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Bandit AlgorithmsOperations ResearchStatistics·Captain: mikedeng1

Dynamic Pricing with an Unknown Demand Model: Asymptotically Optimal Semi-Myopic Policies III: A Logarithmic Regret Lower Bound with a Known Incumbent PriceResearch Paper

Motivation

A seller who does not know how demand responds to price must learn it from sales while it sells. Each price it charges earns revenue, and each price also reveals something about demand. Choosing prices that serve both purposes is the learn-and-earn problem of dynamic pricing. Its standard yardstick is regret: the expected revenue lost, over a horizon of TTT periods, relative to a seller who knew the demand curve from the start.

Keskin and Zeevi (Operations Research 62(5), 2014) study linear demand with unknown intercept and slope. They show that no policy can have worst-case regret of order below T\sqrt TT​, and that simple least-squares-based policies attain Tlog⁡T\sqrt T \log TT​logT. They then consider a variant that is common in practice. A seller has charged one incumbent price p^\hat pp^​ for a long time and knows the expected demand D^\hat DD^ at that price. Only the slope of the demand curve remains uncertain, and the incumbent price is the only price that carries no information about it. In this variant the achievable regret drops to order log⁡T\log TlogT. This mission formalizes the lower bound: no policy does better than log⁡T\log TlogT (Theorem 3 of the paper). Earlier single-parameter models (Broder and Rusmevichientong, Operations Research 2012) assumed the intercept is known exactly, so that the only uninformative price is zero. The incumbent price model instead has a strictly positive uninformative price, and a seller that charges it stops learning.

Setting

Prices are chosen from an interval [l,u][l,u][l,u] with 0≤l<u0 \le l < u0≤l<u. The seller knows an incumbent price p^∈[l,u]\hat p \in [l,u]p^​∈[l,u] and an incumbent demand D^≠0\hat D \ne 0D^=0. The unknown slope β\betaβ lies in a compact interval B=[bmin⁡,bmax⁡]\mathfrak B = [b_{\min}, b_{\max}]B=[bmin​,bmax​] with bmin⁡<bmax⁡<0b_{\min} < b_{\max} < 0bmin​<bmax​<0. The expected demand at p^\hat pp^​ is D^\hat DD^, which is the incumbent price relation D^=α+βp^\hat D = \alpha + \beta \hat pD^=α+βp^​. Write the price in period ttt as pt=p^+xtp_t = \hat p + x_tpt​=p^​+xt​, where xtx_txt​ is the price deviation. Demand in period ttt is

Dt=D^+βxt+ϵt,t=1,2,…,D_t = \hat D + \beta x_t + \epsilon_t, \qquad t = 1, 2, \dots,Dt​=D^+βxt​+ϵt​,t=1,2,…,

where the demand shocks ϵ1,ϵ2,…\epsilon_1, \epsilon_2, \dotsϵ1​,ϵ2​,… are i.i.d. N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2) with σ>0\sigma > 0σ>0.

The single-period revenue of a deviation xxx is rβ(x)=(p^+x)(D^+βx)r_\beta(x) = (\hat p + x)(\hat D + \beta x)rβ​(x)=(p^​+x)(D^+βx). It is maximized at the optimal deviation

ψ(β)=−p^2−D^2β.\psi(\beta) = -\frac{\hat p}{2} - \frac{\hat D}{2\beta}.ψ(β)=−2p^​​−2βD^​.

The model assumes that the optimal price p^+ψ(β)\hat p + \psi(\beta)p^​+ψ(β) lies strictly inside (l,u)(l,u)(l,u) for every β∈B\beta \in \mathfrak Bβ∈B.

A pricing policy π\piπ is a sequence of measurable functions. The first price π1\pi_1π1​ is a constant, and the price in period t+1t+1t+1 is a function πt+1(Ht)\pi_{t+1}(H_t)πt+1​(Ht​) of the observed history Ht=((D1,p1),…,(Dt,pt))H_t = ((D_1,p_1),\dots,(D_t,p_t))Ht​=((D1​,p1​),…,(Dt​,pt​)), with values in [l,u][l,u][l,u]. A policy never observes β\betaβ or the shocks. The regret of π\piπ under slope β\betaβ over TTT periods is

Δβπ(T)=T rβ(ψ(β))−Eβπ∑t=1Trβ(xt).\Delta^\pi_\beta(T) = T\,r_\beta(\psi(\beta)) - \mathbb E^\pi_\beta \sum_{t=1}^T r_\beta(x_t).Δβπ​(T)=Trβ​(ψ(β))−Eβπ​t=1∑T​rβ​(xt​).

The worst-case regret excludes the slopes at which the incumbent price is itself optimal:

Δπ(T)=sup⁡{Δβπ(T):bmin⁡≤β≤bmax⁡, ψ(β)≠0}.\Delta^\pi(T) = \sup\{\Delta^\pi_\beta(T) : b_{\min} \le \beta \le b_{\max},\ \psi(\beta) \ne 0\}.Δπ(T)=sup{Δβπ​(T):bmin​≤β≤bmax​, ψ(β)=0}.

The accumulated information is measured by J^t=∑s=1txs2\hat J_t = \sum_{s=1}^t x_s^2J^t​=∑s=1t​xs2​; the Fisher information of the history about β\betaβ is σ−2Eβπ[J^t]\sigma^{-2}\mathbb E^\pi_\beta[\hat J_t]σ−2Eβπ​[J^t​].

In Lean these objects are Model (with fields l u pHat DHat bMin bMax σ and the standing assumptions), Policy, pricePath, dev, regret, worstRegret, sqErr and expInfo, all in the namespace KeskinZeevi.IncumbentLowerBound; the i.i.d. N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2) shocks are the shared definition RobustBooking.Shared.GaussianNoise.

Formalization targets

Goal: Theorem 3 (p. 1149)

There is a finite positive constant ccc, depending only on the model, such that for every pricing policy π\piπ and every horizon T≥3T \ge 3T≥3,

Δπ(T)  ≥  clog⁡T.\Delta^\pi(T) \;\ge\; c \log T.Δπ(T)≥clogT.

The constant is not fixed; the statement asserts only the logarithmic rate, uniformly over policies.

Milestones

  1. Lemma 4 (p. 1149). There are finite positive constants c0,c1c_0, c_1c0​,c1​ such that for every policy π\piπ and horizon TTT,
sup⁡β∈B, ψ(β)≠0∑t=2TEβπ(xt−ψ(β))2  ≥  ∑t=2Tc0c1+sup⁡β∈BEβπ[J^t−1].\sup_{\beta\in\mathfrak B,\,\psi(\beta)\ne0} \sum_{t=2}^T \mathbb E^\pi_\beta (x_t-\psi(\beta))^2 \;\ge\; \sum_{t=2}^T \frac{c_0}{c_1 + \sup_{\beta\in\mathfrak B}\mathbb E^\pi_\beta[\hat J_{t-1}]}.β∈B,ψ(β)=0sup​t=2∑T​Eβπ​(xt​−ψ(β))2≥t=2∑T​c1​+supβ∈B​Eβπ​[J^t−1​]c0​​.
  1. The same bound with the information replaced by its trivial maximum (§A.3, p. 1158): the right side with (u−l)2(t−1)(u-l)^2(t-1)(u−l)2(t−1) in place of sup⁡βEβπ[J^t−1]\sup_\beta \mathbb E^\pi_\beta[\hat J_{t-1}]supβ​Eβπ​[J^t−1​].
  2. The regret identity and its lower bound (§A.3, p. 1159): with the constants of Lemma 4,
Δπ(T)=sup⁡β∈B, ψ(β)≠0{−β∑t=1TEβπ(xt−ψ(β))2}  ≥  ∣bmax⁡∣∑t=2Tc0c1+(u−l)2(t−1).\Delta^\pi(T) = \sup_{\beta\in\mathfrak B,\,\psi(\beta)\ne0} \Big\{-\beta\sum_{t=1}^T \mathbb E^\pi_\beta (x_t - \psi(\beta))^2\Big\} \;\ge\; |b_{\max}| \sum_{t=2}^T \frac{c_0}{c_1 + (u-l)^2(t-1)}.Δπ(T)=β∈B,ψ(β)=0sup​{−βt=1∑T​Eβπ​(xt​−ψ(β))2}≥∣bmax​∣t=2∑T​c1​+(u−l)2(t−1)c0​​.
  1. The harmonic bound (§A.3, p. 1159): there are K1,K2>0K_1, K_2 > 0K1​,K2​>0 with Δπ(T)≥K1∑t=1T−11/(K2+t)≥K11+K2∑t=1T−11/t\Delta^\pi(T) \ge K_1\sum_{t=1}^{T-1} 1/(K_2+t) \ge \frac{K_1}{1+K_2}\sum_{t=1}^{T-1} 1/tΔπ(T)≥K1​∑t=1T−1​1/(K2​+t)≥1+K2​K1​​∑t=1T−1​1/t.

Significance

Theorem 3 identifies log⁡T\log TlogT as the minimal asymptotic loss rate of the incumbent price problem. Together with the matching upper bound (Theorem 4 of the paper, a separate mission in this series), it separates two regimes. When both demand parameters are unknown the rate is T\sqrt TT​. When the demand at one strictly positive price is known it is log⁡T\log TlogT, even though an uninformative price exists and a myopic seller can stop learning. The lower bound is what makes "asymptotically optimal" meaningful for the semi-myopic policies the paper proposes. The paper places it next to the logarithmic lower bound of Broder and Rusmevichientong (2012, Theorem 4.5), whose binary-response model has no uninformative action; the incumbent price model adds one.

The result is proved on paper and, as far as the platform's corpus shows, not formalized anywhere. A formal development would produce a reusable model of history-dependent policies driven by i.i.d. noise, a scalar Van Trees (Bayesian Cramér–Rao) inequality for adaptively collected Gaussian data, and a template for minimax regret lower bounds that quantify over all policies. The companion missions of this series (the T\sqrt TT​ lower bound, and the two upper bounds) share the model.

Difficulty

The bound quantifies over every non-anticipating policy, including policies that adapt their exploration to the observed history. A frequentist Cramér–Rao bound does not apply, because a policy's prices are neither unbiased estimators nor fixed designs, and the information Eβπ[J^t]\mathbb E^\pi_\beta[\hat J_t]Eβπ​[J^t​] depends on the unknown β\betaβ through the policy's own choices. A two-point argument that compares two slopes controls the error at one pair of parameters. It does not by itself give the per-period trade-off between information and pricing error that must be summed over ttt. The set over which the worst case is taken also excludes the slope at which the incumbent price is optimal. The lower bound must therefore come from slopes where the seller is forced to deviate from p^\hat pp^​, and every deviation earns information but also costs revenue.

Formalization scope

The model is a Lean structure carrying all standing assumptions as fields: 0≤l<u0 \le l < u0≤l<u, p^∈[l,u]\hat p\in[l,u]p^​∈[l,u], D^≠0\hat D\ne 0D^=0, bmin⁡<bmax⁡<0b_{\min}<b_{\max}<0bmin​<bmax​<0, σ>0\sigma>0σ>0, and interiority of the optimal price p^/2−D^/(2β)\hat p/2-\hat D/(2\beta)p^​/2−D^/(2β) for every β∈B\beta\in\mathfrak Bβ∈B. Two of these are corrections that make implicit hypotheses explicit. The first is p^∈[l,u]\hat p\in[l,u]p^​∈[l,u]: p. 1148 calls p^\hat pp^​ the uninformative price "within the feasible price domain", and the proof uses J^s≤(u−l)2s\hat J_s\le(u-l)^2sJ^s​≤(u−l)2s. The second is D^≠0\hat D\ne0D^=0. With D^=0\hat D = 0D^=0 the optimal price p^/2\hat p/2p^​/2 is known and the theorem is false. The paper's reading is D^>0\hat D>0D^>0, and D^≠0\hat D\neq 0D^=0 is the weaker hypothesis the proof needs.

The optimal deviation ψ\psiψ is the closed form, which equals the maximizer (21) under the interiority assumption. Policies are deterministic. The rule of period t+1t+1t+1 is a Borel measurable map from histories encoded as Fin t → ℝ × ℝ into [l,u][l,u][l,u]. The price process is defined by recursion from the shocks on an arbitrary probability space (Ω,P)(\Omega,P)(Ω,P), which realizes the law of the history under π\piπ and β\betaβ. Lean periods start at 000 (Lean period ttt is the paper's period t+1t+1t+1). Expectations are Bochner integrals of bounded measurable functions. The worst-case regret is a real supremum over the subtype {β∈B:ψ(β)≠0}\{\beta\in\mathfrak B:\psi(\beta)\ne0\}{β∈B:ψ(β)=0}, which is nonempty and on which the regrets are uniformly bounded. The constant ccc is quantified before the probability space, the noise, the policy and the horizon. A statement whose constant may depend on π\piπ or TTT, whose supremum is over an empty or unbounded index set, or whose policies can read β\betaβ would be trivially true or false, and none of these is the theorem stated here.

A complete development needs the scalar Van Trees inequality, Fisher information of the Gaussian location-scale history density, measurability of the price process, and harmonic-sum estimates (Real.log against partial sums of 1/t1/t1/t), on top of Mathlib's gaussianReal, iIndepFun and Bochner integration. The Van Trees inequality and the policy/price-process model are reusable beyond this mission. Proofs of the milestones individually, and a general Van Trees inequality in Mathlib style, are welcome.

Selected references

  • N. Bora Keskin and Assaf Zeevi, Dynamic Pricing with an Unknown Demand Model: Asymptotically Optimal Semi-Myopic Policies, Operations Research 62(5):1142–1167, 2014. https://doi.org/10.1287/opre.2014.1294
  • Josef Broder and Paat Rusmevichientong, Dynamic Pricing Under a General Parametric Choice Model, Operations Research 60(4):965–980, 2012. https://doi.org/10.1287/opre.1120.1057
  • Alexander Goldenshluger and Assaf Zeevi, Woodroofe's One-Armed Bandit Problem Revisited, Annals of Applied Probability 19(4):1603–1633, 2009. https://doi.org/10.1214/08-AAP589
  • Richard D. Gill and Boris Y. Levit, Applications of the van Trees Inequality: A Bayesian Cramér–Rao Bound, Bernoulli 1(1–2):59–79, 1995. https://doi.org/10.2307/3318681
9 thms1 active userReviewed
Linear OptimizationOperations ResearchOptimization+1·Captain: mikedeng1

A Randomized Linear Programming Method for Computing Network Bid Prices II: Directional Derivatives of Expected Perfect-Information Revenue Are Expected LP ValuesResearch Paper

Motivation

Airlines, hotels and railways sell a fixed stock of capacity on several resources at once: a passenger flying from Boston to Los Angeles through Chicago uses a seat on two flight legs. Network revenue management decides which requests to accept, and the standard control is a bid price per leg: accept an itinerary if its fare exceeds the sum of the bid prices of the legs it uses. A good bid price is the marginal expected value of one more unit of capacity.

Talluri and van Ryzin (Transportation Science 33(2), 1999) proposed the randomized linear programming (RLP) method: simulate demand scenarios, solve a linear program with perfect knowledge of each scenario's demand, and average the optimal dual prices. Their main result (a companion mission) says the average is an unbiased estimate of the gradient of expected perfect-information revenue when that gradient exists. This mission is about their §3, the case where it does not: when the LP is degenerate with positive probability, the expected revenue has kinks, averaged dual prices estimate only a supergradient, and the right object is the directional derivative. Proposition 2 of the paper computes it as the expectation of an auxiliary LP value, which again gives an unbiased simulation estimator, now one direction at a time.

Setting

There are mmm legs and nnn itineraries. The incidence matrix A∈{0,1}m×nA \in \{0,1\}^{m \times n}A∈{0,1}m×n has aij=1a_{ij} = 1aij​=1 if itinerary jjj uses leg iii; every column AjA^jAj is nonzero. Fares are r∈Rnr \in \mathbb{R}^nr∈Rn, r≥0r \ge 0r≥0; capacities are x∈Rmx \in \mathbb{R}^mx∈Rm. For a demand vector Y∈RnY \in \mathbb{R}^nY∈Rn, Y≥0Y \ge 0Y≥0, the perfect-information LP value is

v(x,Y)=max⁡{r⊤y:Ay≤x, 0≤y≤Y},v(x, Y) = \max\{r^\top y : Ay \le x,\ 0 \le y \le Y\},v(x,Y)=max{r⊤y:Ay≤x, 0≤y≤Y},

the best revenue obtainable if the demand YYY were known in advance. With YYY a random vector on a probability space (Ω,P)(\Omega, P)(Ω,P), the perfect-information approximation of the value function is JPI(x)=E v(x,Y)J^{PI}(x) = \mathbb{E}\, v(x, Y)JPI(x)=Ev(x,Y).

The Lagrangian of the capacity constraints is

L(x,μ)=∑j=1nYj(rj−μ⊤Aj)++μ⊤x,μ≥0,L(x, \mu) = \sum_{j=1}^n Y^j (r^j - \mu^\top A^j)^+ + \mu^\top x, \qquad \mu \ge 0,L(x,μ)=j=1∑n​Yj(rj−μ⊤Aj)++μ⊤x,μ≥0,

and an optimal vector of dual prices is a minimizer of L(x,⋅)L(x, \cdot)L(x,⋅) over μ≥0\mu \ge 0μ≥0. Since z↦v(z,Y)z \mapsto v(z, Y)z↦v(z,Y) is concave on z≥0z \ge 0z≥0, its superdifferential at xxx is

∂v(x,Y)={μ:v(z,Y)≤v(x,Y)+μ⊤(z−x) for all z≥0}\partial v(x, Y) = \{\mu : v(z, Y) \le v(x, Y) + \mu^\top (z - x) \text{ for all } z \ge 0\}∂v(x,Y)={μ:v(z,Y)≤v(x,Y)+μ⊤(z−x) for all z≥0}

(the paper calls its elements subgradients). For a direction d∈Rmd \in \mathbb{R}^md∈Rm let

u(x,Y;d)=min⁡{d⊤μ:μ an optimal vector of dual prices},u(x, Y; d) = \min\{d^\top \mu : \mu \text{ an optimal vector of dual prices}\},u(x,Y;d)=min{d⊤μ:μ an optimal vector of dual prices},

and let D(x;d)=lim⁡h↓01h[JPI(x+hd)−JPI(x)]D(x; d) = \lim_{h \downarrow 0} \frac1h [J^{PI}(x + hd) - J^{PI}(x)]D(x;d)=limh↓0​h1​[JPI(x+hd)−JPI(x)] be the one-sided directional derivative of JPIJ^{PI}JPI. In Lean these are piValue, JPI, lagr, IsDualOpt, superdiff and u in the namespace RLPBidPrice.Directional.

Formalization targets

Goal: Proposition 2 (corrected)

For xxx with every xi>0x^i > 0xi>0, YYY measurable with Y≥0Y \ge 0Y≥0 almost surely, and every direction ddd,

D(x;d)=lim⁡h↓01h[JPI(x+hd)−JPI(x)]=E u(x,Y;d).D(x; d) = \lim_{h \downarrow 0} \frac1h\big[J^{PI}(x + hd) - J^{PI}(x)\big] = \mathbb{E}\, u(x, Y; d).D(x;d)=h↓0lim​h1​[JPI(x+hd)−JPI(x)]=Eu(x,Y;d).

No condition on the distribution of YYY is imposed, which is the point: this is the nondifferentiable case.

Milestones

  1. Lemma 2. ∣v(x+hei,Y)−v(x,Y)∣≤hmax⁡jrj|v(x + h e^i, Y) - v(x, Y)| \le h \max_j r^j∣v(x+hei,Y)−v(x,Y)∣≤hmaxj​rj for x,Y≥0x, Y \ge 0x,Y≥0, h≥0h \ge 0h≥0.
  2. §3.1, pointwise. An optimal dual price vector μ\muμ satisfies v(z,Y)≤v(x,Y)+μ⊤(z−x)v(z, Y) \le v(x, Y) + \mu^\top(z - x)v(z,Y)≤v(x,Y)+μ⊤(z−x) for all z≥0z \ge 0z≥0.
  3. §3.1, in expectation. For a measurable selection μ(ω)\mu(\omega)μ(ω) of optimal dual prices and x>0x > 0x>0, JPI(z)≤JPI(x)+(Eμ)⊤(z−x)J^{PI}(z) \le J^{PI}(x) + (\mathbb{E}\mu)^\top(z - x)JPI(z)≤JPI(x)+(Eμ)⊤(z−x).
  4. Superdifferential. For x>0x > 0x>0, ∂v(x,Y)\partial v(x, Y)∂v(x,Y) equals the set of optimal dual prices and lies in [0,max⁡jrj]m[0, \max_j r^j]^m[0,maxj​rj]m.
  5. Pointwise directional derivative. For x>0x > 0x>0, lim⁡h↓01h[v(x+hd,Y)−v(x,Y)]=inf⁡{d⊤μ:μ∈∂v(x,Y)}\lim_{h \downarrow 0} \frac1h[v(x + hd, Y) - v(x, Y)] = \inf\{d^\top\mu : \mu \in \partial v(x, Y)\}limh↓0​h1​[v(x+hd,Y)−v(x,Y)]=inf{d⊤μ:μ∈∂v(x,Y)}.
  6. Proposition 1. For a fixed measurable dual selection fff and pairwise independent samples YiY_iYi​ distributed as YYY, 1N∑i≤Nf(Yi)\frac1N\sum_{i \le N} f(Y_i)N1​∑i≤N​f(Yi​) converges almost surely to a supergradient of JPIJ^{PI}JPI at xxx.

Significance

The result. In the differentiable case the RLP bid prices are the averaged dual prices. When degeneracy has positive probability, which happens for discrete demand and for many network structures, Proposition 2 is what remains true: the marginal value of capacity in any direction, in particular in the direction AjA^jAj of an itinerary (the displacement cost of accepting it), is the expectation of a scenario-wise LP quantity. Averaging u(x,Yi;d)u(x, Y_i; d)u(x,Yi​;d) over simulated scenarios is an unbiased estimator of it. Milestone 3 and Proposition 1 say what the plain RLP average estimates in this case (a supergradient), and why the choice of LP algorithm matters for whether it converges at all.

Formalizing it. The paper's argument is a short paragraph; its printed version is not correct as stated (see the scope section), so a machine-checked proof also settles which version holds. The mission produces a formal theory of the parametric LP value v(x,Y)v(x, Y)v(x,Y) in its right-hand side: concavity, the Lipschitz bound, the identification of its superdifferential with the Lagrangian dual optimal set, and its directional derivatives, together with the interchange of a one-sided limit and an expectation. As far as a search of the platform shows, none of this, and no revenue-management gradient result, is formalized yet; the platform's LP sensitivity theorem is for standard-form LPs with a full-row-rank matrix and does not cover this model.

Difficulty

The pointwise facts are classical convex analysis and LP duality, but they have to be proved for a supremum defined over a polytope, not quoted, and Mathlib has no LP duality theorem in this form. The identification of the superdifferential needs strong duality for the LP with the box 0≤y≤Y0 \le y \le Y0≤y≤Y, and the box is exactly where the paper's own formula (22) goes wrong: the dual variables of y≤Yy \le Yy≤Y cannot be dropped.

The step from the pointwise derivative to the expectation is a dominated convergence argument for one-sided difference quotients, which needs a bound uniform in YYY and measurability of ω↦u(x,Y(ω);d)\omega \mapsto u(x, Y(\omega); d)ω↦u(x,Y(ω);d). The obvious route, differentiating under the integral sign as in the differentiable case, is not available: JPIJ^{PI}JPI is not differentiable, and a two-sided limit is false. The measurability of uuu is not given by a formula; it has to come from uuu being a limit of measurable difference quotients.

Formalization scope

Capacities, demands and fares are real vectors indexed by Fin m and Fin n; AAA is a real matrix with 0/1 entries and nonzero columns (IsIncidence A); r≥0r \ge 0r≥0. The paper's remaining-time index kkk is notation only and is dropped. vvv is a real sSup over the feasible objective values: for x≥0x \ge 0x≥0, Y≥0Y \ge 0Y≥0 it is the LP maximum, and otherwise it is 000, so every statement assumes x≥0x \ge 0x≥0 or x>0x > 0x>0 and Y≥0Y \ge 0Y≥0 (almost surely), and the superdifferential is taken over z≥0z \ge 0z≥0 only. Optimal dual prices are defined through the Lagrangian (13)–(14); they are the μ\muμ-parts of the optimal solutions of the LP dual. uuu is a real sInf, which would be 000 on an empty set; for x>0x > 0x>0 the dual optimal set is nonempty and bounded, so uuu is an attained minimum and the goal is not vacuous. Directional derivatives are one-sided limits (nhdsWithin 0 (Set.Ioi 0)). Expectations are Bochner integrals; no integrability of YYY is assumed or needed, since vvv and uuu are bounded.

The following corrections to the printed text are part of the statements, each with a counterexample to the printed version:

  • Eq. (22) omits the duals of y≤Yy \le Yy≤Y: with one leg, one itinerary, r=1r = 1r=1, x=1x = 1x=1, YYY uniform on [0,2][0, 2][0,2], D(1;1)=1/2D(1; 1) = 1/2D(1;1)=1/2, but the printed (22) gives E u=3/4\mathbb{E}\,u = 3/4Eu=3/4. Here uuu minimizes over the optimal dual prices of (14).
  • The superdifferential formula in the proof of Proposition 2 has the same omission: for r=1r = 1r=1, x=1x = 1x=1, Y=1/2Y = 1/2Y=1/2 the printed set is {1/2}\{1/2\}{1/2}, the true one {0}\{0\}{0}.
  • The §3.1 inequality is printed with ≥\ge≥; vvv is concave, and r=1r = 1r=1, Y=5Y = 5Y=5, x=1x = 1x=1, μ=1\mu = 1μ=1, z=10z = 10z=10 gives 5≥105 \ge 105≥10. The expectation version also misprints z−yz - yz−y for z−xz - xz−x.
  • x>0x > 0x>0 is implicit: at a zero capacity the dual prices of that leg are unbounded and a direction leaving x≥0x \ge 0x≥0 makes the LP infeasible.
  • Proposition 1 is formalized for an algorithm returning a fixed measurable function of the current demand ("initialized with the same data on each run"), with "always exists" read as almost sure convergence.

A statement of the goal with the printed (22), or with uuu defined over an arbitrary or empty set so that sInf returns 000, or with a two-sided limit, is ruled out: the first two are false or vacuous for the reasons above, the third is false.

A complete development needs LP duality for max⁡{r⊤y:Ay≤x,0≤y≤Y}\max\{r^\top y : Ay \le x, 0 \le y \le Y\}max{r⊤y:Ay≤x,0≤y≤Y}, concavity and the Lipschitz bound of the value function, the directional derivative of a finite concave function on an open set, and dominated convergence (Mathlib's MeasureTheory.tendsto_integral_filter_of_dominated_convergence); Proposition 1 uses ProbabilityTheory.strong_law_ae. The LP duality and parametric value-function results are reusable for any mission about LP-based bid prices or two-stage stochastic programs. Contributions of any milestone separately are welcome.

Selected references

  • K. Talluri, G. van Ryzin, A Randomized Linear Programming Method for Computing Network Bid Prices, Transportation Science 33(2):207–216, 1999. https://doi.org/10.1287/trsc.33.2.207
  • M. S. Bazaraa, H. D. Sherali, C. M. Shetty, Nonlinear Programming: Theory and Algorithms, 2nd ed., Wiley, 1993 (the paper cites p. 218 of this edition; 3rd ed. 2006: https://doi.org/10.1002/0471787779).
  • K. Talluri, G. van Ryzin, An Analysis of Bid-Price Controls for Network Revenue Management, Management Science 44(11):1577–1593, 1998. https://doi.org/10.1287/mnsc.44.11.1577
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Linear OptimizationOperations ResearchOptimization+1·Captain: mikedeng1

A Randomized Linear Programming Method for Computing Network Bid Prices I: Averaged LP Dual Prices Are an Unbiased Estimate of the Gradient of Expected Perfect-Information RevenueResearch Paper

Motivation

Airlines, hotels and railways sell fixed capacity on networks of resources. In network revenue management a request for an itinerary that uses several flight legs is accepted or rejected in real time, and the dominant industrial control is the bid-price control: every leg carries a price, and a request is accepted only if its fare is at least the sum of the bid prices of the legs it uses. A good bid price is the marginal expected value of one more seat on the leg, which is a gradient of an expected-revenue function with respect to capacity.

The classical way to compute bid prices, the deterministic linear program, replaces random demand by its mean and reads off the dual prices of the capacity constraints. It ignores all distributional information and gives a zero bid price to every leg whose mean demand is below capacity. Talluri and van Ryzin (Transp. Sci. 33(2), 1999) studied the randomized linear programming (RLP) method instead: simulate demand vectors Y1,…,YNY_1, \dots, Y_NY1​,…,YN​, solve one linear program per sample with the realized demand as an upper bound, and average the dual prices. Their Theorem 1 asserts that this average is an unbiased estimator of the gradient of the expected perfect-information revenue. For one leg and one fare class it recovers Littlewood's rule, ddxE v(x,Y)=r P(Y>x)\frac{d}{dx}\mathbb{E}\,v(x,Y) = r\,P(Y > x)dxd​Ev(x,Y)=rP(Y>x) (Littlewood 1972, cited on p. 209 of the paper).

Setting

A network has mmm legs and nnn itineraries. The incidence matrix A∈{0,1}m×nA \in \{0,1\}^{m\times n}A∈{0,1}m×n has aij=1a_{ij} = 1aij​=1 exactly when itinerary jjj uses leg iii, and every column AjA^jAj is nonzero. Fares are r=(r1,…,rn)≥0r = (r^1, \dots, r^n) \ge 0r=(r1,…,rn)≥0 and capacities are a real vector x≥0x \ge 0x≥0. Demand to come is a random vector Y=(Y1,…,Yn)≥0Y = (Y^1, \dots, Y^n) \ge 0Y=(Y1,…,Yn)≥0 on a probability space (Ω,P)(\Omega, P)(Ω,P).

The perfect-information LP value is

v(x,Y)=max⁡{ r⊤y  :  Ay≤x, 0≤y≤Y },v(x, Y) = \max\{\, r^\top y \;:\; Ay \le x,\ 0 \le y \le Y \,\},v(x,Y)=max{r⊤y:Ay≤x, 0≤y≤Y},

the revenue obtainable if the demand were known in advance, and the perfect-information approximation of the value function is JPI(x)=E v(x,Y)J^{PI}(x) = \mathbb{E}\,v(x, Y)JPI(x)=Ev(x,Y). The Lagrangian dual function of the capacity constraints is

L(x,μ)=∑j=1nYj (rj−μ⊤Aj)++μ⊤x,L(x, \mu) = \sum_{j=1}^n Y^j\,(r^j - \mu^\top A^j)^+ + \mu^\top x ,L(x,μ)=j=1∑n​Yj(rj−μ⊤Aj)++μ⊤x,

and an optimal dual price vector μ(x,Y)\mu(x, Y)μ(x,Y) is a minimizer of L(x,⋅)L(x, \cdot)L(x,⋅) over μ≥0\mu \ge 0μ≥0. In Lean these are piValue, JPI, lagr and IsDualOpt in the namespace RLPBidPrice.Unbiased.

Two conditions govern the result. Condition C1′: whenever xxx lies in the linear span of a set of columns of [A I][A\ I][A I] (columns of AAA and unit vectors eie^iei), that set spans Rm\mathbb{R}^mRm. Condition 2: every distribution function t↦P(Yj≤t)t \mapsto P(Y^j \le t)t↦P(Yj≤t) is continuous. The components Y1,…,YnY^1, \dots, Y^nY1,…,Yn are also assumed mutually independent.

Formalization targets

Goal: Theorem 1 (corrected)

Under C1′, Condition 2 and independence,

∇xE v(x,Y)=E ∇xv(x,Y)=E μ(x,Y).\nabla_x \mathbb{E}\,v(x, Y) = \mathbb{E}\,\nabla_x v(x, Y) = \mathbb{E}\,\mu(x, Y).∇x​Ev(x,Y)=E∇x​v(x,Y)=Eμ(x,Y).

In Lean (theorem1_unbiased_gradient) this is three clauses: v(⋅,Y)v(\cdot, Y)v(⋅,Y) is differentiable at xxx almost surely; JPIJ^{PI}JPI is Fréchet differentiable at xxx with derivative the expectation of the pathwise derivatives; and for every measurable, almost surely optimal dual selection μ\muμ, JPIJ^{PI}JPI has gradient E μ(x,Y)\mathbb{E}\,\mu(x, Y)Eμ(x,Y) at xxx.

Milestones

  1. Lemma 1 (Glasserman): a random function that is Lipschitz in θ\thetaθ with a constant KKK and almost surely differentiable at θ\thetaθ can be differentiated under the expectation.
  2. Lemma 2: ∣v(x+hei,Y)−v(x,Y)∣≤h rˉ|v(x + h e^i, Y) - v(x, Y)| \le h\,\bar r∣v(x+hei,Y)−v(x,Y)∣≤hrˉ with rˉ=max⁡jrj\bar r = \max_j r^jrˉ=maxj​rj.
  3. Differentiability and uniqueness (§2.1, p. 210): for x>0x > 0x>0, v(⋅,Y)v(\cdot, Y)v(⋅,Y) is differentiable at xxx if and only if the optimal dual price vector is unique.
  4. Strong duality (§2.1, p. 211): an optimal μ∗\mu_*μ∗​ exists, v(x,Y)=L(x,μ∗)v(x, Y) = L(x, \mu_*)v(x,Y)=L(x,μ∗​), v(z,Y)≤v(x,Y)+μ∗⊤(z−x)v(z, Y) \le v(x, Y) + \mu_*^\top(z - x)v(z,Y)≤v(x,Y)+μ∗⊤​(z−x) for all z≥0z \ge 0z≥0, and a unique μ∗\mu_*μ∗​ is the gradient at x>0x > 0x>0.
  5. Lemma 3 (corrected): under C1′, a feasible direction ddd from μ∗\mu_*μ∗​ with d⊤Aj=0d^\top A^j = 0d⊤Aj=0 on the index sets E0∪E1E_0 \cup E_1E0​∪E1​ of Eqs. (16)–(17) and d⊤x=0d^\top x = 0d⊤x=0 is zero.
  6. Lemma 4 (corrected): under C1′, Condition 2 and independence, ∇xv(x,Y)\nabla_x v(x, Y)∇x​v(x,Y) exists with probability one.

Significance

The theorem justifies a widely used method: it says that the simple procedure of averaging simulated LP dual prices targets the gradient of a well-defined expected-revenue function, and by the strong law of large numbers the average is also consistent. It separates the RLP method from the deterministic LP, whose dual prices are gradients of a different function, and it isolates exactly when that justification fails (degenerate LPs with positive probability, discussed in §2.2 of the paper and treated by directional derivatives in its §3).

The printed statement is false, and the formalization records that. Condition 1 of the paper looks only at the columns of AAA and ignores the slack columns of Ay≤xAy \le xAy≤x; the paper's Condition 2 is marginal and does not rule out dependent demands whose sum hits capacity. The corrected statement, with C1′ and independence, is the one this mission targets. No machine-checked version of this result, or of LP sensitivity analysis under random right-hand sides of this kind, is known to exist; formalizing it gives a checked statement of the hypotheses under which the RLP estimator is unbiased.

Difficulty

The pathwise facts are LP duality; the delicate step is the almost-sure uniqueness of the dual prices. Degeneracy of an LP is a condition on finitely many bases, but the set of dual optima depends on YYY, and the natural argument that fixes a direction ddd and shows that d⊤(x−∑jYjAj)=0d^\top(x - \sum_{j} Y^j A^j) = 0d⊤(x−∑j​YjAj)=0 has probability zero does not work as written: the direction depends on YYY, and a direction that improves the Lagrangian may leave the orthant μ≥0\mu \ge 0μ≥0. This is precisely where the printed Condition 1 fails. A second difficulty is the passage from almost-sure differentiability of v(⋅,Y)v(\cdot, Y)v(⋅,Y) to a full Fréchet derivative of JPIJ^{PI}JPI on Rm\mathbb{R}^mRm, with the measurability of the random derivative and of the dual selection.

Formalization scope

Legs and itineraries are Fin m and Fin n; AAA is a real matrix with entries in {0,1}\{0,1\}{0,1} and nonzero columns; capacities are real vectors. The paper's remaining-time index kkk is notation only and is dropped. vvv is a real sSup over feasible objective values; since the feasible set is empty when xxx or YYY has a negative entry (the value is then 000), every statement assumes x≥0x \ge 0x≥0 and Y≥0Y \ge 0Y≥0 almost surely, and derivatives are taken where xxx is interior (C1′ forces xi≠0x^i \neq 0xi=0). Optimal dual prices are minimizers of the Lagrangian (13) over μ≥0\mu \ge 0μ≥0, which are the μ\muμ-parts of the optimal solutions of the LP dual of (6)–(8). Gradients are Fréchet derivatives on Fin m → ℝ, encoded by the linear functional h↦∑igihih \mapsto \sum_i g^i h^ih↦∑i​gihi (gradCLM g). Condition 2 is continuity of t↦P(Yj≤t)t \mapsto P(Y^j \le t)t↦P(Yj≤t); independence is iIndepFun. YYY is measurable; no integrability of YYY is assumed, since 0≤v(x,Y)≤rˉ∑ixi0 \le v(x, Y) \le \bar r\sum_i x^i0≤v(x,Y)≤rˉ∑i​xi.

Every correction is labelled in the statements. C1 → C1′: with AAA having rows (0,1,1),(1,1,0),(1,0,1)(0,1,1),(1,1,0),(1,0,1)(0,1,1),(1,1,0),(1,0,1), r=(100,1,1)r = (100,1,1)r=(100,1,1), x=(1,1,1)x = (1,1,1)x=(1,1,1) and YjY^jYj i.i.d. uniform on [0,2][0,2][0,2], Conditions 1 and 2 hold but E v(⋅,Y)\mathbb{E}\,v(\cdot, Y)Ev(⋅,Y) has one-sided slopes of about 0.740.740.74 and 50.550.550.5 in the second coordinate at xxx. Independence added: with one leg, x=1x = 1x=1, fares (2,1)(2,1)(2,1) and Y2=1−Y1Y^2 = 1 - Y^1Y2=1−Y1, Y1Y^1Y1 uniform on [0,1][0,1][0,1], the LP is degenerate almost surely. Implicit hypotheses made explicit: x≥0x \ge 0x≥0, Y≥0Y \ge 0Y≥0, r≥0r \ge 0r≥0 (Lemma 2's bound needs rˉ≥0\bar r \ge 0rˉ≥0), nonzero 0/1 columns.

