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Operations ResearchOptimizationProbability·Captain: mikedeng1

Supply Chain Coordination Under Channel Rebates with Sales Effort Effects IV: A Larger Return Credit Strictly Increases the Retailer's Sales EffortResearch Paper

Returns and the retailer's incentive for sales effort

A manufacturer that sells through a retailer can accept returns: it pays a return credit bbb for every unit the retailer has not sold at the end of the season. Returns policies are common in publishing, software and computer hardware, and since Pasternack (Marketing Science, 1985) they have been studied as a way to make the retailer order more. Retailers also raise demand through sales effort: merchandising, shelf space, point-of-sale advertising. A recurring view in the marketing and operations literature is that returns weaken this incentive. Padmanabhan and Png (1995, p. 70) write that "by reducing the risk of losses due to excess inventory, a returns policy lessens some of the retailer's incentive to invest in such efforts", and Kandel (1996, p. 348) makes the same argument for consignment.

T. A. Taylor, Supply Chain Coordination Under Channel Rebates with Sales Effort Effects (Management Science 48(8), 2002), studies a newsvendor retailer who chooses an order quantity and a sales effort level before demand is observed. Its Proposition 4 shows that in this model the conventional view is reversed: a larger return credit makes the retailer exert strictly more effort. This mission formalizes that proposition and the solution of the retailer's problem it rests on.

Setting

Prices satisfy 0<c<w<p0<c<w<p0<c<w<p and s<cs<cs<c (Assumption A1): ppp is the retail price, www the wholesale price, ccc the manufacturing cost and sss the salvage value, which may be negative. A demand factor ξ≥0\xi\ge 0ξ≥0 has a density φ\varphiφ with φ(ξ)>0\varphi(\xi)>0φ(ξ)>0 for every ξ≥0\xi\ge0ξ≥0 (Assumption A4), distribution function Φ(Q)=∫0Qφ\Phi(Q)=\int_0^Q\varphiΦ(Q)=∫0Q​φ and partial mean Γ(Q)=∫0Qξ dΦ(ξ)\Gamma(Q)=\int_0^Q\xi\,d\Phi(\xi)Γ(Q)=∫0Q​ξdΦ(ξ).

The retailer chooses an effort level e≥0e\ge0e≥0, and demand is eξe\xieξ. Effort costs V(e)V(e)V(e), where VVV is strictly convex and strictly increasing with V(0)=0V(0)=0V(0)=0 (Assumption A5; the paper declares every convexity and monotonicity statement strict). Write Λ(γ)=γV′(γ)−V(γ)\Lambda(\gamma)=\gamma V'(\gamma)-V(\gamma)Λ(γ)=γV′(γ)−V(γ).

Under a returns-only contract (w,b)(w,b)(w,b) with b∈[s,w)b\in[s,w)b∈[s,w), the retailer orders Q≥0Q\ge0Q≥0, exerts effort e≥0e\ge 0e≥0, and earns the expected profit

R‾b(Q,e)=−wQ+p Emin⁡(Q,eξ)+b E(Q−eξ)+−V(e).\underline R_b(Q,e)=-wQ+p\,E\min(Q,e\xi)+b\,E(Q-e\xi)^+-V(e).R​b​(Q,e)=−wQ+pEmin(Q,eξ)+bE(Q−eξ)+−V(e).

This is the integrated channel's profit Π(Q,e)=−cQ+pEmin⁡(Q,eξ)+sE(Q−eξ)+−V(e)\Pi(Q,e)=-cQ+pE\min(Q,e\xi)+sE(Q-e\xi)^+-V(e)Π(Q,e)=−cQ+pEmin(Q,eξ)+sE(Q−eξ)+−V(e) with www in place of ccc and bbb in place of sss. An optimal pair is a maximizer of R‾b\underline R_bR​b​ over Q≥0Q\ge0Q≥0, e≥0e\ge0e≥0. The paper's e‾\underline ee​ is the effort of such a pair, and Q‾0\underline Q_0Q​0​ is the critical fractile Φ(Q‾0)=(p−w)/(p−b)\Phi(\underline Q_0)=(p-w)/(p-b)Φ(Q​0​)=(p−w)/(p−b).

Formalization targets

Goal: Proposition 4 (p. 1004)

If s≤b2<b1<ws\le b_2<b_1<ws≤b2​<b1​<w, (Q1,e1)(Q_1,e_1)(Q1​,e1​) is an optimal pair under the credit b1b_1b1​, (Q2,e2)(Q_2,e_2)(Q2​,e2​) is an optimal pair under b2b_2b2​, and e2>0e_2>0e2​>0, then

e2<e1.e_2<e_1 .e2​<e1​.

The paper writes this as ∂e‾/∂b>0\partial\underline e/\partial b>0∂e​/∂b>0. Its proof shows strict monotonicity, and that is the statement here.

Milestone 1: the order for a given effort (§4.2, p. 1000)

For a fixed e>0e>0e>0, the unique maximizer of Q↦R‾b(Q,e)Q\mapsto\underline R_b(Q,e)Q↦R​b​(Q,e) over Q≥0Q\ge0Q≥0 is Q2=e Q‾0Q_2=e\,\underline Q_0Q2​=eQ​0​, and

max⁡Q≥0R‾b(Q,e)=e (p−b) Γ(Q‾0)−V(e).\max_{Q\ge0}\underline R_b(Q,e)=e\,(p-b)\,\Gamma(\underline Q_0)-V(e).Q≥0max​R​b​(Q,e)=e(p−b)Γ(Q​0​)−V(e).

Milestone 2: the optimal effort (§4.2, p. 1000)

An optimal pair (Q,e‾)(Q,\underline e)(Q,e​) with e‾>0\underline e>0e​>0 satisfies

V′(e‾)=(p−b) Γ(Q‾0),Q=e‾ Q‾0,R‾b(Q,e‾)=Λ(e‾),V'(\underline e)=(p-b)\,\Gamma(\underline Q_0),\qquad Q=\underline e\,\underline Q_0,\qquad \underline R_b(Q,\underline e)=\Lambda(\underline e),V′(e​)=(p−b)Γ(Q​0​),Q=e​Q​0​,R​b​(Q,e​)=Λ(e​),

and conversely every e>0e>0e>0 solving this first-order condition gives the optimal pair (eQ‾0,e)(e\underline Q_0,e)(eQ​0​,e).

Significance

The result. Proposition 4 separates two effects of a return credit. For a fixed order quantity, a larger credit lowers the marginal value of effort: it pays the retailer for unsold units, and effort only matters through sold units. This is the fixed-quantity comparison on which the conventional view rests; Cachon's survey states it for buy-backs as Eq. (19) (on Prove2Me as CachonCoord.EffortNewsvendor.sec_6_4_1_effort_coordination, clause 1). Once the order quantity is chosen together with the effort, the larger credit raises the order, and the effort follows. For the multiplicative demand model the net effect is unambiguous for every demand density and every convex effort cost. A manufacturer that wants more retailer effort can therefore use the return credit as a lever, and a model that ignores the quantity response gets the sign wrong.

Formalizing it. The result is proved in the paper, in a four-line appendix argument that relies on the §4.2 solution of the retailer's problem; neither is machine-checked anywhere. The mission produces a checked newsvendor-with-effort solution (the scaling Q2=eQ‾0Q_2=e\underline Q_0Q2​=eQ​0​ and the profit Λ(e‾)\Lambda(\underline e)Λ(e​)), which the other missions of this series and any multiplicative-effort supply-chain model can reuse, and a checked statement of the comparative statics in the return credit.

Difficulty

The obvious argument differentiates the retailer's first-order condition in bbb with the order held fixed, and it gives the wrong sign; the order quantity must be re-optimized. The correct comparison runs through the reduced problem in the effort alone, and it needs the §4.2 solution in full: the scaling of the optimal order with the effort, which turns Emin⁡(Q,eξ)E\min(Q,e\xi)Emin(Q,eξ) and E(Q−eξ)+E(Q-e\xi)^+E(Q−eξ)+ into newsvendor expectations of ξ\xiξ at Q/eQ/eQ/e; the value of the optimal order as a function of eee; and the first-order characterization of the optimal effort. The comparison across credits then involves two objects: the function Λ\LambdaΛ, and the retailer's reduced profits under the two credits at a common effort level. The statement compares maximizers of two different optimization problems, not roots of an equation, so a formal proof must connect optimality of the pair to the first-order condition, which uses the strict convexity of VVV and the positivity of the density.

Formalization scope

Everything lives in the namespace ChannelRebate.ReturnsEffort. The definitions file holds:

  • Demand: a measurable density φ\varphiφ, zero on (−∞,0)(-\infty,0)(−∞,0), positive on [0,∞)[0,\infty)[0,∞), integrating to 111, with finite mean;
  • the law of ξ\xiξ;
  • Φ\PhiΦ and Γ\GammaΓ as interval integrals;
  • EffortCost: A5 with strict convexity and strict monotonicity on [0,∞)[0,\infty)[0,∞) and V(0)=0V(0)=0V(0)=0;
  • Λ\LambdaΛ;
  • the retailer's profit returnsProfit;
  • optimal orders and optimal pairs as maximizers over Q≥0Q\ge0Q≥0 (and e≥0e\ge0e≥0).

The expectations are the published CachonCoord.Newsvendor.expSales and expLeftover applied to the law of eξe\xieξ (the image of the law of ξ\xiξ under x↦exx\mapsto exx↦ex).

The formalization makes the following commitments, each recorded on its item:

  • Φ−1\Phi^{-1}Φ−1 is never an inverse function: Q‾0\underline Q_0Q​0​ is a positive solution of Φ(Q‾0)=(p−w)/(p−b)\Phi(\underline Q_0)=(p-w)/(p-b)Φ(Q​0​)=(p−w)/(p−b).
  • The paper writes (∂/∂e)V(\partial/\partial e)V(∂/∂e)V without stating that VVV is differentiable. Differentiability on (0,∞)(0,\infty)(0,∞), with derivative V′V'V′, is a hypothesis.
  • The paper restricts attention to strictly positive effort (p. 1000). The goal therefore assumes e2>0e_2>0e2​>0; without it both optimal efforts could be 000 when V′(0+)V'(0^+)V′(0+) is large, and the strict inequality would fail.
  • Existence of optimal pairs is a hypothesis, as on p. 999 ("assume the cost of effort function and demand distribution are chosen such that the existence of an optimal solution is assured").
  • The credit satisfies b<wb<wb<w strictly; at b=wb=wb=w the critical fractile is undefined.

The goal is about optimal pairs of the joint problem. Defining e‾\underline ee​ as the root of the first-order condition, or fixing the order quantity and varying bbb, would give a different and, in the second case, false statement; neither is the target.

Contributions are welcome:

  • a proof of the scaling identity Emin⁡(Q,eξ)=e Emin⁡(Q/e,ξ)E\min(Q,e\xi)=e\,E\min(Q/e,\xi)Emin(Q,eξ)=eEmin(Q/e,ξ);
  • a proof of the newsvendor value identity (p−b)Emin⁡(q,ξ)−(w−b)q=(p−b)Γ(q)(p-b)E\min(q,\xi)-(w-b)q=(p-b)\Gamma(q)(p−b)Emin(q,ξ)−(w−b)q=(p−b)Γ(q) at the critical fractile, reusable for any newsvendor with a density;
  • proofs of the two milestones;
  • the goal theorem.

The two facts the paper's proof uses — that Λ\LambdaΛ is strictly increasing on (0,∞)(0,\infty)(0,∞), and that the retailer's reduced profit at a fixed effort increases with the credit — may be posted as supporting theorems.

Selected references

  • T. A. Taylor, Supply Chain Coordination Under Channel Rebates with Sales Effort Effects, Management Science 48(8):992–1007, 2002. https://doi.org/10.1287/mnsc.48.8.992.168
  • B. A. Pasternack, Optimal Pricing and Return Policies for Perishable Commodities, Marketing Science 4(2):166–176, 1985. https://doi.org/10.1287/mksc.4.2.166
  • V. Padmanabhan, I. P. L. Png, Returns Policies: Make Money by Making Good, Sloan Management Review 37(1):65–72, 1995.
  • E. Kandel, The Right to Return, Journal of Law and Economics 39(1):329–356, 1996. https://doi.org/10.1086/467352
  • G. P. Cachon, Supply Chain Coordination with Contracts, in Handbooks in OR & MS 11, Elsevier, 2003, §6.4.1. https://doi.org/10.1016/S0927-0507(03)11006-7
5 thms1 active userReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

Supply Chain Coordination Under Channel Rebates with Sales Effort Effects II: A Target Rebate and Returns Contract Coordinates Effort and Quantity Under Uniform DemandResearch Paper

Motivation

Manufacturers of computer hardware, software and automobiles routinely pay their retailers channel rebates: a payment per unit the retailer sells to end customers. A target rebate pays only for units sold beyond a target level. These industries also commonly offer returns: a credit for each unsold unit. Both instruments are used to change the retailer's behaviour, and the retailer controls two things that matter to the manufacturer: how much stock she orders, and how much sales effort she exerts to raise demand. Effort cannot be observed or written into a contract, but sales can.

T. A. Taylor's paper (Management Science 48(8), 2002) asks whether a contract built on sales and returns can make an independent retailer choose the effort level and the order quantity that maximize the profit of the whole supply chain, while splitting that profit in any desired proportion. Its Proposition 2 shows that returns alone, linear rebates alone, or target rebates alone cannot do this. Its Theorem 2, the goal of this mission, shows that a target rebate combined with returns can, when demand is uniform and effort cost is quadratic.

Setting

A manufacturer with unit production cost ccc sells to a retailer at wholesale price www; the retailer sells at the fixed retail price ppp, and unsold units have salvage value sss. The standing assumption is 0<c<w<p0<c<w<p0<c<w<p and s<cs<cs<c (sss may be negative). Before demand is seen, the retailer chooses an order quantity Q≥0Q\ge0Q≥0 and an effort level e≥0e\ge0e≥0. Demand is eξe\xieξ, where ξ\xiξ is uniform on [0,1][0,1][0,1], with distribution function Φ\PhiΦ and Γ(x)=∫0xξ dΦ(ξ)\Gamma(x)=\int_0^x\xi\,d\Phi(\xi)Γ(x)=∫0x​ξdΦ(ξ). Effort costs V(e)=ae2/2V(e)=ae^2/2V(e)=ae2/2, a>0a>0a>0.

The integrated channel, which owns both firms, earns

Π(Q,e)=−cQ+pEmin⁡(Q,eξ)+sE(Q−eξ)+−V(e).\Pi(Q,e)=-cQ+pE\min(Q,e\xi)+sE(Q-e\xi)^+-V(e).Π(Q,e)=−cQ+pEmin(Q,eξ)+sE(Q−eξ)+−V(e).

Its optimum uses the critical fractile Qˉ0\bar Q_0Qˉ​0​, defined by Φ(Qˉ0)=(p−c)/(p−s)\Phi(\bar Q_0)=(p-c)/(p-s)Φ(Qˉ​0​)=(p−c)/(p−s), the effort eˉ=(p−s)Γ(Qˉ0)/a\bar e=(p-s)\Gamma(\bar Q_0)/aeˉ=(p−s)Γ(Qˉ​0​)/a and the order Qˉ=eˉQˉ0\bar Q=\bar e\bar Q_0Qˉ​=eˉQˉ​0​. Its optimal profit is Π=Λ(eˉ)\Pi=\Lambda(\bar e)Π=Λ(eˉ), where Λ(γ)=γV′(γ)−V(γ)\Lambda(\gamma)=\gamma V'(\gamma)-V(\gamma)Λ(γ)=γV′(γ)−V(γ).

A target rebate and returns contract (w,u,b,T)(w,u,b,T)(w,u,b,T) pays the retailer u>0u>0u>0 for every unit sold beyond the target TTT, and credits her b∈[s,w)b\in[s,w)b∈[s,w) for every unsold unit. Her profit is

R(Q,e∣T)=−wQ+pEmin⁡(Q,eξ)+uE(min⁡(Q,eξ)−T)++bE(Q−eξ)+−V(e).R(Q,e\mid T)=-wQ+pE\min(Q,e\xi)+uE(\min(Q,e\xi)-T)^+ +bE(Q-e\xi)^+-V(e).R(Q,e∣T)=−wQ+pEmin(Q,eξ)+uE(min(Q,eξ)−T)++bE(Q−eξ)+−V(e).

The manufacturer earns M(Q,e∣T)=(w−c)Q−uE(min⁡(Q,eξ)−T)+−(b−s)E(Q−eξ)+M(Q,e\mid T)=(w-c)Q-uE(\min(Q,e\xi)-T)^+-(b-s)E(Q-e\xi)^+M(Q,e∣T)=(w−c)Q−uE(min(Q,eξ)−T)+−(b−s)E(Q−eξ)+. The other quantities the statements use are:

  • the fractiles Q‾0\underline Q_0Q​0​ and Q‾1\underline Q_1Q​1​, with Φ(Q‾0)=(p−w)/(p−b)\Phi(\underline Q_0)=(p-w)/(p-b)Φ(Q​0​)=(p−w)/(p−b) and Φ(Q‾1)=(p+u−w)/(p+u−b)\Phi(\underline Q_1)=(p+u-w)/(p+u-b)Φ(Q​1​)=(p+u−w)/(p+u−b);
  • the returns-only effort e‾=(p−b)Γ(Q‾0)/a\underline e=(p-b)\Gamma(\underline Q_0)/ae​=(p−b)Γ(Q​0​)/a;
  • a threshold τ∈[Q‾0,Q‾1]\tau\in[\underline Q_0,\underline Q_1]τ∈[Q​0​,Q​1​] that separates the retailer's low and high orders;
  • the retailer's best profit at effort eee, A(e∣T)=max⁡Q≥0R(Q,e∣T)A(e\mid T)=\max_{Q\ge0}R(Q,e\mid T)A(e∣T)=maxQ≥0​R(Q,e∣T).

Contract terms of Theorem 2. Put ζ(T)=4a2(p−s)3T2\zeta(T)=4a^2(p-s)^3T^2ζ(T)=4a2(p−s)3T2 and

u(T)=(w−c)(p−c)5(p−c)5−ζ(T),b(T)=s+(w−c)(p−c)6−(p−s)ζ(T)(p−c)6−(p−c)ζ(T),T3=(p−c)32a(p−s)2.u(T)=(w-c)\frac{(p-c)^5}{(p-c)^5-\zeta(T)},\qquad b(T)=s+(w-c)\frac{(p-c)^6-(p-s)\zeta(T)}{(p-c)^6-(p-c)\zeta(T)},\qquad T_3=\frac{(p-c)^3}{2a(p-s)^2}.u(T)=(w−c)(p−c)5−ζ(T)(p−c)5​,b(T)=s+(w−c)(p−c)6−(p−c)ζ(T)(p−c)6−(p−s)ζ(T)​,T3​=2a(p−s)2(p−c)3​.

T1T_1T1​ and T2T_2T2​ are the fixed points on [0,T3][0,T_3][0,T3​] of T↦e‾τT\mapsto\underline e\tauT↦e​τ and T↦eˉτT\mapsto\bar e\tauT↦eˉτ, with e‾\underline ee​ and τ\tauτ evaluated at u(T)u(T)u(T), b(T)b(T)b(T). L‾(T,w)\underline L(T,w)L​(T,w) and Lˉ(T)\bar L(T)Lˉ(T) are the retailer's profits at effort e‾\underline ee​ and at effort eˉ\bar eeˉ.

Formalization targets

Goal: Theorem 2 (p. 1002)

For every κ∈(0,Π)\kappa\in(0,\Pi)κ∈(0,Π) there is ε0>0\varepsilon_0>0ε0​>0 such that for every ε∈(0,min⁡(κ,ε0))\varepsilon\in(0,\min(\kappa,\varepsilon_0))ε∈(0,min(κ,ε0​)) the following holds. Pairs (w∗,T∗)(w^*,T^*)(w∗,T∗) with

w∗∈(c,p),T∗∈(T1,T2),L‾(T∗,w∗)=κ−ε,Lˉ(T∗)=κw^*\in(c,p),\qquad T^*\in(T_1,T_2),\qquad \underline L(T^*,w^*)=\kappa-\varepsilon,\qquad \bar L(T^*)=\kappaw∗∈(c,p),T∗∈(T1​,T2​),L​(T∗,w∗)=κ−ε,Lˉ(T∗)=κ

exist. Every such pair gives u∗=u(T∗)>0u^*=u(T^*)>0u∗=u(T∗)>0, b∗=b(T∗)∈(s,w∗)b^*=b(T^*)\in(s,w^*)b∗=b(T∗)∈(s,w∗) and T∗>0T^*>0T∗>0. The pair (Qˉ,eˉ)(\bar Q,\bar e)(Qˉ​,eˉ) is the retailer's unique optimum under (w∗,u∗,b∗,T∗)(w^*,u^*,b^*,T^*)(w∗,u∗,b∗,T∗), and

R(Qˉ,eˉ∣T∗)=κ,M(Qˉ,eˉ∣T∗)=Π−κ.R(\bar Q,\bar e\mid T^*)=\kappa,\qquad M(\bar Q,\bar e\mid T^*)=\Pi-\kappa.R(Qˉ​,eˉ∣T∗)=κ,M(Qˉ​,eˉ∣T∗)=Π−κ.

Milestones

  1. §4.1: (Qˉ,eˉ)(\bar Q,\bar e)(Qˉ​,eˉ) is the unique maximizer of Π\PiΠ, with value Λ(eˉ)\Lambda(\bar e)Λ(eˉ).
  2. §4.2: under returns alone, (e‾ Q‾0,e‾)(\underline e\,\underline Q_0,\underline e)(e​Q​0​,e​) is the retailer's unique optimum, with value Λ(e‾)\Lambda(\underline e)Λ(e​).
  3. Lemma 2: at effort eee the retailer orders eQ‾0e\underline Q_0eQ​0​ if e<T/τe<T/\taue<T/τ, eQ‾1e\underline Q_1eQ​1​ if e>T/τe>T/\taue>T/τ, and either if e=T/τe=T/\taue=T/τ.
  4. The two-branch formula for A(e∣T)A(e\mid T)A(e∣T). Its derivative jumps up at T/τT/\tauT/τ, so T/τT/\tauT/τ is never optimal.
  5. Lemma 3: A(⋅∣T)A(\cdot\mid T)A(⋅∣T) is concave on [0,T/τ)[0,T/\tau)[0,T/τ), and either convex then concave, or concave, on (T/τ,∞)(T/\tau,\infty)(T/τ,∞).
  6. Lemma 4: a unique threshold Υ\UpsilonΥ decides whether the optimal effort lies above T/τT/\tauT/τ (at e^\hat ee^) or equals e‾\underline ee​.
  7. Lemma 5: the retailer's optimal (Q,e)(Q,e)(Q,e) in the three cases T<ΥT<\UpsilonT<Υ, T>ΥT>\UpsilonT>Υ, T=ΥT=\UpsilonT=Υ.
  8. Lemma 6: T1T_1T1​ and T2T_2T2​ exist, are unique, and 0<T1<T2<T30<T_1<T_2<T_30<T1​<T2​<T3​.

Significance

The result. Theorem 2 shows that two contractible instruments can align two decisions, one of them not contractible. The rebate pushes effort and quantity up when sales are high, and the return credit raises both when demand is low. Together they reproduce the integrated channel's optimum (Qˉ,eˉ)(\bar Q,\bar e)(Qˉ​,eˉ), and the free parameter κ\kappaκ allocates the profit Π\PiΠ between the firms in any proportion. Proposition 2 of the same paper rules out each instrument alone. This makes Theorem 2 the basis for the paper's recommendation that rebates and returns be used together. The uniform instance is the only one in which the paper proves this; for normal demand it gives only numerical evidence.

Formalizing it. The theorem is proved in the paper; it has not been formalized. The printed proof treats the wholesale price as fixed while it varies: u(T)u(T)u(T) and b(T)b(T)b(T) contain www, so T1T_1T1​, T2T_2T2​ and Lˉ\bar LLˉ move with w∗w^*w∗. A machine-checked proof therefore has to repair the argument, not only transcribe it. A numerical check (p = 10, c = 4, s = 1, a = 1; for example κ = 1.2, ε = 0.012 gives w* ≈ 4.889, T* ≈ 1.095) found the statement itself consistent.

Difficulty

The retailer's problem is not concave. For fixed effort, R(⋅,e∣T)R(\cdot,e\mid T)R(⋅,e∣T) has a kink at Q=TQ=TQ=T, and the optimal order jumps from eQ‾0e\underline Q_0eQ​0​ to eQ‾1e\underline Q_1eQ​1​ at e=T/τe=T/\taue=T/τ. After the order is optimized out, the profit in effort, A(⋅∣T)A(\cdot\mid T)A(⋅∣T), has an upward kink at T/τT/\tauT/τ and can be convex and then concave beyond it. Checking the first-order condition at eˉ\bar eeˉ is therefore not enough. Coordination is a statement about the global maximum of a kinked, non-concave function, and comparing the two local candidates is what the threshold Υ\UpsilonΥ and the profits L‾\underline LL​, Lˉ\bar LLˉ do. The contract is then pinned down by two equations in (w,T)(w,T)(w,T) whose coefficients themselves depend on www through u(T)u(T)u(T) and b(T)b(T)b(T).

Formalization scope

Everything is stated for ξ∼Uniform(0,1)\xi\sim\mathrm{Uniform}(0,1)ξ∼Uniform(0,1), taken as Lebesgue measure on [0,1][0,1][0,1], and for V(e)=ae2/2V(e)=ae^2/2V(e)=ae2/2, as in all of Lemmas 3–6 and Theorem 2. Lemma 2 and the §4.1–4.2 solutions, which the paper states for general demand, are specialised to this instance. The uniform law has bounded support, so the paper's Assumption A4 (positive density on [0,∞)[0,\infty)[0,∞)) is not imposed; the paper allows that relaxation on p. 995.

The expectations use the published expSales and expLeftover (Cachon's newsvendor definitions) of the image law of ξ\xiξ under x↦exx\mapsto exx↦ex. Φ\PhiΦ and Γ\GammaΓ are integrals of the uniform density, not hard-coded closed forms. Every inverse (Qˉ0\bar Q_0Qˉ​0​, Q‾0\underline Q_0Q​0​, Q‾1\underline Q_1Q​1​), the threshold τ\tauτ, the function jjj and its root Υ\UpsilonΥ, the fixed points T1T_1T1​, T2T_2T2​ and the profits L‾\underline LL​, Lˉ\bar LLˉ are stated by their defining equations, never by a choice function. "Optimal" means a maximizer over Q≥0Q\ge0Q≥0, e≥0e\ge0e≥0. Channel coordination means that the retailer's set of maximizers is exactly {(Qˉ,eˉ)}\{(\bar Q,\bar e)\}{(Qˉ​,eˉ)}. The manufacturer's profit MMM, which the paper does not display, is written from the contract's cash flows: units bought back at bbb are salvaged at sss.

A trivializing formalization is ruled out: coordination is global optimality of (Qˉ,eˉ)(\bar Q,\bar e)(Qˉ​,eˉ), not a first-order condition at eˉ\bar eeˉ. ε0\varepsilon_0ε0​ may depend on κ\kappaκ but not on ε\varepsilonε. T1T_1T1​ and T2T_2T2​ are tied to their fixed-point equations and are not free variables.

A complete development needs:

  • the closed forms of Φ\PhiΦ, Γ\GammaΓ and the three expectations under the uniform law;
  • scaling identities in eee;
  • maximization of piecewise concave functions with a kink;
  • one-dimensional intermediate value arguments, with the monotonicity needed to repair the proof of Theorem 2.

The uniform newsvendor identities and the kinked-maximization lemmas are reusable beyond this mission. Contributions to any milestone, and alternative proofs of the existence part of Theorem 2, are welcome.

Selected references

  • T. A. Taylor, Supply Chain Coordination Under Channel Rebates with Sales Effort Effects, Management Science 48(8):992–1007, 2002. https://doi.org/10.1287/mnsc.48.8.992.168
  • G. P. Cachon, Supply Chain Coordination with Contracts, in Handbooks in Operations Research and Management Science, Vol. 11, 2003. https://doi.org/10.1016/S0927-0507(03)11006-7
  • B. A. Pasternack, Optimal Pricing and Return Policies for Perishable Commodities, Marketing Science 4(2):166–176, 1985. https://doi.org/10.1287/mksc.4.2.166
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Control TheoryOperations ResearchProbability+1·Captain: mikedeng1

On Minimizing the Ruin Probability by Investment and Reinsurance I: An Increasing Solution f of the HJB Equation Is Bounded, δ(u) = f(u)/f(∞), and the Feedback Strategy A*, b* Is OptimalResearch Paper

Motivation

An insurance company that collects premiums and pays random claims is ruined when its surplus becomes negative. The probability of ultimate ruin is the classical solvency criterion of risk theory, going back to Lundberg and Cramér. Real insurers have two levers on this probability: they can invest part of the surplus in a risky asset, and they can cede part of every claim to a reinsurer, at a price. The question of how to use both levers dynamically, as a function of the current surplus, so as to make the probability of ruin as small as possible, is a stochastic control problem for a jump-diffusion.

H. Schmidli, On minimizing the ruin probability by investment and reinsurance, Ann. Appl. Probab. 12 (2002), solves this problem for the Cramér–Lundberg model with proportional reinsurance and investment in a Black–Scholes asset. The main results are a verification theorem (Theorem 1, the subject of this mission) and an existence theorem for the associated integral equation (Theorem 2, the companion mission).

Timeline. Hipp and Plum (2000) treated investment in the Cramér–Lundberg model through the Hamilton–Jacobi–Bellman equation, assuming a bounded solution. Schmidli (2001) treated optimal proportional reinsurance alone. The 2002 paper combines investment and reinsurance, and proves the verification theorem without assuming the solution to be bounded.

Setting

Claims arrive at the jumps T1<T2<…T_1<T_2<\dotsT1​<T2​<… of a Poisson process NNN with rate λ>0\lambda>0λ>0; the claim sizes Y1,Y2,…Y_1,Y_2,\dotsY1​,Y2​,… are i.i.d. with continuous distribution function GGG, G(0)=0G(0)=0G(0)=0, independent of NNN. The insurer receives premiums at rate c>0c>0c>0. A risky asset Zt=exp⁡{σWt+(μ−12σ2)t}Z_t=\exp\{\sigma W_t+(\mu-\frac12\sigma^2)t\}Zt​=exp{σWt​+(μ−21​σ2)t}, with μ,σ>0\mu,\sigma>0μ,σ>0 and WWW a standard Brownian motion independent of the claims, is available.

A strategy is a pair of processes (At,bt)(A_t,b_t)(At​,bt​), predictable for the smallest right-continuous filtration generated by the claims and WWW: At∈RA_t\in\mathbb RAt​∈R is the amount invested in the risky asset (locally bounded), and bt∈[0,1]b_t\in[0,1]bt​∈[0,1] is the retention level, meaning the insurer pays btYb_tYbt​Y of a claim YYY occurring at time ttt, at a reinsurance premium rate c(bt)c(b_t)c(bt​). The surplus X=XAbX=X^{Ab}X=XAb starting from u≥0u\ge0u≥0 solves

dXt=(c−c(bt)+μAt) dt+σAt dWt−bt dSt,X0=u,dX_t=\big(c-c(b_t)+\mu A_t\big)\,dt+\sigma A_t\,dW_t-b_t\,dS_t,\qquad X_0=u,dXt​=(c−c(bt​)+μAt​)dt+σAt​dWt​−bt​dSt​,X0​=u,

where St=∑i≤NtYiS_t=\sum_{i\le N_t}Y_iSt​=∑i≤Nt​​Yi​ is the aggregate claims process. The ruin time is τ=inf⁡{t≥0:Xt<0}\tau=\inf\{t\ge0:X_t<0\}τ=inf{t≥0:Xt​<0}, the survival probability is δAb(u)=P[τ=∞]\delta^{Ab}(u)=\mathbb P[\tau=\infty]δAb(u)=P[τ=∞], and the value function is δ(u)=sup⁡A,bδAb(u)\delta(u)=\sup_{A,b}\delta^{Ab}(u)δ(u)=supA,b​δAb(u).

The premium function c(b)c(b)c(b) is decreasing and continuous on [0,1][0,1][0,1], c(1)=0c(1)=0c(1)=0, lim inf⁡b↑1c(b)/(1−b)>0\liminf_{b\uparrow1}c(b)/(1-b)>0liminfb↑1​c(b)/(1−b)>0, and there is b‾>0\underline b>0b​>0 with c(b)>cc(b)>cc(b)>c for b<b‾b<\underline bb<b​ and c(b)≤cc(b)\le cc(b)≤c for b≥b‾b\ge\underline bb≥b​ (full reinsurance is too expensive).

The Hamilton–Jacobi–Bellman equation for δ\deltaδ is, with the convention f(u)=0f(u)=0f(u)=0 for u<0u<0u<0,

sup⁡b∈[0,1]sup⁡A≥0[12σ2A2f′′(u)+(c−c(b)+μA)f′(u)+λ(E[f(u−bY)]−f(u))]=0.(1)\sup_{b\in[0,1]}\sup_{A\ge0}\Big[\tfrac12\sigma^2A^2f''(u)+\big(c-c(b)+\mu A\big)f'(u)+\lambda\big(\mathbb E[f(u-bY)]-f(u)\big)\Big]=0.\tag{1}b∈[0,1]sup​A≥0sup​[21​σ2A2f′′(u)+(c−c(b)+μA)f′(u)+λ(E[f(u−bY)]−f(u))]=0.(1)

For strictly concave fff the maximum over AAA is attained at A∗(u)=−μf′(u)/(σ2f′′(u))A^*(u)=-\mu f'(u)/(\sigma^2f''(u))A∗(u)=−μf′(u)/(σ2f′′(u)) (equation (2)); b∗(u)b^*(u)b∗(u) denotes a measurable maximiser in bbb.

Formalization targets

Goal: Theorem 1 (p. 896)

Let fff be strictly increasing and nonnegative on [0,∞)[0,\infty)[0,∞), continuous there, twice continuously differentiable on (0,∞)(0,\infty)(0,∞), zero on (−∞,0)(-\infty,0)(−∞,0), and a solution of (1) at every u>0u>0u>0. Then fff is bounded, f(∞)=lim⁡x→∞f(x)∈(0,∞)f(\infty)=\lim_{x\to\infty}f(x)\in(0,\infty)f(∞)=limx→∞​f(x)∈(0,∞),

δ(u)=f(u)f(∞)(u≥0),\delta(u)=\frac{f(u)}{f(\infty)}\qquad(u\ge0),δ(u)=f(∞)f(u)​(u≥0),

and every surplus process from u>0u>0u>0 following At=A∗(Xt−)A_t=A^*(X_{t-})At​=A∗(Xt−​), bt=b∗(Xt−)b_t=b^*(X_{t-})bt​=b∗(Xt−​) has survival probability δ(u)\delta(u)δ(u).

Milestones

The proof of Theorem 1 runs through: Lemma 3 (for small surplus the optimal retention is b∗=1b^*=1b∗=1); the identity E[f(Xτ∗∧t∗)]=f(u)\mathbb E[f(X^*_{\tau^*\wedge t})]=f(u)E[f(Xτ∗∧t∗​)]=f(u) along the feedback strategy; the inequality E[f(Xt∧τ)]≤f(u)\mathbb E[f(X_{t\wedge\tau})]\le f(u)E[f(Xt∧τ​)]≤f(u) for every strategy; Lemma 1 (almost surely, either ruin occurs or Xt→∞X_t\to\inftyXt​→∞); the existence of a strategy with P[τ=∞]>0\mathbb P[\tau=\infty]>0P[τ=∞]>0; the comparison δAb(u)≤f(u)/f(∞)\delta^{Ab}(u)\le f(u)/f(\infty)δAb(u)≤f(u)/f(∞) with equality for the feedback strategy; and the absence of ruin by creeping, P[τ∗<∞,Xτ∗∗=0]=0\mathbb P[\tau^*<\infty,X^*_{\tau^*}=0]=0P[τ∗<∞,Xτ∗∗​=0]=0.

Companion statements

The second sentence of Theorem 1 (that f(x)=1+∫0xg(z) dzf(x)=1+\int_0^xg(z)\,dzf(x)=1+∫0x​g(z)dz satisfies the hypotheses whenever ggg is a decreasing solution of the integral equation (5)) and its last sentence (at most one such solution of (1) with f(0)=1f(0)=1f(0)=1) are separate items.

Significance

Theorem 1 reduces a control problem over all predictable strategies to an analytic question: find one increasing smooth solution of (1). Combined with Theorem 2 (existence of a solution of (5)), it shows that the optimal survival probability is f(u)/f(∞)f(u)/f(\infty)f(u)/f(∞) and that the optimal strategy is a Markov feedback rule in the current surplus. It also yields that this solution is bounded, which Hipp and Plum (2000) had to assume, and closes the gap they left open on ruin by creeping (Remark (iii), p. 897). Numerical procedures for the optimal strategy (§5 of the paper) rest on this identification.

The theorem is proved in the paper; nothing in it is formalized. The mission produces a machine-checked verification theorem for a controlled jump-diffusion with an Itô integral against Brownian motion, a Poisson claim stream and a predictable control, together with a formal model of the Cramér–Lundberg process with investment and reinsurance that later results in risk theory can reuse.

Difficulty

The standard verification argument applies Itô's formula to f(Xt)f(X_t)f(Xt​) and uses (1) to show that f(Xt∧τ)f(X_{t\wedge\tau})f(Xt∧τ​) is a supermartingale, and a martingale under the feedback strategy. Here fff is not C2C^2C2 at 000 (f′′(0+)=−∞f''(0+)=-\inftyf′′(0+)=−∞), is discontinuous at 000 after the extension by 000, and is not assumed bounded, so the stochastic integral is only a local martingale and the passage t→∞t\to\inftyt→∞ needs both Lemma 1 and a separate argument that the feedback process does not creep through 000. Lemma 1 itself is only sketched in the paper ("We will just describe the argument"). The optimality part needs a surplus process following the feedback rule; its existence is not proved in the paper.

Formalization scope

The model is formalized on a measurable space with a probability measure: i.i.d. exponential interarrival times (realising the Poisson process), i.i.d. claim sizes with law ν\nuν, and a real Brownian motion (IsBrownianReal), the three families mutually independent. Independence of WWW from the claims is not printed in the paper but is used by (1) and its proof; it is a disclosed standing assumption. The filtration is Ft=⋂s>tσ(Sr,Wr:r≤s)\mathcal F_t=\bigcap_{s>t}\sigma(S_r,W_r:r\le s)Ft​=⋂s>t​σ(Sr​,Wr​:r≤s), not completed. The Itô integral is the published relation EthierKurtz.HasBrownianItoIntegral, and its paths are required to be continuous, so that the pathwise ruin event is well defined. The surplus equation holds for every ttt and every sample point.

Conventions: the premium c(b)c(b)c(b) is real valued (so c(0)<∞c(0)<\inftyc(0)<∞, which the paper allows to fail when E[Y]<∞\mathbb E[Y]<\inftyE[Y]<∞); the supremum in (1) is stated as a least upper bound equal to 000, so an unbounded family never counts as a solution; fff is C2C^2C2 on (0,∞)(0,\infty)(0,∞) and (1) is required for u>0u>0u>0; δ\deltaδ is a supremum over all admissible triples (strategy and surplus process); the controls of the feedback rule at non-positive pre-jump surplus are left free, and optimality is stated for u>0u>0u>0. Expectations of f(Xt∧τ)f(X_{t\wedge\tau})f(Xt∧τ​) are lower Lebesgue integrals of nonnegative functions, so no default value of a non-integrable expectation satisfies an inequality. The optimality clause is stated for every process following the feedback rule; it would be vacuous if no such process existed, and its existence is not part of the target.

