
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(t−h),r(t))dt+g(X(t),X(t−h),r(t))dB(t)+∫Rn0H(X(t−),X((t−h)−),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 t≥0. 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(t−h),r(t))+u(X([t/τ]τ),r(t))]dt+g(X(t),X(t−h),r(t))dB(t)+∫Rn0H(X(t−),X((t−h)−),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 τ≤τ∗. 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}t≥0,P) signifies a complete probability space whose filtration {Ft}t≥0 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,ξ2∈Dh, define the Skorohod metric dS(ξ1,ξ2)=infλ∈Λ{‖λ‖∘∨‖ξ1−ξ2∘λ‖h}, where Λ denotes the class of strictly increasing, continuous mappings of [−h,0] onto itself, ξ2∘λ denotes the composition of two functions ξ2 and λ, ‖λ‖∘=sup−h≤s<t≤0|logλ(t)−λ(s)t−s|, and ‖ξ‖h=sup−h≤s≤0|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), t≥0, 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)=j∣r(t)=i}={γijΔ+o(Δ) if i≠j,1+γijΔ+o(Δ) if i=j, |
where Δ>0 satisfies limΔ→0o(Δ)Δ=0 and γij is the transition rate from i to j satisfying γij>0 if i≠j while γii=−∑i≠jγij. 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×S→Rd, g:Rd×Rd×S→Rd×m, and H:Rd×Rd×S×Rn0→Rd×n are Borel measurable functions, X(t−)=lims↑tX(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), 1≤l≤d, in (1.1), that is
dXl(t)=fl(X(t),X(t−h),r(t))dt+m∑j=1glj(X(t),X(t−h),r(t))dBj(t)+n∑k=1∫R∖{0}Hlk(X(t−),X((t−h)−),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)|2≤a1(|x−y|2+|ˉx−ˉy|2),|g(x,ˉx,i)−g(y,ˉy,i)|2≤a2(|x−y|2+|ˉx−ˉy|2), |
and
n∑k=1∫R∖{0}|H(k)(x,ˉx,i,zk)−H(k)(y,ˉy,i,zk)|2νk(dzk)≤a3(|x−y|2+|ˉx−ˉy|2), |
for all x,ˉx,y,ˉy∈Rd and i∈S.
It is easy to see from Assumption (2.1) that
|f(x,ˉx,i)|2≤2a1(|x|2+|ˉx|2)+a0,|g(x,ˉx,i)|2≤2a2(|x|2+|ˉx|2)+a0 | (2.1) |
and
n∑k=1∫R∖{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 i∈S, where a0=2maxi∈S(|f(0,0,i)|2∨|g(0,0,i)|2)∨∑nk=1∫R∖{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 t≥0. 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)≡Ai∈Rd×d(1≤i≤N), δ(t)=[t/τ]τ. In addition, throughout this paper, we will set a4=maxi∈S‖Ai‖2. The controlled system (1.2) therefore becomes
dX(t)=[f(X(t),X(t−h),r(t))+A(r(t))X(δ(t))]dt+g(X(t),X(t−h),r(t))dB(t)+∫Rn0H(X(t−),X((t−h)−),r(t),z)˜N(dt,dz) | (2.3) |
with the initial data as
{{X(s):−h≤s≤0}=ξ∈Dh,r(0)=i∈S. | (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):−h≤s≤0} for t≥0, 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,it‖2h]<Ct(1+‖ξ‖2h)∀t≥0, | (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 k≥0, 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)=∑j∈J∫Ep(k,ξ,i;dζ×{j}) | (2.6) |
for any E∈B(Dh) and J∈S.
