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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Introduction to Online Convex Optimization XIII: Blackwell's Approachability Theorem and Online Convex OptimizationTextbook

Motivation

Von Neumann's minimax theorem (Chapter VIII) settles two-player zero-sum games with scalar payoffs. In 1956, Blackwell asked the natural generalization: what can a player guarantee in a repeated game with vector-valued payoffs, where "winning" means driving the average payoff into a target set rather than above a target value? For decades the resulting theory — approachability — and the regret-minimization theory this book develops were believed to be different, with approachability seen as the stronger notion. Chapter 13 closes that gap: approachability and online convex optimization are shown to be algorithmically equivalent, each reducible to the other with no loss of efficiency, and along the way this equivalence yields a constructive, rate-quantified proof of Blackwell's own theorem.

Setting

A generalized vector game (Definition 13.2) is given by bounded convex closed decision sets K1,K2K_1,K_2K1​,K2​ and a vector payoff u:K1×K2→Rdu:K_1\times K_2\to\mathbb R^du:K1​×K2​→Rd. A set SSS is approachable (Definition 13.3) if some non-anticipating algorithm, playing in K1K_1K1​ against any sequence y1,y2,⋯∈K2y_1,y_2,\dots\in K_2y1​,y2​,⋯∈K2​, drives the average payoff's distance to SSS to zero. Blackwell's theorem (13.4) characterizes exactly which SSS are approachable via a purely geometric condition: every column-player strategy yyy admits a row-player best response xxx landing the payoff in SSS.

Section 13.2 constructs an explicit approachability algorithm from any OCO algorithm: given a best-response oracle realizing Blackwell's condition, Algorithm 37 runs the OCO algorithm on the proxy losses ft(w)=w⊤ut−1−hS(w)f_t(w) = w^\top u_{t-1} - h_S(w)ft​(w)=w⊤ut−1​−hS​(w) (the support function hS(w)=max⁡x∈S{w⊤x}h_S(w)=\max_{x\in S}\{w^\top x\}hS​(w)=maxx∈S​{w⊤x} letting distance-to-SSS be written, via Lemma 13.5's minimax duality, as a convex optimization problem over the unit ball), queries the oracle at the OCO algorithm's play wtw_twt​, and averages the resulting rewards.

Formalization targets

Theorem 13.7 (OCO-to-approachability rate, milestone)

Dist(uˉT,S)≤RegretT(A)T.\mathrm{Dist}(\bar u_T, S) \le \frac{\mathrm{Regret}_T(A)}{T}.Dist(uˉT​,S)≤TRegretT​(A)​.

Theorem 13.4 — the mission's goal (sufficiency direction only)

(∀y∈K2, ∃x∈K1, u(x,y)∈S)  ⟹  S is approachable.\big(\forall y\in K_2,\ \exists x\in K_1,\ u(x,y)\in S\big) \implies S\ \text{is approachable}.(∀y∈K2​, ∃x∈K1​, u(x,y)∈S)⟹S is approachable.

Significance

This chapter's headline claim — approachability and OCO are equivalent — is proved in two directions in the book (§13.2 and §13.3); this mission drafts the direction the book itself foregrounds as "the more interesting implication" and constructively proves: any sublinear-regret OCO algorithm converts directly into an explicit approachability algorithm with an explicit convergence rate, giving a self-contained, algorithmic proof of a 1956 game-theory theorem using 1990s–2000s online-learning machinery. Historically, this equivalence resolved a standing misconception (approachability believed strictly stronger) and reframes Blackwell's theorem as a special case of regret minimization rather than a separate theory requiring its own toolkit. No prior art was found on the platform for Blackwell approachability (planning search: q=Blackwell — the one hit, PRNGCompression.prng_no_free_lunch's cousin, an unrelated Rao-Blackwellization result, is not a substitute); this mission drafts both items fresh.

Difficulty

Theorem 13.4's statement is a clean geometric implication, but the book is explicit that its proof is entirely carried by Theorem 13.7 plus an unstated "explicit conclusion" left as an exercise (the passage from a finite-horizon rate bound to the asymptotic Dist → 0 claim, using any of the book's own sublinear-regret OCO algorithms as a witness). Theorem 13.7's own proof combines three nontrivial facts: Lemma 13.5's minimax-duality rewriting of Dist(⋅,S)\mathrm{Dist}(\cdot, S)Dist(⋅,S) as a linear optimization over the unit ball (itself proved via Sion's minimax theorem, not excerpted here), the best-response oracle's defining inequality (13.2) applied pointwise at each round's wtw_twt​, and the OCO algorithm's own regret guarantee applied to the specific proxy-loss sequence ftf_tft​ built from the realized game trajectory — a genuine composition of three separate pieces of machinery from earlier in the book (Chapters III–VIII), not a routine substitution.

Formalization scope

IsApproachable is declared as its own definition (per BRIEF.md's explicit instruction, since Theorem 13.4 depends on it), with the non-anticipation clause made explicit (matching the series' IsOnlineAlgorithm convention from Chunk 03) even though the book's own Definition 13.3 states it only informally ("x_t ← A(y_1,\dots,y_{t-1})"). SupportFunction is h_S exactly as displayed, as a real supremum (a genuine maximum given the chapter's standing "closed, bounded" hypothesis on S). Dist(⋅,S)\mathrm{Dist}(\cdot,S)Dist(⋅,S) throughout is Euclidean distance, rendered as Mathlib's Metric.infDist — confirmed the chapter uses no other distance notion (checked §13.1-13.3 directly, per the pitfall BRIEF.md flags). Theorem 13.7 transcribes Algorithm 37's ft(w)=w⊤ut−1−hS(w)f_t(w)=w^\top u_{t-1}-h_S(w)ft​(w)=w⊤ut−1​−hS​(w) construction faithfully, including its one-round offset (using the previous round's realized reward to build the current round's proxy loss, while the conclusion averages the current round's rewards) — exactly as the book's own pseudocode has it, not smoothed over.

Scope decision on Theorem 13.4's biconditional. The book states Theorem 13.4 as an ↔ but proves, and explicitly flags as proved, only the sufficiency direction (←): "The necessity of this condition is left as an exercise... Our reductions henceforth give an explicit proof of Blackwell's theorem [meaning: of the sufficiency direction]." Per CAPTAIN_BRIEF.md rule 6 and BRIEF.md's explicit instruction, this mission drafts only that direction, named as such in the goal item's own docstring; see STATUS.md.

Not formalized (out of scope for this mission, given the remaining budget and the explicit "exercise" status of several results on these pages): the necessity direction of Theorem 13.4; Lemma 13.5 (minimax duality for Dist, itself relying on Sion's theorem, not separately formalized here); Lemma 13.6 (the equivalent best-response-oracle condition); §13.3's entire approachability-to-OCO direction (Theorem 13.9, Lemma 13.8, the cone/polar-cone machinery of §13.3.1) and §13.3.3 (existence of a best-response oracle for the constructed set); the "explicit conclusion" of Blackwell's theorem from Theorem 13.7, left as an exercise by the book itself.

Selected references

  • E. Hazan, Introduction to Online Convex Optimization, 2nd ed., arXiv:1909.05207v3, Chapter 13.
  • D. Blackwell, "An analog of the minimax theorem for vector payoffs," Pacific Journal of Mathematics 6(1), 1956, 1-8.
  • N. Abernethy, P. Bartlett, E. Hazan, "Blackwell approachability and no-regret learning are equivalent," COLT 2011.
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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Introduction to Online Convex Optimization V: RFTL and the Regret Bound of Follow-the-Regularized-LeaderTextbook

Motivation

Online convex optimization (OCO) asks a learner to repeatedly pick a point in a convex set KKK, pay a cost that an adversary reveals only after the choice is made, and be judged against the best fixed point in hindsight. Chapter III of this series formalized the simplest general-purpose answer, online gradient descent (OGD): take a gradient step, project back onto KKK. OGD's analysis, however, is tied to the Euclidean geometry of the projection step — it treats every coordinate of KKK alike, and its regret bound degrades badly when KKK's natural geometry is not Euclidean (the probability simplex under the ℓ1\ell_1ℓ1​ norm is the standard example, where a Euclidean-projection algorithm's regret scales with n\sqrt{n}n​ in the dimension nnn, while an algorithm that exploits the simplex's own geometry attains regret scaling only with log⁡n\sqrt{\log n}logn​).

Regularized Follow the Leader (RFTL) is the meta-algorithm this chapter introduces to fix this: rather than fixing a specific geometry, RFTL is parameterized by an arbitrary regularization function RRR, and its regret bound depends on RRR only through two scalar quantities the mission makes explicit — the range of RRR over KKK, and a RRR-dependent "local norm" of the gradients. Choosing RRR to match KKK's geometry (entropy regularization on the simplex, for instance) recovers the sharp bounds that plain OGD cannot. RFTL and its close relative Online Mirror Descent (OMD), also introduced here, are the ancestors of essentially every regularization-based online learning algorithm in use today, including the multiplicative-weights/Hedge algorithm of Chapter I as a special case (entropy regularization on the simplex) and the exponentiated-gradient algorithm this book's own Chapter VIII reuses (Corollary 5.7, a further specialization of Theorem 5.2 this mission's Theorem 5.2 underlies). The naive "Follow the Leader" strategy this chapter opens by refuting — always play the empirically best point so far — is a natural first idea and provably fails: the book gives an explicit two-point cost sequence on which it incurs regret linear in the horizon. Regularization is the fix, and quantifying exactly how much it costs and buys is this chapter's content.

Setting

Fix a convex, nonempty decision set KKK in a real inner product space EEE and a sequence of convex cost functions f1,f2,⋯:K→Rf_1, f_2, \dots : K \to \mathbb{R}f1​,f2​,⋯:K→R. As in Chapter III, regret after TTT rounds is

RegretT=∑t=1Tft(xt)−min⁡x⋆∈K∑t=1Tft(x⋆).\mathrm{Regret}_T = \sum_{t=1}^{T} f_t(x_t) - \min_{x^\star \in K} \sum_{t=1}^{T} f_t(x^\star).RegretT​=t=1∑T​ft​(xt​)−x⋆∈Kmin​t=1∑T​ft​(x⋆).

A regularization function R:K→RR : K \to \mathbb{R}R:K→R is a strongly convex, smooth, twice differentiable function with a positive-definite Hessian on the interior of KKK. Its Bregman divergence measures the gap between RRR and its own first-order Taylor approximation:

BR(x∥y)=R(x)−R(y)−∇R(y)⊤(x−y).B_R(x \| y) = R(x) - R(y) - \nabla R(y)^\top(x - y).BR​(x∥y)=R(x)−R(y)−∇R(y)⊤(x−y).

By the mean value theorem, BR(x∥y)=12∥x−y∥z2B_R(x\|y) = \tfrac12\|x-y\|_z^2BR​(x∥y)=21​∥x−y∥z2​ for some point zzz on the segment [x,y][x,y][x,y], where ∥⋅∥z\|\cdot\|_z∥⋅∥z​ is the norm induced by the Hessian ∇2R(z)\nabla^2 R(z)∇2R(z); its dual norm, denoted ∥⋅∥z∗\|\cdot\|_z^*∥⋅∥z∗​, is the local norm at zzz. Writing ∥⋅∥t\|\cdot\|_t∥⋅∥t​ for the local norm between consecutive iterates xt,xt+1x_t, x_{t+1}xt​,xt+1​, the RRR-diameter of KKK is DR2=max⁡x,y∈K(R(x)−R(y))D_R^2 = \max_{x,y\in K}(R(x)-R(y))DR2​=maxx,y∈K​(R(x)−R(y)).

The RFTL algorithm (Algorithm 13), with step size η>0\eta > 0η>0, plays x1=arg⁡min⁡x∈KR(x)x_1 = \arg\min_{x\in K} R(x)x1​=argminx∈K​R(x), then at every round updates

xt+1=arg⁡min⁡x∈K{η∑s=1t∇s⊤x+R(x)},∇t:=∇ft(xt).x_{t+1} = \arg\min_{x \in K}\Big\{\eta \sum_{s=1}^{t} \nabla_s^\top x + R(x)\Big\}, \qquad \nabla_t := \nabla f_t(x_t).xt+1​=argx∈Kmin​{ηs=1∑t​∇s⊤​x+R(x)},∇t​:=∇ft​(xt​).

The agile Online Mirror Descent algorithm (Algorithm 14, agile version) instead maintains a dual point yty_tyt​ with ∇R(y1)=0\nabla R(y_1) = 0∇R(y1​)=0, updates it by ∇R(yt+1)=∇R(xt)−η∇t\nabla R(y_{t+1}) = \nabla R(x_t) - \eta \nabla_t∇R(yt+1​)=∇R(xt​)−η∇t​, and projects via the Bregman divergence, xt+1=arg⁡min⁡x∈KBR(x∥yt+1)x_{t+1} = \arg\min_{x\in K} B_R(x\|y_{t+1})xt+1​=argminx∈K​BR​(x∥yt+1​) (with x1x_1x1​ defined the same way from y1y_1y1​). RFTL and the lazy variant of OMD coincide for linear costs (Lemma 5.5, not formalized here — it is not used by either target); the agile variant's analysis is genuinely different and is the mission's second target.

Formalization targets

Target (Theorem 5.2 — RFTL's regret bound)

RegretT  ≤  2η∑t=1T∥∇t∥t∗2  +  R(u)−R(x1)η,for every u∈K.\mathrm{Regret}_T \;\le\; 2\eta \sum_{t=1}^{T} \|\nabla_t\|_t^{*2} \;+\; \frac{R(u) - R(x_1)}{\eta}, \qquad \text{for every } u \in K.RegretT​≤2ηt=1∑T​∥∇t​∥t∗2​+ηR(u)−R(x1​)​,for every u∈K.

This is the mission's goal: RFTL, run with any admissible regularizer, attains a regret bound governed only by the cumulative squared local norm of the gradients and RRR's range over KKK. The bound is proved via two milestones: Lemma 5.3 (regret controlled by the total "prediction drift" ∑t∇t⊤(xt−xt+1)\sum_t \nabla_t^\top(x_t - x_{t+1})∑t​∇t⊤​(xt​−xt+1​) plus DR2/ηD_R^2/\etaDR2​/η), which in turn rests on Lemma 5.4 (a "follow-the-leader beats be-the-leader" comparison inequality, proved by induction on the horizon).

Further target (Theorem 5.6 — agile OMD's regret bound)

RegretT  ≤  η4∑t=1T∥∇t∥t∗2  +  R(u)−R(x1)2η,for every u∈K.\mathrm{Regret}_T \;\le\; \frac{\eta}{4} \sum_{t=1}^{T} \|\nabla_t\|_t^{*2} \;+\; \frac{R(u) - R(x_1)}{2\eta}, \qquad \text{for every } u \in K.RegretT​≤4η​t=1∑T​∥∇t​∥t∗2​+2ηR(u)−R(x1​)​,for every u∈K.

A structurally similar bound for the agile variant, included as its own goal-level item since — as the book states explicitly — its proof technique is unrelated to RFTL's, not a corollary of it.

Both targets are the book's own tightest, non-asymptotic statements: neither is weakened to an O(⋅)O(\cdot)O(⋅) form, and the book's own further (unnumbered) corollary specializing Theorem 5.2 to a uniform local-norm bound ∥∇t∥t∗≤GR\|\nabla_t\|_t^* \le G_R∥∇t​∥t∗​≤GR​ is left out, matching this series' convention of formalizing only the numbered results.

Significance

The results themselves. Theorem 5.2 is the general regret theorem behind every regularization scheme in online learning: instantiating RRR recovers the projected-gradient bound of Chapter III (Euclidean RRR), the multiplicative-weights bound of Chapter I (entropy RRR on the simplex), and — through the exponentiated-gradient specialization (Corollary 5.7, not itself a target here) — the row-player regret bound this book's own Chapter VIII cites as "Eq. (8.1)" in its reduction of zero-sum games to regret minimization. Theorem 5.6 gives the same guarantee for an algorithm (agile OMD) that, unlike RFTL, maintains a feasible point at every round, which the book notes is preferable in the adaptive-regret setting of Chapter X.

Formalizing it. Both theorems have complete, elementary proofs in the source (no gaps, no "with high probability", no hidden regularity conditions); the mission's work is converting the analytic argument — the Bregman-divergence identity, the generalized Cauchy-Schwarz inequality bounding the drift term by the local norm, and the two induction arguments underlying Lemma 5.4 — into machine-checked statements. No formalization of RFTL, OMD, or the local-norm machinery exists on the platform (checked below); the closest Formalpedia entries state a related but distinctly narrower result.

Difficulty

The central obstacle is that the regularizer RRR is a hypothesis, not a fixed function: the theorem must hold for every admissible RRR simultaneously, so nothing about RRR beyond its stated properties (strong convexity, smoothness, twice differentiability) may be used. A newcomer's first instinct — bound the local norm ∥∇t∥t∗\|\nabla_t\|_t^*∥∇t​∥t∗​ by a fixed multiple of the Euclidean dual norm ∥∇t∥2\|\nabla_t\|_2∥∇t​∥2​ — fails in general and is exactly the bound RFTL is designed to avoid needing; the whole point of the local-norm formulation is that it can be tight for regularizers (like entropy) whose Hessian is very far from a multiple of the identity. A second obstacle is Lemma 5.4's induction, which compares xt+1x_{t+1}xt+1​ (a minimizer over t+1t+1t+1 terms) against uuu using the minimality of xt+1x_{t+1}xt+1​ at exactly the right instantiation — an argument that looks almost circular until the induction hypothesis is applied at u=xt+2u = x_{t+2}u=xt+2​, not at the theorem's free variable.

Formalization scope

KKK ranges over an arbitrary real, complete inner product space (a real Hilbert space), matching Chapters III and IV, not a fixed Rn\mathbb{R}^nRn. The RFTL and agile-OMD update rules are represented relationally (IsArgMinOn), since Mathlib has no canonical argmin operator for a general convex set — mirroring IsMetricProjection's precedent from Chapter III. The Hessian at the mean-value-theorem's intermediate point is represented via the second Fréchet derivative of RRR's gradient map (HasFDerivAt), since Mathlib has no dedicated Hessian type; the local dual norm is then any value satisfying the resulting existential characterization (IsLocalDualNormSq), stated once and shared by both targets. A boundedness hypothesis on RRR over KKK is added to Lemma 5.3's statement to keep the RRR-diameter DR2D_R^2DR2​ from collapsing to Mathlib's junk value for an unbounded supremum — a condition every regularizer the book actually uses (strongly convex and smooth over a bounded KKK) already satisfies, so it narrows nothing.

Trivializing formalization ruled out. A regret bound stated for an "algorithm" defined loosely enough to include the after-the-fact optimal choice would be vacuous; IsRFTLRun and IsOMDAgileRun instead pin down the exact history-dependent update rule of Algorithms 13 and 14 (the current gradient sequence, the current regularizer, and nothing else) as a hypothesis, so a proof must genuinely use the specific update. Theorem 5.2 and Theorem 5.6 are kept as two separate items rather than one theorem parameterized by an algorithm choice, since — per the chapter's own remark that their analyses are unrelated — a merged statement would either need to branch internally on the algorithm or silently identify two genuinely different update rules.

Reuse and prior art. OnlineConvexOpt.FirstOrder.RegretT (Chapter III, published) is imported and reused verbatim, keeping the regret functional identical across the whole book. Definitions specific to Chapter IV (OnlineConvexOpt.SecondOrder, not yet published) are not imported per this series' convention that a draft cannot import another draft; quadForm is redeclared locally instead. On the platform, BanditAlgorithm.ftrl_regret_bound, BanditAlgorithm.mirror_descent_regret_bound, and BanditAlgorithm.ftrl_simplex_exp_weights_regret (the Bandit Algorithms series, Chapter XII) state regret bounds for FTRL and Mirror Descent in the linear-cost, bandit-idiom setting (a fixed linear loss ⟨a,yt⟩\langle a, y_t\rangle⟨a,yt​⟩ at each round, regret compared via a Bregman-divergence potential at fixed points). Hazan's Theorem 5.2 and 5.6 are for general convex ftf_tft​ and use the book's own local-norm object, which has no counterpart in those statements; they are read in full and are not faithful substitutes (different hypothesis class), so this mission drafts its own, independent items rather than reusing them.

Selected references

  • Hazan, Introduction to Online Convex Optimization, 2nd ed., Chapter 5. arXiv:1909.05207v3
  • Shalev-Shwartz, Online Learning and Online Convex Optimization, Foundations and Trends in Machine Learning, 2012 (surveys RFTL/Mirror Descent under the name "Online Mirror Descent"). https://doi.org/10.1561/2200000018
  • Zinkevich, Online Convex Programming and Generalized Infinitesimal Gradient Ascent, ICML 2003 (the Euclidean special case this chapter generalizes). https://www.aaai.org/Papers/ICML/2003/ICML03-120.pdf
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Machine LearningReinforcement LearningStatistics·Captain: mikedeng1

Foundations of Reinforcement Learning V: General Decision Making and the Decision-Estimation Coefficient Lower BoundTextbook

Motivation

Online decision-making problems — multi-armed bandits, contextual bandits, structured bandits, and episodic reinforcement learning — look superficially different but share a common shape: a learner repeatedly acts, observes feedback, and is scored by regret against the best action in hindsight. Foster, Kakade, Qian and Rakhlin's Foundations of Reinforcement Learning and Interactive Decision Making (Foster & Rakhlin, arXiv:2312.16730v1) develops a unifying account of this shape and asks a sharper question than "does this specific algorithm work?": for a given class of possible environments, what is the best regret any algorithm can achieve? The Decision-Estimation Coefficient (DEC), introduced by Foster, Kakade, Qian and Rakhlin (2021, "The Statistical Complexity of Interactive Decision Making") and refined by Foster, Golowich, Qian, Rakhlin and Sekhari (2023), was proposed as the answer: a single real-valued complexity measure of a model class that simultaneously (i) drives a generic optimal-up-to-constants algorithm (Estimation-to-Decisions, E2D), and (ii) lower-bounds the regret of every algorithm. Item (ii) is what turns the DEC from "a complexity measure that happens to work for the algorithms we know" into a genuine characterization of statistical difficulty, in the same sense that minimax rates characterize the difficulty of estimation problems in classical statistics. This mission formalizes that lower bound.