The goal is not trivialized by a selection: it states the selection-free identity ∇xE v=E ∇xv\nabla_x \mathbb{E}\,v = \mathbb{E}\,\nabla_x v∇x​Ev=E∇x​v, and the dual-price form quantifies only over measurable selections that are optimal almost surely; it assumes neither almost-sure differentiability, nor almost-sure uniqueness of the dual, nor a joint density, nor nondegeneracy.

A complete development needs LP duality for bounded-variable LPs in Lagrangian form, concave polyhedral functions and their superdifferentials, a finite enumeration of bases of [A I][A\ I][A I], and differentiation under the integral sign for Lipschitz integrands (Mathlib has hasFDerivAt_integral_of_dominated_loc_of_lip). The LP duality and sensitivity results are reusable for other revenue-management and stochastic-programming missions. Contributions of any milestone, of the counterexamples as formal statements, and of alternative proofs are welcome.

Selected references

  • K. Talluri, G. van Ryzin, A Randomized Linear Programming Method for Computing Network Bid Prices, Transportation Science 33(2):207–216, 1999. https://doi.org/10.1287/trsc.33.2.207
  • P. Glasserman, Perturbation Analysis of Production Networks, in D. Yao (ed.), Stochastic Modeling and Analysis of Manufacturing Systems, Springer-Verlag, Berlin, 1994 (source of Lemma 1; as cited in the paper).
  • K. Littlewood, Forecasting and Control of Passengers, 12th AGIFORS Symposium Proceedings, 1972 (as cited in the paper).
  • M. S. Bazaraa, H. D. Sherali, C. M. Shetty, Nonlinear Programming: Theory and Algorithms, John Wiley, New York, 1993, Chapter 6 (Lagrangian duality; as cited in the paper).
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Dynamic ProgrammingOperations ResearchProbability·Captain: mikedeng1

Airline Yield Management with Overbooking, Cancellations, and No-Shows I: Time- and State-Dependent Booking Limits Are OptimalResearch Paper

Motivation

Airlines sell the seats of one flight leg in several fare classes over a booking horizon of weeks. Each time a request arrives, the booking agent must decide whether to sell a seat now at the requested fare or keep it for a later, possibly higher-paying, customer. Real reservations are also cancelled, and some ticket holders fail to show up at departure, so airlines deliberately overbook and pay a penalty when more passengers show up than the airplane can carry. The question this mission formalizes is what an optimal accept/reject rule looks like when all three effects (multiple fares, cancellations, no-shows) are present.

For the model without cancellations and no-shows, Lee and Hersh (Transp. Sci. 27(3), 1993) showed that the optimal rule is given by booking limits: in each period and for each fare class there is a threshold on the number of seats sold, and a request is accepted exactly when the current bookings are below it. Subramanian, Stidham and Lautenbacher (Transp. Sci. 33(2), 1999) extend the model to state-dependent cancellations and binomial no-shows with a convex overbooking penalty. Their §1 shows that booking limits, now depending on both the stage and the fare class, are still optimal. The structural step behind this is the concavity of the value function, in the style of Lippman and Stidham's analysis of admission control to a queue (Oper. Res. 25(2), 1977).

Setting

There are mmm fare classes and NNN stages n=N,N−1,…,0n = N, N-1, \dots, 0n=N,N−1,…,0, counting the periods remaining: stage NNN opens reservations, stage 000 is departure. The state x∈{0,1,2,… }x \in \{0,1,2,\dots\}x∈{0,1,2,…} is the number of seats reserved. At each stage n≥1n \ge 1n≥1 exactly one event happens:

  • a request in fare class iii, with probability pin≥0p_{in} \ge 0pin​≥0;
  • a cancellation, with probability qn(x)q_n(x)qn​(x), which is non-negative, nondecreasing and concave in xxx, with qn(0)=0q_n(0) = 0qn​(0)=0;
  • nothing, with probability p0n(x)=1−∑ipin−qn(x)p_{0n}(x) = 1 - \sum_i p_{in} - q_n(x)p0n​(x)=1−∑i​pin​−qn​(x) (Eq. (1)).

Accepting a class-iii request at stage nnn earns rin≥0r_{in} \ge 0rin​≥0. At departure each reservation holder independently shows up with probability 1−β1 - \beta1−β (0≤β≤10 \le \beta \le 10≤β≤1), so the number who show up is Y(x)∼Bin(x,1−β)Y(x) \sim \mathrm{Bin}(x, 1-\beta)Y(x)∼Bin(x,1−β). If Y(x)=yY(x) = yY(x)=y, an overbooking penalty π(y)\pi(y)π(y) is paid. Here π\piπ is non-negative, convex and nondecreasing on y≥0y \ge 0y≥0, and π(y)=0\pi(y) = 0π(y)=0 for y≤Cy \le Cy≤C, the capacity. Starting empty and accepting at most one request per stage, the states reachable at stage nnn are 0≤x≤N−n0 \le x \le N - n0≤x≤N−n, and p0n(x)≥0p_{0n}(x) \ge 0p0n​(x)≥0 is assumed on that range.

The value functions UnU_nUn​ are defined by the recursion (2)–(3):

U0(x)=E[−π(Y(x))],U_0(x) = \mathrm{E}\big[-\pi(Y(x))\big],U0​(x)=E[−π(Y(x))], Un(x)=∑i=1mpinmax⁡{rin+Un−1(x+1), Un−1(x)}+qn(x) Un−1(x−1)+p0n(x) Un−1(x).U_n(x) = \sum_{i=1}^m p_{in}\max\{r_{in} + U_{n-1}(x+1),\,U_{n-1}(x)\} + q_n(x)\,U_{n-1}(x-1) + p_{0n}(x)\,U_{n-1}(x).Un​(x)=i=1∑m​pin​max{rin​+Un−1​(x+1),Un−1​(x)}+qn​(x)Un−1​(x−1)+p0n​(x)Un−1​(x).

The first branch of each maximum is "accept", the second "reject". The booking limit of class iii at stage nnn is Eq. (7):

bin=min⁡{x:Un−1(x)−Un−1(x+1)>rin},b_{in} = \min\{x : U_{n-1}(x) - U_{n-1}(x+1) > r_{in}\},bin​=min{x:Un−1​(x)−Un−1​(x+1)>rin​},

with bin=∞b_{in} = \inftybin​=∞ when there is no such xxx. The difference Un−1(x)−Un−1(x+1)U_{n-1}(x) - U_{n-1}(x+1)Un−1​(x)−Un−1​(x+1) is the opportunity cost of one more booking. In Lean all of this is AirlineYieldMgmt.BookingLimits.Model with Model.U, Model.p0, Model.Standing and Model.bookingLimit.

Formalization targets

Goal: booking limits are optimal (§1, Eq. (7), p. 151)

For every stage 1≤n≤N1 \le n \le N1≤n≤N, fare class iii and reachable state 0≤x≤N−n0 \le x \le N - n0≤x≤N−n,

rin+Un−1(x+1)  ≥  Un−1(x)  ⟺  x<bin.r_{in} + U_{n-1}(x+1) \;\ge\; U_{n-1}(x) \iff x < b_{in}.rin​+Un−1​(x+1)≥Un−1​(x)⟺x<bin​.

The optimal rule accepts a class-iii request exactly while fewer than binb_{in}bin​ seats are booked.

Milestones

  1. Lemma 1 (p. 151). If fff is nondecreasing and convex on y≥0y \ge 0y≥0 and 0<γ<10 < \gamma < 10<γ<1, then h(x)=Ef(Bin(x,γ))h(x) = \mathrm{E} f(\mathrm{Bin}(x,\gamma))h(x)=Ef(Bin(x,γ)) is nondecreasing and convex in x∈{0,1,… }x \in \{0,1,\dots\}x∈{0,1,…}.
  2. Terminal value (p. 151). U0U_0U0​ is concave and nonincreasing.
  3. All stages (p. 151). For every 0≤n≤N0 \le n \le N0≤n≤N, UnU_nUn​ is nonincreasing and concave on {0,…,N−n}\{0,\dots,N-n\}{0,…,N−n}, so Un(x)−Un(x+1)U_n(x) - U_n(x+1)Un​(x)−Un​(x+1) is nondecreasing in x=0,…,N−n−1x = 0,\dots,N-n-1x=0,…,N−n−1.

Significance

The result. Booking limits are how single-leg seat inventory is controlled in practice. The theorem says this simple class of rules loses nothing, even with cancellations whose rate grows with the number of bookings and with random no-shows at departure. The limits depend on the stage, and they need not be nested across classes (Remark 3 of the paper). The same concavity property identifies Un(x)−Un(x+1)U_n(x) - U_n(x+1)Un​(x)−Un​(x+1) as the optimal bid price for the leg. The companion mission (II, equivalent charging) reduces a model with class-dependent refunds to this one-dimensional recursion, so a formal proof of the present goal is the input needed to carry booking-limit optimality over to that model.

Formalizing it. The paper proves neither the concavity induction nor Lemma 1. It cites Lippman and Stidham (1977, Theorem 1) for the first and Shaked and Shanthikumar (1994, Example 6.A.2) for the second. The authors note that the cited induction carries over to their recursion (p. 151), but neither source states the result for exactly this recursion, with its state-dependent cancellation term and range-restricted probabilities. A machine-checked proof would therefore supply an argument the paper only points to, not just its bookkeeping. To our knowledge none of these statements has a machine-checked proof.

Difficulty

The goal follows quickly once milestone 3 is available. The work is in milestone 3. The obvious induction pushes concavity through each term of the recursion. It fails at the cancellation term qn(x) Un−1(x−1)q_n(x)\,U_{n-1}(x-1)qn​(x)Un−1​(x−1): a product of a concave nondecreasing function and a concave nonincreasing one is not concave in general, so the term is not concave by itself. The null-event term p0n(x) Un−1(x)p_{0n}(x)\,U_{n-1}(x)p0n​(x)Un−1​(x) has the same problem, because its coefficient depends on the state. Only the combination of the two terms, together with ∑ipin+qn(x)≤1\sum_i p_{in} + q_n(x) \le 1∑i​pin​+qn​(x)≤1 on the reachable range, keeps the result concave. That constraint holds only on the range, not for every xxx: in the linear case qn(x)=qnxq_n(x) = q_n xqn​(x)=qn​x it fails for large xxx. This interaction between the range and the induction has to be handled with care. Lemma 1 is a separate, self-contained piece of discrete probability about binomial sums.

Formalization scope

  • Fare classes are Fin m; the paper's class iii is i.val + 1. Stages and states are ℕ; probabilities, fares, β\betaβ, π\piπ and values are ℝ.
  • Model.U is defined by structural recursion on the stage, for every x∈Nx \in \mathbb Nx∈N. Every theorem restricts its hypotheses and conclusions to the paper's range 0≤x≤N−n0 \le x \le N - n0≤x≤N−n.
  • x−1x - 1x−1 is natural-number subtraction. At x=0x = 0x=0 it is multiplied by qn(0)=0q_n(0) = 0qn​(0)=0, a convention the page leaves implicit (a cancellation needs a reservation).
  • The null-event probability is defined by Eq. (1), and its non-negativity is assumed only for 1≤n≤N1 \le n \le N1≤n≤N, 0≤x≤N−n0 \le x \le N-n0≤x≤N−n. This keeps the paper's linear-cancellation case inside the model.
  • Concavity, convexity and monotonicity of functions on N\mathbb NN are discrete (differences). π\piπ is a real function, convex and nondecreasing on [0,∞)[0,\infty)[0,∞) as on the page.
  • Binomial expectations are finite sums ∑k=0x(xk)γk(1−γ)x−kf(k)\sum_{k=0}^x \binom xk \gamma^k(1-\gamma)^{x-k} f(k)∑k=0x​(kx​)γk(1−γ)x−kf(k). The milestone for U0U_0U0​ allows 0≤β≤10 \le \beta \le 10≤β≤1.
  • The minimum in (7) ranges over the reachable states and lives in WithTop ℕ, with ⊤ meaning bin=∞b_{in} = \inftybin​=∞.
  • "An optimal policy accepts" means the accept branch attains the maximum in (2). No dynamic-programming optimality principle, policy space or claim about expected revenue is stated.
  • Ruling out the trivializing formalization: binb_{in}bin​ is defined by Eq. (7) as a minimum of a strict-inequality set. It is not defined as the number of states where acceptance is optimal, a definition under which the goal would hold by construction and lose its content (that the accepted states form an initial segment).
  • A proof needs finite binomial sums and discrete concavity arguments; Mathlib covers both. The discrete-concavity and binomial lemmas would carry over to other admission-control and inventory models. Proofs of any milestone, and of the goal assuming milestone 3, are welcome separately.

Selected references

  • J. Subramanian, S. Stidham Jr., C. J. Lautenbacher, Airline Yield Management with Overbooking, Cancellations, and No-Shows, Transportation Science 33(2), 147–167, 1999. https://doi.org/10.1287/trsc.33.2.147
  • S. A. Lippman, S. Stidham Jr., Individual versus Social Optimization in Exponential Congestion Systems, Operations Research 25(2), 233–247, 1977. https://doi.org/10.1287/opre.25.2.233
  • T. C. Lee, M. Hersh, A Model for Dynamic Airline Seat Inventory Control with Multiple Seat Bookings, Transportation Science 27(3), 252–265, 1993. https://doi.org/10.1287/trsc.27.3.252
  • M. Shaked, J. G. Shanthikumar, Stochastic Orders and Their Applications, Academic Press, San Diego, 1994 (Example 6.A.2).
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Dynamic ProgrammingOperations ResearchOptimization·Captain: mikedeng1

Dynamic Pricing Strategies with Reference Effects I: Under Loss Aversion the Steady States Form an Interval and Optimal Paths ConvergeResearch Paper

Motivation

Consumers judge a price against a reference price, an internal standard formed from the prices they have seen before. A price below the reference is perceived as a gain and stimulates demand; a price above it is perceived as a loss and depresses demand. Prospect theory (Kahneman and Tversky 1979) adds that losses loom larger than gains of the same size: this is loss aversion. A firm that sets prices over many periods therefore faces a dynamic trade-off, because today's price moves tomorrow's reference price and with it tomorrow's demand.

Popescu and Wu (Operations Research 55(3), 2007) analyze this problem for general nonlinear demand. Earlier work of Kopalle, Rao and Assunção (1996) and of Fibich, Gavious and Lowengart (2003) had treated linear or piecewise-linear reference effects with explicit solutions. Popescu and Wu replace explicit solutions by structural arguments (supermodularity, monotone policies, comparison of value functions), which is what makes the results reusable for any demand model satisfying their assumptions. Their headline result for loss-averse consumers is that the long-run prices form a whole interval rather than a single point, and that optimal prices outside the interval move monotonically to its nearer endpoint.

Setting

A monopolist chooses a price ptp_tpt​ from P=[0,pˉ]P=[0,\bar p]P=[0,pˉ​], pˉ>0\bar p>0pˉ​>0, in each period t=0,1,2,…t=0,1,2,\dotst=0,1,2,…. The reference price follows exponential smoothing,

rt+1=αrt+(1−α)pt,α∈[0,1),r_{t+1}=\alpha r_t+(1-\alpha)p_t,\qquad \alpha\in[0,1),rt+1​=αrt​+(1−α)pt​,α∈[0,1),

from a given initial reference price r0r_0r0​. Demand is D(p,r)=d(p)+R(r−p,r)D(p,r)=d(p)+R(r-p,r)D(p,r)=d(p)+R(r−p,r), where d(p)=D(p,p)d(p)=D(p,p)d(p)=D(p,p) is the base demand and R(x,r)R(x,r)R(x,r) is the reference effect of the perceived gain x=r−px=r-px=r−p, so that R(0,r)=0R(0,r)=0R(0,r)=0. The per-period profit (zero unit cost) is Π(p,r)=p D(p,r)\Pi(p,r)=p\,D(p,r)Π(p,r)=pD(p,r), the base profit is π(p)=p d(p)\pi(p)=p\,d(p)π(p)=pd(p), and λ(r)\lambda(r)λ(r) denotes the slope of R(⋅,r)R(\cdot,r)R(⋅,r) at x=0x=0x=0.

For a discount factor β∈(0,1)\beta\in(0,1)β∈(0,1), the value function is the supremum of discounted profit over all price sequences in PPP:

V(r0)=sup⁡(pt)∈PN∑t≥0βt Π(pt,rt).V(r_0)=\sup_{(p_t)\in P^{\mathbb N}}\sum_{t\ge 0}\beta^t\,\Pi(p_t,r_t).V(r0​)=(pt​)∈PNsup​t≥0∑​βtΠ(pt​,rt​).

The Bellman objective is W(p,r)=Π(p,r)+βV(αr+(1−α)p)W(p,r)=\Pi(p,r)+\beta V(\alpha r+(1-\alpha)p)W(p,r)=Π(p,r)+βV(αr+(1−α)p). The optimal pricing policy p∗(r)p^*(r)p∗(r) is the largest maximizer of W(⋅,r)W(\cdot,r)W(⋅,r) over PPP, and q∗(r)=αr+(1−α)p∗(r)q^*(r)=\alpha r+(1-\alpha)p^*(r)q∗(r)=αr+(1−α)p∗(r) is the next reference price. The state path is rt+1∗=q∗(rt∗)r^*_{t+1}=q^*(r^*_t)rt+1∗​=q∗(rt∗​) and the price path is pt∗=p∗(rt∗)p^*_t=p^*(r^*_t)pt∗​=p∗(rt∗​). A steady state is a price p∗∗∈Pp^{**}\in Pp∗∗∈P with p∗(p∗∗)=p∗∗p^*(p^{**})=p^{**}p∗(p∗∗)=p∗∗.

The standing Assumption 1 requires DDD to be nonnegative, bounded and continuous, decreasing in ppp, increasing in rrr, and RRR increasing in xxx. For a smooth (loss-neutral) RRR, Assumptions 2–3 require RRR to be twice differentiable, π\piπ to be nonmonotonic and concave, π′(r)−rλ(r)\pi'(r)-r\lambda(r)π′(r)−rλ(r) to be strictly decreasing, and the reference profit ΠR(p,r)=pR(r−p,r)\Pi^R(p,r)=pR(r-p,r)ΠR(p,r)=pR(r−p,r) to be concave in ppp and supermodular.

Under loss aversion the reference effect is kinked: RK(x,r)=RG(x,r)R_K(x,r)=R_G(x,r)RK​(x,r)=RG​(x,r) for gains x≥0x\ge 0x≥0 and RK(x,r)=RL(x,r)R_K(x,r)=R_L(x,r)RK​(x,r)=RL​(x,r) for losses x<0x<0x<0. Assumption 4 makes RGR_GRG​ and RLR_LRL​ twice differentiable and increasing in xxx, makes RG−RLR_G-R_LRG​−RL​ single crossing, and imposes λL(r)>λG(r)\lambda_L(r)>\lambda_G(r)λL​(r)>λG​(r). Assumption 5 requires the gain and loss profits to satisfy Assumption 3. The problems (K)(K)(K), (PL)(P_L)(PL​) and (PG)(P_G)(PG​) are the pricing problem with reference effect RKR_KRK​, RLR_LRL​ and RGR_GRG​, respectively, and (Pθ)(P_\theta)(Pθ​) uses Rθ=θRG+(1−θ)RLR_\theta=\theta R_G+(1-\theta)R_LRθ​=θRG​+(1−θ)RL​ for θ∈[0,1]\theta\in[0,1]θ∈[0,1].

Formalization targets

Goal: Theorem 4 of the paper

There exist prices pL∗∗≤pG∗∗p^{**}_L\le p^{**}_GpL∗∗​≤pG∗∗​ such that pL∗∗p^{**}_LpL∗∗​ is the unique steady state of (PL)(P_L)(PL​), pG∗∗p^{**}_GpG∗∗​ is the unique steady state of (PG)(P_G)(PG​), and

{ r: r is a steady state of (K) }=[pL∗∗,pG∗∗].\{\,r:\ r \text{ is a steady state of }(K)\,\}=[p^{**}_L,p^{**}_G].{r: r is a steady state of (K)}=[pL∗∗​,pG∗∗​].

Moreover, the following hold:

  • from r0∈[pL∗∗,pG∗∗]r_0\in[p^{**}_L,p^{**}_G]r0​∈[pL∗∗​,pG∗∗​], the optimal price path of (K)(K)(K) is constant, pt∗=r0p^*_t=r_0pt∗​=r0​;
  • from r0<pL∗∗r_0<p^{**}_Lr0​<pL∗∗​, the state path of (K)(K)(K) is nondecreasing and converges to pL∗∗p^{**}_LpL∗∗​, and so does the price path;
  • from r0>pG∗∗r_0>p^{**}_Gr0​>pG∗∗​, the state path is nonincreasing and converges to pG∗∗p^{**}_GpG∗∗​, and so does the price path.

Milestones

In attack order, the milestones are:

  • Remark 2 (VVV increasing);
  • Lemma 2 (q∗q^*q∗ increasing);
  • Theorem 1, first sentence (a steady state is the unique solution of π′(p)/(1−β)=pλ(p)/(1−αβ)\pi'(p)/(1-\beta)=p\lambda(p)/(1-\alpha\beta)π′(p)/(1−β)=pλ(p)/(1−αβ));
  • Theorem 2 (a unique steady state exists and attracts every optimal path, with monotone state paths);
  • Remark 3 (a steeper reference effect gives a lower steady state);
  • Lemma 4 ((Pθ)(P_\theta)(Pθ​) satisfies Assumptions 1–3, Vθ≥VKV_\theta\ge V_KVθ​≥VK​, and steady states of (Pθ)(P_\theta)(Pθ​) are steady states of (K)(K)(K));
  • the §5.2 statement that the steady states pθ∗∗p^{**}_\thetapθ∗∗​ span [pL∗∗,pG∗∗][p^{**}_L,p^{**}_G][pL∗∗​,pG∗∗​];
  • the §A.11 identity VK(r0)=VL(r0)V_K(r_0)=V_L(r_0)VK​(r0​)=VL​(r0​) for r0<pL∗∗r_0<p^{**}_Lr0​<pL∗∗​.

Significance

The theorem separates loss-averse markets from loss-neutral ones. With a smooth reference effect, Theorem 2 gives one long-run price. Under loss aversion, every price in [pL∗∗,pG∗∗][p^{**}_L,p^{**}_G][pL∗∗​,pG∗∗​] is self-sustaining: a firm that starts there gains nothing by moving. Prices therefore exhibit stickiness, an interval of rigid prices, which is the dynamic counterpart of the kink in the reference effect. The paper uses this result to derive price monotonicity under loss aversion (its Proposition 4) and the behavior of myopic firms (its Proposition 5).

The result is proved in the paper; nothing here is open. What the mission adds is a machine-checked proof, and that proof has to supply steps the paper passes over quickly. Among them are the existence of steady states in Theorem 2 (the paper argues it in two sentences) and the largest-maximizer bookkeeping when steady states are transferred from (Pθ)(P_\theta)(Pθ​) to (K)(K)(K).

Difficulty

The bulk of the work sits in the infinite-horizon dynamic program itself. The value function is a supremum over infinite price sequences. Before any comparative statics can be done, one must show that it satisfies the Bellman equation (2), that it is continuous, and that the argmax is nonempty, so that the largest maximizer is well defined and actually maximizes. The monotonicity of q∗q^*q∗ does not follow from supermodularity of Π\PiΠ alone, because the policy maximizes current profit plus a continuation value evaluated at a state that itself depends on the price.

For the kinked problem, RKR_KRK​ is not differentiable at x=0x=0x=0, so the first-order analysis behind Theorem 1 does not apply to (K)(K)(K). A first-order condition with one-sided derivatives is the natural first idea. It yields inequalities that every steady state must satisfy, but it establishes neither that steady states exist nor that the whole interval consists of steady states. The set equality also depends on the largest-maximizer convention, since a price that is merely a maximizer of the Bellman objective is not a steady state under the paper's definition.

Formalization scope

All declarations live in the namespace ReferencePricing.LossAversion.

  • Data. The model data are a base demand d : ℝ → ℝ and reference effects R : ℝ → ℝ → ℝ, with demand d p + R (r - p) r. R(0,r)=0R(0,r)=0R(0,r)=0 is a field of Assumption 1.
  • Value function. value takes the per-period profit as a parameter and is the real supremum ⨆ over sequences ℕ → Set.Icc 0 pbar of the tsum of discounted profits. It is not a function assumed to solve (2).
  • Policy. optPrice is sSup of the set of maximizers in PPP of the Bellman objective, following the paper's largest-maximizer convention. Nonemptiness of that set is to be proved, never assumed.
  • Steady states. IsSteadyState r is r ∈ P ∧ optPrice r = r.
  • Encodings. Monotonicity, concavity and supermodularity hypotheses are required on PPP or P×PP\times PP×P, and monotonicity in xxx and single crossing on the reachable gains [r−pˉ,r][r-\bar p,r][r−pˉ​,r]. "Twice differentiable" means that the uncurried function and its Fréchet derivative are differentiable. "Nonmonotonic" means neither monotone nor antitone on PPP.
  • Added hypotheses. Two hypotheses are added and disclosed in each item. The base demand ddd is differentiable, because π′\pi'π′ appears in Assumption 3(b). The demands of RGR_GRG​ and RLR_LRL​ satisfy Assumption 1, which the paper's proof of Lemma 4 uses.
  • Typos. The page's typo "r0>pG∗r_0>p^*_Gr0​>pG∗​" in Theorem 4 is read as pG∗∗p^{**}_GpG∗∗​.
  • Ruling out trivial versions. The goal quantifies pL∗∗p^{**}_LpL∗∗​ and pG∗∗p^{**}_GpG∗∗​ existentially with uniqueness, so the existence of these steady states is part of the claim. It is not a formalization with arbitrary endpoints supplied as hypotheses, nor one with "some optimal policy" in place of the largest maximizer. The hypotheses are jointly satisfiable: the linear instance pˉ=3/4\bar p=3/4pˉ​=3/4, d(p)=1−pd(p)=1-pd(p)=1−p, RL=x/4R_L=x/4RL​=x/4, RG=x/8R_G=x/8RG​=x/8 meets all of them.

A complete development needs:

  • the Bellman equation and continuity of the value function for bounded continuous rewards on a compact action set (Berge's maximum theorem);
  • Topkis-type monotone comparative statics on intervals;
  • convergence of monotone bounded sequences.

The first two are reusable beyond this mission, and contributions of either as general lemmas are welcome.

Selected references

  • I. Popescu and Y. Wu, Dynamic Pricing Strategies with Reference Effects, Operations Research 55(3):413–429, 2007. https://doi.org/10.1287/opre.1070.0393
  • D. Kahneman and A. Tversky, Prospect Theory: An Analysis of Decision under Risk, Econometrica 47(2):263–291, 1979. https://doi.org/10.2307/1914185
  • P. K. Kopalle, A. G. Rao and J. L. Assunção, Asymmetric Reference Price Effects and Dynamic Pricing Policies, Marketing Science 15(1):60–85, 1996. https://doi.org/10.1287/mksc.15.1.60
  • G. Fibich, A. Gavious and O. Lowengart, Explicit Solutions of Optimization Models and Differential Games with Nonsmooth (Asymmetric) Reference-Price Effects, Operations Research 51(5):721–734, 2003. https://doi.org/10.1287/opre.51.5.721.16758
  • D. M. Topkis, Supermodularity and Complementarity, Princeton University Press, 1998. https://doi.org/10.1515/9781400822539
  • N. L. Stokey, R. E. Lucas and E. C. Prescott, Recursive Methods in Economic Dynamics, Harvard University Press, 1989. https://www.hup.harvard.edu/books/9780674750968
13 thms1 active userReviewed
Dynamic ProgrammingLinear OptimizationOperations Research+2·Captain: mikedeng1

On the Choice-Based Linear Programming Model for Network Revenue Management I: The CDLP Is Asymptotically Optimal under Proportional ScalingResearch Paper

Motivation

Airlines, hotels and railways sell a fixed stock of perishable capacity (seats on flight legs, room-nights) to customers who arrive over a finite selling horizon. Network revenue management decides, at each moment, which products to keep open for sale. In the classical independent-demand model each product has its own demand stream. In practice customers choose among the products on offer, and closing a cheap fare shifts some of its demand to a more expensive one. Talluri and van Ryzin (Management Science 2004) modelled this with choice-based demand on a single resource: the firm chooses an offer set SSS, and an arriving customer buys product jjj with probability Pj(S)P_j(S)Pj​(S).

On a network the exact dynamic program has one state per vector of remaining leg capacities, and cannot be solved at realistic sizes. Gallego, Iyengar, Phillips and Dubey (CORC Technical Report TR-2004-01, 2004) proposed replacing it with a linear program over the time allotted to each offer set, the choice-based deterministic linear program (CDLP). Liu and van Ryzin (MSOM 2008) analysed this LP. Their first result has two parts: the CDLP value is an upper bound on the optimal expected revenue, and the bound is asymptotically tight when capacity and horizon are scaled up together. For the independent-demand deterministic LP the analogous statement goes back to Gallego and van Ryzin (Operations Research 1997) and Cooper (Operations Research 2002). This mission targets the choice-based version.

Setting

A choice-based network instance has mmm legs and nnn products N={1,…,n}N = \{1,\dots,n\}N={1,…,n}, and consists of:

  • an incidence matrix A=[aij]A = [a_{ij}]A=[aij​] with aij∈{0,1}a_{ij} \in \{0,1\}aij​∈{0,1}, where aij=1a_{ij}=1aij​=1 when product jjj uses leg iii; AjA_jAj​ is its jjjth column;
  • a revenue rj∈Rr_j \in \mathbb{R}rj​∈R for each product (no sign assumed);
  • an arrival probability λ∈[0,1]\lambda \in [0,1]λ∈[0,1] per period;
  • choice probabilities Pj(S)P_j(S)Pj​(S) for every offer set S⊆NS \subseteq NS⊆N, with Pj(S)≥0P_j(S) \ge 0Pj​(S)≥0, Pj(S)=0P_j(S)=0Pj​(S)=0 for j∉Sj \notin Sj∈/S, and ∑j∈SPj(S)≤1\sum_{j\in S} P_j(S) \le 1∑j∈S​Pj​(S)≤1. The no-purchase probability is P0(S)=1−∑j∈SPj(S)P_0(S) = 1 - \sum_{j\in S}P_j(S)P0​(S)=1−∑j∈S​Pj​(S).

λ\lambdaλ and PPP are the same in every period. Each offer set has an expected revenue R(S)=∑j∈SrjPj(S)R(S) = \sum_{j\in S} r_j P_j(S)R(S)=∑j∈S​rj​Pj​(S) and a capacity-consumption vector Q(S)=AP(S)Q(S) = AP(S)Q(S)=AP(S).

The dynamic program. With remaining capacity x∈Nmx \in \mathbb{N}^mx∈Nm, an offer set is allowed if x−Aj≥0x - A_j \ge 0x−Aj​≥0 for all j∈Sj \in Sj∈S (no overbooking). The empty set is always allowed. The value with kkk periods left is V(0)≡0V^{(0)} \equiv 0V(0)≡0 and

V(k+1)(x)=max⁡S allowed at x{∑j∈SλPj(S)(rj+V(k)(x−Aj))+(λP0(S)+1−λ)V(k)(x)}.V^{(k+1)}(x) = \max_{S \text{ allowed at } x}\Big\{\sum_{j\in S}\lambda P_j(S)\big(r_j + V^{(k)}(x-A_j)\big) + \big(\lambda P_0(S)+1-\lambda\big)V^{(k)}(x)\Big\}.V(k+1)(x)=S allowed at xmax​{j∈S∑​λPj​(S)(rj​+V(k)(x−Aj​))+(λP0​(S)+1−λ)V(k)(x)}.

The optimal expected revenue over TTT periods from capacity c∈Nmc \in \mathbb{N}^mc∈Nm is V∗(c,T)=V(T)(c)V^*(c,T) = V^{(T)}(c)V∗(c,T)=V(T)(c) (dpValue).

The CDLP. Its variables are times t(S)≥0t(S) \ge 0t(S)≥0, one for each S⊆NS \subseteq NS⊆N, and

VCDLP(c,T)=max⁡{∑SλR(S)t(S)  :  ∑SλQ(S)t(S)≤c, ∑St(S)≤T, t≥0}V^{\mathrm{CDLP}}(c,T) = \max\Big\{\sum_{S}\lambda R(S)t(S) \;:\; \sum_S \lambda Q(S)t(S) \le c,\ \sum_S t(S) \le T,\ t \ge 0\Big\}VCDLP(c,T)=max{S∑​λR(S)t(S):S∑​λQ(S)t(S)≤c, S∑​t(S)≤T, t≥0}

(cdlpValue).

Scaling. For θ∈N\theta \in \mathbb{N}θ∈N, the θ\thetaθ-scaled problems have capacities θc\theta cθc and horizon θT\theta TθT. Write Vθ∗=V∗(θc,θT)V^*_\theta = V^*(\theta c,\theta T)Vθ∗​=V∗(θc,θT) and VθCDLP=VCDLP(θc,θT)V^{\mathrm{CDLP}}_\theta = V^{\mathrm{CDLP}}(\theta c, \theta T)VθCDLP​=VCDLP(θc,θT).

Formalization targets

Goal: Proposition 2 (p. 294)

lim⁡θ→∞1θVθ∗  =  lim⁡θ→∞1θVθCDLP  =  VCDLP(c,T),\lim_{\theta\to\infty}\frac1\theta V^*_\theta \;=\; \lim_{\theta\to\infty}\frac1\theta V^{\mathrm{CDLP}}_\theta \;=\; V^{\mathrm{CDLP}}(c,T),θ→∞lim​θ1​Vθ∗​=θ→∞lim​θ1​VθCDLP​=VCDLP(c,T),

for every instance, every c∈Nmc \in \mathbb{N}^mc∈Nm and every T∈NT\in\mathbb{N}T∈N. It is stated as two Tendsto statements along θ→∞\theta \to \inftyθ→∞ in N\mathbb{N}N.

Milestones

  1. Proposition 1 (p. 294): V∗(c,T)≤VCDLP(c,T)V^*(c,T) \le V^{\mathrm{CDLP}}(c,T)V∗(c,T)≤VCDLP(c,T) for every ccc and TTT.
  2. Scaling of the CDLP (proof of Proposition 2, first paragraph): VCDLP(θc,θT)=θ VCDLP(c,T)V^{\mathrm{CDLP}}(\theta c,\theta T) = \theta\,V^{\mathrm{CDLP}}(c,T)VCDLP(θc,θT)=θVCDLP(c,T) for every θ∈N\theta \in \mathbb{N}θ∈N.
  3. Lower half of the first limit (proof of Proposition 2, pp. 294–295): for every ε>0\varepsilon>0ε>0, eventually in θ\thetaθ, VCDLP(c,T)−ε≤1θVθ∗V^{\mathrm{CDLP}}(c,T) - \varepsilon \le \frac1\theta V^*_\thetaVCDLP(c,T)−ε≤θ1​Vθ∗​.

The goal follows from the three milestones.

Significance

The result. Proposition 1 makes the CDLP a certified upper bound on what any control policy can earn, whatever the choice model. Numerical studies use it to benchmark heuristics. Proposition 2 says the bound is exact to first order in large systems, so policies driven by the CDLP solution (time allocations, bid prices from its dual) lose only a vanishing fraction of revenue. It is the justification for the whole family of CDLP-based controls that the paper and later work study (column generation, decomposition, and later the affine and piecewise-linear relaxations of the choice-based network problem).

Formalizing it. The result is proved in the paper. No machine-checked version exists: no revenue-management DP with choice-based demand on a network, no CDLP, and no fluid-limit argument of this kind is on the platform. The existing RevenueManagement material from the Talluri–van Ryzin textbook covers single-resource and dynamic-pricing models. Formalizing the result produces a reusable network-RM DP with an offer-set action space, the CDLP as a Lean object, and a checked asymptotic-optimality theorem that other deterministic-approximation results (independent demand, bid-price heuristics) can follow.

Difficulty

The upper bound compares a stochastic dynamic program with a linear program. The natural route builds a feasible LP point from the optimal policy (expected times each set is offered), but the DP here is a recursion over capacity vectors, not a policy class with a notion of "expected time offered". That connection has to be made from the recursion itself.

The lower bound is harder. The paper's policy offers each set for a fractional number of periods and caps accepted demand at its mean after customers have chosen. Neither is an action available in the DP, where the firm can only pick an allowed offer set each period and must accept whatever the customer picks. The obvious transcription therefore does not type-check against the model: one needs a genuine DP policy whose revenue is θVCDLP−o(θ)\theta V^{\mathrm{CDLP}} - o(\theta)θVCDLP−o(θ) while it respects capacity on every sample path. The no-overbooking rule forbids offering a set once any of its products would exceed remaining capacity. Negative revenues are allowed, and λ\lambdaλ may be 000 or 111.

Formalization scope

Legs are Fin m, products Fin n, offer sets Finset (Fin n). The instance is a structure ChoiceNetwork m n carrying AAA (entries in N\mathbb{N}N, each 000 or 111), rrr, λ∈[0,1]\lambda\in[0,1]λ∈[0,1] and PPP with the three choice-model axioms. The DP and CDLP use one λ\lambdaλ and one PPP for every period, matching the paper's time-homogeneous model. Capacities and horizon are natural numbers; CDLP times and all values are real. θ\thetaθ ranges over N\mathbb{N}N, because θT\theta TθT must be a whole number of periods, and the limits use real division by θ\thetaθ.

V∗V^*V∗ is defined by the Bellman recursion (1), which the paper states is equivalent to the stochastic control problem (4). No measure-theoretic policy class is built. The maximization runs over the offer sets allowed at the current capacity, so the DP can neither overbook nor pick products outside an offer set. The paper's boundary condition Vt(0)=0V_t(0)=0Vt​(0)=0 is not imposed separately: it follows from the recursion whenever every product uses a leg, and imposing it on top could contradict the recursion. VCDLPV^{\mathrm{CDLP}}VCDLP is sSup of the objective over the feasible set. That set is nonempty (t=0t=0t=0) and bounded (0≤t(S)≤T0 \le t(S) \le T0≤t(S)≤T), so the value is the LP optimum.

The goal is the limit equality with both capacity and horizon scaled. A statement with only the upper bound, only capacity scaled, or a DP that ignores capacity or chooses products freely would be a trivializing formalization, and the definitions rule each of these out. Milestone 3 is the paper's conclusion stated on the DP value, not on the paper's informal policy. It is not a repair.