Infrastructure needed: Itô's formula for a semimartingale with Brownian and compound-Poisson parts, the compensator of the compound Poisson random measure, localisation, and optional stopping. The model definitions, the HJB predicate and the comparison lemmas are reusable for other ruin-minimisation and dividend problems. Contributions to any milestone, and to general stochastic-calculus lemmas they need, are welcome.

Selected references

  • H. Schmidli, On minimizing the ruin probability by investment and reinsurance, Ann. Appl. Probab. 12(3) (2002), 890–907. https://doi.org/10.1214/aoap/1031863173
  • C. Hipp, M. Plum, Optimal investment for insurers, Insurance Math. Econom. 27 (2000), 215–228. https://doi.org/10.1016/S0167-6687(00)00049-4
  • H. Schmidli, Optimal proportional reinsurance policies in a dynamic setting, Scand. Actuar. J. (2001), 55–68. https://doi.org/10.1080/034612301750077338
  • P. Brémaud, Point Processes and Queues: Martingale Dynamics, Springer (1981). https://doi.org/10.1007/978-1-4684-9477-8
11 thms1 active userReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

Supply Chain Coordination Under Channel Rebates with Sales Effort Effects I: A Target Rebate Coordinates the Newsvendor Channel and Splits Its Profit in Any ProportionResearch Paper

Motivation

Manufacturers in computer hardware, software and automobiles routinely pay channel rebates to their retailers: a payment per unit the retailer sells to end consumers, as opposed to per unit the retailer buys. A target rebate pays only for units sold beyond a target level, a linear rebate pays for every unit sold. T. A. Taylor, Supply Chain Coordination Under Channel Rebates with Sales Effort Effects, Management Science 48(8) (2002), doi:10.1287/mnsc.48.8.992.168, asks whether such payments can make an independent retailer act in the interest of the whole supply chain.

The question belongs to the supply-chain contracting literature built on the newsvendor model. A wholesale price above cost makes the retailer under-order relative to the integrated channel (double marginalization, Spengler 1950). Returns contracts (Pasternack 1985) and revenue sharing (Pasternack 1999; Cachon and Lariviere 2000, as cited by Taylor) are known remedies. Cachon's survey, Supply Chain Coordination with Contracts (Handbooks in OR & MS 11, 2003), discusses sales-rebate contracts through a first-order condition. Taylor's Theorem 1 is the global statement for the target rebate, with an explicit contract and an arbitrary profit split, and without any lump-sum side payment.

This mission covers §3 of the paper, the model without sales effort. Missions II–IV of the series cover §4, where the retailer's effort also affects demand.

Setting

A manufacturer sells to a retailer who places one order of size Q≥0Q \ge 0Q≥0 before observing demand ξ\xiξ. Demand has a density φ\varphiφ with φ(x)=0\varphi(x) = 0φ(x)=0 for x<0x < 0x<0 and φ(x)>0\varphi(x) > 0φ(x)>0 for every x≥0x \ge 0x≥0 (Assumption A4), and a finite mean. Write

Φ(Q)=∫0Qφ(x) dx,Γ(Q)=∫0Qx φ(x) dx.\Phi(Q) = \int_0^Q \varphi(x)\,dx, \qquad \Gamma(Q) = \int_0^Q x\,\varphi(x)\,dx .Φ(Q)=∫0Q​φ(x)dx,Γ(Q)=∫0Q​xφ(x)dx.

The retail price ppp, the production cost ccc and the salvage value sss are fixed with 0<c<p0 < c < p0<c<p and s<cs < cs<c; sss may be negative. A contract specifies a wholesale price www, a rebate u>0u > 0u>0 and a target T≥0T \ge 0T≥0 (Assumption A1: 0<c<w<p0 < c < w < p0<c<w<p, s<cs < cs<c, u>0u > 0u>0, T≥0T \ge 0T≥0). No other transfer is allowed (Assumption A3).

  • The integrated channel earns π(Q)=−cQ+pEmin⁡(Q,ξ)+sE(Q−ξ)+\pi(Q) = -cQ + pE\min(Q,\xi) + sE(Q-\xi)^+π(Q)=−cQ+pEmin(Q,ξ)+sE(Q−ξ)+. Its optimal order Qˉ0\bar Q_0Qˉ​0​ solves Φ(Qˉ0)=(p−c)/(p−s)\Phi(\bar Q_0) = (p-c)/(p-s)Φ(Qˉ​0​)=(p−c)/(p−s), and its optimal profit is π=(p−s)Γ(Qˉ0)\pi = (p-s)\Gamma(\bar Q_0)π=(p−s)Γ(Qˉ​0​).
  • Under the target rebate (w,u,T)(w,u,T)(w,u,T) the retailer earns
r(Q∣T)=−wQ+pEmin⁡(Q,ξ)+sE(Q−ξ)++uE(min⁡(Q,ξ)−T)+,r(Q\mid T) = -wQ + pE\min(Q,\xi) + sE(Q-\xi)^+ + uE(\min(Q,\xi)-T)^+,r(Q∣T)=−wQ+pEmin(Q,ξ)+sE(Q−ξ)++uE(min(Q,ξ)−T)+,

and the manufacturer earns m(Q∣T)=(w−c)Q−uE(min⁡(Q,ξ)−T)+m(Q\mid T) = (w-c)Q - uE(\min(Q,\xi)-T)^+m(Q∣T)=(w−c)Q−uE(min(Q,ξ)−T)+.

  • Under the wholesale price-only contract (u=0u = 0u=0) the retailer orders Q0Q_0Q0​ with Φ(Q0)=(p−w)/(p−s)\Phi(Q_0) = (p-w)/(p-s)Φ(Q0​)=(p−w)/(p−s) and earns r‾=(p−s)Γ(Q0)\underline r = (p-s)\Gamma(Q_0)r​=(p−s)Γ(Q0​).

The contract coordinates the channel when Qˉ0\bar Q_0Qˉ​0​ is the retailer's unique optimal order. Finally u^(w)=(w−c)(p−s)/(c−s)\hat u(w) = (w-c)(p-s)/(c-s)u^(w)=(w−c)(p−s)/(c−s).

Formalization targets

Goal: Theorem 1 (p. 996)

Fix κ∈(0,π)\kappa \in (0,\pi)κ∈(0,π). For every sufficiently small ε∈(0,κ)\varepsilon \in (0,\kappa)ε∈(0,κ) there is exactly one triple (w∗,u∗,T∗)(w^*,u^*,T^*)(w∗,u∗,T∗) with r‾(w∗)=κ−ε\underline r(w^*) = \kappa-\varepsilonr​(w∗)=κ−ε, u∗=u^(w∗)u^* = \hat u(w^*)u∗=u^(w∗), T∗≥0T^* \ge 0T∗≥0 and

(p+u∗−s)Γ(Qˉ0)−u∗(Γ(T∗)+T∗[1−Φ(T∗)])=κ,(1)(p+u^*-s)\Gamma(\bar Q_0) - u^*\big(\Gamma(T^*) + T^*[1-\Phi(T^*)]\big) = \kappa, \qquad (1)(p+u∗−s)Γ(Qˉ​0​)−u∗(Γ(T∗)+T∗[1−Φ(T∗)])=κ,(1)

and this triple has w∗∈(c,p)w^* \in (c,p)w∗∈(c,p), u∗>0u^*>0u∗>0, T∗>0T^*>0T∗>0, coordinates the channel, and gives the retailer r∗=κr^* = \kappar∗=κ and the manufacturer m∗=π−κm^* = \pi-\kappam∗=π−κ.

Milestones

  1. §3.1, p. 995. The newsvendor solutions: Qˉ0\bar Q_0Qˉ​0​ and Q0Q_0Q0​ are the unique optimal orders, with values (p−s)Γ(Qˉ0)(p-s)\Gamma(\bar Q_0)(p−s)Γ(Qˉ​0​) and (p−s)Γ(Q0)(p-s)\Gamma(Q_0)(p−s)Γ(Q0​), and Q0<Qˉ0Q_0 < \bar Q_0Q0​<Qˉ​0​.
  2. §3.2, p. 995. The piecewise form of r(⋅∣T)r(\cdot\mid T)r(⋅∣T), its derivative p−w−(p−s)Φ(Q)p-w-(p-s)\Phi(Q)p−w−(p−s)Φ(Q) below TTT and p+u−w−(p+u−s)Φ(Q)p+u-w-(p+u-s)\Phi(Q)p+u−w−(p+u−s)Φ(Q) above, strict concavity on [0,T)[0,T)[0,T) and (T,∞)(T,\infty)(T,∞), and an upward kink of the derivative at TTT.
  3. Lemma 1, p. 995. With Φ(Q1)=(p+u−w)/(p+u−s)\Phi(Q_1) = (p+u-w)/(p+u-s)Φ(Q1​)=(p+u−w)/(p+u−s), the equation r(Q0∣τ0)=r(Q1∣τ0)r(Q_0\mid\tau_0) = r(Q_1\mid\tau_0)r(Q0​∣τ0​)=r(Q1​∣τ0​) has exactly one root τ0∈[Q0,Q1]\tau_0 \in [Q_0,Q_1]τ0​∈[Q0​,Q1​], lying in (Q0,Q1)(Q_0,Q_1)(Q0​,Q1​); the retailer's optimal order set is {Q1}\{Q_1\}{Q1​} for T<τ0T<\tau_0T<τ0​, {Q0}\{Q_0\}{Q0​} for T>τ0T>\tau_0T>τ0​, and {Q0,Q1}\{Q_0,Q_1\}{Q0​,Q1​} for T=τ0T=\tau_0T=τ0​.
  4. §3.2, p. 996. The retailer's optimal profit is (p+u−s)Γ(Q1)−u(Γ(T)+T[1−Φ(T)])(p+u-s)\Gamma(Q_1) - u(\Gamma(T)+T[1-\Phi(T)])(p+u−s)Γ(Q1​)−u(Γ(T)+T[1−Φ(T)]) if T<τ0T<\tau_0T<τ0​ and (p−s)Γ(Q0)(p-s)\Gamma(Q_0)(p−s)Γ(Q0​) if T≥τ0T \ge \tau_0T≥τ0​.
  5. Proposition 1, p. 996. If T=0T = 0T=0, channel coordination requires m∗<0m^* < 0m∗<0.

Significance

Theorem 1 shows that a single sales-based instrument, a target rebate, achieves what a wholesale price alone cannot: the retailer orders the channel-optimal quantity, and the channel profit π\piπ is split in any proportion κ:π−κ\kappa : \pi-\kappaκ:π−κ. The parameter κ\kappaκ can be set to the retailer's opportunity cost, so a manufacturer with all the bargaining power extracts the rest of the channel profit without a side payment. Proposition 1 explains why the target is needed: a linear rebate that coordinates the channel leaves the manufacturer with a loss. The quantity-only analysis is also the base case of §4, where the paper shows that a target rebate combined with returns coordinates effort and quantity as well.

The results are proved in the paper (Appendix, p. 1005). No machine-checked proof of any of them is known to exist. The mission produces a Lean statement of the model and of each result, and invites formal proofs of the newsvendor solution, the shape of the kinked profit, the threshold lemma and the coordination theorem.

Difficulty

The retailer's profit r(⋅∣T)r(\cdot\mid T)r(⋅∣T) is not concave: its derivative jumps up at the target. The usual newsvendor argument, a stationary point of a concave function is a global maximum, therefore fails. A first-order condition at Qˉ0\bar Q_0Qˉ​0​ shows only that Qˉ0\bar Q_0Qˉ​0​ is a local candidate on (T,∞)(T,\infty)(T,∞). The retailer may still prefer the smaller candidate Q0Q_0Q0​ on [0,T][0,T][0,T], and coordination fails exactly when she does. Theorem 1(b) requires comparing the two branches globally, through the threshold τ0\tau_0τ0​ of Lemma 1, and then showing that the contract's target lies strictly below τ0\tau_0τ0​.

The contract itself is defined implicitly. w∗w^*w∗ solves an equation involving the critical fractile Q0(w)Q_0(w)Q0​(w), and T∗T^*T∗ solves (1). Existence and uniqueness of both, and the placement of T∗T^*T∗ relative to τ0\tau_0τ0​, are part of the claim.

Formalization scope

All definitions are in ChannelRebate.Quantity.Setting. Demand is a structure Demand carrying the density φ\varphiφ with the properties listed under Setting; its law is Lebesgue measure with density φ\varphiφ. Emin⁡(Q,ξ)E\min(Q,\xi)Emin(Q,ξ) and E(Q−ξ)+E(Q-\xi)^+E(Q−ξ)+ are expSales and expLeftover of the published definition CachonCoord_Newsvendor_Contracts, applied to this law. E(min⁡(Q,ξ)−T)+E(\min(Q,\xi)-T)^+E(min(Q,ξ)−T)+ is the local rebateUnits. Φ\PhiΦ and Γ\GammaΓ are interval integrals from 000.

Conventions:

  • Φ−1\Phi^{-1}Φ−1 is never a function. Each critical fractile (Qˉ0\bar Q_0Qˉ​0​, Q0Q_0Q0​, Q1Q_1Q1​) is a hypothesis giving its defining equation, and τ0\tau_0τ0​ is any solution of f0(τ0)=0f_0(\tau_0) = 0f0​(τ0​)=0 in [Q0,Q1][Q_0,Q_1][Q0​,Q1​].
  • An optimal order maximizes over Q≥0Q \ge 0Q≥0. "Coordination" and the order sets of Lemma 1 are equalities of the set of maximizers, so a tie with Q0Q_0Q0​ does not count as coordination.
  • "For ε\varepsilonε sufficiently small" is "there exists ε0>0\varepsilon_0 > 0ε0​>0 such that for all ε∈(0,min⁡(ε0,κ))\varepsilon \in (0,\min(\varepsilon_0,\kappa))ε∈(0,min(ε0​,κ))".
  • In Theorem 1 the uniqueness ranges over all real triples satisfying the specification, with www unrestricted; w∗∈(c,p)w^* \in (c,p)w∗∈(c,p) is a conclusion.
  • The manufacturer's profit is its own formula, never channel profit minus retailer profit; m∗=π−κm^* = \pi-\kappam∗=π−κ is a conclusion.
  • The standing assumptions A1, A3 and A4 appear as hypotheses or in Demand; no continuity of φ\varphiφ is assumed.

A formalization that reads coordination as the first-order condition at Qˉ0\bar Q_0Qˉ​0​, or that defines T∗T^*T∗ or w∗w^*w∗ by a choice function, would make Theorem 1 vacuous or weaker, and is ruled out by the statements above.

A complete development needs the newsvendor calculus for a density (derivatives of Emin⁡(Q,ξ)E\min(Q,\xi)Emin(Q,ξ) and E(Q−ξ)+E(Q-\xi)^+E(Q−ξ)+ in QQQ, strict monotonicity of Φ\PhiΦ on [0,∞)[0,\infty)[0,∞)), the intermediate value theorem for the two implicit equations, and the global comparison of the two concave branches. The newsvendor calculus is reusable for missions II–IV of this series and for other newsvendor contracts. Proofs of the milestones in any order are welcome.

Selected references

  • T. A. Taylor, Supply Chain Coordination Under Channel Rebates with Sales Effort Effects, Management Science 48(8):992–1007, 2002. doi:10.1287/mnsc.48.8.992.168
  • G. P. Cachon, Supply Chain Coordination with Contracts, in Handbooks in Operations Research and Management Science 11, 2003. doi:10.1016/S0927-0507(03)11006-7
  • B. A. Pasternack, Optimal Pricing and Return Policies for Perishable Commodities, Marketing Science 4(2):166–176, 1985. doi:10.1287/mksc.4.2.166
  • J. J. Spengler, Vertical Integration and Antitrust Policy, Journal of Political Economy 58(4):347–352, 1950. doi:10.1086/256964
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Quantitative Stability in Stochastic Programming: The Method of Probability Metrics 3: Mixed-Integer Two-Stage Programs Are Hölder Stable in the Polyhedral DiscrepancyResearch Paper

Motivation

Two-stage stochastic programs are solved with an approximation of the true distribution of the random data: an empirical measure, a scenario tree, or a discretization. Whether the computed decisions mean anything depends on how the optimal value and the solution set react when the underlying probability measure is replaced by a nearby one, and on which distance between measures "nearby" refers to. Rachev and Römisch (preprint, edoc.hu-berlin.de; published in Math. Oper. Res. 27 (2002) 792–818, doi:10.1287/moor.27.4.792.304) organize this question in two steps. First, a minimal information distance dFUd_{\mathcal F_{\mathcal U}}dFU​​, built from the integrands of the problem itself, controls optimal values and solution sets (their Theorems 2.2 and 2.3). Second, for a given class of models, dFUd_{\mathcal F_{\mathcal U}}dFU​​ is bounded by a canonical probability metric that depends only on the analytical properties of the integrands.

For linear two-stage programs the integrands are locally Lipschitz in the random parameter and the canonical metric is a Fortet–Mourier metric. When the second stage has integer variables, the recourse function is discontinuous, and metrics of Fortet–Mourier type no longer control the problem. This mission formalizes the paper's answer for that case (§3.2): mixed-integer two-stage programs are Hölder stable with respect to a polyhedral discrepancy d1,phkd_{1,phk}d1,phk​ built from Lipschitz functions restricted to polyhedra. The structure of mixed-integer value functions that makes this possible goes back to Blair and Jeroslow (1977), Bank et al. (1982) and Schultz (1996), all cited in the paper.

Setting

Let c∈Rmc\in\mathbb R^mc∈Rm, let X⊆RmX\subseteq\mathbb R^mX⊆Rm be closed and Ξ⊆Rs\Xi\subseteq\mathbb R^sΞ⊆Rs a polyhedron, i.e. an intersection of finitely many closed half-spaces. The second stage has costs q∈Rm^q\in\mathbb R^{\hat m}q∈Rm^, qˉ∈Rmˉ\bar q\in\mathbb R^{\bar m}qˉ​∈Rmˉ and (r,m^)(r,\hat m)(r,m^)- and (r,mˉ)(r,\bar m)(r,mˉ)-matrices WWW, Wˉ\bar WWˉ. Its value function is

Φ(t)=min⁡{qy+qˉyˉ: Wy+Wˉyˉ=t, y∈Z+m^, yˉ∈R+mˉ}(t∈Rr),\Phi(t)=\min\{qy+\bar q\bar y:\ Wy+\bar W\bar y=t,\ y\in\mathbb Z^{\hat m}_+,\ \bar y\in\mathbb R^{\bar m}_+\}\qquad(t\in\mathbb R^r),Φ(t)=min{qy+qˉ​yˉ​: Wy+Wˉyˉ​=t, y∈Z+m^​, yˉ​∈R+mˉ​}(t∈Rr),

and T\mathcal TT is the set of right-hand sides ttt for which the constraint set is nonempty. The right-hand side h(ξ)∈Rrh(\xi)\in\mathbb R^rh(ξ)∈Rr and the technology matrix T(ξ)T(\xi)T(ξ) depend affinely on ξ∈Rs\xi\in\mathbb R^sξ∈Rs. For a Borel probability measure μ\muμ on Ξ\XiΞ the program is

min⁡{∫Ξf0(ξ,x) μ(dξ): x∈X},f0(ξ,x)=cx+Φ(h(ξ)−T(ξ)x).(9)\min\Big\{\int_\Xi f_0(\xi,x)\,\mu(d\xi):\ x\in X\Big\},\qquad f_0(\xi,x)=cx+\Phi(h(\xi)-T(\xi)x). \tag{9}min{∫Ξ​f0​(ξ,x)μ(dξ): x∈X},f0​(ξ,x)=cx+Φ(h(ξ)−T(ξ)x).(9)

Three conditions make (9) well defined: (B1) WWW and Wˉ\bar WWˉ have rational entries; (B2) h(ξ)−T(ξ)x∈Th(\xi)-T(\xi)x\in\mathcal Th(ξ)−T(ξ)x∈T for all (ξ,x)∈Ξ×X(\xi,x)\in\Xi\times X(ξ,x)∈Ξ×X (relatively complete recourse); (B3) there is uuu with W′u≤qW'u\le qW′u≤q and Wˉ′u≤qˉ\bar W'u\le\bar qWˉ′u≤qˉ​ (dual feasibility).

v(ν)v(\nu)v(ν) and S(ν)S(\nu)S(ν) denote the optimal value and solution set of (9) under ν\nuν; for an open bounded U⊆Rm\mathcal U\subseteq\mathbb R^mU⊆Rm, vU(ν)v_{\mathcal U}(\nu)vU​(ν) and SU(ν)S_{\mathcal U}(\nu)SU​(ν) are the same objects with XXX replaced by X∩cl⁡UX\cap\operatorname{cl}\mathcal UX∩clU. SU(ν)S_{\mathcal U}(\nu)SU​(ν) is a complete local minimizing (CLM) set if it is nonempty and contained in U\mathcal UU. The minimal information distance is dFU(μ,ν)=sup⁡x∈X∩cl⁡U∣∫Ξf0(ξ,x)(μ−ν)(dξ)∣d_{\mathcal F_{\mathcal U}}(\mu,\nu)=\sup_{x\in X\cap\operatorname{cl}\mathcal U}|\int_\Xi f_0(\xi,x)(\mu-\nu)(d\xi)|dFU​​(μ,ν)=supx∈X∩clU​∣∫Ξ​f0​(ξ,x)(μ−ν)(dξ)∣. The moment classes are Pp,K(Ξ)={ν:∫Ξ∥ξ∥pν(dξ)≤K}\mathcal P_{p,K}(\Xi)=\{\nu:\int_\Xi\|\xi\|^p\nu(d\xi)\le K\}Pp,K​(Ξ)={ν:∫Ξ​∥ξ∥pν(dξ)≤K}, and the polyhedral metric is

d1,phk(μ,ν)=sup⁡{∣∫Pf(ξ)(μ−ν)(dξ)∣: P a polyhedron with at most k faces, f 1-Lipschitz on P, ∣f(ξ)∣≤max⁡{1,∥ξ∥}}.d_{1,phk}(\mu,\nu)=\sup\Big\{\Big|\int_P f(\xi)(\mu-\nu)(d\xi)\Big|:\ P \text{ a polyhedron with at most } k \text{ faces},\ f \text{ 1-Lipschitz on } P,\ |f(\xi)|\le\max\{1,\|\xi\|\}\Big\}.d1,phk​(μ,ν)=sup{​∫P​f(ξ)(μ−ν)(dξ)​: P a polyhedron with at most k faces, f 1-Lipschitz on P, ∣f(ξ)∣≤max{1,∥ξ∥}}.

Finally, ψ(τ)=inf⁡{∫Ξf0(ξ,x)μ(dξ)−v(μ):d(x,S(μ))≥τ, x∈X∩cl⁡U}\psi(\tau)=\inf\{\int_\Xi f_0(\xi,x)\mu(d\xi)-v(\mu): d(x,S(\mu))\ge\tau,\ x\in X\cap\operatorname{cl}\mathcal U\}ψ(τ)=inf{∫Ξ​f0​(ξ,x)μ(dξ)−v(μ):d(x,S(μ))≥τ, x∈X∩clU} is the growth function at μ\muμ, ψ−1(t)=sup⁡{τ≥0:ψ(τ)≤t}\psi^{-1}(t)=\sup\{\tau\ge0:\psi(\tau)\le t\}ψ−1(t)=sup{τ≥0:ψ(τ)≤t}, and Ψ(η)=η+ψ−1(2η)\Psi(\eta)=\eta+\psi^{-1}(2\eta)Ψ(η)=η+ψ−1(2η).

Formalization targets

Goal: Theorem 3.6

Under (B1)–(B3), with μ∈Pp,K(Ξ)\mu\in\mathcal P_{p,K}(\Xi)μ∈Pp,K​(Ξ) for some p>1p>1p>1, K>0K>0K>0, S(μ)≠∅S(\mu)\ne\emptysetS(μ)=∅ and U\mathcal UU an open bounded neighbourhood of S(μ)S(\mu)S(μ), there are L>0L>0L>0, δ>0\delta>0δ>0 and k∈Nk\in\mathbb Nk∈N such that for all ν∈Pp,K(Ξ)\nu\in\mathcal P_{p,K}(\Xi)ν∈Pp,K​(Ξ) with d1,phk(μ,ν)<δd_{1,phk}(\mu,\nu)<\deltad1,phk​(μ,ν)<δ

∣v(μ)−vU(ν)∣≤L d1,phk(μ,ν)11+rp−1,∅≠SU(ν)⊆S(μ)+Ψ(L d1,phk(μ,ν)11+rp−1)B,|v(\mu)-v_{\mathcal U}(\nu)|\le L\,d_{1,phk}(\mu,\nu)^{\frac{1}{1+\frac{r}{p-1}}},\qquad \emptyset\ne S_{\mathcal U}(\nu)\subseteq S(\mu)+\Psi\Big(L\,d_{1,phk}(\mu,\nu)^{\frac{1}{1+\frac{r}{p-1}}}\Big)\mathbb B,∣v(μ)−vU​(ν)∣≤Ld1,phk​(μ,ν)1+p−1r​1​,∅=SU​(ν)⊆S(μ)+Ψ(Ld1,phk​(μ,ν)1+p−1r​1​)B,

and SU(ν)S_{\mathcal U}(\nu)SU​(ν) is a CLM set. The constants and the number of faces are existential; only the exponent is fixed.

Milestones

  1. Lemma 3.5 (i)–(ii): a countable, locally finite Borel partition of T\mathcal TT into translates of pos⁡Wˉ\operatorname{pos}\bar WposWˉ minus finitely many translates, on each piece of which Φ\PhiΦ is Lipschitz with a common constant.
  2. Lemma 3.5, last assertion: Φ\PhiΦ is finite and lower semicontinuous on T\mathcal TT, and ∣Φ(t)−Φ(t~)∣≤α∥t−t~∥+β|\Phi(t)-\Phi(\tilde t)|\le\alpha\|t-\tilde t\|+\beta∣Φ(t)−Φ(t~)∣≤α∥t−t~∥+β.
  3. Growth bound (proof of Theorem 3.6): ∣f0(ξ,x)∣≤∥c∥∥x∥+α(∥h(ξ)∥+∥T(ξ)∥∥x∥)+β|f_0(\xi,x)|\le\|c\|\|x\|+\alpha(\|h(\xi)\|+\|T(\xi)\|\|x\|)+\beta∣f0​(ξ,x)∣≤∥c∥∥x∥+α(∥h(ξ)∥+∥T(ξ)∥∥x∥)+β, hence every measure with finite first moment lies in the domain of dFUd_{\mathcal F_{\mathcal U}}dFU​​.
  4. Theorem 2.2 for d=0d=0d=0: ∣v(μ)−vU(ν)∣≤dFU(μ,ν)|v(\mu)-v_{\mathcal U}(\nu)|\le d_{\mathcal F_{\mathcal U}}(\mu,\nu)∣v(μ)−vU​(ν)∣≤dFU​​(μ,ν) for all admissible ν\nuν, Berge upper semicontinuity of SUS_{\mathcal U}SU​, CLM sets near μ\muμ.
  5. Theorem 2.3 for d=0d=0d=0: ∅≠SU(ν)⊆S(μ)+Ψ(L^dFU(μ,ν))B\emptyset\ne S_{\mathcal U}(\nu)\subseteq S(\mu)+\Psi(\hat L d_{\mathcal F_{\mathcal U}}(\mu,\nu))\mathbb B∅=SU​(ν)⊆S(μ)+Ψ(L^dFU​​(μ,ν))B with Ψ(η)=η+ψ−1(η)\Psi(\eta)=\eta+\psi^{-1}(\eta)Ψ(η)=η+ψ−1(η).
  6. Estimate (12): dFU(μ,ν)≤C d1,phk(μ,ν)1/(1+r/(p−1))d_{\mathcal F_{\mathcal U}}(\mu,\nu)\le C\,d_{1,phk}(\mu,\nu)^{1/(1+r/(p-1))}dFU​​(μ,ν)≤Cd1,phk​(μ,ν)1/(1+r/(p−1)) for small d1,phk(μ,ν)d_{1,phk}(\mu,\nu)d1,phk​(μ,ν).

Companion: Corollary 3.7

For bounded Ξ\XiΞ and every μ∈P(Ξ)\mu\in\mathcal P(\Xi)μ∈P(Ξ) the same conclusions hold with the Lipschitz rate L αphk(μ,ν)L\,\alpha_{phk}(\mu,\nu)Lαphk​(μ,ν), where αphk(μ,ν)=sup⁡{∣μ(P)−ν(P)∣}\alpha_{phk}(\mu,\nu)=\sup\{|\mu(P)-\nu(P)|\}αphk​(μ,ν)=sup{∣μ(P)−ν(P)∣} over polyhedra with at most kkk faces.

Significance

Theorem 3.6 says that, for mixed-integer recourse, closeness of the distributions in d1,phkd_{1,phk}d1,phk​ is enough for closeness of optimal values and of localized solution sets, with an explicit Hölder exponent (p−1)/(p−1+r)(p-1)/(p-1+r)(p−1)/(p−1+r) that degrades with the second-stage dimension rrr and improves with the number of moments. Two consequences follow. Scenario reduction and discretization methods for mixed-integer models can be judged by a polyhedral discrepancy; and, through the entropy estimates of §4 of the paper, empirical approximations converge at rates governed by uniform laws for polyhedra. Corollary 3.7 shows that for bounded supports the rate becomes Lipschitz in the polyhedral discrepancy.

The results are proved in the paper, partly by reference: Lemma 3.5 is quoted from Bank et al., Schultz, and Blair–Jeroslow, and the partition argument behind (12) refers to Schultz (1996). None of it has a machine-checked proof. Formalizing the mission produces the first formal treatment of mixed-integer value functions with rational data, a formal version of the minimal-information-distance stability theorems in the objective-only case, and the polyhedral metric itself.

Difficulty

The obvious route to a stability estimate, a Lipschitz bound on ξ↦f0(ξ,x)\xi\mapsto f_0(\xi,x)ξ↦f0​(ξ,x) followed by a Fortet–Mourier or Wasserstein bound, fails at the first step: Φ\PhiΦ jumps across the boundaries of the pieces Bi\mathcal B_iBi​, so f0(⋅,x)f_0(\cdot,x)f0​(⋅,x) is only piecewise Lipschitz, with pieces that move with xxx. Any metric that controls dFUd_{\mathcal F_{\mathcal U}}dFU​​ must therefore see the indicator functions of these pieces, which is why polyhedra enter. The second obstacle is that there are countably many unbounded pieces: a single polyhedral bound covers only a bounded region of T\mathcal TT, and the tail outside it must be paid for with moments, which is the origin of the exponent. Lemma 3.5 itself, in particular the uniform Lipschitz constant and the local finiteness of the partition, rests on rationality of WWW and Wˉ\bar WWˉ; without (B1) the value function need not be lower semicontinuous.

Formalization scope

Rm\mathbb R^mRm, Rs\mathbb R^sRs, Rr\mathbb R^rRr are Euclidean spaces (the paper never fixes its norm, and every constant in the statements is existential). Measures are Borel probability measures on Rs\mathbb R^sRs with ν(Rs∖Ξ)=0\nu(\mathbb R^s\setminus\Xi)=0ν(Rs∖Ξ)=0. The integral of the extended-real integrand f0f_0f0​ is the published DupacovaWets.Consistency.expect (+∞+\infty+∞ when ∫f0+=∞\int f_0^+=\infty∫f0+​=∞). Φ\PhiΦ, optimal values and ψ\psiψ are extended-real infima, +∞+\infty+∞ on empty sets; the paper's "min" is read as an infimum. Distances and Ψ\PsiΨ take values in [0,∞][0,\infty][0,∞], and every estimate between optimal values states explicitly that both are finite, so that no convention for ∞−∞\infty-\infty∞−∞ can make a bound vacuous. T(ξ)T(\xi)T(ξ) is a linear map Rm→Rr\mathbb R^m\to\mathbb R^rRm→Rr and ∥T(ξ)∥\|T(\xi)\|∥T(ξ)∥ its operator norm. Integer vectors are tuples of natural numbers; WWW, Wˉ\bar WWˉ are real matrices with rational entries.

Disclosed reading: a "polyhedron with at most kkk faces" is an intersection of kkk closed half-spaces. Because kkk is existential in Theorem 3.6 and Corollary 3.7, the theorems are equivalent under this reading and under a facet count. The clause "piecewise polyhedral" of Lemma 3.5 is not defined in the paper and is not formalized. The page states "PFU(Ξ)⊆P1(Ξ)\mathcal P_{\mathcal F_{\mathcal U}}(\Xi)\subseteq\mathcal P_1(\Xi)PFU​​(Ξ)⊆P1​(Ξ)"; the argument proves and uses P1(Ξ)⊆PFU(Ξ)\mathcal P_1(\Xi)\subseteq\mathcal P_{\mathcal F_{\mathcal U}}(\Xi)P1​(Ξ)⊆PFU​​(Ξ), and that direction is the one formalized. Theorems 2.2 and 2.3 are stated in their objective-only (d=0d=0d=0) form for a general normal integrand.

The integrals in d1,phkd_{1,phk}d1,phk​ are Bochner integrals over PPP, which are meaningful because measures in Pp,K(Ξ)\mathcal P_{p,K}(\Xi)Pp,K​(Ξ) with p>1p>1p>1 integrate max⁡{1,∥ξ∥}\max\{1,\|\xi\|\}max{1,∥ξ∥}. A formalization that took the supremum over all of Rs\mathbb R^sRs instead of PPP, quantified ν\nuν over all of P(Ξ)\mathcal P(\Xi)P(Ξ), or let a non-integrable function contribute 000 would not state the paper's theorem, and these readings are excluded.

Needed infrastructure: the structure theory of mixed-integer value functions with rational data (the partition of Lemma 3.5 and the attainment of the minimum in (10)), lower semicontinuity of integral functionals of normal integrands via Fatou's lemma, Berge's upper semicontinuity of parametric argmin maps, and approximation of polyhedral pieces by polyhedra. The value-function results and the general d=0d=0d=0 stability theorems are reusable beyond this mission. Proofs of any milestone, and alternative arguments for Lemma 3.5, are welcome.

Selected references

  • S. T. Rachev, W. Römisch, Quantitative stability in stochastic programming: The method of probability metrics, Math. Oper. Res. 27(4) (2002) 792–818. doi:10.1287/moor.27.4.792.304. Preprint used here: edoc.hu-berlin.de.
  • B. Bank, J. Guddat, D. Klatte, B. Kummer, K. Tammer, Non-Linear Parametric Optimization, Akademie-Verlag, Berlin, 1982. doi:10.1007/978-3-0348-6328-5
  • R. Schultz, Rates of convergence in stochastic programs with complete integer recourse, SIAM J. Optim. 6 (1996) 1138–1152. doi:10.1137/S1052623494271655
  • C. E. Blair, R. G. Jeroslow, The value function of a mixed integer program: I, Discrete Math. 19 (1977) 121–138. doi:10.1016/0012-365X(77)90028-0
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. doi:10.1007/978-3-642-02431-3
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 1: Infinite Source Poisson Input Under Slow Growth Converges (fidi) to Totally Skewed α-Stable Lévy MotionResearch Paper

Motivation

Measurements of Ethernet and Internet traffic in the 1990s showed that the amount of data offered to a link is bursty on every time scale and that the lengths of transmissions (file sizes, connection durations) have heavy, regularly varying tails. Two families of approximations for the cumulative input were proposed: fractional Brownian motion, which has dependent Gaussian increments, and α-stable Lévy motion, which has independent, heavy-tailed increments. The two lead to very different predictions for buffer overflow and link dimensioning.

T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman (Ann. Appl. Probab. 12 (2002) 23–68) showed that both answers are correct in different regimes, and that the regime is decided by how fast the connection rate grows relative to the time scale. This mission formalizes their result for the infinite source Poisson model under slow growth, where the limit is a totally skewed α-stable Lévy motion. Companion missions treat the ON/OFF model and the fast-growth regime with its fractional Brownian limit.

Setting

A transmission length has law FonF_{\mathrm{on}}Fon​ on [0,∞)[0,\infty)[0,∞) with tail Fˉon(x)=Fon((x,∞))\bar F_{\mathrm{on}}(x)=F_{\mathrm{on}}((x,\infty))Fˉon​(x)=Fon​((x,∞)). Condition (2.8) asks

Fˉon(x)=x−αL(x),x>0,1<α<2,\bar F_{\mathrm{on}}(x)=x^{-\alpha}L(x),\qquad x>0,\quad 1<\alpha<2,Fˉon​(x)=x−αL(x),x>0,1<α<2,

with LLL slowly varying (L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0). The mean μon\mu_{\mathrm{on}}μon​ is finite and the variance infinite. The quantile function (2.9) is b(t)=(1/Fˉon)←(t)=inf⁡{x:1/Fˉon(x)≥t}b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)=\inf\{x:1/\bar F_{\mathrm{on}}(x)\ge t\}b(t)=(1/Fˉon​)←(t)=inf{x:1/Fˉon​(x)≥t}.

In the TTT-th model, connections start at the points (Γk)k∈Z(\Gamma_k)_{k\in\mathbb Z}(Γk​)k∈Z​ of a homogeneous Poisson process on R\mathbb RR with rate λ=λ(T)\lambda=\lambda(T)λ=λ(T), labelled so that Γ0<0<Γ1\Gamma_0<0<\Gamma_1Γ0​<0<Γ1​. Connection kkk transmits at unit rate for a time XkX_kXk​; the XkX_kXk​ are iid with law FonF_{\mathrm{on}}Fon​ and independent of the Γk\Gamma_kΓk​. The number of active connections and the cumulative input are

N(t)=∑k∈Z1[Γk≤t<Γk+Xk],A(t)=∫0tN(s) ds.N(t)=\sum_{k\in\mathbb Z}\mathbf 1[\Gamma_k\le t<\Gamma_k+X_k],\qquad A(t)=\int_0^tN(s)\,ds .N(t)=k∈Z∑​1[Γk​≤t<Γk​+Xk​],A(t)=∫0t​N(s)ds.

The rate λ(T)\lambda(T)λ(T) is a positive non-decreasing function of TTT. Slow Growth Condition 1 is

lim⁡T→∞b(λT)T=0,\lim_{T\to\infty}\frac{b(\lambda T)}{T}=0,T→∞lim​Tb(λT)​=0,

where b(λT)b(\lambda T)b(λT) is bbb evaluated at λ(T) T\lambda(T)\,Tλ(T)T.

