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Research article

Stabilization in distribution of hybrid stochastic differential delay equations with Lévy noise by discrete-time state feedback controls

  • Received: 08 December 2024 Revised: 28 January 2025 Accepted: 14 February 2025 Published: 24 February 2025
  • MSC : 93C55, 93D15, 93E03

  • This paper was concerned with stabilization in distribution by feedback controls based on discrete-time state observations for a class of nonlinear stochastic differential delay equations with Markovian switching and Lévy noise (SDDEs-MS-LN). Compared with previous literature, we employed Lévy noise in the discussion about stabilization in distribution for hybrid stochastic delay systems and we considered using a discrete-time linear feedback control which is more realistic and costs less. In addition, by constructing a new Lyapunov functional, stabilization in distribution of controlled systems can be achieved with the coefficients satisfying globally Lipschitz conditions. In particular, we discussed the design of feedback controls in two structure cases: state feedback and output injection. At the same time, the lower bound for the duration between two consecutive observations τ (τ) was obtained as well. Finally, a numerical experiment with some computer simulations was given to illustrate the new results.

    Citation: Jingjing Yang, Jianqiu Lu. Stabilization in distribution of hybrid stochastic differential delay equations with Lévy noise by discrete-time state feedback controls[J]. AIMS Mathematics, 2025, 10(2): 3457-3483. doi: 10.3934/math.2025160

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  • This paper was concerned with stabilization in distribution by feedback controls based on discrete-time state observations for a class of nonlinear stochastic differential delay equations with Markovian switching and Lévy noise (SDDEs-MS-LN). Compared with previous literature, we employed Lévy noise in the discussion about stabilization in distribution for hybrid stochastic delay systems and we considered using a discrete-time linear feedback control which is more realistic and costs less. In addition, by constructing a new Lyapunov functional, stabilization in distribution of controlled systems can be achieved with the coefficients satisfying globally Lipschitz conditions. In particular, we discussed the design of feedback controls in two structure cases: state feedback and output injection. At the same time, the lower bound for the duration between two consecutive observations τ (τ) was obtained as well. Finally, a numerical experiment with some computer simulations was given to illustrate the new results.



    Stochastic differential equations (SDEs) with Markovian switching (also known as hybrid SDEs) has been widely used to model many systems in biological systems, financial systems, and other fields. A field of common interest in the study of hybrid SDEs is automatic control, taking subsequent emphasis on the stability analysis [1,2]. Most of the literature, such as [3,4,5,6,7], only consider Brown motions. However, Brown motions are continuous and cannot describe discontinuous noises like jump-type noises. Compared with Brown motions, Lévy noise, which contains both continuous Brown motions and discontinuous Poisson jumps, can model the extreme sudden events, such as earthquakes, storms, floods, wars, and so on. For example, in [8] some sufficient conditions were put forward to achieve almost surely exponential stability of neural networks with Markovian switching and Lévy noise. Therefore, with the development of stochastic analysis, stochastic differential equations with Markovian switching and Lévy noise are considered by many researchers, see [9,10,11,12].

    It is well known that time delays are often and inevitably encountered for various reasons in many fields such as population systems, manufacturing, chemistry and chemical engineering, finance, etc. Meanwhile, a time delay is often one of the main causes of poor performance in systems, see [13,14]. Hence, taking time delays into account is reasonable and necessary when studying the stability of SDDEs-MS-LN. Nowadays, stability and stabilization of such SDDEs have been studied, see [15,16,17]. For example, Yuan et al. in [16] investigated sufficient conditions for stability of delay jump diffusion processes. Li in [17] focused on the mean square stability of stochastic differential equations with Lévy noise.

    A common feature in these papers is that most of the research is focused on the stability of the trivial solutions. However, many hybrid systems do not have an equilibrium state or their solutions do not converge to zero, see [18,19]. It is not sufficient to only study the stability of trivial solutions in the real world. For example, for many population systems under realistic backdrops, stochastic permanence is a more suitable control goal than extinction (see [20,21,22]). In this case, it is of great significance to know whether the solution will converge to some distribution or not (but not necessarily to zero). This property is known as asymptotic stability in distribution. Stability in distribution of SDEs-MS with Brownian motion has attracted some attention of scholars recently, for example, Yuan et al. [19] and You et al. [23]. In 2010, Yuan et al. [16] studied stability in distribution of hybrid delay systems with jumps. As a classical area of stability of hybrid systems, Li et al. [24] recently considered to employ delay feedback controls to stabilize a given SDEs-MS-LN in distribution. But for the stabilization in distribution of SDDEs-MS-LN, the discussion is still open. In addition, to reduce the practical cost of control design, feedback controls based on discrite-time state observations[1,14] are considered in this paper.

    Mathematically speaking, let us consider an unstable SDDE-MS-LN

    dX(t)=f(X(t),X(th),r(t))dt+g(X(t),X(th),r(t))dB(t)+Rn0H(X(t),X((th)),r(t),z)˜N(dt,dz), (1.1)

    where X(t)Rd, h is a time delay of the system, r(t) is a Markov chain, B(t) is a Brownian motion, ˜N(dt,dz) is a compensated Poisson random measure, and Rn0=Rn{0} (For formal definitions, see Section 2.) Such a regular feedback control requires the continuous observations of the state X(t) for all t0. This is of course expensive and sometimes not possible as the observations are often of discrete time. Now we can design a feedback control u(X([t/τ]τ),r(t)) based on the discrete-time observations of the state X(t) at times 0, τ, 2τ, ..., so that the controlled system

    dX(t)=[f(X(t),X(th),r(t))+u(X([t/τ]τ),r(t))]dt+g(X(t),X(th),r(t))dB(t)+Rn0H(X(t),X((th)),r(t),z)˜N(dt,dz), (1.2)

    becomes stable in distribution.

    The main aim of this paper is to explore how to use feedback control u(X([t/τ]τ),r(t)) to stabilize a given unstable SDDE-MS-LN in distribution. The key points of this paper are as follows.

    ● We introduce Lévy noise to remodel hybrid stochastic delay systems and study the stability in distribution for controlled SDDEs-MS-LN.

    ● Due to the discontinuity of Lévy noise, we need to study the stability in distribution for SDDEs-MS-LN in functional space Dh (for formal definitions, see Section 2) rather than Ch in [23].

    ● Making use of the generalized Itˆo formula for Lévy-type stochastic integrals [25], we construct a special Lyapunov functional based on Lévy noise, the property of stability and discrete-time feedback control to achieve the asymptotic stability in distribution for controlled SDDEs-MS-LN.

    ● In order to reduce the cost of the continuous working time of the controller, feedback control u(X([t/τ]τ),r(t)) based on the discrete-time observations is an efficient strategy to stabilize the unstable systems. Moreover, we show that there is a positive number τ such that the feedback control u(X([t/τ]τ),r(t)) will make the controlled system (1.2) asymptotically stable in distribution provided ττ. We will also give a lower bound on τ which is computable numerically.