A complete development needs: LP duality or a direct feasibility construction for Proposition 1; the scaling identity for the CDLP; and, for the lower bound, a concrete DP policy together with a law-of-large-numbers or concentration estimate for sums of per-period sales (Mathlib's ProbabilityTheory.strong_law_ae and Hoeffding-type bounds are available). A policy-evaluation lemma that bounds the DP value below by the expected revenue of any feasible offer-set policy is reusable beyond this mission, as is the CDLP scaling lemma. Contributions to either are welcome.

Selected references

  • Q. Liu, G. van Ryzin, On the Choice-Based Linear Programming Model for Network Revenue Management, Manufacturing & Service Operations Management 10(2):288–310, 2008. https://doi.org/10.1287/msom.1070.0169
  • K. Talluri, G. van Ryzin, Revenue Management Under a General Discrete Choice Model of Consumer Behavior, Management Science 50(1):15–33, 2004. https://doi.org/10.1287/mnsc.1030.0147
  • G. Gallego, G. Iyengar, R. Phillips, A. Dubey, Managing Flexible Products on a Network, CORC Technical Report TR-2004-01, Columbia University, 2004.
  • G. Gallego, G. van Ryzin, A Multiproduct Dynamic Pricing Problem and Its Applications to Network Yield Management, Operations Research 45(1):24–41, 1997. https://doi.org/10.1287/opre.45.1.24
  • W. L. Cooper, Asymptotic Behavior of an Allocation Policy for Revenue Management, Operations Research 50(4):720–727, 2002. https://doi.org/10.1287/opre.50.4.720.2862
7 thms1 active userReviewed
Operations ResearchOptimization·Captain: mikedeng1

The d-Level Nested Logit Model: Assortment and Price Optimization Problems II: The Push-Up-Then-Push-Down Prices Converge to a Stationary PointResearch Paper

Motivation

Retailers that sell many substitutable products must set all their prices at once, and a customer's reaction to one price depends on what else is on the shelf. The nested logit model captures this by grouping similar products into nests, so that raising one price shifts demand mostly to close substitutes. The ddd-level nested logit model extends the familiar two-level version to a whole taxonomy tree of depth ddd (for example category → brand → size). It is consistent with random utility maximization (McFadden 1978) and is widely used in demand estimation.

Pricing under logit-type models is harder than it looks. Already for the multinomial logit model, which is the one-level case, Hanson and Martin (1996) point out that the expected revenue is not necessarily concave in the prices. For the two-level nested logit, Gallego and Wang (2014) show that the expected revenue is not concave and can have several local maxima. Li, Rusmevichientong and Topaloglu (Oper. Res. 63(2), 2015) treat the general ddd-level model. Their pricing result, Theorem 7.3, is the target of this mission. It shows that a simple gradient-free iteration, the push-up-then-push-down (PUPD) algorithm, produces prices that converge to a stationary point of the expected revenue.

Setting

The products l=1,…,nl=1,\dots,nl=1,…,n are the leaves of a rooted tree T=(V,E)T=(V,E)T=(V,E), all at depth ddd. A further leaf, node 000 (the no-purchase option), hangs directly from root\mathrm{root}root. Every other node jjj is a nonleaf node with a nonempty set Children(j)\mathrm{Children}(j)Children(j) and a parameter ηj\eta_jηj​. The standing assumptions are ηj∈(0,1]\eta_j\in(0,1]ηj​∈(0,1] for nonleaf j≠rootj\neq\mathrm{root}j=root and ηroot=0\eta_{\mathrm{root}}=0ηroot​=0. Each product carries parameters αl∈R\alpha_l\in\mathbb Rαl​∈R and βl>0\beta_l>0βl​>0, and node 000 carries α0∈R\alpha_0\in\mathbb Rα0​∈R.

Given a price vector p=(p1,…,pn)\mathbf p=(p_1,\dots,p_n)p=(p1​,…,pn​), where the no-purchase price is fixed at p0=0p_0=0p0​=0, the preference weights are computed bottom-up:

Vl(p)=eαl−βlpl,V0(p)=eα0,Vj(p)=(∑k∈Children(j)Vk(p))ηj.V_l(\mathbf p)=e^{\alpha_l-\beta_lp_l},\qquad V_0(\mathbf p)=e^{\alpha_0},\qquad V_j(\mathbf p)=\Big(\sum_{k\in\mathrm{Children}(j)}V_k(\mathbf p)\Big)^{\eta_j}.Vl​(p)=eαl​−βl​pl​,V0​(p)=eα0​,Vj​(p)=(k∈Children(j)∑​Vk​(p))ηj​.

The expected revenues are Rl(p)=plR_l(\mathbf p)=p_lRl​(p)=pl​, R0(p)=0R_0(\mathbf p)=0R0​(p)=0, and

Rj(p)=∑k∈Children(j)Vk(p)Rk(p)∑k∈Children(j)Vk(p)R_j(\mathbf p)=\frac{\sum_{k\in\mathrm{Children}(j)}V_k(\mathbf p)R_k(\mathbf p)}{\sum_{k\in\mathrm{Children}(j)}V_k(\mathbf p)}Rj​(p)=∑k∈Children(j)​Vk​(p)∑k∈Children(j)​Vk​(p)Rk​(p)​

at a nonleaf node. The expected revenue of p\mathbf pp is Rroot(p)R_{\mathrm{root}}(\mathbf p)Rroot​(p). A customer walks down from root\mathrm{root}root, choosing a child with probability proportional to its weight. The probability θl(p)\theta_l(\mathbf p)θl​(p) of ending at product lll is the product, over the levels h=1,…,dh=1,\dots,dh=1,…,d, of VAn(l,h)/∑k∈Sibling(An(l,h))VkV_{\mathrm{An}(l,h)}/\sum_{k\in\mathrm{Sibling}(\mathrm{An}(l,h))}V_kVAn(l,h)​/∑k∈Sibling(An(l,h))​Vk​, where An(l,h)\mathrm{An}(l,h)An(l,h) is the ancestor of lll in level hhh.

Top-down, the scalars uj(p)u_j(\mathbf p)uj​(p) are uroot=Rrootu_{\mathrm{root}}=R_{\mathrm{root}}uroot​=Rroot​ and uj=ηjuParent(j)+(1−ηj)Rju_j=\eta_ju_{\mathrm{Parent}(j)}+(1-\eta_j)R_juj​=ηj​uParent(j)​+(1−ηj​)Rj​. A stationary point of RrootR_{\mathrm{root}}Rroot​ is a price vector at which the gradient of RrootR_{\mathrm{root}}Rroot​ is zero.

The PUPD algorithm starts from p0=0\mathbf p^0=\mathbf 0p0=0. Given ps\mathbf p^sps, it sets troots=Rroot(ps)t^s_{\mathrm{root}}=R_{\mathrm{root}}(\mathbf p^s)troots​=Rroot​(ps) and, for every other nonleaf node,

tjs=max⁡{tParent(j)s, ηjtParent(j)s+(1−ηj)Rj(ps)}.t^s_j=\max\big\{t^s_{\mathrm{Parent}(j)},\ \eta_jt^s_{\mathrm{Parent}(j)}+(1-\eta_j)R_j(\mathbf p^s)\big\}.tjs​=max{tParent(j)s​, ηj​tParent(j)s​+(1−ηj​)Rj​(ps)}.

It then updates pls+1=1/βl+tParent(l)sp^{s+1}_l=1/\beta_l+t^s_{\mathrm{Parent}(l)}pls+1​=1/βl​+tParent(l)s​ for every product lll.

Formalization targets

Goal: Theorem 7.3 (p. 336)

∃ p∗∈Rn:lim⁡s→∞ps=p∗and∇Rroot(p∗)=0.\exists\,\mathbf p^*\in\mathbb R^n:\qquad \lim_{s\to\infty}\mathbf p^s=\mathbf p^* \quad\text{and}\quad \nabla R_{\mathrm{root}}(\mathbf p^*)=0 .∃p∗∈Rn:s→∞lim​ps=p∗and∇Rroot​(p∗)=0.

The whole sequence converges and its limit is stationary. No rate is claimed, and none is asked for.

Milestones

  • Lemma 7.1 (p. 335). For p∈R+n\mathbf p\in\mathbb R^n_+p∈R+n​ and every product lll,
∂Rroot∂pl(p)=−θl(p) βl(pl−1βl−uParent(l)(p)).\frac{\partial R_{\mathrm{root}}}{\partial p_l}(\mathbf p)=-\theta_l(\mathbf p)\,\beta_l\Big(p_l-\frac1{\beta_l}-u_{\mathrm{Parent}(l)}(\mathbf p)\Big).∂pl​∂Rroot​​(p)=−θl​(p)βl​(pl​−βl​1​−uParent(l)​(p)).
  • Corollary 7.2 (p. 336). For p∈R+n\mathbf p\in\mathbb R^n_+p∈R+n​, p\mathbf pp is a stationary point of RrootR_{\mathrm{root}}Rroot​ if and only if pl=1/βl+uParent(l)(p)p_l=1/\beta_l+u_{\mathrm{Parent}(l)}(\mathbf p)pl​=1/βl​+uParent(l)​(p) for all lll.

Significance

The result itself. Theorem 7.3 turns a nonconcave, many-product pricing problem into an iteration that needs no gradient evaluations and no step size. Each iteration costs one bottom-up and one top-down pass over the tree. The paper's numerical experiments (§8) report that it reaches a stationary point much faster than gradient ascent. Lemma 7.1 gives the gradient of the expected revenue in closed form for any depth. Corollary 7.2 turns stationarity into a fixed-point equation in the prices, which is what makes a price-update scheme like PUPD natural.

Formalizing it. The proofs of Lemma 7.1 and Theorem 7.3 are in the paper's online Appendix E. The acknowledgments (pp. 340–341) record that an error found in an earlier version led to a new proof that the revenues under the PUPD algorithm are always bounded. A machine-checked proof would settle the convergence claim independently of that history. No nested logit or multinomial logit pricing result, and no part of this one, has a machine-checked proof on Prove2Me.

Difficulty

Lemma 7.1 is a chain-rule computation through a tree of power means, and it is technical rather than deep. The hard part is Theorem 7.3. The obvious fixed-point iteration pls+1=1/βl+uParent(l)(ps)p^{s+1}_l=1/\beta_l+u_{\mathrm{Parent}(l)}(\mathbf p^s)pls+1​=1/βl​+uParent(l)​(ps) suggested by Corollary 7.2 is not the algorithm. PUPD replaces uuu by the scalars tst^sts, which involve a maximum, and the update direction ps+1−ps\mathbf p^{s+1}-\mathbf p^sps+1−ps is in general not parallel to the gradient. So neither contraction arguments for the plain fixed-point map nor the standard ascent analysis of gradient methods applies directly. RrootR_{\mathrm{root}}Rroot​ is not concave and may have several stationary points, so convergence of the whole sequence, not only of a subsequence or of the gradient norms, is the substance of the claim.

Formalization scope

The node type is Option (Fin n) ⊕ Inner. Sum.inl (some l) is product lll, indexed by Fin n, so the paper's products 1,…,n1,\dots,n1,…,n are 0,…,n−10,\dots,n-10,…,n−1. Sum.inl none is node 000. Inner is a finite type of nonleaf nodes containing root, with a parent map into Inner and a level function that encodes the ddd levels. Every nonleaf node has a child. Prices are Fin n → ℝ, so node 000 has no price coordinate, and all nnn products are priced (there is no assortment decision). The conventions:

  • Powers xηjx^{\eta_j}xηj​ are Real.rpow. Since ηroot=0\eta_{\mathrm{root}}=0ηroot​=0, Vroot=1V_{\mathrm{root}}=1Vroot​=1 and it is never used. Division is Lean's, but every denominator is positive under the standing assumptions.
  • RrootR_{\mathrm{root}}Rroot​, θl\theta_lθl​ and uju_juj​ are defined on all of Rn\mathbb R^nRn by the paper's formulas. The paper restricts to R+n\mathbb R^n_+R+n​, and Lemma 7.1 and Corollary 7.2 keep that hypothesis as printed.
  • The partial derivative in Lemma 7.1 is HasDerivAt of x↦Rroot(px\mapsto R_{\mathrm{root}}(\mathbf px↦Rroot​(p with pl:=x)p_l:=x)pl​:=x) at plp_lpl​. "Stationary point" is HasFDerivAt R_root 0 p (the gradient is zero). This is the unconstrained gradient, as on p. 335, with no boundary condition, and it is the same notion in Corollary 7.2 and in the goal.
  • θl\theta_lθl​ is defined by the printed product along the root-to-leaf path, and An(l,h)\mathrm{An}(l,h)An(l,h) is reached by d−hd-hd−h parent steps. θl\theta_lθl​ is not a free parameter.
  • The PUPD iterates are a definition (pupd) with p0=0\mathbf p^0=\mathbf 0p0=0 and the max-based tst^sts, and troots=Rroot(ps)t^s_{\mathrm{root}}=R_{\mathrm{root}}(\mathbf p^s)troots​=Rroot​(ps). The goal is not stated for an arbitrary start point or for the uuu-based iteration.

A trivializing formalization is ruled out: convergence is Filter.Tendsto of the full sequence to a point at which HasFDerivAt holds with derivative 000. It is not a statement about limit points, gradient norms, or an arbitrary sequence satisfying a hypothesis.

A complete development needs derivatives of Real.rpow compositions over a finite tree, positivity of the weights and choice probabilities, and a convergence argument for the PUPD iteration. The weight and revenue recursions over a finite rooted tree could be reused for the assortment half of the same paper and for other tree-structured choice models. Contributions to any milestone, and alternative proofs of Lemma 7.1, are welcome.

Selected references

  • H. Li, P. Rusmevichientong, H. Topaloglu, The d-Level Nested Logit Model: Assortment and Price Optimization Problems, Operations Research 63(2):325–341, 2015. https://doi.org/10.1287/opre.2015.1355
  • G. Gallego, R. Wang, Multiproduct Price Optimization and Competition Under the Nested Logit Model with Product-Differentiated Price Sensitivities, Operations Research 62(2):450–461, 2014. https://doi.org/10.1287/opre.2013.1249
  • W. Hanson, K. Martin, Optimizing Multinomial Logit Profit Functions, Management Science 42(7):992–1003, 1996. https://doi.org/10.1287/mnsc.42.7.992
  • D. McFadden, Modelling the Choice of Residential Location, in A. Karlqvist et al. (eds.), Spatial Interaction Theory and Planning Models, North-Holland, 1978, 75–96 (cited as McFadden 1978 on p. 328 of Li et al.).
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CombinatoricsGraph TheoryOperations Research+1·Captain: mikedeng1

Budgeted Prize-Collecting Traveling Salesman and Minimum Spanning Tree Problems: The Primal-Dual Upper Bound on the Optimal TourResearch Paper

Motivation

Many routing problems come with a hard limit on distance or time rather than a requirement to visit everything. A repair crew with a fixed shift wants to service as many stations as possible; a vehicle with a fixed range wants to cover as many customers as possible. The budgeted prize-collecting traveling salesman problem captures this: given edge costs and a budget, find a closed tour of cost at most the budget that visits as many vertices as possible. Paul, Freund, Ferber, Shmoys and Williamson met the problem in work with New York City's bikeshare system (Paul et al., Math. Oper. Res. 2020).

The problem is NP-hard, and the question is how close a polynomial-time algorithm can come to the optimum. Before this paper, the best guarantee for the rooted tour version was 2+ε2+\varepsilon2+ε, obtained from the orienteering algorithm of Chekuri, Korula and Pál (reference [6] of Paul et al.), with running time nO(1/ε2)n^{O(1/\varepsilon^2)}nO(1/ε2). Paul et al. give a parameterized primal-dual algorithm with guarantee exactly 2, in the style of the Goemans–Williamson primal-dual method for prize-collecting Steiner trees and tours (Goemans and Williamson, SIAM J. Comput. 1995). The analysis rests on one upper bound on the optimum, Theorem 1 of the paper, which this mission formalizes.

Setting

An instance consists of an undirected graph G=(V,E)G=(V,E)G=(V,E) on a finite vertex set, not necessarily complete, edge costs ce≥0c_e \ge 0ce​≥0, a budget D≥0D \ge 0D≥0 and a root r∈Vr \in Vr∈V. A feasible tour is a closed walk in GGG that starts and ends at rrr and whose cost, the sum of cec_ece​ over its edges counted with multiplicity, is at most DDD. Vertices may be revisited. The tour's vertex set is written O⋆O^\starO⋆.

A dual vector assigns a real number ySy_SyS​ to every S⊆VS \subseteq VS⊆V. For an edge eee, e∈δ(S)e \in \delta(S)e∈δ(S) means that eee has exactly one endpoint in SSS. The potential of SSS is

π(S)=∣S∣−2∑T⊊SyT,\pi(S) = |S| - 2\sum_{T \subsetneq S} y_T ,π(S)=∣S∣−2T⊊S∑​yT​,

and SSS is neutral when 2∑T⊆SyT=∣S∣2\sum_{T \subseteq S} y_T = |S|2∑T⊆S​yT​=∣S∣.

The primal-dual subroutine PD(λ1\lambda_1λ1​), for a parameter λ1≥0\lambda_1 \ge 0λ1​≥0, starts with y≡0y \equiv 0y≡0, no tight edges, and every singleton {i}\{i\}{i} an active component. It raises ySy_SyS​ at unit rate for all active components SSS at once, until an event happens: either an active set becomes neutral and is marked inactive, or the dual constraint ∑S:e∈δ(S)yS≤λ1ce\sum_{S : e \in \delta(S)} y_S \le \lambda_1 c_e∑S:e∈δ(S)​yS​≤λ1​ce​ of an edge eee between two different components becomes tight. In that case eee is added to the forest TTT and the two components merge into one active component. The process stops when no set is active. Simultaneous events are processed in an arbitrary order. The family S\mathcal SS collects every set that was ever active, including for zero time, and S+=S∪{V}\mathcal S^+ = \mathcal S \cup \{V\}S+=S∪{V}.

In the Lean development the instance is BudgetedPCTSP.Rooted.Instance, tours are SimpleGraph.Walks from r to r, the potential is potential, and PD(λ1\lambda_1λ1​) is the event relation PDStep with final states IsCompleteRun. The family S+\mathcal S^+S+ is sPlus.

Formalization targets

Goal: Theorem 1 (the upper bound)

Fix λ1≥0\lambda_1 \ge 0λ1​≥0. PD(λ1\lambda_1λ1​) has a complete run. For every complete run, under every order of breaking ties, every feasible tour with vertex set O⋆O^\starO⋆, and OOO the minimal set of S+\mathcal S^+S+ containing O⋆O^\starO⋆:

∣O⋆∣≤λ1D+π(O).|O^\star| \le \lambda_1 D + \pi(O).∣O⋆∣≤λ1​D+π(O).

Milestones

In the order a proof would take them:

  1. S+\mathcal S^+S+ is laminar (p. 6): any two members are nested or disjoint.
  2. Dual feasibility throughout the run (p. 6): ∑S:e∈δ(S)yS≤λ1ce\sum_{S : e \in \delta(S)} y_S \le \lambda_1 c_e∑S:e∈δ(S)​yS​≤λ1​ce​ for every edge eee, and y≥0y \ge 0y≥0.
  3. Lemma 1 (p. 7): 2∑T⊆SyT≤∣S∣2\sum_{T \subseteq S} y_T \le |S|2∑T⊆S​yT​≤∣S∣ for every S⊆VS \subseteq VS⊆V at the end of the run.

Significance

Theorem 1 is the dual-fitting half of the paper's 2-approximation. Together with the lower bound ∣SA∣>12λ1D+π(Q)−1|S_A| > \tfrac12\lambda_1 D + \pi(Q) - 1∣SA​∣>21​λ1​D+π(Q)−1 on the tour the algorithm builds (Theorem 2), and the threshold choice of λ1\lambda_1λ1​ (Lemma 2), it yields the main result, Theorem 3: the parameterized primal-dual algorithm is a 2-approximation for the rooted budgeted prize-collecting TSP. The paper extends the analysis to the weighted, tree and unrooted variants in Section 8, stating that the proofs continue to hold.

The result is proved in the paper; it has not been formalized. This mission produces a precise, checkable model of a Goemans–Williamson-style moat-growing process: a discrete event semantics for a continuous dual-ascent process, with every tie-breaking order admitted. That model is reusable for the rest of the paper (the threshold analysis, the tour construction and Theorem 3) and for other primal-dual approximation algorithms built on the same process, such as prize-collecting Steiner tree.

Difficulty

The paper states the process continuously and argues about it informally ("raise ySy_SyS​ uniformly … until"). A proof must turn the invariants it relies on into statements about every reachable state of a discrete process in which event times are recomputed after each event and ties are broken arbitrarily. The paper gives one-sentence justifications for dual feasibility and laminarity and a two-line proof of Lemma 1; none of them addresses zero-length events, ties, or the fact that the next event time is only known to be nonnegative once these same invariants hold. Laminarity has to hold for the whole family of ever-active sets, not only for the current partition.

In the goal itself, the step that goes beyond bookkeeping is a counting argument. It relates the dual mass of sets inside the minimal set OOO to how often a closed walk crosses those sets. A closed walk is a list of edges with repetitions, not a set, and the obvious set-based count does not apply to it directly.

Formalization scope

  • Instance. A SimpleGraph on a Fintype vertex type with decidable equality. Costs are a real function on Sym2 V, nonnegative on edges; budget D≥0D \ge 0D≥0; a root rrr. Unit prizes only. The weighted problem (Theorem 4), the tree problem (Theorem 5) and the unrooted problem (Section 8) are out of scope.
  • Tours. A feasible tour is a closed walk at rrr with cost at most DDD, costs counted with multiplicity, and its vertex set is the walk's support. This is equivalent to the paper's multiset of edges forming a tour on a vertex set containing rrr.
  • The subroutine. PD(λ1\lambda_1λ1​) is an inductive step relation on states: components, active components, the dual vector indexed by Finset V, tight edges and the family S\mathcal SS. One step raises all active duals by the minimum event time Δ\DeltaΔ and processes one event whose time is Δ\DeltaΔ. Any tied event may be chosen, so every statement quantified over complete runs holds for every tie-breaking order, as the paper's Theorem 1 does ("for any fixed λ1\lambda_1λ1​"). The pruning phase, which produces the tree T′T'T′, is not modelled; no statement here uses T′T'T′.
  • Readings. "The minimal set in S+\mathcal S^+S+ containing O⋆O^\starO⋆" is any member of S+\mathcal S^+S+ containing O⋆O^\starO⋆ with no strict subset in S+\mathcal S^+S+ that also contains O⋆O^\starO⋆. Theorem 1 is stated for every feasible tour rather than only an optimal one, which is the form its proof gives. Dual feasibility is stated for every reachable state ("throughout the subroutine").
  • Not stated. The threshold search (Lemma 2), whose "ε arbitrarily small" and "in polynomial time" would need explicit quantifier readings and are not part of this mission; Lemma 3; the tour construction and Theorem 2; the main Theorem 3. No running-time claim is formalized.
  • Ruling out trivial readings. The goal asserts that a complete run exists, so its universally quantified part cannot hold vacuously on an empty set of runs. It bounds every feasible tour by quantities computed from the subroutine's own output, not by quantities chosen freely.
  • Infrastructure. Edge cuts δ(S)\delta(S)δ(S) of vertex sets, laminar families, crossing counts of closed walks, and invariants of the event process. Lemmas about any of these, including sorry-free proofs of the milestones, are welcome contributions.

Selected references

  • A. Paul, D. Freund, A. Ferber, D. B. Shmoys, D. P. Williamson, Budgeted Prize-Collecting Traveling Salesman and Minimum Spanning Tree Problems, Mathematics of Operations Research, 2020. https://doi.org/10.1287/moor.2019.1002
  • M. X. Goemans, D. P. Williamson, A General Approximation Technique for Constrained Forest Problems, SIAM Journal on Computing 24(2), 1995. https://doi.org/10.1137/S0097539793242618
  • C. Chekuri, N. Korula, M. Pál, Improved Algorithms for Orienteering and Related Problems, ACM Transactions on Algorithms, 2012; cited as reference [6] of Paul et al. (https://doi.org/10.1287/moor.2019.1002).
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Bandit AlgorithmsDynamic ProgrammingOperations Research+1·Captain: mikedeng1

The Complexity of Optimal Queuing Network Control II: Restless Bandits with Deterministic Transitions are PSPACE-hardResearch Paper

Motivation

Among queueing control problems, a small class admits efficiently computable optimal policies: a single server choosing among several customer streams (Klimov 1974). These problems can be recast as multi-armed bandit problems, whose optimal policies are given by Gittins indices (Gittins 1979), and those indices are computable in polynomial time. The most studied generalization that could have extended this tractability is the restless bandit problem of Whittle (1988), in which bandits that are not played also change state and incur cost. Whittle's index heuristic and its asymptotic optimality (Weber and Weiss 1990) made the model a standard tool in scheduling, sensor management and resource allocation.

Papadimitriou and Tsitsiklis (1999) settled whether restless bandits are as easy as ordinary bandits. Their Theorem 4 shows that finding an optimal policy is PSPACE-hard, even when every transition is deterministic. The same paper shows that general queueing network control is EXP-complete (Theorem 1, the subject of a companion mission).

Setting

A restless bandit instance with deterministic transition rules consists of:

  • n≥1n \ge 1n≥1 bandits, indexed 1,…,n1, \dots, n1,…,n, on a common finite state space S={1,…,M}S = \{1, \dots, M\}S={1,…,M};
  • initial states X1(0),…,Xn(0)∈SX_1(0), \dots, X_n(0) \in SX1​(0),…,Xn​(0)∈S;
  • two maps P,Q:S→SP, Q : S \to SP,Q:S→S: PPP moves the bandit that is played, QQQ moves every other bandit;
  • two rational cost functions c,d:S→Qc, d : S \to \mathbb{Q}c,d:S→Q;
  • a rational threshold KKK.

A policy is a map π:Sn→{1,…,n}\pi : S^n \to \{1, \dots, n\}π:Sn→{1,…,n}. At each time t=0,1,2,…t = 0, 1, 2, \dotst=0,1,2,… it plays the bandit i(t)=π(X1(t),…,Xn(t))i(t) = \pi(X_1(t), \dots, X_n(t))i(t)=π(X1​(t),…,Xn​(t)); then Xi(t)(t+1)=P(Xi(t)(t))X_{i(t)}(t+1) = P(X_{i(t)}(t))Xi(t)​(t+1)=P(Xi(t)​(t)) and Xi(t+1)=Q(Xi(t))X_i(t+1) = Q(X_i(t))Xi​(t+1)=Q(Xi​(t)) for every i≠i(t)i \ne i(t)i=i(t). The cost at time ttt is

C(t)=c(Xi(t)(t))+∑i≠i(t)d(Xi(t)),C(t) = c\bigl(X_{i(t)}(t)\bigr) + \sum_{i \ne i(t)} d\bigl(X_i(t)\bigr),C(t)=c(Xi(t)​(t))+i=i(t)∑​d(Xi​(t)),

and the average cost of π\piπ is

J(π)=lim sup⁡T→∞1T∑t=1TC(t).J(\pi) = \limsup_{T \to \infty} \frac{1}{T}\sum_{t=1}^{T} C(t).J(π)=T→∞limsup​T1​t=1∑T​C(t).

The classical multi-armed bandit is the case Q=idQ = \mathrm{id}Q=id, d=0d = 0d=0. The paper's general model has transition probability matrices; the deterministic case is a special case, so hardness for it implies hardness in general.

The decision problem RESTLESS BANDITS asks whether there is a policy π\piπ with J(π)≤KJ(\pi) \le KJ(π)≤K.

Problems are sets of instances, and instances are bit strings under a fixed binary encoding. A problem is in PSPACE if a multi-stack Turing machine decides it on every input using a number of stack cells polynomial in the input length. It is PSPACE-hard if every PSPACE language reduces to it by a polynomial-time many-one reduction: a map computable in polynomial time that sends yes-instances to yes-instances and no-instances to no-instances. It is PSPACE-complete if it is also in PSPACE.

The proof starts from an auxiliary problem, CIRCULAR-TAPE HALTING. The input is a circular tape with squares 1,…,n1, \dots, n1,…,n holding values in {1,…,A}\{1, \dots, A\}{1,…,A}, a rule F:{1,…,A}2→{1,…,A}F : \{1,\dots,A\}^2 \to \{1,\dots,A\}F:{1,…,A}2→{1,…,A} with F(1,1)=1F(1,1) = 1F(1,1)=1, and an initial configuration v(0)v(0)v(0). At time ttt the head points at the square i≡t(modn)i \equiv t \pmod ni≡t(modn), replaces its value by F(vi−1 mod n(t),vi(t))F(v_{i-1 \bmod n}(t), v_i(t))F(vi−1modn​(t),vi​(t)) and moves on; every other square keeps its value. The process halts if at some time every square holds 111. The question is whether the process halts.

Formalization targets

Goal: Theorem 4

RESTLESS BANDITS with deterministic transition rules is PSPACE-hard.\text{RESTLESS BANDITS with deterministic transition rules is PSPACE-hard.}RESTLESS BANDITS with deterministic transition rules is PSPACE-hard.

In Lean: PSPACEHard Instance.enc restlessBandits. Every language in PSPACE reduces to the decision problem in polynomial time.

Milestone 1: the circular-tape claim

CIRCULAR-TAPE HALTING is PSPACE-complete.\text{CIRCULAR-TAPE HALTING is PSPACE-complete.}CIRCULAR-TAPE HALTING is PSPACE-complete.

In Lean: PSPACEComplete TapeInstance.enc circularTapeHalting, meaning the problem is in PSPACE and PSPACE-hard. The paper claims completeness at this point. The goal uses only the hardness half.

Milestone 2: the reduction

CIRCULAR-TAPE HALTING  ≤p  RESTLESS BANDITS (deterministic).\text{CIRCULAR-TAPE HALTING} \;\le_p\; \text{RESTLESS BANDITS (deterministic)}.CIRCULAR-TAPE HALTING≤p​RESTLESS BANDITS (deterministic).

In Lean: PolyReduces TapeInstance.enc circularTapeHalting Instance.enc restlessBandits. This is the existence of a polynomial-time reduction. It is not a statement about the specific construction in the paper.

Significance

The result. Theorem 4 shows that the index theory of multi-armed bandits does not extend to restless bandits. The index-based approach has no efficient exact counterpart unless P = PSPACE, even with no randomness at all. It is why the restless-bandit literature works with heuristics (Whittle's index) and asymptotic optimality results, not exact polynomial-time algorithms. It is also one of the standard hardness results cited for average-cost Markov decision problems whose state space is a product of many small components.

Formalizing it. The paper's argument is informal. It assumes the simulation of polynomial-space machines by circular-tape processes, and it describes the bandit construction in prose. A complete formalization produces a machine-checked PSPACE-hardness proof for a controlled-dynamics problem. It also produces a reusable space-bounded computation layer on Mathlib's Turing machines, which has polynomial time but no space measure. No part of this result has a machine-checked proof yet.

Difficulty

The obvious first idea is to encode a space-bounded machine's configuration in the bandits' joint state. The difficulty is that a policy sees only the product state and plays exactly one bandit per step. The rules PPP and QQQ are shared by all bandits, so no bandit knows its own index. The reduction also has to be exact for the average-cost criterion. A policy that simulates the computation correctly for a long but finite time, then deviates, must not reach average cost zero. A policy that halts must reach it. Milestone 1 needs its own work as well: a polynomial-space machine has to be recast as an in-place computation on a circular tape whose local rule FFF sees only a square and its predecessor.

Formalization scope

Conventions fixed in Lean:

  • Encoding. Instances are bit strings built by concatenating self-delimiting binary numerals (each bit doubled, then 01), sign-magnitude integers, (numerator, denominator) rationals, and tables listed in index order after their dimensions. The encoded length is polynomial in the instance's bit size and vice versa. Mathlib's Encodable/Nat.pair encodings are not used.
  • Machines. Time is Mathlib's Turing.TM2ComputableInPolyTime. PSPACE is defined here: a Turing.FinTM2 that halts on every input with the correct output bit, and in which every reachable configuration has total stack length at most p(∣input∣)p(|\text{input}|)p(∣input∣). The input stack is counted.
  • Decision version. The paper states only the optimization problem ("finding a policy with minimal average expected cost"). The decision version asks for ∃π, J(π)≤K\exists \pi,\ J(\pi) \le K∃π, J(π)≤K, with the rational KKK part of the input; the paper's reduction uses K=0K = 0K=0. Instances with n=0n = 0n=0 are no-instances.
  • Decision epochs and policies. Time is discrete, and t=0t = 0t=0 is the first decision. Policies are all deterministic stationary maps Sn→{1,…,n}S^n \to \{1,\dots,n\}Sn→{1,…,n}, as on the page. The dynamics are deterministic, so E[C(t)]=C(t)E[C(t)] = C(t)E[C(t)]=C(t). The average is the real limsup of 1T∑t=1TC(t)\frac1T \sum_{t=1}^T C(t)T1​∑t=1T​C(t). The running averages are bounded, so the limsup has no junk value.
  • Indices. Bandits, states, squares and values are Fin n, Fin M, Fin n, Fin A (0-based). Square j+1j+1j+1 is index jjj, and the value 111 is index 000.
  • Circular tape. The display on p. 303 prints "vi(t)v_i(t)vi​(t) if i=t mod ni = t \bmod ni=tmodn", which would update every square but one. The prose says that only the square under the head is updated, and the formalization follows the prose. The head is at square i≡t(modn)i \equiv t \pmod ni≡t(modn) at time ttt, so it starts at square nnn. Well-formedness (n≥1n \ge 1n≥1, F(1,1)=1F(1,1) = 1F(1,1)=1) is part of the problem.

Excluded trivialization. The goal quantifies over every PSPACE language and asks for a reduction computable in polynomial time on a compact encoding. Exhibiting one hard instance, stating the correctness of the paper's construction for the constructed instance, or measuring against a padded encoding would not prove Theorem 4.

Theorem 4 is stated as hardness only. The proof's last sentence and the introduction say "PSPACE-complete", but membership in PSPACE is not argued in the paper.

Infrastructure. A complete development needs: closure of polynomial-time TM2 computations under composition, which gives transitivity of ≤p\le_p≤p​ and turns the two milestones into the goal; a space-bounded simulation of TM2 machines by circular-tape processes; and the bandit construction with an average-cost analysis of eventually periodic deterministic trajectories. The encoding and PSPACE layer can be reused by any complexity result on the platform. Contributions to the polynomial-time composition lemmas are especially welcome.

Selected references

  • C. H. Papadimitriou and J. N. Tsitsiklis, The Complexity of Optimal Queuing Network Control, Mathematics of Operations Research 24(2):293–305, 1999. https://doi.org/10.1287/moor.24.2.293
  • P. Whittle, Restless Bandits: Activity Allocation in a Changing World, Journal of Applied Probability 25A:287–298, 1988. https://doi.org/10.2307/3214163
  • R. R. Weber and G. Weiss, On an Index Policy for Restless Bandits, Journal of Applied Probability 27(3):637–648, 1990. https://doi.org/10.2307/3214547
  • J. C. Gittins, Bandit Processes and Dynamic Allocation Indices, Journal of the Royal Statistical Society B 41(2):148–177, 1979. https://doi.org/10.1111/j.2517-6161.1979.tb01068.x
  • G. P. Klimov, Time-Sharing Service Systems I, Theory of Probability and Its Applications 19(3):532–551, 1974. https://doi.org/10.1137/1119060
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The Complexity of Optimal Queuing Network Control I: NETWORK OF QUEUES is EXP-completeResearch Paper

Motivation

Multiclass queueing networks model manufacturing lines, computer systems and communication networks. In these systems jobs of several types move between shared resources, and a controller decides where to send a job next (routing) and which waiting job a free resource works on (sequencing). The central design question is to find a control policy that maximizes long-run throughput. For decades this was attacked with heuristics, approximations and performance bounds (Walrand 1988; Bertsimas, Paschalidis and Tsitsiklis 1994; Kumar and Kumar 1994, all cited in the introduction of Papadimitriou and Tsitsiklis 1999). No general exact algorithm faster than solving a Markov decision process over all network states was found.

Papadimitriou and Tsitsiklis (1999) explained why. For closed networks with exponential service times, computing an optimal policy is EXP-complete, and therefore provably requires exponential time, independently of whether P equals NP. The paper describes this as, in its authors' experience, the first intractability result of this strength for a practical optimization problem that had been attacked for decades. This mission formalizes that theorem, Theorem 1 of the paper.

Setting

A network of queues has a finite set CCC of customer classes and a finite set SSS of servers. Each class ccc has a single server σ(c)∈S\sigma(c) \in Sσ(c)∈S that can serve it, a mean service time μ(c)≥0\mu(c) \ge 0μ(c)≥0 and a weight w(c)∈Qw(c) \in \mathbb{Q}w(c)∈Q. Service times are independent and exponentially distributed with the prescribed mean. The classes are partitioned into DDD and RRR. When a class-ccc customer completes service it changes to a new class c′c'c′: the controller chooses c′c'c′ from a given nonempty set N(c)⊆CN(c) \subseteq CN(c)⊆C if c∈Dc \in Dc∈D, and c′c'c′ is drawn with given rational probabilities pcc′p_{cc'}pcc′​ if c∈Rc \in Rc∈R. The network is closed: no customer arrives or leaves.

The state records the number of customers of each class waiting, and the class (if any) being served at each server. A policy π\piπ makes decisions as a function of the current state. At time 000 and at every service completion it routes the completing customer (if its class is in DDD), and then lets each free server either idle or start a waiting customer of one of its own classes. Service is nonpreemptive. Under a fixed policy the state evolves as a continuous-time Markov chain. Let acπ(t)a^\pi_c(t)acπ​(t) be the number of class-ccc completions up to time ttt from the given initial state. The weighted throughput is

Jπ=lim sup⁡t→∞1t∑c∈Cw(c) E[acπ(t)].J^\pi = \limsup_{t\to\infty} \frac1t \sum_{c\in C} w(c)\, \mathbb{E}\big[a^\pi_c(t)\big].Jπ=t→∞limsup​t1​c∈C∑​w(c)E[acπ​(t)].

NETWORK OF QUEUES is the decision problem: given all these data (with the initial counts in binary) and a rational KKK, is there a policy π\piπ with Jπ>KJ^\pi > KJπ>K?

