
For a hybrid stochastic system, most existing feedback controllers need to observe modes at continuous times, which is feasible when the system's mode is observable and does not incur any cost. However, in most cases, the mode is not readily apparent, and identifying it always incurs a certain expense. Therefore, in order to reduce control costs, when designing a feedback controller, both the state and the mode should be observed at discrete moments. This paper introduces an intermittent feedback controller for stabilizing an unstable hybrid stochastic system through discrete delayed observations of state and mode. By utilizing M-matrix theory, intermittent control approach, and the comparison principle, we propose sufficient conditions for the stabilization theory of hybrid stochastic systems. An illustrative example is taken to validate the proposed theory.
Citation: Lichao Feng, Dongxue Li, Chunyan Zhang, Yanmei Yang. Note on control for hybrid stochastic systems by intermittent feedback rooted in discrete observations of state and mode with delays[J]. Electronic Research Archive, 2024, 32(1): 17-40. doi: 10.3934/era.2024002
[1] | Ramalingam Sakthivel, Palanisamy Selvaraj, Oh-Min Kwon, Seong-Gon Choi, Rathinasamy Sakthivel . Robust memory control design for semi-Markovian jump systems with cyber attacks. Electronic Research Archive, 2023, 31(12): 7496-7510. doi: 10.3934/era.2023378 |
[2] | Huan Luo . Heterogeneous anti-synchronization of stochastic complex dynamical networks involving uncertain dynamics: an approach of the space-time discretizations. Electronic Research Archive, 2025, 33(2): 613-641. doi: 10.3934/era.2025029 |
[3] | Yang Song, Beiyan Yang, Jimin Wang . Stability analysis and security control of nonlinear singular semi-Markov jump systems. Electronic Research Archive, 2025, 33(1): 1-25. doi: 10.3934/era.2025001 |
[4] | Sida Lin, Dongyao Yang, Jinlong Yuan, Changzhi Wu, Tao Zhou, An Li, Chuanye Gu, Jun Xie, Kuikui Gao . A new computational method for sparse optimal control of cyber-physical systems with varying delay. Electronic Research Archive, 2024, 32(12): 6553-6577. doi: 10.3934/era.2024306 |
[5] | Lingling Zhang . Vibration analysis and multi-state feedback control of maglev vehicle-guideway coupling system. Electronic Research Archive, 2022, 30(10): 3887-3901. doi: 10.3934/era.2022198 |
[6] | Zhizhou Zhang, Yueliang Pan, Weilong Zhao, Jinchu Zhang, Zheng Zi, Yuan Xie, Hehong Zhang . Frequency analysis of a discrete-time fast nonlinear tracking differentiator algorithm based on isochronic region method. Electronic Research Archive, 2024, 32(9): 5157-5175. doi: 10.3934/era.2024238 |
[7] | Meiyu Sui, Yejuan Wang, Peter E. Kloeden . Pullback attractors for stochastic recurrent neural networks with discrete and distributed delays. Electronic Research Archive, 2021, 29(2): 2187-2221. doi: 10.3934/era.2020112 |
[8] | Xinling Li, Xueli Qin, Zhiwei Wan, Weipeng Tai . Chaos synchronization of stochastic time-delay Lur'e systems: An asynchronous and adaptive event-triggered control approach. Electronic Research Archive, 2023, 31(9): 5589-5608. doi: 10.3934/era.2023284 |
[9] | Fang Yan, Changyong Dai, Haihong Liu . Oscillatory dynamics of p53 pathway in etoposide sensitive and resistant cell lines. Electronic Research Archive, 2022, 30(6): 2075-2108. doi: 10.3934/era.2022105 |
[10] | Yilin Li, Jianwen Feng, Jingyi Wang . Mean square synchronization for stochastic delayed neural networks via pinning impulsive control. Electronic Research Archive, 2022, 30(9): 3172-3192. doi: 10.3934/era.2022161 |
For a hybrid stochastic system, most existing feedback controllers need to observe modes at continuous times, which is feasible when the system's mode is observable and does not incur any cost. However, in most cases, the mode is not readily apparent, and identifying it always incurs a certain expense. Therefore, in order to reduce control costs, when designing a feedback controller, both the state and the mode should be observed at discrete moments. This paper introduces an intermittent feedback controller for stabilizing an unstable hybrid stochastic system through discrete delayed observations of state and mode. By utilizing M-matrix theory, intermittent control approach, and the comparison principle, we propose sufficient conditions for the stabilization theory of hybrid stochastic systems. An illustrative example is taken to validate the proposed theory.
Stochastic systems have occupied significant positions in diverse fields. Hybrid stochastic differential equations (SDEs) are an important class of stochastic systems, which can effectively describe sudden changes in structures and parameters. Therefore, many scholars have conducted research on hybrid SDEs.
In the study of hybrid SDEs, stability analysis is one of the important research topics [1,2,3,4,5,6,7,8]. Feedback control is referred to as an important approach to ensure the stability of stochastic systems. However, conventional feedback controllers are rooted in the continuous observations of the system's states. Due to practical limitations, data can only be observed at discrete moments, even if the underlying system is continuous. To address this issue and reduce control costs, Mao [9] proposed a feedback control approach for stabilizing a hybrid SDE through discrete-time state observations. Unlike continuous-time controllers, feedback controllers rooted in discrete-time state observations have significant advantages in terms of accuracy and cost. Therefore, discrete-time control strategies [10,11,12,13,14,15,16,17] have been widely studied. Moreover, a delay is frequently present between the state observed moment and its actual time. Thus, delayed feedback control strategy [18,19,20,21,22,23,24,25,26,27] has also received extensive attention. Therein, Zhu et al. [22] considered both discrete and time-delay issues in designing the controller. They studied exponential stabilization for hybrid SDEs through feedback control rooted in delayed and discrete observations of the state. In addition, Li et al. [26] developed a delayed feedback controller for stabilizing the switching diffusion system by discrete observations of state and mode.
Moreover, intermittent control strategy has attracted extensive attention from scholars [28,29,30,31,32,33,34,35], particularly been applied in multiagent systems [32,33], complex networks [34] and other fields. Intermittent control splits time into work and rest periods. The controller switches on during the work period and turns off during the rest period, effectively switching the controlled system between closed-loop and open-loop modes. Compared to classical continuous control strategies, intermittent control strategy is more easily acceptable, which can reduce controller wear, extend the controller's lifespan, and lower costs.
To enhance control performance, a growing number of scholars have used hybrid control strategies, which involves the simultaneous use of multiple control strategies. In particular, Jiang et al. [35] considered discrete delayed observations of state and intermittent control method to design the controller. Inspired by these aforementioned works, this paper employs a hybrid control strategy to achieve stabilization, which involves discrete, time-delayed and intermittent components in controller design. Particularly, in this paper, not only the state but also the mode is observed at discrete times. When designing a controller, if the mode is readily apparent (meaning it can be observed without any cost), it can be observed in continuous time. For instance, within a financial system where the mode is referred to as interest rate, this is entirely feasible. However, in most cases, the mode is not evident, and identifying it incurs costs. To lower control expenses, observations pertaining to the state and mode should occur at discrete times. Therefore, our aim is to develop an intermittent feedback controller, rooted in discrete delayed observations related to state and mode, to stabilize an unstable hybrid SDE.