Setting

Chapter 6 of the book (pp. 93–128) introduces Decision Making with Structured Observations (DMSO), a protocol general enough to subsume the contextual-bandit, structured-bandit and episodic tabular-RL protocols of earlier chapters. Over TTT rounds, the learner selects a decision πt\pi_tπt​ from a decision space Π\PiΠ; nature draws a reward-observation pair (rt,ot)(r_t, o_t)(rt​,ot​) from a fixed, unknown model M⋆(⋅∣πt)M^\star(\cdot \mid \pi_t)M⋆(⋅∣πt​), where a model MMM maps each decision to a distribution over a reward space RRR and an observation space OOO. The learner has access to a model class M\mathcal{M}M containing M⋆M^\starM⋆ (realizability). For M∈MM \in \mathcal{M}M∈M, write fM(π):=EM,π[r]f^M(\pi) := \mathbb{E}_{M,\pi}[r]fM(π):=EM,π​[r] for the mean reward function and πM:=arg⁡max⁡πfM(π)\pi_M := \arg\max_\pi f^M(\pi)πM​:=argmaxπ​fM(π) for the optimal decision; regret is Reg:=∑t=1TfM⋆(πM⋆)−Eπt∼pt[fM⋆(πt)]\mathrm{Reg} := \sum_{t=1}^T f^{M^\star}(\pi_{M^\star}) - \mathbb{E}_{\pi_t \sim p_t}[f^{M^\star}(\pi_t)]Reg:=∑t=1T​fM⋆(πM⋆​)−Eπt​∼pt​​[fM⋆(πt​)], exactly as in the bandit chapters, now for the general model class.

Because observations, not just mean rewards, now carry information, the DEC needs a way to measure distance between the full conditional distributions M(π)M(\pi)M(π) and M^(π)\hat M(\pi)M^(π), not just between scalars fM(π)f^M(\pi)fM(π) and fM^(π)f^{\hat M}(\pi)fM^(π). The chapter uses the squared Hellinger distance DH2D_H^2DH2​, one of a family of Csiszár fff-divergences that also includes total variation (DTVD_{TV}DTV​) and Kullback-Leibler (DKLD_{KL}DKL​) divergence. For a reference model M^\hat MM^ and scale γ>0\gamma > 0γ>0, the general Decision-Estimation Coefficient is the min-max game value

decγ(M,M^):=inf⁡p∈Δ(Π)sup⁡M∈MEπ∼p[fM(πM)−fM(π)−γ⋅DH2(M(π),M^(π))],\mathrm{dec}_\gamma(\mathcal{M}, \hat M) := \inf_{p \in \Delta(\Pi)} \sup_{M \in \mathcal{M}} \mathbb{E}_{\pi \sim p}\bigl[f^M(\pi_M) - f^M(\pi) - \gamma \cdot D_H^2(M(\pi), \hat M(\pi))\bigr],decγ​(M,M^):=p∈Δ(Π)inf​M∈Msup​Eπ∼p​[fM(πM​)−fM(π)−γ⋅DH2​(M(π),M^(π))],

and decγ(M):=sup⁡M^∈co(M)decγ(M,M^)\mathrm{dec}_\gamma(\mathcal{M}) := \sup_{\hat M \in \mathrm{co}(\mathcal{M})} \mathrm{dec}_\gamma(\mathcal{M}, \hat M)decγ​(M):=supM^∈co(M)​decγ​(M,M^). This mission's Lean development (FoundationsRL.GeneralDM) formalizes discrete versions of DTVD_{TV}DTV​, DH2D_H^2DH2​, DKLD_{KL}DKL​ for a finite outcome type, the DMSO regret, and this DEC.

Formalization targets

The goal is Proposition 28 (DEC Lower Bound), p. 105:

∃ c>0 (sufficiently small):∀ T with decεTc(M)≥10 εT,  εT:=c/T,  ∀ algorithm  p,  ∃ M∈M:regret(M,p)≥120 decεTc(M)⋅T.\exists\, c > 0 \text{ (sufficiently small)} : \forall\, T \text{ with } \mathrm{dec}^c_{\varepsilon_T}(\mathcal{M}) \ge 10\,\varepsilon_T,\; \varepsilon_T := c/\sqrt{T},\; \forall\, \text{algorithm}\; p,\; \exists\, M \in \mathcal{M} : \mathrm{regret}(M, p) \ge \tfrac{1}{20}\, \mathrm{dec}^c_{\varepsilon_T}(\mathcal{M}) \cdot T.∃c>0 (sufficiently small):∀T with decεT​c​(M)≥10εT​,εT​:=c/T​,∀algorithmp,∃M∈M:regret(M,p)≥201​decεT​c​(M)⋅T.

Here decεc\mathrm{dec}^c_\varepsilondecεc​ is the constrained DEC (§6.5.1), a variant of the offset DEC above that hard-constrains the information gain rather than subtracting it — a technical refinement needed to make the lower-bound direction go through — and the "localization condition" decεTc(M)≥10εT\mathrm{dec}^c_{\varepsilon_T}(\mathcal{M}) \ge 10\varepsilon_TdecεT​c​(M)≥10εT​ is a genuine hypothesis of the proposition, not a footnote. Unlike almost every other target in this series of missions, the statement quantifies over every algorithm rather than naming one: it is a genuine impossibility result. Two supporting divergence facts are included as milestones because the DEC's information-theoretic argument rests on them: Lemma 19 (DTV2≤DH2≤DKLD_{TV}^2 \le D_H^2 \le D_{KL}DTV2​≤DH2​≤DKL​) and Lemma 20 (a bounded-likelihood-ratio refinement bounding DKLD_{KL}DKL​ in terms of DH2D_H^2DH2​). The chapter's own matching upper bound, Proposition 26 (the E2D regret bound for the general DMSO protocol, the direct analogue of Chapter 4's Proposition 13), is included as a milestone to give the reader the matching pair the chapter presents together. Finally, Corollary 1 restates the lower bound in terms of the localized offset DEC (combining Proposition 28 with Proposition 27), included as a milestone showing the lower bound's reach beyond the constrained DEC alone.

Significance

Proposition 28 is what makes the DEC a genuine characterization of the statistical complexity of interactive decision making, rather than merely a sufficient condition for a particular algorithm family to succeed. Combined with the (uncited, technically deeper) matching upper bound for the constrained DEC — Proposition 29, stated but not proved in the book — it shows that for any finite model class, the constrained DEC is necessary and sufficient for low regret up to a log⁡∣M∣\sqrt{\log|\mathcal{M}|}log∣M∣​ factor in the localization radius: no complexity measure that is substantially different from the DEC can characterize the same problems. This is the general decision-making analogue of how minimax rates pin down statistical estimation, now for interactive protocols with adaptive feedback.

Formalizing the lower bound is new work: no result of this shape exists on the Prove2Me platform (searches for "decision-estimation", "general divergence", "constrained DEC" and "Hellinger" — the last of which surfaces two related-but-distinct affinity/Le Cam bounds from a different mission on bandit lower bounds — return no faithful prior art; see MODERATION_NOTES.md). The formal statement is the boxed proposition; the book gives a self-contained but simplified proof (two named simplifying assumptions, §6.5.3) and cites Foster, Golowich, Qian, Rakhlin & Sekhari (2023) for the unrestricted argument. This mission's Lean items are draft statements (:= by sorry), not proofs; formalizing the proof itself — a two-point adaptive testing argument using the chain rule for KL divergence and a change-of-measure step — is the open contribution this mission proposes.

Difficulty

The obvious first attempt is to try to prove the lower bound by exhibiting one fixed pair of hard models M,M^M, \hat MM,M^, as in classical two-point minimax lower bounds (Le Cam's method, Fano's inequality). This fails here because the decision-making protocol is interactive and adaptive: the algorithm's queries depend on what it has observed, so a model pair chosen obliviously (before seeing the algorithm) cannot in general be made indistinguishable to every algorithm — an adaptive algorithm can be constructed that distinguishes any two fixed models quickly by querying where they differ. The book's proof instead selects the "hard" alternative model MMM as a function of the algorithm's own strategy (via the constrained DEC's arg max, Eq. (6.36)), so that the pair is hard specifically for the algorithm under consideration, then uses the chain rule for KL divergence plus the change-of-measure identity between the algorithm's induced distributions under MMM and M^\hat MM^ to conclude that the algorithm's realized decisions must look similar under both models — hence it cannot get low regret on both simultaneously. Every step of this argument depends on the exact game structure of the constrained DEC, not just its numerical value; a formalization that leaves decεc\mathrm{dec}^c_\varepsilondecεc​ as an unconstrained real parameter (rather than the actual inf⁡\infinf-sup⁡\supsup game with its information-gain constraint) would make the lower bound's conclusion vacuous, since the hypothesis decεTc(M)≥10εT\mathrm{dec}^c_{\varepsilon_T}(\mathcal{M}) \ge 10\varepsilon_TdecεT​c​(M)≥10εT​ would no longer track any actual property of M\mathcal{M}M.

Formalization scope

The decision space Π\PiΠ and the outcome (reward, observation) alphabet YYY are both taken as finite types (Fintype); a model m:Π→Y→Rm : \Pi \to Y \to \mathbb{R}m:Π→Y→R is a conditional probability vector, and a reward-extraction map rew:Y→R\mathrm{rew} : Y \to \mathbb{R}rew:Y→R recovers the mean reward fm(π)=∑ym(π)(y)⋅rew(y)f^m(\pi) = \sum_y m(\pi)(y)\cdot\mathrm{rew}(y)fm(π)=∑y​m(π)(y)⋅rew(y). hellingerSq, totalVariationDiscrete, klDivDiscrete specialize the book's general dominating-measure divergence formula (Eq. (6.5)) to the counting measure on this finite type; klDivDiscrete returns an ENNReal so its +∞+\infty+∞ case (when PPP is not absolutely continuous w.r.t. QQQ) is represented honestly. The DEC, the constrained DEC and the localized subclass are literal sInf-of-sSup/sSup-of-sSup transcriptions of the book's min-max games — the same convention this series uses for the Chapter-4 DEC — not opaque free real numbers, which rules out the trivializing formalization named above.

Three deviations from this series' usual convention of pinning every constant to the value the book's own proof derives are deliberate and disclosed. First, the numerical constant ccc in εT:=c/T\varepsilon_T := c/\sqrt{T}εT​:=c/T​ is explicitly called "not important" by the authors themselves (footnote a, p. 105); it is existentially quantified (∃ c > 0) rather than pinned to a numeral. Second — added at moderation, round 2, 2026-09-19, after the constant was found to be pinned incorrectly — the lower bound's own multiplicative constant is also existentially quantified (∃ c' > 0) rather than pinned to 1/20. The book's printed proof (§6.5.3, pp. 107–110) derives 1/20 (p. 110, not p. 109 as an earlier draft of this mission stated) only under two named simplifying assumptions the theorem's hypotheses do not carry (p. 107, "Simplifications": a class-wide bounded-curvature hypothesis, Eq. (6.34); and a bound on the unaugmented sup⁡M^∈Mdeccε(M,M^)\sup_{\hat M\in\mathcal M}\mathrm{decc}_\varepsilon(M,\hat M)supM^∈M​deccε​(M,M^) rather than the officially-defined, augmented deccε(M)=sup⁡M^∈co(M)deccε(M∪{M^},M^)\mathrm{decc}_\varepsilon(M) = \sup_{\hat M\in\mathrm{co}(\mathcal M)} \mathrm{decc}_\varepsilon(M\cup\{\hat M\},\hat M)deccε​(M)=supM^∈co(M)​deccε​(M∪{M^},M^) this mission's decC implements). Since augmenting either supremum's domain can only raise its value, the printed proof's bound on the narrower, unaugmented quantity does not license a pinned 1/20 against the fully general decC this theorem states; the book itself attributes the proof of the general statement to an external reference (Foster, Golowich, Qian, Rakhlin & Sekhari 2023) not in this document. The existential c' matches the book's own unpinned ≳\gtrsim≳ for Proposition 28 as printed on pp. 105–106. Third, "any algorithm" and E[Reg(T)]\mathbb{E}[\mathrm{Reg}(T)]E[Reg(T)] are formalized, as throughout this series, without a full stochastic-process/history model: regret is a deterministic quantity evaluated at a fixed realized decision-distribution sequence p:Fin T→Π→Rp : \mathrm{Fin}\,T \to \Pi \to \mathbb{R}p:FinT→Π→R, rather than an expectation over an adaptive, history-dependent algorithm's own randomness. Formalizing the fully adaptive, measure-theoretic version of "any algorithm" — with an explicit filtration and expectation over the induced process law PMP_MPM​ — is future work a solver could add; the current statement is faithful to the book's deterministic-per-realization content but not to its full generality over randomized, history-dependent strategies. The DMSO protocol (Def_FoundationsRL_GeneralDM_Protocol) and the DEC (Def_FoundationsRL_GeneralDM_DEC) are restated locally rather than imported from Chapter 4's mission (FoundationsRL.Structured), since draft items cannot import another chunk's drafts; contributions extending either mission to reuse the other's substrate once both are published are welcome.

Selected references

  • Foster, D. J., Kakade, S. M., Qian, J., & Rakhlin, A. (2023). Foundations of Reinforcement Learning and Interactive Decision Making. arXiv:2312.16730.
  • Foster, D. J., Kakade, S. M., Qian, J., & Rakhlin, A. (2021). The Statistical Complexity of Interactive Decision Making. arXiv:2112.13487.
  • Foster, D. J., Golowich, N., Qian, J., Rakhlin, A., & Sekhari, A. (2023). A Unified Model and Dimension for Interactive Estimation. arXiv:2306.06184.
  • Polyanskiy, Y., & Wu, Y. Information Theory: From Coding to Learning. Cambridge University Press (draft edition cited by the book as [68]).
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Introduction to Stochastic Programming VIII: Multistage Jensen Bounds and AggregationTextbook

Motivation

A multistage stochastic program's exact deterministic equivalent grows exponentially with the number of periods, even when each period's random data takes only a handful of values (Chapter 9's concern was the growth in the number of realizations; Chapter 10 adds growth in the number of periods). One remedy, generalizing Chapter 8's single-period Jensen bound, is to replace the exact per-period random data by a coarser, aggregated version — conditional expectations over a partition of the history space at each stage — and solve the resulting smaller deterministic equivalent instead. This is only useful if the aggregated problem's optimal value is provably a bound (here, a lower bound) on the exact problem's, and Birge & Louveaux's Chapter 10, §10.1, Theorem 1 is exactly the statement that makes this legitimate, together with a genuinely necessary extra condition the book states explicitly two paragraphs before the theorem: "if not [i.e. if the extra condition fails], then the conditional expectation form ... may not actually achieve a bound." This mission formalizes that theorem.

Setting

The book's exact multistage stochastic linear program (Eq. 1.1, p. 418) is

min c¹x¹ + E_Ω[c²x² + ⋯ + cᴴxᴴ]
s.t. W¹x¹ = h¹,  Tᵗ⁻¹xᵗ⁻¹ + Wᵗxᵗ = hᵗ (t=2,…,H, a.s.),  xᵗ ≥ 0 a.s., xᵗ nonanticipative (Σᵗ-measurable),

over the exact event space Ω = Ω₁ × ⋯ × Ω_H. Given a consistent nested partition of each Ωᵗ = Ω₁ × ⋯ × Ωₜ into finitely many blocks Sᵗ₁, …, Sᵗ_νₜ, and aggregated data (h̄ᵗᵢ, T̄ᵗᵢ) = E^{Sᵗᵢ}[(hᵗ,Tᵗ)] (the conditional expectation of the true random data over block i), the aggregated problem (Eq. 1.2, p. 419) replaces the exact recursion by a finite tree of blocks, one decision per block, linked to its parent block's decision. Both (1.1) and (1.2) are, structurally, the same kind of object — a finite-tree deterministic-equivalent recourse LP — differing only in which tree and which node data they use; this mission formalizes that shared shape once (Tree, Instance, Feasible, obj) and instantiates it twice.

Formalized as: a shared Tree H structure (a finite node type, per-node stage, anc, and a root), the same representation Chunk 06's Multistage.Tree uses for the exact scenario tree of its own (different) chapter, restated here rather than imported (a draft cannot import another chunk's draft). An Instance H n m T bundles a tree's node-varying LP data (c, W, Tmat, h, p); Feasible/obj give its feasible set and objective. The exact problem (1.1) is Instance H n m TFine for a fine/exact tree TFine; the aggregated problem (1.2) is Instance H n m TCoarse for a coarser tree TCoarse, connected to TFine by an aggregation map agg : TFine.Node → TCoarse.Node.

Formalization targets

Goal — Chapter 10, Theorem 1 (p. 419)

agg respects the tree structure (root, stage, ancestor);
W, c agree between the fine and coarse instances (up to agg);
coarse.h, coarse.Tmat are the p-weighted conditional expectations of fine.h, fine.Tmat over
  each aggregation fiber;
∀ coarse nodes i,i' at the same stage sharing a "current-period outcome",
  coarse.h i = coarse.h i' ∧ coarse.Tmat i = coarse.Tmat i'
  ⟹ zCoarse ≤ zFine

This is the mission's only formalization target: BRIEF.md records that no separately numbered lemma precedes Theorem 1's proof in this section to serve as an independent milestone (the proof is a direct LP-duality argument against the theorem's own hypotheses), and that Chapter 8's Theorem 1 — the two-period case this theorem generalizes — is a cross-chapter dependency belonging to Chunk 08's own mission, not a milestone here. milestones.yaml is accordingly empty; see STATUS.md for the explicit accounting of what else in this chapter was considered and left out (Theorem 3, the aggregation error bound of §10.2, an unrelated and substantially heavier result).

Significance

Theorem 1 is what licenses every aggregation-based approximation scheme the rest of the book's multistage material builds on: it says precisely when replacing a multistage recourse problem's random data by within-period conditional expectations preserves a valid lower bound, and precisely identifies the condition (aggregated nodes sharing a current-period outcome must carry identical aggregated data) whose failure breaks the bound — a condition the book states is not decorative ("if not, then the conditional expectation form ... may not actually achieve a bound," p. 418). Formalizing it gives Prove2Me a first structural result connecting Chapter 8's single-period Jensen bound (Chunk 08) to genuinely multistage approximation, using the same finite-scenario-tree deterministic-equivalent representation Chunk 06 uses for the exact nested Benders decomposition — the two missions' shared representation choice (documented in both STATUS.md files) means a future mission relating them formally (e.g. instantiating Chunk 06's exact tree as this mission's TFine) has a compatible object to work with, even though neither imports the other's draft.

Difficulty

The theorem's proof (p. 419-420) is a direct LP weak-duality argument: given an optimal dual solution to the aggregated problem, the book constructs a dual-feasible solution to the exact problem attaining the same value, using precisely the "common outcome ⟹ equal aggregated data" hypothesis to make the constructed dual solution well-defined across the exact tree's finer structure. This is a real argument, not a citation, but it is left as sorry: formalizing the proof would need the multistage LP duality machinery (the "multistage version of Theorem 3.13" the book's own proof invokes, itself left as Exercise 1) that no chunk of this series has built. The value of this mission is the faithful statement of the bound and its exact hypotheses.

Formalization scope

  • The book's own printed typo, resolved and documented. Theorem 1's hypothesis clause reads, as printed, "such that (ωt−1,ωt) ∈ Stj if and only if there exist some (ω̂t−1,ωt) ∈ Stj" — S^t_j appears on both sides of the "if and only if," where the sentence's own subject ("S^t_i and S^t_j that have a common outcome") requires the left side to range over S^t_i. Confirmed against a direct render of PDF page 436 (uv run --with pymupdf python), not assumed from OCR: the PDF's own typesetting has this repetition, not an artefact of text extraction. This formalization reads the corrected clause as "S^t_i and S^t_j project onto the same set of period-t outcomes" and states it via an explicit label type Θ and curOutcome : TCoarse.Node → Θ, since the aggregated tree alone does not carry a literal per-period outcome space to project onto (see Setting above — Tree records only history-node structure, not the underlying product space Ω = Ω₁ × ⋯ × Ω_H).
  • W, c shared exactly, not aggregated, matching the book's explicit assumption that the recourse matrix and per-stage cost are deterministic and identical across (1.1) and (1.2) ("Wt known and not random," "ct = ct," p. 418) — formalized as direct equality hypotheses (hW_agree, hc_agree) rather than folding W/c into the conditional-expectation machinery that h/Tmat go through.
  • zFine/zCoarse are hypothesis-characterized, not sInf-defined, avoiding the real infimum's junk value 0 on an unbounded-below or empty feasible set (reference/FAITHFULNESS_TRAPS.md trap 5) — neither tree-LP's feasible set is shown bounded or nonempty by the hypotheses alone.
  • The conditional-expectation defining equations are weighted, p·h/p·Tmat, not h/Tmat alone, matching the book's own E^{Sti}[·] = (h̄ti,T̄ti) read as "the fiber-sum of p·(h,T) equals p_i·(h̄ti,T̄ti)" — the standard definition of a conditional expectation against counting measure on a finite partition. Instance's own hp_pos (every node's probability is strictly positive) rules out the degenerate case a bare unweighted equation would need to guard separately (a coarse node of probability 0, which cannot occur, is what the read-back of this theorem flags as the one case where the weighted equation would not pin down h_coarse/ Tmat_coarse themselves — moot here since hp_pos excludes it).
  • Trivialization risk (this chapter's own). A formalization that let coarse.h/coarse.Tmat be arbitrary constants unrelated to fine.h/fine.Tmat (dropping the conditional-expectation defining equations) would still typecheck a "lower bound" conclusion but assert nothing about aggregation — exactly the risk BRIEF.md flags: "a formalization that treats (h̄ti,T̄ti) as arbitrary constants rather than as conditional expectations over a partition of the scenario space at time t loses the theorem's actual content." Both hCoarse_h/hCoarse_T (the defining equations) and hCommonOutcome (the theorem's own extra hypothesis) are load-bearing and present.

Selected references

  • Birge, J.R., Louveaux, F. Introduction to Stochastic Programming, 2nd ed., Springer 2011, Chapter 10, §10.1 (pp. 417-420), Theorem 1 (p. 419).
  • Birge, J.R. "Decomposition and partitioning methods for multistage stochastic linear programs." Operations Research 33 (1985), 989-1007 — the source Chapter 10's aggregation bounds draw on (cited in §10.2, the neighboring section this mission does not formalize).
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Introduction to Stochastic Programming III: The L-Shaped Method and Its Finite ConvergenceTextbook

Motivation

Two-stage stochastic programs with recourse — choose a first-stage decision xxx now, observe a random outcome ξ\xiξ, then choose a second-stage recourse decision y(ξ)y(\xi)y(ξ) to repair whatever xxx left infeasible or suboptimal — are the workhorse model of the field, used for capacity planning, inventory and financial portfolio problems since the 1950s (Dantzig 1955; Beale 1955). When ξ\xiξ ranges over a finite set of scenarios, the recourse function QQQ that averages the second-stage cost over scenarios is piecewise linear and convex in xxx, so the overall problem is itself a large linear program — but one whose constraint matrix has a scenario for every column block and can be far too large to hand to a general-purpose LP solver directly. Van Slyke and Wets' L-shaped method (1969), the subject of this mission, is the algorithm that made two-stage recourse problems with finite scenario sets practically solvable: it is Benders decomposition specialized to this block structure, alternating between a small master program over xxx (and a scalar θ\thetaθ approximating the recourse cost) and, at each candidate xxx, a batch of second-stage linear programs that either certify xxx's second-stage feasibility or supply a linear underestimate — a cut — of QQQ around xxx. Birge & Louveaux's Introduction to Stochastic Programming (2nd ed., Springer 2011), Chapter 5 §5.1, gives the algorithm and proves its two central guarantees: a shortcut feasibility test for a special case (Theorem 1) and the algorithm's finite convergence in general (Theorem 2), which is this mission's goal.