Denote by P(Dh) the family of probability measures on the measurable space (Dh,B(Dh)). For P1,P2∈P(Dh), metric dL is given by
dL(P1,P2)=supϕ∈L|∫Dhϕ(ξ)P1(dξ)−∫Dhϕ(ξ)P2(dξ)|, |
where L={ϕ:Dh→R satisfying |ϕ(ξ)−ϕ(ζ)|≤dS(ξ,ζ) and |ϕ(ξ)|≤1 for ξ,ζ∈Dh}. 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 μh∈P(Dh) such that
limk→∞dL(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 i∈S. Assume that there exists one Ψ∈C2(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}n∑k=1[Ψ(x+H(k)(x,ˉx,i,zk),i)−Ψ(x,i)−Ψx(x,i)H(k)(x,ˉx,i,zk)]νk(dzk)+N∑j=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)∂xi∂xj)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)=ξ−ζ+∫t0[f(Xξ,i(s),Xξ,i(s−h),ri(s))−f(Xζ,i(s),Xζ,i(s−h),ri(s))+A(ri(s))(Xξ,i(δ(t))−Xζ,i(δ(t)))]ds+∫t0[g(Xξ,i(s),Xξ,i(s−h),ri(s))−g(Xζ,i(s),Xζ,i(s−h),ri(s))]dB(s)+∫t0∫Rn0[H(Xξ,i(s−),Xξ,i((s−h)−),ri(s),z)−H(Xζ,i(s−),Xζ,i((s−h)−),ri((s−h)),z)]˜N(ds,dz). | (3.2) |
Let Φ∈C2(Rd×S;R+), and define an operator LΦ:Rd×Rd×Rd×Rd×S→R concerning Eq (3.2) by
LΦ(x,y,ˉx,ˉy,i)=Φx(x−y,i)[f(x,ˉx,i)−f(y,ˉy,i)+Ai(x−y)]+12trace[(g(x,ˉx,i)−g(y,ˉy,i))TΦxx(x−y,i)(g(x,ˉx,i)−g(y,ˉy,i))]+∫R∖{0}n∑k=1[Φ(x−y+H(k)(x,ˉx,i,zk)−H(k)(y,ˉy,i,zk),i)−Φ(x−y,i)−Φx(x−y,i)(H(k)(x,ˉx,i,zk)−H(k)(y,ˉy,i,zk))]νk(dzk)+N∑j=1γijΦ(x−y,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>b1≥0, function Ψ(x,i)∈C2(Rd×S;R+), and Q1(x)∈C(Rd;R+) such that
c1|x|2≤Ψ(x,i)≤Q1(x),LΨ(x,ˉx,i)+θ1|Ψx(x,i)|2≤−b0Q1(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>b4≥0, function Φ(x,i)∈C2(Rd×S;R+), and Q2(x)∈C(Rd;R+) such that
c2|x−y|2≤Φ(x,y,i)≤Q2(x−y),LΦ(x,y,ˉx,ˉy,i)+θ2|Φx(x−y,i)|2≤−b3Q2(x−y)+b4Q2(ˉx−ˉy) | (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):−τ−h≤s≤0} and ˆrt={r(t+s):−τ−h≤s≤0} for t≥τ. Let r(s)=r(0) for −τ−h≤s≤0. Evidently, ˆXt is D([−τ−h,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 t≥h, | (3.6) |
where
ˆV(ˆXt,ˆrt,t)=α∫tt−τ∫ts[τ|f(X(v),f(X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),g(X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),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)|2≤V(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 t≥τ, where M(t) is a martingale with M(0)=0, and