Consider a complete probability space (Ω,F,{Fμ}μ≥0,P) satisfying the usual conditions. Let w(μ)=(w1(μ)⋯wI(μ))T be an I dimensional Brownian motion defined on the aforementioned probability space. In this probability space, consider a continuous-time Markov chain Γ:R+→S={1,2,⋯N}, whose generator Λ=(γuv)N×N is provided by
P(Γ(μ+Δ)=v|Γ(μ)=u)={γuvΔ+o(Δ)u≠v,1+γuvΔ+o(Δ)u=v, |
in which Δ>0, γuv represents the rate of transition from state u to state v, and γuu=−∑v≠uγuv. Let w(μ) be independent of Γ(μ).
Let υ0 be a positive number, C([−υ0,0],Rn) represent the family of continuous real-valued functions ξ:[−υ0,0]→Rn with ||ξ||=sup−υ0≤θ≤0|ξ(θ)|. LpFμ([−υ0,0];Rn) denotes the family of all Fμ measurable C([−υ0,0],Rn) valued random variables γ={γ(θ):−υ0≤θ≤0} with E||γ||p<∞, where E represents the expectation for probability P.
Consider an unstable hybrid SDE
dη(μ)=h(η(μ),Γ(μ),μ)dμ+k(η(μ),Γ(μ),μ)dw(μ), | (2.1) |
on μ≥0 along with initial data η(0)=η0≠0 and Γ(0)=Γ0, where h:Rn×S×R+→Rn and k:Rn×S×R+→Rn×I. For system (2.1), our objective is to develop a discrete controller ϖ:Rn×S×R→Rn with a time delay υ0 in the drift term to achieve stabilization. Additionally, an intermittent control strategy is incorporated. Thus, the controlled system is as follows:
dλ(μ)=(h(λ(μ),Γ(μ),μ)+ϖ(λ(δμ),Γ(δμ),μ)I(μ))dμ+k(λ(μ),Γ(μ),μ)dw(μ), | (2.2) |
in which δμ=[μ/υ]υ−υ0, υ>0 is the duration separating two consecutive discrete observations, [μ/υ] represents the integer part of μ/υ, and I(μ)=∑∞l=0I[μl,μl+φΔ](μ), μl=lΔ, l=0,1,2,⋯, Δ>0 represents the control period, φ∈[0,1] represents the control width, and I[μl,μl+1](μ)={1,μ∈[μl,μl+φΔ)0,μ∈[μl+φΔ,μl+1). Namely, the controller will switch on during [0,φΔ), [Δ,(1+φ)Δ), [2Δ,(2+φ)Δ),⋯, switch off during [φΔ,Δ), [(1+φ)Δ,2Δ),[(2+φ)Δ,3Δ),⋯.
The original system (2.1) has initial data only at μ=0, while the controlled system (2.2) requires initial data
{λ(θ):−υ0≤θ≤0}=ξ∈C([−υ0,0];Rn),{Γ(θ):−υ0≤θ≤0}=ς∈S. | (2.3) |
To address this issue, set λ(θ)=η(0), Γ(θ)=Γ(0), θ∈[−υ0,0].
To study the properties of system (2.2), we introduce the auxiliary system as follows:
dσ(μ)=(h(σ(μ),Γ(μ),μ)+ϖ(σ(μ),Γ(μ),μ)I(μ))dμ+k(σ(μ),Γ(μ),μ)dw(μ) | (2.4) |
The system (2.4) is continuous and has no delay term with initial values σ(0)=σ0=η0≠0 and Γ(0)=Γ0.
Assumption 1. There are three positive constants K1, K2 and K3 such that
|h(λ,u,μ)−h(σ,u,μ)|≤K1|λ−σ|, |
|ϖ(λ,u,μ)−ϖ(σ,u,μ)|≤K2|λ−σ|, |
|k(λ,u,μ)−k(σ,u,μ)|≤K3|λ−σ|, |
for ∀(λ,σ,u,μ)∈Rn×Rn×S×R+. Additionally,
h(0,u,μ)=0,ϖ(0,u,μ)=0,k(0,u,μ)=0, |
for ∀(u,μ)∈S×R+.
This assumption implies the linear growth condition
|h(λ,u,μ)|≤K1|λ|,|ϖ(λ,u,μ)|≤K2|λ|,|k(λ,u,μ)|≤K3|λ|, | (2.5) |
for ∀(λ,u,μ)∈Rn×S×R+.
Remark 1: Under Assumption 1, from the reference [3], it can be inferred that the system (2.2) has a unique solution λ(μ;ξ,ς,0) on μ≥0 and
E|λ(μ;ξ,ς,0)|p<∞,μ≥0,p>0. |
Similarly, under Assumption 1, the auxiliary system (2.4) also has a unique solution denoted by σ(μ;σ0,Γ0,0) for μ≥0.
Remark 2: Under Assumption 1, here we emphasize the important property from Lemma 2.1 of [1], for ∀σ0≠0, P{σ(μ;σ0,Γ0,0)≠0:μ≥0}=1. Specifically speaking, when any initial data of system (2.4) is nonzero, almost all trajectories will never reach the origin.
Assumption 2. There exist m>0, non-negative numbers τu, βu and cu, u∈S, satisfying
λTϖ(λ,u,μ)≤−τu|λ|2, |
and
1|λ|2(λTh(λ,u,μ)+12|k(λ,u,μ)|2)−2−m2|λ|4|λTk(λ,u,μ)|2≤βu, |
for ∀(λ,u,μ)∈(Rn−{0})×S×R+, and βu−τu≤−cu.
Assumption 3. Let m be a positive constant, and N×N matrix
A(m)=diag(α1(m),α2(m)⋯αN(m))−Λ, | (2.6) |
be a non-singular M-matrix, in which αu(m)=cum.
Define
(b1,⋯bN)T=A−1(m)(1,⋯,1)TN, | (2.7) |
and let
bmin=minu∈Sbu,bmax=maxu∈Sbu,M=bmaxbmin,,χ=maxu∈S(βu+cu). | (2.8) |
Theorem 1. For a free parameter ε∈(0,1), let Θ=1χ1log22m3bmaxbminε>0, and υ∗>0 be the unique root of Eq (2.9) with respect to υ0≥0,
ε(1+K2υ0)m2eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4(m,υ0,Θ)+L3(m,υ0,υ0+Θ))=1, | (2.9) |
where χ1=−(mχ−1bmax−mχφ), m>0, m1=2∨m, m3=0∨(m−1),
L3(m,υ0,Θ)={{3(1+K2υ0)e(Θ+υ0)2(K1+0.5K32+K2)×[υ02(K12+K22)+4υ0K32]}m2,m∈(0,2),3m−1(1+K2υ0)e(Θ+υ0)m(K1+12(m−1)K32+K2)×[υ0m(K1m+K2m)+(m32(m−1))m2×υ0m2K3m,m∈[2,∞). |
L4(m,υ0,Θ)={{32(Θ+υ0)2K22[L3(2,υ0,Θ)+4(1−e−ˆγυ)NL1(2,υ0,Θ)]×e3[K12+(Θ+υ0)−1K32+3K22](Θ+υ0)2}m2,m∈(0,2),32m−2(Θ+υ0)mK2m[L3(m,υ0,Θ)+2m(1−e−ˆγυ)NL1(m,υ0,Θ)]×e3m−1[K1m+(m(m−1)2)m2(Θ+υ0)−m2K3m+3m−1K2m](Θ+υ0)m,m∈[2,∞). |
Under Assumptions 1–3, let N+ be a positive integer, for ∀υ0∈(0,υ∗), an intermittent control period Δ=(Θ+2υ0)/N+υ0 and a control width φ∈(1−1mχbmax,1) can be selected to make the controlled system (2.2) almost surely exponentially stable.