The stable law Sα(σ,β,μ)S_\alpha(\sigma,\beta,\mu)Sα​(σ,β,μ) is the law with characteristic function exp⁡{−σα∣θ∣α(1−iβ sign(θ)tan⁡(πα/2))+iμθ}\exp\{-\sigma^\alpha|\theta|^\alpha(1-i\beta\,\mathrm{sign}(\theta)\tan(\pi\alpha/2))+i\mu\theta\}exp{−σα∣θ∣α(1−iβsign(θ)tan(πα/2))+iμθ} for α≠1\alpha\ne1α=1. α-stable Lévy motion Xα,σ,βX_{\alpha,\sigma,\beta}Xα,σ,β​ has independent stationary increments with X(t)−X(s)∼Sα(σ(t−s)1/α,β,0)X(t)-X(s)\sim S_\alpha(\sigma(t-s)^{1/\alpha},\beta,0)X(t)−X(s)∼Sα​(σ(t−s)1/α,β,0). Write

Cα=1−αΓ(2−α)cos⁡(πα/2)(5.1).C_\alpha=\frac{1-\alpha}{\Gamma(2-\alpha)\cos(\pi\alpha/2)}\quad(5.1).Cα​=Γ(2−α)cos(πα/2)1−α​(5.1).

Formalization targets

Goal: Theorem 1 (corrected scale)

Under (2.8) and Condition 1,

A(T⋅)−Tλμon(⋅)b(λT)→ fidi Xα,Cα−1/α,1(⋅),\frac{A(T\cdot)-T\lambda\mu_{\mathrm{on}}(\cdot)}{b(\lambda T)}\xrightarrow{\ fidi\ }X_{\alpha,C_\alpha^{-1/\alpha},1}(\cdot),b(λT)A(T⋅)−Tλμon​(⋅)​ fidi ​Xα,Cα−1/α​,1​(⋅),

convergence of the finite-dimensional distributions to a totally skewed (β=1\beta=1β=1) α-stable Lévy motion.

On the scale. The paper prints the limit Xα,1,1X_{\alpha,1,1}Xα,1,1​. Its own proof establishes λT P(j1>b(λT)x)→x−α\lambda T\,P(j_1>b(\lambda T)x)\to x^{-\alpha}λTP(j1​>b(λT)x)→x−α (pp. 37–38), which makes αx−α−1dx\alpha x^{-\alpha-1}dxαx−α−1dx the Lévy measure of the limit. The totally skewed stable law with that Lévy measure has σα=Γ(1−α)cos⁡(πα/2)=Cα−1\sigma^\alpha=\Gamma(1-\alpha)\cos(\pi\alpha/2)=C_\alpha^{-1}σα=Γ(1−α)cos(πα/2)=Cα−1​ (Samorodnitsky–Taqqu, Property 1.2.15; also the paper's own criterion on p. 47 with c=1c=1c=1, and the σ\sigmaσ the paper prints in Theorem 2). Since CαC_\alphaCα​ decreases from 2/π2/\pi2/π to 000 on (1,2)(1,2)(1,2) (C1.5≈0.399C_{1.5}\approx0.399C1.5​≈0.399), the printed limit has the wrong scale and the theorem as printed is false. The goal states the corrected scale Cα−1/αC_\alpha^{-1/\alpha}Cα−1/α​; milestones quote the page as printed.

Milestones, in attack order

(2.14), the covariance of NNN; Lemma 1 part 1 (Condition 1   ⟺  λTFˉon(T)→0  ⟺  Cov(NT(0),NT(T))→0\iff\lambda T\bar F_{\mathrm{on}}(T)\to0\iff\mathrm{Cov}(N_T(0),N_T(T))\to0⟺λTFˉon​(T)→0⟺Cov(NT​(0),NT​(T))→0); Lemma 2, slow part (λT2Fˉon(T)/b(λT)→0\lambda T^2\bar F_{\mathrm{on}}(T)/b(\lambda T)\to0λT2Fˉon​(T)/b(λT)→0); (4.15), negligibility of the boundary pieces A2,A3,A4A_2,A_3,A_4A2​,A3​,A4​; the tail limit of j1j_1j1​; (4.17), A12=OP([λT]1/2)=oP(b(λT))A_{12}=O_P([\lambda T]^{1/2})=o_P(b(\lambda T))A12​=OP​([λT]1/2)=oP​(b(λT)); (4.20)–(4.21), A13=o(b(λT))A_{13}=o(b(\lambda T))A13​=o(b(λT)); (4.19), corrected, the stable limit of A11A_{11}A11​; the corrected one-dimensional limit of A(T)A(T)A(T); and EA22=o(b(λT))EA_{22}=o(b(\lambda T))EA22​=o(b(λT)) of §4.5, which reduces the fidi convergence to the one-dimensional one.

Significance

The theorem shows that under slow connection growth the cumulative input is asymptotically a process with independent, infinite-variance increments. Long-range dependence present in each model (the covariance (2.14) decays like h−(α−1)L(h)h^{-(\alpha-1)}L(h)h−(α−1)L(h)) disappears on the time scale TTT, and the heavy tail of the transmission lengths dominates. Together with the fast-growth result (fractional Brownian motion) it explains why both approximations are found in measured traffic, and it identifies the critical quantity b(λT)/Tb(\lambda T)/Tb(λT)/T.

The result is proved in the paper, modulo the scale. No part of it is machine-checked. The mission produces a formal statement of the infinite source Poisson model with its marked point process structure, a formal statement of stable laws and stable Lévy motion through their characteristic functions, and machine-checked versions of the paper's estimates. Correcting the printed scale is part of the output.

Difficulty

The pieces A2,A3,A4,A12,A13,A22A_2,A_3,A_4,A_{12},A_{13},A_{22}A2​,A3​,A4​,A12​,A13​,A22​ are controlled by first moments, regular variation and Lemma 2. The central step is the stable limit of A11A_{11}A11​: a sum of a Poisson number of iid, heavy-tailed summands whose law changes with TTT. A classical central limit theorem does not apply because the variance is infinite, and the summands form a triangular array. The paper cites a point-process limit (Resnick's Exercise 4.4.2.8) for this step; a formal proof needs a convergence theorem for row-wise iid triangular arrays to stable laws, with the constant CαC_\alphaCα​ computed exactly.

Formalization scope

Each TTT has its own probability space carrying the TTT-th model, and every statement quantifies over all such families. The Poisson points are given by their iid exponential spacings −Γ0,Γ1,Γk+1−Γk-\Gamma_0,\Gamma_1,\Gamma_{k+1}-\Gamma_k−Γ0​,Γ1​,Γk+1​−Γk​ (k≠0)(k\ne0)(k=0), indexed by Z\mathbb ZZ. (2.8) is stated as "x↦xαFˉon(x)x\mapsto x^\alpha\bar F_{\mathrm{on}}(x)x↦xαFˉon​(x) is slowly varying", with lengths non-negative. b(t)b(t)b(t) is inf⁡{x>0:tFˉon(x)≤1}\inf\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}inf{x>0:tFˉon​(x)≤1}, which equals the page's generalized inverse for t>0t>0t>0. N(t)N(t)N(t) is a cardinality and the region sums are sums of non-negative terms; their junk values (an infinite set, a non-summable family) occur only on null events. AAA is an interval integral. The growth hypothesis is: λ>0\lambda>0λ>0, non-decreasing, Condition 1. No other hypothesis is added.

The fidi limit is pinned by its characteristic function on Rk\mathbb R^kRk for sorted times 0≤t1≤⋯≤tk0\le t_1\le\dots\le t_k0≤t1​≤⋯≤tk​: the product of the characteristic functions of Sα(σ(tj−tj−1)1/α,1,0)S_\alpha(\sigma(t_j-t_{j-1})^{1/\alpha},1,0)Sα​(σ(tj​−tj−1​)1/α,1,0) evaluated at θj+⋯+θk\theta_j+\dots+\theta_kθj​+⋯+θk​. The existence of the limit law is part of the claim. One-dimensional limits are stated the same way on R\mathbb RR. Convergence in probability to 000 is PT(∣YT∣>η)→0P_T(|Y_T|>\eta)\to0PT​(∣YT​∣>η)→0 for every η>0\eta>0η>0.

Trivializing formalizations are excluded:

  • bbb is never the junk value 000, since its defining set is nonempty and bounded below.
  • The model hypothesis is satisfiable for every rate and length law; a sanity file builds it from product measures, together with a Pareto law satisfying (2.8) and a rate satisfying Condition 1.
  • The limit object is fixed by its characteristic function, not merely asserted to exist.
  • Only fidi convergence is claimed, as on the page. Convergence in the Skorokhod J1J_1J1​ topology fails for this model (Remark after Theorem 1).

A complete development needs regular variation (Karamata's theorem, Potter bounds, generalized inverses), the Poisson random measure of the marked points, and stable limits for triangular arrays. All three are reusable beyond this mission. Proofs of the milestones are welcome separately, as are general Mathlib-style lemmas on regular variation.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén, A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1) (2002) 23–68. https://doi.org/10.1214/aoap/1015961155
  • G. Samorodnitsky, M. S. Taqqu, Stable Non-Gaussian Random Processes, Chapman & Hall, 1994. https://doi.org/10.1201/9780203738818
  • N. H. Bingham, C. M. Goldie, J. L. Teugels, Regular Variation, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511721434
  • S. I. Resnick, Extreme Values, Regular Variation, and Point Processes, Springer, 1987. https://doi.org/10.1007/978-0-387-75953-1
12 thms1 active userReviewed
Graph TheoryMathematical PhysicsProbability·Captain: mikedeng1

Ising Models on Locally Tree-Like Graphs 1: On Uniformly Sparse Locally Tree-Like Graphs the Ising Free Entropy Density Converges to the Bethe PredictionResearch Paper

Motivation

The ferromagnetic Ising model is the basic model of statistical mechanics for interacting binary variables. On a finite graph it is a probability distribution over spin configurations, and its normalizing constant, the partition function, encodes the thermodynamics: the free entropy per vertex determines the magnetization, the correlations, and the location of phase transitions. On lattices this quantity is understood only in special cases. On sparse random graphs, such as random regular graphs and Erdős–Rényi graphs with bounded average degree, physicists predicted it with the cavity method (Mézard and Parisi, The Bethe lattice spin glass revisited, 2001): locally these graphs look like trees, and on trees the model can be solved by a recursion. The same recursion underlies belief propagation, the message-passing algorithm used in coding theory and machine learning.

Timeline:

  • Dembo and Montanari (2008/2010), Ising models on locally tree-like graphs, Ann. Appl. Probab. 20 (2010) 565–592: for every uniformly sparse graph sequence converging locally to a Galton–Watson tree whose offspring law has finite mean, the free entropy density converges at every temperature β≥0\beta \ge 0β≥0 and every field BBB, and for B>0B > 0B>0 the limit is the Bethe prediction. Earlier rigorous results covered special cases, among them Erdős–Rényi graphs in a restricted range of parameters (reference [7] of the paper) and random regular graphs (reference [11]).
  • Dembo, Montanari and Sun (2013), Factor models on locally tree-like graphs, extended the approach to a class of factor models on locally tree-like graphs.

Setting

Let Gn=(Vn=[n],En)G_n = (V_n = [n], E_n)Gn​=(Vn​=[n],En​) be a sequence of finite graphs. The Ising measure at inverse temperature β≥0\beta \ge 0β≥0 and magnetic field B∈RB \in \mathbb RB∈R is

μ(x‾)=1Zn(β,B)exp⁡{β∑(i,j)∈Enxixj+B∑i∈Vnxi},xi∈{+1,−1},\mu(\underline x) = \frac{1}{Z_n(\beta,B)} \exp\Big\{\beta \sum_{(i,j)\in E_n} x_i x_j + B \sum_{i \in V_n} x_i\Big\}, \qquad x_i \in \{+1,-1\},μ(x​)=Zn​(β,B)1​exp{β(i,j)∈En​∑​xi​xj​+Bi∈Vn​∑​xi​},xi​∈{+1,−1},

each edge counted once, and the free entropy density is ϕn(β,B)=1nlog⁡Zn(β,B)\phi_n(\beta,B) = \frac1n \log Z_n(\beta,B)ϕn​(β,B)=n1​logZn​(β,B).

A degree distribution is a law P={Pk}P = \{P_k\}P={Pk​} on {0,1,2,… }\{0,1,2,\dots\}{0,1,2,…} with 0<Pˉ=∑kkPk<∞0 < \bar P = \sum_k k P_k < \infty0<Pˉ=∑k​kPk​<∞; its size-biased version is ρk=kPk/Pˉ\rho_k = k P_k/\bar Pρk​=kPk​/Pˉ, and ρˉ=∑k(k−1)ρk\bar\rho = \sum_k (k-1)\rho_kρˉ​=∑k​(k−1)ρk​. The Galton–Watson tree T(P,ρ,∞)T(P,\rho,\infty)T(P,ρ,∞) has a root with kkk children with probability PkP_kPk​, and every other vertex independently has k−1k-1k−1 children with probability ρk\rho_kρk​; T(P,ρ,t)T(P,\rho,t)T(P,ρ,t) is its first ttt generations.

The ball Bi(t)B_i(t)Bi​(t) is the subgraph induced by the vertices within distance ttt of iii, rooted at iii. The sequence converges locally to T(P,ρ,∞)T(P,\rho,\infty)T(P,ρ,∞) if, for every ttt and every rooted tree TTT, the fraction of vertices iii with Bi(t)≃TB_i(t) \simeq TBi​(t)≃T (root-preserving isomorphism) tends to P{T(P,ρ,t)≃T}\mathbb P\{T(P,\rho,t) \simeq T\}P{T(P,ρ,t)≃T}. It is uniformly sparse if lim⁡l→∞lim sup⁡n1n∑i∣∂i∣ I(∣∂i∣≥l)=0\lim_{l\to\infty}\limsup_n \frac1n\sum_i |\partial i|\,\mathbb I(|\partial i| \ge l) = 0liml→∞​limsupn​n1​∑i​∣∂i∣I(∣∂i∣≥l)=0.

The cavity recursion acts on laws of a real random variable hhh:

h=dB+∑i=1K−1ξ(β,hi),ξ(β,h)=atanh⁡[tanh⁡βtanh⁡h],h \overset{d}{=} B + \sum_{i=1}^{K-1} \xi(\beta, h_i), \qquad \xi(\beta,h) = \operatorname{atanh}[\tanh\beta \tanh h],h=dB+i=1∑K−1​ξ(β,hi​),ξ(β,h)=atanh[tanhβtanhh],

with K∼ρK \sim \rhoK∼ρ and hih_ihi​ i.i.d. copies of hhh independent of KKK. For B>0B > 0B>0 it has a unique fixed point h∗h^*h∗ supported on [0,∞)[0,\infty)[0,∞). The Bethe functional of a law of hhh is

φh(β,B)=Pˉ2log⁡cosh⁡β−Pˉ2Elog⁡[1+tanh⁡βtanh⁡h1tanh⁡h2]+Elog⁡{eB∏i=1L[1+tanh⁡βtanh⁡hi]+e−B∏i=1L[1−tanh⁡βtanh⁡hi]},\varphi_h(\beta,B) = \frac{\bar P}{2}\log\cosh\beta - \frac{\bar P}{2}\mathbb E\log[1+\tanh\beta\tanh h_1\tanh h_2] + \mathbb E\log\Big\{e^B\prod_{i=1}^L[1+\tanh\beta\tanh h_i] + e^{-B}\prod_{i=1}^L[1-\tanh\beta\tanh h_i]\Big\},φh​(β,B)=2Pˉ​logcoshβ−2Pˉ​Elog[1+tanhβtanhh1​tanhh2​]+Elog{eBi=1∏L​[1+tanhβtanhhi​]+e−Bi=1∏L​[1−tanhβtanhhi​]},

with L∼PL \sim PL∼P independent of the hih_ihi​.

Formalization targets

Goal: Theorem 2.4

Assume {Gn}\{G_n\}{Gn​} is uniformly sparse, converges locally to T(P,ρ,∞)T(P,\rho,\infty)T(P,ρ,∞), and ∑kkρk<∞\sum_k k\rho_k < \infty∑k​kρk​<∞. Then for every β≥0\beta \ge 0β≥0:

lim⁡n→∞ϕn(β,B)=φh∗(β,∣B∣)(B≠0),\lim_{n\to\infty}\phi_n(\beta,B) = \varphi_{h^*}(\beta,|B|) \quad (B \ne 0),n→∞lim​ϕn​(β,B)=φh∗​(β,∣B∣)(B=0),

and φh∗(β,B)\varphi_{h^*}(\beta,B)φh∗​(β,B) has a limit L0L_0L0​ as B↓0B \downarrow 0B↓0, with ϕn(β,0)→L0\phi_n(\beta,0) \to L_0ϕn​(β,0)→L0​. This is the paper's statement that the limit exists for every BBB, equals (2.9) for B>0B > 0B>0, is even in BBB, and is continuous at B=0B = 0B=0.

Milestones

  1. Tools on Ising models: Griffiths' inequality (Theorem 3.1), the GHS inequality (Theorem 3.2), the subtree-marginal identity (Lemma 4.1).
  2. Trees: the boundary effect on the root magnetization, E{mℓ,+−mℓ,0}≤M/ℓ\mathbb E\{m^{\ell,+}-m^{\ell,0}\} \le M/\ellE{mℓ,+−mℓ,0}≤M/ℓ (Lemma 4.3); the correlation factorization (Lemma 4.4); exponential decay of root-to-generation correlations (Corollary 4.5, (4.13)).
  3. The recursion: monotone convergence to the unique nonnegative fixed point (Lemma 2.3) and its Lipschitz dependence on β\betaβ in Monge–Kantorovich distance (Lemma 4.6).
  4. The Bethe functional: the second-order perturbation bound (Lemma 6.1, Remark 6.2) and its consequence, stationarity of φh\varphi_hφh​ at fixed points (Corollary 6.3, with corrected constant).
  5. From trees to graphs: edge averages converge to averages over the edge-rooted tree Tˉ(ρ,t)\bar T(\rho,t)Tˉ(ρ,t) (Lemma 6.4), and ∂βϕn=1n∑(i,j)∈En⟨xixj⟩n\partial_\beta\phi_n = \frac1n\sum_{(i,j)\in E_n}\langle x_ix_j\rangle_n∂β​ϕn​=n1​∑(i,j)∈En​​⟨xi​xj​⟩n​ (6.10).

Significance

The result. Theorem 2.4 establishes the replica-symmetric (Bethe) formula for the ferromagnetic Ising model on the standard sparse random graph ensembles at all temperatures, including below the critical temperature tanh⁡βc=1/ρˉ\tanh\beta_c = 1/\bar\rhotanhβc​=1/ρˉ​ where the Gibbs measure on the limiting tree is not unique. It identifies the free energy of random regular graphs, Erdős–Rényi graphs and configuration models with arbitrary degree distributions of finite variance, and the derivative identities that follow give the limiting magnetization and energy per edge. The tree estimates of Section 4 also yield the convergence of belief propagation (the companion mission of this series).

Formalizing it. The theorem is proved; nothing in this mission has been machine-checked before. A formal proof requires infrastructure that Lean's Mathlib does not have: Ising measures with boundary conditions, correlation inequalities, Galton–Watson trees as laws of offspring functions, local weak convergence of graph sequences, distributional fixed-point equations, and the Monge–Kantorovich distance on the real line. While stating the milestones, Corollary 6.3 turned out to be false as printed (the constant Pˉρˉ\bar P\bar\rhoPˉρˉ​ should be E[L2]\mathbb E[L^2]E[L2]; a counterexample is P=δ1P = \delta_1P=δ1​); the mission states the corrected version, which is what the paper's proof gives.

Difficulty

The obvious route through uniqueness of the Gibbs measure on the tree fails below the critical temperature: different boundary conditions give different limits, so local quantities are not determined by the local graph structure alone. The paper replaces uniqueness by insensitivity to positive boundary conditions when B>0B > 0B>0 (Lemma 4.3), which rests on Griffiths and GHS monotonicity and on averaging over the random tree; the deterministic statement is false. Passing from derivatives to the free entropy itself requires that the Bethe functional be stationary in the cavity law (Corollary 6.3), so that the β\betaβ-dependence of h∗h^*h∗ can be ignored. Finally, the case B=0B = 0B=0 at low temperature is reached only as a limit: there is no fixed-point characterization at B=0B = 0B=0.

Formalization scope

  • Spins are Booleans (+1+1+1 = true); edges are unordered and counted once. Graphs GnG_nGn​ live on Fin n.
  • A field Bi=+∞B_i = +\inftyBi​=+∞ (plus boundary) is encoded by pinning vertex iii to +1+1+1, never by a large real field.
  • Rooted trees are offspring functions List ℕ → ℕ in Ulam–Harris form; random trees are laws of offspring functions under the product σ-algebra. Galton–Watson trees are infinite product measures. Fields on trees are nonrandom functions of the vertex.
  • Laws of cavity fields are probability measures on R\mathbb RR; the recursion is a map on ProbabilityMeasure ℝ, and convergence in distribution is weak convergence. Expectations over L∼PL \sim PL∼P are series ∑lPl E[⋅]\sum_l P_l\,\mathbb E[\cdot]∑l​Pl​E[⋅] with product laws.
  • The Monge–Kantorovich distance takes values in [0,∞][0,\infty][0,∞]. Uniform sparsity is computed in [0,∞][0,\infty][0,∞] so that an unbounded sequence does not get a junk lim sup⁡\limsuplimsup of 000.
  • The fixed point h∗h^*h∗ in the goal is the one supported on [0,∞)[0,\infty)[0,∞), selected by choice; Lemma 2.3 shows it exists and is unique, so an arbitrary fixed point cannot be substituted. Theorem 2.4 is stated with β≥0\beta \ge 0β≥0 and asserts convergence for B>0B > 0B>0, B<0B < 0B<0 and B=0B = 0B=0 separately; the B=0B = 0B=0 clause asserts the existence of the one-sided limit rather than assuming it.

A complete development needs: Griffiths and GHS inequalities for finite Ising models (reusable for any ferromagnetic model); Ulam–Harris random trees with conditional independence; local weak convergence of graph sequences (reusable for random graph theory); distributional recursions with stochastic ordering; and the coupling characterization of the Wasserstein-1 distance on R\mathbb RR. Contributions of any milestone are welcome, as are proofs of the classical inequalities of Section 3 independent of this paper.

Selected references

  • A. Dembo, A. Montanari, Ising models on locally tree-like graphs, Ann. Appl. Probab. 20(2) (2010) 565–592. https://arxiv.org/abs/0804.4726v3 , https://doi.org/10.1214/09-AAP627
  • M. Mézard, G. Parisi, The Bethe lattice spin glass revisited, Eur. Phys. J. B 20 (2001) 217–233. https://doi.org/10.1007/PL00011099
  • R. B. Griffiths, C. A. Hurst, S. Sherman, Concavity of magnetization of an Ising ferromagnet in a positive external field, J. Math. Phys. 11 (1970) 790–795. https://doi.org/10.1063/1.1665211
  • T. M. Liggett, Interacting Particle Systems, Springer, 1985 (Theorem IV.1.21, Griffiths' inequality). https://doi.org/10.1007/978-1-4613-8542-4
  • A. Dembo, A. Montanari, N. Sun, Factor models on locally tree-like graphs, Ann. Probab. 41(6) (2013) 4162–4213. https://doi.org/10.1214/12-AOP828
27 thms1 active userReviewed
Discrete GeometryNumber TheoryTheoretical Computer Science·Captain: mikedeng1

On Lattices, Learning with Errors, Random Linear Codes, and Cryptography 6: The Smoothing Parameter Satisfies η_ε(L) ≥ √(ln(1/ε)/π)/λ₁(L*) ≥ √(ln(1/ε)/π)·λ_n(L)/nResearch Paper

Motivation

The learning with errors (LWE) problem underlies much of post-quantum public-key cryptography, and its hardness rests on Regev's reduction from worst-case lattice problems to LWE (Regev, J. ACM 2009). Every step of that reduction is calibrated by the smoothing parameter ηϵ(L)\eta_\epsilon(L)ηϵ​(L) of Micciancio and Regev (SIAM J. Comput. 2007): the Gaussian width above which a discrete Gaussian on a lattice behaves like a continuous one. The approximation factors of the reduction are stated in terms of ηϵ(L)\eta_\epsilon(L)ηϵ​(L), and they are converted into factors for the standard lattice problems (GapSVP, SIVP) by comparing ηϵ(L)\eta_\epsilon(L)ηϵ​(L) with the successive minima of LLL and of its dual.

Upper bounds on ηϵ(L)\eta_\epsilon(L)ηϵ​(L) (Lemmas 2.11 and 2.12 of the paper, from Micciancio–Regev) say the smoothing parameter is not too large. Claim 2.13 is the matching lower bound: the smoothing parameter cannot be much smaller than 1/λ1(L∗)1/\lambda_1(L^*)1/λ1​(L∗), and hence than λn(L)/n\lambda_n(L)/nλn​(L)/n. The second comparison goes through Banaszczyk's transference theorem (Banaszczyk, Math. Ann. 296 (1993)), 1≤λ1(L)λn(L∗)≤n1 \le \lambda_1(L)\lambda_n(L^*) \le n1≤λ1​(L)λn​(L∗)≤n, which relates the geometry of a lattice to that of its dual.

This mission formalizes Claim 2.13 from the published J. ACM article (Article 34, 2009), together with the steps of its proof and the transference theorem it cites. The paper's main theorem, Theorem 3.1, is a quantum reduction about efficient algorithms; it is outside this series of missions.

Setting

Work in Rn\mathbb{R}^nRn, n≥1n \ge 1n≥1, with the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥ and inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩. A lattice L⊂RnL \subset \mathbb{R}^nL⊂Rn is the set of integer combinations of nnn linearly independent vectors. Its dual is

L∗={y∈Rn:⟨x,y⟩∈Z for all x∈L},L^* = \{y \in \mathbb{R}^n : \langle x, y\rangle \in \mathbb{Z} \text{ for all } x \in L\},L∗={y∈Rn:⟨x,y⟩∈Z for all x∈L},

again a lattice, with (L∗)∗=L(L^*)^* = L(L∗)∗=L.

The successive minima used here are λ1(L)\lambda_1(L)λ1​(L), the length of a shortest nonzero vector of LLL, and λn(L)\lambda_n(L)λn​(L), the least rrr such that LLL contains nnn linearly independent vectors of length at most rrr.

For s>0s > 0s>0 the Gaussian function is ρs(x)=exp⁡(−π∥x/s∥2)\rho_s(x) = \exp(-\pi\|x/s\|^2)ρs​(x)=exp(−π∥x/s∥2) (Eq. (4)), and for a countable set AAA, ρs(A)=∑x∈Aρs(x)\rho_s(A) = \sum_{x\in A}\rho_s(x)ρs​(A)=∑x∈A​ρs​(x). In particular ρ1/s(y)=exp⁡(−πs2∥y∥2)\rho_{1/s}(y) = \exp(-\pi s^2\|y\|^2)ρ1/s​(y)=exp(−πs2∥y∥2).

For ϵ>0\epsilon > 0ϵ>0 the smoothing parameter ηϵ(L)\eta_\epsilon(L)ηϵ​(L) is the smallest sss such that ρ1/s(L∗∖{0})≤ϵ\rho_{1/s}(L^*\setminus\{0\}) \le \epsilonρ1/s​(L∗∖{0})≤ϵ (Definition 2.10).

Formalization targets

Goal: Claim 2.13 (p. 34:20)

For any lattice LLL and any ϵ>0\epsilon > 0ϵ>0,

ηϵ(L)  ≥  ln⁡1/ϵπ⋅1λ1(L∗)  ≥  ln⁡1/ϵπ⋅λn(L)n.\eta_\epsilon(L) \;\ge\; \sqrt{\frac{\ln 1/\epsilon}{\pi}}\cdot\frac{1}{\lambda_1(L^*)} \;\ge\; \sqrt{\frac{\ln 1/\epsilon}{\pi}}\cdot\frac{\lambda_n(L)}{n}.ηϵ​(L)≥πln1/ϵ​​⋅λ1​(L∗)1​≥πln1/ϵ​​⋅nλn​(L)​.

Both inequalities of the chain are part of the goal. The asymptotic "In particular" sentence of the claim (ϵ(n)=o(1)\epsilon(n) = o(1)ϵ(n)=o(1), large enough nnn) is not.

Milestones, in attack order

  1. The remark after Definition 2.10 (p. 34:19). The map s↦ρ1/s(L∗∖{0})s \mapsto \rho_{1/s}(L^*\setminus\{0\})s↦ρ1/s​(L∗∖{0}) is continuous and strictly decreasing on (0,∞)(0,\infty)(0,∞), tends to ∞\infty∞ as s→0s \to 0s→0 and to 000 as s→∞s \to \inftys→∞, and ϵ↦ηϵ(L)\epsilon \mapsto \eta_\epsilon(L)ϵ↦ηϵ​(L) is its inverse; in particular ρ1/ηϵ(L)(L∗∖{0})=ϵ\rho_{1/\eta_\epsilon(L)}(L^*\setminus\{0\}) = \epsilonρ1/ηϵ​(L)​(L∗∖{0})=ϵ.
  2. The display of the proof of Claim 2.13 (p. 34:20). For s=ηϵ(L)s = \eta_\epsilon(L)s=ηϵ​(L) and v∈L∗v \in L^*v∈L∗ of length λ1(L∗)\lambda_1(L^*)λ1​(L∗),
ϵ=ρ1/s(L∗∖{0})≥ρ1/s(v)=exp⁡(−π(sλ1(L∗))2).\epsilon = \rho_{1/s}(L^*\setminus\{0\}) \ge \rho_{1/s}(v) = \exp\bigl(-\pi(s\lambda_1(L^*))^2\bigr).ϵ=ρ1/s​(L∗∖{0})≥ρ1/s​(v)=exp(−π(sλ1​(L∗))2).
  1. Lemma 2.3, Banaszczyk's transference theorem (p. 34:18). For any nnn-dimensional lattice LLL,
1≤λ1(L)⋅λn(L∗)≤n.1 \le \lambda_1(L)\cdot\lambda_n(L^*) \le n .1≤λ1​(L)⋅λn​(L∗)≤n.

Significance

The result. Claim 2.13 shows that the smoothing parameter for a negligible ϵ\epsilonϵ exceeds every constant multiple of 1/λ1(L∗)1/\lambda_1(L^*)1/λ1​(L∗) and of λn(L)/n\lambda_n(L)/nλn​(L)/n. Together with the upper bound ηϵ(L)≤ln⁡(2n(1+1/ϵ))/π λn(L)\eta_\epsilon(L) \le \sqrt{\ln(2n(1+1/\epsilon))/\pi}\,\lambda_n(L)ηϵ​(L)≤ln(2n(1+1/ϵ))/π​λn​(L) of Lemma 2.12, it locates ηϵ(L)\eta_\epsilon(L)ηϵ​(L) within a polynomial factor of λn(L)\lambda_n(L)λn​(L). This is what lets the reduction's guarantees, phrased in ηϵ(L)\eta_\epsilon(L)ηϵ​(L), be read as approximation factors for SIVP and GapSVP. The transference theorem is used throughout the geometry of numbers and in lattice-based cryptography to pass between a lattice and its dual.

Formalizing it. The claim and its proof are classical and short, but neither is machine-checked. The mission produces formal definitions of the dual lattice, the successive minima λ1\lambda_1λ1​, λn\lambda_nλn​ and the smoothing parameter on EuclideanSpace ℝ (Fin n), a proof that Definition 2.10 is well posed, and a statement of Banaszczyk's transference theorem. The upper bound of the transference theorem is a substantial result in its own right (the paper cites it without proof), and a formal proof of it would be reusable well beyond this mission.

Difficulty

The first inequality of the goal is elementary once the smoothing parameter is known to be attained, with ρ1/η(L∗∖{0})=ϵ\rho_{1/\eta}(L^*\setminus\{0\}) = \epsilonρ1/η​(L∗∖{0})=ϵ exactly. That step is not a formality: it needs the continuity and strict monotonicity of an infinite lattice sum in the scale parameter, and the fact that a shortest nonzero dual vector exists, both of which rest on the discreteness of L∗L^*L∗.

The second inequality is a single line in the paper, "by Lemma 2.3", but it uses the upper bound of Banaszczyk's theorem, applied to the dual lattice. The easy lower bound 1≤λ1(L)λn(L∗)1 \le \lambda_1(L)\lambda_n(L^*)1≤λ1​(L)λn​(L∗) does not suffice, and a Minkowski-type argument gives a bound worse than linear in nnn. Applying the lemma to L∗L^*L∗ also needs L∗L^*L∗ to be a lattice with dual LLL.

Formalization scope

  • Rn\mathbb{R}^nRn is EuclideanSpace ℝ (Fin n). A lattice is L : Submodule ℤ _ with [DiscreteTopology L] [IsZLattice ℝ L]. The dual is LinearMap.BilinForm.dualSubmodule (innerₗ _) L.
  • Every theorem assumes 0<n0 < n0<n: the paper's lattices are nnn-dimensional with n≥1n \ge 1n≥1. This is the only added hypothesis.
  • Gaussian sums are real tsums. They are summable over discrete subgroups, so no summability hypotheses are added.
  • ηϵ(L)\eta_\epsilon(L)ηϵ​(L), λ1\lambda_1λ1​ and λn\lambda_nλn​ are infima (sInf). The paper's "smallest" is the attainment proved in milestones 1 and 2, not built into the definition. λ1\lambda_1λ1​ and λn\lambda_nλn​ are defined for every Z\mathbb{Z}Z-submodule, so they apply to L∗L^*L∗ without extra instances.
  • For ϵ≥1\epsilon \ge 1ϵ≥1 the paper's ln⁡(1/ϵ)/π\sqrt{\ln(1/\epsilon)/\pi}ln(1/ϵ)/π​ is the square root of a non-positive number; Lean's Real.sqrt gives 000 there and the goal reduces to true statements. No hypothesis ϵ<1\epsilon < 1ϵ<1 is added, since the page says "any ϵ>0\epsilon > 0ϵ>0".
  • The goal is a conjunction of both inequalities of the chain, not only the outer comparison ηϵ(L)≥ln⁡(1/ϵ)/π λn(L)/n\eta_\epsilon(L) \ge \sqrt{\ln(1/\epsilon)/\pi}\,\lambda_n(L)/nηϵ​(L)≥ln(1/ϵ)/π​λn​(L)/n, which would be weaker. Lemma 2.3 states both bounds; stating only the easy lower bound would leave the goal's second inequality without its milestone.
  • No printed statement needed correction.

Contributions welcome: the attainment of λ1\lambda_1λ1​ and λn\lambda_nλn​ for IsZLattice (and for the dual), the identity (L∗)∗=L(L^*)^* = L(L∗)∗=L in this setting, continuity and monotonicity of Gaussian lattice sums, and above all Banaszczyk's transference theorem.

Selected references

  • O. Regev, On Lattices, Learning with Errors, Random Linear Codes, and Cryptography, J. ACM 56(6), Article 34, 2009. https://doi.org/10.1145/1568318.1568324
  • W. Banaszczyk, New bounds in some transference theorems in the geometry of numbers, Math. Ann. 296, 625–635, 1993. https://doi.org/10.1007/BF01445125
  • D. Micciancio, O. Regev, Worst-case to average-case reductions based on Gaussian measures, SIAM J. Comput. 37(1), 267–302, 2007. https://doi.org/10.1137/S0097539705447360
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CombinatoricsGraph Theory·Captain: mikedeng1

Graph Minors XXIII. Nash-Williams' Immersion Conjecture: In Every Infinite Sequence of Finite Graphs, Some Graph Is Immersed in a Later OneResearch Paper

Motivation

A well-quasi-order is a reflexive, transitive relation in which every infinite sequence x1,x2,…x_1,x_2,\dotsx1​,x2​,… contains a pair i<ji<ji<j with xi≤xjx_i\le x_jxi​≤xj​. Showing that a class of finite combinatorial objects is well-quasi-ordered by a containment relation is a standard way to prove that every property closed under that containment is characterised by finitely many forbidden objects. The best-known instance is the Graph Minor Theorem (Wagner's conjecture), completed by Robertson and Seymour in Graph Minors XX (JCTB 92, 2004).

Nash-Williams proposed the analogous conjecture for a different containment, immersion, in which edges of the smaller graph are mapped to edge-disjoint paths of the larger graph. Graph Minors XXIII (JCTB 100, 2010) proves it by deriving a general well-quasi-ordering theorem for labelled hypergraphs from the machinery of Graph Minors XX.

Timeline.

  • 1963 (published 1964): Nash-Williams conjectures that finite graphs are well-quasi-ordered by immersion ([Theory of Graphs and Its Applications, Smolenice 1963, pp. 83–84]).
  • 1965: Nash-Williams proposes a second, "strong" immersion conjecture, in which the image paths may not pass through images of non-incident vertices (Proc. Cambridge Philos. Soc. 61).
  • 2004: Graph Minors XX proves Wagner's conjecture: finite graphs are well-quasi-ordered by minors.
  • 2010: Graph Minors XXIII proves the (weak) immersion conjecture together with a labelled hypergraph generalisation. The paper states that it does not prove the strong conjecture.

Setting

All graphs and hypergraphs are finite. A graph GGG has a vertex set V(G)V(G)V(G), an edge set E(G)E(G)E(G), and for each edge an unordered pair of ends; an edge with equal ends is a loop, and several edges may have the same ends (parallel edges). A graph is loopless if no edge is a loop. A path has at least one vertex and no repeated vertices; a circuit has at least one edge and no repeated vertices, so a loop and a pair of parallel edges are circuits.

An immersion of HHH in GGG is a map α\alphaα on V(H)∪E(H)V(H)\cup E(H)V(H)∪E(H) such that α\alphaα is injective on vertices; every non-loop edge eee with ends u,vu,vu,v goes to a path α(e)\alpha(e)α(e) of GGG with ends α(u),α(v)\alpha(u),\alpha(v)α(u),α(v); every loop at vvv goes to a circuit α(e)\alpha(e)α(e) of GGG through α(v)\alpha(v)α(v); and α(e)\alpha(e)α(e), α(f)\alpha(f)α(f) share no edge when e≠fe\ne fe=f.

A hypergraph GGG has finite sets V(G)V(G)V(G), E(G)E(G)E(G) and an incidence relation; V(e)V(e)V(e) is the set of ends of the edge eee, of any size. Write KVK_VKV​ for the complete graph on VVV. A collapse of GGG to HHH maps each vertex vvv of HHH to a non-null connected subgraph η(v)\eta(v)η(v) of KV(G)K_{V(G)}KV(G)​, pairwise vertex-disjoint, and each edge eee of HHH injectively to an edge η(e)\eta(e)η(e) of GGG, so that η(e)\eta(e)η(e) meets η(v)\eta(v)η(v) whenever eee is incident with vvv, and every edge xyxyxy of every η(v)\eta(v)η(v) is covered by some edge of GGG incident with both xxx and yyy. The transpose of a graph GGG is the hypergraph with vertex set E(G)E(G)E(G), edge set V(G)V(G)V(G) and the same incidence.

A quasi-order Ω\OmegaΩ is an ideal of Ω′\Omega'Ω′ if it is a sub-quasi-order closed downwards in Ω′\Omega'Ω′; a shadow is a tuple (Ω∞,m,Ωm,…,Ω1,R2,R1)(\Omega_\infty,m,\Omega_m,\dots,\Omega_1,R_2,R_1)(Ω∞​,m,Ωm​,…,Ω1​,R2​,R1​) of well-quasi-orders and finite sets, ordered lexicographically (Section 3 of the paper).

Formalization targets

Goal: Nash-Williams' immersion conjecture (1.1)

∀ (Gi)i≥1 finite graphs:∃ j>i≥1,  Gi is immersed in Gj.\forall\,(G_i)_{i\ge1}\text{ finite graphs}:\quad \exists\, j>i\ge1,\ \ G_i \text{ is immersed in } G_j .∀(Gi​)i≥1​ finite graphs:∃j>i≥1,  Gi​ is immersed in Gj​.

