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Stochastic Systems

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The mathematics of systems that evolve under randomness, modeled as families of random variables indexed by time — from Markov chains and martingales to Brownian motion and stochastic differential equations. The field spans stochastic analysis, filtering and optimal control under uncertainty, ergodic behavior of random dynamics, and concentration of measure, with models reaching across physics, engineering, finance, and biology.

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Operations ResearchOptimization·Captain: mikedeng1

Stochastic Dual Dynamic Integer Programming 1: With Valid, Tight and Finite Cuts, Stochastic Nested Decomposition Finds an Optimal Solution in Finitely Many Iterations with Probability OneResearch Paper

Motivation

Multistage stochastic programs model decisions taken over time while uncertain data are revealed: generation scheduling in hydro-thermal power systems, capacity expansion, unit commitment, portfolio management. When the uncertainty is represented by a finite scenario tree, the problem becomes one very large deterministic program, and decomposition algorithms solve it stage by stage. For linear problems the standard methods are nested Benders decomposition and its sampling variant, stochastic dual dynamic programming (SDDP), introduced by Pereira and Pinto (1991). Both rely on the convexity of the value functions, which they approximate from below by linear cuts.

Many applications need integer decisions (on/off status of generators, investment choices), and integer variables destroy convexity. Zou, Ahmed and Sun (Math. Program. 175 (2019) 461–502) observed that when the state variables passed between stages are binary, exact convex polyhedral representations still exist on the binary points. They proposed stochastic nested decomposition (SND) and its stage-wise independent special case SDDiP, and identified three properties of cuts (valid, tight, finite) under which the algorithms converge. This mission formalizes that convergence theorem, Theorem 2 of the paper.

Timeline. Birge (1985) gave nested decomposition for multistage linear programs; Pereira and Pinto (1991) introduced SDDP. Philpott and Guan (2008) proved almost sure finite convergence of SDDP-type methods for linear problems, and Girardeau, Leclère and Philpott (2015) extended convergence to convex problems. Zou, Ahmed and Sun (2019) proved finite convergence with probability one for mixed integer problems with binary states and abstract valid, tight and finite cuts, and showed that their Lagrangian cuts have the first two properties.

Setting

Let T\mathcal TT be a scenario tree with stages 1,…,T1,\dots,T1,…,T, root 111, parent map a(n)a(n)a(n) and children C(n)\mathcal C(n)C(n). The nodes of the last stage are the scenarios. Node probabilities satisfy pn>0p_n>0pn​>0, p1=1p_1=1p1​=1, and pn=∑m∈C(n)pmp_n=\sum_{m\in\mathcal C(n)}p_mpn​=∑m∈C(n)​pm​ before the last stage, and qnm=pm/pnq_{nm}=p_m/p_nqnm​=pm​/pn​. Each node has a linear cost fn(xn,yn)f_n(x_n,y_n)fn​(xn​,yn​) and a nonempty compact mixed integer polyhedral set XnX_nXn​ (assumption (A1)). The state xn∈{0,1}dx_n\in\{0,1\}^dxn​∈{0,1}d is binary, the local variables yny_nyn​ are general, and the root's parent state xˉ0\bar x_0xˉ0​ is fixed. The problem in local-copy form (2.1) is

min⁡∑n∈Tpnfn(xn,yn)s.t.(zn,xn,yn)∈Xn, zn=xa(n), xn∈{0,1}d.\min\sum_{n\in\mathcal T}p_nf_n(x_n,y_n)\quad\text{s.t.}\quad(z_n,x_n,y_n)\in X_n,\ z_n=x_{a(n)},\ x_n\in\{0,1\}^d .minn∈T∑​pn​fn​(xn​,yn​)s.t.(zn​,xn​,yn​)∈Xn​, zn​=xa(n)​, xn​∈{0,1}d.

Its value functions satisfy the recursion (2.3): Qn(xa(n))=min⁡{fn(xn,yn)+Qn(xn)}Q_n(x_{a(n)})=\min\{f_n(x_n,y_n)+\mathcal Q_n(x_n)\}Qn​(xa(n)​)=min{fn​(xn​,yn​)+Qn​(xn​)} over the nodal feasible set, with the expected cost-to-go function Qn(x)=∑m∈C(n)qnmQm(x)\mathcal Q_n(x)=\sum_{m\in\mathcal C(n)}q_{nm}Q_m(x)Qn​(x)=∑m∈C(n)​qnm​Qm​(x).

The SND algorithm keeps an under-approximation ψni\psi^i_nψni​ of each Qn\mathcal Q_nQn​: the maximum of a lower bound LnL_nLn​ and the aggregated cuts ∑m∈C(n)qnm(vmℓ+(πmℓ)⊤x)\sum_{m\in\mathcal C(n)}q_{nm}(v^\ell_m+(\pi^\ell_m)^\top x)∑m∈C(n)​qnm​(vmℓ​+(πmℓ​)⊤x) collected so far (3.2). Each iteration iii samples MMM scenarios with replacement. In the forward step it solves the nodal problems Pni(xa(n)i,ψni)P^i_n(x^i_{a(n)},\psi^i_n)Pni​(xa(n)i​,ψni​) from the root down, which yields the forward tree solution {(xni,yni)}\{(x^i_n,y^i_n)\}{(xni​,yni​)} of (3.6). In the backward step, at every sampled node it generates one cut per child at the state xnix^i_nxni​ and adds their aggregate to ψn\psi_nψn​. Cuts are valid if Qm(x)≥vmi+(πmi)⊤xQ_m(x)\ge v^i_m+(\pi^i_m)^\top xQm​(x)≥vmi​+(πmi​)⊤x on {0,1}d\{0,1\}^d{0,1}d (3.4). They are tight if they equal the value Q‾mi(xni,ψmi+1)\underline Q^i_m(x^i_n,\psi^{i+1}_m)Q​mi​(xni​,ψmi+1​) of the child's updated nodal problem at xnix^i_nxni​ (3.5). They are finite if only finitely many distinct cuts occur. Assumption (A3) requires the nodal solver to return the same optimal solution whenever it is given the same problem.

Formalization targets

Goal: Theorem 2 (p. 474)

With sampling with replacement, valid, tight and finite cuts, and a solver satisfying (A3), the following holds with probability one:

∃ i0  ∀i≥i0:{(xni,yni)}n∈T is an optimal solution of (2.1).\exists\, i_0\ \ \forall i\ge i_0:\quad \{(x^i_n,y^i_n)\}_{n\in\mathcal T}\ \text{is an optimal solution of (2.1)}.∃i0​  ∀i≥i0​:{(xni​,yni​)}n∈T​ is an optimal solution of (2.1).

Milestones, in the order the proof uses them

  1. Valid cuts give under-approximations, ψni≤Qn\psi^i_n\le\mathcal Q_nψni​≤Qn​ and Q‾ni≤Qn\underline Q^i_n\le Q_nQ​ni​≤Qn​ (proof of Claim 1, p. 475).
  2. Claim 1: if ψni(xni)=Qn(xni)\psi^i_n(x^i_n)=\mathcal Q_n(x^i_n)ψni​(xni​)=Qn​(xni​) for all nnn, the forward solution is optimal for (2.1) (p. 475).
  3. With finitely many possible cuts, the approximations {ψni}\{\psi^i_n\}{ψni​} change only in finitely many iterations (pp. 474–475).
  4. (3.8a)–(3.8f): a sampled node whose children are exact becomes exact after its backward step (p. 476).
  5. Under sampling with replacement, every scenario is sampled in infinitely many iterations, almost surely (p. 476).
  6. Claim 2: almost surely, no infinite block of unchanged approximations has a non-optimal forward solution (p. 475).

Significance

Theorem 2 separates the convergence of nested decomposition from the choice of cuts. Any cut family with the three properties yields an exact algorithm for multistage stochastic integer programs with binary states. The paper verifies the properties for integer optimality cuts and, through its Theorem 3, shows that Lagrangian cuts from the local-copy reformulation are valid and tight. The convergence of SDDiP, the variant used in computations, follows from the same theorem, and binary expansion of general integer states extends the reach to mixed integer state spaces.

The result is proved in the paper; no machine-checked proof exists. A formal development would turn its informal points into checked statements: that the minima are attained, that the DP recursion is equivalent to the extensive form, and that the finiteness of cuts is global. It would also supply a reusable framework (scenario trees with node probabilities, cut-based approximations, sampled runs) for the convergence theory of SDDP-type methods.

Difficulty

No single step is deep; the difficulty is the interaction of the pieces. A tempting argument says the approximations stop changing, so the algorithm stops at an optimum. But a stalled run need not be optimal: if a node at which ψn\psi_nψn​ is inexact is never sampled again, nothing changes and the forward solution stays suboptimal. The proof must therefore combine three things: the deterministic finiteness of changes, an almost sure statement about sampling, and the exactness chain (3.8). That chain depends on tightness with respect to the updated approximation of the child, and it fails if tightness refers to the approximation from before the backward step. The equivalence between optimality for the DP recursion and for the extensive form (2.1), used without proof in Claim 1, also requires a backward induction over the tree.

Formalization scope

The tree is the platform definition StochasticProg.Multistage.Tree H, with stage ttt of the paper equal to stage = t − 1. Binary vectors are Fin d → Bool, embedded in Rd\mathbb R^dRd. The copy variable znz_nzn​ is eliminated through zn=xa(n)z_n=x_{a(n)}zn​=xa(n)​. Minima are written as infima over sets that the standing assumptions make nonempty, bounded below and attained. Lean iterations are numbered from 000, and the run is infinite (stopping criteria and bounds play no role).

Readings of informal words. "Optimal solution of (2.1)" means a feasible tree solution of least cost ∑npnfn\sum_np_nf_n∑n​pn​fn​ among all feasible tree solutions. "After a finite number of iterations" means from some iteration on, in every iteration (∀ᶠ i in atTop). "With probability one" refers to a probability space carrying independent draws, M≥1M\ge1M≥1 per iteration, each with law {pn:n∈ST}\{p_n:n\in S_T\}{pn​:n∈ST​}. "Finite" cuts means one finite set for the whole run, as the proof uses it, not a different finite set per iteration. (A3) means the solver is a function of the node, the parent state and the approximation, and returns an optimal solution.

Added hypotheses, which the paper uses without stating them: pn>0p_n>0pn​>0; every nodal problem is feasible for every binary parent state, which replaces (A2) (not used by Theorem 2); and the lower bounds under-estimate, Ln≤QnL_n\le\mathcal Q_nLn​≤Qn​, which is Algorithm 1's "initial under-approximation".

Trivializing formalizations are ruled out: tightness refers to the child's approximation after its own update, optimality is for the true extensive form and not relative to ψ\psiψ, and the probability statement is over independent sampling, not over a fixed sample sequence assumed to visit every scenario.

Contributions welcome: the attainment lemmas for nodal minima, the DP/extensive-form equivalence on trees, and the second Borel–Cantelli argument for repeated sampling. All of these are reusable for other SDDP-type convergence results.

Selected references

  • J. Zou, S. Ahmed, X. A. Sun, Stochastic dual dynamic integer programming, Math. Program. 175 (2019) 461–502. https://doi.org/10.1007/s10107-018-1249-5
  • M. V. F. Pereira, L. M. V. G. Pinto, Multi-stage stochastic optimization applied to energy planning, Math. Program. 52 (1991) 359–375. https://doi.org/10.1007/BF01582895
  • A. B. Philpott, Z. Guan, On the convergence of stochastic dual dynamic programming and related methods, Oper. Res. Lett. 36 (2008) 450–455. https://doi.org/10.1016/j.orl.2008.01.013
  • P. Girardeau, V. Leclère, A. B. Philpott, On the convergence of decomposition methods for multistage stochastic convex programs, Math. Oper. Res. 40 (2015) 130–145. https://doi.org/10.1287/moor.2014.0664
  • J. R. Birge, Decomposition and partitioning methods for multistage stochastic linear programs, Oper. Res. 33 (1985) 989–1007. https://doi.org/10.1287/opre.33.5.989
10 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Universality of Power-of-d Load Balancing in Many-Server Systems 2: JSQ(d(N)) with d(N)/(√N log N) → ∞ Has the Same Halfin–Whitt Diffusion Limit as the Join-the-Shortest-Queue PolicyResearch Paper

Motivation

A data center or cloud platform routes each incoming task to one of NNN parallel servers. Sending each task to a server with the shortest queue, the join-the-shortest-queue (JSQ) policy, minimizes waiting in a strong sense, but the dispatcher must learn all NNN queue lengths for every arrival. The power-of-d schemes cut this communication: the dispatcher samples ddd servers and joins the shortest of them. Mukherjee, Borst, van Leeuwaarden and Whiting ask how large d=d(N)d=d(N)d=d(N) must be for the sampled scheme to perform as well as JSQ as N→∞N\to\inftyN→∞. They answer at two scales. At the fluid scale (mission 1 of this series) d(N)→∞d(N)\to\inftyd(N)→∞ suffices. At the diffusion scale of the Halfin–Whitt regime, the subject of this mission, d(N)/(Nlog⁡N)→∞d(N)/(\sqrt N\log N)\to\inftyd(N)/(N​logN)→∞ suffices, and d(N)/(Nlog⁡N)→0d(N)/(\sqrt N\log N)\to 0d(N)/(N​logN)→0 does not.

Timeline:

  • Halfin and Whitt (1981) introduced the heavy-traffic regime (N−λ(N))/N→β>0(N-\lambda(N))/\sqrt N\to\beta>0(N−λ(N))/N​→β>0 for many-server systems.
  • Eschenfeldt and Gamarnik (2018, arXiv:1502.00999) proved the diffusion limit of ordinary JSQ in this regime, the system (2.4) below.
  • Mukherjee, Borst, van Leeuwaarden and Whiting (Stochastic Systems 8(4), 2018; arXiv:1612.00723v2) proved that JSQ(d(N)) has the same diffusion limit when d(N)/(Nlog⁡N)→∞d(N)/(\sqrt N\log N)\to\inftyd(N)/(N​logN)→∞ (Theorem 2.4), and that the limit differs when d(N)/(Nlog⁡N)→0d(N)/(\sqrt N\log N)\to 0d(N)/(N​logN)→0 (Theorem 2.5).

Setting

There are NNN servers, each with a buffer of size b∈{2,3,… }∪{∞}b\in\{2,3,\dots\}\cup\{\infty\}b∈{2,3,…}∪{∞} that counts the task in service. Tasks arrive as a Poisson process of rate λ(N)\lambda(N)λ(N), and each needs a unit-mean exponential amount of work, served at unit rate. A task sent to a full server is discarded. Under JSQ(d) the dispatcher samples ddd servers without replacement (1≤d≤N1\le d\le N1≤d≤N) and sends the task to a server with the shortest queue among them. For d=Nd=Nd=N this is JSQ.

The state is the occupancy vector Q=(Q1,…,Qb)Q=(Q_1,\dots,Q_b)Q=(Q1​,…,Qb​), where QiQ_iQi​ is the number of servers with at least iii tasks. The conventions are Q0=NQ_0=NQ0​=N and Qi=0Q_i=0Qi​=0 for i>bi>bi>b. With the servers ordered by nondecreasing queue length, the ccc-th ordered server has queue length I(c)=max⁡{i≥0:Qi≥N−c+1}I(c)=\max\{i\ge0:Q_i\ge N-c+1\}I(c)=max{i≥0:Qi​≥N−c+1}. An arrival at position ccc raises QI(c)+1Q_{I(c)+1}QI(c)+1​ by one when I(c)<bI(c)<bI(c)<b. A departure at position kkk lowers QI(k)Q_{I(k)}QI(k)​ by one when I(k)≥1I(k)\ge1I(k)≥1. JSQ(d) routes to the smallest position in a uniform ddd-subset of {1,…,N}\{1,\dots,N\}{1,…,N}.

In the Halfin–Whitt regime (N−λ(N))/N→β>0(N-\lambda(N))/\sqrt N\to\beta>0(N−λ(N))/N​→β>0, the diffusion-scaled state is

Qˉ1=−N−Q1N,Qˉi=QiN(i≥2).\bar Q_1=-\frac{N-Q_1}{\sqrt N},\qquad \bar Q_i=\frac{Q_i}{\sqrt N}\quad(i\ge2).Qˉ​1​=−N​N−Q1​​,Qˉ​i​=N​Qi​​(i≥2).

Here −Qˉ1-\bar Q_1−Qˉ​1​ is the scaled number of idle servers.

Formalization targets

Goal: Theorem 2.4 (pp. 7–8)

Let β>0\beta>0β>0, b≥2b\ge2b≥2 and k≥2k\ge2k≥2. Assume Qˉk+1(0)=0\bar Q_{k+1}(0)=0Qˉ​k+1​(0)=0 for large NNN and (Qˉ1(0),…,Qˉk(0))⇒ν(\bar Q_1(0),\dots,\bar Q_k(0))\Rightarrow\nu(Qˉ​1​(0),…,Qˉ​k​(0))⇒ν. If d(N)/(Nlog⁡N)→∞d(N)/(\sqrt N\log N)\to\inftyd(N)/(N​logN)→∞, then Qˉd(N)⇒Qˉ\bar Q^{d(N)}\Rightarrow\bar QQˉ​d(N)⇒Qˉ​ in Dℓ1[0,∞)D_{\ell_1}[0,\infty)Dℓ1​​[0,∞), where Qˉi≡0\bar Q_i\equiv 0Qˉ​i​≡0 for i≥k+1i\ge k+1i≥k+1 and

Qˉ1(t)=Qˉ1(0)+2W(t)−βt+∫0t(−Qˉ1+Qˉ2) ds−U1(t),Qˉ2(t)=Qˉ2(0)+U1(t)−∫0t(Qˉ2−Qˉ3) ds,Qˉi(t)=Qˉi(0)−∫0t(Qˉi−Qˉi+1) ds,3≤i≤k.\begin{aligned}\bar Q_1(t)&=\bar Q_1(0)+\sqrt2W(t)-\beta t+\int_0^t(-\bar Q_1+\bar Q_2)\,ds-U_1(t),\\ \bar Q_2(t)&=\bar Q_2(0)+U_1(t)-\int_0^t(\bar Q_2-\bar Q_3)\,ds,\\ \bar Q_i(t)&=\bar Q_i(0)-\int_0^t(\bar Q_i-\bar Q_{i+1})\,ds,\quad 3\le i\le k.\end{aligned}Qˉ​1​(t)Qˉ​2​(t)Qˉ​i​(t)​=Qˉ​1​(0)+2​W(t)−βt+∫0t​(−Qˉ​1​+Qˉ​2​)ds−U1​(t),=Qˉ​2​(0)+U1​(t)−∫0t​(Qˉ​2​−Qˉ​3​)ds,=Qˉ​i​(0)−∫0t​(Qˉ​i​−Qˉ​i+1​)ds,3≤i≤k.​

Here WWW is a standard Brownian motion and U1U_1U1​ is the nonnegative nondecreasing regulator with ∫0∞1[Qˉ1<0] dU1=0\int_0^\infty\mathbb 1_{[\bar Q_1<0]}\,dU_1=0∫0∞​1[Qˉ​1​<0]​dU1​=0. The goal also asserts that this solution is unique.

Milestones

  1. Uniqueness clause of Theorem 2.4: (2.4), with the constraint Qˉ1≤0\bar Q_1\le0Qˉ​1​≤0, has at most one solution for every driving path.
  2. Theorem 2.4 for d(N)=Nd(N)=Nd(N)=N: the JSQ diffusion limit of [8, Theorem 2], stated along an arbitrary sequence of server counts Nj→∞N_j\to\inftyNj​→∞.
  3. Proposition 5.1 (p. 32): if JSQ has the diffusion limit along every such sequence, then so does JSQ(d(N)) with d(N)/(Nlog⁡N)→∞d(N)/(\sqrt N\log N)\to\inftyd(N)/(N​logN)→∞.

The goal follows from 1–3.

Significance

The result. Theorem 2.4 shows that O(Nlog⁡N)O(\sqrt N\log N)O(N​logN) queue-length queries per arrival already achieve diffusion-level optimality: over any finite horizon only OP(N)O_P(\sqrt N)OP​(N​) servers are idle and only OP(N)O_P(\sqrt N)OP​(N​) hold two or more tasks, exactly as under JSQ. With Theorem 2.5 it identifies Nlog⁡N\sqrt N\log NN​logN as the minimal order of d(N)d(N)d(N). The diffusion limit is also the input for the steady-state analyses of JSQ in this regime (Braverman; Banerjee and Mukherjee).

Formalizing it. The result is proved on paper; nothing in it is machine-checked. A formalization needs:

  • a rigorous construction of the many-server JSQ(d) process;
  • the stochastic-coupling comparison of §3;
  • weak convergence of ℓ1\ell_1ℓ1​-valued processes;
  • a reflected integral equation of Skorokhod type.

The Eschenfeldt–Gamarnik limit (milestone 2) is cited by the paper, not proved in it, so its formalization is a separate, substantial contribution.

Difficulty

JSQ(d(N)) cannot be compared with JSQ path by path. The same arrival is routed to different servers under the two schemes, so their occupancy vectors drift apart and do not stay ordered. The obvious generator-based diffusion argument for JSQ(d(N)) itself does not close either. The routing probabilities depend on the whole ordered queue-length profile through (⋅d)/(Nd)\binom{\cdot}{d}/\binom{N}{d}(d⋅​)/(dN​)-type terms, and these do not reduce to a function of Qˉ1,Qˉ2\bar Q_1,\bar Q_2Qˉ​1​,Qˉ​2​ at scale N\sqrt NN​ unless d(N)d(N)d(N) is large enough.

The threshold is sharp: for d(N)≪Nlog⁡Nd(N)\ll\sqrt N\log Nd(N)≪N​logN the limit is different (Theorem 2.5). Any argument therefore has to use the growth rate quantitatively, controlling at scale oP(N)o_P(\sqrt N)oP​(N​) over a finite horizon how often JSQ(d(N)) fails to make a near-shortest choice. A qualitative fluid-type argument cannot do this. A second difficulty is the limit itself: (2.4) is a reflected equation whose regulator enters two coordinates, so even its well-posedness needs a Skorokhod-type argument with feedback.

Formalization scope

Lean conventions:

  • Levels and positions use the paper's index base: Q i is QiQ_iQi​ for i≥1i\ge1i≥1, with Q 0 = N, and positions are 1,…,N1,\dots,N1,…,N. The initial vector Fin k → ℝ lists levels 1,…,k1,\dots,k1,…,k.
  • Buffer b : ℕ∞ with 2 ≤ b; ⊤ is an infinite buffer.
  • Process construction is by uniformization. A Poisson clock of rate λ+N\lambda+Nλ+N is built from i.i.d. expMeasure (λ + N) interarrival times through the published renewalCount/partialSum. Its i.i.d. marks are arrivals, with probability λ/(λ+N)\lambda/(\lambda+N)λ/(λ+N) and a uniform ddd-subset, or departures at a uniform position. Marks are independent of the clock and of a random initial state. The model is therefore the paper's in law. Sampling is without replacement, so JSQ(N) is JSQ.
  • Path space. DS[0,∞)D_{\mathbb S}[0,\infty)DS​[0,∞) is read as ℓ1\ell_1ℓ1​-valued càdlàg paths, as the proof controls ℓ1\ell_1ℓ1​ distances. Weak convergence to the continuous limit is stated in coupling form: a common probability space with copies of the laws and almost sure uniform convergence in ℓ1\ell_1ℓ1​ on compacts.
  • Initial convergence is joint convergence in law of (Qˉ1(0),…,Qˉk(0))(\bar Q_1(0),\dots,\bar Q_k(0))(Qˉ​1​(0),…,Qˉ​k​(0)), via bounded continuous test functions. The page's coordinatewise convergence does not determine the limit. The limit's initial value is independent of WWW.
  • Solution concept of (2.4) includes Qˉ1≤0\bar Q_1\le0Qˉ​1​≤0, implicit in the paper; without it U1≡0U_1\equiv0U1​≡0 satisfies the complementarity condition and uniqueness fails. ∫1[Qˉ1<0]dU1=0\int\mathbb 1_{[\bar Q_1<0]}dU_1=0∫1[Qˉ​1​<0]​dU1​=0 is a Lebesgue–Stieltjes measure condition. WWW is Mathlib's IsBrownianReal.
  • "Same diffusion limit" in Proposition 5.1 is the paper's reduction: the JSQ result, for all server-count sequences, implies the JSQ(d(N)) result.

Trivializing formalizations are ruled out. The goal asserts the existence of the limit (Brownian motion, initial value and solution), not merely that every limit point solves (2.4). The system hypotheses are satisfiable: the mark law has total mass one, which is checked in Lean. The convergence is of the whole ℓ1\ell_1ℓ1​ path, including the tail above level kkk.

Infrastructure needed and welcome:

  • a library for ℓ1\ell_1ℓ1​-valued càdlàg processes;
  • the one-sided Skorokhod map with Lipschitz feedback, reusable for many reflected limits;
  • the S-coupling of §3, posed as milestones in mission 1 of this series;
  • a formal proof of the Eschenfeldt–Gamarnik JSQ limit.

Selected references

  • D. Mukherjee, S. C. Borst, J. S. H. van Leeuwaarden, P. A. Whiting, Universality of power-of-d load balancing in many-server systems, Stochastic Systems 8(4), 2018. arXiv:1612.00723v2, doi:10.1287/stsy.2018.0016
  • P. Eschenfeldt, D. Gamarnik, Join the shortest queue with many servers. The heavy-traffic asymptotics, Mathematics of Operations Research 43(3), 2018. arXiv:1502.00999
  • S. Halfin, W. Whitt, Heavy-traffic limits for queues with many exponential servers, Operations Research 29(3), 1981. doi:10.1287/opre.29.3.567
  • A. Braverman, Steady-state analysis of the join-the-shortest-queue model in the Halfin–Whitt regime, Mathematics of Operations Research 45(3), 2020. arXiv:1801.05121
10 thms1 active userReviewed
Control TheoryMarkov Chain·Captain: mikedeng1

Strong and Weak Equilibria for Time-Inconsistent Stochastic Control in Continuous Time 2: Under Pseudo-Exponential Discounting, a Two-State Generator Is a Weak but Not a Strong EquilibriumResearch Paper

Motivation

An agent whose preferences change over time cannot simply optimize once: a plan that is optimal today may be abandoned tomorrow by the agent's own "future selves". This is time inconsistency, and its standard source is non-exponential discounting, studied since Strotz (1955). The usual response, going back to Strotz and made rigorous in continuous time by Ekeland and Lazrak (2006), is to look for an equilibrium strategy: a strategy from which no future self wants to deviate. In continuous time "no incentive to deviate" is encoded through a first-order condition, which Huang and Zhou call a weak equilibrium.

Björk, Khapko and Murgoci (2017, Remark 3.5) observed that this first-order condition need not express the absence of an incentive to deviate: it only says that a derivative vanishes or is nonnegative, and a stationary point need not be a maximum. Huang and Zhou (Math. Oper. Res. 46(2), 2021; read here as arXiv:1809.09243v3) introduce a strong equilibrium, which requires the agent's payoff to be no better after any short deviation, and study the two notions for continuous-time Markov chains with controlled generators. This mission formalizes their main example (Example 4.3): a concrete two-state model in which a weak equilibrium fails to be strong, so that an agent in one state strictly gains from deviating on every short interval.

Setting

The state space is S={1,…,N}S=\{1,\dots,N\}S={1,…,N}. A generator is a matrix Q∈RN×NQ\in\mathbb R^{N\times N}Q∈RN×N whose iii-th row QiQ_iQi​ lies in Ei={q:qj≥0 (j≠i), qi=−∑j≠iqj}E_i=\{q: q_j\ge0\ (j\ne i),\ q_i=-\sum_{j\ne i}q_j\}Ei​={q:qj​≥0 (j=i), qi​=−∑j=i​qj​}. Admissible rows form sets Di⊆EiD_i\subseteq E_iDi​⊆Ei​, and the control space is Q={Q:Qi∈Di ∀i}\mathcal Q=\{Q: Q_i\in D_i\ \forall i\}Q={Q:Qi​∈Di​ ∀i}. A payoff function f(t,i,q)f(t,i,q)f(t,i,q) gives the payment rate at time difference ttt in state iii when row qqq is in force. The expected payoff of using QQQ from state iii is

F(i,Q)=Ei,Q[∫0∞f(t,Xt,QXt) dt]=∫0∞∑j(etQ)ij f(t,j,Qj) dt.F(i,Q)=\mathbb E_{i,Q}\Big[\int_0^\infty f(t,X_t,Q_{X_t})\,dt\Big]=\int_0^\infty\sum_j (e^{tQ})_{ij}\,f(t,j,Q_j)\,dt .F(i,Q)=Ei,Q​[∫0∞​f(t,Xt​,QXt​​)dt]=∫0∞​j∑​(etQ)ij​f(t,j,Qj​)dt.

The concatenation Q⊗εQ∗Q\otimes_\varepsilon Q^*Q⊗ε​Q∗ uses QQQ on [0,ε][0,\varepsilon][0,ε] and Q∗Q^*Q∗ afterwards. A generator Q∗∈QQ^*\in\mathcal QQ∗∈Q is a weak equilibrium if lim inf⁡ε↓0[F(i,Q∗)−F(i,Q⊗εQ∗)]/ε≥0\liminf_{\varepsilon\downarrow0}[F(i,Q^*)-F(i,Q\otimes_\varepsilon Q^*)]/\varepsilon\ge0liminfε↓0​[F(i,Q∗)−F(i,Q⊗ε​Q∗)]/ε≥0 for all i∈Si\in Si∈S, Q∈QQ\in\mathcal QQ∈Q, and a strong equilibrium if for all i,Qi,Qi,Q there is ε>0\varepsilon>0ε>0 with F(i,Q∗)≥F(i,Q⊗ε′Q∗)F(i,Q^*)\ge F(i,Q\otimes_{\varepsilon'}Q^*)F(i,Q∗)≥F(i,Q⊗ε′​Q∗) for every ε′∈(0,ε]\varepsilon'\in(0,\varepsilon]ε′∈(0,ε].

The paper's first-order and second-order quantities are

ΓQ∗(Qi)=f(0,i,Qi)+Qi⋅F(Q∗),ΛQ∗(i,Q)=ft(0,i,Qi)+Qi⋅(2G(Q∗)+ΓQ∗(Q)),\Gamma^{Q^*}(Q_i)=f(0,i,Q_i)+Q_i\cdot F(Q^*),\qquad \Lambda^{Q^*}(i,Q)=f_t(0,i,Q_i)+Q_i\cdot\big(2G(Q^*)+\Gamma^{Q^*}(Q)\big),ΓQ∗(Qi​)=f(0,i,Qi​)+Qi​⋅F(Q∗),ΛQ∗(i,Q)=ft​(0,i,Qi​)+Qi​⋅(2G(Q∗)+ΓQ∗(Q)),

with GGG the payoff computed with the time derivative ftf_tft​ in place of fff.

In the two-state model of §4, S={1,2}S=\{1,2\}S={1,2}, Di=EiD_i=E_iDi​=Ei​, every generator is Q∼(a,b)=[−aab−b]Q\sim(a,b)=\begin{bmatrix}-a&a\\ b&-b\end{bmatrix}Q∼(a,b)=[−ab​a−b​] with a,b≥0a,b\ge0a,b≥0, and f(t,1,(−a,a))=δ(t)g1(a)f(t,1,(-a,a))=\delta(t)g_1(a)f(t,1,(−a,a))=δ(t)g1​(a), f(t,2,(b,−b))=δ(t)g2(b)f(t,2,(b,-b))=\delta(t)g_2(b)f(t,2,(b,−b))=δ(t)g2​(b) with the pseudo-exponential discount δ(t)=λe−ρt+(1−λ)e−ρ′t\delta(t)=\lambda e^{-\rho t}+(1-\lambda)e^{-\rho't}δ(t)=λe−ρt+(1−λ)e−ρ′t. Example 4.3 takes λ=12\lambda=\tfrac12λ=21​, ρ=1\rho=1ρ=1, ρ′=2\rho'=2ρ′=2, g1(a)=−a2g_1(a)=-a^2g1​(a)=−a2, and g2(b)=193144+56bg_2(b)=\tfrac{193}{144}+\tfrac56bg2​(b)=144193​+65​b for b<712b<\tfrac7{12}b<127​, g2(b)=2−(1−b)2g_2(b)=2-(1-b)^2g2​(b)=2−(1−b)2 for b≥712b\ge\tfrac7{12}b≥127​.

Formalization targets

Goal: Example 4.3

Q∗∼(512,712) is a weak equilibrium and not a strong equilibrium.Q^*\sim\Big(\frac5{12},\frac7{12}\Big)\ \text{is a weak equilibrium and not a strong equilibrium.}Q∗∼(125​,127​) is a weak equilibrium and not a strong equilibrium.

The statement is fully explicit and has no hypotheses.

Milestones

  1. (4.3)–(4.4): closed forms of F1−F2F_1-F_2F1​−F2​ and G1−G2G_1-G_2G1​−G2​ for Q∼(a,b)Q\sim(a,b)Q∼(a,b) under pseudo-exponential discounting.
  2. (4.5), (4.6), (4.8): ΓQ∗(Q1)\Gamma^{Q^*}(Q_1)ΓQ∗(Q1​), ΓQ∗(Q2)\Gamma^{Q^*}(Q_2)ΓQ∗(Q2​) and ΛQ∗(2,Q)\Lambda^{Q^*}(2,Q)ΛQ∗(2,Q) in the two-state model.
  3. Theorem 3.1: under (2.3) and (3.3), Q∗Q^*Q∗ is weak iff ΓQ∗(Qi∗)≥ΓQ∗(Qi)\Gamma^{Q^*}(Q^*_i)\ge\Gamma^{Q^*}(Q_i)ΓQ∗(Qi∗​)≥ΓQ∗(Qi​) for all (i,Q)(i,Q)(i,Q).
  4. (4.11): at Q∗Q^*Q∗, Γ1\Gamma_1Γ1​ is maximized uniquely at a∗a^*a∗ and arg max⁡b≥0Γ2(b)=[0,7/12]\operatorname{arg\,max}_{b\ge0}\Gamma_2(b)=[0,7/12]argmaxb≥0​Γ2​(b)=[0,7/12].
  5. Proposition 3.3: the second-order test on the set RRR of equality cases.
  6. (4.12): Λ2(a∗,b)=−b/12−579/288\Lambda_2(a^*,b)=-b/12-579/288Λ2​(a∗,b)=−b/12−579/288 on [0,7/12][0,7/12][0,7/12], so Λ2(a∗,b∗)<Λ2(a∗,b)\Lambda_2(a^*,b^*)<\Lambda_2(a^*,b)Λ2​(a∗,b∗)<Λ2​(a∗,b) for b∈[0,7/12)b\in[0,7/12)b∈[0,7/12).

Further statements

Remark 4.1: for Q∼(5/12,b)Q\sim(5/12,b)Q∼(5/12,b), b∈[0,7/12)b\in[0,7/12)b∈[0,7/12), F(2,Q∗)<F(2,Q⊗εQ∗)F(2,Q^*)<F(2,Q\otimes_\varepsilon Q^*)F(2,Q∗)<F(2,Q⊗ε​Q∗) for all small ε>0\varepsilon>0ε>0. And (4.13): the equation 56≤2a=12(11+a+12+a)(a2+193144)\tfrac56\le2a=\tfrac12(\tfrac1{1+a}+\tfrac1{2+a})(a^2+\tfrac{193}{144})65​≤2a=21​(1+a1​+2+a1​)(a2+144193​) has a unique solution aˉ≥0\bar a\ge0aˉ≥0, and Qˉ∗∼(aˉ,0)\bar Q^*\sim(\bar a,0)Qˉ​∗∼(aˉ,0) is a strong equilibrium.

Significance

The example shows that the weak equilibrium concept, the standard one in the time-inconsistency literature since Ekeland and Lazrak, admits strategies that an agent would abandon: Remark 4.1 exhibits a deviation that strictly increases the payoff on every short interval. Together with (4.13), it shows that in one and the same model a weak-but-not-strong equilibrium and a strong equilibrium coexist, so the choice of equilibrium concept changes which strategies are predicted. The example is the paper's justification for introducing strong equilibria.

The result is proved in the paper, through the first-order characterization (Theorem 3.1), the second-order test (Proposition 3.3, resting on the second-order expansion Lemma 3.2) and explicit computations in the two-state model. None of it has been machine-checked. A formal proof would provide checked versions of Theorem 3.1 and Proposition 3.3 for finite-state chains, reusable for any other example, and an independent check of the arithmetic of Example 4.3, where the source contains at least one misprinted formula.

Difficulty

Both conjuncts of the goal concern the small-ε\varepsilonε behaviour of F(2,Q⊗εQ∗)F(2,Q\otimes_\varepsilon Q^*)F(2,Q⊗ε​Q∗), an integral of products of matrix exponentials. Weakness reduces to a first-order comparison by Theorem 3.1, but its proof needs the expansion (3.6) with an o(ε)o(\varepsilon)o(ε) remainder controlled uniformly enough to pass under the integral over [0,∞)[0,\infty)[0,∞). Failure of strong equilibrium cannot be read off the first-order term: at b∗=7/12b^*=7/12b∗=7/12 the maximizer of Γ2\Gamma_2Γ2​ is not unique, every b∈[0,7/12)b\in[0,7/12)b∈[0,7/12) ties at first order, and the decision moves to the second-order coefficient Λ\LambdaΛ of Lemma 3.2, whose derivation needs a second-order expansion of the concatenated payoff. The regularity hypotheses of Lemma 3.2 and of (3.3) must also be verified for the example's discount function.

Formalization scope

States are Fin N; the paper's state kkk is index k−1k-1k−1, so in the two-state model state 1 is 0 : Fin 2 and state 2 is 1 : Fin 2. Expectations are written through the transition matrices etQe^{tQ}etQ (NormedSpace.exp (t • Q)) and Fubini, exactly as the paper computes on p. 23; no Markov process is constructed. Payoffs are Bochner integrals over (0,∞)(0,\infty)(0,∞). The weak-equilibrium condition is written as "for every η>0\eta>0η>0, eventually as ε↓0\varepsilon\downarrow0ε↓0 the quotient is ≥−η\ge-\eta≥−η", which is lim inf⁡≥0\liminf\ge0liminf≥0 without a real-valued liminf. The norm in (2.3) is the sup norm, equivalent to the paper's Euclidean norm because (2.3) quantifies over every c>0c>0c>0.

Standing assumptions: Di⊆EiD_i\subseteq E_iDi​⊆Ei​, continuity of fff in ttt (2.2) and the integrability condition (2.3). Theorem 3.1 adds the shift bound (3.3)–(3.5); Proposition 3.3 assumes the conditions of Lemma 3.2, with the derivative ftf_tft​ tied to fff. The closed forms (4.3)–(4.4) assume ρ,ρ′>0\rho,\rho'>0ρ,ρ′>0 (the page allows ρ,ρ′≥0\rho,\rho'\ge0ρ,ρ′≥0, but with a zero rate the payoff integral diverges); the algebraic identities (4.5)–(4.8) keep the page's ρ,ρ′≥0\rho,\rho'\ge0ρ,ρ′≥0; Example 4.3 has ρ=1\rho=1ρ=1, ρ′=2\rho'=2ρ′=2. Statement (4.11) gives Γ2(b)=g2(b)−56b\Gamma_2(b)=g_2(b)-\tfrac56bΓ2​(b)=g2​(b)−65​b and the argmax; the page's case formula for b≥7/12b\ge7/12b≥7/12 contains a misprint and is not used.

No trivializing reading is available: the goal has no hypotheses, FFF is built from etQe^{tQ}etQ and the concatenation uses QQQ before and Q∗Q^*Q∗ after ε\varepsilonε, so neither conjunct holds by a junk value. Integrability of every payoff follows from (2.3) and is never assumed.

Theorem 3.1 and the second-order package are also drafted in the companion mission on existence of equilibria; they are restated here in the sub-namespace StrongWeakEq.TwoState. The goal needs the verification of (2.3), (3.3) and the Lemma 3.2 conditions for the example (convexity of δ\deltaδ gives (3.15)), the closed forms of etQe^{tQ}etQ for two-state generators, and the expansions of the paper. Contributions of proofs of the general results (Theorem 3.1, Proposition 3.3) are welcome independently of the example.

Selected references

  • Y.-J. Huang and Z. Zhou, Strong and Weak Equilibria for Time-Inconsistent Stochastic Control in Continuous Time, Math. Oper. Res. 46(2), 2021; arXiv:1809.09243v3. https://arxiv.org/abs/1809.09243, https://doi.org/10.1287/moor.2020.1066
  • I. Ekeland and A. Lazrak, Being serious about non-commitment: subgame perfect equilibrium in continuous time, 2006. https://arxiv.org/abs/math/0604264
  • T. Björk, M. Khapko and A. Murgoci, On time-inconsistent stochastic control in continuous time, Finance Stoch. 21 (2017), pp. 331–360.
  • R. H. Strotz, Myopia and inconsistency in dynamic utility maximization, Rev. Econ. Stud. 23 (1955), pp. 165–180.
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Control TheoryDynamic ProgrammingMarkov Chain·Captain: mikedeng1

Strong and Weak Equilibria for Time-Inconsistent Stochastic Control in Continuous Time 4: Limits of Equilibria of the Time-Discretized Problems Are Weak Equilibria in Continuous TimeResearch Paper

Motivation

A decision maker is time-inconsistent when the plan that is optimal today stops being optimal tomorrow. The standard source is non-exponential discounting: a reward ttt units of time ahead is weighted by δ(t)\delta(t)δ(t), and unless δ\deltaδ is exponential the relative weight of two future dates changes as time passes. Hyperbolic and pseudo-exponential discount functions, which fit experimental and group-decision data better than exponential ones, all have this property. For such an agent "optimal control" is not a meaningful target, and the literature instead looks for equilibrium policies: plans that no current self wants to deviate from, given that all future selves follow the plan.

In discrete time the definition is unambiguous: a policy is an equilibrium if deviating at the current step alone does not help. In continuous time there is no "current step", and the usual definition, due to Ekeland and Lazrak (2006), compares the payoff of the plan with that of a deviation on a short interval [0,ε][0,\varepsilon][0,ε] through a first-order condition as ε↓0\varepsilon\downarrow0ε↓0. Huang and Zhou (arXiv:1809.09243, Math. Oper. Res. 2021) call this a weak equilibrium, introduce a strong equilibrium that requires the deviation to be unprofitable for every small ε\varepsilonε, and study both for a controlled finite-state Markov chain.

A natural question is whether continuous-time equilibria are the limits of the discrete-time ones as the time step shrinks. This mission formalizes the paper's answer (§5.1): limits of discrete equilibria are always weak equilibria. The paper's Example 5.1 shows they need not be strong.