LV(ˆXt,ˆrt,t)=LΨ(X(t),X(t−h),r(t))−ΨX(X(t),r(t))Ar(t)(X(t)−X(δ(t)))+ατ[τ|f(X(t),X(t−h),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(t−h),r(t))|2+∫Rn0|H(X(t−),X((t−h)−),r(t),z)|2ν(dz)]−α∫tt−τ[τ|f(X(s),X(s−h),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(s−h),r(s))|2+∫Rn0|H(X(s−),X((s−h)−),r(s),z)|2ν(dz)]ds≤LΨ(X(t),X(t−h),r(t))+θ1|ΨX(X(t),r(t))|2+14θ1‖Ar(t)‖2|X(t)−X(δ(t))|2+ατ[τ|f(X(t),X(t−h),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(t−h),r(t))|2+∫Rn0|H(X(t−),X((t−h)−),r(t),z)|2ν(dz)]−α∫tt−τ[τ|f(X(s),X(s−h),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(s−h),r(s))|2+∫Rn0|H(X(s−),X((s−h)−),r(s),z)|2ν(dz)]ds. | (3.8) |
By Assumption 2.1, we can derive
ατ[τ|f(X(t),X(t−h),r(t))+Ar(t)X(δ(t))|2+|g(X(t),X(t−h),r(t))|2+∫Rn0|H(X(t−),X((t−h)−),r(t),z)|2ν(dx)]≤ατ[4a1τ(|X(t)|2+|X(t−h)|2)+2a0τ+2a4τ|X(δ(t))|2+2a2(|X(t)|2+|X(t−h)|2)+a0+2a3(|X(t)|2+|X(t−h)|2)+a0]≤ατ[2(2a1τ+a2+a3)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(t−h)|2+2a4τ|X(δ(t))|2]≤ατ[2(2a1τ+a2+a3)|X(t)|2+a0(2τ+1)+2(2a1τ+a2+a3)|X(t−h)|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(t−h)|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(t−h))+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(t−h)|2]−α∫tt−τ[τ|f(X(s),X(s−h),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(s−h),r(s))|2+∫Rn0|H(X(s−),X((s−h)−),r(s),z)|2ν(dz)]ds≤−bQ1(X(t))+b1Q1(X(t−h))+b2+(a44θ1+4a4ατ2)|X(t)−X(δ(t))|2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)|X(t−h)|2−α∫tt−τ[τ|f(X(s),X(s−h),r(s))+Ar(s)X(δ(s))|2+|g(X(s),X(s−h),r(s))|2+∫Rn0|H(X(s−),X((s−h)−),r(s),z)|2ν(dz)]ds | (3.10) |
for t≥τ, where b=b0−2ατ(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=b0−2ατ(2a1τ+a2+a3+2a4τ)/c1>0andτ<1√15a4, | (3.11) |
then the solution of Eq (2.3) with initial data (2.4) satisfies
E‖Xξ,it‖2≤C(1+‖ξ‖2) | (3.12) |
for all t≥0, 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))=E∫tτeβ0s(β0V(ˆXs,ˆrs,s)+LV(ˆXs,ˆrs,s))ds, |
for t≥τ, where β0 is a positive number to be chosen later. Using Eqs (2.5) and (3.7), one can see that