Milestones, in the order the proof uses them

  • 3.1 No sequence Ω1,Ω2,…\Omega_1,\Omega_2,\dotsΩ1​,Ω2​,… with Ω1\Omega_1Ω1​ a well-quasi-order and Ωi+1\Omega_{i+1}Ωi+1​ a proper ideal of Ωi\Omega_iΩi​ for all iii.
  • 3.2 No sequence of shadows with Σi+1<Σi\Sigma_{i+1}<\Sigma_iΣi+1​<Σi​ for all iii.
  • 1.6 For a well-quasi-order Ω\OmegaΩ and hypergraphs GiG_iGi​ with edge labels ϕi\phi_iϕi​, distinguished edges MiM_iMi​ of at most kkk ends and orderings μi(e)\mu_i(e)μi​(e) of their ends, some j>ij>ij>i admit a collapse η\etaη of GjG_jGj​ to GiG_iGi​ with ϕi(e)≤ϕj(η(e))\phi_i(e)\le\phi_j(\eta(e))ϕi​(e)≤ϕj​(η(e)), η(e)∈Mj  ⟺  e∈Mi\eta(e)\in M_j\iff e\in M_iη(e)∈Mj​⟺e∈Mi​, and preserving the orderings.
  • 1.4 The same with Mi=∅M_i=\emptysetMi​=∅: ϕi(e)≤ϕj(η(e))\phi_i(e)\le\phi_j(\eta(e))ϕi​(e)≤ϕj​(η(e)) for all edges.
  • 1.2 For every sequence of hypergraphs there is a collapse of some GjG_jGj​ to some earlier GiG_iGi​.
  • 1.3 For loopless graphs G,HG,HG,H, a collapse of the transpose of GGG to the transpose of HHH yields an immersion of HHH in GGG.
  • 1.5 Vertex-labelled loopless graphs: an immersion α\alphaα of GiG_iGi​ in GjG_jGj​ with ϕi(v)≤ϕj(α(v))\phi_i(v)\le\phi_j(\alpha(v))ϕi​(v)≤ϕj​(α(v)).
  • 1.7 (off the goal's path) A labelled form of Wagner's conjecture for directed graphs with loops.

Significance

The immersion theorem implies that every class of finite graphs closed under taking immersions is characterised by finitely many excluded immersions. Theorem 1.6 is stronger than both 1.1 and Wagner's conjecture: it handles hypergraphs, labels from an arbitrary well-quasi-order and ordered edges, which is the form in which the Graph Minors machinery is reused by later work.

All results here are proved in the paper. None of them has a machine-checked proof: Mathlib has well-quasi-orders and Higman's lemma, but not the Graph Minor Theorem or any notion of graph immersion. The value of this mission is a faithful formal statement of the immersion theorem and of the reductions the paper performs in Section 1 (1.3 and the passage from 1.6 to 1.4, 1.5 and 1.1), each of which can be formalized independently of Graph Minors XX, plus the order-theoretic lemmas 3.1 and 3.2.

Difficulty

The reductions in Section 1 (1.3, and the passages from 1.6 to 1.4, 1.5 and 1.1) are short on paper but require a working library of multigraph walks, paths and circuits, which Mathlib does not have for graphs with loops and parallel edges. The real difficulty is 1.6, which the paper derives from a theorem on patchworks of Graph Minors XX (its 2.2) together with tangle results of Graph Minors X, and therefore rests on the structure theory of the whole Graph Minors series. No route around that theory is known: when the hypergraphs are loopless graphs, a collapse of GjG_jGj​ to GiG_iGi​ makes GiG_iGi​ a minor of GjG_jGj​, so already 1.2 contains Wagner's conjecture. Nor does 1.2 alone give 1.1: loops cannot be routed through the transpose construction of 1.3, and the paper handles them by counting loops at each vertex as a label from the well-quasi-order N\mathbb NN, which is why the labelled forms 1.4–1.6 are needed.

Formalization scope

A graph is Graph V E with ends : E → Sym2 V; a hypergraph is Hypergraph V E with inc : E → V → Prop; each lives on its own finite types, and a sequence is a family indexed by ℕ (from 000; the paper's j>i≥1j>i\ge1j>i≥1 becomes i<ji<ji<j). Paths and circuits are walks with vertex and edge lists; the ends of a path are unordered. An immersion is the structure GraphImmersion H G; a collapse of GGG to HHH is Collapse G H, whose branch sets are Subgraphs of ⊤ : SimpleGraph V(G) (Mathlib's Subgraph.Connected includes non-emptiness). Well-quasi-orders are Mathlib's WellQuasiOrdered on a type with a preorder for 1.4–1.7, and QO.IsWQO on subsets of an ambient type for 3.1–3.2, where quasi-orders are compared by inclusion. Directed graphs for 1.7 are DirGraph V E with heads and tails.

Three trivializing formalizations are excluded: the collapse keeps condition (iv), so branch sets cannot use arbitrary pairs of vertices; immersion paths are edge-disjoint, not vertex-disjoint (which would give topological minors, not a well-quasi-order); and each graph lives on its own type, never all on one fixed finite type, which would make the goal a pigeonhole statement. Strong immersion is not stated.

Contributions welcome: proofs of 3.1, 3.2 and 1.3, the reductions 1.6 ⇒ 1.4 ⇒ 1.2 and 1.4 + 1.3 ⇒ 1.5 ⇒ 1.1, and library material on multigraph walks, paths and circuits, which is reusable beyond this mission. A proof of 1.6 would require formalizing the Graph Minors series.

Selected references

  • N. Robertson, P. Seymour, Graph Minors XXIII. Nash-Williams' immersion conjecture, J. Combin. Theory Ser. B 100 (2010) 181–205 (authors' manuscript rev. April 18, 2011, used here). https://doi.org/10.1016/j.jctb.2009.07.003
  • N. Robertson, P. Seymour, Graph Minors XX. Wagner's conjecture, J. Combin. Theory Ser. B 92 (2004) 325–357. https://doi.org/10.1016/j.jctb.2004.08.001
  • C. St. J. A. Nash-Williams, On well-quasi-ordering infinite trees, Proc. Cambridge Philos. Soc. 61 (1965) 697–720. https://doi.org/10.1017/S0305004100039062
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AnalysisControl TheoryDynamical Systems·Captain: mikedeng1

Small Gain Theorems for Large Scale Systems and Construction of ISS Lyapunov Functions 1: Rescaling Along an Ω-Path Gives the Network ISS Lyapunov Function maxᵢ σᵢ⁻¹(Vᵢ(xᵢ))Research Paper

Motivation

Large engineered systems — power grids, chemical plants, logistics and communication networks — are usually modelled as many interacting subsystems. A stability certificate for the whole network is rarely available directly, but each subsystem can often be analysed on its own, treating the states of its neighbours as disturbances. Input-to-state stability (ISS), introduced by Sontag (Sontag 1989), is the robustness notion that makes this decomposition work: it bounds the state by a decaying function of the initial condition plus a gain of the input. A small-gain theorem states that if the gains by which the subsystems influence each other are "small" in a suitable sense, the interconnection is again ISS.

Timeline. Jiang, Teel and Praly proved a nonlinear small-gain theorem for two ISS systems in trajectory form (1994), and Jiang, Mareels and Wang gave its Lyapunov version for two subsystems (1996). Dashkovskiy, Rüffer and Wirth extended the trajectory version to nnn subsystems with the condition Γ≱id\Gamma\not\ge\mathrm{id}Γ≥id on a nonlinear gain operator (2007). The paper of this mission (arXiv:0901.1842, SIAM J. Control Optim. 48(6), 2010) gives the Lyapunov version for nnn subsystems with general monotone aggregation of the gains, and constructs the network's ISS Lyapunov function explicitly.

Setting

The network consists of n≥1n\ge 1n≥1 subsystems

Σi: x˙i=fi(x1,…,xn,u),xi∈RNi, u∈RM,\Sigma_i:\ \dot x_i=f_i(x_1,\dots,x_n,u),\qquad x_i\in\mathbb R^{N_i},\ u\in\mathbb R^M,Σi​: x˙i​=fi​(x1​,…,xn​,u),xi​∈RNi​, u∈RM,

with overall state x=(x1T,…,xnT)T∈RNx=(x_1^T,\dots,x_n^T)^T\in\mathbb R^Nx=(x1T​,…,xnT​)T∈RN and dynamics x˙=f(x,u)\dot x=f(x,u)x˙=f(x,u), f=(f1,…,fn)f=(f_1,\dots,f_n)f=(f1​,…,fn​). ∥⋅∥\|\cdot\|∥⋅∥ is the Euclidean norm.

A function γ:R+→R+\gamma:\mathbb R_+\to\mathbb R_+γ:R+​→R+​ is of class K\mathcal KK if it is continuous, strictly increasing and γ(0)=0\gamma(0)=0γ(0)=0, and of class K∞\mathcal K_\inftyK∞​ if moreover unbounded. A positive definite function α:R+→R+\alpha:\mathbb R_+\to\mathbb R_+α:R+​→R+​ is continuous with α(r)=0\alpha(r)=0α(r)=0 only at r=0r=0r=0. A Lyapunov function candidate V:Rd→R+V:\mathbb R^d\to\mathbb R_+V:Rd→R+​ is continuous, satisfies ψ1(∥x∥)≤V(x)≤ψ2(∥x∥)\psi_1(\|x\|)\le V(x)\le\psi_2(\|x\|)ψ1​(∥x∥)≤V(x)≤ψ2​(∥x∥) for some ψ1,ψ2∈K∞\psi_1,\psi_2\in\mathcal K_\inftyψ1​,ψ2​∈K∞​, and is locally Lipschitz away from the origin.

A candidate VVV is an ISS Lyapunov function for x˙=f(x,u)\dot x=f(x,u)x˙=f(x,u) if there are γ∈K\gamma\in\mathcal Kγ∈K and a positive definite α\alphaα with

V(x)≥γ(∥u∥) ⟹ ∇V(x)f(x,u)≤−α(∥x∥)V(x)\ge\gamma(\|u\|)\ \Longrightarrow\ \nabla V(x)f(x,u)\le-\alpha(\|x\|)V(x)≥γ(∥u∥) ⟹ ∇V(x)f(x,u)≤−α(∥x∥)

at every point of differentiability of VVV.

On R+n\mathbb R^n_+R+n​, v<wv<wv<w means vi<wiv_i<w_ivi​<wi​ for every iii. A monotone aggregation function (MAF) μ:R+m→R+\mu:\mathbb R^m_+\to\mathbb R_+μ:R+m​→R+​ is continuous, positive off the origin, strictly increasing for this strict order, and unbounded as ∥s∥→∞\|s\|\to\infty∥s∥→∞. Subsystem Σi\Sigma_iΣi​ has an ISS Lyapunov function ViV_iVi​ with gains γij∈K∞∪{0}\gamma_{ij}\in\mathcal K_\infty\cup\{0\}γij​∈K∞​∪{0}, γiu∈K∪{0}\gamma_{iu}\in\mathcal K\cup\{0\}γiu​∈K∪{0} and MAF μi\mu_iμi​ on R+n+1\mathbb R^{n+1}_+R+n+1​ if, wherever ViV_iVi​ is differentiable,

Vi(xi)≥μi(γi1(V1(x1)),…,γin(Vn(xn)),γiu(∥u∥)) ⟹ ∇Vi(xi)fi(x,u)≤−αi(∥xi∥).V_i(x_i)\ge\mu_i\big(\gamma_{i1}(V_1(x_1)),\dots,\gamma_{in}(V_n(x_n)),\gamma_{iu}(\|u\|)\big)\ \Longrightarrow\ \nabla V_i(x_i)f_i(x,u)\le-\alpha_i(\|x_i\|).Vi​(xi​)≥μi​(γi1​(V1​(x1​)),…,γin​(Vn​(xn​)),γiu​(∥u∥)) ⟹ ∇Vi​(xi​)fi​(x,u)≤−αi​(∥xi​∥).

The diagonal gains vanish, γii≡0\gamma_{ii}\equiv0γii​≡0. The gain operators are

Γ‾μ(s,r)i=μi(γi1(s1),…,γin(sn),γiu(r)),Γμ(s)=Γ‾μ(s,0).\overline\Gamma_\mu(s,r)_i=\mu_i\big(\gamma_{i1}(s_1),\dots,\gamma_{in}(s_n),\gamma_{iu}(r)\big),\qquad\Gamma_\mu(s)=\overline\Gamma_\mu(s,0).Γμ​(s,r)i​=μi​(γi1​(s1​),…,γin​(sn​),γiu​(r)),Γμ​(s)=Γμ​(s,0).

An Ω-path with respect to Γμ\Gamma_\muΓμ​ is a continuous σ:R+→R+n\sigma:\mathbb R_+\to\mathbb R^n_+σ:R+​→R+n​ with every σi∈K∞\sigma_i\in\mathcal K_\inftyσi​∈K∞​, such that each σi−1\sigma_i^{-1}σi−1​ is locally Lipschitz on (0,∞)(0,\infty)(0,∞), its derivative lies in [c,C][c,C][c,C], 0<c<C0<c<C0<c<C, at its points of differentiability in any compact K⊂(0,∞)K\subset(0,\infty)K⊂(0,∞) (constants depending on KKK only), and Γμ(σ(r))<σ(r)\Gamma_\mu(\sigma(r))<\sigma(r)Γμ​(σ(r))<σ(r) for all r>0r>0r>0.

Formalization targets

Goal: Theorem 5.3

Assume each ViV_iVi​ is an ISS Lyapunov function for Σi\Sigma_iΣi​ with gains Γ\GammaΓ, γiu\gamma_{iu}γiu​ and MAFs μi\mu_iμi​; σ\sigmaσ is an Ω-path with respect to Γμ\Gamma_\muΓμ​; φ∈K∞\varphi\in\mathcal K_\inftyφ∈K∞​ satisfies

Γ‾μ(σ(r),φ(r))<σ(r)∀r>0;\overline\Gamma_\mu(\sigma(r),\varphi(r))<\sigma(r)\qquad\forall r>0;Γμ​(σ(r),φ(r))<σ(r)∀r>0;

and each fif_ifi​ is continuous. Then

V(x)=max⁡i=1,…,nσi−1(Vi(xi))V(x)=\max_{i=1,\dots,n}\sigma_i^{-1}(V_i(x_i))V(x)=i=1,…,nmax​σi−1​(Vi​(xi​))

is an ISS Lyapunov function for the network, with gain φ−1\varphi^{-1}φ−1:

V(x)≥φ−1(∥u∥) ⟹ ∇V(x)f(x,u)≤−α(∥x∥)V(x)\ge\varphi^{-1}(\|u\|)\ \Longrightarrow\ \nabla V(x)f(x,u)\le-\alpha(\|x\|)V(x)≥φ−1(∥u∥) ⟹ ∇V(x)f(x,u)≤−α(∥x∥)

for a positive definite α\alphaα. The rate α\alphaα is existential and is not fixed by the statement.

Milestones

The milestones follow the proof on pp. 14–15:

  1. VVV is a Lyapunov function candidate.
  2. The maximum rule (5.7) for Clarke generalized gradients.
  3. The chain of inequalities showing that the subsystem trigger holds strictly at every active index.
  4. The Clarke-gradient form (5.8) of the subsystem decrease.
  5. The chain rule for σi−1∘Vi\sigma_i^{-1}\circ V_iσi−1​∘Vi​, with multipliers bounded away from zero.
  6. Positivity of the rate: active blocks on a sphere stay away from the origin.
  7. The uniform decrease (5.9).

Significance

The result. Theorem 5.3 converts a small-gain condition into an explicit Lyapunov function for the network. Combined with the converse ISS Lyapunov theorem, it gives ISS of the interconnection, and with zero input it gives global asymptotic stability. It covers additive, maximum-type and multiplicative aggregation of gains, and it handles nnn subsystems without iterating a two-system result. A second main result of the paper (Theorem 5.2, a separate mission) supplies the Ω-path from the condition Γμ≱id\Gamma_\mu\not\ge\mathrm{id}Γμ​≥id. Together they reduce the stability of a network to a property of its gain operator.

Formalizing it. The result is proved on paper. As far as we know, no ISS notion, small-gain theorem or monotone aggregation framework has been machine-checked in Lean. This mission produces a Lean statement of the construction, and of its nonsmooth-analysis steps, against which a complete proof can be checked. It also corrects a misprint in the theorem's implication (see Formalization scope).

Difficulty

The function VVV is a maximum of rescaled functions and is not differentiable on the set where two indices are active, even when every ViV_iVi​ is smooth. The subsystem hypotheses only control derivatives at points where the corresponding ViV_iVi​ is differentiable. At a point where VVV is differentiable, the active ViV_iVi​ may not be. So the obvious argument — differentiate the active branch and apply (2.7) — fails, and the decrease must be transported through generalized gradients. A second obstacle is uniformity: the rate α\alphaα must depend on ∥x∥\|x\|∥x∥ alone. This requires the lower derivative bound in the Ω-path definition and a compactness argument on spheres. Dropping the lower bound breaks the theorem, because σi−1\sigma_i^{-1}σi−1​ could flatten and remove the decrease.

Formalization scope

Blocks are EuclideanSpace ℝ (Fin (N i)). The network state is the L2L^2L2 product PiLp 2 (the Euclidean norm, not the sup norm), and the input is EuclideanSpace ℝ (Fin M). Subsystems are indexed by Fin n (0-based) with n≥1n\ge1n≥1. Gains, MAFs, Ω-paths and rates live on ℝ≥0. Lyapunov functions are real-valued with an explicit nonnegativity clause. The strict order on R+n\mathbb R^n_+R+n​ is a named predicate, not Lean's Pi <. The inverses σi−1\sigma_i^{-1}σi−1​ and φ−1\varphi^{-1}φ−1 are explicit arguments with both compositions the identity. Every derivative is guarded by a differentiability hypothesis. Clarke's generalized gradient (2.5) is the published ClarkeGradients.Shared.generalizedGradient on the blocks, and the same definition restated on a general Hilbert space for RN\mathbb R^NRN and R\mathbb RR.

Implicit hypotheses made explicit:

  • Continuity of every fif_ifi​. It is the regularity behind the equivalence of the derivative form (2.4) and the Clarke form (2.6) of the decrease condition, which the proof uses.
  • γii≡0\gamma_{ii}\equiv0γii​≡0. The paper's convention.
  • Compatibility of Γ\GammaΓ and μ\muμ. Remark 2.6, the standing assumption from p. 8 on; it imposes nothing on a zero row of Γ\GammaΓ.

Corrected statement. The printed implication (5.5) has the trigger V(x)≥max⁡iφ−1(γiu(∥u∥))V(x)\ge\max_i\varphi^{-1}(\gamma_{iu}(\|u\|))V(x)≥maxi​φ−1(γiu​(∥u∥)). With Γ‾μ\overline\Gamma_\muΓμ​ as defined in (2.9), and as the paper's corollaries use it, that implication is false. A counterexample is one subsystem x˙=−x+u/6\dot x=-x+u/6x˙=−x+u/6 with V1=∣x∣V_1=|x|V1​=∣x∣, γ1u(s)=s/10\gamma_{1u}(s)=s/10γ1u​(s)=s/10, μ1(a,b)=a+2b\mu_1(a,b)=a+2bμ1​(a,b)=a+2b and σ=φ=id\sigma=\varphi=\mathrm{id}σ=φ=id, at x=1x=1x=1, u=10u=10u=10. The proof's chain of inequalities writes φ(r)\varphi(r)φ(r) where (2.9) gives γiu(φ(r))\gamma_{iu}(\varphi(r))γiu​(φ(r)). The goal keeps (2.9) and uses the trigger V(x)≥φ−1(∥u∥)V(x)\ge\varphi^{-1}(\|u\|)V(x)≥φ−1(∥u∥), under which the proof closes.

The hypotheses are jointly satisfiable. An example is n=2n=2n=2 with Vi(xi)=∥xi∥V_i(x_i)=\|x_i\|Vi​(xi​)=∥xi​∥, μi=max⁡\mu_i=\maxμi​=max, γ12=γ21=s/4\gamma_{12}=\gamma_{21}=s/4γ12​=γ21​=s/4, γiu=s/2\gamma_{iu}=s/2γiu​=s/2, σ(r)=(r,r)\sigma(r)=(r,r)σ(r)=(r,r), φ=id\varphi=\mathrm{id}φ=id and dynamics fi=−xif_i=-x_ifi​=−xi​. The conclusion is a decrease inequality at the points of differentiability of VVV for an existential positive definite rate, so it cannot be met by a vacuous choice: α\alphaα must be positive away from zero. Trajectory-level ISS (Theorem 2.3, cited by the paper) and the corollaries that conclude ISS are out of scope.

Reusable infrastructure: comparison classes, monotone aggregation functions, gain operators and Ω-paths (shared with the Ω-path mission), and the maximum and chain rules for Clarke gradients. Proofs of the nonsmooth calculus milestones are welcome independently of the goal.

Selected references

  • S. N. Dashkovskiy, B. S. Rüffer, F. R. Wirth, Small Gain Theorems for Large Scale Systems and Construction of ISS Lyapunov Functions, SIAM J. Control Optim. 48(6), 2010; preprint arXiv:0901.1842v2. https://arxiv.org/abs/0901.1842
  • S. Dashkovskiy, B. S. Rüffer, F. R. Wirth, An ISS small gain theorem for general networks, Math. Control Signals Systems 19, 2007. https://doi.org/10.1007/s00498-007-0014-8
  • Z.-P. Jiang, A. R. Teel, L. Praly, Small-gain theorem for ISS systems and applications, Math. Control Signals Systems 7, 1994. https://doi.org/10.1007/BF01211469
  • Z.-P. Jiang, I. M. Y. Mareels, Y. Wang, A Lyapunov formulation of the nonlinear small-gain theorem for interconnected ISS systems, Automatica 32(8), 1996. https://doi.org/10.1016/0005-1098(96)00051-9
  • E. D. Sontag, Smooth stabilization implies coprime factorization, IEEE Trans. Automat. Control 34(4), 1989. https://doi.org/10.1109/9.28018
  • F. H. Clarke, Optimization and Nonsmooth Analysis, Wiley, 1983. https://doi.org/10.1137/1.9781611971309
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Quantitative Stability in Stochastic Programming: The Method of Probability Metrics 2: Linear Two-Stage Programs Are Lipschitz Stable in the Fortet–Mourier Metric ζ₂Research Paper

Why stability of two-stage programs matters

A linear two-stage stochastic program with fixed recourse chooses a here-and-now decision xxx before a random vector ξ\xiξ is observed, and pays a recourse cost afterwards. It is the basic model of stochastic programming, used in capacity planning, energy and supply-chain models. In practice the distribution μ\muμ of ξ\xiξ is never known exactly: it is estimated from data, replaced by a discrete scenario approximation, or perturbed for robustness. The question is how much the optimal value and the optimal decisions can move when μ\muμ is replaced by a nearby ν\nuν, and in which distance between probability measures "nearby" should be measured.

Rachev and Römisch (Math. Oper. Res. 27(4), 2002, doi:10.1287/moor.27.4.792.304; the mission cites the authors' preprint from edoc.hu-berlin.de) answer this with the method of probability metrics: they derive from the structure of the integrand a canonical distance on measures for each class of models. For linear two-stage programs the canonical distance is the Fortet–Mourier metric of order 2.

Timeline. Robinson and Wets (1987) studied qualitative stability of two-stage programs with respect to weak convergence of measures. Walkup and Wets (1969) had earlier established the piecewise-bilinear structure of the second-stage value function used here. Römisch and Schultz (1991) proved a quantitative stability result for two-stage programs with complete recourse in the Wasserstein metric W2W_2W2​. The present paper (published 2002) replaces complete recourse by relatively complete recourse plus dual feasibility, and W2W_2W2​ by the metric ζ2\zeta_2ζ2​, which it bounds by a multiple of W2W_2W2​ (p. 13).

Setting

Let X⊆RmX\subseteq\mathbb R^mX⊆Rm be a nonempty polyhedron and Ξ⊆Rs\Xi\subseteq\mathbb R^sΞ⊆Rs a polyhedron. Fix c∈Rmc\in\mathbb R^mc∈Rm, an (r,m‾)(r,\overline m)(r,m)-matrix WWW, and data q(ξ)∈Rm‾q(\xi)\in\mathbb R^{\overline m}q(ξ)∈Rm, h(ξ)∈Rrh(\xi)\in\mathbb R^rh(ξ)∈Rr and an (r,m)(r,m)(r,m)-matrix T(ξ)T(\xi)T(ξ) depending affine linearly on ξ\xiξ. The second-stage value is

Φ(u,t)=inf⁡{uy: Wy=t, y≥0},\Phi(u,t)=\inf\{uy:\ Wy=t,\ y\ge0\},Φ(u,t)=inf{uy: Wy=t, y≥0},

with pos⁡W={Wy:y≥0}\operatorname{pos}W=\{Wy:y\ge0\}posW={Wy:y≥0} and D={u:{z:W′z≤u}≠∅}D=\{u:\{z:W'z\le u\}\ne\emptyset\}D={u:{z:W′z≤u}=∅}. The integrand is f0(ξ,x)=cx+Φ(q(ξ),h(ξ)−T(ξ)x)f_0(\xi,x)=cx+\Phi(q(\xi),h(\xi)-T(\xi)x)f0​(ξ,x)=cx+Φ(q(ξ),h(ξ)−T(ξ)x) when h(ξ)−T(ξ)x∈pos⁡Wh(\xi)-T(\xi)x\in\operatorname{pos}Wh(ξ)−T(ξ)x∈posW and q(ξ)∈Dq(\xi)\in Dq(ξ)∈D, and +∞+\infty+∞ otherwise. For a Borel probability measure ν\nuν on Ξ\XiΞ the problem is

min⁡{∫Ξf0(ξ,x) ν(dξ):x∈X},\min\Big\{\int_\Xi f_0(\xi,x)\,\nu(d\xi):x\in X\Big\},min{∫Ξ​f0​(ξ,x)ν(dξ):x∈X},

with optimal value v(ν)v(\nu)v(ν) and solution set S(ν)S(\nu)S(ν). Two assumptions are made: (A1) h(ξ)−T(ξ)x∈pos⁡Wh(\xi)-T(\xi)x\in\operatorname{pos}Wh(ξ)−T(ξ)x∈posW and q(ξ)∈Dq(\xi)\in Dq(ξ)∈D for all (ξ,x)∈Ξ×X(\xi,x)\in\Xi\times X(ξ,x)∈Ξ×X; (A2) μ\muμ has a finite second moment.

The Fortet–Mourier metric ζ2\zeta_2ζ2​ on P2(Ξ)\mathcal P_2(\Xi)P2​(Ξ), the probability measures on Ξ\XiΞ with finite second moment, is

ζ2(μ,ν)=sup⁡f∈F2(Ξ)∣∫Ξf dμ−∫Ξf dν∣,F2(Ξ)={f:∣f(ξ)−f(ξ~)∣≤max⁡{1,∥ξ∥,∥ξ~∥}∥ξ−ξ~∥}.\zeta_2(\mu,\nu)=\sup_{f\in\mathcal F_2(\Xi)}\Big|\int_\Xi f\,d\mu-\int_\Xi f\,d\nu\Big|,\quad \mathcal F_2(\Xi)=\{f:|f(\xi)-f(\tilde\xi)|\le\max\{1,\|\xi\|,\|\tilde\xi\|\}\|\xi-\tilde\xi\|\}.ζ2​(μ,ν)=f∈F2​(Ξ)sup​​∫Ξ​fdμ−∫Ξ​fdν​,F2​(Ξ)={f:∣f(ξ)−f(ξ~​)∣≤max{1,∥ξ∥,∥ξ~​∥}∥ξ−ξ~​∥}.

For an open bounded U⊇S(μ)\mathcal U\supseteq S(\mu)U⊇S(μ), the growth function is ψ(τ)=inf⁡{∫Ξf0(ξ,x) μ(dξ)−v(μ):d(x,S(μ))≥τ, x∈X∩cl⁡U}\psi(\tau)=\inf\{\int_\Xi f_0(\xi,x)\,\mu(d\xi)-v(\mu): d(x,S(\mu))\ge\tau,\ x\in X\cap\operatorname{cl}\mathcal U\}ψ(τ)=inf{∫Ξ​f0​(ξ,x)μ(dξ)−v(μ):d(x,S(μ))≥τ, x∈X∩clU}, and Ψ(η)=η+ψ−1(2η)\Psi(\eta)=\eta+\psi^{-1}(2\eta)Ψ(η)=η+ψ−1(2η) with ψ−1(t)=sup⁡{τ≥0:ψ(τ)≤t}\psi^{-1}(t)=\sup\{\tau\ge0:\psi(\tau)\le t\}ψ−1(t)=sup{τ≥0:ψ(τ)≤t}.

Formalization targets

Goal: Theorem 3.3 (p. 13)

Under (A1), (A2), S(μ)≠∅S(\mu)\ne\emptysetS(μ)=∅ and U\mathcal UU an open bounded neighbourhood of S(μ)S(\mu)S(μ), there are L>0L>0L>0 and δ>0\delta>0δ>0 such that for every ν∈P2(Ξ)\nu\in\mathcal P_2(\Xi)ν∈P2​(Ξ) with ζ2(μ,ν)<δ\zeta_2(\mu,\nu)<\deltaζ2​(μ,ν)<δ:

∣v(μ)−v(ν)∣≤L ζ2(μ,ν),∅≠S(ν)⊆S(μ)+Ψ(L ζ2(μ,ν)) B.|v(\mu)-v(\nu)|\le L\,\zeta_2(\mu,\nu),\qquad \emptyset\ne S(\nu)\subseteq S(\mu)+\Psi(L\,\zeta_2(\mu,\nu))\,\mathbb B.∣v(μ)−v(ν)∣≤Lζ2​(μ,ν),∅=S(ν)⊆S(μ)+Ψ(Lζ2​(μ,ν))B.

The constants are existential, so the goal does not depend on any particular estimate of them.

Milestones

  1. Lemma 3.1 (p. 11): Φ\PhiΦ is finite and continuous on the polyhedral cone D×pos⁡WD\times\operatorname{pos}WD×posW, piecewise of the form Cju⋅tC_ju\cdot tCj​u⋅t on finitely many polyhedral cones with disjoint interiors, convex in ttt and concave in uuu.
  2. Proposition 3.2 (p. 11): f0f_0f0​ is a normal convex integrand, and for ∥x∥≤r\|x\|\le r∥x∥≤r it satisfies ∣f0(ξ,x)−f0(ξ~,x)∣≤Lrmax⁡{1,∥ξ∥,∥ξ~∥}∥ξ−ξ~∥|f_0(\xi,x)-f_0(\tilde\xi,x)|\le Lr\max\{1,\|\xi\|,\|\tilde\xi\|\}\|\xi-\tilde\xi\|∣f0​(ξ,x)−f0​(ξ~​,x)∣≤Lrmax{1,∥ξ∥,∥ξ~​∥}∥ξ−ξ~​∥, a Lipschitz bound in xxx with factor L^max⁡{1,∥ξ∥2}\hat L\max\{1,\|\xi\|^2\}L^max{1,∥ξ∥2}, and ∣f0(ξ,x)∣≤Krmax⁡{1,∥ξ∥2}|f_0(\xi,x)|\le Kr\max\{1,\|\xi\|^2\}∣f0​(ξ,x)∣≤Krmax{1,∥ξ∥2}.
  3. PFU⊇P2(Ξ)\mathcal P_{\mathcal F_{\mathcal U}}\supseteq\mathcal P_2(\Xi)PFU​​⊇P2​(Ξ) (p. 13): every measure with finite second moment satisfies the integrability conditions of the general theory.
  4. Corollary 2.8 (p. 10): the general Lipschitz stability theorem in the metric ζg\zeta_gζg​ for convex models whose integrands lie, up to a factor LLL, in the class Fg\mathcal F_gFg​.

Significance

The theorem says that, under the two natural well-posedness conditions of linear recourse models, optimal values are Lipschitz continuous and solution sets move by at most Ψ(Lζ2)\Psi(L\zeta_2)Ψ(Lζ2​), where ζ2\zeta_2ζ2​ only sees test functions with the local Lipschitz growth of the integrand. Since ζ2≤(1+∫∥ξ∥2dμ+∫∥ξ∥2dν)1/2W2\zeta_2\le(1+\int\|\xi\|^2d\mu+\int\|\xi\|^2d\nu)^{1/2}W_2ζ2​≤(1+∫∥ξ∥2dμ+∫∥ξ∥2dν)1/2W2​, the result contains the earlier W2W_2W2​ stability theorem.

The results are proved in the paper, except Lemma 3.1, which it cites from Walkup and Wets (1969). None of them is formalized in Mathlib or on Prove2Me. A formalization would provide a checked model of the two-stage recourse function, the Fortet–Mourier metrics, and an end-to-end quantitative stability theorem for stochastic programs, none of which exist in Mathlib.

Difficulty

The obvious argument bounds ∣v(μ)−v(ν)∣|v(\mu)-v(\nu)|∣v(μ)−v(ν)∣ by sup⁡x∣∫f0(⋅,x) d(μ−ν)∣\sup_x|\int f_0(\cdot,x)\,d(\mu-\nu)|supx​∣∫f0​(⋅,x)d(μ−ν)∣ and then by Lζ2L\zeta_2Lζ2​. Two steps fail. First, the supremum ranges over all of XXX, which may be unbounded, while f0(⋅,x)/Lf_0(\cdot,x)/Lf0​(⋅,x)/L lies in F2\mathcal F_2F2​ only for xxx in a bounded set; the argument must localize to X∩cl⁡UX\cap\operatorname{cl}\mathcal UX∩clU and then show, using convexity, that for ν\nuν close to μ\muμ the localized and global problems coincide. Second, the Lipschitz estimate in ξ\xiξ for f0f_0f0​ requires the piecewise-bilinear structure of Φ\PhiΦ (Lemma 3.1) and a chaining argument across the polyhedral pieces of Ξ\XiΞ; the integrand is not differentiable.

Formalization scope

  • Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). The paper never fixes its norm and all its constants are existential, so the Euclidean norm is a faithful instance. Second-stage vectors u,t,y,zu,t,y,zu,t,y,z are coordinate vectors Fin k → ℝ; index sets are 0-based.
  • A polyhedron is a finite intersection of closed half-spaces. The standing assumptions are: XXX a nonempty polyhedron, Ξ\XiΞ a polyhedron, q,h,Tq,h,Tq,h,T affine maps.
  • A measure in P(Ξ)\mathcal P(\Xi)P(Ξ) is a Borel probability measure on Rs\mathbb R^sRs with ν(Ξc)=0\nu(\Xi^c)=0ν(Ξc)=0; ∫Ξf0(ξ,x) ν(dξ)\int_\Xi f_0(\xi,x)\,\nu(d\xi)∫Ξ​f0​(ξ,x)ν(dξ) is the extended-real integral of the published DupacovaWets.Consistency.expect over ν\nuν restricted to Ξ\XiΞ.
  • Φ\PhiΦ, f0f_0f0​, vvv and ψ\psiψ are extended-real infima (+∞+\infty+∞ over an empty set); "min" in ψ\psiψ is read as an infimum. ζ2\zeta_2ζ2​, ζg\zeta_gζg​, ψ−1\psi^{-1}ψ−1 and Ψ\PsiΨ take values in [0,∞][0,\infty][0,∞], and the distance to a set is the extended distance (+∞+\infty+∞ to ∅\emptyset∅).
  • To rule out trivializations: every value bound states that v(μ)v(\mu)v(μ), v(ν)v(\nu)v(ν) are finite before comparing them, so the extended-real arithmetic ∞−∞\infty-\infty∞−∞ cannot make it vacuous; in ζ2\zeta_2ζ2​ a test function that is not integrable for both measures contributes +∞+\infty+∞, never a junk 000.
  • Disclosed readings: Proposition 3.2 leaves its radius rrr unquantified; it is stated with the constants first and then every r≥1r\ge1r≥1. Lemma 3.1's "pos⁡W×D\operatorname{pos}W\times DposW×D" is read as D×pos⁡WD\times\operatorname{pos}WD×posW, in the order of Φ\PhiΦ's arguments. Corollary 2.8 adds μ,ν∈PFU(Ξ)\mu,\nu\in\mathcal P_{\mathcal F_{\mathcal U}}(\Xi)μ,ν∈PFU​​(Ξ), an assumption of Theorem 2.2 that its proof invokes; Theorem 3.3 needs no such addition, because milestone 3 supplies it.
  • Needed infrastructure: LP duality and the Walkup–Wets decomposition of Φ\PhiΦ; normal integrands and measurability of their infima; integrability under moment conditions; the general stability theorems (Theorems 2.2–2.3 of the paper) for d=0d=0d=0. The definitions of ζp\zeta_pζp​, Fg\mathcal F_gFg​ and normal integrands are reusable well beyond this mission. Contributions toward any milestone, and proofs of the auxiliary facts (for example, that every f∈F2(Ξ)f\in\mathcal F_2(\Xi)f∈F2​(Ξ) is integrable for ν∈P2(Ξ)\nu\in\mathcal P_2(\Xi)ν∈P2​(Ξ)), are welcome.

Selected references

  • S. T. Rachev, W. Römisch, Quantitative stability in stochastic programming: The method of probability metrics, Mathematics of Operations Research 27(4) (2002) 792–818. https://doi.org/10.1287/moor.27.4.792.304 (cited here from the authors' preprint, edoc.hu-berlin.de)
  • D. W. Walkup, R. J-B Wets, Lifting projections of convex polyhedra, Pacific Journal of Mathematics 28 (1969) 465–475 (the paper's [55]).
  • S. M. Robinson, R. J-B Wets, Stability in two-stage stochastic programming, SIAM Journal on Control and Optimization 25 (1987) 1409–1416 (the paper's [37]).
  • W. Römisch, R. Schultz, Stability analysis for stochastic programs, Annals of Operations Research 30 (1991) 241–266 (the paper's [40]).
  • R. T. Rockafellar, R. J-B Wets, Variational Analysis, Springer (the paper's [38]; normal integrands, Chapter 14).
  • S. T. Rachev, Probability Metrics and the Stability of Stochastic Models, Wiley, Chichester 1991 (the paper's [32]).
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 4: Superposed ON/OFF Input Under Fast Growth Converges in C[0,∞) to Fractional Brownian MotionResearch Paper

Why heavy-tailed input matters

Measurements of Ethernet and Internet traffic in the 1990s showed that cumulative traffic is self-similar and long-range dependent: correlations of the input rate decay so slowly that they are not summable, and fluctuations at large time scales do not average out the way Poisson-type models predict (Leland et al. 1994). A widely accepted explanation is that the lengths of individual transmissions (file sizes, session durations) are heavy tailed, with infinite variance. Queueing and capacity-planning calculations then depend on which stochastic process approximates the cumulative input over long horizons.

Two approximations had been proposed: fractional Brownian motion, a Gaussian self-similar process with dependent increments, and α-stable Lévy motion, a heavy-tailed process with independent increments. Mikosch, Resnick, Rootzén and Stegeman (Ann. Appl. Probab. 12 (2002) 23–68) showed that both arise from the same models and that the answer depends on how fast the number of sources grows relative to the time scale. This mission formalizes their Gaussian answer for the superposition of ON/OFF sources: Theorem 4.