Setting

The state space is S={1,…,N}S=\{1,\dots,N\}S={1,…,N}. A continuous-time Markov chain on SSS is controlled through its generator Q=(qij)Q=(q_{ij})Q=(qij​): in state iii the row QiQ_iQi​ is chosen from an admissible set Di⊆Ei={q:qj≥0 (j≠i), qi=−∑j≠iqj}D_i\subseteq E_i=\{q: q_j\ge0\ (j\ne i),\ q_i=-\sum_{j\ne i}q_j\}Di​⊆Ei​={q:qj​≥0 (j=i), qi​=−∑j=i​qj​}, and the control space is Q={Q:Qi∈Di ∀i}\mathcal Q=\{Q: Q_i\in D_i\ \forall i\}Q={Q:Qi​∈Di​ ∀i}. A payoff function f(t,i,q)f(t,i,q)f(t,i,q) gives the reward at time-distance ttt from now, in state iii, under row qqq. The standing assumptions are continuity of t↦f(t,i,q)t\mapsto f(t,i,q)t↦f(t,i,q) on [0,∞)[0,\infty)[0,∞) and, for each c>0c>0c>0, integrability over [0,∞)[0,\infty)[0,∞) of sup⁡i, q∈Di, ∥q∥≤c∣f(t,i,q)∣\sup_{i,\,q\in D_i,\,\|q\|\le c}|f(t,i,q)|supi,q∈Di​,∥q∥≤c​∣f(t,i,q)∣ (condition (2.3)). The expected payoff from state iii is

F(i,Q)=Ei,Q[∫0∞f(t,Xt,QXt) dt]=∫0∞∑j(etQ)ijf(t,j,Qj) dt,F(i,Q)=\mathbb E_{i,Q}\Big[\int_0^\infty f(t,X_t,Q_{X_t})\,dt\Big]=\int_0^\infty\sum_j(e^{tQ})_{ij}f(t,j,Q_j)\,dt,F(i,Q)=Ei,Q​[∫0∞​f(t,Xt​,QXt​​)dt]=∫0∞​j∑​(etQ)ij​f(t,j,Qj​)dt,

and F(Q)=(F(1,Q),…,F(N,Q))F(Q)=(F(1,Q),\dots,F(N,Q))F(Q)=(F(1,Q),…,F(N,Q)). With Q⊗εQ∗Q\otimes_\varepsilon Q^*Q⊗ε​Q∗ the generator that uses QQQ on [0,ε][0,\varepsilon][0,ε] and Q∗Q^*Q∗ afterwards, Q∗∈QQ^*\in\mathcal QQ∗∈Q is a weak equilibrium if lim inf⁡ε↓0(F(i,Q∗)−F(i,Q⊗εQ∗))/ε≥0\liminf_{\varepsilon\downarrow0}\big(F(i,Q^*)-F(i,Q\otimes_\varepsilon Q^*)\big)/\varepsilon\ge0liminfε↓0​(F(i,Q∗)−F(i,Q⊗ε​Q∗))/ε≥0 for all iii and Q∈QQ\in\mathcal QQ∈Q. The first-order quantity is ΓQ∗(q)=f(0,i,q)+q⋅F(Q∗)\Gamma^{Q^*}(q)=f(0,i,q)+q\cdot F(Q^*)ΓQ∗(q)=f(0,i,q)+q⋅F(Q∗).

Discretization. Fix a mesh δn>0\delta_n>0δn​>0. A transition matrix uuu (rows in the probability simplex P\mathfrak PP) has generator Qu,n=(u−I)/δnQ^{u,n}=(u-I)/\delta_nQu,n=(u−I)/δn​, the admissible matrices are An={u:Qu,n∈Q}\mathcal A^n=\{u: Q^{u,n}\in\mathcal Q\}An={u:Qu,n∈Q}, and the discrete payoff is κn(k,i,α)=f(kδn,i,(α−ei)/δn) δn\kappa^n(k,i,\alpha)=f\big(k\delta_n,i,(\alpha-e_i)/\delta_n\big)\,\delta_nκn(k,i,α)=f(kδn​,i,(α−ei​)/δn​)δn​. The discrete value is Vn(i,u)=Ei,u[∑k≥0κn(k,Xk,uXk)]V^n(i,u)=\mathbb E_{i,u}\big[\sum_{k\ge0}\kappa^n(k,X_k,u_{X_k})\big]Vn(i,u)=Ei,u​[∑k≥0​κn(k,Xk​,uXk​​)], and un∈Anu^n\in\mathcal A^nun∈An is a discrete equilibrium if Vn(i,un)≥Vn(i,u⊗1un)V^n(i,u^n)\ge V^n(i,u\otimes_1u^n)Vn(i,un)≥Vn(i,u⊗1​un) for all iii and u∈Anu\in\mathcal A^nu∈An, where u⊗1unu\otimes_1u^nu⊗1​un uses uuu at time 000 and unu^nun afterwards. The continuation values are Hin(un)=Ei,un[∑k≥0κn(k+1,Xk,uXkn)]H^n_i(u^n)=\mathbb E_{i,u^n}\big[\sum_{k\ge0}\kappa^n(k+1,X_k,u^n_{X_k})\big]Hin​(un)=Ei,un​[∑k≥0​κn(k+1,Xk​,uXk​n​)]. Theorem 5.2 additionally assumes (5.8): for some T>0T>0T>0, t↦∣f(t,i,q)∣t\mapsto|f(t,i,q)|t↦∣f(t,i,q)∣ is nonincreasing on [T,∞)[T,\infty)[T,∞).

Formalization targets

Goal: Theorem 5.2

Let δn↓0\delta_n\downarrow0δn​↓0, let unu^nun be an equilibrium of the problem with mesh δn\delta_nδn​, Qn=Qun,nQ^n=Q^{u^n,n}Qn=Qun,n, and suppose f(⋅,i,⋅)f(\cdot,i,\cdot)f(⋅,i,⋅) is continuous on [0,∞)×Di[0,\infty)\times D_i[0,∞)×Di​. If Qnk→Q∗∈QQ^{n_k}\to Q^*\in\mathcal QQnk​→Q∗∈Q along a subsequence, then

ΓQ∗(Qi∗)≥ΓQ∗(Qi)for all (i,Q)∈S×Q,and Q∗ is a weak equilibrium.\Gamma^{Q^*}(Q^*_i)\ge\Gamma^{Q^*}(Q_i)\quad\text{for all }(i,Q)\in S\times\mathcal Q,\qquad\text{and } Q^* \text{ is a weak equilibrium.}ΓQ∗(Qi∗​)≥ΓQ∗(Qi​)for all (i,Q)∈S×Q,and Q∗ is a weak equilibrium.

Milestones

  1. (5.12): an equilibrium unu^nun satisfies κn(0,i,uin)+Hn(un)⋅uin≥κn(0,i,ui)+Hn(un)⋅ui\kappa^n(0,i,u^n_i)+H^n(u^n)\cdot u^n_i\ge\kappa^n(0,i,u_i)+H^n(u^n)\cdot u_iκn(0,i,uin​)+Hn(un)⋅uin​≥κn(0,i,ui​)+Hn(un)⋅ui​ for all u∈Anu\in\mathcal A^nu∈An.
  2. Generator form (proof of Theorem 5.2): dividing by δn\delta_nδn​, the same inequality reads f(0,i,Qin)+H⋅Qin≥f(0,i,Qiu,n)+H⋅Qiu,nf(0,i,Q^n_i)+H\cdot Q^n_i\ge f(0,i,Q^{u,n}_i)+H\cdot Q^{u,n}_if(0,i,Qin​)+H⋅Qin​≥f(0,i,Qiu,n​)+H⋅Qiu,n​.
  3. Continuity of Q↦F(Q)Q\mapsto F(Q)Q↦F(Q) on Q\mathcal QQ (proof of Theorem 3.3).
  4. Lemma 5.1: Hink(unk)→F(i,Q∗)H^{n_k}_i(u^{n_k})\to F(i,Q^*)Hink​​(unk​)→F(i,Q∗) along the subsequence.

Significance

The theorem justifies the weak-equilibrium notion from discrete time: whatever a time-inconsistent agent does on a fine time grid, the continuous-time limit satisfies the first-order condition (3.10). Combined with the paper's discrete existence result (Theorem 5.1) and compactness of Q\mathcal QQ, it yields weak equilibria by approximation (Remark 5.3). It also locates the gap between the two notions: the limit is weak but in general not strong.

The result is proved in the paper; nothing about it is open. No part of it has a machine-checked proof. A formal development adds a checked Euler-scheme comparison between (I+δQ)k(I+\delta Q)^k(I+δQ)k and ekδQe^{k\delta Q}ekδQ for generator matrices, a dominated passage to the limit for Riemann sums of the payoff, and continuity of the payoff in the generator, each reusable for other finite-state continuous-time control problems.

Difficulty

The obvious argument is to divide the discrete one-step inequality (5.12) by δn\delta_nδn​ and let n→∞n\to\inftyn→∞. Its algebraic part is immediate. The difficulty is the convergence of the discrete continuation values Hn(un)H^n(u^n)Hn(un), which are infinite sums along a discrete chain with transition matrix unu^nun, to the continuous payoff F(Q∗)F(Q^*)F(Q∗), an integral along the continuous chain with generator Q∗Q^*Q∗. Three errors must be controlled at once: the discrete chain against the chain sampled from etQne^{tQ^n}etQn (the difference of kkk-th powers grows with k≈M/δnk\approx M/\delta_nk≈M/δn​), the Riemann sum against the integral (needs uniform continuity of fff jointly in ttt and qqq), and F(Qn)F(Q^n)F(Qn) against F(Q∗)F(Q^*)F(Q∗). The tail of the infinite sums is not controlled by (2.3) alone: integrability of a majorant does not make its samples on a grid summable, which is why (5.8) is assumed. A second subtlety concerns the last step: the paper passes from (3.10) to the weak-equilibrium property through Theorem 3.1, which assumes a condition (3.3) that Theorem 5.2 does not. The conclusion is still true without (3.3), but no numbered statement of the paper provides that step.

Formalization scope

  • States are Fin N; rows are Fin N → ℝ with the sup norm, generators and transition matrices are Matrix (Fin N) (Fin N) ℝ with the product topology.
  • Expectations are written through marginals: F(i,Q)=∫0∞∑j(etQ)ijf(t,j,Qj) dtF(i,Q)=\int_0^\infty\sum_j(e^{tQ})_{ij}f(t,j,Q_j)\,dtF(i,Q)=∫0∞​∑j​(etQ)ij​f(t,j,Qj​)dt (Bochner integral) and Hin(u)=∑k∑j(uk)ijκn(k+1,j,uj)H^n_i(u)=\sum_k\sum_j(u^k)_{ij}\kappa^n(k+1,j,u_j)Hin​(u)=∑k​∑j​(uk)ij​κn(k+1,j,uj​) (tsum). No Markov process is constructed.
  • The weak-equilibrium liminf is encoded as "for every η>0\eta>0η>0, eventually as ε↓0\varepsilon\downarrow0ε↓0 the quotient is ≥−η\ge-\eta≥−η".
  • "f(⋅,i,⋅)f(\cdot,i,\cdot)f(⋅,i,⋅) is continuous" is joint continuity on [0,∞)×Di[0,\infty)\times D_i[0,∞)×Di​; (5.8) is required for q∈Diq\in D_iq∈Di​; δn↓0\delta_n\downarrow0δn​↓0 is positivity, monotonicity and convergence to 000; the subsequence is a strictly increasing φ:N→N\varphi:\mathbb N\to\mathbb Nφ:N→N.
  • Not assumed: integrability of FFF, summability of HnH^nHn or (5.2) for κn\kappa^nκn (they follow from (2.3) and (5.8)), compactness of DiD_iDi​, and condition (3.3).
  • The equilibria unu^nun, the generators Qn=(un−I)/δnQ^n=(u^n-I)/\delta_nQn=(un−I)/δn​ and the subsequence are part of the goal's data. A version that only assumes "Qn→Q∗Q^n\to Q^*Qn→Q∗" for arbitrary Qn∈QQ^n\in\mathcal QQn∈Q would be false and is ruled out.
  • The continuity milestone is proved in the paper for compact DiD_iDi​; it is stated here without compactness, since only convergent sequences in Q\mathcal QQ matter.
  • Needed infrastructure: bounds on ∥(I+δQ)k−ekδQ∥\|(I+\delta Q)^k-e^{k\delta Q}\|∥(I+δQ)k−ekδQ∥ for generator matrices, stochasticity of etQe^{tQ}etQ for generator QQQ, dominated convergence for the payoff integral and for the discrete series. Contributions of these general lemmas are welcome.

Selected references

  • Y.-J. Huang and Z. Zhou, Strong and Weak Equilibria for Time-Inconsistent Stochastic Control in Continuous Time, Math. Oper. Res. 46(2), 2021; read as arXiv:1809.09243v3. https://arxiv.org/abs/1809.09243 , https://doi.org/10.1287/moor.2020.1066
  • I. Ekeland and A. Lazrak, Being serious about non-commitment: subgame perfect equilibrium in continuous time, tech. rep., University of British Columbia, 2006. http://arxiv.org/abs/math/0604264
  • S. N. Ethier and T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
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Bandit AlgorithmsOperations ResearchProbability·Captain: mikedeng1

Learning Unknown Service Rates in Queues 2: Q-UCB Has Queue-Regret at Most 6K v_u(t) log² t / t + (24.004 + UK)/(6t²) in the Late StageResearch Paper

Motivation

Many service systems must match jobs to servers whose quality is not known in advance: crowdsourcing platforms routing tasks to worker types, wireless schedulers assigning users to channels, and switches in data networks. The scheduler learns server quality only by trying servers, and every poor assignment lets work pile up. The natural performance measure is therefore not the cumulative reward loss of classical bandits but the queue-regret: the expected excess backlog compared with a genie that knows the best assignment.

Krishnasamy, Sen, Johari and Shakkottai, Learning Unknown Service Rates in Queues: A Multiarmed Bandit Approach (Operations Research, 2021; arXiv:1604.06377), show that queue-regret has two regimes. In an early stage it grows like the regret of a bandit. In a late stage, once the queue regularly empties, past mistakes are forgotten at every empty instant and the queue-regret decays. This mission formalizes their upper bound for the late stage: a UCB scheduler with forced exploration, Q-UCB, has queue-regret of order log⁡3t/t\log^3 t/tlog3t/t.

Setting

A discrete-time switch has UUU queues and K≥UK\ge UK≥U servers. In every slot t≥1t\ge1t≥1, queue uuu receives an arrival Au(t)∼Bernoulli(λu)A_u(t)\sim\mathrm{Bernoulli}(\lambda_u)Au​(t)∼Bernoulli(λu​) and link (u,k)(u,k)(u,k) offers a potential service Ruk(t)∼Bernoulli(μuk)R_{uk}(t)\sim\mathrm{Bernoulli}(\mu_{uk})Ruk​(t)∼Bernoulli(μuk​), all independent and i.i.d. over slots. The scheduler picks a matching κ(t)\kappa(t)κ(t), an injective assignment of a server κu(t)\kappa_u(t)κu​(t) to every queue, and queue uuu evolves as

Qu(t)=(Qu(t−1)+Au(t)−Su(t))+,Su(t)=Ruκu(t)(t).Q_u(t)=\big(Q_u(t-1)+A_u(t)-S_u(t)\big)^+,\qquad S_u(t)=R_{u\kappa_u(t)}(t).Qu​(t)=(Qu​(t−1)+Au​(t)−Su​(t))+,Su​(t)=Ruκu​(t)​(t).

The scheduler observes only past schedules and the services offered on scheduled links.

Write μu∗=max⁡kμuk\mu^*_u=\max_k\mu_{uk}μu∗​=maxk​μuk​, ku∗k^*_uku∗​ for its maximizer, ϵu=μu∗−λu\epsilon_u=\mu^*_u-\lambda_uϵu​=μu∗​−λu​, and Δ=min⁡u, k≠ku∗(μu∗−μuk)\Delta=\min_{u,\,k\ne k^*_u}(\mu^*_u-\mu_{uk})Δ=minu,k=ku∗​​(μu∗​−μuk​). Assumption 1: each queue has a unique best server and the best servers are distinct, so k∗k^*k∗ is the unique optimal matching. Assumption 2: ϵu>0\epsilon_u>0ϵu​>0 for all uuu. The genie queue Qu∗Q^*_uQu∗​ always uses ku∗k^*_uku∗​. Assumption 3: the system starts from the stationary law of Q∗Q^*Q∗. The queue-regret is

Ψu(t)=E[Qu(t)−Qu∗(t)].\Psi_u(t)=\mathbb E\big[Q_u(t)-Q^*_u(t)\big].Ψu​(t)=E[Qu​(t)−Qu∗​(t)].

Q-UCB (Algorithm 1) explores in slot ttt with probability min⁡{1,3Klog⁡2t/t}\min\{1,3K\log^2t/t\}min{1,3Klog2t/t}, scheduling a uniformly random member of a fixed family X\mathcal XX of KKK matchings that together cover all UKUKUK links. Otherwise it exploits: for each queue it picks the server with the largest index μ^uk(t)+log⁡2t/(2Nuk(t))\hat\mu_{uk}(t)+\sqrt{\log^2t/(2N_{uk}(t))}μ^​uk​(t)+log2t/(2Nuk​(t))​, with μ^uk\hat\mu_{uk}μ^​uk​ the empirical mean and NukN_{uk}Nuk​ the number of past assignments of link (u,k)(u,k)(u,k), and schedules a matching closest in Hamming distance to these choices. Fix β>1\beta>1β>1 and set

w(t)=t1−1/β,vu′(t)=6Kϵuw(t),vu(t)=24ϵu2log⁡t+60Kϵuvu′(t)log⁡2tt.w(t)=t^{1-1/\beta},\qquad v'_u(t)=\frac{6K}{\epsilon_u}w(t),\qquad v_u(t)=\frac{24}{\epsilon_u^2}\log t+\frac{60K}{\epsilon_u}\frac{v'_u(t)\log^2t}{t}.w(t)=t1−1/β,vu′​(t)=ϵu​6K​w(t),vu​(t)=ϵu2​24​logt+ϵu​60K​tvu′​(t)log2t​.

Formalization targets

Goal: Theorem 5 for Q-UCB (p. 16)

For every t≥5800t\ge5800t≥5800 with t≥exp⁡(4/(Δ2(1−1/β)3))t\ge\exp\big(4/(\Delta^2(1-1/\beta)^3)\big)t≥exp(4/(Δ2(1−1/β)3)), w(t)/log⁡t≥2/ϵuw(t)/\log t\ge2/\epsilon_uw(t)/logt≥2/ϵu​ and vu(t)+vu′(t)≤t/2v_u(t)+v'_u(t)\le t/2vu​(t)+vu′​(t)≤t/2,

Ψu(t)≤6Kvu(t)log⁡2tt+24.004+UK6t2.\Psi_u(t)\le 6K\frac{v_u(t)\log^2t}{t}+\frac{24.004+UK}{6t^2}.Ψu​(t)≤6Ktvu​(t)log2t​+6t224.004+UK​.

The constants are the paper's, stated exactly.

Milestones (§8.2, pp. 24–34)

  • Lemma 10: the number of forced-exploration slots in a window exceeds 5max⁡(log⁡t,K(log⁡3t2−log⁡3t1))5\max(\log t,K(\log^3t_2-\log^3t_1))5max(logt,K(log3t2​−log3t1​)) with probability at most t−4t^{-4}t−4. Over [1,t][1,t][1,t] it exceeds Kw(t)Kw(t)Kw(t) with probability at most t−2Kt^{-2K}t−2K.
  • Lemma 11: with probability at least 1−UK/(6t3)1-UK/(6t^3)1−UK/(6t3), no exploit slot in (w(t),t](w(t),t](w(t),t] schedules a sub-optimal link (event E1\mathcal E_1E1​).
  • Lemma 12: pathwise, Qu(t)−Qu∗(t)Q_u(t)-Q^*_u(t)Qu​(t)−Qu∗​(t) is at most the number of sub-optimal schedules since queue uuu was last empty, at time t−Bu(t)t-B_u(t)t−Bu​(t).
  • Lemmas 13–17: on E1∩E2\mathcal E_1\cap\mathcal E_2E1​∩E2​, a coarse queue bound 2Kw(t)2Kw(t)2Kw(t) (13), a first bound on the regenerative cycle (14), a maximal inequality for the arrival-minus-service walk (15), a refined polylogarithmic queue bound (16), and the refined cycle bound Bu(t)≤vu(t)B_u(t)\le v_u(t)Bu​(t)≤vu​(t) (17), each failing with probability O(t−3)O(t^{-3})O(t−3).

Significance

The theorem shows that a simple learning scheduler loses only O(Klog⁡3t/(ϵu2t))O(K\log^3t/(\epsilon_u^2t))O(Klog3t/(ϵu2​t)) in expected backlog in the late stage. Together with the paper's Ω(1/t)\Omega(1/t)Ω(1/t) lower bound for consistent policies (Theorem 3), this places the optimal late-stage queue-regret within a polylogarithmic factor. The analysis method has two parts: a high-probability statement that the learner has locked onto the optimal matching, and a regenerative argument that converts it into a bound on queue length. It applies to other learning-in-queues problems in the same way.

All results are proved in the paper (§8.2). None of them has a machine-checked proof. The mission produces a formal model of the learning switch, including the algorithm with arbitrary tie-breaking, the coupled genie and the stationary start, and checks the explicit constants. These constants rely on numerical facts stated in the proofs, for example a positivity check for x≥log⁡5800x\ge\log5800x≥log5800 in Lemma 10(b) and the absorption of lower-order terms into 24.00424.00424.004, which a formal proof must verify.

Difficulty

The obvious argument says that UCB eventually identifies the best server, so the queue behaves like the genie's. This fails for two reasons. First, the regret is an expectation of a queue length, and a queue remembers every early mistake until it next empties. So one must bound the current regenerative cycle, and that bound itself depends on the queue length, which forces the recursion of Lemmas 13, 14, 16 and 17. Second, UCB's standard logarithmic-regret analysis bounds the expected number of sub-optimal pulls. It says nothing about whether a sub-optimal pull happens in a specific late window. Forced exploration at rate log⁡2t/t\log^2t/tlog2t/t is what makes all indices concentrate at once, and Lemma 11 requires a union bound over every link, slot and sample count with explicit exponents.

Formalization scope

  • Probability space. One canonical space: the initial queue vector together with an i.i.d. sequence of slot seeds, namely uniforms for arrivals, links and the explore coin, and a uniform explore index.
    • Arrivals and services are threshold events of the uniforms.
    • Q(0)Q(0)Q(0) has the product geometric law P(Qu(0)=n)=(1−ρu)ρun\mathbb P(Q_u(0)=n)=(1-\rho_u)\rho_u^nP(Qu​(0)=n)=(1−ρu​)ρun​ with ρu=λu(1−μu∗)/((1−λu)μu∗)\rho_u=\lambda_u(1-\mu^*_u)/((1-\lambda_u)\mu^*_u)ρu​=λu​(1−μu∗​)/((1−λu​)μu∗​), the stationary law of the genie chain under the printed recursion.
  • Indexing and coupling. Queues and servers are Fin U and Fin K, and slots are t≥1t\ge1t≥1. The genie shares arrivals, services and Q(0)Q(0)Q(0) with the system. This coupling is implicit in the paper's proofs and does not change Ψu\Psi_uΨu​.
  • Algorithm. Q-UCB is formalized for every covering family X\mathcal XX and every tie-breaking rule, deterministic in the slot and history, for the UCB argmax and the Hamming projection.
    • Nuk(t)N_{uk}(t)Nuk​(t) counts slots 1,…,t−11,\dots,t-11,…,t−1.
    • An unsampled link has index +∞+\infty+∞.
    • Bu(t)=tB_u(t)=tBu​(t)=t when queue uuu never emptied on [0,t][0,t][0,t].
  • Disclosed additions.
    • K≥2K\ge2K≥2 in every statement; K=1K=1K=1 is trivial, and the constants fail there.
    • t,t1≥1t,t_1\ge1t,t1​≥1 in Lemma 10(a).
    • log⁡w(t)≥(2log⁡t)2/3\log w(t)\ge(2\log t)^{2/3}logw(t)≥(2logt)2/3 in Lemma 10(b); the printed statement is false without it, and its proof uses it.
    • Lemmas 14 and 16 take the "arbitrary function" vuv_uvu​ natural-valued.
  • Excluded trivializations. Theorem 5 also asserts that Qu(t)−Qu∗(t)Q_u(t)-Q^*_u(t)Qu​(t)−Qu∗​(t) is integrable, so Ψu(t)\Psi_u(t)Ψu​(t) cannot be a default value of a non-integrable integral. Every probability bound concerns the actual events, and every hypothesis set is satisfiable. For example, with U=1U=1U=1, K=2K=2K=2, λ=0.5\lambda=0.5λ=0.5, μ=(0.9,0.1)\mu=(0.9,0.1)μ=(0.9,0.1), β=2\beta=2β=2, the range of Theorem 5 contains t=⌈e50⌉t=\lceil e^{50}\rceilt=⌈e50⌉.
  • Out of scope. Theorem 5 and Lemma 11 for Q-ThS (Algorithm 2) are not formalized, and neither is Corollary 6.
  • Infrastructure needed and welcome. Chernoff bounds for sums of independent non-identically distributed Bernoulli variables (Lemma 10), Hoeffding's inequality and a maximal suffix-sum bound (Lemmas 14, 15), measurability of the algorithm's trajectory in the seeds, and regenerative-cycle arguments for the reflected random walk. The Chernoff and stationary-queue lemmas are reusable well beyond this mission.

The source is the arXiv v4 preprint; the paper's proofs are in its §8 and §9.

Selected references

  • S. Krishnasamy, R. Sen, R. Johari, S. Shakkottai, Learning Unknown Service Rates in Queues: A Multiarmed Bandit Approach, Operations Research 69(1), 2021. Preprint arXiv:1604.06377v4. https://arxiv.org/abs/1604.06377 ; https://doi.org/10.1287/opre.2020.1995
  • P. Auer, N. Cesa-Bianchi, P. Fischer, Finite-time Analysis of the Multiarmed Bandit Problem, Machine Learning 47, 2002. https://doi.org/10.1023/A:1013689704352
  • M. J. Neely, Stochastic Network Optimization with Application to Communication and Queueing Systems, Morgan & Claypool, 2010. https://doi.org/10.2200/S00271ED1V01Y201006CNT007
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Operations ResearchProbability·Captain: mikedeng1

Universality of Power-of-d Load Balancing in Many-Server Systems 1: JSQ(d(N)) with d(N) → ∞ Has the Same Fluid Limit as the Join-the-Shortest-Queue PolicyResearch Paper

Motivation

Large data centers and cloud platforms route each incoming job to one of NNN parallel servers through a single dispatcher. The join-the-shortest-queue (JSQ) policy, which sends each job to a server with the fewest jobs, has strong optimality properties for identical exponential servers, but it needs the queue length of every server at every arrival, which is costly when NNN is in the thousands. The power-of-ddd scheme JSQ(ddd) polls only ddd servers chosen at random and joins the shortest among them. For fixed d≥2d\ge2d≥2 it improves dramatically over random routing, which is the supermarket model of Mitzenmacher and of Vvedenskaya, Dobrushin and Karpelevich, but it does not match JSQ.

Mukherjee, Borst, van Leeuwaarden and Whiting (arXiv:1612.00723, Stochastic Systems 2018) ask how fast d=d(N)d=d(N)d=d(N) must grow for JSQ(d(N)d(N)d(N)) to behave like JSQ in the large-NNN limit. This mission concerns their fluid-scale answer: any growth d(N)→∞d(N)\to\inftyd(N)→∞ suffices.

Timeline.

  • 1996–2001: Vvedenskaya–Dobrushin–Karpelevich and Mitzenmacher derive the fluid limit of JSQ(ddd) for fixed ddd (the supermarket ODE).
  • 2015–2018: Eschenfeldt and Gamarnik obtain the Halfin–Whitt diffusion limit of ordinary JSQ (arXiv:1502.00999).
  • 2016–2018: Mukherjee et al. prove the first transient fluid limit of ordinary JSQ in ℓ1\ell_1ℓ1​ (their Theorem 4.1). They show that JSQ(d(N)d(N)d(N)) has the same fluid limit whenever d(N)→∞d(N)\to\inftyd(N)→∞ (Theorem 2.1) and the same diffusion limit whenever d(N)/(Nlog⁡N)→∞d(N)/(\sqrt N\log N)\to\inftyd(N)/(N​logN)→∞ (Theorem 2.4, a separate mission).

Setting

There are NNN identical servers, each with a buffer of size b∈{1,2,… }∪{∞}b\in\{1,2,\dots\}\cup\{\infty\}b∈{1,2,…}∪{∞} counting the job in service. Jobs arrive as a Poisson process of rate λ(N)\lambda(N)λ(N) and need independent unit-mean exponential service. A job sent to a full server is discarded. The occupancy vector is Q(t)=(Q1(t),Q2(t),… )\mathbf Q(t)=(Q_1(t),Q_2(t),\dots)Q(t)=(Q1​(t),Q2​(t),…), where Qi(t)Q_i(t)Qi​(t) is the number of servers with at least iii jobs, with the convention Q0≡NQ_0\equiv NQ0​≡N. If the servers are listed in nondecreasing order of queue length, the ccc-th ordered server holds I(c)=max⁡{i≥0:Qi≥N−c+1}I(c)=\max\{i\ge0:Q_i\ge N-c+1\}I(c)=max{i≥0:Qi​≥N−c+1} jobs. A dispatch scheme picks an ordered position c∈{1,…,N}c\in\{1,\dots,N\}c∈{1,…,N} for each arrival, and the arrival raises QI(c)+1Q_{I(c)+1}QI(c)+1​ by one (or is discarded if I(c)=bI(c)=bI(c)=b).

The schemes are:

  • JSQ picks c=1c=1c=1;
  • JSQ(ddd) picks the lowest position among ddd positions sampled uniformly without replacement, so JSQ(NNN) is JSQ;
  • MJSQ(nnn) picks c=n+1c=n+1c=n+1;
  • CJSQ(nnn) is the class of all rules that pick some c≤n+1c\le n+1c≤n+1;
  • JSQ(n,dn,dn,d) keeps the JSQ(ddd) choice when it is at most n+1n+1n+1 and otherwise picks uniformly among the first n+1n+1n+1 positions.

Two systems are S-coupled when they share the arrival clock and the departure clock of the kkk-th ordered server for every kkk.

The fluid-scaled state is q(t)=Q(t)/N\mathbf q(t)=\mathbf Q(t)/Nq(t)=Q(t)/N. It lives in

S={q∈[0,1]b: qi≤qi−1 (i≥2), ∑i≥1qi<∞},\mathcal S=\Big\{\mathbf q\in[0,1]^b:\ q_i\le q_{i-1}\ (i\ge2),\ \sum_{i\ge1}q_i<\infty\Big\},S={q∈[0,1]b: qi​≤qi−1​ (i≥2), i≥1∑​qi​<∞},

which carries the ℓ1\ell_1ℓ1​ distance. For q∈S\mathbf q\in\mathcal Sq∈S let m(q)=min⁡{i:qi+1<1}m(\mathbf q)=\min\{i:q_{i+1}<1\}m(q)=min{i:qi+1​<1}. The coefficients pi(q)p_i(\mathbf q)pi​(q) of (4.4) send all incoming work to level m(q)−1m(\mathbf q)-1m(q)−1 while the rate λ\lambdaλ can be absorbed there, and the excess to level m(q)m(\mathbf q)m(q): if m(q)=0m(\mathbf q)=0m(q)=0 then p0=1p_0=1p0​=1; otherwise pm−1=min⁡{(1−qm+1)/λ,1}p_{m-1}=\min\{(1-q_{m+1})/\lambda,1\}pm−1​=min{(1−qm+1​)/λ,1}, pm=1−pm−1p_m=1-p_{m-1}pm​=1−pm−1​, and all other pip_ipi​ vanish.

Formalization targets

Goal: Theorem 2.1

Assume λ(N)/N→λ<1\lambda(N)/N\to\lambda<1λ(N)/N→λ<1, d(N)→∞d(N)\to\inftyd(N)→∞ and qd(N)(0)→q∞\mathbf q^{d(N)}(0)\to\mathbf q^\inftyqd(N)(0)→q∞ in S\mathcal SS. Then every subsequence of {qd(N)(t)}t≥0\{\mathbf q^{d(N)}(t)\}_{t\ge0}{qd(N)(t)}t≥0​ has a further subsequence converging weakly (Skorohod J1J_1J1​) to a limit satisfying

qi(t)=qi∞+λ∫0tpi−1(q(s)) ds−∫0t(qi(s)−qi+1(s)) ds,i=1,…,b.(2.1)q_i(t)=q^\infty_i+\lambda\int_0^t p_{i-1}(\mathbf q(s))\,ds-\int_0^t\big(q_i(s)-q_{i+1}(s)\big)\,ds,\qquad i=1,\dots,b. \tag{2.1}qi​(t)=qi∞​+λ∫0t​pi−1​(q(s))ds−∫0t​(qi​(s)−qi+1​(s))ds,i=1,…,b.(2.1)

The statement fixes no rate for d(N)d(N)d(N), which is what makes it the right goal.

Milestones

The milestones follow the paper's proof.

  • §3, coupling. Proposition 3.1 is a deterministic stack ordering. Proposition 3.2 and Corollary 3.3 sandwich any CJSQ(nnn) scheme between JSQ and MJSQ(nnn). Proposition 3.5 bounds the ℓ1\ell_1ℓ1​ distance of two S-coupled systems by 2Δ(t)2\Delta(t)2Δ(t), and Proposition 3.6 bounds Δ\DeltaΔ for JSQ(ddd) against JSQ(n,dn,dn,d).
  • §4.1, JSQ fluid limit. Proposition 4.3 makes the martingales negligible, Lemmas 4.6 and 4.7 characterize compactness and tightness in ℓ1\ell_1ℓ1​, Lemma 4.8 gives level confinement, and Theorem 4.1 is the fluid limit of JSQ itself.
  • §4.2. Proposition 4.9 is the reduction "JSQ fluid limit ⇒\Rightarrow⇒ JSQ(d(N)d(N)d(N)) fluid limit".

Significance

The result. Theorem 2.1 shows that on the fluid scale the optimality of JSQ costs nothing beyond d(N)→∞d(N)\to\inftyd(N)→∞ queue inquiries per job, far fewer than NNN. In particular the fluid limit is the same as that of JSQ, which is fluid-optimal. The coupling framework of §3 (the class CJSQ(nnn), stack orderings, S-coupling) is not tied to JSQ(ddd). The paper uses the same tools for the diffusion-scale Theorem 2.4, for batch arrivals and for the interchange of limits, Proposition 2.2.

Formalizing it. Proofs of the paper's results exist; no machine-checked version does. The mission produces:

  • a reusable model of many-server systems with ordered-position dispatch;
  • a formal stack-ordering and S-coupling toolkit;
  • compactness and tightness criteria for ℓ1\ell_1ℓ1​-valued random sequences;
  • a complete fluid-limit theorem for a load-balancing policy.

The proof of Theorem 4.1 in the paper is sketched in places (the time-scale separation is argued "analogously" to Hunt and Kurtz), so a formal proof would also settle those steps.

Difficulty

The obvious argument would compare JSQ(d(N)d(N)d(N)) directly with JSQ: the two disagree whenever the d(N)d(N)d(N) sampled servers miss every shortest queue. When a constant fraction of servers is idle this is rare, but when few servers share the minimum queue length the disagreement rate does not vanish, and a direct coupling fails. The paper instead passes through CJSQ(n(N)n(N)n(N)) with n(N)/N→0n(N)/N\to0n(N)/N→0, which is close to JSQ(d(N)d(N)d(N)) for a suitable n(N)n(N)n(N) and sandwiched between JSQ and MJSQ(n(N)n(N)n(N)).

The second difficulty is the topology. The sandwich controls tail sums ∑i≥mQi\sum_{i\ge m}Q_i∑i≥m​Qi​, so the fluid limit of JSQ is needed in ℓ1\ell_1ℓ1​, not coordinatewise. With b=∞b=\inftyb=∞ the state space is infinite-dimensional, and tightness requires uniform control of tails. Finally, the JSQ fluid limit itself involves a separation of time scales: the drift pi(q)p_i(\mathbf q)pi​(q) is discontinuous in q\mathbf qq and arises as an averaged stationary behaviour of a fast process.

Formalization scope

  • Occupancy. Occupancy vectors are finitely supported functions ℕ →₀ ℕ with the paper's level index; coordinate 000 holds Q0=NQ_0=NQ0​=N. The buffer is b∈N∞b\in\mathbb N_\inftyb∈N∞​ with b≥1b\ge1b≥1; both finite and infinite bbb are covered.
  • Construction. Systems are built by uniformization: a Poisson clock of rate λ+N\lambda+Nλ+N with i.i.d. Uniform[0,1][0,1][0,1] marks. A mark decides arrival versus departure, the departure position, the random ddd-subset (sampling without replacement) and the uniform choice of JSQ(n,dn,dn,d). S-coupled systems share the clock and the marks.
  • Schemes. A scheme maps the event index, the current state and the current mark to a position. CJSQ(nnn) rules must be measurable in the mark.
  • Fluid states. Fluid states are functions ℕ → ℝ with q0=1q_0=1q0​=1. S\mathcal SS carries the ℓ1\ell_1ℓ1​ distance, computed in [0,∞][0,\infty][0,∞].
  • Coefficients. pm−1p_{m-1}pm−1​ is written as "111 if λ≤1−qm+1\lambda\le1-q_{m+1}λ≤1−qm+1​, else (1−qm+1)/λ(1-q_{m+1})/\lambda(1−qm+1​)/λ", which equals (4.4) for λ>0\lambda>0λ>0 and never divides by zero.
  • Limit equation. A solution of (2.1) must take values in S\mathcal SS, have integrable integrands, and satisfy every equation i=1,…,bi=1,\dots,bi=1,…,b.
  • Weak convergence. Weak J1J_1J1​ convergence to a continuous limit is stated in coupling form: copies of the processes on one probability space converge almost surely uniformly on compacts in ℓ1\ell_1ℓ1​. "Any subsequence has a further subsequence" asserts the existence of the limit.
  • Initial states. Theorem 2.1 has deterministic initial states with ℓ1\ell_1ℓ1​ convergence and allows λ=0\lambda=0λ=0. Theorem 4.1, Proposition 4.3 and Lemma 4.8 have random initial states converging in probability, and λ>0\lambda>0λ>0.
  • Stochastic order. ≤st\le_{st}≤st​ for processes means the existence of an ordered coupling with the right path laws. Proposition 3.6's conditional probability is stated for each value of the integer A(T)A(T)A(T).
  • Correction. Proposition 3.1 as printed quantifies over m≤bm\le bm≤b. For finite bbb the proof also needs the ordering of the discarded counts, m=b+1m=b+1m=b+1, and the formal statement orders every level m≥1m\ge1m≥1.

A formalization that states only "every limit point solves (2.1)", or that measures convergence coordinatewise, would be vacuous or weaker: it is ruled out by requiring the limit's existence and ℓ1\ell_1ℓ1​ convergence.

Needed infrastructure. The development needs Poisson clocks and thinning, martingale bounds for counting processes, compactness in ℓ1\ell^1ℓ1, tightness and Prokhorov's theorem on Polish spaces, and the Skorohod representation. The ℓ1\ell_1ℓ1​ compactness and tightness criteria (Lemmas 4.6, 4.7) and the stack ordering (Proposition 3.1) are reusable on their own. Proofs of any milestone are welcome, as are proofs of Theorem 2.1 that bypass Theorem 4.1.

Selected references

  • D. Mukherjee, S. C. Borst, J. S. H. van Leeuwaarden, P. A. Whiting, Universality of Power-of-d Load Balancing in Many-Server Systems, Stochastic Systems 8(4), 2018. arXiv:1612.00723v2, https://arxiv.org/abs/1612.00723
  • P. Eschenfeldt, D. Gamarnik, Join the Shortest Queue with Many Servers. The Heavy-Traffic Asymptotics, Mathematics of Operations Research 43(3), 2018. https://arxiv.org/abs/1502.00999
  • M. Mitzenmacher, The Power of Two Choices in Randomized Load Balancing, IEEE Transactions on Parallel and Distributed Systems 12(10), 2001. https://doi.org/10.1109/71.963420
  • N. D. Vvedenskaya, R. L. Dobrushin, F. I. Karpelevich, Queueing System with Selection of the Shortest of Two Queues: An Asymptotic Approach, Problems of Information Transmission 32(1), 1996.
  • P. J. Hunt, T. G. Kurtz, Large Loss Networks, Stochastic Processes and their Applications 53(2), 1994. https://doi.org/10.1016/0304-4149(94)90063-9
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
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Mathematical PhysicsPartial Differential EquationsProbability·Captain: mikedeng1

Global-in-Time Mean-Field Convergence for Singular Riesz-Type Diffusive Flows 2: A Uniform-in-Time Modulated-Energy Bound for Globally Superharmonic Riesz-Type PotentialsResearch Paper

Motivation

Systems of many particles that interact through a singular pair potential and are subject to independent noise appear in plasma physics (Coulomb interactions), in vortex models of fluids, in models of collective behaviour and in the analysis of training dynamics of wide neural networks. When the number of particles NNN is large, the empirical measure of the system is expected to follow a deterministic nonlinear partial differential equation, the mean-field limit. For singular interactions the classical coupling arguments, which need Lipschitz forces, do not apply. The modulated-energy method of Serfaty (Duke Math. J. 2020) and its extensions by Duerinckx, Nguyen, Rosenzweig and Serfaty (NRS21, arXiv:2107.02592) give quantitative convergence for Riesz-type potentials ∣x∣−s|x|^{-s}∣x∣−s, but with rates that degrade exponentially in time.

M. Rosenzweig and S. Serfaty (arXiv:2108.09878v1, 2021) show that additive noise improves this: the expected modulated energy grows at most polynomially in time for sub-Coulombic potentials (their Theorem 1.1, the subject of the first mission of this series), and stays bounded uniformly in time when the potential is globally superharmonic (their Theorem 1.2, the subject of this mission). Uniform-in-time propagation of chaos had been known for smooth or convex interactions; this result covers singular, non-gradient interactions on the whole space.

Setting

Fix d≥3d\ge3d≥3, an exponent 0≤s<d−20\le s<d-20≤s<d−2, a diffusion strength σ>0\sigma>0σ>0 and a d×dd\times dd×d matrix M\mathbb MM with Mξ⋅ξ≤0\mathbb M\xi\cdot\xi\le0Mξ⋅ξ≤0 for all ξ\xiξ. The particle system is

dxit=1N∑j≠iM∇g(xit−xjt) dt+2σ dWit,i=1,…,N,dx^t_i=\frac1N\sum_{j\ne i}\mathbb M\nabla\mathsf g(x^t_i-x^t_j)\,dt+\sqrt{2\sigma}\,dW^t_i,\qquad i=1,\dots,N,dxit​=N1​j=i∑​M∇g(xit​−xjt​)dt+2σ​dWit​,i=1,…,N,

started from pairwise distinct points xN0=(x10,…,xN0)x^0_N=(x^0_1,\dots,x^0_N)xN0​=(x10​,…,xN0​) and driven by independent standard Brownian motions W1,…,WNW_1,\dots,W_NW1​,…,WN​ in Rd\mathbb R^dRd. The potential g\mathsf gg is admissible: it satisfies ten assumptions (i)–(x) on symmetry, blow-up at 000, superharmonicity near 000, derivative bounds of order ∣x∣−s−k|x|^{-s-k}∣x∣−s−k, a doubling property, a Fourier transform comparable to ∣ξ∣−(d−s)|\xi|^{-(d-s)}∣ξ∣−(d−s), an extension to Rd+m\mathbb R^{d+m}Rd+m when d−4<sd-4<sd−4<s, a Calderón–Zygmund property in the cases s=d−2ks=d-2ks=d−2k, and M:∇⊗2g≥0\mathbb M:\nabla^{\otimes2}\mathsf g\ge0M:∇⊗2g≥0. The model case is g(x)=∣x∣−s\mathsf g(x)=|x|^{-s}g(x)=∣x∣−s.

The mean-field equation is

∂tμ=−div⁡(μ M∇g∗μ)+σΔμ,μ∣t=0=μ0,\partial_t\mu=-\operatorname{div}(\mu\,\mathbb M\nabla\mathsf g*\mu)+\sigma\Delta\mu,\qquad\mu|_{t=0}=\mu^0,∂t​μ=−div(μM∇g∗μ)+σΔμ,μ∣t=0​=μ0,

for a probability density μ0∈L∞\mu^0\in L^\inftyμ0∈L∞, solved in the mild (Duhamel) sense in C([0,∞);L1∩L∞)C([0,\infty);L^1\cap L^\infty)C([0,∞);L1∩L∞). Closeness of the empirical measure μNt=1N∑iδxit\mu_N^t=\frac1N\sum_i\delta_{x^t_i}μNt​=N1​∑i​δxit​​ to μt\mu^tμt is measured by the modulated energy

FN(xN,μ)=∫(Rd)2∖△g(x−y) d(1N∑i=1Nδxi−μ)⊗2(x,y),F_N(x_N,\mu)=\int_{(\mathbb R^d)^2\setminus\triangle}\mathsf g(x-y)\,d\Big(\frac1N\sum_{i=1}^N\delta_{x_i}-\mu\Big)^{\otimes2}(x,y),FN​(xN​,μ)=∫(Rd)2∖△​g(x−y)d(N1​i=1∑N​δxi​​−μ)⊗2(x,y),

where the diagonal △\triangle△ is removed. The potential is globally superharmonic if Δg≤0\Delta\mathsf g\le0Δg≤0 on all of Rd∖{0}\mathbb R^d\setminus\{0\}Rd∖{0} ("r0=∞r_0=\inftyr0​=∞" in assumption (iii)).