Remark 3: It is easy to see that the function
h(υ0)≜ε(1+K2υ0)m2eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4(m,υ0,Θ)+L3(m,υ0,υ0+Θ)) |
on the left side of Eq (2.9) is continuous and increasing. Moreover, h(0)<1 and h(+∞)=+∞. Therefore, Eq (2.9) has a unique positive root.
To prove Theorem 1, a series of lemmas will be introduced in the following section.
Lemma 1. For ∀μ≥0, j>0 and u∈S, if s∈[μ,μ+j], then
P(Γ(s)≠u,|Γ(μ)=u)≤1−e−ˆγj, | (3.1) |
where ˆγ=maxu∈S(−γuu).
As for the proof, please refer to the Appendix.
Lemma 2. Under Assumptions 1–3, when 0≤1−1mχbmax<φ<1, the solution of the auxiliary system (2.4) has
E|σ(μ)|m≤ME|σ0|me−χ1μ, | (3.2) |
limμ→∞sup1μlog|σ(μ)|<0,a.s., | (3.3) |
where χ1=−(mχ−1bmax−mχφ)>0.
As for the proof, please refer to the Appendix.
Lemma 3. Under Assumption 1, for ∀Θ>0,
sup0≤μ≤Θ+υ0E|λ(μ)|m≤L1(m,υ0,Θ)E||λ(0)||m, | (3.4) |
where L1(m,υ0,Θ)={(1+K2υ0)m2e(Θ+υ0)m(K1+12K32+K2),m∈(0,2),(1+K2υ0)e(Θ+υ0)m(K1+12(m−1)K32+K2),m∈[2,∞).
Proof. For simplicity, denote L1(m,υ0,Θ)=L1. When m≥2, for initial data ξ∈C([−υ0,0],Rn), apply the Itˆo formula to |λ(μ)|m, and have that
E|λ(μ)|m|λ(0)|m+E∫μ0m|λ(s)|m−2[λ(s)Th(λ(s),Γ(s),s)+12(m−1)×|k(λ(s),Γ(s),s)|2]ds+E∫μ0m|λ(s)|m−1|ϖ(λ(δs),Γ(δs),s)I(s)|ds. |
By Assumption 1, derive that
E|λ(μ)|m≤E|λ(0)|m+(mK1+12m(m−1)K23)E∫μ0|λ(s)|mds+E∫μ0mK2|λ(s)|m−1|λ(δs)|ds≤E|λ(0)|m+(mK1+12m(m−1)K23)E∫μ0|λ(s)|mds+E∫μ0K2[(m−1)|λ(s)|m |
+|λ(δs)|m]ds. |
Substitute ∫μ0E|λ(δs)|mds≤∫μ0sup−υ0≤θ≤sE|λ(θ)|mds≤υ0E||λ(0)||m+∫μ0sup0≤θ≤sE|λ(θ)|mds into the above, then
E|λ(μ)|m≤E|λ(0)|m+(mK1+12m(m−1)K32)E∫μ0|λ(s)|mds+∫μ0K2(m−1)E|λ(s)|mds+K2υ0E||λ(0)||m+K2∫μ0sup0≤θ≤sE|λ(θ)|mds. |
Using the Gronwall inequality,
sup0≤θ≤Θ+υ0E|λ(θ)|m≤(1+K2υ0)e(Θ+υ0)m(K1+12(m−1)K32+K2)E||λ(0)||m. | (3.5) |
When m∈(0,2),
sup0≤θ≤Θ+υ0E|λ(θ)|m≤(sup0≤θ≤Θ+υ0E|λ(θ)|2)m2≤(1+K2υ0)m2e(Θ+υ0)m(K1+12K32+K2)E||λ(0)||m. |
Therefore, the inequality (3.4) is proven.
Lemma 4. Under Assumption 1, for ∀Θ>0,
E(sup0≤μ≤Θ+υ0|λ(μ)|m)≤L2(m,υ0,Θ)E||λ(0)||m, | (3.6) |
where
L2(m,υ0,Θ)={{(3+(6(Θ+υ0))K22υ0)+[(6(Θ+υ0))K21+12(Θ+υ0)K23+(6(Θ+υ0))×K22](1+K2υ0)(e(Θ+υ0)2(K1+12K23+K2)−1)(2(K1+12K23+K2))−1}m2,m∈(0,2),{[3m−1+(6(Θ+υ0))m−1Km2υ0]+[(6(Θ+υ0))m−1Km1+3m−1(m32(m−1))m2(Θ+υ0)m−22Km3+(6(Θ+υ0))m−1Km2](1+K2υ0)(e(Θ+υ0)m(K1+12(m−1)K23+K2)−1)(m(K1+12(m−1)K23+K2))−1},m∈[2,∞). |
Proof. Denote L2(m,υ0,Θ)=L2. When m≥2,
E(sup0≤s≤θ+υ0|λ(s)|m)≤3m−1E|λ(0)|m+(3(Θ+υ0))m−1E∫Θ+υ00(|h(λ(s),Γ(s),s)+ϖ(λ(δs),Γ(δs),s)I(s)|)mds+3m−1E(sup0≤μ≤θ+υ0|∫μ0k(λ(s),Γ(s),s)dw(s)|m)≤3m−1E|λ(0)|m+(3(Θ+υ0))m−12m−1∫Θ+υ00(E|h(λ(s),Γ(s),s)|m+|ϖ(λ(δs),Γ(δs),s)I(s)|m)ds+3m−1(m32m−2)m2(Θ+υ0)m−22∫Θ+υ00E|k(λ(s),Γ(s),s)|mds≤3m−1E|λ(0)|m+[(3(Θ+υ0))m−12m−1Km1+3m−1(m32m−2)m2(Θ+υ0)m−22Km3]×∫Θ+υ00E(|λ(s)|m)ds+(3(Θ+υ0))m−12m−1Km2∫Θ+υ00sup−υ0≤θ≤sE|λ(θ)|mds≤[3m−1+(3(Θ+υ0))m−12m−1Km2υ0]E||λ(0)||m+[(3(Θ+υ0))m−12m−1Km1+3m−1×(m32m−2)m2(Θ+υ0)m−22Km3+(3(Θ+υ0))m−12m−1Km2]∫Θ+υ00sup0≤θ≤sE|λ(θ)|mds. |
By (3.5), have that
E(sup0≤s≤θ+υ0|λ(s)|m)≤{[3m−1+(6(Θ+υ0))m−1Km2υ0]+[(6(Θ+υ0))m−1Km1+3m−1(m32m−2)m2(Θ+υ0)m−22Km3 |
+(6(Θ+υ0))m−1Km2](1+K2υ0)(e(Θ+υ0)m(K1+12(m−1)K23+K2)−1) |
×(m(K1+12(m−1)K23×K2))−1}E||λ(0)||m. |
When m∈(0,2),
E(sup0≤s≤θ+υ0|λ(s)|m)≤(Esup0≤s≤θ+υ0|λ(s)|2)m2≤{(3+(6(Θ+υ0))K22υ0)+[(6(Θ+υ0))K12+12(Θ+υ0)K32+(6(Θ+υ0))K22]×(1+K2υ0)(e(Θ+υ0)2(K1+12K32+K2)−1)(2(K1+12K32+K2))−1}m2E||λ(0)||m. |
Inequality (3.6) has been proven.
Lemma 5. Under Assumption 1, for ∀Θ>0,
sup0≤μ≤ΘE(sup0≤θ≤υ0|λ(μ+θ)−λ(μ)|m)≤L3(m,υ0,Θ)E||λ(0)||m, | (3.7) |
where L3(m,υ0,Θ) can be seen from Theorem 1.