  • 1995–1997: Willinger, Taqqu, Sherman and Wilson derive fractional Brownian motion from superposed ON/OFF sources with heavy-tailed periods, as an iterated limit: first the number of sources M→∞M\to\inftyM→∞, then the time scale T→∞T\to\inftyT→∞, and for finite-dimensional distributions only.
  • 1998: Heath, Resnick and Samorodnitsky (Math. Oper. Res. 23) give the exact decay of the covariance of a single stationary ON/OFF source.
  • 2002: Mikosch, Resnick, Rootzén and Stegeman let MMM and TTT grow together and show that fast growth gives fractional Brownian motion as a functional limit in C[0,∞)\mathbb C[0,\infty)C[0,∞), while slow growth gives stable Lévy motion.

The superposed ON/OFF model

A single ON/OFF source alternates between ON-periods, during which it sends work at rate 111, and silent OFF-periods. The ON-periods X1,X2,…X_1,X_2,\dotsX1​,X2​,… are iid with law FonF_{\mathrm{on}}Fon​ and the OFF-periods Yoff,Y1,Y2,…Y_{\mathrm{off}},Y_1,Y_2,\dotsYoff​,Y1​,Y2​,… iid with law FoffF_{\mathrm{off}}Foff​, both on [0,∞)[0,\infty)[0,∞), all independent, with means μon\mu_{\mathrm{on}}μon​, μoff\mu_{\mathrm{off}}μoff​ and μ=μon+μoff\mu=\mu_{\mathrm{on}}+\mu_{\mathrm{off}}μ=μon​+μoff​. The tails are regularly varying: for x>0x>0x>0,

Fˉon(x)=x−αLon(x),Fˉoff(x)=x−αoffLoff(x),1<α<αoff<2,\bar F_{\mathrm{on}}(x)=x^{-\alpha}L_{\mathrm{on}}(x),\qquad \bar F_{\mathrm{off}}(x)=x^{-\alpha_{\mathrm{off}}}L_{\mathrm{off}}(x),\qquad 1<\alpha<\alpha_{\mathrm{off}}<2,Fˉon​(x)=x−αLon​(x),Fˉoff​(x)=x−αoff​Loff​(x),1<α<αoff​<2,

with Lon,LoffL_{\mathrm{on}},L_{\mathrm{off}}Lon​,Loff​ slowly varying (L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0). So both periods have finite mean and infinite variance, and the ON-periods have the heavier tail.

To make the source stationary, a delay T0=B(Xon(0)+Yoff)+(1−B)Yoff(0)T_0=B(X^{(0)}_{\mathrm{on}}+Y_{\mathrm{off}})+(1-B)Y^{(0)}_{\mathrm{off}}T0​=B(Xon(0)​+Yoff​)+(1−B)Yoff(0)​ is used, where BBB is Bernoulli with P(B=1)=μon/μP(B=1)=\mu_{\mathrm{on}}/\muP(B=1)=μon​/μ and Xon(0),Yoff(0)X^{(0)}_{\mathrm{on}},Y^{(0)}_{\mathrm{off}}Xon(0)​,Yoff(0)​ have the integrated-tail laws F(0)(x)=μF−1∫0xFˉ(s) dsF^{(0)}(x)=\mu_F^{-1}\int_0^x\bar F(s)\,dsF(0)(x)=μF−1​∫0x​Fˉ(s)ds. With Tn=T0+∑i=1n(Xi+Yi)T_n=T_0+\sum_{i=1}^n(X_i+Y_i)Tn​=T0​+∑i=1n​(Xi​+Yi​) the source's activity is

Wt=B 1[0,Xon(0))(t)+∑n≥01[Tn,Tn+Xn+1)(t),t≥0,W_t=B\,\mathbf 1_{[0,X^{(0)}_{\mathrm{on}})}(t)+\sum_{n\ge0}\mathbf 1_{[T_n,T_n+X_{n+1})}(t),\qquad t\ge0,Wt​=B1[0,Xon(0)​)​(t)+n≥0∑​1[Tn​,Tn​+Xn+1​)​(t),t≥0,

a stationary process with EWt=μon/μEW_t=\mu_{\mathrm{on}}/\muEWt​=μon​/μ.

The TTT-th model superposes M=M(T)M=M(T)M=M(T) independent copies W(1),…,W(M)W^{(1)},\dots,W^{(M)}W(1),…,W(M), where MMM is integer valued, non-decreasing and M(T)→∞M(T)\to\inftyM(T)→∞. The cumulative input is A(t)=∫0t∑m=1MWs(m) dsA(t)=\int_0^t\sum_{m=1}^MW^{(m)}_s\,dsA(t)=∫0t​∑m=1M​Ws(m)​ds. With the quantile b(t)=(1/Fˉon)←(t)b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)b(t)=(1/Fˉon​)←(t), the fast growth condition is

Condition 2:lim⁡T→∞b(MT)T=∞,\text{Condition 2:}\qquad \lim_{T\to\infty}\frac{b(MT)}{T}=\infty,Condition 2:T→∞lim​Tb(MT)​=∞,

equivalently MTFˉon(T)→∞MT\bar F_{\mathrm{on}}(T)\to\inftyMTFˉon​(T)→∞. The normalisation and limit constants are

dT=[T3−αLon(T)M]1/2,σ02=2μoff2Γ(2−α)/(α−1)μ3Γ(4−α),H=3−α2∈(12,1).d_T=[T^{3-\alpha}L_{\mathrm{on}}(T)M]^{1/2},\qquad \sigma_0^2=\frac{2\mu_{\mathrm{off}}^2\Gamma(2-\alpha)/(\alpha-1)}{\mu^3\Gamma(4-\alpha)},\qquad H=\frac{3-\alpha}{2}\in(\tfrac12,1).dT​=[T3−αLon​(T)M]1/2,σ02​=μ3Γ(4−α)2μoff2​Γ(2−α)/(α−1)​,H=23−α​∈(21​,1).

A standard fractional Brownian motion BHB_HBH​ is a mean-zero Gaussian process on [0,∞)[0,\infty)[0,∞) with continuous paths and Cov(BH(t),BH(s))=12(t2H+s2H−∣t−s∣2H)\mathrm{Cov}(B_H(t),B_H(s))=\tfrac12(t^{2H}+s^{2H}-|t-s|^{2H})Cov(BH​(t),BH​(s))=21​(t2H+s2H−∣t−s∣2H).

Formalization targets

Goal: Theorem 4

If Condition 2 holds, then

A(T⋅)−TMμ−1μon(⋅)dT →d σ0BH(⋅)weakly in C[0,∞).\frac{A(T\cdot)-TM\mu^{-1}\mu_{\mathrm{on}}(\cdot)}{d_T}\ \xrightarrow{d}\ \sigma_0B_H(\cdot)\qquad\text{weakly in }\mathbb C[0,\infty).dT​A(T⋅)−TMμ−1μon​(⋅)​ d​ σ0​BH​(⋅)weakly in C[0,∞).

Intermediate targets

In the order of the paper's argument: the mean EWt=μon/μEW_t=\mu_{\mathrm{on}}/\muEWt​=μon​/μ (p. 27); the covariance decay (2.5) γW(h)∼μoff2(α−1)μ3h−(α−1)Lon(h)\gamma_W(h)\sim\frac{\mu_{\mathrm{off}}^2}{(\alpha-1)\mu^3}h^{-(\alpha-1)}L_{\mathrm{on}}(h)γW​(h)∼(α−1)μ3μoff2​​h−(α−1)Lon​(h); Condition 2 ⇔T=o(dT)\Leftrightarrow T=o(d_T)⇔T=o(dT​) (p. 61); the variance asymptotic (7.1) Var(GT)∼σ02T3−αLon(T)\mathrm{Var}(G_T)\sim\sigma_0^2T^{3-\alpha}L_{\mathrm{on}}(T)Var(GT​)∼σ02​T3−αLon​(T) for GT=∫0T(Wu−EWu) duG_T=\int_0^T(W_u-EW_u)\,duGT​=∫0T​(Wu​−EWu​)du; Lemma 13, the one-dimensional limit dT−1∑mGTt(m)→N(0,σ02t3−α)d_T^{-1}\sum_mG^{(m)}_{Tt}\to N(0,\sigma_0^2t^{3-\alpha})dT−1​∑m​GTt(m)​→N(0,σ02​t3−α); the covariance limit (7.4); and the second-moment bound E∣dT−1∑mGTu(m)∣2≤c u1+εE|d_T^{-1}\sum_mG^{(m)}_{Tu}|^2\le c\,u^{1+\varepsilon}E∣dT−1​∑m​GTu(m)​∣2≤cu1+ε behind tightness (p. 63). (2.5) and (7.1) are cited by the paper from Heath–Resnick–Samorodnitsky and Willinger–Taqqu–Sherman–Wilson; they are stated here as the paper states them.

Significance

Theorem 4 justifies fractional Brownian motion as the model of aggregate traffic from many heavy-tailed sources in a single, simultaneous limit, replacing the iterated limit of earlier work, and it upgrades finite-dimensional convergence to weak convergence of paths. Functionals of the path, such as the supremum of A(Tt)−ctA(Tt)-ctA(Tt)−ct that governs the buffer content of a fluid queue, therefore inherit Gaussian approximations. Together with Theorem 2 it shows that a single growth condition on MMM decides between Gaussian and stable approximations.

The result is proved in the paper; it is not formalized anywhere. A formalization adds a machine-checked statement of the theorem and reusable developments of regularly varying functions, the stationary alternating renewal process, fractional Brownian motion, and convergence in C[0,∞)\mathbb C[0,\infty)C[0,∞).

Difficulty

The obvious route is a central limit theorem for ∑mGTt(m)\sum_{m}G^{(m)}_{Tt}∑m​GTt(m)​, a sum of MMM iid bounded terms; but the number of terms and their distribution change with TTT, so one needs a triangular-array limit theorem whose variance condition rests on the exact asymptotic (7.1). That asymptotic in turn needs the covariance decay (2.5) of a single stationary source, which requires renewal theory for the alternating process with infinite-variance periods. Convergence of finite-dimensional distributions alone does not give the theorem: tightness in C[0,K]\mathbb C[0,K]C[0,K] needs a moment bound on increments that is uniform in TTT for small time lags, which requires Potter-type bounds for the regularly varying function x↦EGx2x\mapsto EG_x^2x↦EGx2​.

Formalization scope

  • Time and models. T→∞T\to\inftyT→∞ along atTop on R\mathbb RR. Each model TTT has its own probability space carrying M(T)M(T)M(T) independent sources; the theorems hold for every such family. Lean's X n, Y n are the paper's Xn+1X_{n+1}Xn+1​, Yn+1Y_{n+1}Yn+1​ and Lean's sources 0,…,M−10,\dots,M-10,…,M−1 are the paper's 1,…,M1,\dots,M1,…,M. Time in the normalised process runs over R≥0\mathbb R_{\ge0}R≥0​.
  • Standing hypotheses. Fon,FoffF_{\mathrm{on}},F_{\mathrm{off}}Fon​,Foff​ are probability measures on [0,∞)[0,\infty)[0,∞) (non-negativity is implicit in "lengths"); (2.1) is stated as "x↦xαFˉ(x)x\mapsto x^{\alpha}\bar F(x)x↦xαFˉ(x) is slowly varying"; 1<α<αoff<21<\alpha<\alpha_{\mathrm{off}}<21<α<αoff​<2; MMM non-decreasing with M→∞M\to\inftyM→∞ (§3.2); Condition 2 where §7 assumes it. No other hypothesis is added.
  • Junk values ruled out. bbb is an infimum over {x>0:tFˉon(x)≤1}\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}{x>0:tFˉon​(x)≤1}, never a division by zero; the series defining WtW_tWt​ has non-negative terms and fails to converge only on a null event; equalities of laws come with measurability. The limit is pinned completely: Gaussian, mean zero, the covariance above with σH=1\sigma_H=1σH​=1 and H=(3−α)/2H=(3-\alpha)/2H=(3−α)/2, continuous paths, multiplied by σ0\sigma_0σ0​. Fidi convergence in place of the functional limit, a free scale in the limit, or a limit identified only by its marginals would each be a different, weaker theorem.
  • Weak convergence is stated in coupling form: for every sequence Tn→∞T_n\to\inftyTn​→∞ there are one probability space, copies YnY_nYn​ with continuous paths of the laws of the normalised processes at TnT_nTn​, and a standard fractional Brownian motion Y′Y'Y′ such that Yn→σ0Y′Y_n\to\sigma_0Y'Yn​→σ0​Y′ uniformly on every [0,K][0,K][0,K] almost surely. On the Polish space C[0,∞)\mathbb C[0,\infty)C[0,∞) this is equivalent to weak convergence.
  • Infrastructure needed: Karamata's theorem and Potter bounds; the stationary alternating renewal process and its covariance asymptotics; a triangular-array central limit theorem; existence of fractional Brownian motion; a moment criterion for tightness in C[0,K]\mathbb C[0,K]C[0,K]. The regular-variation and path-space material is reusable well beyond this mission; contributions of any of these pieces, and of any milestone, are welcome.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1) (2002), 23–68. https://doi.org/10.1214/aoap/1015961155
  • D. Heath, S. Resnick and G. Samorodnitsky, Heavy tails and long range dependence in on/off processes and associated fluid models, Math. Oper. Res. 23 (1998), 145–165. https://doi.org/10.1287/moor.23.1.145
  • W. Willinger, M. S. Taqqu, R. Sherman and D. V. Wilson, Self-similarity through high-variability: statistical analysis of Ethernet LAN traffic at the source level, IEEE/ACM Trans. Networking 5 (1997), 71–86. https://doi.org/10.1109/90.554723
  • W. E. Leland, M. S. Taqqu, W. Willinger and D. V. Wilson, On the self-similar nature of Ethernet traffic (extended version), IEEE/ACM Trans. Networking 2 (1994), 1–15. https://doi.org/10.1109/90.282603
  • N. H. Bingham, C. M. Goldie and J. L. Teugels, Regular Variation, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511721434
  • P. Billingsley, Convergence of Probability Measures, Wiley, 1968 (Theorem 12.3, moment criterion for tightness).
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Stochastic Kriging for Simulation Metamodeling II: The MSE of the Optimal Stochastic Kriging Predictor Exceeds the Kriging MSE by a Positive Definite FormResearch Paper

Motivation

A simulation metamodel is a cheap surrogate for an expensive stochastic simulation: after running the simulation at a few design settings, one predicts the mean response at settings never simulated. Kriging, the interpolation method of geostatistics and of the design and analysis of computer experiments (DACE; Sacks, Welch, Mitchell and Wynn 1989; Santner, Williams and Notz 2003), treats the unknown response surface as a realization of a random field and predicts by the best linear predictor. Kriging was developed for deterministic computer codes, where an observation is the exact response. A stochastic simulation returns the response plus sampling noise, and the noise may be correlated across settings when the experimenter uses common random numbers (CRN).

Ankenman, Nelson and Staum, Stochastic Kriging for Simulation Metamodeling (Proc. 2008 Winter Simulation Conference, pp. 362–370), extend kriging to this setting. The mission formalizes §2 of that paper: the form of the optimal linear predictor, called stochastic kriging, and the formula for its mean squared error, which shows how much the simulation noise costs. The source used throughout is the WSC 2008 proceedings paper, not the later Operations Research 58(2) 2010 article, whose numbering differs.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) and a set of design settings x\mathbf xx. On replication j=1,2,…j=1,2,\dotsj=1,2,… at setting x\mathbf xx the simulation outputs (display (3), with constant trend)

Yj(x)=β0+M(x)+εj(x).\mathcal Y_j(\mathbf x)=\beta_0+\mathsf M(\mathbf x)+\varepsilon_j(\mathbf x).Yj​(x)=β0​+M(x)+εj​(x).

The constant β0\beta_0β0​ is the overall mean. M\mathsf MM is a mean-zero random field, the extrinsic uncertainty imposed by the modeller. εj(x)\varepsilon_j(\mathbf x)εj​(x) is mean-zero sampling noise, the intrinsic uncertainty of the simulation; its variance may depend on x\mathbf xx, and noises at different settings may be correlated (CRN). All of these have finite second moments, and the field is uncorrelated with the noise.

An experiment design runs ni≥1n_i\ge1ni​≥1 replications at each of kkk design points x1,…,xk\mathbf x_1,\dots,\mathbf x_kx1​,…,xk​. The data are the sample means (4)

Yˉ(xi)=1ni∑j=1niYj(xi),Yˉ=(Yˉ(x1),…,Yˉ(xk))⊤,\bar{\mathcal Y}(\mathbf x_i)=\frac1{n_i}\sum_{j=1}^{n_i}\mathcal Y_j(\mathbf x_i),\qquad\bar{\mathcal Y}=(\bar{\mathcal Y}(\mathbf x_1),\dots,\bar{\mathcal Y}(\mathbf x_k))^\top,Yˉ​(xi​)=ni​1​j=1∑ni​​Yj​(xi​),Yˉ​=(Yˉ​(x1​),…,Yˉ​(xk​))⊤,

and the target at a point x0\mathbf x_0x0​ is the noise-free response Y(x0)=β0+M(x0)\mathsf Y(\mathbf x_0)=\beta_0+\mathsf M(\mathbf x_0)Y(x0​)=β0​+M(x0​).

Write ΣM(x,x′)=Cov[M(x),M(x′)]\Sigma_{\mathsf M}(\mathbf x,\mathbf x')=\mathrm{Cov}[\mathsf M(\mathbf x),\mathsf M(\mathbf x')]ΣM​(x,x′)=Cov[M(x),M(x′)]. Then ΣM\Sigma_{\mathsf M}ΣM​ is the k×kk\times kk×k matrix of these covariances at the design points, ΣM(x0,⋅)\Sigma_{\mathsf M}(\mathbf x_0,\cdot)ΣM​(x0​,⋅) is the vector (Cov[M(x0),M(xi)])i(\mathrm{Cov}[\mathsf M(\mathbf x_0),\mathsf M(\mathbf x_i)])_{i}(Cov[M(x0​),M(xi​)])i​, and Σε\Sigma_\varepsilonΣε​ is the k×kk\times kk×k covariance matrix of the averaged noises ∑j=1niεj(xi)/ni\sum_{j=1}^{n_i}\varepsilon_j(\mathbf x_i)/n_i∑j=1ni​​εj​(xi​)/ni​. A linear predictor (5) is λ0+λ⊤Yˉ\lambda_0+\lambda^\top\bar{\mathcal Y}λ0​+λ⊤Yˉ​ with arbitrary weights (λ0,λ)∈R×Rk(\lambda_0,\lambda)\in\mathbb R\times\mathbb R^k(λ0​,λ)∈R×Rk; its mean squared error is E[(λ0+λ⊤Yˉ−Y(x0))2]\mathrm E[(\lambda_0+\lambda^\top\bar{\mathcal Y}-\mathsf Y(\mathbf x_0))^2]E[(λ0​+λ⊤Yˉ​−Y(x0​))2]. The optimal MSE MSE⋆\mathrm{MSE}^\starMSE⋆ is the infimum of this quantity over all weights.

Formalization targets

Goal: display (7)

There is a rule Ξ\XiΞ, assigning a positive definite matrix Ξ(ΣM,Σε)\Xi(\Sigma_{\mathsf M},\Sigma_\varepsilon)Ξ(ΣM​,Σε​) to every pair of positive definite matrices, such that in every model as above with ΣM≻0\Sigma_{\mathsf M}\succ0ΣM​≻0 and Σε≻0\Sigma_\varepsilon\succ0Σε​≻0, and at every x0\mathbf x_0x0​,

MSE⋆=ΣM(x0,x0)−ΣM(x0,⋅)⊤[ΣM+Σε]−1ΣM(x0,⋅)=[ΣM(x0,x0)−ΣM(x0,⋅)⊤ΣM−1ΣM(x0,⋅)]+ΣM(x0,⋅)⊤ Ξ ΣM(x0,⋅).\begin{aligned}\mathrm{MSE}^\star&=\Sigma_{\mathsf M}(\mathbf x_0,\mathbf x_0)-\Sigma_{\mathsf M}(\mathbf x_0,\cdot)^\top[\Sigma_{\mathsf M}+\Sigma_\varepsilon]^{-1}\Sigma_{\mathsf M}(\mathbf x_0,\cdot)\\&=\Big[\Sigma_{\mathsf M}(\mathbf x_0,\mathbf x_0)-\Sigma_{\mathsf M}(\mathbf x_0,\cdot)^\top\Sigma_{\mathsf M}^{-1}\Sigma_{\mathsf M}(\mathbf x_0,\cdot)\Big]+\Sigma_{\mathsf M}(\mathbf x_0,\cdot)^\top\,\Xi\,\Sigma_{\mathsf M}(\mathbf x_0,\cdot).\end{aligned}MSE⋆​=ΣM​(x0​,x0​)−ΣM​(x0​,⋅)⊤[ΣM​+Σε​]−1ΣM​(x0​,⋅)=[ΣM​(x0​,x0​)−ΣM​(x0​,⋅)⊤ΣM−1​ΣM​(x0​,⋅)]+ΣM​(x0​,⋅)⊤ΞΣM​(x0​,⋅).​

The bracket is the usual kriging MSE. The goal also states that MSE⋆\mathrm{MSE}^\starMSE⋆ strictly exceeds it whenever ΣM(x0,⋅)≠0\Sigma_{\mathsf M}(\mathbf x_0,\cdot)\neq0ΣM​(x0​,⋅)=0. The matrix Ξ\XiΞ is existential and depends only on the two covariance matrices, not on x0\mathbf x_0x0​.

Milestone: display (6)

If ΣM+Σε≻0\Sigma_{\mathsf M}+\Sigma_\varepsilon\succ0ΣM​+Σε​≻0, the stochastic kriging predictor

Y^(x0)=β0+ΣM(x0,⋅)⊤[ΣM+Σε]−1(Yˉ−β01k)\widehat{\mathsf Y}(\mathbf x_0)=\beta_0+\Sigma_{\mathsf M}(\mathbf x_0,\cdot)^\top[\Sigma_{\mathsf M}+\Sigma_\varepsilon]^{-1}(\bar{\mathcal Y}-\beta_0\mathbf 1_k)Y(x0​)=β0​+ΣM​(x0​,⋅)⊤[ΣM​+Σε​]−1(Yˉ​−β0​1k​)

is of the form (5), attains the smallest MSE among all predictors of that form, and is the only one that does.

Further items (not milestones)

  • (9)–(10): the two-point example, with closed forms for the predictor and its MSE in terms of τ2\tau^2τ2, r12r_{12}r12​, r0r_0r0​, V\mathsf VV, ρ\rhoρ and nnn.
  • (14): the equicorrelated example, MSE⋆=τ2(1−kr02/(1+(k−1)r+γ/n))\mathrm{MSE}^\star=\tau^2\big(1-k r_0^2/(1+(k-1)r+\gamma/n)\big)MSE⋆=τ2(1−kr02​/(1+(k−1)r+γ/n)).
  • §3, p. 365: under the Gaussian Assumption 1, Y^(x0)=E[Y(x0)∣Yˉ]\widehat{\mathsf Y}(\mathbf x_0)=\mathrm E[\mathsf Y(\mathbf x_0)\mid\bar{\mathcal Y}]Y(x0​)=E[Y(x0​)∣Yˉ​] almost surely.

Significance

Display (7) quantifies the price of simulation noise. With exact observations the best achievable error is the kriging MSE; with noisy observations it is larger by a positive definite form in the cross-covariance vector. Every point x0\mathbf x_0x0​ that is correlated with the design therefore loses accuracy. The two examples make this concrete. In (10) the MSE increases with the intrinsic correlation ρ\rhoρ, which is why the paper concludes that common random numbers, a standard variance-reduction device for comparing systems, do not help prediction. Display (14) is the baseline against which the paper measures the cost of estimating the noise variance. The conditional-expectation statement shows that under Gaussian assumptions stochastic kriging is optimal among all predictors, not only linear ones.

The results are classical in substance: they are the best-linear-prediction formulas of second-order random-field theory, applied to data whose covariance is ΣM+Σε\Sigma_{\mathsf M}+\Sigma_\varepsilonΣM​+Σε​. The paper states them without proof ("we can show"). No machine-checked version exists. Formalizing them yields a reusable, measure-theoretic best-linear-predictor theorem for random vectors defined from a model rather than postulated, together with the Loewner-order fact behind the positive definiteness of Ξ\XiΞ.

Difficulty

The algebra is short; the difficulty is in deriving the second-moment structure from the model, not assuming it. The covariance of Yˉ\bar{\mathcal Y}Yˉ​ must be computed from the sample-mean definition, using bilinearity of covariance over finite sums of square-integrable variables, and shown to equal ΣM+Σε\Sigma_{\mathsf M}+\Sigma_\varepsilonΣM​+Σε​. The cross-covariance with Y(x0)\mathsf Y(\mathbf x_0)Y(x0​) must be shown to equal ΣM(x0,⋅)\Sigma_{\mathsf M}(\mathbf x_0,\cdot)ΣM​(x0​,⋅). The MSE of an arbitrary affine predictor then has to be written as a quadratic in (λ0,λ)(\lambda_0,\lambda)(λ0​,λ), and its infimum identified.

A first idea is to take "a random vector with mean β01\beta_0\mathbf 1β0​1 and covariance Σ\SigmaΣ" as the hypothesis. That proves a different, more abstract statement and leaves the model's content unproved.

For the second line of (7), the positive definiteness of Ξ\XiΞ does not follow from a scalar argument. It is a matrix inequality, (A+B)−1≺A−1(A+B)^{-1}\prec A^{-1}(A+B)−1≺A−1 for A,B≻0A,B\succ0A,B≻0, and it fails without Σε≻0\Sigma_\varepsilon\succ0Σε​≻0: when Σε=0\Sigma_\varepsilon=0Σε​=0 the two lines coincide.

Formalization scope

  • The model. Settings form an arbitrary type X; design points are x : Fin k → X, so the paper's index iii is i.val + 1. Replication j≥1j\ge1j≥1 is index j - 1 of a sequence ε : ℕ → X → Ω → ℝ.
  • Moments and covariances. Field and noise are in L2L^2L2 and have mean zero. Covariances are Mathlib's covariance. The optimal MSE is an infimum over all of R×Rk\mathbb R\times\mathbb R^kR×Rk, with no unbiasedness constraint and no sign constraint.
  • Hypotheses not printed in §2. Three are added and disclosed:
    1. uncorrelatedness of M\mathsf MM and ε\varepsilonε, the second-order content of Assumption 1's "independent of M\mathsf MM", without which the covariance of Yˉ\bar{\mathcal Y}Yˉ​ is not ΣM+Σε\Sigma_{\mathsf M}+\Sigma_\varepsilonΣM​+Σε​;
    2. square integrability;
    3. ΣM≻0\Sigma_{\mathsf M}\succ0ΣM​≻0 and Σε≻0\Sigma_\varepsilon\succ0Σε​≻0 in the goal. Lean's matrix inverse returns 000 for a singular matrix, and Ξ≻0\Xi\succ0Ξ≻0 is false when Σε\Sigma_\varepsilonΣε​ is singular.
  • Generality kept. No Gaussianity, no independence across replications and no "no CRN" restriction is imposed on (6) and (7).
  • Examples. ∣r12∣<1|r_{12}|<1∣r12​∣<1 in (10) and r≤1r\le1r≤1 in (14) are added, since both are correlations.
  • Non-trivializing. A positive semidefinite Ξ\XiΞ, or a Ξ\XiΞ chosen after x0\mathbf x_0x0​, would make the goal trivial or strictly weaker; the statement fixes Ξ\XiΞ as a function of (ΣM,Σε)(\Sigma_{\mathsf M},\Sigma_\varepsilon)(ΣM​,Σε​) before the model and the point.

Infrastructure needed and reusable beyond this mission:

  • covariance of averages of L2L^2L2 random variables;
  • the MSE of an affine predictor as a quadratic form;
  • minimization of a positive definite quadratic;
  • the Loewner antitonicity of the inverse;
  • for the conditional-expectation item, Gaussian conditioning via uncorrelated-hence-independent residuals.

Contributions to any of these are welcome.

Selected references

  • B. Ankenman, B. L. Nelson, J. Staum, Stochastic Kriging for Simulation Metamodeling, Proceedings of the 2008 Winter Simulation Conference, IEEE, pp. 362–370, 2008. http://www.informs-sim.org/wsc08papers/042.pdf
  • B. Ankenman, B. L. Nelson, J. Staum, Stochastic Kriging for Simulation Metamodeling, Operations Research 58(2), 371–382, 2010 (later journal version, not used here). https://doi.org/10.1287/opre.1090.0754
  • J. Sacks, W. J. Welch, T. J. Mitchell, H. P. Wynn, Design and Analysis of Computer Experiments, Statistical Science 4(4), 409–423, 1989. https://doi.org/10.1214/ss/1177012413
  • T. J. Santner, B. J. Williams, W. I. Notz, The Design and Analysis of Computer Experiments, Springer, 2003. https://doi.org/10.1007/978-1-4757-3799-8
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Stochastic Kriging for Simulation Metamodeling I: The Plug-In Stochastic Kriging Predictor Is UnbiasedResearch Paper

Motivation

Stochastic simulation models of queues, supply chains and manufacturing systems are often too slow to run at every input setting of interest. A metamodel fitted to a moderate number of simulation runs then stands in for the simulation, for instance inside an optimization or a sensitivity analysis. Kriging, developed in geostatistics and in the design and analysis of deterministic computer experiments (DACE), predicts an unknown response surface by treating it as a realization of a Gaussian random field. Deterministic kriging interpolates its data exactly, which is wrong for stochastic simulation, where each run returns the response plus sampling noise.

Ankenman, Nelson and Staum's stochastic kriging separates the two sources of uncertainty: the extrinsic uncertainty of the unknown surface and the intrinsic uncertainty of the simulation output. Its optimal predictor requires the intrinsic noise variances, which are never known in practice and are replaced by sample variances computed from the same replications. This mission formalizes the paper's first key result: this plug-in step introduces no prediction bias.

The source is the Winter Simulation Conference 2008 proceedings version of the paper (pp. 362–370). The later Operations Research 58(2) (2010) article numbers its results differently and is not the reference here.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) and design variables x∈Rd\mathbf x\in\mathbb R^dx∈Rd. On replication j=1,2,…j=1,2,\dotsj=1,2,… at setting x\mathbf xx the simulation returns

Yj(x)=β0+M(x)+εj(x),\mathcal Y_j(\mathbf x)=\beta_0+\mathsf M(\mathbf x)+\varepsilon_j(\mathbf x),Yj​(x)=β0​+M(x)+εj​(x),

where β0∈R\beta_0\in\mathbb Rβ0​∈R is a constant trend, M\mathsf MM is a mean-zero random field on Rd\mathbb R^dRd (the unknown surface) and εj(x)\varepsilon_j(\mathbf x)εj​(x) is the noise of replication jjj. The quantity to predict at any point x0\mathbf x_0x0​, simulated or not, is the noise-free response Y(x0)=β0+M(x0)\mathsf Y(\mathbf x_0)=\beta_0+\mathsf M(\mathbf x_0)Y(x0​)=β0​+M(x0​).

An experiment design is a list of pairs (xi,ni)(\mathbf x_i,n_i)(xi​,ni​), i=1,…,ki=1,\dots,ki=1,…,k, with distinct design points xi\mathbf x_ixi​ and nin_ini​ replications at xi\mathbf x_ixi​. The data are summarized by the sample means Yˉ(xi)=1ni∑j=1niYj(xi)\bar{\mathcal Y}(\mathbf x_i)=\frac1{n_i}\sum_{j=1}^{n_i}\mathcal Y_j(\mathbf x_i)Yˉ​(xi​)=ni​1​∑j=1ni​​Yj​(xi​), collected in the vector Yˉ∈Rk\bar{\mathcal Y}\in\mathbb R^kYˉ​∈Rk, and the sample variances

S2(xi)=1ni−1∑j=1ni(Yj(xi)−Yˉ(xi))2.\mathcal S^2(\mathbf x_i)=\frac1{n_i-1}\sum_{j=1}^{n_i}\big(\mathcal Y_j(\mathbf x_i)-\bar{\mathcal Y}(\mathbf x_i)\big)^2 .S2(xi​)=ni​−11​j=1∑ni​​(Yj​(xi​)−Yˉ​(xi​))2.

The extrinsic covariances are the k×kk\times kk×k matrix ΣM=(Cov[M(xh),M(xi)])h,i\Sigma_{\mathsf M}=(\mathrm{Cov}[\mathsf M(\mathbf x_h),\mathsf M(\mathbf x_i)])_{h,i}ΣM​=(Cov[M(xh​),M(xi​)])h,i​ and the vector ΣM(x0,⋅)=(Cov[M(x0),M(xi)])i\Sigma_{\mathsf M}(\mathbf x_0,\cdot)=(\mathrm{Cov}[\mathsf M(\mathbf x_0),\mathsf M(\mathbf x_i)])_{i}ΣM​(x0​,⋅)=(Cov[M(x0​),M(xi​)])i​.

Assumption 1. M\mathsf MM is a stationary Gaussian random field: all its finite-dimensional laws are multivariate normal with mean 000, the covariance is τ2R(x−x′)\tau^2R(\mathbf x-\mathbf x')τ2R(x−x′) with τ2>0\tau^2>0τ2>0 and R(0)=1R(\mathbf 0)=1R(0)=1, and the covariance matrix at finitely many distinct points is positive definite. At each design point the noises ε1(xi),ε2(xi),…\varepsilon_1(\mathbf x_i),\varepsilon_2(\mathbf x_i),\dotsε1​(xi​),ε2​(xi​),… are i.i.d. N(0,V(xi))N(0,\mathsf V(\mathbf x_i))N(0,V(xi​)) with V(xi)>0\mathsf V(\mathbf x_i)>0V(xi​)>0; noises at different design points are independent (no common random numbers); and the whole noise family is independent of M\mathsf MM.

The intrinsic variance at a design point is estimated by V^(xi)=S2(xi)\widehat{\mathsf V}(\mathbf x_i)=\mathcal S^2(\mathbf x_i)V(xi​)=S2(xi​), giving Σ^ε=Diag{V^(x1)/n1,…,V^(xk)/nk}\widehat\Sigma_\varepsilon=\mathrm{Diag}\{\widehat{\mathsf V}(\mathbf x_1)/n_1,\dots,\widehat{\mathsf V}(\mathbf x_k)/n_k\}Σε​=Diag{V(x1​)/n1​,…,V(xk​)/nk​} and the plug-in stochastic kriging predictor

Y^^(x0)=β0+ΣM(x0,⋅)⊤[ΣM+Σ^ε]−1(Yˉ−β01k).(13)\widehat{\widehat{\mathsf Y}}(\mathbf x_0)=\beta_0+\Sigma_{\mathsf M}(\mathbf x_0,\cdot)^\top\big[\Sigma_{\mathsf M}+\widehat\Sigma_\varepsilon\big]^{-1}\big(\bar{\mathcal Y}-\beta_0\mathbf 1_k\big).\tag{13}Y(x0​)=β0​+ΣM​(x0​,⋅)⊤[ΣM​+Σε​]−1(Yˉ​−β0​1k​).(13)

Formalization targets

Goal: Theorem 1 (p. 366)

Under Assumption 1, with ni≥2n_i\ge2ni​≥2 replications at every design point, the prediction error is integrable and

E[Y^^(x0)−Y(x0)]=0.\mathrm E\Big[\widehat{\widehat{\mathsf Y}}(\mathbf x_0)-\mathsf Y(\mathbf x_0)\Big]=0 .E[Y(x0​)−Y(x0​)]=0.

Milestones (p. 365)

  1. Under Assumption 1, (Y(x0),Yˉ(x1),…,Yˉ(xk))(\mathsf Y(\mathbf x_0),\bar{\mathcal Y}(\mathbf x_1),\dots,\bar{\mathcal Y}(\mathbf x_k))(Y(x0​),Yˉ​(x1​),…,Yˉ​(xk​)) is multivariate normal.
  2. Under Assumption 1, S2(xi)\mathcal S^2(\mathbf x_i)S2(xi​) has a scaled chi-squared distribution: (ni−1)S2(xi)/V(xi)∼χni−12(n_i-1)\mathcal S^2(\mathbf x_i)/\mathsf V(\mathbf x_i)\sim\chi^2_{n_i-1}(ni​−1)S2(xi​)/V(xi​)∼χni​−12​.
  3. Under Assumption 1, S2(xi)\mathcal S^2(\mathbf x_i)S2(xi​) is strongly consistent for V(xi)\mathsf V(\mathbf x_i)V(xi​): the sample variance of the first mmm replications converges to V(xi)\mathsf V(\mathbf x_i)V(xi​) almost surely as m→∞m\to\inftym→∞.

Significance

Theorem 1 says that the practitioner's shortcut, estimating the noise variances from the replications and plugging them into the optimal predictor, keeps the predictor unbiased; the cost of not knowing the intrinsic variance is paid entirely in mean squared error. This is what makes the paper's subsequent comparison of the plug-in MSE with the known-variance MSE the right measure of the penalty for estimation.

None of these statements has a machine-checked proof, and Mathlib has neither the chi-squared law of the normal sample variance nor the independence of the normal sample mean and sample variance. A complete development produces these classical facts of normal sampling theory for the first time in Lean, together with a reusable model of noisy observations of a Gaussian random field.

Difficulty

The predictor is a nonlinear function of the data: its weight vector [ΣM+Σ^ε]−1ΣM(x0,⋅)[\Sigma_{\mathsf M}+\widehat\Sigma_\varepsilon]^{-1}\Sigma_{\mathsf M}(\mathbf x_0,\cdot)[ΣM​+Σε​]−1ΣM​(x0​,⋅) is random and depends on the same replications as Yˉ\bar{\mathcal Y}Yˉ​. Linearity of expectation therefore does not apply directly: the obvious argument, which treats the weights as constants, fails, and the dependence between the estimated variances, the sample means and the field has to be controlled exactly. The joint independence structure of Assumption 1 — across replications, across design points, and between noise and field — is load-bearing; a weaker pairwise or pointwise independence does not suffice. Integrability of the error must also be established, since the weights depend on random variances.

Formalization scope

Design points are indexed by Fin k (the paper's iii is i.val + 1) and lie in EuclideanSpace ℝ (Fin d); replication j≥1j\ge1j≥1 of the paper is index j - 1 of a sequence, so sums run over Finset.range. The field is M : EuclideanSpace ℝ (Fin d) → Ω → ℝ with Mathlib's IsGaussianProcess; covariances are ProbabilityTheory.covariance; stationarity is Cov[M(y),M(y′)]=τ2R(y−y′)\mathrm{Cov}[\mathsf M(\mathbf y),\mathsf M(\mathbf y')]=\tau^2R(\mathbf y-\mathbf y')Cov[M(y),M(y′)]=τ2R(y−y′) with R(0)=1R(\mathbf 0)=1R(0)=1. The noise law is HasLaw … (gaussianReal 0 (V (x i))); independence is one iIndepFun over the family indexed by Fin k × ℕ plus one IndepFun between that whole family and the whole field. The variance function is ℝ≥0-valued with V(xi)>0\mathsf V(\mathbf x_i)>0V(xi​)>0 assumed; replication counts satisfy ni≥2n_i\ge2ni​≥2 wherever S2\mathcal S^2S2 appears and ni≥1n_i\ge1ni​≥1 where only means appear. The chi-squared law χν2\chi^2_\nuχν2​ is gammaMeasure (ν/2) (1/2).

