a_sz=min{asz,asz},
    ¯bsz=max{bsz,bsz},b_sz=min{bsz,bsz},amaxsz=max{|a_sz|,|¯asz|},bmaxsz=max{|b_sz|,|¯bsz|},
    cmaxsz=max{|c_sz|,|¯csz|},cminsz=min{|c_sz|,|¯csz|},  s,zW={1,2,,}.

    The SDSNNs with mixed delays are

    dχs(t)dt=ȷs(χs(t))χs(t)+z=1asz(χs(t))z(χz(t))+z=1bsz(χs(t))z(χz(tτz(t)))+z=1csz(χs(t))ttrz(t)z(χz(υ))dυ,t0,sW, (1)

    with the initial values as

    χ(υ)=(χ1(υ),χ2(υ),,χ(υ))TC([h,0],R),

    in which

    h=max{τ,r},χ(t)=(χ1(t),,χ(t))TRn

    is state variable, ȷs(χs(t)) is self-feedback weight, asz(χs(t)),bsz(χs(t)),csz(χs(t)) are memristor-based weights, fs() is a nonlinear activation function, τz() is discrete time-varying delays, where τz()<τz, τz is a constant, and rz() is distributed time-varying delays, 0rz(t)rz, ˙rz(t)h, in which τz,h<1 are constants above s,zW.

    Based on the previous work [34], it is expected that the state-dependent parameters in (1) fulfill the following conditions:

    ȷs(χs(t))={ȷs,ds(χs(t))dtdχs(t)dt,ȷs,ds(χs(t))dt>dχs(t)dt,asz(χs(t))={asz,ϱszdz(χz(t))dtdχs(t)dt,asz,ϱszdz(χz(t))dt>dχs(t)dt,bsz(χs(t))={bsz,ϱszdz(χz(tτz(t)))dtdχs(t)dt,bsz,ϱszdz(χz(tτz(t)))dt>dχs(t)dt,csz(χs(t))={csz,ϱsz{z(χz(t))z(χz(trz(t)))}dχs(t)dt,csz,ϱsz{z(χz(t))z(χz(trz(t)))}>dχs(t)dt, (2)

    where ȷs,ȷs,asz,asz,bsz,bsz,csz,csz are constant numbers, s,zW={1,2,,}, and ϱsz=1, if sz holds; otherwise, -1.

    To achieve FTS and PTS of system (3), we consider the following stabilization system:

    dχs(t)dt=ȷs(χs(t))χs(t)+z=1asz(χs(t))z(χz(t))+z=1bsz(χs(t))z(χz(tτz(t)))+z=1csz(χs(t))ttrz(t)z(χz(υ))dυ+us(t),t0,sW. (3)

    Remark 1. The switching condition for defining parameters ȷs(χs(t)),asz(χs(t)),bsz(χs(t)),csz(χs(t)) is determined by the state of the neurons, and us(t) is the controller.

    By utilizing the theory of differential inclusion [33] and set-valued mapping, we know that

    dχs(t)dtco[ȷs(χs(t))]χs(t)+z=1co[asz(χs(t))]z(χz(t))+z=1co[bsz(χs(t))]z(χz(tτz(t))+z=1co[csz(χs(t)]ttrz(t)z(χz(υ))dυ+co[us(t)],fora.e.t0,sW, (4)

    where

    co[ȷs(χs(t))]={ȷs,ds(χs(t))dtdχs(t)dt,[ȷ_s,¯ȷs],ds(χs(t))dt=dχs(t)dt,ȷs,ds(χs(t))dt>dχs(t)dt,co[asz(χs(t))]={asz,ϱszdz(χz(t))dtdχs(t)dt,[a_sz,¯asz],ϱszdz(χz(t))dt=dχs(t)dt,asz,ϱszdz(χz(t))dt>dχs(t)dt,co[bsz(χs(t))]={bsz,ϱszdz(χz(tτz(t)))dtdχs(t)dt,[b_sz,¯bsz],ϱszdz(χz(tτz(t)))dt=dχs(t)dt,bsz,ϱszdz(χz(tτz(t)))dt>dχs(t)dt,co[csz(χs(t))]={csz,ϱsz{z(χz(t))z(χz(trz(t)))}dχs(t)dt,[c_sz,¯csz],ϱsz{z(χz(t))z(χz(trz(t)))}=dχs(t)dt,csz,ϱsz{z(χz(t))z(χz(trz(t)))}>dχs(t)dt. (5)

