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Research article

Photobiomodulation with low-level laser (λ = 808nm) to treat experimental rheumatoid arthritis: A morphological study, collagen fiber analysis and IL-6 protein expression

  • # These two authors contributed equally to this study.
  • Received: 07 January 2025 Revised: 26 March 2025 Accepted: 10 April 2025 Published: 22 April 2025
  • Rheumatoid arthritis is a chronic systemic autoimmune disease that affects the synovial joints. Low-level laser photobiomodulation (LLLT) has microcirculatory, analgesic, and anti-inflammatory effects. In this paper, the percentage of collagen fibrils and IL-6 protein expression in the synovia were measured to evaluate the effects of photobiomodulation (PBM) with LLLT (λ = 808 nm) on the morphology. Eighteen female Wistar rats were assigned into three groups: Control, Sham, and PBM. To induce arthritis, animals from the Sham and PBM groups received one intraarticular dose of zymosan (200 µg) under anesthesia. Twenty-four hours after induction, an LLLT treatment (λ = 808 nm, 25 mW nominal power, fluence of 20J/cm2, beam area of 0.02 mm2, time of 33 s, total energy of 0.825 J) was applied. Seven days after induction, samples from the animals' knees were subjected to histological and morphometric analyses, and the percentage of collagen fibers in the synovial area (% total area) with and without polarized light and IL-6 protein expression were measured by immunohistochemistry. Statistical analyses were performed an ANOVA and Tukey's post-test with p < 0.05 to compare the experimental groups using. Inflammation of the synovial region showed significant differences between Sham vs. Control, p < 0.0001, and PBM vs. Sham, p < 0.001. The areas of collagen fibers (total percentage) showed differences between Sham vs. Control, p < 0.0001, and Sham vs. PBM, p = 0.0149. IL-6 showed differences between Sham vs. Control and PBM vs. Sham, p < 0.001. Treatment with PBM using LLLT showed decreased synovial inflammation, collagen fiber formation, fibrosis, and IL-6 protein expression, and consequently decreased joint degradation.

    Citation: Luiz Felipe Barreta, Danielly Mandato Oliveira, Bruna Silva Gomes, Sabrina Zanchetta Lanza, Marcelo Augusto Marretto Esquisatto, Gaspar de Jesus Lopes-Filho, Fernando Russo Costa do Bomfim. Photobiomodulation with low-level laser (λ = 808nm) to treat experimental rheumatoid arthritis: A morphological study, collagen fiber analysis and IL-6 protein expression[J]. AIMS Molecular Science, 2025, 12(2): 122-132. doi: 10.3934/molsci.2025008

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  • Rheumatoid arthritis is a chronic systemic autoimmune disease that affects the synovial joints. Low-level laser photobiomodulation (LLLT) has microcirculatory, analgesic, and anti-inflammatory effects. In this paper, the percentage of collagen fibrils and IL-6 protein expression in the synovia were measured to evaluate the effects of photobiomodulation (PBM) with LLLT (λ = 808 nm) on the morphology. Eighteen female Wistar rats were assigned into three groups: Control, Sham, and PBM. To induce arthritis, animals from the Sham and PBM groups received one intraarticular dose of zymosan (200 µg) under anesthesia. Twenty-four hours after induction, an LLLT treatment (λ = 808 nm, 25 mW nominal power, fluence of 20J/cm2, beam area of 0.02 mm2, time of 33 s, total energy of 0.825 J) was applied. Seven days after induction, samples from the animals' knees were subjected to histological and morphometric analyses, and the percentage of collagen fibers in the synovial area (% total area) with and without polarized light and IL-6 protein expression were measured by immunohistochemistry. Statistical analyses were performed an ANOVA and Tukey's post-test with p < 0.05 to compare the experimental groups using. Inflammation of the synovial region showed significant differences between Sham vs. Control, p < 0.0001, and PBM vs. Sham, p < 0.001. The areas of collagen fibers (total percentage) showed differences between Sham vs. Control, p < 0.0001, and Sham vs. PBM, p = 0.0149. IL-6 showed differences between Sham vs. Control and PBM vs. Sham, p < 0.001. Treatment with PBM using LLLT showed decreased synovial inflammation, collagen fiber formation, fibrosis, and IL-6 protein expression, and consequently decreased joint degradation.