Setting

A two-stage recourse instance consists of a first-stage feasible region K1={x∣Ax=b, x≥0}K_1 = \{x \mid Ax = b,\ x \ge 0\}K1​={x∣Ax=b, x≥0} for x∈Rn1x \in \mathbb{R}^{n_1}x∈Rn1​, and, for each of KKK finite scenarios k=1,…,Kk = 1, \dots, Kk=1,…,K (occurring with probability pkp_kpk​), second-stage data (qk,hk,Tk)(q_k, h_k, T_k)(qk​,hk​,Tk​) defining the recourse subproblem

Q(x,ξk)=min⁡y≥0{qk⊤y∣Wy=hk−Tkx},Q(x, \xi_k) = \min_{y \ge 0} \{ q_k^\top y \mid W y = h_k - T_k x \},Q(x,ξk​)=y≥0min​{qk⊤​y∣Wy=hk​−Tk​x},

where the recourse matrix WWW is fixed — the same across every scenario, the case this chapter treats. K2={x∣Q(x,ξk)<∞ for all k}K_2 = \{x \mid Q(x,\xi_k) < \infty \text{ for all } k\}K2​={x∣Q(x,ξk​)<∞ for all k} is the set of xxx for which every scenario's subproblem is feasible, and the two-stage problem is

min⁡x c⊤x+Q(x)s.t.x∈K1∩K2,Q(x)=∑k=1Kpk Q(x,ξk).\min_{x} \ c^\top x + Q(x) \quad \text{s.t.} \quad x \in K_1 \cap K_2, \qquad Q(x) = \sum_{k=1}^K p_k\, Q(x, \xi_k).xmin​ c⊤x+Q(x)s.t.x∈K1​∩K2​,Q(x)=k=1∑K​pk​Q(x,ξk​).

A basis of the recourse subproblem is an injective choice of m2m_2m2​ of WWW's columns (where m2m_2m2​ is WWW's row count); each basis bbb determines a simplex multiplier π=(Wb⊤)−1qb\pi = (W_b^\top)^{-1} q_bπ=(Wb⊤​)−1qb​, and when bbb attains the true optimum of Q(x,ξk)Q(x,\xi_k)Q(x,ξk​), LP duality gives Q(x,ξk)=π⊤(hk−Tkx)Q(x,\xi_k) = \pi^\top(h_k - T_k x)Q(x,ξk​)=π⊤(hk​−Tk​x) — the mechanism that turns a batch of second-stage LP solves into linear cuts on xxx.

Formalization targets

The L-shaped algorithm proceeds in three steps, repeated until neither applies:

  • Step 1 solves the current master program (the K1K_1K1​-feasible xxx, plus θ\thetaθ once at least one optimality cut exists, minimizing c⊤x+θc^\top x + \thetac⊤x+θ subject to every cut recorded so far — or just c⊤xc^\top xc⊤x over K1K_1K1​ before the first optimality cut, matching the book's convention that θ\thetaθ "is set equal to −∞-\infty−∞ and is not considered" until then).
  • Step 2 tests each scenario's second-stage feasibility at the Step-1 optimum via an auxiliary LP; if some scenario fails (the LP's optimal value is positive), its optimal basis yields a feasibility cut and the algorithm returns to Step 1.
  • Step 3, once every scenario is feasible, checks whether θ\thetaθ already dominates the true recourse cost at xxx (using each scenario's optimal basis via LP duality); if not, an optimality cut is added and the algorithm returns to Step 1; if so, xxx is optimal and the algorithm stops.

Goal — Chapter 5, Theorem 2 (p. 198)

When ξ is a finite random variable, the L-shaped algorithm finitely converges to\text{When } \xi \text{ is a finite random variable, the L-shaped algorithm finitely converges to}When ξ is a finite random variable, the L-shaped algorithm finitely converges to an optimal solution when it exists, or proves K1∩K2=∅.\text{an optimal solution when it exists, or proves } K_1 \cap K_2 = \varnothing.an optimal solution when it exists, or proves K1​∩K2​=∅.

Formalized as: starting from the empty cut set, there is a finite-length run of the algorithm's Step-1/2/3 transition relation, of length bounded by the total number of distinct feasibility- and optimality-cut witnesses available, ending at a state admitting no further step — at which point either the master program has become infeasible (certifying K1∩K2=∅K_1 \cap K_2 = \varnothingK1​∩K2​=∅) or its optimum is second-stage feasible, passes every fresh Step-3 test, and is optimal for the two-stage problem.

Milestone — Chapter 5, Theorem 1 (p. 194)

If T is deterministic, W is such that every t≥0 lies in pos W,\text{If } T \text{ is deterministic, } W \text{ is such that every } t \ge 0 \text{ lies in } \mathrm{pos}\,W,If T is deterministic, W is such that every t≥0 lies in posW, and a=min⁡khk (componentwise) is attained by some scenario hℓ,\text{and } a = \min_k h_k \text{ (componentwise) is attained by some scenario } h_\ell,and a=kmin​hk​ (componentwise) is attained by some scenario hℓ​, then x∈K2  ⟺  ∃ y≥0, Wy=a−Tx.\text{then } x \in K_2 \iff \exists\, y \ge 0,\ Wy = a - Tx.then x∈K2​⟺∃y≥0, Wy=a−Tx.

A shortcut avoiding KKK separate feasibility LPs at Step 2: under these structural assumptions on WWW, checking feasibility at the single componentwise-worst right-hand side certifies feasibility at every scenario simultaneously.

Significance

Van Slyke and Wets' method (and Benders decomposition more generally, of which it is the recourse-problem specialization) underlies essentially every large-scale two-stage stochastic program solved in practice, and its finite-convergence guarantee — not merely that an optimum exists, but that this specific cutting-plane procedure reaches it in finitely many outer iterations — is what makes the method a decision procedure rather than a heuristic. The proof's content is an explicit finiteness argument (the number of distinct simplex bases of the recourse subproblem and the feasibility-test LP is finite, so the algorithm cannot generate infinitely many distinct cuts before either exhausting the feasible region or converging), not a general compactness or fixed-point argument; formalizing it means formalizing the cutting-plane mechanism itself as a transition system and proving termination combinatorially, over the finite type of available bases, rather than proving only that some optimal xxx exists.

Difficulty

The natural shortcut — state only "an optimal xxx exists, or K1∩K2=∅K_1 \cap K_2 = \varnothingK1​∩K2​=∅" — is not Theorem 2's actual content and is not what this mission targets: that weaker claim would already follow from K1∩K2K_1 \cap K_2K1​∩K2​ being a nonempty polyhedron (or empty), with no reference to the algorithm at all, and would not require the finiteness-of-bases argument the book's proof turns on. The genuine difficulty is representing Steps 1-3 faithfully as a relation on accumulating cut sets, and pinning the termination bound to the actual combinatorial object the book cites (the finite set of bases of the two LPs the algorithm solves at each iteration) rather than to a numeral or an abstract compactness bound. A second, quieter difficulty is Step 1's own optimum: once optimality cuts exist, the master program optimizes c⊤x+θc^\top x + \thetac⊤x+θ jointly, but before the first one it optimizes c⊤xc^\top xc⊤x alone; conflating the two (e.g. always requiring θ\thetaθ to be part of the optimum) does not match Step 1 as the book states it.

Formalization scope

First-stage and second-stage vectors are Fin n1 → ℝ / Fin n2 → ℝ; the finite scenario set is Fin K with probability vector p. A basis is {b : Fin m2 → Fin n2 // Function.Injective b} (m2 = the recourse matrix's row count), matching "an injective choice of m2m_2m2​ columns of WWW"; its finiteness is definitional, from Fin m2 → Fin n2 being finite. Simplex multipliers use Matrix.inv, whose junk value 0 on a singular matrix is never reachable in a proof because multipliers are only ever used through an IsOptimalAt/IsFeasBasisOptimalAt hypothesis that pins the basis to one genuinely attaining the LP's true optimum. The recourse value Q(x,ξk)Q(x,\xi_k)Q(x,ξk​) is EReal-valued (reusing this series' Instance/QVal convention from Chunk 03), so an optimality-cut witness's claimed value is compared to it by an explicit EReal cast, never by EReal arithmetic. The algorithm's state is a pair of finite sets of witnesses recorded so far (Finset (Fin K × FeasBasis n2 m2) × Finset (Fin K → Basis n2 m2)); Step is an inductive relation with one constructor per Step-2 and Step-3 branch, each requiring its witness not already recorded, and the goal states a bounded-length Step-path from the empty state to a state admitting no further Step. This mission does not restate Chapter 3's polyhedrality fact about K2K_2K2​ as a separate lemma: the finiteness fact it is invoked for is already exposed directly and structurally by the finite Fintype bound on the number of bases, so no additional axiom stands in for it (see MODERATION_NOTES.md). Lemmas 3-9 and Theorem 10 of §5.2 (Regularized Decomposition, a different algorithm) are out of scope. The trivializing formalization this mission rules out is exactly the one named under Difficulty above: a bare existence-of-optimal-or- infeasible-xxx statement with no reference to Steps 1-3 or to a finite bound on the number of iterations — such a statement would be true of any nonempty polyhedron and would not be Theorem 2.

Selected references

  • R. Van Slyke and R. Wets, L-Shaped Linear Programs with Applications to Optimal Control and Stochastic Programming, SIAM Journal on Applied Mathematics, 17(4), 1969, pp. 638-663. https://doi.org/10.1137/0117061
  • J. Birge and F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer, 2011, Chapter 5. https://doi.org/10.1007/978-1-4614-0237-4
  • G. Dantzig, Linear Programming under Uncertainty, Management Science, 1(3-4), 1955, pp. 197-206. https://doi.org/10.1287/mnsc.1.3-4.197
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Group Theory·Captain: dbenbenn

Chou: elementary amenable groupsResearch Paper

Motivation

Von Neumann introduced amenable groups in 1929 to explain the Hausdorff–Banach–Tarski paradox, and showed that the class AGAGAG of amenable groups contains all finite and all abelian groups and is closed under four processes: (I) subgroups, (II) quotients, (III) extensions and (IV) directed unions. Day named the smallest class with these properties EGEGEG, the elementary amenable groups. For fifty years these were the only amenable groups anyone could exhibit, and von Neumann's question whether every non-amenable group contains a free subgroup on two generators — whether AGAGAG equals the class NFNFNF of groups without such a subgroup — was open. (It was answered in the negative by Ol'shanskii in 1980, the year of this paper, by different methods.)

Ching Chou's Elementary amenable groups (Illinois J. Math. 24 (1980) 396–407, doi:10.1215/ijm/1256047608) gives the structure theory of EGEGEG that everything later relies on. Its central result is that the class can be built from finite and abelian groups by extensions and directed unions alone — subgroups and quotients add nothing (Proposition 2.2). From that description three things follow: periodic elementary amenable groups are locally finite, so the periodic non-locally-finite groups of Golod and Novikov–Adjan show EG⊊NFEG \subsetneq NFEG⊊NF (Theorem 2.3); a finitely generated simple elementary amenable group is finite (Corollary 2.4); and Wolf's conjecture holds in EGEGEG: a finitely generated elementary amenable group is almost nilpotent or has exponential growth (Theorem 3.2, extending Milnor and Wolf's theorem for solvable groups). A final section introduces a packing property (P) of groups and proves it for every elementary amenable group (Proposition 4.2) and every residually elementary amenable group (Corollary 4.7).

On this platform the definition of EGEGEG is already published (the bundle Chou_ElementaryAmenable, from the mission Cannon–Floyd–Parry: Thompson's group F and the simplicity of its commutator subgroup), together with the theorem that Thompson's group FFF is not elementary amenable (Theorem 4.10) and, from Brin and Squier, that FFF has no free subgroup on two generators (CannonFloydParry.no_free_subgroup_of_rank_two). This mission formalizes Chou's paper on top of that definition.

Setting

The class EGEGEG and its constructible core. Chou.ElementaryAmenable G is an inductive predicate on groups: finite groups and abelian groups are in the class, and the class is closed under isomorphism, subgroups, quotients, extensions and directed unions of subgroups; each rule is a constructor of the published bundle Chou_ElementaryAmenable, where it is stated precisely. Chou builds the hierarchy EG0⊆EG1⊆⋯EG_0 \subseteq EG_1 \subseteq \cdotsEG0​⊆EG1​⊆⋯ by transfinite recursion, applying only extensions and directed unions to the finite and abelian groups, and proves that ⋃αEGα\bigcup_\alpha EG_\alpha⋃α​EGα​ is closed under subgroups and quotients, hence equals EGEGEG. The union ⋃αEGα\bigcup_\alpha EG_\alpha⋃α​EGα​ is realised here without ordinals, as the inductive predicate Chou.Constructible, whose constructors are of_finite, of_commGroup, of_mulEquiv, extension and directedUnion; Chou's transfinite induction over α\alphaα becomes structural induction over a derivation, with the same case analysis.

Periodic and locally finite groups. A group is periodic if every element has finite order (Mathlib's IsMulTorsion) and locally finite if every finitely generated subgroup is finite (Chou.IsLocallyFinite). Day's class NFNFNF is Chou.NoFreeSubgroupOfRankTwo: no homomorphism from the free group on two generators into GGG is injective.

Growth. For a finite generating set SSS of GGG, Chou.wordBall S n is the set of products of at most nnn factors, each in SSS or with inverse in SSS. GGG has exponential growth if for some finite generating set the ball of radius nnn has at least cnc^ncn elements for some c>1c > 1c>1 and all nnn; it is exponentially bounded if for some finite generating set and every c>1c > 1c>1 the balls are eventually smaller than cnc^ncn. Chou works with ∣Fn∣|F^n|∣Fn∣ for products of exactly nnn elements of a finite generating set FFF; for FFF symmetric and containing the identity the two agree, and Wolf's observation that the growth type is independent of the generating set is one of the milestones. "Almost nilpotent" is Mathlib's Group.IsVirtuallyNilpotent: a nilpotent subgroup of finite index. A free subsemigroup on two generators means two elements a,ba, ba,b such that distinct positive words in a,ba, ba,b are distinct in GGG (Chou.HasFreeSubsemigroupOfRankTwo).

Packings. A pair of subsets (S,X)(S, X)(S,X) is a packing of GGG if (s,x)↦sx(s, x) \mapsto sx(s,x)↦sx is a bijection S×X→GS \times X \to GS×X→G (Chou.IsPacking), and GGG has property (P) if every finite subset lies in a finite SSS for which some (S,X)(S, X)(S,X) is a packing (Chou.HasPackingProperty). GGG is residually elementary amenable if every x≠1x \neq 1x=1 survives in some elementary amenable quotient (Chou.ResiduallyElementaryAmenable).

Target

The goal is Chou's description of the class, Proposition 2.2 (b) (p. 397): “EGEGEG is the smallest class of groups which contains all finite groups and all abelian groups and is closed under processes (III) and (IV).” It is stated as the equivalence ElementaryAmenable G ↔ Constructible G. The milestones follow the paper's order.

Section 2. Proposition 2.1 in two halves — the constructible groups are closed under subgroups and under quotients — which is the whole proof of the goal. Theorem 2.3: periodic elementary amenable groups are locally finite; and its consequence that NF∖EGNF \setminus EGNF∖EG is nonempty. Corollary 2.4: finitely generated simple elementary amenable groups are finite.

Section 3. Lemma 3.1 (an extension of almost nilpotent by almost nilpotent is almost nilpotent or of exponential growth), Theorem 3.2 and Rosenblatt's sharpening Theorem 3.2′, together with the facts Chou uses on the way: a finite-by-nilpotent group is almost nilpotent; a free subsemigroup forces exponential growth; Wolf's independence of the generating set; and Milnor's existence of the growth rate, in the form "exponentially bounded means not of exponential growth".

Section 4. Property (P) for finite groups, for Z\mathbb ZZ, for finitely generated abelian groups; Lemma 4.1 (directed unions and extensions preserve (P)); Proposition 4.2 (every elementary amenable group has (P)); Lemma 4.6 (a) and Corollary 4.7 (residually elementary amenable groups have (P)); and the free groups.

External theorems as milestones

Chou's Section 3 rests on results the paper cites rather than proves, none of which is in Mathlib. They are stated here as milestones in their own right, so that the dependence is visible and each is a well-defined target: the Milnor–Wolf theorem (a finitely generated solvable group that is exponentially bounded is almost nilpotent); M. Hall's theorem that a finitely generated group has finitely many subgroups of each finite index; that finitely generated nilpotent groups are finitely presented and that a group with a finitely presented subgroup of finite index is finitely presented; Milnor's Lemmas 1–2 in the form Chou states on p. 400 (in a finitely generated exponentially bounded group, a normal subgroup with finitely presented quotient is finitely generated); and Rosenblatt's variant of Lemma 3.1. Section 4 needs one more: free groups are residually finite. Lemma 3.1 and Theorems 3.2, 3.2′ can be closed only once these are; every other milestone is provable from Mathlib and the published library.

Two remarks on Theorem 2.3. Chou's witness for NF∖EGNF \setminus EGNF∖EG is a periodic group that is not locally finite (Golod; Novikov–Adjan), whose existence is not formalized. The platform already holds a different witness: Thompson's group FFF is not elementary amenable (Cannon–Floyd–Parry, Theorem 4.10) and has no free subgroup on two generators (Brin–Squier); both are published and proved, and the milestone is proved from them. The inclusion EG⊆NFEG \subseteq NFEG⊆NF itself is von Neumann's theorem that amenable groups contain no free subgroup of rank two, which passes through the definition of amenability and is not part of this mission.

What is left out

The ordinal-indexed hierarchy EGαEG_\alphaEGα​ and the remark that it stabilises at some α0+1\alpha_0 + 1α0​+1 (Proposition 2.2 (a)) are replaced by the inductive predicate. Chou's two examples of finitely generated groups in EGEGEG that are not almost solvable (p. 402), the Golod–Shafarevich discussion, and Lemma 4.6 (b) (ordinal-indexed normal series) are omitted. Propositions 4.3–4.5 on almost convergent sets, and Milnor's remark that exponentially bounded groups are amenable, need invariant means on ℓ∞(G)\ell^\infty(G)ℓ∞(G); amenability itself is the subject of Garrido I.

References

  • C. Chou, Elementary amenable groups, Illinois J. Math. 24 (1980), 396–407.
  • M. M. Day, Amenable semigroups, Illinois J. Math. 1 (1957), 509–544.
  • J. Milnor, Growth of finitely generated solvable groups, J. Differential Geometry 2 (1968), 447–449; J. A. Wolf, Growth of finitely generated solvable groups and curvature of Riemannian manifolds, ibid. 421–446.
  • J. M. Rosenblatt, Invariant measures and growth conditions, Trans. Amer. Math. Soc. 193 (1974), 33–53.
  • J. W. Cannon, W. J. Floyd, W. R. Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Math. 42 (1996), 215–256 (Theorem 4.10); M. G. Brin, C. C. Squier, Groups of piecewise linear homeomorphisms of the real line, Invent. Math. 79 (1985), 485–498.
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AnalysisProbability·Captain: naimengye

Probability Theory and Examples I: Kolmogorov's Three-Series TheoremTextbook

Motivation

Given independent random variables X1,X2,…X_1,X_2,\dotsX1​,X2​,…, when does ∑nXn\sum_n X_n∑n​Xn​ converge? Not absolutely — that question is settled by ∑nE∣Xn∣<∞\sum_n\mathbb{E}|X_n|<\infty∑n​E∣Xn​∣<∞ and is usually too strong. The interesting question is when the partial sums converge for almost every outcome, and here independence buys something that holds for no general sequence: convergence is not a delicate matter of cancellation but is decided, once and for all, by three numerical series.

Chapter 2 of Rick Durrett's Probability: Theory and Examples (Version 5, 2019) reaches this in section 2.5. Kolmogorov's three-series theorem fixes a truncation level A>0A>0A>0, replaces each XnX_nXn​ by Yn=Xn1(∣Xn∣≤A)Y_n=X_n\mathbb{1}(|X_n|\le A)Yn​=Xn​1(∣Xn​∣≤A), and asserts that ∑nXn\sum_n X_n∑n​Xn​ converges almost surely if and only if

∑nP(∣Xn∣>A)<∞,∑nEYn converges,∑nvar⁡(Yn)<∞.\sum_n\mathbb{P}(|X_n|>A)<\infty,\qquad \sum_n\mathbb{E}Y_n \text{ converges},\qquad \sum_n\operatorname{var}(Y_n)<\infty .n∑​P(∣Xn​∣>A)<∞,n∑​EYn​ converges,n∑​var(Yn​)<∞.

Three deterministic conditions on the distributions decide an almost-sure question about paths, and the answer does not depend on which AAA is chosen. Through Kronecker's lemma this is also the route to the strong law of large numbers, which is how the chapter uses it.

Setting

Let X1,X2,…X_1,X_2,\dotsX1​,X2​,… be independent real random variables on a probability space, with partial sums SN=∑n<NXnS_N=\sum_{n<N}X_nSN​=∑n<N​Xn​. Say that ∑nXn\sum_n X_n∑n​Xn​ converges almost surely when for almost every ω\omegaω the sequence SN(ω)S_N(\omega)SN​(ω) has a real limit; following Durrett, "∑an\sum a_n∑an​ converges" means lim⁡N∑n≤Nan\lim_N\sum_{n\le N}a_nlimN​∑n≤N​an​ exists, not that it converges absolutely.

Three tools from the same section support the theorem. Kolmogorov's maximal inequality strengthens Chebyshev from P(∣Sn∣≥x)\mathbb{P}(|S_n|\ge x)P(∣Sn​∣≥x) to the maximum of the whole path,

P(max⁡1≤k≤n∣Sk∣≥x)≤x−2var⁡(Sn),\mathbb{P}\Bigl(\max_{1\le k\le n}|S_k|\ge x\Bigr)\le x^{-2}\operatorname{var}(S_n),P(1≤k≤nmax​∣Sk​∣≥x)≤x−2var(Sn​),

for independent, centred, square-integrable summands. From it comes the convergence criterion: if EXn=0\mathbb{E}X_n=0EXn​=0 and ∑nvar⁡(Xn)<∞\sum_n\operatorname{var}(X_n)<\infty∑n​var(Xn​)<∞ then ∑nXn\sum_n X_n∑n​Xn​ converges almost surely. Kronecker's lemma is the deterministic bridge to averages: if an↑∞a_n\uparrow\inftyan​↑∞ and ∑nxn/an\sum_n x_n/a_n∑n​xn​/an​ converges then an−1∑m≤nxm→0a_n^{-1}\sum_{m\le n}x_m\to0an−1​∑m≤n​xm​→0. And the Hewitt–Savage 0-1 law says that for an i.i.d. sequence every permutable event — one unchanged by rearranging finitely many coordinates — has probability 000 or 111.

