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Operations ResearchOptimizationStochastic Systems·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 ResearchProbabilityStochastic Systems·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
Operations ResearchOptimization·Captain: mikedeng1

Strict Constraint Qualifications and Sequential Optimality Conditions for Constrained Optimization IV: CAKKT-Regularity Implies Abadie's Constraint QualificationResearch Paper

Motivation

Algorithms for smooth nonlinear programming, such as augmented Lagrangian, interior point and sequential quadratic programming methods, do not stop at exact Karush–Kuhn–Tucker (KKT) points. They stop at points where the KKT conditions hold approximately. Sequential optimality conditions make this precise: they are properties of sequences xk→x∗x^k\to x^*xk→x∗ with approximate multipliers, satisfied at every local minimizer without any constraint qualification, and verified by the iterates of practical methods. To conclude that a limit point is a KKT point, one still needs a condition on the constraints. Andreani, Martínez, Ramos and Silva (Optimization Online 5197, 2015; Math. Oper. Res. 43(3), 2018, doi:10.1287/moor.2017.0879) identify, for each of several sequential conditions, the weakest such condition. They call it the weakest strict constraint qualification associated with that condition, and they place each one within the classical hierarchy of constraint qualifications.

This mission concerns the Complementary AKKT condition (CAKKT) of Andreani, Martínez and Svaiter (SIAM J. Optim. 20(6), 2010). CAKKT is strictly stronger than AKKT and is satisfied by the limit points of an augmented Lagrangian method under a weak Łojasiewicz-type hypothesis. The paper's §6.1 compares the associated weakest strict CQ, CAKKT-regularity, with Abadie's constraint qualification, one of the classical conditions of nonlinear programming. The answer is that CAKKT-regularity implies Abadie's CQ, and the converse fails.

Timeline:

  • 1967: Abadie introduces the condition LΩ(x∗)=TΩ(x∗)L_\Omega(x^*)=T_\Omega(x^*)LΩ​(x∗)=TΩ​(x∗).
  • 1969: Guignard weakens it to equality of the polars.
  • 1971: Gould and Tolle prove that Guignard's condition is the weakest CQ guaranteeing KKT at local minimizers.
  • 2010: Andreani, Martínez and Svaiter introduce CAKKT.
  • 2016: Andreani, Martínez, Ramos and Silva characterize the weakest strict CQ for AKKT, the cone continuity property (SIAM J. Optim. 26(1)).
  • 2015/2018: the present paper defines CAKKT-regularity and proves Theorems 4.3 and 6.4.

Setting

Let h1,…,hm,g1,…,gp:Rn→Rh_1,\dots,h_m,g_1,\dots,g_p:\mathbb R^n\to\mathbb Rh1​,…,hm​,g1​,…,gp​:Rn→R be continuously differentiable, and let

Ω={x∈Rn: hi(x)=0 (i≤m), gj(x)≤0 (j≤p)}.\Omega=\{x\in\mathbb R^n:\ h_i(x)=0\ (i\le m),\ g_j(x)\le 0\ (j\le p)\}.Ω={x∈Rn: hi​(x)=0 (i≤m), gj​(x)≤0 (j≤p)}.

For feasible x∗x^*x∗, J(x∗)={j:gj(x∗)=0}J(x^*)=\{j: g_j(x^*)=0\}J(x∗)={j:gj​(x∗)=0} is the set of active inequalities. The polar of a set KKK is K∘={v:⟨v,k⟩≤0 ∀k∈K}K^\circ=\{v:\langle v,k\rangle\le 0\ \forall k\in K\}K∘={v:⟨v,k⟩≤0 ∀k∈K}.

  • The tangent cone TΩ(x∗)T_\Omega(x^*)TΩ​(x∗) is the set of ddd for which there are tk↓0t_k\downarrow 0tk​↓0 and dk→dd^k\to ddk→d with x∗+tkdk∈Ωx^*+t_kd^k\in\Omegax∗+tk​dk∈Ω.
  • The linearized cone is LΩ(x∗)={d:⟨∇hi(x∗),d⟩=0 ∀i, ⟨∇gj(x∗),d⟩≤0 ∀j∈J(x∗)}L_\Omega(x^*)=\{d:\langle\nabla h_i(x^*),d\rangle=0\ \forall i,\ \langle\nabla g_j(x^*),d\rangle\le 0\ \forall j\in J(x^*)\}LΩ​(x∗)={d:⟨∇hi​(x∗),d⟩=0 ∀i, ⟨∇gj​(x∗),d⟩≤0 ∀j∈J(x∗)}.
  • The regular normal cone N^Ω(z)\widehat N_\Omega(z)NΩ​(z) is the set of www with ⟨w,y−z⟩≤o(∥y−z∥)\langle w,y-z\rangle\le o(\|y-z\|)⟨w,y−z⟩≤o(∥y−z∥) for y∈Ωy\in\Omegay∈Ω.
  • The limiting normal cone NΩ(x∗)N_\Omega(x^*)NΩ​(x∗) is the set of limits of wk∈N^Ω(zk)w^k\in\widehat N_\Omega(z^k)wk∈NΩ​(zk) along zk→x∗z^k\to x^*zk→x∗ in Ω\OmegaΩ.

Abadie's CQ holds at x∗x^*x∗ when LΩ(x∗)=TΩ(x∗)L_\Omega(x^*)=T_\Omega(x^*)LΩ​(x∗)=TΩ​(x∗).

An objective fff satisfies CAKKT at x∗x^*x∗ if there are xk→x∗x^k\to x^*xk→x∗, λk∈Rm\lambda^k\in\mathbb R^mλk∈Rm and μk∈R+p\mu^k\in\mathbb R^p_+μk∈R+p​ with

∇f(xk)+∑iλik∇hi(xk)+∑jμjk∇gj(xk)→0,∑i∣λikhi(xk)∣+∑j∣μjkgj(xk)∣→0.\nabla f(x^k)+\sum_i\lambda_i^k\nabla h_i(x^k)+\sum_j\mu_j^k\nabla g_j(x^k)\to 0,\qquad \sum_i|\lambda_i^kh_i(x^k)|+\sum_j|\mu_j^kg_j(x^k)|\to 0.∇f(xk)+i∑​λik​∇hi​(xk)+j∑​μjk​∇gj​(xk)→0,i∑​∣λik​hi​(xk)∣+j∑​∣μjk​gj​(xk)∣→0.

For x∈Rnx\in\mathbb R^nx∈Rn and r≥0r\ge 0r≥0, let KC(x,r)K_C(x,r)KC​(x,r) be the set of vectors ∑iλi∇hi(x)+∑j∈J(x∗)μj∇gj(x)\sum_i\lambda_i\nabla h_i(x)+\sum_{j\in J(x^*)}\mu_j\nabla g_j(x)∑i​λi​∇hi​(x)+∑j∈J(x∗)​μj​∇gj​(x) with μ≥0\mu\ge 0μ≥0 and ∑i∣λihi(x)∣+∑j∈J(x∗)∣μjgj(x)∣≤r\sum_i|\lambda_ih_i(x)|+\sum_{j\in J(x^*)}|\mu_jg_j(x)|\le r∑i​∣λi​hi​(x)∣+∑j∈J(x∗)​∣μj​gj​(x)∣≤r. The point x∗x^*x∗ is CAKKT-regular if (x,r)⇉KC(x,r)(x,r)\rightrightarrows K_C(x,r)(x,r)⇉KC​(x,r) is outer semicontinuous at (x∗,0)(x^*,0)(x∗,0):

lim sup⁡(x,r)→(x∗,0)KC(x,r)⊆KC(x∗,0).\limsup_{(x,r)\to(x^*,0)}K_C(x,r)\subseteq K_C(x^*,0).(x,r)→(x∗,0)limsup​KC​(x,r)⊆KC​(x∗,0).

Formalization targets

Goal: Theorem 6.4

x∗∈Ω CAKKT-regular⟹LΩ(x∗)=TΩ(x∗).x^*\in\Omega\ \text{CAKKT-regular}\quad\Longrightarrow\quad L_\Omega(x^*)=T_\Omega(x^*).x∗∈Ω CAKKT-regular⟹LΩ​(x∗)=TΩ​(x∗).

Milestones

The inclusion TΩ(x∗)⊆LΩ(x∗)T_\Omega(x^*)\subseteq L_\Omega(x^*)TΩ​(x∗)⊆LΩ​(x∗) always holds, so the content of the goal is the reverse inclusion. The milestones are the statements the paper's proof uses, in attack order:

  1. Lemma 6.1: every y∈TΩ(xˉ)∘y\in T_\Omega(\bar x)^\circy∈TΩ​(xˉ)∘ equals −∇F(xˉ)-\nabla F(\bar x)−∇F(xˉ) for a C1C^1C1 function FFF that has a strict global minimum over Ω\OmegaΩ at xˉ\bar xxˉ.
  2. Lemma 6.2: such a yyy is the limit of multiplier combinations ωk\omega^kωk at points xk→xˉx^k\to\bar xxk→xˉ. The multipliers satisfy μjk=ckmax⁡{0,gj(xk)}\mu^k_j=c_k\max\{0,g_j(x^k)\}μjk​=ck​max{0,gj​(xk)}, and the complementarity residual rkr^krk tends to 000.
  3. N^S(z)=TS(z)∘\widehat N_S(z)=T_S(z)^\circNS​(z)=TS​(z)∘ for every set SSS.
  4. TΩ(x∗)⊆LΩ(x∗)T_\Omega(x^*)\subseteq L_\Omega(x^*)TΩ​(x∗)⊆LΩ​(x∗).
  5. KC(x∗,0)=LΩ(x∗)∘K_C(x^*,0)=L_\Omega(x^*)^\circKC​(x∗,0)=LΩ​(x∗)∘.
  6. Under CAKKT-regularity, NΩ(x∗)⊆LΩ(x∗)∘N_\Omega(x^*)\subseteq L_\Omega(x^*)^\circNΩ​(x∗)⊆LΩ​(x∗)∘.
  7. NS(z)∘⊆TS(z)N_S(z)^\circ\subseteq T_S(z)NS​(z)∘⊆TS​(z) for closed SSS.

Companion: Theorem 4.3

x∗ CAKKT-regular  ⟺  (∀f∈C1: CAKKT at x∗⇒KKT at x∗),x^*\ \text{CAKKT-regular}\iff\big(\forall f\in C^1:\ \text{CAKKT at }x^*\Rightarrow\text{KKT at }x^*\big),x∗ CAKKT-regular⟺(∀f∈C1: CAKKT at x∗⇒KKT at x∗),

with the equivalence of the two formulations (4.12)–(4.13) and (4.14)–(4.15) of CAKKT as a milestone.

Significance

Theorem 6.4 places CAKKT-regularity in the classical hierarchy. Every point at which CAKKT forces KKT for all objectives also satisfies Abadie's CQ, and therefore Guignard's. The paper's Example 6.1 shows that Abadie's CQ does not imply CAKKT-regularity. A convergence theorem for an algorithm that produces CAKKT sequences therefore cannot be stated under Abadie's CQ alone. Together with Theorem 4.3, this fixes exactly what a CAKKT-based method needs from the constraints.

The results are proved in the paper. None of them, and none of the variational-analysis facts they rest on, is formalized on Prove2Me, and Mathlib has no regular or limiting normal cones of nonconvex sets. The work is to formalize the paper's proof together with the parts of Rockafellar–Wets it cites: Theorem 6.11 (gradients of smooth functions as normals), Proposition 6.5, and Theorems 6.26 and 6.28(b). The last is Clarke's theorem that the regular tangent cone of a closed set is the polar of its limiting normal cone. These facts are reusable well beyond this mission.

Difficulty

The inclusion TΩ⊆LΩT_\Omega\subseteq L_\OmegaTΩ​⊆LΩ​ is elementary. The reverse inclusion cannot be obtained from CAKKT-regularity at x∗x^*x∗ alone, because CAKKT-regularity is a statement about multiplier combinations, which live on the polar side. The argument therefore has to pass through normal cones at points xk≠x∗x^k\ne x^*xk=x∗ near x∗x^*x∗. At such points the active set may differ from J(x∗)J(x^*)J(x∗), and the complementarity residual must be controlled uniformly. Returning from polars to cones requires the passage from the limiting normal cone to the tangent cone (milestone 7). That is a deep fact about closed sets in finite dimension; it is not a formal manipulation of cones. Equality of polars would only give Guignard's CQ.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n), indices are Fin m and Fin p, and gradients are Mathlib's gradient. The objects are:

  • Constraints. The constraints are a structure Constraints n m p of two index families. Every theorem assumes IsC1 (each hih_ihi​ and gjg_jgj​ is C1C^1C1, the paper's standing hypothesis) and feasibility of x∗x^*x∗.
  • KKT is the multiplier form, with μ≥0\mu\ge 0μ≥0 and μj=0\mu_j=0μj​=0 off J(x∗)J(x^*)J(x∗).
  • Cones. The tangent cone uses positive scalars tk→0t_k\to 0tk​→0 (Mathlib's tangentConeAt allows negative scalars and is not used). The regular normal cone is empty off the set. The limiting normal cone and outer semicontinuity use the sequential Painlevé–Kuratowski outer limit, and the outer limit in CAKKT-regularity is taken over pairs with r≥0r\ge 0r≥0.
  • CAKKT includes xk→x∗x^k\to x^*xk→x∗. The page's (4.12)–(4.13) omit it, but p. 1 and (4.14)–(4.15) make it part of the condition.
  • Sums over J(x∗)J(x^*)J(x∗) are written over all indices, with the multipliers forced to 000 off J(x∗)J(x^*)J(x∗).
  • Abadie's CQ is the equality of cones of p. 5. The proof's "TΩ(x∗)=LΩ(x∗)∘T_\Omega(x^*)=L_\Omega(x^*)^\circTΩ​(x∗)=LΩ​(x∗)∘" is a misprint and is not copied.
  • Closedness of Ω\OmegaΩ is not assumed; it follows from continuity.

The following would trivialize the goal and are excluded:

  • a normal cone that is nonempty outside the set;
  • the convex normal cone used for the nonconvex Ω\OmegaΩ;
  • KKT without the sign or complementarity conditions;
  • for Theorem 4.3, an objective quantified outside the equivalence;
  • Abadie's CQ weakened to equality of polars.

A complete development needs Clarke's tangent–normal polarity for closed sets in Rn\mathbb R^nRn, the existence of C1C^1C1 functions realizing regular normals, and a penalty argument for Lemma 6.2. Proofs of the general variational-analysis milestones (3 and 7) are especially welcome, since they serve any mission on nonconvex constraint sets.

Selected references

  • R. Andreani, J. M. Martínez, A. Ramos, P. J. S. Silva, Strict constraint qualifications and sequential optimality conditions for constrained optimization, Optimization Online 5197, 2015 (https://optimization-online.org/wp-content/uploads/2015/11/5197.pdf); Math. Oper. Res. 43(3), 2018. https://doi.org/10.1287/moor.2017.0879
  • R. Andreani, J. M. Martínez, B. F. Svaiter, A new sequential optimality condition for constrained optimization and algorithmic consequences, SIAM J. Optim. 20(6):3533–3554, 2010. https://doi.org/10.1137/090777189
  • R. Andreani, J. M. Martínez, A. Ramos, P. J. S. Silva, A cone-continuity constraint qualification and algorithmic consequences, SIAM J. Optim. 26(1):96–110, 2016. https://doi.org/10.1137/15M1008488
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
  • F. J. Gould, J. W. Tolle, A necessary and sufficient qualification for constrained optimization, SIAM J. Appl. Math. 20(2):164–172, 1971. https://doi.org/10.1137/0120021
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Bandit AlgorithmsOperations ResearchProbability+1·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 ResearchProbabilityStochastic Systems·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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Algorithmic Game TheoryOperations ResearchProbability·Captain: mikedeng1

Prophet Secretary Through Blind Strategies 1: A Nonincreasing Blind Strategy Earns at Least 0.669 of the Prophet's Expected Maximum When Values Arrive in Uniformly Random OrderResearch Paper

Motivation

In the prophet inequality a gambler observes independent nonnegative random values V1,…,VnV_1,\dots,V_nV1​,…,Vn​ with known laws one at a time and must decide irrevocably, after seeing each one, whether to stop and keep it. Her expected reward is compared with that of a prophet who knows all realizations and earns E(max⁡iVi)\mathbb E(\max_i V_i)E(maxi​Vi​). When the values arrive in a fixed adversarial order the best guarantee is 1/21/21/2 (Krengel, Sucheston and Garling, 1977; Samuel-Cahn, 1984). Prophet inequalities are the stopping-theoretic core of posted-price mechanisms in online auctions, where a guarantee for the gambler translates into a welfare or revenue approximation for sequential pricing.

The prophet secretary problem keeps arbitrary independent laws but lets the values arrive in a uniformly random order, as in the secretary problem.

  • 2015: Esfandiari, HajiAghayi, Liaghat and Monemizadeh introduce the problem and give a 1−1/e≈0.6321-1/e\approx0.6321−1/e≈0.632 guarantee with nnn time-dependent thresholds (ESA 2015).
  • 2017: Ehsani, Hajiaghayi, Kesselheim and Singla obtain 1−1/e1-1/e1−1/e with a single threshold, using random tie-breaking (SODA 2018).
  • 2018: Azar, Chiplunkar and Kaplan surpass 1−1/e1-1/e1−1/e by a small margin and give an upper bound of 11/1511/1511/15 for deterministic distribution-insensitive algorithms (EC 2018).
  • 2019: Correa, Saona and Ziliotto break 1−1/e1-1/e1−1/e, proving 0.6690.6690.669 with blind strategies, and show that no algorithm beats 3−1\sqrt3-13​−1 (arXiv:1807.07483; Mathematical Programming, doi:10.1007/s10107-020-01544-8). This mission formalizes the 0.6690.6690.669 guarantee.

Setting

An instance is a list of laws F1,…,FnF_1,\dots,F_nF1​,…,Fn​ of independent nonnegative random variables V1,…,VnV_1,\dots,V_nV1​,…,Vn​, all continuous. A uniformly random permutation σ\sigmaσ of [n]={1,…,n}[n]=\{1,\dots,n\}[n]={1,…,n}, independent of the values, is the arrival order: at time jjj the gambler sees VσjV_{\sigma_j}Vσj​​.

The time threshold algorithm TTAτ1,…,τn\mathrm{TTA}_{\tau_1,\dots,\tau_n}TTAτ1​,…,τn​​ stops at the first time jjj with Vσj>τjV_{\sigma_j}>\tau_jVσj​​>τj​. Its stopping time is T=inf⁡{j∈[n]:Vσj>τj}T=\inf\{j\in[n]:V_{\sigma_j}>\tau_j\}T=inf{j∈[n]:Vσj​​>τj​} and the gambler's reward is VσT1T<∞V_{\sigma_T}\mathbf 1_{T<\infty}VσT​​1T<∞​, written VσTV_{\sigma_T}VσT​​.

A blind strategy is a nonincreasing function α:[0,1]→[0,1]\alpha:[0,1]\to[0,1]α:[0,1]→[0,1]. Given an instance, draw u1,…,unu_1,\dots,u_nu1​,…,un​ independently and uniformly from [0,1][0,1][0,1], let u[j]u_{[j]}u[j]​ be the jjj-th smallest, and choose thresholds by

P(max⁡i∈[n]Vi≤τj)=α(u[j]).\mathbb P\big(\max_{i\in[n]}V_i\le\tau_j\big)=\alpha(u_{[j]}).P(i∈[n]max​Vi​≤τj​)=α(u[j]​).

The strategy is called blind because α\alphaα fixes the levels of the distribution of the maximum at which the gambler stops, independently of the instance and of nnn. The deterministic blind strategy (Definition 3.1) uses α(j/n)\alpha(j/n)α(j/n) in place of α(u[j])\alpha(u_{[j]})α(u[j]​). A piecewise-constant strategy αα1,…,αm(x)=∑j∈[m]αj1[j−1m,jm)(x)\alpha_{\alpha_1,\dots,\alpha_m}(x)=\sum_{j\in[m]}\alpha_j\mathbf 1_{[\frac{j-1}m,\frac jm)}(x)αα1​,…,αm​​(x)=∑j∈[m]​αj​1[mj−1​,mj​)​(x) uses at most mmm distinct levels.

Formalization targets

Goal: Theorem 1.1

There is a nonincreasing α:[0,1]→[0,1]\alpha:[0,1]\to[0,1]α:[0,1]→[0,1] such that, for every nnn and every continuous instance,

E(VσT)  ≥  0.669  E(max⁡i∈[n]Vi),\mathbb E(V_{\sigma_T})\;\ge\;0.669\;\mathbb E\big(\max_{i\in[n]}V_i\big),E(VσT​​)≥0.669E(i∈[n]max​Vi​),

where TTT is the stopping time of the blind strategy α\alphaα. One α\alphaα serves every instance.

Milestones, in the order the proof uses them

  1. §3, display after Definition 3.1: the blind strategy's value is the limit of the deterministic blind strategy's values on the instance padded with mmm zeros, as m→∞m\to\inftym→∞.
  2. Lemma 3.1: an exact formula for P(VσT>t)\mathbb P(V_{\sigma_T}>t)P(VσT​​>t) for nonincreasing thresholds.
  3. Lemma 3.3: 1n∑j∈[k](1−αj)≤P(T≤k)≤1−(∏j≤kαj)1/n\frac1n\sum_{j\in[k]}(1-\alpha_j)\le\mathbb P(T\le k)\le1-(\prod_{j\le k}\alpha_j)^{1/n}n1​∑j∈[k]​(1−αj​)≤P(T≤k)≤1−(∏j≤k​αj​)1/n.
  4. Lemma 4.1: P(T≥k∣σk=i)≥P(T>k)/(1−kn+1n∑l∈[k]P(Vi≤τl))\mathbb P(T\ge k\mid\sigma_k=i)\ge\mathbb P(T>k)\big/\big(1-\frac kn+\frac1n\sum_{l\in[k]}\mathbb P(V_i\le\tau_l)\big)P(T≥k∣σk​=i)≥P(T>k)/(1−nk​+n1​∑l∈[k]​P(Vi​≤τl​)).
  5. Lemma 4.2: a weighted replacement of the union bound ∑iP(Vi>t)≥P(max⁡iVi>t)\sum_i\mathbb P(V_i>t)\ge\mathbb P(\max_iV_i>t)∑i​P(Vi​>t)≥P(maxi​Vi​>t).
  6. Lemma 4.3: for α=αα1,…,αm\alpha=\alpha_{\alpha_1,\dots,\alpha_m}α=αα1​,…,αm​​ with αm>0\alpha_m>0αm​>0, E(VσT)≥min⁡j∈[m+1]fj(α1,…,αm) E(max⁡iVi)\mathbb E(V_{\sigma_T})\ge\min_{j\in[m+1]}f_j(\alpha_1,\dots,\alpha_m)\,\mathbb E(\max_iV_i)E(VσT​​)≥minj∈[m+1]​fj​(α1​,…,αm​)E(maxi​Vi​) for explicit functions fjf_jfj​.
  7. Corollary 4.4: some 1≥α1≥⋯≥αm≥01\ge\alpha_1\ge\dots\ge\alpha_m\ge01≥α1​≥⋯≥αm​≥0 gives the constant 0.669750.669750.66975; the paper reports that m=30m=30m=30 suffices.

