Motivation
A forward–backward stochastic differential equation (FBSDE) couples a forward SDE, solved from an initial state, with a backward SDE, solved from a terminal condition that depends on the forward state. Such systems arise from the stochastic maximum principle, from quasilinear parabolic PDEs through Feynman–Kac formulas, and in mathematical finance. Whenever a control problem or a market model is solved through its first-order conditions, a fully coupled FBSDE appears, and the question is whether it has a unique solution.
The history has a recurring gap: each method covers a different regime, and none handles coefficients that are random, fully coupled, and have a forward diffusion depending on the martingale integrand Z, over an arbitrary horizon.
- 1993: F. Antonelli proved well-posedness over a small time interval by contraction, under a smallness condition on the coupling.
- 1994: J. Ma, P. Protter and J. Yong introduced the four-step scheme, solving Markovian FBSDEs with deterministic coefficients over arbitrary horizons through a quasilinear PDE; the forward diffusion may not depend on z in a degenerate way.
- 1995–1999: Y. Hu, S. Peng and Z. Wu developed the method of continuation, which allows random coefficients over arbitrary horizons under a monotonicity condition on the coefficients.
- 1999–2002: E. Pardoux and S. Tang, and F. Delarue, extended the PDE and fixed-point approaches under weak-coupling or strong-monotonicity conditions, in the Markovian setting.
- 2015: J. Ma, Z. Wu, D. Zhang and J. Zhang (the source of this mission) gave a unified approach through the decoupling field and a scalar ordinary differential equation that dominates its spatial derivative.
Setting
Fix a horizon T>0 and a probability space carrying a one-dimensional Brownian motion B, with F its natural filtration augmented by the null sets. All processes are real valued. The FBSDE (1.1) is
Xt=x+∫0tb(s,Θs)ds+∫0tσ(s,Θs)dBs,Yt=g(XT)+∫tTf(s,Θs)ds−∫tTZsdBs,
for t∈[0,T], with Θ=(X,Y,Z). The coefficients b,σ,f depend on (t,ω,x,y,z) and g on (x,ω). Assumption 2.1 asks that they be progressively measurable for fixed (x,y,z), that I02=E{(∫0T[∣b∣+∣f∣](t,0,0,0)dt)2+∫0T∣σ∣2(t,0,0,0)dt+∣g(0)∣2} be finite, and that they be Lipschitz in (x,y,z) with a common constant K0, uniformly in ω. Solutions are sought in the space L2 of progressively measurable Θ with ∥Θ∥L22=E{supt(∣Xt∣2+∣Yt∣2)+∫0T∣Zt∣2dt}<∞.
A decoupling field (Definition 2.2) is a random field u(t,x) with u(T,⋅)=g such that, on every short interval [t1,t2] and from every square-integrable initial state, the FBSDE with terminal map u(t2,⋅) is uniquely solvable and its solution satisfies Yt=u(t,Xt).
The difference quotients (3.1) of the coefficients — b~i,σ~i,f~i in the variables x,y,z (i=1,2,3) and h~ for g — enter the scalar function
F=f1+f2y+y(b1+b2y)+1−σ3y(f3+b3y)y(σ1+σ2y),
and its essential supremum F(t,y) and infimum F(t,y) over all quotients give the dominating ODEs (3.13): yt=h+∫tTF(s,ys)ds and yt=h+∫tTF(s,ys)ds, with h,h the bounds of h~.
Formalization targets
Goal: Theorem 7.4
Fix c1,c2,c3 with c1>0, 0<c2<c3, c1c3<1 (5.13). There are ε>0 and C>0, depending only on T, K0 and c1,c2,c3, such that whenever Assumption 2.1 holds and the quotients satisfy one of the nine conditions of Cases I–III ((5.14); (5.15)–(5.18); (5.19)–(5.22)), uniformly in the quotient arguments, then (i) the FBSDE has a decoupling field u whose quotient (u(t,x1)−u(t,x2))/(x1−x2) obeys the bound assumed of h~ with c2 replaced by c3, and (ii) for every x there is a unique solution in L2, with
∥Θ∥L22≤C[∣x∣2+I02].
Milestones
- Lemma 5.1: comparison for scalar backward ODEs between a sub- and a super-solution.
- Theorems 5.9, 5.10, 5.11: under each case, the dominating ODEs have bounded solutions with the bound of h transported to c3, and 1−σ3y stays away from 0.
- Theorems 6.1, 6.2, 6.3: over a short horizon T≤δ, unique solvability, solutions of (3.13) in a band, and a random field u whose quotients lie between y and y.
- Theorem 2.3: a decoupling field gives a unique global solution with Yt=u(t,Xt).
A companion statement, Corollary 7.5, gives well-posedness over [0,T] under the sign conditions (7.5) or (7.6), with no smallness constant.
Significance
The theorem replaces structural assumptions (small horizon, monotonicity, deterministic coefficients, σ independent of z) by conditions that can be read off the coefficients through a scalar ODE. It covers random coefficients and a forward diffusion that depends on z, the case in which the classical Riccati-type obstruction σ3h=1 appears, and it recovers the earlier sufficient conditions as special cases (§7.4 of the paper). The decoupling field produced in (i) is uniformly Lipschitz, which is the input to the comparison and stability results of §8 and to numerical schemes based on Yt=u(t,Xt).