EXP is the class of problems solvable in time 2p(n)2^{p(n)}2p(n) for a polynomial ppp, on inputs of length nnn. A problem is EXP-complete if it lies in EXP and every problem in EXP reduces to it by a polynomial-time many-one reduction.

The reduction source in the paper is STOCHASTIC IN-PLACE ACCEPTANCE (SIPA). A stochastic Turing machine has nondeterministic and stochastic states, each with two continuations. Its computation tree is evaluated bottom-up, taking the maximum at nondeterministic nodes and the average at stochastic nodes, and the machine accepts if the value exceeds 1/21/21/2. SIPA asks, for a machine MMM and an integer nnn in unary, whether MMM accepts nnn zeroes without leaving the nnn input squares.

Formalization targets

Goal: Theorem 1

NETWORK OF QUEUES is EXP-complete.\text{NETWORK OF QUEUES is EXP-complete.}NETWORK OF QUEUES is EXP-complete.

In Lean, EXPComplete Instance.enc networkOfQueues. The problem is in EXP, and every language L∈EXPL \in \mathrm{EXP}L∈EXP reduces to it in polynomial time.

Milestones

  1. Lemma 1: SIPA is EXP-complete.
  2. Upper bound (proof of Theorem 1, p. 296): NETWORK OF QUEUES ∈\in∈ EXP.
  3. Completeness (proof of Theorem 1, pp. 296–300): SIPA ≤p\le_p≤p​ NETWORK OF QUEUES.

Milestones 2 and 3, Lemma 1, and the transitivity of polynomial-time reductions together give the goal.

Significance

The result. Theorem 1 separates what can be computed exactly for queueing networks from what cannot. Since EXP strictly contains P by the time hierarchy theorem, no algorithm computes optimal throughput policies for all closed exponential networks in polynomial time. Unlike NP-hardness, this is unconditional. The result justifies the literature's turn to approximations, bounds and asymptotic regimes, and it motivated the complexity analysis of restless bandits in the same paper. The stochastic-machine characterization of EXP, polynomial space with stochastic and nondeterministic states, is a tool of independent interest.

Formalizing it. The theorem is proved on paper, with a reduction that the paper itself presents in sketched form. It has no machine-checked proof. The formal work includes an exponential-time Markov decision process solver expressed as a Turing machine, a simulation of alternating polynomial-space machines by stochastic ones, and the queueing-network gadget with its optimality argument. It also produces a reusable layer: EXP and polynomial-time reductions over Mathlib's Turing.FinTM2, and a controlled continuous-time Markov chain for closed queueing networks.

Difficulty

The membership half needs an exponential-time decision procedure for the average-reward criterion. This is a multichain Markov decision process with instantaneous transitions, and it must be implemented and timed on an actual Turing machine rather than argued about informally. The hardness half is harder. The network has to encode a stochastic machine's configuration. In the paper, one customer per tape square carries the square's bit and a single test customer carries the machine's state and head position. The weights are chosen so that an optimal policy is forced to simulate the machine faithfully. The paper argues optimality through the average-reward optimality equation with explicit error bounds, and it states several steps (the normal forms of the machine, the padding to linear space) as standard. Every one of these has to be made precise. Finally, composing reductions needs the composition of polynomial-time Turing machines, which Mathlib states only as proof_wanted TM2ComputableInPolyTime.comp.

Formalization scope

All declarations are in the namespace OptimalQueuingComplexity.Network. The following conventions are fixed:

  • Encoding. Instances are bit strings built by concatenating self-delimiting pieces. Naturals (including customer counts) are in binary with doubled digits and a terminator, integers in sign–magnitude form, rationals as reduced numerator/denominator pairs, and tables in index order. Classes are Fin nC and servers Fin nS. SIPA's nnn is in unary. Encodable and Nat.pair are not used: their exponential padding would make membership in EXP trivial.
  • Well-formedness is part of the problem, and ill-formed instances are no-instances. It requires σ(cs)=s\sigma(c_s) = sσ(cs​)=s for busy servers, μ≥0\mu \ge 0μ≥0, probability vectors on RRR, and N(c)≠∅N(c) \ne \emptysetN(c)=∅ on DDD. It also requires, as an added hypothesis, that no routing cycle consists of zero-mean classes.
  • Zero mean service time means instantaneous service. Simultaneous instantaneous completions are processed in increasing server index.
  • Decision epochs are time 000 and every completion. Routing precedes sequencing. Policies are deterministic and stationary. The count of a class excludes the customers in service.
  • Throughput. E[acπ(t)]\mathbb{E}[a^\pi_c(t)]E[acπ​(t)] is an extended nonnegative real computed from the embedded chain and convolutions of exponential laws (ProbabilityTheory.expMeasure). The lim sup⁡\limsuplimsup is taken in EReal. The inequality Jπ>KJ^\pi > KJπ>K is strict.
  • SIPA uses the binary alphabet. Leaving the input squares is rejection. Acceptance means that some finite-depth tree value exceeds 1/21/21/2, which equals the paper's tree value for precise machines.
  • EXP means TM2ComputableInTime with time bounded by 2p(n)2^{p(n)}2p(n). Reductions are TM2ComputableInPolyTime. Hardness quantifies over every EXP language, not over one constructed instance.

A statement about the paper's specific gadget (its servers, router and weights) is a proof step and not a target. Contributions welcome beyond the targets include composition of polynomial-time machines, a decision procedure for finite average-reward MDPs, and structural facts about the throughput (finiteness under well-formedness, attainment by stationary policies).

Selected references

  • C. H. Papadimitriou and J. N. Tsitsiklis, The Complexity of Optimal Queuing Network Control, Mathematics of Operations Research 24(2):293–305, 1999. https://doi.org/10.1287/moor.24.2.293
  • A. K. Chandra, D. C. Kozen and L. J. Stockmeyer, Alternation, Journal of the ACM 28(1):114–133, 1981. https://doi.org/10.1145/322234.322243
  • C. H. Papadimitriou, Games Against Nature, Journal of Computer and System Sciences 31(2):288–301, 1985. https://doi.org/10.1016/0022-0000(85)90045-5
  • M. L. Puterman, Markov Decision Processes: Discrete Stochastic Dynamic Programming, Wiley, 1994. https://doi.org/10.1002/9780470316887
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Stochastic Dynamic Programming and the Control of Queueing Systems V: The Average Cost Optimality Equation and Value Iteration for Finite State SpacesTextbook

Motivation

Average cost Markov decision chains model systems that run indefinitely and are judged by their long-run cost per step: admission and routing control in queues, inventory replenishment, machine maintenance. For a finite state space the classical tool is the average cost optimality equation (ACOE)

J+h(i)=min⁡a∈Ai{C(i,a)+∑jPij(a) h(j)},J + h(i) = \min_{a \in A_i}\Big\{C(i,a) + \sum_j P_{ij}(a)\,h(j)\Big\},J+h(i)=a∈Ai​min​{C(i,a)+j∑​Pij​(a)h(j)},

whose solution gives both the minimum average cost JJJ and an optimal stationary policy. To be useful the equation has to be solved numerically, and the method used in practice is value iteration: compute the minimum nnn-horizon costs vnv_nvn​ and extract JJJ and hhh from their growth. This mission formalizes Sections 6.4–6.6 of L. I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems (Wiley, 1999, doi:10.1002/9780470317037): when the minimum average cost is constant, the ACOE holds, any solution of it is optimal, and value iteration converges, provided the optimal policies are aperiodic. When they are not, a transformation of the model makes them so.

Related classical work includes Blackwell's discrete dynamic programming (1962) and Schweitzer–Federgruen's analysis of undiscounted value iteration (1977); Sennott's treatment derives the ACOE from the discounted value function VαV_\alphaVα​ as α→1−\alpha \to 1^-α→1−, which is the route that extends to countable state spaces in later chapters of the book.

Setting

A Markov decision chain (MDC) Δ\DeltaΔ has a finite state space SSS; in each state iii a finite nonempty action set AiA_iAi​; nonnegative costs C(i,a)C(i,a)C(i,a); and transition probabilities Pij(a)P_{ij}(a)Pij​(a). A policy θ\thetaθ may use the whole history and randomize; a stationary policy eee always chooses e(i)∈Aie(i) \in A_ie(i)∈Ai​ in state iii and induces a Markov chain with transitions Pij(e)=Pij(e(i))P_{ij}(e) = P_{ij}(e(i))Pij​(e)=Pij​(e(i)).

For a policy θ\thetaθ and initial state iii: vθ,n(i)v_{\theta,n}(i)vθ,n​(i) is the expected cost of the first nnn steps, Vθ,α(i)V_{\theta,\alpha}(i)Vθ,α​(i) the expected α\alphaα-discounted cost, and Jθ(i)=lim sup⁡nvθ,n(i)/nJ_\theta(i) = \limsup_n v_{\theta,n}(i)/nJθ​(i)=limsupn​vθ,n​(i)/n the average cost. The value functions are the infima over all policies: vnv_nvn​, VαV_\alphaVα​ and the minimum average cost J(i)J(i)J(i). A policy is average cost optimal if Jθ≡JJ_\theta \equiv JJθ​≡J.

Section 6.2 of the book provides a stationary policy fff that is α\alphaα discount optimal for all α\alphaα close to 111 (a Blackwell optimal policy), and Section 6.3 builds from it a relative value function w∗w^*w∗. For a distinguished state zzz put

hα(i)=Vα(i)−Vα(z),h(i)=lim⁡α→1−hα(i),dn(i)=h(i)+nJ−vn(i).h_\alpha(i) = V_\alpha(i) - V_\alpha(z), \qquad h(i) = \lim_{\alpha\to1^-} h_\alpha(i), \qquad d_n(i) = h(i) + nJ - v_n(i).hα​(i)=Vα​(i)−Vα​(z),h(i)=α→1−lim​hα​(i),dn​(i)=h(i)+nJ−vn​(i).

For a distinguished state xxx the finite horizon relative value function is rn(i)=vn(i)−vn(x)r_n(i) = v_n(i) - v_n(x)rn​(i)=vn​(i)−vn​(x).

A positive recurrent class RRR of a Markov chain is aperiodic if Pij(n)→πjP^{(n)}_{ij} \to \pi_jPij(n)​→πj​ for i,j∈Ri, j \in Ri,j∈R, where π\piπ is the steady state distribution. Assumption OPA ("optimal policies are aperiodic") requires every positive recurrent class of every average cost optimal stationary policy to be aperiodic. The aperiodicity transformation Δ∗\Delta^*Δ∗ with 0<τ<10<\tau<10<τ<1 keeps states and actions, scales costs by τ\tauτ, and sets Pij∗(a)=τPij(a)P^*_{ij}(a) = \tau P_{ij}(a)Pij∗​(a)=τPij​(a) for j≠ij \ne ij=i, Pii∗(a)=τPii(a)+(1−τ)P^*_{ii}(a) = \tau P_{ii}(a) + (1-\tau)Pii∗​(a)=τPii​(a)+(1−τ).

Formalization targets

Goal: convergence of value iteration (Proposition 6.6.3)

If J(i)≡JJ(i) \equiv JJ(i)≡J and Assumption OPA holds, then for any distinguished state xxx

lim⁡n→∞[vn(x)−vn−1(x)]=J,lim⁡n→∞rn(i)=:r(i) exists,\lim_{n\to\infty}[v_n(x) - v_{n-1}(x)] = J, \qquad \lim_{n\to\infty} r_n(i) =: r(i) \text{ exists},n→∞lim​[vn​(x)−vn−1​(x)]=J,n→∞lim​rn​(i)=:r(i) exists,

(J,r)(J, r)(J,r) solves the ACOE, and every limit point of the finite horizon optimal stationary policies is average cost optimal.

Milestones

  1. Proposition 6.4.1: unichain structure, bounded ∣Vα(i)−Vα(z)∣|V_\alpha(i) - V_\alpha(z)|∣Vα​(i)−Vα​(z)∣, or pairwise reachability imply J(i)≡JJ(i) \equiv JJ(i)≡J, with the implication diagram (6.26).
  2. Theorem 6.4.2: under J(i)≡JJ(i) \equiv JJ(i)≡J, hhh exists, solves the ACOE (6.31), yields optimal policies, ∣dn∣≤L|d_n| \le L∣dn​∣≤L and vn/n→Jv_n/n \to Jvn​/n→J.
  3. Proposition 6.5.1: any finite solution (F,r)(F, r)(F,r) of the ACOE (or of the inequality (6.36)) gives J≡FJ \equiv FJ≡F and optimal policies, and differs from hhh by constants on recurrent classes.
  4. Lemma 6.6.2: on an aperiodic positive recurrent class of an optimal policy, dnd_ndn​ converges to a constant.
  5. Lemma 6.6.5 and Proposition 6.6.6: Δ∗\Delta^*Δ∗ has the same recurrent classes and steady states, all of them aperiodic, costs scaled by τ\tauτ; value iteration on Δ∗\Delta^*Δ∗ produces a solution (J∗/τ,r∗)(J^*/\tau, r^*)(J∗/τ,r∗) of the ACOE of Δ\DeltaΔ.

Significance

The ACOE with constant JJJ is the standard certificate of optimality for finite average cost models, and Proposition 6.5.1 is what allows any numerical solution of it to be trusted. Proposition 6.6.3 is the correctness theorem of the value iteration algorithm (VIA 6.6.4 of the book), and Proposition 6.6.6 removes its one extra hypothesis at the price of a model transformation. Chapter 8 of the book runs this algorithm on a sequence of finite truncations to compute optimal policies for countable-state queueing models, so these results are the base of the book's computational method.

All results in this mission are proved in the book; none has a machine-checked proof. Existing formalizations on the platform treat average reward models under a unichain hypothesis with a single action set type; this mission assumes only a constant minimum average cost (multichain models allowed) and uses the general policy class throughout.

Difficulty

The ACOE itself is not the obstacle; convergence of vn(x)−vn−1(x)v_n(x) - v_{n-1}(x)vn​(x)−vn−1​(x) is. Theorem 6.4.2 bounds dnd_ndn​ but does not make it converge, and Example 6.6.1 of the book (a two-state periodic chain) shows that without aperiodicity vn(x)−vn−1(x)v_n(x) - v_{n-1}(x)vn​(x)−vn−1​(x) oscillates. The naive argument, passing to the limit in the finite horizon optimality equation, assumes the limits exist, which is exactly what is in question. Chain structure is the obstruction: a multichain optimal policy has several recurrent classes, and the Cesàro-type convergence that suffices for the ACOE itself is weaker than the pointwise convergence value iteration needs. The policy statement is also delicate, since the finite horizon minimizers fnf_nfn​ need not converge.

Formalization scope

  • The state type S is finite ([Fintype S]); actions are a type Act with per-state nonempty Finset action sets. Costs are in ℝ≥0, transition probabilities in ℝ≥0∞, and all value functions are defined in [0,∞] as infima over all history-dependent randomized policies, then converted to ℝ (they are finite for finite SSS).
  • JJJ constant is stated as J(i)=JJ(i) = JJ(i)=J for all iii, with J∈R≥0J \in \mathbb R_{\ge 0}J∈R≥0​. The relative value hhh is defined as the limit α→1−\alpha \to 1^-α→1− of hαh_\alphahα​, not taken as an arbitrary solution of the ACOE; Theorem 6.4.2(i) asserts the limit exists. The Blackwell optimal policy fff enters as a hypothesis: any stationary policy discount optimal on an interval (α0,1)(\alpha_0,1)(α0​,1).
  • min_a is Finset.inf' over AiA_iAi​. Limit points of policy sequences follow Definition B.1 (a subsequence agreeing eventually in every state). Finite horizon optimal policies fnf_nfn​ are any minimizers of vn(i)=min⁡a{C(i,a)+∑jPij(a)vn−1(j)}v_n(i) = \min_a\{C(i,a) + \sum_j P_{ij}(a) v_{n-1}(j)\}vn​(i)=mina​{C(i,a)+∑j​Pij​(a)vn−1​(j)}.
  • Aperiodicity of a class is the book's definition (Pij(n)→πjP^{(n)}_{ij} \to \pi_jPij(n)​→πj​ on the class), with πj=1/mjj\pi_j = 1/m_{jj}πj​=1/mjj​. Assumption OPA quantifies over average cost optimal stationary policies only, not over all stationary policies.
  • A trivializing formalization is ruled out: hhh, rnr_nrn​, dnd_ndn​ and vnv_nvn​ are computed from the model, not free functions constrained by the ACOE, and the ACOE conclusions are equalities of real numbers with the minimum over the actual action sets.
  • The model, criteria and Markov chain definitions restate those of mission IV of this series in their own namespace; they are reusable for any finite average cost result. Contributions of general Markov chain facts (convergence of P(n)P^{(n)}P(n) on aperiodic classes, Cesàro limits 1n∑tP(t)\frac1n\sum_t P^{(t)}n1​∑t​P(t)) are welcome.

Selected references

  • L. I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems, Wiley Series in Probability and Statistics, Wiley, 1999. https://doi.org/10.1002/9780470317037
  • D. Blackwell, Discrete dynamic programming, Annals of Mathematical Statistics 33 (1962), 719–726. https://doi.org/10.1214/aoms/1177704593
  • P. J. Schweitzer and A. Federgruen, The asymptotic behavior of undiscounted value iteration in Markov decision problems, Mathematics of Operations Research 2 (1977), 360–381. https://doi.org/10.1287/moor.2.4.360
  • M. L. Puterman, Markov Decision Processes: Discrete Stochastic Dynamic Programming, Wiley, 1994. https://doi.org/10.1002/9780470316887
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Lost-Sales Problems with Stochastic Lead Times: Convexity Results for Base-Stock Policies: Expected Discounted Cost Is Convex in the Base-Stock LevelResearch Paper

Why base-stock levels in lost-sales systems

In many inventory systems, demand that cannot be met from stock is lost rather than backordered: a customer who finds the shelf empty buys elsewhere. For such lost-sales systems with positive lead times the optimal replenishment policy is known to be complex and to depend on the whole pipeline of outstanding orders (Karlin and Scarf, 1958; Morton, 1969). In practice, firms nonetheless use base-stock (order-up-to-SSS) policies, which reorder every period whatever was sold. Choosing such a policy comes down to choosing one number, the base-stock level SSS. How easy that choice is depends on how the expected cost behaves as a function of SSS.

Earlier work had established convexity in SSS for backordered demand (Healy, 1992, for (s,S)(s,S)(s,S) policies) and for lost sales with deterministic lead times (Downs, Metters and Semple, 2001). Nahmias (1979) observed in simulation that the cost surface looked convex for lost-sales systems with random lead times, but had no proof. Janakiraman and Roundy (2004) proved convexity for lost-sales systems whose lead times are stochastic but do not cross. On every sample path this holds when holding cost is charged only on the inventory position. In expectation it holds for the full cost under the lead-time model of Kaplan (1970). This mission formalizes the finite-horizon part of that paper (Sections 3–4).

Setting

Periods are indexed n=0,1,…,Nn = 0, 1, \dots, Nn=0,1,…,N. The demand in period nnn is Dn≥0D_n \ge 0Dn​≥0. The order placed in period ttt has a lead time L(t)∈{0,1,2,… }L(t) \in \{0, 1, 2, \dots\}L(t)∈{0,1,2,…} and arrives in period t+L(t)t + L(t)t+L(t). The arrival index is

λn=max⁡{t:t+L(t)≤n},\lambda_n = \max\{t : t + L(t) \le n\},λn​=max{t:t+L(t)≤n},

the index of the latest order that has arrived by period nnn, with λn=0\lambda_n = 0λn​=0 when no order has arrived (in particular λ0=0\lambda_0 = 0λ0​=0). Assumption 1 (orders do not cross) requires n+L(n)n + L(n)n+L(n) to be weakly increasing in nnn.

Under an order-up-to-SSS policy, the system starts with SSS units on hand and nothing on order. Each period it orders what was sold in the previous period. With orders qn(S)q_n(S)qn​(S), the quantities of period nnn are:

  • the order q0(S)=0q_0(S) = 0q0​(S)=0 and qn+1(S)=yn(S)q_{n+1}(S) = y_n(S)qn+1​(S)=yn​(S);
  • the inventory on hand after receipts, xn(S)=S−∑λn<t≤nqt(S)x_n(S) = S - \sum_{\lambda_n < t \le n} q_t(S)xn​(S)=S−∑λn​<t≤n​qt​(S);
  • the sales yn(S)=min⁡(xn(S),Dn)y_n(S) = \min(x_n(S), D_n)yn​(S)=min(xn​(S),Dn​);
  • the end-of-period inventory on hand in(S)=xn(S)−yn(S)i_n(S) = x_n(S) - y_n(S)in​(S)=xn​(S)−yn​(S);
  • the end-of-period inventory position πn(S)=S−yn(S)\pi_n(S) = S - y_n(S)πn​(S)=S−yn​(S);
  • the lost sales ln(S)=Dn−yn(S)l_n(S) = D_n - y_n(S)ln​(S)=Dn​−yn​(S).

For a discount factor 0<α≤10 < \alpha \le 10<α≤1 and cost rates h1,h2,p≥0h_1, h_2, p \ge 0h1​,h2​,p≥0, the discounted cost (3.1) is

CN(S)=∑n=0Nαn(h1 πn(S)+h2 in(S)+p ln(S)).C_N(S) = \sum_{n=0}^{N} \alpha^n \big(h_1\,\pi_n(S) + h_2\,i_n(S) + p\,l_n(S)\big).CN​(S)=n=0∑N​αn(h1​πn​(S)+h2​in​(S)+pln​(S)).

Here h1h_1h1​ is charged on the inventory position (on hand plus in transit), h2h_2h2​ on stock physically on hand, and ppp on each lost unit.

In the Kaplan lead-time model (Assumption 2) the arrival index is random: λ0=0\lambda_0 = 0λ0​=0 and λn=max⁡(λn−1,n−ρn)\lambda_n = \max(\lambda_{n-1}, n - \rho_n)λn​=max(λn−1​,n−ρn​) for n≥1n \ge 1n≥1, where (ρn)(\rho_n)(ρn​) is an i.i.d. sequence of nonnegative integer-valued random variables. The same dynamics, driven by λ(ρ)\lambda(\rho)λ(ρ), give random quantities xn(S,ρ)x_n(S,\rho)xn​(S,ρ), in(S,ρ)i_n(S,\rho)in​(S,ρ), πn(S,ρ)\pi_n(S,\rho)πn​(S,ρ) and ln(S,ρ)l_n(S,\rho)ln​(S,ρ). EρE_\rhoEρ​ is the expectation over ρ\rhoρ with the demands held fixed.

Formalization targets

Goal: Theorem 8

Under Assumption 2, for every realization of demands D0,…,DN≥0D_0, \dots, D_N \ge 0D0​,…,DN​≥0, every 0<α≤10 < \alpha \le 10<α≤1 and all h1,h2,p≥0h_1, h_2, p \ge 0h1​,h2​,p≥0,

S↦Eρ[∑n=0Nαn(h1 πn(S,ρ)+h2 in(S,ρ)+p ln(S,ρ))] is convex on [0,∞).S \mapsto E_\rho\Big[\sum_{n=0}^{N} \alpha^n\big(h_1\,\pi_n(S,\rho) + h_2\,i_n(S,\rho) + p\,l_n(S,\rho)\big)\Big] \text{ is convex on } [0,\infty).S↦Eρ​[n=0∑N​αn(h1​πn​(S,ρ)+h2​in​(S,ρ)+pln​(S,ρ))] is convex on [0,∞).

Milestones

  1. Lemma 3. On a noncrossing sample path, for every m≤N+1m \le N+1m≤N+1 and every nonnegative, weakly decreasing (βn)(\beta_n)(βn​), S↦∑n=0mβn qn(S)S \mapsto \sum_{n=0}^{m} \beta_n\, q_n(S)S↦∑n=0m​βn​qn​(S) is concave.
  2. Corollary 4. On a noncrossing sample path, for every m≤Nm \le Nm≤N and every such (βn)(\beta_n)(βn​), ∑n=0mβn ln(S)\sum_{n=0}^{m}\beta_n\, l_n(S)∑n=0m​βn​ln​(S) and ∑n=0mβn πn(S)\sum_{n=0}^{m}\beta_n\,\pi_n(S)∑n=0m​βn​πn​(S) are convex in SSS.
  3. Theorem 5. On a noncrossing sample path, ∑n=0Nαn(h1 πn(S)+p ln(S))\sum_{n=0}^{N}\alpha^n\big(h_1\,\pi_n(S) + p\,l_n(S)\big)∑n=0N​αn(h1​πn​(S)+pln​(S)) is convex in SSS.
  4. Lemma 6. Under Assumption 2, ∑n=0mβn Eρ[xn(S,ρ)]\sum_{n=0}^{m}\beta_n\, E_\rho[x_n(S,\rho)]∑n=0m​βn​Eρ​[xn​(S,ρ)] is convex in SSS for every m≤Nm \le Nm≤N and every such (βn)(\beta_n)(βn​).
  5. Corollary 7. The same holds for ∑n=0mβn Eρ[in(S,ρ)]\sum_{n=0}^{m}\beta_n\, E_\rho[i_n(S,\rho)]∑n=0m​βn​Eρ​[in​(S,ρ)].

Significance

Theorem 5 shows that, when the only holding cost is charged on the inventory position, the discounted cost of every noncrossing sample path is convex in SSS. It therefore stays convex under any distribution of noncrossing lead times and any demand process independent of them. Theorem 8 extends convexity to storage costs on stock on hand, which matter whenever payment is due on arrival. A sample-path statement cannot do this. On a sample path the extension fails: the paper's Example 1 exhibits a concave kink at S=1S = 1S=1 when h2>0h_2 > 0h2​>0. Both results make the choice of the best base-stock level a one-dimensional convex minimization, so bisection or simulation-based search methods are guaranteed to converge to a global optimum. The paper's Example 2 shows that noncrossing cannot be dropped.

The results are proved in the paper. As far as is known, none has a machine-checked proof. A formalization adds a precise, reusable model of periodic-review lost-sales dynamics with stochastic lead times, and a checked account of exactly which hypotheses (noncrossing, h2=0h_2 = 0h2​=0 on sample paths, the Kaplan structure in expectation) each convexity claim needs.

Difficulty

Individual per-period quantities are not convex: qn(S)q_n(S)qn​(S), xn(S)x_n(S)xn​(S), in(S)i_n(S)in​(S) and πn(S)\pi_n(S)πn​(S) are piecewise linear with slopes in {0,1}\{0,1\}{0,1} and are neither convex nor concave in SSS. The obvious approach, proving each term of the cost convex and summing, therefore fails. Convexity appears only in the weighted sums, and only for nonnegative, weakly decreasing weights. The recursion defining xnx_nxn​ refers back to earlier orders through a window (λn,n](\lambda_n, n](λn​,n] that moves with the lead-time path, so an induction on mmm has to carry a family of weight sequences rather than one fixed sum.

In expectation, the storage-cost term ∑nβn in\sum_n \beta_n\, i_n∑n​βn​in​ is not convex path by path. Convexity of its expectation depends on the distributional structure of the Kaplan model, namely that the lead time of the order placed in period nnn is independent of the state of the system at that time. Stating this correctly requires a genuine probability space, not a sample-path argument.

Formalization scope

  • Model. One definition of the dynamics, parametrised by an arrival-index path λ:N→N\lambda : \mathbb{N} \to \mathbb{N}λ:N→N, a demand path D:N→RD : \mathbb{N} \to \mathbb{R}D:N→R and a real SSS (orderQty, onHand, sales, endOnHand, invPosition, lostSales). The sample-path results use arrivalIndex L (via Nat.findGreatest). The Kaplan results use kaplanIndex ρ, the recursion of Assumption 2 with λ0=0\lambda_0 = 0λ0​=0. The discounted cost (3.1) is discountedCost.
  • Hypotheses. Assumption 1 is MonotoneOn (fun n => n + L n) (Set.Iic N). Demands satisfy Dn≥0D_n \ge 0Dn​≥0 for n≤Nn \le Nn≤N. Weight sequences are β : ℕ → ℝ with 0 ≤ β n and Antitone β. Costs satisfy 0<α≤10 < \alpha \le 10<α≤1 and h1,h2,p≥0h_1, h_2, p \ge 0h1​,h2​,p≥0, the paper's Section 3 standing assumptions. "Increasing" and "decreasing" are weak, as the paper states.
  • Domain. Every convexity or concavity claim is ConvexOn ℝ (Set.Ici 0) / ConcaveOn ℝ (Set.Ici 0): the base-stock level is an initial stock, S≥0S \ge 0S≥0.
  • Expectation. (Ω,P)(\Omega, P)(Ω,P) is a probability space. ρ:N→Ω→N\rho : \mathbb{N} \to \Omega \to \mathbb{N}ρ:N→Ω→N has measurable coordinates, iIndepFun ρ P, and IdentDistrib (ρ n) (ρ 0) P P for all nnn. Eρ[f]E_\rho[f]Eρ​[f] is the Bochner integral ∫f(λ(ρ(ω))) dP(ω)\int f(\lambda(\rho(\omega)))\,dP(\omega)∫f(λ(ρ(ω)))dP(ω). For S≥0S \ge 0S≥0 the integrands are bounded and depend on finitely many coordinates, so they are integrable and the integral is the paper's expectation. Measurability of ρ\rhoρ is the field's standing convention.
  • Ruled out. The Kaplan statements are about the Kaplan index of an i.i.d. sequence, not about an arbitrary nondecreasing arrival process. The sample-path statements carry the noncrossing hypothesis, without which they are false. The convexity domain is the half-line, not a finite or degenerate set.
  • Needed infrastructure. Convexity and concavity of finite sums and minima (Mathlib's ConvexOn/ConcaveOn), integrals of bounded functions of finitely many independent discrete variables, and the independence and identical distribution facts of the Kaplan model. The dynamics and the Kaplan index are reusable for any further analysis of base-stock lost-sales systems, including the paper's infinite-horizon results. Proofs of the milestones in any order are welcome, as are auxiliary lemmas identifying the Kaplan index as the arrival index of a noncrossing lead-time path.

Selected references

  • G. Janakiraman and R. O. Roundy, Lost-Sales Problems with Stochastic Lead Times: Convexity Results for Base-Stock Policies, Operations Research 52(5):795–803, 2004. https://doi.org/10.1287/opre.1040.0130
  • R. S. Kaplan, A Dynamic Inventory Model with Stochastic Lead Times, Management Science 16(7):491–507, 1970. https://doi.org/10.1287/mnsc.16.7.491
  • S. Karlin and H. Scarf, Inventory Models of the Arrow–Harris–Marschak Type with Time Lag, in Studies in the Mathematical Theory of Inventory and Production, Stanford University Press, 1958.
  • T. E. Morton, Bounds on the Solution of the Lagged Optimal Inventory Equation with No Demand Backlogging and Proportional Costs, SIAM Review 11(4):572–596, 1969. https://doi.org/10.1137/1011090
  • S. Nahmias, Simple Approximations for a Variety of Dynamic Leadtime Lost-Sales Inventory Models, Operations Research 27(5):904–924, 1979. https://doi.org/10.1287/opre.27.5.904
  • B. Downs, R. Metters and J. Semple, Managing Inventory with Multiple Products, Lags in Delivery, Resource Constraints, and Lost Sales: A Mathematical Programming Approach, Management Science 47(3):464–479, 2001. https://doi.org/10.1287/mnsc.47.3.464.9775
  • R. Ehrhardt, (s, S) Policies for a Dynamic Inventory Model with Stochastic Lead Times, Operations Research 32(1):121–132, 1984. https://doi.org/10.1287/opre.32.1.121
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Functional Analysis·Captain: savarin

Does the sharp diagonal Hlawka constant work for all complex matrices when p ≥ 256?Open Problem

The Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. The question is how large a comparison constant is needed to make this inequality hold.

Does the sharp diagonal constant work for general matrices?

For every real p≥256p\ge256p≥256, the optimal Hlawka constant for complex diagonal matrices is already proved in Lean. This mission asks whether that same constant works for all complex matrices, including rectangular ones. The statement is a conjecture. Accepted diagonal result

Audenaert and Kittaneh's Problem 7 asks for the best constant in the Schatten-norm setting, if one exists. Existence of some finite dimension-independent constant for every real p>1p>1p>1 is already settled by the project's Lean theorem. The task here is to establish the specified sharp candidate in the range p≥256p\ge256p≥256. Audenaert–Kittaneh, §8.2, proved existence result

Definitions and the goal

For a complex matrix AAA with singular values si(A)s_i(A)si​(A), its Schatten norm is

Np(A)=(∑isi(A)p)1/p.N_p(A)=\left(\sum_i s_i(A)^p\right)^{1/p}.Np​(A)=(i∑​si​(A)p)1/p.

There is no normalization by dimension. For three matrices of the same shape, define

Δ3=Np(A)+Np(B)+Np(C)−Np(A+B+C),\Delta_3=N_p(A)+N_p(B)+N_p(C)-N_p(A+B+C),Δ3​=Np​(A)+Np​(B)+Np​(C)−Np​(A+B+C), Δ2=2(Np(A)+Np(B)+Np(C))−Np(A+B)−Np(A+C)−Np(B+C).\Delta_2=2\bigl(N_p(A)+N_p(B)+N_p(C)\bigr) -N_p(A+B)-N_p(A+C)-N_p(B+C).Δ2​=2(Np​(A)+Np​(B)+Np​(C))−Np​(A+B)−Np​(A+C)−Np​(B+C).

Formal Schatten-norm definition

The shared cyclic candidate is

Kp=sup⁡t∈[1/2,2]3(tp+2)1/p−31/p∣2−t∣6(tp+2)1/p−3(2∣1−t∣p+2p)1/p.K_p=\sup_{t\in[1/2,2]} \frac{3(t^p+2)^{1/p}-3^{1/p}|2-t|} {6(t^p+2)^{1/p}-3(2|1-t|^p+2^p)^{1/p}}.Kp​=t∈[1/2,2]sup​6(tp+2)1/p−3(2∣1−t∣p+2p)1/p3(tp+2)1/p−31/p∣2−t∣​.

The fraction is the deficit ratio for the coordinate triple (−t,1,1),(1,−t,1),(1,1,−t)(-t,1,1),(1,-t,1),(1,1,-t)(−t,1,1),(1,−t,1),(1,1,−t). For p>1p>1p>1, its denominator is positive on the displayed interval and the supremum is attained. Cyclic definitions and attainment

The goal asks whether Δ3≤KpΔ2\Delta_3\le K_p\Delta_2Δ3​≤Kp​Δ2​ for every real p≥256p\ge256p≥256 and every triple of complex matrices of every finite shape. One constant for each exponent must work across all dimensions and triples. The endpoint 256, noninteger exponents, zero dimensions, singular and zero matrices, unequal norms and zero pair deficit are included.

Lean states the goal for complex-linear maps between any two finite-dimensional complex inner-product spaces, allowing different dimensions. No positivity, self-adjointness, commutativity or common diagonalization assumption is imposed.

Why the diagonal proof does not settle this

The singular values determine a matrix's own norm. However, the separate singular-value lists of three matrices do not determine the norms of their pair sums and total sum. The diagonal theorem therefore does not supply the seven matrix norms needed in this inequality. Their relative directions matter as well.

The existing existence theorem supplies a constant, but does not identify it with KpK_pKp​. A proof here needs the exact cyclic constant. A proof only for even integer exponents or a restricted class of matrices would not settle this goal.

What a resolution would establish

If the conjectured bound holds, it is automatically optimal uniformly over all finite matrix shapes: diagonal three-dimensional examples already require at least KpK_pKp​. Thus the missing step is that this constant works for arbitrary matrices. A counterexample would show that the diagonal constant is insufficient somewhere in the stated range. Cyclic lower bound, diagonal Schatten identity

Either outcome addresses this range of exponents; it would not settle the optimal general-matrix constant for every 1<p<2561<p<2561<p<256.

The foundation mission establishes the optimal diagonal constant for every real p≥256p\ge256p≥256. The cutoff-90 mission has since extended the diagonal result in Lean to every real p≥90p\ge90p≥90. The diagonal campaign invites contributors to lower that cutoff below 90.

This mission keeps p≥256p\ge256p≥256 and asks whether the same optimal constant works for arbitrary complex matrices, including rectangular ones. It can be pursued independently of improvements to the diagonal cutoff.

Its three linked milestones are already-proved background: existence, the sharp diagonal result, and the diagonal norm identity. The main general-matrix goal remains open. No complete proof is supplied for it.

References

  • K. M. R. Audenaert and F. Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, 2012, §8.2, Problem 7. arXiv:1201.5232
  • Ezzeri Esa and contributors, Hlawka–Schatten inequalities, Lean source repository, revision 79aa498bfcf7b22bd91d771fb32ec278e2d4704b. Existence and diagonal libraries

Established results on Prove2Me

  • The accepted sharp diagonal bound for every real p ≥ 256.
  • The accepted diagonal Schatten norm identity.
  • The public existence theorem for every real p > 1.
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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

Minimization Methods for Non-Differentiable Functions IX: Convergence of the r-Algorithm with Exact Directional MinimizationTextbook

Motivation

The r-algorithm of N. Z. Shor is a variable-metric method for minimizing functions that are not differentiable everywhere, such as maxima of smooth functions, penalty functions and Lagrangian dual functions of integer and decomposition problems. It combines a subgradient step with a space dilation along the difference of two successive almost-gradients, and the book reports it competitive with the best variable-metric and conjugate-gradient methods on "gully"-shaped test problems (Shor 1985, §3.6, pp. 68–77). Its convergence theory is limited. Section 3.7 of Shor's book gives a convergence proof only for an idealized version with exact directional minimization, on a class of piecewise smooth functions, and the book itself calls a weakening of the assumptions and rate estimates desirable (p. 85). This mission formalizes that section.

Timeline. Shor and Zhurbenko introduced the r-algorithm in 1971 (Kibernetika, no. 3, 51–59). Shor analysed the convergence of its exact-line-search version in 1975 (Kibernetika, no. 4, 48–53). Section 3.7 of the 1979 Russian monograph, translated in 1985, gives that analysis for piecewise smooth functions. The book states on p. 85 that weaker assumptions and rate estimates would be desirable.

Setting

Let EnE_nEn​ be nnn-dimensional Euclidean space with inner product (x,y)(x, y)(x,y), n≥1n \ge 1n≥1. For a unit vector ξ\xiξ and α>0\alpha > 0α>0 the operator of space dilation is Rα(ξ)x=x+(α−1)(x,ξ)ξR_\alpha(\xi)x = x + (\alpha - 1)(x, \xi)\xiRα​(ξ)x=x+(α−1)(x,ξ)ξ.