Formalization targets

Goal: Theorem 1.2 for 0<s<d−20<s<d-20<s<d−2

For globally superharmonic admissible g\mathsf gg and every d/(s+2)<p≤∞d/(s+2)<p\le\inftyd/(s+2)<p≤∞ there are βp>0\beta_p>0βp​>0 (depending on s,d,ps,d,ps,d,p), C>0C>0C>0 (depending on s,d,σ,M,g,∥μ0∥L∞s,d,\sigma,\mathbb M,\mathsf g,\|\mu^0\|_{L^\infty}s,d,σ,M,g,∥μ0∥L∞​), Cp>0C_p>0Cp​>0 and N0N_0N0​ such that for all t≥0t\ge0t≥0 and N≥N0N\ge N_0N≥N0​,

E(∣FN(xNt,μt)∣)≤C(∣FN(xN0,μ0)∣+CpN−βp).\mathbb E\big(|F_N(x^t_N,\mu^t)|\big)\le C\big(|F_N(x^0_N,\mu^0)|+C_pN^{-\beta_p}\big).E(∣FN​(xNt​,μt)∣)≤C(∣FN​(xN0​,μ0)∣+Cp​N−βp​).

The right side does not depend on ttt. The case s=0s=0s=0 of the paper's display (1.19) is not part of the goal (see Formalization scope).

Milestones

The proof combines an inequality for the time derivative of the expected modulated energy (Proposition 6.3), lower bounds for the energy and for the diffusion term (Remarks 5.10, 5.11, Proposition 5.12, Remark 5.13, Corollary 5.14), a commutator estimate for the transport term (Proposition 5.15), and decay of ∥μt∥Lp\|\mu^t\|_{L^p}∥μt∥Lp​ (Remark 3.4, Proposition 3.8), with the potential estimates of Lemma 2.3 and Remark 2.5.

Significance

A uniform-in-time bound means that the mean-field description is valid on time scales that do not shrink as the accuracy requirement grows. Combined with the control of negative Sobolev norms by the modulated energy, it yields uniform-in-time convergence in law of the empirical measure and, for chaotic initial data, uniform-in-time propagation of chaos at an explicit rate, for singular interactions such as sub-Coulombic Riesz gases with dissipative or conservative dynamics.

The result is proved in the paper. No part of it, nor of the modulated-energy method, is formalized in any proof assistant. A formalization would produce a reusable library: Riesz potentials and their L1L^1L1–LpL^pLp interpolation, heat-type decay of nonlinear Fokker–Planck equations, smeared potentials and electric-energy lower bounds, renormalized commutator estimates, and a pathwise treatment of interacting diffusions with additive noise. The milestones are independent statements and can be proved separately.

Difficulty

The obvious Gronwall argument on the modulated energy fails twice. First, FNF_NFN​ is not nonnegative; it is bounded below only up to errors involving ∥μ∥L∞\|\mu\|_{L^\infty}∥μ∥L∞​, and the lower bounds near the singularity need the smearing of point charges on spheres. Second, the error terms produced when the commutator and diffusion terms are bounded must be integrable on [0,∞)[0,\infty)[0,∞); with the estimates of the general (local superharmonicity) case they grow linearly in time. Global superharmonicity removes an η2\eta^2η2 error term and lets every error carry a power of ∥μt∥L∞\|\mu^t\|_{L^\infty}∥μt∥L∞​, which decays like (σt)−d/2(\sigma t)^{-d/2}(σt)−d/2 by the Carlen–Loss method; for s=0s=0s=0 long-range effects still produce growth, which is why that case is excluded. Itô's formula cannot be applied directly to the singular energy and requires a truncation, whose stochastic integrals are removed in expectation only in the limit.

Formalization scope

All objects live in the Lean namespace RieszMF.Global and in one definitions module. Space is EuclideanSpace ℝ (Fin d); derivatives are iteratedFDeriv (operator norm), gradient and the Laplacian of Mathlib. The committed conventions:

  1. Fourier conditions (vi) and (1.17) are read away from the origin: a function g^\hat{\mathsf g}g^​ with ∫g Fφ=∫g^φ\int\mathsf g\,\mathcal F\varphi=\int\hat{\mathsf g}\varphi∫gFφ=∫g^​φ for Schwartz φ\varphiφ vanishing near 000.
  2. Assumption (iv) has a constant CkC_kCk​ for each kkk; quantities singular at 000 are required for x≠0x\neq0x=0 only; (ix) is stated componentwise with an L2L^2L2-bounded operator represented by the kernel off the support.
  3. Global superharmonicity is Δg≤0\Delta\mathsf g\le0Δg≤0 on Rd∖{0}\mathbb R^d\setminus\{0\}Rd∖{0}, together with (1.15)–(1.16) on all of Rd+m∖{0}\mathbb R^{d+m}\setminus\{0\}Rd+m∖{0} when d−4<sd-4<sd−4<s; (v) and (vii) keep a finite radius.
  4. Doubling condition (vii) for s>0s>0s>0 is read as g(y)<csg(x)\mathsf g(y)<c_s\mathsf g(x)g(y)<cs​g(x) whenever ∣y∣≥2∣x∣|y|\ge2|x|∣y∣≥2∣x∣, x≠0x\ne0x=0, with cs<1c_s<1cs​<1. The page prints g(x)<csg(y)\mathsf g(x)<c_s\mathsf g(y)g(x)<cs​g(y), which contradicts the blow-up (ii) and would leave no admissible potential, so the goal would hold vacuously. The model potential ∣x∣−s|x|^{-s}∣x∣−s satisfies the reading used here.
  5. The particle system is the pathwise integral equation (no Itô integral is needed for additive noise), with continuous paths and no collisions almost surely; the Brownian family is N⋅dN\cdot dN⋅d jointly independent standard real Brownian motions.
  6. The mild formulation of (1.5) requires every integral to converge absolutely and continuity in L1∩L∞L^1\cap L^\inftyL1∩L∞.
  7. Expectations of ∣FN∣|F_N|∣FN​∣ are lower Lebesgue integrals, and Proposition 6.3 moves positive and negative parts across the inequality, so no integrability is presupposed and no ∞−∞\infty-\infty∞−∞ arises.
  8. Constants are quantified after exactly the objects they may depend on: βp\beta_pβp​ after s,d,ps,d,ps,d,p; CCC after σ,M,g\sigma,\mathbb M,\mathsf gσ,M,g and ∥μ0∥L∞\|\mu^0\|_{L^\infty}∥μ0∥L∞​; CpC_pCp​ and N0N_0N0​ after ppp; all before μ0\mu^0μ0, NNN, the configuration, the probability space and ttt.

Restriction. The goal is Theorem 1.2 for 0<s<d−20<s<d-20<s<d−2 only, where the paper's time factor 1+(t1/σlog⁡(1+t))1s=01+(t^{1/\sigma}\log(1+t))\mathbf 1_{s=0}1+(t1/σlog(1+t))1s=0​ equals 111. For s=0s=0s=0 the proof yields a factor of order tC/σt^{C/\sigma}tC/σ rather than the printed t1/σlog⁡(1+t)t^{1/\sigma}\log(1+t)t1/σlog(1+t); the logarithmic case is covered by the first mission of this series.

Excluded trivializations. A statement in which CCC is chosen after μ0\mu^0μ0, NNN or the configuration, in which a divergent integral is read as 000, in which the solution classes are empty, or which uses N=0N=0N=0 or a division by zero is not a formalization of the theorem; the statements here avoid each of these.

Contributions are welcome on any milestone, on the existence of solutions in the classes used (which shows the hypotheses are satisfiable), and on general infrastructure (Riesz potentials, sphere averages, heat-kernel estimates) that other missions can reuse.

Selected references

  • M. Rosenzweig, S. Serfaty, Global-in-time mean-field convergence for singular Riesz-type diffusive flows, arXiv:2108.09878v1, 2021; Ann. Appl. Probab. 33(2), 2023. https://arxiv.org/abs/2108.09878
  • Q.-H. Nguyen, M. Rosenzweig, S. Serfaty, Mean-field limits of Riesz-type singular flows, Ars Inveniendi Analytica, 2022. https://arxiv.org/abs/2107.02592
  • S. Serfaty, Mean field limit for Coulomb-type flows, Duke Math. J. 169(15), 2020. https://doi.org/10.1215/00127094-2020-0019
  • M. Duerinckx, Mean-field limits for some Riesz interaction gradient flows, SIAM J. Math. Anal. 48(3), 2016. https://doi.org/10.1137/15M1042620
  • E. A. Carlen, M. Loss, Optimal smoothing and decay estimates for viscously damped conservation laws, with applications to the 2-D Navier–Stokes equation, Duke Math. J. 81(1), 1995. https://doi.org/10.1215/S0012-7094-95-08110-1
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Real-Time Dynamic Pricing for Revenue Management with Reusable Resources, Advance Reservation, and Deterministic Service Time Requirements II: Average-Loss Bound for Batch-Adjusted DPCResearch Paper

Motivation

Hotel rooms, rental cars, cloud servers, operating rooms and rental equipment are reusable resources: a customer occupies capacity for a fixed service time, and the capacity returns to the firm afterwards. Many of these settings also allow advance reservation, where a request made today is for a service that starts later. Lei and Jasin study dynamic pricing in this setting. Prices are posted period by period, demand is non-stationary, and the firm wants revenue close to the best achievable while never booking more units than it owns.

Classical network revenue management, where capacity is sold once and never returns, has an extensive asymptotic theory. In that literature, controls that re-solve or adjust a fluid (deterministic) plan are known to lose a vanishing fraction of the optimal revenue as demand and capacity grow (Gallego and van Ryzin 1997; Jasin 2014). Reusable resources break the standard argument, because each sale removes capacity for a window of time and not for the rest of the horizon. Lei and Jasin give the first control for reusable resources with non-stationary arrivals, deterministic service times and advance reservation whose average loss is o(θ−1/2)o(\theta^{-1/2})o(θ−1/2) in the scale parameter θ\thetaθ (Lei and Jasin, Operations Research 2020).

Setting

A firm manages III resource types with integer capacities Ci≥1C_i \ge 1Ci​≥1 and sells K≥1K \ge 1K≥1 service types over periods t=1,…,Tt = 1, \dots, Tt=1,…,T. At most one request arrives per period. A type-kkk request made at the beginning of period ttt uses aik∈{0,1}a_{ik} \in \{0,1\}aik​∈{0,1} units of resource iii during periods t+ℓk,…,t+ℓk+nk−1t+\ell_k, \dots, t+\ell_k+n_k-1t+ℓk​,…,t+ℓk​+nk​−1. Here nkn_knk​ is the service time and ℓk\ell_kℓk​ the reservation lead time.

In each period the firm chooses a demand-rate vector λt∈Ωλ=[0,λU]K\lambda^t \in \Omega_\lambda = [0,\lambda_U]^Kλt∈Ωλ​=[0,λU​]K, which is equivalent to choosing prices. A type-kkk request then arrives with probability λkt\lambda^t_kλkt​, independently of the past given λt\lambda^tλt, and the expected revenue rate is rt(λt)r^t(\lambda^t)rt(λt). The deterministic relaxation DET-H maximizes ∑t=1Trt(λt)\sum_{t=1}^T r^t(\lambda^t)∑t=1T​rt(λt) over λt∈Ωλ\lambda^t \in \Omega_\lambdaλt∈Ωλ​, subject to

∑k=1K∑s : s+ℓk≤t≤s+ℓk+nk−1aikλks≤Cifor every resource i and period t≤T.\sum_{k=1}^K \sum_{s \,:\, s+\ell_k \le t \le s+\ell_k+n_k-1} a_{ik}\lambda^s_k \le C_i \qquad \text{for every resource } i \text{ and period } t \le T.k=1∑K​s:s+ℓk​≤t≤s+ℓk​+nk​−1∑​aik​λks​≤Ci​for every resource i and period t≤T.

Its optimal value JHDJ^D_HJHD​ bounds the optimal expected revenue, and the average loss of a control π\piπ is L(π)=(JHD−E[Rπ])/T\mathcal{L}(\pi) = (J^D_H - \mathbf{E}[R^\pi])/TL(π)=(JHD​−E[Rπ])/T. Let λD\lambda^DλD be an optimal solution of DET-H. The quantity n‾k\underline{n}_kn​k​ is the smallest number of periods with λkt,D>0\lambda^{t,D}_k > 0λkt,D​>0 inside any service cycle of type kkk that carries positive demand.

The control DPC-B(m,ϵ)(m,\epsilon)(m,ϵ) splits the horizon, for each type kkk, into adjacent batches Tkb\mathcal{T}_k^bTkb​, each with mkm_kmk​ positive-rate periods. In period ttt it posts

λkt=Proj[0,λU][λkt,D−(ϵkn‾k+1mk∑s∈Tkβk(t)−1(Dks−λks))1{λkt,D>0}],\lambda^t_k = \mathrm{Proj}_{[0,\lambda_U]}\Bigl[\lambda^{t,D}_k - \Bigl(\frac{\epsilon_k}{\underline{n}_k} + \frac{1}{m_k}\sum_{s \in \mathcal{T}_k^{\beta_k(t)-1}} (D^s_k - \lambda^s_k)\Bigr)\mathbf{1}\{\lambda^{t,D}_k > 0\}\Bigr],λkt​=Proj[0,λU​]​[λkt,D​−(n​k​ϵk​​+mk​1​s∈Tkβk​(t)−1​∑​(Dks​−λks​))1{λkt,D​>0}],

where βk(t)\beta_k(t)βk​(t) is the batch containing ttt. The rate is set to 000 when fewer than aika_{ik}aik​ units of some resource iii are free at the service start t+ℓkt+\ell_kt+ℓk​. The buffer ϵk\epsilon_kϵk​ protects capacity, and the batch term corrects for the demand surprises of the previous batch.

Formalization targets

Goal: Theorem 3, display (8)

There is a constant M3>0M_3>0M3​>0, depending only on KKK, the curvature constant Ψ\PsiΨ of Assumption A5 and a bound RRR on ∣rt∣|r^t|∣rt∣, such that for every instance, every valid batch partition with mk≤n‾km_k \le \underline{n}_kmk​≤n​k​ and every ϵk\epsilon_kϵk​ in the stated range,

L(DPC-B(m,ϵ))≤M3∑k=1K[ϵkn‾k+1mk+Tmkexp⁡{−(min⁡jϵj−1)2256K2min⁡{max⁡iCi,mk}}].\mathcal{L}(\text{DPC-B}(m,\epsilon)) \le M_3 \sum_{k=1}^K \Bigl[\frac{\epsilon_k}{\underline{n}_k} + \frac{1}{m_k} + \frac{T}{m_k}\exp\Bigl\{-\frac{(\min_j\epsilon_j-1)^2}{256K^2\min\{\max_i C_i, m_k\}}\Bigr\}\Bigr].L(DPC-B(m,ϵ))≤M3​k=1∑K​[n​k​ϵk​​+mk​1​+mk​T​exp{−256K2min{maxi​Ci​,mk​}(minj​ϵj​−1)2​}].

The constant is uniform in TTT, CCC, nkn_knk​, ℓk\ell_kℓk​, mkm_kmk​ and ϵk\epsilon_kϵk​, which is what makes the bound informative.

Milestones

  1. Lemma EC.3: on the good event G(ϵ,m,δ)\mathcal{G}(\epsilon,m,\delta)G(ϵ,m,δ), the free capacity satisfies Ct⪰eC^t \succeq eCt⪰e and the corrected rates stay inside (0,λU)(0,\lambda_U)(0,λU​).
  2. (EC.22): on G\mathcal{G}G, the posted rate equals the unprojected corrected rate.
  3. Lemma EC.4, as proved in (EC.23): P(Gˉ)≤∑k4Tmkexp⁡{min⁡{max⁡iCi,mk}γk2−min⁡jϵj−18Kγk}\mathbf{P}(\bar{\mathcal{G}}) \le \sum_k \frac{4T}{m_k}\exp\{\min\{\max_i C_i, m_k\}\gamma_k^2 - \frac{\min_j\epsilon_j-1}{8K}\gamma_k\}P(Gˉ​)≤∑k​mk​4T​exp{min{maxi​Ci​,mk​}γk2​−8Kminj​ϵj​−1​γk​} for all γk∈(0,1]\gamma_k \in (0,1]γk​∈(0,1].
  4. E[(∑s∈TkbΔks)2]≤mk\mathbf{E}[(\sum_{s\in\mathcal{T}_k^b}\Delta^s_k)^2] \le m_kE[(∑s∈Tkb​​Δks​)2]≤mk​ for every batch.
  5. E([∇rt(λt,D)]⊤(ηδt⊙ηet))=0\mathbf{E}([\nabla r^t(\lambda^{t,D})]^\top(\eta^t_\delta\odot\eta^t_e)) = 0E([∇rt(λt,D)]⊤(ηδt​⊙ηet​))=0.

A companion item states Lemma 2 in this setting: stretching λD\lambda^DλD in time solves DET-H for the θ\thetaθ-th system of display (7).

Significance

Along the scaling (7), Theorem 3 with mk≈n‾k2/3m_k \approx \underline{n}_k^{2/3}mk​≈n​k2/3​ gives an average loss of O(θ−2/3log⁡1/2θ)O(\theta^{-2/3}\log^{1/2}\theta)O(θ−2/3log1/2θ). The non-adaptive control DPC of the same paper achieves O(θ−1/2log⁡1/2θ)O(\theta^{-1/2}\log^{1/2}\theta)O(θ−1/2log1/2θ) (its Theorem 1). The result shows that batch-level feedback improves on the square-root barrier for reusable resources, and it does so with heterogeneous service times and advance reservation, which cover car rental and hotel bookings.

Theorem 3 and its lemmas are proved in the paper's e-companion. No machine-checked proof of them, and no formal model of reusable-resource revenue management, is known. The mission produces a Lean model of the setting: capacity windows with lead times, the availability table C~(t,s)\tilde C(t,s)C~(t,s), an adapted control on finite sample paths, and its exact path law. On top of that model it states the paper's main bound in full. Several printed steps need repair (see the scope section), so a formal proof would also settle the exact constants.

Difficulty

The obvious route bounds each period's loss by a Taylor expansion around λt,D\lambda^{t,D}λt,D and controls the deviations by a martingale inequality. That route needs the control to coincide with the unprojected corrected rate for the whole horizon, that is, no capacity shortfall and no clipping. Capacity is a moving window of overlapping services with different lengths and lead times, so a shortfall at one period depends on requests made up to nk+ℓkn_k+\ell_knk​+ℓk​ periods earlier, in other batches and other types. The batch correction makes the rates depend on past errors, so the errors are martingale differences, not independent variables. The concentration bound must hold uniformly over batches whose number grows with TTT, with a variance proxy min⁡{max⁡iCi,mk}\min\{\max_i C_i, m_k\}min{maxi​Ci​,mk​} that is not the batch length. The early periods, before any service of type kkk has completed, need a separate threshold (the two cases of (EC.17)).

Formalization scope

All objects are defined in the namespace ReusablePricing.DPCB. The conventions are fixed as follows.

  • Periods are 1,…,T1,\dots,T1,…,T. A sample path is a function Fin T → Option (Fin K), recording no request or one request of a type in each period. Expectations are finite sums against the exact path law: the product over periods of the one-period law, whose probabilities are the rates posted given the past. The demand law is never left as a hypothesis.
  • Decisions are rates. A turn-off is rate 000. Prices and A1–A3 do not appear. The bound RRR on ∣rt∣|r^t|∣rt∣ over Ωλ\Omega_\lambdaΩλ​ replaces the proofs' rur^uru. KλU≤1K\lambda_U \le 1KλU​≤1 is assumed, as implied by at most one request per period.
  • Capacity windows are empty for t≤ℓkt \le \ell_kt≤ℓk​. Ct=C~(t,t)C^t = \tilde C(t,t)Ct=C~(t,t), and C~\tilde CC~ is defined by its defining sentence on p. 18, not by the update rule of Step 2a, whose indices do not match its own explanation. Admission is tested for services starting within the horizon.
  • n‾\underline{n}n​ in (EC.17) is min⁡kn‾k\min_k\underline{n}_kmink​n​k​. The events of (EC.16) are read over the batches Tkb\mathcal{T}_k^bTkb​. Statements "on G\mathcal{G}G" are made on paths of positive probability.
  • Lemma EC.4 is stated with the 8K8K8K that its proof establishes, not the printed 4K4K4K.
  • Goal statements carry every standing hypothesis of Section 6: optimality of λD\lambda^DλD, the convention λkt,D∈{0}∪(0,λU)\lambda^{t,D}_k\in\{0\}\cup(0,\lambda_U)λkt,D​∈{0}∪(0,λU​), A4, A5, and the existence of a demand-carrying cycle for every type, which n‾k\underline{n}_kn​k​ presupposes. The sanity check exhibits instances, with and without lead time, where all hypotheses of Theorem 3 hold and the ϵ\epsilonϵ-range is nonempty.

The constant M3M_3M3​ is quantified before the instance, after only KKK, Ψ\PsiΨ and RRR. Choosing it after the instance would make the bound trivial, because the loss never exceeds 2R2R2R.

A complete development needs Freedman- or Doob-type inequalities for bounded martingale differences on finite path spaces, second-order Taylor bounds for C2C^2C2 functions on boxes in RK\mathbb{R}^KRK, and window-counting lemmas for capacity. The first two are reusable well beyond this mission. Contributions of any of the milestones, of general martingale tools for finite adapted processes, or of a proof of the companion Lemma 2 are welcome.

Selected references

  • Y. Lei and S. Jasin, Real-Time Dynamic Pricing for Revenue Management with Reusable Resources, Advance Reservation, and Deterministic Service Time Requirements, Operations Research, 2020. https://doi.org/10.1287/opre.2019.1906 (author manuscript: SSRN 2816718, https://ssrn.com/abstract=2816718)
  • G. Gallego and G. van Ryzin, A Multiproduct Dynamic Pricing Problem and Its Applications to Network Yield Management, Operations Research 45(1), 1997. https://doi.org/10.1287/opre.45.1.24
  • S. Jasin, Reoptimization and Self-Adjusting Price Control for Network Revenue Management, Operations Research 62(5), 2014. https://doi.org/10.1287/opre.2014.1276
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Real-Time Dynamic Pricing for Revenue Management with Reusable Resources, Advance Reservation, and Deterministic Service Time Requirements I: Average-Loss Bound for Deterministic Price ControlResearch Paper

Motivation

Hotel rooms, rental cars, cloud servers, hospital beds and event spaces are reusable resources: a customer occupies a unit for a while and then returns it. Pricing them differs from classical revenue management, where a sold unit is gone for good. A sale now blocks capacity only for the length of the service, so the binding constraint is how many services overlap at once. Lei and Jasin (Oper. Res. 2020) study dynamic pricing in this setting with deterministic service times and, in the general model, advance reservations. They measure a pricing control by its average loss against a deterministic (fluid) benchmark.

The paper has two main results. Theorem 1 bounds the loss of a static heuristic, the Deterministic Price Control DPC(ϵ\epsilonϵ). Theorem 3 bounds the loss of an adaptive variant and is treated in the companion mission (II). This mission formalizes Theorem 1, the lemmas its proof rests on (Lemmas EC.1–EC.2 and the displays (EC.14), (EC.15) of the e-companion), and two structural lemmas of the model: the fluid upper bound J∗≤JDJ^* \le J^DJ∗≤JD (Lemma 1) and the scaling of the fluid solution (Lemma 2).

Setting

A firm manages III resource types with integer capacities C=(Ci)⪰eC = (C_i) \succeq eC=(Ci​)⪰e and offers JJJ service types over periods t=1,…,Tt = 1, \dots, Tt=1,…,T. At most one request arrives per period. A type-jjj request uses aij∈{0,1}a_{ij} \in \{0,1\}aij​∈{0,1} units of resource iii for nnn consecutive periods (a service cycle), and nnn divides TTT.

The firm posts a demand-rate vector λt∈Ωλ=[0,λU]J\lambda^t \in \Omega_\lambda = [0,\lambda_U]^Jλt∈Ωλ​=[0,λU​]J with λU≤1\lambda_U \le 1λU​≤1. A type-jjj request then arrives with probability λjt\lambda^t_jλjt​, independently of earlier periods given the posted rates, and the firm earns the revenue rate rt(λt)r^t(\lambda^t)rt(λt). Writing Djs∈{0,1}D^s_j \in \{0,1\}Djs​∈{0,1} for realized arrivals and (x)+=max⁡{1,x}(x)^+ = \max\{1,x\}(x)+=max{1,x}, the capacity free at the beginning of period ttt is

Ct=C−∑s=(t−n+1)+t−1ADs.C^t = C - \sum_{s=(t-n+1)^+}^{t-1} A D^s .Ct=C−s=(t−n+1)+∑t−1​ADs.

The deterministic relaxation is

DET:JD=max⁡{∑t=1Trt(λt):λt∈Ωλ, ∑s=(t−n+1)+tAλs⪯C  ∀t≤T},\mathbf{DET}:\quad J^D = \max\Big\{\sum_{t=1}^T r^t(\lambda^t) : \lambda^t \in \Omega_\lambda,\ \sum_{s=(t-n+1)^+}^{t} A\lambda^s \preceq C \ \ \forall t \le T\Big\},DET:JD=max{t=1∑T​rt(λt):λt∈Ωλ​, s=(t−n+1)+∑t​Aλs⪯C  ∀t≤T},

with optimal solution λD=(λt,D)\lambda^D = (\lambda^{t,D})λD=(λt,D). The revenue rates are strictly concave, bounded by RRR in absolute value, and have interior maximizers (A4). Near λt,D\lambda^{t,D}λt,D their gradients and Hessians are bounded by Ψ\PsiΨ (A5, with margins φL,φU\varphi_L, \varphi_UφL​,φU​).

The quantity n‾\underline nn​ of display (2) is the smallest number of periods with λjs,D>0\lambda^{s,D}_j > 0λjs,D​>0 in any service cycle that carries positive demand for some type jjj.

DPC(ϵ\epsilonϵ) posts, in period ttt, the rate λjt,D−(ϵ/n‾)1{λjt,D>0}\lambda^{t,D}_j - (\epsilon/\underline n)\mathbf 1\{\lambda^{t,D}_j > 0\}λjt,D​−(ϵ/n​)1{λjt,D​>0}, clamped to [0,λU][0,\lambda_U][0,λU​], for every type jjj with Ct⪰AjC^t \succeq A^jCt⪰Aj. It turns off every other type (rate 000). The average loss of a control π\piπ is L(π)=(JD−E[Rπ])/T\mathcal L(\pi) = (J^D - \mathbf E[R^\pi])/TL(π)=(JD−E[Rπ])/T.

Formalization targets

Goal: Theorem 1 (p. 13)

For ϵ∈(1,min⁡{min⁡{φL,φU}n‾, 6min⁡{max⁡iCi,n}+1}]\epsilon \in \big(1, \min\{\min\{\varphi_L,\varphi_U\}\underline n,\ 6\min\{\max_i C_i, n\} + 1\}\big]ϵ∈(1,min{min{φL​,φU​}n​, 6min{maxi​Ci​,n}+1}],

L(DPC(ϵ))≤M1[ϵn‾+Tnexp⁡{−(ϵ−1)236min⁡{max⁡iCi,n}}],\mathcal L(DPC(\epsilon)) \le M_1\Big[\frac{\epsilon}{\underline n} + \frac{T}{n}\exp\Big\{-\frac{(\epsilon-1)^2}{36\min\{\max_i C_i, n\}}\Big\}\Big],L(DPC(ϵ))≤M1​[n​ϵ​+nT​exp{−36min{maxi​Ci​,n}(ϵ−1)2​}],

with M1>0M_1 > 0M1​>0 depending only on JJJ, Ψ\PsiΨ and RRR, and not on TTT, CCC, nnn, ϵ\epsilonϵ or the other data.

Milestones (EC.3)

  1. Lemma EC.1. On the event G(ϵ,δ)\mathcal G(\epsilon,\delta)G(ϵ,δ) that cumulative demand errors stay below δ=(n‾−1)(ϵ−1)/(3n‾)\delta = (\underline n-1)(\epsilon-1)/(3\underline n)δ=(n​−1)(ϵ−1)/(3n​) within every cycle, Ct⪰eC^t \succeq eCt⪰e and λjt,D−ϵ/n‾∈(0,λU)\lambda^{t,D}_j - \epsilon/\underline n \in (0,\lambda_U)λjt,D​−ϵ/n​∈(0,λU​).
  2. (EC.14). On G(ϵ,δ)\mathcal G(\epsilon,\delta)G(ϵ,δ), DPC posts exactly λjt,D−(ϵ/n‾)1{λjt,D>0}\lambda^{t,D}_j - (\epsilon/\underline n)\mathbf 1\{\lambda^{t,D}_j>0\}λjt,D​−(ϵ/n​)1{λjt,D​>0}.
  3. (EC.15). E[exp⁡{±γ∑s∈cycle bΔjs}]≤exp⁡{min⁡{max⁡iCi,n}γ2}\mathbf E[\exp\{\pm\gamma\sum_{s\in\text{cycle }b}\Delta^s_j\}] \le \exp\{\min\{\max_i C_i,n\}\gamma^2\}E[exp{±γ∑s∈cycle b​Δjs​}]≤exp{min{maxi​Ci​,n}γ2} for γ∈(0,1]\gamma \in (0,1]γ∈(0,1].
  4. Lemma EC.2. P(Gˉ(ϵ,δ))≤(2JT/n)exp⁡{min⁡{max⁡iCi,n}γ2−δγ}\mathbf P(\bar{\mathcal G}(\epsilon,\delta)) \le (2JT/n)\exp\{\min\{\max_i C_i,n\}\gamma^2 - \delta\gamma\}P(Gˉ​(ϵ,δ))≤(2JT/n)exp{min{maxi​Ci​,n}γ2−δγ}.
  5. Step 2. JD−E[RDPC(ϵ)]≤T(ΨJϵ/n‾+(4RJT/n)exp⁡{min⁡{max⁡iCi,n}γ2−δγ})J^D - \mathbf E[R^{DPC(\epsilon)}] \le T\big(\Psi J\epsilon/\underline n + (4RJT/n)\exp\{\min\{\max_i C_i,n\}\gamma^2 - \delta\gamma\}\big)JD−E[RDPC(ϵ)]≤T(ΨJϵ/n​+(4RJT/n)exp{min{maxi​Ci​,n}γ2−δγ}).

Companion statements: Lemma 1 (J∗≤JDJ^* \le J^DJ∗≤JD for every feasible non-anticipating control) and Lemma 2 (for integer θ≥1\theta \ge 1θ≥1, λ⌈t/θ⌉,D\lambda^{\lceil t/\theta\rceil,D}λ⌈t/θ⌉,D solves the DET of the θ\thetaθ-th system T(θ)=θTT^{(\theta)} = \theta TT(θ)=θT, C(θ)=θCC^{(\theta)} = \theta CC(θ)=θC, n(θ)=θnn^{(\theta)} = \theta nn(θ)=θn).

Significance

Along the scaling (1), choosing ϵ\epsilonϵ of order θlog⁡θ\sqrt{\theta\log\theta}θlogθ​ in Theorem 1 gives an average loss of O(θ−1/2log⁡1/2θ)O(\theta^{-1/2}\log^{1/2}\theta)O(θ−1/2log1/2θ). A control computed entirely before the selling horizon is therefore asymptotically optimal for reusable resources, with an explicit rate. This bound is the baseline against which the paper's adaptive control (Theorem 3, rate O(θ−2/3log⁡1/2θ)O(\theta^{-2/3}\log^{1/2}\theta)O(θ−2/3log1/2θ)) is measured.

The proof shows a pattern common to fluid-based revenue management: a high-probability event on which the heuristic follows the fluid plan exactly, a martingale maximal inequality bounding the complement, and a Taylor bound for the cost of the buffer. Reusable resources add one ingredient: capacity is checked over sliding windows of length nnn.

The results are proved on paper; none is machine-checked. The formalization would provide a checked version of the model (sliding-window capacity, at most one arrival per period, turn-off), of the high-probability analysis, and of the uniform constant. The printed proof has slips that a checked proof must repair. In particular, the exponent obtained by EC.3's choice of γ\gammaγ is −n‾−2n‾⋅(ϵ−1)236min⁡{⋅}-\frac{\underline n-2}{\underline n}\cdot\frac{(\epsilon-1)^2}{36\min\{\cdot\}}−n​n​−2​⋅36min{⋅}(ϵ−1)2​; it differs from the printed one by an amount that a larger M1M_1M1​ absorbs.

Difficulty

The obvious argument says that DPC keeps an ϵ\epsilonϵ buffer, so it rarely runs out of capacity. The difficulty is that "rarely" has to hold uniformly over every sliding window of nnn periods. The rates DPC posts are themselves random, because a type is turned off whenever the realized free capacity is short.

Lemma EC.1 breaks this circularity by induction over periods on a fixed event. A capacity window of length n−1n-1n−1 straddles two consecutive cycles, which costs a factor 333 in δ\deltaδ, and only the periods with positive deterministic demand carry a buffer, which is why n‾\underline nn​ appears. The demand errors form a martingale-difference sequence with predictable, path-dependent rates, so (EC.15) needs a pathwise bound on the cumulative rate within a cycle. That bound comes from the DET constraint, not from independence.

Finally, the constant M1M_1M1​ must not depend on the instance. A bound in which M1M_1M1​ may depend on TTT or CCC is trivial, since the loss never exceeds 2R2R2R.

Formalization scope

Everything is stated in demand rates, as the paper does for DET and in all its proofs. Prices, A1–A3 and the price-derivative part of A5 do not appear. A turned-off type has rate 000.

A sample path is a function from {1,…,T}\{1,\dots,T\}{1,…,T} to "no request" or "one request of type jjj". Its probability is the product of the per-period probabilities under the rates the control posts, so expectations are finite sums. Expected revenue is E[∑trt(λt)]\mathbf E[\sum_t r^t(\lambda^t)]E[∑t​rt(λt)], the tower-property form of the proofs. Periods are 1,…,T1,\dots,T1,…,T, and window sums whose upper limit falls below the lower limit are empty.

The standing hypotheses, bundled as Standing φL φU Ψ R n̲, are:

  • I,J,n,T≥1I, J, n, T \ge 1I,J,n,T≥1, n∣Tn \mid Tn∣T, aij∈{0,1}a_{ij} \in \{0,1\}aij​∈{0,1} with a 111 in every column, C⪰eC \succeq eC⪰e, λU∈(0,1]\lambda_U \in (0,1]λU​∈(0,1];
  • JλU≤1J\lambda_U \le 1JλU​≤1 (added: one arrival per period on all of Ωλ\Omega_\lambdaΩλ​);
  • λD\lambda^DλD optimal for DET, with λjt,D∈{0}∪(0,λU)\lambda^{t,D}_j \in \{0\} \cup (0,\lambda_U)λjt,D​∈{0}∪(0,λU​);
  • A4 with the explicit bound RRR on ∣rt∣|r^t|∣rt∣, which replaces the paper's rur^uru;
  • A5, with the Hessian condition as a bound on the quadratic form;
  • n‾\underline nn​ as in (2), stated as an attained minimum, so n‾≥1\underline n \ge 1n​≥1;
  • the cycle assumption of p. 11.

The statements "on G(ϵ,δ)\mathcal G(\epsilon,\delta)G(ϵ,δ)" are claimed for every path of positive probability in the event. Theorem 1 quantifies M1M_1M1​ after JJJ, Ψ\PsiΨ, RRR and before everything else. This rules out the trivial reading in which M1M_1M1​ is chosen per instance. Step 2 uses n‾\underline nn​ where the printed line has nnn, and RRR for rur^uru. θ\thetaθ in Lemma 2 is an integer.

Two definition files carry the model: ReusablePricing.DPC.Model holds the instance, DET, A4–A5, n‾\underline nn​ and the θ\thetaθ-th system; ReusablePricing.DPC.Control holds the path law, DPC, loss, events and general controls. A complete proof needs a finite-path martingale toolkit: a Doob-type maximal inequality for exponential submartingales on a finite product space, and the Bernoulli moment-generating-function bound. It also needs a multivariate mean-value or Taylor estimate on a box and an induction over sliding capacity windows. The martingale tools are reusable beyond this mission. Contributions of those general lemmas, of proofs of individual milestones, and of the optional asymptotic corollary (4) are welcome.

Selected references

  • Y. Lei and S. Jasin, Real-Time Dynamic Pricing for Revenue Management with Reusable Resources, Advance Reservation, and Deterministic Service Time Requirements, Operations Research 68(3), 2020. https://doi.org/10.1287/opre.2019.1906 (author manuscript: SSRN 2816718, https://ssrn.com/abstract=2816718)
  • G. Gallego and G. van Ryzin, A Multiproduct Dynamic Pricing Problem and Its Applications to Network Yield Management, Operations Research 45(1), 1997. https://doi.org/10.1287/opre.45.1.24
  • S. Jasin, Reoptimization and Self-Adjusting Price Control for Network Revenue Management, Operations Research 62(5), 2014. https://doi.org/10.1287/opre.2014.1294
  • D. Williams, Probability with Martingales, Cambridge University Press, 1991. https://doi.org/10.1017/CBO9780511813658
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Mathematical PhysicsPartial Differential EquationsProbability·Captain: mikedeng1

Global-in-Time Mean-Field Convergence for Singular Riesz-Type Diffusive Flows 1: The Expected Modulated Energy Grows at Most Polynomially in TimeResearch Paper

Motivation

Systems of NNN particles that interact through a singular pair potential and are driven by independent noise are used to model vortices in viscous fluids, collective motion of micro-organisms, aggregation phenomena and, more recently, the training dynamics of wide neural networks and stochastic gradient methods. When NNN is large, one expects the empirical measure of the particles to be close to the solution of a deterministic nonlinear PDE, the mean-field limit. Proving this with an explicit rate is difficult when the interaction is singular, because the classical coupling arguments need a Lipschitz force.

The modulated-energy method (Duerinckx 2016, Serfaty 2020, Nguyen–Rosenzweig–Serfaty 2021) measures the distance between the particles and the limit through a renormalized Coulomb/Riesz energy and closes a Gronwall argument on it. Rosenzweig and Serfaty (arXiv:2108.09878) extended it to systems with additive noise in the sub-Coulombic range. This mission formalizes their first main result, Theorem 1.1: the expected modulated energy grows at most linearly in time (polynomially for logarithmic interactions). A companion mission covers their uniform-in-time Theorem 1.2.

Setting

Fix d≥3d\ge3d≥3 and 0≤s<d−20\le s<d-20≤s<d−2. Positions live in Rd\mathbb R^dRd with Lebesgue measure. A d×dd\times dd×d real matrix M\mathbb MM satisfies Mξ⋅ξ≤0\mathbb M\xi\cdot\xi\le0Mξ⋅ξ≤0 for all ξ\xiξ (gradient flows M=−I\mathbb M=-\mathbb IM=−I, Hamiltonian flows M\mathbb MM antisymmetric, and mixtures). The interaction potential g:Rd→R\mathsf g:\mathbb R^d\to\mathbb Rg:Rd→R is admissible: it satisfies ten assumptions (i)–(x), with model cases g(x)=−log⁡∣x∣\mathsf g(x)=-\log|x|g(x)=−log∣x∣ (s=0s=0s=0) and g(x)=∣x∣−s\mathsf g(x)=|x|^{-s}g(x)=∣x∣−s (0<s<d−20<s<d-20<s<d−2). In short: g\mathsf gg is even, blows up at 000, is superharmonic on a punctured ball B(0,r0)∖{0}B(0,r_0)\setminus\{0\}B(0,r0​)∖{0}, is smooth off the origin with ∣∇⊗kg(x)∣≤Ck∣x∣−(s+k)|\nabla^{\otimes k}\mathsf g(x)|\le C_k|x|^{-(s+k)}∣∇⊗kg(x)∣≤Ck​∣x∣−(s+k) (plus a logarithm when s=k=0s=k=0s=k=0), has a Fourier transform comparable to ∣ξ∣s−d|\xi|^{s-d}∣ξ∣s−d, has a doubling property near 000, admits a superharmonic extension to Rd+m\mathbb R^{d+m}Rd+m when d−4<sd-4<sd−4<s, has a Calderón–Zygmund kernel condition when s=d−2ks=d-2ks=d−2k, and satisfies M:∇⊗2g≥0\mathbb M:\nabla^{\otimes2}\mathsf g\ge0M:∇⊗2g≥0.

The particle system (1.1) is

dxit=1N∑j≠iM∇g(xit−xjt) dt+2σ dWit,xit∣t=0=xi0,dx^t_i=\frac1N\sum_{j\ne i}\mathbb M\nabla\mathsf g(x^t_i-x^t_j)\,dt+\sqrt{2\sigma}\,dW^t_i,\qquad x^t_i|_{t=0}=x^0_i,dxit​=N1​j=i∑​M∇g(xit​−xjt​)dt+2σ​dWit​,xit​∣t=0​=xi0​,

with distinct initial points, σ>0\sigma>0σ>0, and W1,…,WNW_1,\dots,W_NW1​,…,WN​ independent standard Brownian motions in Rd\mathbb R^dRd. The mean-field equation (1.5) is

∂tμ=−div⁡(μ M∇g∗μ)+σΔμ,μ∣t=0=μ0,\partial_t\mu=-\operatorname{div}(\mu\,\mathbb M\nabla\mathsf g*\mu)+\sigma\Delta\mu,\qquad\mu|_{t=0}=\mu^0,∂t​μ=−div(μM∇g∗μ)+σΔμ,μ∣t=0​=μ0,

for a bounded probability density μ0\mu^0μ0, solved in the class C([0,∞);P(Rd)∩L∞(Rd))C([0,\infty);\mathcal P(\mathbb R^d)\cap L^\infty(\mathbb R^d))C([0,∞);P(Rd)∩L∞(Rd)). The modulated energy (1.6) is

FN(xN,μ)=∫(Rd)2∖△g(x−y) d(1N∑i=1Nδxi−μ)⊗2(x,y),F_N(x_N,\mu)=\int_{(\mathbb R^d)^2\setminus\triangle}\mathsf g(x-y)\,d\Big(\frac1N\sum_{i=1}^N\delta_{x_i}-\mu\Big)^{\otimes2}(x,y),FN​(xN​,μ)=∫(Rd)2∖△​g(x−y)d(N1​i=1∑N​δxi​​−μ)⊗2(x,y),

the diagonal △\triangle△ being removed to discard the infinite self-interaction of each particle.

Formalization targets

Goal: Theorem 1.1

There are β>0\beta>0β>0 depending on s,ds,ds,d only and, for every σ\sigmaσ, M\mathbb MM, admissible g\mathsf gg and value of ∥μ0∥L∞\|\mu^0\|_{L^\infty}∥μ0∥L∞​, a constant C>0C>0C>0 and a threshold N0N_0N0​ such that for all N≥N0N\ge N_0N≥N0​ and t≥0t\ge0t≥0

E(∣FN(xNt,μt)∣)≤C(1+t+tσ+Cσ1s=0)(∣FN(xN0,μ0)∣+N−β).\mathbb E\big(|F_N(x^t_N,\mu^t)|\big)\le C\Big(1+t+t^{\frac{\sigma+C}\sigma}\mathbf 1_{s=0}\Big)\Big(|F_N(x^0_N,\mu^0)|+N^{-\beta}\Big).E(∣FN​(xNt​,μt)∣)≤C(1+t+tσσ+C​1s=0​)(∣FN​(xN0​,μ0)∣+N−β).