The result is proved in the paper; nothing here is open mathematically. None of it is formalized: there is no machine-checked existence theory for coupled FBSDEs in any proof assistant this mission is aware of. A complete development would be the first formal well-posedness theorem for a fully coupled FBSDE, and the milestones — the ODE comparison lemma, the small-time theory, and the patching argument of Theorem 2.3 — are each self-contained.
Difficulty
The obvious approach is a contraction argument on [0,T]. It works only when T is small, because the Lipschitz constant of the solution map grows with the coupling; iterating it over a partition requires a terminal condition u(ti,⋅) whose Lipschitz constant does not deteriorate from one subinterval to the next. Controlling that constant is the whole problem. Its spatial derivative satisfies a backward stochastic Riccati equation with quadratic growth in both y and z and a singularity where 1−σ3y=0; such equations need not have bounded solutions, and the standard comparison theory for quadratic BSDEs does not apply off the region where the generator is Lipschitz. A second difficulty is the small-time theory itself: when σ depends on z, even a linear FBSDE with constant coefficients is well posed on short intervals only if σ3h=1 (Theorem 7.1 of the paper), so in Cases II and III, where σ3 and h are large, the contraction argument does not apply even for small T.
Formalization scope
The development reuses the platform's Peng1990.SMP.Stochastic (standard Brownian motion, LF2, the L2 Itô integral IsItoIntegral) and the augmented Brownian filtration of ReflectedBSDE.Existence.Setting. Time is R≥0, time integrals are over real intervals, and the stochastic integral ∫t1tσdB is Jt−Jt1 for an Itô integral process J of 1(t1,t2]σ(s,Θs).
Committed conventions:
- Lipschitz bounds use the ℓ1 norm on R3 and hold for every ω; I02 and ∥Θ∥L22 are lower Lebesgue integrals in [0,∞].
- Uniqueness is uniqueness in L2: X,Y agree a.s. at each time and Z agrees dt⊗dP-a.e.
- Solutions are unique only up to modification, so (7.2) is asserted for one solution in L2.
- Definition 2.2's "0=t1<t2≤T" is read as 0≤t1, as the proof of Theorem 2.3 uses it.
- Every condition on the quotients holds for every t∈[0,T], almost surely, for all arguments with distinct coordinates. F(t,c)≤ε is stated in exactly that form. F,F,h,h as functions are EReal-valued, and solutions of (3.13) keep them finite.
- "(1−σ3y)−1 is bounded" is ∣1−σ~3yt∣≥κ>0. Every use of α3=b2−b3σ2/σ3 carries σ~3=0, and (5.19), (5.21) carry the heading σ3=0 of Table 3 in the goal.
- The quotient bounds on u hold for each t and each pair x1=x2 almost surely.
- Lemma 5.1 additionally assumes y1≤y2 and L≥0, both implicit on the page.
The constants ε, δ and C are chosen before the probability space and the coefficients. A formalization that places them after the coefficients, integrates without integrability, divides at the pole 1−σ3y=0, uses a real-valued essential supremum of an unbounded family, or states uniqueness without a solution class would make the statements vacuous or false; none of these is used.
Contributions are welcome on every milestone. The ODE layer (Lemma 5.1 and the a priori bounds of Theorems 5.9–5.11) needs only real analysis and is a natural first target. The stochastic layer needs Itô-integral facts (linearity, restriction to subintervals, the Burkholder–Davis–Gundy and Doob inequalities in L2) and the Lipschitz BSDE theory; these are reusable well beyond this mission.
Selected references
- J. Ma, Z. Wu, D. Zhang, J. Zhang, On well-posedness of forward–backward SDEs—a unified approach, Ann. Appl. Probab. 25(4):2168–2214, 2015. https://arxiv.org/abs/1110.4658
- F. Antonelli, Backward–forward stochastic differential equations, Ann. Appl. Probab. 3(3):777–793, 1993. https://doi.org/10.1214/aoap/1177005363
- J. Ma, P. Protter, J. Yong, Solving forward–backward stochastic differential equations explicitly — a four step scheme, Probab. Theory Related Fields 98:339–359, 1994. https://doi.org/10.1007/BF01192258
- Y. Hu, S. Peng, Solution of forward–backward stochastic differential equations, Probab. Theory Related Fields 103:273–283, 1995. https://doi.org/10.1007/BF01204218
- S. Peng, Z. Wu, Fully coupled forward–backward stochastic differential equations and applications to optimal control, SIAM J. Control Optim. 37(3):825–843, 1999. https://doi.org/10.1137/S0363012996313549
- F. Delarue, On the existence and uniqueness of solutions to FBSDEs in a non-degenerate case, Stochastic Process. Appl. 99:209–286, 2002. https://doi.org/10.1016/S0304-4149(02)00085-6
- J. Ma, J. Yong, Forward–Backward Stochastic Differential Equations and their Applications, Lecture Notes in Math. 1702, Springer, 1999. https://doi.org/10.1007/978-3-540-48831-6