Stochastic Functional Differential Equation under Regime Switching
Abstract
We discuss stochastic functional differential equation under regime switching dx(t) = f(xt, r(t), t)dt + q(r(t))x(t)dW1(t) + σ(r(t)) | x(t)|βx(t)dW2(t). We obtain unique global solution of this system without the linear growth condition; furthermore, we prove its asymptotic ultimate boundedness. Using the ergodic property of the Markov chain, we give the sufficient condition of almost surely exponentially stable of this system.
1. Introduction
Recently, many papers devoted their attention to the hybrid system, they concerned that how to change if the system undergoes the environmental noise and the regime switching. For the detailed understanding of this subject, [1] is good reference.
Assumption A. For each integer k ≥ 1, …, there is a positive number Hk such that
Throughout this paper, unless otherwise specified, we let (Ω, ℱ, {ℱt} t≥0, P) be a complete probability space with a filtration {ℱt} t≥0 satisfying the usual conditions (i.e., it is right continuous and ℱ0 contains all P-null sets). Let Wi(t) (i = 1,2), t ≥ 0, be the standard Brownian motion defined on this probability space. We also denote by . Let r(t) be a right-continuous Markov chain on the probability space taking values in a finite state space 𝕊 = {1,2, …, N} with the generator given by
In addition, throughout this paper, let denote the family of all positive real-valued functions V(x, t, k) on Rn × [−τ, ∞) × 𝕊 which are continuously twice differentiable in x and once in t. If for the following equation
2. Global Solution
Firstly, in this paper, we are concerned about that the existence of global solution of stochastic functional differential equation (1.1).
In order to have a global solution for any given initial data for a stochastic functional equation, it is usually required to satisfy the local Lipschitz condition and the linear growth condition [1, 2]. In addition, as a generation of linear condition, it is also mentioned in [3, 4] with one-sided linear growth condition. The authors improve the results using polynomial growth condition in [5, 6]. After that, these conditions were mentioned under regime systems [7–9].
Replacing the linear growth condition or the one-sided linear growth condition, we impose the so-called polynomial growth condition on the function f for (1.1).
Assumption B. For each i ∈ 𝕊, there exist nonnegative constants and probability measures μ, on [−τ, 0] such that
Theorem 2.1. Under the conditions of Assumptions A and B, if 2β > α, and σ(i) ≠ 0 for i = 1,2, …, n, there almost surely exists a unique globally solution x(t) to (1.1) on t ≥ −τ for any given initial data φ ∈ C([−τ, 0]; Rn).
Proof. Since the coefficients of (1.1) are locally Lipschitz, there is a unique maximal local solution x(t) on t ∈ [−τ, τe), where τe is the explosion time. In order to prove this solution is global, we need to show that τe = ∞ a.s. Let m0 > 0 be sufficiently large such that 1/m0 < min −τ≤θ≤0 |ξ(θ)| < max −τ≤θ≤0 |ξ(θ)| < m0. For each m ≥ m0, we define the stopping time
To prove the conclusion that we desired, for any p ∈ (0,1/2), define a C2-function: by
Let . For any k, l ∈ 𝕊, we get
Therefore,
According to Assumption B, the first term in (2.7)
By the Young inequality and noting that p ∈ (0,1/2), it is obvious that
By the Fubini theorem and a substitution technique, we may compute that
By the definition of τm, x(τm) = m or 1/m, so let Ωm = {τm ≤ T} for m ≥ m1 and by (2.6), noting that for every ω ∈ Ωm, there is some m such that xm(τm, ω) equals either m or 1/m hence
3. Asymptotic Boundedness
Theorem 2.1 shows that the solution of SDE (1.1) exists globally and will not explode under some reasonable conditions. In the study of stochastic system, stochastically ultimate boundedness is more important topic comparing with nonexplosion of the solution, which means that the solution of this system will survive under finite boundedness in the future. Here we examine the 2pth moment boundedness.
Lemma 3.1. Under the conditions of Theorem 2.1, for any p ∈ (0,1/2), there exists a constant Kp independent on the initial data such that the global solution x(t) of SDE (1.1) has the property that
Proof. First, Theorem 2.1 indicates that the solution x(t) of (1.1) almost surely remain in Rn for all t ≥ −τ with probability 1.