Widths. For a compact convex set WWW and a unit vector η\etaη, the width in direction η\etaη is dη(W)=max⁡x∈W(η,x)−min⁡x∈W(η,x)d_\eta(W) = \max_{x \in W}(\eta, x) - \min_{x \in W}(\eta, x)dη​(W)=maxx∈W​(η,x)−minx∈W​(η,x). The width is d(W)=min⁡∥η∥=1dη(W)d(W) = \min_{\|\eta\| = 1} d_\eta(W)d(W)=min∥η∥=1​dη​(W) and the diameter is D(W)=max⁡∥η∥=1dη(W)D(W) = \max_{\|\eta\| = 1} d_\eta(W)D(W)=max∥η∥=1​dη​(W). With eρ(W)=inf⁡z∈W∣(ρ,z)∣e_\rho(W) = \inf_{z \in W}|(\rho, z)|eρ​(W)=infz∈W​∣(ρ,z)∣ put Kρ(W)=dρ(W)/eρ(W)K_\rho(W) = d_\rho(W)/e_\rho(W)Kρ​(W)=dρ​(W)/eρ​(W) (or +∞+\infty+∞ when eρ(W)=0e_\rho(W) = 0eρ​(W)=0) and p(W)=inf⁡∥ρ∥=1Kρ(W)p(W) = \inf_{\|\rho\| = 1} K_\rho(W)p(W)=inf∥ρ∥=1​Kρ​(W).

The class KKK. EnE_nEn​ is partitioned into closed sets Dˉ1,…,Dˉm\bar D_1, \dots, \bar D_mDˉ1​,…,Dˉm​, each the closure of its interior, whose interiors are disjoint and homeomorphic to an open ball or open halfspace; fif_ifi​ is continuously differentiable on an open set containing Dˉi\bar D_iDˉi​; and f=fif = f_if=fi​ on Dˉi\bar D_iDˉi​. At a point xxx, the set of almost-gradients Gf(x)G_f(x)Gf​(x) is the set of gradients ∇fi(x)\nabla f_i(x)∇fi​(x) of the pieces with x∈Dˉix \in \bar D_ix∈Dˉi​. For δ,ε>0\delta, \varepsilon > 0δ,ε>0, Pˉδ,ε(x)\bar P_{\delta,\varepsilon}(x)Pˉδ,ε​(x) is the closed convex hull of all Gf(y)G_f(y)Gf​(y), ∥y−x∥<δ\|y - x\| < \delta∥y−x∥<δ, together with the ε\varepsilonε-balls around the elements of Gf(x)G_f(x)Gf​(x).

The r(α)r(\alpha)r(α)-algorithm. Fix α>1\alpha > 1α>1, β=1/α\beta = 1/\alphaβ=1/α. Start from x0x_0x0​, g~0=0\tilde g_0 = 0g~​0​=0 and a nonsingular B0B_0B0​. At iteration k+1k + 1k+1 choose gf(xk)∈Gf(xk)g_f(x_k) \in G_f(x_k)gf​(xk​)∈Gf​(xk​) with (Bk∗gf(xk),g~k)≤0(B_k^* g_f(x_k), \tilde g_k) \le 0(Bk∗​gf​(xk​),g~​k​)≤0; set gk∗=Bk∗gf(xk)g_k^* = B_k^* g_f(x_k)gk∗​=Bk∗​gf​(xk​), rk=gk∗−g~kr_k = g_k^* - \tilde g_krk​=gk∗​−g~​k​, ξk+1=rk/∥rk∥\xi_{k+1} = r_k/\|r_k\|ξk+1​=rk​/∥rk​∥, Bk+1=BkRβ(ξk+1)B_{k+1} = B_k R_\beta(\xi_{k+1})Bk+1​=Bk​Rβ​(ξk+1​), g~k+1=Rβ(ξk+1)gk∗\tilde g_{k+1} = R_\beta(\xi_{k+1}) g_k^*g~​k+1​=Rβ​(ξk+1​)gk∗​, and xk+1=xk−hk+1Bk+1g~k+1x_{k+1} = x_k - h_{k+1}B_{k+1}\tilde g_{k+1}xk+1​=xk​−hk+1​Bk+1​g~​k+1​ with hk+1≥0h_{k+1} \ge 0hk+1​≥0 such that fff does not increase along the step and some almost-gradient at xk+1x_{k+1}xk+1​ makes a non-acute angle with g~k+1\tilde g_{k+1}g~​k+1​ in the transformed metric. The standing assumption is f(x)→+∞f(x) \to +\inftyf(x)→+∞ as ∥x∥→∞\|x\| \to \infty∥x∥→∞ (3.50).

Formalization targets

Goal: convergence to an isolated local minimum (Theorem 3.13)

Assume (3.50) and ∥xk+1−xk∥→0\|x_{k+1} - x_k\| \to 0∥xk+1​−xk​∥→0 (3.52). If x∗x^*x∗ is an isolated local minimum, the component of {x:f(x∗)≤f(x)≤f(x0)}\{x : f(x^*) \le f(x) \le f(x_0)\}{x:f(x∗)≤f(x)≤f(x0​)} containing x0x_0x0​ also contains x∗x^*x∗, and no other point zzz of that component has linearly dependent Gf(z)G_f(z)Gf​(z), then

lim⁡k→∞xk=x∗.\lim_{k \to \infty} x_k = x^* .k→∞lim​xk​=x∗.

Milestones

  • Lemma 3.2 (p. 80): for B=SOB = SOB=SO with minimum eigenvalue λ(B)\lambda(B)λ(B) of SSS, λ(B)d(W)≤d(BW)≤λ(B)D(W)\lambda(B)d(W) \le d(BW) \le \lambda(B)D(W)λ(B)d(W)≤d(BW)≤λ(B)D(W).
  • Lemma 3.3 (p. 80): for z1,z2∈Wz_1, z_2 \in Wz1​,z2​∈W, 0<β≤10 < \beta \le 10<β≤1 and γ=∥z1−z2∥/d(W)≥1\gamma = \|z_1 - z_2\|/d(W) \ge 1γ=∥z1​−z2​∥/d(W)≥1,
d(Rβ(z1−z2∥z1−z2∥)W)≥d(W)1+(1−β2)/(β2γ2).d\Big(R_\beta\big(\tfrac{z_1 - z_2}{\|z_1 - z_2\|}\big)W\Big) \ge \frac{d(W)}{\sqrt{1 + (1-\beta^2)/(\beta^2\gamma^2)}} .d(Rβ​(∥z1​−z2​∥z1​−z2​​)W)≥1+(1−β2)/(β2γ2)​d(W)​.
  • Theorem 3.11 (p. 82): for every βn<v<1\sqrt[n]{\beta} < v < 1nβ​<v<1, ε,δ>0\varepsilon, \delta > 0ε,δ>0 and r≥1r \ge 1r≥1 there is kˉ>r\bar k > rkˉ>r with
p(Pˉδ,ε(xkˉ))≥v2α2n−1α2−1.p\big(\bar P_{\delta,\varepsilon}(x_{\bar k})\big) \ge \sqrt{\frac{v^2\sqrt[n]{\alpha^2} - 1}{\alpha^2 - 1}} .p(Pˉδ,ε​(xkˉ​))≥α2−1v2nα2​−1​​.
  • Theorem 3.12 (p. 84): the level set {f=f∞}\{f = f_\infty\}{f=f∞​}, f∞=lim⁡kf(xk)f_\infty = \lim_k f(x_k)f∞​=limk​f(xk​), contains a point x∗x^*x∗ with Gf(x∗)G_f(x^*)Gf​(x∗) linearly dependent.

Significance

Theorem 3.13 is the only convergence theorem the book gives for the r-algorithm. Theorems 3.11 and 3.12 hold for any function of the class KKK, convex or not, and say that iterates of the exact version cannot stall at a point where the local almost-gradients are linearly independent: linear dependence of Gf(x)G_f(x)Gf​(x) is a generalized stationarity condition that includes 0∈conv⁡Gf(x)0 \in \operatorname{conv} G_f(x)0∈convGf​(x). Lemmas 3.2 and 3.3 are statements about widths of convex bodies under linear maps and single dilations, and apply to any analysis of space-dilation methods, including the ellipsoid method.

All four results and the goal are proved in the book, the goal as a corollary without a written proof. None of them is formalized. The formalization adds a machine-checked definition of the class KKK and of the algorithm as a relation on sequences covering every admissible choice of almost-gradients and stepsizes, a verified proof of the book's argument, and a check of the corollary step, which the book leaves to the reader.

Difficulty

The obvious argument for descent methods is that the function value drops by a fixed amount at every step unless the gradient is small. That argument fails here. The r-algorithm can make null steps, with xk+1=xkx_{k+1} = x_kxk+1​=xk​ while BkB_kBk​ and g~k\tilde g_kg~​k​ change, and its steps are measured in a metric that degenerates as the dilations accumulate (det⁡Bk=βkdet⁡B0\det B_k = \beta^k \det B_0detBk​=βkdetB0​). A small step does not certify near-stationarity, and a large accumulated dilation does not certify progress.

The difficulty is to relate the geometry of the transformed almost-gradient sets Bk∗Pˉδ,ε(xk)B_k^*\bar P_{\delta,\varepsilon}(x_k)Bk∗​Pˉδ,ε​(xk​) to the decay forced on BkB_kBk​. This needs width estimates for convex bodies under linear maps and single dilations, which Mathlib does not have. Theorem 3.12 also needs a uniform lower bound, near a compact level set, on the Gram determinants of the piece gradients, and the book's proof of it is only sketched. Theorem 3.13 is stated as a corollary with no proof at all. Deriving it requires showing that the iterates cannot leave the prescribed component of {f(x∗)≤f≤f(x0)}\{f(x^*) \le f \le f(x_0)\}{f(x∗)≤f≤f(x0​)}, and that their accumulation points reduce to x∗x^*x∗.

Formalization scope

  • EnE_nEn​ is EuclideanSpace ℝ (Fin n) with n≥1n \ge 1n≥1; operators are continuous linear maps; Bk∗B_k^*Bk∗​ is the adjoint. KρK_\rhoKρ​ and ppp are valued in [0,+∞][0, +\infty][0,+∞], so Kρ(W)=+∞K_\rho(W) = +\inftyKρ​(W)=+∞ is represented exactly. Widths are sInf/sSup of support values, equal to the book's minima and maxima on nonempty compact sets.
  • A function of class KKK is given with its representation (pieces, open domains, smooth fif_ifi​), and Gf(x)G_f(x)Gf​(x) is the set of gradients of the incident pieces, as on p. 79. Linear dependence of Gf(x)G_f(x)Gf​(x) is the negation of linear independence of that set.
  • A run of the algorithm is a predicate on sequences xk,g~k,Bk,gf(xk),hk+1x_k, \tilde g_k, B_k, g_f(x_k), h_{k+1}xk​,g~​k​,Bk​,gf​(xk​),hk+1​; every theorem holds for every run. Step (3) divides by ∥rk∥\|r_k\|∥rk​∥, so rk≠0r_k \ne 0rk​=0 is part of the run: a run that reaches a point where no admissible choice gives rk≠0r_k \ne 0rk​=0 has no continuation, as in the book. The stepsize hk+1=argmin⁡h_{k+1} = \operatorname{argmin}hk+1​=argmin is one admissible choice, not the definition.
  • The standing assumption (3.50) is a hypothesis of Theorem 3.11 as well as of 3.12 and 3.13, because the book imposes it for the rest of the section on p. 79.
  • In Lemma 3.3, β>0\beta > 0β>0 is added (the bound divides by β2\beta^2β2). "Body" means nonempty interior. An isolated local minimum is a local minimum with a neighbourhood containing no other local minimum.
  • Runs exist, so the hypotheses are not vacuous. For f(t)=∣t1∣+2∣t2∣f(t) = |t_1| + 2|t_2|f(t)=∣t1​∣+2∣t2​∣ (four quadrant pieces), started at the minimizer x0=0x_0 = 0x0​=0 with null steps, one can choose gf(xk+1)=−gf(xk)g_f(x_{k+1}) = -g_f(x_k)gf​(xk+1​)=−gf​(xk​) at every step, and 0∉Gf0 \notin G_f0∈/Gf​ keeps rk≠0r_k \neq 0rk​=0. A formalization under which no infinite run exists would make every theorem vacuous. The run predicate also forbids the degenerate reading hk+1<0h_{k+1} < 0hk+1​<0, under which the monotonicity condition (a) would hold vacuously on an empty segment.
  • Needed infrastructure: widths of compact convex sets under linear maps (via the singular values of BBB), the effect of a rank-one dilation on widths, determinant bounds for products of dilations, and Gram-determinant continuity. The first three apply to any space-dilation method and are welcome as independent lemmas.

Selected references

  • N. Z. Shor, Minimization Methods for Non-Differentiable Functions, Springer Series in Computational Mathematics 3, Springer 1985, §3.7, pp. 77–85. doi:10.1007/978-3-642-82118-9
  • N. Z. Shor, N. G. Zhurbenko, A minimization method using the operation of space dilation in the direction of the difference of two successive gradients, Kibernetika (Kiev), no. 3, 51–59, 1971 (listed in the bibliography of Shor 1985; no online copy known).
  • N. Z. Shor, The analysis of convergence of a gradient type method with space dilation in the direction of the difference of two successive gradients, Kibernetika (Kiev), no. 4, 48–53, 1975 (listed in the bibliography of Shor 1985; no online copy known).
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AnalysisGeometry & Topology·Captain: Tamas Fulop

Moving Sofa ProblemOpen Problem

Motivation

The question of the largest area that can be moved around a corner has been studied since the late 1960s. Leo Moser posed it in 1966, and F. H. Hammersley gave the lower bound π/2+2/π≈2.2074\pi/2+2/\pi\approx2.2074π/2+2/π≈2.2074 and the upper bound 22≈2.8282\sqrt{2}\approx2.82822​≈2.828 in 1968. Joseph Gerver constructed a shape of area approximately 2.21952.21952.2195 in 1992 and described four constants AAA, BBB, φ\varphiφ, θ\thetaθ satisfying four equations, from which the shape is built. Dan Romik rewrote those equations in exact form as equations (1)-(4) in 2018 and reported high-precision values of the constants. Jineon Baek proved in 2024 that Gerver's shape is optimal: no larger shape can be moved around the corner. The proof was autoformalized in Lean 4 by Dean Cureton and AI agents in 2026, as the repository deancureton/MovingSofa, building on Dawid Trela's formalization of Gerver's constants and motion, Jonathan Ho's Brunn-Minkowski development, the Jordan-curve developments of R. Kirov and the TauCeti project, and Google DeepMind's formal-conjectures statement.

Timeline: Moser poses the problem (1966); Hammersley gives the π/2+2/π≈2.2074\pi/2+2/\pi\approx2.2074π/2+2/π≈2.2074 lower bound and the 22≈2.8282\sqrt{2}\approx2.82822​≈2.828 upper bound (1968); Gerver exhibits the 2.21952.21952.2195 shape and its differential equations (1992); Romik gives the exact equations and numerics (2018); Baek proves optimality (2024, arXiv:2411.19826); Cureton et al. complete a Lean 4 proof of optimality, existence and uniqueness of the constants, and movability of Gerver's shape (2026).

Setting

Work in the plane R2\mathbb{R}^2R2. The hallway is (−∞,1]×[0,1]∪[0,1]×(−∞,1](-\infty,1]\times[0,1]\cup[0,1]\times(-\infty,1](−∞,1]×[0,1]∪[0,1]×(−∞,1], the union of its horizontal and vertical sides. A moving sofa is a nonempty closed connected set sss in the horizontal side together with a continuous path mmm of plane isometries indexed by the unit interval, starting at the identity, keeping the image of sss inside the hallway at all times, and ending with the image inside the vertical side. Motions take values in the full isometry group E(2)E(2)E(2); continuity together with m(0)=idm(0)=\mathrm{id}m(0)=id forces the path to lie in the orientation-preserving component. The sofa constant is the supremum, in the extended nonnegative reals, of the areas volume(s)\mathrm{volume}(s)volume(s) over all moving sofas. The supremum is finite, at least 11/511/511/5, and attained.

Gerver's shape is defined from a rotation path. For constants AAA, BBB, φ\varphiφ, θ\thetaθ, let rrr be the piecewise function with breakpoints φ\varphiφ, θ\thetaθ, π/2−θ\pi/2-\thetaπ/2−θ, π/2−φ\pi/2-\varphiπ/2−φ from Romik's Theorem 2, let xxx and yyy be its cosine and sine integrals, and let ppp be the associated translation path. The sofa for those constants is the intersection over angles in [0,π/2][0,\pi/2][0,π/2] of the correspondingly rotated and translated hallways, with the endpoints using the horizontal and vertical sides. The four equations ABphiThetaSpec cut out the constants. They have exactly one solution with 0≤φ≤θ≤π/40\le\varphi\le\theta\le\pi/40≤φ≤θ≤π/4 and 0≤A0\le A0≤A, 0≤B0\le B0≤B. The same Lean development uses the identical notation as the formal statements, so prose and code read as one document.

Formalization targets

Goal: optimality of Gerver's sofa

For every AAA, BBB, φ\varphiφ, θ\thetaθ satisfying ABphiThetaSpec,

sofaConstant=volume(gerversSofaWith(A,B,φ,θ)).\mathrm{sofaConstant} = \mathrm{volume}(\mathrm{gerversSofaWith}(A,B,\varphi,\theta)).sofaConstant=volume(gerversSofaWith(A,B,φ,θ)).

The goal leaves unfixed which solution of the spec is used; by uniqueness all choices give the same shape up to the proved identification, so this is the stable form of Baek's Theorem 1.1. It asserts that the supremum equals the area of Gerver's shape, hence that no moving sofa has larger area and that the supremum is attained.

Supporting targets

∃! (A,B,φ,θ), ABphiThetaSpec(A,B,φ,θ).\exists!\,(A,B,\varphi,\theta),\ \mathrm{ABphiThetaSpec}(A,B,\varphi,\theta).∃!(A,B,φ,θ), ABphiThetaSpec(A,B,φ,θ). ∀ A,B,φ,θ, ABphiThetaSpec(A,B,φ,θ)  ⟹  ∃ m, IsMovingSofa(gerversSofaWith(A,B,φ,θ),m).\forall\,A,B,\varphi,\theta,\ \mathrm{ABphiThetaSpec}(A,B,\varphi,\theta)\implies \exists\,m,\ \mathrm{IsMovingSofa}(\mathrm{gerversSofaWith}(A,B,\varphi,\theta),m).∀A,B,φ,θ, ABphiThetaSpec(A,B,φ,θ)⟹∃m, IsMovingSofa(gerversSofaWith(A,B,φ,θ),m).

The first is Gerver's Theorem 2 in Romik's equation form on the closed domain. The second says every such shape admits a hallway motion. Together they supply the constants and the witness that the supremum is attained. The live mission records a root sketch composing the upper-bound half (every moving sofa is bounded by Gerver's area) with the movability witness into the supremum equality.

Significance

The result itself closes a problem open since 1966. It identifies the maximum area, shows the maximum is attained by an explicit shape, and determines that shape from four equations whose solution is unique. Consequences include the numerical enclosure 11/5≤volume≤∞11/5\le\mathrm{volume}\le\infty11/5≤volume≤∞ proved by interval arithmetic, the finiteness of the supremum, and the reduction of future improvements to the analysis of the functional QQQ on caps. Without it the exact maximum remains unknown.

Formalizing it adds a machine-checked proof that makes no classical area assumption: the Green-type curve-area identity and the Minkowski-type mixed-area facts quoted by the paper are proved, the paper's 11 proof gaps and 33 misprints are repaired, and the numerical certificate is kernel-checked. The hallway, motion, cap, convex-body, and surface-measure infrastructure is reusable for related isoperimetric and kinematic formalizations. Status honesty: the underlying paper proof is complete and has been formalized in the source repository; on this platform the three statements above are open targets awaiting proofs, and the uniqueness of the maximizer up to rigid motion remains open and is not part of this mission.

Difficulty

The obvious argument bounds the area of an arbitrary sofa by the area of a circumscribed cap, but caps need not satisfy the injectivity condition that makes the functional QQQ an upper bound, and QQQ need not be concave on the full space of caps. Maximizing sequences of polygons need not converge to a sofa, and limits need not be connected or attain the supremum. The naive idea of taking a supremum over all connected closed sets and extracting a convergent subsequence fails until compactness of motions, closedness of the moving-sofa predicate, and a balanced maximum with rotation angle π/2\pi/2π/2 are established. Each step fails for general sets and only holds after the polygon approximation and monotonization constructions.

Formalization scope

Lean represents the plane as EuclideanSpace ℝ (Fin 2) with its standard orientation, hallway sides as explicit sets, motions as I → E(2) where E(2) is ℝ² ≃ᵃⁱ[ℝ] ℝ² with the topology induced from continuous maps, and area as MeasureSpace.volume. The supremum is in ℝ≥0∞. Statements target the c5ea003 (Lean v4.30.0) environment, an older supported revision against which the development was verified locally. The spec uses non-strict inequalities, which makes uniqueness stronger than the strict-inequality literature form. The functions rrr, xxx, yyy, ppp take the constants as explicit arguments rather than reading global chosen constants, so the definition bundle stays independent of the existence proof; given uniqueness this implies the source statements. Boundedness and measurability are not assumed; every moving sofa is proved compact in the source development. A submission that drops closedness or connectedness, that allows a discontinuous motion, or that hard-codes the numerical value 2.21952.21952.2195 instead of proving equality with the volume of the defined shape, does not satisfy the statements. Contributions welcome: direct proofs of the three targets, sharper enclosures of the volume, and reusable hallway and motion lemmas. Out of scope: uniqueness up to congruence, the 11/511/511/5 certificate details beyond the stated lower bound, and the 20 unformalized numbered environments listed in the source NOTES.md that none of the three targets depends on.

Selected references

  • Jineon Baek, Optimality of Gerver's Sofa, arXiv:2411.19826, 2024. https://arxiv.org/abs/2411.19826
  • Joseph L. Gerver, On moving a sofa around a corner, Geometriae Dedicata 42 (1992), 267-283.
  • Dan Romik, Differential equations and exact solutions in the moving sofa problem, Experimental Mathematics 27 (2018), 316-330. https://arxiv.org/abs/1606.08111
  • Dean Cureton et al., MovingSofa: Autoformalization of Baek's solution, 2026. https://github.com/deancureton/MovingSofa
  • Google DeepMind, formal-conjectures, FormalConjectures/Wikipedia/MovingSofa.lean at ddfbaf90. https://github.com/google-deepmind/formal-conjectures
  • Dawid Trela, GerverSofaLean v1.1.0. https://github.com/dawidmtrela-dotcom/GerverSofaLean
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Theoretical Computer Science·Captain: Goku

QMA Strong Error Reduction with No Witness-Length IncreaseResearch Paper

Motivation

A QMA verifier receives a quantum witness and checks it with a circuit generated efficiently from the input. An acceptance probability separated by an inverse-polynomial gap is enough to define the class, but applications often need the probability of a wrong answer to be exponentially small. Repeating the verifier on many supplied witness registers achieves this error reduction while allowing the witness to grow. Marriott and Watrous proved the stronger statement that the same error reduction can be obtained without increasing the number of witness qubits Quantum Arthur–Merlin Games, Section 3.

The existing Lean development verifies the copy-based theorem, including soundness for witnesses entangled across the copies, and constructs a uniform circuit family with polynomial resources. This mission asks for the separate witness-preserving theorem. The paper already proves that mathematical statement; the open work here is its formalization in the stated QMA circuit model.

Setting

At each input length nnn, a verifier has m(n)m(n)m(n) witness qubits, a finite work register, a designated output wire, and a quantum circuit. A uniformly generated family has a polynomial-time classical procedure that emits the complete circuit description, including the witness and work-register sizes. On yes-instances, some normalized witness makes the verifier accept with probability at least a(n)a(n)a(n). On no-instances, every normalized witness is accepted with probability at most b(n)b(n)b(n). The thresholds satisfy 0≤b(n)≤a(n)≤10\le b(n)\le a(n)\le10≤b(n)≤a(n)≤1 and a(n)−b(n)≥1/q(n)a(n)-b(n)\ge1/q(n)a(n)−b(n)≥1/q(n) for a polynomial qqq.

The existing formalization represents witnesses as complex amplitude functions on bit strings, requires normalization explicitly, and uses layered circuits over its specified finite gate set. It also represents efficiently available real thresholds by polynomial-time procedures that output dyadic approximations. These are part of the formal statement's interface and must be made visible to users of the mission.

Target

For every polynomial error exponent rrr and every source verifier satisfying the conditions above, construct a uniformly generated, well-formed, polynomial-resource verifier for the same language, with completeness at least 1−2−r(n)1-2^{-r(n)}1−2−r(n) and soundness at most 2−r(n)2^{-r(n)}2−r(n), while keeping the witness count exactly m(n)m(n)m(n) at every input length:

mnew(n)=mold(n).m_{\mathrm{new}}(n)=m_{\mathrm{old}}(n).mnew​(n)=mold​(n).

This is the witness-preserving strong error-reduction result of Marriott and Watrous (Theorem 4). The existing copy-based result corresponds to the weaker QMA class inclusion in Theorem 3 and will be linked as a proved background result. The mission goal must state the witness-count equation explicitly so that a copy-based amplifier cannot satisfy it.

Significance

Witness-preserving amplification lets a QMA protocol demand much stronger reliability without asking the prover for a longer message. That matters whenever witness size is itself a resource being compared or bounded. The copy-based theorem shows that the QMA class is robust under error reduction, but does not establish this fixed-message guarantee.

Formalizing the stronger result would add a reusable account of a verifier that reuses one witness, proves soundness for every normalized input state, and compiles its behavior into an ordinary uniform circuit family. Those components can support later formalizations that reason about repeated quantum verification under a fixed witness budget.

Difficulty

The completed copy-based proof uses three independent verifier blocks in each amplification round and bounds arbitrary entangled witnesses across those blocks. Its circuit resource analysis therefore allows the witness count to grow. A witness-preserving argument cannot use that construction. It must analyze repeated verification on one register and establish exponentially small error without assuming the input witness has a special spectral form. The formal circuit model currently exposes final-output measurements; any additional measurement behavior used in the analysis must be justified in that model and shown implementable by a finite, uniformly generated circuit.

The central audit point is the exact witness-length equation. A theorem that merely returns another polynomial-size witness, or that changes the source verifier's witness definition, is a useful class-level result but does not prove this mission's target.

Formalization scope

The goal is parameterized by input-length-dependent completeness and soundness thresholds with an inverse-polynomial gap, and by a polynomial target exponent. Every witness quantifier is over normalized states. The output verifier must satisfy the same well-formedness and polynomial-resource conditions as the completed copy-based development. The platform statement uses its existing ShiClassQMAU.UniformQMA circuit-family encoding, which includes the witness and ancilla counts separately. A final proof should be kernel checked with only Lean's standard logical axioms and should not assume an amplification transducer or an unproved measurement lemma.

The paper quantifies over the class poly of unary-time constructible functions. This proposal represents the gap denominator and target exponent as literal Polynomial ℕ values, matching the checked copy-based development. It therefore formalizes a polynomial-parameter instance of Theorem 4 rather than the paper's full function-class generality. The threshold functions are supplied by polynomial-time dyadic approximators in place of the paper's informal efficient-computation convention. These interface choices are explicit in the Lean goal and should not be read as a proof of the broader formulation.

The local copy-based proof is complete and audited, but it has not yet been transplanted to Prove2Me. Its publication is preparatory work for this mission, not evidence that the witness-preserving goal is already solved. The proposal should reference the published copy-based endpoint and include only a few substantial milestones, so each item is meaningful to audit.

Selected references

  • C. Marriott and J. Watrous, Quantum Arthur–Merlin Games, Computational Complexity 14 (2005), Section 3, Theorems 3 and 4. Paper.
  • A. Kitaev, A. Shen, and M. Vyalyi, Classical and Quantum Computation, Graduate Studies in Mathematics 47, American Mathematical Society (2002), Section 14.2, cited by Marriott and Watrous for the copy-based amplification proof.
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Number Theory·Captain: Lucas

Brocard's Conjecture: Four Primes Between Consecutive Prime SquaresOpen Problem

Motivation

For n≥1n \ge 1n≥1 let pnp_npn​ denote the nnn-th prime. Brocard's conjecture, named after Henri Brocard, asserts that for every n≥2n \ge 2n≥2 there are at least four primes strictly between pn2p_n^2pn2​ and pn+12p_{n+1}^2pn+12​ (Wikipedia). It belongs to the family of "primes between consecutive squares" problems together with Legendre's conjecture, and it is a concrete, elementary-looking question about short-interval prime distribution that remains open.

Timeline

  • Early 20th century — Brocard states the conjecture.
  • 2023 — L. A. Ferreira (arXiv:2307.08725) proves that the conjecture holds for all sufficiently large nnn.

Setting

Primes are listed in increasing order. In the Lean development the list is 0-indexed: Nat.nth Nat.Prime k is the kkk-th prime counting from 000, so nth 0 = 2, nth 1 = 3, nth 2 = 5, and so on. For an index nnn write prev=\mathrm{prev} = prev= n.nth Nat.Prime and next=\mathrm{next} = next= (n+1).nth Nat.Prime, two consecutive primes. The quantity of interest is

#{ q prime:prev2<q<next2 }.\#\{\, q \text{ prime} : \mathrm{prev}^2 < q < \mathrm{next}^2 \,\}.#{q prime:prev2<q<next2}.

Target

Milestone (Ferreira): for all sufficiently large indices nnn,

4≤#{ q prime:prev2<q<next2 }.4 \le \#\{\, q \text{ prime} : \mathrm{prev}^2 < q < \mathrm{next}^2 \,\}.4≤#{q prime:prev2<q<next2}.

Goal (Brocard's conjecture): the same inequality for every 0-indexed n≥1n \ge 1n≥1, i.e. for every pair of consecutive primes starting from (3,5)(3,5)(3,5).

Significance

A proof of the goal settles Brocard's conjecture outright. Given Ferreira's asymptotic result, the remaining work splits into making the threshold effective and closing the finite range below it, both of which would be new formal content; the milestone itself (formalizing Ferreira's analytic argument) is a substantial analytic-number-theory formalization project.

Difficulty

Unconditional results on primes in short intervals [x,x+xθ][x, x + x^{\theta}][x,x+xθ] only reach exponents θ\thetaθ well above 1/21/21/2, while the interval (pn2,pn+12)(p_n^2, p_{n+1}^2)(pn2​,pn+12​) has length about 2pngn2 p_n g_n2pn​gn​ where gn=pn+1−png_n = p_{n+1} - p_ngn​=pn+1​−pn​ can be small (e.g. twin primes), i.e. length on the order of the square root of its endpoint. Standard short-interval theorems therefore do not apply uniformly, and Legendre's conjecture — which would only give two primes here — is itself open.

Formalization scope

Everything is stated with Mathlib's Nat.nth Nat.Prime, Finset.Ioo (open interval, endpoints excluded) and Finset.filter Nat.Prime, followed by Finset.card. The hypothesis 1 ≤ n in the goal is the 0-indexed form of the source's "n≥2n \ge 2n≥2"; it is necessary, since for index 000 (primes 2,32, 32,3) the interval (4,9)(4, 9)(4,9) contains only the two primes 5,75, 75,7. The milestone uses Filter.atTop ("for all sufficiently large nnn"), with no explicit threshold. No custom definitions are required.

Selected references

  • Brocard's conjecture, Wikipedia. https://en.wikipedia.org/wiki/Brocard%27s_conjecture
  • L. A. Ferreira, Real exponential sums over primes and prime gaps, arXiv:2307.08725 (2023). https://arxiv.org/abs/2307.08725
  • Statement adapted from the Formal Conjectures project (Apache-2.0), file BrocardConjecture.lean.
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Numerical AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Euler Approximations with Varying Coefficients II: Strong Order 1/2 in Lp for Superlinearly Growing Diffusion CoefficientsResearch Paper

Motivation

Stochastic differential equations with superlinearly growing coefficients appear throughout applied probability: population models with cubic damping, Langevin dynamics with polynomial potentials, and stochastic volatility models such as the 3/2-model used for pricing VIX options, whose diffusion coefficient grows like ∣x∣3/2|x|^{3/2}∣x∣3/2. For such equations the classical explicit Euler–Maruyama method fails: Hutzenthaler, Jentzen and Kloeden (2011) proved that its ppp-th moments diverge whenever a coefficient grows superlinearly, so it cannot converge in Lp\mathcal L^pLp. Implicit methods converge (Higham–Mao–Stuart 2002) but cost a nonlinear solve per step.

The tamed Euler schemes are the explicit response.

  • Hutzenthaler, Jentzen and Kloeden (2012) tamed a superlinear drift and proved strong order 1/21/21/2 for globally Lipschitz diffusion coefficients.
  • Sabanis (2013) gave a simpler proof for a family of tamed drifts.
  • Hutzenthaler and Jentzen (2015) treated superlinear diffusion coefficients, obtaining Lp\mathcal L^pLp-convergence without a rate and only for small ppp.
  • Sabanis (2016), the source of this mission, tames drift and diffusion together and proves the optimal strong rate 1/21/21/2 in Lp\mathcal L^pLp under a one-sided (monotonicity) condition and polynomial growth. For the 3/2-model with p1=3.5p_1=3.5p1​=3.5, p0=6p_0=6p0​=6 this gives L2\mathcal L^2L2-convergence with order 1/21/21/2, which earlier results did not cover (p. 2).

This mission is the second of three on the paper. Mission I formalizes Lp\mathcal L^pLp-convergence without a rate (Theorem 1), mission III the uniform-in-time rate (Theorem 3).

Setting

Fix a filtered probability space (Ω,{Ft}t≥0,F,P)(\Omega,\{\mathcal F_t\}_{t\ge0},\mathcal F,P)(Ω,{Ft​}t≥0​,F,P) with right-continuous filtration, a horizon T>0T>0T>0, dimensions d,d1d,d_1d,d1​, and a d1d_1d1​-dimensional Wiener martingale WWW: a standard Brownian motion adapted to {Ft}\{\mathcal F_t\}{Ft​} whose future increments are independent of Ft\mathcal F_tFt​. The coefficients are Borel maps b:[0,∞)×Rd→Rdb:[0,\infty)\times\mathbb R^d\to\mathbb R^db:[0,∞)×Rd→Rd and σ:[0,∞)×Rd→Rd×d1\sigma:[0,\infty)\times\mathbb R^d\to\mathbb R^{d\times d_1}σ:[0,∞)×Rd→Rd×d1​; ∣x∣|x|∣x∣ is the Euclidean norm, ∣A∣|A|∣A∣ the Hilbert–Schmidt norm, xyxyxy the scalar product. The SDE is

dX(t)=b(t,X(t)) dt+σ(t,X(t)) dW(t),t∈[0,T],(2.1)dX(t)=b(t,X(t))\,dt+\sigma(t,X(t))\,dW(t),\qquad t\in[0,T],\qquad(2.1)dX(t)=b(t,X(t))dt+σ(t,X(t))dW(t),t∈[0,T],(2.1)

with an F0\mathcal F_0F0​-measurable initial value X(0)=ξX(0)=\xiX(0)=ξ. For n≥1n\ge1n≥1 let κn(t)=⌊nt⌋/n\kappa_n(t)=\lfloor nt\rfloor/nκn​(t)=⌊nt⌋/n and consider the scheme

dXn(t)=bn(t,Xn(κn(t))) dt+σn(t,Xn(κn(t))) dW(t),Xn(0)=ξ,(2.2)dX_n(t)=b_n(t,X_n(\kappa_n(t)))\,dt+\sigma_n(t,X_n(\kappa_n(t)))\,dW(t),\qquad X_n(0)=\xi,\qquad(2.2)dXn​(t)=bn​(t,Xn​(κn​(t)))dt+σn​(t,Xn​(κn​(t)))dW(t),Xn​(0)=ξ,(2.2)

whose coefficients are frozen at the last grid point, so that XnX_nXn​ is computable step by step. The tamed coefficients of Model 2 are

bn(t,x)=b(t,x)1+n−α∣x∣l,σn(t,x)=σ(t,x)1+n−α∣x∣l.(2.11)–(2.12)b_n(t,x)=\frac{b(t,x)}{1+n^{-\alpha}|x|^l},\qquad \sigma_n(t,x)=\frac{\sigma(t,x)}{1+n^{-\alpha}|x|^l}.\qquad(2.11)\text{–}(2.12)bn​(t,x)=1+n−α∣x∣lb(t,x)​,σn​(t,x)=1+n−α∣x∣lσ(t,x)​.(2.11)–(2.12)

The hypotheses, with constants p0,p1≥2p_0,p_1\ge2p0​,p1​≥2:

  • A-2: bbb is bounded on balls, uniformly in t∈[0,T]t\in[0,T]t∈[0,T].
  • A-4 (coercivity): 2xb(t,x)+(p0−1)∣σ(t,x)∣2≤K(1+∣x∣2)2xb(t,x)+(p_0-1)|\sigma(t,x)|^2\le K(1+|x|^2)2xb(t,x)+(p0​−1)∣σ(t,x)∣2≤K(1+∣x∣2).
  • A-5: E∣X(0)∣p0<∞\mathbb E|X(0)|^{p_0}<\inftyE∣X(0)∣p0​<∞.
  • A-6 (global monotonicity, polynomial growth): for positive lll and LLL, 2(x−y)(b(t,x)−b(t,y))+(p1−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣22(x-y)(b(t,x)-b(t,y))+(p_1-1)|\sigma(t,x)-\sigma(t,y)|^2\le L|x-y|^22(x−y)(b(t,x)−b(t,y))+(p1​−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣2 and ∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣|b(t,x)-b(t,y)|\le L(1+|x|^l+|y|^l)|x-y|∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣.
  • The p\mathfrak pp-condition: the scheme uses (2.11)–(2.12) with α=1/2\alpha=1/2α=1/2, l≤p0−24l\le\frac{p_0-2}{4}l≤4p0​−2​, and 0<p<p10<p<p_10<p<p1​, p≤p02l+1p\le\frac{p_0}{2l+1}p≤2l+1p0​​.
  • B-2 and B-3 (for the milestones): ∣bn∣≤min⁡(Cnα(1+∣x∣),∣b∣)|b_n|\le\min(Cn^\alpha(1+|x|),|b|)∣bn​∣≤min(Cnα(1+∣x∣),∣b∣), ∣σn∣2≤min⁡(Cnα(1+∣x∣2),∣σ∣2)|\sigma_n|^2\le\min(Cn^\alpha(1+|x|^2),|\sigma|^2)∣σn​∣2≤min(Cnα(1+∣x∣2),∣σ∣2), and A-4 for bn,σnb_n,\sigma_nbn​,σn​ with a constant uniform in nnn.