c1eβ0tE|X(t)|2−β1(1+‖ξ‖2)≤E∫tτeβ0s[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))≤ατE∫ss−τ[τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),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)|2−β1(1+‖ξ‖2)≤∫tτeβ0sβ0E(Q1(X(s))ds+∫tτeβ0sβ0ατ∫ss−τE(τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),r(v),z)|2ν(dz))dvds+∫tτeβ0sELV(ˆXs,ˆrs,s)ds≤∫tτeβ0sβ0E(Q1(X(s))ds+∫tτeβ0sβ0ατ∫ss−τE(τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),r(v),z)|2ν(dz))dvds+∫tτeβ0s[−bEQ1(X(s))+b1EQ1(X(s−h))+b2+(a44θ1+4a4ατ2)E|X(s)−X(δ(s))|2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)E|X(s−h)|2−α∫ss−τE(τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),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(s−h),r(s))+A(r(s))X(δ(s))]ds+∫tδ(t)g(X(s),X(s−h),r(s))dB(s)+∫tδ(t)∫Rn0H(X(s−),X((s−h)−),r(s),z)˜N(ds,dz)|2≤3τE∫tt−τ|f(X(s),X(s−h),r(s))+A(r(s))X(δ(s))|2ds+3E|∫tt−τg(X(s),X(s−h),r(s))dB(s)|2+3E|∫tt−τ∫Rn0H(X(s−),X((s−h)−),r(s),z)˜N(ds,dz)|2. | (3.16) |
By Itô isometry,
E|X(t)−X(δ(t))|2≤3τE∫tt−τ|f(X(s),X(s−h),r(s))+A(r(s))X(δ(s))|2ds+3E∫tt−τ|g(X(s),X(s−h),r(s))|2ds+3E∫tt−τ∫Rn0|H(X(s−),X((s−h)−),r(s),z)|2ν(dx)ds. | (3.17) |
Set α=15a44θ1 and τ<1√15a4, 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,β0−b+eβ0hb1+2ατeβ0h(2a1τ+a2+a3)/c1<0. | (3.18) |
Using Eqs (3.17) and (3.18), we derive that
∫tτeβ0sβ0ατ∫ss−τE(τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),r(v),z)|2ν(dz))dvds+∫tτeβ0s(a44θ1+4a4ατ2)E|X(s)−X(δ(s))|2ds−∫tτeβ0s[α∫ss−τE(τ|f(X(v),X(v−h),r(v))+Ar(v)X(δ(v))|2+|g(X(v),X(v−h),r(v))|2+∫Rn0|H(X(v−),X((v−h)−),r(v),z)|2ν(dz))dv]ds<0. | (3.19) |
It follows from Eq (3.15) that one gains
c1eβ0tE|X(t)|2−β1(1+‖ξ‖2)≤∫tτeβ0sβ0E(Q1(X(s))ds+∫tτeβ0s[−bEQ1(X(s))+b1EQ1(X(s−h))+b2+ατa0(2τ+1)+2ατ(2a1τ+a2+a3)E|X(s−h)|2]ds. |
Note that
∫tτeβ0s[b1EQ1(X(s−h))+2ατ(2a1τ+a2+a3)E|X(s−h)|2]ds,≤eβ0h∫t−hτ−heβ0s[b1EQ1(X(s))+2ατ(2a1τ+a2+a3)E|X(s)|2]ds,≤eβ0h∫tτeβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]ds,+eβ0h∫ττ−heβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]ds. |
By condition (3.18), we derive that
c1eβ0tE|X(t)|2−β1(1+‖ξ‖2)≤∫tτeβ0s(β0−b+eβ0hb1+2ατeβ0h(2a1τ+a2+a3)/c1)E(Q1(X(s))ds+∫tτeβ0s[b2+ατa0(2τ+1)]ds+eβ0h∫ττ−heβ0s[(b1+2ατ(2a1τ+a2+a3)/c1)EQ1(X(s))]ds≤β2eβ0t, |
where β2 is a positive number. Hence
E|X(t)|2≤β3(1+‖ξ‖2),t≥τ. | (3.20) |
After that, we can make an estimate of the segment process Xt. Let t≥τ+h and θ∈[0,τ]. According to the Itˆo formula and Eq (2.3), we obtain that