    Chaotic systems exhibit intricate nonlinear dynamics, characterized by features such as pseudo-random behavior and a heightened sensitivity to initial conditions. Lur'e systems (LSs), which encompass a wide range of chaotic systems such as Chua's circuits [1] neural networks [2], and n-scroll attractors [3], have attracted significant research attention in the past decades. Chaos synchronization of LSs has found applications in diverse areas including image encryption [4,5,6], cryptography [7,8] and confidential communication [9,10,11]. The existence of time delay and stochastic perturbations are often unavoidable in a real-world control system and can cause the system to be unstable. Correspondingly, substantial efforts have been devoted to chaos synchronization of stochastic time-delay LSs, and a few results have been reported [12,13,14,15].

    When implementing chaos synchronization in a networked environment, network-induced phenomena, such as packet losses [16], link failures [17] and cyber attacks [18,19,20], can introduce inconsistencies between the system and the controller/filter modes [21]. Therefore, researchers have shown interest in studying chaos synchronization using asynchronous/mode-unmatched controllers. The hidden Markov model (HMM), proposed by Rabiner [22], serves as a suitable tool for describing the asynchronous phenomena. Building upon the HMM framework, Li et al. [23] investigated the synchronization control in Markov-switching neural networks, while Ma et al. [24] explored the drive-response synchronization in fuzzy complex dynamic networks. Despite these advancements, to our knowledge, there is a scarcity of research addressing chaos synchronization in stochastic time-delay LSs under asynchronous controllers.

    Moreover, in networked control systems, the bandwidth of the communication network is usually limited, which can impact the control performance significantly. To eliminate unnecessary resource waste and achieve efficient resource allocation, recent studies on chaos synchronization of LSs have utilized event-triggered mechanism (ETM)-based control methods. For instance, Wu et al. [25] conducted research on exponential synchronization and joint performance issues of chaotic LSs by designing a switching ETM based on perturbation terms. He et al. [26] proposed a secure communication scheme through synchronized chaotic neural networks based on quantized output feedback ETM. Besides, several studies on memory-based ETM for chaos synchronization in LSs have been reported in [27,28,29]. Notably, the above literature employed fixed thresholds in the designed ETM, limiting their ability to conserve communication resources.

    Motivated by the above discussion, we explore the master-slave chaos synchronization of stochastic time-delay LSs within an asynchronous and adaptive event-triggered (AAET) control framework. Unlike previous works [25,26,27,28,29], the thresholds of the ETM used can be adjusted adaptively with real-time system states. The objective is to determine the required AAET controller gains to ensure that the synchronization-error system (SES) has both stochastic stability (SS) and L2L disturbance-suppression performance (LDSP) [30]. The contributions of this paper are:

    1) The AAET controller is first applied to tackle the chaos synchronization issue of stochastic time-delay LSs;

    2) A criterion on the SS and LDSP is proposed using a Lyapunov-Krasovskii functional (LKF), a Wirtinger-type inequality, the Itô formula, as well as a convex combination inequality (CCI);

    3) A method for determining the desired AAET controller is proposed by decoupling the nonlinearities that arise from the Lyapunov matrices and controller gains.

    Throughout, we employ Rn1, Rn1×n2 and N to stand for the n1-dimensional Euclidean space, the set of all n1×n2 real matrices, and the set of natural numbers, respectively. The symbol is the Euclidean vector norm, ()T represents the matrix transposition, He(G) means the sum of matrix G and its transpose GT, indicates the symmetric term in a matrix and E{} and Prob{} indicate, respectively, the expectation and probability operator. Furthermore, we utilize col{} to denote a column vector, diag{} to stand for a block-diagonal matrix and sup{} and inf{} to indicate the supremum and infimum of a set of real numbers, respectively.

    Consider the following master-slave stochastic time-delay LSs:

    {dxm(t)=[Aα(t)xm(t)+Bα(t)xm(tτ(t))+Wα(t)ψ(Fxm(t))]dt+Dα(t)xm(t)dϖ(t),ym(t)=Cα(t)xm(t),xm(t)=ξm0,t[τ2,0], (2.1)
    {dxs(t)=[Aα(t)xs(t)+Bα(t)xs(tτ(t))+Wα(t)ψ(Fxs(t))+u(t)+Eα(t)v(t)]dt+Dα(t)xs(t)dϖ(t),ys(t)=Cα(t)xs(t),xs(t)=ξs0,t[τ2,0] (2.2)

    with xm(t)Rnx and xs(t)Rnx being the state vectors, ξm0 and ξs0 being the initial values, ym(t)Rny and ys(t)Rny being the output vectors, ψ()Rq being the nonlinear term with all components within [ˊgr,ˊgr] for r=1,2,,q, u(t)Rq being the control signal to be designed, v(t) being the disturbance in L2[0,) [31], one-dimension Brownian motion ϖ(t) satisfying E{dϖ(t)}=0 and E{dϖ2(t)}=dt, and time-varying delay τ(t) satisfying 0<τ1τ(t)τ2 and μ1˙τ(t)μ2, where τ1, τ2, μ1, and μ2 are constants. {α(t),t0} is the Markovian process and belongs to the state space N={1,2,,N}. The transition rate (TR) matrix and transition probability is given by Π=[πij]N×N and