Significance

Theorem 1.1 raised the guarantee for the prophet secretary problem from just above 1−1/e1-1/e1−1/e to 0.6690.6690.669, and it separates random-order arrival from adversarial arrival by more than the classical single-threshold analysis. The strategies are distribution-insensitive in a precise sense: the gambler needs only the distribution of the maximum, not the individual laws, and α\alphaα does not depend on nnn. The milestones are general facts about multi-threshold stopping in random order (Lemmas 3.1, 3.3, 4.1, 4.2) that apply to any nonincreasing thresholds, not only to blind ones.

The result is proved in the paper, with one numerical step: Corollary 4.4 evaluates the bound of Lemma 4.3 at a specific vector (α1,…,α30)(\alpha_1,\dots,\alpha_{30})(α1​,…,α30​) found by optimization, which the paper does not print. No part of this argument has a machine-checked proof. The formalization would make the reduction from blind to deterministic strategies, the stopping-time estimates and the final numerical certificate explicit and checked. The paper also shows that no blind strategy guarantees more than 0.6750.6750.675 (Theorem 1.2, outside this mission); any later improvement of the constant leaves this goal, which asserts only 0.6690.6690.669, intact.

Difficulty

The obvious argument fixes a threshold and bounds the probability that some value exceeds it; with one threshold this cannot beat 1−1/e1-1/e1−1/e, and with time-varying thresholds the events "the gambler has not stopped by time kkk" and "value iii arrives at time kkk" are dependent, because the arrival of iii at time kkk removes iii from the earlier times. The union bound ∑iP(Vi>t)≥P(max⁡iVi>t)\sum_i\mathbb P(V_i>t)\ge\mathbb P(\max_iV_i>t)∑i​P(Vi​>t)≥P(maxi​Vi​>t) loses exactly the constant one is trying to gain. The analysis must therefore bound the law of the stopping time uniformly over all instances (Lemma 3.3), sharpen the conditional survival probability (Lemma 4.1) and the union bound (Lemma 4.2), and then pass to the limit of large instances. The final constant depends on a numerical optimization over m=30m=30m=30 levels, so the closing step is a certified evaluation of an explicit but long expression involving mmm-th roots and logarithms.

Formalization scope

All statements import one definitions file, BlindProphetSec.Blind.Setting.

  • Instances: μ : Fin n → Measure ℝ with IsProbabilityMeasure, NullSingletonClass (continuity, the paper's standing assumption of §1.2 and §3) and μ i (Set.Iio 0) = 0 (nonnegativity). Independence is built in: the values are the coordinates of Measure.pi μ. Indices and times are 0-based; the paper's time jjj is j.val + 1.
  • Random order: the average over all n!n!n! permutations. A conditional probability P(⋅∣σk=i)\mathbb P(\cdot\mid\sigma_k=i)P(⋅∣σk​=i) is written n P(⋅, σk=i)n\,\mathbb P(\cdot,\ \sigma_k=i)nP(⋅, σk​=i).
  • Expectations are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], so E(max⁡iVi)=∞\mathbb E(\max_iV_i)=\inftyE(maxi​Vi​)=∞ is allowed; the paper's ratios are stated multiplied out, c E(max⁡iVi)≤E(VσT)c\,\mathbb E(\max_iV_i)\le\mathbb E(V_{\sigma_T})cE(maxi​Vi​)≤E(VσT​​). The reward is 000 if the gambler never stops.
  • Thresholds of blind strategies are encoded through their levels: stop at time jjj iff α(u[j])<P(max⁡iVi≤Vσj)\alpha(u_{[j]})<\mathbb P(\max_iV_i\le V_{\sigma_j})α(u[j]​)<P(maxi​Vi​≤Vσj​​). For continuous laws this agrees almost surely with Vσj>τjV_{\sigma_j}>\tau_jVσj​​>τj​ when the level is positive; level 111 means "never stop", and at level 000, where the paper's threshold is not unique, the encoding takes the largest threshold.
  • Pinned hypotheses: E(max⁡iVi)<∞\mathbb E(\max_iV_i)<\inftyE(maxi​Vi​)<∞ in the §3 limit display; t≥0t\ge0t≥0 in Lemma 3.1 (the printed identity fails for t<0t<0t<0 because the reward is 000 on {T=∞}\{T=\infty\}{T=∞}); α1<1\alpha_1<1α1​<1 in Lemma 4.3, so that every term of fjf_jfj​ is the paper's and none is a 0/00/00/0 junk value.
  • Generalizations: Lemmas 3.1, 4.1 and 4.2 are stated without continuity, and 4.1, 4.2 without nonnegativity, as printed.

A trivializing formalization is ruled out: the strategy α\alphaα (and the vector α1,…,αm\alpha_1,\dots,\alpha_mα1​,…,αm​ of Corollary 4.4) is quantified before nnn and the instance, the constants 0.6690.6690.669 and 0.669750.669750.66975 are exact rationals, and expectations cannot collapse to 000 through non-integrability.

A complete development needs order statistics of uniform samples, exchangeability arguments for uniformly random permutations, convergence of the padded deterministic strategies, and a certified numerical evaluation of fjf_jfj​. The random-order stopping vocabulary is reusable for other prophet secretary results, including the 3−1\sqrt3-13​−1 upper bound of the companion mission. Contributions to any milestone, including partial results such as Lemma 3.2 (P(T≥k∣σk=i)≥P(T>k)\mathbb P(T\ge k\mid\sigma_k=i)\ge\mathbb P(T>k)P(T≥k∣σk​=i)≥P(T>k)), are welcome. The PDF used is the arXiv preprint, version 2 (arXiv:1807.07483v2, 12 March 2019); all labels and pages refer to it.

Selected references

  • J. Correa, R. Saona, B. Ziliotto, Prophet Secretary Through Blind Strategies, arXiv:1807.07483v2, 2019; Mathematical Programming, 2021. https://arxiv.org/abs/1807.07483, https://doi.org/10.1007/s10107-020-01544-8
  • H. Esfandiari, M. Hajiaghayi, V. Liaghat, M. Monemizadeh, Prophet Secretary, Proceedings of ESA 2015, pp. 496–508.
  • S. Ehsani, M. Hajiaghayi, T. Kesselheim, S. Singla, Prophet Secretary for Combinatorial Auctions and Matroids, Proceedings of SODA 2018, pp. 700–714.
  • Y. Azar, A. Chiplunkar, H. Kaplan, Prophet Secretary: Surpassing the 1 − 1/e Barrier, Proceedings of EC 2018, pp. 303–318.
  • E. Samuel-Cahn, Comparison of Threshold Stop Rules and Maximum for Independent Nonnegative Random Variables, The Annals of Probability 12(4), pp. 1213–1216.
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Mathematical PhysicsPartial Differential EquationsProbability+1·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+1·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+1·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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CombinatoricsOperations ResearchProbability+1·Captain: mikedeng1

Online Stochastic Matching: New Algorithms with Better Bounds 1: Every Random-Lists Algorithm Has ALG/OPT ≥ E[ALG]/E[OPT] − 2ε/(c+ε) with Probability at Least 1 − 2exp(−2nε²)Research Paper

Motivation

Online bipartite matching with stochastic arrivals models the assignment of display-advertising impressions to advertisers: requests arrive one at a time, each must be assigned irrevocably on arrival or dropped, and the arrival sequence is random rather than adversarial. Since Feldman, Mehta, Mirrokni and Muthukrishnan beat the 1−1/e1 - 1/e1−1/e barrier in the i.i.d. arrival model (FOCS 2009), a line of work has designed algorithms with better guarantees. Jaillet and Lu (Math. Oper. Res. 2014) introduce a whole class of such algorithms, the Random Lists Algorithms, and obtain ratios 0.7290.7290.729, 0.7250.7250.725 and 0.7060.7060.706 for integral arrival rates, vertex weights and general arrival rates.

Two notions of performance coexist in this literature. One compares expectations, E[ALG]/E[OPT]\mathbb E[\mathrm{ALG}]/\mathbb E[\mathrm{OPT}]E[ALG]/E[OPT]; the other asks that ALG/OPT\mathrm{ALG}/\mathrm{OPT}ALG/OPT be large on most realizations, as in Feldman et al. Section 2 of Jaillet and Lu shows that, for every algorithm of their class, the two notions are quantitatively linked by an explicit exponential tail bound. This mission formalizes that section.

Setting

A bipartite graph G={A∪I,E}G = \{A \cup I, E\}G={A∪I,E} has a finite set AAA of advertisers, a set III of impression types, and edges E⊆A×IE \subseteq A \times IE⊆A×I; (a,i)∈E(a, i) \in E(a,i)∈E means advertiser aaa is interested in type iii. A fixed number nnn of requests arrive at periods 1,…,n1, \dots, n1,…,n, and their types are drawn i.i.d. from a known distribution on III. Every advertiser can receive at most one request.

A list for type iii is an ordered sequence of advertisers interested in iii. A Random Lists Algorithm fixes, for each type iii, a distribution Di\mathcal D_iDi​ over lists (constructed from an LP solution; the construction is irrelevant here). When a request of type iii arrives it draws a list from Di\mathcal D_iDi​ and assigns the request to the first advertiser on the list not yet matched, or drops it if every listed advertiser is matched.

Formally, each request carries an outcome xxx in a finite set X\mathcal XX determining its type typ(x)\mathrm{typ}(x)typ(x) and its list lst(x)\mathrm{lst}(x)lst(x); outcomes ω1,…,ωn\omega_1, \dots, \omega_nω1​,…,ωn​ are i.i.d. with law ν\nuν. Starting from W0=∅W_0 = \emptysetW0​=∅, the set WjW_jWj​ of matched advertisers after the jjj-th request is obtained from Wj−1W_{j-1}Wj−1​ by adding the first advertiser of lst(ωj)\mathrm{lst}(\omega_j)lst(ωj​) outside Wj−1W_{j-1}Wj−1​, if any. Then:

  • ALG(ω)=∣Wn∣\mathrm{ALG}(\omega) = |W_n|ALG(ω)=∣Wn​∣, the number of assigned requests;
  • OPT(ω)\mathrm{OPT}(\omega)OPT(ω) is the cardinality of a maximum matching of the realized graph, in which request jjj may go to aaa iff (a,typ(ωj))∈E(a, \mathrm{typ}(\omega_j)) \in E(a,typ(ωj​))∈E;
  • E[ALG]\mathbb E[\mathrm{ALG}]E[ALG], E[OPT]\mathbb E[\mathrm{OPT}]E[OPT] are expectations under ν⊗n\nu^{\otimes n}ν⊗n, and c=E[OPT]/nc = \mathbb E[\mathrm{OPT}]/nc=E[OPT]/n.

Formalization targets

Goal: the concluding display of Section 2 (p. 6)

If every list contains only interested advertisers, then for every n≥1n \ge 1n≥1 and every ϵ>0\epsilon > 0ϵ>0,

P(ALGOPT≥E[ALG]E[OPT]−2ϵc+ϵ)≥1−2exp⁡(−2nϵ2).\mathbb P\left(\frac{\mathrm{ALG}}{\mathrm{OPT}} \ge \frac{\mathbb E[\mathrm{ALG}]}{\mathbb E[\mathrm{OPT}]} - \frac{2\epsilon}{c + \epsilon}\right) \ge 1 - 2\exp(-2n\epsilon^2).P(OPTALG​≥E[OPT]E[ALG]​−c+ϵ2ϵ​)≥1−2exp(−2nϵ2).

It holds for every instance and every law ν\nuν, with no assumption on the size of E[OPT]\mathbb E[\mathrm{OPT}]E[OPT].

Milestones

  1. Claim 1 (p. 5). If two list sequences differ in one position, the cardinalities of the resulting matchings differ by at most one.
  2. Lemma 1 (p. 5). P(ALG−E[ALG]<−nϵ)≤exp⁡(−2nϵ2)\mathbb P(\mathrm{ALG} - \mathbb E[\mathrm{ALG}] < -n\epsilon) \le \exp(-2n\epsilon^2)P(ALG−E[ALG]<−nϵ)≤exp(−2nϵ2).
  3. Lemma 2 (p. 5). P(OPT−E[OPT]>nϵ)≤exp⁡(−2nϵ2)\mathbb P(\mathrm{OPT} - \mathbb E[\mathrm{OPT}] > n\epsilon) \le \exp(-2n\epsilon^2)P(OPT−E[OPT]>nϵ)≤exp(−2nϵ2).

A supporting theorem, not a milestone, records the fact the display uses without stating it: with interested lists, ALG≤OPT\mathrm{ALG} \le \mathrm{OPT}ALG≤OPT on every realization.

Significance

The display shows that the paper's guarantees, proved for the ratio of expectations, transfer to realizations: when E[OPT]=Θ(n)\mathbb E[\mathrm{OPT}] = \Theta(n)E[OPT]=Θ(n), ALG/OPT\mathrm{ALG}/\mathrm{OPT}ALG/OPT is at least E[ALG]/E[OPT]−O(ϵ)\mathbb E[\mathrm{ALG}]/\mathbb E[\mathrm{OPT}] - O(\epsilon)E[ALG]/E[OPT]−O(ϵ) except with probability 2e−2nϵ22e^{-2n\epsilon^2}2e−2nϵ2. It applies uniformly to the whole class of Random Lists Algorithms, whatever the LP and the list distributions, so it covers each of the paper's later algorithms at once.

The result is proved in the paper; nothing about it is open. It has no machine-checked proof. Formalizing it produces a precise model of list-based online matching (the greedy run, the realization-graph optimum, the joint type–list law) that later formalizations of the paper's competitive ratios can build on, and a worked application of the bounded-differences method to a combinatorial online algorithm.

Difficulty

The concluding display is elementary once Lemmas 1 and 2 are available. The two lemmas need McDiarmid's bounded-differences inequality in one-sided form, which Mathlib does not provide, and the bounded-difference properties of ALG and OPT.

Claim 1 is the step where the naive argument fails. Changing one list can change the assignment of every later request, so ALG is not a sum of local contributions, and a single changed list could a priori cascade into many changed assignments; the claim asserts that the cascade never changes the total by more than one. The analogous property for OPT (changing one request's type moves the maximum matching by at most one) is used in Lemma 2's proof but is not stated in the paper.

Formalization scope

  • Arrivals. Outcomes live in a finite type X\mathcal XX with the discrete σ-algebra, and the law of the arrivals is the product measure ν⊗n\nu^{\otimes n}ν⊗n (Measure.pi). Any joint law of type and list is allowed; every Random Lists Algorithm is the case X={(i,l)}\mathcal X = \{(i, l)\}X={(i,l)}, ν(i,l)=pi Di(l)\nu(i, l) = p_i\,\mathcal D_i(l)ν(i,l)=pi​Di​(l). Types and lists are not modelled as independent sequences, which would break ALG≤OPT\mathrm{ALG} \le \mathrm{OPT}ALG≤OPT.
  • Expectations are Bochner integrals of functions on the finite space Xn\mathcal X^nXn, hence honest finite sums.
  • Matchings. OPT is the maximum size of a partial assignment Fin n → Option A that uses only edges and gives each advertiser at most one request; the empty assignment qualifies, so the maximum is over a nonempty set. ALG is ∣Wn∣|W_n|∣Wn​∣ for the greedy recursion.
  • Pinned hypotheses. The goal assumes n≥1n \ge 1n≥1 (the paper's c=E[OPT]/nc = \mathbb E[\mathrm{OPT}]/nc=E[OPT]/n) and that every list only contains interested advertisers (stated in §2, p. 5). Claim 1 and Lemma 1 hold for arbitrary lists and carry neither hypothesis. Lists need not be nonempty or repetition-free.
  • Division by zero. No hypothesis E[OPT]>0\mathbb E[\mathrm{OPT}] > 0E[OPT]>0 or OPT>0\mathrm{OPT} > 0OPT>0 is made. On realizations with OPT=0\mathrm{OPT} = 0OPT=0, and when E[OPT]=0\mathbb E[\mathrm{OPT}] = 0E[OPT]=0, Lean's x/0=0x/0 = 0x/0=0 applies; the statement remains true under it, and adding a positivity hypothesis would weaken the result.
  • Not posed. Theorems 1–3 (the competitive ratios, which hold up to 1+O(1/n)1 + O(1/n)1+O(1/n)) and the LP constructions of the algorithms are out of scope. McDiarmid's inequality is a proof tool, not an item. A one-sided version is posed elsewhere on the platform and not yet proved.

Contributions welcome: a one-sided McDiarmid inequality for Measure.pi (reusable well beyond this mission), the bounded-difference property of maximum bipartite matchings, and Claim 1.

Selected references

  • P. Jaillet and X. Lu, Online Stochastic Matching: New Algorithms with Better Bounds, Mathematics of Operations Research 39(3), 2014; accepted manuscript, rev. June 2013. https://doi.org/10.1287/moor.2013.0621
  • J. Feldman, A. Mehta, V. Mirrokni and S. Muthukrishnan, Online Stochastic Matching: Beating 1 − 1/e, FOCS 2009. https://arxiv.org/abs/0905.4100
  • C. McDiarmid, On the method of bounded differences, Surveys in Combinatorics, London Math. Soc. Lecture Note Series 141, 1989. https://doi.org/10.1017/CBO9781107359949.008
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Mathematical PhysicsPartial Differential EquationsProbability+1·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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Actuarial ScienceOperations ResearchProbability·Captain: mikedeng1

Inf-Convolution, Optimal Allocations, and Model Uncertainty for Tail Risk Measures II: The Inf-Convolution of a VaR and a Monetary Tail Risk Measure, Its Optimal Allocation and Its Tail ParameterResearch Paper

Motivation

Banks and insurers hold capital against the risk of their positions, and regulators compute that capital with a risk measure, a functional that maps a random loss to a number. The two standard ones are the Value-at-Risk (VaR), a quantile of the loss, and the Expected Shortfall, an average of the upper quantiles (BCBS 2019). Both look only at the upper tail of the loss distribution. Liu and Wang (2021) called such functionals tail risk measures.

When a total loss XXX is split among several agents, each judging its share with its own risk measure, the smallest total capital achievable is the inf-convolution of the agents' risk measures, and a split attaining it is an optimal allocation. Embrechts, Liu and Wang (2018) computed the inf-convolution for VaR and Expected Shortfall agents. Liu, Mao, Wang and Wei (SSRN 3490348, version of January 16, 2022; published in Mathematics of Operations Research, 2022) extend this to agents with general tail risk measures. This mission formalizes their Theorem 2: one agent uses a VaR, the other an arbitrary monetary tail risk measure.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be an atomless probability space: every event of positive probability contains an event of strictly smaller positive probability. A random variable XXX is a measurable map Ω→R\Omega\to\mathbb RΩ→R, a positive value being a loss, and L0L^0L0 is the set of all of them. Its distribution function is FX(x)=P(X≤x)F_X(x)=\mathbb P(X\le x)FX​(x)=P(X≤x). For a level α∈(0,1)\alpha\in(0,1)α∈(0,1) the left and right VaR are

VaRαL(X)=inf⁡{x:FX(x)≥1−α},VaRαR(X)=inf⁡{x:FX(x)>1−α}.\mathrm{VaR}^L_\alpha(X)=\inf\{x: F_X(x)\ge 1-\alpha\},\qquad \mathrm{VaR}^R_\alpha(X)=\inf\{x: F_X(x)>1-\alpha\}.VaRαL​(X)=inf{x:FX​(x)≥1−α},VaRαR​(X)=inf{x:FX​(x)>1−α}.

A small α\alphaα is a high quantile. The quantile function is FX−1(p)=VaR1−pL(X)F_X^{-1}(p)=\mathrm{VaR}^L_{1-p}(X)FX−1​(p)=VaR1−pL​(X), and UXU_XUX​ denotes a random variable that is uniform on [0,1][0,1][0,1] with FX−1(UX)=XF^{-1}_X(U_X)=XFX−1​(UX​)=X almost surely.

A risk measure ρ\rhoρ is monotone if X≤YX\le YX≤Y a.s. implies ρ(X)≤ρ(Y)\rho(X)\le\rho(Y)ρ(X)≤ρ(Y). It is translation-invariant if ρ(X−m)=ρ(X)−m\rho(X-m)=\rho(X)-mρ(X−m)=ρ(X)−m for every constant mmm, and monetary if it is both. For p∈(0,1)p\in(0,1)p∈(0,1), the ppp-tail XpX_pXp​ of XXX has distribution function (FX(x)−(1−p))+/p(F_X(x)-(1-p))_+/p(FX​(x)−(1−p))+​/p (display (6) of the paper). A risk measure ρ\rhoρ is a ppp-tail risk measure if ρ(X)=ρ(Y)\rho(X)=\rho(Y)ρ(X)=ρ(Y) whenever XpX_pXp​ and YpY_pYp​ have the same law.

The allocations of XXX between two agents are the pairs (X1,X2)(X_1,X_2)(X1​,X2​) with X1+X2=XX_1+X_2=XX1​+X2​=X, and the inf-convolution is

ρ1 □ ρ2(X)=inf⁡{ρ1(X1)+ρ2(X2):X1+X2=X}∈[−∞,∞).\rho_1\,\square\,\rho_2(X)=\inf\{\rho_1(X_1)+\rho_2(X_2): X_1+X_2=X\}\in[-\infty,\infty).ρ1​□ρ2​(X)=inf{ρ1​(X1​)+ρ2​(X2​):X1​+X2​=X}∈[−∞,∞).

For ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1) and α∈(0,1−ε)\alpha\in(0,1-\varepsilon)α∈(0,1−ε) the paper introduces the truncation

X[α]=X 1{UX≤1−α}+VaRα+εR(X) 1{UX>1−α}.X^{[\alpha]}=X\,\mathbb 1_{\{U_X\le 1-\alpha\}}+\mathrm{VaR}^R_{\alpha+\varepsilon}(X)\,\mathbb 1_{\{U_X>1-\alpha\}}.X[α]=X1{UX​≤1−α}​+VaRα+εR​(X)1{UX​>1−α}​.