Formalization targets

Goal — Theorem 2.5.8, Kolmogorov's three-series theorem

∑nXn converges a.s.  ⟺  {∑nP(∣Xn∣>A)<∞,∑nE[Xn1(∣Xn∣≤A)] converges,∑nvar⁡(Xn1(∣Xn∣≤A))<∞.\sum_n X_n \text{ converges a.s.} \iff \begin{cases} \sum_n\mathbb{P}(|X_n|>A)<\infty,\\ \sum_n\mathbb{E}\bigl[X_n\mathbb{1}(|X_n|\le A)\bigr]\ \text{converges},\\ \sum_n\operatorname{var}\bigl(X_n\mathbb{1}(|X_n|\le A)\bigr)<\infty . \end{cases}n∑​Xn​ converges a.s.⟺⎩⎨⎧​∑n​P(∣Xn​∣>A)<∞,∑n​E[Xn​1(∣Xn​∣≤A)] converges,∑n​var(Xn​1(∣Xn​∣≤A))<∞.​

Both directions are asserted, as Durrett states the theorem. The truncation level A>0A>0A>0 is arbitrary and fixed in the statement; that the three conditions hold for one AAA exactly when they hold for every AAA is a consequence, not an assumption.

Supporting levels

Kolmogorov's maximal inequality (2.5.5); the convergence criterion under summable variances (2.5.6); Kronecker's lemma (2.5.9); and the Hewitt–Savage 0-1 law (2.5.4).

Significance

The result itself. The three-series theorem is the complete answer to a question that has no complete answer without independence, and the shape of the answer is the interesting part: a pathwise, almost-sure property is equivalent to three conditions each computable from the marginal distributions alone. Each of the three does a separate job — the first says XnX_nXn​ and its truncation differ only finitely often, so Borel–Cantelli lets them be exchanged; the second controls the drift of the truncated sums; the third controls their fluctuation. The theorem is also the standard route to the strong law: applying it to Xn/nX_n/nXn​/n and then Kronecker's lemma gives Sn/n→μS_n/n\to\muSn​/n→μ, which is why section 2.5 sits where it does.

Formalizing it. Mathlib has the strong law of large numbers (strong_law_ae), both Borel–Cantelli lemmas, and Kolmogorov's 0-1 law for the tail σ-field. It has none of the following: Kolmogorov's maximal inequality, the almost-sure convergence criterion for random series with summable variances, Kronecker's lemma, the Hewitt–Savage 0-1 law, or the three-series theorem. The mission therefore contributes the whole of section 2.5, and the pieces are reusable well beyond it — the maximal inequality and Kronecker's lemma in particular are standard tools with no probabilistic content in the second case at all.

Difficulty

The maximal inequality is the step where the argument stops being routine. Chebyshev bounds P(∣Sn∣≥x)\mathbb{P}(|S_n|\ge x)P(∣Sn​∣≥x) and no more; controlling the maximum over the whole path needs the first passage decomposition Ak={∣Sk∣≥x, ∣Sj∣<x for j<k}A_k=\{|S_k|\ge x,\ |S_j|<x \text{ for } j<k\}Ak​={∣Sk​∣≥x, ∣Sj​∣<x for j<k} and the observation that Sk1AkS_k\mathbb{1}_{A_k}Sk​1Ak​​ is measurable with respect to the first kkk variables while Sn−SkS_n-S_kSn​−Sk​ is independent of them, so the cross terms vanish. That is a stopping-time argument in disguise, and it is what makes the whole section work.

The sufficiency half of the goal is then assembly: the third series and the convergence criterion give ∑(Yn−EYn)\sum(Y_n-\mathbb{E}Y_n)∑(Yn​−EYn​) convergent, the second adds the means back, and the first plus Borel–Cantelli replaces YnY_nYn​ by XnX_nXn​. Necessity is the harder direction, and Durrett does not prove it in Chapter 2 at all — he defers it to Example 3.4.12, where it follows from the Lindeberg–Feller central limit theorem. A solver attacking the goal should expect the reverse implication to need machinery from outside this section.

The Hewitt–Savage law has a difficulty of its own kind: the natural statement is about a σ-field of events on a sequence space, and the proof approximates a permutable event by cylinder events and then applies the permutation that swaps the first nnn coordinates with the next nnn.

Formalization scope

Random variables are measurable real-valued functions on a probability space and independence is Mathlib's iIndepFun. Variance is Mathlib's variance, and square-integrability is stated as membership in L2L^2L2 where the maximal inequality and the convergence criterion need it. The three-series theorem itself assumes no integrability: the truncated variables are bounded, so their means and variances exist automatically, which is exactly why the truncation is there.

"∑nan\sum_n a_n∑n​an​ converges" is formalized as convergence of the sequence of partial sums to a real limit, not as Summable, which in Mathlib means unconditional and hence absolute convergence for real series. This distinction is not pedantic here: condition (ii) of the theorem is convergence of ∑EYn\sum\mathbb{E}Y_n∑EYn​ in Durrett's sense and would be a strictly stronger condition if read as summability. Conditions (i) and (iii) are series of non-negative terms, where the two notions agree, and are stated as Summable.

Almost-sure convergence of ∑nXn\sum_n X_n∑n​Xn​ is "for almost every ω\omegaω there exists a real LLL with SN(ω)→LS_N(\omega)\to LSN​(ω)→L" — the limit is not asserted to be measurable in ω\omegaω, and does not need to be for the statement to say what it should.

For the Hewitt–Savage law the sequence space is the countable product N→S\mathbb{N}\to SN→S carrying the infinite product of copies of one law, which is Mathlib's Measure.infinitePi, and a permutable event is a measurable set invariant under every finitely supported permutation of the coordinates. That is Durrett's exchangeable σ-field stated directly rather than constructed as a σ-field object.

Contributions welcome beyond the listed items: the converse direction via Lindeberg–Feller (Example 3.4.12); the derivation of the strong law from the three-series theorem and Kronecker's lemma; the Marcinkiewicz–Zygmund law (2.5.12); and the rates of convergence of section 2.5.1.

Selected references

  • Rick Durrett, Probability: Theory and Examples, Version 5 (January 11, 2019), section 2.5 (pp. 81–90); Theorems 2.5.4, 2.5.5, 2.5.6, 2.5.8, 2.5.9. Published as Cambridge Series in Statistical and Probabilistic Mathematics, 5th edition, 2019, DOI 10.1017/9781108591034
  • A. N. Kolmogorov, Grundbegriffe der Wahrscheinlichkeitsrechnung, Springer, 1933.
  • E. Hewitt and L. J. Savage, Symmetric measures on Cartesian products, Transactions of the American Mathematical Society 80 (1955), 470–501. DOI 10.1090/S0002-9947-1955-0076206-8
  • P. Billingsley, Probability and Measure, 3rd ed., Wiley, 1995, section 22.
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Algorithmic Game TheoryOperations ResearchOptimization·Captain: naimengye

Stochastic Networks IV: Decentralized Optimization and Wardrop EquilibriaTextbook

Motivation

A network of resistors solves an optimization problem. Nobody tells the electrons what to do; each one moves under a purely local rule, and the current distribution that emerges minimizes energy dissipation over all distributions satisfying Kirchhoff's node law. Add a wire and the network can only become easier to traverse. This is the encouraging case, and Chapter 4 of Frank Kelly and Elena Yudovina's Stochastic Networks (Cambridge University Press, 2014) opens with it.

Road traffic is the discouraging case. Drivers also follow a local rule — take the fastest route — and the pattern that emerges is again characterized by an optimization problem, but not the one anyone wants solved. Braess's paradox is the sharp form of the discrepancy: in a small road network carrying six cars per unit time, every route takes 83 time units at equilibrium; open an extra road, and at the new equilibrium every route takes 92. Building road capacity made everyone slower. The difference from the electrical case is that a driver's choice imposes a delay on everyone else sharing the road and the driver does not pay for it, and correcting that — pricing the externality — is how a decentralized rule can be made to produce good global behaviour. That idea recurs in Chapters 7 and 8 of the book as the basis of Internet congestion control.

Setting

The network is a set J\mathcal{J}J of JJJ directed links. A route rrr is a subset of links, and R\mathcal{R}R is the set of RRR routes under consideration — not necessarily all physically possible ones. The link-route incidence matrix AAA has Ajr=1A_{jr}=1Ajr​=1 when j∈rj \in rj∈r and Ajr=0A_{jr}=0Ajr​=0 otherwise. Writing xrx_rxr​ for the flow on route rrr, the flow on link jjj is

yj=∑rAjrxr,that is y=Ax.y_j=\sum_{r}A_{jr}x_r, \qquad\text{that is } y = Ax.yj​=r∑​Ajr​xr​,that is y=Ax.

Each link has a delay function Dj(yj)D_j(y_j)Dj​(yj​), continuous and increasing in the flow on that link, and the delay along a route is the sum of the delays of its links, ∑jDj(yj)Ajr\sum_j D_j(y_j)A_{jr}∑j​Dj​(yj​)Ajr​. Drivers care only about getting from origin to destination: S\mathcal{S}S is the set of source–destination pairs, each route rrr serves exactly one of them, written s(r)s(r)s(r), and the flow requirement between pair σ\sigmaσ is fσf_\sigmafσ​.

A routing pattern is stable when no driver has an incentive to switch. Definition 4.2 makes this precise: a Wardrop equilibrium is a feasible vector of route flows xxx such that

xr>0  ⟹  ∑jDj(yj)Ajr=min⁡r′∈s(r)∑jDj(yj)Ajr′,y=Ax.x_r>0 \;\Longrightarrow\; \sum_{j}D_j(y_j)A_{jr}=\min_{r'\in s(r)}\sum_{j}D_j(y_j)A_{jr'}, \qquad y = Ax .xr​>0⟹j∑​Dj​(yj​)Ajr​=r′∈s(r)min​j∑​Dj​(yj​)Ajr′​,y=Ax.

Every route actually carrying traffic is a shortest route, in delay, for the traffic it carries.

Formalization targets

Goal — Theorem 4.3, a Wardrop equilibrium exists

∃ x≥0  with Hx=f  such that x is a Wardrop equilibrium.\exists\, x \ge 0 \ \text{ with } Hx=f \ \text{ such that } x \text{ is a Wardrop equilibrium.}∃x≥0  with Hx=f  such that x is a Wardrop equilibrium.

The goal asserts existence only, for an arbitrary network, arbitrary route set and arbitrary continuous increasing delay functions. It fixes no uniqueness claim, because the equilibrium flows need not be unique even though the link loads are, and no efficiency claim, because Braess's paradox is precisely the statement that the equilibrium is not efficient.

Supporting levels

Kirchhoff's node law as the equations satisfied by the expected reward in the random-walk game of section 4.1; the two Braess networks of Figures 4.4a and 4.4b, with their equilibrium delays 838383 and 929292; convexity of ∫0yD(u) du\int_0^{y}D(u)\,du∫0y​D(u)du for increasing DDD; the optimization characterization that makes the goal reachable — a minimizer of ∑j∫0yjDj(u) du\sum_j\int_0^{y_j}D_j(u)\,du∑j​∫0yj​​Dj​(u)du over the feasible flows is a Wardrop equilibrium; and the exact externality decomposition of the queueing network of section 4.3.1.

Significance

The result itself. Theorem 4.3 is what makes the Wardrop equilibrium a usable object: a traffic model that could fail to have an equilibrium would be describing nothing. Its proof does more than establish existence — it identifies the equilibrium as the solution of a specific convex program, minimizing ∑j∫0yjDj(u) du\sum_j\int_0^{y_j}D_j(u)\,du∑j​∫0yj​​Dj​(u)du. That function is not the total delay ∑jyjDj(yj)\sum_j y_jD_j(y_j)∑j​yj​Dj​(yj​), and the gap between the two is exactly Braess's paradox: selfish routing optimizes the wrong objective. Once the two objectives are written side by side, the fix is readable off them, and it is the fix used in practice — a toll on link jjj equal to yjDj′(yj)y_jD_j'(y_j)yj​Dj′​(yj​), the marginal delay a driver imposes on everyone else, makes the selfish objective coincide with the social one. Section 4.3 then carries the same accounting into queueing and loss networks, where the derivative of the mean cost splits into a term for the delay a customer suffers and a term for the knock-on cost it inflicts.

Formalizing it. Nothing here is open; Wardrop stated the principle in 1952 and Beckmann, McGuire and Winsten gave the optimization formulation in 1956. What the mission produces is a machine-checked model of selfish routing — incidence matrix, link flows, delay functions, the equilibrium condition — and a formal record of Braess's paradox as a concrete pair of networks rather than a story. Mathlib has no traffic or congestion-game theory.

Difficulty

Existence is not a fixed-point argument in the obvious variable: the best-response map of the routing game is not continuous, since a small change in flows can flip which route is shortest and move all the traffic. The book's route is to replace the equilibrium condition by the stationarity conditions of a convex program on a compact feasible set, where existence is routine and the content is the translation. The translation is where the care is needed, and it is stated here as a separate milestone: the first-order conditions say the Lagrange multiplier λs(r)\lambda_{s(r)}λs(r)​ equals the route delay on routes carrying traffic and is a lower bound on the others, which is Definition 4.2 restated.

The subtlety worth naming in advance is that "increasing" is doing real work in two different places. It makes ∫0yD(u) du\int_0^{y}D(u)\,du∫0y​D(u)du convex, which is what makes the program tractable; and it is what makes each Dj(yj)D_j(y_j)Dj​(yj​) interpretable as a price. Neither convexity of DjD_jDj​ itself nor strict monotonicity is needed, and assuming them would be assuming more than the book does.

Formalization scope

Links, routes and source–destination pairs are indexed by finite types. The incidence matrix is real-valued with entries constrained to be 000 or 111, matching the book's definition in this chapter (unlike Chapter 3, which allows general non-negative integers). The map from routes to source–destination pairs is given as a function sss rather than as the matrix HHH, which is exactly the book's statement that each column of HHH sums to 111.

Delay functions are total functions R→R\mathbb{R}\to\mathbb{R}R→R, continuous and monotone. This excludes the vertical asymptote that Figure 4.5 permits — a link with a finite capacity at which delay blows up — and that restriction is recorded here rather than left implicit. The equilibrium condition is stated as the inequality "delay on r≤delay on r′\text{delay on } r \le \text{delay on } r'delay on r≤delay on r′ for every r′r'r′ serving the same pair", which is Definition 4.2 with the minimum written out; the two are equivalent because rrr itself serves s(r)s(r)s(r), and the inequality form avoids having to produce a minimum over a possibly empty set.

The goal is not vacuous: the feasibility hypotheses (fσ≥0f_\sigma\ge0fσ​≥0, and each source–destination pair served by at least one route) are exactly what makes the feasible set non-empty, and without them the existence claim would be false rather than trivial.

Contributions welcome beyond the listed items: uniqueness of the equilibrium link loads yyy; the marginal-cost toll that aligns the selfish and social optima; Rayleigh monotonicity (Exercise 4.3, that effective resistance does not decrease when a resistance is increased); the price of anarchy for affine delays; and Theorem 4.6 on the derivatives of the loss-network rate of return with respect to offered traffic and capacity.

Selected references

  • Frank Kelly and Elena Yudovina, Stochastic Networks, Cambridge University Press, 2014, Chapter 4 (pp. 85–107); Definition 4.2, Theorem 4.3, sections 4.1–4.3. DOI 10.1017/cbo9781139565363
  • J. G. Wardrop, Some theoretical aspects of road traffic research, Proceedings of the Institution of Civil Engineers 1 (1952), 325–362. DOI 10.1680/ipeds.1952.11259
  • M. Beckmann, C. B. McGuire and C. B. Winsten, Studies in the Economics of Transportation, Yale University Press, 1956.
  • D. Braess, Über ein Paradoxon aus der Verkehrsplanung, Unternehmensforschung 12 (1968), 258–268. DOI 10.1007/BF01918335
  • Peter Doyle and J. Laurie Snell, Random Walks and Electric Networks, Mathematical Association of America, 1984. arXiv:math/0001057
  • R. G. Gallager, A minimum delay routing algorithm using distributed computation, IEEE Transactions on Communications 25 (1977), 73–85. DOI 10.1109/TCOM.1977.1093711
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Stochastic Networks II: Migration Processes and Product FormTextbook

Motivation

A queueing network is a collection of service stations through which customers — jobs, packets, telephone calls, patients — move one at a time. The state of such a network is a vector of occupancy counts, one per station, and the number of states grows exponentially in the number of stations, so solving the equilibrium equations directly is hopeless for any network worth modelling. The product form is what rescues the subject: for a large and identifiable class of networks the equilibrium distribution factorizes into one term per station, as if the stations were independent, and a network of JJJ stations costs JJJ one-dimensional calculations instead of one exponentially large one.

Chapter 2 of Frank Kelly and Elena Yudovina's Stochastic Networks (Cambridge University Press, 2014) establishes this for migration processes, the Markov model in which individuals move between colonies one at a time at a rate that factorizes as λjkφj(nj)\lambda_{jk}\varphi_j(n_j)λjk​φj​(nj​): a part depending only on the two colonies and a part depending only on the occupancy of the source. The class covers single-server and sss-server queues, infinite-server queues, and networks of them, open or closed.

Setting

There are JJJ colonies, and a state is a vector n=(n1,…,nJ)n = (n_1,\dots,n_J)n=(n1​,…,nJ​) of non-negative integers, njn_jnj​ being the number of individuals in colony jjj. Three operators move one individual:

Tjkn  moves one from j to k,Tj→n  removes one from j,T→kn  adds one to k.T^{jk}n \ \text{ moves one from } j \text{ to } k, \qquad T^{j\to}n \ \text{ removes one from } j, \qquad T^{\to k}n \ \text{ adds one to } k .Tjkn  moves one from j to k,Tj→n  removes one from j,T→kn  adds one to k.

An open migration process is the Markov process on Z+J\mathbb{Z}_+^JZ+J​ with transition rates

q(n,Tjkn)=λjkφj(nj),q(n,Tj→n)=μjφj(nj),q(n,T→kn)=νk,q(n, T^{jk}n)=\lambda_{jk}\varphi_j(n_j), \qquad q(n, T^{j\to}n)=\mu_j\varphi_j(n_j), \qquad q(n, T^{\to k}n)=\nu_k ,q(n,Tjkn)=λjk​φj​(nj​),q(n,Tj→n)=μj​φj​(nj​),q(n,T→kn)=νk​,

where φj(0)=0\varphi_j(0)=0φj​(0)=0: nothing leaves an empty colony. Immigration into colony kkk is Poisson of rate νk\nu_kνk​. Taking μ≡0\mu\equiv 0μ≡0 and ν≡0\nu\equiv 0ν≡0 and restricting to states of a fixed total ∑jnj=N\sum_j n_j = N∑j​nj​=N gives a closed migration process. Setting φj(n)=min⁡(n,s)\varphi_j(n)=\min(n,s)φj​(n)=min(n,s) models an sss-server queue at colony jjj; φj(n)=n\varphi_j(n)=nφj​(n)=n models individuals moving independently.

The traffic equations define (αj)(\alpha_j)(αj​) from the rates. In the open case they are

αj(μj+∑kλjk)  =  νj+∑kαkλkj,j=1,…,J,\alpha_j\Bigl(\mu_j+\sum_k \lambda_{jk}\Bigr) \;=\; \nu_j+\sum_k \alpha_k\lambda_{kj}, \qquad j = 1,\dots,J,αj​(μj​+k∑​λjk​)=νj​+k∑​αk​λkj​,j=1,…,J,

and in the closed case αj∑kλjk=∑kαkλkj\alpha_j\sum_k \lambda_{jk}=\sum_k \alpha_k\lambda_{kj}αj​∑k​λjk​=∑k​αk​λkj​ with αj>0\alpha_j>0αj​>0 and ∑jαj=1\sum_j\alpha_j=1∑j​αj​=1. Finally set

gj=∑n=0∞αj n∏r=1nφj(r).g_j=\sum_{n=0}^{\infty}\frac{\alpha_j^{\,n}}{\prod_{r=1}^{n}\varphi_j(r)} .gj​=n=0∑∞​∏r=1n​φj​(r)αjn​​.

Formalization targets

Goal — Theorem 2.8, the product form of an open migration process

If g1,…,gJ<∞g_1,\dots,g_J<\inftyg1​,…,gJ​<∞ then

π(n)=∏j=1Jπj(nj),πj(m)=gj−1 αj m∏r=1mφj(r)\pi(n)=\prod_{j=1}^{J}\pi_j(n_j), \qquad \pi_j(m)=g_j^{-1}\,\frac{\alpha_j^{\,m}}{\prod_{r=1}^{m}\varphi_j(r)}π(n)=j=1∏J​πj​(nj​),πj​(m)=gj−1​∏r=1m​φj​(r)αjm​​

is an equilibrium distribution: it satisfies the equilibrium equations for the open migration rates, and it sums to one over Z+J\mathbb{Z}_+^JZ+J​. Both halves are asserted, because the first alone is satisfied by every positive multiple of π\piπ and the second is what makes the convergence hypothesis gj<∞g_j<\inftygj​<∞ do work.

Supporting levels

The closed-network product form of Theorem 2.4; the two families of partial balance equations (2.3) and (2.4) that the proof reduces to; Theorem 2.9, that the time reversal of a stationary open migration process is again an open migration process with rates λjk′=αkλkj/αj\lambda'_{jk}=\alpha_k\lambda_{kj}/\alpha_jλjk′​=αk​λkj​/αj​, μj′=νj/αj\mu'_j=\nu_j/\alpha_jμj′​=νj​/αj​ and νk′=αkμk\nu'_k=\alpha_k\mu_kνk′​=αk​μk​; the single M/M/1 queue that the chapter starts from; the cycle identity (2.6) behind Little's law; and the traffic equations of Kendall's family-size process, an open migration process with infinitely many colonies.

Significance

The result itself. Theorem 2.8 says that at a fixed time the occupancies n1,…,nJn_1,\dots,n_Jn1​,…,nJ​ of an open migration network are independent, each distributed as if its colony were fed by a Poisson stream of rate αjλj\alpha_j\lambda_jαj​λj​ — even though the actual arrival stream into a colony is in general not Poisson, and the occupancies are emphatically not independent as processes. That gap between the one-time-marginal and the process is the reason the theorem is useful and the reason it is easy to misapply. Everything downstream in the book rests on it: the loss networks of Chapter 3 are the truncation of a product-form process to a capacity set, and the flow-level models of Chapter 8 ask when a product form survives a bandwidth-sharing policy. Theorem 2.9 supplies the reversibility argument from which Burke's theorem and the Poisson character of the exit streams follow.