    Prob{α(t+ς)=j|α(t)=i}={πijς+o(ς),ij.1+πiiς+o(ς),i=j,

    with ς>0, limς0o(ς)/ς=0, πij0, ij and πii=Ni=1,ijπij [32,33,34]. Aα(t), Bα(t), Cα(t), Dα(t), Eα(t) and Wα(t), which can be abbreviated as Ai, Bi, Ci, Di, Ei, and Wi for α(t)=iN, are matrices with appropriate dimensions.

    In order to minimize information transmission, the adaptive ETM is employed to determine whether the current sampled data should be transmitted to the controller, as illustrated in Figure 1. Let tkh denote the latest transmission time of the output signal, where h>0 is the sampling period. y(tkh) and y(t) denote the latest output signal and the current one, respectively. Defining e(t)=y(tkh)y(t), the event-triggered condition is designed as follows:

    t0h=0,tk+1h=tkh+infpN{ph|eT(t)Ψie(t)<ρ(t)yT(tkh)Ψiy(tkh)},t[tkh,tk+1h), (2.3)
    Figure 1.  Master-Slave stochastic time-delay LSs.

    where Ψi>0 is the trigger matrix and ρ(t) is a threshold parameter adjusted by an adaptive law as

    ρ(t)=ρ1+(ρ2ρ1)2πarccot(κe(t)2), (2.4)

    where ρ1 and ρ2 are predetermined parameters with 0<ρ1ρ2<1, κ is a positive scalar used to adjust the sensitivity of the function e(k)2.

    Remark 1. The value of ρ(t) has a certain influence on the trigger condition (2.3). The trigger condition will be stricter with the value of ρ(t) being higher, resulting in less data being transmitted to the controller. Conversely, the trigger condition will be relaxed with the value of ρ(t) being lower, allowing more data to be transmitted. Furthermore, it is worth to mention that, when ρ(t) takes a constant on (0,1], the adaptive ETM will be transformed into the periodic ETM (PETM); when ρ(t) is set as 0, it will be transformed into the sampled-data mechanism (SDM).

    Remark 2. The arccot function, incorporated in the adaptive law (2.4), enables the threshold parameter of ETM to be dynamically adjusted as the output error changes within the range of (ρ1,ρ2]. The presence of the arccot function results in an inverse relationship between the threshold parameter ρ(t) and the output error e(t). It can be observed that ρ(t) tends to ρ2 as e(t)2 approaches 0, and ρ(t) tends to ρ1 as e(t)2 approaches .

    Consider the following controller:

    u(t)=Kβ(t)(ym(tkh)ys(tkh)),t[tkh,tk+1h). (2.5)

    Unlike [35,36,37], the controller is based on output feedback, which is known to be more easily implemented. In the controller, we introduce another stochastic variable with state space M={1,2,,M} to describe this stochastic process {β(t),t0}. The conditional transition probability (CTP) matrix is signed as Φ=[φiι]N×M with

    φiι=Prob{β(t)=ι|α(t)=i}

    and Mι=1φiι=1. Kβ(t), which will be abbreviated as Kι, is the controller gain to be designed. Note that {{α(t),t0}{β(t),t0}} constitutes a HMM [38,39].

    Define x(t)=xm(t)xs(t). Then, from (2.1), (2.2) and (2.5), one can establish the following SES:

    dx(t)=F(t)dt+G(t)dϖ(t),t[tkh,tk+1h), (2.6)

    where F(t)=(AiKιCi)x(t)+Bix(tτ(t))+Wi˜ψ(Fx(t))Kιe(t)Eiv(t), G(t)=Dix(t), ˜ψ(Fx(t))=ψ(F(x(t)+xs(t)))ψ(Fxs(t)) that satisfies

    ˊgrψr(fTr(x+xs))ψr(fTrxs)fTrx=˜ψr(fTrx)fTrxˊgr,x,xs,r=1,2,,q, (2.7)

    where fTr indicates the r-th row of F. From (2.7), one can get

    [˜ψr(fTrx)ˊgrfTrx][˜ψr(fTrx)ˊgrfTrx]0. (2.8)

    Remark 3. The constants ˊgr and ˊgr can be taken as positive, negative, or zero. By allowing ˊgr and ˊgr to have a wide range of values, the sector bounded nonlinearity can flexibly adapt to the needs of different systems and provide a more flexible regulation and control mechanism.