Formalization targets

Goal: Theorem 2 (p. 13)

Let ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1), let ρ\rhoρ be a monetary ε\varepsilonε-tail risk measure, and let α∈(0,1−ε)\alpha\in(0,1-\varepsilon)α∈(0,1−ε). For every X∈L0X\in L^0X∈L0 and every choice of UXU_XUX​:

VaRαL □ ρ(X)=ρ(X[α]);\mathrm{VaR}^L_\alpha\,\square\,\rho(X)=\rho\big(X^{[\alpha]}\big);VaRαL​□ρ(X)=ρ(X[α]);
  1. (X−X[α],X[α])(X-X^{[\alpha]},X^{[\alpha]})(X−X[α],X[α]) is an optimal allocation of XXX for (VaRαL,ρ)(\mathrm{VaR}^L_\alpha,\rho)(VaRαL​,ρ);
VaRαR □ ρ(X)=lim⁡δ↓0ρ(X[α−δ]);\mathrm{VaR}^R_\alpha\,\square\,\rho(X)=\lim_{\delta\downarrow0}\rho\big(X^{[\alpha-\delta]}\big);VaRαR​□ρ(X)=δ↓0lim​ρ(X[α−δ]);
  1. VaRαR □ ρ\mathrm{VaR}^R_\alpha\,\square\,\rhoVaRαR​□ρ and VaRαL □ ρ\mathrm{VaR}^L_\alpha\,\square\,\rhoVaRαL​□ρ are monetary (α+ε)(\alpha+\varepsilon)(α+ε)-tail risk measures.

Milestones

  • (17), p. 13. The distribution function of X[α]X^{[\alpha]}X[α] is FXF_XFX​ below VaRα+εR(X)\mathrm{VaR}^R_{\alpha+\varepsilon}(X)VaRα+εR​(X), equals FX+αF_X+\alphaFX​+α from there up to VaRαL(X)\mathrm{VaR}^L_\alpha(X)VaRαL​(X), and equals 111 from VaRαL(X)\mathrm{VaR}^L_\alpha(X)VaRαL​(X) on.
  • (18), p. 13. VaRεR(X[α])=VaRα+εR(X)\mathrm{VaR}^R_\varepsilon(X^{[\alpha]})=\mathrm{VaR}^R_{\alpha+\varepsilon}(X)VaRεR​(X[α])=VaRα+εR​(X).
  • Proof of (i), p. 14. If VaRαL(Y)=0\mathrm{VaR}^L_\alpha(Y)=0VaRαL​(Y)=0, then FX−Y(x)≤FX[α](x)F_{X-Y}(x)\le F_{X^{[\alpha]}}(x)FX−Y​(x)≤FX[α]​(x) for all x≥VaRα+εR(X)x\ge\mathrm{VaR}^R_{\alpha+\varepsilon}(X)x≥VaRα+εR​(X).
  • Proof of (iv), p. 15. If Yα+εY_{\alpha+\varepsilon}Yα+ε​ and Zα+εZ_{\alpha+\varepsilon}Zα+ε​ have the same law, then so do (Y[α−δ])ε(Y^{[\alpha-\delta]})_\varepsilon(Y[α−δ])ε​ and (Z[α−δ])ε(Z^{[\alpha-\delta]})_\varepsilon(Z[α−δ])ε​ for every δ∈[0,α)\delta\in[0,\alpha)δ∈[0,α).

Significance

Theorem 2 gives a closed form for the inf-convolution and an explicit optimal allocation. The VaR agent takes the loss above the (1−α)(1-\alpha)(1−α)-quantile, minus a constant, and the other agent keeps the rest, which has the same ε\varepsilonε-tail as the truncated X[α]X^{[\alpha]}X[α]. No convexity, law-invariance or distortion structure is assumed for ρ\rhoρ beyond its being a monetary tail risk measure. The theorem generalizes Theorem 5.3 of Wang and Wei (2020, Insurance: Mathematics and Economics 93), which required a distortion risk measure. Specialized to ρ=ESβ\rho=\mathrm{ES}_\betaρ=ESβ​, it gives VaRαL □ ESβ=RVaRα,β\mathrm{VaR}^L_\alpha\,\square\,\mathrm{ES}_\beta=\mathrm{RVaR}_{\alpha,\beta}VaRαL​□ESβ​=RVaRα,β​. Part 4 says that the tail parameters add: the representative agent of a VaR and an ε\varepsilonε-tail agent is an (α+ε)(\alpha+\varepsilon)(α+ε)-tail agent. This is the two-agent instance of the paper's Theorem 3. Parts 1 and 3 together contrast the left and right VaR: an optimal allocation always exists for VaRαL\mathrm{VaR}^L_\alphaVaRαL​, while for VaRαR\mathrm{VaR}^R_\alphaVaRαR​ the value is only a limit.

The result is proved in the paper. As far as a search of the platform shows, it has no machine-checked proof, and the platform has no development of quantile-based risk measures on a general atomless probability space. The mission produces the definitions of left and right VaR, tails, tail risk measures and inf-convolution on L0L^0L0, and a checked proof of the theorem.

Difficulty

The upper bound in part 1 is a single allocation. The lower bound must hold against every allocation (Y,X−Y)(Y,X-Y)(Y,X−Y). It reduces to comparing the distribution function of X−YX-YX−Y with that of X[α]X^{[\alpha]}X[α], but only on the ε\varepsilonε-tail. Turning that comparison into ρ(X[α])≤ρ(X−Y)\rho(X^{[\alpha]})\le\rho(X-Y)ρ(X[α])≤ρ(X−Y) needs both monotonicity and the tail property of ρ\rhoρ. Monotonicity is almost-sure and pointwise, the tail property is distributional, and no coupling between X−YX-YX−Y and X[α]X^{[\alpha]}X[α] is given, so the two cannot simply be chained. Part 3 needs an interchange of a limit and an infimum together with the one-sided continuity VaRα−δL→VaRαR\mathrm{VaR}^L_{\alpha-\delta}\to\mathrm{VaR}^R_\alphaVaRα−δL​→VaRαR​. Part 4 needs the law of the ε\varepsilonε-tail of X[α−δ]X^{[\alpha-\delta]}X[α−δ] to depend only on the (α+ε)(\alpha+\varepsilon)(α+ε)-tail of XXX. All of this rests on careful quantile bookkeeping: left versus right inverses, and strict versus weak inequalities at atoms of FXF_XFX​.

Formalization scope

Random variables are functions Ω→R\Omega\to\mathbb RΩ→R, and the domain is L0L^0L0, the measurable functions. The paper allows any convex cone containing L∞L^\inftyL∞ that is closed under equality in law and under taking tails, and fixing L0L^0L0 is one of the instances it names. The probability space is atomless, as §2.1 assumes throughout. FXF_XFX​, the VaRs and UXU_XUX​ are encoded as above. UXU_XUX​ is not chosen: parts 1–3 are asserted for every uniform UUU with FX−1(U)=XF^{-1}_X(U)=XFX−1​(U)=X a.s. The equality in law of tails is encoded through display (6), as equality of (FX−(1−p))+(F_X-(1-p))_+(FX​−(1−p))+​ and (FY−(1−p))+(F_Y-(1-p))_+(FY​−(1−p))+​. The risk measure ρ\rhoρ is real-valued; the paper allows the value −∞-\infty−∞, but the agents of §2.3 are real-valued. Monotonicity and translation invariance are required on L0L^0L0, with monotonicity for almost-sure inequalities.

Allocations sum pointwise. The inf-convolution takes values in the extended reals, so no junk value from a real infimum arises. Part 3 is a one-sided limit in the extended reals, which asserts both that the limit exists and its value. Part 4 uses extended-real versions of "monetary" and "tail risk measure". The level ranges ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1) and α∈(0,1−ε)\alpha\in(0,1-\varepsilon)α∈(0,1−ε) are hypotheses.

Dropping the tail hypothesis on ρ\rhoρ makes part 1 false: on integrable losses the expectation is monetary but not a tail risk measure. A real-valued infimum in place of the extended one would make the inf-convolution a junk 000 when it is −∞-\infty−∞. A choice of UXU_XUX​ by Classical.choose would weaken parts 1–3 to one uniform. None of these is used.

A complete development needs quantile calculus for VaRL\mathrm{VaR}^LVaRL and VaRR\mathrm{VaR}^RVaRR (right-continuity of FXF_XFX​, the Galois connection FX−1(u)≤x  ⟺  u≤FX(x)F^{-1}_X(u)\le x\iff u\le F_X(x)FX−1​(u)≤x⟺u≤FX​(x)), the distribution of FX−1(U)F^{-1}_X(U)FX−1​(U), and basic facts on infima in EReal. The quantile lemmas are reusable for every other mission of this series and for any formalization of VaR. Proofs of the milestones, and of the folklore fact that inf-convolutions of monetary risk measures are monetary, are welcome as separate contributions.

Selected references

  • F. Liu, T. Mao, R. Wang, L. Wei, Inf-convolution, optimal allocations, and model uncertainty for tail risk measures, SSRN 3490348, version of January 16, 2022; Mathematics of Operations Research, 2022. https://ssrn.com/abstract=3490348
  • F. Liu, R. Wang, A theory for measures of tail risk, Mathematics of Operations Research 46(3), 1109–1128, 2021. https://doi.org/10.1287/moor.2020.1072
  • P. Embrechts, H. Liu, R. Wang, Quantile-based risk sharing, Operations Research 66(4), 936–949, 2018. https://doi.org/10.1287/opre.2017.1716
  • R. Wang, Y. Wei, Characterizing optimal allocations in quantile-based risk sharing, Insurance: Mathematics and Economics 93, 288–300, 2020. https://doi.org/10.1016/j.insmatheco.2020.05.001
  • H. Föllmer, A. Schied, Stochastic Finance: An Introduction in Discrete Time, 4th ed., De Gruyter, 2016. https://doi.org/10.1515/9783110463453
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Optimal TransportOptimizationProbability+1·Captain: mikedeng1

Bridging Bayesian and Minimax Mean Square Error Estimation via Wasserstein Distributionally Robust Optimization 1: The Gelbrich Minimax and Normal-Prior Maximin Values Coincide (Sandwich Theorem)Research Paper

Motivation

Estimating an unknown parameter from a noisy linear measurement is the basic problem behind Kalman filtering, signal recovery and linear inverse problems. A Bayesian statistician picks the estimator that minimizes the mean square error under a prior distribution; a minimax statistician guards against the worst prior in some family. The Bayesian answer depends on a prior that is rarely known, and the minimax answer is often intractable.

Nguyen, Shafieezadeh-Abadeh, Kuhn and Mohajerin Esfahani (Math. Oper. Res. 48(1), 2023) bridge the two by letting nature choose the joint distribution of parameter and noise from a ball of radius ρ\rhoρ around a nominal distribution in the type-2 Wasserstein distance. At ρ=0\rho=0ρ=0 the problem is Bayesian; as ρ\rhoρ grows it becomes more conservative. For a normal nominal distribution they show that this distributionally robust problem is solved by an affine estimator, that a normal distribution is least favourable, and that both are computable from a finite convex program. The paper extends the Wasserstein Kalman filter of Shafieezadeh-Abadeh et al. (NeurIPS 2018), which treated a joint normal ball on (x,y)(x,y)(x,y), to the model with independent parameter and noise.

Setting

The parameter is x∈Rnx\in\mathbb R^nx∈Rn and the observation is y=Hx+w∈Rmy=Hx+w\in\mathbb R^my=Hx+w∈Rm, with a known observation matrix H∈Rm×nH\in\mathbb R^{m\times n}H∈Rm×n and noise www independent of xxx. Write M(Rd)\mathcal M(\mathbb R^d)M(Rd) for the probability distributions on Rd\mathbb R^dRd with finite second moments.

  • An estimator is a measurable ψ:Rm→Rn\psi:\mathbb R^m\to\mathbb R^nψ:Rm→Rn with ∥ψ(y)∥≤C(1+∥y∥)\|\psi(y)\|\le C(1+\|y\|)∥ψ(y)∥≤C(1+∥y∥) for some C>0C>0C>0; the family of estimators is F\mathcal FF, and A⊆F\mathcal A\subseteq\mathcal FA⊆F is the family of affine estimators ψ(y)=Ay+b\psi(y)=Ay+bψ(y)=Ay+b.
  • The average risk of ψ\psiψ under a joint distribution Q\mathbb QQ of (x,w)(x,w)(x,w) is R(ψ,Q)=EQ[∥x−ψ(Hx+w)∥2]\mathcal R(\psi,\mathbb Q)=\mathbb E_{\mathbb Q}[\|x-\psi(Hx+w)\|^2]R(ψ,Q)=EQ​[∥x−ψ(Hx+w)∥2].
  • The type-2 Wasserstein distance W(Q1,Q2)\mathbb W(\mathbb Q_1,\mathbb Q_2)W(Q1​,Q2​) is the square root of the least expected squared distance E∥ξ1−ξ2∥2\mathbb E\|\xi_1-\xi_2\|^2E∥ξ1​−ξ2​∥2 over all couplings of Q1\mathbb Q_1Q1​ and Q2\mathbb Q_2Q2​.
  • The Gelbrich distance between mean–covariance pairs is
G((μ1,Σ1),(μ2,Σ2))=∥μ1−μ2∥2+Tr⁡[Σ1+Σ2−2(Σ21/2Σ1Σ21/2)1/2].\mathbb G((\mu_1,\Sigma_1),(\mu_2,\Sigma_2))=\sqrt{\|\mu_1-\mu_2\|^2+\operatorname{Tr}\big[\Sigma_1+\Sigma_2-2(\Sigma_2^{1/2}\Sigma_1\Sigma_2^{1/2})^{1/2}\big]}.G((μ1​,Σ1​),(μ2​,Σ2​))=∥μ1​−μ2​∥2+Tr[Σ1​+Σ2​−2(Σ21/2​Σ1​Σ21/2​)1/2]​.

The nominal distribution is a product P^=P^x×P^w\widehat{\mathbb P}=\widehat{\mathbb P}_x\times\widehat{\mathbb P}_wP=Px​×Pw​ with radii ρx,ρw≥0\rho_x,\rho_w\ge0ρx​,ρw​≥0. Three ambiguity sets of product distributions Qx×Qw\mathbb Q_x\times\mathbb Q_wQx​×Qw​ appear:

  • the Wasserstein ball B(P^)\mathbb B(\widehat{\mathbb P})B(P): Qx∈M(Rn)\mathbb Q_x\in\mathcal M(\mathbb R^n)Qx​∈M(Rn), Qw∈M(Rm)\mathbb Q_w\in\mathcal M(\mathbb R^m)Qw​∈M(Rm), W(Qx,P^x)≤ρx\mathbb W(\mathbb Q_x,\widehat{\mathbb P}_x)\le\rho_xW(Qx​,Px​)≤ρx​, W(Qw,P^w)≤ρw\mathbb W(\mathbb Q_w,\widehat{\mathbb P}_w)\le\rho_wW(Qw​,Pw​)≤ρw​;
  • the Gelbrich ball G(P^)\mathbb G(\widehat{\mathbb P})G(P): the marginals' mean–covariance pairs lie within Gelbrich distance ρx\rho_xρx​, ρw\rho_wρw​ of those of P^x\widehat{\mathbb P}_xPx​, P^w\widehat{\mathbb P}_wPw​;
  • for normal P^x=N(μ^x,Σ^x)\widehat{\mathbb P}_x=\mathcal N(\widehat\mu_x,\widehat\Sigma_x)Px​=N(μ​x​,Σx​), P^w=N(μ^w,Σ^w)\widehat{\mathbb P}_w=\mathcal N(\widehat\mu_w,\widehat\Sigma_w)Pw​=N(μ​w​,Σw​), the normal ball BN(P^)\mathbb B_{\mathcal N}(\widehat{\mathbb P})BN​(P): products N(μ^x,Σx)×N(μ^w,Σw)\mathcal N(\widehat\mu_x,\Sigma_x)\times\mathcal N(\widehat\mu_w,\Sigma_w)N(μ​x​,Σx​)×N(μ​w​,Σw​) in B(P^)\mathbb B(\widehat{\mathbb P})B(P) with Σx⪰0\Sigma_x\succeq0Σx​⪰0, Σw≻0\Sigma_w\succ0Σw​≻0.

Then BN(P^)⊆B(P^)⊆G(P^)\mathbb B_{\mathcal N}(\widehat{\mathbb P})\subseteq\mathbb B(\widehat{\mathbb P})\subseteq\mathbb G(\widehat{\mathbb P})BN​(P)⊆B(P)⊆G(P).

Formalization targets

Goal: Theorem 4.1 (sandwich theorem)

For P^\widehat{\mathbb P}P normal with Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0,

inf⁡ψ∈A sup⁡Q∈G(P^) R(ψ,Q)=sup⁡Q∈BN(P^) inf⁡ψ∈F R(ψ,Q).\inf_{\psi\in\mathcal A}\ \sup_{\mathbb Q\in\mathbb G(\widehat{\mathbb P})}\ \mathcal R(\psi,\mathbb Q)=\sup_{\mathbb Q\in\mathbb B_{\mathcal N}(\widehat{\mathbb P})}\ \inf_{\psi\in\mathcal F}\ \mathcal R(\psi,\mathbb Q).ψ∈Ainf​ Q∈G(P)sup​ R(ψ,Q)=Q∈BN​(P)sup​ ψ∈Finf​ R(ψ,Q).

The left side is the Gelbrich MMSE problem (2.1), the right side the dual problem over normal priors (3.3). The Wasserstein problem (1.7), inf⁡Fsup⁡B\inf_{\mathcal F}\sup_{\mathbb B}infF​supB​, and its dual (3.1), sup⁡Binf⁡F\sup_{\mathbb B}\inf_{\mathcal F}supB​infF​, lie between them, so all four values coincide.

Milestones

  1. Proposition A.3: the closed form of sup⁡Σ⪰0⟨D,Σ⟩−γTr⁡[Σ−2(Σ^1/2ΣΣ^1/2)1/2]\sup_{\Sigma\succeq0}\langle D,\Sigma\rangle-\gamma\operatorname{Tr}[\Sigma-2(\widehat\Sigma^{1/2}\Sigma\widehat\Sigma^{1/2})^{1/2}]supΣ⪰0​⟨D,Σ⟩−γTr[Σ−2(Σ1/2ΣΣ1/2)1/2] and its maximizer.
  2. Theorem 2.7: problem (2.1) equals a finite convex program (2.2), and for ρx,ρw>0\rho_x,\rho_w>0ρx​,ρw​>0 an affine estimator attains it.
  3. Lemma A.6: the covariance Gelbrich set S\mathcal SS is convex and compact, with Tr⁡[Σ]≤(ρ+Tr⁡[Σ^]1/2)2\operatorname{Tr}[\Sigma]\le(\rho+\operatorname{Tr}[\widehat\Sigma]^{1/2})^2Tr[Σ]≤(ρ+Tr[Σ]1/2)2.
  4. Proposition A.4 (i): max⁡Σ∈S⟨D,Σ⟩\max_{\Sigma\in\mathcal S}\langle D,\Sigma\ranglemaxΣ∈S​⟨D,Σ⟩ equals a one-dimensional infimum (A.6).
  5. Lemma A.5: a max–min problem over S\mathcal SS has a maximizer Σ⋆⪰λmin⁡(Σ^)I\Sigma^\star\succeq\lambda_{\min}(\widehat\Sigma)IΣ⋆⪰λmin​(Σ)I.
  6. Display (3.5): over normal priors, affine estimators suffice.
  7. Display (3.8): for Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0 the value of (3.3) is a finite sup–inf over covariance matrices.

Companion statements, not milestones: Theorem 3.5 (problem (3.3) equals the finite program (3.4)), Corollary 4.2 (the optimal affine estimator and the optimal normal prior form a Nash equilibrium on B(P^)\mathbb B(\widehat{\mathbb P})B(P)) and Corollary 4.3 (the minimax estimator from a maximizer of (3.4)).

Significance

The sandwich theorem says that robustifying the MMSE problem against Wasserstein uncertainty around a normal distribution costs nothing in tractability: the optimal estimator is affine, the worst-case distribution is normal, and both follow from a convex program in the covariance matrices. The resulting estimator is a Kalman-type update with a least favourable covariance in place of the nominal one, which is what makes the result usable in filtering. The paper also extends it to elliptical nominal distributions (Section 5) and develops a Frank–Wolfe method for (3.4) (Section 6).

The results are proved in the paper; none of them is machine-checked. A formalization adds a checked account of a minimax argument that combines optimal transport (the Gelbrich bound and its equality for normal laws), nonlinear semidefinite programming (Propositions A.3 and A.4) and Bayesian estimation for Gaussian laws. The appendix statements are general facts about the Gelbrich ball of covariance matrices and serve beyond this paper.

Difficulty

The left side of the goal is an infimum over affine estimators of a supremum over an infinite-dimensional set of distributions; the right side reverses the order and restricts nature to normal laws while allowing every estimator. Weak duality gives ≥\ge≥ at once. For the reverse inequality, Sion's minimax theorem cannot be applied to the distributions directly: BN(P^)\mathbb B_{\mathcal N}(\widehat{\mathbb P})BN​(P) is not convex, since mixtures of normal laws are not normal, and G(P^)\mathbb G(\widehat{\mathbb P})G(P) is not compact in any useful topology. The equality has to pass through the finite matrix problems, where the worst covariance matrices must be shown to stay bounded away from singularity so that the normal noise covariance remains positive definite. That is the role of Lemma A.5 and of the hypothesis Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0.

Formalization scope

  • Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d). The risk is a lower Lebesgue integral in [0,∞][0,\infty][0,∞], and every optimal value is a [0,∞][0,\infty][0,∞]- or EReal-valued infimum or supremum restricted by a membership predicate. The finite programs (2.2), (3.4), (A.3), (A.5), (A.6), (A.9) take values in EReal.
  • M(Rd)\mathcal M(\mathbb R^d)M(Rd) is "probability measure with E∥ξ∥2<∞\mathbb E\|\xi\|^2<\inftyE∥ξ∥2<∞" and is required wherever the page requires it, because means and covariances are Bochner integrals with junk value 000 otherwise.
  • F\mathcal FF keeps both measurability and linear growth.
  • N(μ,Σ)\mathcal N(\mu,\Sigma)N(μ,Σ) is Mathlib's multivariateGaussian. W\mathbb WW, means, covariances, the PSD square root and the Gelbrich ball are the published definitions WassersteinDRO.Gelbrich.{wassersteinDistance, meanVector, covarianceMatrix, psdSqrt, meanCovarianceUncertaintySet}.
  • λmin⁡\lambda_{\min}λmin​ and λmax⁡\lambda_{\max}λmax​ are 000 at dimension 000, where every statement reduces to a trivial one.
  • Added hypothesis. The goal assumes Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0, which the page omits. The theorem fails without it: for n=m=1n=m=1n=m=1, H=0H=0H=0, Σ^x=1\widehat\Sigma_x=1Σx​=1, Σ^w=0\widehat\Sigma_w=0Σw​=0 and ρx=ρw=0\rho_x=\rho_w=0ρx​=ρw​=0, the normal ball is empty while the left side equals 111. The page's own proof uses (3.8), which it derives only for Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0.
  • Theorem 3.5. The bounds Σ⋆⪰λmin⁡(Σ^)I\Sigma^\star\succeq\lambda_{\min}(\widehat\Sigma)IΣ⋆⪰λmin​(Σ)I are stated for some maximizer of (3.4), not for every maximizer.
  • Omitted. Proposition A.4 (ii)–(iii) is false as printed in two places and is not posed (see the mission notes). Propositions 2.4 and 3.4 (the Gelbrich bound and its equality for normal laws) are already on the platform and are not posed again.
  • Ruled out. A formalization in which BN(P^)\mathbb B_{\mathcal N}(\widehat{\mathbb P})BN​(P) is empty, the risk is a Bochner integral, or the optimal values are real sSup/sInf would make the goal trivial or false. A sanity check exhibits a member of BN(P^)\mathbb B_{\mathcal N}(\widehat{\mathbb P})BN​(P) whenever Σ^w≻0\widehat\Sigma_w\succ0Σw​≻0, and an affine estimator.