    The structure of this paper is organized as follows. In Section 2, we present some notations, definitions, and assumptions related to Eq (1.1). In Section 3, we study the stability in distribution of the solution to Eq (1.2) based on the Lyapunov functionl and Itˆo formula. In Section 4, the method for designing the control function is discussed. In Section 5, we provide a numerical example to verify the effectiveness of the new results. Finally, this article is concluded in Section 6.

    Throughout this paper, unless otherwise specified, we use the following notations. Let Rd be the d-dimensional Euclidean space and B(Rd) denote the family of all Borel measurable sets in Rd. Let || denote the Euclidean norm or the matric trace norm, respectively. For a matrix A, |A|=trace(ATA) denotes its trace norm and A=max{|Ax|:|x|=1} denotes its operator norm. If A is a symmetric matrix, the largest and smallest eigenvalue are denoted by λmax(A) and λmin(A), respectively. In general, (Ω,F,{Ft}t0,P) signifies a complete probability space whose filtration {Ft}t0 satisfies the usual conditions. Denote by Dh (or D([h,0];Rd)) the family of all càdlàg (i.e., right continuous with left limits) functions ξ : [h,0]Rd in the Skorokhod topology. For any ξ1,ξ2Dh, define the Skorohod metric dS(ξ1,ξ2)=infλΛ{λξ1ξ2λh}, where Λ denotes the class of strictly increasing, continuous mappings of [h,0] onto itself, ξ2λ denotes the composition of two functions ξ2 and λ, λ=suphs<t0|logλ(t)λ(s)ts|, and ξh=suphs0|ξ(s)|. Under the Skorohod metric dS,D([h,0];Rd) is complete and separable ([26], Theorem 12.2, p. 128). In addition, B(Dh) denotes the family of all Borel measurable sets in Dh. Let B(t)=(B1,,Bm) be an m-dimensional Brownian motion. Denote by N(t,z) an n-dimensional Poisson process, and denote the compensated Poisson random measure by

    ˜N(dt,dz)T=N(dt,dz)ν(dz)dt=(N1(dt,dz1)ν1(dz1)dt,,Nn(dt,dzn)νn(dzn)dt),

    where {Nk,k=1,,n} are independent 1-dimensional Poisson random measures with characteristic measure {νk,k=1,,n} coming from n independent 1-dimensional Poisson point processes.

    Let r(t), t0, be a right-continuous irreducible Markov chain on the probability space taking values in a finite state space S={1,2,,N} with the generator Γ=(γij)N×N given by

    P{r(t+Δ)=jr(t)=i}={γijΔ+o(Δ) if ij,1+γijΔ+o(Δ) if i=j,

    where Δ>0 satisfies limΔ0o(Δ)Δ=0 and γij is the transition rate from i to j satisfying γij>0 if ij while γii=ijγij. We assume that r(t),B(t), and N(t,z) are independent of each other.

    Let us consider a d-dimension SDDE-MS-LN (1.1), where f:Rd×Rd×SRd, g:Rd×Rd×SRd×m, and H:Rd×Rd×S×Rn0Rd×n are Borel measurable functions, X(t)=limstX(s). We note that each column H(k) of the d×n matrix H=[Hlj] depends on z only through the kth coordinate zk, that is

    H(k)(X,i,z)=H(k)(X,i,zk);z=(z1,,zn)Rn0.

    We refer to [16,27] where this type of dependence is discussed and investigated for SDDEs-MS-LN. We can rewrite out in detail component Xl(t), 1ld, in (1.1), that is

    dXl(t)=fl(X(t),X(th),r(t))dt+mj=1glj(X(t),X(th),r(t))dBj(t)+nk=1R{0}Hlk(X(t),X((th)),r(t),zk)˜Nk(dt,dzk).

    Next we will state an assumption about the coefficients of SDDE-MS-LN (1.1).

    Assumption 2.1. There exist positive constants a1, a2, and a3 such that

    |f(x,ˉx,i)f(y,ˉy,i)|2a1(|xy|2+|ˉxˉy|2),|g(x,ˉx,i)g(y,ˉy,i)|2a2(|xy|2+|ˉxˉy|2),

    and

    nk=1R{0}|H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk)|2νk(dzk)a3(|xy|2+|ˉxˉy|2),

    for all x,ˉx,y,ˉyRd and iS.

    It is easy to see from Assumption (2.1) that

    |f(x,ˉx,i)|22a1(|x|2+|ˉx|2)+a0,|g(x,ˉx,i)|22a2(|x|2+|ˉx|2)+a0 (2.1)

    and

    nk=1R{0}|H(k)(x,ˉx,i,zk)|2νk(dzk)2a3(|x|2+|ˉx|2)+a0 (2.2)

    for all (x,ˉx,i)Rd×Rd×S and iS, where a0=2maxiS(|f(0,0,i)|2|g(0,0,i)|2)nk=1R{0}|H(k)(0,0,i,zk)|2νk(dzk).

    By Assumption 2.1, it is known (see [16]) that the SDDE-MS-LN (1.1) has a unique global solution X(t) for all t0. Assume that the original SDDE-MS-LN (1.1) does not have the desired property of stability in distribution. Therefore we need to design a feedback control to stabilize the system (1.1). To make the design more concise and simple, we use the linear form of feedback control u(X(δ(t)),r(t))=A(r(t))X(δ(t)), where A(i)AiRd×d(1iN), δ(t)=[t/τ]τ. In addition, throughout this paper, we will set a4=maxiSAi2. The controlled system (1.2) therefore becomes

    dX(t)=[f(X(t),X(th),r(t))+A(r(t))X(δ(t))]dt+g(X(t),X(th),r(t))dB(t)+Rn0H(X(t),X((th)),r(t),z)˜N(dt,dz) (2.3)

    with the initial data as

    {{X(s):hs0}=ξDh,r(0)=iS. (2.4)

    It is well known to all (see [28]), under Assumption 2.1, SDDE-MS-LN (2.3) has a unique global solution for any initial data (2.4). Define Xt={X(t+s):hs0} for t0, which is a Dh-valued process. Xξ,i(t) denotes the solution of SDDE-MS-LN (2.3) with initial data (2.4). ri(t) denotes the Markov chain starting from i. It is also known that (see [29])

    E[Xξ,it2h]<Ct(1+ξ2h)t0, (2.5)

    where Ct is a positive constant that depends on t but is independent of the initial data (ξ,i).

    We notice that the joint process (Xt,r(t)) is not a time-homogeneous Markov process. But when h can be divisible by τ, for k0, we can easily get that the joint process (Xkτ,r(kτ)) is a time-homogeneous Markov process with transition probability p(k,ξ,i;dζ×{j}), where p(k,ξ,i;dζ×{j}) denotes the transition probability measure on Dh×S, that is

    P((Xξ,ikτ,ri(kτ))E×J)=jJEp(k,ξ,i;dζ×{j}) (2.6)

    for any EB(Dh) and JS.