    By using measurable selection theory [33], we know that there exist

    ȷs(t)co[ȷsz(χs(t))],asz(t)co[asz(χs(t))],bsz(t)co[bsz(χs(t))],csz(t)co[csz(χs(t))]

    and

    ˘us(t)co[us(t)],

    such that

    dχs(t)dt=ȷs(t)χs(t)+z=1asz(t)z(χz(t))+z=1bsz(t)z(χz(tτz(t))+z=1csz(t)ttrz(t)z(χz(υ))dυ+˘us(t),fora.e.t0,sW. (6)

    Assumption 1. The feedback function z(), z=1,2,, is bounded, there exists a number M such that |z()|M, and it satisfies the condition z(0)=0.

    Definition 1. [28] For any χ0=χ(0)Rn, let

    T(χ0)={t:χ(t)=0,t>t}

    be the settling time function. If there exists a constant Tmax>0, such that T(χ(0))Tmax for any χ(0)Rn, and if

    limtTmaxχ(υ)=0

    holds, then the system (3) is called FTS and Tmax is called setting-time.

    Definition 2. [35] If there exists a preassigned constant Tp>0, such that the function T(χ(0))Tp for any χ(0)Rn, and if

    limtTpχ(υ)=0

    holds, then the system (3) is called PTS and Tp is called preassigned-time.

    For deriving the main results, the following lemmas are needed.

    Lemma 1. [36] Let πs0,(s=1,2,,),0<p11, and p21; one has

    s=1πp1s(s=1πs)p1,s=1πp2s1p2(s=1πs)p2.

    Lemma 2. [30,37] There exists a continuous, positive-definite, and radically unbounded function

    V(y(t)):RnR,y(t)=0V(y(t))=0,

    such that any solution y(t) of system (6) satisfies the inequality

    dV(y(t))dt{ζV(y(t))1Vω(y(t)),ifV(y(t))(0,1),ζV(y(t))2Vω(y(t)),ifV(y(t))1,

    where

    ζ>0,1>0,2>0,ζ<min{1,2},ω=λ+sign(V(y(t))1),1<λ<2.

    The settling-time of FTS is

    Tmax=1ζ(λ2)ln11+ζ1λζln22+ζ.

    Lemma 3. If there exists a continuous, positive-definite, and radically unbounded function

    V(y(t)):RnR,y(t)=0V(y(t))=0,

    such that any solution y(t) of system (6) satisfies the inequality

    dV(y(t))dtTmaxTp(ζV(y(t))Vω(y(t))),

    then the origin of SDSNNs (3) is PTS within setting-time Tmax and preassigned-time Tp, in which

    Tmax=1ζ(λ2)ln+ζ1λζln+ζ,

    where other parameters are the same as in Lemma 2.

    Remark 2. Based on the FTS lemma provided in [30], this paper establishes Lemma 2 while ensuring the condition -ζ<0 in the inequality

    dV(y(t))dtζV(y(t))Vω(y(t)).

    Building upon this lemma, the paper extends its findings and introduces a new PTS lemma, namely Lemma 3.

    Remark 3. Many previous studies have focused on FTS [18,19,20,21,22,23,24], with some PTS results provided in the researches [23,24,35]. However, these systems often do not involve state switching, and the controllers do not utilize ETC. In comparison to the main systems incorporating state switching [4,14,15,18,19], this paper optimizes the model's state switching by employing derivative-enhanced complex switching, resulting in more general outcomes. Additionally, an ETC strategy is implemented to reduce power consumption. For the model in this paper, FTS and PTS results have not been studied yet, therefore, this paper will supplement the following content.