Proofs of any milestone are welcome, and so are reusable lemmas on the Gelbrich ball, the matrix square root and Gaussian conditioning.

Selected references

  • V. A. Nguyen, S. Shafieezadeh-Abadeh, D. Kuhn, P. Mohajerin Esfahani, Bridging Bayesian and minimax mean square error estimation via Wasserstein distributionally robust optimization, Math. Oper. Res. 48(1), 2023. https://arxiv.org/abs/1911.03539v2, https://doi.org/10.1287/moor.2021.1176
  • S. Shafieezadeh-Abadeh, V. A. Nguyen, D. Kuhn, P. Mohajerin Esfahani, Wasserstein distributionally robust Kalman filtering, NeurIPS 31, 2018. https://arxiv.org/abs/1809.08830
  • M. Gelbrich, On a formula for the L2 Wasserstein metric between measures on Euclidean and Hilbert spaces, Math. Nachr. 147, 1990. https://doi.org/10.1002/mana.19901470121
  • C. R. Givens, R. M. Shortt, A class of Wasserstein metrics for probability distributions, Michigan Math. J. 31(2), 1984. https://doi.org/10.1307/mmj/1029003026
  • M. Sion, On general minimax theorems, Pacific J. Math. 8, 1958. https://doi.org/10.2140/pjm.1958.8.171
  • V. A. Nguyen, D. Kuhn, P. Mohajerin Esfahani, Distributionally robust inverse covariance estimation: the Wasserstein shrinkage estimator, Oper. Res. 70(1), 2022. https://arxiv.org/abs/1805.07194
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Operations ResearchPartial Differential EquationsProbability+1·Captain: mikedeng1

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+1·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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Nonlinear Quasi-hemivariational Inequalities: Existence and Optimal Control: Existence of Solutions to the Generalized Quasi-Hemivariational InequalityResearch Paper

Motivation

Hemivariational inequalities were introduced by Panagiotopoulos in the 1980s to model mechanical problems whose energy functional is neither convex nor smooth: nonmonotone friction, adhesion, delamination and unilateral contact with nonmonotone multivalued laws. Where a variational inequality expresses the optimality condition of a convex energy, a hemivariational inequality expresses a stationarity condition of a locally Lipschitz energy through Clarke's generalized directional derivative. When in addition the admissible set depends on the unknown state, as in contact problems with a solution-dependent gap or in Nash-type equilibrium problems with coupled constraints, the problem becomes a quasi-hemivariational inequality.

Zeng, Migórski and Khan (SIAM J. Control Optim. 59 (2021)) treat a general form of this problem that contains a multivalued operator TTT, a bifunction φ\varphiφ and a constraint map KKK at once. Their existence theorem for it, Theorem 3.8, is the base of an optimal control result (Section 4) and of an application to a frictional contact problem in elasticity (Section 5). This mission formalizes the existence part, Sections 2 and 3 of the paper.

Setting

Let VVV be a real reflexive Banach space with dual V∗V^*V∗ and pairing ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩, and let XXX, YYY be real Banach spaces. The data are: a nonempty closed convex set C⊆VC\subseteq VC⊆V; a multivalued constraint map K:C→2CK:C\to2^CK:C→2C; a multivalued operator T:C→2V∗T:C\to2^{V^*}T:C→2V∗; a function φ:V×V→R\varphi:V\times V\to\mathbb Rφ:V×V→R; a locally Lipschitz functional J:X→RJ:X\to\mathbb RJ:X→R; bounded linear operators γ:V→X\gamma:V\to Xγ:V→X and π:V→Y\pi:V\to Yπ:V→Y; a functional f∈Y∗f\in Y^*f∈Y∗; and an auxiliary function h:V→Rh:V\to\mathbb Rh:V→R.

For a locally Lipschitz JJJ, the Clarke generalized directional derivative and the generalized gradient are

J0(u;v)=lim sup⁡λ→0+, w→uJ(w+λv)−J(w)λ,∂J(u)={ξ∈X∗: J0(u;v)≥⟨ξ,v⟩ ∀v∈X}.J^0(u;v)=\limsup_{\lambda\to0^+,\ w\to u}\frac{J(w+\lambda v)-J(w)}{\lambda},\qquad \partial J(u)=\{\xi\in X^*:\ J^0(u;v)\ge\langle\xi,v\rangle\ \forall v\in X\}.J0(u;v)=λ→0+, w→ulimsup​λJ(w+λv)−J(w)​,∂J(u)={ξ∈X∗: J0(u;v)≥⟨ξ,v⟩ ∀v∈X}.

Problem 1.1 asks for u∈Cu\in Cu∈C and u∗∈T(u)u^*\in T(u)u∗∈T(u) such that u∈K(u)u\in K(u)u∈K(u) and

⟨u∗,v−u⟩+φ(v,u)+J0(γu;γ(v−u))≥⟨f,π(v−u)⟩Y∗×Yfor all v∈K(u).\langle u^*,v-u\rangle+\varphi(v,u)+J^0(\gamma u;\gamma(v-u))\ge\langle f,\pi(v-u)\rangle_{Y^*\times Y}\quad\text{for all }v\in K(u).⟨u∗,v−u⟩+φ(v,u)+J0(γu;γ(v−u))≥⟨f,π(v−u)⟩Y∗×Y​for all v∈K(u).

Its solution set is Γ(f)\Gamma(f)Γ(f). Fixing the constraint set gives Problem 3.3: find u∈Cu\in Cu∈C and u∗∈T(u)u^*\in T(u)u∗∈T(u) with the same inequality for all v∈Cv\in Cv∈C; its solution set is SOL(C;T,J,φ,f)\mathrm{SOL}(C;T,J,\varphi,f)SOL(C;T,J,φ,f). The variational selection S:C→2CS:C\to2^CS:C→2C maps w∈Cw\in Cw∈C to the solution set of Problem 3.3 with CCC replaced by K(w)K(w)K(w); its fixed points are exactly the solutions of Problem 1.1.

The hypotheses of the paper (p. 1250) are: TTT has nonempty, compact, convex values and is upper semicontinuous; T(⋅)+γ∗∂J(γ ⋅)T(\cdot)+\gamma^*\partial J(\gamma\,\cdot)T(⋅)+γ∗∂J(γ⋅) is (φ,h)(\varphi,h)(φ,h)-stably pseudomonotone with respect to π∗f\pi^*fπ∗f, where lim sup⁡t→0+h(tu)/t≥0\limsup_{t\to0^+}h(tu)/t\ge0limsupt→0+​h(tu)/t≥0 and hhh is weakly sequentially upper semicontinuous in the limsup sense (3.1); φ\varphiφ is convex and l.s.c. in its first argument, concave and u.s.c. in its second, and vanishes on the diagonal; KKK has nonempty closed convex values and satisfies two Mosco-type conditions (HK); a bounded set C0C_0C0​ meets every K(u)K(u)K(u) and, if CCC is unbounded, a coercivity condition (3.2) holds at each point of C0C_0C0​. Theorem 3.8 adds that γ\gammaγ is compact, hhh is convex, and lim sup⁡nφ(vn,un)≤φ(v,u)\limsup_n\varphi(v_n,u_n)\le\varphi(v,u)limsupn​φ(vn​,un​)≤φ(v,u) whenever vn→vv_n\to vvn​→v strongly and un⇀uu_n\rightharpoonup uun​⇀u weakly (3.19).

Formalization targets

Goal: Theorem 3.8 (ii)

Under all hypotheses of Theorem 3.8,

Γ(f)≠∅,Γ(f) is bounded,Γ(f) is weakly closed in V.\Gamma(f)\neq\emptyset,\qquad \Gamma(f)\ \text{is bounded},\qquad \Gamma(f)\ \text{is weakly closed in }V.Γ(f)=∅,Γ(f) is bounded,Γ(f) is weakly closed in V.

Milestones

  1. Proposition 2.5 (i)–(iii): J0(x;⋅)J^0(x;\cdot)J0(x;⋅) is sublinear, J0(x;v)=max⁡{⟨ξ,v⟩:ξ∈∂J(x)}J^0(x;v)=\max\{\langle\xi,v\rangle:\xi\in\partial J(x)\}J0(x;v)=max{⟨ξ,v⟩:ξ∈∂J(x)}, and (u,v)↦J0(u;v)(u,v)\mapsto J^0(u;v)(u,v)↦J0(u;v) is upper semicontinuous.
  2. Theorem 2.7 (Kluge): a multivalued self-map of a nonempty closed convex subset of a reflexive Banach space, with nonempty closed convex values and a sequentially weakly closed graph, has a fixed point if its domain or its range is bounded.
  3. Theorem 3.4 (i)–(iii): for Problem 3.3, the Minty-type characterization
⟨v∗,v−u⟩+φ(v,u)+⟨ηv,γ(v−u)⟩≥⟨f,π(v−u)⟩+h(v−u)∀v∈C, v∗∈T(v), ηv∈∂J(γv);\langle v^*,v-u\rangle+\varphi(v,u)+\langle\eta_v,\gamma(v-u)\rangle\ge\langle f,\pi(v-u)\rangle+h(v-u)\quad\forall v\in C,\ v^*\in T(v),\ \eta_v\in\partial J(\gamma v);⟨v∗,v−u⟩+φ(v,u)+⟨ηv​,γ(v−u)⟩≥⟨f,π(v−u)⟩+h(v−u)∀v∈C, v∗∈T(v), ηv​∈∂J(γv);

nonemptiness, boundedness and weak closedness of SOL(C;T,J,φ,f)\mathrm{SOL}(C;T,J,\varphi,f)SOL(C;T,J,φ,f); and its convexity when hhh is convex. 4. Theorem 3.8 (i): the same characterization for Problem 1.1, with CCC replaced by K(u)K(u)K(u). 5. Two claims from the proof of Theorem 3.8 (ii): the graph of SSS is sequentially weakly closed, and S(C)=⋃w∈CS(w)S(C)=\bigcup_{w\in C}S(w)S(C)=⋃w∈C​S(w) is bounded.

Significance

Theorem 3.8 is the existence result on which the rest of the paper rests: the optimal control problem of Section 4 minimizes F(f)=inf⁡u∈Γ(f)g(u,f)F(f)=\inf_{u\in\Gamma(f)}g(u,f)F(f)=infu∈Γ(f)​g(u,f) over f∈Y∗f\in Y^*f∈Y∗, and Section 5 casts an approximate static elastic contact model, with a multivalued normal compliance condition and a frictional law with slip-dependent friction coefficient, in the form of Problem 1.1 on a space of displacements. The theorem unifies several existence results for variational, hemivariational and quasi-variational inequalities: for single-valued TTT, J=0J=0J=0, π=id\pi=\mathrm{id}π=id, h=0h=0h=0 and φ(v,u)=ϕ(v)−ϕ(u)\varphi(v,u)=\phi(v)-\phi(u)φ(v,u)=ϕ(v)−ϕ(u), its Corollary 3.9 reduces to an earlier existence result for quasi-variational inequalities (Remark 3.10), and Theorem 3.4 removes the compactness of γ\gammaγ required in earlier work (Remark 3.6).

The results are proved in the paper. None of them, nor Clarke's calculus on a Banach space, nor Kluge's fixed point theorem, has a machine-checked proof to our knowledge. A formalization adds a checked version of a proof that combines a KKM-type fixed point theorem, Minty's trick for pseudomonotone multivalued operators, and a fixed point argument for the variational selection.

Difficulty

The obvious route to Problem 1.1 is to fix www, solve the inequality on K(w)K(w)K(w), and take a fixed point of the solution map. Two steps resist. First, the solution map is multivalued and its values are only weakly closed, so a Schauder- or Kakutani-type theorem in the norm topology does not apply; the fixed point theorem must work with sequentially weakly closed graphs, and the graph closedness of SSS has to be proved by passing to the limit in inequalities in which unu_nun​ converges only weakly while the test points vn∈K(wn)v_n\in K(w_n)vn​∈K(wn​) must converge strongly. That passage uses the compactness of γ\gammaγ, the upper semicontinuity of J0J^0J0, condition (3.19) and the Mosco-type conditions together. Second, in the "there exists u∗∈T(u)u^*\in T(u)u∗∈T(u)" form of the problem the inequality is not stable under weak limits in uuu, which is why the Minty reformulation and the stable pseudomonotonicity with the auxiliary function hhh are needed.

Formalization scope

All spaces are real normed spaces with CompleteSpace; V∗V^*V∗ is V →L[ℝ] ℝ with the operator-norm topology; reflexivity is surjectivity of NormedSpace.inclusionInDoubleDual ℝ V. No inner product and no finite dimension is assumed. Multivalued maps are total functions V → Set _, constrained on CCC only. Weak convergence xn⇀xx_n\rightharpoonup xxn​⇀x means ℓ(xn)→ℓ(x)\ell(x_n)\to\ell(x)ℓ(xn​)→ℓ(x) for every ℓ∈V∗\ell\in V^*ℓ∈V∗; "weakly closed" is sequential weak closedness, which for the bounded sets Γ(f)\Gamma(f)Γ(f) and SOL\mathrm{SOL}SOL in a reflexive space agrees with weak closedness. Adjoints are composition: ⟨γ∗η,w⟩=η(γw)\langle\gamma^*\eta,w\rangle=\eta(\gamma w)⟨γ∗η,w⟩=η(γw), ⟨π∗f,w⟩=f(πw)\langle\pi^*f,w\rangle=f(\pi w)⟨π∗f,w⟩=f(πw). J0J^0J0 is a real Filter.limsup and is used only under LocallyLipschitz J. Every lim sup⁡\limsuplimsup, infimum and limit in the hypotheses (lim sup⁡t→0+h(tu)/t≥0\limsup_{t\to0^+}h(tu)/t\ge0limsupt→0+​h(tu)/t≥0, (3.1), (3.2), (3.19)) is written with explicit ε\varepsilonε–NNN quantifiers, so no default value of a real lim sup⁡\limsuplimsup or inf⁡\infinf can make a hypothesis vacuous.

Four corrections to the printed hypotheses are built in and stated in each item's note: the pairing in (3.2) is ⟨ηu,γ(u−v0)⟩\langle\eta_u,\gamma(u-v_0)\rangle⟨ηu​,γ(u−v0​)⟩ (the page's ⟨ηu,u−v0⟩\langle\eta_u,u-v_0\rangle⟨ηu​,u−v0​⟩ does not typecheck); T(u)T(u)T(u) is nonempty for u∈Cu\in Cu∈C; the condition (3.2) assumed in Theorem 3.4 refers to a bounded set C0C_0C0​ that meets CCC; and for Theorem 3.8 (ii) and the boundedness of S(C)S(C)S(C), (3.2) in (HC0) holds uniformly in v0∈C0v_0\in C_0v0​∈C0​ (one RRR for each MMM), which is what the proof on pp. 1260–1261 uses. With (3.2) only at each fixed v0∈C0v_0\in C_0v0​∈C0​, as printed, Γ(f)\Gamma(f)Γ(f) can be unbounded; the counterexample is in the note of Theorem 3.8 (ii). Theorem 3.8 (i) and the graph-closedness of SSS keep (HC0) as printed. A formalization in which TTT may have empty values, C0C_0C0​ may be empty or disjoint from CCC, VVV is a Hilbert or finite-dimensional space, a real lim sup⁡\limsuplimsup default value makes the conditions on hhh or (3.19) vacuous, or "bounded" or "weakly closed" is dropped from the conclusion, would be a different and weaker theorem.

The development needs Clarke's calculus on a Banach space (Proposition 2.5, which relies on the Hahn–Banach theorem), Eberlein–Šmulian or Kakutani's theorem on weak compactness of bounded closed convex sets in reflexive spaces, Mazur's lemma, a KKM-type fixed point theorem in Hausdorff topological vector spaces, and Kluge's fixed point theorem. These pieces are reusable beyond this mission: Clarke's calculus for every nonsmooth optimization statement on Banach spaces, and the fixed point theorems for variational and quasi-variational inequalities in general. Contributions of any of them, of alternative proofs, and of proofs of the milestones in any order are welcome.

Selected references

  • S. Zeng, S. Migórski, A. A. Khan, Nonlinear quasi-hemivariational inequalities: existence and optimal control, SIAM J. Control Optim. 59(2) (2021) 1246–1274. https://doi.org/10.1137/19M1282210
  • F. H. Clarke, Optimization and Nonsmooth Analysis, Wiley, 1983; reprinted SIAM Classics in Applied Mathematics 5, 1990. https://doi.org/10.1137/1.9781611971309
  • R. Kluge, Nichtlineare Variationsungleichungen und Extremalaufgaben, VEB Deutscher Verlag der Wissenschaften, Berlin, 1979.
  • S. Migórski, A. Ochal, M. Sofonea, Nonlinear Inclusions and Hemivariational Inequalities, Springer, 2013. https://doi.org/10.1007/978-1-4614-4232-5
  • P. D. Panagiotopoulos, Hemivariational Inequalities: Applications in Mechanics and Engineering, Springer, 1993. https://doi.org/10.1007/978-3-642-51677-1
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Control TheoryDynamic ProgrammingPartial Differential Equations+1·Captain: mikedeng1

Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 3: The Closed-Loop McKean–Vlasov Value Function Is a Viscosity Solution of the HJB Master EquationResearch Paper

Motivation

Mean field control asks a central planner to steer a large population of interacting agents. Each agent's state follows a stochastic differential equation whose coefficients depend on the agent's own state and on the empirical distribution of the population; as the population grows, the system is described by a single McKean–Vlasov equation whose coefficients depend on the law of the solution itself. The planner's value is then a function V(t,μ)V(t,\mu)V(t,μ) of time and of a probability measure, and its dynamic programming equation, the HJB master equation, is a partial differential equation on the Wasserstein space of measures.

C. Wu and J. Zhang (Ann. Appl. Probab. 30(2), 2020) develop a viscosity theory for such master equations in a path-dependent setting and apply it to McKean–Vlasov control with closed-loop controls, i.e. controls that depend on the observed state path rather than on the driving Brownian motion. Closed-loop information is the natural one when the noise is not observable, and it is the information structure relevant for games; but the value function is then not known to be smooth, so classical solutions are out of reach. This mission formalizes the paper's §5: the value function of the closed-loop problem with piecewise constant controls is a viscosity solution of the HJB master equation.

Setting

Fix d≥1d\ge1d≥1 and a horizon TTT. The path space is Ω=C([0,T],Rd)\Omega=C([0,T],\mathbb R^d)Ω=C([0,T],Rd) with the uniform norm, the canonical process is Xs(ω)=ωsX_s(\omega)=\omega_sXs​(ω)=ωs​, and F=(Ft)\mathbb F=(\mathcal F_t)F=(Ft​) is its natural filtration. P2\mathcal P_2P2​ is the set of probability measures μ\muμ on Ω\OmegaΩ with Eμ[∥X∥2]<∞\mathbb E^\mu[\|X\|^2]<\inftyEμ[∥X∥2]<∞; μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of the stopped path Xt∧⋅X_{t\wedge\cdot}Xt∧⋅​. On Θ=[0,T]×P2\Theta=[0,T]\times\mathcal P_2Θ=[0,T]×P2​ the pseudometric is

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

with W2\mathcal W_2W2​ the 2-Wasserstein distance on laws of paths.

The data are a control set AAA and coefficients b(t,ω,μ,a)∈Rdb(t,\omega,\mu,a)\in\mathbb R^db(t,ω,μ,a)∈Rd, σ(t,ω,μ,a)∈Rd×d\sigma(t,\omega,\mu,a)\in\mathbb R^{d\times d}σ(t,ω,μ,a)∈Rd×d, f(t,ω,μ,a)∈Rf(t,\omega,\mu,a)\in\mathbb Rf(t,ω,μ,a)∈R, g(ω,μ)∈Rg(\omega,\mu)\in\mathbb Rg(ω,μ)∈R satisfying Assumption 5.1: measurability and adaptedness, boundedness of b,σb,\sigmab,σ by C0C_0C0​, Lipschitz continuity of b,σb,\sigmab,σ and uniform continuity of f,gf,gf,g in (ω,μ)(\omega,\mu)(ω,μ), local uniform continuity in ttt, and positive definiteness of σσ⊤\sigma\sigma^\topσσ⊤.

An admissible control α∈At\alpha\in\mathcal A_tα∈At​ (5.3) is piecewise constant: αs=∑i<nhi1[ti,ti+1)(s)\alpha_s=\sum_{i<n}h_i\mathbf 1_{[t_i,t_{i+1})}(s)αs​=∑i<n​hi​1[ti​,ti+1​)​(s) for a partition t=t0<⋯<tn=Tt=t_0<\dots<t_n=Tt=t0​<⋯<tn​=T, with hi:Ω→Ah_i:\Omega\to Ahi​:Ω→A Fti\mathcal F_{t_i}Fti​​-measurable. The controlled law Pt,μ,α∈P2\mathbb P^{t,\mu,\alpha}\in\mathcal P_2Pt,μ,α∈P2​ agrees with μ\muμ on [0,t][0,t][0,t] and solves, for a Brownian motion BαB^\alphaBα,

Xs=Xt+∫tsb(r,Xr∧⋅,P[0,r]t,μ,α,αr)dr+∫tsσ(r,Xr∧⋅,P[0,r]t,μ,α,αr)dBrα,s∈[t,T].X_s=X_t+\int_t^s b\big(r,X_{r\wedge\cdot},\mathbb P^{t,\mu,\alpha}_{[0,r]},\alpha_r\big)dr+\int_t^s\sigma\big(r,X_{r\wedge\cdot},\mathbb P^{t,\mu,\alpha}_{[0,r]},\alpha_r\big)dB^\alpha_r,\quad s\in[t,T].Xs​=Xt​+∫ts​b(r,Xr∧⋅​,P[0,r]t,μ,α​,αr​)dr+∫ts​σ(r,Xr∧⋅​,P[0,r]t,μ,α​,αr​)dBrα​,s∈[t,T].