The exponent β\betaβ and the constant are left unspecified, as in the paper.

Milestones

In the order the proof uses them:

  1. Lemma 2.3 and Remark 2.5: L∞L^\inftyL∞ bounds for Riesz potentials and for ∇⊗kg∗f\nabla^{\otimes k}\mathsf g*f∇⊗kg∗f.
  2. Remark 3.4, Proposition 3.9 and Proposition 3.8: LpL^pLp monotonicity, the sharp log-Sobolev inequality, and heat-equation decay ∥μt∥Lq≲(σt)−d2(1p−1q)∥μ0∥Lp\|\mu^t\|_{L^q}\lesssim(\sigma t)^{-\frac d2(\frac1p-\frac1q)}\|\mu^0\|_{L^p}∥μt∥Lq​≲(σt)−2d​(p1​−q1​)∥μ0∥Lp​.
  3. Proposition 4.5: the particle system has a unique strong solution whose particles never collide, obtained as the limit of smoothly truncated systems.
  4. Remarks 5.2, 5.3 and Proposition 5.4: lower bounds on FNF_NFN​ through smeared point charges.
  5. Corollary 5.6: the diffusion term ∬(−Δg) d(μN−μ)⊗2\iint(-\Delta\mathsf g)\,d(\mu_N-\mu)^{\otimes2}∬(−Δg)d(μN​−μ)⊗2 is bounded below by −C(1+∥μ∥L∞)N−min⁡{2,d−s−2}/min⁡{s+4,d}-C(1+\|\mu\|_{L^\infty})N^{-\min\{2,d-s-2\}/\min\{s+4,d\}}−C(1+∥μ∥L∞​)N−min{2,d−s−2}/min{s+4,d}.
  6. Proposition 5.7: the renormalized commutator estimate.
  7. Proposition 6.3: the expected Itô inequality for FNF_NFN​.

Significance

The theorem is a quantitative mean-field limit for singular interactions with additive noise on the whole space, covering conservative and dissipative dynamics at once. Since FNF_NFN​ controls a negative-order Sobolev distance between μNt\mu_N^tμNt​ and μt\mu^tμt, it gives convergence of the empirical measure, at a rate in NNN that deteriorates at most linearly in ttt for s>0s>0s>0. Its proof isolates estimates (the LpL^pLp decay of the nonlinear equation, the sign of the diffusion term, the commutator bound) that are reused for the uniform-in-time result of the companion mission.

The paper's results are proved; none of them has a machine-checked proof. Formalizing the theorem requires the modulated-energy machinery (smeared charges, Fourier positivity, commutator estimates), a Carlen–Loss decay argument, and an Itô-free treatment of the stochastic system. The milestones of §§2–3 are classical harmonic analysis (Riesz potentials, the Gross–Carlen log-Sobolev inequality) and are of independent use.

Difficulty

A direct Gronwall argument on E∣FN∣\mathbb E|F_N|E∣FN​∣ fails twice. The diffusion term σ∬Δg d(μN−μ)⊗2\sigma\iint\Delta\mathsf g\,d(\mu_N-\mu)^{\otimes2}σ∬Δgd(μN​−μ)⊗2 has no sign for a general configuration, because the singularity of Δg\Delta\mathsf gΔg at the origin is integrated against a signed measure with atoms; its control needs a second modulated-energy estimate for −Δg-\Delta\mathsf g−Δg, which is a potential of order s+2s+2s+2 and may be super-Coulombic, hence the extension of assumption (viii). The commutator term requires ∥∇ut∥L∞\|\nabla u^t\|_{L^\infty}∥∇ut∥L∞​, and bounding it by ∥μ0∥L∞\|\mu^0\|_{L^\infty}∥μ0∥L∞​ alone produces exponential growth in time; the polynomial bound needs the time decay of ∥μt∥L∞\|\mu^t\|_{L^\infty}∥μt∥L∞​, which for a nonlinear, non-divergence-free drift is not given by comparison with the heat equation. Finally, the Itô computation for FNF_NFN​ along the singular dynamics needs truncation and stopping times, since g\mathsf gg is not C2C^2C2 at collisions.

Formalization scope

All objects are defined in one module RieszMF.Linear.Setting. Space is EuclideanSpace ℝ (Fin d) with Lebesgue measure; derivatives are iteratedFDeriv with operator norms, Δ\DeltaΔ is Mathlib's Laplacian, and the Fourier transform is Mathlib's ∫e−2πix⋅ξφ(x) dx\int e^{-2\pi ix\cdot\xi}\varphi(x)\,dx∫e−2πix⋅ξφ(x)dx. Assumption (iv) is read with a constant CkC_kCk​ for each kkk; (vi) and (1.17) as Fourier transforms paired with Schwartz functions vanishing near the origin; (iii) pointwise on the punctured ball; one radius r0r_0r0​ for (iii), (v), (vii), (viii); m≥1m\ge1m≥1 in (viii). Assumption (vii) for s>0s>0s>0 is printed as g(x)<csg(y)\mathsf g(x)<c_s\mathsf g(y)g(x)<cs​g(y) for ∣y∣≥2∣x∣|y|\ge2|x|∣y∣≥2∣x∣, which together with (ii) is unsatisfiable; it is stated as g(y)<csg(x)\mathsf g(y)<c_s\mathsf g(x)g(y)<cs​g(x).

The solution of (1.5) is a mild solution (3.1) in C([0,∞);L1∩L∞)C([0,\infty);L^1\cap L^\infty)C([0,∞);L1∩L∞) with continuity in the L1+L∞L^1+L^\inftyL1+L∞ norm, with each μt\mu^tμt a probability density; every integral of (3.1) is required to converge. Because the noise is additive, a solution of (1.1) is a measurable process whose paths almost surely are continuous, never collide, and satisfy the integral equation with the Brownian path; no stochastic integral appears. Brownian motions are Mathlib's IsBrownianReal coordinates, jointly independent over all N⋅dN\cdot dN⋅d coordinates. Expectations are lower Lebesgue integrals of nonnegative quantities, and Proposition 6.3 is stated in [0,∞][0,\infty][0,∞] with positive and negative parts on opposite sides, so no ∞−∞\infty-\infty∞−∞ and no default value of a divergent integral enters.

The constants follow the paper's dependency lists: β\betaβ depends on s,ds,ds,d only and is chosen before σ,M,g\sigma,\mathbb M,\mathsf gσ,M,g; CCC and N0N_0N0​ are chosen after σ,M,g,r0\sigma,\mathbb M,\mathsf g,r_0σ,M,g,r0​ and ∥μ0∥L∞\|\mu^0\|_{L^\infty}∥μ0∥L∞​, before the data, NNN, the configuration, the probability space and ttt. A formalization with constants chosen after μ0\mu^0μ0, NNN or the configuration, with N=0N=0N=0, with a junk-zero integral in FNF_NFN​ or in (3.1), or with an empty solution class does not count. Corollary 5.6 is posed exactly under its printed assumptions, although its proof for 0≤s≤d−40\le s\le d-40≤s≤d−4 uses the superharmonicity of −Δg-\Delta\mathsf g−Δg, which those assumptions do not list.

Contributions welcome: proofs of the milestones, a Lean development of Riesz potentials and of the sharp log-Sobolev inequality on Rd\mathbb R^dRd, and the well-posedness of the mean-field equation that the goal takes as a hypothesis (Proposition 3.1 and its global continuation, not posed here).

Selected references

  • M. Rosenzweig, S. Serfaty, Global-in-time mean-field convergence for singular Riesz-type diffusive flows, arXiv:2108.09878v1, 2021; Ann. Appl. Probab. 33(2), 2023. https://arxiv.org/abs/2108.09878
  • Q. H. Nguyen, M. Rosenzweig, S. Serfaty, Mean-field limits of Riesz-type singular flows with possible multiplicative transport noise, arXiv:2107.02592, 2021. https://arxiv.org/abs/2107.02592
  • S. Serfaty, Mean field limit for Coulomb-type flows, Duke Math. J. 169(15), 2887–2935, 2020 (appendix with M. Duerinckx). https://arxiv.org/abs/1803.08345
  • E. Carlen, M. Loss, Optimal smoothing and decay estimates for viscously damped conservation laws, with applications to the 2-D Navier–Stokes equation, Duke Math. J. 81(1), 1995. https://doi.org/10.1215/S0012-7094-95-08110-1
  • L. Gross, Logarithmic Sobolev inequalities, Amer. J. Math. 97(4), 1975. https://doi.org/10.2307/2373688
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Diffusion Approximation for Fully Coupled Stochastic Differential Equations 2: The Slow Component Converges Weakly to the Averaged SDE at an Explicit Rate (Regime 1)Research Paper

Motivation

Many stochastic models evolve on two time scales: a fast component that equilibrates quickly and a slow component driven by it. Planetary motion, climate models, geophysical flows and intracellular reaction networks are standard examples, and multiscale numerical methods for them approximate the slow component by a reduced equation. Such approximations are only useful with an error bound, and for the fully coupled case, where the fast and slow equations each depend on both components and the slow equation contains a large fluctuating drift, rates of convergence were missing.

Röckner and Xie (Ann. Probab. 49 (2021) 1205–1236) treat this case with only Hölder continuous coefficients and obtain explicit rates in four regimes. This mission poses the first regime, the classical averaging principle.

Timeline. Papanicolaou, Stroock and Varadhan (1977) proved the diffusion approximation for αε=βε=γε\alpha_\varepsilon=\beta_\varepsilon=\gamma_\varepsilonαε​=βε​=γε​ with a compact fast state space and time-independent coefficients. Pardoux and Veretennikov (2001, 2003, 2005) treated a noncompact homogeneous case with c≡0c\equiv0c≡0 and αε=γε\alpha_\varepsilon=\gamma_\varepsilonαε​=γε​ by martingale problems and the Poisson equation. Rates for the averaging principle when c=H≡0c=H\equiv0c=H≡0 were obtained by several authors, e.g. Givon (2007) and Liu (2010). Röckner and Xie (2021) give rates for the fully coupled system with Hölder coefficients in all four regimes.

Setting

Let x∈Rd1x\in\mathbb R^{d_1}x∈Rd1​ (fast) and y∈Rd2y\in\mathbb R^{d_2}y∈Rd2​ (slow), d1,d2≥1d_1,d_2\ge1d1​,d2​≥1. For small parameters αε,βε,γε>0\alpha_\varepsilon,\beta_\varepsilon,\gamma_\varepsilon>0αε​,βε​,γε​>0 tending to 000, with αε2/βε→0\alpha_\varepsilon^2/\beta_\varepsilon\to0αε2​/βε​→0, the two-scale system (1.4) is

dXtε=αε−2b(Xtε,Ytε)dt+βε−1c(Xtε,Ytε)dt+αε−1σ(Xtε,Ytε)dWt1,dX^\varepsilon_t=\alpha_\varepsilon^{-2}b(X^\varepsilon_t,Y^\varepsilon_t)dt+\beta_\varepsilon^{-1}c(X^\varepsilon_t,Y^\varepsilon_t)dt+\alpha_\varepsilon^{-1}\sigma(X^\varepsilon_t,Y^\varepsilon_t)dW^1_t,dXtε​=αε−2​b(Xtε​,Ytε​)dt+βε−1​c(Xtε​,Ytε​)dt+αε−1​σ(Xtε​,Ytε​)dWt1​, dYtε=F(t,Xtε,Ytε)dt+γε−1H(t,Xtε,Ytε)dt+G(t,Xtε,Ytε)dWt2,dY^\varepsilon_t=F(t,X^\varepsilon_t,Y^\varepsilon_t)dt+\gamma_\varepsilon^{-1}H(t,X^\varepsilon_t,Y^\varepsilon_t)dt+G(t,X^\varepsilon_t,Y^\varepsilon_t)dW^2_t,dYtε​=F(t,Xtε​,Ytε​)dt+γε−1​H(t,Xtε​,Ytε​)dt+G(t,Xtε​,Ytε​)dWt2​,

with X0ε=xX^\varepsilon_0=xX0ε​=x, Y0ε=yY^\varepsilon_0=yY0ε​=y and independent Brownian motions W1,W2W^1,W^2W1,W2.

Freezing yyy gives the frozen equation dXty=b(Xty,y)dt+σ(Xty,y)dWt1dX^y_t=b(X^y_t,y)dt+\sigma(X^y_t,y)dW^1_tdXty​=b(Xty​,y)dt+σ(Xty​,y)dWt1​ (1.7), with generator L0(x,y)=∑ijaij∂xixj2+∑ibi∂xi\mathscr L_0(x,y)=\sum_{ij}a^{ij}\partial^2_{x_ix_j}+\sum_ib^i\partial_{x_i}L0​(x,y)=∑ij​aij∂xi​xj​2​+∑i​bi∂xi​​, a=σσ∗/2a=\sigma\sigma^*/2a=σσ∗/2, and invariant probability measure μy\mu^yμy. A function is centered if its μy\mu^yμy-average vanishes for every yyy. The standing assumptions are: (Aσ), uniform nondegeneracy of σσ∗\sigma\sigma^*σσ∗; (Ab), lim⁡∣x∣→∞sup⁡y⟨x,b(x,y)⟩=−∞\lim_{|x|\to\infty}\sup_y\langle x,b(x,y)\rangle=-\inftylim∣x∣→∞​supy​⟨x,b(x,y)⟩=−∞; (AG), uniform nondegeneracy of GG∗GG^*GG∗; (AH), HHH is centered; and (2.7), the analogue of (Ab) for b+κcb+\kappa cb+κc, κ>0\kappa>0κ>0 small.

The averaged coefficients of Regime 1 are F^1(t,y)=∫F(t,x,y)μy(dx)\hat F_1(t,y)=\int F(t,x,y)\mu^y(dx)F^1​(t,y)=∫F(t,x,y)μy(dx) and G^1=(∫GG∗(t,x,y)μy(dx))1/2\hat G_1=(\int GG^*(t,x,y)\mu^y(dx))^{1/2}G^1​=(∫GG∗(t,x,y)μy(dx))1/2, and the averaged equation (2.9) is dY^t1=F^1(t,Y^t1)dt+G^1(t,Y^t1)dWt2d\hat Y^1_t=\hat F_1(t,\hat Y^1_t)dt+\hat G_1(t,\hat Y^1_t)dW^2_tdY^t1​=F^1​(t,Y^t1​)dt+G^1​(t,Y^t1​)dWt2​, Y^01=y\hat Y^1_0=yY^01​=y.

Regularity is measured in weighted Hölder classes: Cpδ,ϑC^{\delta,\vartheta}_pCpδ,ϑ​ (index δ\deltaδ in xxx, ϑ\varthetaϑ in yyy, polynomial growth in xxx), its bounded version Cbδ,ϑC^{\delta,\vartheta}_bCbδ,ϑ​, the time-dependent Cpϑ/2,δ,ϑC^{\vartheta/2,\delta,\vartheta}_pCpϑ/2,δ,ϑ​, the class Lp∞L^\infty_pLp∞​ of measurable functions of polynomial growth, and Cb2+ϑ(Rd2)C^{2+\vartheta}_b(\mathbb R^{d_2})Cb2+ϑ​(Rd2​) for test functions.

Formalization targets

Goal: Theorem 2.3(i)

In Regime 1, αε/γε→0\alpha_\varepsilon/\gamma_\varepsilon\to0αε​/γε​→0 and αε2/(βεγε)→0\alpha_\varepsilon^2/(\beta_\varepsilon\gamma_\varepsilon)\to0αε2​/(βε​γε​)→0, assume b,σ∈Cbδ,ϑb,\sigma\in C^{\delta,\vartheta}_bb,σ∈Cbδ,ϑ​, F,H,G∈Cpϑ/2,δ,ϑF,H,G\in C^{\vartheta/2,\delta,\vartheta}_pF,H,G∈Cpϑ/2,δ,ϑ​ with ϑ∈(0,2]\vartheta\in(0,2]ϑ∈(0,2], c∈Lp∞c\in L^\infty_pc∈Lp∞​ and αεϑ/γε→0\alpha_\varepsilon^\vartheta/\gamma_\varepsilon\to0αεϑ​/γε​→0. Then for every T>0T>0T>0 and φ∈Cb2+ϑ\varphi\in C^{2+\vartheta}_bφ∈Cb2+ϑ​,

sup⁡t∈[0,T]∣Eφ(Ytε)−Eφ(Y^t1)∣≤CT(αεϑγε+αε2γε2+αε2βεγε).\sup_{t\in[0,T]}\big|\mathbb E\varphi(Y^\varepsilon_t)-\mathbb E\varphi(\hat Y^1_t)\big|\le C_T\Big(\frac{\alpha_\varepsilon^\vartheta}{\gamma_\varepsilon}+\frac{\alpha_\varepsilon^2}{\gamma_\varepsilon^2}+\frac{\alpha_\varepsilon^2}{\beta_\varepsilon\gamma_\varepsilon}\Big).t∈[0,T]sup​​Eφ(Ytε​)−Eφ(Y^t1​)​≤CT​(γε​αεϑ​​+γε2​αε2​​+βε​γε​αε2​​).

Milestones

  1. Lemma 4.1: mollification in (t,y)(t,y)(t,y) at scales n−2n^{-2}n−2 and n−1n^{-1}n−1 costs n−ϑn^{-\vartheta}n−ϑ and gains n2−ϑn^{2-\vartheta}n2−ϑ on ∂t\partial_t∂t​ and ∇y2\nabla_y^2∇y2​.
  2. Lemma 4.2: for centered fff, E∫0tf(s,Xsε,Ysε)ds≤Ct(αεϑ+αεϑ∧1αε/γε+αε2/βε)\mathbb E\int_0^tf(s,X^\varepsilon_s,Y^\varepsilon_s)ds\le C_t(\alpha_\varepsilon^\vartheta+\alpha_\varepsilon^{\vartheta\wedge1}\alpha_\varepsilon/\gamma_\varepsilon+\alpha_\varepsilon^2/\beta_\varepsilon)E∫0t​f(s,Xsε​,Ysε​)ds≤Ct​(αεϑ​+αεϑ∧1​αε​/γε​+αε2​/βε​).
  3. Lemma 4.4(i): in Regime 1, E γε−1∫0tf ds≤Ct(αεϑ/γε+αε2/γε2+αε2/(βεγε))\mathbb E\,\gamma_\varepsilon^{-1}\int_0^tf\,ds\le C_t(\alpha_\varepsilon^\vartheta/\gamma_\varepsilon+\alpha_\varepsilon^2/\gamma_\varepsilon^2+\alpha_\varepsilon^2/(\beta_\varepsilon\gamma_\varepsilon))Eγε−1​∫0t​fds≤Ct​(αεϑ​/γε​+αε2​/γε2​+αε2​/(βε​γε​)).
  4. Lemma 5.1 (k=1k=1k=1): G^1=G^1G^1∗/2\hat{\mathcal G}_1=\hat G_1\hat G_1^*/2G^​1​=G^1​G^1∗​/2 is uniformly nondegenerate and F^1,G^1∈Cbϑ/2,ϑ\hat F_1,\hat{\mathcal G}_1\in C^{\vartheta/2,\vartheta}_bF^1​,G^​1​∈Cbϑ/2,ϑ​.

Significance

The result. The theorem gives a rate for the weak error of the averaging principle under Hölder regularity only, and the rate depends only on the regularity in the slow variable yyy, not on δ\deltaδ. It covers the fully coupled case, in which the slow equation contains the singular drift γε−1H\gamma_\varepsilon^{-1}Hγε−1​H, and it identifies the extra condition αεϑ/γε→0\alpha_\varepsilon^\vartheta/\gamma_\varepsilon\to0αεϑ​/γε​→0 under which this drift averages out. For c=H≡0c=H\equiv0c=H≡0 it reduces to the rate αεϑ\alpha_\varepsilon^\varthetaαεϑ​ (Remark 2.5), optimal for ϑ=2\vartheta=2ϑ=2. Error bounds of this kind are what heterogeneous multiscale methods need to be quantitative.

Formalizing it. The result is proved in the paper; nothing in it is machine-checked. A formalization needs an Itô calculus for weak solutions, the elliptic Poisson equation in xxx with parameter yyy (the companion mission's Theorem 2.1), and the parabolic Kolmogorov equation of the averaged SDE. The two fluctuation lemmas are stated for general centered functions and are reusable for other limit theorems.

Difficulty

The obvious argument writes Eφ(YTε)−Eφ(Y^T1)\mathbb E\varphi(Y^\varepsilon_T)-\mathbb E\varphi(\hat Y^1_T)Eφ(YTε​)−Eφ(Y^T1​) through the Kolmogorov equation of the averaged SDE and Itô's formula, which leaves E∫0T(L1−L^1)u~ ds\mathbb E\int_0^T(\mathscr L_1-\hat{\mathscr L}_1)\tilde u\,dsE∫0T​(L1​−L^1​)u~ds and γε−1E∫0TH⋅∇yu~ ds\gamma_\varepsilon^{-1}\mathbb E\int_0^TH\cdot\nabla_y\tilde u\,dsγε−1​E∫0T​H⋅∇y​u~ds. Both integrands are centered but only Hölder continuous in (t,y)(t,y)(t,y), so the standard corrector argument, which applies Itô's formula to the solution of the Poisson equation along (Xε,Yε)(X^\varepsilon,Y^\varepsilon)(Xε,Yε), needs derivatives in ttt and yyy that do not exist. The term with γε−1\gamma_\varepsilon^{-1}γε−1​ is a central-limit-scale fluctuation, which is why its control needs the regime conditions. Existence and regularity of the averaged coefficients also have to come from the Poisson equation, since μy\mu^yμy is not explicit.

Formalization scope

Spaces are EuclideanSpace ℝ (Fin d). Coefficients are b,c:Rd1×Rd2→Rd1b,c:\mathbb R^{d_1}\times\mathbb R^{d_2}\to\mathbb R^{d_1}b,c:Rd1​×Rd2​→Rd1​, σ\sigmaσ a d1×d1d_1\times d_1d1​×d1​ matrix, F,H:R+×Rd1×Rd2→Rd2F,H:\mathbb R_+\times\mathbb R^{d_1}\times\mathbb R^{d_2}\to\mathbb R^{d_2}F,H:R+​×Rd1​×Rd2​→Rd2​, GGG a d2×d2d_2\times d_2d2​×d2​ matrix. The Itô layer (Brownian motion, Itô integral, Itô processes, SDE solutions) is the published Peng1990.SMP.Stochastic. A solution of (1.4) is a weak solution: any filtered probability space, any Brownian motion for that filtration, any progressive process satisfying the integral equation. The theorem compares every weak solution of (1.4) with every weak solution of (2.9). The paper does not prove existence for (1.4), so the statement is conditional on solutions, as it is used in the paper. A sanity file shows the parameter hypotheses are consistent (αε=ε\alpha_\varepsilon=\varepsilonαε​=ε, βε=γε=ε1/2\beta_\varepsilon=\gamma_\varepsilon=\varepsilon^{1/2}βε​=γε​=ε1/2) and that (2.7) holds for a bounded dissipative drift.

Committed conventions and readings of the page:

  • μy\mu^yμy is any family of probability measures that are infinitesimally invariant for L0\mathscr L_0L0​ with a=σσ∗/2a=\sigma\sigma^*/2a=σσ∗/2, the generator of (1.7). Under the standing assumptions this is the unique invariant measure.
  • (2.7) is read with κ=αε2/βε\kappa=\alpha_\varepsilon^2/\beta_\varepsilonκ=αε2​/βε​, the factor that actually multiplies ccc in the fast drift, for all small κ>0\kappa>0κ>0.
  • G^1\hat G_1G^1​ is any measurable matrix field with G^1G^1∗=∫GG∗ dμy\hat G_1\hat G_1^*=\int GG^*\,d\mu^yG^1​G^1∗​=∫GG∗dμy, which covers the printed square root.
  • The Hölder classes include polynomial growth, constrain all lower yyy-derivatives, and take their constants uniformly in time, including in the time-Hölder clause.
  • The constants CTC_TCT​, CtC_tCt​, C0C_0C0​ exist after all data are fixed (coefficients, μ\muμ, TTT, φ\varphiφ, xxx, yyy, the parameter functions) and before ε\varepsilonε or nnn.
  • Lemma 4.1 takes fff on all of R\mathbb RR in time, since (4.1) evaluates fff at negative times, and assumes the kernels have the finite moments ∫∣r∣ϑ/2ρ1<∞\int|r|^{\vartheta/2}\rho_1<\infty∫∣r∣ϑ/2ρ1​<∞, ∫∣z∣ϑρ2<∞\int|z|^\vartheta\rho_2<\infty∫∣z∣ϑρ2​<∞ that its proof uses; without them (4.2) fails for a Cauchy-type kernel.
  • Solutions are Itô processes in the sense of the referenced layer: progressive, with sup⁡t≤TE∣Zt∣2<∞\sup_{t\le T}\mathbb E|Z_t|^2<\inftysupt≤T​E∣Zt​∣2<∞ and square-integrable diffusion integrands.
  • Lemma 4.4(i) carries the Regime 1 limits of its label.
  • Lemmas 4.2 and 4.4(i) are one-sided, as printed, and include integrability of the path integral in their conclusion.

A formalization in which the expectations are junk Bochner integrals, the constant depends on ε\varepsilonε, or a single strong solution is fixed would be a different and weaker statement; the posed statements rule these out.

Not posed: Regimes 2–4 of Theorem 2.3 and Lemma 4.4(ii)–(iv). The printed G^3=G^4\hat G_3=\hat G_4G^3​=G^4​ differs by a factor 222 in the HΦ∗H\Phi^*HΦ∗ term from the generator used in the proof, so a faithful statement needs a correction that is left to moderation. Regime 2 needs the Poisson solution Φ\PhiΦ in the averaged drift. Lemma 5.2 is also not posed: as printed, uk(t,y)=Eφ(Y^tk(y))u_k(t,y)=\mathbb E\varphi(\hat Y^k_t(y))uk​(t,y)=Eφ(Y^tk​(y)) solves (5.1) only for time-independent coefficients, and its class Cb(2+ϑ)/2,2+ϑC^{(2+\vartheta)/2,2+\vartheta}_bCb(2+ϑ)/2,2+ϑ​ has time index above 111, which the paper's notations do not define. Contributions toward Itô's formula for these processes, the Poisson equation (companion mission 1) and parabolic Schauder theory are welcome.

Selected references

  • M. Röckner, L. Xie, Diffusion approximation for fully coupled stochastic differential equations, Ann. Probab. 49(3) (2021) 1205–1236. https://doi.org/10.1214/20-AOP1475
  • G. Papanicolaou, D. Stroock, S. R. S. Varadhan, Martingale approach to some limit theorems, Duke Turbulence Conference, Duke Univ. Math. Ser. III (1977).
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. I, Ann. Probab. 29 (2001) 1061–1085. https://doi.org/10.1214/aop/1015345596
  • E. Pardoux, A. Yu. Veretennikov, On Poisson equation and diffusion approximation. II, Ann. Probab. 31 (2003) 1166–1192. https://doi.org/10.1214/aop/1055425774
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. III, Ann. Probab. 33 (2005) 1111–1133. https://doi.org/10.1214/009117905000000062
  • D. Givon, Strong convergence rate for two-time-scale jump-diffusion stochastic differential systems, Multiscale Model. Simul. 6 (2007) 577–594. https://doi.org/10.1137/060673345
  • D. Liu, Strong convergence of principle of averaging for multiscale stochastic dynamical systems, Commun. Math. Sci. 8 (2010) 999–1020.
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28 (1990) 966–979 (source of the Itô layer). https://doi.org/10.1137/0328054
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AnalysisPartial Differential EquationsProbability·Captain: mikedeng1

Diffusion Approximation for Fully Coupled Stochastic Differential Equations 1: The Parametric Poisson Equation Has a Unique Centered Solution with Optimal Regularity in x and yResearch Paper

Motivation

Poisson equations for the generator of an ergodic diffusion are a standard tool in stochastic averaging, homogenization and diffusion approximation: to show that a fast ergodic component averages out in a slow equation, one writes the fluctuation f(Xt,Yt)f(X_t,Y_t)f(Xt​,Yt​) as L0u\mathscr L_0 uL0​u and applies Itô's formula to uuu. This requires a solution uuu whose regularity is controlled in two variables at once: the fast variable xxx, in which the operator is elliptic, and the slow variable yyy, which enters as a parameter.

  • Pardoux and Veretennikov (Ann. Probab. 2001, 2003, 2005) studied this equation in the whole space Rd1\mathbb R^{d_1}Rd1​ and used it for diffusion approximation of slow–fast SDEs. In parts I and III the operator does not depend on the parameter, and the solution's regularity in xxx is of Sobolev type; regularity in yyy was obtained by differentiating the associated semigroup in the parameter (Röckner–Xie, Remark 2.2(iii) and p. 1213).
  • Röckner and Xie (2021) prove optimal Hölder regularity in xxx and show that regularity in yyy follows from it, for fully coupled coefficients that depend on both variables and are only Hölder continuous. This mission formalizes that result (their Theorem 2.1) and the steps of its proof.

Setting

Fix d1,d2≥1d_1,d_2\ge1d1​,d2​≥1, a matrix field a(x,y)=(aij(x,y))a(x,y)=(a^{ij}(x,y))a(x,y)=(aij(x,y)) and a vector field b(x,y)∈Rd1b(x,y)\in\mathbb R^{d_1}b(x,y)∈Rd1​ on Rd1×Rd2\mathbb R^{d_1}\times\mathbb R^{d_2}Rd1​×Rd2​. The frozen operator acts on functions of xxx with yyy held fixed:

L0(x,y)=∑i,j=1d1aij(x,y)∂2∂xi∂xj+∑i=1d1bi(x,y)∂∂xi.\mathscr L_0(x,y)=\sum_{i,j=1}^{d_1}a^{ij}(x,y)\frac{\partial^2}{\partial x_i\partial x_j}+\sum_{i=1}^{d_1}b^i(x,y)\frac{\partial}{\partial x_i}.L0​(x,y)=i,j=1∑d1​​aij(x,y)∂xi​∂xj​∂2​+i=1∑d1​​bi(x,y)∂xi​∂​.

The Poisson equation (1.1) is L0(x,y)u(x,y)=f(x,y)\mathscr L_0(x,y)u(x,y)=f(x,y)L0​(x,y)u(x,y)=f(x,y) for all x∈Rd1x\in\mathbb R^{d_1}x∈Rd1​, for each parameter y∈Rd2y\in\mathbb R^{d_2}y∈Rd2​.

The standing assumptions are:

  • (Aσ): a=σσ∗a=\sigma\sigma^*a=σσ∗ is uniformly nondegenerate, i.e. λ−1∣ξ∣2≤∣a(x,y)ξ∣2≤λ∣ξ∣2\lambda^{-1}|\xi|^2\le|a(x,y)\xi|^2\le\lambda|\xi|^2λ−1∣ξ∣2≤∣a(x,y)ξ∣2≤λ∣ξ∣2 for some λ>1\lambda>1λ>1;
  • (Ab): lim⁡∣x∣→∞sup⁡y⟨x,b(x,y)⟩=−∞\lim_{|x|\to\infty}\sup_y\langle x,b(x,y)\rangle=-\inftylim∣x∣→∞​supy​⟨x,b(x,y)⟩=−∞, a weak recurrence condition.

Under these, for each yyy the frozen diffusion dXt=b(Xt,y) dt+σ(Xt,y) dWtdX_t=b(X_t,y)\,dt+\sigma(X_t,y)\,dW_tdXt​=b(Xt​,y)dt+σ(Xt​,y)dWt​ has a unique invariant measure μy\mu^yμy. Since constants solve L0u=0\mathscr L_0u=0L0​u=0, the equation is only solvable for centered right-hand sides, ∫f(x,y) μy(dx)=0\int f(x,y)\,\mu^y(dx)=0∫f(x,y)μy(dx)=0 for every yyy (1.3), and the solution is fixed by requiring it to be centered as well.

Regularity is measured in weighted Hölder classes. f∈Cpδ,0f\in C^{\delta,0}_pf∈Cpδ,0​ (0<δ≤10<\delta\le10<δ≤1) means ∣f(x,y)∣≤C(1+∣x∣m)|f(x,y)|\le C(1+|x|^m)∣f(x,y)∣≤C(1+∣x∣m) and ∣f(x1,y)−f(x2,y)∣≤C(∣x1−x2∣δ∧1)(1+∣x1∣m+∣x2∣m)|f(x_1,y)-f(x_2,y)|\le C(|x_1-x_2|^\delta\wedge1)(1+|x_1|^m+|x_2|^m)∣f(x1​,y)−f(x2​,y)∣≤C(∣x1​−x2​∣δ∧1)(1+∣x1​∣m+∣x2​∣m), uniformly in yyy. Cpδ,ηC^{\delta,\eta}_pCpδ,η​ adds η\etaη derivatives in yyy, with a (η−[η])(\eta-[\eta])(η−[η])-Hölder top derivative. The subscript bbb denotes the bounded version, and Cp2+δ,ηC^{2+\delta,\eta}_pCp2+δ,η​ asks the same of ∇x2u\nabla^2_xu∇x2​u together with growth bounds on uuu and ∇xu\nabla_xu∇x​u.

Formalization targets

Goal: Theorem 2.1

If (Aσ), (Ab) hold and a,b∈Cbδ,ηa,b\in C^{\delta,\eta}_ba,b∈Cbδ,η​ with 0<δ≤10<\delta\le10<δ≤1, η≥0\eta\ge0η≥0, then for every centered f∈Cpδ,ηf\in C^{\delta,\eta}_pf∈Cpδ,η​ there is a unique centered u∈Cp2+δ,ηu\in C^{2+\delta,\eta}_pu∈Cp2+δ,η​ with L0u=f\mathscr L_0u=fL0​u=f. For some C0,m>0C_0,m>0C0​,m>0,

∣u∣+∣∇xu∣+∣∇x2u∣≤C0(1+∣x∣m),∣∇x2u(x1,y)−∇x2u(x2,y)∣≤C0(∣x1−x2∣δ∧1)(1+∣x1∣m+∣x2∣m),|u|+|\nabla_xu|+|\nabla^2_xu|\le C_0(1+|x|^m),\qquad|\nabla^2_xu(x_1,y)-\nabla^2_xu(x_2,y)|\le C_0(|x_1-x_2|^\delta\wedge1)(1+|x_1|^m+|x_2|^m),∣u∣+∣∇x​u∣+∣∇x2​u∣≤C0​(1+∣x∣m),∣∇x2​u(x1​,y)−∇x2​u(x2​,y)∣≤C0​(∣x1​−x2​∣δ∧1)(1+∣x1​∣m+∣x2​∣m),

and, for η>0\eta>0η>0, ∥u(x,⋅)∥Cbη≤C0(1+∣x∣m)\|u(x,\cdot)\|_{C^\eta_b}\le C_0(1+|x|^m)∥u(x,⋅)∥Cbη​​≤C0​(1+∣x∣m).

Milestones, in the order of the proof

  1. The transfer formula for η=1\eta=1η=1 (Remark 3.3(ii), Lemma 3.2(i)): if u∈Cp2+δ,0u\in C^{2+\delta,0}_pu∈Cp2+δ,0​ solves L0u=h−hˉ\mathscr L_0u=h-\bar hL0​u=h−hˉ, then
∂y∫h(x,y) μy(dx)=∫[∂yh−∂L0∂yu](x,y) μy(dx).\partial_y\int h(x,y)\,\mu^y(dx)=\int\Big[\partial_yh-\frac{\partial\mathscr L_0}{\partial y}u\Big](x,y)\,\mu^y(dx).∂y​∫h(x,y)μy(dx)=∫[∂y​h−∂y∂L0​​u](x,y)μy(dx).
  1. The increment formula (3.10) for η∈(0,1)\eta\in(0,1)η∈(0,1) (Lemma 3.2(ii)), with hˉ∈Cbη\bar h\in C^\eta_bhˉ∈Cbη​.
  2. Theorem 2.1 for η=0\eta=0η=0: existence, uniqueness and the xxx-estimates (2.1)–(2.2).
  3. Step 3: the right-hand side ∂yf−∂yL0 u\partial_yf-\partial_y\mathscr L_0\,u∂y​f−∂y​L0​u of the differentiated equation is centered.
  4. Step 3: for η=1\eta=1η=1 the solution satisfies ∂yu∈Cp2+δ,0\partial_yu\in C^{2+\delta,0}_p∂y​u∈Cp2+δ,0​ and ∣∂yu∣≤C(1+∣x∣m)|\partial_yu|\le C(1+|x|^m)∣∂y​u∣≤C(1+∣x∣m).
  5. Step 4: for η∈(0,1)\eta\in(0,1)η∈(0,1), ∣u(x,y1)−u(x,y2)∣≤C(∣y1−y2∣η∧1)(1+∣x∣m)|u(x,y_1)-u(x,y_2)|\le C(|y_1-y_2|^\eta\wedge1)(1+|x|^m)∣u(x,y1​)−u(x,y2​)∣≤C(∣y1​−y2​∣η∧1)(1+∣x∣m).

Significance

The theorem supplies the corrector used in Theorem 2.3 of the same paper, the weak convergence rate of the slow component of a fully coupled multiscale SDE to its averaged limit. Its form, regularity in yyy matching that of the data and no derivative of μy\mu^yμy in yyy, is what lets the rates depend only on the regularity of the coefficients in the slow variable. The transfer formulas (3.9)–(3.10) also show that averaged coefficients hˉ(y)=∫h dμy\bar h(y)=\int h\,d\mu^yhˉ(y)=∫hdμy inherit the yyy-regularity of hhh, a question that comes up in every averaging or homogenization limit.

The result is proved in the paper. None of it is formalized: Lean and Mathlib have no fundamental solutions of non-divergence elliptic operators, no Schauder theory and no invariant measures of diffusions. The mission poses the statements, so that the proof can be built in layers and the parts that do not depend on the Gaussian kernel bounds (the transfer formulas given a solution, the induction in Steps 3–4) can be proved separately.

Difficulty

Existence and the estimates (2.1)–(2.2) rest on the probabilistic representation u=∫0∞Ttf dtu=\int_0^\infty T_tf\,dtu=∫0∞​Tt​fdt and on Gaussian bounds and ergodic decay for the fundamental solution pt(x,x′;y)p_t(x,x';y)pt​(x,x′;y) of L0(⋅,y)\mathscr L_0(\cdot,y)L0​(⋅,y) (Lemma 3.1, cited from Ladyzhenskaya–Solonnikov–Ural'tseva and Pardoux–Veretennikov II, Proposition 3). The coefficients are only Hölder in xxx, so the Hessian bound needs the cancellation ∫∇x2pt dx′\int\nabla^2_xp_t\,dx'∫∇x2​pt​dx′ (3.3), not just a size estimate on ∇x2pt\nabla^2_xp_t∇x2​pt​. The obvious approach to yyy-regularity, differentiating TtfT_tfTt​f or μy\mu^yμy in yyy, needs derivatives of the invariant density in the parameter, which are hard to control. The paper's route, differentiating the equation and using the transfer formula to recenter, only works if the differentiated right-hand side is again centered. That centering is the content of Lemma 3.2.

Formalization scope

  • Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d); ∇x\nabla_x∇x​, ∇x2\nabla^2_x∇x2​ are fderiv and iteratedFDeriv ℝ 2 in xxx, ∂yj\partial^j_y∂yj​ is iteratedFDeriv ℝ j in yyy, with operator norms. yyy-derivatives in the milestones are directional.
  • (Aσ) includes symmetric positive semidefiniteness of aaa (the content of a=σσ∗a=\sigma\sigma^*a=σσ∗). (Ab) is the ∀M ∃R\forall M\,\exists R∀M∃R form.
  • μy\mu^yμy is a hypothesis: a family of probability measures, each infinitesimally invariant for L0(⋅,y)\mathscr L_0(\cdot,y)L0​(⋅,y) (∫L0g dμy=0\int\mathscr L_0g\,d\mu^y=0∫L0​gdμy=0 for smooth compactly supported ggg). Under the assumptions this is the unique invariant measure of the frozen SDE (1.7); the SDE itself is not formalized. No moment bounds on μy\mu^yμy are assumed, since they are consequences.
  • Centering includes μy\mu^yμy-integrability, and every integral formula in a conclusion asserts integrability of its integrand, so no statement can hold through a junk zero integral.
  • The classes include the polynomial growth bound and all lower yyy-derivatives; matrix coefficients are in Cbδ,ηC^{\delta,\eta}_bCbδ,η​ entrywise; η≥0\eta\ge0η≥0 is real, split as [η]+[\eta]+[η]+ fractional part; a yyy-derivative is read as continuous (CkC^kCk in yyy). The CbηC^\eta_bCbη​ norm is in max form.
  • Not posed: the clause that C0,mC_0,mC0​,m depend "only on d1,d2d_1,d_2d1​,d2​, ∥a∥Cbδ,0\|a\|_{C^{\delta,0}_b}∥a∥Cbδ,0​​, ∥b∥Cbδ,0\|b\|_{C^{\delta,0}_b}∥b∥Cbδ,0​​, [f]Cpδ,0[f]_{C^{\delta,0}_p}[f]Cpδ,0​​", which is false as printed ([f]Cpδ,0[f]_{C^{\delta,0}_p}[f]Cpδ,0​​ is a supremum over the unit ball, and λ\lambdaλ and the rate in (Ab) are missing), and the recursive constant Kη\mathcal K_\etaKη​ of (2.4)–(2.5). The constants exist for each fixed (a,b,f)(a,b,f)(a,b,f). (2.1)–(2.2), printed under "Case η = 0", are asserted for every η\etaη.
  • Uniqueness is stated for the whole class Cp2+δ,ηC^{2+\delta,\eta}_pCp2+δ,η​, not only among solutions that satisfy the estimates. Without the invariance of μy\mu^yμy for the same a,ba,ba,b, or without centering, the statement would be false; both are part of the hypotheses.
  • Useful contributions beyond this mission: Hölder spaces with polynomial weights, fundamental solutions of non-divergence-form operators, invariant measures of elliptic diffusions, and the identification of infinitesimally invariant measures with invariant measures of the diffusion.

Selected references

  • M. Röckner, L. Xie, Diffusion approximation for fully coupled stochastic differential equations, Ann. Probab. 49(3), 1205–1236, 2021. https://doi.org/10.1214/20-AOP1475
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. I, Ann. Probab. 29(3), 1061–1085, 2001. https://doi.org/10.1214/aop/1015345596
  • E. Pardoux, A. Yu. Veretennikov, On Poisson equation and diffusion approximation. II, Ann. Probab. 31(3), 1166–1192, 2003. https://doi.org/10.1214/aop/1055425774
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation 3, Ann. Probab. 33(3), 1111–1133, 2005. https://doi.org/10.1214/009117905000000062
  • O. A. Ladyzhenskaya, V. A. Solonnikov, N. N. Ural'tseva, Linear and Quasi-linear Equations of Parabolic Type, AMS Translations of Mathematical Monographs 23, 1968. https://mathscinet.ams.org/mathscinet-getitem?mr=0241822
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Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games 2: The Mean-Field Equilibrium Policy Is an ε-Markov-Nash Equilibrium of Every Large Enough N-Agent GameResearch Paper

Motivation

Games with many interacting agents, such as traffic participants, users of a shared communication channel or firms in a market, are rarely solvable exactly: a Nash equilibrium of an NNN-player stochastic game requires each agent to track the whole population, and its computation grows with NNN. Mean-field game theory replaces the population by its limiting distribution. A single representative agent faces a deterministic flow of state distributions, and consistency requires that this flow is the one the agent's own optimal policy generates. The equilibrium of this limit problem is then used as an approximate equilibrium of the finite game, with each agent acting only on its own state.

