Existence and Uniqueness of Solutions for a Class of Nonlinear Stochastic Differential Equations
Abstract
By using successive approximation, we prove existence and uniqueness result for a class of nonlinear stochastic differential equations. Moreover, it is shown that the solution of such equations is a diffusion process and its diffusion coefficients are found.
1. Introduction
Differential equations, which are not solved for the derivative, have found diverse applications in many fields. Examples of equations of this type are Lagrange equations of classical mechanics or Euler equations.
Consideration of real objects under the influence of random factors leads to nonlinear stochastic differential equations, which are not solved for stochastic differential. Such equations were introduced by Kolmanovskii and Nosov in [1] for construction of stochastic analogues of neutral functional differential equations. Works [1–5] were devoted to the problems of existence, uniqueness, and properties of solutions of neutral stochastic differential (delay) equations in finite dimensional spaces. Existence of solutions for such equations in Hilbert spaces was studied in papers [6–9]. In the paper [9] the author considered a stochastic equation without delay. In the monograph of Kolmanovskiĭ and Shaĭkhet [10] conditions were obtained for optimality in control problems for these equations.
In this paper we will study the existence and uniqueness of solutions for a class of nonlinear stochastic differential equations, which are not solved for the stochastic differential.
Here x ∈ Rd, t ≥ t0, G(t, x), and a(t, x) are d-dimensional vector functions; σ(t, x) is a d × m matrix and W(t) is an m-dimensional Wiener process with independent components. Let x be a random vector in Rd, such that E|x|2 < ∞. Assume that x does not depend on W(t) − W(t0), Ft = σ{x, W(s) − W(t0), t0 ≤ s ≤ t}.
Definition 1. An Ft-dimensional process x(t) is said to be the solution of (1) if x(t0) = x and
A solution x(t) is said to be unique if for any continuous solutions x(t), y(t) such that x(t0) = y(t0) = x one has for all t ≥ t0.
In this work we use the method of successive approximations to establish existence and uniqueness (pathwise) of the solution of (1). We study its probability properties. We prove that x(t) is diffusion process and find coefficients of diffusion.
2. Main Results
Firstly we prove the theorem of existence and uniqueness of the solution.
Theorem 2. Assume that G(t, x) is a continuous function; a(t, x), σ(t, x) are measurable functions for x ∈ Rd, t ≥ t0 and satisfy the following conditions:
- (1)
there exists a constant C > 0, such that |G(t, x)| + |a(t, x)| + ∥σ(t, x)∥ ≤ C(1 + |x|) for x ∈ Rd, t ≥ t0;
- (2)
there exist constants L1 > 0 and L > 0 such that |G(t, x) − G(t, x′)| ≤ L1|x − x′| and
() -
for x, x′ ∈ Rd, t ≥ t0.
If L1 < (1/6) 3/4, then there exists a unique continuous solution x(t) of (1) with probability 1 for all t ≥ t0. Moreover it has a bounded second moment such that E|x(t)|2 < ∞ for all t ≥ t0.
Proof. To find a solution of the integral equation (2), we use the method of successive approximations. We start by choosing an initial approximation x0(t) = x.
At the next step,
We prove that a solution exists on this interval.
From (4) it follows that
Next, estimate
This implies the uniform convergence with probability 1 of the series
Then prove uniqueness of this continuous solution. Assume that there exists a second continuous solution y(t) of (1). Denote by ϰN(t) the random variable which equals 1 if |x(s)| ≤ N, |y(s)| ≤ N and it equals 0 otherwise. Then
We conclude that
Next, we show boundedness of a second moment of the solution. Denote again by ϰN(t) the indicator of the set
Thus existence, uniqueness, and boundedness of the second moment of the solution x(t) are proved on [t0, T]. Since the constant B is dependent only on T − t0 and E|x|2 < ∞, and x(T) is independent of W(s) − W(T) for s⩾T, then by similar manner we can prove the existence and uniqueness of the solution of the IVP with initial conditions (T, x(T)) on the interval [T, T1], where T1 is chosen such that the inequality .