The value function (3.20) is

V(t,μ)=sup⁡α∈AtEPt,μ,α[g(X,Pt,μ,α)+∫tTf(s,X,Pt,μ,α,αs) ds],V(t,\mu)=\sup_{\alpha\in\mathcal A_t}\mathbb E^{\mathbb P^{t,\mu,\alpha}}\Big[g(X,\mathbb P^{t,\mu,\alpha})+\int_t^Tf(s,X,\mathbb P^{t,\mu,\alpha},\alpha_s)\,ds\Big],V(t,μ)=α∈At​sup​EPt,μ,α[g(X,Pt,μ,α)+∫tT​f(s,X,Pt,μ,α,αs​)ds],

and V0V_0V0​ is the same supremum over the controls At0\mathcal A^0_tAt0​ (5.12) whose pieces depend on the path before ttt only through finitely many values Xs1,…,XsmX_{s_1},\dots,X_{s_m}Xs1​​,…,Xsm​​.

The HJB master equation (3.22) is LV=0\mathbb LV=0LV=0 with LV(t,μ)=∂tV(t,μ)+G(t,μ,∂μV(t,μ,⋅),∂ω∂μV(t,μ,⋅))\mathbb LV(t,\mu)=\partial_tV(t,\mu)+G(t,\mu,\partial_\mu V(t,\mu,\cdot),\partial_\omega\partial_\mu V(t,\mu,\cdot))LV(t,μ)=∂t​V(t,μ)+G(t,μ,∂μ​V(t,μ,⋅),∂ω​∂μ​V(t,μ,⋅)), where

G(t,μ,Z,Γ)=Eμ[sup⁡a∈A(12Γ(X):σσ⊤(t,X,μ,a)+Z(X)⋅b(t,X,μ,a)+f(t,X,μ,a))].G(t,\mu,Z,\Gamma)=\mathbb E^\mu\Big[\sup_{a\in A}\Big(\tfrac12\Gamma(X):\sigma\sigma^\top(t,X,\mu,a)+Z(X)\cdot b(t,X,\mu,a)+f(t,X,\mu,a)\Big)\Big].G(t,μ,Z,Γ)=Eμ[a∈Asup​(21​Γ(X):σσ⊤(t,X,μ,a)+Z(X)⋅b(t,X,μ,a)+f(t,X,μ,a))].

Viscosity solutions (Definition 4.4) are defined by test functions φ\varphiφ that satisfy a functional Itô formula on [t,t+δ]×PL(t,μ)[t,t+\delta]\times\mathcal P_L(t,\mu)[t,t+δ]×PL​(t,μ), where PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the set of laws agreeing with μ\muμ on [0,t][0,t][0,t] under which XXX is a semimartingale on [t,T][t,T][t,T] with drift and diffusion bounded by LLL, and touch VVV from above or below at (t,μ)(t,\mu)(t,μ) on that set.

Formalization targets

Goal: Theorem 5.8

Under Assumption 5.1, VVV is finite on Θ\ThetaΘ and is a viscosity solution of (3.22).

Milestones

  • (4.1)(4.1)(4.1): sup⁡P∈PL(t,μ)EP[sup⁡t≤s≤t+δ∣Xt,s∣p]≤Cp,Lδp/2\sup_{\mathbb P\in\mathcal P_L(t,\mu)}\mathbb E^{\mathbb P}[\sup_{t\le s\le t+\delta}|X_{t,s}|^p]\le C_{p,L}\delta^{p/2}supP∈PL​(t,μ)​EP[supt≤s≤t+δ​∣Xt,s​∣p]≤Cp,L​δp/2.
  • Remark 5.4(i): (3.18) has a unique solution, and it lies in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) for L≥C0∨12C02L\ge C_0\vee\frac12C_0^2L≥C0​∨21​C02​.
  • Remark 5.4(ii): the dynamic programming principle (3.21),
V(t1,μ)=sup⁡α∈At1[V(t2,Pt1,μ,α)+∫t1t2EPt1,μ,α[f(s,X,Pt1,μ,α,αs)]ds].V(t_1,\mu)=\sup_{\alpha\in\mathcal A_{t_1}}\Big[V(t_2,\mathbb P^{t_1,\mu,\alpha})+\int_{t_1}^{t_2}\mathbb E^{\mathbb P^{t_1,\mu,\alpha}}[f(s,X,\mathbb P^{t_1,\mu,\alpha},\alpha_s)]ds\Big].V(t1​,μ)=α∈At1​​sup​[V(t2​,Pt1​,μ,α)+∫t1​t2​​EPt1​,μ,α[f(s,X,Pt1​,μ,α,αs​)]ds].
  • Lemma 5.11: a coupling construction with an independent Brownian motion.
  • Lemma 5.13: ∣V0(t,μ)−V0(t,ν)∣≤ρ(W2(μ[0,t],ν[0,t]))|V_0(t,\mu)-V_0(t,\nu)|\le\rho(\mathcal W_2(\mu_{[0,t]},\nu_{[0,t]}))∣V0​(t,μ)−V0​(t,ν)∣≤ρ(W2​(μ[0,t]​,ν[0,t]​)) for a modulus ρ\rhoρ.
  • Lemma 5.14: V=V0V=V_0V=V0​.
  • Theorem 5.7: ∣V(t1,μ)−V(t2,ν)∣≤Cρ(W2((t1,μ),(t2,ν)))+C[1+W2(μ[0,t1],δ{0})][t2−t1]|V(t_1,\mu)-V(t_2,\nu)|\le C\rho(\mathcal W_2((t_1,\mu),(t_2,\nu)))+C[1+\mathcal W_2(\mu_{[0,t_1]},\delta_{\{0\}})][t_2-t_1]∣V(t1​,μ)−V(t2​,ν)∣≤Cρ(W2​((t1​,μ),(t2​,ν)))+C[1+W2​(μ[0,t1​]​,δ{0}​)][t2​−t1​], and uniform continuity when fff is bounded.

Significance

The result characterizes the closed-loop value function through a PDE on the space of path laws without assuming any smoothness of VVV. Combined with a comparison principle for (3.22), which the paper leaves open, it would identify the closed-loop and open-loop values (Remark 5.9). The regularity result (Theorem 5.7) is itself delicate: Example 5.6 shows that a natural restricted class of closed-loop controls produces a value function that is discontinuous in μ\muμ, and the piecewise constant class (5.3) is chosen to avoid this.

The theorems are proved in the paper; none of them is formalized. A formalization would supply a machine-checked path from a path-dependent McKean–Vlasov control problem to its HJB master equation, together with reusable statements on weak solutions of path-dependent McKean–Vlasov equations, their uniform moment bounds, and the dynamic programming principle in the Wasserstein space.

Difficulty

Definition 4.4 requires V∈C0(Θ)V\in C^0(\Theta)V∈C0(Θ), and the central difficulty is continuity in μ\muμ. Closed-loop controls are functions of the observed path; changing the initial law from μ\muμ to ν\nuν changes the information available to the control, and when ν[0,t]\nu_{[0,t]}ν[0,t]​ is degenerate a control adapted to μ\muμ cannot be written as a function of the ν\nuν-path. The obvious argument, transporting an ε\varepsilonε-optimal control for μ\muμ along an optimal coupling of μ\muμ and ν\nuν, fails for exactly this reason (Example 5.6).

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​ and every statement quantifies over t≤Tt\le Tt≤T and μ∈P2\mu\in\mathcal P_2μ∈P2​. Paths are continuous maps [0,T]→Rd[0,T]\to\mathbb R^d[0,T]→Rd with the sup norm and Borel σ\sigmaσ-algebra; W2\mathcal W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance with p=2p=2p=2. Brownian motion and Itô integrals are the published EthierKurtz.IsStandardBrownian and EthierKurtz.HasBrownianItoIntegral.

Committed conventions:

  • The control set AAA is a nonempty Polish space with its Borel σ\sigmaσ-algebra (the paper says "some appropriate set AAA"); this provides continuity in aaa, measurability of hih_ihi​ and of ω↦sup⁡aG2\omega\mapsto\sup_aG_2ω↦supa​G2​.
  • "Progressively measurable in all variables" is joint measurability (Giry σ\sigmaσ-algebra on laws) plus adaptedness in ω\omegaω and μ\muμ. The bound ∣σ∣≤C0|\sigma|\le C_0∣σ∣≤C0​ uses the Frobenius norm; the joint Lipschitz bound on (b,σ)(b,\sigma)(b,σ) is two bounds with the same L0L_0L0​. δ{0}\delta_{\{0\}}δ{0}​ is the Dirac mass at the zero path.
  • (3.18) is solved in the weak sense: a law with a semimartingale representation, carrying its own Brownian motion, whose characteristics are the controlled coefficients on [t,T)[t,T)[t,T). PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is defined through the same representations.
  • VVV and V0V_0V0​ are suprema in the extended reals over admissible pairs; statements that subtract values or use VVV as a real function assert finiteness explicitly.
  • Test functions carry their derivatives as witnesses; the Itô formula of Definition 4.2 is stated in drift form for every representation; "inf⁡(φ−V)=0\inf(\varphi-V)=0inf(φ−V)=0" is read as φ−V≥0\varphi-V\ge0φ−V≥0 on the test set with equality at (t,μ)(t,\mu)(t,μ), and the test function's data at (t,μ)(t,\mu)(t,μ) are those at (t,P)(t,\mathbb P)(t,P) for P∈PL(t,μ)\mathbb P\in\mathcal P_L(t,\mu)P∈PL​(t,μ).
  • Statements are for general ddd; §5.3 of the paper argues for d=1d=1d=1 only.

The test classes are not vacuous: constant functions satisfy every clause of the test-function class, and Assumption 5.1 holds for b≡0b\equiv0b≡0, σ≡I\sigma\equiv Iσ≡I, f≡g≡0f\equiv g\equiv0f≡g≡0. A formalization that makes PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) or the admissible set empty, or that lets VVV be −∞-\infty−∞, does not prove the theorem.

Needed infrastructure: weak existence and uniqueness for path-dependent McKean–Vlasov SDEs with Lipschitz coefficients; Burkholder–Davis–Gundy-type moment bounds; measurable selection on Polish spaces; couplings and gluing on P2\mathcal P_2P2​ of a path space. The moment bound and the McKean–Vlasov well-posedness are reusable beyond this mission. Contributions to any milestone are welcome.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2), 936–986, 2020. https://doi.org/10.1214/19-AAP1521
  • 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
  • D. Lacker, Limit theory for controlled McKean–Vlasov dynamics, SIAM J. Control Optim. 55(3), 2017. https://doi.org/10.1137/16M1095895
  • I. Ekren, N. Touzi, J. Zhang, Viscosity solutions of fully nonlinear parabolic path dependent PDEs: Part I, Ann. Probab. 44(2), 2016. https://doi.org/10.1214/14-AOP999
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Optimal TransportPartial Differential EquationsProbability·Captain: mikedeng1

Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 1: A Functional Itô Formula for Path-Dependent Functionals of Semimartingale LawsResearch Paper

Motivation

Master equations are partial differential equations whose state variable is a probability measure. They arise as the Hamilton–Jacobi–Bellman equations of mean field control problems, where a planner steers a large population through its distribution, and as the limit description of large games. Their basic computational tool is an Itô formula for functions of measures: if XXX is a semimartingale with law PXt\mathbb P_{X_t}PXt​​ at time ttt, how does f(PXt)f(\mathbb P_{X_t})f(PXt​​) evolve? For functions on the Wasserstein space P2(Rd)\mathcal P_2(\mathbb R^d)P2​(Rd) this formula is due to Buckdahn, Li, Peng and Rainer (Ann. Probab. 2017) and Chassagneux, Crisan and Delarue (arXiv:1411.3009), with the derivative in the measure introduced by Lions through the lifting to random variables.

Many models are path dependent: exotic options, rough volatility, and control problems with constant controls all lead to functions of the law of a whole path rather than of its time marginal. Wu and Zhang (Ann. Appl. Probab. 2020) extend the measure derivative and the Itô formula to this setting, following Dupire's functional Itô calculus (Dupire 2009). This mission formalizes §2 of their paper: the derivative of a function of a path law and the functional Itô formula of Theorem 2.7. It is the first of three missions on the paper; the other two treat viscosity solutions of master equations and McKean–Vlasov control.

Setting

Fix d≥1d\ge1d≥1 and T>0T>0T>0. Continuous paths form Ω=C([0,T],Rd)\Omega=C([0,T],\mathbb R^d)Ω=C([0,T],Rd) with ∥ω∥=sup⁡t∣ωt∣\|\omega\|=\sup_t|\omega_t|∥ω∥=supt​∣ωt​∣. Càdlàg paths form Ω^=D([0,T],Rd)\widehat\Omega=\mathbb D([0,T],\mathbb R^d)Ω=D([0,T],Rd) with the Skorokhod distance

dSK(ω^,ω^′)=inf⁡λsup⁡0≤t≤T[∣t−λ(t)∣+∣ω^t−ω^λ(t)′∣],d_{SK}(\hat\omega,\hat\omega')=\inf_\lambda\sup_{0\le t\le T}\big[|t-\lambda(t)|+|\hat\omega_t-\hat\omega'_{\lambda(t)}|\big],dSK​(ω^,ω^′)=λinf​0≤t≤Tsup​[∣t−λ(t)∣+∣ω^t​−ω^λ(t)′​∣],

the infimum over continuous strictly increasing bijections λ\lambdaλ of [0,T][0,T][0,T]. The canonical process is X^t(ω^)=ω^t\widehat X_t(\hat\omega)=\hat\omega_tXt​(ω^)=ω^t​, with natural filtration F^\widehat{\mathbb F}F; ω^t∧⋅\hat\omega_{t\wedge\cdot}ω^t∧⋅​ is the path stopped at ttt.

P^2\widehat{\mathcal P}_2P2​ is the set of probability measures μ\muμ on Ω^\widehat\OmegaΩ with Eμ∥X^∥2<∞\mathbb E^\mu\|\widehat X\|^2<\inftyEμ∥X∥2<∞, with the Wasserstein distance W2\mathcal W_2W2​ whose cost is dSK2d_{SK}^2dSK2​. The state space is Θ^=[0,T]×P^2\widehat\Theta=[0,T]\times\widehat{\mathcal P}_2Θ=[0,T]×P2​ with the pseudometric

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

where μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of X^t∧⋅\widehat X_{t\wedge\cdot}Xt∧⋅​.

For f:Θ^→Rf:\widehat\Theta\to\mathbb Rf:Θ→R the time derivative is the right derivative ∂tf(t,μ)=lim⁡δ↓0[f(t+δ,μ[0,t])−f(t,μ)]/δ\partial_tf(t,\mu)=\lim_{\delta\downarrow0}[f(t+\delta,\mu_{[0,t]})-f(t,\mu)]/\delta∂t​f(t,μ)=limδ↓0​[f(t+δ,μ[0,t]​)−f(t,μ)]/δ. The spatial derivative ∂μf(t,μ,ω^)∈Rd\partial_\mu f(t,\mu,\hat\omega)\in\mathbb R^d∂μ​f(t,μ,ω^)∈Rd comes from lifting fff to F(t,X~)=f(t,P~X~)F(t,\tilde X)=f(t,\tilde{\mathbb P}_{\tilde X})F(t,X~)=f(t,P~X~​) on square-integrable path-valued random variables of an atomless Polish probability space: the Fréchet derivative of FFF under the perturbation X~+ξ1[t,T]\tilde X+\xi\mathbf 1_{[t,T]}X~+ξ1[t,T]​ has the form DF(t,X~)=∂μf(t,P~X~t∧⋅,X~t∧⋅)DF(t,\tilde X)=\partial_\mu f(t,\tilde{\mathbb P}_{\tilde X_{t\wedge\cdot}},\tilde X_{t\wedge\cdot})DF(t,X~)=∂μ​f(t,P~X~t∧⋅​​,X~t∧⋅​). The second derivative ∂ω∂μf∈Rd×d\partial_\omega\partial_\mu f\in\mathbb R^{d\times d}∂ω​∂μ​f∈Rd×d is the pathwise (Dupire vertical) derivative of ∂μf\partial_\mu f∂μ​f. Cb1,1,1(Θ^)C^{1,1,1}_b(\widehat\Theta)Cb1,1,1​(Θ) consists of the continuous fff with continuous derivatives, bounded ∂tf\partial_tf∂t​f, and ∣∂μf∣+∣∂ω∂μf∣≤C[1+∥ω^∥]|\partial_\mu f|+|\partial_\omega\partial_\mu f|\le C[1+\|\hat\omega\|]∣∂μ​f∣+∣∂ω​∂μ​f∣≤C[1+∥ω^∥].

P^L\widehat{\mathcal P}_LPL​ is the set of laws μ=P~∘X~−1\mu=\tilde{\mathbb P}\circ\tilde X^{-1}μ=P~∘X~−1 of Itô processes X~t=X~0+∫0tb~s ds+∫0tσ~s dB~s\tilde X_t=\tilde X_0+\int_0^t\tilde b_s\,ds+\int_0^t\tilde\sigma_s\,d\tilde B_sX~t​=X~0​+∫0t​b~s​ds+∫0t​σ~s​dB~s​ with ∣b~∣≤L|\tilde b|\le L∣b~∣≤L, 12∣σ~∣2≤L\tfrac12|\tilde\sigma|^2\le L21​∣σ~∣2≤L and X~0\tilde X_0X~0​ square integrable.

Formalization targets

Goal: the functional Itô formula (Theorem 2.7)

For f∈Cb1,1,1(Θ^)f\in C^{1,1,1}_b(\widehat\Theta)f∈Cb1,1,1​(Θ), μ∈P^L\mu\in\widehat{\mathcal P}_Lμ∈PL​ and t∈[0,T]t\in[0,T]t∈[0,T],

f(t,μ)=f(0,μ)+∫0t∂tf(s,μ) ds+Eμ[∫0t∂μf(s,μ,X^)⋅dX^s+12∫0t∂ω∂μf(s,μ,X^):d⟨X^⟩s].f(t,\mu)=f(0,\mu)+\int_0^t\partial_tf(s,\mu)\,ds+\mathbb E^\mu\Big[\int_0^t\partial_\mu f(s,\mu,\widehat X)\cdot d\widehat X_s+\tfrac12\int_0^t\partial_\omega\partial_\mu f(s,\mu,\widehat X):d\langle\widehat X\rangle_s\Big].f(t,μ)=f(0,μ)+∫0t​∂t​f(s,μ)ds+Eμ[∫0t​∂μ​f(s,μ,X)⋅dXs​+21​∫0t​∂ω​∂μ​f(s,μ,X):d⟨X⟩s​].

Milestones

  1. Theorem 2.2: the Fréchet derivative of the lift is ψ(X~t∧⋅)\psi(\tilde X_{t\wedge\cdot})ψ(X~t∧⋅​) for an F^t\widehat{\mathcal F}_tFt​-measurable ψ\psiψ determined by fff and the law of X~\tilde XX~.
  2. Corollary 2.3: under uniform continuity of DFDFDF, a single jointly measurable ∂μf\partial_\mu f∂μ​f represents DFDFDF, unique if continuous.
  3. (2.21): the discrete expansion f(T,μn)−f(0,μn)=I1n+I2n+I3nf(T,\mu^n)-f(0,\mu^n)=I_1^n+I_2^n+I_3^nf(T,μn)−f(0,μn)=I1n​+I2n​+I3n​ along a uniform partition.
  4. (2.22) and the W2\mathcal W_2W2​ limit after it: the discretized paths and laws converge.
  5. The four limits on p. 946, which turn (2.21) into (2.20) as n→∞n\to\inftyn→∞.

Significance

The formula is the chain rule of calculus on path laws. It is what makes Cb1,1,1C^{1,1,1}_bCb1,1,1​ functions admissible test functions for viscosity solutions of path-dependent master equations, and what identifies the value function of a McKean–Vlasov control problem with a solution of its HJB master equation (§§4–5 of the paper, the other two missions of this series). Without it, the notion of viscosity solution in that paper has no link to the underlying dynamics.

The result is proved in the paper. It has no machine-checked proof: Lean's Mathlib has neither the Skorokhod space, nor Wasserstein spaces of path laws, nor a derivative with respect to a measure. Formalizing it would also produce a reusable Lean account of càdlàg path spaces and of the Lions derivative, both of which are absent today.

Difficulty

The obvious argument would expand fff along the time marginals of X~\tilde XX~. That fails for path-dependent fff: the stopped laws μ[0,t]\mu_{[0,t]}μ[0,t]​ do not change continuously when a path is perturbed after ttt, and the perturbation X~+ξ1[t,T]\tilde X+\xi\mathbf 1_{[t,T]}X~+ξ1[t,T]​ of the derivative's definition leaves the space of continuous paths. This is why the paper passes to càdlàg paths and the Skorokhod distance. Any argument then has to control fff and its derivatives along laws of discontinuous paths, which is where the joint continuity of all derivatives in (t,μ,ω^)(t,\mu,\hat\omega)(t,μ,ω^) under W2+dSK\mathcal W_2+d_{SK}W2​+dSK​ and convergence of laws in W2\mathcal W_2W2​ become unavoidable. Separately, Theorem 2.2 must show that a derivative defined through one probability space is a deterministic function of the stopped path, and atomlessness of that space is essential to it.

Formalization scope

Paths are functions on [0,∞)[0,\infty)[0,∞), constant after TTT; Ω\OmegaΩ is C(Set.Icc 0 T, ℝ^d) with the sup norm, embedded in Ω^\widehat\OmegaΩ. Ω^\widehat\OmegaΩ carries the σ\sigmaσ-algebra of the evaluations. Distances, sup norms and W2\mathcal W_2W2​ are [0,∞][0,\infty][0,∞]-valued. A law in P^L\widehat{\mathcal P}_LPL​ is given with an explicit representation: a filtered probability space, a standard Brownian motion with independent increments, progressively measurable bounded coefficients, and the Itô integral of the published EthierKurtz.HasBrownianItoIntegral. The goal holds for every representation of μ\muμ, and (2.20) is stated in drift form: E∫0t(∂μf⋅b~s+12∂ω∂μf:σ~sσ~s⊤) ds\mathbb E\int_0^t(\partial_\mu f\cdot\tilde b_s+\tfrac12\partial_\omega\partial_\mu f:\tilde\sigma_s\tilde\sigma_s^\top)\,dsE∫0t​(∂μ​f⋅b~s​+21​∂ω​∂μ​f:σ~s​σ~s⊤​)ds, the stochastic integral having mean zero.