Most of this theory concerns risk-neutral agents, who minimize an expected cost. Saldi, Başar and Raginsky (arXiv:1808.03929; Math. Oper. Res. 2020) treat discrete-time agents with an exponential utility of the discounted cost, the classical risk-sensitive criterion that penalizes the variance of the cost as well as its mean. The paper proves two results: a mean-field equilibrium exists (Theorem 1, the first mission of this series), and the equilibrium policy is an approximate Nash equilibrium of every large enough finite game (Theorem 3, this mission). The risk-neutral counterpart is Saldi, Başar and Raginsky, SIAM J. Control Optim. 2018 (arXiv:1612.07878).

Setting

States lie in a Polish metric space X\mathsf XX, actions in a compact Polish space A\mathsf AA, and P(X)\mathcal P(\mathsf X)P(X) is the set of Borel probability measures with the weak topology. The model consists of a transition kernel p(⋅∣x,a,μ)p(\cdot\mid x,a,\mu)p(⋅∣x,a,μ), a one-stage cost c(x,a,μ)≥0c(x,a,\mu)\ge0c(x,a,μ)≥0, an initial law μ0\mu_0μ0​, a discount factor β∈(0,1)\beta\in(0,1)β∈(0,1) and a risk factor λ>0\lambda>0λ>0.

In the NNN-agent game, the states xiN(0)x^N_i(0)xiN​(0) are i.i.d. μ0\mu_0μ0​. At each time ttt, agent iii draws aiN(t)∼πti(⋅∣xiN(t))a^N_i(t)\sim\pi^i_t(\cdot\mid x^N_i(t))aiN​(t)∼πti​(⋅∣xiN​(t)) from its Markov policy πi\pi^iπi, and the next states are drawn independently from p(⋅∣xiN(t),aiN(t),et(N))p(\cdot\mid x^N_i(t),a^N_i(t),e^{(N)}_t)p(⋅∣xiN​(t),aiN​(t),et(N)​), where et(N)=1N∑jδxjN(t)e^{(N)}_t=\frac1N\sum_{j}\delta_{x^N_j(t)}et(N)​=N1​∑j​δxjN​(t)​ is the empirical distribution of the states. Agent iii's cost is

Ji(N)(π(N))=Eπ(N)[eλ∑t=0∞βtc(xiN(t),aiN(t),et(N))].J^{(N)}_i(\boldsymbol\pi^{(N)})=E^{\boldsymbol\pi^{(N)}}\Big[e^{\lambda\sum_{t=0}^\infty\beta^tc(x^N_i(t),a^N_i(t),e^{(N)}_t)}\Big].Ji(N)​(π(N))=Eπ(N)[eλ∑t=0∞​βtc(xiN​(t),aiN​(t),et(N)​)].

A profile is an ε\varepsilonε-Markov-Nash equilibrium if no agent can lower its Ji(N)J^{(N)}_iJi(N)​ by more than ε\varepsilonε by switching to another Markov policy.

In the mean-field game, one agent faces a flow μ=(μt)\boldsymbol\mu=(\mu_t)μ=(μt​): x(t+1)∼p(⋅∣x(t),a(t),μt)x(t+1)\sim p(\cdot\mid x(t),a(t),\mu_t)x(t+1)∼p(⋅∣x(t),a(t),μt​), with cost Jμ(π)=Eπ[eλ∑tβtc(x(t),a(t),μt)]J_{\boldsymbol\mu}(\pi)=E^\pi[e^{\lambda\sum_t\beta^tc(x(t),a(t),\mu_t)}]Jμ​(π)=Eπ[eλ∑t​βtc(x(t),a(t),μt​)]. A mean-field equilibrium is a pair (π,μ)(\pi,\boldsymbol\mu)(π,μ) in which π\piπ minimizes JμJ_{\boldsymbol\mu}Jμ​ and μ=Λ(π)\boldsymbol\mu=\Lambda(\pi)μ=Λ(π) is the flow of state laws that π\piπ generates.

The hypotheses are Assumption 1 (bounded continuous ccc with ∣c∣≤K|c|\le K∣c∣≤K, weakly continuous ppp, compact A\mathsf AA, and a moment function www with ∫w dp≤αw\int w\,dp\le\alpha w∫wdp≤αw and ∫w dμ0<∞\int w\,d\mu_0<\infty∫wdμ0​<∞) and Assumption 2. Part (a) of Assumption 2 asks that the moduli

ωp(r)=sup⁡x,asup⁡dBL(μ,ν)≤r∥p(⋅∣x,a,μ)−p(⋅∣x,a,ν)∥TV,ωc(r)=sup⁡x,asup⁡dBL(μ,ν)≤r∣c(x,a,μ)−c(x,a,ν)∣\omega_p(r)=\sup_{x,a}\sup_{d_{BL}(\mu,\nu)\le r}\|p(\cdot\mid x,a,\mu)-p(\cdot\mid x,a,\nu)\|_{TV},\qquad\omega_c(r)=\sup_{x,a}\sup_{d_{BL}(\mu,\nu)\le r}|c(x,a,\mu)-c(x,a,\nu)|ωp​(r)=x,asup​dBL​(μ,ν)≤rsup​∥p(⋅∣x,a,μ)−p(⋅∣x,a,ν)∥TV​,ωc​(r)=x,asup​dBL​(μ,ν)≤rsup​∣c(x,a,μ)−c(x,a,ν)∣

tend to 000, where dBLd_{BL}dBL​ is the bounded-Lipschitz metric. Part (b) asks that the equilibrium policy π\piπ be weakly continuous in the state.

Formalization targets

Goal: Theorem 3 (p. 23)

For every ε>0\varepsilon>0ε>0 there is N(ε)N(\varepsilon)N(ε) such that, for every N≥N(ε)N\ge N(\varepsilon)N≥N(ε), the profile (π,…,π)(\pi,\dots,\pi)(π,…,π) is an ε\varepsilonε-Markov-Nash equilibrium:

Ji(N)(π,…,π)≤inf⁡σ∈MJi(N)(π,…,σ,…,π)+εfor all i.J^{(N)}_i(\pi,\dots,\pi)\le\inf_{\sigma\in\mathsf M}J^{(N)}_i(\pi,\dots,\sigma,\dots,\pi)+\varepsilon\qquad\text{for all }i .Ji(N)​(π,…,π)≤σ∈Minf​Ji(N)​(π,…,σ,…,π)+εfor all i.

The statement fixes no rate. It is the paper's main approximation result.

Milestones

The milestones follow the paper's proof. The first seven work in an augmented model, whose state s=(x,c)s=(x,c)s=(x,c) carries the accumulated discounted cost, so that the exponential criterion becomes a terminal cost eλc(n+1)e^{\lambda c(n+1)}eλc(n+1). They are: Proposition 6 (the augmented model has the same finite-horizon costs); Lemma 5 (the augmented flow Δt+1=ΔtPt,Δtπ\Delta_{t+1}=\Delta_tP^\pi_{t,\Delta_t}Δt+1​=Δt​Pt,Δt​π​); Proposition 7 (propagation of chaos, L(Δt(N))→δΔt\mathcal L(\Delta^{(N)}_t)\to\delta_{\Delta_t}L(Δt(N)​)→δΔt​​); Proposition 8 (convergence of the augmented cost); Proposition 9 (propagation of chaos with one deviating agent); Proposition 10 (the deviating agent's state law); Proposition 11 (the deviating agent's augmented cost). The last three are stated in the original model: Theorem 4 (the finite-horizon limits (14)–(15)), Corollary 1 (the infinite-horizon comparison), and the first display of the proof of Theorem 3 (deviations may be restricted to weakly continuous policies).

Significance

Theorem 3 justifies the use of a mean-field equilibrium as a decentralized policy in risk-sensitive games with many players. The equilibrium is computed once, from a single-agent problem, and each agent uses only its own state, yet no agent of a large enough population gains more than ε\varepsilonε by deviating. The result extends the risk-neutral approximation theorem to the multiplicative criterion. Because the exponential cost does not decompose over time, the risk-neutral argument cannot be applied directly: the proof first passes through the augmented model and a finite-horizon truncation.

The result is proved in the paper; none of it is formalized. The mission formalizes the statement and the proof's intermediate results. That requires the NNN-agent law, a product of NNN kernels driven by the empirical measure, built from Mathlib's Ionescu-Tulcea construction, and propagation of chaos for an interacting Markov chain on a Polish space. Alternative proofs of any milestone are welcome, as are quantitative versions of the limits.

Difficulty

The cost is the expectation of a product of one-stage factors, not a sum, so the convergence of the empirical measure gives no direct control of it. The paper therefore enlarges the state with the accumulated cost, and the finite-horizon limits must then be transferred back to the infinite horizon through a uniform tail bound. The coupling between agents runs through the empirical measure, which enters both the transition and the cost. Propagation of chaos (Proposition 7) is an induction over time that needs continuity of ppp and ccc in the measure argument uniformly in (x,a)(x,a)(x,a) (Assumption 2-(a)) and a conditional variance bound. The deviating agent is not exchangeable with the others: its state law must be compared with that of a mean-field chain under its own policy (Proposition 10), uniformly over arbitrary sequences of deviations. Finally, a best response may be only measurable. The reduction to weakly continuous deviations, which the paper takes from its risk-neutral predecessor, is needed before any weak-convergence argument applies.

Formalization scope

Lean namespace RiskSensMFG.Nash. The definitions are in four files: the model, policies, the single-agent law and the flow (Model); the mean-field equilibrium, dBLd_{BL}dBL​, total variation and Assumption 2-(a) (Equilibrium); the NNN-agent game (Game); and the augmented model (Augmented). Conventions:

  • X\mathsf XX is a complete separable metric space with its Borel σ\sigmaσ-field, and A\mathsf AA is a compact Polish space. P(X)\mathcal P(\mathsf X)P(X) is Mathlib's ProbabilityMeasure with the weak topology and its Borel σ\sigmaσ-field (not the Giry one), and ppp is a Markov Kernel. The standing assumptions β∈(0,1)\beta\in(0,1)β∈(0,1), λ>0\lambda>0λ>0 and c≥0c\ge0c≥0 measurable are a predicate Model.Standing. Assumption 1 is stated in full, including the moment function, although the proof of Theorem 3 does not use parts (d)–(e).
  • Time is 0-based. Agents are indexed by Fin N, and the paper's Agent 1 is index 0; limits in NNN are taken along N+1N+1N+1 so that Agent 1 exists. The empirical measure of the empty configuration is set to μ0\mu_0μ0​ and enters no statement.
  • The equilibrium's optimality is required against Markov policies only, which is a weaker hypothesis than Definition 3's optimality over all policies, so the goal is at least as strong as printed. The ε\varepsilonε of Definition 2 is on the scale of J=E[eλ∑βtc]J=E[e^{\lambda\sum\beta^tc}]J=E[eλ∑βtc]. Equilibrium and optimality are stated in "for every deviation" form, with no infimum over a type.
  • Assumption 2-(a) and the modulus ωg\omega_gωg​ of Proposition 10 are written as ε\varepsilonε–δ\deltaδ statements, which is equivalent to "ω(r)→0\omega(r)\to0ω(r)→0" because the moduli are nondecreasing. Total variation is sup⁡∣g∣≤1∣∫g dμ−∫g dν∣\sup_{|g|\le1}|\int g\,d\mu-\int g\,d\nu|sup∣g∣≤1​∣∫gdμ−∫gdν∣.
  • The augmented cost coordinate is the discounted sum ∑k<tβkc(⋅)\sum_{k<t}\beta^kc(\cdot)∑k<t​βkc(⋅); the page prints it without βk\beta^kβk, which contradicts PtP_tPt​. The coordinate lies in R\mathbb RR rather than [0,L][0,L][0,L], because X×[0,L]\mathsf X\times[0,L]X×[0,L] is not invariant under PtP_tPt​, and the terminal cost is eλmax⁡(0,min⁡(c,L))e^{\lambda\max(0,\min(c,L))}eλmax(0,min(c,L)), which equals eλce^{\lambda c}eλc on reachable states. Corollary 1's printed "lim⁡≥\lim\gelim≥" (the limit is not shown to exist) is stated as three limit and eventual-inequality claims.

No hypothesis is vacuous: a sorry-free check exhibits a model satisfying the standing assumptions, Assumptions 1 and 2 and the equilibrium condition simultaneously, with Ji(N)≥1J^{(N)}_i\ge1Ji(N)​≥1. This rules out the trivial reading in which a non-integrable integrand makes every cost 000 and every profile an ε\varepsilonε-equilibrium. Theorem 1 (existence of the equilibrium) is the other mission of the series; here the equilibrium is a hypothesis.

Selected references

  • N. Saldi, T. Başar, M. Raginsky, Discrete-time Risk-sensitive Mean-field Games, arXiv:1808.03929v2, 2018; published as Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games, Math. Oper. Res. 45(4), 2020. https://arxiv.org/abs/1808.03929, https://doi.org/10.1287/moor.2019.1044
  • N. Saldi, T. Başar, M. Raginsky, Markov–Nash Equilibria in Mean-Field Games with Discounted Cost, SIAM J. Control Optim. 56(6), 2018. https://arxiv.org/abs/1612.07878
  • N. Bäuerle, U. Rieder, More Risk-Sensitive Markov Decision Processes, Math. Oper. Res. 39(1), 2014. https://doi.org/10.1287/moor.2013.0601
  • O. Hernández-Lerma, J. B. Lasserre, Discrete-Time Markov Control Processes: Basic Optimality Criteria, Springer, 1996. https://doi.org/10.1007/978-1-4612-0729-0
  • R. M. Dudley, Real Analysis and Probability, Cambridge University Press, 2002 (§11.3, the bounded-Lipschitz metric). https://doi.org/10.1017/CBO9780511755347
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Dynamical SystemsProbability·Captain: mikedeng1

Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions 2: The Neuronal Network Converges in L² to Its McKean–Vlasov LimitResearch Paper

Motivation

Large networks of neurons are often modelled as systems of coupled stochastic differential equations: each neuron carries a low-dimensional state (a membrane potential and recovery variables, as in the FitzHugh–Nagumo model), receives synaptic input from the other neurons with a transmission delay, and is perturbed by noise. Because the number of neurons is large, one studies the mean-field limit: as the population grows, each neuron should evolve independently of every other fixed neuron, driven by its own noise and by an averaged population input. This asymptotic independence is called propagation of chaos, and the limiting single-neuron equation is a McKean–Vlasov equation.

Mehri, Scheutzow, Stannat and Zangeneh (arXiv:1805.01654v3, Ann. Appl. Probab. 2020, DOI 10.1214/19-AAP1499) prove propagation of chaos for a model combining features that earlier work treated separately: monotone (one-sided Lipschitz) local dynamics, general path-dependent delays, Lévy-type jump noise, spatial structure with several subpopulations, and a random environment (disorder). Earlier mean-field results for neuronal networks were obtained under global Lipschitz assumptions (Quiñinao and Touboul 2015; Touboul 2014, two papers), for locally Lipschitz coefficients (Baladron, Fasoli, Faugeras and Touboul 2012, with the clarification note of Bossy, Faugeras and Talay 2015) and for one-sided Lipschitz coefficients (Luçon and Stannat 2014; Touboul 2012); with jump noise, only under global Lipschitz or gradient-type local dynamics (Andreis, Dai Pra and Fischer 2018). This mission formalizes the paper's second main result, Theorem 1.8. The first mission of the series formalizes the well-posedness of the McKean–Vlasov equation (Theorem 1.5).

Setting

Neurons sit at positions rrr in a bounded set Γ⊂Rk\Gamma\subset\mathbb R^kΓ⊂Rk, partitioned into PPP measurable subpopulation regions Γα\Gamma_\alphaΓα​. The NNN-th network consists of a finite set AN⊂Γ\mathcal A_N\subset\GammaAN​⊂Γ of NNN positions, and neurons of subpopulation α\alphaα carry the weight 1/SAN,α1/\mathcal S_{\mathcal A_N,\alpha}1/SAN​,α​. The state Xtr,AN∈RdX^{r,\mathcal A_N}_t\in\mathbb R^dXtr,AN​​∈Rd of the neuron at rrr solves the network equation (1)

dXtr,AN=f dt+g dWtr+∫Uh N~r(dt,dξ)+∑α=1P1SAN,α∑r~∈AN∩Γα[θ dt+β dBtr,α+∫Uη N~r,α(dt,dξ)],dX^{r,\mathcal A_N}_t=f\,dt+g\,dW^r_t+\int_U h\,\tilde N^r(dt,d\xi)+\sum_{\alpha=1}^P\frac{1}{\mathcal S_{\mathcal A_N,\alpha}}\sum_{\tilde r\in\mathcal A_N\cap\Gamma_\alpha}\Big[\theta\,dt+\beta\,dB^{r,\alpha}_t+\int_U\eta\,\tilde N^{r,\alpha}(dt,d\xi)\Big],dXtr,AN​​=fdt+gdWtr​+∫U​hN~r(dt,dξ)+α=1∑P​SAN​,α​1​r~∈AN​∩Γα​∑​[θdt+βdBtr,α​+∫U​ηN~r,α(dt,dξ)],

where f,g,hf,g,hf,g,h are evaluated at (t,r,Xt−r,AN,ω′)(t,r,X^{r,\mathcal A_N}_{t-},\omega')(t,r,Xt−r,AN​​,ω′) and θ,β,η\theta,\beta,\etaθ,β,η at (t,r,r~,Xt−r,AN,X(t−τ)−:t−r~,AN,ω′)(t,r,\tilde r,X^{r,\mathcal A_N}_{t-},X^{\tilde r,\mathcal A_N}_{(t-\tau)^-:t^-},\omega')(t,r,r~,Xt−r,AN​​,X(t−τ)−:t−r~,AN​​,ω′), the last argument being the path of the presynaptic neuron over the delay window [t−τ,t][t-\tau,t][t−τ,t]. The noises WrW^rWr, Br,αB^{r,\alpha}Br,α are independent Brownian motions, N~r\tilde N^rN~r, N~r,α\tilde N^{r,\alpha}N~r,α independent compensated Poisson random measures with intensity dt⊗νdt\otimes\nudt⊗ν, and ω′\omega'ω′ is a random disorder with expectation E\mathcal EE. Each neuron starts from a path zrz^rzr on [−τ,0][-\tau,0][−τ,0].

Given a finite measure R\mathcal RR on Γ\GammaΓ with R(Γα)=1\mathcal R(\Gamma_\alpha)=1R(Γα​)=1, the McKean–Vlasov equation (6) describes a continuum of neurons XrX^rXr, r∈Γr\in\Gammar∈Γ, whose interaction is ∑α∫ΓαE~[θ(t,r,r′,Xt−r,X~(t−τ)−:t−r′,ω′)]R(dr′)\sum_\alpha\int_{\Gamma_\alpha}\tilde{\mathbb E}[\theta(t,r,r',X^r_{t-},\tilde X^{r'}_{(t-\tau)^-:t^-},\omega')]\mathcal R(dr')∑α​∫Γα​​E~[θ(t,r,r′,Xt−r​,X~(t−τ)−:t−r′​,ω′)]R(dr′), with X~\tilde XX~ an independent copy of XXX (and likewise for β\betaβ, η\etaη). The mean-field equation (5) for a neuron rrr of the network has the same form, with XrX^rXr replaced by a process Xˉr\bar X^rXˉr that starts from the same zrz^rzr and is driven by the same noises Wr,Br,α,N~r,N~r,αW^r, B^{r,\alpha}, \tilde N^r,\tilde N^{r,\alpha}Wr,Br,α,N~r,N~r,α as neuron rrr of the network, while the interaction is computed from the law of the solution of (6).

Formalization targets

Goal: Theorem 1.8

Under Hypothesis 1.6 and the chaotic initial condition (the zrz^rzr are independent, with zrz^rzr distributed as z^α\hat z^\alphaz^α for r∈Γαr\in\Gamma_\alphar∈Γα​),

lim⁡N→∞Esup⁡t∈[−τ,T], r∈ANE∣Xtr,AN−Xˉtr∣2=0.\lim_{N\to\infty}\mathcal E\sup_{t\in[-\tau,T],\,r\in\mathcal A_N}\mathbb E\big|X^{r,\mathcal A_N}_t-\bar X^r_t\big|^2=0 .N→∞lim​Et∈[−τ,T],r∈AN​sup​E​Xtr,AN​​−Xˉtr​​2=0.

The theorem asserts convergence without a rate, which is the stable form of the result.

Milestones

  1. Proposition 1.2: the network equation (1) is well posed.
  2. Lemma 1.7: positions in one cell Γαm,ε\Gamma^{m,\varepsilon}_\alphaΓαm,ε​ of the partition of Hypothesis 1.6 have solutions of (6) within C2(t,ω′)εC_2(t,\omega')\varepsilonC2​(t,ω′)ε in mean square.
  3. Display (18): the first moment estimate for Xr,AN−XˉrX^{r,\mathcal A_N}-\bar X^rXr,AN​−Xˉr, in terms of the fluctuation terms IαθI^\theta_\alphaIαθ​, IαβI^\beta_\alphaIαβ​, IαηI^\eta_\alphaIαη​.
  4. The bound (p. 20) of each III-term by 6(⋯ )C2(t,ω′)6(\cdots)C_2(t,\omega')6(⋯)C2​(t,ω′).
  5. The Gronwall bound (p. 21) with constant 363636, at a fixed disorder.
  6. The bound (p. 21) after integration over the disorder, with a constant C(T)C(T)C(T) independent of ε\varepsilonε and NNN.

The proof also uses Lemma 1.4 (the moment bound C1C_1C1​ for solutions of (6)), which is a milestone of the first mission of this series and is not restated here.

Significance

Theorem 1.8 justifies replacing a large, spatially structured network of delayed, jump-driven neurons by a single McKean–Vlasov equation indexed by position. The limit is the object on which neural field models and their bifurcation analysis are built; the theorem identifies the hypotheses on the spatial distribution of neurons (condition (10): the neuron counts per cell, normalized by the weights, converge to R\mathcal RR) under which that replacement is valid in a random environment.

The result is proved in the paper; no machine-checked proof exists. Formalizing it requires a coherent Lean layer for strong solutions of delay SDEs with jumps, mean-field interaction terms, Poisson random measures with product marks, and independence of countable families of drivers. The intermediate bounds of §3 are explicit and quantitative, and each is a self-contained target.

Difficulty

The interaction of the network is an empirical average over finitely many neurons, while the limit uses an expectation over a continuum of positions. The difference splits into three errors of different nature: a fluctuation term, whose control requires that the limit processes Xˉr~\bar X^{\tilde r}Xˉr~ of distinct neurons be independent (which holds only because each is driven by its own noise and starts from an independent initial condition); a spatial discretization error within each cell, which requires a quantitative regularity of the solution of (6) in the position variable; and a counting error between the neuron counts and the measure R\mathcal RR. A naive comparison of the network with (6) directly, without the coupled processes Xˉr\bar X^rXˉr of (5), gives no pathwise relation and does not work. The coefficients are only one-sided Lipschitz in the local variable, so moment bounds must come from monotonicity rather than from global Lipschitz estimates, and the disorder enters the constants through exponentials whose integrability is exactly assumption (H6).

Formalization scope

Positions are EuclideanSpace ℝ (Fin k), states EthierKurtz.SDEState d, and subpopulations Fin P (0-based). Neurons carry labels in ℕ with an injective position map, so AN\mathcal A_NAN​ is a finite set of labels and ⋃NAN\bigcup_N\mathcal A_N⋃N​AN​ is countable. Brownian integrals are the published EthierKurtz.HasBrownianItoIntegral per coordinate, compensated jump integrals the published JacodTodorov10.LLN.HasCompInt, and all Poisson measures of the network form one (𝓕_t)-Poisson random measure on a product mark space. Integrands are cut off after the horizon TTT. All expectations, suprema and the disorder expectation E\mathcal EE are taken in [0,∞][0,\infty][0,∞], so no statement can be satisfied by a junk value of a real integral or supremum; (H6) states the boundedness of its supremum explicitly. The copy X^\hat XX^ enters only through its law: the solution of (6) lives on its own probability space and the mean-field terms are expectations over it.

Conventions and corrections, all disclosed in the items: the theorem is stated for every family of solutions of (1), (5) and (6) (hypotheses), not for "the" solutions; (H1′) is printed with x−yx-yx−y and is read as x−x~x-\tilde xx−x~; IαηI^\eta_\alphaIαη​ carries the expectation of (17), which the display on p. 20 omits; the second Gronwall inequality on p. 21 (constant 144144144) drops a factor of C1C_1C1​ and is not posed; the coefficients' path argument carries the product σ-algebra; the filtration satisfies the usual conditions (Appendix A); the solution class of (6) is a bound for every time. The solution notions are not trivializing: every stochastic integral is tied to the given noise by a published predicate, the mean-field terms are computed from the solution of (6) itself, the limit processes share the network's noise and initial conditions, and the finite constant of the integrated bound is quantified before ε\varepsilonε and NNN.

Reusable beyond this mission: the strong-solution predicate for jump SDEs with delay, the noise predicates for countable families of drivers, and the network and mean-field interaction terms. Contributions toward a stochastic calculus for these predicates (Itô's formula for ∣X∣2|X|^2∣X∣2 with jumps, Gronwall arguments with left limits) are welcome.

Selected references

  • S. Mehri, M. Scheutzow, W. Stannat, B. Z. Zangeneh, Propagation of chaos for stochastic spatially structured neuronal networks with delay driven by jump diffusions, Ann. Appl. Probab. 30 (2020); arXiv:1805.01654v3. https://arxiv.org/abs/1805.01654
  • J. Baladron, D. Fasoli, O. Faugeras, J. Touboul, Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons, J. Math. Neurosci. 2:10 (2012). https://doi.org/10.1186/2190-8567-2-10
  • M. Bossy, O. Faugeras, D. Talay, Clarification and complement to "Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons", J. Math. Neurosci. 5:19 (2015). https://doi.org/10.1186/s13408-015-0031-8
  • J. Touboul, Propagation of chaos in neural fields, Ann. Appl. Probab. 24(3):1298–1328 (2014); arXiv:1108.2414. https://arxiv.org/abs/1108.2414
  • J. Touboul, Spatially extended networks with singular multi-scale connectivity patterns, J. Stat. Phys. 156(3):546–573 (2014).
  • C. Quiñinao, J. Touboul, Limits and dynamics of randomly connected neuronal networks, Acta Appl. Math. 136(1):167–192 (2015).
  • E. Luçon, W. Stannat, Mean field limit for disordered diffusions with singular interactions, Ann. Appl. Probab. 24(5):1946–1993 (2014).
  • J. Touboul, Limits and dynamics of stochastic neuronal networks with random heterogeneous delays, J. Stat. Phys. 149(4):569–597 (2012).
  • L. Andreis, P. Dai Pra, M. Fischer, McKean–Vlasov limit for interacting systems with simultaneous jumps, Stoch. Anal. Appl. (2018).
15 thms1 active userReviewed
Probability·Captain: mikedeng1

Liouville Quantum Gravity and the Brownian Map II: Geodesics and Continuity of the Embedding: A Quantitative Kolmogorov–Čentsov Criterion, P[M ≥ t] ≤ c₁t^(−α) for the Hölder Norm MResearch Paper

Motivation

The Kolmogorov–Čentsov continuity criterion is the standard way to prove that a random field has a continuous version: a moment bound on increments, E∣Xu−Xv∣α≤c0∣u−v∣d+β\mathbf E|X_u - X_v|^\alpha \le c_0|u - v|^{d+\beta}E∣Xu​−Xv​∣α≤c0​∣u−v∣d+β, yields a modification whose paths are Hölder continuous of every order γ<β/α\gamma < \beta/\alphaγ<β/α (Karatzas–Shreve 1991, §2.2; Revuz–Yor 1999, Ch. I). It is used for Brownian motion, Brownian sheets, solutions of stochastic PDEs, Gaussian free field approximations and many other random fields.

The classical statement says only that the Hölder constant MMM is finite almost surely. Many applications need more: a bound on the tail P[M≥t]\mathbf P[M \ge t]P[M≥t] whose constant depends only on the parameters α,β,c0\alpha, \beta, c_0α,β,c0​ and not on the particular field, so that the bound holds uniformly over a family of fields.

This mission formalizes such a quantitative version, Proposition 2.3 in §2.3 of J. Miller and S. Sheffield, Liouville quantum gravity and the Brownian map II: geodesics and continuity of the embedding (Ann. Probab. 2021). The authors state it, note that it follows "by carefully following the proof" of the classical criterion, and write the proof out (pp. 30–31). They apply it to the circle-average process of the Gaussian free field (Proposition 2.4, p. 33) and again in Lemma 5.12 (p. 63).

The paper's main theorems (the 8/3\sqrt{8/3}8/3​-Liouville quantum gravity sphere equipped with the QLE(8/3, 0) metric has the law of the Brownian map; continuity of the embedding) are not part of this mission. Their objects, among them the Gaussian free field, SLE6_66​, quantum surfaces, the QLE metric of Miller–Sheffield 2020 and the Brownian map, have no formal substrate in Mathlib or on the platform. Proposition 2.3 is a self-contained probabilistic tool that the paper proves in full, and it is statable today.

Setting

Fix a dimension d∈Nd \in \mathbb Nd∈N. The index set is the cube [0,1]d[0,1]^d[0,1]d with the Euclidean distance ∣u−v∣|u - v|∣u−v∣. A random field is a family (Xu)u∈[0,1]d(X_u)_{u \in [0,1]^d}(Xu​)u∈[0,1]d​ of real random variables on a probability space (Ω,F,P)(\Omega, \mathcal F, \mathbf P)(Ω,F,P). The field satisfies the Kolmogorov condition with constants α,β,c0>0\alpha, \beta, c_0 > 0α,β,c0​>0 if

E[∣Xu−Xv∣α]≤c0∣u−v∣d+βfor all u,v∈[0,1]d.(2.6)\mathbf E\big[|X_u - X_v|^\alpha\big] \le c_0 |u - v|^{d+\beta} \qquad \text{for all } u, v \in [0,1]^d. \tag{2.6}E[∣Xu​−Xv​∣α]≤c0​∣u−v∣d+βfor all u,v∈[0,1]d.(2.6)

A modification of XXX is a field YYY on the same space with P[Yu=Xu]=1\mathbf P[Y_u = X_u] = 1P[Yu​=Xu​]=1 for every uuu. For γ>0\gamma > 0γ>0, the γ\gammaγ-Hölder norm of a function fff on the cube is

Mγ(f)=sup⁡u≠v∣f(u)−f(v)∣∣u−v∣γ∈[0,∞].M_\gamma(f) = \sup_{u \ne v} \frac{|f(u) - f(v)|}{|u - v|^\gamma} \in [0, \infty].Mγ​(f)=u=vsup​∣u−v∣γ∣f(u)−f(v)∣​∈[0,∞].

The proof works on the dyadic grid Dk\mathcal D_kDk​, the points of the cube whose coordinates are integer multiples of 2−k2^{-k}2−k, and on the set D~k\widetilde{\mathcal D}_kDk​ of adjacent pairs {u,v}⊆Dk\{u, v\} \subseteq \mathcal D_k{u,v}⊆Dk​, which differ in exactly one coordinate, by 2−k2^{-k}2−k. In Lean the cube is Cube d, and the grid and the pairs are dyadicGrid d k and IsAdjacentPair d k u v.

Formalization targets

Goal: Proposition 2.3 (p. 30)

For every γ∈(0,β/α)\gamma \in (0, \beta/\alpha)γ∈(0,β/α) there is a constant c1(γ)>0c_1(\gamma) > 0c1​(γ)>0, depending only on d,α,β,γ,c0d, \alpha, \beta, \gamma, c_0d,α,β,γ,c0​, such that every field satisfying (2.6) has one modification YYY with, for every γ∈(0,β/α)\gamma \in (0, \beta/\alpha)γ∈(0,β/α),

∀ω ∃M>0: ∣Yu(ω)−Yv(ω)∣≤M∣u−v∣γ  ∀u,v,(2.7)\forall \omega\ \exists M > 0:\ |Y_u(\omega) - Y_v(\omega)| \le M|u - v|^\gamma \ \ \forall u, v, \tag{2.7}∀ω ∃M>0: ∣Yu​(ω)−Yv​(ω)∣≤M∣u−v∣γ  ∀u,v,(2.7) P[Mγ(Y(ω))≥t]≤c1(γ) t−αfor all t≥1.(2.8)\mathbf P\big[M_\gamma(Y(\omega)) \ge t\big] \le c_1(\gamma)\, t^{-\alpha} \qquad \text{for all } t \ge 1. \tag{2.8}P[Mγ​(Y(ω))≥t]≤c1​(γ)t−αfor all t≥1.(2.8)

Milestones (attack order)

  1. (2.9), p. 30: P[∣Xu−Xv∣≥δ]≤c0δ−α∣u−v∣d+β\mathbf P[|X_u - X_v| \ge \delta] \le c_0 \delta^{-\alpha}|u - v|^{d+\beta}P[∣Xu​−Xv​∣≥δ]≤c0​δ−α∣u−v∣d+β.
  2. (2.10), p. 31: for {u,v}∈D~k\{u, v\} \in \widetilde{\mathcal D}_k{u,v}∈Dk​, P[∣Xu−Xv∣≥t2−γk]≤c0t−α2−k(d+β−αγ)\mathbf P[|X_u - X_v| \ge t2^{-\gamma k}] \le c_0 t^{-\alpha} 2^{-k(d+\beta-\alpha\gamma)}P[∣Xu​−Xv​∣≥t2−γk]≤c0​t−α2−k(d+β−αγ).
  3. (2.11), p. 31: P[max⁡D~k∣Xu−Xv∣≥t2−γk]≤c1t−α2−k(β−αγ)\mathbf P[\max_{\widetilde{\mathcal D}_k} |X_u - X_v| \ge t2^{-\gamma k}] \le c_1 t^{-\alpha}2^{-k(\beta-\alpha\gamma)}P[maxDk​​∣Xu​−Xv​∣≥t2−γk]≤c1​t−α2−k(β−αγ), with c1c_1c1​ uniform in kkk, ttt and the field (this c1c_1c1​ is not the one of (2.8)).
  4. (2.12), p. 31: P[sup⁡kmax⁡D~k2γk∣Xu−Xv∣≥t]≤c2t−α\mathbf P[\sup_k \max_{\widetilde{\mathcal D}_k} 2^{\gamma k}|X_u - X_v| \ge t] \le c_2 t^{-\alpha}P[supk​maxDk​​2γk∣Xu​−Xv​∣≥t]≤c2​t−α.
  5. Closing claim of the proof, p. 31: a deterministic statement. If 2γk∣f(u)−f(v)∣≤t2^{\gamma k}|f(u) - f(v)| \le t2γk∣f(u)−f(v)∣≤t for all adjacent pairs at all levels, then ∣f(u)−f(v)∣≤c3t∣u−v∣γ|f(u) - f(v)| \le c_3 t|u - v|^\gamma∣f(u)−f(v)∣≤c3​t∣u−v∣γ for all dyadic u,vu, vu,v, with c3c_3c3​ depending on d,γd, \gammad,γ only.
  6. (2.7), p. 30: the classical criterion alone, a modification that is γ\gammaγ-Hölder for every γ∈(0,β/α)\gamma \in (0, \beta/\alpha)γ∈(0,β/α).

Significance

The tail bound (2.8) is what makes the criterion usable for families of fields. In the paper, it bounds the modulus of continuity of the Gaussian free field circle averages at every scale with a single constant, which feeds the estimates on the Liouville quantum gravity metric. More generally, polynomial tails for Hölder norms with field-independent constants are the input to tightness arguments for sequences of random fields, to union bounds over many scales or many fields, and to moment bounds for Hölder norms.

The result itself is known: the authors derive it from the textbook proof, which they write out. What is missing is a machine-checked version. At the pinned Mathlib revision, ProbabilityTheory.IsKolmogorovProcess defines the hypothesis (2.6), but no continuity theorem is proved from it, qualitative or quantitative. The platform has an Open goal for the qualitative one-parameter theorem on [0,∞)[0, \infty)[0,∞), KolmogorovChentsov.exists_modification_holderOnWith_Icc, a different statement that the mission does not duplicate. A proof of this mission's goal would give the classical ddd-parameter criterion on the cube (milestone 6) and its quantitative form together.

Difficulty

The probabilistic steps (2.9)–(2.12) are Markov's inequality and two union bounds. They become concrete once the adjacent pairs are counted: ∣D~k∣|\widetilde{\mathcal D}_k|∣Dk​∣ is of order d 2dkd\,2^{dk}d2dk, and summing over scales needs γ<β/α\gamma < \beta/\alphaγ<β/α. Formalizing them requires care with suprema in [0,∞][0,\infty][0,∞] and with outer measures of events that are not obviously measurable.

The central difficulty is the deterministic chaining claim and the passage from dyadic points to the whole cube. The paper calls the claim "not difficult to see", but its constant must be uniform over pairs of dyadic points of arbitrarily fine and unequal levels, and the obvious attempt, comparing values along the straight segment between two points, fails because the points of the segment are not dyadic, so the hypothesis says nothing about them. The second difficulty is the modification itself: one field YYY must serve every γ<β/α\gamma < \beta/\alphaγ<β/α at once, must agree with XXX almost surely at every point, and the tail bound for the dyadic supremum must transfer to the Hölder norm over the whole cube, an uncountable supremum whose event is not obviously measurable.

Formalization scope

  • Index set: Cube d, the subtype of EuclideanSpace ℝ (Fin d) with coordinates in [0,1][0,1][0,1], so ∣u−v∣|u - v|∣u−v∣ is Euclidean. Because all constants are existential, the statements do not depend on the norm, but Euclidean is the default reading.
  • Hypothesis (2.6): Mathlib's IsKolmogorovProcess X P α (d + β) c₀ with c₀ : ℝ≥0, plus 0 < α, 0 < β, 0 < c₀. It reads (2.6) with the lower Lebesgue integral in [0,∞][0,\infty][0,∞], so it cannot hold through a junk value of a non-integrable expectation. It also requires each pair (Xu,Xv)(X_u, X_v)(Xu​,Xv​) to be Borel measurable, which is the measurability included in "random field". The probability space is [IsProbabilityMeasure P].
  • Hölder norm: MγM_\gammaMγ​ is eHolderNorm γ, valued in [0,∞][0,\infty][0,∞]. A real supremum, which is 0 on unbounded families and would make (2.8) trivially true, is ruled out. The supremum of (2.12) is likewise an ℝ≥0∞-valued ⨆, and its event is {t≤sup⁡}\{t \le \sup\}{t≤sup}, not the weaker "some term is ≥t\ge t≥t".
  • Uniformity: the constants c1c_1c1​ of (2.8) (a function of γ\gammaγ), c1c_1c1​ of (2.11), c2c_2c2​ and c3c_3c3​ are quantified before the probability space and the field. A version in which the constant may depend on the field, or one with a different modification for each γ\gammaγ, is a weaker theorem and is ruled out. The probability space ranges over Type (universe 0).
  • Conventions: (2.7) holds for every ω\omegaω (the paper states it for the modification itself). Probabilities of events not shown measurable are outer measures. The dyadic level kkk ranges over N\mathbb NN including 000. Adjacent pairs are ordered, which doubles a count that the constants absorb. The milestones add t>0t > 0t>0 and δ>0\delta > 0δ>0, which the paper leaves implicit, and carry γ∈(0,β/α)\gamma \in (0, \beta/\alpha)γ∈(0,β/α) from (2.10) on. The constants may depend on ddd, which the paper's list "α,β,γ,c0\alpha, \beta, \gamma, c_0α,β,γ,c0​" leaves implicit.

A complete development needs counting lemmas for the dyadic grid, a chaining lemma on dyadic points, and the extension of a uniformly Hölder function from a dense subset (Mathlib's HolderOnWith and uniform-continuity extension tools apply). The chaining lemma and the quantitative criterion are reusable for any Hölder-regularity argument on cubes. Contributions are welcome for each milestone independently and for an alternative proof of the goal through Mathlib's PairReduction chaining machinery.

Selected references

  • J. Miller, S. Sheffield, Liouville quantum gravity and the Brownian map II: geodesics and continuity of the embedding, Ann. Probab., 2021 (accepted manuscript, Apollo repository, University of Cambridge). https://doi.org/10.1214/21-AOP1506
  • J. Miller, S. Sheffield, Liouville quantum gravity and the Brownian map I: the QLE(8/3, 0) metric, Invent. Math. 219(1), 75–152, 2020. https://arxiv.org/abs/1507.00719
  • I. Karatzas, S. E. Shreve, Brownian Motion and Stochastic Calculus, 2nd ed., Graduate Texts in Mathematics 113, Springer, 1991. https://doi.org/10.1007/978-1-4612-0949-2
  • D. Revuz, M. Yor, Continuous Martingales and Brownian Motion, 3rd ed., Grundlehren der Mathematischen Wissenschaften 293, Springer, 1999. https://doi.org/10.1007/978-3-662-06400-9
  • Mathlib, Mathlib/Probability/Process/Kolmogorov.lean (the predicate IsKolmogorovProcess). https://github.com/leanprover-community/mathlib4/blob/master/Mathlib/Probability/Process/Kolmogorov.lean
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Dynamical SystemsProbability·Captain: mikedeng1

Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions 1: The Spatially Structured McKean–Vlasov Delay Equation with Jumps Is Well-PosedResearch Paper

Motivation

Networks of conductance-based neurons, such as FitzHugh–Nagumo networks, are modelled by systems of stochastic differential equations in which each neuron interacts with the others through synapses, and the signal from one neuron reaches another only after a transmission delay. Biological neurons sit at positions in space, belong to a few distinct subpopulations, are driven by Brownian and Poisson (jump) noise, and vary from one to another; the last feature is modelled by a random disorder parameter. When the number of neurons tends to infinity, the state of a typical neuron is expected to follow a McKean–Vlasov equation: an SDE whose coefficients depend on the law of its own solution. S. Mehri, M. Scheutzow, W. Stannat and B. Z. Zangeneh (arXiv:1805.01654; Ann. Appl. Probab. 30 (2020), DOI 10.1214/19-AAP1499) prove that this limit equation is well-posed, with coefficients that are only monotone (one-sided Lipschitz), a general delay, jump noise, spatial structure and disorder all at once, and then prove propagation of chaos towards it.

Earlier work, as surveyed on p. 3 of the paper, covered parts of this setting: global Lipschitz coefficients (Quiñinao and Touboul 2015, and the paper's references [10, 11]), locally Lipschitz coefficients (Baladron, Fasoli, Faugeras and Touboul 2012, with the clarification of Bossy, Faugeras and Talay 2015 on the localization by hitting times; the same issue affects Touboul 2012), one-sided Lipschitz coefficients with diffusive noise (Luçon and Stannat 2014), and Lévy noise under global Lipschitz assumptions or gradient-type local dynamics (Andreis, Dai Pra and Fischer 2018). The paper constructs the solution by an Euler approximation, which, by the authors' account, had not been applied to McKean–Vlasov equations before.

Setting

Fix dimensions ddd (state), mmm, nnn (noise), kkk (space), a delay τ>0\tau > 0τ>0 and P≥1P \ge 1P≥1 subpopulations, located at pairwise disjoint measurable regions Γ1,…,ΓP⊂Rk\Gamma_1,\dots,\Gamma_P \subset \mathbb R^kΓ1​,…,ΓP​⊂Rk whose union Γ\GammaΓ is bounded. A finite Borel measure R\mathcal RR on Γ\GammaΓ with R(Γα)=1\mathcal R(\Gamma_\alpha) = 1R(Γα​)=1 describes the spatial distribution of neurons. A disorder probability space (Ω′,F′,P′)(\Omega',\mathcal F',\mathbb P')(Ω′,F′,P′) is fixed. On a filtered probability space (Ω,F,(Ft),P)(\Omega,\mathcal F,(\mathcal F_t),\mathbb P)(Ω,F,(Ft​),P) there are an mmm-dimensional Brownian motion WWW, nnn-dimensional Brownian motions B1,…,BPB^1,\dots,B^PB1,…,BP, Poisson random measures N,N1,…,NPN, N^1, \dots, N^PN,N1,…,NP on [0,∞)×U[0,\infty)\times U[0,∞)×U with intensity dt⊗νdt\otimes\nudt⊗ν (ν\nuν σ-finite; N~=N−dt⊗ν\tilde N = N - dt\otimes\nuN~=N−dt⊗ν), all independent, and initial paths z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd))\hat z^\zeta \in L^2(\Omega;\text{Càdlàg}([-\tau,0];\mathbb R^d))z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd)).