    Denote by P(Dh) the family of probability measures on the measurable space (Dh,B(Dh)). For P1,P2P(Dh), metric dL is given by

    dL(P1,P2)=supϕL|Dhϕ(ξ)P1(dξ)Dhϕ(ξ)P2(dξ)|,

    where L={ϕ:DhR satisfying |ϕ(ξ)ϕ(ζ)|dS(ξ,ζ) and |ϕ(ξ)|1 for ξ,ζDh}. In addition, let L(Xt) denote the probability measure generated by Xt on (Dh,B(Dh)).

    Definition 2.1. The SDDE-MS-LN (2.3) is said to be asymptotically stable in distribution if there exists a probability measure μhP(Dh) such that

    limkdL(L(Xξ,ikτ),μh)=0

    for all (ξ,i)Dh×S.

    Let C2(Rd×S;R+) denote the family of all non-negative continuous functions Ψ(x,i) defined on Rd×S which are twice continuously differentiable in x for all iS. Assume that there exists one ΨC2(Rd×S;R+), and define an operator LΨ from Rd×Rd×S to R by:

    LΨ(x,ˉx,i)=Ψx(x,i)[f(x,ˉx,i)+Aix]+12trace[g(x,ˉx,i)TΨxx(x,i)g(x,ˉx,i)]+R{0}nk=1[Ψ(x+H(k)(x,ˉx,i,zk),i)Ψ(x,i)Ψx(x,i)H(k)(x,ˉx,i,zk)]νk(dzk)+Nj=1γijΨ(x,j), (3.1)

    where Ψx(x,i)=(Ψ(x,i)x1,Ψ(x,i)x2,,Ψ(x,i)xd),Ψxx(x,i)=(2Ψ(x,i)xixj)d×d.

    The difference between two solutions of the system (2.3) with different initial values is as follows:

    Xξ,i(t)Xζ,i(t)=ξζ+t0[f(Xξ,i(s),Xξ,i(sh),ri(s))f(Xζ,i(s),Xζ,i(sh),ri(s))+A(ri(s))(Xξ,i(δ(t))Xζ,i(δ(t)))]ds+t0[g(Xξ,i(s),Xξ,i(sh),ri(s))g(Xζ,i(s),Xζ,i(sh),ri(s))]dB(s)+t0Rn0[H(Xξ,i(s),Xξ,i((sh)),ri(s),z)H(Xζ,i(s),Xζ,i((sh)),ri((sh)),z)]˜N(ds,dz). (3.2)

    Let ΦC2(Rd×S;R+), and define an operator LΦ:Rd×Rd×Rd×Rd×SR concerning Eq (3.2) by

    LΦ(x,y,ˉx,ˉy,i)=Φx(xy,i)[f(x,ˉx,i)f(y,ˉy,i)+Ai(xy)]+12trace[(g(x,ˉx,i)g(y,ˉy,i))TΦxx(xy,i)(g(x,ˉx,i)g(y,ˉy,i))]+R{0}nk=1[Φ(xy+H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk),i)Φ(xy,i)Φx(xy,i)(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))]νk(dzk)+Nj=1γijΦ(xy,j). (3.3)

    To study stabilization in distribution of system (2.3), we need the following assumptions.

    Assumption 3.1. There exist positive constants c1, θ1, b2, and b0>b10, function Ψ(x,i)C2(Rd×S;R+), and Q1(x)C(Rd;R+) such that

    c1|x|2Ψ(x,i)Q1(x),LΨ(x,ˉx,i)+θ1|Ψx(x,i)|2b0Q1(x)+b1Q1(ˉx)+b2 (3.4)

    for all (x,ˉx,i)Rd×Rd×S.

    Assumption 3.2. There exist positive constants c2, θ2, and b3>b40, function Φ(x,i)C2(Rd×S;R+), and Q2(x)C(Rd;R+) such that

    c2|xy|2Φ(x,y,i)Q2(xy),LΦ(x,y,ˉx,ˉy,i)+θ2|Φx(xy,i)|2b3Q2(xy)+b4Q2(ˉxˉy) (3.5)

    for all (x,y,ˉx,ˉy,i)Rd×Rd×Rd×Rd×S.

    To obtain our results, we need to establish the Lyapunov functional on the segments ˆXt:={X(t+s):τhs0} and ˆrt={r(t+s):τhs0} for tτ. Let r(s)=r(0) for τhs0. Evidently, ˆXt is D([τh,0];Rd)-valued which is different with Xt. The Lyapunov functional will be of the form

    V(ˆXt,ˆrt,t):=Ψ(X(t),r(t))+ˆV(ˆXt,ˆrt,t), for th, (3.6)

    where

    ˆV(ˆXt,ˆrt,t)=αttτts[τ|f(X(v),f(X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),g(X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz)]dvds

    and α is a positive constant selected later.

    Remark 3.1. Since our feedback control is based on discrete-time state observations, the Lyapunov functional in [23,24] is not appropriate which is employed for the stabilization in distribution problem by delay feedback control. Therefore, we consider to employ a new Lyapunov functional motivated by [14,24] to prove the stability in distribution of controlled system (2.3).

    We can observe that

    c1|X(t)|2V(ˆXt,ˆrt,t)Q1(X(t))+ˆV(ˆXt,ˆrt,t). (3.7)

    For convenience, X(t) denotes Xξ,i(t) and we fix the initial data (ξ,i) arbitrarily. Applying the generalized functional Itˆo formula to the Lyapunov functional defined by (3.6) yields

    dV(ˆXt,ˆrt,t)=LV(ˆXt,ˆrt,t)dt+dM(t)

    for tτ, where M(t) is a martingale with M(0)=0, and

    LV(ˆXt,ˆrt,t)=LΨ(X(t),X(th),r(t))ΨX(X(t),r(t))Ar(t)(X(t)X(δ(t)))+ατ[τ|f(X(t),X(th),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(th),r(t))|2+Rn0|H(X(t),X((th)),r(t),z)|2ν(dz)]αttτ[τ|f(X(s),X(sh),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(sh),r(s))|2+Rn0|H(X(s),X((sh)),r(s),z)|2ν(dz)]dsLΨ(X(t),X(th),r(t))+θ1|ΨX(X(t),r(t))|2+14θ1Ar(t)2|X(t)X(δ(t))|2+ατ[τ|f(X(t),X(th),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(th),r(t))|2+Rn0|H(X(t),X((th)),r(t),z)|2ν(dz)]αttτ[τ|f(X(s),X(sh),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(sh),r(s))|2+Rn0|H(X(s),X((sh)),r(s),z)|2ν(dz)]ds. (3.8)