The class C1,1,1(Θ^)C^{1,1,1}(\widehat\Theta)C1,1,1(Θ) fixes fff together with its derivatives and states that they are the derivatives (2.7), (2.16), (2.18). It also requires ∂μf(t,μ,⋅)\partial_\mu f(t,\mu,\cdot)∂μ​f(t,μ,⋅) and ∂ω∂μf(t,μ,⋅)\partial_\omega\partial_\mu f(t,\mu,\cdot)∂ω​∂μ​f(t,μ,⋅) to be F^t\widehat{\mathcal F}_tFt​-adapted, a property the paper's ∂μf\partial_\mu f∂μ​f has by Theorem 2.2. Without these clauses every continuous function would qualify, and (2.20) would be false. The printed D([0,T),Rd)\mathbb D([0,T),\mathbb R^d)D([0,T),Rd) is read as D([0,T],Rd)\mathbb D([0,T],\mathbb R^d)D([0,T],Rd). The proof's d=1d=1d=1 computations are stated in dimension ddd. Limits indexed by ti≤t<ti+1t_i\le t<t_{i+1}ti​≤t<ti+1​ are stated for t<Tt<Tt<T.

A complete development needs: the Skorokhod space and the fact that its Borel σ\sigmaσ-algebra is the evaluation σ\sigmaσ-algebra; Wasserstein distances on it; dominated convergence for path laws; and Itô's formula for the drift–diffusion representation. These are reusable well beyond this mission. Contributions to any milestone, or to these foundations as separate lemmas, are welcome.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2) (2020), 936–986. https://doi.org/10.1214/19-AAP1521
  • R. Buckdahn, J. Li, S. Peng, C. Rainer, Mean-field stochastic differential equations and associated PDEs, Ann. Probab. 45(2) (2017), 824–878. https://doi.org/10.1214/15-AOP1076
  • J.-F. Chassagneux, D. Crisan, F. Delarue, A probabilistic approach to classical solutions of the master equation for large population equilibria, Mem. Amer. Math. Soc. (2022). https://arxiv.org/abs/1411.3009
  • B. Dupire, Functional Itô calculus, Bloomberg Portfolio Research Paper 2009-04 (2009); Quant. Finance 19(5) (2019). https://doi.org/10.2139/ssrn.1435551
  • 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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CombinatoricsLinear OptimizationOptimization·Captain: mikedeng1

The Running Intersection Relaxation of the Multilinear Polytope 3: Running Intersection Inequalities Meeting Three Support Conditions Define Facets of the Multilinear PolytopeResearch Paper

Motivation

Binary polynomial optimization asks for the maximum of a polynomial over {0,1}n\{0,1\}^n{0,1}n. Linearizing each monomial ∏v∈ezv\prod_{v\in e}z_v∏v∈e​zv​ by a new variable zez_eze​ turns the problem into a linear program over the convex hull of a set of 0/1 points, the multilinear polytope of the hypergraph whose edges are the monomials. Global solvers such as BARON build polyhedral relaxations of this polytope at every node of their branch-and-bound trees, so valid inequalities that are as strong as possible, that is, facet-defining, translate directly into smaller root gaps.

Del Pia and Khajavirad introduced running intersection inequalities in The running intersection relaxation of the multilinear polytope (Math. Oper. Res. 46 (2021) 1008–1037, doi:10.1287/moor.2021.1121). They generalize the flower inequalities of the same authors (SIAM J. Optim. 2018), which are facet-defining when the support hypergraph is γ\gammaγ-acyclic, to support hypergraphs that are not. This mission formalizes the paper's sufficient condition for a running intersection inequality to define a facet (§2.4, Proposition 4) together with the structural results it rests on.

Timeline. Crama (1993) studied the standard linearization; Del Pia and Khajavirad (2017, Math. Oper. Res.) proved that the multilinear polytope is full dimensional and gave lifting theorems for facets; flower inequalities followed in 2018; running intersection inequalities and the facet conditions formalized here appeared in 2021.

Setting

A hypergraph G=(V,E)G=(V,E)G=(V,E) has a finite node set VVV and a set EEE of subsets of VVV of cardinality at least two. Its multilinear set is

SG={z∈{0,1}V+E: ze=∏v∈ezv  ∀e∈E},\mathcal S_G=\Big\{z\in\{0,1\}^{V+E}:\ z_e=\prod_{v\in e}z_v\ \ \forall e\in E\Big\},SG​={z∈{0,1}V+E: ze​=v∈e∏​zv​  ∀e∈E},

and its multilinear polytope is MPG=conv⁡SG\mathrm{MP}_G=\operatorname{conv}\mathcal S_GMPG​=convSG​.

A multiset FFF of sets has the running intersection property if its elements can be ordered p1,…,pmp_1,\dots,p_mp1​,…,pm​ so that each pk∩(p1∪⋯∪pk−1)p_k\cap(p_1\cup\dots\cup p_{k-1})pk​∩(p1​∪⋯∪pk−1​), k≥2k\ge 2k≥2, is contained in a single earlier pjp_jpj​. Such an ordering defines N(p1)=∅N(p_1)=\emptysetN(p1​)=∅ and N(pk)=pk∩⋃i<kpiN(p_k)=p_k\cap\bigcup_{i<k}p_iN(pk​)=pk​∩⋃i<k​pi​. A leaf of FFF is an element that comes last in some such ordering.

Fix an edge e0e_0e0​ (the center) and edges eke_kek​, k∈Kk\in Kk∈K, adjacent to e0e_0e0​ (the neighbors), such that the multiset E~={e0∩ek:k∈K}\tilde E=\{e_0\cap e_k:k\in K\}E~={e0​∩ek​:k∈K} has the running intersection property. Choose an ordering of E~\tilde EE~, and for each kkk with N(e0∩ek)≠∅N(e_0\cap e_k)\neq\emptysetN(e0​∩ek​)=∅ a node uk∈N(e0∩ek)u_k\in N(e_0\cap e_k)uk​∈N(e0​∩ek​). The running intersection inequality is

−∑k∈K: N(e0∩ek)≠∅zuk+∑v∈e0∖⋃kekzv+∑k∈Kzek−ze0 ≤ ω−1,-\sum_{k\in K:\,N(e_0\cap e_k)\neq\emptyset} z_{u_k}+\sum_{v\in e_0\setminus\bigcup_{k}e_k} z_v+\sum_{k\in K}z_{e_k}-z_{e_0}\ \le\ \omega-1,−k∈K:N(e0​∩ek​)=∅∑​zuk​​+v∈e0​∖⋃k​ek​∑​zv​+k∈K∑​zek​​−ze0​​ ≤ ω−1,

where ω\omegaω is the number of connected components of the hypergraph G~=(e0,E~)\tilde G=(e_0,\tilde E)G~=(e0​,E~). Its support hypergraph GGG has node set e0∪⋃keke_0\cup\bigcup_k e_ke0​∪⋃k​ek​ and edge set {e0}∪{ek:k∈K}\{e_0\}\cup\{e_k:k\in K\}{e0​}∪{ek​:k∈K}. An inequality defines a facet of MPG\mathrm{MP}_GMPG​ if it is valid and the face it cuts out is nonempty of dimension dim⁡MPG−1\dim\mathrm{MP}_G-1dimMPG​−1.

Formalization targets

Goal: Proposition 4 (p. 1016)

Assume

  1. ∣e0∩ek∣≥2|e_0\cap e_k|\ge 2∣e0​∩ek​∣≥2 for every k∈Kk\in Kk∈K;
  2. for every K′⊆KK'\subseteq KK′⊆K with e0∩⋂k∈K′ek≠∅e_0\cap\bigcap_{k\in K'}e_k\neq\emptysete0​∩⋂k∈K′​ek​=∅:  e0∩(ei∖⋃k∈K′∖{i}ek)≠∅\ e_0\cap\big(e_i\setminus\bigcup_{k\in K'\setminus\{i\}}e_k\big)\neq\emptyset e0​∩(ei​∖⋃k∈K′∖{i}​ek​)=∅ for all i∈K′i\in K'i∈K′;
  3. each nonempty N(e0∩ek)N(e_0\cap e_k)N(e0​∩ek​) meets U={uk:N(e0∩ek)≠∅}U=\{u_k: N(e_0\cap e_k)\neq\emptyset\}U={uk​:N(e0​∩ek​)=∅} in exactly one node.

Then the running intersection inequality defines a facet of MPG\mathrm{MP}_GMPG​ for its support hypergraph GGG.

Milestones

Lemma 1 (p. 1011, leaves and reorderings), Lemma 2 (p. 1011, components =n0+∣{e:N(e)=∅}∣=n_0+|\{e:N(e)=\emptyset\}|=n0​+∣{e:N(e)=∅}∣), Proposition 1 (p. 1012, validity), and the full dimensionality of MPG\mathrm{MP}_GMPG​ (cited on p. 1016 from [12]):

dim⁡MPG=∣V∣+∣E∣.\dim\mathrm{MP}_G=|V|+|E|.dimMPG​=∣V∣+∣E∣.

Companions

Corollary 2 (p. 1017): ∣e0∩ek∣≥2|e_0\cap e_k|\ge 2∣e0​∩ek​∣≥2 and ∣e0∩ek∩ek′∣≤1|e_0\cap e_k\cap e_{k'}|\le 1∣e0​∩ek​∩ek′​∣≤1 for k≠k′k\neq k'k=k′ suffice. Proposition 2 and Corollary 1 (pp. 1013–1014): the multiset {N(e)}\{N(e)\}{N(e)}, hence the system of inequalities, does not depend on the ordering. Proposition 3 (p. 1014): necessary conditions for a facet of the running intersection relaxation MPGRI\mathrm{MP}^{\mathrm{RI}}_GMPGRI​.

Significance

Proposition 4 certifies a large family of facets of multilinear polytopes whose support hypergraphs contain cycles that flower inequalities cannot handle. Together with the lifting theorems of Del Pia and Khajavirad (2017), it yields sufficient conditions under which these inequalities define facets of the multilinear polytope of general hypergraphs (p. 1015); §2.5 of the paper reports that running intersection cuts reduce BARON's root-node relaxation gap on image-restoration instances. Proposition 3 and Example 1 show that condition 1 is necessary while conditions 2–3 are not, so the result is a sufficient condition and not a characterization.

The results are proved in the paper; none is formalized. A Lean development would provide the first machine-checked library for the running intersection property (orderings, leaves, the multiset of NNN-sets), the connected-component count of Lemma 2, and the multilinear polytope as a convex hull with an exact dimension count, all reusable for the companion missions on the tightness of MPGRI\mathrm{MP}^{\mathrm{RI}}_GMPGRI​ for kite-free β\betaβ-acyclic hypergraphs and its strictness otherwise.

Difficulty

Validity (Proposition 1) decomposes over the connected components of G~\tilde GG~; the facet claim does not, because a face of codimension one is a global object and the neighbors of different components, and the nodes uku_kuk​ shared between neighbors, interact in it. Conditions 2 and 3 are exactly where this interaction is controlled, and Example 1 of the paper shows that dropping condition 3 does not destroy facetness, so no simple equivalence is available to fall back on. Formally, three nontrivial ingredients have no Mathlib counterpart: the combinatorics of running intersection orderings (Lemma 1, Proposition 2), the count of connected components of a hypergraph with loops and parallel edges (Lemma 2), and the affine dimension of a convex hull of 0/1 points in a space indexed by nodes and edges.

Formalization scope

Nodes form a finite type α; every hypergraph's space RV+E\mathbb R^{V+E}RV+E lives inside α ⊕ Finset α → ℝ, with the coordinates outside V+EV+EV+E pinned to 000 in the definition of SG\mathcal S_GSG​, so dim⁡MPG=∣V∣+∣E∣\dim\mathrm{MP}_G=|V|+|E|dimMPG​=∣V∣+∣E∣ is meaningful. Orderings are lists indexed from 000. The number of components is that of the 2-section graph on the node set. An inequality is given by its data: center, a set KKK of distinct neighbors other than e0e_0e0​, an ordering of KKK whose traces form a running intersection ordering of E~\tilde EE~, and the choice k↦ukk\mapsto u_kk↦uk​; the first sum runs over neighbors, so a node chosen for two neighbors has coefficient −2-2−2. "Defines a facet" requires a nonempty face and compares dimensions as dim⁡F+1=dim⁡P\dim F+1=\dim PdimF+1=dimP, so the empty face can never qualify and no truncated subtraction occurs. The facet statement is about MPG\mathrm{MP}_GMPG​ for the support hypergraph only, not for a larger host hypergraph, which would require the lifting theorems. The reading k≠k′k\neq k'k=k′ is used where the page's "for all k,k′k,k'k,k′" would otherwise be contradictory (Corollary 2, Proposition 3(i)); Lemma 2 is stated for lists of nonempty sets, which covers its use on G~\tilde GG~.

Contributions welcome: proofs of the milestones, a reusable library for the running intersection property and α\alphaα-acyclic hypergraphs, and the full-dimensionality proof.

Selected references

  • A. Del Pia, A. Khajavirad, The running intersection relaxation of the multilinear polytope, Math. Oper. Res. 46(3):1008–1037, 2021. https://doi.org/10.1287/moor.2021.1121
  • A. Del Pia, A. Khajavirad, A polyhedral study of binary polynomial programs, Math. Oper. Res. 42(2):389–410, 2017. https://doi.org/10.1287/moor.2016.0804
  • A. Del Pia, A. Khajavirad, The multilinear polytope for acyclic hypergraphs, SIAM J. Optim. 28(2):1049–1076, 2018. https://doi.org/10.1137/16M1095998
  • C. Beeri, R. Fagin, D. Maier, M. Yannakakis, On the desirability of acyclic database schemes, J. ACM 30(3):479–513, 1983. https://doi.org/10.1145/2402.322389
  • Y. Crama, Concave extensions for nonlinear 0–1 maximization problems, Math. Programming 61:53–60, 1993. https://doi.org/10.1007/BF01582138
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Convex OptimizationOperations ResearchProbability·Captain: mikedeng1

Arbitrage and Duality in Nondominated Discrete-Time Models II: Nondominated Optional Decomposition — a Supermartingale Under Every Martingale Measure Is V₀ + H•S − KResearch Paper

Motivation

In a financial market with a single probability model, the Optional Decomposition Theorem describes the processes that can be dominated by trading. If a process VVV is a supermartingale under every equivalent martingale measure, then it can be written as an initial value plus a stochastic integral against the stock price, minus an increasing process that represents consumption. El Karoui and Quenez proved it for diffusion models (SIAM J. Control Optim. 33 (1995)) and Kramkov for locally bounded semimartingales (Probab. Theory Related Fields 105 (1996)). It is the step that turns the superhedging price, a supremum of expectations over martingale measures, into an actual dynamic hedging strategy.

Model uncertainty replaces the single model by a set P\mathcal PP of probability measures that may be mutually singular. This happens, for example, when volatility is only known to lie in an interval. There is then no reference measure, "almost surely" becomes "quasi surely" (outside a set that is null under every model), and the classical proofs, which rely on one dominating measure, do not apply. Bouchard and Nutz (Ann. Appl. Probab. 2015, arXiv:1305.6008) built the discrete-time theory of this setting: no-arbitrage, the fundamental theorem of asset pricing, superhedging duality and, in §6, a nondominated optional decomposition. This mission formalizes that last result.

Timeline:

  • 1995: El Karoui and Quenez, optional decomposition in diffusion models.
  • 1996: Kramkov, for locally bounded semimartingales.
  • 2014: Nutz, superreplication duality under model uncertainty in discrete time (Finance Stoch. 18 (2014)).
  • 2015: Bouchard and Nutz, the fundamental theorem, superhedging duality and the optional decomposition in nondominated discrete time (Theorem 6.1).

Setting

Fix a Polish space Ω1\Omega_1Ω1​, a horizon T∈NT \in \mathbb NT∈N and d∈Nd \in \mathbb Nd∈N. Let Ωt:=Ω1t\Omega_t := \Omega_1^tΩt​:=Ω1t​ for t=0,…,Tt = 0, \dots, Tt=0,…,T. Then Ω0\Omega_0Ω0​ is a single point and Ω:=ΩT\Omega := \Omega_TΩ:=ΩT​, and a point of Ωt\Omega_tΩt​ is read as the first ttt coordinates of a path. The σ\sigmaσ-field Ft\mathcal F_tFt​ is the universal completion of B(Ωt)\mathcal B(\Omega_t)B(Ωt​).

For each t<Tt < Tt<T and each node ω∈Ωt\omega \in \Omega_tω∈Ωt​ a nonempty convex set Pt(ω)\mathcal P_t(\omega)Pt​(ω) of probability measures on Ω1\Omega_1Ω1​ is given, and its graph is an analytic set. The set of possible models P\mathcal PP consists of all products P0⊗P1⊗⋯⊗PT−1P_0 \otimes P_1 \otimes \cdots \otimes P_{T-1}P0​⊗P1​⊗⋯⊗PT−1​ whose kernels take values in Pt(⋅)\mathcal P_t(\cdot)Pt​(⋅). A set is P\mathcal PP-polar if it is null under every P∈PP \in \mathcal PP∈P. A property holds P\mathcal PP-quasi surely (q.s.) if it holds outside a polar set.

Stock prices St:Ωt→RdS_t : \Omega_t \to \mathbb R^dSt​:Ωt​→Rd are Borel. A strategy H∈HH \in \mathcal HH∈H is predictable: HuH_uHu​ is a function of the first u−1u-1u−1 coordinates. The wealth at time ttt is

H∙St=∑u=1tHuΔSu,ΔSu=Su−Su−1.H \bullet S_t = \sum_{u=1}^t H_u \Delta S_u, \qquad \Delta S_u = S_u - S_{u-1}.H∙St​=u=1∑t​Hu​ΔSu​,ΔSu​=Su​−Su−1​.

NA(P\mathcal PP) holds if H∙ST≥0H \bullet S_T \ge 0H∙ST​≥0 q.s. implies H∙ST=0H \bullet S_T = 0H∙ST​=0 q.s. A martingale measure is a probability QQQ under which SSS is a martingale. The set

Q={Q⋘P:Q is a martingale measure}\mathcal Q = \{Q \lll \mathcal P : Q \text{ is a martingale measure}\}Q={Q⋘P:Q is a martingale measure}

contains those QQQ that are absolutely continuous with respect to some P∈PP \in \mathcal PP∈P (written Q⋘PQ \lll \mathcal PQ⋘P). A function fff with values in [−∞,∞][-\infty, \infty][−∞,∞] is upper semianalytic if every set {f>c}\{f > c\}{f>c} is analytic.

At one node ω∈Ωt\omega \in \Omega_tω∈Ωt​, the increment ΔSt+1(ω,⋅)\Delta S_{t+1}(\omega, \cdot)ΔSt+1​(ω,⋅) defines a one-period market under Pt(ω)\mathcal P_t(\omega)Pt​(ω), with its own no-arbitrage condition NA(Pt(ω)\mathcal P_t(\omega)Pt​(ω)) and one-period martingale measures Qt(ω)\mathcal Q_t(\omega)Qt​(ω). The conditional sublinear expectation is

Et(f)(ω)=sup⁡Q∈Qt(ω)EQ[f(ω,⋅)].\mathcal E_t(f)(\omega) = \sup_{Q \in \mathcal Q_t(\omega)} E_Q[f(\omega, \cdot)].Et​(f)(ω)=Q∈Qt​(ω)sup​EQ​[f(ω,⋅)].

Formalization targets

Goal: Theorem 6.1 (nondominated optional decomposition)

Let NA(P\mathcal PP) hold and let VVV be an adapted process such that VtV_tVt​ is upper semianalytic and in L1(Q)L^1(Q)L1(Q) for all Q∈QQ \in \mathcal QQ∈Q and t∈{1,…,T}t \in \{1, \dots, T\}t∈{1,…,T}. Then the following are equivalent:

  1. VVV is a supermartingale under each Q∈QQ \in \mathcal QQ∈Q;
  2. there exist H∈HH \in \mathcal HH∈H and an adapted increasing process KKK with K0=0K_0 = 0K0​=0 such that
Vt=V0+H∙St−KtP-q.s.,t=0,1,…,T.V_t = V_0 + H \bullet S_t - K_t \quad \mathcal P\text{-q.s.}, \qquad t = 0, 1, \dots, T.Vt​=V0​+H∙St​−Kt​P-q.s.,t=0,1,…,T.

Milestones

  • Lemma 4.6: the set NtN_tNt​ of nodes where NA(Pt(ω)\mathcal P_t(\omega)Pt​(ω)) fails is universally measurable, and it is polar under NA(P\mathcal PP).
  • Theorem 4.5: NA(P\mathcal PP) holds if and only if every NtN_tNt​ is polar, if and only if every P∈PP \in \mathcal PP∈P is absolutely continuous with respect to some Q∈QQ \in \mathcal QQ∈Q.
  • Lemma 4.10: Et(f)\mathcal E_t(f)Et​(f) is upper semianalytic, and there is a universally measurable yyy with
Et(f)(ω)+y(ω) ΔSt+1(ω,⋅)≥f(ω,⋅)Pt(ω)-q.s.\mathcal E_t(f)(\omega) + y(\omega)\,\Delta S_{t+1}(\omega, \cdot) \ge f(\omega, \cdot) \quad \mathcal P_t(\omega)\text{-q.s.}Et​(f)(ω)+y(ω)ΔSt+1​(ω,⋅)≥f(ω,⋅)Pt​(ω)-q.s.

at every arbitrage-free node where f(ω,⋅)>−∞f(\omega,\cdot) > -\inftyf(ω,⋅)>−∞ q.s.

  • (6.1): under condition 1 of the goal, Et(Vt+1)≤Vt\mathcal E_t(V_{t+1}) \le V_tEt​(Vt+1​)≤Vt​ P\mathcal PP-q.s. for every t<Tt < Tt<T.

Significance

The decomposition is the dynamic counterpart of superhedging duality. Duality identifies the price sup⁡QEQ[f]\sup_{Q} E_Q[f]supQ​EQ​[f]. The optional decomposition, applied to the process of conditional superhedging prices, produces one strategy that superhedges under all models at once and a nonnegative increasing process recording the surplus. The proof works in a nondominated model with one strategy HHH that is measurable in the universal completion, and this is what makes the theorem usable under volatility or model uncertainty, where no single model can be singled out. The equivalence also characterizes the processes that are supermartingales under every Q∈QQ \in \mathcal QQ∈Q: up to a polar set they are exactly the wealth processes of strategies that consume.