    To streamline the subsequent analysis, we define

    ζ(t)=col{x(t),x(tτ1),x(tτ(t)),x(tτ2),ϕ1,ϕ2,ϕ3},ϱd=[0n×(d1)nIn×n0n×(9d)n](d=1,2,,9),ϕ1=1τ1ttτ1x(s)ds,ϕ2=1τ(t)τ1tτ1tτ(t)x(s)ds,ϕ3=1τ2τ(t)tτ(t)tτ2x(s)ds,τ12=τ2τ1,

    and provide two definitions and four lemmas.

    Definition 1. The SES (2.6) is said to be with SS if there exists a scalar M(α0,ξ()) satisfying

    E{0x(t)2dt|α0,x(t)=ξ0,t[τ2,0]}<M(α0,ξ())

    when v(t)0.

    Definition 2. Under the zero initial condition, for a given scalar γ>0, the SES (2.6) is said to have a LDSP if

    E{supt0{y(t)2}}γ2E{t0v(s)2ds}

    holds for v(t)0.

    Lemma 1. Given stochastic differential equation

    dx(t)=F(t)dt+G(t)dϖ(t), (2.9)

    where ϖ(t) is one-dimension Brownian motion, for scalars a, b (b>a), and a matrix R, one has

    baFT(s)RF(s)ds1baΩT(a,b)˜RΩ(a,b)+2baΩT(a,b)˜Rμ(a,b),

    where ˜R=diag{R,3R} and

    Ω(a,b)=[x(b)x(a)x(b)+x(a)2babax(s)ds],μ(a,b)=[baG(s)dϖ(s)1baba(b+a2s)G(s)dϖ(s)].

    Remark 4. Following the approaches used in [40,41], the Wirtinger-type inequality of Lemma 1 can be readily established. It should be noted that the integral term in μ(a,b) should be 1baba(b+a2s)G(s)dϖ(s) instead of 1baba(ba+2s)G(s)dϖ(s).

    Lemma 2. [40] Consider the stochastic differential equation (2.9). For n×n real matrix R>0 and the piecewise function τ(t) satisfying 0<τ1τ(t)τ2, where τ1 and τ2 are two constants, and for SR2n×2n satisfying [˜RST˜R]0 with ˜R=diag{R,3R}, the following CCI holds:

    τ12tτ1tτ2FT(s)RF(s)ds2T2S1T1˜R1T2˜R22(dϖ(t)),

    where

    1=Ω(tτ(t),tτ1),2=Ω(tτ2,tτ(t)),(dϖ(t))=τ12τ(t)τ1T1˜Rμ(tτ(t),tτ1)+τ12τ2τ(t)T2˜Rμ(tτ2,tτ(t)).

    Lemma 3. [42] For any two matrices G and R>0 with appropriate dimensions,

    GTR1GRGTG

    holds true.

    Lemma 4. [43] For a given scalar ε>0, suppose there are matrices Λ, U, V and W ensuring

    [ΛU+εVεXεXT]<0.

    Then, one gets

    Λ+He(UX1VT)<0.

    In contrast to the common H performance, LDSP imposes a limitation on the energy-to-peak gain from disturbance to the output signal, ensuring it does not exceed a specified disturbance-suppression index [44]. In this paper, we intend to develop an asynchronous controller in (2.5) with the adaptive ETM in (2.3) to guarantee the SS and LDSP of SES (2.6). First, we give a condition to ensure the SS and LDSP of SES (2.6).

    Theorem 1. Given scalars γ>0 and ρ2, suppose that there exist matrices Pi>0, Q1>0, Q2>0, Q3>0, R1>0, R2>0, Ψi>0, diagonal matrix L>0, and matrices S, Kι, for any iN, ιM satisfying

    [˜R2ST˜R2]0, (3.1)
    CTiCiPi<0, (3.2)
    Λi=Mc=1φiι([Λ1,1iιΛ1,2iγ2I]+[˜ATiιETi](τ21R1+τ212R2)[˜ATiιETi]T)<0. (3.3)