Formalizing it. The mathematics is classical — Jackson (1957), Whittle (1968), Kelly (1979) — and none of it is open. What the mission produces is a machine-checked model of a queueing network: the migration operators, the rate matrix, the traffic equations and the product form, in a form later missions in this series import rather than restate. Mathlib has no queueing theory and no theory of continuous-time Markov chains on a countable state space, so this is the first such development. It builds on the DetailedBalance / FullBalance layer published in mission I.

Difficulty

An open migration process is not reversible — the detailed balance equations fail, as Figure 2.5 of the book shows with an arrival stream of geometrically sized bursts — so the method of Chapter 1 does not apply and the equilibrium equations must be met head on. The content of the proof is that they split: a separate balance holds for each colony jjj (rate of individuals leaving colony jjj equals rate arriving into it) and one more across the boundary with the outside world, and each of those is equivalent to a traffic equation. Finding that split is the step, and it is why the partial balance equations are milestones in their own right.

The formal obstacle is different and worth naming. The equilibrium equation at a state nnn sums over the states that can jump into nnn, and the naive transcription ∑j,kπ(Tjkn)q(Tjkn,n)\sum_{j,k}\pi(T^{jk}n)q(T^{jk}n,n)∑j,k​π(Tjkn)q(Tjkn,n) silently assumes TjknT^{jk}nTjkn is a state, which fails when nj=0n_j=0nj​=0. Over Z+J\mathbb{Z}_+^JZ+J​ such a term must be dropped, and a formalization that keeps it — with nj−1n_j-1nj​−1 read as truncated subtraction — states something false.

Formalization scope

The state space is Fin J → ℕ, a function from a finite index type of colonies to occupancy counts, with J finite; no irreducibility is assumed, since none of the statements below need it. Rates are real-valued and the whole rate matrix is a single function of two states, assembled as a sum of indicator terms over the possible transitions, so the equilibrium equations can be stated as the FullBalance predicate of mission I, with unconditional sums over the countable state space. This is what avoids the trap above: a sum over actual states never includes a would-be-negative one, and any spurious coincidence of operators at a boundary carries a φj(0)=0\varphi_j(0)=0φj​(0)=0 factor and contributes nothing.

Conventions the development commits to: λjj=0\lambda_{jj}=0λjj​=0, so a transfer is always between distinct colonies; φj(0)=0\varphi_j(0)=0φj​(0)=0 and φj(r)>0\varphi_j(r)>0φj​(r)>0 for r≥1r\ge 1r≥1; αj>0\alpha_j>0αj​>0; and gjg_jgj​ is asserted via HasSum, which states convergence and the value at once, rather than as an extended real that might be infinite. Occupancy vectors use truncated natural subtraction, so the partial balance and reversed-rate statements carry an explicit nj≥1n_j\ge 1nj​≥1 where the book's state space carries it implicitly; the goal itself does not need such a guard.

A trivializing formalization is ruled out by the second conjunct of the goal: the equilibrium equations alone are a homogeneous linear condition satisfied by π≡0\pi\equiv 0π≡0, whereas the requirement that π\piπ sum to 111 forces the constants gjg_jgj​ to be exactly the ones stated.

Contributions welcome beyond the listed items: Burke's theorem (2.1) and the Poisson character of the exit streams, Corollary 2.10, the closed-form of the telephone banking example (Exercise 2.6), the Chinese restaurant process of Exercise 2.13, and Bartlett's theorem (2.17) on linear migration processes over a general space.

Selected references

  • Frank Kelly and Elena Yudovina, Stochastic Networks, Cambridge University Press, 2014, Chapter 2 (pp. 22–48); Theorems 2.4, 2.8, 2.9, 2.13, equations (2.1)–(2.6). DOI 10.1017/cbo9781139565363
  • James R. Jackson, Networks of waiting lines, Operations Research 5 (1957), 518–521. DOI 10.1287/opre.5.4.518
  • P. Whittle, Equilibrium distributions for an open migration process, Journal of Applied Probability 5 (1968), 567–571. DOI 10.2307/3211921
  • Frank Kelly, Reversibility and Stochastic Networks, Cambridge University Press, 2011 (reissue of the 1979 edition), Chapters 2 and 3.
  • David G. Kendall, Some problems in mathematical genealogy, in Perspectives in Probability and Statistics (J. Gani, ed.), Academic Press, 1975, 325–345.
  • John D. C. Little, A proof for the queuing formula: L=λWL = \lambda WL=λW, Operations Research 9 (1961), 383–387. DOI 10.1287/opre.9.3.383
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High-Dimensional Probability III: Grothendieck's InequalityTextbook

Motivation

Many hard combinatorial optimization problems — finding the maximum cut of a graph, deciding the ground state of an Ising spin system, bounding the correlation of a physical system — can be written as maximizing a bilinear form over sign vectors xi∈{−1,1}x_i \in \{-1, 1\}xi​∈{−1,1}. Exhaustive search over 2n2^n2n sign patterns is intractable, so practitioners relax the problem: replace each sign xix_ixi​ by a unit vector XiX_iXi​ in a higher-dimensional space and optimize the resulting inner products instead. This relaxation, a semidefinite program, is convex and solvable in polynomial time. The question is how much is lost in the relaxation — whether its optimal value can be far from the true, combinatorial optimum.

Grothendieck's inequality, proved by Alexander Grothendieck in 1953 in the context of Banach space theory (Résumé de la théorie métrique des produits tensoriels topologiques, Bol. Soc. Mat. São Paulo 8 (1953), 1–79), answers this for a broad class of such relaxations: replacing signs by unit vectors in an arbitrary Hilbert space changes the optimal value by at most an absolute, dimension-free constant factor. The inequality has since become a standard tool across combinatorial optimization, Banach space geometry, and (via the Goemans-Williamson algorithm for maximum cut, Section 3.6 of the source) approximation algorithms; see U. Haagerup, The Grothendieck inequality for bilinear forms on C∗C^*C∗-algebras, Adv. Math. 56 (1985) for the tightest known constant, and Alon–Naor, Approximating the cut-norm via Grothendieck's inequality, SIAM J. Comput. 35 (2006), for the algorithmic connection this mission's Theorem 3.5.6 sets up.

Setting

Fix positive integers m,nm, nm,n. Consider a real m×nm \times nm×n matrix A=(aij)A = (a_{ij})A=(aij​). Say AAA is normalized if for every choice of numbers x1,…,xm,y1,…,yn∈{−1,1}x_1, \dots, x_m, y_1, \dots, y_n \in \{-1, 1\}x1​,…,xm​,y1​,…,yn​∈{−1,1},

∣∑i=1m∑j=1naij xiyj∣  ≤  1.\Bigl| \sum_{i=1}^m \sum_{j=1}^n a_{ij}\, x_i y_j \Bigr| \;\le\; 1.​i=1∑m​j=1∑n​aij​xi​yj​​≤1.

This says AAA, viewed as a bilinear form on {−1,1}m×{−1,1}n\{-1,1\}^m \times \{-1,1\}^n{−1,1}m×{−1,1}n, has sup-norm at most 111. Now let HHH be any real Hilbert space — a real vector space equipped with an inner product ⟨⋅,⋅⟩\langle \cdot, \cdot \rangle⟨⋅,⋅⟩ complete in the induced norm — and consider vectors u1,…,um∈Hu_1, \dots, u_m \in Hu1​,…,um​∈H and v1,…,vn∈Hv_1, \dots, v_n \in Hv1​,…,vn​∈H, each of unit norm ∥ui∥=∥vj∥=1\|u_i\| = \|v_j\| = 1∥ui​∥=∥vj​∥=1. Replacing the scalar product xiyjx_i y_jxi​yj​ by the inner product ⟨ui,vj⟩\langle u_i, v_j \rangle⟨ui​,vj​⟩ in the same bilinear form gives ∑i,jaij⟨ui,vj⟩\sum_{i,j} a_{ij} \langle u_i, v_j \rangle∑i,j​aij​⟨ui​,vj​⟩, a real number depending on the choice of HHH and of the unit vectors. The question is how large this can be, uniformly over every such choice.

Formalization targets

Grothendieck's inequality (Theorem 3.5.1)

A normalized  ⟹  ∣∑i,jaij ⟨ui,vj⟩∣  ≤  KA \text{ normalized} \;\Longrightarrow\; \Bigl| \sum_{i,j} a_{ij}\, \langle u_i, v_j\rangle \Bigr| \;\le\; KA normalized⟹​i,j∑​aij​⟨ui​,vj​⟩​≤K

for every real Hilbert space HHH and unit vectors ui,vj∈Hu_i, v_j \in Hui​,vj​∈H, where KKK is a constant depending on neither AAA, its dimensions, nor HHH. This mission's goal formalizes the book's own first-pass bound K≤288K \le 288K≤288 (Section 3.5), proved by a Gaussian truncation argument; it does not fix a numeral for KKK, only that some absolute constant works, matching the shape of the true statement rather than a specific numeral that a sharper argument (the book's own Section 3.7 gives K≤1.783K \le 1.783K≤1.783) would immediately obsolete. See Formalization scope below for why this is the goal, not the sharper bound.

Significance

The result itself. Grothendieck's inequality is the single fact that makes semidefinite relaxation a provably good algorithmic strategy rather than a heuristic: whatever the true, hard-to-compute combinatorial optimum of a {−1,1}\{-1,1\}{−1,1}-valued bilinear optimization is, the tractable Hilbert-space relaxation cannot overshoot it by more than the constant KKK. Milestone Theorem 3.5.6 makes this concrete for positive-semidefinite matrices, showing the semidefinite relaxation SDP(A)(A)(A) of the integer program INT(A)(A)(A) satisfies INT(A)≤(A) \le(A)≤ SDP(A)≤2K⋅(A) \le 2K \cdot(A)≤2K⋅ INT(A)(A)(A) — the guarantee underlying the Goemans-Williamson 0.878-approximation algorithm for maximum cut (Theorem 3.6.5 of the source, out of scope for this mission; see Formalization scope).

Formalizing it. The inequality and its two chapter milestones are proved but not previously formalized on this platform (checked by concept search for "Grothendieck", "semidefinite", "positive-semidefinite", and "max-cut" — no hits beyond the unrelated Grothendieck-Teichmüller group). What remains after this mission is the sharper K≤1.783K \le 1.783K≤1.783 argument of Section 3.7 (the "kernel trick"), a separate, heavier development building on positive-definite kernels, and full proofs of every milestone below (currently open sorry goals).

Difficulty

The statement of Grothendieck's inequality contains no randomness, yet every known elementary proof is probabilistic; this is itself a striking feature of the result. The obvious approach — bound ∑i,jaij⟨ui,vj⟩\sum_{i,j} a_{ij}\langle u_i,v_j\rangle∑i,j​aij​⟨ui​,vj​⟩ directly by exploiting the normalization hypothesis on AAA — fails because the normalization hypothesis only controls AAA against sign vectors, and there is no way to project an arbitrary unit vector in a Hilbert space onto {−1,1}\{-1,1\}{−1,1} without losing information. The book's proof instead represents each unit vector ui,vju_i, v_jui​,vj​ via a scalar Gaussian random variable ⟨g,ui⟩\langle g, u_i\rangle⟨g,ui​⟩ for a single Gaussian vector ggg, recovering the inner products in expectation (Exercise 3.3.5); but these Gaussian variables are unbounded, so the normalization hypothesis (which bounds AAA against bounded ±1\pm 1±1 inputs) cannot be applied to them directly. The core technical step is a truncation argument: splitting each Gaussian variable into a bounded part and a small-L2L^2L2-norm unbounded remainder, applying the hypothesis to the bounded parts, and bounding the remainder terms by treating them as elements of the Hilbert space L2L^2L2 and invoking the very inequality being proved (Theorem 3.5.1 itself, applied with H=L2H = L^2H=L2) as a self-referential bootstrap — this is why the proof fixes KKK as the smallest valid constant before starting, rather than building it up from scratch.

Formalization scope

The goal and both milestones work with the real matrix and real inner product space directly; H is required to be a complete real inner product space (NormedAddCommGroup, InnerProductSpace ℝ, CompleteSpace), matching the book's "any Hilbert space." No dimension bound on HHH is imposed — the inequality's content is exactly that KKK does not grow with dim⁡H\dim HdimH.

This mission does not formalize the sharper K≤1.783K \le 1.783K≤1.783 bound of Section 3.7, nor Theorem 3.6.5 (the 0.878-approximation guarantee for maximum cut via randomized rounding): the latter's statement quantifies over "the result of a randomized rounding of the solution of the semidefinite program," which would drag a specific algorithm into the audited statement rather than keeping it a self-contained mathematical claim (the statement/proof-separation trap this series' triage rubric flags). Grothendieck's identity (Lemma 3.6.6), the key fact behind that rounding step, is included on its own as a milestone, stated with an explicit, named random sign variable rather than an opaque "rounding procedure."

A trivializing formalization would state the goal with KKK allowed to depend on AAA, mmm, nnn, or HHH — every such bound is easy (e.g. K=∑ij∣aij∣K = \sum_{ij} |a_{ij}|K=∑ij​∣aij​∣) and carries none of the theorem's content; the Lean statement rules this out by quantifying KKK before every other object. INT(A)\mathrm{INT}(A)INT(A) and SDP(A)\mathrm{SDP}(A)SDP(A) (Theorem 3.5.6) are defined from scratch in this chunk's namespace, using Matrix.PosSemidef from Mathlib for the positive-semidefiniteness hypothesis (which bundles the real-symmetric condition); Mathlib has no ready-made SDP-value construction to reuse. The sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm used by Theorem 3.1.1 is reused, unchanged, from the 01-concentration mission in this series (HighDimProb.Concentration.SubgaussianNorm) rather than redefined.

Selected references

  • A. Grothendieck, Résumé de la théorie métrique des produits tensoriels topologiques, Bol. Soc. Mat. São Paulo 8 (1953), 1–79.
  • U. Haagerup, The Grothendieck inequality for bilinear forms on C∗C^*C∗-algebras, Adv. Math. 56 (1985), 93–116.
  • N. Alon, A. Naor, Approximating the cut-norm via Grothendieck's inequality, SIAM J. Comput. 35 (2006), 787–803.
  • M. X. Goemans, D. P. Williamson, Improved approximation algorithms for maximum cut and satisfiability problems using semidefinite programming, J. ACM 42 (1995), 1115–1145.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 3, DOI 10.1017/9781108231596.
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High-Dimensional Probability V: The Johnson-Lindenstrauss LemmaTextbook

Motivation

Any dataset of NNN points can be described exactly by embedding it in Rn\mathbb R^nRn for nnn large enough — but a large nnn is expensive: nearest-neighbor search, clustering, and streaming algorithms all scale with the ambient dimension, not with NNN. The question that opens this mission is whether the dimension can be cut down while leaving the data's geometry — the pairwise distances between points — essentially untouched.

Johnson and Lindenstrauss answered this in 1984, while studying extensions of Lipschitz maps into Hilbert space (W. Johnson, J. Lindenstrauss, Extensions of Lipschitz mappings into a Hilbert space, Contemp. Math. 26 (1984), 189–206): NNN points in any Euclidean space, of any dimension nnn, can be mapped by a single linear map into a space of dimension only O(ε−2log⁡N)O(\varepsilon^{-2}\log N)O(ε−2logN), distorting every pairwise distance by at most a factor of 1±ε1\pm\varepsilon1±ε. The map does not depend on the data beyond its cardinality — a single random object works simultaneously for the whole point set with high probability. This is now one of the standard tools of randomized dimension reduction, cited across nearest-neighbor search, streaming linear algebra, compressed sensing, and machine learning pipelines that need to shrink feature dimension before a downstream algorithm runs.

Setting

Fix a probability space (Ω,F,Prob)(\Omega,\mathcal F,\mathrm{Prob})(Ω,F,Prob). A random orthogonal projection of rank mmm in Rn\mathbb R^nRn is a map P:Ω→(Rn→Rn)P:\Omega\to(\mathbb R^n\to\mathbb R^n)P:Ω→(Rn→Rn), continuous and linear for each ω\omegaω, such that almost surely PωP_\omegaPω​ is idempotent (Pω∘Pω=PωP_\omega\circ P_\omega = P_\omegaPω​∘Pω​=Pω​), self-adjoint, and has range of dimension mmm — i.e. PωP_\omegaPω​ is the orthogonal projection onto some mmm-dimensional subspace Eω⊂RnE_\omega\subset\mathbb R^nEω​⊂Rn. It is uniformly distributed in the Grassmannian Gn,mG_{n,m}Gn,m​ (written E∼Unif(Gn,m)E\sim\mathrm{Unif}(G_{n,m})E∼Unif(Gn,m​)) when its law is rotation invariant: for every orthogonal transformation UUU of Rn\mathbb R^nRn, the conjugated map ω↦U∘Pω∘U−1\omega\mapsto U\circ P_\omega\circ U^{-1}ω↦U∘Pω​∘U−1 has the same law as PPP. Conjugating a projection by UUU is exactly the projection onto the image of its range under UUU, so this says the law of the random subspace E=range(P)E=\mathrm{range}(P)E=range(P) is invariant under the full orthogonal group — the operational definition Vershynin himself uses for a "uniformly distributed" random subspace, since no coordinate-free formula for such a subspace's law is given directly.

A companion notion drives the proof: a random vector XXX is uniform on the Euclidean sphere of radius rrr, X∼Unif(r Sn−1)X\sim\mathrm{Unif}(r\,S^{n-1})X∼Unif(rSn−1), when it lies on that sphere almost surely and its law is likewise rotation invariant. And a real random variable YYY is sub-gaussian with sub-gaussian (ψ2\psi_2ψ2​) norm ∥Y∥ψ2:=inf⁡{t>0:Eexp⁡(Y2/t2)≤2}\|Y\|_{\psi_2} := \inf\{t>0:\mathbb E\exp(Y^2/t^2)\le 2\}∥Y∥ψ2​​:=inf{t>0:Eexp(Y2/t2)≤2}, the standard non-asymptotic measure of how light-tailed YYY's distribution is (a bounded or Gaussian random variable has finite ψ2\psi_2ψ2​ norm; the tail probability P{∣Y∣≥s}\mathbb P\{|Y|\ge s\}P{∣Y∣≥s} then decays at least as fast as 2exp⁡(−cs2/∥Y∥ψ22)2\exp(-cs^2/\|Y\|_{\psi_2}^2)2exp(−cs2/∥Y∥ψ2​2​)).

Formalization targets

Goal (Theorem 5.3.1, Johnson-Lindenstrauss Lemma)

∃ C,c>0:m≥Cε2log⁡∣X∣  ⟹  Prob{∀x,y∈X: (1−ε)∥x−y∥2≤∥nm Pω(x−y)∥2≤(1+ε)∥x−y∥2}  ≥  1−2exp⁡(−cε2m)\exists\,C,c>0:\quad m\ge\frac{C}{\varepsilon^2}\log|X| \;\Longrightarrow\; \mathrm{Prob}\Bigl\{\forall x,y\in X:\ (1-\varepsilon)\|x-y\|_2\le \bigl\|\sqrt{\tfrac nm}\,P_\omega(x-y)\bigr\|_2\le(1+\varepsilon)\|x-y\|_2\Bigr\} \;\ge\;1-2\exp(-c\varepsilon^2 m)∃C,c>0:m≥ε2C​log∣X∣⟹Prob{∀x,y∈X: (1−ε)∥x−y∥2​≤​mn​​Pω​(x−y)​2​≤(1+ε)∥x−y∥2​}≥1−2exp(−cε2m)

for every finite X⊂RnX\subset\mathbb R^nX⊂Rn, every ε>0\varepsilon>0ε>0, and every random orthogonal projection PPP of rank mmm uniformly distributed in Gn,mG_{n,m}Gn,m​. The universal quantifier over pairs x,y∈Xx,y\in Xx,y∈X sits inside the single probability event — this is the union-bound content that makes the statement a genuine simultaneous guarantee for the whole point set, not a restatement of the single-vector lemma below for one fixed pair. Both constants are the book's own unnamed absolute constants, never depending on nnn, mmm, N=∣X∣N=|X|N=∣X∣, or ε\varepsilonε; this is the weakest stable form of the claim (no numeral is hard-coded for CCC or ccc), matching the book's own statement exactly.

Significance

The lemma gives a universal, data-oblivious dimension-reduction guarantee: the target dimension m=O(ε−2log⁡N)m=O(\varepsilon^{-2}\log N)m=O(ε−2logN) depends only on the number of points and the desired distortion, never on the ambient dimension nnn or on the geometry of the specific point set. This is what makes it usable as a black-box preprocessing step ahead of an algorithm whose cost scales with nnn — the projection is drawn once, without looking at the data, and works with high probability for every pairwise distance simultaneously. The bound is also known to be essentially optimal in NNN: Alon (Problems and results in extremal combinatorics, Discrete Math. 273 (2003)) showed a lower bound of Ω(ε−2log⁡N/log⁡(1/ε))\Omega(\varepsilon^{-2}\log N/\log(1/\varepsilon))Ω(ε−2logN/log(1/ε)) on the target dimension, so the log⁡N\log NlogN dependence cannot be removed.

The theorem itself has been proved for decades and admits several proof strategies (this book's route through Lipschitz concentration on the sphere; the original volume/measure-concentration argument; later "sparse" or structured variants of the projection for faster computation). This mission formalizes the classical dense-Gaussian-projection proof route as Vershynin presents it, building the sphere-concentration engine (Theorem 5.1.4) and the single-vector projection lemma (Lemma 5.3.2) that the union-bound argument for the goal rests on. No machine-checked formal proof of this chain is known to exist on the platform prior to this mission (see Formalization scope below); what is contributed is the statement infrastructure — the goal and its two direct supporting lemmas, stated with explicit, unpinned absolute constants — for solvers to close.

Difficulty

The natural first idea — bound the distortion of a single fixed vector under a random projection, then take a union bound over the (N2)\binom N2(2N​) pairwise differences — is exactly the strategy Lemma 5.3.2 and the goal use, but it does not by itself explain why the single-vector concentration bound (Lemma 5.3.2(b)) holds with the stated sub-gaussian-type tail. That bound is not elementary: it reduces to a uniform concentration statement for an arbitrary Lipschitz function of a uniformly random point on a high-dimensional sphere (Theorem 5.1.4), since ∥Pz∥2\|Pz\|_2∥Pz∥2​, viewed as a function of a rotated copy of zzz, is a 111-Lipschitz function on the sphere. Proving that every Lipschitz function concentrates — not just linear ones, for which sub-gaussianity was already established in Chapter 3 — needs a genuinely different tool: comparing the sub-level sets of an arbitrary Lipschitz function to spherical caps via an isoperimetric inequality on the sphere. This geometric input is what makes the concentration phenomenon behind Johnson-Lindenstrauss a dimension-free fact rather than a special property of coordinate projections.