    By Assumption 2.1, we can derive

    ατ[τ|f(X(t),X(th),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(th),r(t))|2+Rn0|H(X(t),X((th)),r(t),z)|2ν(dx)]ατ[4a1τ(|X(t)|2+|X(th)|2)+2a0τ+2a4τ|X(δ(t))|2+2a2(|X(t)|2+|X(th)|2)+a0+2a3(|X(t)|2+|X(th)|2)+a0]ατ[2(2a1τ+a2+a3)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(th)|2+2a4τ|X(δ(t))|2]ατ[2(2a1τ+a2+a3)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(th)|2+4a4τ|X(t)|2+4a4τ|X(t)X(δ(t))|2]ατ[2(2a1τ+a2+a3+2a4τ)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(th)|2+4a4τ|X(t)X(δ(t))|2]. (3.9)

    Under Assumption 3.1, we get from Eqs (3.8) and (3.9) that

    LV(ˆXt,ˆrt,t)b0Q1(X(t))+b1Q1(X(th))+b2+(a44θ+4a4ατ2)|X(t)X(δ(t))|2+ατ[2(2a1τ+a2+a3+2a4τ)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(th)|2]αttτ[τ|f(X(s),X(sh),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(sh),r(s))|2+Rn0|H(X(s),X((sh)),r(s),z)|2ν(dz)]dsbQ1(X(t))+b1Q1(X(th))+b2+(a44θ1+4a4ατ2)|X(t)X(δ(t))|2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)|X(th)|2αttτ[τ|f(X(s),X(sh),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(sh),r(s))|2+Rn0|H(X(s),X((sh)),r(s),z)|2ν(dz)]ds (3.10)

    for tτ, where b=b02ατ(2a1τ+a2+a3+2a4τ)/c1.

    Before proving the key theorem, we need to prove two lemmas, where Lemma 3.1 will prove the uniform boundedness and Lemma 3.2 will prove the exponential convergence.

    Lemma 3.1. Let Assumptions 2.1 and 3.1 hold. If τ>0 is sufficiently small for

    b=b02ατ(2a1τ+a2+a3+2a4τ)/c1>0andτ<115a4, (3.11)

    then the solution of Eq (2.3) with initial data (2.4) satisfies

    EXξ,it2C(1+ξ2) (3.12)

    for all t0, where C is a positive constant.

    Proof. Applying the functional Itˆo formula to eβ0t(V(ˆXt,ˆrt,t)), we can show that

    eβ0tE(V(ˆXt,ˆrt,t))eβ0τE(V(ˆXτ,ˆrτ,τ))=Etτeβ0s(β0V(ˆXs,ˆrs,s)+LV(ˆXs,ˆrs,s))ds,

    for tτ, where β0 is a positive number to be chosen later. Using Eqs (2.5) and (3.7), one can see that

    c1eβ0tE|X(t)|2β1(1+ξ2)Etτeβ0s[β0(Q1(X(s))+ˆV(ˆXs,ˆrs,s))+LV(ˆXs,ˆrs,s)]ds, (3.13)

    where β1 is a positive number. Moreover, we note that

    E(ˆV(ˆXs,ˆrs,s))ατEssτ[τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz)]dv. (3.14)

    Substituting Eqs (3.10) and (3.14) into Eq (3.13), we can obtain

    c1eβ0tE|X(t)|2β1(1+ξ2)tτeβ0sβ0E(Q1(X(s))ds+tτeβ0sβ0ατssτE(τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz))dvds+tτeβ0sELV(ˆXs,ˆrs,s)dstτeβ0sβ0E(Q1(X(s))ds+tτeβ0sβ0ατssτE(τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz))dvds+tτeβ0s[bEQ1(X(s))+b1EQ1(X(sh))+b2+(a44θ1+4a4ατ2)E|X(s)X(δ(s))|2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)E|X(sh)|2αssτE(τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz))dv]ds. (3.15)

    It follows from Eq (2.3) that

    E|X(t)X(δ(t))|2=E|tδ(t)[f(X(s),X(sh),r(s))+A(r(s))X(δ(s))]ds+tδ(t)g(X(s),X(sh),r(s))dB(s)+tδ(t)Rn0H(X(s),X((sh)),r(s),z)˜N(ds,dz)|23τEttτ|f(X(s),X(sh),r(s))+A(r(s))X(δ(s))|2ds+3E|ttτg(X(s),X(sh),r(s))dB(s)|2+3E|ttτRn0H(X(s),X((sh)),r(s),z)˜N(ds,dz)|2. (3.16)

    By Itô isometry,

    E|X(t)X(δ(t))|23τEttτ|f(X(s),X(sh),r(s))+A(r(s))X(δ(s))|2ds+3Ettτ|g(X(s),X(sh),r(s))|2ds+3EttτRn0|H(X(s),X((sh)),r(s),z)|2ν(dx)ds. (3.17)

    Set α=15a44θ1 and τ<115a4, and we have that 3(a44θ1+4a4ατ2)α<0. Then we can find a sufficiently small β0 which satisfies the following condition:

    β0ατ+3(a44θ1+4a4ατ2)α<0,β0b+eβ0hb1+2ατeβ0h(2a1τ+a2+a3)/c1<0. (3.18)

    Using Eqs (3.17) and (3.18), we derive that

    tτeβ0sβ0ατssτE(τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz))dvds+tτeβ0s(a44θ1+4a4ατ2)E|X(s)X(δ(s))|2dstτeβ0s[αssτE(τ|f(X(v),X(vh),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(vh),r(v))|2+Rn0|H(X(v),X((vh)),r(v),z)|2ν(dz))dv]ds<0. (3.19)

    It follows from Eq (3.15) that one gains

    c1eβ0tE|X(t)|2β1(1+ξ2)tτeβ0sβ0E(Q1(X(s))ds+tτeβ0s[bEQ1(X(s))+b1EQ1(X(sh))+b2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)E|X(sh)|2]ds.

    Note that

    tτeβ0s[b1EQ1(X(sh))+2ατ(2a1τ+a2+a3)E|X(sh)|2]ds,eβ0hthτheβ0s[b1EQ1(X(s))+2ατ(2a1τ+a2+a3)E|X(s)|2]ds,eβ0htτeβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]ds,+eβ0hττheβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]ds.

    By condition (3.18), we derive that

    c1eβ0tE|X(t)|2β1(1+ξ2)tτeβ0s(β0b+eβ0hb1+2ατeβ0h(2a1τ+a2+a3)/c1)E(Q1(X(s))ds+tτeβ0s[b2+ατa0(2τ+1)]ds+eβ0hττheβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]dsβ2eβ0t,

    where β2 is a positive number. Hence

    E|X(t)|2β3(1+ξ2),tτ. (3.20)

    After that, we can make an estimate of the segment process Xt. Let tτ+h and θ[0,τ]. According to the Itˆo formula and Eq (2.3), we obtain that

    |X(tθ)|2=|X(tτ)|2+2tθtτXT(s)[f(X(s),X(sh),r(s))+Ar(s)X(δ(s))]ds+2tθtτXT(s)g(X(s),X(sh),r(s))dB(s)+tθtτ|g(X(s),X(sh),r(s))|2ds+tθtτR{0}nk=1[|X(s)+H(k)(X(s),X((sh)),r(s),zk)|2|X(s)|22XT(s)H(k)(X(s),X((sh)),r(s),zk)]νk(dzk)ds+nk=1tθtτR{0}[|X(s)+H(k)(X(s),X((sh)),r(s),zk)|2|X(s)|2]˜N(ds,dzk).