Formalization targets

Goal: Theorem 2 (p. 6)

Under A-2, A-4–A-6, the p\mathfrak pp-condition and p1>2p_1>2p1​>2, there is a constant CCC independent of nnn with

sup⁡0≤t≤TE[∣X(t)−Xn(t)∣p]≤Cn−p/2(n≥1).(2.13)\sup_{0\le t\le T}\mathbb E\big[|X(t)-X_n(t)|^p\big]\le Cn^{-p/2}\qquad(n\ge1).\qquad(2.13)0≤t≤Tsup​E[∣X(t)−Xn​(t)∣p]≤Cn−p/2(n≥1).(2.13)

The constant is existential and may depend on all data except nnn.

Milestones

  1. Lemma 2 (p. 8): sup⁡tE∣X(t)∣p\sup_t\mathbb E|X(t)|^psupt​E∣X(t)∣p and sup⁡n≥1sup⁡tE∣Xn(t)∣p\sup_{n\ge1}\sup_t\mathbb E|X_n(t)|^psupn≥1​supt​E∣Xn​(t)∣p are finite for 0<p≤p00<p\le p_00<p≤p0​, under A-1–A-5, B-2, B-3.
  2. Lemma 3 (p. 15): for Model 2, E∫0T∣b(s,Xn(κn(s)))−bn(s,Xn(κn(s)))∣p ds≤Cn−αp\mathbb E\int_0^T|b(s,X_n(\kappa_n(s)))-b_n(s,X_n(\kappa_n(s)))|^p\,ds\le Cn^{-\alpha p}E∫0T​∣b(s,Xn​(κn​(s)))−bn​(s,Xn​(κn​(s)))∣pds≤Cn−αp, and the same for σ\sigmaσ.
  3. Lemma 4 (p. 16): sup⁡tE∣Xn(t)−Xn(κn(t))∣p≤Cn−p/2\sup_t\mathbb E|X_n(t)-X_n(\kappa_n(t))|^p\le Cn^{-p/2}supt​E∣Xn​(t)−Xn​(κn​(t))∣p≤Cn−p/2.

Significance

Theorem 2 shows that an explicit scheme costing one coefficient evaluation per step attains the same strong order as the classical Euler method under global Lipschitz conditions. It does so for drift and diffusion coefficients that grow polynomially, and for moment orders ppp that are small relative to p0p_0p0​ and p1p_1p1​. Strong Lp\mathcal L^pLp rates are what multilevel Monte Carlo needs: the variance of level corrections is controlled by the L2\mathcal L^2L2 rate. When lll could be taken to be 000 the statement specializes to the classical globally Lipschitz rate (Remark 6).

The result is proved on paper; it has no machine-checked proof. Stochastic integrals are not in Mathlib; this mission uses the Brownian Itô-integral relation published by the Ethier–Kurtz series on the platform. A formal proof would give the first verified strong convergence rate for any Euler-type scheme. Along the way it produces reusable moment bounds for tamed schemes and the LpL^pLp control of one-step increments.

Difficulty

The obvious argument applies Itô's formula to ∣X−Xn∣p|X-X_n|^p∣X−Xn​∣p and closes a Gronwall inequality. Two steps of it fail without taming. First, the error splits into the monotone part, handled by A-6, and cross terms such as ∣Xn(s)−Xn(κn(s))∣p|X_n(s)-X_n(\kappa_n(s))|^p∣Xn​(s)−Xn​(κn​(s))∣p multiplied by (1+∣Xn∣2l)p/2(1+|X_n|^{2l})^{p/2}(1+∣Xn​∣2l)p/2; they are controlled only through moments of XnX_nXn​ of order well above ppp that are uniform in nnn, which the untamed scheme lacks. Second, the taming itself introduces an error b−bnb-b_nb−bn​ that must be shown to be O(n−1/2)O(n^{-1/2})O(n−1/2) in Lp\mathcal L^pLp and not merely o(1)o(1)o(1). The exponents in the p\mathfrak pp-condition are exactly what the Hölder splittings of these two terms require.

Formalization scope

  • Processes. Solutions are hypotheses, not constructed: XXX solves (2.1) and each XnX_nXn​ solves (2.2), on one probability space, with one WWW and one ξ\xiξ, on [0,T][0,T][0,T] only. An Itô process is a measurable process adapted to the null-set completion of the filtration, with continuous paths on [0,T][0,T][0,T], and a.s. for all t≤Tt\le Tt≤T simultaneously X(t)=ξ+∫0tB ds+∫0tS dWX(t)=\xi+\int_0^t B\,ds+\int_0^t S\,dWX(t)=ξ+∫0t​Bds+∫0t​SdW. The stochastic integral is the platform relation EthierKurtz_HasBrownianItoIntegral, with the integrand cut off after TTT.
  • Expectations and suprema are computed in [0,∞][0,\infty][0,∞] (lower Lebesgue integrals), so no junk value of a non-integrable Bochner integral or of an unbounded real supremum enters. Rates are stated as ≤Cn−p/2\le Cn^{-p/2}≤Cn−p/2 for every n≥1n\ge1n≥1, with CCC real and quantified after all data.
  • Added hypotheses, disclosed. Theorem 2 carries p1>2p_1>2p1​>2: the printed proof covers 2≤p<p12\le p<p_12≤p<p1​ and reduces p<2p<2p<2 to p=2p=2p=2, which the p\mathfrak pp-condition admits exactly when p1>2p_1>2p1​>2. Lemma 4 carries B-3, which its proof uses through Lemma 2. Lemma 2 drops the stated dependence of CCC on (p,T,K,E∣X(0)∣p)(p,T,K,\mathbb E|X(0)|^p)(p,T,K,E∣X(0)∣p) and keeps only its finiteness uniformly in nnn.
  • Ruling out trivialization. The hypotheses are satisfiable, e.g. by b=σ=0b=\sigma=0b=σ=0 with constant solutions and p0=6p_0=6p0​=6, p1=3p_1=3p1​=3, l=1l=1l=1, p=2p=2p=2. The rate is a bound for every n≥1n\ge1n≥1, not an eventual or o(1)o(1)o(1) statement. A proof that uses a constant depending on nnn, or treats only X≡XnX\equiv X_nX≡Xn​, does not prove the goal.
  • Infrastructure needed: Itô's formula for ∣x∣p|x|^p∣x∣p against the platform's Itô integral, the Burkholder–Davis–Gundy inequality (or its Lp\mathcal L^pLp moment form), the zero-expectation property of Itô integrals of square-integrable integrands, and Gronwall's lemma in integral form. These are reusable far beyond this mission, and contributions of any of them are welcome.

Selected references

  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2016. https://arxiv.org/abs/1308.1796 (v4)
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong and weak divergence in finite time of Euler's method for stochastic differential equations with non-globally Lipschitz continuous coefficients, Proc. R. Soc. A 467, 2011. https://doi.org/10.1098/rspa.2010.0348
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with non-globally Lipschitz continuous coefficients, Ann. Appl. Probab. 22, 2012. https://mathscinet.ams.org/mathscinet-getitem?mr=MR2985171
  • M. Hutzenthaler, A. Jentzen, Numerical approximations of stochastic differential equations with non-globally Lipschitz continuous coefficients, Mem. Amer. Math. Soc. 236(1112), 2015. https://doi.org/10.1090/memo/1112
  • S. Sabanis, A note on tamed Euler approximations, Electron. Commun. Probab. 18, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3070913
  • D. J. Higham, X. Mao, A. M. Stuart, Strong convergence of Euler-type methods for nonlinear stochastic differential equations, SIAM J. Numer. Anal. 40, 2002. https://mathscinet.ams.org/mathscinet-getitem?mr=MR1949404
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Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks II: Exponential Decay under Delayed Internal DampingResearch Paper

Motivation

Feedback laws that damp vibrations in elastic structures are implemented by sensors and actuators, and a physical loop always reacts with some time delay τ>0\tau>0τ>0: the damping force at time ttt is computed from the velocity measured at time t−τt-\taut−τ. Datko, Lagnese and Polis showed in 1986 that an arbitrarily small delay in a boundary feedback can destroy the stability of a one-dimensional wave equation (Datko–Lagnese–Polis, SIAM J. Control Optim. 24 (1986)), and Datko showed that such fragility is common to a broad class of feedback-stabilized hyperbolic systems (Datko, SIAM J. Control Optim. 26 (1988)). Delay-robustness is therefore a genuine question for every stabilizing feedback, not a technicality.

Nicaise and Pignotti (SIAM J. Control Optim. 45 (2006) 1561–1585) identified a simple sufficient condition in several space dimensions: if the feedback contains an undelayed velocity term with gain μ1\mu_1μ1​ and a delayed one with gain μ2\mu_2μ2​, and μ2<μ1\mu_2<\mu_1μ2​<μ1​, the energy still decays exponentially; if μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​, instabilities appear for some delays. This mission formalizes the stability half for internal (distributed) damping, localized near the Neumann part of the boundary.

Timeline.

  • 1986: Datko, Lagnese, Polis — small delays destabilize a boundary-damped 1D wave equation.
  • 1988: Datko — many feedback-stabilized hyperbolic systems are not robust with respect to small delays.
  • 1990: Zuazua — exponential decay for the semilinear wave equation with locally distributed damping, without delay (Comm. PDE 15 (1990)); Liu (1997) treats locally distributed damping for general conservative systems (SIAM J. Control Optim. 35 (1997)).
  • 2006: Nicaise, Pignotti — exponential decay with a delayed boundary or internal feedback under μ2<μ1\mu_2<\mu_1μ2​<μ1​ (Theorems 1.1 and 1.3), and instability examples when μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​ (Theorems 1.2 and 1.4).

Setting

Let Ω⊂Rn\Omega\subset\mathbb{R}^nΩ⊂Rn, n≥1n\ge1n≥1, be a bounded open set with boundary Γ\GammaΓ of class C2C^2C2, split as Γ=ΓD∪ΓN\Gamma=\Gamma_D\cup\Gamma_NΓ=ΓD​∪ΓN​ with ΓD‾∩ΓN‾=∅\overline{\Gamma_D}\cap\overline{\Gamma_N}=\emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D\neq\emptysetΓD​=∅. Write ν\nuν for the outer unit normal, dΓd\GammadΓ for the surface measure, ut,uttu_t,u_{tt}ut​,utt​ for time derivatives and Δ\DeltaΔ for the Laplacian in xxx.

Geometric hypothesis (1.6)–(1.7): there are a C2C^2C2 function vvv and α>0\alpha>0α>0 with ⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2\langle D^2v(x)\xi,\xi\rangle\ge2\alpha|\xi|^2⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2 for all x∈Ω‾x\in\overline\Omegax∈Ω, ξ∈Rn\xi\in\mathbb{R}^nξ∈Rn, and ∇v(x)⋅ν(x)≤0\nabla v(x)\cdot\nu(x)\le0∇v(x)⋅ν(x)≤0 on ΓD\Gamma_DΓD​.

Damping coefficient. ω⊂Ω\omega\subset\Omegaω⊂Ω is an open neighbourhood of ΓN\Gamma_NΓN​ (in Ω\OmegaΩ), and a∈L∞(Ω)a\in L^\infty(\Omega)a∈L∞(Ω) satisfies

a(x)≥0 a.e. in Ω(1.17),a(x)>a0>0 a.e. in ω(1.18).a(x)\ge0\ \text{a.e. in }\Omega\quad(1.17),\qquad a(x)>a_0>0\ \text{a.e. in }\omega\quad(1.18).a(x)≥0 a.e. in Ω(1.17),a(x)>a0​>0 a.e. in ω(1.18).

The system (1.12)–(1.16): for gains μ1,μ2>0\mu_1,\mu_2>0μ1​,μ2​>0 and delay τ>0\tau>0τ>0,

utt(x,t)−Δu(x,t)+a(x)[μ1ut(x,t)+μ2ut(x,t−τ)]=0in Ω×(0,∞),u_{tt}(x,t)-\Delta u(x,t)+a(x)\big[\mu_1u_t(x,t)+\mu_2u_t(x,t-\tau)\big]=0\quad\text{in }\Omega\times(0,\infty),utt​(x,t)−Δu(x,t)+a(x)[μ1​ut​(x,t)+μ2​ut​(x,t−τ)]=0in Ω×(0,∞),

with u=0u=0u=0 on ΓD\Gamma_DΓD​, ∂u/∂ν=0\partial u/\partial\nu=0∂u/∂ν=0 on ΓN\Gamma_NΓN​, initial data u(⋅,0)=u0u(\cdot,0)=u_0u(⋅,0)=u0​, ut(⋅,0)=u1u_t(\cdot,0)=u_1ut​(⋅,0)=u1​, and history ut(x,t−τ)=g0(x,t−τ)u_t(x,t-\tau)=g_0(x,t-\tau)ut​(x,t−τ)=g0​(x,t−τ) for t∈(0,τ)t\in(0,\tau)t∈(0,τ).

The energy. Assume μ2<μ1\mu_2<\mu_1μ2​<μ1​ (1.8) and fix ξ\xiξ with τμ2<ξ<τ(2μ1−μ2)\tau\mu_2<\xi<\tau(2\mu_1-\mu_2)τμ2​<ξ<τ(2μ1​−μ2​) (1.10). Then

F(t)=12∫Ω{ut2(x,t)+∣∇u(x,t)∣2}dx+ξ2∫Ωa(x)∫01ut2(x,t−τρ) dρ dx(1.19).\mathcal F(t)=\frac12\int_\Omega\big\{u_t^2(x,t)+|\nabla u(x,t)|^2\big\}dx+\frac\xi2\int_\Omega a(x)\int_0^1u_t^2(x,t-\tau\rho)\,d\rho\,dx\qquad(1.19).F(t)=21​∫Ω​{ut2​(x,t)+∣∇u(x,t)∣2}dx+2ξ​∫Ω​a(x)∫01​ut2​(x,t−τρ)dρdx(1.19).

The first summand is the standard energy E(t)\mathcal E(t)E(t); the second accounts for the velocity history on the delay window.

Formalization targets

Goal: Theorem 1.3

There exist C1,C2>0C_1,C_2>0C1​,C2​>0, depending on the data but not on the solution, such that every solution satisfies

F(t)≤C1 F(0) e−C2t∀t≥0.\mathcal F(t)\le C_1\,\mathcal F(0)\,e^{-C_2t}\qquad\forall t\ge0.F(t)≤C1​F(0)e−C2​t∀t≥0.

The constants are left existential, as in the paper, so no later sharpening of rates invalidates the goal.

Milestones (in the order of the proof)

  1. (4.4) The energy identity
F′(t)=−μ1 ⁣∫Ωaut2(t)−μ2 ⁣∫Ωaut(t)ut(t−τ)+ξτ−12 ⁣∫Ωaut2(t)−ξτ−12 ⁣∫Ωaut2(t−τ).\mathcal F'(t)=-\mu_1\!\int_\Omega a u_t^2(t)-\mu_2\!\int_\Omega a u_t(t)u_t(t-\tau)+\frac{\xi\tau^{-1}}2\!\int_\Omega a u_t^2(t)-\frac{\xi\tau^{-1}}2\!\int_\Omega a u_t^2(t-\tau).F′(t)=−μ1​∫Ω​aut2​(t)−μ2​∫Ω​aut​(t)ut​(t−τ)+2ξτ−1​∫Ω​aut2​(t)−2ξτ−1​∫Ω​aut2​(t−τ).
  1. Proposition 4.1 F\mathcal FF is nonincreasing and F′(t)≤−C∫Ωa{ut2(t)+ut2(t−τ)}dx\mathcal F'(t)\le-C\int_\Omega a\{u_t^2(t)+u_t^2(t-\tau)\}dxF′(t)≤−C∫Ω​a{ut2​(t)+ut2​(t−τ)}dx with C>0C>0C>0.
  2. Proposition 4.2 Observability for the undamped mixed problem: for TTT larger than some T0T_0T0​, Ew(0)≤C1∫0T∫ωwt2 dx dt\mathcal E_w(0)\le C_1\int_0^T\int_\omega w_t^2\,dx\,dtEw​(0)≤C1​∫0T​∫ω​wt2​dxdt.
  3. Proposition 4.3 Observability for the delayed system: for TTT larger than some T‾\overline TT, F(0)≤C0∫0T∫Ωa{ut2(t)+ut2(t−τ)}dx dt\mathcal F(0)\le C_0\int_0^T\int_\Omega a\{u_t^2(t)+u_t^2(t-\tau)\}dx\,dtF(0)≤C0​∫0T​∫Ω​a{ut2​(t)+ut2​(t−τ)}dxdt.
  4. Contraction step (p. 1579): some T>0T>0T>0 and C~∈[0,1)\widetilde C\in[0,1)C∈[0,1) with F(T)≤C~ F(0)\mathcal F(T)\le\widetilde C\,\mathcal F(0)F(T)≤CF(0) for every solution.

Significance

The result. Theorem 1.3 shows that a localized viscous damping acting only near the Neumann boundary keeps its exponential stabilizing effect when part of the feedback is delayed, provided the delayed gain is dominated by the undelayed one. Together with Theorem 1.4 of the same paper (instability for μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​ and suitable delays) it gives a sharp threshold in terms of the gains. The energy F\mathcal FF with its history term became the standard Lyapunov functional for delayed wave and plate equations in the literature that followed.

Formalizing it. The theorem is proved in the paper; no machine-checked proof of it, or of any exponential decay result for a multidimensional wave equation, is known to exist. A complete development would produce reusable Lean infrastructure: energy identities for the wave equation on C2C^2C2 domains via the divergence theorem, the delay-energy calculus, and an observability inequality for the wave equation with mixed boundary conditions. Each milestone has value on its own; Proposition 4.2 in particular is a classical control-theoretic result.

Difficulty

The energy estimates (milestones 1 and 2) are calculus once the divergence theorem is available. The central difficulty is observability. Energy dissipation alone gives only F\mathcal FF nonincreasing; exponential decay needs the energy at time 000 to be controlled by the energy dissipated on [0,T][0,T][0,T] (Proposition 4.3), and that needs the conservative wave equation to be observable from ω\omegaω (Proposition 4.2). The observability inequality does not follow from energy identities: the paper relies on Carleman estimates of Lasiecka–Triggiani–Yao (1999) and a compactness–uniqueness argument, neither of which is available in Mathlib. The obvious attempt, a multiplier identity with ∇v⋅∇u\nabla v\cdot\nabla u∇v⋅∇u alone, leaves boundary terms on ΓN\Gamma_NΓN​ that cannot be absorbed without a localization near ΓN\Gamma_NΓN​ and a lower-order compactness step.

Formalization scope

  • Points are EuclideanSpace ℝ (Fin n) with 1 ≤ n; solutions are real valued.
  • The C2C^2C2 boundary is given by a global C2C^2C2 defining function ψ\psiψ with Ω={ψ<0}\Omega=\{\psi<0\}Ω={ψ<0}, ∂Ω={ψ=0}\partial\Omega=\{\psi=0\}∂Ω={ψ=0}, ∇ψ≠0\nabla\psi\ne0∇ψ=0 on ∂Ω\partial\Omega∂Ω; ν=∇ψ/∣∇ψ∣\nu=\nabla\psi/|\nabla\psi|ν=∇ψ/∣∇ψ∣.
  • The surface measure dΓd\GammadΓ is a finite measure carried by ∂Ω\partial\Omega∂Ω for which the Gauss–Green formula holds for every C1C^1C1 vector field; this determines it uniquely. It is not Mathlib's unnormalized Hausdorff measure.
  • Solutions are classical: uuu is C2C^2C2 on Rn×R\mathbb{R}^n\times\mathbb{R}Rn×R, the equation holds for every t>0t>0t>0 and almost every x∈Ωx\in\Omegax∈Ω (because aaa is only L∞L^\inftyL∞), and the initial data and history are the values of uuu and utu_tut​ at t≤0t\le0t≤0. This is a subclass of the paper's solutions, so the formal theorems are consequences of the paper's.
  • aaa is measurable and essentially bounded on Ω\OmegaΩ; (1.17) and (1.18) are almost-everywhere conditions. "Open neighbourhood of ΓN\Gamma_NΓN​" means ω⊇O∩Ω\omega\supseteq O\cap\Omegaω⊇O∩Ω for some open O⊇ΓNO\supseteq\Gamma_NO⊇ΓN​ (a subset of Ω\OmegaΩ cannot contain ΓN\Gamma_NΓN​ itself).
  • Added hypothesis (Propositions 4.2, 4.3, the contraction step and Theorem 1.3): the closure of every connected component of Ω\OmegaΩ meets ΓD\Gamma_DΓD​; this holds whenever Ω\OmegaΩ is connected. The proof of Proposition 4.2 uses Poincaré's inequality for functions vanishing on ΓD\Gamma_DΓD​, and its compactness–uniqueness step concludes that a harmonic function vanishing on ΓD\Gamma_DΓD​ with zero normal derivative on ΓN\Gamma_NΓN​ is zero; both need this condition.
  • "Decreasing" in Proposition 4.1 is read as nonincreasing; its constant C>0C>0C>0 is existential, chosen before the solution.
  • Printed slips on p. 1575: the last line of (4.3) integrates with dΓd\GammadΓ where dxdxdx is meant, and its first line repeats uρ(x,t−τ)u_\rho(x,t-\tau)uρ​(x,t−τ) for uρ(x,t−τρ)u_\rho(x,t-\tau\rho)uρ​(x,t−τρ). Neither affects any formal statement; (4.4) itself is correct.
  • A formalization in which the aaa-weighted integrals are Lean's junk value 000 (non-measurable aaa), in which ω\omegaω is required to contain ΓN\Gamma_NΓN​ (unsatisfiable), or in which the surface measure is arbitrary, would trivialize or falsify the targets; all three are excluded by the definitions.

Needed infrastructure: the divergence theorem on C2C^2C2 domains (assumed here as a structure field), differentiation under the integral sign for the energies, Carleman estimates or another route to observability for the mixed wave problem, and a compactness argument (Rellich). Contributions of any of these as standalone lemmas are welcome.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5):1561–1585, 2006. https://doi.org/10.1137/060648891
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24:152–156, 1986. https://doi.org/10.1137/0324007
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26:697–713, 1988. https://doi.org/10.1137/0326040
  • E. Zuazua, Exponential decay for the semilinear wave equation with locally distributed damping, Comm. Partial Differential Equations 15:205–235, 1990. https://doi.org/10.1080/03605309908820684
  • K. Liu, Locally distributed control and damping for the conservative systems, SIAM J. Control Optim. 35:1574–1590, 1997. https://doi.org/10.1137/S0363012995284928
  • I. Lasiecka, R. Triggiani, P. F. Yao, Inverse/observability estimates for second-order hyperbolic equations with variable coefficients, J. Math. Anal. Appl. 235:13–57, 1999 (reference [14] of the paper; the Carleman estimates used in Proposition 4.2). https://doi.org/10.1006/jmaa.1999.6348
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AnalysisFunctional AnalysisMathematical Physics+1·Captain: mikedeng1

Mathematical Methods in Quantum Mechanics XIV: Wave Operators and Cook's CriterionTextbook

Motivation

In a scattering experiment a particle arrives from far away, interacts with a target, and leaves again. Far from the target the forces are negligible, so long before and long after the collision the particle should move like a free particle. Scattering theory makes this precise by comparing two quantum dynamics: the free evolution e−itH0\mathrm e^{-\mathrm itH_0}e−itH0​ generated by the kinetic energy H0=−ΔH_0 = -\DeltaH0​=−Δ, and the full evolution e−itH\mathrm e^{-\mathrm itH}e−itH generated by H=H0+VH = H_0 + VH=H0​+V. The objects that compare them are the wave operators (Møller operators) Ω±\Omega_\pmΩ±​, introduced by Møller (1945) and put on a rigorous footing by Jauch (1958) and Kato. Cook (1957) gave the first practical criterion for their existence. Kuroda, Birman, Agmon, Enß and others later developed the theory up to asymptotic completeness for short-range potentials.

This mission formalizes the abstract part of Chapter 12 of Teschl's Mathematical Methods in Quantum Mechanics (AMS GSM 99, 2009): the definition and basic structure of the wave operators, Cook's criterion, and the existence of the wave operators for a square-integrable potential in three dimensions.

Setting

Let H\mathfrak HH be a complex Hilbert space. An operator AAA is a linear map on a subspace D(A)\mathfrak D(A)D(A), its domain; AAA is self-adjoint if D(A)\mathfrak D(A)D(A) is dense and A=A∗A = A^*A=A∗. A projection-valued measure PPP assigns to each Borel set Ω⊆R\Omega \subseteq \mathbb RΩ⊆R an orthogonal projection P(Ω)P(\Omega)P(Ω), with P(R)=IP(\mathbb R) = \mathbb IP(R)=I and P(⋃nΩn)ψ=∑nP(Ωn)ψP(\bigcup_n\Omega_n)\psi = \sum_n P(\Omega_n)\psiP(⋃n​Ωn​)ψ=∑n​P(Ωn​)ψ for disjoint Ωn\Omega_nΩn​. The spectral measure of ψ\psiψ is μψ(Ω)=⟨ψ,P(Ω)ψ⟩\mu_\psi(\Omega) = \langle\psi, P(\Omega)\psi\rangleμψ​(Ω)=⟨ψ,P(Ω)ψ⟩. By the spectral theorem every self-adjoint AAA equals ∫λ dP(λ)\int\lambda\,dP(\lambda)∫λdP(λ) for a unique PPP: D(A)={ψ∣∫λ2 dμψ<∞}\mathfrak D(A) = \{\psi \mid \int\lambda^2\,d\mu_\psi < \infty\}D(A)={ψ∣∫λ2dμψ​<∞} and ⟨ψ,Aψ⟩=∫λ dμψ\langle\psi, A\psi\rangle = \int\lambda\,d\mu_\psi⟨ψ,Aψ⟩=∫λdμψ​. The time evolution e−itA\mathrm e^{-\mathrm itA}e−itA is the bounded operator with ⟨ψ,e−itAψ⟩=∫e−itλ dμψ(λ)\langle\psi, \mathrm e^{-\mathrm itA}\psi\rangle = \int\mathrm e^{-\mathrm it\lambda}\,d\mu_\psi(\lambda)⟨ψ,e−itAψ⟩=∫e−itλdμψ​(λ).

For two self-adjoint operators H0H_0H0​, HHH the wave operators are

D(Ω±)={ψ∈H∣∃lim⁡t→±∞eitHe−itH0ψ},Ω±ψ=lim⁡t→±∞eitHe−itH0ψ.\mathfrak D(\Omega_\pm) = \{\psi \in \mathfrak H \mid \exists\lim_{t\to\pm\infty}\mathrm e^{\mathrm itH}\mathrm e^{-\mathrm itH_0}\psi\}, \qquad \Omega_\pm\psi = \lim_{t\to\pm\infty}\mathrm e^{\mathrm itH}\mathrm e^{-\mathrm itH_0}\psi .D(Ω±​)={ψ∈H∣∃t→±∞lim​eitHe−itH0​ψ},Ω±​ψ=t→±∞lim​eitHe−itH0​ψ.

D(Ω±)\mathfrak D(\Omega_\pm)D(Ω±​) is the set of asymptotic states and Ran⁡(Ω±)=Ω±D(Ω±)\operatorname{Ran}(\Omega_\pm) = \Omega_\pm\mathfrak D(\Omega_\pm)Ran(Ω±​)=Ω±​D(Ω±​) the set of states that have one. A closed subspace H1\mathfrak H_1H1​ with projection P1P_1P1​ reduces AAA if P1D(A)⊆D(A)P_1\mathfrak D(A) \subseteq \mathfrak D(A)P1​D(A)⊆D(A) and P1Aψ=AP1ψP_1A\psi = AP_1\psiP1​Aψ=AP1​ψ for ψ∈D(A)\psi \in \mathfrak D(A)ψ∈D(A).

On L2(Rn)L^2(\mathbb R^n)L2(Rn) the free Schrödinger operator is H0=−ΔH_0 = -\DeltaH0​=−Δ with domain the Sobolev space H2(Rn)H^2(\mathbb R^n)H2(Rn): under the Fourier transform it is multiplication by p2p^2p2 on {φ∣p2φ∈L2}\{\varphi \mid p^2\varphi \in L^2\}{φ∣p2φ∈L2}. For a real potential VVV, H=H0+VH = H_0 + VH=H0​+V has D(H)=H2(Rn)\mathfrak D(H) = H^2(\mathbb R^n)D(H)=H2(Rn) and (Hψ)(x)=(H0ψ)(x)+V(x)ψ(x)(H\psi)(x) = (H_0\psi)(x) + V(x)\psi(x)(Hψ)(x)=(H0​ψ)(x)+V(x)ψ(x).

Formalization targets

Goal: existence of the wave operators for V∈L2(R3)V \in L^2(\mathbb R^3)V∈L2(R3) (Theorem 12.4)

Let H0H_0H0​ be the free Schrödinger operator on L2(R3)L^2(\mathbb R^3)L2(R3) and H=H0+VH = H_0 + VH=H0​+V with a real V∈L2(R3)V \in L^2(\mathbb R^3)V∈L2(R3). Then

D(Ω+)=D(Ω−)=L2(R3),\mathfrak D(\Omega_+) = \mathfrak D(\Omega_-) = L^2(\mathbb R^3),D(Ω+​)=D(Ω−​)=L2(R3),

that is, lim⁡t→±∞eitHe−itH0ψ\lim_{t\to\pm\infty}\mathrm e^{\mathrm itH}\mathrm e^{-\mathrm itH_0}\psilimt→±∞​eitHe−itH0​ψ exists for every ψ\psiψ and both signs. Since the spectrum of H0H_0H0​ is purely absolutely continuous, this is exactly what Teschl calls "the wave operators exist" (12.14).

Milestones

  • Lemma 12.1. D(Ω±)\mathfrak D(\Omega_\pm)D(Ω±​) and Ran⁡(Ω±)\operatorname{Ran}(\Omega_\pm)Ran(Ω±​) are closed and Ω±:D(Ω±)→Ran⁡(Ω±)\Omega_\pm : \mathfrak D(\Omega_\pm) \to \operatorname{Ran}(\Omega_\pm)Ω±​:D(Ω±​)→Ran(Ω±​) is unitary.
  • Theorem 12.2. D(Ω±)\mathfrak D(\Omega_\pm)D(Ω±​) reduces H0H_0H0​, Ran⁡(Ω±)\operatorname{Ran}(\Omega_\pm)Ran(Ω±​) reduces HHH, and the restricted operators are unitarily equivalent: Ω±H0ψ=HΩ±ψ\Omega_\pm H_0\psi = H\Omega_\pm\psiΩ±​H0​ψ=HΩ±​ψ for ψ∈D(Ω±)∩D(H0)\psi \in \mathfrak D(\Omega_\pm) \cap \mathfrak D(H_0)ψ∈D(Ω±​)∩D(H0​).
  • Lemma 12.3 (Cook). If D(H)⊆D(H0)\mathfrak D(H) \subseteq \mathfrak D(H_0)D(H)⊆D(H0​), ψ∈D(H0)\psi \in \mathfrak D(H_0)ψ∈D(H0​) and ∫0∞∥(H−H0)exp⁡(∓itH0)ψ∥ dt<∞\int_0^\infty\|(H - H_0)\exp(\mp\mathrm itH_0)\psi\|\,dt < \infty∫0∞​∥(H−H0​)exp(∓itH0​)ψ∥dt<∞, then ψ∈D(Ω±)\psi \in \mathfrak D(\Omega_\pm)ψ∈D(Ω±​) and ∥(Ω±−I)ψ∥≤∫0∞∥(H−H0)exp⁡(∓itH0)ψ∥ dt\|(\Omega_\pm - \mathbb I)\psi\| \le \int_0^\infty\|(H - H_0)\exp(\mp\mathrm itH_0)\psi\|\,dt∥(Ω±​−I)ψ∥≤∫0∞​∥(H−H0​)exp(∓itH0​)ψ∥dt.

Significance

Existence of the wave operators is the first step of every scattering theory for Schrödinger operators: without it the scattering operator S=Ω+−1Ω−S = \Omega_+^{-1}\Omega_-S=Ω+−1​Ω−​ is not defined on a useful set of states, and the questions of completeness and asymptotic completeness (Enß's theorem, Theorem 12.12 of the same chapter) cannot be posed. Lemma 12.1 and Theorem 12.2 are the structural facts that make Ω±\Omega_\pmΩ±​ partial isometries intertwining the two Hamiltonians; they imply that HHH restricted to Ran⁡(Ω±)\operatorname{Ran}(\Omega_\pm)Ran(Ω±​) has absolutely continuous spectrum whenever H0H_0H0​ does, and that kinetic energy is conserved in scattering. Cook's criterion is the tool used in practice to prove existence for concrete potentials, including Coulomb-type and time-dependent problems.

The results are classical and proved in the literature. They are not formalized. Mathlib has neither the spectral theorem nor a functional calculus for unbounded self-adjoint operators, and no scattering theory. The platform has no statement about wave operators; its BookProof development contains Stone's theorem for its own structure of unbounded operators, which this mission does not use.

Difficulty

The limit defining Ω±\Omega_\pmΩ±​ involves two unitary groups whose generators do not commute, and neither group is explicit for the perturbed operator HHH. For Cook's criterion the product eitHe−itH0ψ\mathrm e^{\mathrm itH}\mathrm e^{-\mathrm itH_0}\psieitHe−itH0​ψ has to be differentiated in ttt, which needs control of domains: e−itH0ψ\mathrm e^{-\mathrm itH_0}\psie−itH0​ψ must stay in the domain of H−H0H - H_0H−H0​, and the derivative of a strongly continuous unitary group exists only on the domain of its generator. For the goal, the time evolution of a general ψ∈L2(R3)\psi \in L^2(\mathbb R^3)ψ∈L2(R3) has no decay rate at all, and the potential V∈L2V \in L^2V∈L2 is unbounded and has no decay assumption beyond square integrability, so the integrability condition of Cook's criterion cannot be checked for every ψ\psiψ directly. The intertwining relation (12.8) concerns unbounded operators and needs the reduction of the domains, not only an identity between bounded operators.

Formalization scope

The formalization uses Lean 4 with Mathlib. Operators are LinearPMaps H →ₗ.[ℂ] H on a complex Hilbert space; self-adjointness is Mathlib's IsSelfAdjoint. Separability is not assumed.

The spectral theorem is not part of this mission. Every statement takes projection-valued measures P0P_0P0​ and PPP as data, with the hypotheses H0=∫λ dP0(λ)H_0 = \int\lambda\,dP_0(\lambda)H0​=∫λdP0​(λ) and H=∫λ dP(λ)H = \int\lambda\,dP(\lambda)H=∫λdP(λ) (domain and quadratic form as above), which is the form the spectral theorem guarantees and which determines P0P_0P0​ and PPP. The time evolutions are e−itH0=∫e−itλ dP0\mathrm e^{-\mathrm itH_0} = \int\mathrm e^{-\mathrm it\lambda}\,dP_0e−itH0​=∫e−itλdP0​ and e−itH=∫e−itλ dP\mathrm e^{-\mathrm itH} = \int\mathrm e^{-\mathrm it\lambda}\,dPe−itH=∫e−itλdP. In the goal, the self-adjointness of H=H0+VH = H_0 + VH=H0​+V (Theorem 10.2 of the book) enters only through the existence of PPP. Nothing is assumed about Ω±\Omega_\pmΩ±​.

The sign of Ω±\Omega_\pmΩ±​ is a unit s : ℤˣ, and t→±∞t \to \pm\inftyt→±∞ is written as t→+∞t \to +\inftyt→+∞ in the variable ststst. Ω±\Omega_\pmΩ±​ is Mathlib's limUnder and is used only on D(Ω±)\mathfrak D(\Omega_\pm)D(Ω±​). A formalization that set Ω±ψ=0\Omega_\pm\psi = 0Ω±​ψ=0 where the limit fails and then proved only that Ω±\Omega_\pmΩ±​ is isometric would lose the content of the goal; here the goal asserts that the limit exists for every ψ∈L2(R3)\psi \in L^2(\mathbb R^3)ψ∈L2(R3). In Cook's lemma the finiteness of the integral is integrability on (0,∞)(0,\infty)(0,∞), the bound uses the Bochner integral, and the hypothesis that exp⁡(∓itH0)ψ\exp(\mp\mathrm itH_0)\psiexp(∓itH0​)ψ lies in D(H)\mathfrak D(H)D(H) for t≥0t \ge 0t≥0, which the integrand presupposes, is explicit.

L2(R3)L^2(\mathbb R^3)L2(R3) is Mathlib's Lp ℂ 2 on EuclideanSpace ℝ (Fin 3). The free Schrödinger operator is characterized through Mathlib's unitary L2L^2L2 Fourier transform FMf(ξ)=∫e−2πi⟨x,ξ⟩f(x) dx\mathcal F_M f(\xi) = \int\mathrm e^{-2\pi\mathrm i\langle x,\xi\rangle}f(x)\,dxFM​f(ξ)=∫e−2πi⟨x,ξ⟩f(x)dx, not the book's (2π)−n/2∫e−ipxf(x) dx(2\pi)^{-n/2}\int\mathrm e^{-\mathrm ipx}f(x)\,dx(2π)−n/2∫e−ipxf(x)dx. The constants are translated: D(H0)={ψ∣∣ξ∣2FMψ∈L2}\mathfrak D(H_0) = \{\psi \mid |\xi|^2\mathcal F_M\psi \in L^2\}D(H0​)={ψ∣∣ξ∣2FM​ψ∈L2} and FM(H0ψ)=4π2∣ξ∣2FMψ\mathcal F_M(H_0\psi) = 4\pi^2|\xi|^2\mathcal F_M\psiFM​(H0​ψ)=4π2∣ξ∣2FM​ψ. H=H0+VH = H_0 + VH=H0​+V has D(H)=D(H0)\mathfrak D(H) = \mathfrak D(H_0)D(H)=D(H0​) and Hψ=H0ψ+VψH\psi = H_0\psi + V\psiHψ=H0​ψ+Vψ almost everywhere.