Formalization scope

XXX is a Finset of points in EuclideanSpace ℝ (Fin n), matching "a set of NNN points"; NNN is read off as X.card. The random subspace E∈Gn,mE\in G_{n,m}E∈Gn,m​ is represented throughout by the orthogonal projection PPP onto it (IsUniformProjection), following the book's own statements, which are phrased in terms of PPP rather than EEE; the scaled map Q=n/m PQ=\sqrt{n/m}\,PQ=n/m​P of the goal is written Real.sqrt (n/m) • P ω applied to x - y, using linearity of PωP_\omegaPω​ to realize Qx−Qy=Q(x−y)Qx-Qy = Q(x-y)Qx−Qy=Q(x−y). Both "uniform on the sphere" and "uniform in the Grassmannian" are defined operationally by rotation invariance of the underlying law, since Mathlib has no ready-made normalized surface measure on a general-radius Euclidean sphere or Haar-measure construction on the Grassmannian/orthogonal group to build a canonical uniform object from; rotation invariance uniquely determines the corresponding measure among those supported on the relevant set, so the operational and constructive definitions coincide extensionally. Every "absolute constant" in the book (CCC in Theorem 5.3.1's sample-complexity hypothesis, ccc in every failure-probability bound, and the sub-gaussian constant CCC of Theorem 5.1.4) is existentially quantified ahead of the dimension, sample size, and every other object, and pinned to no numeral — a formalization that hard-coded a specific numeral for any of these would be invalidated by the next sharper constant in the literature and would not match what the book actually proves.

A trivializing formalization is one that states the conclusion for a single fixed pair x,yx,yx,y rather than universally over all pairs inside one event; that would collapse the union-bound content that makes this a dimension-reduction statement for a whole point set (with NNN points), rather than a restatement of the single-vector Lemma 5.3.2(b). This mission's goal statement is built to rule that out explicitly (see Formalization targets above).

Reusable infrastructure: subgaussianNorm (the Orlicz ψ2\psi_2ψ2​ norm, restated per Vershynin Definition 2.5.6) and the rotation-invariance idiom for "uniformly distributed" random geometric objects are of independent interest to any later chapter needing sub-gaussian random vectors or random subspaces/projections (e.g. Chapters 4, 6, 7, 9, 11 of this same book series). Solvers' contributions are welcome on: the isoperimetric inequality on the sphere and its use to prove Theorem 5.1.4 (the mission's hardest open leaf); the coordinate-projection computation underlying Lemma 5.3.2(a); and the concentration-plus-union-bound argument closing the goal from the three supporting lemmas.

Selected references

  • W. Johnson, J. Lindenstrauss, Extensions of Lipschitz mappings into a Hilbert space, Contemporary Mathematics 26 (1984), 189–206.
  • N. Alon, Problems and results in extremal combinatorics, I, Discrete Mathematics 273 (2003), 31–53. https://doi.org/10.1016/S0012-365X(03)00227-9
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 5. https://doi.org/10.1017/9781108231596
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Supermodularity and Complementarity II: Topkis's Monotonicity Theorem for Parameterized OptimizationTextbook

Motivation

A recurring question in economics and operations research is: when a decision problem depends on a parameter, does the optimal decision move monotonically as the parameter changes? A firm's optimal input mix as a price rises, a consumer's optimal consumption bundle as income grows, a Cournot firm's optimal output as a rival's output changes — in each case one wants "more of the parameter implies (weakly) more of the optimum" without assuming convexity, differentiability, or a unique optimizer. The classical tool for such comparative statics questions is the implicit function theorem, which needs smoothness and a nondegenerate Hessian and breaks down the moment the optimum is not unique or the objective is not differentiable. Topkis [1978] showed that a purely order-theoretic condition — supermodularity of the objective jointly in the decision variable and the parameter — is sufficient on its own, with no smoothness, uniqueness, or convexity assumed at all, and Milgrom and Roberts [1990a, 1994] later showed this lattice-theoretic approach subsumes and strengthens the classical monotone-comparative-statics results in economics. This mission formalizes the two central results this book calls "Topkis's theorem" (Theorem 2.8.1 and Theorem 2.8.2), together with the structural fact about maximizers of a supermodular function (Theorem 2.7.1) that both rest on, and the strengthening to strictly ordered optimal selections (Theorem 2.8.4).

Setting

Let XXX be a lattice: a partially ordered set (X,⪯)(X, \preceq)(X,⪯) in which every pair x,x′x, x'x,x′ has a join x∨x′x \vee x'x∨x′ and a meet x∧x′x \wedge x'x∧x′. A real-valued function f:X→Rf : X \to \mathbb{R}f:X→R is supermodular on XXX if f(x′)+f(x′′)≤f(x′∨x′′)+f(x′∧x′′)f(x') + f(x'') \le f(x' \vee x'') + f(x' \wedge x'')f(x′)+f(x′′)≤f(x′∨x′′)+f(x′∧x′′) for all x′,x′′∈Xx', x'' \in Xx′,x′′∈X; this is the same relativized notion (SupermodularOn) used, with S=XS = XS=X, throughout chunk I of this series.

Now let TTT also be a partially ordered set (the parameter set), and let f:X×T→Rf : X \times T \to \mathbb{R}f:X×T→R be a real-valued function of the pair (x,t)(x, t)(x,t). fff has increasing differences in (x,t)(x, t)(x,t) if, for every t′≺t′′t' \prec t''t′≺t′′ in TTT, the map x↦f(x,t′′)−f(x,t′)x \mapsto f(x, t'') - f(x, t')x↦f(x,t′′)−f(x,t′) is monotone (order-preserving) in xxx; equivalently, the marginal gain from raising ttt is itself increasing in xxx. Replacing "monotone" with "strictly monotone" gives strictly increasing differences. To compare the resulting sets of optimizers rather than single points, this mission reuses the induced set ordering ⊑\sqsubseteq⊑ from chunk I: for A,B⊆XA, B \subseteq XA,B⊆X, A⊑BA \sqsubseteq BA⊑B holds when a∧b∈Aa \wedge b \in Aa∧b∈A and a∨b∈Ba \vee b \in Ba∨b∈B for all a∈Aa \in Aa∈A, b∈Bb \in Bb∈B.

Formalization targets

Goal — Theorem 2.8.2 (Topkis's theorem)

Let XXX and TTT be lattices, let SSS be a sublattice of the product lattice X×TX \times TX×T, and let St={x∈X:(x,t)∈S}S_t = \{x \in X : (x, t) \in S\}St​={x∈X:(x,t)∈S} be the section of SSS at t∈Tt \in Tt∈T. If f:X×T→Rf : X \times T \to \mathbb{R}f:X×T→R is supermodular on SSS (jointly in the pair (x,t)(x, t)(x,t)), then

t  ⟼  argmax⁡x∈Stf(x,t)t \;\longmapsto\; \operatorname{argmax}_{x \in S_t} f(x, t)t⟼argmaxx∈St​​f(x,t)

is increasing in ttt, with respect to ⊑\sqsubseteq⊑, on {t∈T:argmax⁡x∈Stf(x,t)≠∅}\{t \in T : \operatorname{argmax}_{x \in S_t} f(x, t) \neq \emptyset\}{t∈T:argmaxx∈St​​f(x,t)=∅}.

Theorem 2.8.1 (the underlying, more elementary sufficient condition)

With St⊆XS_t \subseteq XSt​⊆X increasing in ttt (with respect to ⊑\sqsubseteq⊑), f(x,t)f(x,t)f(x,t) supermodular in xxx for each fixed ttt, and f(x,t)f(x,t)f(x,t) having increasing differences in (x,t)(x,t)(x,t) on X×TX \times TX×T, the same conclusion — t↦argmax⁡x∈Stf(x,t)t \mapsto \operatorname{argmax}_{x \in S_t} f(x,t)t↦argmaxx∈St​​f(x,t) increasing in ⊑\sqsubseteq⊑ — holds. Theorem 2.8.2's joint-supermodularity hypothesis on a sublattice of X×TX \times TX×T automatically forces both of Theorem 2.8.1's hypotheses, so 2.8.1 is the logically weaker, more elementary statement from which 2.8.2's proof proceeds.

Theorem 2.8.4 (strict strengthening)

Under the hypotheses of Theorem 2.8.1 but with strictly increasing differences, every individual optimal solution at a larger parameter value dominates every individual optimal solution at a smaller one: t′≺t′′t' \prec t''t′≺t′′, x′∈argmax⁡x∈St′f(x,t′)x' \in \operatorname{argmax}_{x \in S_{t'}} f(x,t')x′∈argmaxx∈St′​​f(x,t′), and x′′∈argmax⁡x∈St′′f(x,t′′)x'' \in \operatorname{argmax}_{x \in S_{t''}} f(x,t'')x′′∈argmaxx∈St′′​​f(x,t′′) together force x′⪯x′′x' \preceq x''x′⪯x′′ — a genuinely stronger conclusion than ⊑\sqsubseteq⊑ alone gives.

A supporting result is formalized as a milestone because both goals' proofs use it directly: Theorem 2.7.1, that argmax⁡x∈Xf(x)\operatorname{argmax}_{x \in X} f(x)argmaxx∈X​f(x) is a sublattice of XXX whenever fff is supermodular on XXX — the structural fact that makes it meaningful to compare optimal-solution sets with ⊑\sqsubseteq⊑ in the first place.

Significance

The result itself. Theorem 2.8.2 is the book's own headline theorem, cited throughout the rest of the monograph: it underlies the assortative-matching existence theorem (Chapter 3), monotone optimal policies in Markov decision processes (Chapter 3), and equilibrium comparative statics in supermodular games (Chapter 4) — each a later mission in this series. Its distinguishing feature relative to the implicit function theorem is that it needs no differentiability, no uniqueness of the optimizer, and no interiority: it applies equally to discrete decision problems (integer programming, combinatorial selection) and continuous ones.

Formalizing it. Nothing in Mathlib currently states a parametric monotone-comparative- statics result of this shape: the closest neighboring material (order-preserving maps, MonotoneOn, lattice structures) supplies only the vocabulary, not the theorem. This mission is the first formalization of Topkis's theorem on this platform and introduces the increasing-differences vocabulary (IncreasingDifferencesOn, StrictlyIncreasingDifferencesOn) that later missions in this series (matching, MDPs, supermodular games) reuse directly.

Difficulty

The natural first idea — differentiate fff in xxx, set the gradient to zero, and use the implicit function theorem on the resulting first-order condition — fails immediately because nothing here is assumed differentiable, and argmax⁡x∈Stf(x,t)\operatorname{argmax}_{x \in S_t} f(x,t)argmaxx∈St​​f(x,t) need not be a single point. The correct argument instead compares two arbitrary elements x′∈St′x' \in S_{t'}x′∈St′​, x′′∈St′′x'' \in S_{t''}x′′∈St′′​ directly through the supermodularity inequality applied to the pair (x′,t′)(x', t')(x′,t′) against (x′∨x′′,t′)(x' \vee x'', t')(x′∨x′′,t′) (a chain of inequalities Topkis calls "Lemma 2.8.1"), using increasing differences only to move the parameter from t′t't′ to t′′t''t′′ inside that chain — at no point is a derivative, a selection function, or an interior point used. A second subtlety is that "increasing" in the conclusion is with respect to the induced set order ⊑\sqsubseteq⊑, not a claim that some selection t↦x(t)t \mapsto x(t)t↦x(t) is monotone: proving the stronger, pointwise-ordered conclusion (Theorem 2.8.4) genuinely needs the strict form of increasing differences, not merely increasing differences plus an extra hypothesis.

Formalization scope

XXX and TTT are kept as abstract Lattice/PartialOrder types throughout, matching the book's own generality — Theorem 2.8.1's and 2.8.2's Rn\mathbb{R}^nRn/Rm\mathbb{R}^mRm corollary via second partial derivatives (discussed in the book's prose immediately after Theorem 2.8.2, p. 77) is not itself a numbered theorem and is not formalized here. Supermodularity, increasing differences, and strictly increasing differences are each formalized as a single relativized definition (SupermodularOn f S, IncreasingDifferencesOn f S, StrictlyIncreasingDifferencesOn f S) so the same declaration expresses both "supermodular on the whole lattice XXX" (used by Theorem 2.7.1 and Theorem 2.8.1's per-ttt hypothesis) and "jointly supermodular on a sublattice SSS of X×TX \times TX×T" (Theorem 2.8.2) — a formalization that instead only ever supermodularized f(⋅,t)f(\cdot, t)f(⋅,t) for fixed ttt would collapse Theorem 2.8.2's genuinely joint hypothesis into a restatement of Theorem 2.8.1, which is exactly the trivialization this mission's chunk brief warns against. argmax⁡x∈Stf(x,t)\operatorname{argmax}_{x \in S_t} f(x,t)argmaxx∈St​​f(x,t) is written out as the set of x∈Stx \in S_tx∈St​ that dominate every other element of StS_tSt​ under f(⋅,t)f(\cdot, t)f(⋅,t), and every conclusion is stated only for pairs t⪯t′t \preceq t't⪯t′ at which both argmax sets are assumed nonempty — matching the book's own restriction to {t∈T:argmax⁡x∈Stf(x,t)≠∅}\{t \in T : \operatorname{argmax}_{x \in S_t} f(x,t) \neq \emptyset\}{t∈T:argmaxx∈St​​f(x,t)=∅}, since ⊑\sqsubseteq⊑ holds vacuously whenever either side is empty. This mission depends on chunk I's InducedSetOrder; it introduces no reusable infrastructure beyond its own three definitions, which later missions in the series (matching, MDPs, supermodular games) are expected to import directly rather than redefine.

Selected references

  • Topkis, D. M., Minimizing a submodular function on a lattice, Operations Research 26(2), 1978, pp. 305–321. https://doi.org/10.1287/opre.26.2.305
  • Topkis, D. M., Supermodularity and Complementarity, Princeton University Press, 2011 (DOI 10.1515/9781400822539), Chapter 2, §2.6–2.8.
  • Milgrom, P. and Shannon, C., Monotone comparative statics, Econometrica 62(1), 1994, pp. 157–180. https://doi.org/10.2307/2951479
  • Milgrom, P. and Roberts, J., Rationalizability, learning, and equilibrium in games with strategic complementarities, Econometrica 58(6), 1990, pp. 1255–1277. https://doi.org/10.2307/2938316
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Introduction to Stochastic Programming II: The Value of Perfect Information and of the Stochastic SolutionTextbook

Motivation

Every stochastic program is, in practice, compared against a shortcut. A decision maker facing genuine uncertainty is tempted either to replace the random data by its mean and solve one deterministic problem, or to imagine that perfect information about the future were available and solve a separate deterministic problem per scenario. Both temptations have precise answers: the expected value of perfect information (EVPI) measures how much a decision maker should be willing to pay for a perfect forecast, and the value of the stochastic solution (VSS) measures the cost of ignoring uncertainty altogether by solving the mean-value problem. Both concepts originate in decision analysis — EVPI traces to Raiffa and Schlaifer (1961) — and were brought into stochastic programming by Madansky (1960), who proved the first chain of inequalities relating the wait-and-see value, the recourse value and the expected-value-solution's cost. Birge and Louveaux, Introduction to Stochastic Programming, 2nd ed. (Springer, 2011), Chapter 4, gives the standard modern treatment, including a refined family of bounds — built from pairs subproblems against a chosen reference scenario — that sharpen VSS beyond the original mean-scenario comparison. This mission formalizes that chapter's capstone: the five-quantity, four-inequality chain that pins VSS between two computable optimal values.

Setting

Fix a two-stage stochastic program with fixed recourse: a finite family of K scenarios ξ1,…,ξK\xi_1,\dots,\xi_Kξ1​,…,ξK​ in Rd\mathbb R^dRd, each occurring with probability pk≥0p_k \ge 0pk​≥0, ∑kpk=1\sum_k p_k = 1∑k​pk​=1; a first-stage feasible set K1⊆Rn1K_1 \subseteq \mathbb R^{n_1}K1​⊆Rn1​; and, for every first-stage decision x∈Rn1x \in \mathbb R^{n_1}x∈Rn1​ and every scenario ξ∈Rd\xi \in \mathbb R^dξ∈Rd, a scenario cost z(x,ξ)z(x,\xi)z(x,ξ) — the optimal value of cTx+min⁡{qTy∣Wy=h(ξ)−Tx, y≥0}c^Tx + \min\{q^Ty \mid Wy = h(\xi) - Tx,\ y \ge 0\}cTx+min{qTy∣Wy=h(ξ)−Tx, y≥0}. By convention z(x,ξ)=+∞z(x,\xi) = +\inftyz(x,ξ)=+∞ when xxx has no feasible second-stage recourse under ξ\xiξ, and z(x,ξ)=−∞z(x,\xi) = -\inftyz(x,ξ)=−∞ when the second-stage program is unbounded below.

From zzz, five basic quantities are defined (Birge & Louveaux §4.1–§4.2):

  • The recourse problem's value, RP=min⁡x∈K1Eξ z(x,ξ)RP = \min_{x \in K_1} \mathbb E_\xi\, z(x,\xi)RP=minx∈K1​​Eξ​z(x,ξ) — the best a decision maker can do without foreknowledge of ξ\xiξ (the "here-and-now" solution).
  • The wait-and-see value, WS=Eξ[min⁡x∈K1z(x,ξ)]WS = \mathbb E_\xi\big[\min_{x \in K_1} z(x,\xi)\big]WS=Eξ​[minx∈K1​​z(x,ξ)] — the average cost if ξ\xiξ were revealed before choosing xxx.
  • The expected value of perfect information, EVPI=RP−WSEVPI = RP - WSEVPI=RP−WS.
  • The expected value problem's solution xˉ(ξˉ)\bar x(\bar\xi)xˉ(ξˉ​), optimal for the deterministic problem at the mean scenario ξˉ=E(ξ)\bar\xi = \mathbb E(\xi)ξˉ​=E(ξ); its recourse cost, the expected result of using the EV solution, is EEV=Eξ z(xˉ(ξˉ),ξ)EEV = \mathbb E_\xi\, z(\bar x(\bar\xi), \xi)EEV=Eξ​z(xˉ(ξˉ​),ξ).
  • The value of the stochastic solution, VSS=EEV−RPVSS = EEV - RPVSS=EEV−RP — the extra cost of implementing the mean-scenario decision instead of solving the recourse problem.

Section 4.6 refines VSS by replacing the mean scenario with an arbitrary reference scenario ξr\xi^rξr (not necessarily one of the KKK possible scenarios, e.g. a worst case), with assumed probability pr=P(ξ=ξr)p_r = P(\xi=\xi^r)pr​=P(ξ=ξr):

  • xˉr\bar x^rxˉr, optimal for min⁡x∈K1z(x,ξr)\min_{x\in K_1} z(x,\xi^r)minx∈K1​​z(x,ξr), gives the expected value of the reference-scenario solution, EVRS=Eξ z(xˉr,ξ)EVRS = \mathbb E_\xi\, z(\bar x^r,\xi)EVRS=Eξ​z(xˉr,ξ), and the generalized VSS=EVRS−RPVSS = EVRS - RPVSS=EVRS−RP.
  • For each scenario ξk\xi^kξk, the pairs subproblem of ξr\xi^rξr and ξk\xi^kξk treats them as a two-point distribution with weights prp_rpr​ and 1−pr1-p_r1−pr​: its optimal value is min⁡x∈K1[pr z(x,ξr)+(1−pr) z(x,ξk)]\min_{x\in K_1}\big[p_r\,z(x,\xi^r) + (1-p_r)\,z(x,\xi^k)\big]minx∈K1​​[pr​z(x,ξr)+(1−pr​)z(x,ξk)], attained at some xˉk\bar x^kxˉk. Averaging these optimal values over kkk (rescaled by 1/(1−pr)1/(1-p_r)1/(1−pr​)) gives the sum of pairs expected values, SPEVSPEVSPEV. Taking, instead, the smallest full expected cost Eξ z(xˉk,ξ)\mathbb E_\xi\,z(\bar x^k,\xi)Eξ​z(xˉk,ξ) among the K+1K{+}1K+1 candidate solutions {xˉ1,…,xˉK,xˉr}\{\bar x^1,\dots,\bar x^K,\bar x^r\}{xˉ1,…,xˉK,xˉr} gives the expectation of pairs expected value, EPEVEPEVEPEV.

Formalization targets

Goal — Chapter 4, Theorem 9 (p. 174)

0  ≤  EVRS−EPEV  ≤  VSS  ≤  EVRS−SPEV  ≤  EVRS−WS.0 \;\le\; EVRS - EPEV \;\le\; VSS \;\le\; EVRS - SPEV \;\le\; EVRS - WS .0≤EVRS−EPEV≤VSS≤EVRS−SPEV≤EVRS−WS.

Four links, each with independent content: nonnegativity of the leftmost gap, then two genuine inequalities (from the pairs-subproblem comparisons of Propositions 7 and 8), then the identity VSS=EVRS−RPVSS = EVRS - RPVSS=EVRS−RP folded against RP≥WSRP \ge WSRP≥WS's reverse-direction cousin. This is the weakest statement that keeps all five quantities distinct — stating only the outer bound 0≤VSS≤EVRS−WS0 \le VSS \le EVRS-WS0≤VSS≤EVRS−WS would erase exactly the refinement (via pairs subproblems) that makes the chapter's method useful.

Supporting propositions (milestones, in attack order)

  • Proposition 1 (p. 166): WS≤RP≤EEVWS \le RP \le EEVWS≤RP≤EEV.
  • Proposition 5(a) (pp. 167–168): 0≤EVPI0 \le EVPI0≤EVPI and 0≤VSS0 \le VSS0≤VSS (mean-scenario form), for any stochastic program.
  • Proposition 7 (p. 173): WS≤SPEV≤RPWS \le SPEV \le RPWS≤SPEV≤RP.
  • Proposition 8 (p. 174): RP≤EPEV≤EVRSRP \le EPEV \le EVRSRP≤EPEV≤EVRS.

Significance

The chain gives a decision maker two computable, non-obvious bounds on VSS — a quantity that is otherwise expensive to pin down exactly, since RPRPRP itself already requires solving the full recourse problem. EVRS−EPEVEVRS - EPEVEVRS−EPEV and EVRS−SPEVEVRS - SPEVEVRS−SPEV are both computable from K+1K+1K+1 (or KKK) two-scenario LPs, far cheaper than the full KKK-scenario recourse problem, so Theorem 9 turns an expensive exact quantity into a pair of cheap certified bounds. Formalizing it fixes, once and for all, the exact hypotheses and quantifier structure of Madansky's original inequality (Proposition 1) together with the later pairs-subproblem refinement (Propositions 6–8, Birge 1982), often cited informally as "the VSS bounds" without distinguishing EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV and SPEVSPEVSPEV. No part of this chain is on Mathlib or Formalpedia today (checked by concept query, not title); this is a first, from-scratch treatment of two-stage recourse value-of-information theory as formal objects.