The covariance quantities ΣM\Sigma_{\mathsf M}ΣM​ and ΣM(x0,⋅)\Sigma_{\mathsf M}(\mathbf x_0,\cdot)ΣM​(x0​,⋅) in (13) are the true ones; only Σε\Sigma_\varepsilonΣε​ is estimated, and Σ^ε\widehat\Sigma_\varepsilonΣε​ is built from the same replications as Yˉ\bar{\mathcal Y}Yˉ​. A formalization in which Σ^ε\widehat\Sigma_\varepsilonΣε​ is deterministic or independent of the data, in which the matrix ΣM+Σ^ε\Sigma_{\mathsf M}+\widehat\Sigma_\varepsilonΣM​+Σε​ may be singular (Lean's Matrix.inv returns 000 there, reducing the claim to E[M(x0)]=0\mathrm E[\mathsf M(\mathbf x_0)]=0E[M(x0​)]=0), or in which the expectation is asserted without integrability, would trivialize the goal and is ruled out: positive definiteness of ΣM\Sigma_{\mathsf M}ΣM​ at distinct design points is part of Assumption 1, and integrability is part of the conclusion. x0\mathbf x_0x0​ may coincide with a design point.

A complete development needs: the law of linear images of independent Gaussian vectors; independence of the sample mean and the residual vector for i.i.d. normal samples (Cochran's theorem); the chi-squared law of the normal sample variance; the strong law of large numbers for the sample variance; and a measurability and boundedness argument for the random weight vector. The normal-sampling results are reusable well beyond this mission and are welcome as separate contributions.

Selected references

  • B. Ankenman, B. L. Nelson, J. Staum, Stochastic Kriging for Simulation Metamodeling, Proceedings of the 2008 Winter Simulation Conference, IEEE, pp. 362–370, 2008. http://www.informs-sim.org/wsc08papers/042.pdf
  • B. Ankenman, B. L. Nelson, J. Staum, Stochastic Kriging for Simulation Metamodeling, Operations Research 58(2):371–382, 2010. https://doi.org/10.1287/opre.1090.0754
  • T. J. Santner, B. J. Williams, W. I. Notz, The Design and Analysis of Computer Experiments, Springer, 2003. https://doi.org/10.1007/978-1-4757-3799-8
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Dynamic ProgrammingOperations ResearchOptimization+1·Captain: mikedeng1

Negative Dynamic Programming III: If the Actions Are Essentially Finite, Value Iteration from Zero Converges to the Optimal Return and a Stationary Policy Is OptimalResearch Paper

Motivation

A dynamic programming problem in Blackwell's sense describes a controller who observes the state of a system, picks an action, collects a return, and watches the system move at random to a new state, forever. Blackwell treated the discounted case, with a bounded return and a discount factor below one (Blackwell 1965), and the positive bounded case. Strauch's paper (Strauch 1966) studies the third case, the negative case: the return is non-positive and there is no discounting. Equivalently, a non-negative cost is minimized over an infinite horizon. This is the setting of stochastic shortest-path, optimal stopping with costs, and many inventory and search problems in which the total cost may be infinite.

In the negative case two standard tools of the discounted theory break down. An optimal policy need not exist, and the natural algorithm, value iteration from the zero function, need not converge to the optimal return. Strauch's §9 gives a condition on the action sets, essential finiteness, under which both are restored. The introduction (p. 872) summarizes the finite case: "In the negative case, … if A is finite, there is an optimal policy (Section 9)." In the later terminology of Bertsekas and Shreve (1978), Strauch's negative case is their positive-cost model, for which value iteration from zero is known to require such finiteness or compactness conditions.

Setting

The state space SSS and the action space AAA are non-empty Borel sets. The law of motion q(⋅∣s,a)q(\cdot\mid s,a)q(⋅∣s,a) is a probability measure on SSS depending measurably on (s,a)(s,a)(s,a). The return r(s,a,t)r(s,a,t)r(s,a,t), collected when action aaa is taken in state sss and the next state is ttt, is a Borel function with −∞<r≤0-\infty<r\le 0−∞<r≤0 and ∫r(s,a,t) dq(t∣s,a)>−∞\int r(s,a,t)\,dq(t\mid s,a)>-\infty∫r(s,a,t)dq(t∣s,a)>−∞ for every (s,a)(s,a)(s,a).

A policy π=(π1,π2,… )\pi=(\pi_1,\pi_2,\dots)π=(π1​,π2​,…) chooses the nnnth action at random, with a law depending measurably on the whole history (s1,a1,…,sn)(s_1,a_1,\dots,s_n)(s1​,a1​,…,sn​). A Markov policy (f1,f2,… )(f_1,f_2,\dots)(f1​,f2​,…) is a sequence of measurable maps S→AS\to AS→A; the stationary policy f(∞)f^{(\infty)}f(∞) uses one map fff at every stage. The expected return from the initial state sss is

I(π)(s)=∑n=1∞π1q⋯πnq r (s)∈[−∞,0],I(\pi)(s)=\sum_{n=1}^\infty \pi_1q\cdots\pi_nq\,r\,(s)\in[-\infty,0],I(π)(s)=n=1∑∞​π1​q⋯πn​qr(s)∈[−∞,0],

the sum of the expected stage returns. The optimal return is v∗=sup⁡πI(π)v^*=\sup_\pi I(\pi)v∗=supπ​I(π), over all policies, and π∗\pi^*π∗ is optimal if I(π∗)≥v∗I(\pi^*)\ge v^*I(π∗)≥v∗ at every state.

For a measurable f:S→Af:S\to Af:S→A and a non-positive Borel uuu, the operator TTT of fff is

Tu(s)=∫[r(s,f(s),t)+u(t)] dq(t∣s,f(s)),Tu(s)=\int\big[r(s,f(s),t)+u(t)\big]\,dq(t\mid s,f(s)),Tu(s)=∫[r(s,f(s),t)+u(t)]dq(t∣s,f(s)),

and the operator of a Markov policy π∗=(f1,f2,… )\pi^*=(f_1,f_2,\dots)π∗=(f1​,f2​,…) is Uu=sup⁡nTnuUu=\sup_nT_nuUu=supn​Tn​u, with TnT_nTn​ the operator of fnf_nfn​. Value iteration is the sequence Un0U^n0Un0.

Actions aaa and bbb are equivalent at sss if r(s,a,⋅)=r(s,b,⋅)r(s,a,\cdot)=r(s,b,\cdot)r(s,a,⋅)=r(s,b,⋅) and q(⋅∣s,a)=q(⋅∣s,b)q(\cdot\mid s,a)=q(\cdot\mid s,b)q(⋅∣s,a)=q(⋅∣s,b). AAA is essentially finite by π∗\pi^*π∗ if there is a partition of SSS into Borel sets S1,S2,…S_1,S_2,\dotsS1​,S2​,… such that for s∈Sns\in S_ns∈Sn​ every action is equivalent at sss to one of f1(s),…,fn(s)f_1(s),\dots,f_n(s)f1​(s),…,fn​(s). A finite AAA is essentially finite by any Markov policy whose first ∣A∣|A|∣A∣ rules are the constant rules.

Formalization targets

Goal: Theorem 9.1 (N), p. 887

If AAA is essentially finite by π∗\pi^*π∗ and UUU is the operator of π∗\pi^*π∗, then

Un0(s)→n→∞v∗(s)=sup⁡πI(π)(s)for every s,and∃f: I(f(∞))≥v∗.U^n0(s)\xrightarrow[n\to\infty]{}v^*(s)=\sup_\pi I(\pi)(s)\quad\text{for every } s,\qquad\text{and}\qquad \exists f:\ I(f^{(\infty)})\ge v^*.Un0(s)n→∞​v∗(s)=πsup​I(π)(s)for every s,and∃f: I(f(∞))≥v∗.

Both parts are kept together, as printed. The goal fixes no constants and no rate.

Milestones

  1. Lemma 6.1 (N), p. 880. For every Markov policy π^\hat\piπ^ with operator UUU, lim⁡nUn0\lim_nU^n0limn​Un0 exists and
lim⁡nUn0 ≥ sup⁡π∈G(π^)I(π) ≥ sup⁡f(∞)∈G(π^)I(f(∞)),\lim_nU^n0\ \ge\ \sup_{\pi\in G(\hat\pi)}I(\pi)\ \ge\ \sup_{f^{(\infty)}\in G(\hat\pi)}I(f^{(\infty)}),nlim​Un0 ≥ π∈G(π^)sup​I(π) ≥ f(∞)∈G(π^)sup​I(f(∞)),

where G(π^)G(\hat\pi)G(π^) is the set of π^\hat\piπ^-generated policies (each rule equal to fnf_nfn​ on the nnnth piece of a Borel partition). 2. Proof of Theorem 8.4, p. 887. sup⁡πI(π)=sup⁡{I(π^)∣π^ Markov}\sup_\pi I(\pi)=\sup\{I(\hat\pi)\mid\hat\pi\text{ Markov}\}supπ​I(π)=sup{I(π^)∣π^ Markov} pointwise. 3. Proof of Theorem 9.1, p. 887, first step. Under essential finiteness, Un0U^n0Un0 is non-increasing and I(π)≤v∞:=lim⁡nUn0I(\pi)\le v^\infty:=\lim_nU^n0I(π)≤v∞:=limn​Un0 for every policy π\piπ. 4. Proof of Theorem 9.1, p. 887, second step. Under essential finiteness, Uv∞≥v∞Uv^\infty\ge v^\inftyUv∞≥v∞.

Inside the proof of Theorem 9.1 the paper writes v∗v^*v∗ for lim⁡nUn0\lim_nU^n0limn​Un0; the mission writes v∞v^\inftyv∞ for it and reserves v∗v^*v∗ for sup⁡πI(π)\sup_\pi I(\pi)supπ​I(π).

An optional extra item states the introduction's special case: if AAA is finite, an optimal policy exists (§1, p. 872).

Significance

Theorem 9.1 gives, in the negative case, both a computational and an existential conclusion. Value iteration from zero computes the optimal return, so the optimal total cost of an essentially finite problem is the limit of the optimal finite-horizon costs. An optimal policy exists and can be taken stationary, so the controller needs only a single measurable decision rule. Without a hypothesis of this kind neither conclusion holds in the negative case; Example 6.1 of the paper exhibits a problem where the limit of value iteration, the best return among generated policies, and the best stationary return all differ.

The result is proved in the paper. What the mission adds is a machine-checked statement and, eventually, proof of it on general Borel spaces, with the return allowed to equal −∞-\infty−∞. Blackwell's discounted analogue already has a published statement on Prove2Me (DiscountedDP.Stationary.theorem7b_optimal_stationary), in a bounded-return model; the negative case is a separate statement in a separate model. No formalization of the negative case is known to exist.

Difficulty

The discounted proof rests on the contraction property of UUU in the supremum norm, and in the negative case that property is missing: returns are unbounded below and there is no discount. The obvious argument, "Un0U^n0Un0 decreases to some v∞v^\inftyv∞, and v∞v^\inftyv∞ is the optimal return because finite-horizon play approximates infinite play", fails at the second step. The finite-horizon optimum can stay strictly above the infinite-horizon optimum, because a policy can postpone a cost beyond every fixed horizon; this is exactly the gap Example 6.1 exhibits. Closing it needs the essential finiteness of the actions together with the reduction of arbitrary policies to Markov ones (milestone 2), whose proof in the paper passes through the measurable-selection results of §7–§8.

Formalization scope

  • The state and action spaces are non-empty standard Borel types; "Baire function" means Borel measurable.
  • The law of motion is a Markov kernel; the return is real-valued, non-positive, Borel, and integrable against every q(⋅∣s,a)q(\cdot\mid s,a)q(⋅∣s,a) (the paper's r>−∞r>-\inftyr>−∞ and qr>−∞qr>-\inftyqr>−∞).
  • Returns live in EReal and are computed as minus the lintegral of the loss −r-r−r, which keeps the value −∞-\infty−∞. I(π)I(\pi)I(π) is the sum over stages of the expected stage loss, which equals the paper's integral over futures by monotone convergence.
  • v∗v^*v∗ is the supremum over every randomized history-dependent plan, never over Markov or stationary policies only, and it is not defined through UUU. Defining v∗v^*v∗ as lim⁡nUn0\lim_nU^n0limn​Un0 would make part (a) of the goal hold by unfolding; this trivializing formalization is excluded.
  • Optimality is against every plan, at every state.
  • UUU is the operator of the fixed π∗\pi^*π∗ of the hypothesis, applied from the zero function; convergence is pointwise in EReal.
  • Stages are numbered from 000 in Lean. Essential finiteness is zero-based: Lean's piece nnn is the paper's Sn+1S_{n+1}Sn+1​ and allows the rules f1,…,fn+1f_1,\dots,f_{n+1}f1​,…,fn+1​. The pieces are measurable, pairwise disjoint and cover SSS; empty pieces are allowed, as in the paper.
  • Explicit choices: the existence of lim⁡Un0\lim U^n0limUn0 in Lemma 6.1 is part of the statement; the limit in the steps of Theorem 9.1 is written as the infimum of the non-increasing sequence.
  • Only the negative case is formalized; the paper's discounted and positive parts are not.

Policies, Markov policies, stationary policies and π^\hat\piπ^-generated rules come from the published definitions DiscountedDP.Stationary.Model, .Return and .Operators; the negative model is defined locally because the published Problem has a bounded return and a discount factor below one. A complete development needs the Ionescu-Tulcea construction of the history laws (already encoded as iterated composition products), monotone convergence for kernels, the measurable-selection step behind milestone 2, and a pigeonhole argument over the essentially finite action classes. The model and the Markov-reduction milestone are reusable by the other missions of this series. Proofs of any milestone, and alternative routes to milestone 2, are welcome.

Selected references

  • R. E. Strauch, Negative Dynamic Programming, The Annals of Mathematical Statistics 37(4), 871–890, 1966. https://doi.org/10.1214/aoms/1177699369
  • D. Blackwell, Discounted Dynamic Programming, The Annals of Mathematical Statistics 36(1), 226–235, 1965. https://doi.org/10.1214/aoms/1177700285
  • D. P. Bertsekas and S. E. Shreve, Stochastic Optimal Control: The Discrete-Time Case, Academic Press, 1978. http://web.mit.edu/dimitrib/www/soc.html
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AnalysisOperations ResearchProbability+1·Captain: mikedeng1

Some Useful Functions for Functional Limit Theorems 2: Addition, Supremum and the Reflecting Barrier Preserve J₁ Convergence of Linearly Centered PathsResearch Paper

Motivation

Queueing models often represent work arriving to and leaving a server by a real-valued input path. The resulting workload cannot fall below a barrier. Functional limit theorems describe what happens to such paths under scaling, but a limit for the input path is useful only when it can be carried through the workload transformation. Ward Whitt’s 1980 paper studies several path transformations that occur in stochastic-process limits and states conditions under which their limits can be computed in Skorohod topologies. Section 6 treats the running supremum and a reflecting barrier, including paths with a linear drift that changes with the scaling index. This mission formalizes the three-regime reflection result, Theorem 6.4, and the source results on its dependency path. Whitt (1980)

The result is already proved in the paper. Its formal Lean statement remains an open proof target here. The mission is therefore concerned with formalizing the known theorem, including its exact jump conditions and convergence modes, rather than proposing a new queueing claim. Whitt (1980), pp. 80–81

Setting

A càdlàg path on a real interval TTT is right-continuous and has a limit from the left wherever TTT approaches a time from the left. The collection of such real-valued paths is D(T,R)D(T,\mathbb R)D(T,R). For a compact interval [a,b][a,b][a,b], the J1J_1J1​ distance between xxx and yyy allows an increasing homeomorphism λ\lambdaλ of time and measures the larger of its distance from the identity and the uniform distance between xxx and y∘λy\circ\lambday∘λ. On a general interval, J1J_1J1​ convergence is specified by restrictions to compact subintervals whose endpoints are continuity points of the limit or endpoints of TTT. The paper uses complete separable metric spaces for general path-space results; Section 6 specializes to real-valued paths and intervals with 000 as a closed left endpoint. Whitt (1980), pp. 70, 80

For x∈D(T,R)x\in D(T,\mathbb R)x∈D(T,R) and t∈Tt\in Tt∈T, define the running supremum x↑(t)=sup⁡0≤s≤tx(s)x^{\uparrow}(t)=\sup_{0\le s\le t}x(s)x↑(t)=sup0≤s≤t​x(s) and running infimum x↓(t)=inf⁡0≤s≤tx(s)x^{\downarrow}(t)=\inf_{0\le s\le t}x(s)x↓(t)=inf0≤s≤t​x(s). The reflecting-barrier map is f(x)(t)=x(t)−x↓(t)f(x)(t)=x(t)-x^{\downarrow}(t)f(x)(t)=x(t)−x↓(t). This is the paper’s definition: it subtracts the full running infimum. The identity path is e(t)=te(t)=te(t)=t, and θ\thetaθ denotes the zero path. A path has no positive jumps if x(t)≤x(t−)x(t)\le x(t-)x(t)≤x(t−) for each t>0t>0t>0 in TTT; no negative jumps reverses that inequality. Whitt (1980), pp. 80–81

Formalization targets

The goal is Theorem 6.4. Suppose xn−cne→xx_n-c_ne\to xxn​−cn​e→x in J1J_1J1​ and x(0)=0x(0)=0x(0)=0. Its three conclusions are

cn→c  ⟹  f(xn)→f(x+ce)(J1),cn→+∞  ⟹  f(xn)−cne→x(J1),cn→−∞ and x has no positive jumps  ⟹  f(xn)→θ(U).\begin{aligned} c_n\to c &\implies f(x_n)\to f(x+ce) &&(J_1),\\ c_n\to+\infty &\implies f(x_n)-c_ne\to x &&(J_1),\\ c_n\to-\infty\ \text{and }x\text{ has no positive jumps} &\implies f(x_n)\to\theta &&(U). \end{aligned}cn​→ccn​→+∞cn​→−∞ and x has no positive jumps​⟹f(xn​)→f(x+ce)⟹f(xn​)−cn​e→x⟹f(xn​)→θ​​(J1​),(J1​),(U).​

Here UUU means uniform convergence on every compact subinterval. The goal keeps all three drift regimes together, as the printed theorem does. Its milestones are the finite-partition fact cited from Billingsley, the interval-splitting Lemma 2.2, continuity of addition at limits without shared discontinuities in Theorem 4.1, the running-supremum inequality in Theorem 6.1, the three-regime supremum theorem 6.2, and the paper’s explicit claim that fff is J1J_1J1​-continuous. Whitt (1980), pp. 71, 79–81

Significance

The theorem specifies which output path appears after reflection as the linear centering changes. Finite drift leaves a reflected limit with drift included; large positive drift leaves the centered input limit; large negative drift drives the reflected path uniformly to zero when upward jumps of the limit are excluded. The distinction between J1J_1J1​ and the stronger compact-uniform mode in the last case is part of the result. These statements make the paper’s barrier transformation usable when an input-process limit is already known. Whitt (1980), Theorem 6.4

A completed formal development would establish reusable path-space components: a precise J1J_1J1​ convergence interface for real intervals, a theorem about addition with disjoint discontinuities, and continuity properties of running extrema and reflection. The present Lean items state these results and compile with proof placeholders. No machine-checked proof of these mission theorems is claimed here. The milestone list follows the claims Whitt states or cites, so later proofs can be attached to the same mathematical targets. Whitt (1980), §§2, 4, 6

Difficulty

A uniform estimate alone does not establish a J1J_1J1​ limit: separate paths may converge using different changes of time, and addition can fail when the limiting paths jump together. Whitt’s Theorem 4.1 gives continuity precisely at pairs with disjoint discontinuity sets. In the reflection theorem, a linearly growing drift also changes which extrema matter, and the sign of a jump decides whether the large-drift conclusion can hold. The negative-drift conclusion asks for compact-uniform convergence, which is stronger than merely retaining J1J_1J1​ convergence. These are real constraints on the statement; dropping a jump condition or replacing UUU by J1J_1J1​ changes the theorem. Whitt (1980), pp. 78–81

Formalization scope

Paths are total functions R→S\mathbb R\to SR→S, but only their values on the stated interval count. The Lean definitions require càdlàg membership of both prelimit and limit paths in each J1J_1J1​ convergence claim. A time change on [a,b][a,b][a,b] is strictly increasing, continuous, and onto; this represents the paper’s increasing homeomorphism. Uniform and J1J_1J1​ distances take values in the extended nonnegative reals, so an unbounded supremum cannot silently become zero. Continuity points use continuity within TTT, and the discontinuity set likewise contains only points of TTT. Sequential convergence is used because the paper’s J1J_1J1​ spaces are metrizable. These choices encode the paper’s path-space conventions rather than imposing conditions on values outside TTT. Whitt (1980), §§2, 4, 6

The compact form of Theorem 6.1 uses metric (2.1); the noncompact metric (2.2) is outside this mission’s definition layer. Theorem 4.1 retains the paper’s complete separable metric-space setting and metric compatibility of addition. Its measurability clause is omitted: this mission does not construct the Borel measurable space of D(T,S)D(T,S)D(T,S), and a product measurable structure on all total functions would express a different claim. The source’s f(x)=x−x↓f(x)=x-x^{\downarrow}f(x)=x−x↓ is used on both prelimit and limit paths; it is not replaced by a clipped running infimum. Whitt (1980), pp. 70, 78–81

The definition layer, the addition theorem, the running-extremum results, and the barrier continuity statement are welcome proof targets. The theorem’s centered-path hypothesis remains a genuine J1J_1J1​ convergence assertion, and the jump conditions apply to the limit path only. A vacuous convergence predicate or an independently assumed conclusion would not represent this mission’s goal.

Selected references

  • Ward Whitt, Some Useful Functions for Functional Limit Theorems, Mathematics of Operations Research 5(1), 1980, pp. 67–85. DOI: 10.1287/moor.5.1.67
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Operations ResearchOptimizationTheoretical Computer Science·Captain: mikedeng1

A Scheduling Model for Reduced CPU Energy: For P(s) = s², the Average Rate Heuristic Has Competitive Ratio Between 4 and 8Research Paper

Why processor speed changes the scheduling problem

A processor can save energy by running slowly when work is light, but a deadline may force it to run faster. Yao, Demers, and Shenker formulated this tradeoff as an offline and online scheduling problem for a variable-speed processor in their 1995 FOCS paper. Their Average Rate Heuristic (AVR) uses only each job's arrival, deadline, and required work to set speed. This mission formalizes their quadratic-power analysis: AVR's worst-case energy is at least four and at most eight times the minimum possible energy. The authors prove these bounds in Theorem 2, rather than an exact value.

The question matters when an online scheduler must choose speed before seeing later jobs. Deadline feasibility alone does not measure energy: processing the same number of cycles at twice the speed for half as long can cost more when power grows superlinearly. The paper's model isolates that dependence in a power function P(s)P(s)P(s), so the competitive guarantee measures the energy price of AVR's speed choices. The initial motivation, model, and heuristic are in §§1–4 of the paper.

Jobs, schedules, and the average-rate rule

Fix a nondegenerate time window [t0,t1][t_0,t_1][t0​,t1​]. A finite job instance JJJ assigns each job jjj an arrival time aja_jaj​, deadline bj>ajb_j>a_jbj​>aj​, and nonnegative required work RjR_jRj​ in CPU cycles. Every job window [aj,bj][a_j,b_j][aj​,bj​] lies inside [t0,t1][t_0,t_1][t0​,t1​]. A schedule S=(s,job⁡)S=(s,\operatorname{job})S=(s,job) has nonnegative processor speed s(t)s(t)s(t) and selects at most one job at each time. Speed and job selection are constant between finitely many breakpoints. The schedule is feasible if each job receives its full work inside its own window:

∫ajbjs(t) 1{job⁡(t)=j} dt=Rjfor every j.\int_{a_j}^{b_j}s(t)\,\mathbf 1\{\operatorname{job}(t)=j\}\,dt=R_j \qquad\text{for every }j.∫aj​bj​​s(t)1{job(t)=j}dt=Rj​for every j.

For a power function PPP, its energy is EP(S)=∫t0t1P(s(t)) dtE_P(S)=\int_{t_0}^{t_1}P(s(t))\,dtEP​(S)=∫t0​t1​​P(s(t))dt. An optimal schedule minimizes this quantity among feasible schedules. These definitions follow §2, p. 375. The intensity of an interval [z,z′][z,z'][z,z′] is the total work of jobs whose full windows it contains, divided by z′−zz'-zz′−z. An interval with maximum intensity is critical; Theorem 1 identifies the processor speed on that interval in an optimal schedule §3, p. 375.

Each job's density is dj=Rj/(bj−aj)d_j=R_j/(b_j-a_j)dj​=Rj​/(bj​−aj​), extended as a step function equal to djd_jdj​ on [aj,bj][a_j,b_j][aj​,bj​] and zero elsewhere. AVR runs at speed ∑jdj(t)\sum_j d_j(t)∑j​dj​(t) and chooses the earliest-deadline available job. For quadratic power, its energy is

AVR⁡(J)=∫t0t1(∑jdj(t))2dt.\operatorname{AVR}(J)=\int_{t_0}^{t_1}\left(\sum_jd_j(t)\right)^2dt.AVR(J)=∫t0​t1​​(j∑​dj​(t))2dt.

The competitive ratio is the least upper bound of AVR⁡(J)/OPT⁡(J)\operatorname{AVR}(J)/\operatorname{OPT}(J)AVR(J)/OPT(J) over instances, where OPT⁡(J)\operatorname{OPT}(J)OPT(J) is the least feasible energy §4, p. 376, Eq. (2).

Formalization targets

The goal is the paper's Theorem 2, p. 381:

4≤r≤8(P(s)=s2).4\le r\le 8\qquad(P(s)=s^2).4≤r≤8(P(s)=s2).

The upper bound compares AVR with every feasible schedule. The lower bound says that every constant strictly below four is exceeded by the AVR-to-feasible-energy ratio on some instance. This formulation does not claim that one finite instance attains four.

The milestone path follows the paper: Theorem 1 characterizes optimal speed; Lemma 5.1 reduces to jobs of type A or B; Eq. (5) splits their costs; Lemma 5.2 and Eq. (7) control the A contribution; Lemmas 5.3–5.6 reduce the analysis to canonical instances; Lemma 5.8 supplies a matrix bound; Lemma 5.7 gives FA≤4OPT⁡AF_A\le4\operatorname{OPT}_AFA​≤4OPTA​ and FB≤4OPT⁡BF_B\le4\operatorname{OPT}_BFB​≤4OPTB​; Example 2 approaches the lower constant. These statements and their order come from §5, pp. 378–381. The paper also states a higher-power result, Theorem 3, for real p≥2p\ge2p≥2:

pp≤rp≤2p−1pp.p^p\le r_p\le 2^{p-1}p^p.pp≤rp​≤2p−1pp.

That result is a companion item. The extended abstract leaves its full proof to a longer paper §6, pp. 381–382.

What the bounds provide

The upper bound guarantees that AVR's energy is controlled by a fixed multiple of the offline optimum for every finite job set, even though AVR sets speed from individual job densities. The lower family rules out a guarantee below four for this heuristic. Together they delimit the performance of AVR under quadratic power; they do not give its exact worst-case ratio. The A/B reductions and the tree-induced matrix estimate are useful mathematical interfaces for later analyses of interval-structured schedules.

The paper proves Theorem 2 in the mathematical sense. This mission supplies machine-checkable statements and definitions, with proofs left open for solvers. Closing it requires formal proofs of the reduction steps, the matrix estimate, and the limiting example, plus an explicit connection from the optimal-schedule analysis to comparison with every feasible schedule. No completed Lean proof is claimed here.

The main difficulty

The simple calculation (∑jdj(t))2\left(\sum_j d_j(t)\right)^2(∑j​dj​(t))2 exposes overlap between job windows but does not say how that overlap compares with an optimal schedule. An optimal schedule may run jobs in a different order and may preempt them. The paper therefore changes the instance while preserving the optimal speed profile: it first separates cumulative execution into two types, then reduces to single execution intervals and specially aligned, nested windows. The matrix inequality controls the resulting expression. A pointwise comparison of AVR speed with optimal speed cannot replace these reductions, because an optimal schedule can concentrate work on critical intervals while AVR spreads each job's density across its entire window §5, pp. 377–381.

Formalization scope

Jobs use Fin n, allowing the empty instance. The instance requires t0<t1t_0<t_1t0​<t1​, aj<bja_j<b_jaj​<bj​, containment in the window, and Rj≥0R_j\ge0Rj​≥0. A schedule uses real-valued speed and an optional job label; none denotes no assigned job. Its piecewise-constant requirement is witnessed by finitely many increasing breakpoints. Values at breakpoints are unrestricted by the piecewise-constant clauses, and speed comparisons in the theorems are almost-everywhere statements. Job windows are closed, as printed; endpoints do not affect the integrals. A schedule may have positive speed while no job is assigned, since the source does not equate idleness with zero speed.

Every energy expression is a real interval integral. The schedule conditions ensure the integrands in theorem hypotheses are piecewise constant away from finitely many points. Density denominators are positive. An execution-speed quotient for a zero-work job can have zero denominator, in which case Lean returns zero; such a job contributes no executed work. The goal uses quantified comparisons with feasible schedules rather than a real infimum, and Lemma 5.6 uses all upper bounds on a nonempty canonical family rather than a real supremum. The lower bounds quantify over every smaller constant, avoiding a false attainment claim. These choices guard against default values for empty or unbounded extrema.

Theorem 1's printed convexity hypothesis is strengthened to strict convexity and nondecreasing power on nonnegative speeds: its stated speed uniqueness fails for a linear power function, and a decreasing power function rewards idle speed. This repair is explicit in that item's description. Existence of a quadratic optimum is included as a milestone from the algorithm of §3, although it is not a separately numbered theorem. Example 2 includes the variable exponent e≥1e\ge1e≥1, the limiting ratios at e=1e=1e=1 and e=3/2e=3/2e=3/2, and an eventual upper bound of four across the family. The A-job order resolves exact ties by index. For canonical and tree-induced nesting, intervals that meet only at an endpoint count as disjoint; this admits the paper's displayed four-interval matrix.

The development needs Mathlib's real interval integrals, finite sums, measures of intervals, matrix eigenvalues, and real-power limits. The finite schedule model, canonical-instance data, and tree-induced matrix interface can be reused beyond this particular ratio bound. Contributions may establish these interfaces' elementary properties, the paper's milestone theorems, or independent proofs of the goal, provided they preserve the stated job and schedule classes.

Selected references

  • Frances Yao, Alan Demers, and Scott Shenker, A Scheduling Model for Reduced CPU Energy, Proceedings of the 36th IEEE Symposium on Foundations of Computer Science, 1995, pp. 374–382. DOI 10.1109/SFCS.1995.492493.
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Dynamic ProgrammingMarkov ChainOperations Research·Captain: mikedeng1

Discrete Dynamic Programming with Sensitive Discount Optimality Criteria 2: No Improvement of Order n+1 Implies n-Discount Optimality, Which Rules Out Improvement of Order nResearch Paper

Motivation

A finite Markov decision process is usually solved under one of two criteria: the expected total discounted reward, for a fixed interest rate, or the long-run average reward. Neither is satisfactory when the interest rate is small and not known precisely. Blackwell (Blackwell 1962) showed that some stationary policy is optimal for every discount factor close enough to one, and that the average-reward criterion cannot tell apart policies with the same gain but very different transient rewards. Veinott's 1969 paper interpolates between these two: it introduces a hierarchy of nnn-discount optimality criteria, indexed by n=−1,0,1,…n=-1,0,1,\dotsn=−1,0,1,…, each more selective than the previous, and characterizes the stationary policies that meet each level through the Laurent expansion of the discounted return in the interest rate.

Timeline. Blackwell (1962) introduced the expansion of the discounted return near β=1\beta=1β=1 to first order and the criteria now called −1+-1^+−1+ and ∞+\infty^+∞+ discount optimality. Veinott (1966) gave a policy improvement method for the bias (0+0^+0+) criterion. Miller and Veinott (1969) gave the full Laurent expansion and a policy improvement algorithm for Blackwell optimality in the stochastic case. The present paper (1969) extends this to substochastic transition matrices and to negative interest rates in the transient case, defines the n±n^\pmn± criteria, and proves Theorem 4, the subject of this mission.

Setting

There are finitely many states sss (the paper's 1,…,S1,\dots,S1,…,S); in each state a finite nonempty action set AsA_sAs​. Action aaa in state sss earns r(s,a)∈Rr(s,a)\in\mathbb Rr(s,a)∈R and leads to state ttt with weight p(t∣s,a)≥0p(t\mid s,a)\ge0p(t∣s,a)≥0, where ∑tp(t∣s,a)≤1\sum_t p(t\mid s,a)\le1∑t​p(t∣s,a)≤1 (the remaining mass is the probability of stopping). A decision rule f∈F=×sAsf\in F=\times_s A_sf∈F=×s​As​ picks one action per state; r(f)r(f)r(f) and P(f)P(f)P(f) are its reward vector and substochastic transition matrix, Q(f)=P(f)−IQ(f)=P(f)-IQ(f)=P(f)−I. A policy is a sequence π=(f1,f2,… )\pi=(f_1,f_2,\dots)π=(f1​,f2​,…) of decision rules, f∞=(f,f,… )f^\infty=(f,f,\dots)f∞=(f,f,…) is a stationary policy, and PN(π)=P(f1)⋯P(fN)P^N(\pi)=P(f_1)\cdots P(f_N)PN(π)=P(f1​)⋯P(fN​).

For an interest rate ρ>−1\rho>-1ρ>−1 and β=(1+ρ)−1\beta=(1+\rho)^{-1}β=(1+ρ)−1, the discounted return is

Vρ(π)=∑N=1∞βNPN−1(π) r(fN).V_\rho(\pi)=\sum_{N=1}^{\infty}\beta^N P^{N-1}(\pi)\,r(f_N).Vρ​(π)=N=1∑∞​βNPN−1(π)r(fN​).

For a substochastic PPP, P∗P^*P∗ is the Cesàro limit of its powers and H=(I−P+P∗)−1−P∗H=(I-P+P^*)^{-1}-P^*H=(I−P+P∗)−1−P∗ its deviation matrix.

A policy π∗\pi^*π∗ is n±n^\pmn± discount optimal if, componentwise,

lim inf⁡ρ→0±∣ρ∣−n [Vρ(π∗)−Vρ(π)]≥0for all policies π.\liminf_{\rho\to0\pm}|\rho|^{-n}\,[V_\rho(\pi^*)-V_\rho(\pi)]\ge0\quad\text{for all policies }\pi .ρ→0±liminf​∣ρ∣−n[Vρ​(π∗)−Vρ​(π)]≥0for all policies π.

Dn±D_n^\pmDn±​ is the set of fff with f∞f^\inftyf∞ n±n^\pmn± discount optimal, and D−2=FD_{-2}=FD−2​=F. The sign −-− (interest rate approaching zero from below) is considered only in the transient case, where ∑NP(f)N\sum_N P(f)^N∑N​P(f)N converges for every fff.

The Laurent coefficients of Vρ(f∞)V_\rho(f^\infty)Vρ​(f∞) are y−1±(f)=±P∗(f)r(f)y_{-1}^\pm(f)=\pm P^*(f)r(f)y−1±​(f)=±P∗(f)r(f) and yn±(f)=(∓1)nH(f)n+1r(f)y_n^\pm(f)=(\mp1)^nH(f)^{n+1}r(f)yn±​(f)=(∓1)nH(f)n+1r(f), n≥0n\ge0n≥0; with y−2±=0y_{-2}^\pm=0y−2±​=0 and r0=rr_0=rr0​=r, rn=0r_n=0rn​=0 otherwise, the test quantities are

ψn±(g,f)=rn(g)+Q(g) yn±(f)∓yn−1±(f),n≥−1.\psi_n^\pm(g,f)=r_n(g)+Q(g)\,y_n^\pm(f)\mp y_{n-1}^\pm(f),\qquad n\ge-1 .ψn±​(g,f)=rn​(g)+Q(g)yn±​(f)∓yn−1±​(f),n≥−1.

Ψn±(g,f)\Psi_n^\pm(g,f)Ψn±​(g,f) is the matrix with columns ψ−1±,…,ψn±\psi_{-1}^\pm,\dots,\psi_n^\pmψ−1±​,…,ψn±​, and Gn±(f)={g∈F:Ψn±(g,f)≻0}G_n^\pm(f)=\{g\in F:\Psi_n^\pm(g,f)\succ0\}Gn±​(f)={g∈F:Ψn±​(g,f)≻0}, where C≻0C\succ0C≻0 means that the first nonzero entry of every row of CCC is positive and C≠0C\ne0C=0.

Formalization targets

Goal: Theorem 4

For f∈Ff\in Ff∈F and n=−2,−1,…,S−1n=-2,-1,\dots,S-1n=−2,−1,…,S−1:

Gn+1±(f)=∅ ⟹ f∈Dn±,f∈Dn± ⟹ Gn±(f)=∅.G_{n+1}^\pm(f)=\varnothing\ \Longrightarrow\ f\in D_n^\pm,\qquad f\in D_n^\pm\ \Longrightarrow\ G_n^\pm(f)=\varnothing .Gn+1±​(f)=∅ ⟹ f∈Dn±​,f∈Dn±​ ⟹ Gn±​(f)=∅.

The two halves bracket Dn±D_n^\pmDn±​ between two finitely checkable conditions.

Milestones

In the order the proof uses them: the Cesàro limit and (15); Lemma 5 (the reduced resolvent); Theorem 2 (the Laurent expansion Rρ(Q)=ρ−1P∗+∑n≥0(−ρ)nHn+1R_\rho(Q)=\rho^{-1}P^*+\sum_{n\ge0}(-\rho)^nH^{n+1}Rρ​(Q)=ρ−1P∗+∑n≥0​(−ρ)nHn+1); Lemma 7 (P∗+ρHP^*+\rho HP∗+ρH nonnegative, positive diagonal, nonsingular for small ρ>0\rho>0ρ>0); Theorem 3 (the expansion of Vρ(f∞)V_\rho(f^\infty)Vρ​(f∞)); (30)–(31) (the comparison identity); Lemma 8 (the expansion of the test quantity); Lemma 9 (the coefficient identity); the nonemptiness of D∞±D_\infty^\pmD∞±​; the characterization Dn±={f:Yn±(f)⪰Yn±(g) ∀g}D_n^\pm=\{f: Y_n^\pm(f)\succeq Y_n^\pm(g)\ \forall g\}Dn±​={f:Yn±​(f)⪰Yn±​(g) ∀g}; Theorem 5 (lexicographic improvement).

Significance

Theorem 4 turns a criterion stated through limits over all, possibly non-stationary, policies into a finite test on one-step switches. It is what lets the policy improvement method of Miller and Veinott stop early when only an n±n^\pmn± discount optimal policy is sought, rather than an S±S^\pmS± (Blackwell) optimal one, and it recovers Blackwell's algorithm for −1+-1^+−1+ and Veinott's 1966 algorithm for 0+0^+0+ as the cases n=−1,0n=-1,0n=−1,0. The nnn-discount hierarchy is the standard framework for sensitive optimality in Markov decision processes and underlies the average-overtaking and bias criteria used in later work.

