Stochastic PDEs and Infinite Horizon Backward Doubly Stochastic Differential Equations
Abstract
We give a sufficient condition on the coefficients of a class of infinite horizon BDSDEs, under which the infinite horizon BDSDEs have a unique solution for any given square integrable terminal values. We also show continuous dependence theorem and convergence theorem for this kind of equations. A probabilistic interpretation for solutions to a class of stochastic partial differential equations is given.
1. Introduction
This paper studies the existence and uniqueness of BDSDE (1.1) when T = ∞. Our method is different from Zhang and Zhao. Due to sufficient utilization of the properties of martingales, this method is essential to the theory of BSDEs. In this paper we give a sufficient condition on coefficients f, g under which, for any square integrable random variable ξ, BDSDE (1.1) still has a unique solution pair when T = ∞. Our conditions are a special kind of Lipschitz conditions, which even include some cases of unbounded coefficients. This allows us to give a probabilistic interpretation for the solutions to a class of stochastic partial differential equations (SPDEs in short).
The paper is organized as follows: in Section 2 we introduce some preliminaries and notations; in Section 3 we prove the existence and uniqueness theorem of BDSDEs; in Section 4 we discuss continuous dependence theorem and convergence theorem; at the end, we give the connection of the solutions of SPDEs and BDSDEs in Section 5.
2. Setting of Infinite Horizon BDSDEs
Notation The Euclidean norm of a vector x ∈ Rk will be denoted by |x|, and, for a d × k matrix A, we define , where A* is the transpose of A.
Let (Ω, ℱ, P) be a completed probability space and let {Wt} t≥0 and {Bt} t≥0 be two mutually independent standard Brownian motions, with values, respectively, in Rd and Rl, defined on (Ω, ℱ, P). Let 𝒩 denote the class of P-null sets of ℱ. For each t ∈ [0, ∞), we define
Suppose
For any n ∈ N, let S2(R+; Rn) denote the space of all {ℱt}-measurable n-dimensional processes v with norm of | | v | |S≐[E(sup s≥0 |v(s) | ) 2] 1/2 < ∞.
We denote similarly by M2(R+; Rn) the space of all (classes of dP ⊗ dt a.e. equal) {ℱt}-measurable n-dimensional processes v with norm of .
For any t ≥ 0, let L2(Ω, ℱt, P; Rn) denote the space of all {ℱt}-measurable n-valued random variables ξ satisfying E | ξ|2 < ∞.
We also denote
Consider the following infinite horizon backward doubly stochastic differential equation:
Definition 2.1. A pair of processes (y, z) : Ω × R+ → Rk × Rk×d is called a solution of BDSDE (2.5), if (y, z) ∈ B2 and satisfies BDSDE (2.5).
Let
- (H1)
for any (y, z) ∈ Rk × Rk×d, f(·, y, z) and g(·, y, z) are {ℱt}-progressively measurable processes, such that
() - (H2)
f and g satisfy Lipschitz condition with Lipschitz coefficient v : = {v(t)}; that is, there exists a positive nonrandom function {v(t)} such that
()for all (t, yi, zi) ∈ R+ × Rk × Rk×d, i = 1,2, - (H3)
.
3. Existence and Uniqueness Theorem
The following existence and uniqueness theorem is our main result.
Theorem 3.1. Under the above conditions, in particular (H1), (H2), and (H3), (2.5) has unique solution (y, z) ∈ B2.
In order to prove the existence and uniqueness theorem, one first gives an a priori estimate.
Lemma 3.2. Suppose (H1), (H2), and (H3) hold for f and g. For any T ∈ [0, ∞], let , (Yi, Zi) and (yi, zi) ∈ B2 (i = 1,2) satisfy the following equation:
Proof. Firstly, we assume that τ = 0, T = ∞.
Set
On the other hand, from (3.4) it follows that
Consequently, (3.8) and (3.9) imply that
For any τ, T ∈ [0, ∞], we set f1(t, yt, zt) = f(t, yt, zt)I[τ,T], and g1(t, yt, zt) = g(t, yt, zt)I[τ,T]. Then f1, and g1 satisfy the assumptions (H1), (H2), and (H3), and their Lipschitz constants are vI[τ,T].
Obviously,
On the other hand, from (3.11) it follows that
Martingale Representation Theorem [4] Suppose Y is a random variable, such that E | Y2 | < ∞. Note that Mt = E[Y∣𝒢t] is a square integrable martingale with respect to 𝒢t and can be represented using martingale representation theorem as , where .
Now we give the proof of the Theorem 3.1.
Proof. The proof of Theorem 3.1 is divided into two steps.