Applying the Itô formula to eɛtV(x, k) and taking expectation yields
Now we consider the function
Similar to the proof of Theorem 2.1, then we know (3.3) is upper bounded; there exists constant ψk such that Φk(x)≤(1 + |x|2) 2−pΦk(x) ≤ ψk ≤ Ψ : = max 1≤k≤N ψk; therefore, (3.2) implies that
We have the following calculus transformation:
We therefore have from (3.4)
Clearly,
Definition 3.2. The solutions x(t) of SDE (1.1) are called stochastically ultimately bounded, if for any ϵ ∈ (0,1), there is a positive constant χ( = χ(ϵ)), such that the solution of SDE (1.1) with any positive initial value has the property that
Theorem 3.3. The solution of (1.1) is stochastically ultimately bounded under the condition Lemma 3.1; that is, for any ϵ ∈ (0,1), there is a positive constant χ( = χ(ϵ)), such that for any positive initial value the solution of Lemma 3.1 has the property that
Proof. This can be easily verified by Chebyshev′s inequality and Lemma 3.1 by choosing sufficiently large because of the following
4. Stabilization of Noise
From Sections 2 and 3, we know that under the condition σ(i) ≠ 0 and 2β > α, the Brownian noise σ(i)|x(t)|βx(t)dW1(t) can suppress the potential explosion of the solution and guarantee this global solution to be bounded in the sense of the 2pth moment. Clearly, the boundedness results are also dependent only on the choice of β under the condition σ(i) ≠ 0 and independent of q(i). This implies that the noise W1(t) plays no role to guarantee existence and boundedness of the global solution to (1.1). This section is devoted to consider the effect of noise q(i)x(t)dW1(t), we will show that the system (1.1) is exponential stability if for some sufficiently large q(i).
For the purpose of stability study, we impose the following the general polynomial growth condition.
Assumption C. For each i ∈ 𝕊, there exist nonnegative constants and probability measures μ, on [−τ, 0] such that
Clearly, Assumption C is stronger than the one-sided polynomial growth condition Assumption B. Therefore, Theorems 2.1 and Lemma 3.1 still hold under Assumption C.
In [10, Page 165], for a given nonlinear SDE with Markovian switching
Lemma 4.1. Let x(t) be the global solution of (1.1). Under Assumption C, if 2β > α and σ(i) ≠ 0, for any non-zero initial data x(0) ≠ 0
Proof. For any initial data ξ ∈ C([−τ, 0]; Rn) satisfying x(0) ≠ 0, for sufficiently large positive number i0, such that |x(0)| > 1/i0. For each integer i ≥ i0, define the stopping time
To prove this statement, define a C2-function
Furthermore, we may estimate that
We know that
This lemma shows that almost all the sample path of any solution of (1.1) starting from a non-zero state will never reach the origin. Because of this nice property, the Lyapunov functions we can choose need not be imposed globally but only in a deleted neighborhood of the origin.
Especially, the hybrid system always switch from any regime to another regime, so it is reasonable to assume that the Markov chain r(t) is irreducible. It means to the condition that irreducible Markov chain has a unique stationary probability distribution π = (π1, π2, …, πN) ∈ R1×N which can be determined by solving the following linear equation πΓ = 0 subject to and πk > 0 for any k ∈ 𝕊, where Γ is generator .
Theorem 4.2. Suppose the Markov chain r(t) is irreducible, under Assumption A and C, if for δ ∈ (0,1), k ∈ 𝕊, σ(k) ≠ 0 and 2β > α, the solution x(t) of SDE (1.1) with any initial data ξ ∈ C([−τ, 0]; Rn) satisfying x(0) ≠ 0 has the property
Proof. By Theorem 2.1 and Lemma 4.1, (1.1) almost surely admits a global solution x(t) for all t ≥ 0 and x(t) ≠ 0 almost surely. Applying the Itô formula to the function log | x(t)| leads to
Since , by the Borel-Cantelli lemma, there exists an Ω0 ⊂ Ω with ℙ(Ω0) = 1 such that for any ω ∈ Ω0, there exists an integer n(ω), when n > n(ω) and n − 1 ≤ t ≤ n,
Applying the strong law of large number [2, Page 12] to the Brownian motion, we therefore have
Clearly, if
Remark 4. This results is generation of Theorem 4.2 in [6]. The author consider functional differential equation:

Example 4.3. Let us assume that the Markov chain r(t) is on the state space S = {1,2} with the generator
As pointed out in Section,we may regard SDE (1.1) as the result of the following two equations:
Noting that has the form
However, as the result of Markovian switching, the overall behavior, that is SDE (1.1) will be almost surely exponentially stable as long as
Example 4.4. Consider another stochastic differential equation with Markovian switching, where r(t) is a Markov chain taking values in S = {1,2, 3}. Here subsystem of (1.1) is writtern as three different equations:
Case 1. Let the generator of the Markov chain r(t) be
Case 2. Suppose the generator of the Markov chain r(t) be
By solving the linear equation πΓ = 0 subject to and πk > 0 for any k ∈ 𝕊, we obtain the unique stationary distribution
Then
We can see the impact of the Markov chain r(t). The distribution (π = (π1, π2, …, πn)) of r(t) plays a very important role, which, combined with , determine that system (1.1) is almost surely exponentially stable. If r(t) spends enough time in the “good” states (the state where ϕ(i) − (q2(i)/2) < 0 for some i), even if there exist some “bad” states (the states where ϕ(i) − (q2(i)/2) > 0 for some i), the system (1.1) will still be almost surely exponentially stable.
Acknowledgment
This work is partially supported by the National Natural Science Foundation of China (11101183, 11171056, 11171081 and 11271157), 985 program of Jilin University. We also wish to thank the high performance computing center of Jilin University.