The result is proved in the paper; no part of it has a machine-checked proof, on the platform or in Mathlib. Mathlib has martingales, conditional expectation and analytic sets. It has no quasi-sure analysis, no product of measurable selectors of a random set of measures, no conditional sublinear expectation and no superhedging. The mission produces a machine-checked development of the one-period-to-multi-period machinery of the paper (Theorem 4.5, Lemmas 4.6 and 4.10) and of the decomposition itself.

Difficulty

With one dominating measure, the classical proof works under a fixed equivalent martingale measure and uses conditional expectations and a single null-set structure. Here the measures in P\mathcal PP may be mutually singular, so conditional expectations under different QQQ disagree off their supports, and no countable family of measures controls all null sets. The proof has to work node by node, ω↦Pt(ω)\omega \mapsto \mathcal P_t(\omega)ω↦Pt​(ω). Every object built at a node (the worst-case conditional expectation, a near-optimal measure, a hedging ratio) must then be glued back together measurably in ω\omegaω. Borel measurability is not preserved by taking suprema over the random set Qt(ω)\mathcal Q_t(\omega)Qt​(ω). Upper semianalyticity is, but only together with measurable selection theorems for analytic sets (Jankov–von Neumann) and the universal completion. The first idea, which is to apply the classical theorem under each P∈PP \in \mathcal PP∈P separately, fails. It gives one strategy per model, and in general uncountably many models cannot be aggregated into one strategy.

Formalization scope

The Lean development uses the following conventions.

  • Paths and measures. Ωt\Omega_tΩt​ is Fin t → Ω₁, and measures are Borel. Ft\mathcal F_tFt​-measurability is universal measurability, which is the published platform definition BertsekasShreve.AnalyticSelection.IsUniversallyMeasurable.
  • Polar sets. A polar set is null in outer measure under every model. The exceptional sets in the statements are universally measurable, and for such sets this agrees with the paper's definition.
  • The model set. P\mathcal PP consists of the laws of Borel Markov kernels that lie in Pt\mathcal P_tPt​ almost surely, which is the paper's equivalent formulation on p. 4.
  • Processes. A process is a family V t : (Fin t → Ω₁) → ℝ, so adaptedness is built into the type.
  • Strategies. The Lean strategy H u is the paper's Hu+1H_{u+1}Hu+1​.
  • Expectations. Expectations of functions with values in [−∞,∞][-\infty, \infty][−∞,∞] follow (1.1) in EReal, with ∞−∞=−∞\infty - \infty = -\infty∞−∞=−∞. Suprema over Qt(ω)\mathcal Q_t(\omega)Qt​(ω) are taken in EReal.
  • Options. The setting has no options (e=0e = 0e=0).
  • Page numbers. Pages and indices are those of the arXiv v3 reprint (arXiv:1305.6008v3), not the journal pagination 823–859.

The increasing process KKK must be adapted and nondecreasing on every path. Dropping monotonicity would make condition 2 trivially true, with K:=V0+H∙S−VK := V_0 + H \bullet S - VK:=V0​+H∙S−V for any HHH. Integrability and supermartingale properties are always stated with explicit QQQ-integrability, so Bochner integrals of non-integrable functions cannot make a statement vacuous.

The development needs the following infrastructure:

  • analytic sets and measurable selection (some of it exists for Bertsekas–Shreve on the platform);
  • measurability of (ω,Q)↦EQ[f(ω,⋅)](\omega, Q) \mapsto E_Q[f(\omega,\cdot)](ω,Q)↦EQ​[f(ω,⋅)];
  • products of kernels;
  • the one-period fundamental theorem and superhedging duality.

These pieces are shared with the companion mission Arbitrage and Duality in Nondominated Discrete-Time Models I, which formalizes the superhedging theorem. Contributions to either side are welcome. The paper derives (ii) ⇒ (i) from Lemma A.1, a classical fact about local and generalized martingales under one measure, which is not posed as a milestone here.

Selected references

  • B. Bouchard, M. Nutz, Arbitrage and duality in nondominated discrete-time models, Ann. Appl. Probab. 25(2), 823–859, 2015. https://doi.org/10.1214/14-AAP1011, arXiv:1305.6008v3 https://arxiv.org/abs/1305.6008
  • N. El Karoui, M.-C. Quenez, Dynamic programming and pricing of contingent claims in an incomplete market, SIAM J. Control Optim. 33, 29–66, 1995. MR1311659, https://mathscinet.ams.org/mathscinet-getitem?mr=1311659
  • D. O. Kramkov, Optional decomposition of supermartingales and hedging contingent claims in incomplete security markets, Probab. Theory Related Fields 105, 459–479, 1996. MR1402653, https://mathscinet.ams.org/mathscinet-getitem?mr=1402653
  • M. Nutz, Superreplication under model uncertainty in discrete time, Finance Stoch. 18, 791–803, 2014. MR3255751, https://mathscinet.ams.org/mathscinet-getitem?mr=3255751
  • D. P. Bertsekas, S. E. Shreve, Stochastic Optimal Control: The Discrete Time Case, Mathematics in Science and Engineering 139, Academic Press, 1978. MR0511544, https://mathscinet.ams.org/mathscinet-getitem?mr=0511544
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Control TheoryPartial Differential EquationsProbability·Captain: mikedeng1

Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 2: Comparison Principle and Uniqueness for Viscosity Solutions of Parabolic Master EquationsResearch Paper

Motivation

Master equations are partial differential equations whose state variable is a probability measure. They arise as the dynamic programming equations of mean-field control problems, as the limits of large particle systems, and as the pricing equations of options on a whole population. Their coefficients and solutions are functions on a Wasserstein space, which is infinite dimensional, and classical (smooth) solutions are known only under strong regularity assumptions (Cardaliaguet–Delarue–Lasry–Lions 2019). A notion of weak solution for which existence, comparison and uniqueness can all be proved is therefore the basic missing tool.

C. Wu and J. Zhang (Ann. Appl. Probab. 2020) propose such a notion for parabolic master equations on the space of laws of continuous paths, in the spirit of the viscosity theory for path-dependent PDEs of Ekren, Keller, Touzi and Zhang (Ann. Probab. 2014). This mission formalizes its §4: the definition of viscosity solutions and the comparison principle that makes them unique.

Setting

Fix a horizon TTT and a dimension ddd. The canonical space is Ω=C([0,T];Rd)\Omega=C([0,T];\mathbb R^d)Ω=C([0,T];Rd) with the uniform norm ∥ω∥\|\omega\|∥ω∥, the canonical process is Xt(ω)=ωtX_t(\omega)=\omega_tXt​(ω)=ωt​, and Ft=σ(Xs:s≤t)\mathcal F_t=\sigma(X_s:s\le t)Ft​=σ(Xs​:s≤t). P2\mathcal P_2P2​ is the set of probability measures μ\muμ on Ω\OmegaΩ with Eμ∥X∥2<∞\mathbb E^\mu\|X\|^2<\inftyEμ∥X∥2<∞; μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of the stopped path Xt∧⋅X_{t\wedge\cdot}Xt∧⋅​. The state space is Θ=[0,T]×P2\Theta=[0,T]\times\mathcal P_2Θ=[0,T]×P2​ with the pseudometric

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

where W2\mathcal W_2W2​ on laws is the 2-Wasserstein distance. A function V:Θ→RV:\Theta\to\mathbb RV:Θ→R has a time derivative ∂tV\partial_tV∂t​V, a path derivative ∂μV(t,μ,ω)∈Rd\partial_\mu V(t,\mu,\omega)\in\mathbb R^d∂μ​V(t,μ,ω)∈Rd and a second derivative ∂ω∂μV(t,μ,ω)∈Rd×d\partial_\omega\partial_\mu V(t,\mu,\omega)\in\mathbb R^{d\times d}∂ω​∂μ​V(t,μ,ω)∈Rd×d, defined through a functional Itô formula along semimartingale laws.

The master equation (3.1) is

LV(t,μ):=∂tV(t,μ)+G(t,μ,V(t,μ),∂μV(t,μ,⋅),∂ω∂μV(t,μ,⋅))=0,\mathbb LV(t,\mu):=\partial_tV(t,\mu)+G\big(t,\mu,V(t,\mu),\partial_\mu V(t,\mu,\cdot),\partial_\omega\partial_\mu V(t,\mu,\cdot)\big)=0,LV(t,μ):=∂t​V(t,μ)+G(t,μ,V(t,μ),∂μ​V(t,μ,⋅),∂ω​∂μ​V(t,μ,⋅))=0,

with a generator GGG that is continuous in (t,μ)(t,\mu)(t,μ), Lipschitz in yyy, and Lipschitz in (Z,Γ)(Z,\Gamma)(Z,Γ) in the averaged sense (3.2) of Assumption 3.1.

For L>0L>0L>0, PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the set of laws P∈P2\mathbb P\in\mathcal P_2P∈P2​ that agree with μ\muμ up to time ttt and under which XXX is a semimartingale on [t,T][t,T][t,T] with drift bounded by LLL and half squared diffusion bounded by LLL. Test functions at (t,μ)(t,\mu)(t,μ) are C1,1,1C^{1,1,1}C1,1,1 functions on [t,t+δ]×PL(t,μ)[t,t+\delta]\times\mathcal P_L(t,\mu)[t,t+δ]×PL​(t,μ) touching VVV from above or below there, (4.2). V∈C0(Θ)V\in C^0(\Theta)V∈C0(Θ) is an LLL-viscosity subsolution (supersolution) if Lφ(t,μ)≥0\mathbb L\varphi(t,\mu)\ge0Lφ(t,μ)≥0 (≤0\le0≤0) for every such test function, and a viscosity solution if it is both for one L>0L>0L>0 (Definition 4.4). The Perron envelopes V‾\overline VV, V‾\underline VV​ of (4.17) are the infimum of piecewise classical supersolutions above ggg and the supremum of piecewise classical subsolutions below ggg.

Formalization targets

Goal: comparison and uniqueness (Theorem 4.13)

Under Assumption 3.1 and g∈C0(P2)g\in C^0(\mathcal P_2)g∈C0(P2​), if V1V_1V1​ is a viscosity subsolution, V2V_2V2​ a viscosity supersolution, V1(T,⋅)≤g≤V2(T,⋅)V_1(T,\cdot)\le g\le V_2(T,\cdot)V1​(T,⋅)≤g≤V2​(T,⋅), the classes U‾g,U‾g\underline{\mathcal U}_g,\overline{\mathcal U}_gU​g​,Ug​ are nonempty, and

V‾=V‾=:V,(4.19)\overline V=\underline V=:V,\qquad(4.19)V=V​=:V,(4.19)

then V1≤V≤V2V_1\le V\le V_2V1​≤V≤V2​ on Θ\ThetaΘ, and VVV is the unique viscosity solution with terminal condition ggg.

Milestones

  1. the moment estimate (4.1) over PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ);
  2. Lemma 4.1: [t,T]×PL(t,μ)[t,T]\times\mathcal P_L(t,\mu)[t,T]×PL​(t,μ) is compact under W2\mathcal W_2W2​;
  3. Theorem 4.7: viscosity solutions are characterized by semi-jets of paraboloids;
  4. Theorem 4.9: the change of variable V~=eλtV\tilde V=e^{\lambda t}VV~=eλtV;
  5. Theorem 4.6: consistency with classical solutions;
  6. Theorem 4.11: partial comparison when one side is smooth;
  7. Proposition 4.12: a continuous lower envelope V‾\underline VV​ is a viscosity subsolution.

Significance

The comparison principle is what turns a definition into a theory: it gives uniqueness, it identifies value functions of mean-field control problems with the solution of their master equation, and it is the input of stability and convergence arguments for numerical schemes. Theorem 4.13 reduces well-posedness to condition (4.19), and the authors verify (4.19) in examples (§4.6) via Theorem 4.14. The compactness of PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) (Lemma 4.1) is the device that replaces local compactness, which the Wasserstein space lacks; it is reusable for any viscosity theory over semimartingale laws.

These results are proved on paper. No machine-checked development of viscosity solutions on Wasserstein spaces, or of the path-dependent functional Itô calculus on laws, is known to exist. A formalization would produce a checked notion of viscosity solution for master equations, the compactness of bounded-characteristic semimartingale laws, and the comparison machinery, and would expose the points where the printed proofs are sketched (see below).

Difficulty

The obvious route, copying the finite-dimensional theory, fails at two places. First, the doubling-of-variables argument for comparison needs a penalization on the state space that is smooth and coercive; on P2\mathcal P_2P2​ under W2\mathcal W_2W2​ neither is available, which is why comparison is reached through partial comparison and Perron envelopes. Second, maxima of φ−V\varphi-Vφ−V need not be attained on Wasserstein balls, which are not compact; the theory therefore tests only on [t,T]×PL(t,μ)[t,T]\times\mathcal P_L(t,\mu)[t,T]×PL​(t,μ), and Lemma 4.1 (via Zheng's tightness criterion for semimartingale laws and uniform integrability of ∥X∥2\|X\|^2∥X∥2) is what makes the extrema exist. The printed proof of Theorem 4.13 opens with "V‾\overline VV is lower semicontinuous and V‾\underline VV​ is upper semicontinuous"; as printed the directions are swapped (an infimum of functions continuous in μ\muμ is upper semicontinuous in μ\muμ), and the members of U\mathcal UU are only càdlàg in ttt, so the continuity of VVV needed for the conclusion requires an argument of its own.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​, and every condition is imposed only at t≤Tt\le Tt≤T, μ∈P2\mu\in\mathcal P_2μ∈P2​. Rd\mathbb R^dRd is the Euclidean space, matrices are d×dd\times dd×d real matrices with the Frobenius norm, and A:B=∑ijAijBijA:B=\sum_{ij}A_{ij}B_{ij}A:B=∑ij​Aij​Bij​. W2\mathcal W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance on laws of paths; Brownian motion and the Itô integral are the published EthierKurtz definitions. Membership in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the existence of a representation of P\mathbb PP as the law of an Itô process from time ttt with ∣b∣≤L|b|\le L∣b∣≤L, 12∣σ∣2≤L\tfrac12|\sigma|^2\le L21​∣σ∣2≤L (§2.4). A C1,1,1C^{1,1,1}C1,1,1 object is a record of a function and three derivative functions, and the functional Itô formula (2.25) is required in drift form for every representation, which equals (2.25) because the stochastic integral has mean zero. Test sets encode "inf⁡(φ−V)=0\inf(\varphi-V)=0inf(φ−V)=0" literally, and the data of a test function at (t,μ)(t,\mu)(t,μ) are its values at (t,P)(t,\mathbb P)(t,P), P∈PL(t,μ)\mathbb P\in\mathcal P_L(t,\mu)P∈PL​(t,μ). The Perron envelopes are extended-real infima and suprema over the classes (4.18); (4.19) is stated with a real-valued VVV.

Two readings are fixed. Assumption 3.1(i) is continuity of (t,μ)↦G(t,μ,y,Z(Xt∧⋅),Γ(Xt∧⋅))(t,\mu)\mapsto G(t,\mu,y,Z(X_{t\wedge\cdot}),\Gamma(X_{t\wedge\cdot}))(t,μ)↦G(t,μ,y,Z(Xt∧⋅​),Γ(Xt∧⋅​)) for fixed continuous Z,ΓZ,\GammaZ,Γ of linear growth. "V∈Cb1,1,1(Θ)V\in C_b^{1,1,1}(\Theta)V∈Cb1,1,1​(Θ)" in Theorems 4.6 and 4.11 is replaced by the larger class it is used through (Remark 4.3(i)): data continuous on Θ\ThetaΘ lying in Cb1,1,1([t1,t2]×PL(t1,μ))C_b^{1,1,1}([t_1,t_2]\times\mathcal P_L(t_1,\mu))Cb1,1,1​([t1​,t2​]×PL​(t1​,μ)) for all t1<t2t_1<t_2t1​<t2​, LLL, μ\muμ, so those statements are at least as strong as printed.

The definitions cannot be satisfied vacuously: every test set requires a witness law in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ), the class Cb1,1,1C_b^{1,1,1}Cb1,1,1​ contains the constants (checked in Lean), and a viscosity solution uses one LLL for both halves. The semi-jets range only over Ft\mathcal F_tFt​-measurable continuous arguments of linear growth, as printed.

Contributions are welcome at every level: the moment bound (4.1) and Lemma 4.1 need tightness and uniform-integrability results for semimartingale laws on path space that Mathlib does not have; Theorems 4.7 and 4.9 are self-contained manipulations of the definitions; Theorems 4.6 and 4.11 and Proposition 4.12 need the compactness lemma and the Itô identity of test functions.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2) (2020) 936–986. https://doi.org/10.1214/19-AAP1521
  • I. Ekren, C. Keller, N. Touzi, J. Zhang, On viscosity solutions of path dependent PDEs, Ann. Probab. 42(1) (2014) 204–236. https://doi.org/10.1214/12-AOP788
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The Master Equation and the Convergence Problem in Mean Field Games, Annals of Mathematics Studies 201, Princeton University Press, 2019. https://doi.org/10.2307/j.ctvckq7qf
  • 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
  • W. A. Zheng, Tightness results for laws of diffusion processes application to stochastic mechanics, Ann. Inst. H. Poincaré Probab. Statist. 21(2) (1985) 103–124. http://www.numdam.org/item/AIHPB_1985__21_2_103_0/
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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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The Bayesian Prophet: A Low-Regret Framework for Online Decision Making: Constant Regret of the Fluid Bayes Selector for the Multi-Secretary ProblemResearch Paper

Motivation

In online allocation, requests arrive one at a time and each must be accepted or rejected on arrival, using a limited budget of resources. Revenue management, ad allocation and hiring all fit this pattern. A natural benchmark for an online policy is the prophet, or Offline: the decision maker who sees the whole arrival sequence in advance and acts optimally on it. The regret of a policy is the expected gap between Offline's value and the policy's value. Policies that track a fixed solution of a fluid relaxation lose on the order of T\sqrt TT​ (Proposition 1 of the paper), so the question is whether a simple adaptive policy can achieve regret bounded independently of TTT and of the budget.

The simplest such problem is the multi-secretary problem: hire at most BBB of TTT sequentially arriving candidates, each drawn i.i.d. from finitely many ability classes. Arlotto and Gurvich (Stochastic Systems 2019) showed that a budget-ratio policy has regret bounded uniformly in TTT and BBB, using a martingale argument. Vera and Banerjee (SSRN 3158062; Management Science 2021) introduced the compensated coupling, a sample-path identity that expresses the regret of any online policy as the compensation Offline must be paid to follow it. They used it to prove constant regret for a simple re-solve-and-threshold rule, the Fluid Bayes Selector, with the explicit constant rmax⁡∑j>12/pjr_{\max}\sum_{j>1}2/p_jrmax​∑j>1​2/pj​. This mission formalizes that result together with the compensated coupling it rests on.

Setting

A finite-horizon online decision problem has states SSS, arrival types Θ\ThetaΘ, actions AAA, a transition function T(a,s,j)T(a,s,j)T(a,s,j), a reward function R(a,s,j)R(a,s,j)R(a,s,j), and a set F(s)\mathcal F(s)F(s) of feasible actions in each state. Time is counted as time to go: decisions are made at t=T,T−1,…,1t=T,T-1,\dots,1t=T,T−1,…,1, and θt\theta^tθt is the type arriving at time-to-go ttt. A standing assumption requires the best feasible reward in every state to be attained and to lie in a fixed bounded interval.

Given the whole arrival sequence, Offline's value obeys the Bellman equation

Voff(0,s)=0,Voff(t,s)=max⁡a∈F(s){R(a,s,θt)+Voff(t−1,T(a,s,θt))}.V^{\mathrm{off}}(0,s)=0,\qquad V^{\mathrm{off}}(t,s)=\max_{a\in\mathcal F(s)}\{R(a,s,\theta^t)+V^{\mathrm{off}}(t-1,T(a,s,\theta^t))\}.Voff(0,s)=0,Voff(t,s)=a∈F(s)max​{R(a,s,θt)+Voff(t−1,T(a,s,θt))}.

An online policy chooses a feasible action at each time from the arrivals observed so far. Starting from ST=s0S^T=s_0ST=s0​ it produces a state process StS^tSt and a value Von=∑tR(πon(t,St,θt),St,θt)V^{\mathrm{on}}=\sum_{t}R(\pi^{\mathrm{on}}(t,S^t,\theta^t),S^t,\theta^t)Von=∑t​R(πon(t,St,θt),St,θt), and its regret on a path is Reg=Voff(T,s0)−Von\mathrm{Reg}=V^{\mathrm{off}}(T,s_0)-V^{\mathrm{on}}Reg=Voff(T,s0​)−Von. An action is satisfying for Offline at (t,s)(t,s)(t,s) when it attains the Bellman maximum. The disagreement set Q(t,a,s)Q(t,a,s)Q(t,a,s) is the set of paths on which it does not, and the marginal compensation ∂R(t,a,s)\partial R(t,a,s)∂R(t,a,s) is the amount by which it falls short.

In the multi-secretary problem there are nnn classes with rewards r1≥r2≥⋯≥rn≥0r_1\ge r_2\ge\dots\ge r_n\ge0r1​≥r2​≥⋯≥rn​≥0 and arrival probabilities pj>0p_j>0pj​>0, i.i.d. over time (multinomial arrivals). The state is the remaining budget bbb. Accepting needs b≥1b\ge1b≥1, earns rjr_jrj​ and lowers the budget by one; rejecting earns nothing. With pˉj=∑i≤jpi\bar p_j=\sum_{i\le j}p_ipˉ​j​=∑i≤j​pi​, the Fluid Bayes Selector (Algorithm 2, in the rounded form of Appendix B.3) behaves as follows at time-to-go ttt with budget bbb. If b=0b=0b=0 it rejects. Otherwise it always accepts class 111, and it accepts a class j>1j>1j>1 iff b/t≥pˉj−pj/2b/t\ge\bar p_j-p_j/2b/t≥pˉ​j​−pj​/2.

Formalization targets

Goal: Theorem 2 (p. 18)

For every horizon TTT and every initial budget BBB,

E[Reg] ≤ rmax⁡∑j>12pj ≤ 2(n−1) rmax⁡pmin⁡,\mathbb E[\mathrm{Reg}]\ \le\ r_{\max}\sum_{j>1}\frac{2}{p_j}\ \le\ \frac{2(n-1)\,r_{\max}}{p_{\min}},E[Reg] ≤ rmax​j>1∑​pj​2​ ≤ pmin​2(n−1)rmax​​,

where rmax⁡=max⁡jrjr_{\max}=\max_jr_jrmax​=maxj​rj​ and pmin⁡=min⁡jpjp_{\min}=\min_jp_jpmin​=minj​pj​. The goal keeps the paper's explicit constant: neither TTT nor BBB appears in it.