Proof. Denote L3(m,υ0,Θ)=L3, when m≥2,
E(sup0≤θ≤υ0|λ(μ+θ)−λ(μ)|m)≤(3υ0)m−1K1m∫μ+υ0μE|λ(s)|mds+(3υ0)m−1K2m∫μ+υ0μE|λ(δs)|mds+3m−1(m32m−2)m2υ0m−22×K3m∫μ+υ0μE|λ(s)|mds≤[(3υ0)m−1K1m+3m−1(m32m−2)m2υ0m−22K3m]∫μ+υ0μE|λ(s)|mds |
+(3υ0)m−1K2m∫μ+υ0μE|λ(δs)|mds. |
For ∀μ≤s≤μ+υ0, by (3.5), obtain that
E|λ(s)|m≤(1+K2υ0)e(μ+υ0)m(K1+12(m−1)K32+K2)E||λ(0)||m. |
E|λ(δs)|m≤(1+K2υ0)eμm(K1+12(m−1)K32+K2)E||λ(0)||m. |
Therefore,
E(sup0≤θ≤υ0|λ(μ+θ)−λ(μ)|m)≤[(3υ0)m−1K1m+3m−1(m32m−2)m2υ0m−22K3m]∫μ+υ0μ(1+K2υ0)e(μ+υ0)m(K1+12(m−1)K32+K2)×E||λ(0)||mds+(3υ0)m−1K2m∫μ+υ0μ(1+K2υ0)e(μ+υ0)m(K1+12(m−1)K32+K2)E||λ(0)||mds. |
Furthermore,
sup0≤μ≤ΘE(sup0≤θ≤υ0|λ(μ+θ)−λ(μ)|m)≤[3m−1υ0mK1m+3m−1(m32(m−1))m2υ0m2K3m](1+K2υ0)e(Θ+υ0)m(K1+12(m−1)K32+K2)E||λ(0)||m+3m−1υ0mK2m(1+K2υ0)eΘm(K1+12(m−1)K32+K2)E||λ(0)||m≤3m−1(1+K2υ0)e(Θ+υ0)m(K1+12(m−1)K32+K2)[υ0m(K1m+K2m)+(m32(m−1))m2υ0m2K3m] |
×E||λ(0)||m. |
For m∈(0,2),
sup0≤μ≤ΘE(sup0≤θ≤υ0|λ(μ+θ)−λ(μ)|m)≤{3(1+K2υ0)e(Θ+υ0)2(K1+12K32+K2)×[υ02(K12+K22)+4υ0K32]}m2E||λ(0)||m. |
Inequality (3.7) has been proven.
Lemma 6. Under Assumption 1, and Θ>0, for μ∈[0,Θ+υ0],
E|λ(μ)−σ(μ)|m≤L4(m,υ0,Θ)E||λ(0)||m, |
where L4(m,υ0,Θ) can be seen from Theorem 1.
Proof. Let L4(m,υ0,Θ)=L4, σ(μ;σ0,Γ0,0)=σ(μ). Taking the difference between system (2.2) and system (2.4), obtain that
λ(μ)−σ(μ)=∫μ0(h(λ(s),Γ(s),s)−h(σ(s),Γ(s),s))ds+∫μ0(ϖ(λ(δs),Γ(δs),s)−ϖ(σ(s),Γ(s),s))I(s)ds+∫μ0(k(λ(s),Γ(s),s)−k(σ(s),Γ(s),s))dw(s), |
when m≥2. Taking the expectation, yield that
E|λ(μ)−σ(μ)|m≤(3μ)m−1∫μ0E|h(λ(s),Γ(s),s)−h(σ(s),Γ(s),s)|mds+(3μ)m−1∫μ0E|(ϖ(λ(δs),Γ(δs),s)−ϖ(σ(s),Γ(s),s))I(s)|mds+3m−1(m(m−1)2)m2μm−22∫μ0E|k(λ(s),Γ(s),s)−k(σ(s),Γ(s),s)|mds≤[(3μ)m−1Km1+3m−1(m(m−1)2)m2μm−22Km3]∫μ0E|λ(μ)−σ(μ)|mds+(3μ)m−1T1, |
where
T1∫μ0|(ϖ(λ(δs),Γ(δs),s)−ϖ(σ(s),Γ(s),s))I(s)|mds≤3m−1[E∫μ0(|ϖ(λ(δs),Γ(δs),s)−ϖ(λ(δs),Γ(s),s)|m+|ϖ(λ(δs),Γ(s),s)−ϖ(λ(s),Γ(s),s)|m+|ϖ(λ(s),Γ(s),s)−ϖ(σ(s),Γ(s),s))|mds≤3m−1[Km2(Θ+υ0)L3E||λ(0)||m+Km2E∫μ0|λ(s)−σ(s)|mds+T2], |
and T2=∫μ0E|ϖ(λ(δs),Γ(δs),s)−ϖ(λ(δs),Γ(s),s)|mds.
By Assumption 1, for lυ≤s≤μ∧(l+1)υ, derive that
E|ϖ(λ(δs),Γ(δs),s)−ϖ(λ(δs),Γ(s),s)|m=E|ϖ(λ(lυ−υ0),Γ(lυ−υ0),s)−ϖ(λ(lυ−υ0),Γ(s),s)|m=E[E(|ϖ(λ(lυ−υ0),Γ(lυ−υ0),s)−ϖ(λ(lυ−υ0),Γ(s),s)|m|Fδs)]≤E[2mK2m|λ(lυ−υ0)|mE(I{Γ(s)≠Γ(lυ−υ0)}|Fδs)]=E[2mK2m|λ(lυ−υ0)|mE(∑u∈SI{Γ(lυ−υ0)=u}I{Γ(s)≠u}|Fδs)]=E[2mK2m|λ(lυ−υ0)|m∑u∈SI{Γ(lυ−υ0)=u}P(Γ(s)≠u|Γ(lυ−υ0)=u)]. |
By Lemma 1 and inequality (3.4), have that
E|ϖ(λ(δs),Γ(δs),s)−ϖ(λ(δs),Γ(s),s)|m≤E[2mK2m|λ(lυ−υ0)|mN(1−e−ˆγυ)]≤2mK2m(1−e−ˆγυ)NL1E||λ(0)||m. |
Hence, for μ∈[0,Θ+υ0],
T2≤∫μ02mK2m(1−e−ˆγυ)L1E||λ(0)||mds≤(Θ+υ0)2mK2m(1−e−ˆγυ)NL1E||λ(0)||m. |
T1≤3m−1[K2m(Θ+υ0)L3E||λ(0)||m+K2mE∫μ0|λ(s)−σ(s)|mds+2mK2m(1−e−ˆγυ)×(Θ+υ0)NL1E||λ(0)||m]. |
Furthermore,
E|λ(μ)−σ(μ)|m≤[3m−1(Θ+υ0)m−1K1m+3m−1(m(m−1)2)m2(Θ+υ0)m−22K3m]∫μ0E|λ(s)−σ(s)|mds+3m−1(Θ+υ0)m−1T1≤[3m−1(Θ+υ0)m−1K1m+3m−1(m(m−1)2)m2(Θ+υ0)m−22K3m]∫μ0E|λ(s)−σ(s)|mds+32m−2(Θ+υ0)m−1[K2m(Θ+υ0)L3E||λ(0)||m+K2mE∫μ0|λ(s)−σ(s)|mds+2mK2m(1−e−ˆγυ)×(Θ+υ0)NL1E||λ(0)||m]≤[3m−1(Θ+υ0)m−1K1m+3m−1(m(m−1)2)m2(Θ+υ0)m−22K3m+32m−2(Θ+υ0)m−1K2m]×∫μ0E|λ(s)−σ(s)|mds+32m−2(Θ+υ0)mK2m[L3+2m(1−e−ˆγυ)NL1]E||λ(0)||m. |
By Gronwall inequality, we have that
E|λ(μ)−σ(μ)|m≤32m−2(Θ+υ0)mK2m[L3+2m(1−e−ˆγυ)NL1]×e3m−1[(Θ+υ0)m−1K1m+(m(m−1)2)m2(Θ+υ0)m−22K3m+3m−1(Θ+υ0)m−1K2m](Θ+υ0)E||λ(0)||m≤32m−2(Θ+υ0)mK2m[L3+2m(1−e−ˆγυ)NL1]×e3m−1[K1m+(m(m−1)2)m2(Θ+υ0)−m2K3m+3m−1K2m](Θ+υ0)m×E||λ(0)||m. |
When m∈(0,2), by H¨older inequality, we have that