|X(t−θ)|2=|X(t−τ)|2+2∫t−θt−τXT(s)[f(X(s),X(s−h),r(s))+Ar(s)X(δ(s))]ds+2∫t−θt−τXT(s)g(X(s),X(s−h),r(s))dB(s)+∫t−θt−τ|g(X(s),X(s−h),r(s))|2ds+∫t−θt−τ∫R∖{0}n∑k=1[|X(s)+H(k)(X(s−),X((s−h)−),r(s),zk)|2−|X(s)|2−2XT(s)H(k)(X(s−),X((s−h)−),r(s),zk)]νk(dzk)ds+n∑k=1∫t−θt−τ∫R∖{0}[|X(s−)+H(k)(X(s−),X((s−h)−),r(s),zk)|2−|X(s−)|2]˜N(ds,dzk). |
According to Kunita's inequality ([30], Corollary 2.12, p. 332),
Esup0≤θ≤τ|X(t−θ)|2≤c3{E∫tt−τ[|f(X(s),X(s−h),r(s))|2+|Ar(s)X(δ(s))|2]ds+E|X(t−τ)|2+E∫tt−τ|g(X(s),X(s−h),r(s))|2ds+E∫tt−τ∫R∖{0}n∑k=1|H(k)(X(s−),X((s−h)−),r(s),zk)|2νk(dzk)ds}, |
where c3 is a positive constant. It follows from Eqs (2.1) and (2.2) that
Esup0≤θ≤τ|X(t−θ)|2≤c4(E|X(t−τ)|2+∫tt−τE|X(s)|2ds+∫tt−τE|X(δ(s))|2ds+∫tt−τE|X(s−h)|2ds+c5)≤c4(E|X(t−τ)|2+∫tt−τE|X(s)|2ds+∫tt−τE|X(δ(s))|2ds+∫t−ht−τ−hE|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
E‖Xt‖2≤β4(1+‖ξ‖2) |
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=b3−ατ(2a1τ+a2+a3+2a4τ)/c2>0andτ<√215a4, | (3.22) |
then for any (ξ,ζ,i)∈Dh×Dh×S,
E‖Xξ,it−Xζ,it‖2≤α1‖ξ−ζ‖2e−α2t | (3.23) |
for all t≥τ+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):−τ≤s≤0} for t≥0 and ˆOt={O(t+s):−τ−h≤s≤0} for t≥τ+h. Design a new Lyapunov functional ˜V(ˆOt,ˆrt,t):
˜V(ˆOt,ˆrt,t):=Φ(Xξ,i(t)−Xζ,i(t),r(t))+α∫tt−τ∫ts[τ∣f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0∣H(Xξ,i(v−),Xξ,i((v−h)−),,r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz)]dvds | (3.24) |
for t≥τ. Applying the functional Itˆo formula, we have
d˜V(ˆOt,ˆrt,t)=L˜V(ˆOt,ˆrt,t)dt+d˜M(t) |
for t≥τ, 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(t−h),Xζ,i(t−h),r(t))−ΦX(Xξ,i(t),Xζ,i(t),r(t))Ar(t)(O(t)−O(δ(t)))+ατ[τ∣f(Xξ,i(t),Xξ,i(t−h),r(t))−f(Xζ,i(t),Xζ,i(t−h),r(t))+Ar(t)O(δ(t))|2+|g(Xξ,i(t),Xξ,i(t−h),r(t))−g(Xζ,i(t),Xζ,i(t−h),r(t))|2+∫Rn0|H(Xξ,i(t−),Xξ,i((t−h)−),r(t),z)−H(Xζ,i(t−),Xζ,i((t−h)−),r(t),z)|2v(dz)]−α∫tt−τ[τ∣f(Xξ,i(s),Xξ,i(s−h),r(s))−f(Xζ,i(s),Xζ,i(s−h),r(s))+Ar(s)O(δ(s))|2+|g(Xξ,i(s),Xξ,i(s−h),r(s))−g(Xζ,i(s),Xζ,i(s−h),r(s))|2+∫Rn0∣H(Xξ,i(s−),Xξ,i((s−h)−),r(s),z)−H(Xζ,i(s−),Xζ,i((s−h)−),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(t−h))+(a44θ2+2a4ατ2)|O(t)−O(δ(t))|2+ατ(2a1τ+a2+a3)|O(t−h)|2−α∫tt−τ[τ|f(Xξ,i(s),Xξ,i(s−h),r(s))−f(Xζ,i(s),Xζ,i(s−h),r(s))+Ar(s)O(δ(s))|2+|g(Xξ,i(s),Xξ,i(s−h),r(s))−g(Xζ,i(s),Xζ,i(s−h),r(s))|2+∫Rn0|H(Xξ,i(s−),Xξ,i((s−h)−),r(s),z)−H(Xζ,i(s−),Xζ,i((s−h)−),r(s),z)|2ν(dz)]ds | (3.25) |
for t≥τ, where ˉb=b3−ατ(2a1τ+a2+a3+2a4τ)/c2.