Milestones

  1. Lemma 1 (Compensated Coupling), pathwise: Reg=∑t∈[T]∂R(t,πon(t,St,θt),St) 1Q(t,St)\mathrm{Reg}=\sum_{t\in[T]}\partial R(t,\pi^{\mathrm{on}}(t,S^t,\theta^t),S^t)\,\mathbf 1_{Q(t,S^t)}Reg=∑t∈[T]​∂R(t,πon(t,St,θt),St)1Q(t,St)​ for any online policy of any problem.
  2. Lemma 1, in expectation: E[Reg]≤max⁡a,j∂r(a,j)∑tP[Q(t,St)]\mathbb E[\mathrm{Reg}]\le\max_{a,j}\partial r(a,j)\sum_t\mathbb P[Q(t,S^t)]E[Reg]≤maxa,j​∂r(a,j)∑t​P[Q(t,St)].
  3. Eq. (18): P[X−EX≤−tε]\mathbb P[X-\mathbb E X\le-t\varepsilon]P[X−EX≤−tε] and P[X−EX≥tε]\mathbb P[X-\mathbb E X\ge t\varepsilon]P[X−EX≥tε] are at most e−2ε2te^{-2\varepsilon^2t}e−2ε2t for X∼Bin(t,α)X\sim\mathrm{Bin}(t,\alpha)X∼Bin(t,α).
  4. Appendix B.3, conditions (1)–(2): when Offline is not satisfied rejecting or accepting the current arrival.
  5. Appendix B.3, disagreement bound: q1(t,b)=0q_1(t,b)=0q1​(t,b)=0 and qj(t,b)≤e−pj2t/2q_j(t,b)\le e^{-p_j^2t/2}qj​(t,b)≤e−pj2​t/2 for j>1j>1j>1, uniformly in the budget bbb.
  6. Appendix B.3, total compensation: ∑t≤Tq(t,Bt)≤∑j>1pj∑t≤Te−pj2t/2≤∑j>12/pj\sum_{t\le T}q(t,B^t)\le\sum_{j>1}p_j\sum_{t\le T}e^{-p_j^2t/2}\le\sum_{j>1}2/p_j∑t≤T​q(t,Bt)≤∑j>1​pj​∑t≤T​e−pj2​t/2≤∑j>1​2/pj​.

Significance

The result. Theorem 2 gives the best known regret bound for the multi-secretary problem with an explicit, simple constant. The compensated coupling (Lemma 1) holds for any finite-horizon problem with exogenous arrivals. It turns a regret bound into a bound on disagreement probabilities, and the paper reuses it for online packing, online matching and general online allocation, and for Bayes Selectors whose disagreement probabilities are only estimated.

Formalizing it. The theorem is proved in the paper; no machine-checked proof of it, or of the compensated coupling, is known to us. The mission produces a reusable formal model of finite-horizon online decision problems with an Offline benchmark. It also produces a formal compensated-coupling identity that applies to any policy, and a binomial Chernoff–Hoeffding bound in elementary finite-sum form. Each of these supports other missions on prophet benchmarks, resolving heuristics and network revenue management.

Difficulty

Comparing the online policy with one fixed offline solution does not work: Offline's optimal decisions change with every future arrival, and tracking a single offline plan only gives regret of order T\sqrt TT​. The compensated coupling avoids this by re-coupling Offline to Online at every step. That shifts the difficulty to two places. The first is an exact description of when Offline's Bellman equation disagrees with the policy, which involves ties between equal rewards and the boundary budget b=0b=0b=0. The second is a bound on the conditional probability of disagreement that is uniform over all budgets. That conditional probability is a binomial tail evaluated at a budget that is itself random but independent of the remaining arrivals.

Formalization scope

Lean conventions:

  • Types are Fin n with [NeZero n], and Lean index 0 is the paper's class 111.
  • The ordering r1≥⋯≥rnr_1\ge\dots\ge r_nr1​≥⋯≥rn​ is Antitone r, so ties are allowed.
  • Rewards are real and non-negative. This is the paper's implicit assumption (rewards are abilities), made explicit.
  • The probabilities satisfy pj>0p_j>0pj​>0 and ∑jpj=1\sum_jp_j=1∑j​pj​=1.
  • Time is time-to-go. θ t is the arrival at time-to-go t, and the counts Z(t)Z(t)Z(t) include the current arrival.
  • Feasibility is an explicit set of actions rather than a reward of −∞-\infty−∞. Offline's value is a real supremum over feasible actions, which equals the Bellman maximum under the standing assumption.
  • Offline is the integer full-information optimum of the Bellman equation (2). It is not defined through an LP relaxation.
  • For the multi-secretary goal, the expectation is the explicit finite sum over the nTn^TnT type sequences weighted by ∏tpθt\prod_tp_{\theta^t}∏t​pθt​. Lemma 1's expectation bound is stated on an abstract probability space with integrable regret.
  • E[P[Q∣St]]\mathbb E[\mathbb P[Q\mid S^t]]E[P[Q∣St]] is written as P[Q]\mathbb P[Q]P[Q] (tower property).
  • The maximal compensation max⁡a,j∂r(a,j)\max_{a,j}\partial r(a,j)maxa,j​∂r(a,j) is replaced by any upper bound CCC on the compensations of feasible actions.
  • Conditions (1)–(2) of Appendix B.3 are stated through counts of future arrivals with a better (or equal) reward, which is the exact Bellman characterization. The paper phrases them through a solution X⋆tX^{\star t}X⋆t of (Pt⋆)(P^\star_t)(Pt⋆​), which is not unique when rewards tie.
  • The disagreement bounds are stated for every fixed budget bbb, and the total-compensation bound for every budget sequence. Since BtB^tBt is independent of the last ttt arrivals, these imply the paper's statements at the random budget BtB^tBt.

The policy is the rounded rule of Appendix B.3, which always accepts class 111 when the budget is positive. Algorithm 2 read literally would reject class 111 when b<tp1/2b<tp_1/2b<tp1​/2, and the bound ∑j>1\sum_{j>1}∑j>1​, which excludes class 111, is proved for the Appendix B.3 rule. The policy is defined by its explicit thresholds and not through an arbitrary optimal solution of the fluid LP, because with tied rewards that LP has several solutions.

A formalization that replaced the expectation by a Bochner integral of a non-measurable function, or Offline by a fluid relaxation, would make the bound trivial or a different theorem. Both are excluded by construction.

Contributions are welcome at every level: proofs of the milestones, a proof of Eq. (18) from Mathlib's sub-Gaussian machinery, and lemmas computing Offline's value in the multi-secretary problem (the top-bbb rewards among the remaining arrivals), which are reusable beyond this mission.

Selected references

  • A. Vera and S. Banerjee, The Bayesian Prophet: A Low-Regret Framework for Online Decision Making, SSRN 3158062 (Management Science 67(3), 2021). https://doi.org/10.2139/ssrn.3158062
  • A. Arlotto and I. Gurvich, Uniformly bounded regret in the multisecretary problem, Stochastic Systems 9(3), 2019. https://doi.org/10.1287/stsy.2018.0028
  • D. Dubhashi and A. Panconesi, Concentration of Measure for the Analysis of Randomized Algorithms, Cambridge University Press, 2009. https://doi.org/10.1017/CBO9780511581274
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Dynamical SystemsProbabilityStochastic Systems·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
Operations ResearchOptimal TransportOptimization+1·Captain: mikedeng1

Sinkhorn Distributionally Robust Optimization 1: Strong Duality — the Worst-Case Expectation over a Sinkhorn Ball Equals inf over λ ≥ 0 of λρ̄ + λε·E log E_Q[e^{f/(λε)}]Research Paper

Motivation

Distributionally robust optimization (DRO) hedges a decision against uncertainty in the data distribution. It minimizes the worst-case expected loss over an ambiguity set of distributions around a nominal one, typically the empirical distribution of the data. Ambiguity sets built from the Wasserstein (optimal-transport) distance are standard in operations research and machine learning, because they contain distributions with supports different from the nominal one. A known drawback is that the worst case is attained at discrete distributions, which is unrealistic when the true distribution is continuous.

Wang, Gao and Xie (arXiv:2109.11926v5) replace the Wasserstein distance by the Sinkhorn distance, the entropically regularized optimal-transport cost of Cuturi (NeurIPS 2013). Their main theorem is a strong duality result: the infinite-dimensional worst-case problem over a Sinkhorn ball equals a one-dimensional convex minimization. This mission formalizes that theorem.

Timeline:

  • 2013: Cuturi introduces the Sinkhorn distance as a fast surrogate for optimal transport.
  • 2016–2023: strong duality for Wasserstein DRO, by Gao and Kleywegt (arXiv:1604.02199), Blanchet and Murthy (arXiv:1604.01446), and Zhang, Yang and Gao (arXiv:2205.00362).
  • 2021–2025: Wang, Gao and Xie prove strong duality for Sinkhorn DRO for a general measurable sample space, a measurable loss and an arbitrary nominal distribution.

Setting

Let Z\mathcal ZZ be a measurable space. The data are:

  • a nominal probability distribution P^\widehat{\mathbb P}P;
  • a σ-finite reference measure ν≠0\nu\neq0ν=0;
  • a transport cost c:Z×Z→[0,∞]c:\mathcal Z\times\mathcal Z\to[0,\infty]c:Z×Z→[0,∞];
  • a regularization parameter ϵ>0\epsilon>0ϵ>0 and a radius ρ∈R\rho\in\mathbb Rρ∈R;
  • a loss f:Z→R∪{∞}f:\mathcal Z\to\mathbb R\cup\{\infty\}f:Z→R∪{∞}.

For a probability distribution P\mathbb PP, the Sinkhorn distance (Definition 1, with reference measures P^\widehat{\mathbb P}P and ν\nuν) is

Wϵ(P^,P)=inf⁡γ∈Γ(P^,P)E(x,y)∼γ[c(x,y)+ϵlog⁡dγ(x,y)dP^(x) dν(y)],\mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)=\inf_{\gamma\in\Gamma(\widehat{\mathbb P},\mathbb P)}\mathbb E_{(x,y)\sim\gamma}\Big[c(x,y)+\epsilon\log\frac{d\gamma(x,y)}{d\widehat{\mathbb P}(x)\,d\nu(y)}\Big],Wϵ​(P,P)=γ∈Γ(P,P)inf​E(x,y)∼γ​[c(x,y)+ϵlogdP(x)dν(y)dγ(x,y)​],

where Γ(P^,P)\Gamma(\widehat{\mathbb P},\mathbb P)Γ(P,P) is the set of couplings with these marginals. The primal value is the worst-case expected loss over the Sinkhorn ball,

V=sup⁡{EP[f]: Wϵ(P^,P)≤ρ}.V=\sup\big\{\mathbb E_{\mathbb P}[f]:\ \mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)\le\rho\big\}.V=sup{EP​[f]: Wϵ​(P,P)≤ρ}.

The dual problem uses three more objects. The kernel distribution is dQx,ϵ(z)∝e−c(x,z)/ϵ dν(z)d\mathbb Q_{x,\epsilon}(z)\propto e^{-c(x,z)/\epsilon}\,d\nu(z)dQx,ϵ​(z)∝e−c(x,z)/ϵdν(z). The adjusted radius is ρˉ=ρ+ϵ Ex∼P^[log⁡Ez∼νe−c(x,z)/ϵ]\bar\rho=\rho+\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}[\log\mathbb E_{z\sim\nu}e^{-c(x,z)/\epsilon}]ρˉ​=ρ+ϵEx∼P​[logEz∼ν​e−c(x,z)/ϵ]. The dual value is

VD=inf⁡λ≥0{λρˉ+λϵ Ex∼P^[log⁡Ez∼Qx,ϵ[ef(z)/(λϵ)]]},V_D=\inf_{\lambda\ge0}\Big\{\lambda\bar\rho+\lambda\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}\Big[\log\mathbb E_{z\sim\mathbb Q_{x,\epsilon}}\big[e^{f(z)/(\lambda\epsilon)}\big]\Big]\Big\},VD​=λ≥0inf​{λρˉ​+λϵEx∼P​[logEz∼Qx,ϵ​​[ef(z)/(λϵ)]]},

where the objective at λ=0\lambda=0λ=0 is ess sup⁡νf\operatorname{ess\,sup}_\nu fesssupν​f.

Assumption 1 requires:

  • ccc is measurable and, for P^\widehat{\mathbb P}P-a.e. xxx, finite ν\nuν-a.e.;
  • Eνe−c(x,⋅)/ϵ<∞\mathbb E_\nu e^{-c(x,\cdot)/\epsilon}<\inftyEν​e−c(x,⋅)/ϵ<∞ for P^\widehat{\mathbb P}P-a.e. xxx;
  • fff is measurable;
  • every coupling with first marginal P^\widehat{\mathbb P}P disintegrates along P^\widehat{\mathbb P}P.

Condition 1 asks for some λ>0\lambda>0λ>0 with EQx,ϵ[ef/(λϵ)]<∞\mathbb E_{\mathbb Q_{x,\epsilon}}[e^{f/(\lambda\epsilon)}]<\inftyEQx,ϵ​​[ef/(λϵ)]<∞ for P^\widehat{\mathbb P}P-a.e. xxx.

Formalization targets

Goal: Theorem 1 (strong duality)

Under Assumption 1:

(I)  ∃ P: Wϵ(P^,P)≤ρ  ⟺  ρˉ≥0;(II)  ρˉ≥0  ⟹  V=VD.\text{(I) }\ \exists\,\mathbb P:\ \mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)\le\rho\iff\bar\rho\ge0;\qquad \text{(II) }\ \bar\rho\ge0\implies V=V_D.(I)  ∃P: Wϵ​(P,P)≤ρ⟺ρˉ​≥0;(II)  ρˉ​≥0⟹V=VD​.

(III) If ρˉ>0\bar\rho>0ρˉ​>0, then V=VD<∞V=V_D<\inftyV=VD​<∞ when the dual objective is finite at some λ>0\lambda>0λ>0, and V=VD=∞V=V_D=\inftyV=VD​=∞ otherwise.

(IV) If ρˉ>0\bar\rho>0ρˉ​>0 and Condition 1 holds, then 000 is the unique dual minimizer if and only if

ess sup⁡νf<∞andρˉ≥ϵ Ex∼P^[log⁡(1/Qx,ϵ(A))],A={f=ess sup⁡νf}.\operatorname{ess\,sup}_\nu f<\infty\quad\text{and}\quad\bar\rho\ge\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}\big[\log\big(1/\mathbb Q_{x,\epsilon}(A)\big)\big],\qquad A=\{f=\operatorname{ess\,sup}_\nu f\}.esssupν​f<∞andρˉ​≥ϵEx∼P​[log(1/Qx,ϵ​(A))],A={f=esssupν​f}.

Milestones

The milestones are the numbered lemmas of the paper's proof, in the order the proof uses them:

  • Lemma EC.2: the Gibbs variational principle, sup⁡P≪νEP[f−τlog⁡dPdν]=τlog⁡Eνef/τ\sup_{\mathbb P\ll\nu}\mathbb E_{\mathbb P}[f-\tau\log\frac{d\mathbb P}{d\nu}]=\tau\log\mathbb E_\nu e^{f/\tau}supP≪ν​EP​[f−τlogdνdP​]=τlogEν​ef/τ.
  • Lemma EC.3: measurability of the inner value x↦vx(λ)x\mapsto v_x(\lambda)x↦vx​(λ).
  • Lemma 1: weak duality V≤VDV\le V_DV≤VD​.
  • Lemma 2: a KL-constrained reformulation of the primal problem.
  • Lemma EC.4: existence of a dual minimizer.
  • Lemma 3: the first-order condition (9) and uniqueness when λ∗>0\lambda^*>0λ∗>0.
  • Lemma EC.5: the criterion for λ∗=0\lambda^*=0λ∗=0.

Significance

The result. Theorem 1 turns a supremum over an infinite-dimensional set of distributions into a scalar convex program. That program can be solved by first-order methods using only samples from P^\widehat{\mathbb P}P and from the kernels Qx,ϵ\mathbb Q_{x,\epsilon}Qx,ϵ​, which is the basis of the paper's algorithm (Section 4). The proof also constructs the worst-case distribution: it is absolutely continuous with respect to ν\nuν, not discrete. Theorem 1(IV) says exactly when the ambiguity constraint is binding. The finite-support conic reformulation (Corollary 1) and the closed form for linear losses (Example 1) both follow from the theorem.

Formalizing it. The theorem is proved in the paper; no machine-checked proof exists. Formalization adds two things. First, it pins down the extended-valued conventions: VVV, VDV_DVD​ and fff all take values in [−∞,∞][-\infty,\infty][−∞,∞], and the paper does not specify how undefined expectations and the λ=0\lambda=0λ=0 objective are treated. Second, it checks every case of the proof, including the degenerate ones. Doing so has already corrected two statements; see Formalization scope.

Difficulty

Weak duality (Lemma 1) is Lagrangian relaxation plus the Gibbs principle. The difficulty is the reverse inequality V≥VDV\ge V_DV≥VD​. Interchanging the supremum over distributions with the infimum over λ\lambdaλ requires a minimax theorem. The usual minimax theorems need compactness or semicontinuity in the distribution variable. The paper's setting has neither: Z\mathcal ZZ is an arbitrary measurable space, fff is only measurable and may be +∞+\infty+∞, and P^\widehat{\mathbb P}P is arbitrary. So a minimax theorem cannot be applied directly.

The proof instead constructs near-optimal primal distributions from the dual minimizer. This needs three separate cases:

  • λ∗>0\lambda^*>0λ∗>0, with a first-order condition;
  • λ∗=0\lambda^*=0λ∗=0, with a distribution concentrated on the essential maximizers of fff;
  • Condition 1 fails, with a truncation argument.

Each case needs integrability facts about EQx,ϵ[ef/(λϵ)]\mathbb E_{\mathbb Q_{x,\epsilon}}[e^{f/(\lambda\epsilon)}]EQx,ϵ​​[ef/(λϵ)] in which xxx and λ\lambdaλ interact. Disintegrating couplings (Assumption 1(IV)) and making the extended-valued expectations meaningful are a further source of work in Lean.

Formalization scope

All values (primal value, Sinkhorn distance, dual objective) are EReal. Expectations are the published DupacovaWets.Consistency.expect: ∫g+−∫g−\int g^+-\int g^-∫g+−∫g−, with lower Lebesgue integrals in [0,∞][0,\infty][0,∞] and the convention ∞−∞=+∞\infty-\infty=+\infty∞−∞=+∞. The Bochner integral appears only in ρˉ\bar\rhoρˉ​, which every theorem assumes finite.

Further conventions:

  • Sinkhorn distance. The cost and the entropy form a single integrand. A coupling not absolutely continuous with respect to P^⊗ν\widehat{\mathbb P}\otimes\nuP⊗ν contributes +∞+\infty+∞. An infeasible primal has V=−∞V=-\inftyV=−∞.
  • Dual objective. The value at λ=0\lambda=0λ=0 is defined as Mathlib's essSup f ν, not as a limit. Logarithms are ENNReal.log, so log⁡∞=∞\log\infty=\inftylog∞=∞ and log⁡0=−∞\log 0=-\inftylog0=−∞; e+∞=+∞e^{+\infty}=+\inftye+∞=+∞.
  • Kernels. Qx,ϵ\mathbb Q_{x,\epsilon}Qx,ϵ​ is a normalized withDensity measure. Families {γx}x∈supp⁡P^\{\gamma_x\}_{x\in\operatorname{supp}\widehat{\mathbb P}}{γx​}x∈suppP​ are Markov kernels on all of Z\mathcal ZZ.

Hypotheses added to the page:

  • ν\nuν is σ-finite and nonzero;
  • ϵ>0\epsilon>0ϵ>0;
  • x↦log⁡Eνe−c(x,⋅)/ϵx\mapsto\log\mathbb E_\nu e^{-c(x,\cdot)/\epsilon}x↦logEν​e−c(x,⋅)/ϵ is P^\widehat{\mathbb P}P-integrable, so that ρˉ∈R\bar\rho\in\mathbb Rρˉ​∈R.

"ν{0≤c<∞}=1\nu\{0\le c<\infty\}=1ν{0≤c<∞}=1" is read as "ν\nuν-a.e.". "λ∗=0\lambda^*=0λ∗=0" is read as "000 is the unique dual minimizer".

Corrections to the paper:

  • Theorem 1(III). The paper's version with Condition 1 is false: a.e.-finite inner expectations do not make the dual objective finite. A counterexample on N\mathbb NN is in the goal's note. The goal is stated with the integrated condition "the dual objective is finite at some λ>0\lambda>0λ>0".
  • Lemma 3. The lemma is stated under the added hypothesis that the dual objective is finite at some λ1<λ∗\lambda_1<\lambda^*λ1​<λ∗ (and is not −∞-\infty−∞ at λ∗\lambda^*λ∗). Without it, λ∗\lambda^*λ∗ can sit at the edge of the domain where the objective is finite, and (9) fails.

No statement involves an O(⋅)O(\cdot)O(⋅) constant.

A formalization that lets an undefined Sinkhorn integrand evaluate to −∞-\infty−∞ (Mathlib's ⊤+⊥=⊥\top+\bot=\bot⊤+⊥=⊥) is ruled out: it would put every distribution into the ball and make the theorem trivial. The combined integrand and the +∞+\infty+∞ convention exclude this.

A complete development needs:

  • a Gibbs/Donsker–Varadhan variational principle for σ-finite reference measures and extended-valued functions;
  • disintegration of couplings;
  • convexity and differentiation of λ↦λlog⁡Eef/λ\lambda\mapsto\lambda\log\mathbb E e^{f/\lambda}λ↦λlogEef/λ.

The first two are reusable well beyond this mission. Contributions toward any milestone, and toward these general lemmas, are welcome.

Selected references

  • J. Wang, R. Gao, Y. Xie, Sinkhorn Distributionally Robust Optimization, arXiv:2109.11926v5, 2025. https://arxiv.org/abs/2109.11926
  • M. Cuturi, Sinkhorn Distances: Lightspeed Computation of Optimal Transport, NeurIPS, 2013. https://arxiv.org/abs/1306.0895
  • R. Gao, A. Kleywegt, Distributionally Robust Stochastic Optimization with Wasserstein Distance, Mathematics of Operations Research, 2023. https://arxiv.org/abs/1604.02199
  • J. Blanchet, K. Murthy, Quantifying Distributional Model Risk via Optimal Transport, Mathematics of Operations Research, 2019. https://arxiv.org/abs/1604.01446
  • L. Zhang, J. Yang, R. Gao, A Short and General Duality Proof for Wasserstein Distributionally Robust Optimization, Operations Research, 2024. https://arxiv.org/abs/2205.00362
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