Motivation
A McKean–Vlasov or mean-field stochastic differential equation is an SDE whose coefficients depend on the law of the solution itself. Such equations describe the limit of large systems of weakly interacting particles (Kac's kinetic models, McKean's propagation of chaos) and are the state dynamics of mean-field games and mean-field control. For a classical diffusion the expectation of a terminal payoff is a function of time and state and solves a linear parabolic PDE (the Feynman–Kac connection). For a mean-field diffusion the same expectation depends on time, on the state and on the current law of the population, so the associated PDE lives on [0,T]×Rd×P2(Rd), an infinite-dimensional space of probability measures. Buckdahn, Li, Peng and Rainer (arXiv:1407.1215, Ann. Probab. 2017) prove that this value function is the unique classical solution of its PDE, using the derivative with respect to measures introduced by P.-L. Lions in his Collège de France lectures.
Timeline. McKean (1966) introduced the equations; Sznitman (1991) gave the propagation-of-chaos theory. Buckdahn, Djehiche, Li and Peng (2009) and Buckdahn, Li and Peng (2009) studied mean-field backward SDEs and the associated PDEs in a form where the law enters only through the coefficients. Lions (2007–2012 lectures, notes by Cardaliaguet 2013) introduced differentiation on P2(Rd) through lifts to L2. Carmona and Delarue (arXiv:1303.5835, 2013; arXiv:1404.4694, 2014) developed the Itô formula on the Wasserstein space and the master equation for mean-field games. The present paper (2014) proves the classical-solution result for the decoupled forward equation under second-order regularity of the coefficients in (x,μ).
Setting
Let (Ω,F,P) be a complete probability space carrying a d-dimensional Brownian motion B, let T>0, and let F0⊂F be a sub-σ-field independent of B that is rich: every μ∈P2(Rd) is the law Pϑ of some ϑ∈L2(F0;Rd). Here P2(Rd) is the set of probability measures with finite second moment, with the 2-Wasserstein distance W2(μ,ν)=(infρ∫∣x−y∣2dρ)1/2, the infimum over couplings ρ of μ and ν. The filtration is Ft=σ{Br,r≤t}∨F0∨NP.
Given Lipschitz coefficients σ:Rd×P2(Rd)→Rd×d, b:Rd×P2(Rd)→Rd, a time t∈[0,T], x∈Rd and ξ∈L2(Ft;Rd), the processes Xt,ξ and Xt,x,ξ solve on [t,T]
Xst,ξ=ξ+∫tsσ(Xrt,ξ,PXrt,ξ)dBr+∫tsb(Xrt,ξ,PXrt,ξ)dr,
Xst,x,ξ=x+∫tsσ(Xrt,x,ξ,PXrt,ξ)dBr+∫tsb(Xrt,x,ξ,PXrt,ξ)dr.
The second process depends on ξ only through Pξ, so for Φ:Rd×P2(Rd)→R the value function V(t,x,Pξ)=E[Φ(XTt,x,Pξ,PXTt,ξ)] is a function on [0,T]×Rd×P2(Rd).
A function f:P2(Rd)→R has Lions derivative ∂μf(μ,y)∈Rd if its lift ϑ↦f(Pϑ) on L2(F;Rd) is Fréchet differentiable with derivative η↦E[∂μf(Pϑ,ϑ)⋅η]. The classes Cb1,1 and Cb2,1 ask for one or two such derivatives (together with derivatives in x and in the extra variable y), all bounded and Lipschitz. Hypothesis (H.2) asks that σ and b be bounded and that every component be in Cb2,1(Rd×P2(Rd)).
Formalization targets
Goal: Theorem 6.2
Under (H.2) and Φ∈Cb2,1(Rd×P2(Rd)), V belongs to Cb1,(2,1)([0,T]×Rd×P2(Rd)) and is the unique solution in that class of
0=∂tV+i∑∂xiVbi(x,μ)+21i,j,k∑∂xixj2V(σi,kσj,k)(x,μ)+∫[i∑(∂μV)i(t,x,μ,y)bi(y,μ)+21i,j,k∑∂yi(∂μV)j(t,x,μ,y)(σi,kσj,k)(y,μ)]μ(dy),
V(T,x,μ)=Φ(x,μ).
The goal also records that V(t,x,Pξ) does not depend on the choice of ξ with a given law.
Milestones
In the order the proof uses them: the second-order expansion on P2 (Lemma 2.1); symmetry of mixed derivatives (Lemma 4.1); the substitution identity and flow property (3.4)–(3.5); the stability estimate E[sups∣Xst,x1,ξ1−Xst,x2,ξ2∣p]≤Cp(∣x1−x2∣p+W2(Pξ1,Pξ2)p) (Lemma 3.1) and its consequence that Xt,x,ξ depends only on Pξ (Remark 3.1); first- and second-order regularity of V in (x,μ) (Lemmas 5.1, 5.2) and in t (Lemma 6.1); the mean-field Itô formulas (Proposition 6.1, Theorem 6.1); the martingale identity (6.15); and uniqueness (6.19)–(6.20). A companion theorem states the existence and pathwise uniqueness of solutions of both SDEs under Lipschitz coefficients.
Significance
The result is a Feynman–Kac representation on the Wasserstein space: it identifies the expectation functional of a McKean–Vlasov diffusion with the unique classical solution of a second-order PDE in (t,x,μ), of the type that appears as the master equation of mean-field games and as the dynamic-programming equation of mean-field control. It gives a mean-field Itô formula for functions of the state and of the law, which is the basic tool for verification arguments in these problems.