    According to Kunita's inequality ([30], Corollary 2.12, p. 332),

    Esup0θτ|X(tθ)|2c3{Ettτ[|f(X(s),X(sh),r(s))|2+|Ar(s)X(δ(s))|2]ds+E|X(tτ)|2+Ettτ|g(X(s),X(sh),r(s))|2ds+EttτR{0}nk=1|H(k)(X(s),X((sh)),r(s),zk)|2νk(dzk)ds},

    where c3 is a positive constant. It follows from Eqs (2.1) and (2.2) that

    Esup0θτ|X(tθ)|2c4(E|X(tτ)|2+ttτE|X(s)|2ds+ttτE|X(δ(s))|2ds+ttτE|X(sh)|2ds+c5)c4(E|X(tτ)|2+ttτE|X(s)|2ds+ttτE|X(δ(s))|2ds+thtτhE|X(s)|2ds+c5), (3.21)

    where c4 and c5 are positive numbers. By Eqs (3.20) and (3.21), it is easy to show

    EXt2β4(1+ξ2)

    where β4 is a positive number. Together with Eq (2.5), the assertion (3.12) holds. The proof is hence complete.

    Lemma 3.2. Let Assumptions 2.1 and 3.2 hold. If τ>0 is sufficiently small enough for

    ˉb=b3ατ(2a1τ+a2+a3+2a4τ)/c2>0andτ<215a4, (3.22)

    then for any (ξ,ζ,i)Dh×Dh×S,

    EXξ,itXζ,it2α1ξζ2eα2t (3.23)

    for all tτ+h, where α1 and α2 are positive constants.

    Proof. Denote by O(t)=Xξ,i(t)Xζ,i(t) for any (ξ,ζ,i)Dh×Dh×S. Moreover, Ot={O(t+s):τs0} for t0 and ˆOt={O(t+s):τhs0} for tτ+h. Design a new Lyapunov functional ˜V(ˆOt,ˆrt,t):

    ˜V(ˆOt,ˆrt,t):=Φ(Xξ,i(t)Xζ,i(t),r(t))+αttτts[τf(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0H(Xξ,i(v),Xξ,i((vh)),,r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz)]dvds (3.24)

    for tτ. Applying the functional Itˆo formula, we have

    d˜V(ˆOt,ˆrt,t)=L˜V(ˆOt,ˆrt,t)dt+d˜M(t)

    for tτ, where ˜M(t) is a martingale with ˜M(0)=0, and

    L˜V(ˆOt,ˆrt,t)=LΦ(Xξ,i(t),Xζ,i(t),Xξ,i(th),Xζ,i(th),r(t))ΦX(Xξ,i(t),Xζ,i(t),r(t))Ar(t)(O(t)O(δ(t)))+ατ[τf(Xξ,i(t),Xξ,i(th),r(t))f(Xζ,i(t),Xζ,i(th),r(t))+Ar(t)O(δ(t))|2+|g(Xξ,i(t),Xξ,i(th),r(t))g(Xζ,i(t),Xζ,i(th),r(t))|2+Rn0|H(Xξ,i(t),Xξ,i((th)),r(t),z)H(Xζ,i(t),Xζ,i((th)),r(t),z)|2v(dz)]αttτ[τf(Xξ,i(s),Xξ,i(sh),r(s))f(Xζ,i(s),Xζ,i(sh),r(s))+Ar(s)O(δ(s))|2+|g(Xξ,i(s),Xξ,i(sh),r(s))g(Xζ,i(s),Xζ,i(sh),r(s))|2+Rn0H(Xξ,i(s),Xξ,i((sh)),r(s),z)H(Xζ,i(s),Xζ,i((sh)),r(s),z)|2ν(dz)]ds.

    By Assumptions (2.1) and (3.2), we have

    L˜V(ˆOt,ˆrt,t)ˉbQ2(O(t))+b4Q2(O(th))+(a44θ2+2a4ατ2)|O(t)O(δ(t))|2+ατ(2a1τ+a2+a3)|O(th)|2αttτ[τ|f(Xξ,i(s),Xξ,i(sh),r(s))f(Xζ,i(s),Xζ,i(sh),r(s))+Ar(s)O(δ(s))|2+|g(Xξ,i(s),Xξ,i(sh),r(s))g(Xζ,i(s),Xζ,i(sh),r(s))|2+Rn0|H(Xξ,i(s),Xξ,i((sh)),r(s),z)H(Xζ,i(s),Xζ,i((sh)),r(s),z)|2ν(dz)]ds (3.25)

    for tτ, where ˉb=b3ατ(2a1τ+a2+a3+2a4τ)/c2.

    Applying the functional Itˆo formula to eα2tE(˜V(ˆOt,ˆrt,t)), we have

    eα2tE|O(t)|2α4ξζ2τ=eα2tE(˜V(ˆOt,ˆrt,t))eα2τE(˜V(ˆOτ,ˆrτ,τ))=Etτeα2s(α2˜V(ˆOs,ˆrs,s)+L˜V(ˆOs,ˆrs,s))ds, (3.26)

    where α4 is a positive number and α2 is a positive number to be determined. Substituting Eq (3.25) into Eq (3.26) yields

    Etτeα2s(α2˜V(ˆOs,ˆrs,s))ds+Etτeα2sL˜V(ˆOt,ˆrt,t)dsEtτeα2s(α2˜V(ˆOs,ˆrs,s))ds+Etτeα2s[ˉbQ2(O(s))+b4Q2(O(sh))+(a44θ2+2a4ατ2)|O(s)O(δ(s))|2+ατ(2a1τ+a2+a3)|O(sh)|2αttτ(τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz))dv]ds. (3.27)

    Moreover, by Assumption 3.2, one can see that

    E(˜V(ˆOs,ˆrs,s))EQ2(O(s))+Eατssτ[τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz)]dv. (3.28)

    Substituting Eq (3.28) into Eq (3.27), we can get

    Etτeα2s(α2˜V(ˆOs,ˆrs,s))ds+Etτeα2sL˜V(ˆOt,ˆrt,t)dstτeα2s[α2EQ2(O(s))+Eατα2ssτ(τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz))dv]ds+Etτeα2s[ˉbQ2(O(s))+b4Q2(O(sh))+(a44θ2+2a4ατ2)|O(s)O(δ(s))|2+ατ(2a1τ+a2+a3)|O(sh)|2αssτ(τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz))dv]ds.