E|λ(μ)−σ(μ)|m≤[32(Θ+υ0)2K22[L3(2,υ0,Θ)+4(1−e−ˆγυ)NL1(2,υ0,Θ)]×e3[K12+(Θ+υ0)−1K32+3K22](Θ+υ0)2]m2E||λ(0)||m. |
Proof. Write λ(μ;ξ,ς,0)=λ(μ), Γ(μ;ς,0)=Γ(μ) for μ≥0. Similarly, let
σ(υ0+Θ;υ0,λ(υ0),Γ(υ0))=σ(υ0+Θ). |
By Lemmas 2 and 3, have that
E|σ(υ0+Θ)|m≤ME|λ(υ0)|me−χ1Θ≤M(1+K2υ0)m22eυ0m(K1+0.5(m1−1)K32+K2)E||λ(0)||me−χ1Θ, | (4.1) |
where m2=2∧m. By the elementary inequality (a+b)m≤2m3(am+bm) for any a,b≥0 and Lemma 6,
E|λ(υ0+Θ)|m=E|σ(υ0+Θ)+λ(υ0+Θ)−σ(υ0+Θ)|m≤2m3(E|σ(υ0+Θ)|m+E|λ(υ0+Θ)−σ(υ0+Θ)|m)≤2m3(M(1+K2υ0)m22eυ0m(K1+0.5(m1−1)K32+K2)e−χ1Θ+L4)E||λ(0)||m | (4.2) |
Using Lemma 5, obtain that
E||λ(2υ0+Θ)||m≤2m3(E|λ(υ0+Θ)|m+E(sup0≤θ≤υ0|λ(θ+υ0+Θ)−λ(υ0+Θ)|m))≤2m3(E|λ(υ0+Θ)|m+L3(m,υ0,υ0+Θ)E||λ(0)||m)≤2m3(2m3(M(1+K2υ0)m22eυ0m(K1+0.5(m1−1)K32+K2)e−χ1Θ+L4)+L3(m,υ0,υ0+Θ))×E||λ(0)||m≤[22m3Me−χ1Θ(1+K2υ0)m22eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4+L3(m,υ0,υ0+Θ))]×E||λ(0)||m≤[ε(1+K2υ0)m22eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4+L3(m,υ0,υ0+Θ))]E||λ(0)||m, | (4.3) |
where ε=22m3Me−χ1Θ. Since υ0<υ∗, it is obtained from the definition of υ∗ that
ε(1+K2υ0)m2eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4+L3(m,υ0,υ0+Θ))<1. |
Therefore, there exists ζ>0 such that
ε(1+K2υ0)m2eυ0m(K1+0.5(m1−1)K32+K2)+2m3(2m3L4+L3(m,υ0,υ0+Θ))=e−ζ(2υ0+Θ). |
It is concluded from (4.3) that
E||λ(2υ0+Θ)||m≤e−ζ(2υ0+Θ)E||λ(0)||m. |
Further considering the solution λ(μ) on μ≥Θ+2υ0, there is a N+ such that Θ+2υ0=N+Δυ0. Meanwhile, λ(μ) can be referred to as the solution of the Eq (2.2) with the initial value λ(N+Δυ0), Γ(N+Δυ0). By following the same procedure as mentioned above, show that
E||λ(2N+Δυ0)||m≤e−ζN+Δυ0E||λ(N+Δυ0)||m≤e−ζN+Δυ0e−ζ(2υ0+Θ)E||λ(0)||m≤e−2ζN+Δυ0E||λ(0)||m. |
Repeating the above procedure, have that
E||λ(zN+Δυ0)||m≤e−zζN+Δυ0E||λ(0)||m.z=1,2,⋯ |
By Lemma 4, have that
E(supzN+Δυ0≤μ≤(z+1)N+Δυ0E|λ(μ)|m)≤L2(m,υ0,N+Δυ0−υ0)e−zζN+Δυ0E||λ(0)||m. | (4.4) |
From the Markov inequality and inequality (4.4), it can be concluded that, for all z≥0,
P(supzN+Δυ0≤μ≤(z+1)N+Δυ0|λ(μ)|m≥e−0.5zζN+Δυ0)≤e0.5zζN+Δυ0E(supzN+Δυ0≤μ≤(z+1)N+Δυ0|λ(μ)|m)≤e−0.5zζN+Δυ0L2(m,υ0,N+Δυ0−υ0)E||λ(0)||m. |
According to the Borel−Cantelli lemma, there is a set Ω0∈F with P(Ω0)=1, then for almost all ω∈Ω0, there is an integer z0=z0(ω) such that for ∀z>z0(ω),
supzN+Δυ0≤μ≤(z+1)N+Δυ0|λ(μ)|m<e−0.5zζN+Δυ0∀z>z0(ω).a.s. |
Hence,
limμ→∞sup1μlog(|λ(μ,ω)|)≤−0.5zζN+Δυ0mzN+Δυ0=−ζ2m. |
The proof is completed.
Consider a stochastic differential equation
dη(μ)=h(η(μ),Γ(μ),μ)dμ+k(η(μ),Γ(μ),μ)dw(μ), | (5.1) |
in which Γ(μ) represents a Markov chain that takes values in S={1,2} with the generator Λ=(−221−1), and
h(η,1,μ)=0.2η,k(η,1,μ)=0.4η, | (5.2) |
h(η,2,μ)=0.4η,k(η,2,μ)=0.5η. | (5.3) |
Using the Euler-Maruyama numerical method, with η(0)=1, Γ(0)=1 and the step size 10−5, it is seen that the system (5.1) is unstable, as shown in Figure 1.
In order to stabilize the system (5.1), the control function is designed as follows:
ϖ(η,1,μ)=−0.4η,ϖ(η,2,μ)=−0.5η. |
By simple calculations, Assumption 1 is satisfied with K1=0.4, K2=0.5 and K3=0.5. Choosing m=1, we can infer from Assumption 2 that
β1=0.2,β2=0.4,c1=0.2,c2=0.1. |
From (2.6), obtain a non-singular M-matrix.
A=(c1m00c2m)−Λ=(2.2−2−11.1). |
By (2.7) and (2.8), we have
bmax=7.6191bmin=7.3809χ=max(βu+cu)=0.5. |
By Lemma 2, it is known that if φ∈(0.7375,1), then the auxiliary controlled stochastic system dσ(μ)=(h(σ(μ),Γ(μ),μ)+ϖ(σ(μ),Γ(μ),μ)I(μ))dμ+k(σ(μ),Γ(μ),t)dw(μ) is almost surely exponentially stable.