This procedure can be repeated in order to extend the solution of (1) to the entire semiaxis t⩾t0. The theorem is proved.
Notes. The existence and uniqueness of the solution can be obtained as corollary from work [1], where this result was proved for an SDE of neutral type by replacing a condition for Lipschitz constant L1 < (1/6)3/4 with more weak condition L1 < 1. But by using our method, paths of obtained solution are continuous with probability 1. Otherwise, in the pointed work only the measurability of the solution and boundedness of its second moment were stated.
Now, we state some probability properties of the solution obtained in Theorem 2. We prove that under assumptions of Theorem 2, the solution of (1) is a Markov random process. Moreover, if the coefficients are continuous then it is a diffusion process. We will find its diffusion coefficients.
Theorem 3. Under conditions (1)-(2) of Theorem 2 the solution x(t) of (1) is a Markov process with a transition probability defined by
Proof. As in Theorem 2, we solve (1) by the method of successive approximations. It can be shown that xt,x(s) is completely defined by the nonrandom initial value x and the process W(s) − W(t) for s > t, which are independent of Ft. Since x(t) is a solution of (2), it is Ft measurable. Hence xt,x(s) is independent of x(t) and events from Ft. Note that, from the uniqueness of the solution x(s) for s > t, it follows that it is a unique solution of the equation
As for the rest, the proof is the same as the proof of the theorem for ordinary stochastic equations [11]. The theorem is proved.
We have a corollary from this theorem.
Corollary 4. Suppose that conditions of Theorem 2 are satisfied. Then
- (1)
if functions G, a, and σ are independent of t, then the solution x(t) is a homogeneous Markov process;
- (2)
if functions G, a, and σ are periodic functions with period θ, then a transition probability is periodic function; that is, P(t + θ, x, s + θ, A) = P(t, x, s, A).
Now, we investigate conditions for which the solution of (1) is a diffusion process. For this we must find an additional estimate.
Lemma 5. Let xt,x(s) be a solution of (2) such that xt,x(t) = x, x ∈ Rd. If conditions of Theorem 2 are satisfied and Gt(t, x) is continuous for t ≥ t0, x ∈ Rd, then an inequality
Proof. Denote by ϰN(s) the indicator of the set
The last estimate follows from Hölder’s inequality and properties of stochastic integral. From inequality (30) and condition for L1, we have
Further, the right-hand side of (31) can be estimated by
Using the lemma from [11, p.38], we obtain
Now, assume that N → ∞ and obtain estimate (28). This completes the proof of the Lemma.
Theorem 6. If conditions (1)-(2) of Theorem 2 are satisfied and functions a(t, x), σ(t, x), G(t, x), Gt(t, x), , and , , are continuous for t⩾t0, x ∈ Rd. Functions Gt(t, x), , and satisfy Lipschitz condition with respect to x in neighborhood of every point (t, x). Then the solution of (1) is diffusion process with
Proof. Take any point (t, x) from a region t⩾t0, x ∈ Rd. Consider a stochastic ITO equation in a closed neighborhood of this point
From the conditions of the theorem, it follows that there exists a closed neighborhood of the point (t, x), such that coefficients of the equation are Lipschitz with respect to x. Fix this neighborhood. Extend these coefficients on the all region t ≥ t0, x ∈ Rd such that they remain continuous by both variables, Lipschitz and linear with respect to x.
Then the equation
From ITO formula and coincidence of coefficients of (36) and (37) in this neighborhood of the point (t, x), one can show that processes xt,x and y(s) coincide in this neighborhood.
It is known that under these assumptions the process y(s) is diffusion. Its diffusion coefficients in the point (t, x) are defined by coefficients of (36).
Next, show that x(s) has the same diffusion coefficients. To do this it is sufficient to estimate the following limits and use estimation (28)
We get