All results of the mission are proved in the paper, which takes the well-posedness of the SDEs from Carmona and Delarue. None is formalized: the platform has the Itô integral as an L2 definition, but no Itô isometry, no Burkholder–Davis–Gundy inequality, no SDE existence theorem and no Itô formula (the classical Itô formula is posed separately as an open goal). Formalizing the mission produces a calculus on P2(Rd) in Lean, together with existence, stability and flow results for McKean–Vlasov equations.
Difficulty
The obvious route, differentiating V in μ by the chain rule, fails because μ↦Xt,x,μ is not a map between finite-dimensional spaces: the measure derivative of V requires Fréchet differentiability of ξ↦Xst,x,ξ in L2, the identification of the derivative through a family of auxiliary linear SDEs indexed by a point y∈Rd, and estimates uniform in y. A second difficulty is that the second-order expansion on P2 has remainder of order E[∣η∣3∧∣η∣2], not o(∣η∣L22), so the Itô formula is not a direct Taylor argument in L2 and needs a partition argument with control of each increment. A third is regularity in time: V is differentiable in t only after the Itô formula has been applied to Φ, and the time derivative must again be bounded and Hölder. The paper writes its proofs for d=1 and b=0 and leaves some estimates to the reader, so a solver must supply them.
Formalization scope
Time is ℝ≥0, Rd is EuclideanSpace ℝ (Fin d), measures are Measure (E d), and every condition on a measure argument is quantified over P2(Rd) only. W2 is the real value of the published WassersteinDRO.Duality.wassersteinDistance 2, finite on P2. Brownian motion, the Brownian filtration and the Itô integral are the published Peng1990.SMP objects, and the null sets are ReflectedBSDE.Existence.nullSigma. The standing assumptions of §3 are hypotheses of every statement: completeness, T>0, independence of B and F0, richness of F0, and the Lipschitz condition (stated even where (H.2) implies it). Matrices carry the Frobenius norm.
Solutions of (3.1) and (3.2) are processes in S2([t,T];Rd) satisfying the integral equation at every s∈[t,T] almost surely, with ∫tsσdB=J(s)−J(t) for Itô integrals J of 1(t,T]σ. Statements about V take solution families as hypotheses; the companion well-posedness theorem states that such families exist, and a sanity file shows that zero coefficients with constant solutions and Φ(x,μ)=⟨a,x⟩ satisfy every hypothesis. The decoupled equation takes a random initial value, so (3.4) needs no measurable selection in x.
Derivatives in x, y and t are genuine (HasGradientAt; HasDerivWithinAt on [0,T], one-sided at the ends). Derivatives in μ are witness functions with the Fréchet property of the lift, the lift being taken on the paper's own rich space; this rules out the trivializing reading in which every function is differentiable because the underlying space carries only Dirac laws. The subscript b bounds the derivatives, not the function, except that (H.1)/(H.2) also require σ and b themselves to be bounded on Rd×P2(Rd): this is the Cb1(Rd) of (H.1) ii), read uniformly in μ as the paper's proofs use it, and without it the bounded time derivative of V fails (e.g. b(x,μ)=x). The class Cb1,(2,1) additionally requires the derivatives entering the Itô formula to be jointly continuous in (t,x,μ,y) for W2; this is the reading of the letter C, and V satisfies it. E~ over an independent copy is the integral against the corresponding law. Where the page writes C2,1 or C1,(2,1) without b, the bounded classes the paper defines are used. The uniqueness statement ranges over every function of the class with its own derivatives.
A complete development needs the Itô isometry and BDG inequality for the published integral, Gronwall's inequality, strong existence for McKean–Vlasov SDEs, L2-differentiability of SDE solutions with respect to the initial condition, and a classical multidimensional Itô formula. The Lions-derivative calculus and the Wasserstein estimates are reusable for any mean-field mission. Contributions to any of these pieces are welcome.
Selected references
- R. Buckdahn, J. Li, S. Peng, C. Rainer, Mean-field stochastic differential equations and associated PDEs, arXiv:1407.1215v1, 2014; Ann. Probab. 45(2), 2017. https://arxiv.org/abs/1407.1215 , https://doi.org/10.1214/15-AOP1076
- R. Carmona, F. Delarue, Forward-backward stochastic differential equations and controlled McKean-Vlasov dynamics, arXiv:1303.5835, 2013; Ann. Probab. 43(5), 2015. https://arxiv.org/abs/1303.5835
- R. Carmona, F. Delarue, The master equation for large population equilibriums, arXiv:1404.4694, 2014. https://arxiv.org/abs/1404.4694
- P. Cardaliaguet, Notes on mean field games (from P.-L. Lions' lectures at Collège de France), 2013. https://www.ceremade.dauphine.fr/~cardaliaguet/MFG20130420.pdf
- R. Buckdahn, J. Li, S. Peng, Mean-field backward stochastic differential equations and related partial differential equations, Stochastic Process. Appl. 119, 2009. https://doi.org/10.1016/j.spa.2009.05.002
- A.-S. Sznitman, Topics in propagation of chaos, École d'Été de Probabilités de Saint-Flour XIX, Lecture Notes in Math. 1464, Springer, 1991. https://doi.org/10.1007/BFb0085169