For a path yyy, write y(t−τ)−:t−y_{(t-\tau)^-:t^-}y(t−τ)−:t−​ for the segment u↦y(t+u)−u\mapsto y_{(t+u)^-}u↦y(t+u)−​, u∈[−τ,0]u\in[-\tau,0]u∈[−τ,0]. The equation is

dXtr=f(t,r,Xt−r,ω′)dt+g(⋅)dWt+∫Uh(⋅,ξ)N~(dt,dξ)+∑α=1P∫ΓαE~[θ(t,r,r′,Xt−r,X~(t−τ)−:t−r′,ω′)]R(dr′)dtdX^r_t = f(t,r,X^r_{t-},\omega')dt + g(\cdot)dW_t + \int_U h(\cdot,\xi)\tilde N(dt,d\xi) + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}\big[\theta(t,r,r',X^r_{t-},\tilde X^{r'}_{(t-\tau)^-:t^-},\omega')\big]\mathcal R(dr')dtdXtr​=f(t,r,Xt−r​,ω′)dt+g(⋅)dWt​+∫U​h(⋅,ξ)N~(dt,dξ)+α=1∑P​∫Γα​​E~[θ(t,r,r′,Xt−r​,X~(t−τ)−:t−r′​,ω′)]R(dr′)dt +∑α=1P∫ΓαE~[β(⋯ )]R(dr′)dBtα+∑α=1P∫Γα∫UE~[η(⋯ ,ξ)]R(dr′)N~α(dt,dξ),Xtr=z^tζ (r∈Γζ, t∈[−τ,0]),(6)+ \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}[\beta(\cdots)]\mathcal R(dr')dB^\alpha_t + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\int_U\tilde{\mathbb E}[\eta(\cdots,\xi)]\mathcal R(dr')\tilde N^\alpha(dt,d\xi),\qquad X^r_t = \hat z^\zeta_t\ (r\in\Gamma_\zeta,\ t\in[-\tau,0]), \tag{6}+α=1∑P​∫Γα​​E~[β(⋯)]R(dr′)dBtα​+α=1∑P​∫Γα​​∫U​E~[η(⋯,ξ)]R(dr′)N~α(dt,dξ),Xtr​=z^tζ​ (r∈Γζ​, t∈[−τ,0]),(6)

where X~\tilde XX~ is an independent copy of the solution XXX and E~\tilde{\mathbb E}E~ its expectation. The local dynamics f,g,hf, g, hf,g,h satisfy the monotonicity and growth conditions (H1)–(H3) of Hypothesis 1.1 with locally integrable random rates Lt(ω′)L_t(\omega')Lt​(ω′), Kt(ω′)K_t(\omega')Kt​(ω′), K~t(R,ω′)\tilde K_t(R,\omega')K~t​(R,ω′); the synaptic coefficients θ,β,η\theta, \beta, \etaθ,β,η are Lipschitz (H4) and of linear growth (H5) in (x,y)(x, y)(x,y), with rates Lˉt(ω′)\bar L_t(\omega')Lˉt​(ω′), Kˉt(ω′)\bar K_t(\omega')Kˉt​(ω′), the path variable measured through a probability measure λ\lambdaλ on [−τ,0][-\tau,0][−τ,0]. In Lean, the model is the definition module NeuroMV.WellPosed.Setting: Space, Coeffs, Hyp1_1, Noise/IsNoise, IsStrongSol6, InClass and the constant C1 of (7).

Formalization targets

Goal: Theorem 1.5 (p. 7)

For every T>0T>0T>0 there is a process Xtr(ω;ω′)X^r_t(\omega;\omega')Xtr​(ω;ω′), measurable in (r,ω′,ω)(r,\omega',\omega)(r,ω′,ω), such that for P′\mathbb P'P′-almost every ω′\omega'ω′, X(ω′)X(\omega')X(ω′) is a strong solution of (6) on [−τ,T][-\tau,T][−τ,T],

X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),X(\omega') \in L^\infty\big([-\tau,T],dt;L^2(\Omega\times\Gamma,\mathbb P\otimes\mathcal R;\mathbb R^d)\big),X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),

and every other strong solution YYY in that class satisfies ∫ΓE∣Xtr−Ytr∣2R(dr)=0\int_\Gamma\mathbb E|X^r_t - Y^r_t|^2\mathcal R(dr) = 0∫Γ​E∣Xtr​−Ytr​∣2R(dr)=0 for all t∈[−τ,T]t\in[-\tau,T]t∈[−τ,T].

Milestones

  1. Theorem A.2 (p. 23): well-posedness of the general path-dependent delay SDE (20) with jumps under the monotonicity Hypothesis A.1, joint measurability in (t,ω,ω′)(t,\omega,\omega')(t,ω,ω′), the moment bound (22), and convergence of the Euler approximation (21).
  2. The scheme (11) exists and is measurable (p. 9), and satisfies the uniform bound (12): sup⁡t∈[−τ,T]E∣Xtn,r∣2≤C1(T,ω′)\sup_{t\in[-\tau,T]}\mathbb E|X^{n,r}_t|^2 \le C_1(T,\omega')supt∈[−τ,T]​E∣Xtn,r​∣2≤C1​(T,ω′).
  3. Claims (iv) and (v) (p. 10): the schemes are Cauchy in probability uniformly on [0,T][0,T][0,T], and their limit solves (6).
  4. Lemma 1.4 (p. 6): every solution in the class satisfies sup⁡s∈[−τ,t]E∣Xsr∣2≤C1(t,ω′)\sup_{s\in[-\tau,t]}\mathbb E|X^r_s|^2 \le C_1(t,\omega')sups∈[−τ,t]​E∣Xsr​∣2≤C1​(t,ω′).
  5. Uniqueness (pp. 16–17): two solutions in the class agree in L2(Ω×Γ)L^2(\Omega\times\Gamma)L2(Ω×Γ) at every time.

Significance

Theorem 1.5 makes the infinite-population limit of the network well defined; the second main result of the paper, Theorem 1.8, proves that the network converges to it in L2L^2L2. The theorem applies to coefficients that are only monotone in the state, which covers the cubic nonlinearity of FitzHugh–Nagumo neurons (Example 1.3), and to synaptic weights of conductance type driven by jump noise. Theorem A.2, proved in the appendix, is a well-posedness and Euler-convergence result for monotone stochastic delay equations with jumps and random coefficients, stated by the authors as new in this generality; it is reusable beyond this paper.

The results are proved in the paper; none of them has a machine-checked proof. The mission produces a Lean statement of the limit equation with the published Brownian and compensated Poisson integral relations, and invites formal proofs of the scheme estimates, the Cauchy property, the identification of the limit, the moment bound and uniqueness.

Difficulty

Under monotone coefficients there is no global contraction, so the Picard iteration that proves McKean–Vlasov well-posedness under Lipschitz assumptions does not apply. Localization by stopping times, the standard replacement for SDEs with monotone coefficients, does not localize the mean-field terms, which depend on the law of the solution at all positions; mishandling this step is the gap that Bossy, Faugeras and Talay pointed out in earlier work, and the acknowledgements (p. 30) record that the first version of this paper contained an unjustified application of the moment estimate of Lemma 1.4. A priori bounds must therefore be uniform in the approximation, and the limit of the mean-field stochastic integrals must be identified, with jumps and delay present. A second difficulty is measurability: the mean-field integrals require the solution to be measurable in the position r′r'r′, and the theorem asserts measurability in (r,ω′)(r,\omega')(r,ω′).

Formalization scope

  • Representation. Positions are EuclideanSpace ℝ (Fin k), states EthierKurtz.SDEState d, matrices Matrix (Fin d) (Fin m) ℝ with the Hilbert–Schmidt norm; subpopulations are Fin P, 0-based. Processes are indexed by ℝ on [−τ,T][-\tau,T][−τ,T]; drivers by ℝ≥0. Path segments are functions ℝ → ℝ^d read on [−τ,0][-\tau,0][−τ,0] with the product (cylinder) σ-algebra; the paper's sup-norm Borel σ-algebra is larger, so joint measurability of the coefficients for the cylinder σ-algebra is a mild added requirement.
  • Noise and integrals. Brownian integrals are the published EthierKurtz.HasBrownianItoIntegral, compensated jump integrals the published JacodTodorov10.LLN.HasCompInt, coordinatewise, with integrands cut off after TTT. All Poisson measures are one JacodTodorov10.LLN.IsFPoisson measure on a product mark space, equivalent to independent measures N,NαN, N^\alphaN,Nα. Independence of the initial data from the drivers is encoded by F0\mathcal F_0F0​-measurability.
  • Mean field. The copy X~\tilde XX~ enters only through its law, so E~\tilde{\mathbb E}E~ is an expectation over XXX itself; the mean-field integrands are required to be integrable on Γα×Ω\Gamma_\alpha\times\OmegaΓα​×Ω. Expectations and suprema are in [0,∞][0,\infty][0,∞]; Bochner integrals carry integrability clauses.
  • Hypotheses. Hypothesis 1.1 (H1)–(H5) and the regularity of p. 2; (H6) is omitted from every item, because it involves the network data of (1) only and the proof never uses it. The class L∞L^\inftyL∞–L2L^2L2 is a bound for every ttt rather than a.e. ttt.
  • Every position. The goal requires the integral identity at every r∈Γr\in\Gammar∈Γ, as (6) is posed; §2 proves it for R×P′\mathcal R\times\mathbb P'R×P′-a.e. (r,ω′)(r,\omega')(r,ω′) (p. 16), and on the remaining null set of positions (6) is an ordinary delay SDE solved by Theorem A.2 — a step the paper leaves implicit. Claim (v) keeps the R\mathcal RR-a.e. reading.
  • No trivialization. The stochastic integrals are the published relations tied to WWW, BαB^\alphaBα, NNN, NαN^\alphaNα, not free processes; the mean-field terms are computed from the solution's own segments; the solution class is non-empty for zero coefficients (a sorry-free check accompanies the mission); and the scheme and limit are the paper's, not new processes with their own noise.
  • Not stated. Claims (i)–(iii) of §2 (the remainder estimate and the a priori bounds before the stopping time) are not separate items.
  • Welcome contributions. Itô's formula for jump diffusions in this encoding, Gronwall-type lemmas in [0,∞][0,\infty][0,∞], stability of the published integral relations under convergence in probability, and the monotone delay SDE theory of Appendix A are all reusable beyond this mission.

Selected references

  • S. Mehri, M. Scheutzow, W. Stannat, B. Z. Zangeneh, Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions, arXiv:1805.01654v3, 2019; Ann. Appl. Probab. 30, 2020. https://arxiv.org/abs/1805.01654, https://doi.org/10.1214/19-AAP1499
  • J. Baladron, D. Fasoli, O. Faugeras, J. Touboul, Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons, J. Math. Neurosci. 2:10, 2012.
  • M. Bossy, O. Faugeras, D. Talay, Clarification and complement to "Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons", J. Math. Neurosci. 5:19, 2015.
  • E. Luçon, W. Stannat, Mean field limit for disordered diffusions with singular interactions, Ann. Appl. Probab. 24(5):1946–1993, 2014.
  • C. Quiñinao, J. Touboul, Limits and dynamics of randomly connected neuronal networks, Acta Appl. Math. 136(1):167–192, 2015.
  • J. Touboul, Limits and dynamics of stochastic neuronal networks with random heterogeneous delays, J. Stat. Phys. 149(4):569–597, 2012.
  • L. Andreis, P. Dai Pra, M. Fischer, McKean–Vlasov limit for interacting systems with simultaneous jumps, Stoch. Anal. Appl., 2018.
  • W. Liu, M. Röckner, Stochastic Partial Differential Equations: An Introduction, Universitext, Springer, 2015.

The bibliographic data of the last seven entries are taken from the reference list of the paper (pp. 30–31).

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Algorithmic Game TheoryDynamic ProgrammingProbability·Captain: mikedeng1

Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games 1: A Risk-Sensitive Mean-Field Game with Compact Actions and Weakly Continuous Kernel Has a Mean-Field EquilibriumResearch Paper

Motivation

Mean-field games describe large populations of identical agents who interact only through the distribution of their states. Each agent solves a stochastic control problem in which the population appears through a deterministic flow of distributions, and an equilibrium requires that this flow coincide with the distribution the agents generate themselves. The theory goes back to Huang, Malhamé and Caines (2006) and Lasry and Lions (2007) in continuous time. In discrete time, Saldi, Başar and Raginsky (SIAM J. Control Optim. 2018) proved existence of equilibria for risk-neutral agents with discounted costs on Polish state spaces.

Risk-neutral agents care only about expected cost. Many applications in engineering and finance call for agents that also penalize the variability of their cost. A standard way to model this is the exponential (risk-sensitive) criterion E[exp⁡(λ⋅cost)]E[\exp(\lambda\cdot\text{cost})]E[exp(λ⋅cost)] with risk factor λ>0\lambda>0λ>0. Its theory for single-agent Markov decision processes goes back to Howard and Matheson (1972) and Jacobson (1973), and Bäuerle and Rieder (Math. Oper. Res. 2014) treat general utilities. Saldi, Başar and Raginsky (arXiv:1808.03929, Math. Oper. Res. 2020) carry the discrete-time mean-field program over to this criterion. This mission covers its first main result: existence of a mean-field equilibrium (Theorem 1).

Setting

The state space X\mathsf XX and the action space A\mathsf AA are Polish, and A\mathsf AA is compact. P(E)\mathcal P(E)P(E) denotes the probability measures on EEE, with the topology of weak convergence and its Borel σ-field. The model consists of:

  • a stochastic kernel p(⋅ ∣ x,a,μ)p(\cdot\,|\,x,a,\mu)p(⋅∣x,a,μ) on X\mathsf XX given X×A×P(X)\mathsf X\times\mathsf A\times\mathcal P(\mathsf X)X×A×P(X);
  • a one-stage cost c(x,a,μ)∈[0,K]c(x,a,\mu)\in[0,K]c(x,a,μ)∈[0,K];
  • an initial law μ0\mu_0μ0​, a discount factor β∈(0,1)\beta\in(0,1)β∈(0,1) and a risk factor λ>0\lambda>0λ>0.

A Markov policy is a sequence π=(πt)t≥0\pi=(\pi_t)_{t\ge0}π=(πt​)t≥0​ of kernels πt(da ∣ x)\pi_t(da\,|\,x)πt​(da∣x). A policy in general is allowed to depend on the whole history (x(0),a(0),…,x(t))(x(0),a(0),\dots,x(t))(x(0),a(0),…,x(t)). Given a measure flow μ=(μt)t≥0⊂P(X)\mu=(\mu_t)_{t\ge0}\subset\mathcal P(\mathsf X)μ=(μt​)t≥0​⊂P(X), a generic agent evolves as

x(0)∼μ0,a(t)∼πt(⋅ ∣ history),x(t+1)∼p(⋅ ∣ x(t),a(t),μt),x(0)\sim\mu_0,\qquad a(t)\sim\pi_t(\cdot\,|\,\text{history}),\qquad x(t+1)\sim p(\cdot\,|\,x(t),a(t),\mu_t),x(0)∼μ0​,a(t)∼πt​(⋅∣history),x(t+1)∼p(⋅∣x(t),a(t),μt​),

and pays the risk-sensitive cost

Jμ(π)=Eπ[exp⁡(λ∑t=0∞βtc(x(t),a(t),μt))].J_\mu(\pi)=E^\pi\Big[\exp\Big(\lambda\sum_{t=0}^\infty\beta^tc(x(t),a(t),\mu_t)\Big)\Big].Jμ​(π)=Eπ[exp(λt=0∑∞​βtc(x(t),a(t),μt​))].

For a Markov policy, Λ(π)\Lambda(\pi)Λ(π) is the flow of state laws it generates: it starts at μ0\mu_0μ0​ and satisfies μt+1(⋅)=∫p(⋅ ∣ x,a,μt) πt(da∣x) μt(dx)\mu_{t+1}(\cdot)=\int p(\cdot\,|\,x,a,\mu_t)\,\pi_t(da|x)\,\mu_t(dx)μt+1​(⋅)=∫p(⋅∣x,a,μt​)πt​(da∣x)μt​(dx). A pair (π,μ)(\pi,\mu)(π,μ) is a mean-field equilibrium if μ=Λ(π)\mu=\Lambda(\pi)μ=Λ(π) and π\piπ minimizes JμJ_\muJμ​ over all policies.

Assumption 1 asks for the following:

  • (a) ccc is continuous with ∥c∥≤K\|c\|\le K∥c∥≤K;
  • (b) ppp is weakly continuous in (x,a,μ)(x,a,\mu)(x,a,μ);
  • (c) A\mathsf AA is compact;
  • (d) there are α≥0\alpha\ge0α≥0 and a continuous moment function w≥1w\ge1w≥1 (compact sets Kn↑XK_n\uparrow\mathsf XKn​↑X with inf⁡x∉Knw(x)→∞\inf_{x\notin K_n}w(x)\to\inftyinfx∈/Kn​​w(x)→∞) with ∫w(y) p(dy∣x,a,μ)≤αw(x)\int w(y)\,p(dy|x,a,\mu)\le\alpha w(x)∫w(y)p(dy∣x,a,μ)≤αw(x);
  • (e) ∫w dμ0<∞\int w\,d\mu_0<\infty∫wdμ0​<∞.

Formalization targets

Goal: Theorem 1 (p. 10)

Under Assumption 1 there are a Markov policy π\piπ and a flow μ\muμ with

μ=Λ(π)andJμ(π)=inf⁡σ∈ΠJμ(σ).\mu=\Lambda(\pi)\qquad\text{and}\qquad J_\mu(\pi)=\inf_{\sigma\in\Pi}J_\mu(\sigma).μ=Λ(π)andJμ​(π)=σ∈Πinf​Jμ​(σ).

Milestones

In the paper's order of proof:

  1. Proposition 1: Markov policies achieve the optimal value.
  2. Lemmas 1–3: the finite- and infinite-horizon optimal value functions Jkn(⋅,λβk)J^n_k(\cdot,\lambda\beta^k)Jkn​(⋅,λβk) and Jk(⋅,λβk)J_k(\cdot,\lambda\beta^k)Jk​(⋅,λβk) of the nonhomogeneous MDP of a fixed flow are bounded and continuous. They satisfy the dynamic programming equation TkJk+1(⋅,λβk+1)=Jk(⋅,λβk)T_kJ_{k+1}(\cdot,\lambda\beta^{k+1})=J_k(\cdot,\lambda\beta^k)Tk​Jk+1​(⋅,λβk+1)=Jk​(⋅,λβk), and
∥Jkn(⋅,λβk)−Jk(⋅,λβk)∥≤λK1−βeλβkK1−ββn+1.\big\|J^n_k(\cdot,\lambda\beta^k)-J_k(\cdot,\lambda\beta^k)\big\|\le\frac{\lambda K}{1-\beta}e^{\frac{\lambda\beta^kK}{1-\beta}}\beta^{n+1}.​Jkn​(⋅,λβk)−Jk​(⋅,λβk)​≤1−βλK​e1−βλβkK​βn+1.
  1. Theorem 2: a Markov policy is optimal if and only if it almost surely selects minimizers in the dynamic programming equation.
  2. Propositions 2–5 and Lemma 4: equilibria are fixed points of a set-valued map Γ\GammaΓ on state–action flows in Ξ=∏t{ν:ν1(w)≤αtM}\Xi=\prod_t\{\nu:\nu_1(w)\le\alpha^tM\}Ξ=∏t​{ν:ν1​(w)≤αtM}; the optimal value functions depend continuously on the flow; and the graph of Γ\GammaΓ is closed in Ξ×Ξ\Xi\times\XiΞ×Ξ.

Significance

The result. Theorem 1 is what makes the second main result of the paper meaningful. That result, Theorem 3 and the second mission of this series, states that the equilibrium policy is an ε\varepsilonε-Markov–Nash equilibrium of every NNN-agent game with NNN large enough. Equilibria of finite risk-sensitive games with many agents are rarely computable, so a mean-field equilibrium gives an approximately optimal decentralized policy that ignores the other agents' states. Along the way, the paper proves results on nonhomogeneous risk-sensitive MDPs that it describes as "mostly absent and dispersed in the literature": uniform finite-to-infinite horizon bounds and a characterization of optimal Markov policies. These results are useful outside game theory.

Formalizing it. The result is proved on paper. No part of it, nor of the risk-neutral precursor, has a machine-checked proof. Formalization produces a verified theory of nonhomogeneous risk-sensitive MDPs on Polish spaces, a verified closed-graph argument for the mean-field map, and an exact record of the hypotheses. The paper omits or cites several steps: Proposition 1, Proposition 2, Lemma 2, the conditional optimality (8) and the nonemptiness and convexity of Γ(ν)\Gamma(\nu)Γ(ν). A formalization has to supply them.

Difficulty

The obvious route is Banach's fixed point theorem for the dynamic programming operator, as in risk-neutral discounted MDPs. It fails here: the cost is multiplicative, and the operator TkT_kTk​ is not a contraction. Uniform convergence of value iteration has to come from the explicit tail bound of Lemma 3 instead.

The second obstacle is the fixed point itself. The natural map, from a flow to the flows of its optimal policies, is set-valued and lives on an infinite product of spaces of measures. Kakutani–Fan–Glicksberg applies only after three steps:

  • re-encoding the problem on state–action flows (the map Γ=C∩B\Gamma=C\cap BΓ=C∩B);
  • proving compactness of Ξ\XiΞ through the moment function (tightness);
  • proving that the graph of Γ\GammaΓ is closed (Proposition 4).

The last step requires the optimal value functions to vary continuously with the flow (Proposition 5) and a portmanteau argument for sets defined by optimality conditions. None of this machinery (the Kakutani–Fan–Glicksberg theorem in locally convex spaces, Prokhorov compactness via moment functions, continuous convergence) is in Mathlib in the required form.

Formalization scope

P(E)\mathcal P(E)P(E) is a type synonym of Mathlib's ProbabilityMeasure E with the weak topology and its Borel σ-field. The kernel ppp is a Mathlib Kernel on X×A×P(X)\mathsf X\times\mathsf A\times\mathcal P(\mathsf X)X×A×P(X). Policies are sequences of Markov kernels, and history-dependent policies take (X×A)t×X(\mathsf X\times\mathsf A)^t\times\mathsf X(X×A)t×X as input. The law PπP^\piPπ is built with the Ionescu–Tulcea kernel Kernel.trajMeasure, one coordinate (x(t),a(t))(x(t),a(t))(x(t),a(t)) per time step. Time is 000-based.

Standing hypotheses on every statement:

  • X\mathsf XX and A\mathsf AA are Polish and Borel;
  • A\mathsf AA is compact and nonempty (used tacitly by the paper);
  • β∈(0,1)\beta\in(0,1)β∈(0,1), λ>0\lambda>0λ>0, and c≥0c\ge0c≥0 is measurable;
  • Assumption 1.

For §4.2 the pair (α,w)(\alpha,w)(α,w) defining Ξ\XiΞ is an explicit argument. In §4.1, "policy" means Markov policy, as the paper states on p. 11. The conditional expectations "given x(k)=xx(k)=xx(k)=x" are expectations for the chain started at time kkk in xxx. Lemma 1 is stated with ζk,n=∑t=knβt\zeta_{k,n}=\sum_{t=k}^n\beta^tζk,n​=∑t=kn​βt, the quantity its proof uses; the page prints ∑t=knβk\sum_{t=k}^n\beta^k∑t=kn​βk.

The goal asks for a Markov equilibrium policy that is optimal against all history-dependent policies, at least as strong as Definition 3. Optimality is "≤\le≤ the cost of every policy", not an infimum, so it has no junk case. The cost is a genuine integral: with c≥0c\ge0c≥0 bounded, the integrand lies in [1,eλK/(1−β)][1,e^{\lambda K/(1-\beta)}][1,eλK/(1−β)], so no policy is trivially optimal. The moment-function predicate has no infimum, so compact X\mathsf XX is admitted.

Contributions are welcome at every level:

  • risk-sensitive dynamic programming on Borel spaces (reusable for any MDP);
  • the Kakutani–Fan–Glicksberg theorem in locally convex spaces;
  • Prokhorov compactness from moment functions;
  • measurable selection and disintegration of state–action measures.

Selected references

  • N. Saldi, T. Başar, M. Raginsky, Discrete-time Risk-sensitive Mean-field Games, arXiv:1808.03929v2, 2018; published as Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games, Math. Oper. Res. 45(4), 2020. https://arxiv.org/abs/1808.03929
  • N. Saldi, T. Başar, M. Raginsky, Markov–Nash Equilibria in Mean-Field Games with Discounted Cost, SIAM J. Control Optim. 56(6), 2018. https://doi.org/10.1137/17M1112583
  • N. Bäuerle, U. Rieder, More Risk-Sensitive Markov Decision Processes, Math. Oper. Res. 39(1), 2014. https://doi.org/10.1287/moor.2013.0601
  • O. Hernández-Lerma, J. B. Lasserre, Discrete-Time Markov Control Processes: Basic Optimality Criteria, Springer, 1996. https://doi.org/10.1007/978-1-4612-0729-0
  • C. D. Aliprantis, K. C. Border, Infinite Dimensional Analysis, 3rd ed., Springer, 2006. https://doi.org/10.1007/3-540-29587-9
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Algorithmic Game TheoryGraph TheoryProbability·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes II: Large-Graph Limits of the Equilibrium Through the Laplacian Eigenvalue DistributionResearch Paper

Motivation

Mean field games describe large populations of agents who interact symmetrically: every agent sees the same average of all the others. Many populations interact instead along a network, where each agent responds only to its neighbours. Lacker and Soret (arXiv:2005.14102v2, 2021; Math. Oper. Res. 2022) study a linear-quadratic stochastic differential game on a finite graph that is simple enough to solve explicitly on every vertex-transitive graph, and then ask what happens to the equilibrium as the graph grows. The question is the network analogue of the classical convergence problem for mean field games: does the nnn-player equilibrium have a limit, and does that limit depend on the graph only through a small amount of information?

The answer of the paper is that the limit is governed by the empirical eigenvalue distribution of the graph Laplacian. Dense graph sequences (degrees tending to infinity) all have the same limit, the mean field game; sparse ones (bounded degrees) have limits that depend on the graph, through its spectrum. This mission formalizes that large-graph limit theorem, Theorem 2.6 of the paper. Mission I of the series formalizes the explicit equilibrium on a fixed transitive graph (Theorem 2.5), on which this mission builds.

Setting

Let GGG be a finite simple graph on vertex set {1,…,n}\{1,\dots,n\}{1,…,n} with adjacency matrix AGA_GAG​ and degree matrix DGD_GDG​. Its Laplacian is LG=DG−1AG−IL_G = D_G^{-1}A_G - ILG​=DG−1​AG​−I. GGG is transitive if every vertex can be mapped to every other one by a graph automorphism; such a graph is regular, of degree δ(G)\delta(G)δ(G), and LGL_GLG​ is then symmetric with eigenvalues λ1G,…,λnG∈[−2,0]\lambda^G_1,\dots,\lambda^G_n\in[-2,0]λ1G​,…,λnG​∈[−2,0]. The empirical eigenvalue distribution is μG=1n∑iδλiG\mu_G = \frac1n\sum_i\delta_{\lambda^G_i}μG​=n1​∑i​δλiG​​.

Fix a horizon T>0T>0T>0, a volatility σ>0\sigma>0σ>0 and a weight c>0c>0c>0. Player vvv controls the state

dXv(t)=αv(t,X(t)) dt+σ dWv(t),t∈[0,T],dX_v(t) = \alpha_v(t,\boldsymbol X(t))\,dt + \sigma\,dW_v(t),\qquad t\in[0,T],dXv​(t)=αv​(t,X(t))dt+σdWv​(t),t∈[0,T],

driven by independent Brownian motions, with Markovian feedback controls αv\alpha_vαv​, and pays

Jv=12 E[∫0T∣αv(t,X(t))∣2dt+c ∣Xv(T)−1deg⁡(v)∑u∼vXu(T)∣2].J_v = \tfrac12\,\mathbb E\Big[\int_0^T|\alpha_v(t,\boldsymbol X(t))|^2dt + c\,\Big|X_v(T) - \tfrac1{\deg(v)}\sum_{u\sim v}X_u(T)\Big|^2\Big].Jv​=21​E[∫0T​∣αv​(t,X(t))∣2dt+c​Xv​(T)−deg(v)1​u∼v∑​Xu​(T)​2].

On a transitive graph without isolated vertices, Theorem 2.5 gives an explicit Nash equilibrium: with QG(x)=det⁡(I−xLG)1/nQ_G(x) = \det(I - xL_G)^{1/n}QG​(x)=det(I−xLG​)1/n and fGf_GfG​ the solution of fG′=c QG′(fG)f_G' = c\,Q_G'(f_G)fG′​=cQG′​(fG​), fG(0)=0f_G(0) = 0fG​(0)=0 on [0,T][0,T][0,T], the feedback is αiG(t,x)=−ei⊤PG(t)x\alpha^G_i(t,\boldsymbol x) = -e_i^\top P_G(t)\boldsymbol xαiG​(t,x)=−ei⊤​PG​(t)x with PG(t)=−fG′(T−t)LG(I−fG(T−t)LG)−1P_G(t) = -f_G'(T-t)L_G(I - f_G(T-t)L_G)^{-1}PG​(t)=−fG′​(T−t)LG​(I−fG​(T−t)LG​)−1. The resulting equilibrium state process XG\boldsymbol X^GXG is Gaussian, and the value is Val(G)=1n∑vJv\mathrm{Val}(G) = \frac1n\sum_v J_vVal(G)=n1​∑v​Jv​.

For a probability measure μ\muμ define Qμ(x)=exp⁡∫[−2,0]log⁡(1−xλ) μ(dλ)Q_\mu(x) = \exp\int_{[-2,0]}\log(1-x\lambda)\,\mu(d\lambda)Qμ​(x)=exp∫[−2,0]​log(1−xλ)μ(dλ), so that QμG=QGQ_{\mu_G} = Q_GQμG​​=QG​.

Formalization targets

Goal: Theorem 2.6

Let (Gn)(G_n)(Gn​) be finite transitive graphs without isolated vertices, ∣Gn∣→∞|G_n|\to\infty∣Gn​∣→∞, with XGn(0)=0\boldsymbol X^{G_n}(0) = 0XGn​(0)=0, and suppose μGn→μ\mu_{G_n}\to\muμGn​​→μ weakly for a probability measure μ\muμ. Then (1) the ODE fμ′=c Qμ′(fμ)f_\mu' = c\,Q_\mu'(f_\mu)fμ′​=cQμ′​(fμ​), fμ(0)=0f_\mu(0) = 0fμ​(0)=0 has a unique solution on [0,T][0,T][0,T]; (2) for every vertex sequence knk_nkn​ and t∈[0,T]t\in[0,T]t∈[0,T],

Law(XknGn(t))→N(0,Vμ(t)),Vμ(t)=σ2∫0t∫[−2,0](1−λfμ(T−t)1−λfμ(T−s))2μ(dλ) ds;\mathrm{Law}\big(X^{G_n}_{k_n}(t)\big)\to\mathcal N\big(0,V_\mu(t)\big),\qquad V_\mu(t) = \sigma^2\int_0^t\int_{[-2,0]}\Big(\frac{1-\lambda f_\mu(T-t)}{1-\lambda f_\mu(T-s)}\Big)^2\mu(d\lambda)\,ds;Law(Xkn​Gn​​(t))→N(0,Vμ​(t)),Vμ​(t)=σ2∫0t​∫[−2,0]​(1−λfμ​(T−s)1−λfμ​(T−t)​)2μ(dλ)ds;

(3) the empirical measure 1∣Gn∣∑iδXiGn(t)\frac1{|G_n|}\sum_i\delta_{X^{G_n}_i(t)}∣Gn​∣1​∑i​δXiGn​​(t)​ converges weakly in probability to N(0,Vμ(t))\mathcal N(0,V_\mu(t))N(0,Vμ​(t)); (4)

lim⁡n→∞Val(Gn)=−σ22log⁡∫[−2,0]−λ1−λfμ(T) μ(dλ).\lim_{n\to\infty}\mathrm{Val}(G_n) = -\frac{\sigma^2}2\log\int_{[-2,0]}\frac{-\lambda}{1-\lambda f_\mu(T)}\,\mu(d\lambda).n→∞lim​Val(Gn​)=−2σ2​log∫[−2,0]​1−λfμ​(T)−λ​μ(dλ).

Milestones

The milestones are the statements the paper's proof (§3, §6, §7.1) relies on: the stability of fμf_\mufμ​ in μ\muμ (Proposition 3.2, last sentence); the finite-graph variance formula (2.7); monotonicity and concavity of fμf_\mufμ​ (Proposition 3.3, first sentence); correlation decay (Proposition 2.12) for distinct vertices; the relation between degrees and the spectral limit (Lemma 7.1); the Gaussian Poincaré bound (7.3) and the concentration (7.1) of the empirical measure; and the spectral form (2.9) of the value.

Significance

Theorem 2.6 reduces the large-population behaviour of a network game to one spectral object. For complete graphs μ=δ−1\mu = \delta_{-1}μ=δ−1​ and the limit is the mean field game; for sparse sequences such as cycles, tori, or random regular graphs, μ\muμ is a non-degenerate measure and the limiting variance and value differ from the mean field ones. The theorem thereby gives a quantitative criterion for when a mean field approximation of a network game is accurate, and it shows propagation of chaos in both regimes: in the dense case because interactions are weak, in the sparse case because typical players are far apart in the graph.

The result is proved in the paper; none of it has been machine-checked. A complete formalization requires a Lean account of Gaussian laws of linear SDEs with additive noise, of weak convergence of spectral measures of graph Laplacians, and of a Gaussian Poincaré inequality, none of which is currently in Mathlib in the needed form. Each of these is reusable well beyond this mission.

Difficulty

Parts (2) and (4) follow from the finite-graph formulas once fGn→fμf_{G_n}\to f_\mufGn​​→fμ​ uniformly, but that convergence requires stability of a nonlinear ODE whose vector field is defined through the spectral measure, uniformly over a class of measures. The harder step is (3). Convergence of one player's law does not imply convergence of the empirical measure: the players are correlated, and on sparse graphs every player has a bounded number of strong neighbours, so the correlations do not vanish uniformly. Bounding them requires an estimate that decays in the graph distance and in the degree, and combining it with the growth of graph balls, which is controlled differently in the dense and in the sparse regime. The usual mean field route is closed: unless the graph is complete, the state vector is not exchangeable, so propagation-of-chaos arguments based on exchangeability do not apply.

Formalization scope

The Lean development lives in namespace GraphLQGame.Asymptotics.

  • Vertices {1,…,n}\{1,\dots,n\}{1,…,n} are Fin n; a graph sequence is G : ∀ k, SimpleGraph (Fin (N k)) with Nk→∞N_k\to\inftyNk​→∞.
  • LGL_GLG​ is the random-walk Laplacian above, not Mathlib's lapMatrix. μG\mu_GμG​ is built from the real roots of the characteristic polynomial of LGL_GLG​, with multiplicity.
  • Weak convergence of measures on R\mathbb RR is convergence of ∫h dμk\int h\,d\mu_k∫hdμk​ for every bounded continuous hhh. Weak convergence in probability of the empirical measure is convergence in probability of ∫h dmGn(t)\int h\,dm^{G_n}(t)∫hdmGn​(t) for every bounded continuous hhh.
  • A state process is a pathwise strong solution of (2.1) on its own probability space, driven by a standard Brownian motion and adapted to its completed filtration. Statements about several graphs are statements about laws.
  • Costs are [0,∞][0,\infty][0,∞]-valued lower integrals; the value is computed after asserting finiteness.
  • In PGP_GPG​, fG′(T−t)f_G'(T-t)fG′​(T−t) is written as its ODE value c QG′(fG(T−t))c\,Q_G'(f_G(T-t))cQG′​(fG​(T−t)). ODE solutions are constrained on [0,T][0,T][0,T] (or on R+\mathbb R_+R+​ for Propositions 3.2 and 3.3), with uniqueness stated on that domain.
  • The Gaussian law N(0,V)\mathcal N(0,V)N(0,V) is gaussianReal 0 V.toNNReal; Vμ(t)≥0V_\mu(t)\ge0Vμ​(t)≥0.

The goal quantifies over every solution fGnf_{G_n}fGn​​, fμf_\mufμ​ and every equilibrium state process, and also asserts that the graph ODE solutions and the state processes exist, so it cannot be discharged vacuously. Proposition 2.12 is stated for distinct vertices: as printed, (2.17) is also claimed for u=vu = vu=v, where it fails on complete graphs of large degree; the off-diagonal case is the one the proof of Theorem 2.6 uses. Theorem 2.5 (mission I) is not restated here; a solver proves what is needed of it.

Contributions are welcome at every level: Gaussian laws of linear SDEs, spectral measures of graph matrices, ODE stability, a Gaussian Poincaré inequality, and the milestones themselves.

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; published in Math. Oper. Res., 2022, https://doi.org/10.1287/moor.2021.1179. https://arxiv.org/abs/2005.14102
  • F. Chung, Spectral Graph Theory, CBMS Regional Conference Series in Mathematics 92, AMS, 1997. https://doi.org/10.1090/cbms/092
  • S. Boucheron, G. Lugosi, P. Massart, Concentration Inequalities: A Nonasymptotic Theory of Independence, Oxford University Press, 2013 (Theorem 3.20, Gaussian Poincaré inequality). https://doi.org/10.1093/acprof:oso/9780199535255.001.0001
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I, Springer, 2018. https://doi.org/10.1007/978-3-319-58920-6
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Algorithmic Game TheoryGraph TheoryProbability·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes III: The Mean Field Game Control Is an ε-Nash Equilibrium on Any Finite Graph, With ε_v ∝ deg(v)^(-1/2)Research Paper

Why mean field approximations on graphs need a threshold

Mean field games (MFGs) describe the limit of symmetric stochastic differential games as the number of players tends to infinity, when every player interacts with the empirical distribution of all the others. Their main practical use is the converse direction: an equilibrium of the limiting game supplies a simple, decentralized control that is an approximate Nash equilibrium of the game with finitely many players. For the complete graph, where everybody interacts with everybody, this is classical, with the standard rate O(1/n)O(1/\sqrt n)O(1/n​) (Carmona and Delarue, Probabilistic Theory of Mean Field Games, Vol. II, §6.1; Huang, Malhamé and Caines 2006, Theorem 12), as recalled on p. 10 of the paper.

Many interacting systems are not complete graphs: players see only their neighbours in a network. The question is then how dense the network must be for the mean field approximation to remain valid. Lacker and Soret (arXiv:2005.14102v2) answer it exactly for a linear-quadratic "flocking" game, where explicit computations are possible. This mission formalizes their Theorem 2.11, which applies to every finite graph, with no transitivity or regularity assumed.

Setting

Let GGG be a finite simple graph on the vertex set V={1,…,n}V=\{1,\dots,n\}V={1,…,n}; u∼vu\sim vu∼v means uuu and vvv are adjacent and deg⁡G(v)\deg_G(v)degG​(v) is the number of neighbours of vvv. Fix a horizon T>0T>0T>0, a volatility σ>0\sigma>0σ>0 and a cost weight c>0c>0c>0. Each player v∈Vv\in Vv∈V controls a real state XvX_vXv​ through

dXv(t)=αv(t,X(t)) dt+σ dWv(t),t∈[0,T],dX_v(t)=\alpha_v(t,\boldsymbol X(t))\,dt+\sigma\,dW_v(t),\qquad t\in[0,T],dXv​(t)=αv​(t,X(t))dt+σdWv​(t),t∈[0,T],

where W1,…,WnW_1,\dots,W_nW1​,…,Wn​ are independent standard Brownian motions and X=(Xu)u∈V\boldsymbol X=(X_u)_{u\in V}X=(Xu​)u∈V​. A Markovian control αv∈AG\alpha_v\in\mathcal A_Gαv​∈AG​ is a Borel function of time and the full state X(t)∈RV\boldsymbol X(t)\in\mathbb R^VX(t)∈RV, of linear growth. The cost of player vvv under a profile α=(αu)u∈V\boldsymbol\alpha=(\alpha_u)_{u\in V}α=(αu​)u∈V​ is

Jv(α)=12 E[∫0T∣αv(t,X(t))∣2 dt+c ∣Xv(T)−1deg⁡G(v)∑u∼vXu(T)∣2],J_v(\boldsymbol\alpha)=\frac12\,\mathbb E\Big[\int_0^T|\alpha_v(t,\boldsymbol X(t))|^2\,dt+c\,\Big|X_v(T)-\frac1{\deg_G(v)}\sum_{u\sim v}X_u(T)\Big|^2\Big],Jv​(α)=21​E[∫0T​∣αv​(t,X(t))∣2dt+c​Xv​(T)−degG​(v)1​u∼v∑​Xu​(T)​2],

and 12E[∫0T∣αv∣2dt+c∣Xv(T)∣2]\frac12\mathbb E[\int_0^T|\alpha_v|^2dt+c|X_v(T)|^2]21​E[∫0T​∣αv​∣2dt+c∣Xv​(T)∣2] for an isolated vertex: each player wants to end near the average of its neighbours at minimal quadratic effort. For a vector ε∈R+V\boldsymbol\varepsilon\in\mathbb R^V_+ε∈R+V​, a profile is a Markovian ε\boldsymbol\varepsilonε-Nash equilibrium if no player vvv can lower its cost by more than εv\varepsilon_vεv​ by switching unilaterally to another control β∈AG\beta\in\mathcal A_Gβ∈AG​, written (β,α−v)(\beta,\boldsymbol\alpha^{-v})(β,α−v).

The mean-field control is

αMF(t,y)=−cy1+c(T−t),αvMF(t,x)=αMF(t,xv):\alpha^{\mathrm{MF}}(t,y)=\frac{-cy}{1+c(T-t)},\qquad \alpha^{\mathrm{MF}}_v(t,\boldsymbol x)=\alpha^{\mathrm{MF}}(t,x_v):αMF(t,y)=1+c(T−t)−cy​,αvMF​(t,x)=αMF(t,xv​):

each player looks only at its own state, as if its neighbours' average were frozen at its mean.

Formalization targets

Goal: Theorem 2.11

Define ϵvG=σ2cT1+cTcT(2+cT)deg⁡G(v)\epsilon^G_v=\sigma^2\frac{cT}{1+cT}\sqrt{\frac{cT(2+cT)}{\deg_G(v)}}ϵvG​=σ21+cTcT​degG​(v)cT(2+cT)​​ if deg⁡G(v)≥1\deg_G(v)\ge1degG​(v)≥1 and ϵvG=0\epsilon^G_v=0ϵvG​=0 if deg⁡G(v)=0\deg_G(v)=0degG​(v)=0, and with the minimal degree δ(G)=min⁡vdeg⁡G(v)\delta(G)=\min_v\deg_G(v)δ(G)=minv​degG​(v),

ϵG=σ2cT1+cTcT(2+cT)1∨δ(G).\epsilon_G=\sigma^2\frac{cT}{1+cT}\sqrt{\frac{cT(2+cT)}{1\vee\delta(G)}}.ϵG​=σ21+cTcT​1∨δ(G)cT(2+cT)​​.

Then, with zero initial states, the state equation for (αvMF)v∈V(\alpha^{\mathrm{MF}}_v)_{v\in V}(αvMF​)v∈V​ has a solution, and

(αvMF)v∈V is an ϵG-Nash equilibrium and an ϵG-Nash equilibrium on G.(\alpha^{\mathrm{MF}}_v)_{v\in V}\ \text{is an } \epsilon^G\text{-Nash equilibrium and an } \epsilon_G\text{-Nash equilibrium on } G.(αvMF​)v∈V​ is an ϵG-Nash equilibrium and an ϵG​-Nash equilibrium on G.