The results are proved in the paper (Theorem 3 and Lemma 8 by reference to Miller–Veinott). None of them is formalized: the platform has the Cesàro limit matrix and the deviation matrix as definitions (from Blackwell 1962), and an open statement of their basic properties for stochastic matrices only. This mission adds the substochastic matrix theory of §3, the Laurent expansion of discounted returns with Veinott's normalization, and the lexicographic characterization of n±n^\pmn± discount optimality.

Difficulty

The definition of Dn±D_n^\pmDn±​ compares f∞f^\inftyf∞ with every policy, and the comparison is a liminf of a scaled difference of infinite series. The obvious route, comparing Laurent coefficients, applies only to stationary policies, whose returns have Laurent expansions; reducing the comparison with arbitrary policies to stationary ones requires the existence of an ∞±\infty^\pm∞± discount optimal stationary policy, which is a separate existence theorem. The second difficulty is that P∗P^*P∗ may be singular or zero and the chain may have several recurrent classes: Lemma 7 is what replaces an analysis of the chain structure in the inductive step of the proof.

Formalization scope

Lean 4 with Mathlib, namespace VeinottSensitiveDP.Sensitive. States form a nonempty Fintype; each state has its own finite nonempty action type A s; policies are sequences ℕ → F with π 0 the paper's f1f_1f1​. All quantities are real. P∗P^*P∗ and HHH are the published limitMatrix and deviationMatrix; their properties for substochastic matrices are milestones, not assumptions. VρV_\rhoVρ​ is a tsum with Veinott's extra factor β\betaβ; every theorem about it carries the hypotheses under which the series converges. The spectral radius is that of the complexified matrix. The sign ±\pm± is a real parameter σ∈{1,−1}\sigma\in\{1,-1\}σ∈{1,−1}, and statements for σ=−1\sigma=-1σ=−1 assume the transient case. The liminf in (27) is encoded as "for every ε>0\varepsilon>0ε>0, eventually ≥−ε\ge-\varepsilon≥−ε", which is the extended-real liminf. Matrices with columns −1,…,n-1,\dots,n−1,…,n are functions of an integer column index read on [−1,n][-1,n][−1,n].

A trivializing formalization would define Dn±D_n^\pmDn±​ by comparison with stationary policies only, or directly as the lexicographic maximizers of Yn±Y_n^\pmYn±​; here Dn±D_n^\pmDn±​ is defined by (27) against all policies, and the lexicographic characterization is a milestone.

Contributions welcome: proofs of the matrix results of §3 (reusable for any work on deviation matrices and Laurent expansions of Markov chains), of the Laurent expansions, and of the existence of ∞±\infty^\pm∞± discount optimal stationary policies.

Selected references

  • A. F. Veinott, Jr., Discrete dynamic programming with sensitive discount optimality criteria, Ann. Math. Statist. 40(5):1635–1660, 1969. https://doi.org/10.1214/aoms/1177697379
  • D. Blackwell, Discrete dynamic programming, Ann. Math. Statist. 33(2):719–726, 1962. https://doi.org/10.1214/aoms/1177704593
  • A. F. Veinott, Jr., On finding optimal policies in discrete dynamic programming with no discounting, Ann. Math. Statist. 37(5):1284–1294, 1966. https://doi.org/10.1214/aoms/1177699272
  • B. L. Miller and A. F. Veinott, Jr., Discrete dynamic programming with a small interest rate, Ann. Math. Statist. 40(2):366–370, 1969. https://doi.org/10.1214/aoms/1177697700
17 thms1 active userReviewed
Dynamic ProgrammingMarkov ChainOperations Research+1·Captain: mikedeng1

Inventory Control in a Fluctuating Demand Environment II: With a Fixed Order Cost, a World-Dependent (r, S) Policy Is Optimal and Lies within Veinott-Type BoundsResearch Paper

Motivation

Demand for many products is not stationary: it rises and falls with the economy, the season, a product's life cycle or a customer's state. Song and Zipkin (1993) (DOI 10.1287/opre.41.2.351) model this by a world-driven demand process: an exogenous Markov chain AAA (the "state of the world") whose current state sets the rate of a Poisson demand stream. The model contains the classical stationary inventory model as the case of one world state, and it is a standard example of a Markov-modulated decision problem in operations research.

For stationary demand with a fixed order cost, optimal (s,S)(s, S)(s,S) policies go back to Scarf (1960) for finite horizons and Iglehart (1963) for the infinite horizon; Veinott (1966) bounded the optimal parameters by quantities computed from the one-period cost alone. This mission formalizes the extension of both results to the fluctuating-demand model (§3.2 of the paper). A companion mission treats the linear order-cost case, in which a world-dependent basestock policy is optimal.

Setting

The world AAA is a continuous-time Markov chain on a countable set III with generator (qij)(q_{ij})(qij​), qi=−qii=∑j≠iqijq_i = -q_{ii} = \sum_{j\neq i} q_{ij}qi​=−qii​=∑j=i​qij​, and bounded rates. While A=iA = iA=i, unit demands arrive at Poisson rate λi\lambda_iλi​; shortages are backlogged. An order arrives after a random lead time LLL, independent of the world and the demand. The inventory position x∈Zx \in \mathbb Zx∈Z is on-hand stock minus backorders plus stock on order.

Costs: a fixed cost Kˉ\bar KKˉ per order and a unit cost cˉ\bar ccˉ, both paid on arrival; a holding cost rate h>0h > 0h>0 and a penalty cost rate p>0p > 0p>0; a discount rate α>0\alpha > 0α>0. With F~L(α)=E[e−αL]\tilde F_L(\alpha) = E[e^{-\alpha L}]F~L​(α)=E[e−αL], the discounted costs are c=cˉF~L(α)c = \bar c\tilde F_L(\alpha)c=cˉF~L​(α) and K=KˉF~L(α)K = \bar K\tilde F_L(\alpha)K=KˉF~L​(α). If DLiD^i_LDLi​ is the demand during a lead time from world state iii and C^(x)=max⁡{−px,hx}\hat C(x) = \max\{-px, hx\}C^(x)=max{−px,hx},

C(i,y)=E[e−αLC^(y−DLi)].C(i, y) = E\big[e^{-\alpha L}\hat C(y - D^i_L)\big].C(i,y)=E[e−αLC^(y−DLi​)].

Uniformization at a rate μ≥sup⁡iqi+sup⁡iλi\mu \ge \sup_i q_i + \sup_i\lambda_iμ≥supi​qi​+supi​λi​ turns the problem into a discrete-time dynamic program with β=1/(μ+α)\beta = 1/(\mu+\alpha)β=1/(μ+α), γ=βμ\gamma = \beta\muγ=βμ and the myopic cost G+(i,y)=(1−γ)cy+βC(i,y)G^+(i, y) = (1-\gamma)cy + \beta C(i, y)G+(i,y)=(1−γ)cy+βC(i,y). For a terminal cost W0W_0W0​ the nnn-stage costs satisfy the recursion (10):

Wn(i,x)=min⁡y≥x{Kδ(y−x)+Gn(i,y)},W_n(i, x) = \min_{y\ge x}\{K\delta(y-x) + G_n(i, y)\},Wn​(i,x)=y≥xmin​{Kδ(y−x)+Gn​(i,y)}, Gn(i,y)=G+(i,y)+βλic+β{λiWn−1(i,y−1)+∑j≠iqijWn−1(j,y)+(μ−λi−qi)Wn−1(i,y)},G_n(i, y) = G^+(i, y) + \beta\lambda_i c + \beta\Big\{\lambda_i W_{n-1}(i, y-1) + \sum_{j\neq i} q_{ij}W_{n-1}(j, y) + (\mu - \lambda_i - q_i)W_{n-1}(i, y)\Big\},Gn​(i,y)=G+(i,y)+βλi​c+β{λi​Wn−1​(i,y−1)+j=i∑​qij​Wn−1​(j,y)+(μ−λi​−qi​)Wn−1​(i,y)},

where δ(z)=1\delta(z) = 1δ(z)=1 if z>0z > 0z>0 and δ(0)=0\delta(0) = 0δ(0)=0. Throughout, Assumption 1, αcˉ<p\alpha\bar c < pαcˉ<p, holds and K>0K > 0K>0. The terminal cost is the optimal cost W∞W_\inftyW∞​ of the linear model (K=0K = 0K=0); its G∞G_\inftyG∞​ is written G0G_0G0​, and y∗(i)y^*(i)y∗(i) is the smallest minimizer of G0(i,⋅)G_0(i, \cdot)G0​(i,⋅).

A function f:Z→Rf : \mathbb Z \to \mathbb Rf:Z→R is KKK-convex (Definition 2) if f(x)−f(x−b)ba+f(x)≤f(x+a)+K\frac{f(x)-f(x-b)}{b}a + f(x) \le f(x+a) + Kbf(x)−f(x−b)​a+f(x)≤f(x+a)+K for all xxx and all integers a,b>0a, b > 0a,b>0. The (r,S)(r, S)(r,S) policy with parameters {(r(i),S(i))}\{(r(i), S(i))\}{(r(i),S(i))} orders up to S(i)S(i)S(i) when x≤r(i)x \le r(i)x≤r(i) and the world is in state iii, and does not order otherwise. With y+(i)y^+(i)y+(i) the smallest minimizer of G+(i,⋅)G^+(i,\cdot)G+(i,⋅) and ymin⁡+=min⁡iy+(i)y^+_{\min} = \min_i y^+(i)ymin+​=mini​y+(i), the paper defines

S+(i)=min⁡{y≥y+(i):G+(i,y)−G+(i,y+(i))>γK},r+(i)=max⁡{y<y+(i):G+(i,y)−G+(i,y+(i))>(1−γ)K},r−(i)=max⁡{y<y∗(i):G0(i,y)−G0(i,y∗(i))>K},r−−(i)=max⁡{y<ymin⁡+:G+(i,y)−G+(i,ymin⁡+)>K}.\begin{aligned} S^+(i) &= \min\{y \ge y^+(i) : G^+(i, y) - G^+(i, y^+(i)) > \gamma K\},\\ r^+(i) &= \max\{y < y^+(i) : G^+(i, y) - G^+(i, y^+(i)) > (1-\gamma)K\},\\ r^-(i) &= \max\{y < y^*(i) : G_0(i, y) - G_0(i, y^*(i)) > K\},\\ r^{--}(i) &= \max\{y < y^+_{\min} : G^+(i, y) - G^+(i, y^+_{\min}) > K\}. \end{aligned}S+(i)r+(i)r−(i)r−−(i)​=min{y≥y+(i):G+(i,y)−G+(i,y+(i))>γK},=max{y<y+(i):G+(i,y)−G+(i,y+(i))>(1−γ)K},=max{y<y∗(i):G0​(i,y)−G0​(i,y∗(i))>K},=max{y<ymin+​:G+(i,y)−G+(i,ymin+​)>K}.​

Formalization targets

Goal: Theorems 5(e) and 6

Let Sn∗(i)S^*_n(i)Sn∗​(i) be the smallest minimizer of Gn(i,⋅)G_n(i,\cdot)Gn​(i,⋅) and rn∗(i)r^*_n(i)rn∗​(i) the largest y<Sn∗(i)y < S^*_n(i)y<Sn∗​(i) with Gn(i,y)>K+Gn(i,Sn∗(i))G_n(i, y) > K + G_n(i, S^*_n(i))Gn​(i,y)>K+Gn​(i,Sn∗​(i)). For every iii the sequence (rn∗(i),Sn∗(i))(r^*_n(i), S^*_n(i))(rn∗​(i),Sn∗​(i)) has limit points; for any choice of limit points (r∗(i),S∗(i))(r^*(i), S^*(i))(r∗(i),S∗(i)), the world-dependent (r,S)(r, S)(r,S) policy with these parameters is optimal for the infinite-horizon discounted problem, and

y∗(i)≤S∗(i)<S+(i),r−−(i)≤r−(i)≤r∗(i)≤r+(i).y^*(i) \le S^*(i) < S^+(i),\qquad r^{--}(i) \le r^-(i) \le r^*(i) \le r^+(i).y∗(i)≤S∗(i)<S+(i),r−−(i)≤r−(i)≤r∗(i)≤r+(i).

Milestones

Lemma 4 (uniform bounds on the iterates); Theorem 3 (KKK-convexity of GnG_nGn​, WnW_nWn​ and optimality of an (r,S)(r, S)(r,S) rule for each nnn-stage problem); Lemmas 5 and 6 (difference comparisons); Theorem 4 (the bounds above for every nnn); Theorem 5(a)–(d) (convergence of WnW_nWn​, GnG_nGn​, the (r,S)(r, S)(r,S) property of limit points, and the optimality equation (2)).

Significance

The result shows that the classical (s,S)(s, S)(s,S) structure survives Markov modulation of demand with an infinite world space and stochastic lead times: a stationary policy whose two parameters depend only on the current world state is optimal over the infinite horizon. The bounds of Theorem 6 locate those parameters in an interval computed from the myopic cost G+G^+G+ and the linear model alone, uniformly in the horizon.

The results are proved in the paper, except that Theorem 5 refers to Iglehart (1963) and Lemma 4 to Song's thesis. To our knowledge none of them has a machine-checked proof. A formalization would also produce reusable machinery: KKK-convexity on the integers, the Scarf-type inductive argument with a countable world state, and the passage from finite-horizon to infinite-horizon optimality for a nonnegative-cost Markov decision process with unbounded costs.

Difficulty

The one-period cost is unbounded in xxx and the world space may be infinite, so the usual contraction argument for discounted dynamic programs does not apply. Convergence of WnW_nWn​ needs the uniform bound of Lemma 4. Optimality of the limit policy needs a separate argument, because a pointwise limit of (r,S)(r, S)(r,S) rules need not exist: the parameter sequences are only known to have limit points. The lower bounds r−r^-r− and r−−r^{--}r−− hold only because the terminal cost is the linear model's optimal cost, which makes the difference comparisons of Lemma 6 possible; the paper notes that Lemma 6 depends on this choice of W0W_0W0​.

Formalization scope

All definitions live in the namespace SongZipkinFluct.FixedCost. Inventory positions and order-up-to levels are integers. The demand law DLiD^i_LDLi​ is defined through uniformization at rate μ\muμ, as an exact series representation of the Markov-modulated Poisson count, and the lead time is a probability law on [0,∞)[0,\infty)[0,∞) independent of the rest. The standing conventions h,p,α>0h, p, \alpha > 0h,p,α>0, cˉ,Kˉ≥0\bar c, \bar K \ge 0cˉ,Kˉ≥0, μ>0\mu > 0μ>0 and μ≥q∗+λ∗\mu \ge q^* + \lambda^*μ≥q∗+λ∗ are hypotheses of the model. Assumption 1 and Kˉ>0\bar K > 0Kˉ>0 are hypotheses of each theorem.

The iterates WnW_nWn​ are defined by the recursion (10), with the minimum written as an infimum over integers y≥xy \ge xy≥x. W∞W_\inftyW∞​ and G∞G_\inftyG∞​ are the suprema over nnn, which are finite and equal the limits by Lemma 4 and Theorem 3. Every minimizer and every extremal integer (y+y^+y+, ymin⁡+y^+_{\min}ymin+​, y∗y^*y∗, Sn∗S^*_nSn∗​, rn∗r^*_nrn∗​, S+S^+S+, r+r^+r+, r−r^-r−, r−−r^{--}r−−) is passed through its defining property, never through sInf/sSup on Z\mathbb ZZ. The goal also asserts that all of them exist, so its hypotheses can be met. A limit point of an integer sequence is a value taken infinitely often.

Optimality is over all deterministic history-dependent feasible policies and from every initial state. Costs are valued in [0,∞][0,\infty][0,∞], and a policy's cost is the supremum of its finite-horizon discounted costs in the uniformized problem (1). Restricting the comparison to (r,S)(r, S)(r,S) or stationary policies would trivialize the goal and is ruled out. KKK-convexity is the integer version of Definition 2, not convexity over Z\mathbb ZZ-scalars.

Welcome contributions: KKK-convexity calculus on Z\mathbb ZZ, convergence of the uniformized demand series, Lemma 4, and an Iglehart-type limit argument for countable-state Markov decision processes with nonnegative costs.

Selected references

  • J.-S. Song and P. Zipkin, Inventory Control in a Fluctuating Demand Environment, Operations Research 41(2):351–370, 1993. https://doi.org/10.1287/opre.41.2.351
  • H. Scarf, The Optimality of (S, s) Policies in the Dynamic Inventory Problem, in Mathematical Methods in the Social Sciences, Stanford University Press, 1960.
  • D. L. Iglehart, Optimality of (s, S) Policies in the Infinite Horizon Dynamic Inventory Problem, Management Science 9(2):259–267, 1963. https://doi.org/10.1287/mnsc.9.2.259
  • A. F. Veinott, Jr., On the Optimality of (s, S) Inventory Policies: New Conditions and a New Proof, SIAM Journal on Applied Mathematics 14(5):1067–1083, 1966. https://doi.org/10.1137/0114086
  • D. P. Bertsekas and S. E. Shreve, Stochastic Optimal Control: The Discrete-Time Case, Academic Press, 1978.
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Markov ChainProbabilityStochastic Systems·Captain: mikedeng1

Random Walks in a Random Environment 2: lim X_n/n = (1 − Eσ)/(1 + Eσ) if Eσ < 1, −(1 − E(σ⁻¹))/(1 + E(σ⁻¹)) if E(σ⁻¹) < 1, and 0 OtherwiseResearch Paper

Motivation

A random walk in a random environment is a walk whose step probabilities are sampled once at each site and then reused whenever the walk returns there. Repeated visits therefore reveal the same local bias instead of drawing a fresh probability. This makes the walk different from an ordinary random walk with a single averaged step probability. Solomon's 1975 paper asks how the random environment changes the long-run direction and speed of a one-dimensional nearest-neighbor walk. Its Section 1 gives the speed law and the associated limits for first passage times. These results distinguish escape at a nonzero linear rate from escape or recurrence at zero linear rate. Solomon (1975)

The question matters whenever a particle repeatedly crosses the same heterogeneous medium. Averaging the local right-step probabilities predicts the drift of a homogeneous comparison walk, but it does not generally predict the speed in the sampled medium. Sites with a small right-step probability can hold up the walk through repeated excursions. The formula in Theorem (1.16) quantifies this effect using a moment of the ratio of left-step to right-step probability. Solomon (1975), pp. 7–8

Setting

An environment is a sequence α=(αz)z∈Z\alpha=(\alpha_z)_{z\in\mathbb Z}α=(αz​)z∈Z​ of numbers in [0,1][0,1][0,1]. In a fixed environment, a walk at site zzz moves to z+1z+1z+1 with probability αz\alpha_zαz​ and to z−1z-1z−1 with probability βz=1−αz\beta_z=1-\alpha_zβz​=1−αz​. It starts at X0=0X_0=0X0​=0. For the random environment, the variables αz\alpha_zαz​ are independent and identically distributed. First the environment is sampled; then the walk moves according to the fixed probabilities at its sites. The probability law that averages over both choices is the annealed law PPP. The mission's model records this law through every finite path cylinder, jointly with every measurable event concerning the environment. Solomon (1975), pp. 1–2

Write σz=βz/αz\sigma_z=\beta_z/\alpha_zσz​=βz​/αz​ for the ratio of leftward to rightward probability. At the endpoints, σz=∞\sigma_z=\inftyσz​=∞ when αz=0\alpha_z=0αz​=0 and σz=0\sigma_z=0σz​=0 when αz=1\alpha_z=1αz​=1. Let e=Eσ0e=E\sigma_0e=Eσ0​ and e−=E(σ0−1)e_-=E(\sigma_0^{-1})e−​=E(σ0−1​); either may be infinite. For an integer site z≠0z\ne0z=0, the passage time TzT_zTz​ is the first positive time at which XXX visits zzz, with Tz=∞T_z=\inftyTz​=∞ if the site is never reached; put T0=0T_0=0T0​=0. The positive ladder times are τn=Tn−Tn−1\tau_n=T_n-T_{n-1}τn​=Tn​−Tn−1​ where the passage times are finite. Their joint sequence, rather than individual identically distributed variables alone, is relevant to the speed law. Solomon (1975), pp. 5–7

Formalization targets

The goal is the complete three-case statement of Theorem (1.16). All limits below hold almost surely. If e<1e<1e<1, then

Tnn⟶1+e1−e,Xnn⟶1−e1+e.\frac{T_n}{n}\longrightarrow\frac{1+e}{1-e},\qquad \frac{X_n}{n}\longrightarrow\frac{1-e}{1+e}.nTn​​⟶1−e1+e​,nXn​​⟶1+e1−e​.

If e−<1e_-<1e−​<1, the symmetric limits are

T−nn⟶1+e−1−e−,Xnn⟶−1−e−1+e−.\frac{T_{-n}}{n}\longrightarrow\frac{1+e_-}{1-e_-},\qquad \frac{X_n}{n}\longrightarrow-\frac{1-e_-}{1+e_-}.nT−n​​⟶1−e−​1+e−​​,nXn​​⟶−1+e−​1−e−​​.

In the remaining case, e−1≤1≤e−e^{-1}\le1\le e_-e−1≤1≤e−​, both normalized passage times tend to infinity and Xn/nX_n/nXn​/n tends to zero. The reciprocal inequality is understood in the extended nonnegative reals, including e=∞e=\inftye=∞. The milestone list follows the paper's supporting statements: a transience observation, a fixed-environment mean passage-time identity, a separated-block independence lemma, stationarity and ergodicity of ladder times, and the annealed mean ladder-time formula. Solomon (1975), pp. 3, 5–7

Significance

The theorem gives a numerical asymptotic speed in either direction when the corresponding ratio has mean below one. It also identifies a zero-speed regime through explicit conditions on the two reciprocal moments. The passage-time clauses say more than the final speed alone: they describe the time required to reach distant positive and negative sites and distinguish a finite linear time scale from an infinite one. The same section compares the speed with that of a homogeneous walk obtained by replacing every local probability with Eα0E\alpha_0Eα0​; the random environment can slow the walk. Solomon (1975), pp. 7–8

Solomon proved these results in 1975. This mission asks for machine-checked proofs of the known statements and a reusable Lean description of the annealed nearest-neighbor model. The fixed-environment chain, first passage times, and the shift law of a sequence of ladder times are useful interfaces for further formal work on random media. No proof of these draft statements is claimed by the mission proposal. Solomon (1975)

Difficulty

The direct attempt to apply an ordinary law of large numbers to the step increments Xn−Xn−1X_n-X_{n-1}Xn​−Xn−1​ does not fit the model: those increments are not strictly stationary in a nonconstant environment. The walk revisits previously sampled site probabilities, so a later increment depends on the path's history through the sites it has encountered. The paper points out this obstruction before introducing ladder times. An additional issue is that a passage time need not be finite, and the means eee and e−e_-e−​ may also be infinite. Any argument that converts these quantities to ordinary real numbers too early loses the zero-speed cases. Solomon (1975), pp. 5, 7

Formalization scope

Lean represents sites by Z\mathbb ZZ and time indices by N\mathbb NN. A probability space carries the jointly sampled environment and path. The environment lies in [0,1][0,1][0,1] pointwise and is independent and identically distributed across all integer sites. The path law is fixed by its joint finite-dimensional cylinder probabilities, which express the annealed construction from the paper. In particular, the path cannot be chosen independently of the environment merely because its one-step marginal probabilities look right. This rules out a trivializing model that forgets the dependence between the sampled medium and the walk.

The ratios σz\sigma_zσz​, their reciprocal and their expectations take values in R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞}. Passage times take values in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}, and normalized passage-time limits are expressed in extended nonnegative reals. The position ratio Xn/nX_n/nXn​/n has a real limit. The theorem permits both endpoint probabilities, αz=0\alpha_z=0αz​=0 and αz=1\alpha_z=1αz​=1, and imposes no nondegeneracy assumption. Each convergence statement is almost sure. The ergodicity milestone concerns the full joint law of the sequence (τn)n≥1(\tau_n)_{n\ge1}(τn​)n≥1​ under the left shift; shift preservation supplies strict stationarity. Solomon (1975), pp. 1–2, 5–7

A complete development needs measure-theoretic probability, the fixed-environment chain and annealed cylinder law, extended-valued integration and first passage times, and ergodic theory for the ladder-time shift. The model and passage-time interfaces can be reused in later one-dimensional random-environment results. Contributions proving the listed milestones, sharpening their interfaces without changing their meaning, or supplying general probability lemmas used by the known proof are within scope.

Selected references

  • Fred Solomon, Random Walks in a Random Environment, The Annals of Probability 3(1):1–31, 1975. DOI: 10.1214/aop/1176996444
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CombinatoricsGraph Theory·Captain: mikedeng1

Graph Minors. X. Obstructions to Tree-Decomposition IV: Mutually Distinguishable Tangles Have a Tree-Decomposition Separating Them by Their DistinctionsResearch Paper

Why tangles need to be organised into a tree

Robertson and Seymour introduced tangles in Graph Minors. X (J. Combin. Theory Ser. B 52 (1991) 153–190) as the precise obstruction to tree-decompositions of small width: a graph has a tangle of large order exactly when it has no tree-decomposition of small width. A tangle points to a highly connected region of a graph without naming its vertices, by designating for every low-order separation which side is the "small" one. Large grids, large clique minors and surface embeddings with high representativity all induce tangles.

A graph usually contains several such regions. The structure theory of the Graph Minors series needs to look at all of them at once: to decompose a graph along a tree so that each highly connected region sits at its own node, and any two regions are separated as cheaply as possible. Section 10 of the paper provides that decomposition, and its later versions ("tree of tangles" theorems) have become a standard tool in structural graph theory, in matroid theory and in abstract separation systems (see Diestel, Hundertmark and Lemanczyk, Profiles of separations: in graphs, matroids and beyond, Combinatorica 39 (2019), and Carmesin, Diestel, Hundertmark and Stein, Connectivity and tree structure in finite graphs, Combinatorica 34 (2014)). This mission formalizes the original 1991 statement for hypergraphs.

Setting

A hypergraph GGG has a finite vertex set V(G)V(G)V(G), a finite edge set E(G)E(G)E(G) and an incidence relation; an edge may have any number of ends. A subhypergraph is given by a vertex set and an edge set, closed under taking ends of its edges; ∪\cup∪, ∩\cap∩, ⊆\subseteq⊆ act on both sets. A separation is a pair (A,B)(A,B)(A,B) of subhypergraphs with A∪B=GA\cup B=GA∪B=G and E(A∩B)=∅E(A\cap B)=\emptysetE(A∩B)=∅; its order is ∣V(A∩B)∣|V(A\cap B)|∣V(A∩B)∣.

A tangle of order θ≥1\theta\ge1θ≥1 is a set T\mathcal TT of separations of order <θ<\theta<θ such that (i) of every separation (A,B)(A,B)(A,B) of order <θ<\theta<θ, one of (A,B)(A,B)(A,B), (B,A)(B,A)(B,A) is in T\mathcal TT; (ii) no three members (Ai,Bi)(A_i,B_i)(Ai​,Bi​) of T\mathcal TT satisfy A1∪A2∪A3=GA_1\cup A_2\cup A_3=GA1​∪A2​∪A3​=G; (iii) V(A)≠V(G)V(A)\neq V(G)V(A)=V(G) for (A,B)∈T(A,B)\in\mathcal T(A,B)∈T. Two tangles are indistinguishable if one contains the other, and a separation (A,B)(A,B)(A,B) distinguishes T1\mathcal T_1T1​ from T2\mathcal T_2T2​ if (A,B)∈T1(A,B)\in\mathcal T_1(A,B)∈T1​ and (B,A)∈T2(B,A)\in\mathcal T_2(B,A)∈T2​.

A tree-decomposition (T,τ)(T,\tau)(T,τ) assigns a subhypergraph τ(t)\tau(t)τ(t) to each node of a tree TTT, so that the τ(t)\tau(t)τ(t) cover GGG, are pairwise edge-disjoint, and τ(t)∩τ(t′′)⊆τ(t′)\tau(t)\cap\tau(t'')\subseteq\tau(t')τ(t)∩τ(t′′)⊆τ(t′) whenever t′t't′ lies on the path from ttt to t′′t''t′′. An edge eee of TTT, with components T1,T2T_1,T_2T1​,T2​ of T∖eT\setminus eT∖e, makes the separations (G1e,G2e)(G^e_1,G^e_2)(G1e​,G2e​) and (G2e,G1e)(G^e_2,G^e_1)(G2e​,G1e​), where Gie=⋃t∈V(Ti)τ(t)G^e_i=\bigcup_{t\in V(T_i)}\tau(t)Gie​=⋃t∈V(Ti​)​τ(t). Two separations cross unless one of four nestings holds (A1⊆A2A_1\subseteq A_2A1​⊆A2​ and B2⊆B1B_2\subseteq B_1B2​⊆B1​, or the analogous three); a set of separations is laminar if no two members cross.

A tie-breaker λ\lambdaλ maps separations into a linearly ordered set so that (i) λ(A,B)=λ(C,D)\lambda(A,B)=\lambda(C,D)λ(A,B)=λ(C,D) exactly when (A,B)=(C,D)(A,B)=(C,D)(A,B)=(C,D) or (A,B)=(D,C)(A,B)=(D,C)(A,B)=(D,C); (ii) λ(A∪C,B∩D)≤λ(A,B)\lambda(A\cup C,B\cap D)\le\lambda(A,B)λ(A∪C,B∩D)≤λ(A,B) or λ(A∩C,B∪D)<λ(C,D)\lambda(A\cap C,B\cup D)<\lambda(C,D)λ(A∩C,B∪D)<λ(C,D); (iii) separations of smaller order get smaller λ\lambdaλ-order. Given λ\lambdaλ, the (T1,T2)(\mathcal T_1,\mathcal T_2)(T1​,T2​)-distinction is the separation of minimum λ\lambdaλ-order distinguishing T1\mathcal T_1T1​ from T2\mathcal T_2T2​. A separation (A,B)(A,B)(A,B) is λ\lambdaλ-robust if for every separation (C,D)(C,D)(C,D) of the hypergraph AAA, one of (C,B∪D)(C,B\cup D)(C,B∪D), (D,B∪C)(D,B\cup C)(D,B∪C) has λ\lambdaλ-order at least λ(A,B)\lambda(A,B)λ(A,B), and doubly λ\lambdaλ-robust if (B,A)(B,A)(B,A) is λ\lambdaλ-robust too.

Formalization targets

Goal: (10.3), p. 181

Let T1,…,Tn\mathcal T_1,\dots,\mathcal T_nT1​,…,Tn​, n≥1n\ge1n≥1, be mutually distinguishable tangles in GGG (each with its own order) and λ\lambdaλ a tie-breaker. Then there is a tree-decomposition (T,τ)(T,\tau)(T,τ) with V(T)={t1,…,tn}V(T)=\{t_1,\dots,t_n\}V(T)={t1​,…,tn​} such that

(i)ti∈V(T1) ⟹ (⋃t∈V(T1)τ(t), ⋃t∈V(T2)τ(t))∉Tifor every e∈E(T),\text{(i)}\quad t_i\in V(T_1)\ \Longrightarrow\ \Bigl(\textstyle\bigcup_{t\in V(T_1)}\tau(t),\ \bigcup_{t\in V(T_2)}\tau(t)\Bigr)\notin\mathcal T_i\quad\text{for every } e\in E(T),(i)ti​∈V(T1​) ⟹ (⋃t∈V(T1​)​τ(t), ⋃t∈V(T2​)​τ(t))∈/Ti​for every e∈E(T),

and (ii) for i≠ji\neq ji=j, each edge of the tit_iti​–tjt_jtj​ path in TTT whose separations have the smallest λ\lambdaλ-order on that path makes the (Ti,Tj)(\mathcal T_i,\mathcal T_j)(Ti​,Tj​)- and (Tj,Ti)(\mathcal T_j,\mathcal T_i)(Tj​,Ti​)-distinctions, the first with tjt_jtj​'s side first.

Milestones

  • (9.1), p. 177: the separations made by the edges of a tree-decomposition form a laminar set, and every laminar set is the set made by the edges of some tree-decomposition, each member by a unique edge.
  • (9.2), p. 178: every hypergraph has a tie-breaker.
  • (9.3), p. 179: a strict form of the second tie-breaker axiom, with two degenerate exceptions.
  • (9.4), p. 180: doubly λ\lambdaλ-robust separations do not cross.
  • (10.1), p. 180: two tangles are distinguished by some separation if and only if neither contains the other.
  • (10.2), p. 181: the (T1,T2)(\mathcal T_1,\mathcal T_2)(T1​,T2​)-distinction is doubly λ\lambdaλ-robust.

Significance

The theorem gives a single decomposition for all tangles at once: any family of pairwise distinguishable tangles is displayed by a single tree-decomposition, with each tangle "living" at its own node (property (i)) and every pair separated by its cheapest distinction (property (ii)). The paper derives from it that a hypergraph has at most ∣V(G)∣|V(G)|∣V(G)∣ maximal tangles ((10.4), p. 184), and Section 11 uses the same machinery to build tree-decompositions whose pieces "almost" carry a local structure, a step used in the later Graph Minors papers.

None of these statements is formalized in any proof assistant as far as a search of the Prove2Me library shows; the platform has simple-graph tree-decompositions with vertex bags (from Graph Minors V), which are a different object from the hypergraph tree-decompositions here. The mission produces machine-checked statements of the tangle-tree theorem in its original hypergraph form, together with the lemma chain the authors use. The remaining work is a formal proof of each item; (9.1) is "left to the reader" in the paper and therefore needs an argument written from scratch.

Difficulty

The naive approach takes, for every pair of tangles, a separation of minimum order distinguishing them, and tries to arrange these separations in a tree. That fails: minimum-order distinguishing separations for different pairs may cross, and no tree-decomposition makes two crossing separations. Ties among minimum-order separations must be broken consistently across all pairs at once, and even a laminar family of distinctions does not obviously yield a tree whose nodes correspond one-to-one to the tangles, as property (i) and V(T)={t1,…,tn}V(T)=\{t_1,\dots,t_n\}V(T)={t1​,…,tn​} demand.

Formalization scope

  • Hypergraphs are a structure with an incidence relation on types V, E; every theorem assumes [Finite V] [Finite E] (the paper's "all hypergraphs in this paper are finite", p. 154). Subhypergraphs are pairs of a vertex set and an edge set closed under ends.
  • A tangle carries its order as a parameter: IsTangle G θ 𝒯 includes θ≥1\theta\ge1θ≥1. In (10.3) the tangles have independent orders θi\theta_iθi​.
  • The tree of a tree-decomposition is a SimpleGraph on Fin n that is a tree. In the goal, node iii is tit_iti​, which encodes V(T)={t1,…,tn}V(T)=\{t_1,\dots,t_n\}V(T)={t1​,…,tn​} with the tit_iti​ distinct; the hypothesis n≥1n\ge1n≥1 is the paper's.
  • A tie-breaker is a function on all pairs of subhypergraphs into an arbitrary type Λ\LambdaΛ with a linear order; its axioms constrain only its values on separations. The goal quantifies over every such Λ\LambdaΛ, not just the paper's R3\mathbb R^3R3.
  • (10.3)(ii) is stated with an explicit orientation (the one forced by (i)) and for every edge minimising the λ\lambdaλ-order on the path.
  • (10.1) and (10.2) are stated for hypergraphs; §10 opens with "tangles in a graph GGG", but (10.3) applies them to hypergraphs and their proofs do not use edge sizes.
  • A trivializing formalization would make the tie-breaker axioms unsatisfiable, so that (9.3)–(10.3) hold vacuously; (9.2) is part of the mission precisely to rule this out.
  • The definitions of hypergraph, tangle and tree-decomposition are shared with the other missions of the series, Graph Minors. X. Obstructions to Tree-Decomposition I (tangle number equals max⁡(β,γ)\max(\beta,\gamma)max(β,γ)), II (branch-width and tree-width), III (the grid tangle) and V (pervasive classes of designs). The laminar/tie-breaker layer is reusable for any tree-of-tangles statement. Contributions welcome: proofs of the milestones in any order, and a formal proof of (9.1).

Selected references

  • N. Robertson, P. D. Seymour, Graph Minors. X. Obstructions to Tree-Decomposition, J. Combin. Theory Ser. B 52 (1991) 153–190. https://doi.org/10.1016/0095-8956(91)90061-n
  • J. Carmesin, R. Diestel, F. Hundertmark, M. Stein, Connectivity and tree structure in finite graphs, Combinatorica 34 (2014) 11–46. https://arxiv.org/abs/1105.1611
  • R. Diestel, F. Hundertmark, S. Lemanczyk, Profiles of separations: in graphs, matroids and beyond, Combinatorica 39 (2019) 37–75. https://arxiv.org/abs/1608.07144
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Markov ChainProbabilityStochastic Systems·Captain: mikedeng1

The Two-Parameter Poisson–Dirichlet Distribution Derived from a Stable Subordinator 6: n·Y_n → (1 − α)/α Almost Surely under PD(α, θ)Research Paper

Motivation

In a population divided into many species, a ranked frequency VnV_nVn​ is the fraction belonging to the nnnth most common species. The Poisson–Dirichlet distribution is a model for such random ranked frequencies. It also arises from ranked jumps of a stable subordinator, which gives the model its connection to random interval partitions. Pitman and Yor's 1997 paper develops both descriptions and studies quantities derived from the ranked sequence. Its §7.3 asks how much of the remaining total mass belongs to the nnnth ranked component when nnn is large. This is the chain factor YnY_nYn​, the quantity studied here. These interpretations and the result are in Pitman and Yor (1997).

For 0<α<10<\alpha<10<α<1, the paper first analyzes the tail ratio Σn\Sigma_nΣn​ under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) through Proposition 11 and its Laplace transform. Proposition 14 relates PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) to that base law by a local-time density. The limiting behavior in Proposition 44 combines those two themes. The paper states both an almost-sure limit and a Gaussian fluctuation limit, but the variance printed for the latter conflicts with the variance of Σ1\Sigma_1Σ1​ displayed immediately before it. The mission retains the paper's almost-sure assertion as its goal and records the corrected fluctuation assertion separately. Pitman and Yor (1997), pp. 863–865, 890–891.

Setting

Choose 0≤α<10\le\alpha<10≤α<1 and θ>−α\theta> -\alphaθ>−α. Let Y~1,Y~2,…\tilde Y_1,\tilde Y_2,\ldotsY~1​,Y~2​,… be independent random variables, where Y~n\tilde Y_nY~n​ has the beta distribution with parameters (1−α,θ+nα)(1-\alpha,\theta+n\alpha)(1−α,θ+nα). Its density on (0,1)(0,1)(0,1) is Γ(a+b)xa−1(1−x)b−1/(Γ(a)Γ(b))\Gamma(a+b)x^{a-1}(1-x)^{b-1}/(\Gamma(a)\Gamma(b))Γ(a+b)xa−1(1−x)b−1/(Γ(a)Γ(b)) for parameters a,b>0a,b>0a,b>0. Form the stick-breaking lengths

V~1=Y~1,V~n=(1−Y~1)⋯(1−Y~n−1)Y~n(n≥2).\tilde V_1=\tilde Y_1,\qquad \tilde V_n=(1-\tilde Y_1)\cdots(1-\tilde Y_{n-1})\tilde Y_n\quad(n\ge2).V~1​=Y~1​,V~n​=(1−Y~1​)⋯(1−Y~n−1​)Y~n​(n≥2).

Sort these lengths in decreasing order, retaining multiplicities. The law of the resulting sequence V1≥V2≥⋯V_1\ge V_2\ge\cdotsV1​≥V2​≥⋯ is PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ), exactly Definition 1 of the paper. Pitman and Yor (1997), p. 857.