    Moreover, we can obtain that

    E|O(t)O(δ(t))|2E|tδ(t)[f(Xξ,i(s),Xξ,i(sh),r(s))f(Xζ,i(s),Xζ,i(sh),r(s))+A(r(s))O(δ(s))]ds+tδ(t)[g(Xξ,i(s),Xξ,i(sh),r(s))g(Xζ,i(s),Xζ,i(sh),r(s))]dB(s)+tδ(t)Rn0[H(Xξ,i(s),Xξ,i((sh)),r(s),z)H(Xζ,i(s),Xζ,i((sh)),r(s),z)]˜N(ds,dz)|23τEttτ|f(Xξ,i(s),Xξ,i(sh),r(s))f(Xζ,i(s),Xζ,i(sh),r(s))+A(r(s))O(δ(s))|2ds+3Ettτ|g(Xξ,i(s),Xξ,i(sh),r(s))g(Xζ,i(s),Xζ,i(sh),r(s))|2ds+3EttτRn0|H(Xξ,i(s),Xξ,i((sh)),r(s),z)H(Xζ,i(s),Xζ,i((sh)),r(s),z)|2ν(dz)ds. (3.29)

    Set α=15a44θ2 and τ<215a4, and we have that 3(a44θ2+2a4ατ2)α<0. Then we can find a sufficiently small α2 which satisfies the following condition:

    α2ατ+3(a44θ2+2a4ατ2)α<0,ˉb+α2+eα2hb4+ατeα2h(2a1τ+a2+a3)/c2<0. (3.30)

    By Eq (3.30), we can show that

    tτeα2s[ατα2Essτ[τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz)]dv+(a44θ2+2a4ατ2)E|O(s)O(δ(s))|2αEssτ(τ|f(Xξ,i(v),Xξ,i(vh),r(v))f(Xζ,i(v),Xζ,i(vh),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(vh),r(v))g(Xζ,i(v),Xζ,i(vh),r(v))|2+Rn0|H(Xξ,i(v),Xξ,i((vh)),r(v),z)H(Xζ,i(v),Xζ,i((vh)),r(v),z)|2ν(dz))dv]ds<0.

    Following the condition (3.30), we derive that

    eα2tE|O(t)|2α4ξζ2τeα2tE(˜V(ˆOt,ˆrt,t))eα2τE(˜V(ˆOτ,ˆrτ,τ))=Etτeα2s(α2˜V(ˆOs,ˆrs,s))ds+Etτeα2sL˜V(ˆOt,ˆrt,t)dstτeα2s(α2EQ2(O(s)))ds+Etτeα2s[ˉbQ2(O(s))+(b4+ατ(2a1τ+a2+a3)/c2)Q2(O(sh)]dsEtτeα2s[ˉb+α2+eα2hb4+ατeα2h(2a1τ+a2+a3)/c2)Q2(O(s)]ds+eα2hEττheα2s[b4+ατ(2a1τ+a2+a3)/c2]Q2O(s)dsα5. (3.31)

    This implies that

    E|O(t)|2α3ξζ2τeα2t (3.32)

    for tτ, where α5, α3, and α2 are positive constants. However, for tτ+h, we have that

    sup0θτ|O(tθ)|2c6{E|O(tτ)|2+Ettτ[|f(Xξ,i(s),Xξ,i(sh),r(s))f(Xζ,i(s),Xζ,i(sh),r(s))|2+|Ar(s)O(δ(s))|2]ds+Ettτ|g(Xξ,i(s),Xξ,i(sh),r(s))g(Xζ,i(s),Xζ,i(sh),r(s))|2ds+EttτR{0}nk=1|H(k)(Xξ,i(s),Xξ,i((sh)),r(s),zk)H(k)(Xζ,i(s),Xζ,i((sh)),r(s),zk)|2νk(dzk)ds}. (3.33)

    From Assumption 2.1, one can see that

    sup0θτ|O(tθ)|2c7(E|O(tτ)|2+ttτE|O(s)|2ds+ttτE|O(δ(s))|2ds+ttτE|O(sh)|2ds),

    where c6 and c7 are all positive numbers. By Eq (3.32), we have

    EOt2α1ξζ2eα2t,tτ+h,

    where α1 is a positive number. Therefore, the required assertion (3.23) holds. This completes the proof.

    Next, let us prove that the SDDE-MS-LN (2.3) is stable in distribution by Lemmas 3.1 and 3.2.

    Theorem 3.1. Let Assumptions 2.1 and 3.2 hold. Let τ1,τ2,τ3, and τ4 be the unique positive roots to the following equations

    b0c=15a42θτ1(2a1τ1+a2+a3+2a4τ1),τ2=115a4,b3c=15a44θτ3(2a1τ3+a2+a3+2a4τ3),τ4=215a4, (3.34)

    respectively, and set τ=τ1τ2τ3τ4. Then for each τ<τ and where h can be divisible by τ, there exists a unique probability measure μhP(Dh) such that

    limkdL(L(Xξ,ikτ),μh)=0 (3.35)

    for all (ξ,i)Dh×S.

    Proof. Step 1: We first claim that for any compact set KDh,

    limkdL(L(Xξ,ikτ),L(Xζ,jkτ))=0 (3.36)

    uniformly in (ξ,ζ,i,j)K×K×S×S. Define the sequence of the stopping time κij=inf{kτ:ri(kτ)=rj(kτ),k0}. Using the ergodicity of the Markov chain, we can obtain that κij< a.s. Consequently, for any ε(0,1), there exists a number T1>0 such that

    P(κijT1)>1ε6.

    Recalling a known result that

    sup(ξ,i)K×SE(supτtT1|Xξ,i(t)|)<,

    we can find enough large T2>0 such that

    P(Ωξ,i)>1ε12(ξ,i)K×S,

    where Ωξ,i={ωΩ:supτtT1|Xξ,i(t,ω)|q}. For any ϕL and kτT1, we obtain

    |Eϕ(Xξ,ikτ)Eϕ(Xζ,jkτ)|ε3+ρ(t),

    where ρ(t):=E(I{κijT1}|ϕ(Xξ,ikτ)ϕ(Xζ,jkτ)|). Set Ω1=Ωξ,iΩζ,i{κijT1}. By the Markov property of joint process (Xξ,ikτ,ri(kτ)) and the property of conditional expectation, we derive

    ρ(t)=E(I{κijT1}E(ϕ(Xξ,ikτ)ϕ(Xζ,jkτ)||ϕκij))=E(I{κijT1}×E(|ϕ(X˜ξ,lkτκij)ϕ(X˜ζ,lkτκij)|)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij)ε3+E(IΩ1×E(|ϕ(X˜ξ,lkτκij)ϕ(X˜ζ,lkτκij)|)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij)ε3+E(IΩ1EdS(X˜ξ,lkτκij,X˜ζ,lkτκij)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij).

    It is known (see [31]) that dS(ξ1,ξ2)ξ1ξ2, for any ξ1,ξ2Dh. Using this and the Proposition 1.17 in [32], we derive that

    ρ(t)ε3+E(IΩ1E(X˜ξ,lkτκijX˜ζ,lkτκij)).