Milestones

  1. Lemma 7.2: αMF\alpha^{\mathrm{MF}}αMF is optimal for the one-player problem min⁡12E[∫0Tβ2dt+c∣Y(T)∣2]\min\frac12\mathbb E[\int_0^T\beta^2dt+c|Y(T)|^2]min21​E[∫0T​β2dt+c∣Y(T)∣2], dY=β dt+σdWdY=\beta\,dt+\sigma dWdY=βdt+σdW, over all progressively measurable β\betaβ.
  2. Isolated vertices (p. 40): Jv(α)=inf⁡βJv(β,α−v)J_v(\boldsymbol\alpha)=\inf_\beta J_v(\beta,\boldsymbol\alpha^{-v})Jv​(α)=infβ​Jv​(β,α−v) when deg⁡G(v)=0\deg_G(v)=0degG​(v)=0.
  3. (7.7): under αMF\alpha^{\mathrm{MF}}αMF, (Xu(T))u(X_u(T))_u(Xu​(T))u​ are i.i.d. N(0,σ2T/(1+cT))N(0,\sigma^2T/(1+cT))N(0,σ2T/(1+cT)), so the neighbour average has second moment σ2T/(deg⁡G(v)(1+cT))\sigma^2T/(\deg_G(v)(1+cT))σ2T/(degG​(v)(1+cT)).
  4. Steps (1), (2), (3) (p. 41): a lower bound on Jv(β,α−v)J_v(\beta,\boldsymbol\alpha^{-v})Jv​(β,α−v), an energy bound for deviations no worse than the zero control, and the comparison with Jv(αMF)J_v(\boldsymbol\alpha^{\mathrm{MF}})Jv​(αMF).
  5. (7.5): for deg⁡G(v)≥1\deg_G(v)\ge1degG​(v)≥1 and every admissible β\betaβ, Jv(β,α−v)≥Jv(α)−ϵvGJ_v(\beta,\boldsymbol\alpha^{-v})\ge J_v(\boldsymbol\alpha)-\epsilon^G_vJv​(β,α−v)≥Jv​(α)−ϵvG​.

Significance

The result. Theorem 2.11 gives an explicit threshold for the mean field approximation on networks: along any sequence of graphs whose minimal degree diverges, the decentralized control αMF\alpha^{\mathrm{MF}}αMF is an ϵGn\epsilon_{G_n}ϵGn​​-Nash equilibrium with ϵGn→0\epsilon_{G_n}\to0ϵGn​​→0, and the vector form says more: if the average of (1∨deg⁡Gn(v))−1/2(1\vee\deg_{G_n}(v))^{-1/2}(1∨degGn​​(v))−1/2 over vertices tends to zero, the per-player errors vanish on average (the paper's (2.16)). The rate deg⁡G(v)−1/2\deg_G(v)^{-1/2}degG​(v)−1/2 quantifies how the accuracy of the approximation depends on denseness. In the same paper, transitive graphs whose degrees stay bounded lead to equilibria that do not agree with the mean field one, so a denseness condition cannot be dropped.

Formalizing it. The theorem is proved in the paper; to our knowledge no part of it is machine-checked. A formal development needs, beyond the statement, a verification argument for a one-dimensional linear-quadratic control problem with additive noise, Gaussian computations for linear SDEs driven by Brownian motion, and the comparison of costs between the equilibrium system and a system with one deviating player. The one-player result (Lemma 7.2) and the Gaussian facts of (7.7) are reusable well beyond this mission.

Difficulty

The obvious argument compares a deviating player with an isolated player and treats the neighbour average as noise independent of the deviation. Two things stand in the way. The cost of player vvv couples its terminal state with the neighbours' average through a cross term E[1deg⁡G(v)∑u∼vXu(T) Yv(T)]\mathbb E[\frac1{\deg_G(v)}\sum_{u\sim v}X_u(T)\,Y_v(T)]E[degG​(v)1​∑u∼v​Xu​(T)Yv​(T)], and the deviation β(t,Y(t))\beta(t,\boldsymbol Y(t))β(t,Y(t)) may look at the neighbours' states, so the cross term does not vanish; it has to be bounded through the size of the deviation's energy. And an arbitrary deviation has no a priori energy bound: one is available only for deviations that do at least as well as the zero control, which is why the argument passes through a (near-)optimal deviation. Lemma 7.2 itself requires a verification theorem over all progressively measurable controls, not only feedback ones.

Formalization scope

The Lean development lives in the namespace GraphLQGame.DenseApprox and uses the shared encoding of this series:

  • vertices are Fin n (the paper's {1,…,n}\{1,\dots,n\}{1,…,n} become {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}), the state space is EthierKurtz.SDEState n, and GGG is any SimpleGraph (Fin n); isolated vertices are allowed;
  • controls are Borel with linear growth on [0,T][0,T][0,T] only; their values at other times are never used, and the formula for αMF\alpha^{\mathrm{MF}}αMF outside [0,T][0,T][0,T] is evaluated with Lean's total division;
  • a solution of the state equation is a pathwise strong solution carrying its own probability space and an nnn-dimensional standard Brownian motion; costs are [0,∞][0,\infty][0,∞]-valued lower Lebesgue integrals, and the Nash inequality is required for every solution of the profile and of each deviation (faithful by strong uniqueness);
  • T,σ,c>0T,\sigma,c>0T,σ,c>0 are the standing assumptions of §2.1;
  • initial states are zero. The printed theorem does not mention X(0)X(0)X(0); the paper fixes non-random initial states that are "in many cases" zero, and the whole proof is for X(0)=0X(0)=0X(0)=0. With non-zero initial states the claim fails in general, so this is a disclosed hypothesis;
  • the goal also asserts that the state equation for αMF\alpha^{\mathrm{MF}}αMF has a solution, so the Nash property cannot hold vacuously; Lemma 7.2 is stated over every continuous adapted solution of its SDE, and Step (2) carries, as an explicit hypothesis, the comparison with the zero control that its proof uses.

A formalization in which αMF\alpha^{\mathrm{MF}}αMF is compared only with deviations depending on the player's own state, or in which the costs are Bochner integrals that vanish when not integrable, would be trivially or wrongly satisfied; both are ruled out by the encoding above.

Welcome contributions: the verification argument for Lemma 7.2, the Gaussian law of linear SDEs with additive noise, and proofs of the three steps. Related missions in this series: I (an explicit Nash equilibrium on transitive graphs) and II (large-graph limits).

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; Math. Oper. Res. 47 (2022). https://arxiv.org/abs/2005.14102
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications II, Springer, 2018. https://doi.org/10.1007/978-3-319-56436-4
  • M. Huang, R. P. Malhamé, P. E. Caines, Large population stochastic dynamic games: closed-loop McKean–Vlasov systems and the Nash certainty equivalence principle, Commun. Inf. Syst. 6 (2006), 221–252. https://doi.org/10.4310/CIS.2006.v6.n3.a5
  • H. Pham, Continuous-time Stochastic Control and Optimization with Financial Applications, Springer, 2009 (verification theorem, Theorem 3.5.2). https://doi.org/10.1007/978-3-540-89500-8
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Algorithmic Game TheoryGraph TheoryProbability·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes I: An Explicit Markovian Nash Equilibrium on Every Finite Transitive GraphResearch Paper

Motivation

Mean field games describe Nash equilibria of large populations in which every player interacts with every other player symmetrically, through the empirical distribution of all states. Many systems of interest are not of this kind: agents in a network interact only with their neighbours, and the interaction structure is a graph rather than a complete graph. Understanding when equilibria on large graphs behave like mean field equilibria, and when they do not, requires models in which the equilibrium on a finite graph can be computed exactly.

Lacker and Soret (arXiv:2005.14102v2, Math. Oper. Res. 2022) introduced such a model: a linear–quadratic flocking game on an arbitrary finite graph, in which each player steers a Brownian particle and pays a terminal penalty for being far from the average of her neighbours. For vertex-transitive graphs they solved the game in closed form, up to a scalar ODE, with an equilibrium that depends on the graph only through the spectrum of its Laplacian. This mission formalizes that finite-graph result, Theorem 2.5 of the paper. Its large-graph consequences are the subject of missions II and III of this series.

Setting

Let GGG be a finite simple graph on vertices V={1,…,n}V=\{1,\dots,n\}V={1,…,n}, with adjacency matrix AGA_GAG​ and degree matrix DGD_GDG​. When GGG has no isolated vertices its random-walk Laplacian is

LG:=DG−1AG−I.L_G := D_G^{-1}A_G - I .LG​:=DG−1​AG​−I.

GGG is transitive if for every two vertices u,vu,vu,v there is a graph automorphism mapping uuu to vvv. A transitive graph is regular, so its Laplacian LG=AG/δ(G)−IL_G = A_G/\delta(G) - ILG​=AG​/δ(G)−I is symmetric, with eigenvalues in [−2,0][-2,0][−2,0].

Fix a horizon T>0T>0T>0, a noise level σ>0\sigma>0σ>0 and a cost constant c>0c>0c>0. Each vertex vvv is a player with state

dXv(t)=αv(t,X(t)) dt+σ dWv(t),t∈[0,T],dX_v(t) = \alpha_v(t,X(t))\,dt + \sigma\,dW_v(t),\qquad t\in[0,T],dXv​(t)=αv​(t,X(t))dt+σdWv​(t),t∈[0,T],

driven by independent Brownian motions WvW_vWv​, from a non-random initial state X(0)=x0∈RVX(0)=x_0\in\mathbb R^VX(0)=x0​∈RV. A Markovian control αv\alpha_vαv​ is a Borel function of time and the full state vector with at most linear growth. Player vvv minimises

Jv=12 E[∫0T∣αv(t,X(t))∣2 dt+c ∣Xv(T)−1deg⁡(v)∑u∼vXu(T)∣2].J_v = \tfrac12\,\mathbb E\Big[\int_0^T|\alpha_v(t,X(t))|^2\,dt + c\,\Big|X_v(T)-\frac{1}{\deg(v)}\sum_{u\sim v}X_u(T)\Big|^2\Big].Jv​=21​E[∫0T​∣αv​(t,X(t))∣2dt+c​Xv​(T)−deg(v)1​u∼v∑​Xu​(T)​2].

A profile (αv)v(\alpha_v)_v(αv​)v​ is a Markovian Nash equilibrium if no player can lower her cost by switching unilaterally to another Markovian control.

The equilibrium is built from

QG(x):=det⁡(I−xLG)1/n,fG′(t)=c QG′(fG(t)), fG(0)=0,Q_G(x) := \det(I-xL_G)^{1/n},\qquad f_G'(t) = c\,Q_G'(f_G(t)),\ f_G(0)=0,QG​(x):=det(I−xLG​)1/n,fG′​(t)=cQG′​(fG​(t)), fG​(0)=0, PG(t):=−fG′(T−t) LG(I−fG(T−t)LG)−1,αiG(t,x):=−ei⊤PG(t)x.P_G(t) := -f_G'(T-t)\,L_G\big(I-f_G(T-t)L_G\big)^{-1},\qquad \alpha^G_i(t,x) := -e_i^\top P_G(t)x .PG​(t):=−fG′​(T−t)LG​(I−fG​(T−t)LG​)−1,αiG​(t,x):=−ei⊤​PG​(t)x.

Formalization targets

Goal: Theorem 2.5

For a finite transitive graph GGG without isolated vertices:

  1. QGQ_GQG​ is well defined and continuously differentiable on R+\mathbb R_+R+​, and the ODE has a unique solution fG:[0,T]→R+f_G:[0,T]\to\mathbb R_+fG​:[0,T]→R+​.
  2. (αiG)i(\alpha^G_i)_i(αiG​)i​ is a Markovian Nash equilibrium for every initial state.
  3. For every t∈(0,T]t\in(0,T]t∈(0,T], the equilibrium state X(t)X(t)X(t) is Gaussian with
EX(t)=(I−fG(T−t)LG)(I−fG(T)LG)−1x0,Cov X(t)=σ2(I−fG(T−t)LG)2∫0t(I−fG(T−s)LG)−2 ds.\mathbb E X(t) = (I-f_G(T-t)L_G)(I-f_G(T)L_G)^{-1}x_0,\qquad \mathrm{Cov}\,X(t) = \sigma^2(I-f_G(T-t)L_G)^2\int_0^t(I-f_G(T-s)L_G)^{-2}\,ds .EX(t)=(I−fG​(T−t)LG​)(I−fG​(T)LG​)−1x0​,CovX(t)=σ2(I−fG​(T−t)LG​)2∫0t​(I−fG​(T−s)LG​)−2ds.
  1. The average equilibrium cost satisfies
1n∑vJv=∣PG(0)x0∣22 Tr PG(0)−σ22log⁡Tr PG(0)n fG′(T).\frac1n\sum_{v}J_v = \frac{|P_G(0)x_0|^2}{2\,\mathrm{Tr}\,P_G(0)} - \frac{\sigma^2}{2}\log\frac{\mathrm{Tr}\,P_G(0)}{n\,f_G'(T)} .n1​v∑​Jv​=2TrPG​(0)∣PG​(0)x0​∣2​−2σ2​lognfG′​(T)TrPG​(0)​.

All four parts are in the goal statement.

Milestones

The milestones follow the paper's proof in §2.2, §3 and §4.

  • Graph-spectral facts. Transitive graphs are regular with symmetric LGL_GLG​ (§2.2). The spectrum of LGL_GLG​ lies in [−2,0][-2,0][−2,0] (Remark 2.4). The eigenvalue distribution μG\mu_GμG​ has mean −1-1−1 ((3.2)), and QG=QμGQ_G = Q_{\mu_G}QG​=QμG​​ (§2.3).
  • The ODE. Bounds on QμQ_\muQμ​ and its first two derivatives (Proposition 3.1), and well-posedness of fμ′=cQμ′(fμ)f_\mu' = cQ_\mu'(f_\mu)fμ′​=cQμ′​(fμ​) with explicit bounds (Proposition 3.2).
  • Symmetry. Commutation of LGL_GLG​ with automorphism matrices, and constancy of the diagonal of equivariant matrices (Lemma 4.1).
  • The Riccati system. The properties of PG(t)P_G(t)PG​(t) (§4.4 (i)–(iii)), the reduction of the Nash PDE system to matrix Riccati equations (Lemma 4.2), and the verification that the explicit Fi=(Tr P/n)−1Peiei⊤PF^i = (\mathrm{Tr}\,P/n)^{-1}Pe_ie_i^\top PFi=(TrP/n)−1Pei​ei⊤​P solve them (§4.4).
  • Law and value. The fundamental matrix exp⁡(−∫stP)=(I−f(T−t)L)(I−f(T−s)L)−1\exp(-\int_s^tP) = (I-f(T-t)L)(I-f(T-s)L)^{-1}exp(−∫st​P)=(I−f(T−t)L)(I−f(T−s)L)−1 (§4.5) and the averaged value identity (§4.6).

Significance

The result. Theorem 2.5 is one of the few explicit Nash equilibria of a stochastic differential game on a non-complete graph. Two features of it are not visible in mean field theory. The equilibrium controls are nonlocal: each player reacts to the whole state vector, not only to her neighbours. The whole equilibrium (law, value, controls) depends on the graph only through the spectrum of LGL_GLG​. The second feature drives the paper's later results. Weak convergence of the eigenvalue distributions μGn\mu_{G_n}μGn​​ yields limits of the equilibrium, and these separate the dense regime, where the mean field approximation is valid, from the sparse regime, where it is not.

Formalizing it. The result is proved in the paper; nothing here is open. No machine-checked version of it or of its ingredients exists: the random-walk Laplacian of a graph, linear–quadratic stochastic differential games, verification theorems for Nash systems, and Gaussian laws of linear SDEs with time-dependent coefficients. The mission produces a checked statement of the equilibrium together with reusable layers: spectral facts about D−1A−ID^{-1}A - ID−1A−I, an ODE analysis for QμQ_\muQμ​, and a Riccati reduction for quadratic Nash systems.

Difficulty

Three steps resist a direct approach.

  • The verification theorem. The paper passes from a classical solution of the Nash system (4.1) to a Nash equilibrium by appeal to a standard verification argument. Over the full class of Borel controls with linear growth, this requires Itô's formula for the quadratic value functions, together with integrability of the deviated state processes.
  • The Riccati system. The nnn coupled matrix equations (4.6) have no general closed-form solution. The explicit solution exists only because transitivity forces ei⊤P(t)ei=Tr(P(t))/ne_i^\top P(t)e_i = \mathrm{Tr}(P(t))/nei⊤​P(t)ei​=Tr(P(t))/n for every iii. That identity has to be derived from the action of the automorphism group (Lemma 4.1), not from regularity alone.
  • The law of the state. It requires solving a linear SDE with a time-dependent matrix and identifying its Gaussian law, a step for which the library has little support.

Formalization scope

Lean conventions:

  • Vertices. The vertex set is Fin n, so the paper's 1,…,n1,\dots,n1,…,n become 0,…,n−10,\dots,n-10,…,n−1. The state space is the platform's EthierKurtz.SDEState n (Euclidean Rn\mathbb R^nRn).
  • The Laplacian. LGL_GLG​ is the random-walk Laplacian D−1A−ID^{-1}A-ID−1A−I, not Mathlib's D−AD-AD−A.
  • Time and controls. Time is real. Controls are Borel on R×Rn\mathbb R\times\mathbb R^nR×Rn with linear growth on [0,T][0,T][0,T]; their values off [0,T][0,T][0,T] are never used.
  • Solutions of (2.1). A solution is a pathwise strong solution on a probability space that the solution itself carries, adapted to the completed Brownian filtration. Costs are compared across solutions; this is faithful because (2.1) has a unique strong solution.
  • Costs are [0,∞][0,\infty][0,∞]-valued lower Lebesgue integrals. They are converted to reals only after their finiteness is asserted.
  • Existence of the equilibrium state. The goal also asserts that the equilibrium state equation has a solution, so that the Nash property cannot hold vacuously.
  • Derivatives. fG′(T−t)f_G'(T-t)fG′​(T−t) is written as its ODE value cQG′(fG(T−t))cQ_G'(f_G(T-t))cQG′​(fG​(T−t)). The ODE is solved on [0,T][0,T][0,T] with one-sided derivatives at the endpoints, and uniqueness is agreement on [0,T][0,T][0,T].
  • Matrix conventions. Covariance integrals are entrywise. Gaussian laws are Mathlib's multivariateGaussian.
  • Added hypotheses. 0<n0<n0<n is added to three milestones that are false on the empty graph.

A formalization that fixes x0=0x_0=0x0​=0, restricts deviations to linear controls, drops the existence of the equilibrium state process, or replaces LGL_GLG​ by D−AD-AD−A is not this theorem.

Infrastructure that a complete development needs:

  • symmetric-matrix spectral calculus for LGL_GLG​ and for the matrix functions (I−xL)−1(I-xL)^{-1}(I−xL)−1 and log⁡(I−xL)\log(I-xL)log(I−xL);
  • differentiation under the integral for QμQ_\muQμ​;
  • Picard–Lindelöf and Grönwall on R+\mathbb R_+R+​;
  • Itô's formula for quadratic functions of a diffusion with additive noise;
  • the Gaussian law of ∫0tM(t,s) dWs\int_0^t M(t,s)\,dW_s∫0t​M(t,s)dWs​ for deterministic MMM.

The spectral, ODE and Riccati layers are reusable beyond this mission. Proofs of individual milestones are welcome; so are general verification theorems for linear–quadratic games.

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; Math. Oper. Res. 47(2), 2022. https://arxiv.org/abs/2005.14102
  • F. Chung, Spectral Graph Theory, CBMS Regional Conference Series in Mathematics 92, AMS, 1997. https://doi.org/10.1090/cbms/092
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I, Springer, 2018. https://doi.org/10.1007/978-3-319-58920-6
  • A. Veretennikov, On strong solutions and explicit formulas for solutions of stochastic integral equations, Math. USSR-Sb. 39(3), 1981. https://doi.org/10.1070/SM1981v039n03ABEH001522
21 thms1 active userReviewed
Control TheoryOptimizationProbability·Captain: mikedeng1

Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 1: The Cost Is Uniformly Convex iff the Riccati Equation Has a Strongly Regular SolutionResearch Paper

Motivation

The stochastic linear quadratic (LQ) optimal control problem asks to steer a linear stochastic differential equation by a control so as to minimize a quadratic cost. It is the basic model of stochastic control: Wonham studied it in 1968 (Wonham 1968), and it is the model on which feedback design, mean-field control and LQ differential games are built (Yong–Zhou 1999).

Classically the cost weights are assumed nonnegative and the control weight RRR uniformly positive definite, the standard conditions (1.4). Under them the Riccati equation has a unique solution and the optimal control is a linear state feedback. A stochastic problem can however be well posed when RRR is indefinite, because the diffusion term also penalizes the control.

Timeline:

  • 1998: Chen, Li and Zhou observe that a stochastic LQ problem can be solvable with an indefinite RRR (SIAM J. Control Optim. 36).
  • 2002: Ait Rami, Moore and Zhou introduce a generalized Riccati equation with a pseudoinverse and algebraic constraints (SIAM J. Control Optim. 40).
  • 2014: Sun and Yong prove that closed-loop solvability is equivalent to the existence of a regular solution of that Riccati equation (SIAM J. Control Optim. 52).
  • 2016: Sun, Li and Yong characterize strongly regular solvability by the uniform convexity of the cost functional (SIAM J. Control Optim. 54, Theorem 4.5). This mission is that theorem.

Setting

A probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) carries a standard one-dimensional Brownian motion WWW. Its natural filtration, augmented by the P\mathbb PP-null sets, is F\mathbb FF. Fix a horizon T>0T>0T>0 and deterministic coefficients A,C∈Rn×nA,C\in\mathbb R^{n\times n}A,C∈Rn×n, B,D∈Rn×mB,D\in\mathbb R^{n\times m}B,D∈Rn×m, weights Q∈SnQ\in\mathbb S^nQ∈Sn, S∈Rm×nS\in\mathbb R^{m\times n}S∈Rm×n, R∈SmR\in\mathbb S^mR∈Sm (functions of time) and G∈SnG\in\mathbb S^nG∈Sn. The admissible controls U[t,T]\mathcal U[t,T]U[t,T] are the F\mathbb FF-progressively measurable processes uuu with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞. The state from the initial pair (t,x)(t,x)(t,x) solves

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x,dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x,dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x,

and the cost is

J(t,x;u)=E{⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT[⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩]ds}.J(t,x;u)=\mathbb E\Big\{\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle+\int_t^T\big[\langle QX,X\rangle+2\langle SX,u\rangle+\langle Ru,u\rangle+2\langle q,X\rangle+2\langle\rho,u\rangle\big]ds\Big\}.J(t,x;u)=E{⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT​[⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩]ds}.

Standing assumptions (H1)–(H2): A∈L1A\in L^1A∈L1, B,C∈L2B,C\in L^2B,C∈L2, D∈L∞D\in L^\inftyD∈L∞, Q∈L1Q\in L^1Q∈L1, S∈L2S\in L^2S∈L2, R∈L∞R\in L^\inftyR∈L∞ on (0,T)(0,T)(0,T), and square-integrability of the random terms b,σ,q,ρ,gb,\sigma,q,\rho,gb,σ,q,ρ,g. No sign condition is imposed on GGG, QQQ or RRR. The homogeneous problem (SLQ)0^00 sets b,σ,g,q,ρ=0b,\sigma,g,q,\rho=0b,σ,g,q,ρ=0; its cost is J0J^0J0.

The map u↦J0(0,0;u)u\mapsto J^0(0,0;u)u↦J0(0,0;u) is uniformly convex if, for some λ>0\lambda>0λ>0,

J0(0,0;u) ≥ λ E∫0T∣u(s)∣2ds∀u∈U[0,T].(4.2)J^0(0,0;u)\ \ge\ \lambda\,\mathbb E\int_0^T|u(s)|^2ds\qquad\forall u\in\mathcal U[0,T].\qquad(4.2)J0(0,0;u) ≥ λE∫0T​∣u(s)∣2ds∀u∈U[0,T].(4.2)

With ΣP=R+D⊤PD\Sigma_P=R+D^\top PDΣP​=R+D⊤PD and KP=B⊤P+D⊤PC+SK_P=B^\top P+D^\top PC+SKP​=B⊤P+D⊤PC+S, the Riccati equation is

P˙+PA+A⊤P+C⊤PC+Q−KP⊤ΣP†KP=0,P(T)=G,(4.6)\dot P+PA+A^\top P+C^\top PC+Q-K_P^\top\Sigma_P^\dagger K_P=0,\qquad P(T)=G,\qquad(4.6)P˙+PA+A⊤P+C⊤PC+Q−KP⊤​ΣP†​KP​=0,P(T)=G,(4.6)

with †\dagger† the Moore–Penrose pseudoinverse. A solution P∈C([0,T];Sn)P\in C([0,T];\mathbb S^n)P∈C([0,T];Sn) is strongly regular if ΣP≥λI\Sigma_P\ge\lambda IΣP​≥λI a.e. for some λ>0\lambda>0λ>0 (4.10).

Formalization targets

Goal: Theorem 4.5

∃λ>0: J0(0,0;u)≥λ E ⁣∫0T ⁣∣u∣2ds  ∀u∈U[0,T]  ⟺  (4.6) admits a strongly regular solution.\exists\lambda>0:\ J^0(0,0;u)\ge\lambda\,\mathbb E\!\int_0^T\!|u|^2ds\ \ \forall u\in\mathcal U[0,T]\iff(4.6)\text{ admits a strongly regular solution.}∃λ>0: J0(0,0;u)≥λE∫0T​∣u∣2ds  ∀u∈U[0,T]⟺(4.6) admits a strongly regular solution.

The goal fixes no constant: the λ\lambdaλ on each side is existential.

Milestones

  1. Lemma 2.2: the cost of a feedback control ΘX+u\Theta X+uΘX+u, written through the solution of a Lyapunov equation.
  2. Lemma 2.3: u↦u−ΘX(u)u\mapsto u-\Theta X^{(u)}u↦u−ΘX(u) is bounded below, E∫∣u−ΘX(u)∣2≥γ E∫∣u∣2\mathbb E\int|u-\Theta X^{(u)}|^2\ge\gamma\,\mathbb E\int|u|^2E∫∣u−ΘX(u)∣2≥γE∫∣u∣2.
  3. Proposition 4.1: uniform convexity gives unique open-loop solvability and V0(t,x)≥α∣x∣2V^0(t,x)\ge\alpha|x|^2V0(t,x)≥α∣x∣2.
  4. Proposition 4.4: every Lyapunov solution satisfies R+D⊤PD≥λIR+D^\top PD\ge\lambda IR+D⊤PD≥λI and P≥αIP\ge\alpha IP≥αI, with the same λ,α\lambda,\alphaλ,α.
  5. (4.20) and the monotonicity P1≥Pi≥Pi+1≥αIP_1\ge P_i\ge P_{i+1}\ge\alpha IP1​≥Pi​≥Pi+1​≥αI of the iteration (4.18)–(4.19).
  6. Uniform convergence of the iteration to a strongly regular solution.
  7. The completion of squares J0(0,0;u)=E∫⟨ΣP(u−ΘX(u)),u−ΘX(u)⟩dsJ^0(0,0;u)=\mathbb E\int\langle\Sigma_P(u-\Theta X^{(u)}),u-\Theta X^{(u)}\rangle dsJ0(0,0;u)=E∫⟨ΣP​(u−ΘX(u)),u−ΘX(u)⟩ds.

Companion items: Remark 4.6 (the same λ\lambdaλ bounds ΣP\Sigma_PΣP​), the well-posedness of the state equation and the cost (Sun–Yong 2014, Proposition 2.1), and Proposition 3.5 (the standard conditions (1.4) imply uniform convexity).

Significance

Theorem 4.5 gives a checkable sufficient condition for the classical structure of LQ control: under (4.2) the Riccati equation has a solution whose gain matrix R+D⊤PDR+D^\top PDR+D⊤PD is uniformly positive definite, so the optimal control is a state feedback with an invertible gain. It covers indefinite weights, and Proposition 3.5 shows that it contains the classical case (1.4). Combined with Sun–Yong's equivalence it yields Corollary 4.7, the feedback representation of the open-loop optimal control, which later missions of this series use.

The results are proved in the paper. As far as is known they have no machine-checked proof. Formalizing them requires stochastic calculus for controlled SDEs (Itô's formula for quadratic forms of a state process) linked to matrix ODE theory. The definitions this mission fixes (the LQ problem, the Riccati and Lyapunov equations with a pseudoinverse) can be reused by the other missions of the series and by any stochastic LQ formalization.

Difficulty

The direction (ii) ⇒ (i) is a completion of squares followed by Lemma 2.3. Lemma 2.3 is not obvious: it asserts a bounded inverse for an operator defined through an SDE.

The direction (i) ⇒ (ii) is the hard one. The obvious approach would solve (4.6) directly, but (4.6) is nonlinear and its coefficient ΣP†\Sigma_P^\daggerΣP†​ may be singular. No sign condition gives a priori bounds. The paper instead builds a policy-iteration sequence of linear Lyapunov equations. The difficulty is to show that every iterate keeps R+D⊤PiD≥λIR+D^\top P_iD\ge\lambda IR+D⊤Pi​D≥λI, so that the next gain is defined, and stays bounded below. These bounds come from the cost functional (Proposition 4.4), not from the matrix equation. Uniform convergence of the iterates then needs integrable estimates under the weak integrability of (H1).

Formalization scope

  • Basis. The paper's (Ω,F,P,W)(\Omega,\mathcal F,\mathbb P,W)(Ω,F,P,W) is a probability measure with a standard Brownian motion IsStdBrownian (Mathlib's IsBrownianReal per coordinate, published module Peng1990.SMP.Stochastic). F\mathbb FF is augmentedFiltration (published ReflectedBSDE.Existence.Setting).
  • State and cost. The state from (t,x)(t,x)(t,x) is an Itô solution from time 000 whose coefficients are switched on at ttt, with continuous paths and Esup⁡∣X∣2<∞\mathbb E\sup|X|^2<\inftyEsup∣X∣2<∞. JJJ is evaluated along a chosen solution, which is unique; the item state_wellposed poses existence, uniqueness and integrability of the cost. Expectations are Bochner integrals, and ∣u∣2|u|^2∣u∣2 is the Euclidean u⋅uu\cdot uu⋅u.
  • Integrability and values. LpL^pLp conditions on matrix functions are entrywise. The diffusion coefficients C,DC,DC,D are taken Borel measurable on [0,∞)[0,\infty)[0,∞) (a measurable representative of their class), so that the Itô integrand CX+Du+σCX+Du+\sigmaCX+Du+σ of (1.1) is progressively measurable. VVV is an EReal infimum over admissible controls.
  • Matrix ODEs. The Riccati and Lyapunov equations are in integral form: continuous symmetric PPP, an integrable right-hand side, and P(t)=G+∫tTF(s,P(s))dsP(t)=G+\int_t^TF(s,P(s))dsP(t)=G+∫tT​F(s,P(s))ds. The pseudoinverse is the published HarmonicGames.Decomposition.pinv. Where the paper prints (⋅)−1(\cdot)^{-1}(⋅)−1 ((4.19), p. 2290) Lean's matrix inverse is used; it is invertible there by R+D⊤PD≥λIR+D^\top PD\ge\lambda IR+D⊤PD≥λI.
  • The iteration. The sequence of milestones 5–6 is given by hypotheses: P0P_0P0​ solves (4.18) and Pi+1P_{i+1}Pi+1​ the Lyapunov equation of Θi\Theta_iΘi​. Lyapunov solutions are unique, so this is the paper's sequence.
  • Constants. λ\lambdaλ and α\alphaα in Proposition 4.4 and Remark 4.6 are the constants of (4.2) and (4.1), passed as parameters.

Ruling out trivial forms. Uniform convexity is not defined through the operator M2(0)M_2(0)M2​(0) of (3.8), and strong regularity includes the integral Riccati equation. A formalization that drops the Riccati equation, or reads uniform convexity off a matrix condition, is a different theorem. No positivity of GGG, QQQ or RRR is assumed anywhere except in Proposition 3.5, whose hypothesis (1.4) is exactly that.

Contributions welcome: Itô's formula for ⟨P(s)X(s),X(s)⟩\langle P(s)X(s),X(s)\rangle⟨P(s)X(s),X(s)⟩ with a C1C^1C1 (or absolutely continuous) matrix PPP; existence and uniqueness for linear SDEs with L1/L2L^1/L^2L1/L2 coefficients; existence and uniqueness for linear matrix ODEs; the Penrose identities for pinv.

Selected references

  • J. Sun, X. Li, J. Yong, Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems, SIAM J. Control Optim. 54 (2016), 2274–2308. https://doi.org/10.1137/15M103532X
  • J. Sun, J. Yong, Linear Quadratic Stochastic Differential Games: Open-Loop and Closed-Loop Saddle Points, SIAM J. Control Optim. 52 (2014), 4082–4121. https://doi.org/10.1137/140953642
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite Stochastic Linear Quadratic Control and Generalized Differential Riccati Equation, SIAM J. Control Optim. 40 (2002), 1296–1311. https://doi.org/10.1137/S0363012900371083
  • S. Chen, X. Li, X. Y. Zhou, Stochastic Linear Quadratic Regulators with Indefinite Control Weight Costs, SIAM J. Control Optim. 36 (1998), 1685–1702. https://doi.org/10.1137/S0363012996310478
  • W. M. Wonham, On a Matrix Riccati Equation of Stochastic Control, SIAM J. Control 6 (1968), 681–697. https://doi.org/10.1137/0306044
  • J. Yong, X. Y. Zhou, Stochastic Controls: Hamiltonian Systems and HJB Equations, Springer, 1999. https://doi.org/10.1007/978-1-4612-1466-3
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Control TheoryOptimizationProbability·Captain: mikedeng1

Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 4: A Problem Open-Loop Solvable at Every (t, x) but Closed-Loop Solvable on No [t, 1]Research Paper

Why open-loop and closed-loop solvability must be told apart

In a stochastic linear–quadratic (LQ) optimal control problem a controller steers a linear stochastic differential equation and pays a quadratic cost. When the cost weights are allowed to be indefinite — as in mean–variance portfolio selection, where the control weight is zero — the problem can still be well posed, and two different notions of solution appear. An open-loop optimal control is a process chosen for one given initial pair (t,x)(t,x)(t,x). A closed-loop optimal strategy is a feedback law u=ΘX+vu=\Theta X+vu=ΘX+v that is optimal for every initial state at once. A closed-loop optimal strategy yields an open-loop optimal control for each initial state; the converse is the question.

Timeline. Chen, Li and Zhou (1998, doi:10.1137/S0363012996310478) started the theory of indefinite stochastic LQ control. Ait Rami, Moore and Zhou (2002, doi:10.1137/S0363012900371083) introduced the generalized Riccati equation with a Moore–Penrose pseudoinverse and stated that, for Problem (SLQ)0^00 with continuous coefficients and S=0S=0S=0, a continuous open-loop optimal control exists at every initial pair if and only if the Riccati equation has a solution satisfying a range condition and a sign condition. Sun and Yong (2014, doi:10.1137/140953642) characterized closed-loop solvability by regular solutions of that Riccati equation. Sun, Li and Yong (2016, doi:10.1137/15M103532X) showed by two explicit examples that the 2002 equivalence fails in both directions, and that open-loop solvability is strictly weaker than closed-loop solvability. This mission formalizes those examples.

Setting

Let WWW be a standard one-dimensional Brownian motion on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) and F\mathbb FF its augmented natural filtration. For (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn and a control uuu in the space U[t,T]\mathcal U[t,T]U[t,T] of F\mathbb FF-progressively measurable Rm\mathbb R^mRm-valued processes with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞, the state equation is

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x,dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x,dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x,

and the cost J(t,x;u)J(t,x;u)J(t,x;u) is the expectation of ⟨GX(T),X(T)⟩+2⟨g,X(T)⟩\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle⟨GX(T),X(T)⟩+2⟨g,X(T)⟩ plus the time integral of a quadratic form in (X,u)(X,u)(X,u) with weights Q,S,RQ,S,RQ,S,R and linear terms q,ρq,\rhoq,ρ. Problem (SLQ)0^00 is the case b=σ=g=q=ρ=0b=\sigma=g=q=\rho=0b=σ=g=q=ρ=0, with cost J0J^0J0 and value function V0(t,x)=inf⁡u∈U[t,T]J0(t,x;u)V^0(t,x)=\inf_{u\in\mathcal U[t,T]}J^0(t,x;u)V0(t,x)=infu∈U[t,T]​J0(t,x;u).

The Riccati equation (4.6) is

P˙+PA+A⊤P+C⊤PC+Q−(PB+C⊤PD+S⊤)(R+D⊤PD)†(B⊤P+D⊤PC+S)=0,P(T)=G,\dot P+PA+A^\top P+C^\top PC+Q-(PB+C^\top PD+S^\top)(R+D^\top PD)^\dagger(B^\top P+D^\top PC+S)=0,\qquad P(T)=G,P˙+PA+A⊤P+C⊤PC+Q−(PB+C⊤PD+S⊤)(R+D⊤PD)†(B⊤P+D⊤PC+S)=0,P(T)=G,

where M†M^\daggerM† is the Moore–Penrose pseudoinverse. A solution is regular if (4.7) R(B⊤P+D⊤PC+S)⊆R(R+D⊤PD)\mathcal R(B^\top P+D^\top PC+S)\subseteq\mathcal R(R+D^\top PD)R(B⊤P+D⊤PC+S)⊆R(R+D⊤PD) a.e., (4.8) (R+D⊤PD)†(B⊤P+D⊤PC+S)∈L2(R+D^\top PD)^\dagger(B^\top P+D^\top PC+S)\in L^2(R+D⊤PD)†(B⊤P+D⊤PC+S)∈L2, and (4.9) R+D⊤PD≥0R+D^\top PD\ge 0R+D⊤PD≥0 a.e.

Example 7.1 is Problem (SLQ)0^00 with n=1n=1n=1, m=2m=2m=2, T=1T=1T=1:

dX=[u1+u2] ds+[u1−u2] dW,J0(t,x;u)=E X(1)2,dX=[u_1+u_2]\,ds+[u_1-u_2]\,dW,\qquad J^0(t,x;u)=\mathbb E\,X(1)^2,dX=[u1​+u2​]ds+[u1​−u2​]dW,J0(t,x;u)=EX(1)2,

that is, A=C=Q=0A=C=Q=0A=C=Q=0, B=(1,1)B=(1,1)B=(1,1), D=(1,−1)D=(1,-1)D=(1,−1), G=1G=1G=1, S=0S=0S=0, R=0R=0R=0.

Formalization targets

Goal: Example 7.1

For every (t,x)∈[0,1)×R(t,x)\in[0,1)\times\mathbb R(t,x)∈[0,1)×R,

u(t,x)∗(s)=−(x2−2t,x2−2t)⊤ is open-loop optimal,V0(t,x)=0,u^*_{(t,x)}(s)=-\Big(\frac{x}{2-2t},\frac{x}{2-2t}\Big)^\top\ \text{is open-loop optimal},\qquad V^0(t,x)=0,u(t,x)∗​(s)=−(2−2tx​,2−2tx​)⊤ is open-loop optimal,V0(t,x)=0,

while V0(1,x)=x2V^0(1,x)=x^2V0(1,x)=x2, and for every t∈[0,1)t\in[0,1)t∈[0,1) the problem is not closed-loop solvable on [t,1][t,1][t,1].

Milestones

  1. (7.3): the Riccati equation has the unique solution P≡1P\equiv1P≡1, and it violates (4.7).
  2. Theorem 4.3 for (SLQ)0^00: closed-loop solvability on [t,T][t,T][t,T] is equivalent to the existence of a regular solution on [t,T][t,T][t,T].
  3. (7.5)–(7.6): with RRR replaced by R+εIR+\varepsilon IR+εI the Riccati equation has the strongly regular solution Pε(t)=ε/(ε+2−2t)P_\varepsilon(t)=\varepsilon/(\varepsilon+2-2t)Pε​(t)=ε/(ε+2−2t).
  4. (7.7): Pε(t)→0P_\varepsilon(t)\to 0Pε​(t)→0 for t<1t<1t<1 and Pε(1)=1P_\varepsilon(1)=1Pε​(1)=1.
  5. (7.9)–(7.10): the closed-loop state and control of the regularized problem, uε=−(xε+2−2t,xε+2−2t)⊤u_\varepsilon=-\big(\frac{x}{\varepsilon+2-2t},\frac{x}{\varepsilon+2-2t}\big)^\topuε​=−(ε+2−2tx​,ε+2−2tx​)⊤.
  6. uε→u(t,x)∗u_\varepsilon\to u^*_{(t,x)}uε​→u(t,x)∗​ in L2L^2L2 as ε→0\varepsilon\to0ε→0.

Companion: Example 7.2

For dX=u dsdX=u\,dsdX=uds and J=X(1)2+∫t1s2u2dsJ=X(1)^2+\int_t^1s^2u^2dsJ=X(1)2+∫t1​s2u2ds, the Riccati equation (7.12) has the unique solution P(t)=tP(t)=tP(t)=t, which satisfies (4.7) and (4.9), yet no open-loop optimal control exists at (0,x)(0,x)(0,x), x≠0x\neq0x=0.

Significance

The result. Example 7.1 refutes the necessity half of the Ait Rami–Moore–Zhou criterion: a continuous open-loop optimal control exists at every initial pair, but the Riccati equation has no regular solution. Example 7.2 refutes the sufficiency half. Together they show that the Riccati equation with conditions (4.7) and (4.9) characterizes neither notion, and that open-loop solvability is strictly weaker than closed-loop solvability; Example 7.1 also exhibits a finite value function that is discontinuous in time. These facts are why the paper develops separate characterizations of open-loop solvability (through the regularized Riccati solutions PεP_\varepsilonPε​) instead of the Riccati equation itself.

Formalizing it. The examples are proved in the paper by appeal to its Theorems 5.3 and 6.2 and to Theorem 4.3 from Sun–Yong (2014). Nothing in this chain is machine-checked anywhere. A formal proof of the goal must verify the explicit optimal control against the canonical stochastic state equation, compute the value function, and rule out every closed-loop strategy; it can use Theorem 4.3 (posed here as a milestone) or a direct argument. The definitions built here (the stochastic LQ problem, the pseudoinverse Riccati equation, regularity) are shared with the other missions of this series.

Difficulty

Open-loop optimality looks immediate because J0=EX(1)2≥0J^0=\mathbb EX(1)^2\ge0J0=EX(1)2≥0, but it requires showing that the state driven by u∗u^*u∗ hits 000 at time 111, which means identifying the solution of the stochastic state equation for this control. The value at t=1t=1t=1 requires the degenerate interval [1,1][1,1][1,1] to be handled inside the same SDE framework. The hard part is the negative claim: it quantifies over all feedback pairs (Θ,v)(\Theta,v)(Θ,v) with Θ∈L2\Theta\in L^2Θ∈L2, and must show that no such pair drives every initial state to 000 at time 111. The paper reduces this to Theorem 4.3, whose proof (in Sun–Yong 2014) is a substantial piece of stochastic LQ theory; checking that P≡1P\equiv 1P≡1 fails the range condition is the easy end of that chain.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​, vectors are Fin k → ℝ, inner products are dot products, and ∣u∣2=u⋅u|u|^2=u\cdot u∣u∣2=u⋅u. The Brownian motion is the published Peng1990.SMP.IsStdBrownian, the filtration the published augmented filtration, the SDE solution concept the published Peng1990.SMP.SolvesSDE, and the pseudoinverse the published HarmonicGames.Decomposition.pinv.