Step 1. We assume . For any (y, z) ∈ B2, let
Now we are in the position to prove that ϕ is a contractive mapping. Supposing that (yi, zi) ∈ B2, let (Yi, Zi) be the map ϕ of (yi, zi), (i = 1,2), that is
Due to l[0,∞] ≤ 1/2C, it follows that ϕ is a contractive mapping from B2 to B2.
Step 2. Since , then there exists a sufficiently large constant T such that
Remark 3.3. Suppose v is a constant, if we choose v(t) = vI[0,T](t), then Theorem 3.1 is the main theorem in the paper by Pardoux and Peng [1].
Remark 3.4. The condition (H3) is usually necessary. That is, if for any ξ ∈ L2(Ω, ℱ, P; Rk) and f, g hold in (H1) and (H2), BDSDE (2.5) has a unique solution in B2, then the (H3) is necessary.
In fact, let us choose f(s, ys, zs) = (1/(1 + s))zs, g(s, ys, zs) = 0 and any ξ ∈ L2(Ω, ℱ, P; Rk), then the solution of BDSDE
Thus the assumption (H3) is necessary.
Remark 3.5. The following example shows that if the coefficients f and g of BDSDE (2.5) satisfy the uniformly Lipschitz, the BDSDE (2.5) has no solution.
For all T > 0, let , then the BDSDE has a unique solution pair ,
When T → ∞, and in L2(Ω, ℱ, P), but zt = 1/(1 + t) is not the solution of the following infinite horizon BDSDE:
4. Continuous Dependence Theorem
In this section we will discuss the convergence of solutions of infinite horizon BDSDEs. First we give the following continuous dependence theorem.
Theorem 4.1. Suppose ξi ∈ L2(Ω, ℱ, P; Rk), (i = 1,2), and consider (H1)–(H3). Let (yi, zi) be the solutions of BDSDE (2.5) corresponding to the terminal data ξ = ξ1, ξ = ξ2, respectively. Then there exists a constant such that
Proof. Set , . Since , we can choose a strictly increasing sequence 0 = t0 < t1 < ⋯<tn < tn+1 = ∞ such that
Now we can assert the following convergence theorem for infinite horizon BDSDEs.
Theorem 4.2. Suppose ξ, ξi ∈ L2(Ω, ℱ, P; Rk), (i = 1,2, …), (H1)–(H3) hold for f and g. Let (yi, zi) be the solutions of the following BDSDE:
Proof. For any n, m ≥ 1, let (yn, zn) and (ym, zm) be the solutions of (4.7) corresponding to ξn and ξm, respectively. Due to Theorem 4.1, there exists a constant such that
Corollary 4.3. Assume ξ ∈ L2(Ω, ℱ, P; Rk), (H1)–(H3) hold for f and g. Let (y, z) be the solution of BDSDE (2.5). For any T > 0, let (yT, zT) be the solutions of the finite time interval BDSDE (4.11), then(yT, zT)→(y, z) in B2 as T → ∞.
Proof. Note that in L2(Ω, ℱ, P; Rk) as T → ∞. The proof is straightforward from Theorem 4.2.
5. BDSDEs and Systems of Quasilinear SPDEs
In this section, we study the link between BDSDEs and the solution of a class of SPDEs.
Let us first give some notations. Ck(Rp; Rq), , will denote, respectively, the set of functions of classes from Rp into Rq, the set of those functions of class Ck whose partial derivatives of order less than or equal to k are bounded (and hence the function itself grows at most linearly at infinity), and the set of those functions of class Ck which, together with all their partial derivatives of order less than or equal to k, grow at most like a polynomial function of the variable x at infinity.
It is well known that the solution defines a stochastic flow of diffeomorphism and denotes by the inverse flow (see e.g., [15]). The random field ; s ≥ t, x ∈ Rd has a version which is a.s. of class C2 in x, the function and its derivatives being a.s. continuous with respect to (t, s, x).
We assume that for any s ≥ t, (x, y, z)→(f(s, x, y, z), g(s, x, y, z)) is of class C3, and all derivatives are bounded on [0, ∞) × Rd × Rk × Rk×d.
Theorem 5.1. Let κ(t, x); t ≥ 0, x ∈ Rd be a random field such that κ(t, x) is -measurable for each (t, x), κ ∈ C0,2([0, ∞) × Rd; Rk) a.s., and κ satisfies (5.4). Then , where solves the BDSDE (5.3).
Proof. We can apply the extension of the Itô formula [5] to the solution κ of (5.4):
We have also a converse to Theorem 5.1.
Acknowledgments
This work is supported by the Colleges and Universities Outstanding Young Teacher Domestic Visiting Scholar of Shandong Province Project (2012) and the Nature Science Foundation of Shandong Province of China (Grant no. ZR2010AL014).