    Let controller ˘us(t),sW in system (6) be

    ˘u1s(t)=ρsχs(tι)σs[χ2s(tι)]ω1χs(tι)κsϕs(tι),t[tι,tι+1),ι=1,2,, (7)

    in which ρs,σs,κs are all positive constants,

    ω=λ+sign(V(t)1)

    for t[tι,tι+1), 1<λ<2,

    ϕs(t)co[(sign(χs(t))]

    and

    V(t)=s=1χ2s(t).

    Let

    ˘U1s(t)=ρsχs(t)σs[χ2s(t)]ω1χs(t)κsϕs(t).

    The measure error is

    E1s(t)=˘U1s(t)˘u1s(t)

    and event-triggering is

    tι+1={t|t>tι,|E1s(t)|ςs|χs(t)|+αsσs|χ2ω1s(t)|+γs(1ϑs)t}, (8)

    where αs,ϑs(0,1),ςs,γs>0, and tι (ι=0,1,2,,sN) is the ι th triggering instant.

    Let

    κsz=1amaxszM+z=1bmaxszM+z=1cmaxszMrz+γs, (9)
    ζs=2(ȷmins+ρsςs),sW. (10)

    The main results of this subsection are presented as follows.

    Theorem 1. Under Assumption 1, Lemma 2, and ETC (7) and (8), if (9) and ζs>0 (sW) hold, SDSNNs (3) get FTS and the settling-time is Tmax.

    Proof. Now, we construct a Lyapunov functional:

    V(t)=s=1χ2s(t). (11)

    For t[tι,tι+1),ι=1,2,, by using the properties of C-regular functions [38] and taking the derivative of V(t) with respect to any solutions of (6), we obtain

    dV(t)dt=2s=1χs(t)dχs(t)dt=2s=1χs(t)[ȷs(t)χs(t)+z=1asz(t)z(χz(t))+z=1bsz(t)z(χz(tτz(t))+z=1csz(t)ttrz(t)z(χz(υ))dυ+˘u1s(t)]2s=1[ȷs(t)χ2s(t)+z=1asz(t)|χs(t)||z(χz(t))|+z=1bsz(t)|χs(t)||z(χz(tτz(t))|+z=1csz(t)|χs(t)|ttrz(t)|z(χz(υ))|dυ+˘u1s(t)χs(t)]. (12)

    From (7) and (12), one obtains

    dV(t)dt2s=1[ȷminsχ2s(t)+z=1amaxszM|χs(t)|+z=1bmaxszM|χs(t)|+z=1cmaxszrzM|χs(t)|+ϕs(t)χs(t)(˘U1s(t)E1s(t))]2s=1(ȷminsρs+ςs)χ2s(t)+2s=1|χs(t)|[z=1amaxszM+z=1bmaxszM+z=1cmaxszrzMκs+γs]2s=1[χ2s(t)]ω(σsαsσs)+2s=1|χs(t)|[|E1s(t)|ςs|χs(t)|αsσs|χ2ω1s(t)|γs(1ϑs)t]. (13)

    By using conditions (8)–(10), one knows that

    dV(t)dts=1(ζsχ2s(t)2(1αs)σs[χ2s(t)]ω). (14)

    Utilizing Lemma 1 in [36], one can derive

    (1) If V(t)(0,1),

    s=12(1αs)σs[χ2s(t)]ω1s=1[χ2s(t)]ω=1Vω(t), (15)

    in which

    1=minsW{2(1αs)σs}.

    (2) If V(t)1,

    s=12(1αs)σs[χ2s(t)]ω2s=1[χ2s(t)]ω=2Vω(t), (16)

    where 2=1λ. From (13)–(16), one obtains

    dV(y(t))dt{ζV(y(t))1Vω(y(t)),ifV(y(t))(0,1),ζV(y(t))2Vω(y(t)),ifV(y(t))1, (17)

    where

    ζ=minsW{ζs},ζ<min{1,2}.

    From Definition 1 and Lemma 2, we get SDSNNs (3) to achieve FTS at the settling-time Tmax. The proof is finished.

    Theorem 2. The system (6) does not have Zeno-behavior with ETC (7) and (8).