  • The state from (t,x)(t,x)(t,x) is an SDE from time 000 with coefficients switched on at ttt, with a.s. continuous paths and Esup⁡∣X∣2<∞\mathbb E\sup|X|^2<\inftyEsup∣X∣2<∞; the cost uses a chosen solution, unique by [23, Proposition 2.1].
  • Value functions are infima in the extended reals over admissible controls.
  • The Riccati equation is in integral form on [t0,T][t_0,T][t0​,T]; regularity is (4.7)–(4.9) on [t0,T][t_0,T][t0​,T].
  • A closed-loop optimal strategy on [t,T][t,T][t,T] requires Θ∈L2(t,T)\Theta\in L^2(t,T)Θ∈L2(t,T), v∈U[t,T]v\in\mathcal U[t,T]v∈U[t,T], and, for every initial state, a solution of the closed-loop system that is no worse than any admissible control.
  • Theorem 4.3 is stated on [t,T][t,T][t,T] (the paper states it on [0,T][0,T][0,T] and applies it on [t,1][t,1][t,1]).
  • The goal places no hypotheses on the probability space beyond the Brownian motion.

Proving only that P≡1P\equiv1P≡1 violates (4.7) does not settle the goal: the goal is about solvability of the control problem itself, and "not closed-loop solvable on any [t,1][t,1][t,1]" is stated for every t<1t<1t<1, not as the failure on some interval.

Contributions are welcome on any milestone, on the well-posedness of linear SDEs in this framework, and on the pseudoinverse identities (Penrose equations, the pseudoinverse of a scaled symmetric matrix) that the Riccati computations need.

Selected references

  • J. Sun, X. Li, J. Yong, Open-loop and closed-loop solvabilities for stochastic linear quadratic optimal control problems, SIAM J. Control Optim. 54(5) (2016) 2274–2308. doi:10.1137/15M103532X
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite stochastic linear quadratic control and generalized differential Riccati equation, SIAM J. Control Optim. 40 (2002) 1296–1311. doi:10.1137/S0363012900371083
  • J. Sun, J. Yong, Linear quadratic stochastic differential games: open-loop and closed-loop saddle points, SIAM J. Control Optim. 52 (2014) 4082–4121. doi:10.1137/140953642
  • S. Chen, X. Li, X. Y. Zhou, Stochastic linear quadratic regulators with indefinite control weight costs, SIAM J. Control Optim. 36 (1998) 1685–1702. doi:10.1137/S0363012996310478
13 thms1 active userReviewed
Control TheoryOptimizationProbability·Captain: mikedeng1

Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 3: Open-Loop Solvability Is Equivalent to Convergence of the Riccati Minimizing SequenceResearch Paper

Motivation

Linear–quadratic (LQ) optimal control is the basic test case of stochastic control: a linear stochastic differential equation, a quadratic cost, and an optimal control that one expects to be a linear feedback of the state computed from a Riccati equation. In the indefinite stochastic case the weighting matrices GGG, QQQ, RRR carry no sign condition. The cost can then be convex without being uniformly convex, an optimal control may fail to exist although the value is finite, and the Riccati equation may have no solution of the kind the classical theory needs.

Sun, Li and Yong (SIAM J. Control Optim. 54 (2016) 2274–2308) separate finiteness, convexity, open-loop solvability and closed-loop solvability for this problem. This mission covers their Section 6. Under uniform convexity the optimal control is the Riccati feedback of Corollary 4.7. Section 6 removes uniform convexity: it regularizes the control weight RRR to R+εIR+\varepsilon IR+εI, takes the Riccati feedback control uεu_\varepsilonuε​ of each regularized problem, and shows that open-loop solvability of the original problem is exactly the convergence of uεu_\varepsilonuε​ along some sequence εk→0\varepsilon_k\to0εk​→0.

Timeline. Chen, Li and Zhou (SIAM J. Control Optim. 36 (1998)) introduced indefinite stochastic LQ problems. Ait Rami, Moore and Zhou (SIAM J. Control Optim. 40 (2002)) introduced the generalized Riccati equation with a pseudoinverse. Sun and Yong (SIAM J. Control Optim. 52 (2014)) characterized closed-loop solvability by regular solutions of that equation. In 2016 Sun, Li and Yong characterized uniform convexity by strongly regular solutions and open-loop solvability by the regularized feedback sequence treated here.

Setting

Fix a horizon T>0T>0T>0 and a probability space carrying a one-dimensional standard Brownian motion WWW, with F\mathbb FF the augmented natural filtration of WWW. For an initial pair (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn and an admissible control u∈U[t,T]u\in\mathcal U[t,T]u∈U[t,T], an F\mathbb FF-progressively measurable Rm\mathbb R^mRm-valued process with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞, the state solves

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x.dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x .dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x.

The cost is

J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].J(t,x;u)=\mathbb E\Big[\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle+\int_t^T\big(\langle QX,X\rangle+2\langle SX,u\rangle+\langle Ru,u\rangle+2\langle q,X\rangle+2\langle\rho,u\rangle\big)ds\Big].J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT​(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].

The coefficients A,B,C,D,Q,S,RA,B,C,D,Q,S,RA,B,C,D,Q,S,R and GGG are deterministic, b,σ,q,ρ,gb,\sigma,q,\rho,gb,σ,q,ρ,g are random, and the integrability conditions are (H1)–(H2). The value function is V(t,x)=inf⁡uJ(t,x;u)∈[−∞,∞)V(t,x)=\inf_uJ(t,x;u)\in[-\infty,\infty)V(t,x)=infu​J(t,x;u)∈[−∞,∞). A control u∗u^*u∗ is open-loop optimal at (t,x)(t,x)(t,x) if J(t,x;u∗)≤J(t,x;u)J(t,x;u^*)\le J(t,x;u)J(t,x;u∗)≤J(t,x;u) for every u∈U[t,T]u\in\mathcal U[t,T]u∈U[t,T]. Problem (SLQ)0^00 is the case b,σ,g,q,ρ=0b,\sigma,g,q,\rho=0b,σ,g,q,ρ=0, with cost J0J^0J0.

For ε>0\varepsilon>0ε>0 let PεP_\varepsilonPε​ be the strongly regular solution of the Riccati equation (5.7),

P˙ε+PεA+A⊤Pε+C⊤PεC+Q−Kε⊤Σε−1Kε=0,Pε(T)=G,\dot P_\varepsilon+P_\varepsilon A+A^\top P_\varepsilon+C^\top P_\varepsilon C+Q-K_\varepsilon^\top\Sigma_\varepsilon^{-1}K_\varepsilon=0,\qquad P_\varepsilon(T)=G,P˙ε​+Pε​A+A⊤Pε​+C⊤Pε​C+Q−Kε⊤​Σε−1​Kε​=0,Pε​(T)=G,

where Σε=R+εI+D⊤PεD≥λI\Sigma_\varepsilon=R+\varepsilon I+D^\top P_\varepsilon D\ge\lambda IΣε​=R+εI+D⊤Pε​D≥λI for some λ>0\lambda>0λ>0 and Kε=B⊤Pε+D⊤PεC+SK_\varepsilon=B^\top P_\varepsilon+D^\top P_\varepsilon C+SKε​=B⊤Pε​+D⊤Pε​C+S. Let (ηε,ζε)(\eta_\varepsilon,\zeta_\varepsilon)(ηε​,ζε​) be the adapted solution of the linear backward equation (4.11) for these data, and put

Θε=−Σε−1Kε,vε=−Σε−1(B⊤ηε+D⊤ζε+D⊤Pεσ+ρ).\Theta_\varepsilon=-\Sigma_\varepsilon^{-1}K_\varepsilon,\qquad v_\varepsilon=-\Sigma_\varepsilon^{-1}\big(B^\top\eta_\varepsilon+D^\top\zeta_\varepsilon+D^\top P_\varepsilon\sigma+\rho\big).Θε​=−Σε−1​Kε​,vε​=−Σε−1​(B⊤ηε​+D⊤ζε​+D⊤Pε​σ+ρ).

With XεX_\varepsilonXε​ the solution of the closed-loop system dXε=[(A+BΘε)Xε+Bvε+b]ds+[(C+DΘε)Xε+Dvε+σ]dWdX_\varepsilon=[(A+B\Theta_\varepsilon)X_\varepsilon+Bv_\varepsilon+b]ds+[(C+D\Theta_\varepsilon)X_\varepsilon+Dv_\varepsilon+\sigma]dWdXε​=[(A+BΘε​)Xε​+Bvε​+b]ds+[(C+DΘε​)Xε​+Dvε​+σ]dW, Xε(t)=xX_\varepsilon(t)=xXε​(t)=x, the regularized feedback sequence is

uε=ΘεXε+vε,ε>0.u_\varepsilon=\Theta_\varepsilon X_\varepsilon+v_\varepsilon,\qquad\varepsilon>0 .uε​=Θε​Xε​+vε​,ε>0.

U[t,T]=LF2(t,T;Rm)\mathcal U[t,T]=L^2_{\mathbb F}(t,T;\mathbb R^m)U[t,T]=LF2​(t,T;Rm) is a Hilbert space with inner product E∫tT⟨u,v⟩ds\mathbb E\int_t^T\langle u,v\rangle dsE∫tT​⟨u,v⟩ds; weak and strong convergence of controls refer to it.

Formalization targets

Goal: Theorem 6.2

Assume (H1)–(H2) and that u↦J0(0,0;u)u\mapsto J^0(0,0;u)u↦J0(0,0;u) is convex. For (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn the following are equivalent:

(SLQ) is open-loop solvable at (t,x)  ⟺  ∃ εk↓0: uεk⇀u∗  ⟺  ∃ εk↓0: uεk→u∗ in U[t,T],\text{(SLQ) is open-loop solvable at }(t,x)\iff\exists\,\varepsilon_k\downarrow0:\ u_{\varepsilon_k}\rightharpoonup u^*\iff\exists\,\varepsilon_k\downarrow0:\ u_{\varepsilon_k}\to u^*\text{ in }\mathcal U[t,T],(SLQ) is open-loop solvable at (t,x)⟺∃εk​↓0: uεk​​⇀u∗⟺∃εk​↓0: uεk​​→u∗ in U[t,T],

and every weak or strong limit of such a subsequence is an open-loop optimal control at (t,x)(t,x)(t,x). The goal assumes convexity, not uniform convexity, and no finiteness.

Milestones

  1. Corollary 3.4: convexity of J(t,x;⋅)J(t,x;\cdot)J(t,x;⋅) or J0(t,x;⋅)J^0(t,x;\cdot)J0(t,x;⋅) at one xxx, at every xxx, and J0(t,0;u)≥0J^0(t,0;u)\ge0J0(t,0;u)≥0 on U[t,T]\mathcal U[t,T]U[t,T] are equivalent.
  2. The zero extension (4.3): J0(t,0;u)=J0(0,0;0I[0,t)⊕u)J^0(t,0;u)=J^0(0,0;0I_{[0,t)}\oplus u)J0(t,0;u)=J0(0,0;0I[0,t)​⊕u).
  3. Corollary 4.7: under uniform convexity, the Riccati feedback control (4.28) is the unique open-loop optimal control.
  4. Theorem 6.1: if the problem is finite, lim⁡ε→0+J(t,x;uε)=V(t,x)\lim_{\varepsilon\to0^+}J(t,x;u_\varepsilon)=V(t,x)limε→0+​J(t,x;uε​)=V(t,x).
  5. Lemma 6.3: in a Hilbert space the norm is weakly lower semicontinuous, and strong convergence is weak convergence plus convergence of norms.
  6. (6.7): E∫tT∣uε∣2ds≤(Vε−V)/ε≤E∫tT∣v∗∣2ds\mathbb E\int_t^T|u_\varepsilon|^2ds\le(V_\varepsilon-V)/\varepsilon\le\mathbb E\int_t^T|v^*|^2dsE∫tT​∣uε​∣2ds≤(Vε​−V)/ε≤E∫tT​∣v∗∣2ds for any optimal v∗v^*v∗.
  7. Weak lower semicontinuity of u↦J(t,x;u)u\mapsto J(t,x;u)u↦J(t,x;u).

Two further statements follow the goal: open-loop solvability is equivalent to sup⁡ε>0E∫tT∣uε∣2ds<∞\sup_{\varepsilon>0}\mathbb E\int_t^T|u_\varepsilon|^2ds<\inftysupε>0​E∫tT​∣uε​∣2ds<∞ (p. 2303), and Proposition 6.4: if sup⁡ε>0∫0T∣Θε∣2ds<∞\sup_{\varepsilon>0}\int_0^T|\Theta_\varepsilon|^2ds<\inftysupε>0​∫0T​∣Θε​∣2ds<∞, the Riccati equation (4.6) has a regular solution and Problem (SLQ)0^00 is closed-loop solvable.

Significance

Theorem 6.1 gives a minimizing sequence computed from Riccati and backward equations whenever the problem is finite. Theorem 6.2 turns it into a test for open-loop solvability that needs no uniform convexity and no regular solution of the original Riccati equation. When an optimal control exists, it is recovered as the limit of feedback controls. Proposition 6.4 converts a bound on the gains Θε\Theta_\varepsilonΘε​ into closed-loop solvability of the homogeneous problem. Section 7 of the paper shows that open-loop solvability does not imply closed-loop solvability, so a criterion phrased directly in open-loop terms is needed.

All of these results are proved in the paper. None of them, nor the solution theory of stochastic LQ problems they rest on, had a machine-checked proof on Prove2Me or in Mathlib as of October 2026. A formal development needs the well-posedness of linear SDEs and BSDEs with integrable coefficients, the Riccati theory of Section 4, and the Hilbert-space structure of the space of admissible controls. Those parts are reusable for any stochastic LQ problem.

Difficulty

The obvious approach takes any minimizing sequence and extracts a weakly convergent subsequence. That fails without uniform convexity: a minimizing sequence need not be bounded, and boundedness is exactly what open-loop solvability provides in (6.7). The converse direction needs the limit of the regularized costs to identify the value, which requires both the minimizing property of uεu_\varepsilonuε​ (Theorem 6.1) and weak lower semicontinuity of JJJ. That in turn rests on convexity being transported from J0(0,0;⋅)J^0(0,0;\cdot)J0(0,0;⋅) to J(t,x;⋅)J(t,x;\cdot)J(t,x;⋅) through Corollary 3.4 and the zero extension. Upgrading weak to strong convergence uses the norm bound (6.7) with the limit itself as the optimal control. Every step depends on Corollary 4.7, the Riccati representation of the optimal control of the regularized problem, whose proof requires the theory of Section 4.

Formalization scope

The probability basis is a probability space with a one-dimensional standard Brownian motion and its augmented natural filtration. Vectors are Fin k → ℝ and matrices Matrix (Fin k) (Fin l) ℝ. Time is ℝ≥0, and ∣u∣2|u|^2∣u∣2 is the Euclidean dot product u ⬝ᵥ u. (H1)–(H2) are standing assumptions, with entrywise LpL^pLp conditions on the matrix coefficients. The state from (t,x)(t,x)(t,x) is a strong solution of the published SDE notion Peng1990.SMP.SolvesSDE whose coefficients are switched on at ttt; it has a.s. continuous paths and Esup⁡∣X∣2<∞\mathbb E\sup|X|^2<\inftyEsup∣X∣2<∞. The cost is evaluated along a chosen solution, which is unique. VVV is an infimum in the extended reals. Limits in ε\varepsilonε are taken as ε→0+\varepsilon\to0^+ε→0+. "A subsequence" is a sequence εk>0\varepsilon_k>0εk​>0 with εk→0\varepsilon_k\to0εk​→0, and the limit control is required to be admissible. The backward equations use the published Peng1990.SMP.SolvesBSDE, and the pseudoinverse in (4.6) and (4.11) is the published HarmonicGames.Decomposition.pinv.

Theorem 6.1 prints the term −Θε⊤ρ-\Theta_\varepsilon^\top\rho−Θε⊤​ρ in its backward equation. The equation (4.11) that its proof uses through Corollary 4.7 has +Θε⊤ρ+\Theta_\varepsilon^\top\rho+Θε⊤​ρ, and the formalization uses (4.11). Corollary 3.4 is stated without its item (vi), which involves an operator M2(t)M_2(t)M2​(t) that the paper quotes from another source.

The families PεP_\varepsilonPε​, (ηε,ζε)(\eta_\varepsilon,\zeta_\varepsilon)(ηε​,ζε​) and XεX_\varepsilonXε​ are hypotheses pinned by their equations for every ε>0\varepsilon>0ε>0. The sequence uεu_\varepsilonuε​ is therefore the Riccati feedback sequence (6.2), never an arbitrary minimizing sequence or an arbitrary family of ε\varepsilonε-optimal controls; with such a family the implication (ii) ⇒ (i) would be a different theorem.

Contributions are welcome at every level: the solution theory of linear SDEs and BSDEs, Itô's formula for quadratic forms, Riccati and Lyapunov equations in integral form, weak compactness in LF2L^2_{\mathbb F}LF2​, and the milestones themselves.

Selected references

  • J. Sun, X. Li, J. Yong, Open-loop and closed-loop solvabilities for stochastic linear quadratic optimal control problems, SIAM J. Control Optim. 54(5) (2016) 2274–2308. https://doi.org/10.1137/15M103532X
  • J. Sun, J. Yong, Linear quadratic stochastic differential games: open-loop and closed-loop saddle points, SIAM J. Control Optim. 52(6) (2014) 4082–4121. https://doi.org/10.1137/140953642
  • S. Chen, X. Li, X. Y. Zhou, Stochastic linear quadratic regulators with indefinite control weight costs, SIAM J. Control Optim. 36(5) (1998) 1685–1702. https://doi.org/10.1137/S0363012996310478
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite stochastic linear quadratic control and generalized differential Riccati equation, SIAM J. Control Optim. 40(4) (2002) 1296–1311. https://doi.org/10.1137/S0363012900371083
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4) (1990) 966–979. https://doi.org/10.1137/0328054
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Control TheoryOptimizationProbability·Captain: mikedeng1

Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 2: Finiteness Holds iff the Regularized Riccati Solutions P_ε(0) Are Bounded BelowResearch Paper

Motivation

Linear–quadratic (LQ) optimal control is the basic test case of stochastic control: a linear stochastic differential equation, a quadratic cost, and a value function that one expects to be a quadratic form in the initial state. In the indefinite stochastic case the weighting matrices GGG, QQQ, RRR carry no sign condition, and the classical picture breaks down. Without a sign condition the infimum of the cost can be −∞-\infty−∞. Before one can ask whether an optimal control exists, one has to ask whether the problem is finite, i.e. whether its value function stays above −∞-\infty−∞.

Sun, Li and Yong (SIAM J. Control Optim. 54 (2016) 2274–2308) separate the notions of finiteness, convexity, open-loop and closed-loop solvability for this problem. This mission covers their Section 5. Section 5 characterizes finiteness of the homogeneous problem by a family of regularized Riccati equations, and Example 5.2 shows that convexity of the cost alone is not enough.

Timeline. Chen, Li and Zhou (SIAM J. Control Optim. 36 (1998)) introduced indefinite stochastic LQ problems. Ait Rami, Moore and Zhou (SIAM J. Control Optim. 40 (2002)) introduced the generalized Riccati equation with a pseudoinverse. Sun and Yong (SIAM J. Control Optim. 52 (2014)) characterized closed-loop solvability by regular solutions of that equation. In 2016 Sun, Li and Yong characterized uniform convexity by strongly regular solutions, and finiteness by the limit of the regularized solutions treated here.

Setting

Fix a horizon T>0T>0T>0 and a probability space carrying a one-dimensional standard Brownian motion WWW, with F\mathbb FF the augmented natural filtration of WWW. For an initial pair (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn and an admissible control u∈U[t,T]u\in\mathcal U[t,T]u∈U[t,T], an F\mathbb FF-progressively measurable Rm\mathbb R^mRm-valued process with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞, the state solves

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x.dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x .dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x.

The cost is

J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].J(t,x;u)=\mathbb E\Big[\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle+\int_t^T\big(\langle QX,X\rangle+2\langle SX,u\rangle+\langle Ru,u\rangle+2\langle q,X\rangle+2\langle\rho,u\rangle\big)ds\Big].J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT​(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].

The coefficients A,B,C,D,Q,S,RA,B,C,D,Q,S,RA,B,C,D,Q,S,R and GGG are deterministic, and b,σ,q,ρ,gb,\sigma,q,\rho,gb,σ,q,ρ,g are random; the integrability conditions are (H1)–(H2). The value function is V(t,x)=inf⁡uJ(t,x;u)∈[−∞,∞)V(t,x)=\inf_{u}J(t,x;u)\in[-\infty,\infty)V(t,x)=infu​J(t,x;u)∈[−∞,∞). Problem (SLQ)0^00 is the case b,σ,g,q,ρ=0b,\sigma,g,q,\rho=0b,σ,g,q,ρ=0; its cost and value are J0J^0J0 and V0V^0V0. The problem is finite at ttt if V(t,x)>−∞V(t,x)>-\inftyV(t,x)>−∞ for all xxx, and finite if this holds for every t∈[0,T]t\in[0,T]t∈[0,T].

Write Σε(P)=R+εI+D⊤PD\Sigma_\varepsilon(P)=R+\varepsilon I+D^\top PDΣε​(P)=R+εI+D⊤PD and K(P)=B⊤P+D⊤PC+SK(P)=B^\top P+D^\top PC+SK(P)=B⊤P+D⊤PC+S. The regularized Riccati equation (5.7) is

P˙ε+PεA+A⊤Pε+C⊤PεC+Q−K(Pε)⊤Σε(Pε)−1K(Pε)=0,Pε(T)=G.\dot P_\varepsilon+P_\varepsilon A+A^\top P_\varepsilon+C^\top P_\varepsilon C+Q-K(P_\varepsilon)^\top\Sigma_\varepsilon(P_\varepsilon)^{-1}K(P_\varepsilon)=0,\qquad P_\varepsilon(T)=G .P˙ε​+Pε​A+A⊤Pε​+C⊤Pε​C+Q−K(Pε​)⊤Σε​(Pε​)−1K(Pε​)=0,Pε​(T)=G.

A solution is strongly regular if Σε(Pε)≥λI\Sigma_\varepsilon(P_\varepsilon)\ge\lambda IΣε​(Pε​)≥λI a.e. for some λ>0\lambda>0λ>0. Further, M0M_0M0​ solves the Lyapunov equation (3.2), M˙0+M0A+A⊤M0+C⊤M0C+Q=0\dot M_0+M_0A+A^\top M_0+C^\top M_0C+Q=0M˙0​+M0​A+A⊤M0​+C⊤M0​C+Q=0, M0(T)=GM_0(T)=GM0​(T)=G, and ΦA\Phi_AΦA​ solves Φ˙A=AΦA\dot\Phi_A=A\Phi_AΦ˙A​=AΦA​, ΦA(0)=I\Phi_A(0)=IΦA​(0)=I. The comparison function is

N(t)=[ΦA(t)⊤]−1{P(0)−∫0tΦA⊤(C⊤M0C+Q)ΦA ds}ΦA(t)−1.N(t)=[\Phi_A(t)^\top]^{-1}\Big\{P(0)-\int_0^t\Phi_A^\top(C^\top M_0C+Q)\Phi_A\,ds\Big\}\Phi_A(t)^{-1}.N(t)=[ΦA​(t)⊤]−1{P(0)−∫0t​ΦA⊤​(C⊤M0​C+Q)ΦA​ds}ΦA​(t)−1.

Formalization targets

Goal: Theorem 5.3

Assume (H1)–(H2) and (5.6): J0(0,0;u)≥0J^0(0,0;u)\ge0J0(0,0;u)≥0 for all u∈U[0,T]u\in\mathcal U[0,T]u∈U[0,T]. For every ε>0\varepsilon>0ε>0, let PεP_\varepsilonPε​ be the strongly regular solution of (5.7). Then

(SLQ)0 is finite  ⟺  ∃β∈R  ∀ε>0: Pε(0)≥βI.\text{(SLQ)}^0\ \text{is finite}\iff\exists\beta\in\mathbb R\ \ \forall\varepsilon>0:\ P_\varepsilon(0)\ge\beta I .(SLQ)0 is finite⟺∃β∈R  ∀ε>0: Pε​(0)≥βI.

In this case P(t)=lim⁡ε↓0Pε(t)P(t)=\lim_{\varepsilon\downarrow0}P_\varepsilon(t)P(t)=limε↓0​Pε​(t) exists for every t∈[0,T]t\in[0,T]t∈[0,T], and

V0(t,x)=⟨P(t)x,x⟩,R+D⊤PD≥0 a.e.,N(t)≤P(t)≤M0(t).V^0(t,x)=\langle P(t)x,x\rangle,\qquad R+D^\top PD\ge0\ \text{a.e.},\qquad N(t)\le P(t)\le M_0(t).V0(t,x)=⟨P(t)x,x⟩,R+D⊤PD≥0 a.e.,N(t)≤P(t)≤M0​(t).

In particular, finiteness at t=0t=0t=0 implies finiteness.

Milestones

  1. Proposition 5.1: (i) ⇒ (ii) ⇒ (iii) ⇒ (iv) and (v) ⇒ (ii). The statements relate finiteness of (SLQ) and (SLQ)0^00, a quadratic V0V^0V0, convexity of JJJ, and P[t,T]≠∅\mathcal P[t,T]\ne\emptysetP[t,T]=∅.
  2. Remark 4.8: under uniform convexity, V0(t,x)=⟨P(t)x,x⟩V^0(t,x)=\langle P(t)x,x\rangleV0(t,x)=⟨P(t)x,x⟩ with PPP the strongly regular solution.
  3. (5.8): R+εI+D⊤PεD≥εIR+\varepsilon I+D^\top P_\varepsilon D\ge\varepsilon IR+εI+D⊤Pε​D≥εI a.e.
  4. (5.13): Pε2(t)≥Pε1(t)≥P(t)P_{\varepsilon_2}(t)\ge P_{\varepsilon_1}(t)\ge P(t)Pε2​​(t)≥Pε1​​(t)≥P(t) for ε2>ε1>0\varepsilon_2>\varepsilon_1>0ε2​>ε1​>0, and the limit Pˉ(t)=lim⁡ε↓0Pε(t)\bar P(t)=\lim_{\varepsilon\downarrow0}P_\varepsilon(t)Pˉ(t)=limε↓0​Pε​(t) exists with Pˉ(t)≥P(t)\bar P(t)\ge P(t)Pˉ(t)≥P(t).
  5. (5.16): Pε(t)≤M0(t)P_\varepsilon(t)\le M_0(t)Pε​(t)≤M0​(t).
  6. (5.15) and (5.17): P(0)≤Pε(0)P(0)\le P_\varepsilon(0)P(0)≤Pε​(0), and J0(t,x;u)≥⟨N(t)x,x⟩J^0(t,x;u)\ge\langle N(t)x,x\rangleJ0(t,x;u)≥⟨N(t)x,x⟩.

Companions

Theorem 5.6 states the converse of Remark 4.8. Theorem 5.7 gives six equivalent conditions when D=0D=0D=0 and R≫0R\gg0R≫0. Example 5.2 is a problem whose cost is convex but which is not finite. Corollary 5.4 gives a Lyapunov-type sufficient condition for finiteness.

Significance

The result. Theorem 5.3 turns finiteness, a statement about an infimum over an infinite-dimensional space of controls, into a lower bound on a one-parameter family of matrices. Each matrix in the family solves a well-posed Riccati equation. The theorem also says that the value function of a finite homogeneous problem is a quadratic form whose matrix is the monotone limit of PεP_\varepsilonPε​. It shows that this limit satisfies the regularity condition (5.10) and sits between two explicit bounds. Section 6 of the paper builds on the same regularization to construct minimizing sequences. Theorem 5.7 shows that in the case D=0D=0D=0, R≫0R\gg0R≫0, finiteness already forces unique closed-loop solvability.

Formalizing it. The result has been proved on paper since 2016; nothing in this mission is open mathematics. As far as is known, no part of indefinite stochastic LQ theory has been machine-checked, and Lean/Mathlib has no stochastic LQ problem, no matrix Riccati equation and no fundamental-matrix theory for time-varying linear ODEs. The mission produces faithful statements of the theorem, its proof steps and its companions on top of a reusable problem layer, as targets for complete formal proofs.

Difficulty

The naive argument fails at the interchange of the limit ε→0\varepsilon\to0ε→0 with the infimum over controls. Monotonicity in ε\varepsilonε gives a limit Pˉ(t)≥P(t)\bar P(t)\ge P(t)Pˉ(t)≥P(t) directly. The reverse inequality needs near-optimal controls whose L2L^2L2 norm may blow up, so it has to be organized carefully. The sufficiency direction needs more than the bound at t=0t=0t=0. Finiteness at later times is recovered through the comparison function N(t)N(t)N(t), which combines the fundamental matrix ΦA\Phi_AΦA​ with the Lyapunov solution M0M_0M0​. Example 5.2 rules out the tempting shortcut: under (5.6) the cost is convex, yet V0(0,x)=−∞V^0(0,x)=-\inftyV0(0,x)=−∞ for all x≠0x\ne0x=0. Every step also rests on stochastic calculus (Itô's formula for ⟨PX,X⟩\langle PX,X\rangle⟨PX,X⟩, well-posedness of the state equation) and on the representation of the value through the Riccati equation (Theorems 4.3 and 4.5, cited here).

Formalization scope

The problem layer is shared by the four missions of this series: SLQSolv.Finite.Setting and SLQSolv.Finite.Riccati. It builds on the published Itô-calculus and SDE layer Peng1990.SMP.Stochastic, the augmented Brownian filtration of ReflectedBSDE.Existence.Setting, and the Moore–Penrose pseudoinverse HarmonicGames.Decomposition.pinv. The layer commits to these conventions:

  • time is ℝ≥0, vectors are Fin k → ℝ, and ∣u∣2|u|^2∣u∣2 is the dot product u⋅uu\cdot uu⋅u;
  • the state from (t,x)(t,x)(t,x) is an SDE solution from time 0 with coefficients switched on at ttt, with continuous paths and a finite second moment of the supremum; the cost uses this (unique) solution;
  • VVV and V0V^0V0 take values in EReal, so V=−∞V=-\inftyV=−∞ is ⊥ and finiteness is ⊥ < V;
  • matrix ODEs (Riccati, Lyapunov, (5.12)) are in integral form on [t0,T][t_0,T][t0​,T]; the Riccati equation uses the pseudoinverse, which equals the printed inverse on strongly regular solutions;
  • matrix inequalities are Loewner inequalities (PosSemidef of the difference), and LpL^pLp conditions on matrix coefficients are entrywise;
  • "bounded from below" means one scalar β\betaβ with Pε(0)≥βIP_\varepsilon(0)\ge\beta IPε​(0)≥βI for all ε>0\varepsilon>0ε>0; the limit is ε↓0\varepsilon\downarrow0ε↓0;
  • PεP_\varepsilonPε​, M0M_0M0​, ΦA\Phi_AΦA​ are hypotheses pinned by their defining equations, each with a unique solution; the limit PPP is a conclusion, not a hypothesis.

A formalization in which "bounded from below" allows β\betaβ to depend on ε\varepsilonε, or in which finiteness is checked on J0J^0J0 at a fixed control rather than on V0V^0V0, would trivialize the theorem and is excluded.

A complete development needs several pieces, all reusable beyond this mission:

  • Itô's formula for quadratic forms of linear SDEs;
  • existence and uniqueness for linear SDEs with LpL^pLp coefficients;
  • existence, uniqueness and invertibility for time-varying linear matrix ODEs;
  • continuity of the pseudoinverse on uniformly positive matrices;
  • the strongly regular solvability theorem (Theorem 4.5, the goal of mission 1 of this series).

Contributions to any of them are welcome.

Selected references

  • J. Sun, X. Li, J. Yong, Open-loop and closed-loop solvabilities for stochastic linear quadratic optimal control problems, SIAM J. Control Optim. 54 (2016) 2274–2308. https://doi.org/10.1137/15M103532X
  • J. Sun, J. Yong, Linear quadratic stochastic differential games: open-loop and closed-loop saddle points, SIAM J. Control Optim. 52 (2014) 4082–4121. https://doi.org/10.1137/140953642
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite stochastic linear quadratic control and generalized differential Riccati equation, SIAM J. Control Optim. 40 (2002) 1296–1311. https://doi.org/10.1137/S0363012900371083
  • S. Chen, X. Li, X. Y. Zhou, Stochastic linear quadratic regulators with indefinite control weight costs, SIAM J. Control Optim. 36 (1998) 1685–1702. https://doi.org/10.1137/S0363012996310478
  • J. Yong, X. Y. Zhou, Stochastic Controls: Hamiltonian Systems and HJB Equations, Springer, 1999. https://doi.org/10.1007/978-1-4612-1466-3
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AnalysisDynamical Systems·Captain: mikedeng1

On Well-Posedness of Forward–Backward SDEs—A Unified Approach 3: With Constant Coefficients, σ₃ ≠ 0, σ₃h ≠ 1 the Dominating ODE Keeps y and (1 − σ₃y)⁻¹ Bounded for Every T Iff One of Four Cases HoldsResearch Paper

Motivation

A forward–backward stochastic differential equation (FBSDE) couples a forward diffusion XXX with a backward equation for a pair (Y,Z)(Y,Z)(Y,Z) whose terminal value depends on XTX_TXT​. Such systems arise from the stochastic maximum principle, from option pricing with large investors, and from stochastic differential games. Whether an FBSDE with Lipschitz coefficients has a unique solution on an arbitrary horizon [0,T][0,T][0,T] is a classical question: small-time solvability is easy, but global solvability can fail even for linear equations.

J. Ma, Z. Wu, D. Zhang and J. Zhang, On well-posedness of forward–backward SDEs—a unified approach (arXiv:1110.4658v2, Ann. Appl. Probab. 25 (2015)), reduce well-posedness to the existence of bounded solutions of two deterministic dominating ordinary differential equations, obtained from the difference quotients of the coefficients. For linear FBSDEs with constant coefficients the two dominating ODEs coincide, and the authors give sharp criteria for global solvability. This mission formalizes the criterion in the case σ3≠0\sigma_3\neq0σ3​=0, where the dominating ODE has a rational right-hand side with a pole.

Earlier global results for coupled FBSDEs rested on the four-step scheme (Ma–Protter–Yong 1994) or on monotonicity conditions (Hu–Peng 1995); §7.4 of the paper compares the dominating-ODE approach with these methods.

Setting

The linear FBSDE (4.1) with constant coefficients is determined by nine reals b1,b2,b3,σ1,σ2,σ3,f1,f2,f3b_1,b_2,b_3,\sigma_1,\sigma_2,\sigma_3,f_1,f_2,f_3b1​,b2​,b3​,σ1​,σ2​,σ3​,f1​,f2​,f3​ and a terminal slope hhh. Its dominating function is (3.9),

F(y)=f1+f2y+y(b1+b2y)+(f3+b3y) y (σ1+σ2y)1−σ3y,F(y)=f_1+f_2y+y(b_1+b_2y)+\frac{(f_3+b_3y)\,y\,(\sigma_1+\sigma_2y)}{1-\sigma_3y},F(y)=f1​+f2​y+y(b1​+b2​y)+1−σ3​y(f3​+b3​y)y(σ1​+σ2​y)​,

defined for y≠1/σ3y\neq1/\sigma_3y=1/σ3​. When σ3≠0\sigma_3\neq0σ3​=0 it can be rewritten as (5.8),

F(y)=α01/σ3−y+α1+α2y+α3y2,α3=b2−b3σ2σ3,F(y)=\frac{\alpha_0}{1/\sigma_3-y}+\alpha_1+\alpha_2y+\alpha_3y^2,\qquad \alpha_3=b_2-\frac{b_3\sigma_2}{\sigma_3},F(y)=1/σ3​−yα0​​+α1​+α2​y+α3​y2,α3​=b2​−σ3​b3​σ2​​,

for constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​. The dominating ODE (5.3) is the backward integral equation

yt=h+∫tTF(ys) ds,t∈[0,T].y_t=h+\int_t^TF(y_s)\,ds,\qquad t\in[0,T].yt​=h+∫tT​F(ys​)ds,t∈[0,T].

The paper needs a solution satisfying (5.9): both yyy and (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1 are bounded on [0,T][0,T][0,T]. Since yT=hy_T=hyT​=h, this forces σ3h≠1\sigma_3h\neq1σ3​h=1 (Remark 5.5).

The comparison tool is Lemma 5.1. For measurable F0,F1,F2F^0,F^1,F^2F0,F1,F2 it gives a unique solution of yt0=h0+∫tTF0(s,ys0) dsy^0_t=h^0+\int_t^TF^0(s,y^0_s)\,dsyt0​=h0+∫tT​F0(s,ys0​)ds lying between a sub-solution y1y^1y1 and a super-solution y2y^2y2 of perturbed equations (5.2).

Formalization targets

Goal: Theorem 5.6 (corrected)

For σ3≠0\sigma_3\neq0σ3​=0 and hσ3≠1h\sigma_3\neq1hσ3​=1, the ODE (5.3) has a solution satisfying (5.9) for every T>0T>0T>0 if and only if one of the following holds:

  1. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (−∞,h](-\infty,h](−∞,h] or α3=0\alpha_3=0α3​=0;
  2. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,∞)[h,\infty)[h,∞) or α3=0\alpha_3=0α3​=0;
  3. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,1/σ3)[h,1/\sigma_3)[h,1/σ3​) or F(y)→0F(y)\to0F(y)→0 as y↑1/σ3y\uparrow1/\sigma_3y↑1/σ3​;
  4. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (1/σ3,h](1/\sigma_3,h](1/σ3​,h] or F(y)→0F(y)\to0F(y)→0 as y↓1/σ3y\downarrow1/\sigma_3y↓1/σ3​.

The limit alternatives in cases 3 and 4 are not printed in the paper. Without them the equivalence is false. Take σ3=1\sigma_3=1σ3​=1, f1=1f_1=1f1​=1, f2=−1f_2=-1f2​=−1, all other coefficients 000, and h=0h=0h=0. Then F(y)=1−yF(y)=1-yF(y)=1−y, and yt=1−et−Ty_t=1-e^{t-T}yt​=1−et−T satisfies (5.9) on every horizon, yet none of the printed cases holds. The gap is in the Appendix (p. 48): it asserts that FFF is positive on the closed interval [h,σ3−1][h,\sigma_3^{-1}][h,σ3−1​] when α0=0\alpha_0=0α0​=0, which fails when the polynomial part vanishes at the pole. A companion item records the counterexample.

Milestones

The milestones follow the paper's proof:

  • the decomposition (5.8);
  • the comparison Lemma 5.1;
  • the three sufficiency arguments of p. 23 (case (i) with a zero, case (i) with α3=0\alpha_3=0α3​=0, case (iii));
  • the necessity bounds of the Appendix:
    • in case (i): a zero exists when α3>0\alpha_3>0α3​>0, and F(y)≤−ε(h+1−y)2F(y)\le-\varepsilon(h+1-y)^2F(y)≤−ε(h+1−y)2 when α3<0\alpha_3<0α3​<0 and there is no zero;
    • in case (iii): a zero exists when α0<0\alpha_0<0α0​<0, and F(y)≥ε(σ3−1−y)−1F(y)\ge\varepsilon(\sigma_3^{-1}-y)^{-1}F(y)≥ε(σ3−1​−y)−1 when α0>0\alpha_0>0α0​>0 and there is no zero;
  • the comparison with the explicit solution (σ3−1−y~t)2=(σ3−1−h)2−2ε(T−t)(\sigma_3^{-1}-\tilde y_t)^2=(\sigma_3^{-1}-h)^2-2\varepsilon(T-t)(σ3−1​−y~​t​)2=(σ3−1​−h)2−2ε(T−t);
  • the case α0=0\alpha_0=0α0​=0, with the endpoint positivity made a hypothesis.

Significance

In the paper, Theorem 5.6 is the sharp solvability criterion for linear FBSDEs with constant coefficients and σ3≠0\sigma_3\neq0σ3​=0. The paper describes these sharp conditions as setting the "limits" for the solvability of general FBSDEs, and the nonlinear Theorems 5.9–5.11 and the main well-posedness Theorem 7.4 are modelled on them. Because the criterion is an equivalence, it also says when no regular decoupling field can be built from the dominating ODE, whatever the horizon.

The result is proved in the paper, but the printed statement is not correct as an equivalence (see above). The mission states and asks for a corrected version, a machine-checked counterexample to the printed one, and formal versions of each step of the proof. The deterministic parts (comparison for backward integral equations, finite-time blow-up of scalar autonomous ODEs, pole-reaching for rational vector fields) are basic real analysis with no current Lean library. They are reusable well beyond FBSDEs. No part of this paper has a machine-checked proof.

Difficulty

Each sufficiency case is an a priori bound: a comparison with a constant or explicitly solvable equation keeps the solution in a fixed interval away from the pole. The difficulty is on the necessity side, where three kinds of failure must be excluded:

  • blow-up to ±∞\pm\infty±∞ when α3≠0\alpha_3\neq0α3​=0 has the wrong sign;
  • reaching the pole in finite time when α0>0\alpha_0>0α0​>0;
  • reaching the pole when α0=0\alpha_0=0α0​=0.

The obvious argument for the last case, "FFF is bounded below by a positive constant up to the pole", is exactly what fails when FFF tends to 000 at the pole. There the solution approaches the pole only asymptotically, and the right criterion is the corrected one above. A second subtlety is that FFF is only locally Lipschitz off the pole, so comparison must be carried out on a band in which the solution provably stays.

Formalization scope

Time is real, with 0≤t≤T0\le t\le T0≤t≤T and T>0T>0T>0. The coefficients form a record Coeffs of nine reals, and Coeffs.F is (3.9) verbatim. A solution on [0,T][0,T][0,T] is a function y:R→Ry:\mathbb R\to\mathbb Ry:R→R such that, for every t∈[0,T]t\in[0,T]t∈[0,T], the integrand s↦F(ys)s\mapsto F(y_s)s↦F(ys​) is integrable on [t,T][t,T][t,T] and yt=h+∫tTF(ys) dsy_t=h+\int_t^TF(y_s)\,dsyt​=h+∫tT​F(ys​)ds; values outside [0,T][0,T][0,T] are irrelevant. Condition (5.9) is a uniform bound on ∣y∣|y|∣y∣ together with ∣1−σ3yt∣≥κ|1-\sigma_3y_t|\ge\kappa∣1−σ3​yt​∣≥κ for some κ>0\kappa>0κ>0. "For arbitrary TTT" is a universal quantifier over T>0T>0T>0 outside the existential.

Lean's conventions are total, so several trivializing formalizations are ruled out explicitly:

  • Lean's integral of a non-integrable function is 000, so integrability is part of the solution predicate.
  • Lean's x/0=0x/0=0x/0=0 gives Coeffs.F a junk value at the pole. No statement evaluates FFF there: every zero point, bound and limit in the statements lives strictly on one side of 1/σ31/\sigma_31/σ3​.
  • (5.9) is never encoded as a bound on the Lean inverse (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1, which is 000 at the pole.
  • σ3≠0\sigma_3\neq0σ3​=0 is assumed wherever α3\alpha_3α3​ or 1/σ31/\sigma_31/σ3​ appears.
  • Lemma 5.1 adds the hypothesis y1≤y2y^1\le y^2y1≤y2, without which it is false, and asks the cic^ici to be integrable.

The constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​ of (5.8) enter the necessity milestones only through the decomposition hypothesis, never through a formula.

The development needs a Picard–Lindelöf or comparison argument for backward scalar integral equations with locally Lipschitz right-hand sides, monotonicity of autonomous scalar solutions, and the intermediate value theorem. Contributions of a general comparison lemma for scalar integral equations would serve this mission and both other missions of the series.

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. arXiv:1110.4658v2, doi:10.1214/14-AAP1046
  • 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. doi:10.1007/BF01192258
  • Y. Hu, S. Peng, Solution of forward–backward stochastic differential equations, Probab. Theory Related Fields 103:273–283, 1995. doi:10.1007/BF01204218
  • J. Ma, J. Yong, Forward–Backward Stochastic Differential Equations and Their Applications, Lecture Notes in Math. 1702, Springer, 1999. doi:10.1007/978-3-540-48831-6
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