Applying the functional Itˆo formula to eα2tE(˜V(ˆOt,ˆrt,t)), we have
eα2tE|O(t)|2−α4‖ξ−ζ‖2τ=eα2tE(˜V(ˆOt,ˆrt,t))−eα2τE(˜V(ˆOτ,ˆrτ,τ))=E∫tτeα2s(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
E∫tτeα2s(α2˜V(ˆOs,ˆrs,s))ds+E∫tτeα2sL˜V(ˆOt,ˆrt,t)ds≤E∫tτeα2s(α2˜V(ˆOs,ˆrs,s))ds+E∫tτeα2s[−ˉbQ2(O(s))+b4Q2(O(s−h))+(a44θ2+2a4ατ2)|O(s)−O(δ(s))|2+ατ(2a1τ+a2+a3)|O(s−h)|2−α∫tt−τ(τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),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))+Eατ∫ss−τ[τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz)]dv. | (3.28) |
Substituting Eq (3.28) into Eq (3.27), we can get
E∫tτeα2s(α2˜V(ˆOs,ˆrs,s))ds+E∫tτeα2sL˜V(ˆOt,ˆrt,t)ds≤∫tτeα2s[α2EQ2(O(s))+Eατα2∫ss−τ(τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz))dv]ds+E∫tτeα2s[−ˉbQ2(O(s))+b4Q2(O(s−h))+(a44θ2+2a4ατ2)|O(s)−O(δ(s))|2+ατ(2a1τ+a2+a3)|O(s−h)|2−α∫ss−τ(τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz))dv]ds. |
Moreover, we can obtain that
E|O(t)−O(δ(t))|2≤E|∫tδ(t)[f(Xξ,i(s),Xξ,i(s−h),r(s))−f(Xζ,i(s),Xζ,i(s−h),r(s))+A(r(s))O(δ(s))]ds+∫tδ(t)[g(Xξ,i(s),Xξ,i(s−h),r(s))−g(Xζ,i(s),Xζ,i(s−h),r(s))]dB(s)+∫tδ(t)∫Rn0[H(Xξ,i(s−),Xξ,i((s−h)−),r(s),z)−H(Xζ,i(s−),Xζ,i((s−h)−),r(s),z)]˜N(ds,dz)|2≤3τE∫tt−τ|f(Xξ,i(s),Xξ,i(s−h),r(s))−f(Xζ,i(s),Xζ,i(s−h),r(s))+A(r(s))O(δ(s))|2ds+3E∫tt−τ|g(Xξ,i(s),Xξ,i(s−h),r(s))−g(Xζ,i(s),Xζ,i(s−h),r(s))|2ds+3E∫tt−τ∫Rn0|H(Xξ,i(s−),Xξ,i((s−h)−),r(s),z)−H(Xζ,i(s−),Xζ,i((s−h)−),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[ατα2E∫ss−τ[τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz)]dv+(a44θ2+2a4ατ2)E|O(s)−O(δ(s))|2−αE∫ss−τ(τ|f(Xξ,i(v),Xξ,i(v−h),r(v))−f(Xζ,i(v),Xζ,i(v−h),r(v))+Ar(v)O(δ(v))|2+|g(Xξ,i(v),Xξ,i(v−h),r(v))−g(Xζ,i(v),Xζ,i(v−h),r(v))|2+∫Rn0|H(Xξ,i(v−),Xξ,i((v−h)−),r(v),z)−H(Xζ,i(v−),Xζ,i((v−h)−),r(v),z)|2ν(dz))dv]ds<0. |
Following the condition (3.30), we derive that
eα2tE|O(t)|2−α4‖ξ−ζ‖2τ≤eα2tE(˜V(ˆOt,ˆrt,t))−eα2τE(˜V(ˆOτ,ˆrτ,τ))=E∫tτeα2s(α2˜V(ˆOs,ˆrs,s))ds+E∫tτeα2sL˜V(ˆOt,ˆrt,t)ds≤∫tτeα2s(α2EQ2(O(s)))ds+E∫tτeα2s[−ˉbQ2(O(s))+(b4+ατ(2a1τ+a2+a3)/c2)Q2(O(s−h)]ds≤E∫tτeα2s[−ˉb+α2+eα2hb4+ατeα2h(2a1τ+a2+a3)/c2)Q2(O(s)]ds+eα2hE∫ττ−heα2s[b4+ατ(2a1τ+a2+a3)/c2]Q2O(s)ds≤α5. | (3.31) |
This implies that
E|O(t)|2≤α3‖ξ−ζ‖2τe−α2t | (3.32) |
for t≥τ, where α5, α3, and α2 are positive constants. However, for t≥τ+h, we have that
sup0≤θ≤τ|O(t−θ)|2≤c6{E|O(t−τ)|2+E∫tt−τ[|f(Xξ,i(s),Xξ,i(s−h),r(s))−f(Xζ,i(s),Xζ,i(s−h),r(s))|2+|Ar(s)O(δ(s))|2]ds+E∫tt−τ|g(Xξ,i(s),Xξ,i(s−h),r(s))−g(Xζ,i(s),Xζ,i(s−h),r(s))|2ds+E∫tt−τ∫R∖{0}n∑k=1|H(k)(Xξ,i(s−),Xξ,i((s−h)−),r(s),zk)−H(k)(Xζ,i(s−),Xζ,i((s−h)−),r(s),zk)|2νk(dzk)ds}. | (3.33) |
From Assumption 2.1, one can see that
sup0≤θ≤τ|O(t−θ)|2≤c7(E|O(t−τ)|2+∫tt−τE|O(s)|2ds+∫tt−τE|O(δ(s))|2ds+∫tt−τE|O(s−h)|2ds), |
where c6 and c7 are all positive numbers. By Eq (3.32), we have
E‖Ot‖2≤α1‖ξ−ζ‖2e−α2t,∀t≥τ+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 τ∗1,τ∗2,τ∗3, and τ∗4 be the unique positive roots to the following equations
b0c=15a42θτ∗1(2a1τ∗1+a2+a3+2a4τ∗1),τ∗2=1√15a4,b3c=15a44θτ∗3(2a1τ∗3+a2+a3+2a4τ∗3),τ∗4=√215a4, | (3.34) |
respectively, and set τ∗=τ∗1∧τ∗2∧τ∗3∧τ∗4. Then for each τ<τ∗ and where h can be divisible by τ, there exists a unique probability measure μh∈P(Dh) such that
limk→∞dL(L(Xξ,ikτ),μh)=0 | (3.35) |
for all (ξ,i)∈Dh×S.