    Then the SES (2.6) has the SS and LDSP, where

    Λ1,1iι=[Υ1,1iιΥ1,2iΥ1,3iιHe(L)0(ρ21)Ψi],Λ1,2i=[ϱT1PiEi00],Υ1,1iι=He(ϱT1PiAiιϱT1FTˊGTLˊGFϱ1)+ϱT1(DTiPiDi+˜Pi)ϱ1+˜Q2GT2SG1GT0˜R1G0GT1˜R2G1GT2˜R2G2+ϱT1ρ2CTiΨiCiϱ1,Υ1,2i=ϱT1PiWi+ϱT1FT(ˊGT+FT)L,Υ1,3iι=ϱT1ρ2CTiΨiϱT1PiKι,˜Rd=diag{Rd,3Rd}(d=1,2),˜Aiι=[AiιWiKι],˜Q=diag{Q1,Q1+Q2,(1μ1)Q3(1μ2)Q2,Q3,03n×3n},Aiι=[AiKιCi0Bi0000],˜Pi=Ni=1πijPj,G0=[ϱ1ϱ2ϱ1+ϱ22ϱ5],G1=[ϱ2ϱ3ϱ2+ϱ32ϱ6],G2=[ϱ3ϱ4ϱ3+ϱ42ϱ7].

    Proof. Select a LKF candidate as:

    V(t,x(t),α(t),β(t))=4k=1Vk(t,x(t),α(t),β(t)), (3.4)

    where

    V1(t,x(t),α(t),β(t))=xT(t)Pα(t)x(t),V2(t,x(t),α(t),β(t))=ttτ1xT(s)Q1x(s)ds+tτ1tτ(t)xT(s)Q2x(s)ds+tτ(t)tτ2xT(s)Q3x(s)ds,V3(t,x(t),α(t),β(t))=τ1ttτ1tvFT(s)R1F(s)dsdv+τ12tτ1tτ2tvFT(s)R2F(s)dsdv.

    Assume that α(t)=i, α(t+ς)=j, β(t)=ι and define L as the weak infinitesimal operator of the stochastic process {x(t),α(t)}. Then, along SES (2.6), we get

    LV1(t,x(t),i,ι)=2xT(t)PiF(t)+GT(t)PiG(t)+xT(t)Ni=1πijPjx(t)=ζT(t)[He(ϱT1PiAiι)+ϱT1(DTiPiDi+˜Pi)ϱ1]ζ(t)+2ζT(t)ϱT1PiWi˜ψ(Fx(t))2ζT(t)ϱT1PiKιe(t)2ζT(t)ϱT1PiEiv(t), (3.5)
    LV2(t,x(t),i,ι)=xT(t)Q1x(t)+xT(tτ1)(Q1+Q2)x(tτ1)+(1˙τ(t))xT(tτ(t))(Q2+Q3)x(tτ(t))xT(tτ2)Q3x(tτ2)ζT(t)˜Qζ(t), (3.6)
    LV3(t,x(t),i,ι)=FT(t)(τ21R1+τ212R2)F(t)τ1ttτ1FT(s)R1F(s)dsτ12tτ1tτ2FT(s)R2F(s)ds. (3.7)

    Define an augmented vector as ˜ζ(t)=col{ζ(t),˜ψ(Fx(t)),e(t)}. We can derive that

    FT(t)(τ21R1+τ212R2)F(t)=[˜ζ(t)v(t)]T[˜ATiιETi](τ21R1+τ212R2)[˜ATiιETi]T[˜ζ(t)v(t)]. (3.8)

    Based on (3.1), applying Lemmas 1 and 2 to the integral terms in (3.7) yields

    τ1ttτ1FT(s)R1F(s)dsζT(t)GT0˜R1G0ζ(t)2ζT(t)GT0˜R1μ(tτ1,t), (3.9)
    τ12tτ1tτ2FT(s)R2F(s)dsζT(t)[2GT2SG1GT1˜R2G1GT2˜R2G2]ζ(t)2(dϖ(t)), (3.10)

    where (dϖ(t))=τ12τ(t)τ1ζT(t)GT1˜R2μ(tτ(t),tτ1)+τ12τ2τ(t)ζT(t)GT2˜R2μ(tτ2,tτ(t)). Recalling (3.7)–(3.10), we have

    LV3(t,x(t),i,ι)[˜ζ(t)v(t)]T[˜ATiιETi](τ21R1+τ212R2)[˜ATiιETi]T[˜ζ(t)v(t)]+˜(dϖ(t))+ζT(t)[GT0˜R1G02GT2SG1GT1˜R2G1GT2˜R2G2]ζ(t), (3.11)

    where ˜(dϖ(t))=2ζT(t)GT0˜R1μ(tτ1,t)2(dϖ(t)). It follows from (2.8) that

    2(˜ψ(Fx(t))ˊGFx(t))TL(˜ψ(Fx(t))ˊGFx(t))0,

    which means

    02(˜ψ(Fx(t))ˊGFϱ1ζ(t))TL(˜ψ(Fx(t))ˊGFϱ1ζ(t))=˜ψT(Fx(t))He(L)˜ψ(Fx(t))+2ζT(t)ϱT1FT(ˊGT+ˊGT)L˜ψ(Fx(t))ζT(t)He(ϱT1FTˊGTLˊGFϱ1)ζ(t). (3.12)