For that ranked sequence, define the tail ratio and chain factor

Σn=Vn+1+Vn+2+⋯Vn,Yn=VnVn+Vn+1+⋯=11+Σn.\Sigma_n=\frac{V_{n+1}+V_{n+2}+\cdots}{V_n},\qquad Y_n=\frac{V_n}{V_n+V_{n+1}+\cdots}=\frac{1}{1+\Sigma_n}.Σn​=Vn​Vn+1​+Vn+2​+⋯​,Yn​=Vn​+Vn+1​+⋯Vn​​=1+Σn​1​.

The distinction between YnY_nYn​ and the original independent factors Y~n\tilde Y_nY~n​ matters: the former is computed after ranking and is generally dependent across indices. The paper also uses the function ψα(λ)=1+α∫01(1−e−λx)x−α−1 dx\psi_\alpha(\lambda)=1+\alpha\int_0^1(1-e^{-\lambda x})x^{-\alpha-1}\,dxψα​(λ)=1+α∫01​(1−e−λx)x−α−1dx for λ≥0\lambda\ge0λ≥0. It appears in the Laplace transform of Σn\Sigma_nΣn​. Pitman and Yor (1997), pp. 863–865, 890.

Formalization targets

The central target is Proposition 44, display (150): for 0<α<10<\alpha<10<α<1 and θ>−α\theta> -\alphaθ>−α,

nYn⟶1−ααalmost surely under PD(α,θ).nY_n\longrightarrow\frac{1-\alpha}{\alpha}\quad\text{almost surely under }\mathrm{PD}(\alpha,\theta).nYn​⟶α1−α​almost surely under PD(α,θ).

The milestones state the distribution and Laplace transform of Σn\Sigma_nΣn​ from Proposition 11(ii), its mean α/(1−α)\alpha/(1-\alpha)α/(1−α), the almost-sure limit of Σn/n\Sigma_n/nΣn​/n under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), and Proposition 14's change-of-measure formula. The Gaussian companion records the central limit theorem for Σn/n\Sigma_n/nΣn​/n and the corrected version of Proposition 44's display (151):

n(nYn−1−αα)⟹N ⁣(0,(1−α)2α3(2−α)).\sqrt n\left(nY_n-\frac{1-\alpha}{\alpha}\right) \Longrightarrow N\!\left(0,\frac{(1-\alpha)^2}{\alpha^3(2-\alpha)}\right).n​(nYn​−α1−α​)⟹N(0,α3(2−α)(1−α)2​).

The printed variance in (151) is α−2(2−α)−2\alpha^{-2}(2-\alpha)^{-2}α−2(2−α)−2. It differs from the variance forced by the preceding Σn\Sigma_nΣn​ central limit theorem: Var⁡(Σ1)=α/((2−α)(1−α)2)\operatorname{Var}(\Sigma_1)=\alpha/((2-\alpha)(1-\alpha)^2)Var(Σ1​)=α/((2−α)(1−α)2) and the derivative of x↦1/xx\mapsto1/xx↦1/x at α/(1−α)\alpha/(1-\alpha)α/(1−α) give (1−α)2/(α3(2−α))(1-\alpha)^2/(\alpha^3(2-\alpha))(1−α)2/(α3(2−α)). At α=1/2\alpha=1/2α=1/2, the corrected and printed values are 4/34/34/3 and 16/916/916/9. The verbatim milestone text preserves the paper's wording; the companion theorem discloses the correction. Pitman and Yor (1997), pp. 890–891.

Significance

Display (150) identifies the almost-sure scale of the ranked chain factor: YnY_nYn​ behaves like a deterministic constant divided by nnn. This makes the order of magnitude precise for every permitted θ\thetaθ, despite the dependence among ranked components. The companion fluctuation statement gives a distributional scale around that limit and exposes a numerical inconsistency in the printed version. Neither conclusion is simply a statement about the independent beta factors Y~n\tilde Y_nY~n​; the paper compares the two sequences precisely because they have different limiting distributions. Pitman and Yor (1997), p. 891.

The result is proved in the paper, while its statements and their supporting definitions still need a machine-checked development. A completed formalization would make the ranked-frequency law, the tail-ratio limit, and the local-time change of measure available as separately reusable results. It would also settle the corrected variance at the level of a precise probability-law statement rather than silently adopting the paper's printed constant.

Difficulty

The tempting shortcut is to use Proposition 11(ii), which says that each Σn\Sigma_nΣn​ has the law of a sum of nnn independent copies of Σ1\Sigma_1Σ1​, and invoke a strong law. That information concerns each one-dimensional law separately; it does not exhibit the whole sequence (Σn)(\Sigma_n)(Σn​) as partial sums of a single independent sequence. Almost-sure convergence is a statement about their joint coupling, so the shortcut leaves a gap. The Gaussian conclusion raises a different issue: its limit must survive the change from PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) to PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ), and its variance must be consistent with the displayed variance of Σ1\Sigma_1Σ1​. These are the two substantive tasks beyond the calculation of the Laplace transform. Pitman and Yor (1997), pp. 864, 890–891.

Formalization scope

Lean represents a random ranked sequence as V:Ω→(N→R)V:\Omega\to(\mathbb N\to\mathbb R)V:Ω→(N→R) on a probability space. Its index kkk means the paper's n=k+1n=k+1n=k+1. Thus the goal uses (k+1)Yk+1(k+1)Y_{k+1}(k+1)Yk+1​, and the tail-ratio milestones use Σk+1/(k+1)\Sigma_{k+1}/(k+1)Σk+1​/(k+1). The paper's Definition 1 is represented by independent beta coordinate laws followed by a decreasing ranking. The ranking counts multiplicity using extended cardinality, so an infinite set of terms above a threshold cannot acquire a finite fallback count. The law of the ranked sequence is expressed through measurable preimages. This avoids treating a nonmeasurable ranking map as a zero measure through Measure.map.

All targets retain 0<α<10<\alpha<10<α<1; the θ\thetaθ targets also retain θ>−α\theta> -\alphaθ>−α. The beta law and integrals use these parameter ranges. Real expectations state integrability or square integrability where needed, preventing a nonintegrable Bochner integral or variance from supplying a fallback zero. The nonnegative change-of-measure identity uses extended nonnegative integrals, and its local time LLL is identified by the almost-sure limit nVnαnV_n^\alphanVnα​ rather than by an arbitrary extra weight or a limit operator with a default value. The Gaussian variances are positive on this parameter range, despite being represented by nonnegative real parameters in Mathlib. The formalization must use the actual tail ratio of the PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) sequence, not an independently assigned factor process.

The reusable infrastructure includes the ranked-value operation, the stick-breaking law, convolution powers, the tail-ratio and chain-factor definitions, and the bridge between PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) and PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ). Contributions that establish these interfaces or prove the displayed mean, strong law, and central limit assertions directly against them are within scope. Pitman and Yor (1997), Definition 1, Propositions 11, 14, 44.

Selected references

  • J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator, Annals of Probability 25(2):855–900, 1997. DOI: 10.1214/aop/1024404422.
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Control TheoryOperations ResearchStochastic Systems·Captain: mikedeng1

Distributed Scheduling Based on Due Dates and Buffer Priorities 1: First Buffer First Serve Is Stable on Every Nonacyclic Flow Line Whose Bursty Arrival Rate Is Below CapacityResearch Paper

Motivation

Semiconductor wafer fabs are the standard example of a reentrant manufacturing line: a wafer visits the same lithography or etching station many times along a route of hundreds of steps, so each station holds parts at many different stages of completion and must decide, every time a machine frees up, which of them to serve next. Kumar (Re-entrant lines, Queueing Systems 13, 1993) singled these lines out as a third class of manufacturing systems besides flow shops and job shops, and stability of their scheduling policies became a central question in the analysis of queueing networks.

The question is sharp because the obvious conjecture is false. Kumar and Seidman (IEEE TAC 35(3), 1990) gave a deterministic network in which a distributed policy is unstable although every machine has spare capacity, and Lu and Kumar (IEEE TAC 36(12), 1991, Example 1, p. 1409) gave a two-station reentrant line in which a buffer priority policy is unstable at load below one. Their paper then identifies policies that are always stable: first buffer first serve (FBFS, Theorem 1), last buffer first serve (Theorem 3) and the due-date policies least slack and earliest due date (Theorem 4). This mission formalizes Theorem 1.

Timeline:

  • 1990: Kumar and Seidman exhibit instability of clear-a-fraction policies under load below one.
  • 1991: Lu and Kumar prove FBFS and LBFS stable on every nonacyclic flow line with deterministic bursty arrivals, and exhibit an unstable buffer priority policy.
  • 1995–1996: Dai (Ann. Appl. Probab. 5(1), 1995) reduces positive Harris recurrence of multiclass networks to stability of fluid models; Dai and Weiss (Math. Oper. Res. 21(1), 1996) prove the FBFS and LBFS fluid models of reentrant lines stable.

Setting

A nonacyclic flow line has SSS service centers; center σ\sigmaσ has mσ≥1m_\sigma\ge1mσ​≥1 identical machines in parallel, each working on one part at a time. Every part follows the same route: it visits buffers b1,b2,…,blb_1,b_2,\dots,b_lb1​,b2​,…,bl​ in order, buffer bib_ibi​ sits at center σi\sigma_iσi​, and a part in bib_ibi​ needs τi>0\tau_i>0τi​>0 time units of uninterrupted processing on one machine of σi\sigma_iσi​. The same center may appear many times along the route.

Parts enter at b1b_1b1​; part π\piπ is released at time α(π)\alpha(\pi)α(π). The releases are deterministic but may be bursty: with u(t)u(t)u(t) the number of parts released in [0,t][0,t][0,t],

u(t)−u(s)≤λ(t−s)+γfor all 0≤s≤t,(1)u(t)-u(s)\le\lambda(t-s)+\gamma\qquad\text{for all }0\le s\le t,\tag{1}u(t)−u(s)≤λ(t−s)+γfor all 0≤s≤t,(1)

for constants λ,γ≥0\lambda,\gamma\ge0λ,γ≥0. Each part brings wσ=∑i:σi=στi/mσw_\sigma=\sum_{i:\sigma_i=\sigma}\tau_i/m_\sigmawσ​=∑i:σi​=σ​τi​/mσ​ units of work per machine to center σ\sigmaσ, and the load is ρ=max⁡σλwσ\rho=\max_\sigma\lambda w_\sigmaρ=maxσ​λwσ​. The arrival rate is within capacity when ρ<1\rho<1ρ<1 (3). At time 000 the line may hold finitely many initial parts in arbitrary buffers, some of them already in service.

A schedule is nonidling (a machine idles only if every buffer of its center is empty), nonpreemptive (a started service runs to completion) and serves the part at the head of the chosen buffer. Under FBFS a free machine at center σ\sigmaσ takes a part from bib_ibi​ only if every buffer bjb_jbj​ of σ\sigmaσ with j<ij<ij<i is empty. With e(π)e(\pi)e(π) the time part π\piπ exits after its service at blb_lbl​, the schedule is stable if there is Γ≥0\Gamma\ge0Γ≥0 with

e(π)−α(π)≤Γfor all parts π.(4)e(\pi)-\alpha(\pi)\le\Gamma\qquad\text{for all parts }\pi.\tag{4}e(π)−α(π)≤Γfor all parts π.(4)

Γ\GammaΓ may depend on the initial state as well as on λ\lambdaλ.

Formalization targets

Goal: Theorem 1 (p. 1409)

For every line, every λ,γ≥0\lambda,\gamma\ge0λ,γ≥0 with ρ<1\rho<1ρ<1, and every admissible FBFS run whose releases satisfy (1),

∃ Γ≥0  ∀π:e(π)≤α(π)+Γ.\exists\,\Gamma\ge0\ \ \forall\pi:\quad e(\pi)\le\alpha(\pi)+\Gamma .∃Γ≥0  ∀π:e(π)≤α(π)+Γ.

The statement fixes no constant: Γ\GammaΓ is chosen after the run.

Milestones (proof of Theorem 1, pp. 1409–1410)

An interval [T1,T2][T_1,T_2][T1​,T2​] is an iii-busy period if at every instant some part waits in a buffer bjb_jbj​, j≤ij\le ij≤i, at center σi\sigma_iσi​. With τˉ=max⁡jτj\bar\tau=\max_j\tau_jτˉ=maxj​τj​, Γˉi=∑j<i(Γ(j)+τj)\bar\Gamma_i=\sum_{j<i}(\Gamma^{(j)}+\tau_j)Γˉi​=∑j<i​(Γ(j)+τj​) and

Γ(i)=[2τˉ+∑σj=σi, j≤iλτjΓˉi+γτjmσi][1−∑σj=σi, j≤iλτjmσi]−1,\Gamma^{(i)}=\Big[2\bar\tau+\sum_{\sigma_j=\sigma_i,\,j\le i}\frac{\lambda\tau_j\bar\Gamma_i+\gamma\tau_j}{m_{\sigma_i}}\Big]\Big[1-\sum_{\sigma_j=\sigma_i,\,j\le i}\frac{\lambda\tau_j}{m_{\sigma_i}}\Big]^{-1},Γ(i)=[2τˉ+σj​=σi​,j≤i∑​mσi​​λτj​Γˉi​+γτj​​][1−σj​=σi​,j≤i∑​mσi​​λτj​​]−1,
  1. a 1-busy period commencing at T1>0T_1>0T1​>0 has T2−T1≤Γ(1)T_2-T_1\le\Gamma^{(1)}T2​−T1​≤Γ(1);
  2. there are finite times T(i)T^{(i)}T(i) after which every iii-busy period has length at most Γ(i)\Gamma^{(i)}Γ(i);
  3. a part arriving at bjb_jbj​ after T(j)T^{(j)}T(j) leaves bjb_jbj​ within Γ(j)+τj\Gamma^{(j)}+\tau_jΓ(j)+τj​;
  4. a part released after T(l)T^{(l)}T(l) has delay at most ∑j=1l(Γ(j)+τj)\sum_{j=1}^l(\Gamma^{(j)}+\tau_j)∑j=1l​(Γ(j)+τj​).

Milestone 4 has an explicit bound independent of the initial state; the goal additionally covers the finitely many parts present or released during the transient.

Significance

Theorem 1 says that the simplest "push" discipline, always serving the earliest stage first, keeps every part's delay bounded on every reentrant line whose stations have spare capacity, for every initial state and every bursty but rate-limited release pattern. By Little's law it also bounds the work in process. Together with Example 1 it shows that stability is a property of the policy, not of the load condition alone, and it gave one of the first two positive results for a whole class of reentrant lines. The explicit constants Γ(i)\Gamma^{(i)}Γ(i) make the delay guarantee quantitative after the transient.

The result is proved in the paper. As far as the platform record shows it has not been formalized: the related platform items concern the fluid models of Dai and Weiss, which have no parts, no burstiness and no nonpreemption, and a fixed instance of Example 1. This mission produces a machine-checked sample-path model of reentrant lines under buffer priority policies and a checked proof of Theorem 1 with its explicit busy-period constants. The same model serves the sibling mission on LBFS (Theorem 3 of the paper).

Difficulty

A first idea is a work-conservation argument per center: total work arriving at σ\sigmaσ grows at rate ρ<1\rho<1ρ<1 per machine, so the center cannot fall behind. This fails because the work arriving at a center σ\sigmaσ from a later buffer bib_ibi​ depends on how fast the upstream centers have pushed parts to bib_ibi​, and an upstream center can release a burst that the downstream center absorbs only after other buffers have starved; Example 1 is exactly such a cascade under a different priority order. Any argument must therefore bound the delay of a part at a buffer in terms of delays it suffered upstream at other centers, uniformly in the initial state, while nonpreemption lets a part wait up to τˉ\bar\tauτˉ for a machine busy with a lower-priority buffer and the release constraint (1) controls only arrivals to b1b_1b1​, not to later buffers. On sample paths one must also show that the initial parts clear in finite time and that only finitely many parts are served in any bounded interval.

Formalization scope

Lean represents a line by a structure with SSS, mσ>0m_\sigma>0mσ​>0, l>0l>0l>0, the route center : Fin l → Fin S and processing times τ with τi>0\tau_i>0τi​>0. The positivity is a pinned hypothesis: the paper leaves it implicit, its proof divides by τ1\tau_1τ1​, and its only zero processing times are those of Example 1. Buffers are 0-based: the paper's bib_ibi​ is Lean index i−1i-1i−1. The load is written λwˉ\lambda\bar wλwˉ, equal to max⁡σλwσ\max_\sigma\lambda w_\sigmamaxσ​λwσ​ for λ≥0\lambda\ge0λ≥0.

A run is a type of parts with an injective line order, a finite set of initial parts, entry buffers, release times, and for each part and buffer the start of service in WithTop ℝ, ⊤\top⊤ meaning never served. Admissibility imposes, at every t≥0t\ge0t≥0: precedence (service begins after arrival, except that initial parts may be in service at time 000), capacity mσm_\sigmamσ​, nonidling, head of buffer with ties broken by the line order, and the priority rule. All counts use Set.encard. The theorems hold for every admissible run, not for one particular tie-breaking schedule. The constants Γ(i)\Gamma^{(i)}Γ(i) are definitions computed from the line and λ,γ\lambda,\gammaλ,γ; the times T(i)T^{(i)}T(i) are existential after the run.

Two trivializing formalizations are ruled out: start times in ℝ would make every part served by construction and stability half empty, and a capacity constraint stated with Set.ncard would be vacuous for infinitely many parts. Γ\GammaΓ never depends on the part. A sanity file exhibits a nontrivial admissible run satisfying (1) and checks that the empty run is admissible and stable.

The page prints Γ(i)\Gamma^{(i)}Γ(i) (p. 1410) as a product of the two brackets; the inequality it is solved from gives the quotient, which is also the printed form of Γ(1)\Gamma^{(1)}Γ(1), and the formalization uses the quotient.

The sample-path model (Line, Run, Admissible, Arrivals, Stable) is reusable for any buffer priority policy and for the LBFS mission. Contributions welcome: proofs of the milestones in the listed order, lemmas on finiteness of the parts served in bounded time, and interval-counting lemmas for busy periods. Not posed here: Example 1, which is already on the platform as an open problem (QueueingStability.LuKumar.theorem31), Theorems 2–3 (LBFS, sibling mission), Theorems 4–5 and Corollary 1 (due-date policies, several flow lines).

Selected references

  • S. H. Lu and P. R. Kumar, Distributed Scheduling Based on Due Dates and Buffer Priorities, IEEE Transactions on Automatic Control 36(12), 1991, pp. 1406–1416. https://doi.org/10.1109/9.106156
  • P. R. Kumar and T. I. Seidman, Dynamic instabilities and stabilization methods in distributed real-time scheduling of manufacturing systems, IEEE Transactions on Automatic Control 35(3), 1990, pp. 289–298. https://doi.org/10.1109/9.50339
  • P. R. Kumar, Re-entrant lines, Queueing Systems 13, 1993, pp. 87–110. https://doi.org/10.1007/BF01158927
  • J. G. Dai, On positive Harris recurrence of multiclass queueing networks: a unified approach via fluid limit models, Annals of Applied Probability 5(1), 1995, pp. 49–77. https://doi.org/10.1214/aoap/1177004828
  • J. G. Dai and G. Weiss, Stability and instability of fluid models for reentrant lines, Mathematics of Operations Research 21(1), 1996, pp. 115–134. https://doi.org/10.1287/moor.21.1.115
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Control TheoryDynamical SystemsOperations Research·Captain: mikedeng1

Dynamic Instabilities and Stabilization Methods in Distributed Real-Time Scheduling of Manufacturing Systems 2: Stable and Unstable Modes Coexist Under Clearing on a Two-Part-Type SystemResearch Paper

Motivation

Flexible manufacturing systems are often scheduled by simple distributed rules: each machine looks only at its own buffers and decides, in real time, which part type to work on next. Switching from one part type to another costs a set-up time during which the machine produces nothing, so a natural rule is to work on a buffer until it is empty and only then switch. Perkins and Kumar (IEEE Trans. Automat. Control 34, 1989; reference [18] of the paper) showed that such clearing policies, and in particular clear-a-fraction policies, keep every buffer bounded on acyclic systems whenever each machine has spare capacity. Whether the same holds when material flows around a cycle of machines was left open.

Kumar and Seidman (IEEE TAC 35(3), 1990) answered it negatively by two examples. Example 1 is a single re-entrant part type. Example 2, the subject of this mission, has two part types, neither of which ever revisits a machine, and shows two further phenomena: instability without re-entrance, and the coexistence, for one and the same system, of a bounded periodic regime and an unbounded one, selected only by the initial state.

Setting

A manufacturing system has part types ppp arriving at rates dpd_pdp​ and machines mmm. Parts of type ppp follow a fixed route; at stage iii they wait in buffer bp,ib_{p,i}bp,i​ at machine μp,i\mu_{p,i}μp,i​, and processing one of them takes τp,i\tau_{p,i}τp,i​. Switching a machine from buffer bbb to buffer b′b'b′ takes the set-up time δb,b′\delta_{b,b'}δb,b′​. Flows are continuous: xb(t)x_b(t)xb​(t) is the level of buffer bbb, ub(t)u_b(t)ub​(t) and yb(t)y_b(t)yb​(t) are its cumulative input and output, and

xb(t)=xb(0)+ub(t)−yb(t)≥0.x_b(t)=x_b(0)+u_b(t)-y_b(t)\ge 0 .xb​(t)=xb​(0)+ub​(t)−yb​(t)≥0.

A machine works in runs: a set-up for a buffer, then processing it at rate 1/τb1/\tau_b1/τb​ while it is nonempty, and at the rate of its inflow while it is empty. A clearing policy (Definition 1) keeps a machine on a buffer bbb until the first time that bbb is empty and another of its buffers is nonempty, and then sets it up for one of those. The system is stable if sup⁡0≤t<∞xb(t)<∞\sup_{0\le t<\infty}x_b(t)<\inftysup0≤t<∞​xb​(t)<∞ for every buffer bbb.

Example 2 (Fig. 3) has two part types with d1=d2=1d_1=d_2=1d1​=d2​=1 and two machines. Part type 1 visits buffer 1 at machine 1 and then buffer 2 at machine 2; part type 2 visits buffer 3 at machine 2 and then buffer 4 at machine 1. Processing times are τ1,…,τ4\tau_1,\dots,\tau_4τ1​,…,τ4​ and setting up to buffer kkk takes δk>0\delta_k>0δk​>0. The parameters satisfy the capacity condition (1), τ1+τ4<1\tau_1+\tau_4<1τ1​+τ4​<1 and τ2+τ3<1\tau_2+\tau_3<1τ2​+τ3​<1, and

τ2+τ4>1,δ1+δ41−τ1−τ4=δ2+δ31−τ2−τ3=:η,δ4<(1−τ3−τ4)η,δ2<(1−τ1−τ2)η,\tau_2+\tau_4>1,\qquad \frac{\delta_1+\delta_4}{1-\tau_1-\tau_4}=\frac{\delta_2+\delta_3}{1-\tau_2-\tau_3}=:\eta,\qquad \delta_4<(1-\tau_3-\tau_4)\eta,\qquad \delta_2<(1-\tau_1-\tau_2)\eta,τ2​+τ4​>1,1−τ1​−τ4​δ1​+δ4​​=1−τ2​−τ3​δ2​+δ3​​=:η,δ4​<(1−τ3​−τ4​)η,δ2​<(1−τ1​−τ2​)η,

conditions (7)–(10). The paper's feasible instance is (τ1,τ2,τ3,τ4,δ1,δ2,δ3,δ4)=(14,12,14,23,130,15,120,120)(\tau_1,\tau_2,\tau_3,\tau_4,\delta_1,\delta_2,\delta_3,\delta_4)=(\tfrac14,\tfrac12,\tfrac14,\tfrac23,\tfrac1{30},\tfrac15,\tfrac1{20},\tfrac1{20})(τ1​,τ2​,τ3​,τ4​,δ1​,δ2​,δ3​,δ4​)=(41​,21​,41​,32​,301​,51​,201​,201​), with η=1\eta=1η=1. For this system there is exactly one clearing policy.

Formalization targets

Goal: stable and unstable modes coexist

For every parameter set satisfying (1) and (7)–(10):

from x(0)=(0,η,0,η), set-ups (b1,b3): a clearing trajectory exists, and every one is bounded;∃ ξ0 ∀ ξ≥ξ0, from x(0)=(ξ,0,0,0), set-ups (b4,b3): a clearing trajectory exists, and every one has sup⁡t≥0x1(t)=+∞.\begin{aligned} &\text{from } x(0)=(0,\eta,0,\eta),\ \text{set-ups } (b_1,b_3):\ \text{a clearing trajectory exists, and every one is bounded;}\\ &\exists\,\xi_0\ \forall\,\xi\ge\xi_0,\ \text{from } x(0)=(\xi,0,0,0),\ \text{set-ups } (b_4,b_3):\ \text{a clearing trajectory exists, and every one has } \sup_{t\ge0}x_1(t)=+\infty . \end{aligned}​from x(0)=(0,η,0,η), set-ups (b1​,b3​): a clearing trajectory exists, and every one is bounded;∃ξ0​ ∀ξ≥ξ0​, from x(0)=(ξ,0,0,0), set-ups (b4​,b3​): a clearing trajectory exists, and every one has t≥0sup​x1​(t)=+∞.​

Milestones

  1. Case 1, periodic regime: under (1) and (8)–(10), every clearing trajectory from (0,η,0,η)(0,\eta,0,\eta)(0,η,0,η), (b1,b3)(b_1,b_3)(b1​,b3​) satisfies x(η)=(0,η,0,η)x(\eta)=(0,\eta,0,\eta)x(η)=(0,η,0,η) with the same set-ups.
  2. Case 2, Stage 8: under (1) and (7), for large ξ\xiξ, with t9=(ξ+τ2−1(δ1+δ2))/(τ2−1−1)t_9=(\xi+\tau_2^{-1}(\delta_1+\delta_2))/(\tau_2^{-1}-1)t9​=(ξ+τ2−1​(δ1​+δ2​))/(τ2−1​−1): x(t9)=(0,0,t9−δ1,0)x(t_9)=(0,0,t_9-\delta_1,0)x(t9​)=(0,0,t9​−δ1​,0), machine 1 set up for buffer 1, machine 2 for buffer 2.
  3. Case 2, full cycle: under (1) and (7), for large ξ\xiξ, at an explicit time t17t_{17}t17​, x(t17)=(λξ+α,0,0,0)x(t_{17})=(\lambda\xi+\alpha,0,0,0)x(t17​)=(λξ+α,0,0,0) with set-ups (b4,b3)(b_4,b_3)(b4​,b3​), where λ=τ2τ4/((1−τ2)(1−τ4))>1\lambda=\tau_2\tau_4/((1-\tau_2)(1-\tau_4))>1λ=τ2​τ4​/((1−τ2​)(1−τ4​))>1.

Significance

The result shows that stability of a scheduling policy is a property of the initial state as well as of the system: the same parameters admit a bounded periodic orbit and an orbit along which the backlog of buffer 1 is multiplied by λ>1\lambda>1λ>1 in every cycle. The capacity condition (1) holds throughout, so the instability does not come from overload: spare capacity is lost because one machine starves the other. The example also shows that a cycle in the machine graph suffices, without any part type revisiting a machine. Sections IV and V of the paper respond to this by giving a stronger capacity condition under which clear-a-fraction policies are stable, and a supervisory mechanism that stabilizes any policy.

The paper's argument is a stage-by-stage computation of a piecewise-linear trajectory. It has not been machine-checked. A formalization fixes what a clearing trajectory is (including the switching instants at which a buffer is empty but just starting to fill), proves that the trajectories exist and are determined by the initial state, and checks the paper's closed forms. One printed constant is wrong: the offset α\alphaα of the full cycle lacks a final −δ3-\delta_3−δ3​, and the milestone states the corrected value.

Difficulty

The computations within each stage are linear algebra. The difficulty is the event structure. Every stage depends on the order in which the two machines' events occur: whether machine 1 clears buffer 1 before machine 2 has finished its set-ups, whether buffer 2 is still nonempty when buffer 1 empties, and so on. These orderings hold only for ξ\xiξ large, or only because (8) holds with equality and (9)–(10) hold strictly. The periodic regime depends on exact synchronization. In Case 2, a machine processing an empty buffer at the reduced rate must not be forced off it while its other buffer is empty and not yet fed. A proof must also establish existence of each trajectory, not only compute it.

Formalization scope

  • Model. The general system has part types Fin P, machines Fin M, buffers as pairs (p,i)(p,i)(p,i) with Lean index iii for paper stage i+1i+1i+1, real time, and no transport delay or assembly (as in the paper). Example 2 is an instance of this general model, with machines 1, 2 as Lean 0, 1.
  • Runs. Each machine follows a sequence of runs. Run 0 is on the initial set-up and has no set-up phase. Run k≥1k\ge1k≥1 has a set-up phase of length δβk−1,βk\delta_{\beta_{k-1},\beta_k}δβk−1​,βk​​, followed by a processing phase. Runs are never cut during a set-up. If there are infinitely many runs, their start times tend to ∞\infty∞. There is no idling outside runs: a machine serving an empty buffer passes on its inflow.
  • Set-up times. They depend only on the target buffer, and δb,b=0\delta_{b,b}=0δb,b​=0 is never used.
  • Processing law. The rate cap is yb(t)−yb(s)≤(1/τb)⋅y_b(t)-y_b(s)\le(1/\tau_b)\cdotyb​(t)−yb​(s)≤(1/τb​)⋅(processing time of bbb in [s,t][s,t][s,t]). Rate is exactly 1/τb1/\tau_b1/τb​ while the machine is processing a nonempty buffer.
  • Clearing. "Nonempty" in Definition 1 is read as demanding: positive level, or cumulative input strictly increasing from that instant. Under the literal reading the paper's own switching instants would not be "first times", and no clearing trajectory would exist from these initial states. The no-early-exit condition is imposed on the open processing interval.
  • Set up for bbb at ttt. At t>0t>0t>0 this refers to the run whose interval (sk,sk+1](s_k,s_{k+1}](sk​,sk+1​] contains ttt.
  • Ruling out trivial formalizations. The goal asserts existence of a clearing trajectory in both modes, so neither "every trajectory is bounded" nor "every trajectory is unbounded" can hold vacuously. η\etaη is computed from the data rather than pinned by hypotheses, and (8) is an equality.

Contributions welcome: existence and uniqueness of clearing trajectories for the two-machine instance, the event-ordering lemmas for large ξ\xiξ, the restart (time-shift) property of trajectories, and the three milestones.

Selected references

  • P. R. Kumar and T. I. Seidman, Dynamic instabilities and stabilization methods in distributed real-time scheduling of manufacturing systems, IEEE Transactions on Automatic Control 35(3):289–298, 1990. https://doi.org/10.1109/9.50339
  • J. R. Perkins and P. R. Kumar, Stable, distributed, real-time scheduling of flexible manufacturing/assembly/disassembly systems, IEEE Transactions on Automatic Control 34:139–148, February 1989 (reference [18] of the paper).
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Control TheoryConvex OptimizationProbability·Captain: mikedeng1

Convex Duality in Constrained Portfolio Optimization II: The Dual Problem Attains Its Infimum, So an Optimal Constrained Portfolio–Consumption Pair Exists for Every Initial CapitalResearch Paper

Motivation

Portfolio decisions in continuous time must respect both market uncertainty and investment restrictions. A ban on short sales, for example, restricts the vector of wealth fractions a trader may hold at every instant. The corresponding optimal consumption and investment problem is harder than its unrestricted counterpart because a candidate portfolio obtained from the usual pricing equations may violate the constraint. Cvitanić and Karatzas introduced auxiliary markets indexed by a process and used a dual optimization problem to establish existence of an optimal constrained policy in their 1992 paper. This mission formalizes the paper's existence theorem, Theorem 13.1, together with the results in Sections 12–13 that specify its dual target.

Setting

Fix a finite horizon T>0T>0T>0 and a complete probability space carrying a standard ddd-dimensional Brownian motion WWW. Information at time ttt is the probability augmentation of the filtration generated by WWW up to ttt. A bond earns short rate rtr_trt​; ddd stocks have appreciation vector btb_tbt​ and volatility matrix σt\sigma_tσt​. The market assumptions require progressively measurable coefficients, a uniform lower bound on rrr, uniform nondegeneracy of σσT\sigma\sigma^{\mathsf T}σσT, finite expected interest-rate integral, and finite energy of the market price of risk θ=σ−1(b−r1)\theta=\sigma^{-1}(b-r\mathbf1)θ=σ−1(b−r1) §2.

A portfolio πt\pi_tπt​ specifies fractions of wealth held in the stocks, while ct≥0c_t\geq0ct​≥0 is consumption and XtX_tXt​ is wealth. The feasible portfolios lie in a fixed nonempty closed convex set K⊆RdK\subseteq\mathbb R^dK⊆Rd. Its support function is δK(v)=sup⁡π∈K(−π⋅v)\delta_K(v)=\sup_{\pi\in K}(-\pi\cdot v)δK​(v)=supπ∈K​(−π⋅v), which may equal +∞+\infty+∞. The process ν\nuν indexing an auxiliary market belongs to D\mathcal DD when it has finite expected quadratic energy and finite expected integrated support value. Its deflator HνH_\nuHν​ combines an interest-rate discount with a Brownian exponential. The class D′\mathcal D'D′ consists of those ν∈D\nu\in\mathcal Dν∈D for which the budget map Xν(y)\mathcal X_\nu(y)Xν​(y) is finite for every y>0y>0y>0 §§4, 8.

The running utility U1(t,c)U_1(t,c)U1​(t,c) and terminal utility U2(XT)U_2(X_T)U2​(XT​) are strictly increasing and strictly concave for positive arguments. An admissible constrained policy has nonnegative wealth, finite expected negative utility, and πt∈K\pi_t\in Kπt​∈K for Lebesgue-time times probability almost every (t,ω)(t,\omega)(t,ω). The primal value V(x)V(x)V(x) is the supremum of its expected utility over all such policies with initial capital x>0x>0x>0. The dual value V~(y)\widetilde V(y)V(y) is the infimum, over ν∈D\nu\in\mathcal Dν∈D, of expected conjugate utility evaluated at yHνyH_\nuyHν​ §§5–6, 12.

Formalization targets

Dual attainment

The first conclusion of Theorem 13.1 is the paper's condition (12.9):

∀y>0∃λy∈D′V~(y)=J~(y;λy).\forall y>0\quad\exists\lambda_y\in\mathcal D'\quad\widetilde V(y)=\widetilde J(y;\lambda_y).∀y>0∃λy​∈D′V(y)=J(y;λy​).

Thus the infimum is attained by a drift with a finite budget map. It is a conclusion of this mission, even though earlier Section 12 results assume it. The milestones include weak duality (12.8), the dual representation of Proposition 12.1, the capital-matching result of Proposition 12.2, and the analytic properties of the extended dual functional in Proposition 13.2 pp. 792–795.

An optimal constrained policy for every capital

The theorem's second conclusion is

∀x>0∃(π^,c^,X^)∈A′(x)∀(π,c,X)∈A′(x),J(π,c,X)≤J(π^,c^,X^).\forall x>0\quad\exists (\widehat\pi,\widehat c,\widehat X)\in\mathcal A'(x)\quad\forall(\pi,c,X)\in\mathcal A'(x),\quad J(\pi,c,X)\leq J(\widehat\pi,\widehat c,\widehat X).∀x>0∃(π,c,X)∈A′(x)∀(π,c,X)∈A′(x),J(π,c,X)≤J(π,c,X).

Here A′(x)\mathcal A'(x)A′(x) is the constrained admissible class. Theorem 12.4 establishes this conclusion when dual attainment is assumed; Theorem 13.1 provides that assumption under the paper's stated utility and dual-finiteness conditions p. 794.

Significance

The result supplies an optimizer, rather than only a bound on the best attainable utility. It also identifies a minimizing auxiliary market for every positive dual parameter, making the dual description usable at a specified initial capital. The dual representation links the primal value to a convex function that can be studied without choosing a constrained policy first §§12–13.

The theorem is proved in the paper; the remaining work here is a machine-checked development of its definitions, hypotheses, and existence argument. The mission also produces reusable definitions of an almost-surely square-integrable Brownian integral relation, extended-real utility expectations, an extended support function, and constrained wealth classes. The Brownian state space and predictable step-sum substrate credit the published Ethier–Kurtz formalizations. The paper refers some analytic steps to earlier works instead of reproducing full proofs, including Lemma 12.3 and a final finiteness argument pp. 793–796.

Difficulty

Weak duality alone only bounds the constrained value from above. It does not supply a minimizer of J~(y;ν)\widetilde J(y;\nu)J(y;ν), and an arbitrary minimizing auxiliary process need not belong to D′\mathcal D'D′. The dual functional must retain meaningful infinite values on the full finite-energy process space H\mathcal HH; replacing them with total-operation defaults can turn the needed coercivity and lower-semicontinuity statements into different claims. Even after dual attainment, the minimizing parameter for a prescribed capital must match the budget map Xλy(y)\mathcal X_{\lambda_y}(y)Xλy​​(y) §§12–13. These are the precise gaps between a numerical bound and the asserted optimal policy.

Formalization scope

Lean uses Rd\mathbb R^dRd with its Euclidean norm, a finite positive horizon, a complete probability measure, and the augmented Brownian filtration. Processes are functions of time and sample point; ℓ⊗P\ell\otimes Pℓ⊗P almost-everywhere restrictions on portfolios and auxiliary drifts are distinct from pathwise PPP-almost-sure statements. A policy is represented by a triple (π,c,X)(\pi,c,X)(π,c,X) whose wealth process satisfies the integral equation, matching the paper's pair together with its unique wealth solution. The integral operator is bound to the local Itô construction by predictable step approximations; it is not a free function. Integrands must be in its almost-sure square-integrable domain.

Support values, utility at zero, expected utility, and value functions use extended reals. The extension U(0)U(0)U(0) is the right limit U(0+)U(0+)U(0+); an extended-real supremum defines conjugate utility where zero arguments arise. The inverse marginal is a positive-argument inverse of U′U'U′. The minimization in V~\widetilde VV ranges over D\mathcal DD, while (12.9) asks for a minimizer in D′\mathcal D'D′. Its witnesses λy\lambda_yλy​ remain explicit choices in statements involving Xλy\mathcal X_{\lambda_y}Xλy​​; no default-valued inverse Yν\mathcal Y_\nuYν​ is introduced. The functional J~y\widetilde J_yJy​ of (13.3) is defined on H\mathcal HH, uses the paper's formula on G\mathcal GG, and is +∞+\infty+∞ off G\mathcal GG. On D\mathcal DD it agrees almost everywhere with the original dual objective, an equality requiring a formal lemma. Assumption 6.2 and conditions (5.8), (8.25), (12.2), (12.3), and (12.11) are explicit. Their quantifiers cover both utilities and every time in [0,T][0,T][0,T] where stated. The mission rules out a vacuous dual-attainment hypothesis, a zero default for an unbounded support supremum, and an unconstrained stochastic-integral operator. Contributions proving the source milestones and the analytic lemmas they need are in scope.

Selected references

  • Jakša Cvitanić and Ioannis Karatzas, Convex Duality in Constrained Portfolio Optimization, The Annals of Applied Probability 2(4), 1992, 767–818. DOI: 10.1214/aoap/1177005576.
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