    It is easy to observe that ˜ξ˜ζq, for any ωΩ1. By using Lemma 3.2, we are able to find positive number T2 such that

    E(X˜ξ,lkτκijX˜ζ,lkτκijτ)ε3,kτT1+T2

    for any given ωΩ1. Then we have that

    |Eϕ(Xξ,lkτκij)Eϕ(Xζ,lkτκij)|ε,kτT1+T2.

    Due to the arbitrariness of ϕ, for all (ξ,ζ,i,j)K×K×S×S, we get

    dL(L(Xξ,ikτ),L(Xζ,jkτ))ε,kτT1+T2.

    Our claim is proved.

    Step 2: Next, we claim that for any (ξ,i)Dh×S, {L(Xξ,ikτ)}kN+ is a Cauchy sequence in P(Dh) with metric dL. That is, we need to show that for any ε>0, there is a positive number k0 such that

    dL(L(Xξ,i(s+v)τ),L(Xξ,isτ))ε (3.37)

    for all integers sk0 and v1. Let ε(0,1) be arbitrary. By Lemma 3.1, there is a ˉq>0 such that

    P{ωΩ:Xξ,ivτ(ω)ˉq}>1ε/4v1. (3.38)

    For any ϕL and integers s1, we can then derive, using (2.6) and (3.38), that

    |Eϕ(Xξ,i(s+v)τ)Eϕ(Xξ,isτ)|=|jSEϕ(Xζ,jsτ)p(v,ξ,i;dζ×{j})Eϕ(Xξ,isτ)|jS|Eϕ(Xζ,jsτ)Eϕ(Xξ,isτ)|p(v,ξ,i;dζ×{j})ε2+jSZˉqdL(L(Xζ,jsτ),L(Xξ,isτ))p(v,ξ,i;dζ×{j})

    where Zˉq={ζDh:ζˉq}. But, by (3.36), there is a positive integer k0 such that

    dL(L(Xζ,jsτ)),L(Xξ,isτ))ε2sk0

    whenever (ζ,j)Zˉq×S. We, therefore, obtain

    |Eϕ(Xξ,i(s+v)τ)Eϕ(Xξ,isτ)|ε

    for sk0 and v1. As this holds for any ϕL, we must have (3.37) as claimed.

    Step 3: By Eq (3.37), there exists a unique μhP(Dh) such that

    limkdL(L(X0,1kτ),μh)=0,

    which together with Eq (3.36) gains

    limkdL(L(Xξ,ikτ),μh)limkdL((Xξ,ikτ),L(X0,1kτ))+limkdL(L(X0,1kτ),μh)=0

    for all (ξ,i)Dh×S. That is assertion (3.35). The proof is, hence, complete.

    To simplify the calculation and design of matrices, we choose the forms of the function as follows:

    Ψ(x,i)=Φ(x,i)=xTWix

    for some N symmetric positive definite matrices Wi(iS). It follows easily from Eqs (3.1) and (3.3) that

    LΨ(x,ˉx,i)=2xTWi[f(x,ˉx,i)+Ai(x)]+trace[g(x,ˉx,i)TWig(x,ˉx,i)]+R{0}nk=1[(H(k)(x,ˉx,i,zk))TWiH(k)(x,ˉx,i,zk)+(H(k)(x,ˉx,i,zk))TWixxTWiH(k)(x,ˉx,i,zk)]νk(dzk)+Nj=1γijxTWjx,

    and

    LΦ(x,y,ˉx,ˉy,i)=2(xy)TWi[f(x,ˉx,i)f(y,ˉy,i)+Ai(xy)]+trace[(g(x,ˉx,i)g(y,ˉy,i))TWi(g(x,ˉx,i)g(y,ˉy,i))]+R{0}nk=1[(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))T×Wi(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))+(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))TWi(xy)(xy)TWi(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk)]νk(dzk)+Nj=1γij(xy)TWj(xy).

    Assumption 4.1. Let Assumption 2.1 hold. There exist positive numbers j0, b1, j3, b2, b4, j0b1, j3b4, and positive definite matrices Wi such that

    LΨ(x,ˉx,i)j0|x|2+b1|ˉx|2+b2,LΦ(x,y,ˉx,ˉy,i)j3|xy|2+b4|ˉxˉy|2

    for all x, yRd and iS.

    If we set b0=j04ˇc2θ1, b3=j34ˇc2θ2, it reaches the desired conditions (3.4) and (3.5). That is to say, we have shown that Assumption 4.1 implies Assumptions 3.1 and 3.2.

    By Lemmas 3.1, 3.2, and Theorem 3.1, the following corollary therefore follows.

    Corollary 4.1. Let Assumptions 3.1 and 3.2 be replaced by Assumption 4.1. If h can be divisible by τ and is small enough for

    j0c4ˇc2ˉθc2ατ(2a1τ+a2+a3+2a4τ)>0,τ<115a4,j3c4ˇc2ˉθcατ(2a1τ+a2+a3+2a4τ)>0,τ<215a4,

    where ˉθ(0,j0b14ˇc2j3b44ˇc2), c=miniSλminWi, ˇc=maxiSWi, and α=15a44ˉθ. Then the SDDE-MS-LN (2.3) is stable in distribution.

    The key to the problem of stabilization in distribution lies in the design of the matrices Ai(iS). Therefore we need to find the matrices of the form Ai=FiGi with FiRn×l and GiRn×l for some positive integer l. The two cases of state feedback and output injection are discussed below.

    (i) State feedback

    When Gi's are given, we need to seek suitable Fi's to make SDDE-MS-LN (2.3) stable in distribution. The matrices are designed in two steps.

    Step 1: Seek N couples of positive-definite symmetric matrices (Wi,ˆRi,ˆSi) such that

    2(xy)TWi[f(x,ˉx,i)f(y,ˉy,i)]+trace[(g(x,ˉx,i)g(y,ˉy,i))TWi(g(x,ˉx,i)g(y,ˉy,i))]+R{0}nk=1[(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))T×Wi(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))+(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk))TWi(xy)(xy)TWi(H(k)(x,ˉx,i,zk)H(k)(y,ˉy,i,zk)]νk(dzk)(xy)TˆRi(xy)+(ˉxˉy)TˆSi(ˉxˉy), (4.1)

    and then

    LΦ(x,y,ˉx,ˉy,i)(xy)TˆRi(xy)+(ˉxˉy)TˆSi(ˉxˉy)+2(xy)TWiAi(xy)+Nj=1γij(xy)TWj(xy)(xy)T(ˆRi+WiFiGi+GTiFTiWi+Nj=1γijWj)(xy)+(ˉxˉy)TˆSi(ˉxˉy). (4.2)

    Step 2: Seek a solution of matrices F_{i} to the following linear matrix inequalities ensuring that {j}_{3} > {b}_{4} :

    \begin{equation} \hat{R}_{i}+W_{i} F_{i}G_{i} +G_{i}^{T} F_{i}^{T}W_{i}+\sum\limits_{j = 1}^{N} \gamma_{i j} W_{j}+\hat{S}_{i} < 0, \quad i \in \mathbb{S}. \end{equation} (4.3)

    Corollary 4.2. Under Assumption 2.1 , seek matrices F_{i}(i\in\mathbb{S}) with the above Steps 1 and 2. Then Corollary 4.1 holds with A_{i} = F_{i} G_{i} and

    \begin{array}{l} {j}_{3} = -\max _{i \in \mathbb{S}} \lambda_{\max }\left(\hat{R}_{i}+W_{i} F_{i}G_{i} +G_{i}^{T} F_{i}^{T}W_{i}+\sum\limits_{j = 1}^{N} \gamma_{i j} W_{j}\right),\\ {b}_{4} = \max _{i \in \mathbb{S}} \lambda_{\max }\hat{S}_{i}. \end{array}

    (ii) Output injection

    When F_{i} 's are given, we need to seek G_{i} 's. This case is similar to the case of state feedback, and therefore we can get another corollary.