    Proof. When t[tι,tι+1),ι=1,2,,

    d|E1s(t)|dtd|U1s(t)|dt[ρs+(2ω1)σsχ2ω2s(t)]|dχs(t)dt|. (18)

    From systems (6), one has

    dχs(t)dtȷmins|χs(t)|+s=1amaxszM+s=1bmaxszM+s=1cmaxszσzM+|˘u1s(t)|. (19)

    Due to

    dV(t)dt<0,

    thus,

    |χs(t)|V(0),

    then

    dχs(t)dtȷminsV(0)+s=1amaxszM+s=1bmaxszM+s=1cmaxszσzM+|˘u1s(t)|=ϝs(tι)>0. (20)

    Let

    Ψs=maxt[tι,tι+1)[ρs+(2ω1)σsχ2ω2s(t)],

    and by using (17), one gets

    d|E1s(t)|dtΨsϝs(tι). (21)

    Because |E1s(tι)|=0, then

    |E1s(t)|ttιΨsϝs(tι)ds=Ψsϝs(tι)(ttι). (22)

    From ETC (8), one derives

    |E1s(tι+1)|ςs|χs(tι+1)|+αsσs|χ2ω1s(tι+1)|+γs(1ϑs)tι+1γs(1ϑs)tι+1>0. (23)

    From (22) and (23), one has

    tι+1tιγs(1ϑs)tι+1Ψsϝs(tι)>0. (24)

    The proof is finished.

    The subsequent discussion is the exceptional case of the FTS model for system (3) under rz(t)=0.

    If rz(t)=0, s(0)=0, and (1) appears to have prolonged oscillation or chaotic behaviors, the stabilization model on SDSNNs (3) is

    dχs(t)dt=ȷs(χs(t))χs(t)+z=1asz(χs(t))z(χz(t))+z=1bsz(χs(t))z(χz(tτz(t)))+U1s(t),t0,sW, (25)

    in which U1s(t) (sW) is

    U1s(t)=~ρsχs(tι)~σs[χ2(tι)]˜ω1χs(tι)~κsϕs(tι),t[tι,tι+1),ι=1,2,, (26)

    where ~ρs,~σs,~κs are all positive constants,

    ˜ω=˜λ+sign(V(t)1),1<˜λ<2.

    For t[tι,tι+1), let

    U1s(t)=~ρsχs(t)~σs[χ2(t)]˜ω1χs(t)~κsϕs(t).

    The measure error is

    E1s(t)=U1s(t)U1s(t),

    and event-triggering is

    tι+1={t|t>tι,|E1s(t)|~ςs|χs(t)|+~αs~σs|χ2˜ω1s(t)|+~γs(1~ϑs)t}, (27)

    where ˜αs,˜ϑs(0,1),˜ςs,˜γs>0, and tι (ι=0,1,2,,sN) is the ι th triggering instant.

    Let

    ˜κsz=1amaxszM+z=1bmaxszM+˜γs. (28)
    ˜ζs=2(ȷmins+˜ρs˜ςs),sW.

    The following Corollary 1 of Theorem 1 can be derived from above.

    Corollary 1. Under Assumption 1, Lemma 2, ETC (26) and (27), if (28) and ˜ζs>0,rz(t)=0 (s,zW) hold, then SDSNNs (3) achieve FTS, and the settling-time is Tmax.

    In this part, we build some results on PTS about SDSNNs (3) first, then the following controller is proposed:

    ˘u2s(t)=[TmaxTp(ρs+ηs)ηs]χs(tι)[TmaxTp(σsαsσs)+αsσs][χ2s(tι)]ω1χs(tι)κsϕs(tι),t[tι,tι+1),ι=1,2,. (29)

    Here, ρs,σs,κs are all positive constants,

    ω=λ+sign(V(t)1)

    for t[tι,tι+1), 1<λ<2 and ηs=ȷminsςs, Tp is preassigned-time and Tmax is defined in Theorem 2.

    Let

    ˘U2s(t)=[TmaxTp(ρs+ηs)ηs]χs(t)[TmaxTp(σsαsσs)+αsσs][χ2s(t)]ω1χs(t)κsϕs(t). (30)

    The measure error is

    E2s(t)=˘U2s(t)˘u2s(t).