    In addition, recalling the adaptive ETM (2.3), we obtain

    0ρ(t)yT(tkh)Ψiy(tkh)eT(t)Ψie(t)ρ2[y(t)+e(t)]TΨi[y(t)+e(t)]eT(t)Ψie(t)=ρ2[xT(t)CTiΨiCix(t)+2xT(t)CTiΨie(t)+eTΨie(t)]eT(t)Ψie(t)=ζT(t)ϱT1ρ2CTiΨiCiϱ1ζ(t)+2ζT(t)ϱT1ρ2CTiΨie(t)+eT(t)(ρ21)Ψie(t). (3.13)

    Combining (3.5), (3.6), (3.11), (3.12) and (3.13), we find that

    LV(t,x(t),i,ι)ζT(t)Υ1,1iιζ(t)+2ζT(t)Υ1,2i˜ψ(Fx(t))+2ζT(t)Υ1,3iιe(t)2ζT(t)ϱT1PiEiv(t)+eT(t)(ρ21)Ψie(t)˜ψT(Fx(t))He(L)˜ψ(Fx(t))+˜(dϖ(t)+[˜ζ(t)v(t)]T[˜ATiιETi](τ21R1+τ212R2)[˜ATiιETi]T[˜ζ(t)v(t)]. (3.14)

    Noting E{˜(dϖ(t))}=0, we can calculate E{LV(t,x(t),i,ι)} by (3.14) that

    E{LV(t,x(t),i,ι)}[˜ζ(t)v(t)]TDc=1φiι([Λ1,1iιΛ2,2i0]+[˜ATiιETi](τ21R1+τ212R2)[˜ATiιETi]T)[˜ζ(t)v(t)]T. (3.15)

    Next, we discuss the SS of (2.6) under the condition of v(t)0 and the LDSP of (2.6) under the condition of v(t)0, respectively.

    i) v(t)0, we can get the following inequality from (3.15):

    E{LV(t,x(t),i,ι)}˜ζT(t)Λ0i˜ζ(t),

    where Λ0i=Mc=1φiι(Λ1,1iι+˜ATiι(τ21R1+τ212R2)˜Aiι). From (3.3), we can find that there exists a>0 such that for any

    E{LV(t,x(t),i,ι)}ax(t)2,iN.

    Utilizing the Itô formula, we obtain

    E{V(t,x(t),α(t))}E{V(0,x0,α0)}=E{t0V(s,x(s),α(s))ds}aE{t0x(s)2ds},

    which means

    E{t0x(s)2ds}1aV(0,x0,α0).

    Thus, the SS of (2.6) is proved.

    ii) v(t)0, under the zero initial condition, defining J(t)=yT(t)y(t)γ2t0vT(s)v(s)ds leads to

    J(t)=yT(t)y(t)γ2t0vT(s)v(s)ds+E{t0LV(s,x(s),i,ι)ds}(V(t,x(t),i,ι)V(0,x0,α0,β0))xT(t)(CTiCiPi)x(t)+t0[˜ζ(s)v(s)]TΛi[˜ζ(s)v(s)]ds.

    From conditions (3.2) and (3.3), we know that J(t)0. According to Definition 2, the SES (2.6) has a LDSP γ.

    On the basis of Theorem 1, a design method of the AAET controller can be proposed.

    Theorem 2. Given scalars ε, ρ2 and γ>0, suppose that there exist matrices Pi>0, Q1>0, Q2>0, Q3>0, R1>0, R2>0, Ψi>0, diagonal matrix L>0, matrices S, Xι, Yι, and Tiι for any iN, ιM satisfying (3.1), (3.2), and

    [He(Tiι+Yι)PiXιεYTιεXιεXTι]<0, (3.16)
    Θi=Mc=1φiι[Θ1,1iιΛ1,2iΘ1,3iΘ1,4iγ2IΘ2,3iΘ2,4iΘ3,3i0Θ4,4i]<0, (3.17)