A complete development needs a functional calculus for projection-valued measures (strong continuity and differentiability of e−itA\mathrm e^{-\mathrm itA}e−itA on D(A)\mathfrak D(A)D(A), Theorem 5.1), the explicit L1→L∞L^1 \to L^\inftyL1→L∞ decay of the free Schrödinger group in R3\mathbb R^3R3 ((7.31) of the book), and density of L1∩H2L^1 \cap H^2L1∩H2 in L2L^2L2. These pieces are reusable for the rest of Chapter 12 (incoming and outgoing states, short-range potentials, asymptotic completeness). Proofs of any milestone and of such supporting lemmas are welcome.

Selected references

  • G. Teschl, Mathematical Methods in Quantum Mechanics, With Applications to Schrödinger Operators, Graduate Studies in Mathematics 99, American Mathematical Society, 2009. doi:10.1090/gsm/099. Chapter 12, pp. 247–257.
  • J. M. Cook, Convergence to the Møller wave-matrix, J. Math. and Phys. 36 (1957), 82–87. doi:10.1002/sapm195736182.
  • J. M. Jauch, Theory of the scattering operator, Helv. Phys. Acta 31 (1958), 127–158.
  • M. Reed, B. Simon, Methods of Modern Mathematical Physics III: Scattering Theory, Academic Press, 1979.
  • V. Enß, Asymptotic completeness for quantum mechanical potential scattering. I. Short range potentials, Comm. Math. Phys. 61 (1978), 285–291. doi:10.1007/BF01940771.
12 thms1 active userReviewed
AnalysisFunctional AnalysisMathematical Physics·Captain: mikedeng1

Mathematical Methods in Quantum Mechanics VII: Compact, Hilbert–Schmidt and Trace Class OperatorsTextbook

Motivation

Quantum mechanics describes mixed states by density operators: positive operators ρ\rhoρ on a Hilbert space with tr⁡(ρ)=1\operatorname{tr}(\rho) = 1tr(ρ)=1. Expectation values are traces tr⁡(ρA)\operatorname{tr}(\rho A)tr(ρA), perturbation determinants and spectral shift functions are built from traces of resolvent differences, and scattering theory (the Kato–Rosenblum and Birman–Krein theorems) is phrased in terms of trace class perturbations. All of this needs a trace in infinite dimensions, and the trace ∑n⟨φn,Kφn⟩\sum_n \langle \varphi_n, K\varphi_n\rangle∑n​⟨φn​,Kφn​⟩ only makes sense on a restricted class of operators.

This mission formalizes Sections 6.2–6.3 of G. Teschl, Mathematical Methods in Quantum Mechanics, With Applications to Schrödinger Operators (AMS Graduate Studies in Mathematics 99, 2009), the standard route from compact operators through Hilbert–Schmidt operators to the trace class. The theory goes back to von Neumann and Schatten in the 1940s (R. Schatten, Norm Ideals of Completely Continuous Operators, Springer 1960). A modern account is B. Simon, Trace Ideals and Their Applications (AMS 2005).

Setting

Let H\mathfrak{H}H be a complex Hilbert space, with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ conjugate-linear in the first argument, and let L(H)\mathfrak{L}(\mathfrak{H})L(H) be the bounded linear operators on H\mathfrak{H}H with the operator norm ∥A∥\|A\|∥A∥. An operator is of finite rank if its range is finite dimensional, and the compact operators C(H)\mathfrak{C}(\mathfrak{H})C(H) are the norm closure of the finite rank operators.

For K∈L(H)K \in \mathfrak{L}(\mathfrak{H})K∈L(H) with adjoint K∗K^*K∗, the operator K∗KK^*KK∗K is positive. The singular values sj(K)>0s_j(K) > 0sj​(K)>0 of a compact KKK are the square roots of the nonzero eigenvalues of K∗KK^*KK∗K, each repeated according to its multiplicity dim⁡Ker⁡(K∗K−μ)\dim\operatorname{Ker}(K^*K - \mu)dimKer(K∗K−μ). For p≥1p \ge 1p≥1 the Schatten ppp-norm and Schatten ppp-class are

∥K∥p=(∑jsj(K)p)1/p∈[0,∞],Jp(H)={K∈C(H)∣∥K∥p<∞}.\|K\|_p = \Big(\sum_j s_j(K)^p\Big)^{1/p} \in [0,\infty], \qquad \mathcal{J}_p(\mathfrak{H}) = \{K \in \mathfrak{C}(\mathfrak{H}) \mid \|K\|_p < \infty\}.∥K∥p​=(j∑​sj​(K)p)1/p∈[0,∞],Jp​(H)={K∈C(H)∣∥K∥p​<∞}.

A compact KKK is Hilbert–Schmidt if K∈J2(H)K \in \mathcal{J}_2(\mathfrak{H})K∈J2​(H) and trace class if K∈J1(H)K \in \mathcal{J}_1(\mathfrak{H})K∈J1​(H). For an orthonormal basis {φn}\{\varphi_n\}{φn​} of H\mathfrak{H}H the trace is

tr⁡(K)=∑n⟨φn,Kφn⟩.\operatorname{tr}(K) = \sum_n \langle \varphi_n, K\varphi_n\rangle .tr(K)=n∑​⟨φn​,Kφn​⟩.

In Lean these are compactOperators H, schattenNorm p K, schattenClass H p, IsHilbertSchmidt K, IsTraceClass K and trace K, in the namespace TeschlQM.TraceClass.

Formalization targets

Goal: the trace is well defined (Lemma 6.15)

For every trace class KKK and every orthonormal basis {φn}\{\varphi_n\}{φn​} the series (6.26) converges, and for any two orthonormal bases {φn}\{\varphi_n\}{φn​}, {ψm}\{\psi_m\}{ψm​}

∑n⟨φn,Kφn⟩=∑m⟨ψm,Kψm⟩=tr⁡(K).\sum_n \langle \varphi_n, K\varphi_n\rangle = \sum_m \langle \psi_m, K\psi_m\rangle = \operatorname{tr}(K).n∑​⟨φn​,Kφn​⟩=m∑​⟨ψm​,Kψm​⟩=tr(K).

Milestones

  1. Theorem 6.7 (canonical form): a compact KKK has the form K=∑jsj⟨ϕj,⋅⟩ϕ^jK = \sum_j s_j\langle\phi_j, \cdot\rangle\hat\phi_jK=∑j​sj​⟨ϕj​,⋅⟩ϕ^​j​ with orthonormal {ϕj}\{\phi_j\}{ϕj​}, {ϕ^j}\{\hat\phi_j\}{ϕ^​j​}, and the sj2s_j^2sj2​ are the nonzero eigenvalues of K∗KK^*KK∗K and of KK∗KK^*KK∗, counted with multiplicity.
  2. Lemma 6.10: a compact KKK is Hilbert–Schmidt iff ∑n∥Kψn∥2<∞\sum_n\|K\psi_n\|^2 < \infty∑n​∥Kψn​∥2<∞ for some orthonormal basis, and then ∑n∥Kψn∥2=∥K∥22\sum_n\|K\psi_n\|^2 = \|K\|_2^2∑n​∥Kψn​∥2=∥K∥22​ for every orthonormal basis.
  3. Corollary 6.11: the Hilbert–Schmidt operators form a ∗*∗-ideal, with ∥KA∥2,∥AK∥2≤∥A∥∥K∥2\|KA\|_2, \|AK\|_2 \le \|A\|\|K\|_2∥KA∥2​,∥AK∥2​≤∥A∥∥K∥2​.
  4. Lemma 6.12: (Jp(H),∥⋅∥p)(\mathcal{J}_p(\mathfrak{H}), \|\cdot\|_p)(Jp​(H),∥⋅∥p​) is a Banach space, and
∥K∥p=sup⁡{(∑j∣⟨ψj,Kφj⟩∣p)1/p  ∣  {ψj},{φj} orthonormal}.\|K\|_p = \sup\Big\{\Big(\sum_j|\langle\psi_j, K\varphi_j\rangle|^p\Big)^{1/p} \;\Big|\; \{\psi_j\}, \{\varphi_j\} \text{ orthonormal}\Big\}.∥K∥p​=sup{(j∑​∣⟨ψj​,Kφj​⟩∣p)1/p​{ψj​},{φj​} orthonormal}.
  1. Lemma 6.13: KKK is trace class iff K=K1K2K = K_1K_2K=K1​K2​ with K1,K2K_1, K_2K1​,K2​ Hilbert–Schmidt, and then ∥K∥1≤∥K1∥2∥K2∥2\|K\|_1 \le \|K_1\|_2\|K_2\|_2∥K∥1​≤∥K1​∥2​∥K2​∥2​.
  2. Corollary 6.14: the trace class is a ∗*∗-ideal, with ∥KA∥1,∥AK∥1≤∥A∥∥K∥1\|KA\|_1, \|AK\|_1 \le \|A\|\|K\|_1∥KA∥1​,∥AK∥1​≤∥A∥∥K∥1​.
  3. Lemma 6.16 (after the goal): the trace is linear, tr⁡(K∗)=tr⁡(K)‾\operatorname{tr}(K^*) = \overline{\operatorname{tr}(K)}tr(K∗)=tr(K)​, it is monotone for the operator order, and tr⁡(AK)=tr⁡(KA)\operatorname{tr}(AK) = \operatorname{tr}(KA)tr(AK)=tr(KA) for bounded AAA.

Significance

The result itself. Lemma 6.15 is what turns the trace into a linear functional on J1(H)\mathcal{J}_1(\mathfrak{H})J1​(H) at all. Every later use of the trace rests on it: the normalization of density matrices, the duality J1(H)∗≅L(H)\mathcal{J}_1(\mathfrak{H})^* \cong \mathfrak{L}(\mathfrak{H})J1​(H)∗≅L(H), trace formulas and spectral shift functions, and Lidskii's theorem (the trace is the sum of the eigenvalues), which Teschl mentions right after the lemma. The ideal properties (Corollaries 6.11 and 6.14) and the factorization (Lemma 6.13) are the everyday tools for proving that a concrete operator, such as f(x)g(−i∇)f(x)g(-i\nabla)f(x)g(−i∇) in Chapter 7, is trace class.

Formalizing it. Mathlib has compact operators (IsCompactOperator), Hilbert bases, singular values and the trace of linear maps on finite-dimensional spaces (LinearMap.singularValues, LinearMap.trace), but no infinite-dimensional singular values, Schatten classes, Hilbert–Schmidt or trace class operators, and no basis-independent trace. The Prove2Me corpus has finite-dimensional trace norms (matrices) and L2L^2L2 kernel operators, but no statement of this section. The results are classical and fully proved in the literature; the work is to formalize them.

Difficulty

The obvious argument for basis independence is to expand KKK in both bases and interchange the two sums. In infinite dimensions that interchange is not justified for an arbitrary bounded KKK: for the identity on an infinite-dimensional space, or for a non-trace-class compact operator, the diagonal series diverges. The trace class hypothesis must therefore enter through a factorization, and the factorization rests on the canonical form of Theorem 6.7, which in turn needs the spectral theorem for the compact self-adjoint operator K∗KK^*KK∗K, including finite multiplicity of its nonzero eigenvalues. A second difficulty is bookkeeping: the singular values are a family with multiplicities that may be finite or countably infinite, and the Schatten norm, the Hilbert–Schmidt sums over a basis and the supremum formula (6.23) all have to be matched as sums in [0,∞][0,\infty][0,∞].

Formalization scope

  • Hilbert space. {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]. Separability is not assumed. Orthonormal bases are Mathlib HilbertBasis ι ℂ H with arbitrary index types, so every statement covers the book's separable case.
  • Operators. Bounded operators are H →L[ℂ] H, products are compositions, adjoints are ContinuousLinearMap.adjoint, and the operator order in Lemma 6.16 is Mathlib's Loewner order (K1≤K2K_1 \le K_2K1​≤K2​ iff K2−K1K_2 - K_1K2​−K1​ is positive). Traces are compared with the partial order of C\mathbb{C}C.
  • Compactness is the book's definition, membership in the norm closure of the finite rank operators, not Mathlib's IsCompactOperator.
  • Singular values are not enumerated. ∑jsj(K)p\sum_j s_j(K)^p∑j​sj​(K)p is written as ∑μ>0dim⁡Ker⁡(K∗K−μ) μp/2\sum_{\mu > 0} \dim\operatorname{Ker}(K^*K - \mu)\,\mu^{p/2}∑μ>0​dimKer(K∗K−μ)μp/2, with the dimension in {0,1,… }∪{∞}\{0,1,\dots\}\cup\{\infty\}{0,1,…}∪{∞}. Norms and sums live in [0,∞][0,\infty][0,∞], so a divergent series is ∞\infty∞, never a junk 000. Hilbert–Schmidt and trace class are defined by ∥K∥2<∞\|K\|_2 < \infty∥K∥2​<∞ and ∥K∥1<∞\|K\|_1 < \infty∥K∥1​<∞ on compact KKK. The basis characterizations (Lemma 6.10) and the factorization (Lemma 6.13) are theorems, not definitions.
  • Trace. trace K is ∑n⟨φn,Kφn⟩\sum_n\langle\varphi_n, K\varphi_n\rangle∑n​⟨φn​,Kφn​⟩ in one fixed, chosen Hilbert basis. The goal states summability in every Hilbert basis, not merely equality of tsum values. Since the tsum of a non-summable family is 000 in Mathlib, a statement asserting only that all tsums agree would be trivially satisfiable by divergent series. That trivializing reading is ruled out.
  • Lemma 6.12 assumes 1≤p1 \le p1≤p (the book's proof uses the conjugate exponent). "Banach space" is spelled out as closure under the linear operations, the norm axioms, and completeness of ∥⋅∥p\|\cdot\|_p∥⋅∥p​-Cauchy sequences.
  • No projection-valued measure, no functional calculus and no Fourier transform is used, and nothing is taken as data.

Reusable infrastructure a complete development will produce includes the spectral theorem for compact self-adjoint operators with multiplicities, the singular value decomposition in infinite dimensions, and the Hilbert–Schmidt and trace class ideals. All of these are welcome as independent contributions, and any of them would fill gaps in Mathlib.

Selected references

  • G. Teschl, Mathematical Methods in Quantum Mechanics, With Applications to Schrödinger Operators, Graduate Studies in Mathematics 99, AMS, 2009, Sections 6.2–6.3. https://doi.org/10.1090/gsm/099
  • R. Schatten, Norm Ideals of Completely Continuous Operators, Ergebnisse der Mathematik und ihrer Grenzgebiete, Springer, 1960 (no stable link verified).
  • B. Simon, Trace Ideals and Their Applications, 2nd ed., Mathematical Surveys and Monographs 120, AMS, 2005. https://doi.org/10.1090/surv/120
  • M. Reed and B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, Academic Press, 1980, Section VI.6 (no stable link verified).
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AnalysisFunctional AnalysisMathematical Physics+1·Captain: mikedeng1

Mathematical Methods in Quantum Mechanics XIII: Atomic Schrödinger Operators and the HVZ TheoremTextbook

Motivation

An atom with NNN electrons is described, with the nucleus fixed at the origin, by a Schrödinger operator on L2(R3N)L^2(\mathbb R^{3N})L2(R3N) whose potential does not decay in all directions: moving one electron to infinity while the others stay near the nucleus leaves the remaining Coulomb attraction untouched. For this reason the standard route to the essential spectrum of a one-particle operator, showing that the potential is a relatively compact perturbation of −Δ-\Delta−Δ, fails for N≥2N \ge 2N≥2. The HVZ theorem, due to Zhislin (1960), van Winter (1964) and Hunziker (1966), gives the answer anyway: the essential spectrum of the NNN-electron atom begins exactly at the ground state energy of the ion with one electron removed. It is the basic structural result of NNN-body quantum mechanics, and the starting point for every discussion of bound states, ionization energies and the stability of atoms and molecules.

This mission follows Chapter 11 of Teschl, Mathematical Methods in Quantum Mechanics (AMS GSM 99, 2009), which proves self-adjointness by Kato's theorem and the HVZ theorem by the localization method of Ismagilov, Morgan, Simon and Sigal.

Setting

Write Rn\mathbb R^nRn for Euclidean space with Lebesgue measure. The Sobolev space H2(Rn)H^2(\mathbb R^n)H2(Rn) is the set of ψ∈L2(Rn)\psi \in L^2(\mathbb R^n)ψ∈L2(Rn) with ∣p∣2ψ^(p)∈L2(Rn)|p|^2 \hat\psi(p) \in L^2(\mathbb R^n)∣p∣2ψ^​(p)∈L2(Rn), and the free Schrödinger operator is H0ψ=−Δψ=(∣p∣2ψ^)∨H_0\psi = -\Delta\psi = (|p|^2\hat\psi)^\veeH0​ψ=−Δψ=(∣p∣2ψ^​)∨ with domain H2(Rn)H^2(\mathbb R^n)H2(Rn) (units ℏ=1\hbar = 1ℏ=1, mass 1/21/21/2). A measurable function VVV acts as the multiplication operator (Vψ)(x)=V(x)ψ(x)(V\psi)(x) = V(x)\psi(x)(Vψ)(x)=V(x)ψ(x) on its maximal domain {ψ∈L2∣Vψ∈L2}\{\psi \in L^2 \mid V\psi \in L^2\}{ψ∈L2∣Vψ∈L2}.

For an operator AAA with domain D(A)\mathfrak D(A)D(A) in a Hilbert space, the resolvent set ρ(A)\rho(A)ρ(A) is the set of z∈Cz \in \mathbb Cz∈C for which A−zA - zA−z maps D(A)\mathfrak D(A)D(A) bijectively onto the space with bounded inverse RA(z)R_A(z)RA​(z), and σ(A)=C∖ρ(A)\sigma(A) = \mathbb C \setminus \rho(A)σ(A)=C∖ρ(A) is the spectrum. The discrete spectrum σd(A)\sigma_d(A)σd​(A) consists of the eigenvalues that are isolated points of σ(A)\sigma(A)σ(A) and have finite-dimensional eigenspaces; the essential spectrum is σess(A)=σ(A)∖σd(A)\sigma_{ess}(A) = \sigma(A) \setminus \sigma_d(A)σess​(A)=σ(A)∖σd​(A). AAA is bounded from below if ⟨ψ,Aψ⟩≥γ∥ψ∥2\langle\psi, A\psi\rangle \ge \gamma\|\psi\|^2⟨ψ,Aψ⟩≥γ∥ψ∥2 on D(A)\mathfrak D(A)D(A) for some γ∈R\gamma \in \mathbb Rγ∈R. BBB is AAA bounded if D(A)⊆D(B)\mathfrak D(A) \subseteq \mathfrak D(B)D(A)⊆D(B) and ∥Bψ∥≤a∥Aψ∥+b∥ψ∥\|B\psi\| \le a\|A\psi\| + b\|\psi\|∥Bψ∥≤a∥Aψ∥+b∥ψ∥; the infimum of admissible aaa is the AAA-bound. KKK is relatively compact with respect to AAA if KRA(z)K R_A(z)KRA​(z) is compact for one z∈ρ(A)z \in \rho(A)z∈ρ(A).

For an atom with NNN electrons at x=(x1,…,xN)∈R3Nx = (x_1, \dots, x_N) \in \mathbb R^{3N}x=(x1​,…,xN​)∈R3N, xj∈R3x_j \in \mathbb R^3xj​∈R3, and constants γne,γee>0\gamma_{ne}, \gamma_{ee} > 0γne​,γee​>0, the atomic Hamiltonian is

H(N)=−∑j=1NΔj−∑j=1Nγne∣xj∣+∑1≤j<k≤Nγee∣xj−xk∣,D(H(N))=H2(R3N).H^{(N)} = -\sum_{j=1}^N \Delta_j - \sum_{j=1}^N \frac{\gamma_{ne}}{|x_j|} + \sum_{1 \le j < k \le N} \frac{\gamma_{ee}}{|x_j - x_k|}, \qquad \mathfrak D(H^{(N)}) = H^2(\mathbb R^{3N}).H(N)=−j=1∑N​Δj​−j=1∑N​∣xj​∣γne​​+1≤j<k≤N∑​∣xj​−xk​∣γee​​,D(H(N))=H2(R3N).

H(N−1)H^{(N-1)}H(N−1) denotes the same operator for N−1N - 1N−1 electrons with the same constants.

Formalization targets

Goal: the HVZ theorem (Theorem 11.2)

For N≥1N \ge 1N≥1, H(N)H^{(N)}H(N) is bounded from below, and

σess(H(N))=[λN−1,∞),λN−1=min⁡σ(H(N−1)),\sigma_{ess}(H^{(N)}) = [\lambda^{N-1}, \infty), \qquad \lambda^{N-1} = \min \sigma(H^{(N-1)}),σess​(H(N))=[λN−1,∞),λN−1=minσ(H(N−1)),

with λN−1<0\lambda^{N-1} < 0λN−1<0 for N≥2N \ge 2N≥2. The minimum is attained and, for N≥2N \ge 2N≥2, negative; both are part of the claim.

Milestones

  • Kato's theorem (Theorem 11.1). For real-valued Vk∈L∞∞(Rd)+L2(Rd)V_k \in L^\infty_\infty(\mathbb R^d) + L^2(\mathbb R^d)Vk​∈L∞∞​(Rd)+L2(Rd), d≤3d \le 3d≤3, composed with the first ddd coordinates of orthogonal transformations of RNd\mathbb R^{Nd}RNd, each Vk(y(k))V_k(y^{(k)})Vk​(y(k)) has H0H_0H0​-bound 000, and H=H0+∑kVk(y(k))H = H_0 + \sum_k V_k(y^{(k)})H=H0​+∑k​Vk​(y(k)) with D(H)=H2(RNd)\mathfrak D(H) = H^2(\mathbb R^{Nd})D(H)=H2(RNd) is self-adjoint with core C0∞(RNd)C_0^\infty(\mathbb R^{Nd})C0∞​(RNd).
  • IMS localization formula (Lemma 11.3). If φj∈C∞(Rn)\varphi_j \in C^\infty(\mathbb R^n)φj​∈C∞(Rn) satisfy ∑jφj2=1\sum_j \varphi_j^2 = 1∑j​φj2​=1, then for ψ∈H2(Rn)\psi \in H^2(\mathbb R^n)ψ∈H2(Rn)
Δψ=∑j(φjΔ(φjψ)+∣∂φj∣2ψ).\Delta\psi = \sum_{j} \big(\varphi_j\Delta(\varphi_j\psi) + |\partial\varphi_j|^2\psi\big).Δψ=j∑​(φj​Δ(φj​ψ)+∣∂φj​∣2ψ).
  • Localizing partition (Lemma 11.4). For C∈(0,1/N)C \in (0, 1/\sqrt N)C∈(0,1/N​) there are smooth φj:R3N→[0,1]\varphi_j : \mathbb R^{3N} \to [0,1]φj​:R3N→[0,1] with ∑jφj2=1\sum_j \varphi_j^2 = 1∑j​φj2​=1, supp⁡φj∩{∣x∣≥1}⊆{∣xj∣≥C∣x∣}\operatorname{supp}\varphi_j \cap \{|x| \ge 1\} \subseteq \{|x_j| \ge C|x|\}suppφj​∩{∣x∣≥1}⊆{∣xj​∣≥C∣x∣} and ∣∂φj(x)∣→0|\partial\varphi_j(x)| \to 0∣∂φj​(x)∣→0 as ∣x∣→∞|x| \to \infty∣x∣→∞.
  • A compactness criterion (Lemma 11.5). A multiplication operator VVV with H0H_0H0​-bound 000 and ∥χ{∣x∣≥R}VRH0(z)∥→0\|\chi_{\{|x| \ge R\}} V R_{H_0}(z)\| \to 0∥χ{∣x∣≥R}​VRH0​​(z)∥→0 as R→∞R \to \inftyR→∞ is relatively compact with respect to H0H_0H0​.

Significance

The result. The HVZ theorem separates the spectrum of an atom into a continuum [λN−1,∞)[\lambda^{N-1}, \infty)[λN−1,∞), fixed by the (N−1)(N-1)(N−1)-electron ion, and a discrete part below it consisting of bound states. The ionization energy of the atom is λN−λN−1\lambda^N - \lambda^{N-1}λN−λN−1. Questions such as whether a given atom or negative ion has a bound state at all, whether it has infinitely many (Zhislin's theorem for neutral atoms and positive ions), and how many electrons a nucleus can bind are all formulated relative to the threshold the HVZ theorem identifies. The same argument, with additional notation, covers molecules with fixed nuclei and general NNN-body systems.

Formalizing it. The results are classical and proved in the standard texts (Reed–Simon IV, Cycon–Froese–Kirsch–Simon, Teschl). None is formalized. Mathlib now has the unitary Fourier transform on L2L^2L2, tempered distributions and Sobolev spaces defined through the Fourier transform, but no self-adjoint Schrödinger operators, no essential spectrum and no many-body Hamiltonians. This mission asks for formal proofs of Teschl's four supporting results and of the HVZ theorem, and in doing so fixes a concrete representation of H0H_0H0​, of Coulomb-type multiplication operators and of the NNN-electron atom on which later work (bound states of atoms, scattering) can build.

Difficulty

The obvious argument for the essential spectrum of −Δ+V-\Delta + V−Δ+V, relative compactness of VVV followed by Weyl's theorem, is not available: γne/∣xj∣\gamma_{ne}/|x_j|γne​/∣xj​∣ does not vanish as ∣x∣→∞|x| \to \infty∣x∣→∞ in directions where xjx_jxj​ stays bounded, and it is not relatively compact with respect to H0H_0H0​ on L2(R3N)L^2(\mathbb R^{3N})L2(R3N). The inclusion σess(H(N))⊆[λN−1,∞)\sigma_{ess}(H^{(N)}) \subseteq [\lambda^{N-1}, \infty)σess​(H(N))⊆[λN−1,∞) therefore requires decomposing configuration space into regions in which one specific electron is far from the nucleus, controlling the error terms of that decomposition, and comparing the localized pieces with decoupled operators whose spectrum is known; this uses self-adjointness and relative bounds for operators built from the same potentials with one electron removed. The reverse inclusion requires approximate eigenfunctions built from those of H(N−1)H^{(N-1)}H(N−1) and of the free one-electron operator, and a statement that λN−1\lambda^{N-1}λN−1 is attained. Negativity of λN−1\lambda^{N-1}λN−1 needs the hydrogen-like ground state and a comparison argument across NNN.

Behind all of this sits the analytic layer: Kato's theorem requires that 1/∣x∣1/|x|1/∣x∣ in three dimensions is infinitesimally bounded with respect to −Δ-\Delta−Δ and that this survives the passage to R3N\mathbb R^{3N}R3N through an orthogonal change of variables; the IMS formula requires relating the Fourier definition of H0H_0H0​ to derivatives of products.

Formalization scope

The Hilbert space is Lp ℂ 2 volume over EuclideanSpace ℝ ι; for the atom, ι=Fin N × Fin 3\iota = \texttt{Fin N × Fin 3}ι=Fin N × Fin 3, so ∣x∣|x|∣x∣ is the Euclidean norm on R3N\mathbb R^{3N}R3N and xjx_jxj​ is electron x j. Operators are Mathlib LinearPMaps, self-adjointness is Mathlib's IsSelfAdjoint, and sums of unbounded operators are LinearPMap sums with the intersection of the domains. H0H_0H0​ (freeHamiltonian) is defined as F−1 (4π2∥ξ∥2) F\mathcal F^{-1}\,(4\pi^2\|\xi\|^2)\,\mathcal FF−1(4π2∥ξ∥2)F with Mathlib's unitary L2L^2L2 Fourier transform (kernel e−2πi⟨x,ξ⟩e^{-2\pi i\langle x,\xi\rangle}e−2πi⟨x,ξ⟩, no prefactor); this is the same operator −Δ-\Delta−Δ on the same domain H2H^2H2 as Teschl's F−1∣p∣2FF^{-1}|p|^2FF−1∣p∣2F. Multiplication operators (mulOp) have their maximal domains. H(N)H^{(N)}H(N) (atomicHamiltonian) is freeHamiltonian + mulOp V^{(N)}; the equality of its domain with H2(R3N)H^2(\mathbb R^{3N})H2(R3N) is a claim of Theorem 11.1, not an assumption. Resolvent set, spectrum, discrete and essential spectrum are defined from the bounded two-sided inverse of A−zA - zA−z, not from Mathlib's Banach-algebra spectrum. The AAA-bound takes values in [0,∞][0, \infty][0,∞]. The IMS formula is stated in the sense of distributions, tested against C0∞C_0^\inftyC0∞​ functions, since for merely smooth φj\varphi_jφj​ its right-hand side need not lie in L2L^2L2. No projection-valued measure or functional calculus is taken as data.

A trivializing formalization is ruled out: λN−1\lambda^{N-1}λN−1 is defined as the minimum of the spectrum of the independently constructed (N−1)(N-1)(N−1)-electron operator, never as the infimum of σess(H(N))\sigma_{ess}(H^{(N)})σess​(H(N)), which would make (11.9) circular; its attainment and negativity are conclusions. The goal covers N≥1N \ge 1N≥1; for N=1N = 1N=1 the ion has no electrons, λ0=0\lambda^0 = 0λ0=0 is not negative, so the negativity of λN−1\lambda^{N-1}λN−1 is claimed for N≥2N \ge 2N≥2 only.

A complete development needs the L2L^2L2 theory of the Fourier transform and H2H^2H2, Hardy- or Sobolev-type bounds for 1/∣x∣1/|x|1/∣x∣ in R3\mathbb R^3R3, the Kato–Rellich theorem, Weyl's theorem on relatively compact perturbations, a smooth partition of unity on the sphere, and the Weyl criterion for essential spectrum. The definitions of H0H_0H0​, multiplication operators, resolvent and essential spectrum are shared with other chapters of this series and are intended for reuse; contributions of general lemmas about them are welcome.

Selected references

  • G. Teschl, Mathematical Methods in Quantum Mechanics, With Applications to Schrödinger Operators, Graduate Studies in Mathematics 99, AMS, 2009, Chapter 11. https://doi.org/10.1090/gsm/099
  • G. M. Zhislin, Discussion of the spectrum of Schrödinger operators for systems of many particles, Trudy Moskovskogo Matematicheskogo Obshchestva 9 (1960), 81–120.
  • C. van Winter, Theory of finite systems of particles I. The Green function, Matematisk-Fysiske Skrifter Danske Videnskabernes Selskab 2 (1964), no. 8.
  • W. Hunziker, On the spectra of Schrödinger multiparticle Hamiltonians, Helvetica Physica Acta 39 (1966), 451–462.
  • T. Kato, Fundamental properties of Hamiltonian operators of Schrödinger type, Transactions of the AMS 70 (1951), 195–211. https://doi.org/10.1090/S0002-9947-1951-0041010-X
  • H. L. Cycon, R. G. Froese, W. Kirsch, B. Simon, Schrödinger Operators with Application to Quantum Mechanics and Global Geometry, Springer, 1987.
  • M. Reed and B. Simon, Methods of Modern Mathematical Physics IV: Analysis of Operators, Academic Press, 1978, Section XIII.5.
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Numerical AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Euler Approximations with Varying Coefficients I: Lp-Convergence of Explicit Euler Schemes under Local MonotonicityResearch Paper

Motivation

Stochastic differential equations (SDEs) whose coefficients grow faster than linearly appear throughout applied probability: population and epidemic models with cubic damping, Langevin dynamics with non-quadratic potentials, and stochastic volatility models such as the 3/2-model used for pricing VIX options (Goard–Mazur 2013). Their solutions are almost never available in closed form, so they are simulated, and the method of choice is the explicit Euler–Maruyama scheme, because it is cheap and easy to implement.

For superlinearly growing coefficients the classical explicit scheme fails: its moments can diverge even when those of the true solution are finite, so it does not converge in Lp\mathcal L^pLp. Implicit schemes repair this at a higher computational cost (Higham–Mao–Stuart 2002). A second repair is to keep the scheme explicit but modify ("tame") its coefficients by an amount that vanishes as the step size goes to zero.

Timeline.

  • 2002: Higham, Mao and Stuart prove strong convergence of implicit Euler-type methods under a one-sided Lipschitz condition (MR1949404).
  • 2012: Hutzenthaler, Jentzen and Kloeden introduce the tamed Euler scheme for superlinearly growing drift and globally Lipschitz diffusion (Ann. Appl. Probab. 22, MR2985171).
  • 2013: Sabanis gives a short proof of convergence of tamed schemes with rate, again for superlinear drift (Electron. Commun. Probab. 18, MR3070913); Gyöngy and Sabanis prove convergence in probability of Euler approximations under local monotonicity conditions (Appl. Math. Optim. 68, MR3131501).
  • 2015: Hutzenthaler and Jentzen obtain Lp\mathcal L^pLp-convergence of explicit schemes with superlinear diffusion coefficients, in the 3/2-model only for p<1/2p<1/2p<1/2 (Mem. Amer. Math. Soc. 236, no. 1112).
  • 2016: Sabanis treats superlinearly growing drift and diffusion coefficients under a local monotonicity condition, with Lp\mathcal L^pLp-convergence for every p<p0p<p_0p<p0​ (Ann. Appl. Probab. 26, arXiv:1308.1796). This mission formalizes that Lp\mathcal L^pLp-convergence theorem.

Setting

Fix a filtered probability space (Ω,{Ft}t≥0,F,P)(\Omega,\{\mathcal F_t\}_{t\ge0},\mathcal F,P)(Ω,{Ft​}t≥0​,F,P) satisfying the usual conditions, a Wiener martingale WWW in Rd1\mathbb R^{d_1}Rd1​ (a standard Brownian motion adapted to Ft\mathcal F_tFt​ whose future increments are independent of Ft\mathcal F_tFt​), and a horizon T>0T>0T>0. For x∈Rdx\in\mathbb R^dx∈Rd, ∣x∣|x|∣x∣ is the Euclidean norm and xyxyxy the scalar product; for a d×d1d\times d_1d×d1​ matrix, ∣A∣|A|∣A∣ is the Hilbert–Schmidt norm.

The SDE is

dX(t)=b(t,X(t)) dt+σ(t,X(t)) dW(t),t∈[0,T],(2.1)dX(t)=b(t,X(t))\,dt+\sigma(t,X(t))\,dW(t),\qquad t\in[0,T],\tag{2.1}dX(t)=b(t,X(t))dt+σ(t,X(t))dW(t),t∈[0,T],(2.1)

with Borel coefficients b(t,x)∈Rdb(t,x)\in\mathbb R^db(t,x)∈Rd, σ(t,x)∈Rd×d1\sigma(t,x)\in\mathbb R^{d\times d_1}σ(t,x)∈Rd×d1​ and an F0\mathcal F_0F0​-measurable initial value X(0)X(0)X(0).

For n≥1n\ge1n≥1 let κn(t)=⌊nt⌋/n\kappa_n(t)=\lfloor nt\rfloor/nκn​(t)=⌊nt⌋/n, the last grid point of mesh 1/n1/n1/n before ttt. The scheme is

dXn(t)=bn(t,Xn(κn(t))) dt+σn(t,Xn(κn(t))) dW(t),t∈[0,T],(2.2)dX_n(t)=b_n(t,X_n(\kappa_n(t)))\,dt+\sigma_n(t,X_n(\kappa_n(t)))\,dW(t),\qquad t\in[0,T],\tag{2.2}dXn​(t)=bn​(t,Xn​(κn​(t)))dt+σn​(t,Xn​(κn​(t)))dW(t),t∈[0,T],(2.2)

with the same initial value X(0)X(0)X(0) and Borel coefficient sequences bn,σnb_n,\sigma_nbn​,σn​ ("varying coefficients"). Between grid points the coefficients are frozen at Xn(κn(t))X_n(\kappa_n(t))Xn​(κn​(t)), so the scheme is explicit.

The hypotheses, with p0,p1∈[2,∞)p_0,p_1\in[2,\infty)p0​,p1​∈[2,∞): A-1 continuity of bbb in xxx; A-2 local boundedness of bbb; A-3 local monotonicity 2(x−y)(b(t,x)−b(t,y))+(p1−1)∣σ(t,x)−σ(t,y)∣2≤LR∣x−y∣22(x-y)(b(t,x)-b(t,y))+(p_1-1)|\sigma(t,x)-\sigma(t,y)|^2\le L_R|x-y|^22(x−y)(b(t,x)−b(t,y))+(p1​−1)∣σ(t,x)−σ(t,y)∣2≤LR​∣x−y∣2 on ∣x∣,∣y∣≤R|x|,|y|\le R∣x∣,∣y∣≤R; A-4 coercivity 2xb(t,x)+(p0−1)∣σ(t,x)∣2≤K(1+∣x∣2)2xb(t,x)+(p_0-1)|\sigma(t,x)|^2\le K(1+|x|^2)2xb(t,x)+(p0​−1)∣σ(t,x)∣2≤K(1+∣x∣2); A-5 E∣X(0)∣p0<∞\mathbb E|X(0)|^{p_0}<\inftyE∣X(0)∣p0​<∞. For the scheme: B-1 ∫0Tsup⁡∣x∣≤R[∣bn−b∣p0+∣σn−σ∣p0] dt→0\int_0^T\sup_{|x|\le R}[|b_n-b|^{p_0}+|\sigma_n-\sigma|^{p_0}]\,dt\to0∫0T​sup∣x∣≤R​[∣bn​−b∣p0​+∣σn​−σ∣p0​]dt→0 for every RRR; B-2 ∣bn∣≤min⁡(Cnα(1+∣x∣),∣b∣)|b_n|\le\min(Cn^\alpha(1+|x|),|b|)∣bn​∣≤min(Cnα(1+∣x∣),∣b∣) and ∣σn∣2≤min⁡(Cnα(1+∣x∣2),∣σ∣2)|\sigma_n|^2\le\min(Cn^\alpha(1+|x|^2),|\sigma|^2)∣σn​∣2≤min(Cnα(1+∣x∣2),∣σ∣2) for some α∈(0,1/2]\alpha\in(0,1/2]α∈(0,1/2]; B-3 the coercivity bound of A-4 for bn,σnb_n,\sigma_nbn​,σn​, uniformly in nnn.

Formalization targets

Goal: Theorem 1 (p. 5)

Under A-1–A-5 and B-1–B-3 with α∈(0,1/2]\alpha\in(0,1/2]α∈(0,1/2], for every 0<p<p00<p<p_00<p<p0​,

lim⁡n→∞sup⁡0≤t≤TE[∣X(t)−Xn(t)∣p]=0.\lim_{n\to\infty}\sup_{0\le t\le T}\mathbb E\big[|X(t)-X_n(t)|^p\big]=0.n→∞lim​0≤t≤Tsup​E[∣X(t)−Xn​(t)∣p]=0.

No rate is claimed; the statement holds for every coefficient sequence satisfying B-1–B-3, not only for the paper's tamed Models 1 and 2.