    The event-triggering is

    tι+1={t|t>tι,|E2s(t)|ςs|χs(t)|+αsσs|χ2ω1s(t)|+γs(1ϑs)t}, (31)

    where αs,ϑs(0,1),ςs,γs>0, and tι (ι=0,1,2,,sN) is the ιth triggering instant.

    Let

    κsz=1amaxszM+z=1bmaxszM+z=1cmaxszMrz+γs, (32)
    ηs=ȷminsςs, (33)
    ζs=2(ȷmins+ρsςs),sW, (34)

    The main results of this subsection are presented as follows.

    Remark 4. Differing from studies on asymptotic stability in [5,25,31] and finite-time stability in [14,15,27,28], the fixed/preassigned-time stability performance ensures that the settling time is independent of initial conditions. In [18,19,21,22,23,24,30,35], the control methods commonly used are feedback control, requiring continuous system control. However, the ETC strategy adopted in this paper, ETC (7), (8), (30) and (31), can reduce the frequency of control operations, thereby decreasing system energy consumption.

    Theorem 3. Under Assumption 1, Lemma 3, and ETC (30) and (31), if (32), (33), and ζs>0 (sW) hold, SDSNNs (3) get PTS, the settling-time is Tmax, and the preassigned-time is Tp.

    Proof. Introduce a Lyapunov function

    V(t)=s=1χ2s(t). (35)

    Similar to the proof of Theorem 1, one has

    dV(t)dt2s=1ȷminsχ2s(t)+2s=1z=1amaxszM|χs(t)|+2s=1z=1bmaxszM|χs(t)|+2s=1z=1cmaxszrzM|χs(t)|+2s=1ϕs(t)χs(t)(˘U2s(t)E2s(t))2s=1ȷminsχ2s(t)+2s=1z=1amaxszM|χs(t)|+2s=1z=1bmaxszM|χs(t)|+2s=1z=1cmaxszrzM|χs(t)|+2s=1ϕs(t)χs(t){[TmaxTp(ρs+ηs)ηs]χs(t)[TmaxTp(σsαsσs)+αsσs][χ2(t)]ω1χs(t)κsϕs(t)}2s=1[ȷminsςsηs+TmaxTp(ρs+ηs)]χ2s(t)+2s=1|χs(t)|[z=1amaxszM+z=1bmaxszM+z=1cmaxszrzMκs+γs]2s=1[χ2s(t)]ω[TmaxTp(σsαsσs)+αsσsαsσs]+2s=1|χs(t)|[|E2s(t)|ςs|χs(t)|αsσs|χ2ω1s(t)|γs(1ϑs)t]z=1TmaxTp{ζsχ2s(t)2(1αs)σs[χ2s(t)]ω}. (36)

    By using conditions (31)–(34), one knows

    dV(t)dts=1TmaxTp{ζsχ2s(t)2(1αs)σs[χ2s(t)]ω}. (37)

    Utilizing Lemma 1 in [36], one can derive:

    (1) If V(t)(0,1),

    s=12(1αs)σs[χ2s(t)]ω1s=1[χ2s(t)]ω=1Vω(t), (38)

    in which

    1=minsW{2(1αs)σs}.

    (2) If V(t)1,

    s=12(1αs)σs[χ2s(t)]ω2s=1[χ2s(t)]ω=2Vω(t), (39)

    where 2=1λ. From (36)–(39), one obtains

    dV(y(t))dtTmaxTp[ζV(y(t))Vω(y(t))], (40)

    where

    =min{1,2},ζ=minsW{ζs},ζ<{1,2}.

    From Definition 2 and Lemma 3, we get SDSNNs (3) to achieve PTS at the preassigned-time Tp. The proof is finished.

    Remark 5. The system (6) can also avoid Zeno-behavior under ETC (30) and (31) and its proof process is the same as Theorem 2.

    The subsequent discussion is the exceptional case of the PTS model for system (3) under rz(t)=0.