Proof. Step 1: We first claim that for any compact set K⊂Dh,
limk→∞dL(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),k≥0}. 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(κij≤T1)>1−ε6. |
Recalling a known result that
sup(ξ,i)∈K×SE(sup−τ≤t≤T1|Xξ,i(t)|)<∞, |
we can find enough large T2>0 such that
P(Ωξ,i)>1−ε12∀(ξ,i)∈K×S, |
where Ωξ,i={ω∈Ω:sup−τ≤t≤T1|Xξ,i(t,ω)|≤q}. For any ϕ∈L and kτ≥T1, we obtain
|Eϕ(Xξ,ikτ)−Eϕ(Xζ,jkτ)|≤ε3+ρ(t), |
where ρ(t):=E(I{κij≤T1}|ϕ(Xξ,ikτ)−ϕ(Xζ,jkτ)|). Set Ω1=Ωξ,i∩Ωζ,i∩{κij≤T1}. By the Markov property of joint process (Xξ,ikτ,ri(kτ)) and the property of conditional expectation, we derive
ρ(t)=E(I{κij≤T1}E(∣ϕ(Xξ,ikτ)−ϕ(Xζ,jkτ)||ϕκij))=E(I{κij≤T1}×E(|ϕ(X˜ξ,lkτ−κij)−ϕ(X˜ζ,lkτ−κij)|)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij)≤ε3+E(IΩ1×E(|ϕ(X˜ξ,lkτ−κij)−ϕ(X˜ζ,lkτ−κij)|)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij)≤ε3+E(IΩ1EdS(X˜ξ,lkτ−κij,X˜ζ,lkτ−κij)|˜ξ=Xξ,iκij,˜ζ=Xζ,jκij,l=qiκij=qjκij). |
It is known (see [31]) that dS(ξ1,ξ2)≤‖ξ1−ξ2‖, for any ξ1,ξ2∈Dh. Using this and the Proposition 1.17 in [32], we derive that
ρ(t)≤ε3+E(IΩ1E(‖X˜ξ,lkτ−κij−X˜ζ,lkτ−κij‖)). |
It is easy to observe that ‖˜ξ‖∨‖˜ζ‖≤q, for any ω∈Ω1. By using Lemma 3.2, we are able to find positive number T2 such that
E(‖X˜ξ,lkτ−κij−X˜ζ,lkτ−κij‖τ)≤ε3,∀kτ≥T1+T2 |
for any given ω∈Ω1. Then we have that
|Eϕ(Xξ,lkτ−κij)−Eϕ(Xζ,lkτ−κij)|≤ε,∀kτ≥T1+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,∀kτ≥T1+T2. |
Our claim is proved.