This paper aims to develop an intermittent feedback controller with discrete observations of both state and mode with delays for stabilizing system (5.1). The controlled system becomes
dλ(μ)=(h(λ(μ),Γ(μ),μ)+ϖ(λ(δμ),Γ(δμ),μ)I(μ))dμ+k(λ(μ),Γ(μ),μ)dw(μ). | (5.4) |
We choose φ=0.95, ε=0.9, and it can be obtained that χ1=0.1062, Θ=1.0126. Then (2.9) becomes
0.9(1+0.5υ0)12e1.025υ0+L4(1,υ0,1.0126)+L3(1,υ0,1.0126+υ0)=1, |
and its unique root is υ∗=4.6436×10−5. Taking υ=10−4, υ0=10−5, Δ=10−5, from Theorem 1, we can get that the system (5.4) is almost surely exponentially stable. The simulated trajectory is shown in Figure 2 with the step size 10−5.
This paper delves into the issue of exponential stabilization for hybrid stochastic systems by employing an intermittent feedback control with discrete delayed observations related to both state and mode. Compared to state discrete observations of the feedback controller, model observations are also performed at discrete times, which is more practical and cost-saving. Using M-matrix theory and intermittent control approach, the feedback stabilization theory of hybrid stochastic systems is established. However, this study focuses on the stabilization for hybrid stochastic systems and the underlying systems do not consider some important practical factors, such as time delay, which will be addressed in future work.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The authors would like to thank Humanities and Social Science Fund of Ministry of Education of China (No. 23YJAZH031), Natural Science Foundation of Hebei Province of China (Nos. A2023209002, A2019209005), China Postdoctoral Science Foundation (No. 2017M621588), Tangshan Science and Technology Bureau Program of Hebei Province of China (No. 19130222g) for their financial support.
The authors declare there is no conflict of interest.
Proof of Lemma 1.
Given Γ(μ)=u, define stopping time ˉκu=inf{s≥μ:Γ(s)≠u}. Let infΦ=∞. Since ˉκu−μ conforms to an exponential distribution with the parameter −γuu, one has that, for s∈[μ,μ+j],
P(Γ(s)≠u|Γ(μ)=u)≤P(ˉκu−μ≤j|Γ(μ)=u)=∫j0−γuueγuusds=1−eγuuj≤1−e−ˆγj. | (A1) |
Thus, assertion (3.1) is obtained.
Proof of Lemma 2.
Define H(σ,u,μ)=bu|σ|m, (σ,u,μ)∈(Rn−{0})×S×R+, then
EH(σ(μ),Γ(μ),μ)=EH(σ(0),Γ(0),0)+E∫μ0LH(σ(s),Γ(s),s)ds, | (A2) |
where generalized Itˆo operator LH:(Rn−{0})×R+×S→R is given by
LH(σ,u,μ)=bum|σ|m[1|σ|2(σT(h(σ,u,μ)+ϖ(σ,u,μ)I(μ))+12|k(σ,u,μ)|2)−(2−m)2|σ|4|σTk(σ,u,μ)|2]+∑Nv=1γuvbv|σ|m. | (A3) |
As μ∈[μl,μl+φΔ), I(μ)=1. By Assumptions 2 and 3, conclude that
LH(σ,u,μ)≤bum|σ|m(βμ−τμ)N∑v=1γuvbv|σ|m≤−bumcu|σ|m+N∑v=1γuvbv|σ|m=−|σ|m(buαu(m)−N∑v=1γuvbv). |
By (2.6) and (2.7), have that
buαu(m)−∑Nv=1γuvbv=1, |
hence,
LH(σ,u,μ)≤−|σ|m=−bu|σ|m1bu≤−1bmaxH(σ,u,μ). | (A4) |
As μ∈[μl+φΔ,μl+1), I(μ)=0, then
LH(σ,u,μ)≤bum|σ|mβμ+N∑v=1γuvbv|σ|m≤bum|σ|m(χ−cu)+N∑v=1γuvbv|σ|m≤mχ|σ|mbu−|σ|m(mbucu−N∑v=1γuvbv)=mχ|σ|mbu−|σ|m(buαu(m)−N∑v=1γuvbv). |
Since buαu(m)−∑Nv=1γuvbv=1,
LH(σ,u,μ)≤mχ|σ|mbu−|σ|m=bu|σ|m(mχ−1bu)≤(mχ−1bmax)H(σ,u,μ). | (A5) |
From (A4) and (A5),
LH(σ,u,μ)≤[−1bmaxI(μ)+(mχ−1bmax)(1−I(μ))]H(σ,u,μ). |
For any integer ι≥1, define stopping time κι=inf{μ≥μ0:|σ(μ)|≥ι}. It is evident that when ι→∞, κι→∞. When μ≥0, by utilizing the Itˆo formula, yield that
E[H(σ(μ∧κι),Γ(μ∧κι),μ∧κι)]e−∫μ∧κι0[1−bmaxI(s)+(mχ−1bmax)(1−I(s))ds]=EH(σ0,Γ0,0)+E∫μ∧κι0e−∫s0[−1bmaxI(θ)+(mχ−1bmax)(1−I(θ))dθ]×[LH(σ(s),Γ(s),s)−(−1bmaxI(s)+(mχ−1bmax)(1−I(s)))H(σ(s),Γ(s),s)]ds≤EH(σ0,Γ0,0). |
When ι→∞, get that
EH(σ(μ),Γ(μ),μ)e−∫μ0[−1bmaxI(s)+(mχ−1bmax)(1−I(s))ds]≤EH(σ0,Γ0,0), |
which means that
bminE|σ(μ)|m≤bmaxE|σ0|me∫μ0[−1bmaxI(s)+(mχ−1bmax)(1−I(s))]ds | (A6) |
By 0≤1−1mχbmax<φ<1, μl=lΔ,
−1bmax≤−1bmaxφ≤−1bmaxφ+(mχ−1bmax)(1−φ)=mχ−1bmax−mχφ. |
Let l>N+, when μ∈[μl,μl+φΔ),
∫μ0[−1bmaxI(s)+(mχ−1bmax)(1−I(s))]ds=(mχ−mχφ)lΔ+(mχ−1bmax−mχ)μ=(mχ−1bmax−mχφ)lΔ−1bmax(μ−lΔ)≤(mχ−1bmax−mχφ)μ. |
When μ∈[μl+φΔ,μl+1),
∫μ0[−1bmaxI(s)+(mχ−1bmax)(1−I(s))]ds=(mχ−1bmax)μ−mχ(l+1)φΔ≤(mχ−1bmax−mχφ)μ. |
Substituting this into (A6), yield that
E|σ(μ)|m≤bmaxbminE|σ0|me(mχ−1bmax−mχφ)μ≤ME|σ0|me(mχ−1bmax−mχφ)μ, |
hence E|σ(μ)|m≤ME|σ0|me−χ1μ. Inequality (3.2) has been proven.