    Corollary 4.3. Under Assumption 2.1 , find matrices W_{i} , \hat{R}_{i} , \hat{S}_{i} , and G_{i}(i\in\mathbb{S}) with the above Steps 1 and 2. Then Corollary 4.1 holds with A_{i} = F_{i} G_{i} , and moreover {j}_{3} and {b}_{4} are the same as in Corollary 4.2 .

    \begin{array}{l} {j}_{3} = -\max _{i \in \mathbb{S}} \lambda_{\max }\left(\hat{R}_{i}+W_{i} F_{i}G_{i} +G_{i}^{T} F_{i}^{T}W_{i}+\sum\limits_{j = 1}^{N} \gamma_{i j} W_{j}\right),\\ {b}_{4} = \max _{i \in \mathbb{S}} \lambda_{\max }\hat{S}_{i}. \end{array}

    In this section, we will give an example to illustrate our results.

    Example 5.1. Let us consider the following unstable SDDE-MS-LN:

    \begin{equation} \begin{aligned} \mathrm{d} X(t) = &\quad f(X(t), X(t-h),r(t)) \mathrm{d} t+g(X(t),X(t-h), r(t)) \mathrm{d} B(t) \\ & + H\left(X(t^{-}), X((t-h)^{-}),r\left(t\right)\right) \mathrm{\; d}\tilde{N}(t) \end{aligned} \end{equation} (5.1)

    with initial value X(0) = 1 , r(0) = 1 , and N(0) = 0 , where the coefficients f, g, and H are defined by

    \begin{array}{cc} f(x, \bar{x},1) = 0.4+0.2x-0.1\bar{x}, \quad f(x, \bar{x},2) = 0.3+0.1x-0.3\bar{x},\\ g(x, \bar{x}, 1) = 0.3+0.2x+0.1\bar{x}, \quad g(x, \bar{x}, 2) = 0.4+0.1x+0.2\bar{x},\\ H\left(x,\bar{x},1\right) = 0.5x+\bar{x}, \quad H\left(x,\bar{x},2\right) = x+0.5\bar{x}, \end{array}

    for all x, \bar{x}\in \mathbb{R} , B(t) is a scalar Brownian motion, N(t) is a scalar Poisson process with intensity \lambda , \tilde{N}(t) denotes its compensated Poisson random measure, r(t) is a Markov chain on the state space \mathbb{S} = \{1, 2\} with its generator

    \Gamma = \left(\begin{array}{cc} -2 & 2 \\ 2 & -2 \end{array}\right) ,

    and the time delay h = 0.01 .

    From Figure 1, we know the SDDE-MS-LN (5.1) is unstable. Let us now apply our new theory to design a linear feedback control to make the SDDE-MS-LN (5.1) stable in distribution. Suppose that the type of linear feedback control is -k(i) X(\delta(t)) , where k(i) will be computed later. Then the controlled system becomes

    \begin{equation} \begin{aligned} d X(t) = \quad &[f(X(t), X(t-h),r(t))-k(r(t)) X(\delta(t))] d t+g(X(t), X(t-h),r(t))d B(t) \\ &+H\left(X(t^{-}), X((t-h)^{-}),r\left(t\right)\right) d \tilde{N}(t). \end{aligned} \end{equation} (5.2)
    Figure 1.  The sample path of SDDE-MS-LN (5.1) with the initial data X(0) = 1 .

    Let W_{i}(i \in 1, 2) be the identity matrix. Set \lambda = 1 . After the calculation, we can get that {b}_{4} = 2.12 . Next, we need to choose a number j_{3} which satisfies j_{3} > {b}_{4} and -j_{3} = -\max _{i \in \mathbb{S}} \left(1.08-2k(i)\right) < 0 for i \in \mathbb{S} . Hence, Corollary 4.1 holds for j_{3} = 6 . Then we can deduce that k(1) = 3.54 and k(2) = 4.26 . It is easy to verify that Assumption 2.1 holds for a_{1} = 0.18 , a_{2} = 0.08 , and a_{3} = 2 . Furthermore, by a_{4} = \max _{i \in \mathbb{S}}\|k(i)\|^{2} , we can get a_{4} = 18.1476 and \check{c} = 1 . Thus, setting c = 1 , \bar{\theta} = 0.1 , we can derive

    \tau_{1}^{*} = 0.00158,\quad \tau_{2}^{*} = 0.0606, \quad\tau_{3}^{*} = 0.00371,\quad \tau_{4}^{*} = 0.0857.

    Consequently, \tau^{*} = 0.00158 . By Corollary 4.1 , the controlled system (5.2) is stable in distribution when \tau < 0.00158 and h can be divisible by \tau .

    In addition, we plot the marginal density function of X(t) by using of the Euler-Maruyama method with step size 0.001 in Figure 2. From the figure, as t increases, the change in distribution becomes smaller and smaller. This show that the controlled system (5.2) is stable in distribution.

    Figure 2.  Distribution numerical solution of the controlled SDDE-MS-LN (5.2).

    In this paper, stabilization in distribution for given unstable SDDEs-MS-LN whose drift and diffusion coefficients are globally Lipshitz continuous has been investigated. We successfully showed that the stability in distribution of controlled SDDE-MS-LN can be achieved by linear feedback controls based on discrete-time state observations. A lower bound on duration \tau^{*} is given so that the controlled SDDEs-MS-LN is stable in distribution as long as \tau < \tau^{*} and h can be divisible by \tau . We specifically discussed how to design the linear feedback control in two structure cases. Finally, a numerical example is illustrated to support our theory. But the system coefficients are still under a linear growth condition, and the stochastic systems are driven by Markovian switching. Hence we will devote our future work to releasing the linear growth condition on f, g [5] and investigating stabilization in distribution for nonlinear stochastic differential delay equations with semi-Markovian switching and Lévy noise (SDDEs-SMS-LN) controlled by discrete feedback controls [33,34].

    Jingjing Yang: Formal analysis, methodology, investigation, resources, software, writing-original draft. Jianqiu Lu: Conceptualization, methodology, supervision, writing-review and editing, funding acquisition.

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

    All authors declare that there are no conflicts of interest.



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