Difficulty

The obvious first idea — collapse RPRPRP, WSWSWS, EVEVEV, EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV, SPEVSPEVSPEV to one "the optimal value of the LP" and prove a single inequality — throws away the entire content of the chapter. Each quantity restricts the minimization to a different feasible object: RPRPRP minimizes jointly over xxx; WSWSWS swaps the order of min⁡\minmin and E\mathbb EE; EEVEEVEEV/EVRSEVRSEVRS evaluate one fixed xxx under every scenario; SPEVSPEVSPEV and EPEVEPEVEPEV each minimize over a family of pairs subproblems rather than the full KKK-scenario problem. The chain's proof (Propositions 7–8) depends on this precisely: Proposition 7's lower bound uses that each pairs-subproblem-optimal (xˉk,yˉk)(\bar x^k,\bar y^k)(xˉk,yˉ​k) is feasible (not necessarily optimal) for the single-scenario problem at ξr\xi^rξr, and its upper bound uses that the recourse-optimal (x∗,y∗(ξr),y∗(ξk))(x^*, y^*(\xi^r), y^*(\xi^k))(x∗,y∗(ξr),y∗(ξk)) is feasible (not necessarily optimal) for the pairs subproblem — a feasible-but-not-optimal argument in each direction, not a direct comparison of objective values. Losing track of which solution is fixed and which is optimized destroys the argument entirely.

Formalization scope

An Instance bundles the finite scenario set (Fin K, probabilities p : Fin K → ℝ with p ≥ 0, ∑ p = 1, scenarios xi : Fin K → (Fin d → ℝ)), the first-stage feasible set K1 : Set (Fin n1 → ℝ), and the scenario cost z : (Fin n1 → ℝ) → (Fin d → ℝ) → EReal, using the extended reals to carry the book's own +∞/−∞ conventions for infeasibility and unboundedness rather than silently restricting to a finite-valued special case (a genuine risk of trivialization here, since Example 2 of the chapter exhibits EEV=+∞EEV = +\inftyEEV=+∞). All optimal values (RP, WS, EV, EVPI, EEV, VSS, EVRS, generalized VSS, SPEV, EPEV) are defined directly from z, matching the book's own level of abstraction in this chapter (which never unfolds z into the underlying LP's A,b,c,q,W,T,hA,b,c,q,W,T,hA,b,c,q,W,T,h data — those appear only in Chapter 3). Because EEV, the mean-scenario VSS, EVRS, the generalized VSS, and EPEV are each defined relative to an optimal solution of some sub-problem — the book itself only ever says "let xˉ(ξˉ)\bar x(\bar\xi)xˉ(ξˉ​) denote some optimal solution" — every theorem using them states that solution and its optimality as explicit hypotheses (x ∈ K1 and z x … = ⨅ …), never baking it into a Classical.choiced value; this keeps the quantifier structure faithful to the book's own "let ... be an optimal solution" phrasing. Proposition 5's part (b) — the upper bound EVPI≤EEV−EVEVPI \le EEV-EVEVPI≤EEV−EV, VSS≤EEV−EVVSS \le EEV-EVVSS≤EEV−EV "for stochastic programs with fixed recourse matrix and fixed objective coefficients" — needs a different scope: that hypothesis is a structural property of the underlying LP data (WWW, ccc, qqq fixed across scenarios) invisible once zzz is abstracted away as above, and pinning it down would require modeling the LP's A,b,c,q,W,T,h(ξ)A,b,c,q,W,T,h(\xi)A,b,c,q,W,T,h(ξ) data explicitly (as Chapter 3's mission does for its convexity theorem). That part is out of scope here and is not needed for Theorem 9's own chain, which rests only on Proposition 5(a).

Collapsing any two of RPRPRP, WSWSWS, EVEVEV, EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV, SPEVSPEVSPEV to a single "value of the LP" — the trivialization this book-wide series flags for Chapter 4 — is ruled out by construction: each is its own definition over its own feasible object, and Theorem 9's statement names all five quantities in the chain rather than only its outer bound. The two occurrences of "VSS" in the chapter (the original mean-scenario EEV−RPEEV-RPEEV−RP of §4.2, and the reference-scenario EVRS−RPEVRS-RPEVRS−RP generalization of §4.6, used only in Theorem 9) are likewise kept as two distinct definitions rather than conflated under one name.

Every addition and subtraction between EReal values in this mission — inside expect, WS, EVPI, VSS, EVRS's appearance in VSSRef, the pair sum inside pairsValue, the sum inside SPEV, and all four differences in Theorem 9's own chain — uses three explicit operations, badd/bsub/bsum, that implement the book's own convention (p. 164) that +∞ (infeasibility) dominates, i.e. (+∞)+(−∞)=+∞, rather than Mathlib's native EReal addition, whose ⊤+⊥=⊥ would make VSS ≥ 0 (Proposition 5(a)) and the goal's own leftmost inequality false whenever a witness solution is infeasible in a positive-probability scenario — exactly the situation of the book's own Example 2 (pp. 174-175). The reference scenario's probability pr=Pr⁡(ξ=ξr)p_r=\Pr(\xi=\xi^r)pr​=Pr(ξ=ξr) (p. 172) is likewise not a free parameter but a definition, refProb, computed from the instance itself as ∑k: ξk=ξrpk\sum_{k:\,\xi^k=\xi^r}p_k∑k:ξk=ξr​pk​; SPEV's sum is correspondingly restricted to the scenarios other than the reference scenario (ξk≠ξr\xi^k\ne\xi^rξk=ξr), matching the book's own proof of Proposition 7, which uses ∑k≠rpk=1−pr\sum_{k\ne r}p_k=1-p_r∑k=r​pk​=1−pr​. The single hypothesis refProb I xir < 1 on Propositions 7, 8 and the goal says that some other scenario remains possible, which the book's own (1−pr)−1(1-p_r)^{-1}(1−pr​)−1 factor presupposes.

Reusable beyond this mission: the Instance definition and the RP/WS/EV quantities are the natural base for any later chapter of this series that needs the two-stage recourse value (e.g. Chapter 3's convexity mission, Chapter 5's L-shaped method); contributions extending this Instance to the full LP data of the underlying two-stage program, or adding Proposition 5(b) and Proposition 2's Jensen-inequality argument on top of it, are welcome.

Selected references

  • J.R. Birge and F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer Series in Operations Research and Financial Engineering, 2011, Chapter 4. DOI: 10.1007/978-1-4614-0237-4
  • A. Madansky, "Inequalities for Stochastic Linear Programming Problems", Management Science 6(2), 1960, 197–204.
  • H. Raiffa and R. Schlaifer, Applied Statistical Decision Theory, Harvard Business School, 1961.
  • J.R. Birge, "The Value of the Stochastic Solution in Stochastic Linear Programs with Fixed Recourse", Mathematical Programming 24(1), 1982, 314–325.
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Dynamical SystemsGroup Theory·Captain: dbenbenn

Cannon–Floyd–Parry: Thompson's group F and the simplicity of its commutator subgroupTextbook

Motivation

This mission formalizes §4 of Cannon, Floyd and Parry's Introductory notes on Richard Thompson's groups, together with the definition of Thompson's group FFF from their §1. The goal is their Theorem 4.5: the commutator subgroup [F,F][F,F][F,F] is simple.

In the 1960s Richard Thompson defined three groups, now written FFF, TTT and VVV, whose properties have kept them in use ever since as a source of examples at the edge of what groups can do. FFF is the smallest of the three and the least understood. It is finitely presented (§3 of the source) and torsion-free, it has no free subgroup of rank two, and whether it is amenable — whether it carries a finitely additive left-invariant probability measure defined on all its subsets — is open. Cannon, Floyd and Parry record (§4, p. 227) that Geoghegan raised the question and conjectured in 1979 both that FFF contains no non-Abelian free subgroup and that FFF is not amenable.

That question is what makes FFF worth pinning down precisely. Write AGAGAG for the class of amenable discrete groups, EGEGEG for the elementary amenable ones, and NFNFNF for the groups with no free subgroup of rank two. That AG⊂NFAG \subset NFAG⊂NF was noted by Day and follows from von Neumann; whether it is strict is the von Neumann–Day problem. It is: Olshanskii proved AG≠NFAG \neq NFAG=NF in a 1984 ICM address and Gromov gave an independent proof — but by examples that are not finitely presented. Brin and Squier proved in 1985 that F∈NFF \in NFF∈NF, and FFF is not elementary amenable (Theorem 4.10 of the source, CannonFloydParry.not_elementaryAmenable_F). So FFF is a finitely presented group in AG∖EGAG \setminus EGAG∖EG if it is amenable and in NF∖AGNF \setminus AGNF∖AG if it is not — a question with no other finitely presented candidate.

Setting

Call a real number dyadic if it has the form m/2km/2^{k}m/2k with m∈Zm \in \mathbb{Z}m∈Z and k∈Nk \in \mathbb{N}k∈N.

Thompson's group FFF, as §1 of the source defines it, is the set of piecewise linear homeomorphisms of the closed unit interval [0,1][0,1][0,1] onto itself that are differentiable except at finitely many dyadic rationals, and whose derivatives, where they exist, are powers of 222. Since those derivatives are positive, every element preserves orientation, so the elements of FFF are increasing. Composition of two such maps is again one, and so is the inverse of one, so FFF is a group.

The formalization calls such a map piecewise linear over the dyadics, and defines FFF as the subgroup generated by those maps — so that closure under composition and inverses is a theorem rather than part of the construction, as the source has it. What the model fixes rather than derives is under Formalization scope below.

Two particular elements generate it. Write

A(x)={x/20≤x≤12x−1412≤x≤342x−134≤x≤1B(x)={x0≤x≤12x/2+1412≤x≤34x−1834≤x≤782x−178≤x≤1.A(x) = \begin{cases} x/2 & 0 \le x \le \tfrac12\\ x - \tfrac14 & \tfrac12 \le x \le \tfrac34\\ 2x-1 & \tfrac34 \le x \le 1\end{cases} \qquad B(x) = \begin{cases} x & 0 \le x \le \tfrac12 \\ x/2 + \tfrac14 & \tfrac12 \le x \le \tfrac34 \\ x - \tfrac18 & \tfrac34 \le x \le \tfrac78 \\ 2x-1 & \tfrac78 \le x \le 1.\end{cases}A(x)=⎩⎨⎧​x/2x−41​2x−1​0≤x≤21​21​≤x≤43​43​≤x≤1​B(x)=⎩⎨⎧​xx/2+41​x−81​2x−1​0≤x≤21​21​≤x≤43​43​≤x≤87​87​≤x≤1.​

An element of FFF is trivial near 000 if it fixes every point of some interval [0,ε)[0,\varepsilon)[0,ε), and trivial near 111 if it fixes every point of some (1−ε,1](1-\varepsilon, 1](1−ε,1]. The support of fff is the set of points of [0,1][0,1][0,1] that fff moves. The commutator convention throughout is [x,y]=xyx−1y−1[x,y] = xyx^{-1}y^{-1}[x,y]=xyx−1y−1, and [F,F][F,F][F,F] denotes the commutator subgroup.

Formalization targets

Goal

[F,F] is a simple group.[F,F] \ \text{is a simple group.}[F,F] is a simple group.

This is the capstone of §4: it says the commutator subgroup has no normal subgroup other than itself and the trivial one. It is the goal because the rest of the section feeds it — both halves of Theorem 4.1, Theorem 4.3, and both supporting lemmas below are consumed by its proof.

Theorem 4.1, which has two parts

[F,F]  =  { f∈F:f is trivial near 0 and near 1 }[F,F] \;=\; \{\, f \in F : f \text{ is trivial near } 0 \text{ and near } 1 \,\}[F,F]={f∈F:f is trivial near 0 and near 1} F/[F,F]  ≅  Z⊕ZF/[F,F] \;\cong\; \mathbb{Z} \oplus \mathbb{Z}F/[F,F]≅Z⊕Z

Theorem 4.3

N⊴F, N≠1  ⟹  F/N is AbelianN \trianglelefteq F,\ N \neq 1 \;\Longrightarrow\; F/N \text{ is Abelian}N⊴F, N=1⟹F/N is Abelian

So FFF has no interesting proper quotients at all. With the first part of Theorem 4.1 this forces every nontrivial normal subgroup of FFF to contain [F,F][F,F][F,F].

Supporting results

That the piecewise-linear maps are already closed under composition and inverses, so that FFF consists of exactly those maps; a transitivity lemma on dyadic partitions of [0,1][0,1][0,1]; the fact that the subgroup of elements supported in a dyadic interval [a,b][a,b][a,b] of dyadic length is isomorphic to FFF itself; triviality of the center; that FFF contains no non-Abelian free group; and that FFF admits a total order invariant under multiplication on both sides.

Significance

What the results give. Theorem 4.1 identifies [F,F][F,F][F,F] concretely — a subgroup defined by a global algebraic condition turns out to be cut out by local behavior at the two endpoints — and computes the abelianization, making the pair of endpoint slopes a complete invariant of FFF modulo commutators. Theorem 4.3 and the simplicity of [F,F][F,F][F,F] together determine the whole normal subgroup lattice: every normal subgroup of FFF is trivial or contains [F,F][F,F][F,F]. That lattice is the input to the elementary-amenability argument.

What formalizing adds. All of these are proved in the source; none is in Mathlib, which has no piecewise-linear homeomorphism API and no Thompson group. Four of the milestones are proved as part of this proposal: that the piecewise-linear maps form a subgroup, that elements of FFF permute the dyadic rationals, that FFF embeds in the group Brin and Squier work with, and the absence of a free subgroup of rank two, which follows from the already-formalized Brin–Squier theorem via that embedding. The rest are open. The piecewise-linear machinery built along the way — local affineness, dyadic-breakpoint bookkeeping, extension by the identity — is reusable for TTT, for VVV, and for the wider family of piecewise-linear homeomorphism groups.

Difficulty

The obvious approach to the goal is to argue that a normal subgroup of [F,F][F,F][F,F] containing a nontrivial element must be everything, by conjugating that element around. It fails on its own: an element of [F,F][F,F][F,F] is pinned down only by being trivial near the two endpoints, and one still has to manufacture — inside [F,F][F,F][F,F], not merely inside FFF — an element carrying a prescribed pair of neighborhoods into those. That construction is what the dyadic-partition transitivity lemma supplies, and it is where the combinatorics of dyadic subdivision enters.

The second difficulty was that the source proves §4 using the tree-diagram normal form of §2. That section is now formalized in its own mission, Cannon–Floyd–Parry §2: tree diagrams and the normal form (mission ffd1e4ea-9f9a-4cb6-8419-78e70f2545e8), all of whose milestones are proved. Corollary 2.6 — milestone 5 here, the same theorem object — is closed from there, and Theorem 2.5 (represents_word_exponents) and the normal form (existsUnique_normalForm) are available to a solver attacking Theorem 4.3, so the source's argument can now be followed. A solution file imports only definitions, so whatever it uses from §2 must be reproved inline; the §2 solutions are public and written to be reused that way. The piecewise-linear route — dyadic-partition transitivity, Lemma 4.4 and Theorem 4.1 — remains an alternative, and is what Theorem 4.5's own argument uses.

Formalization scope

The unit interval is [0,1]⊆R[0,1] \subseteq \mathbb{R}[0,1]⊆R as a subtype, and an element of FFF is an order isomorphism of it, so orientation preservation is built into the representation rather than derived — faithful to the source's set, but assuming one sentence CFP prove. Piecewise linearity is stated as: there is a finite set BBB of dyadic reals such that the map is affine, with slope a power of two, on every closed interval whose interior misses BBB. Intercepts are not required to be dyadic — that is derived by induction along the breakpoints, not part of the definition.

The definition is not vacuous: AAA and BBB of Example 1.1 are constructed explicitly, and that FFF is not the trivial group is one of the milestones below — so no statement here is satisfied by the trivial group. In particular the goal, which asserts simplicity and therefore nontriviality, is not trivially false.

A companion definition places the same data on the real line, each element extended by the identity outside [0,1][0,1][0,1]; that line realisation is what the bridge statement connects to Brin and Squier's group.

Selected references

  • J. W. Cannon, W. J. Floyd, W. R. Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Mathématique (2) 42 (1996), 215–256. doi:10.5169/seals-87877
  • M. G. Brin, C. C. Squier, Groups of piecewise linear homeomorphisms of the real line, Inventiones Mathematicae 79 (1985), 485–498. doi:10.1007/BF01388519
  • C. Chou, Elementary amenable groups, Illinois Journal of Mathematics 24 (1980), 396–407. doi:10.1215/ijm/1256047608
  • M. M. Day, Amenable semigroups, Illinois Journal of Mathematics 1 (1957), 509–544. doi:10.1215/ijm/1255380675
  • J. von Neumann, Zur allgemeinen Theorie des Maßes, Fundamenta Mathematicae 13 (1929), 73–116. doi:10.4064/fm-13-1-73-116
  • A. Yu. Olshanskii, On a geometric method in the combinatorial group theory, Proceedings of the International Congress of Mathematicians (Warsaw, 1983), vol. 1, 1984, pp. 415–424. IMU archive
  • M. Gromov, Hyperbolic groups, in Essays in Group Theory (S. M. Gersten, ed.), MSRI Publications 8, Springer, 1987, pp. 75–263. doi:10.1007/978-1-4613-9586-7_3
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Harmonic AnalysisNumber Theory·Captain: Lucas

Connes: Weil positivity and the Riemann zeta functionResearch Paper

Motivation

The Riemann hypothesis (RH) asserts that every zero of the Riemann zeta function ζ\zetaζ in the strip 0<Re⁡s<10 < \operatorname{Re} s < 10<Res<1 has Re⁡s=12\operatorname{Re} s = \tfrac12Res=21​. One of the few reformulations that turns RH into a positivity statement, rather than a statement about the location of points, goes back to A. Weil (1952): the explicit formula expresses a sum over the zeros of ζ\zetaζ as a sum of local contributions over the places of Q\mathbb{Q}Q, and RH is equivalent to the resulting functional being positive on elements of the form g⋆g∗g \star g^{*}g⋆g∗.

Connes' 1999 programme paper Noncommutative geometry and the Riemann zeta function takes this reformulation as its endpoint. It builds a geometric framework — the adele class space X=A/k∗X = \mathbb{A}/k^{*}X=A/k∗ carrying an action of the idele class group CkC_kCk​ — in which the explicit formula appears as a Lefschetz formula, the zeros of LLL-functions appear spectrally, and the paper's concluding assertion (§3, p. 22) is that the validity of the global trace formula implies, and is in fact equivalent to, positivity of the Weil distribution, i.e. RH for all LLL-functions with Grössencharakter.

This mission formalizes the arithmetic core of that endpoint in its simplest instance: the global field k=Qk = \mathbb{Q}k=Q with trivial Grössencharakter, so that the LLL-function is ζ\zetaζ itself. Concretely it asks for (i) the Riemann–Weil explicit formula for ζ\zetaζ in the shape of Connes' equation (11), and (ii) both directions of the equivalence between positivity of the resulting Weil distribution and RH.

A rough timeline of the statements involved: Riemann (1859) gave the first explicit formula; von Mangoldt (1895) proved it rigorously; Weil (Sur les "formules explicites" de la théorie des nombres premiers, 1952) extended it to all global fields and isolated the positivity criterion; Bombieri (Remarks on Weil's quadratic functional in the theory of prime numbers, 2000) studied the associated quadratic functional in detail; Connes (1996–1999) gave the trace-formula interpretation formalized in part here.

Setting

All objects live on the group R+∗\mathbb{R}^{*}_{+}R+∗​, the module of the idele class group of Q\mathbb{Q}Q, written additively through u=etu = e^{t}u=et, d∗u=dtd^{*}u = dtd∗u=dt.

A test function is a map g:R→Cg : \mathbb{R} \to \mathbb{C}g:R→C that is C∞C^{\infty}C∞ and has compact support (IsTest).

Its transform is

g^(z)  =  ∫Rg(t) e(z−1/2) t dt,\widehat{g}(z) \;=\; \int_{\mathbb{R}} g(t)\, e^{(z - 1/2)\,t}\, dt ,g​(z)=∫R​g(t)e(z−1/2)tdt,

which is Connes' h^(z)=∫Ckh(u) ∣u∣z d∗u\widehat h(z) = \int_{C_k} h(u)\,|u|^{z}\,d^{*}uh(z)=∫Ck​​h(u)∣u∣zd∗u in the coordinate u=etu = e^{t}u=et, shifted by 12\tfrac1221​ so that zzz is the variable of ζ\zetaζ (mellinHat). On the critical line, g^(12+ir)=∫Rg(t)eirt dt\widehat{g}(\tfrac12 + i r) = \int_{\mathbb{R}} g(t) e^{irt}\,dtg​(21​+ir)=∫R​g(t)eirtdt is the ordinary Fourier transform.

The involution is g∗(t)=g(−t)‾g^{*}(t) = \overline{g(-t)}g∗(t)=g(−t)​, i.e. h∗(u)=h(u−1)‾h^{*}(u) = \overline{h(u^{-1})}h∗(u)=h(u−1)​ (starInv), and convolution is (g1⋆g2)(t)=∫Rg1(s) g2(t−s) ds(g_1 \star g_2)(t) = \int_{\mathbb{R}} g_1(s)\, g_2(t-s)\, ds(g1​⋆g2​)(t)=∫R​g1​(s)g2​(t−s)ds (conv).

The Weil distribution of a test function ggg collects the pole terms, the finite places and the archimedean place:

W(g)  =  g^(0)+g^(1)  −  ∑n≥2Λ(n)n(g(log⁡n)+g(−log⁡n))  +  12π∫Rg^(12+ir)(Re⁡ψ(14+ir2)−log⁡π)dr,W(g) \;=\; \widehat{g}(0) + \widehat{g}(1) \;-\; \sum_{n \ge 2} \frac{\Lambda(n)}{\sqrt{n}}\bigl(g(\log n) + g(-\log n)\bigr) \;+\; \frac{1}{2\pi}\int_{\mathbb{R}} \widehat{g}\left(\tfrac12 + ir\right)\Bigl(\operatorname{Re}\psi\left(\tfrac14 + \tfrac{ir}{2}\right) - \log \pi\Bigr) dr ,W(g)=g​(0)+g​(1)−n≥2∑​n​Λ(n)​(g(logn)+g(−logn))+2π1​∫R​g​(21​+ir)(Reψ(41​+2ir​)−logπ)dr,

where Λ\LambdaΛ is the von Mangoldt function and ψ=Γ′/Γ\psi = \Gamma'/\Gammaψ=Γ′/Γ (weilDistribution, with the three pieces named mellinHat, primeSum, archTerm). The middle sum is Weil's contribution of the finite places v=pv = pv=p, the last integral the contribution of the real place.