    where

    Θ1,1iι=[˜Υ1,1iιΥ1,2i˜Υ1,3iιHe(L)0(ρ21)Ψi],Λ1,2i=[ϱT1PiEi00],Θ1,3i=[τ1φi1˜Ti1τ1φiM˜TiM],Θ1,4i=[τ12φi1˜Ti1τ12˜TiM],Θ2,3i=[τ1φi1ETiPiτ1φiMETiPi],Θ2,4i=[τ12φi1ETiPiτ12φiMETiPi],Θ3,3i=diag{R12Pi,,R12Pi},Θ4,4i=diag{R22Pi,,R22Pi},˜Υ1,1iι=He(ϱT1iιϱT1FTˊGTLˊGFϱ1)+ϱT1(DTiPiDi+˜Pi)ϱ1+˜Q2GT2SG1GT0˜R1G0GT1˜R2G1GT2˜R2G2+ϱT1ρ2CTiΨiCiϱ1,Υ1,2i=ϱT1PiWi+ϱT1FT(ˊGT+ˊGT)L,˜Υ1,3iι=ϱT1ρ2CTiΨi+ϱT1Tiι,˜iι=[iιPiWiTiι],iι=[PiAi+TiιCi0PiBi0000],˜Pi=Ni=1πijPj,˜Rd=diag{Rd,3Rd}(d=1,2),˜Q=diag{Q1,Q1+Q2,(1μ1)Q3(1μ2)Q2,Q3,03n×3n},G0=[ϱ1ϱ2ϱ1+ϱ22ϱ5],G1=[ϱ2ϱ3ϱ2+ϱ32ϱ6],G2=[ϱ3ϱ4ϱ3+ϱ42ϱ7].

    Then, AAET controller (2.5) with gains

    Kι=X1ιYι,ιM (3.18)

    enables the SES (2.6) to have both SS and LDSP.

    Proof. According to (3.18), we have PiKι<Tiι by applying Lemma 4 to (3.16). Then, we can conclude that PiAiι<iι and Pi˜Aiι<˜iι lead to

    Λ1,1iιΘ1,1iι, (3.19)
    Λ1,3iΘ1,3i, (3.20)
    Λ1,4iΘ1,4i, (3.21)

    where

    Λ1,3i=[τ1φi1˜ATi1Piτ1φiD˜ATiDPi],Λ1,4i=[τ12φi1˜ATi1Piτ12φiD˜ATiDPi].

    Based on Lemma 3, we can get that PiR11PiR12Pi and PiR12PiR22Pi, which means

    Λ3,3iΘ3,3i, (3.22)
    Λ4,4iΘ4,4i, (3.23)

    where Λ3,3i=diag{PiR11Pi,,PiR11Pi}, Λ4,4i=diag{PiR12Pi,,PiR12Pi}. Due to φiι>0, combining (3.19)–(3.23) yields

    Λ0iΘi<0, (3.24)

    where

    Λ0i=Dc=1φiι[Λ1,1iιΛ1,2iΛ1,3iΛ1,4iγ2IΘ2,3iΘ2,4iΛ3,3i0Λ4,4i].

    By applying Schur's complement to (3.24), we find that (3.3) can be guaranteed by (3.17). The proof is completed.

    Remark 5. The coupling between parameter Pi and the controller gain Kι in Theorem 1 is addressed by introducing a slack matrix Tiι. It is worth mentioning that directly setting the coupling term KιP1i equal to the matrix Tiι (i.e. Kι=TiιPi) would result in non-uniqueness of controller gains Kι. In this paper, we introduce Tiι such that PiKι<Tiι. By designing the controller gains, as given in equation (3.18), and combining it with Lemma 4, the aforementioned issue is avoided.

    Remark 6. Theorem 1 provides a analysis result of the SS and LDSP for SES (2.6) based on HMM, while Theorem 2 presents a design scheme for the needed AAET controller. The proofs of these theorems involve the use of the LKF in (3.4), Itô formula, as well as the inequalities in Lemmas 1-4. To further reduce the conservatism of the obtained results, one may refer to the augmented LKFs in [45,46], the free-matrix-based approaches in [47,48,49], the refined CCIs in [50,51] and the decoupling methods in [52].

    Example 1. In this example, we consider a three-mode Chua's circuit given by

    {dx1(t)=[ai(x2(t)m1x1(t)+(m1m0)ψ1(x1(t)))cix1(tτ(t))]dt+di(x2(t)m1x1(t))dϖ(t),dx2(t)=[x1(t)x2(t)+x3(t)cix1(tτ(t))]dt+0.1(x1(t)x2(t)+x3(t))dϖ(t),dx3(t)=[bix2(t)+ci(2x1(tτ(t))x3(tτ(t)))]dtm3x2(t)dϖ(t),

    where parameters m0=17, m1=27, m3=0.1, and ai, bi, ci, di (i=1,2,3) are listed in Table 1. The nonlinear characteristics ψ1(x1(t))=12(|x1(t)+1||x1(t)1|) belonging to sector [0,1], and ψ2(x2(t))=ψ3(x3(t))=0. The circuit model can be re-expressed as LS (2.1) with