Next, we start to prove inequality (3.3). Similarly to (A3), employing the Itˆo formula to |σ(μ)|m, obtain that
E|σ(μ)|m≤E|σ(0)|m+E∫μ0m|σ(s)|m[1|σ(s)|2(σ(s)T(h(σ(s),Γ(s),s)+ϖ(σ(s),Γ(s),s)I(s))+12|k(σ(s),Γ(s),s)|2)−(2−m)2|σ(s)|4|σ(s)Tk(σ(s),Γ(s),s)|2]ds. |
As μ∈[μl,μl+φΔ), I(μ)=1. By Assumption 2,
E|σ(μ)|m≤E|σ(0)|m+mE∫μ0(βu−τu)|σ(s)|mds≤E|σ(0)|m−cum∫μ0E|σ(s)|mds. |
As μ∈[μl+φΔ,μl+1), I(μ)=0,
E|σ(μ)|m≤E|σ(0)|m+βum∫μoE|σ(s)|mds. |
By (2.8), we have that
sup0≤s≤μE|σ(s)|m≤E|σ(0)|m+χm∫μ0sup0≤θ≤sE|σ(θ)|mds. |
Gronwall inequality leads to
sup0≤s≤μE|σ(s)|m≤E|σ(0)|meχmμ. |
Hence,
∫Δ0sup0≤θ≤sE|σ(θ)|mds≤1χm(eχmΔ−1)E|σ(0)|m. |
If m=2,
∫Δ0sup0≤θ≤sE|σ(θ)|2ds≤12χ(e2χΔ−1)E|σ(0)|2. | (A7) |
For a non-negative integer l, we have that
E(supμl≤μ≤μl+1|σ(μ)|2)≤3E|σ(μl)|2+3E|∫μl+1μlh(σ(s),Γ(s),s)+ϖ(σ(s),Γ(s),s)×I(s)ds|2+3E(supμl≤s≤μl+1|∫sμlk(σ(s),Γ(s),s)dw(s)|2). | (A8) |
Under Assumption 1 and utilizing the Burkholder−Davis−Gundy inequality, we yield that
E(sup0≤μ≤Δ|σ(μ)|2)|σ(0)|2+6Δ∫Δ0E(|h(σ(s),Γ(s),s)|2+|ϖ(σ(s),Γ(s),s)×I(s)|2)ds+12∫Δ0E|k(σ(s),Γ(s),s)|2ds≤3E|σ(0)|2+(6ΔK21+12K23+6ΔK22)∫Δ0sup0≤μ≤s|σ(μ)|2ds. |
Substituting (A7) into the above inequality, we obtain that
E(sup0≤μ≤Δ|σ(μ)|2)≤3E|σ(0)|2+(6ΔK12+12K32+6ΔK22)12χ(e2χΔ−1)E|σ(0)|2. |
For m∈(0,2), by H¨older inequality, we get that
E(sup0≤μ≤Δ|σ(μ)|m)≤Jm2E|σ(0)|m, |
where J=3+(6ΔK12+12K32+6ΔK22)12χ(e2χΔ−1).
Repeating the above process, we have that
E(supqΔ≤μ≤(q+1)Δ|σ(μ)|m)≤Jm2E|σ(qΔ)|m.q=1,2,⋯ |
Using Chebyshev's inequality, have we that
P(supqΔ≤μ≤(q+1)Δ|σ(μ)|m≥e−0.5χ1qΔ)≤e0.5χ1qΔE(supqΔ≤μ≤(q+1)Δ|σ(μ)|m)≤e0.5χ1qΔJm2E|σ(qΔ)|m≤e−0.5χ1qΔJm2ME|σ(0)|m. |
According to the Borel−Cantelli lemma, there is a set Ω0∈F with P(Ω0)=1, then for almost all ω∈Ω0, there exists an integer q0=q0(ω) such that for ∀q≥q0,
supqΔ≤μ≤(q+1)Δ|σ(μ)|m≤e−0.5χ1qΔ. |
Therefore, for qΔ≤μ≤(q+1)Δ,
1μlog|σ(μ)|≤−0.5χ1qΔ(q+1)Δm. |
Letting μ→∞, obtain that
limμ→∞sup1μlog|σ(μ)|≤−χ12m.a.s. |
This completes the proof.
[1] |
X. Mao, Stability of stochastic differential equations with Markovian switching, Stochastic Processes Appl., 79 (1999), 45–67. https://doi.org/10.1016/S0304-4149(98)00070-2 doi: 10.1016/S0304-4149(98)00070-2
![]() |
[2] |
X. Mao, Exponential stability of stochastic delay interval systems with Markovian switching, IEEE Trans. Autom. Control, 47 (2002), 1604–1612. https://doi.org/10.1109/TAC.2002.803529 doi: 10.1109/TAC.2002.803529
![]() |
[3] | X. Mao, C. Yuan, Stochastic Differential Equations with Markovian Switching, Imperial College press, 2006. https://doi.org/10.1142/p473 |
[4] |
X. Mao, G. Yin, C. Yuan, Stabilization and destabilization of hybrid systems of stochastic differential equations, Automatica, 43 (2007), 264–273. https://doi.org/10.1016/j.automatica.2006.09.006 doi: 10.1016/j.automatica.2006.09.006
![]() |
[5] |
S. Zhu, P. Shi, C. Lim, New criteria for stochastic suppression and stabilization of hybrid functional differential systems, Int. J. Robust Nonlinear Control, 28 (2018), 3946–3958. https://doi.org/10.1002/rnc.4114 doi: 10.1002/rnc.4114
![]() |
[6] |
S. Zhu, K. Sun, W. Chang, M. Wang, Stochastic suppression and stabilization of non-linear hybrid delay systems with general one-sided polynomial growth condition and decay rate, IET Control Theory Appl., 12 (2018), 933–941. https://doi.org/10.1049/iet-cta.2017.0931 doi: 10.1049/iet-cta.2017.0931
![]() |
[7] |
L. Feng, J. Cao, L. Liu, A. Alsaedi, Asymptotic stability of nonlinear hybrid stochastic systems driven by linear discrete time noises, Nonlinear Anal. Hybrid Syst., 33 (2019), 336–352. https://doi.org/10.1016/j.nahs.2019.03.008 doi: 10.1016/j.nahs.2019.03.008
![]() |
[8] |
L. Feng, L. Liu, J. Cao, L. Rutkowski, G. Lu, General decay stability for non-autonomous neutral stochastic systems with time-varying delays and Markovian switching, IEEE Trans. Cybern., 52 (2020), 5441–5453. https://doi.org/10.1109/TCYB.2020.3031992 doi: 10.1109/TCYB.2020.3031992
![]() |
[9] |
X. Mao, Stabilization of continuous-time hybrid stochastic differential equations discrete-time feedback control, Automatica, 49 (2013), 3677–3681. https://doi.org/10.1016/j.automatica.2013.09.005 doi: 10.1016/j.automatica.2013.09.005
![]() |
[10] |
X. Mao, W. Liu, L. Hu, Q. Luo, J. Lu, Stabilization of hybrid stochastic differential equations by feedback control based on discrete-time state observations, Syst. Control Lett., 73 (2014), 88–95. https://doi.org/10.1016/j.sysconle.2014.08.011 doi: 10.1016/j.sysconle.2014.08.011
![]() |
[11] |
S. You, W. Liu, J. Lu, X. Mao, Q. Qiu, Stabilization of hybrid systems by feedback control based on discrete-time state observations, SIAM J. Control Optim., 53 (2015), 905–925. https://doi.org/10.1137/140985779 doi: 10.1137/140985779
![]() |
[12] |
J. Shao, Stabilization of regime-switching processes by feedback control based on discrete time observations, SIAM J. Control Optim., 55 (2017), 724–740. https://doi.org/10.1137/16M1066336 doi: 10.1137/16M1066336
![]() |
[13] |
G. Song, B. Zheng, Q. Luo, X. Mao, Stabilization of hybrid stochastic differential equations by feedback control based on discrete-time observations of state and mode, IET Control Theory Appl., 11 (2017), 301–307. https://doi.org/10.1049/iet-cta.2016.0635 doi: 10.1049/iet-cta.2016.0635
![]() |
[14] |
G. Song, Z. Lu, B. Zheng, X. Mao, Almost sure stabilization of hybrid systems by feedback control based on discrete-time observations of mode and state, Sci. China Inf. Sci., 61 (2018), 130–145. https://doi.org/10.1007/s11432-017-9297-1 doi: 10.1007/s11432-017-9297-1
![]() |
[15] |
R. Dong, Almost sure exponential stabilization by stochastic feedback control based on discrete-time observations, Stochastic Anal. Appl., 36 (2018), 561–583. https://doi.org/10.1080/07362994.2018.1433046 doi: 10.1080/07362994.2018.1433046