    If rz(t)=0, s(0)=0, and (1) appears to have prolonged oscillation or chaotic behaviors, the stabilization model on SDSNNs (3) is

    dχs(t)dt=ȷs(χs(t))χs(t)+z=1asz(χs(t))z(χz(t))+z=1bsz(χs(t))z(χz(tτz(t)))+U2s(t),t0,sW, (41)

    in which U2s(t) (sW) is

    U2s(t)=[TmaxTp(~ρs+~ηs)~ηs]χs(tι)[TmaxTp(~σs~αs~σs)+~αs~σs][χ2(tι)]˜ω1χs(tι)~κsϕs(tι), (42)

    where t[tι,tι+1),ι=1,2,. Here, ~ρs,~σs,~κs are all positive constants,

    ˜ω=˜λ+sign(V(t)1)

    for t[tι,tι+1) and 1<˜λ<2.

    Let

    U2s(t)=[TmaxTp(~ρs+~ηs)~ηs]χs(t)[TmaxTp(~σs~αs~σs)+~αs~σs][χ2(t)]˜ω1χs(t)~κsϕs(t). (43)

    The measure error is

    E2s(t)=U2s(t)U2s(t),

    and event-triggering is

    tι+1={t|t>tι,|E2s(t)|~ςs|χs(t)|+~αs~σs|χ2˜ω1s(t)|+~γs(1~ϑs)t}, (44)

    where ˜αs,˜ϑs(0,1),~ςs,˜γs>0, and tι (ι=0,1,2,,sN) is the ι th triggering instant.

    Let

    ˜κsz=1amaxszM+z=1bmaxszM+˜γs, (45)
    ˜ηs=ȷmins˜ςs, (46)

    and

    ˜ζs=2(ȷmins+˜ρs˜ςs),sW.

    The following Corollary 2 of Theorem 3 can be derived from the above.

    Corollary 2. Under Assumption 1, Lemma 3, and ETC (43) and (44), if (45), (46), ζs>0, and rz(t)=0 (s,zW) hold, SDSNNs (3) achieve PTS and the preassigned-time is Tp.

    Remark 6. In recent years, there have been several studies on finite and FTS with state switching (see [14,15,18,19]). Unfortunately, these studies did not consider PTS results and lacked flexibility in the controllers, leading to higher power consumption for the systems. Additionally, [18,20] only considered systems with time-varying delays and could not adapt to the multiple delays present in some complex systems. This paper optimizes the state switching mechanism, introduces an ETC scheme, and enriches the existing stability results for this model; therefore, the SDSNNs presented in this work exhibit greater flexibility and applicability.

    Remark 7. The control mechanism and state switching mechanism used in this study can be further expanded through the integration with various models, allowing for more complex research. With its performance advantages, they can also be extended to fields such as financial prediction, medical diagnosis, computer vision, etc., thus possessing the ability for broader dissemination and application.

    Now, a numerical simulation example is used to demonstrate the FTS and PTS results separately.

    Consider the following 2-neuron SDSNNs as the FTS system

    dχs(t)dt=ȷs(χs(t))χs(t)+2z=1asz(χs(t))z(χz(t))+2z=1bsz(χs(t))z(χz(tτz(t)))+2z=1csz(χs(t))ttrz(t)z(χz(υ))dυ+˘u1s(t),t0,sW, (47)

    where we take the activation function as

    f1()=f2()=sin(),

    the time-varying delay as

    τz(t)=0.40.1sin(t),

    and the distributed delay as

    rz(t)=0.650.15sin(t),z=1,2.

    The initial conditon of the master system is

    χ1(υ)=2,χ2(υ)=3.5,υ(0.8,0].

    Without ETC, the oscillation state χ1(t),χ2(t) is shown in Figure 1.

    Figure 1.  State trajectory diagram for (47) and (48) without ETC.

    On the basis of satisfying the constraints of parameters in (7) and (8), we randomly select, ρ1=ρ2=27,ς1=28.85,ς2=29,6,γ1=γ2=0.1,α1=α2=0.97,σ1=σ2=4,ϑ1=ϑ2=0.8,λ=1.1, then, by using (9) and (10), we get κ1=16.74,κ2=17.22,ζ=0.1. The values of 1 and 2 obtained from (15) and (16) can be easily calculated to yield 1=0.24,2=0.112.