Step 2: Next, we claim that for any (ξ,i)∈Dh×S, {L(Xξ,ikτ)}k∈N+ 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 s≥k0 and v≥1. Let ε∈(0,1) be arbitrary. By Lemma 3.1, there is a ˉq>0 such that
P{ω∈Ω:‖Xξ,ivτ(ω)‖≤ˉq}>1−ε/4∀v≥1. | (3.38) |
For any ϕ∈L and integers s≥1, we can then derive, using (2.6) and (3.38), that
|Eϕ(Xξ,i(s+v)τ)−Eϕ(Xξ,isτ)|=|∑j∈S∫Eϕ(Xζ,jsτ)p(v,ξ,i;dζ×{j})−Eϕ(Xξ,isτ)|≤∑j∈S∫|Eϕ(Xζ,jsτ)−Eϕ(Xξ,isτ)|p(v,ξ,i;dζ×{j})≤ε2+∑j∈S∫ZˉqdL(L(Xζ,jsτ),L(Xξ,isτ))p(v,ξ,i;dζ×{j}) |
where Zˉq={ζ∈Dh:‖ζ‖≤ˉq}. But, by (3.36), there is a positive integer k0 such that
dL(L(Xζ,jsτ)),L(Xξ,isτ))≤ε2∀s≥k0 |
whenever (ζ,j)∈Zˉq×S. We, therefore, obtain
|Eϕ(Xξ,i(s+v)τ)−Eϕ(Xξ,isτ)|≤ε |
for s≥k0 and v≥1. As this holds for any ϕ∈L, we must have (3.37) as claimed.
Step 3: By Eq (3.37), there exists a unique μh∈P(Dh) such that
limk→∞dL(L(X0,1kτ),μh)=0, |
which together with Eq (3.36) gains
limk→∞dL(L(Xξ,ikτ),μh)≤limk→∞dL((Xξ,ikτ),L(X0,1kτ))+limk→∞dL(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(i∈S). 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}n∑k=1[(H(k)(x,ˉx,i,zk))TWiH(k)(x,ˉx,i,zk)+(H(k)(x,ˉx,i,zk))TWix−xTWiH(k)(x,ˉx,i,zk)]νk(dzk)+N∑j=1γijxTWjx, |
and
LΦ(x,y,ˉx,ˉy,i)=2(x−y)TWi[f(x,ˉx,i)−f(y,ˉy,i)+Ai(x−y)]+trace[(g(x,ˉx,i)−g(y,ˉy,i))TWi(g(x,ˉx,i)−g(y,ˉy,i))]+∫R∖{0}n∑k=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(x−y)−(x−y)TWi(H(k)(x,ˉx,i,zk)−H(k)(y,ˉy,i,zk)]νk(dzk)+N∑j=1γij(x−y)TWj(x−y). |
Assumption 4.1. Let Assumption 2.1 hold. There exist positive numbers j0, b1, j3, b2, b4, j0≥b1, j3≥b4, 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|x−y|2+b4|ˉx−ˉy|2 |
for all x, y∈Rd and i∈S.
If we set b0=j0−4ˇc2θ1, b3=j3−4ˇc2θ2, 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
j0c−4ˇc2ˉθc−2ατ(2a1τ+a2+a3+2a4τ)>0,τ<1√15a4,j3c−4ˇc2ˉθc−ατ(2a1τ+a2+a3+2a4τ)>0,τ<√215a4, |
where ˉθ∈(0,j0−b14ˇc2∧j3−b44ˇc2), c=mini∈SλminWi, ˇc=maxi∈S‖Wi‖, 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(i∈S). Therefore we need to find the matrices of the form Ai=FiGi with Fi∈Rn×l and Gi∈Rn×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(x−y)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}n∑k=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(x−y)−(x−y)TWi(H(k)(x,ˉx,i,zk)−H(k)(y,ˉy,i,zk)]νk(dzk)≤(x−y)TˆRi(x−y)+(ˉx−ˉy)TˆSi(ˉx−ˉy), | (4.1) |
and then
LΦ(x,y,ˉx,ˉy,i)≤(x−y)TˆRi(x−y)+(ˉx−ˉy)TˆSi(ˉx−ˉy)+2(x−y)TWiAi(x−y)+N∑j=1γij(x−y)TWj(x−y)≤(x−y)T(ˆRi+WiFiGi+GTiFTiWi+N∑j=1γijWj)(x−y)+(ˉx−ˉy)TˆSi(ˉx−ˉy). | (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) |
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.
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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