![]() |
[16] |
L. Feng, Q. Liu, J. Cao, C. Zhang, F. Alsaadi, Stabilization in general decay rate of discrete feedback control for non-autonomous Markov jump stochastic systems, Appl. Math. Comput., 417 (2022), 126771. https://doi.org/10.1016/j.amc.2021.126771 doi: 10.1016/j.amc.2021.126771
![]() |
[17] | L. Feng, C. Zhang, J. Cao, Note on general stabilization of discrete feedback control for non-autonomous hybrid neutral stochastic systems with delays, Acta Math. Sci., 2023 (2023). |
[18] |
X. Mao, J. Lam, L. Huang, Stabilization of hybrid stochastic differential equations by delay feedback control, Syst. Control Lett., 57 (2008), 927–935. https://doi.org/10.1016/j.sysconle.2008.05.002 doi: 10.1016/j.sysconle.2008.05.002
![]() |
[19] |
X. Sun, G. Liu, D. Rees, W. Wang, Stability of systems with controller failure and time-varying delay, IEEE Trans. Autom. Control, 53 (2008), 2391–2396. https://doi.org/10.1109/TAC.2008.2007528 doi: 10.1109/TAC.2008.2007528
![]() |
[20] |
W. Chen, S. Xu, Y. Zou, Stabilization of hybrid neutral stochastic differential delay equations by delay feedback control, Syst. Control Lett., 88 (2016), 1–13. https://doi.org/10.1016/j.sysconle.2015.04.004 doi: 10.1016/j.sysconle.2015.04.004
![]() |
[21] |
Q. Qiu, W. Liu, L. Hu, X. Mao, S. You, Stabilization of stochastic differential equations with Markovian switching by feedback control based on discrete-time state observation with a time delay, Stat. Probab. Lett., 115 (2016), 16–26. https://doi.org/10.1016/j.spl.2016.03.024 doi: 10.1016/j.spl.2016.03.024
![]() |
[22] |
Q. Zhu, Q. Zhang, P th moment exponential stabilization of hybrid stochastic differential equations by feedback controls based on discrete-time state observations with a time delay, IET Control Theory Appl., 11 (2017), 1992–2003. https://doi.org/10.1049/iet-cta.2017.0181 doi: 10.1049/iet-cta.2017.0181
![]() |
[23] |
L. Liu, M. Perc, J. Cao, Aperiodically intermittent stochastic stabilization via discrete time or delay feedback control, Sci. China Inf. Sci., 62 (2019). https://doi.org/10.1007/s11432-018-9600-3 doi: 10.1007/s11432-018-9600-3
![]() |
[24] |
X. Li, X. Mao, Stabilization of highly nonlinear hybrid stochastic differential delay equations by delay feedback control, Automatica, 112 (2020), 108657. https://doi.org/10.1016/j.automatica.2019.108657 doi: 10.1016/j.automatica.2019.108657
![]() |
[25] |
J. Hu, W. Liu, F. Deng, X. Mao, Advances in stabilization of hybrid stochastic differential equations by delay feedback control, SIAM J. Control Optim., 58 (2020), 735–754. https://doi.org/10.1137/19M1270240 doi: 10.1137/19M1270240
![]() |
[26] |
X. Li, X. Mao, D. Mukama, C. Yuan, Delay feedback control for switching diffusion systems based on discrete-time observations, SIAM J. Control Optim., 58 (2020), 2900–2926. https://doi.org/10.1137/20M1312356 doi: 10.1137/20M1312356
![]() |
[27] |
L. Feng, L. Liu, J. Cao, F. E. Alsaadi, General stabilization of non-autonomous hybrid systems with delays and random noises via delayed feedback control, Commun. Nonlinear Sci. Numer. Simul., 117 (2023), 106939. https://doi.org/10.1016/j.cnsns.2022.106939 doi: 10.1016/j.cnsns.2022.106939
![]() |
[28] |
C. Li, G. Feng, X. Liao, Stabilization of nonlinear systems via periodically intermittent control, IEEE Trans. Circuits Syst. II Express Briefs, 54 (2007), 1019–1023. https://doi.org/10.1109/TCSII.2007.903205 doi: 10.1109/TCSII.2007.903205
![]() |
[29] |
B. Zhang, F. Deng, S. Peng, S. Xie, Stabilization and destabilization of nonlinear systems via intermittent stochastic noise with application to memristor-based system, J. Franklin Inst., 355 (2018), 3829–3852. https://doi.org/10.1016/j.jfranklin.2017.12.033 doi: 10.1016/j.jfranklin.2017.12.033
![]() |
[30] |
L. Liu, Z. Wu, Intermittent stochastic stabilization based on discrete-time observation with time delay, Syst. Control Lett., 137 (2020), 104626. https://doi.org/10.1016/j.sysconle.2020.104626 doi: 10.1016/j.sysconle.2020.104626
![]() |
[31] |
W. Mao, Y. Jiang, L. Hu, X. Mao, Stabilization by intermittent control for hybrid stochastic differential delay equations, Discrete Contin. Dyn. Syst. Ser. B, 27 (2021), 569–581. https://doi.org/10.3934/dcdsb.2021055 doi: 10.3934/dcdsb.2021055
![]() |
[32] |
R. Zhu, L. Liu, Stochastic stabilization of switching diffusion systems via an intermittent control strategy with delayed and sampled-data observations, Syst. Control Lett., 168 (2022), 105362. https://doi.org/10.1016/j.sysconle.2022.105362 doi: 10.1016/j.sysconle.2022.105362
![]() |
[33] |
C. Liu, L. Liu, J. Cao, M. Abdel-Aty, Intermittent event-triggered optimal leader-following consensus for nonlinear multi-agent systems via Actor-Critic algorithm, IEEE Trans. Neural Networks Learn. Syst., 34 (2023), 3992–4006. https://doi.org/10.1109/TNNLS.2021.3122458 doi: 10.1109/TNNLS.2021.3122458
![]() |
[34] |
S. Li, J. Zhao, X. Ding, Stability of stochastic delayed multi-links complex network with semi-Markov switched topology: A time-varying hybrid aperiodically intermittent control strategy, Inf. Sci., 630 (2023), 623–646. https://doi.org/10.1016/j.ins.2022.11.061 doi: 10.1016/j.ins.2022.11.061
![]() |
[35] |
Y. Jiang, L. Hu, J. Lu, W. Mao, X. Mao, Stabilization of hybrid systems by intermittent feedback controls based on discrete-time observations with a time delay, IET Control Theory Appl., 15 (2021), 2039–2052. https://doi.org/10.1049/cth2.12160 doi: 10.1049/cth2.12160
![]() |
1. | Chidentree Treesatayapun, Finite-time adaptive control based on output feedback and auxiliary variables for time-varying parameters and disturbances, 2024, 361, 00160032, 107273, 10.1016/j.jfranklin.2024.107273 |