    According to Lemma 2, Tmax=9.671 is calculated, and Figure 2 demonstrates that the system (47) can reach stability within Tmax.

    Figure 2.  State trajectory of FTS for χ1(t) and χ2(t) under ETC (7) and (8).

    Combining the notation section in the introduction and (2), the master system parameters are specified as follows:

    ȷ1(t)=1.1,ȷ1(t)=1.2,ȷ2(t)=0.21,ȷ2(t)=0.2,
    a11=0.01,a11=0.2,a12=6,a12=5.8,a21=5.8,a21=5.5,a22=2,a22=1,
    b11=3,b11=3,b12=4,b12=4,b21=5.9,b21=5.9,b22=1.5,b22=1.5,
    c11=4.1,c11=3.9,c12=0.2,vc12=0.15,c21=1.1,c21=1.2,c22=1.2,c22=1.19.

    By utilizing Theorem 1 under the conditions of ETC (7) and (8), we randomly selected 30 starting values. χ1(t), χ2(t) of SDSNNs (47) are shown in Figure 2 and they clearly indicate that FTS is achieved independently of the system's initial values, and the 30 control signals corresponding ˘u1s(t) to Figure 2 are shown in Figure 3. The time intervals between events of ETC are shown in Figure 4; therefore, we can observe that the controller only performs control operations when specific events occur, thereby reducing computational and communication overhead. From Figures 14, it can be concluded that the ETC (7) and (8) proposed in this paper are very effective in achieving the FTS in SDSNNs (47).

    Figure 3.  Control signals for stabilizing states χ1(t) and χ2(t) in Figure 2.
    Figure 4.  ETC (7) and (8) transmission time interval.

    Consider a 2-neuron SDSNNs as the PTS system

    dχs(t)dt=ȷs(χs(t))χs(t)+2z=1asz(χs(t))z(χz(t))+2z=1bsz(χs(t))z(χz(tτz(t)))+2z=1csz(χs(t))ttrz(t)z(χz(υ))dυ+˘u2s(t),t0,sW. (48)

    From (48), we keep all other parameters the same as those shown in the above FTS, and additionally set prescribed-time Tp=9<Tmax=9.671, which does not depend on any master system and the initial values. Under the influence of the preassigned-time Tp=9, the master system can achieve PTS by using the controller described in (48).

    By utilizing Theorem 3 under the conditions of ETC (30) and (31), we randomly selected 30 starting values and state χ1(t), χ2(t) of SDSNNs (48), as shown in Figure 5. The 30 control signals corresponding ˘u2s(t) to Figure 5 are shown in Figure 6, and the time intervals between events of ETC are presented in Figure 7. From Figures 1 and 57, it can be concluded that the ETC (30) and (31) proposed in this paper are very effective in achieving the PTS in SDSNNs (48).

    Figure 5.  State trajectory of PTS for χ1(t) and χ2(t) under ETC (30) and (31).
    Figure 6.  Control signals for stabilizing states χ1(t) and χ2(t) in Figure 5.
    Figure 7.  ETC (30) and (31) transmission time interval.

    This paper considered a kind of SDSNNs architecture that incorporates mixed time delays. The state switching mechanism used here is a complex switching with derivatives, which facilitates a faster adjustment of network parameters and speeds up convergence. Furthermore, an ETC strategy is employed to effectively reduce the frequency of control operations, thereby reducing power consumption. The main system achieves FTS and PTS results, allowing the system's settling time to be free from initial condition control and enriching the stability results of this model.

    As we know, the necessity of studying the synchronicity of neural networks lies in gaining a deeper understanding of the coordination and interactions between neurons in the brain, which is crucial for cognitive functions such as information processing, learning, and memory. Additionally, complex numbers and quaternions have significant applications in information processing within neural systems. Therefore, we plan to discuss the synchronization issues of SDSNNs in future works and expand our research to address problems related to complex numbers and quaternions.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work is supported by the National Science Foundation of China under Grant No. 61976228.

    All authors declare no conflicts of interest in this paper.



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