    Ai=[aim1ai01110bi0],Bi=[ci00ci002ci0ci],Di=[dim1di00.10.10.10m30],Ci=[100010001],Wi=[ai(m1m0)00000000],Ei=[0.100]T.
    Table 1.  The parameters ai, bi, ci, di in the Chua's circuit.
    i ai bi ci di
    1 9 14.28 0.1 0.01
    2 8 10 0.05 0.01
    3 9 14 0.15 0.01

     | Show Table
    DownLoad: CSV

    The delay parameters are specified as τ1=0.1, τ2=0.18, μ1=0.1 and μ2=0.26, the parameters related to the adaptive law are given by ρ1=0.1, ρ2=0.9, κ=0.5 and the TR and CTP matrices are chosen as

    Π=[523363415],Φ=[0.40.30.30.20.30.50.40.50.1].

    By solving the LMIs in Theorem 2, the optimal LDSP is found to be γ=0.0553, and the controller gains and adaptive ETM weight matrices are calculated as

    K1=[2.18033.42170.28400.37750.17680.07480.20381.83112.1877],K2=[2.12233.36410.37040.44170.45620.00720.26600.90162.0248],K3=[2.19692.92520.34380.45440.06310.04530.24411.22442.1906],Ψ1=[12.35816.03930.00596.039324.55615.59300.00595.593012.6577],Ψ2=[12.31879.03771.02799.037722.23124.17521.02794.175212.0248],Ψ3=[12.00079.91280.66699.912824.47704.44050.66694.440512.1092].

    We set the initial states as xm(t)=[0.20.30.2]T, and the disturbance as . The sampling period is chosen to be . A possible mode evolution of system and AAET controller is drawn in Figure 2. When there is no controller applied, we can find from Figure 3 that the system is unstable. By utilizing the devised AAET controller shown in Figure 4, the state response curves of the SES (2.6) are exhibited in Figure 5. It can be seen that the synchronization error between the master and slave LSs approaches zero over time, indicating that the master and slave LSs can successfully achieve synchronization under the presented AAET controller. The trajectory of the adaptive law and release time intervals between two trigger moments are depicted in Figures 6 and 7, respectively. Based on the simulation results, it can be observed that as the SES (2.6) stabilizes, the threshold function gradually converges to a fixed value. Define the function for LDSP. Then the trajectory of under zero initial condition is depicted in Figure 8. It is evident from Figure 8 that the maximum value of is , which is lower than .

    Figure 2.  Possible mode evolution processes of the LSs and AAET controller.
    Figure 3.  Trajectory of SES (2.6) without control.
    Figure 4.  Trajectory of AAET controller (2.5).
    Figure 5.  Trajectory of SES (2.6) with control.
    Figure 6.  Trajectory of the adaptive law.
    Figure 7.  Release time intervals.
    Figure 8.  Trajectory of .

    Table 2 presents the data transmission rates under different triggering mechanisms in the same conditions. The comparison demonstrates that the adaptive ETM employed in this study can effectively reduce data transmission to achieve the goal of conserving channel resources.

    Table 2.  The data transmission rates under different triggering mechanisms.
    SDM in [14] PETM in [53] Adaptive ETM in this paper
    Number of transmitted data 500 236 194
    Data transmission rates 100% 47.20% 38.80%

     | Show Table
    DownLoad: CSV

    The master-slave chaos synchronization of stochastic time-delay LSs (2.1) and (2.2) within a networked environment has been considered. To tackle the challenges posed by potential mode-mismatch behavior and limited networked channel resources, the AAET controller in (2.5) has been employed. A criterion on the SS and LDSP of the SES (2.6) has been proposed in Theorem 1 using a LKF, a Wirtinger-type inequality, the Itô formula, as well as a CCI. Then, a method for determining the desired AAET controller gains has been proposed in Theorem 2 by decoupling the nonlinearities that arise from the Lyapunov matrices and controller gains. Finally, simulation results have confirmed that the designed controller can achieve chaos synchronization between the master LS (2.1) and slave LS (2.2), while significantly reducing data transmission.

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

    This work was supported by the Key Research and Development Project of Anhui Province (Grant No. 202004a07020028).

    All authors declare no conflicts of interest in this paper.


    Acknowledgments



    The study was financially supported by Fundação Hermínio Ometto and this study was also financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior – Brasil (CAPES) – Finance Code 001.

    Conflicts of interest



    All authors declared no conflict of interest.

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