Milestones

  • Lemma 1 (p. 7): under A-5, B-2, B-3, sup⁡n≥1sup⁡0≤u≤TE∣Xn(u)∣2<∞\sup_{n\ge1}\sup_{0\le u\le T}\mathbb E|X_n(u)|^2<\inftysupn≥1​sup0≤u≤T​E∣Xn​(u)∣2<∞.
  • Lemma 2 (p. 8): under A-1–A-5, B-2, B-3, for every p≤p0p\le p_0p≤p0​,
sup⁡0≤t≤TE∣X(t)∣p ∨ sup⁡n≥1sup⁡0≤t≤TE∣Xn(t)∣p<∞.\sup_{0\le t\le T}\mathbb E|X(t)|^p\ \vee\ \sup_{n\ge1}\sup_{0\le t\le T}\mathbb E|X_n(t)|^p<\infty.0≤t≤Tsup​E∣X(t)∣p ∨ n≥1sup​0≤t≤Tsup​E∣Xn​(t)∣p<∞.
  • Theorem 4 (p. 6): under A-1–A-4 and B-1, sup⁡0≤t≤T∣Xn(t)−X(t)∣→0\sup_{0\le t\le T}|X_n(t)-X(t)|\to0sup0≤t≤T​∣Xn​(t)−X(t)∣→0 in probability.

Significance

Theorem 1 gives Lp\mathcal L^pLp-convergence of a whole class of explicit schemes, with no global Lipschitz condition on either coefficient, for every ppp below the coercivity order p0p_0p0​. In the 3/2-model of the introduction (p1=3.5p_1=3.5p1​=3.5, p0=6p_0=6p0​=6), earlier explicit results gave Lp\mathcal L^pLp-convergence only for p<1/2p<1/2p<1/2 (Hutzenthaler–Jentzen 2015, §4.10.3); Theorem 1 gives it for all p<6p<6p<6. The theorem is also the qualitative base on which the paper's rate results (Theorems 2 and 3, separate missions of this series) are built, and it justifies Monte Carlo estimates of moments computed with such schemes.

The result is proved in the paper. It has, to our knowledge, no machine-checked proof anywhere; Mathlib has Brownian motion but no stochastic integral, and the Itô integral used here is the relational definition published by the Ethier–Kurtz series on this platform. A formal proof needs Itô's formula for ∣x∣p|x|^p∣x∣p, Gronwall's lemma for moment functions, the convergence in probability of Theorem 4 (which the paper cites from Gyöngy–Sabanis rather than proving), and a uniform-integrability argument. Each of these is reusable well beyond this paper.

Difficulty

The natural first idea, estimating E∣X(t)−Xn(t)∣p\mathbb E|X(t)-X_n(t)|^pE∣X(t)−Xn​(t)∣p directly by Itô's formula and Gronwall, fails: under only local monotonicity the difference of drifts cannot be bounded by ∣X−Xn∣|X-X_n|∣X−Xn​∣ with a constant uniform in the state, so the Gronwall constant blows up. The route through convergence in probability and uniform moment bounds is forced, and the hard step is Lemma 2: bounding E∣Xn(t)∣p0\mathbb E|X_n(t)|^{p_0}E∣Xn​(t)∣p0​ uniformly in nnn. The coefficients of the scheme may grow like nαn^\alphanα, and the frozen argument Xn(κn(s))X_n(\kappa_n(s))Xn​(κn​(s)) produces a correction term E∫∣Xn(s)∣p0−2(Xn(s)−Xn(κn(s)))bn ds\mathbb E\int|X_n(s)|^{p_0-2}(X_n(s)-X_n(\kappa_n(s)))b_n\,dsE∫∣Xn​(s)∣p0​−2(Xn​(s)−Xn​(κn​(s)))bn​ds whose control is exactly where the restriction α≤1/2\alpha\le1/2α≤1/2 enters. For fixed nnn finiteness of moments is easy (linear growth); uniformity in nnn is the content.

Formalization scope

States are EuclideanSpace ℝ (Fin d); diffusion values are EuclideanSpace ℝ (Fin d × Fin d₁), whose norm is the Hilbert–Schmidt norm. Time is ℝ≥0; coefficients are uncurried maps on ℝ≥0 × ℝ^d, assumed Borel measurable. An Itô process on [0,T][0,T][0,T] is a measurable process, adapted to the filtration augmented by all PPP-null sets, with continuous paths on [0,T][0,T][0,T], satisfying the integral equation almost surely simultaneously for all t≤Tt\le Tt≤T; the stochastic integral is the platform relation EthierKurtz.HasBrownianItoIntegral, applied coordinatewise with the integrand cut off after TTT. Nothing is required of the processes after TTT, so no existence beyond the horizon is assumed. Right-continuity of the filtration is a hypothesis; completeness is replaced by adaptedness to the augmented filtration, which is weaker, so the formal theorems are at least as strong as the paper's.

The solutions XXX and (Xn)n≥1(X_n)_{n\ge1}(Xn​)n≥1​ are hypotheses, all on one probability space with one Wiener process and one initial value; the theorems do not construct them. Expectations are lower Lebesgue integrals in [0,∞][0,\infty][0,∞] and suprema over ttt are taken in [0,∞][0,\infty][0,∞], so no statement can hold because an expectation or a supremum takes a default value. B-1's integrand, a supremum over an uncountable ball, is required to be a.e. measurable in ttt, as the paper's Lebesgue integral presupposes. The exponent in Theorem 1 and Lemma 2 is restricted to p>0p>0p>0, the paper's convention for Lp\mathcal L^pLp. The dependence clauses "C:=C(T,K,E∣X(0)∣2)C:=C(T,K,\mathbb E|X(0)|^2)C:=C(T,K,E∣X(0)∣2)" (Lemma 1) and "C:=C(p,T,K,E∣X(0)∣p)C:=C(p,T,K,\mathbb E|X(0)|^p)C:=C(p,T,K,E∣X(0)∣p)" (Lemma 2) are not formalized: only finiteness, i.e. a bound independent of nnn, is stated, which is what the proofs establish. Theorem 4 is stated with exactly its printed hypotheses.

A trivializing formalization, in which the moment bounds or the limit hold because the expectation or the supremum defaults to 000, or because the hypotheses on the solutions cannot be met, is ruled out: all quantities live in [0,∞][0,\infty][0,∞], and a sorry-free check shows every hypothesis is satisfiable (zero coefficients, constant solutions).

Contributions welcome: Itô's formula for the platform's integral relation, Burkholder–Davis–Gundy or Doob inequalities for it, a Gronwall lemma for measurable moment functions, and the Gyöngy–Sabanis convergence-in-probability theorem.

Selected references

  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2016. https://arxiv.org/abs/1308.1796 (v4)
  • I. Gyöngy, S. Sabanis, A note on Euler approximations for stochastic differential equations with delay, Appl. Math. Optim. 68, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3131501
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with non-globally Lipschitz continuous coefficients, Ann. Appl. Probab. 22, 2012. https://mathscinet.ams.org/mathscinet-getitem?mr=MR2985171
  • M. Hutzenthaler, A. Jentzen, Numerical approximations of stochastic differential equations with non-globally Lipschitz continuous coefficients, Mem. Amer. Math. Soc. 236(1112), 2015. https://doi.org/10.1090/memo/1112
  • S. Sabanis, A note on tamed Euler approximations, Electron. Commun. Probab. 18, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3070913
  • D. J. Higham, X. Mao, A. M. Stuart, Strong convergence of Euler-type methods for nonlinear stochastic differential equations, SIAM J. Numer. Anal. 40, 2002. https://mathscinet.ams.org/mathscinet-getitem?mr=MR1949404
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AnalysisDifferential GeometryPartial Differential Equations+1·Captain: mikedeng1

Tasty Bits of Several Complex Variables VII: The Dolbeault Lemma on Polydiscs and the Cousin I ProblemTextbook

Motivation

In one complex variable, every smooth function ggg on a disc is ∂ψ/∂zˉ\partial\psi/\partial\bar z∂ψ/∂zˉ of some smooth ψ\psiψ, and this is what makes the Mittag-Leffler theorem work: local principal parts can be glued into a global meromorphic function. In several variables the corresponding equation is the ∂ˉ\bar\partial∂ˉ-problem: given a differential form η\etaη with ∂ˉη=0\bar\partial\eta = 0∂ˉη=0, find ω\omegaω with ∂ˉω=η\bar\partial\omega = \eta∂ˉω=η. Whether it is solvable on a domain U⊂CnU \subset \mathbb{C}^nU⊂Cn is measured by the Dolbeault cohomology groups H(p,q)(U)H^{(p,q)}(U)H(p,q)(U). Their vanishing characterizes domains of holomorphy, and it drives the solution of the additive Cousin I problem, the several-variable Mittag-Leffler problem.

This mission follows §4.4–4.6 of Jiří Lebl's open textbook Tasty Bits of Several Complex Variables (version 4.4, 2026). There the ∂ˉ\bar\partial∂ˉ-problem is solved on polydiscs, from the one-variable Cauchy transform through the Dolbeault–Grothendieck lemma. The result is then applied to the Cousin I problem and to domains of holomorphy. The Dolbeault lemma goes back to P. Dolbeault (1953) and A. Grothendieck. The global theory on pseudoconvex domains is due to Hörmander (An Introduction to Complex Analysis in Several Variables, 1966) and to Cartan's Theorem B.

Setting

Write zk=xk+iykz_k = x_k + i y_kzk​=xk​+iyk​ for the coordinates of Cn\mathbb{C}^nCn. The Wirtinger derivative of a function fff is ∂f/∂zˉk=12(∂f/∂xk+i ∂f/∂yk)\partial f/\partial\bar z_k = \tfrac12(\partial f/\partial x_k + i\,\partial f/\partial y_k)∂f/∂zˉk​=21​(∂f/∂xk​+i∂f/∂yk​).

For strictly increasing tuples α=(α1<⋯<αp)\alpha = (\alpha_1<\dots<\alpha_p)α=(α1​<⋯<αp​) and β=(β1<⋯<βq)\beta = (\beta_1<\dots<\beta_q)β=(β1​<⋯<βq​) in {1,…,n}\{1,\dots,n\}{1,…,n}, write dzα=dzα1∧⋯∧dzαpdz_\alpha = dz_{\alpha_1}\wedge\cdots\wedge dz_{\alpha_p}dzα​=dzα1​​∧⋯∧dzαp​​ and dzˉβ=dzˉβ1∧⋯∧dzˉβqd\bar z_\beta = d\bar z_{\beta_1}\wedge\cdots\wedge d\bar z_{\beta_q}dzˉβ​=dzˉβ1​​∧⋯∧dzˉβq​​. A smooth (p,q)(p,q)(p,q)-form on an open U⊂CnU\subset\mathbb{C}^nU⊂Cn is

η=∑α,βηαβ dzα∧dzˉβ,\eta = \sum_{\alpha,\beta}\eta_{\alpha\beta}\,dz_\alpha\wedge d\bar z_\beta,η=α,β∑​ηαβ​dzα​∧dzˉβ​,

where α\alphaα and β\betaβ run over the increasing ppp- and qqq-tuples and each ηαβ\eta_{\alpha\beta}ηαβ​ is C∞C^\inftyC∞ on UUU. The operator

∂ˉη=∑α,β∑k=1n∂ηαβ∂zˉk dzˉk∧dzα∧dzˉβ\bar\partial\eta = \sum_{\alpha,\beta}\sum_{k=1}^n \frac{\partial\eta_{\alpha\beta}}{\partial\bar z_k}\,d\bar z_k\wedge dz_\alpha\wedge d\bar z_\beta∂ˉη=α,β∑​k=1∑n​∂zˉk​∂ηαβ​​dzˉk​∧dzα​∧dzˉβ​

maps (p,q)(p,q)(p,q)-forms to (p,q+1)(p,q+1)(p,q+1)-forms. A form is ∂ˉ\bar\partial∂ˉ-closed if ∂ˉη=0\bar\partial\eta = 0∂ˉη=0 and ∂ˉ\bar\partial∂ˉ-exact if η=∂ˉω\eta = \bar\partial\omegaη=∂ˉω; by convention the only exact (p,0)(p,0)(p,0)-form is 000. The statement H(p,q)(U)=0H^{(p,q)}(U) = 0H(p,q)(U)=0 means that every smooth ∂ˉ\bar\partial∂ˉ-closed (p,q)(p,q)(p,q)-form on UUU is ∂ˉ\bar\partial∂ˉ-exact.

A possibly unbounded polydisc is a product Δ=D1×⋯×Dn\Delta = D_1\times\cdots\times D_nΔ=D1​×⋯×Dn​ in which each DkD_kDk​ is either a disc {∣zk−ak∣<ρk}\{|z_k - a_k|<\rho_k\}{∣zk​−ak​∣<ρk​} or all of C\mathbb{C}C; for example Cn\mathbb{C}^nCn itself. The finite polydisc is Δr(w)={z:∣zℓ−wℓ∣<rℓ ∀ℓ}\Delta_r(w) = \{z : |z_\ell - w_\ell| < r_\ell\ \forall\ell\}Δr​(w)={z:∣zℓ​−wℓ​∣<rℓ​ ∀ℓ}.

Cousin I data on an open UUU consist of an open covering {Uι}ι∈I\{U_\iota\}_{\iota\in I}{Uι​}ι∈I​ of UUU and holomorphic hικh_{\iota\kappa}hικ​ on Uι∩UκU_\iota\cap U_\kappaUι​∩Uκ​ with hικ+hκι=0h_{\iota\kappa}+h_{\kappa\iota}=0hικ​+hκι​=0 and hικ+hκλ+hλι=0h_{\iota\kappa}+h_{\kappa\lambda}+h_{\lambda\iota}=0hικ​+hκλ​+hλι​=0 on the respective intersections. A solution is a family of holomorphic fιf_\iotafι​ on UιU_\iotaUι​ with hικ=fι−fκh_{\iota\kappa} = f_\iota - f_\kappahικ​=fι​−fκ​. The problem is solvable on UUU if all Cousin I data on UUU have solutions.

In Lean these are wirtingerBar, FormCoeffs, dbar, IsSmoothForm, DolbeaultVanishes, polydisc, IsPossiblyUnboundedPolydisc, IsCousinISolvable and IsDomainOfHolomorphy in the namespace LeblSCV.Dolbeault.

Formalization targets

Goal: Theorem 4.4.5

Let Δ⊂Cn\Delta\subset\mathbb{C}^nΔ⊂Cn be a possibly unbounded polydisc, p≥0p\ge0p≥0, q≥1q\ge1q≥1, and η\etaη a smooth (p,q)(p,q)(p,q)-form on Δ\DeltaΔ with ∂ˉη=0\bar\partial\eta = 0∂ˉη=0. Then there is a smooth (p,q−1)(p,q-1)(p,q−1)-form ω\omegaω on Δ\DeltaΔ with

∂ˉω=ηon Δ,that is,H(p,q)(Δ)=0  (q≥1).\bar\partial\omega = \eta\quad\text{on }\Delta,\qquad\text{that is,}\qquad H^{(p,q)}(\Delta) = 0 \ \ (q\ge1).∂ˉω=ηon Δ,that is,H(p,q)(Δ)=0  (q≥1).

Milestones

  1. Lemma 4.4.6 (for a disc UUU). If ggg is smooth near U‾\overline UU, then ψ(z)=12πi∫Ug(ζ)ζ−z dζ∧dζˉ\psi(z) = \frac{1}{2\pi i}\int_U \frac{g(\zeta)}{\zeta-z}\,d\zeta\wedge d\bar\zetaψ(z)=2πi1​∫U​ζ−zg(ζ)​dζ∧dζˉ​ is smooth on UUU and ∂ψ/∂zˉ=g\partial\psi/\partial\bar z = g∂ψ/∂zˉ=g.
  2. Lemma 4.4.7 (Dolbeault–Grothendieck). If 0<sℓ<rℓ0<s_\ell<r_\ell0<sℓ​<rℓ​, every smooth ∂ˉ\bar\partial∂ˉ-closed (p,q)(p,q)(p,q)-form on Δr(w)\Delta_r(w)Δr​(w), q≥1q\ge1q≥1, is ∂ˉ\bar\partial∂ˉ of a smooth (p,q−1)(p,q-1)(p,q−1)-form on Δs(w)\Delta_s(w)Δs​(w).
  3. Lemma 4.6.4. Smooth Cousin I data on any open set have smooth solutions.
  4. Theorem 4.6.5. On a domain with H(0,1)(U)=0H^{(0,1)}(U)=0H(0,1)(U)=0 the Cousin I problem is solvable.
  5. Corollary 4.6.6. The Cousin I problem is solvable on every possibly unbounded polydisc.
  6. Theorem 4.5.6. A domain U⊂CnU\subset\mathbb{C}^nU⊂Cn with H(0,q)(U)=0H^{(0,q)}(U)=0H(0,q)(U)=0 for 1≤q≤n−11\le q\le n-11≤q≤n−1 is a domain of holomorphy.

Significance

Theorem 4.4.5 is the model case of the vanishing theorem H(p,q)(U)=0H^{(p,q)}(U)=0H(p,q)(U)=0, q≥1q\ge1q≥1, on domains of holomorphy. In particular it solves the ∂ˉ\bar\partial∂ˉ-problem on all of Cn\mathbb{C}^nCn. Through Theorem 4.6.5 it gives the Cousin I problem on polydiscs, and therefore the existence of meromorphic functions with prescribed local principal parts there. Theorem 4.5.6 is one half of the cohomological characterization of domains of holomorphy (Remark 4.5.8, item (viii)). The other half is Cartan's Theorem B, which the book states without proof as Theorem 4.4.2.

All targets are classical and fully proved in the book. As far as a search of the Prove2Me corpus and of Mathlib shows, none of them is formalized. Mathlib has real Fréchet derivatives, smooth bump functions and partitions of unity, and Lebesgue measure on C\mathbb{C}C. It has no bidegree forms, no ∂ˉ\bar\partial∂ˉ operator on forms, no Cauchy transform and no Dolbeault cohomology. This mission builds the (p,q)(p,q)(p,q)-form layer and the first global solvability theorem for ∂ˉ\bar\partial∂ˉ.

Difficulty

The one-variable step needs the Cauchy–Pompeiu formula and differentiation under an integral with a weakly singular kernel. Both the smoothness of ψ\psiψ and the identity ∂ψ/∂zˉ=g\partial\psi/\partial\bar z = g∂ψ/∂zˉ=g require care near ζ=z\zeta = zζ=z.

In several variables, the natural idea is to solve ∂ˉω=η\bar\partial\omega=\eta∂ˉω=η on each of an exhausting sequence of polydiscs and take a limit. It fails as stated: solutions on successive polydiscs differ by ∂ˉ\bar\partial∂ˉ-closed forms and need not converge. For q≥2q\ge2q≥2 the discrepancy has to be corrected exactly, by applying the lemma again with a cutoff. For q=1q=1q=1 the discrepancies are holomorphic functions, and they have to be made small by polynomial approximation, so that the corrected solutions converge. The Dolbeault–Grothendieck lemma loses a little of the polydisc at each step, so the argument has to shrink the polydiscs at each stage.

On the formal side, ∂ˉ\bar\partial∂ˉ on forms carries signs from reordering wedge products. A wrong sign changes which forms are closed. So the sign convention is fixed in the definition and checked against ∂ˉ∘∂ˉ=0\bar\partial\circ\bar\partial = 0∂ˉ∘∂ˉ=0.

Formalization scope

  • Cn\mathbb{C}^nCn is Fin n → ℂ with 0-based indices. Polydiscs use the modulus in each coordinate, as in the book, so the sup norm of Fin n → ℂ agrees with them. No Euclidean ball occurs.
  • A form is a coefficient family FormCoeffs n = Finset (Fin n) → Finset (Fin n) → (Fin n → ℂ) → ℂ: an increasing tuple is the set of its entries, and η A B z is the coefficient of dzA∧dzˉBdz_A\wedge d\bar z_BdzA​∧dzˉB​. IsSmoothForm U p q η requires every coefficient to be ContDiffOn ℝ ∞ on UUU and the coefficients of the wrong bidegree to vanish on UUU. Only values on UUU matter.
  • dbar is Definition 4.4.1 written in the increasing basis. The coefficient of dzA∧dzˉCdz_A\wedge d\bar z_CdzA​∧dzˉC​ is ∑k∈C(−1)∣A∣+#{j∈C:j<k} ∂ηA,C∖{k}/∂zˉk\sum_{k\in C}(-1)^{|A|+\#\{j\in C:j<k\}}\,\partial\eta_{A,C\setminus\{k\}}/\partial\bar z_k∑k∈C​(−1)∣A∣+#{j∈C:j<k}∂ηA,C∖{k}​/∂zˉk​. A sorry-free check confirms that this sign convention makes the mixed second derivatives cancel in ∂ˉ∂ˉη\bar\partial\bar\partial\eta∂ˉ∂ˉη, and that ∂zˉ1/∂zˉ1=1\partial\bar z_1/\partial\bar z_1 = 1∂zˉ1​/∂zˉ1​=1.
  • H(p,q)(U)=0H^{(p,q)}(U)=0H(p,q)(U)=0 is stated as "every closed smooth (p,q)(p,q)(p,q)-form is exact"; the quotient space is not built. The solution ω\omegaω is required to be smooth.
  • Radii of a possibly unbounded polydisc lie in ℝ≥0∞, with ∞\infty∞ meaning the factor C\mathbb{C}C.
  • Holomorphic on an open set is DifferentiableOn ℂ. A domain is an open connected set. Cousin index types range over Type, which loses nothing.
  • Restriction: Lemma 4.4.6 is stated for UUU an open disc. The book allows any bounded open set with piecewise-C1C^1C1 boundary. The disc is the case that the Dolbeault–Grothendieck lemma uses. The measure dζ∧dζˉd\zeta\wedge d\bar\zetadζ∧dζˉ​ is −2i-2i−2i times Lebesgue measure.
  • The goal cannot be trivialized through the form layer. A definition of ∂ˉ\bar\partial∂ˉ with a wrong sign, or one that drops the smoothness of ω\omegaω or the ∂ˉ\bar\partial∂ˉ-closedness of η\etaη, states a different theorem and is ruled out. Hypotheses are satisfiable: η=0\eta = 0η=0 is closed, and Cn\mathbb{C}^nCn is a possibly unbounded polydisc (checked sorry-free).
  • Needed infrastructure: the Cauchy transform and Cauchy–Pompeiu formula, differentiation under the integral with parameters, smooth cutoffs, uniform approximation of holomorphic functions by polynomials on polydiscs, and partitions of unity. The form layer is reusable in later work on the ∂ˉ\bar\partial∂ˉ-problem (balls, Hartogs triangle, pseudoconvex domains). Proofs of ∂ˉ2=0\bar\partial^2 = 0∂ˉ2=0 for the dbar defined here, or of the one-variable lemma for general piecewise-C1C^1C1 domains, are welcome.

Selected references

  • J. Lebl, Tasty Bits of Several Complex Variables, version 4.4, 2026, §4.4–4.6. https://www.jirka.org/scv/
  • L. Hörmander, An Introduction to Complex Analysis in Several Variables, North-Holland Mathematical Library 7, 3rd ed., 1990.
  • P. Dolbeault, Sur la cohomologie des variétés analytiques complexes, C. R. Acad. Sci. Paris 236 (1953), 175–177.
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AnalysisControl TheoryPartial Differential Equations·Captain: mikedeng1

Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks I: Exponential Decay under Delayed Boundary FeedbackResearch Paper

Motivation

Boundary feedback stabilization of the wave equation asks whether a vibrating body at rest on part of its boundary can be brought to rest by a damping law on the rest of its boundary. With the undelayed velocity feedback ∂u/∂ν=−μ1ut\partial u/\partial\nu = -\mu_1 u_t∂u/∂ν=−μ1​ut​, the energy decays exponentially under geometric conditions on the domain; results of this kind go back to Chen (1979, 1981), Lagnese (1983, 1988), Lasiecka and Triggiani (1987), and Komornik and Zuazua (1990).

Real controllers act with a delay, and delays can destroy stability. Datko, Lagnese and Polis (1986) and Datko (1988) showed that an arbitrarily small delay in a boundary feedback that stabilizes the one-dimensional wave equation can make the closed loop unstable. For a feedback made of an undelayed part and a delayed part, μ1ut(t)+μ2ut(t−τ)\mu_1 u_t(t) + \mu_2 u_t(t-\tau)μ1​ut​(t)+μ2​ut​(t−τ), Xu, Yung and Li (2006) proved, by spectral analysis in one space dimension, that the system is stable when μ2<μ1\mu_2 < \mu_1μ2​<μ1​. Nicaise and Pignotti (2006) extended the stability result to bounded domains in any dimension nnn. This mission formalizes that extension: Theorem 1.1 of their paper.

Setting

Let Ω⊂Rn\Omega \subset \mathbb R^nΩ⊂Rn (n≥1n \ge 1n≥1) be a bounded open set whose boundary Γ\GammaΓ is of class C2C^2C2. The boundary is split as Γ=ΓD∪ΓN\Gamma = \Gamma_D \cup \Gamma_NΓ=ΓD​∪ΓN​, with ΓD‾∩ΓN‾=∅\overline{\Gamma_D} \cap \overline{\Gamma_N} = \emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D \ne \emptysetΓD​=∅. Let ν\nuν be the outer unit normal and dΓd\GammadΓ the surface measure on Γ\GammaΓ. Fix the undelayed gain μ1>0\mu_1 > 0μ1​>0, the delayed gain μ2>0\mu_2 > 0μ2​>0 and the delay τ>0\tau > 0τ>0. The problem is

utt−Δu=0in Ω×(0,∞),(1.1)u=0on ΓD×(0,∞),(1.2)∂u∂ν(x,t)=−μ1ut(x,t)−μ2ut(x,t−τ)on ΓN×(0,∞),(1.3)\begin{aligned} u_{tt} - \Delta u &= 0 && \text{in } \Omega \times (0,\infty), &(1.1)\\ u &= 0 && \text{on } \Gamma_D \times (0,\infty), &(1.2)\\ \tfrac{\partial u}{\partial \nu}(x,t) &= -\mu_1 u_t(x,t) - \mu_2 u_t(x,t-\tau) && \text{on } \Gamma_N \times (0,\infty), &(1.3) \end{aligned}utt​−Δuu∂ν∂u​(x,t)​=0=0=−μ1​ut​(x,t)−μ2​ut​(x,t−τ)​​in Ω×(0,∞),on ΓD​×(0,∞),on ΓN​×(0,∞),​(1.1)(1.2)(1.3)​

with initial data u(⋅,0)=u0u(\cdot,0) = u_0u(⋅,0)=u0​ and ut(⋅,0)=u1u_t(\cdot,0) = u_1ut​(⋅,0)=u1​ in Ω\OmegaΩ, and a history ut=f0u_t = f_0ut​=f0​ on ΓN×(−τ,0)\Gamma_N \times (-\tau, 0)ΓN​×(−τ,0) (1.4)–(1.5).

The geometric hypothesis requires a function v∈C2(Ω‾)v \in C^2(\overline\Omega)v∈C2(Ω) and a constant α>0\alpha > 0α>0 with two properties:

⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2(x∈Ω‾, ξ∈Rn),(1.6)\langle D^2 v(x)\xi,\xi\rangle \ge 2\alpha|\xi|^2 \quad (x \in \overline\Omega,\ \xi \in \mathbb R^n), \tag{1.6}⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2(x∈Ω, ξ∈Rn),(1.6) ∇v(x)⋅ν(x)≤0(x∈ΓD).(1.7)\nabla v(x)\cdot\nu(x) \le 0 \quad (x \in \Gamma_D). \tag{1.7}∇v(x)⋅ν(x)≤0(x∈ΓD​).(1.7)

For example, v(x)=∣x∣2v(x) = |x|^2v(x)=∣x∣2 satisfies both on an annulus whose inner sphere is ΓD\Gamma_DΓD​.

Assume the gain condition

μ2<μ1,(1.8)\mu_2 < \mu_1, \tag{1.8}μ2​<μ1​,(1.8)

and fix ξ\xiξ with

τμ2<ξ<τ(2μ1−μ2).(1.10)\tau\mu_2 < \xi < \tau(2\mu_1 - \mu_2). \tag{1.10}τμ2​<ξ<τ(2μ1​−μ2​).(1.10)

The energy of a solution is the standard wave energy plus a term that stores the delayed velocity:

E(t)=12∫Ω{ut2(x,t)+∣∇u(x,t)∣2} dx+ξ2∫ΓN∫01ut2(x,t−τρ) dρ dΓ.(1.9)E(t) = \frac12\int_\Omega \{u_t^2(x,t) + |\nabla u(x,t)|^2\}\,dx + \frac{\xi}{2}\int_{\Gamma_N}\int_0^1 u_t^2(x,t-\tau\rho)\,d\rho\,d\Gamma. \tag{1.9}E(t)=21​∫Ω​{ut2​(x,t)+∣∇u(x,t)∣2}dx+2ξ​∫ΓN​​∫01​ut2​(x,t−τρ)dρdΓ.(1.9)

Formalization targets

Goal: Theorem 1.1 (exponential decay)

There are constants C1,C2>0C_1, C_2 > 0C1​,C2​>0, depending on Ω,ΓD,ΓN,v,α,μ1,μ2,τ,ξ\Omega, \Gamma_D, \Gamma_N, v, \alpha, \mu_1, \mu_2, \tau, \xiΩ,ΓD​,ΓN​,v,α,μ1​,μ2​,τ,ξ but not on the solution, such that every regular solution satisfies

E(t)≤C1E(0) e−C2t∀t≥0.(1.11)E(t) \le C_1 E(0)\, e^{-C_2 t} \qquad \forall t \ge 0. \tag{1.11}E(t)≤C1​E(0)e−C2​t∀t≥0.(1.11)

The constants are existential and are not fixed numerically. Any valid pair proves the goal.

Milestones, in the order the paper's proof uses them

  1. (3.6): the energy identity, which expresses E′(t)E'(t)E′(t) through boundary integrals over ΓN\Gamma_NΓN​ only.
  2. Proposition 3.1: EEE is nonincreasing, and
E′(t)≤−C∫ΓN{ut2(x,t)+ut2(x,t−τ)} dΓ,C=min⁡{μ1−μ22−ξ2τ, −μ22+ξ2τ}>0.E'(t) \le -C\int_{\Gamma_N}\{u_t^2(x,t) + u_t^2(x,t-\tau)\}\,d\Gamma, \qquad C = \min\Big\{\mu_1 - \frac{\mu_2}{2} - \frac{\xi}{2\tau},\ -\frac{\mu_2}{2} + \frac{\xi}{2\tau}\Big\} > 0.E′(t)≤−C∫ΓN​​{ut2​(x,t)+ut2​(x,t−τ)}dΓ,C=min{μ1​−2μ2​​−2τξ​, −2μ2​​+2τξ​}>0.
  1. (3.22): the integrated form E(T)−E(0)≤−C∫0T∫ΓN{ut2(t)+ut2(t−τ)} dΓ dtE(T) - E(0) \le -C\int_0^T\int_{\Gamma_N}\{u_t^2(t) + u_t^2(t-\tau)\}\,d\Gamma\,dtE(T)−E(0)≤−C∫0T​∫ΓN​​{ut2​(t)+ut2​(t−τ)}dΓdt.
  2. Proposition 3.2 (observability): there is T‾>0\overline T > 0T>0 such that for every T>T‾T > \overline TT>T some C0>0C_0 > 0C0​>0 satisfies
E(0)≤C0∫0T∫ΓN{ut2(x,t)+ut2(x,t−τ)} dΓ dt.(3.10)E(0) \le C_0\int_0^T\int_{\Gamma_N}\{u_t^2(x,t) + u_t^2(x,t-\tau)\}\,d\Gamma\,dt. \tag{3.10}E(0)≤C0​∫0T​∫ΓN​​{ut2​(x,t)+ut2​(x,t−τ)}dΓdt.(3.10)
  1. Contraction: there are T>0T > 0T>0 and 0≤C~<10 \le \tilde C < 10≤C~<1 with E(T)≤C~E(0)E(T) \le \tilde C E(0)E(T)≤C~E(0) for every regular solution.

Significance

The theorem shows that adding a delayed component to a stabilizing boundary feedback preserves exponential decay if the delayed gain is dominated by the undelayed gain. It holds in every dimension, under the same geometric condition that governs the undelayed problem. The companion Theorem 1.2 of the same paper shows that the condition μ2<μ1\mu_2 < \mu_1μ2​<μ1​ cannot be removed: when it fails, there are delays for which some solutions keep constant, positive standard energy. The Lyapunov functional (1.9) became a standard device for delayed feedbacks in later work on wave, plate and Timoshenko systems.

The result was proved in 2006. It has no machine-checked proof. This mission produces:

  • a formal statement of the theorem on classical solutions;
  • the energy identity and dissipation inequality with explicit constants;
  • the observability inequality as a separate target, which is the deep analytic input and is reusable by any stabilization argument on the same geometry.

Difficulty

The dissipation inequality (Proposition 3.1) is a calculation: Green's formula, a change of variables in the delay variable ρ\rhoρ, and Young's inequality. The difficulty is entirely in the observability inequality (3.10). The obvious multiplier argument, which multiplies the equation by ∇v⋅∇u\nabla v\cdot\nabla u∇v⋅∇u and integrates, leaves a lower-order term ∥u∥\|u\|∥u∥ that the boundary observation does not control.

The paper removes that term in two steps. The first is a Carleman-type estimate of Lasiecka, Triggiani and Yao (1999), which is where hypotheses (1.6)–(1.7) enter. The second is a compactness–uniqueness argument closed by Holmgren's uniqueness theorem. None of these tools exists in Mathlib, and neither does Green's formula on a curved domain. The final step from a one-period contraction to exponential decay uses time-translation invariance and monotonicity of EEE.

Formalization scope

  • Domain. A MixedDomain n bundles the following:

    • a bounded open set given by a global C2C^2C2 defining function ψ\psiψ (Ω={ψ<0}\Omega = \{\psi < 0\}Ω={ψ<0}, ∂Ω={ψ=0}\partial\Omega = \{\psi = 0\}∂Ω={ψ=0}, ∇ψ≠0\nabla\psi \ne 0∇ψ=0 on ∂Ω\partial\Omega∂Ω);
    • the split ΓD∪ΓN=∂Ω\Gamma_D \cup \Gamma_N = \partial\OmegaΓD​∪ΓN​=∂Ω with disjoint closures and ΓD≠∅\Gamma_D \ne \emptysetΓD​=∅;
    • a finite measure σ\sigmaσ carried by ∂Ω\partial\Omega∂Ω satisfying the Gauss–Green formula for every C1C^1C1 vector field.

    The outer normal is ν=∇ψ/∣∇ψ∣\nu = \nabla\psi/|\nabla\psi|ν=∇ψ/∣∇ψ∣. The Gauss–Green requirement determines σ\sigmaσ uniquely as the surface measure, so the normalization of dΓd\GammadΓ in (1.9) and (1.10) is the paper's.

  • Solutions are real-valued and classical: uuu is one C2C^2C2 function on Rn×R\mathbb R^n \times \mathbb RRn×R. It satisfies (1.1)–(1.3) for t>0t > 0t>0, and its values at t≤0t \le 0t≤0 are the initial data and the history. Time derivatives are one-variable derivatives in ttt, and ∂u/∂ν=∇u⋅ν\partial u/\partial\nu = \nabla u \cdot \nu∂u/∂ν=∇u⋅ν. This is a subclass of the paper's solutions, so the formal theorems are the paper's restricted to smooth, compatible data.

  • Added hypothesis. In Proposition 3.2, the contraction step and the goal, every connected component of Ω\OmegaΩ has a boundary point in ΓD\Gamma_DΓD​ (true whenever Ω\OmegaΩ is connected). The paper's uniqueness step ("−Δw=0-\Delta w = 0−Δw=0, w=0w = 0w=0 on ΓD\Gamma_DΓD​, ∂w/∂ν=0\partial w/\partial\nu = 0∂w/∂ν=0 on ΓN\Gamma_NΓN​, so w≡0w \equiv 0w≡0") needs every component of Ω\OmegaΩ to meet ΓD\Gamma_DΓD​.

  • Strengthened statements. The identity (3.6) and Propositions 3.1 and (3.22) omit hypotheses they do not use. Proposition 3.1 states the explicit constant CCC from the end of its proof.

  • Conventions. Condition (1.10) is strict. The energy is EEE of (1.9), with the delay term, and not the standard energy. Derivatives of EEE are asserted with HasDerivAt.

  • Excluded trivializations. Three things would make the statements empty or different, and none of them is allowed:

    • a free measure in place of the surface measure;
    • the standard energy in place of EEE;
    • replacing (1.11) by E(t)→0E(t) \to 0E(t)→0.

    The degenerate case ΓN=∅\Gamma_N = \emptysetΓN​=∅ is already excluded by (1.6), (1.7) and Gauss–Green together.

  • Infrastructure needed and welcome:

    • Gauss–Green and Green's first identity on MixedDomain;
    • differentiation under the integral over Ω\OmegaΩ and ΓN\Gamma_NΓN​;
    • a Carleman or multiplier observability estimate for the wave equation with mixed boundary conditions;
    • unique continuation (Holmgren) for the wave equation;
    • the elementary lemma turning a one-period contraction plus monotonicity into exponential decay.

    The last lemma and Gauss–Green on C2C^2C2 domains are reusable far beyond this mission.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5) (2006), 1561–1585. https://doi.org/10.1137/060648891
  • G. Q. Xu, S. P. Yung, L. K. Li, Stabilization of wave systems with input delay in the boundary control, ESAIM Control Optim. Calc. Var. 12 (2006), 770–785. https://doi.org/10.1051/cocv:2006021
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24 (1986), 152–156. https://doi.org/10.1137/0324007
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26 (1988), 697–713. https://doi.org/10.1137/0326040
  • I. Lasiecka, R. Triggiani, P. F. Yao, Inverse/observability estimates for second-order hyperbolic equations with variable coefficients, J. Math. Anal. Appl. 235 (1999), 13–57. https://doi.org/10.1006/jmaa.1999.6348
  • V. Komornik, E. Zuazua, A direct method for the boundary stabilization of the wave equation, J. Math. Pures Appl. 69 (1990), 33–54.
  • J. Lagnese, Decay of solutions of wave equations in a bounded region with boundary dissipation, J. Differential Equations 50 (1983), 163–182. https://doi.org/10.1016/0022-0396(83)90073-6
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