The spectral side is

Z(g)  =  ∑ρmρ g^(ρ),Z(g) \;=\; \sum_{\rho} m_{\rho}\, \widehat{g}(\rho),Z(g)=ρ∑​mρ​g​(ρ),

the sum over the zeros ρ\rhoρ of ζ\zetaζ with 0<Re⁡ρ<10 < \operatorname{Re}\rho < 10<Reρ<1, each counted with its multiplicity mρm_\rhomρ​ (zeroSum, IsCriticalZero, zeroMult).

Formalization targets

Goal — positivity of the Weil distribution implies RH

(∀ g test:  Re⁡W(g⋆g∗)≥0)  ⟹  (∀ρ, ζ(ρ)=0, 0<Re⁡ρ<1  ⇒  Re⁡ρ=12).\Bigl(\forall\, g \text{ test}:\; \operatorname{Re} W\bigl(g \star g^{*}\bigr) \ge 0\Bigr) \;\Longrightarrow\; \bigl(\forall \rho,\ \zeta(\rho) = 0,\ 0 < \operatorname{Re}\rho < 1 \;\Rightarrow\; \operatorname{Re}\rho = \tfrac12\bigr).(∀g test:ReW(g⋆g∗)≥0)⟹(∀ρ, ζ(ρ)=0, 0<Reρ<1⇒Reρ=21​).

This is the direction that yields RH, and it is the weakest form of the endpoint of the paper: it fixes no rate, no test-function normalization beyond Cc∞C_c^{\infty}Cc∞​, and no numerical constant.

Milestone — the explicit formula (Connes (11))

∑ρmρ g^(ρ)  =  W(g)for every test function g,\sum_{\rho} m_\rho\,\widehat g(\rho) \;=\; W(g) \qquad \text{for every test function } g,ρ∑​mρ​g​(ρ)=W(g)for every test function g,

with the sum over zeros asserted to be (unconditionally) summable.

Milestone — the converse direction

RH  ⟹  ∀ g test: Re⁡W(g⋆g∗)≥0.\text{RH} \;\Longrightarrow\; \forall\, g \text{ test}:\ \operatorname{Re} W\bigl(g \star g^{*}\bigr) \ge 0 .RH⟹∀g test: ReW(g⋆g∗)≥0.

Together with the goal this is the equivalence asserted on p. 22 of the paper, in the case k=Qk = \mathbb{Q}k=Q, trivial Grössencharakter.

Supporting statements

The ∗*∗-identity g⋆g∗^(12+ir)=∣g^(12+ir)∣2\widehat{g \star g^{*}}\left(\tfrac12 + ir\right) = \bigl|\widehat g\left(\tfrac12+ir\right)\bigr|^{2}g⋆g∗​(21​+ir)=​g​(21​+ir)​2 on the critical line, and the fact that g⋆g∗g \star g^{*}g⋆g∗ is again a test function.

Significance

Weil's positivity criterion is one of the standard equivalent forms of RH, and the only one in which the arithmetic input (the primes, through Λ\LambdaΛ) and the archimedean input (the Γ\GammaΓ-factor) enter as separate, explicitly computable local terms. Formalizing it produces a machine-checked bridge between the zeros of ζ\zetaζ and prime sums: the explicit formula milestone is the reusable object here, since essentially every analytic application of zeta zeros — zero-density estimates, prime-counting error terms, pair-correlation statistics — is an instance of it.

Status honesty: neither RH nor the positivity statement is known; the explicit formula and both implications relating positivity to RH are classical theorems, proved but not, as far as the catalog shows, formalized in Lean. Mathlib currently provides ζ\zetaζ, its functional equation, the von Mangoldt function and Γ\GammaΓ, but no explicit formula of any kind. What this mission adds on top of the paper is therefore the formal proof of known results, not new mathematics.

Difficulty

The obvious route to the explicit formula — integrate −ζ′/ζ(s)g^(s)-\zeta'/\zeta(s)\widehat g(s)−ζ′/ζ(s)g​(s) over a vertical line, move the contour to the reflected line, collect residues — fails to be routine at exactly two points. First, moving the contour requires control of ζ′/ζ\zeta'/\zetaζ′/ζ on horizontal segments between zeros, which is where the classical proof invests most of its work; Mathlib has bounds near Re⁡s=1\operatorname{Re} s = 1Res=1 but nothing of this shape inside the strip. Second, the sum over zeros must be shown to converge unconditionally, which needs a zero-counting bound of Riemann–von Mangoldt type (N(T)≪Tlog⁡TN(T) \ll T\log TN(T)≪TlogT) that is not in Mathlib either.

For the goal implication, the naive idea — pick a test function whose transform is supported near a hypothetical off-line zero — is unavailable: g^\widehat gg​ is entire whenever ggg has compact support, so it cannot be localized. The classical argument instead exploits the symmetry ρ↦1−ρˉ\rho \mapsto 1-\bar\rhoρ↦1−ρˉ​ of the zero set and makes the off-line quadruple contribute a negative amount in the limit along a family of test functions.

Formalization scope

Conventions the Lean statements commit to. Test functions are C\mathbb{C}C-valued on R\mathbb{R}R, ContDiff ℝ (⊤ : ℕ∞) (so C∞C^{\infty}C∞, not analytic) with HasCompactSupport; the multiplicative group R+∗\mathbb{R}^{*}_{+}R+∗​ is always written additively. The transform carries the 12\tfrac1221​-shift shown above, so the critical line is Re⁡z=12\operatorname{Re} z = \tfrac12Rez=21​ and g^(0),g^(1)\widehat{g}(0), \widehat{g}(1)g​(0),g​(1) are the two pole terms. Zeros are indexed by the subtype {s:0<Re⁡s<1, ζ(s)=0}\{s : 0 < \operatorname{Re} s < 1,\ \zeta(s) = 0\}{s:0<Res<1, ζ(s)=0} and weighted by (analyticOrderAt riemannZeta s).toNat; the trivial zeros are excluded. Integrals are Bochner integrals and sums are tsum, so both take the junk value 000 when the integrand is not integrable or the family is not summable — for that reason the explicit formula is stated as a HasSum, which carries summability, rather than as an equation between tsums. The archimedean term is written with Re⁡ψ\operatorname{Re}\psiReψ, ψ=\psi = ψ= logDeriv Complex.Gamma, rather than as a principal value, to avoid a second regularization convention.

The goal is not trivially satisfiable: its hypothesis quantifies over a nonempty class (smooth bump functions exist), and its conclusion is RH for ζ\zetaζ, so no vacuous reading is available.

Infrastructure a complete development needs, all reusable beyond this mission: growth bounds for ζ′/ζ\zeta'/\zetaζ′/ζ inside the critical strip, a Riemann–von Mangoldt zero-counting bound, Fourier analysis of Cc∞C^\infty_cCc∞​ functions (Paley–Wiener style decay of g^\widehat gg​), and the Hadamard product / functional equation package for the completed zeta function.

Out of scope, and deliberately so: Connes' operator-theoretic trace formula (equations (41) and (45) of the paper) and the spectral realization theorem of p. 17. Both are statements about traces of operators on Hilbert space, and Mathlib presently has no trace-class operator theory to state them faithfully. The mission therefore formalizes the arithmetic side of the paper's endpoint; contributions that build the missing operator theory, or that extend the statements from ζ\zetaζ to Dirichlet LLL-functions and Hecke LLL-functions with Grössencharakter, are welcome.

Selected references

  • A. Connes, Noncommutative geometry and the Riemann zeta function, in Mathematics: Frontiers and Perspectives, AMS (2000) — the source of this mission (§3, equations (11) and (45), and the concluding assertion on p. 22).
  • A. Connes, Trace formula in noncommutative geometry and the zeros of the Riemann zeta function, Selecta Math. (N.S.) 5 (1999) — reference [9] of the source. https://arxiv.org/abs/math/9811068
  • A. Weil, Sur les "formules explicites" de la théorie des nombres premiers, Comm. Sém. Math. Univ. Lund (1952) — reference [27] of the source.
  • E. Bombieri, Remarks on Weil's quadratic functional in the theory of prime numbers, I (2000).
  • H. Iwaniec and E. Kowalski, Analytic Number Theory, AMS Colloquium Publications 53 (2004), Chapter 5 (explicit formulas).
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Differential GeometryGeometry & Topology·Captain: Lucas

Differential Geometry of Curves and Surfaces IV: Regular Surfaces and Change of ParametersTextbook

Motivation

Before any geometry of surfaces can be done, one has to say what a surface is, in a way that supports calculus: a subset of R3\mathbb{R}^3R3 that is locally the smooth, non-degenerate image of an open piece of the plane. Every statement in the later theory — the first and second fundamental forms, the Gauss map, curvature, geodesics — is written in local coordinates, and is therefore meaningful only once one knows that the answer does not depend on the coordinates chosen. That independence is the content of the change-of-parameters theorem, which is what makes "differentiable function on a surface" and "geometric quantity of a surface" well-defined notions.

The reference for this mission is Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition (Dover, 2016), §2-2 "Regular Surfaces; Inverse Images of Regular Values" (pp. 54–71) and §2-3 "Change of Parameters; Differentiable Functions on Surfaces" (pp. 72–85): Definition 1 (p. 54), Propositions 1–4 of §2-2 (pp. 59, 61, 63, 65) and Proposition 1 of §2-3 (p. 74).

This is the fourth mission of a series formalizing do Carmo's book, sharing the namespace DoCarmoDG with the others.

Setting

A subset S⊆R3S \subseteq \mathbb{R}^3S⊆R3 is a regular surface when every p∈Sp \in Sp∈S has an open neighbourhood V⊆R3V \subseteq \mathbb{R}^3V⊆R3 such that V∩SV \cap SV∩S is the image of a map x:U→R3x : U \to \mathbb{R}^3x:U→R3, defined on an open set U⊆R2U \subseteq \mathbb{R}^2U⊆R2, satisfying the three conditions of do Carmo's Definition 1:

  1. xxx is differentiable, i.e. of class C∞C^\inftyC∞ on UUU;
  2. xxx is a homeomorphism of UUU onto V∩SV \cap SV∩S — it is injective and its inverse is continuous;
  3. (regularity) for every q∈Uq \in Uq∈U the differential dxq:R2→R3dx_q : \mathbb{R}^2 \to \mathbb{R}^3dxq​:R2→R3 is injective.

Such an xxx is a parametrization, or system of local coordinates, and V∩SV \cap SV∩S is a coordinate neighbourhood.

Given a differentiable fff on an open set U⊆R3U \subseteq \mathbb{R}^3U⊆R3, a value aaa is a regular value of fff when dfpdf_pdfp​ is surjective — equivalently, nonzero — at every p∈Up \in Up∈U with f(p)=af(p) = af(p)=a (do Carmo Definition 2, §2-2).

Formalization targets

Goal — Change of parameters (do Carmo §2-3, Proposition 1)

If x:U→Sx : U \to Sx:U→S and y:V→Sy : V \to Sy:V→S are two parametrizations of a regular surface SSS with p∈x(U)∩y(V)=Wp \in x(U) \cap y(V) = Wp∈x(U)∩y(V)=W, then

h=x−1∘y:y−1(W)→x−1(W)h = x^{-1} \circ y : y^{-1}(W) \to x^{-1}(W)h=x−1∘y:y−1(W)→x−1(W)

is a diffeomorphism: hhh is differentiable, bijective, and h−1h^{-1}h−1 is differentiable.

Supporting statements

The graph of a differentiable function of two variables is a regular surface (Proposition 1); the inverse image of a regular value is a regular surface (Proposition 2); a regular surface is locally the graph of a differentiable function of one of the three coordinate pairs (Proposition 3); and an injective map satisfying conditions 1 and 3 whose image lies in a regular surface automatically has a continuous inverse (Proposition 4).

Significance

Proposition 2 is the practical criterion: it is what shows in one line that spheres, ellipsoids, tori and the level sets of generic polynomials are regular surfaces, and it is applied throughout the book. Proposition 3 is the structural statement that a regular surface is locally a graph, which is the form in which most local computations are carried out; Proposition 4 removes the awkward homeomorphism clause from the verification of examples. The change-of-parameters theorem is what allows every subsequent definition — differentiable function on a surface, tangent plane, first fundamental form, curvature — to be given in coordinates and then shown to be independent of them, and it is also the reason a regular surface carries a smooth structure at all.

Mathlib has smooth manifolds, the implicit and inverse function theorems, and ContDiffOn, but it does not contain do Carmo's concrete definition of a regular surface as a subset of R3\mathbb{R}^3R3 or these four propositions about it. Establishing them is what allows the rest of this series to work with patches while knowing that the objects so defined are coordinate-independent.

Difficulty

Everything here rests on the inverse function theorem, but each proposition needs it in a slightly different form. Proposition 2 requires completing fff to a local diffeomorphism F(x,y,z)=(x,y,f(x,y,z))F(x,y,z) = (x,y,f(x,y,z))F(x,y,z)=(x,y,f(x,y,z)) and reading off the level set — with the complication that which partial derivative is nonzero varies from point to point, so the coordinate that is solved for is not fixed in advance. Proposition 3 needs the same case distinction on which 2×22 \times 22×2 Jacobian minor of xxx is nonzero, and this is exactly why the conclusion is a disjunction over the three coordinate pairs. Proposition 4 is where the homeomorphism condition is shown to be redundant, and the argument goes through the local factorization x−1=(π∘x)−1∘πx^{-1} = (\pi \circ x)^{-1} \circ \pix−1=(π∘x)−1∘π.

The change-of-parameters theorem is not a direct application of the inverse function theorem to hhh: the map hhh is defined only on a subset of the plane and x−1x^{-1}x−1 is, a priori, merely continuous. One first extends xxx to a local diffeomorphism of a neighbourhood in R3\mathbb{R}^3R3 and then composes; the continuity of x−1x^{-1}x−1 (condition 2 of Definition 1) is what makes the domain of hhh open, and it cannot be dispensed with.

Formalization scope

A surface is a set S : Set (EuclideanSpace ℝ (Fin 3)), and a parametrization is a map x : ℝ × ℝ → EuclideanSpace ℝ (Fin 3) together with an open U : Set (ℝ × ℝ). Smoothness is ContDiffOn ℝ (⊤ : ℕ∞), matching do Carmo's "differentiable" for C∞C^\inftyC∞; regularity is injectivity of the Fréchet derivative at each point of U, which is do Carmo's condition 3; and the homeomorphism condition is stated as injectivity on U together with the existence of a continuous left inverse on the image, which is the content of "the inverse is continuous". The neighbourhood clause of Definition 1 is x '' U = V ∩ S for an open V containing the point.

Graphs are formalized as three separate sets, one for each of z=f(x,y)z = f(x,y)z=f(x,y), y=g(x,z)y = g(x,z)y=g(x,z) and x=h(y,z)x = h(y,z)x=h(y,z), so that Proposition 3 can state its disjunction faithfully; in that statement the neighbourhood is an open set W of R3\mathbb{R}^3R3 and the claim is W ∩ S = W ∩ graph.

The goal states the diffeomorphism property of hhh explicitly — two maps, mutually inverse on the relevant domains, both ContDiffOn, together with the openness of those domains — rather than through a bundled structure, so that no library convention is assumed. There is no trivializing reading: the domains are those forced by the two parametrizations, and in the degenerate case where the images do not overlap the statement reduces to a true but empty claim about the empty set, while the substance is in the overlapping case.

Selected references

  • Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition, Dover, 2016, §2-2 (Definition 1, p. 54; Propositions 1-4, pp. 59-65) and §2-3 (Proposition 1, p. 74).
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Differential GeometryGeometry & Topology·Captain: Lucas

Differential Geometry of Curves and Surfaces II: Theorema EgregiumTextbook

Motivation

Until 1827 the curvature of a surface in space was understood as a statement about how the surface sits inside R3\mathbb{R}^3R3: it was computed from the way the unit normal turns, that is, from the second fundamental form. Gauss's Disquisitiones generales circa superficies curvas showed that one particular combination of those extrinsic quantities — the product of the principal curvatures — can be recomputed from measurements made entirely inside the surface, using only lengths of curves drawn on it. This is the Theorema Egregium, and it is the reason the subject splits into extrinsic and intrinsic geometry; the latter is what becomes Riemannian geometry.

The reference for this mission is Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition (Dover, 2016), §4-3, "The Gauss Theorem and the Equations of Compatibility" (pp. 235–240). The theorem is stated on page 237 and derived from the Gauss formula, equation (5) of that section; the Mainardi–Codazzi equations (6) and (6a) on page 238 complete the list of compatibility equations.

This is the second mission of a series formalizing do Carmo's book; it shares the namespace DoCarmoDG with the first, on the local theory of curves.

Setting

A regular parametrized patch is a map x:U→R3x : U \to \mathbb{R}^3x:U→R3, defined and smooth on an open set U⊆R2U \subseteq \mathbb{R}^2U⊆R2 with coordinates (u,v)(u,v)(u,v), whose partial derivatives satisfy xu∧xv≠0x_u \wedge x_v \neq 0xu​∧xv​=0 at every point of UUU; the last condition says that dxdxdx is injective, so {xu,xv}\{x_u, x_v\}{xu​,xv​} spans a 222-dimensional tangent plane at each point and

N=xu∧xv∣xu∧xv∣N = \frac{x_u \wedge x_v}{|x_u \wedge x_v|}N=∣xu​∧xv​∣xu​∧xv​​

is a unit normal field along the patch.

The first fundamental form is the restriction of the ambient inner product to the tangent plane; in the parametrization it is recorded by the three functions

E=⟨xu,xu⟩,F=⟨xu,xv⟩,G=⟨xv,xv⟩,E = \langle x_u, x_u\rangle, \qquad F = \langle x_u, x_v\rangle, \qquad G = \langle x_v, x_v\rangle,E=⟨xu​,xu​⟩,F=⟨xu​,xv​⟩,G=⟨xv​,xv​⟩,

and EG−F2=∣xu∧xv∣2>0EG - F^2 = |x_u \wedge x_v|^2 > 0EG−F2=∣xu​∧xv​∣2>0. The second fundamental form is recorded by

e=⟨N,xuu⟩,f=⟨N,xuv⟩,g=⟨N,xvv⟩,e = \langle N, x_{uu}\rangle, \qquad f = \langle N, x_{uv}\rangle, \qquad g = \langle N, x_{vv}\rangle,e=⟨N,xuu​⟩,f=⟨N,xuv​⟩,g=⟨N,xvv​⟩,

and the Gaussian curvature is

K=eg−f2EG−F2.K = \frac{eg - f^2}{EG - F^2}.K=EG−F2eg−f2​.

The three second derivatives xuu,xuv,xvvx_{uu}, x_{uv}, x_{vv}xuu​,xuv​,xvv​ decompose in the basis {xu,xv,N}\{x_u, x_v, N\}{xu​,xv​,N}; the tangential coefficients are the Christoffel symbols Γijk\Gamma^k_{ij}Γijk​ of the patch, and the normal coefficients are eee, fff, ggg, which is do Carmo's system (1) of §4-3:

xuu=Γ111xu+Γ112xv+eN,xuv=Γ121xu+Γ122xv+fN,xvv=Γ221xu+Γ222xv+gN.x_{uu} = \Gamma^1_{11} x_u + \Gamma^2_{11} x_v + eN, \qquad x_{uv} = \Gamma^1_{12} x_u + \Gamma^2_{12} x_v + fN, \qquad x_{vv} = \Gamma^1_{22} x_u + \Gamma^2_{22} x_v + gN.xuu​=Γ111​xu​+Γ112​xv​+eN,xuv​=Γ121​xu​+Γ122​xv​+fN,xvv​=Γ221​xu​+Γ222​xv​+gN.

Two patches over the same parameter domain are isometric when their first fundamental forms coincide, E=EˉE = \bar EE=Eˉ, F=FˉF = \bar FF=Fˉ, G=GˉG = \bar GG=Gˉ at every point: lengths of curves, angles and areas computed in the parameter domain then agree, and a local isometry between the two surfaces is obtained by matching parameters.

Formalization targets

Goal — Theorema Egregium (do Carmo, p. 237)

E=Eˉ, F=Fˉ, G=Gˉ  on U⟹K=Kˉ  on U.E = \bar E,\ F = \bar F,\ G = \bar G \ \text{ on } U \quad \Longrightarrow \quad K = \bar K \ \text{ on } U .E=Eˉ, F=Fˉ, G=Gˉ  on U⟹K=Kˉ  on U.

The Gaussian curvature of a regular patch is determined by its first fundamental form alone, although its definition uses the second fundamental form, i.e. the position of the surface in space.

Supporting statements

The existence and uniqueness of the Christoffel symbols; the linear system (2) expressing them through E,F,GE, F, GE,F,G and their first derivatives; the Gauss formula (5),

(Γ122)u−(Γ112)v+Γ121Γ112+Γ122Γ122−Γ112Γ222−Γ111Γ122=−EK;(\Gamma^2_{12})_u - (\Gamma^2_{11})_v + \Gamma^1_{12}\Gamma^2_{11} + \Gamma^2_{12}\Gamma^2_{12} - \Gamma^2_{11}\Gamma^2_{22} - \Gamma^1_{11}\Gamma^2_{12} = -EK;(Γ122​)u​−(Γ112​)v​+Γ121​Γ112​+Γ122​Γ122​−Γ112​Γ222​−Γ111​Γ122​=−EK;

the Mainardi–Codazzi equations (6) and (6a); the closed formula for KKK in an orthogonal parametrization (Exercise 1, p. 240); the invariance of KKK under a change of parameters; and, as a corollary, that no neighbourhood of a point of the unit sphere is isometric to a piece of a plane (Exercise 4, p. 240).

Significance

The theorem is what makes intrinsic geometry possible: a quantity defined through the embedding turns out to be computable from the metric, so it survives every isometric deformation. Concrete consequences include the impossibility of a distortion-free map of the sphere — the reason every cartographic projection distorts lengths — and the equality of the Gaussian curvatures of the catenoid and the helicoid at corresponding points, which do Carmo notes immediately after the theorem. In the structure of the book, the Gauss formula is also the identity that makes the global Gauss–Bonnet theorem of §4-5 a statement about intrinsic data.

Mathlib has inner product spaces, iterated derivatives and the smooth manifold library, but it does not contain the first and second fundamental forms of a parametrized surface, the Christoffel symbols of a patch, the Gaussian curvature in this sense, or the compatibility equations. This mission produces that vocabulary together with machine-checked proofs of the classical identities. The mathematics is Gauss's, from 1827; what is open is the formalization.

Difficulty

The proof is a computation, but not a short one: one differentiates the system (1), uses xuuv=xuvux_{uuv} = x_{uvu}xuuv​=xuvu​, re-expands every second derivative through (1) again, and equates coefficients in the basis {xu,xv,N}\{x_u, x_v, N\}{xu​,xv​,N}. Formally, the cost sits in three places: justifying the interchange of the mixed partial derivatives; establishing that the coefficient functions Γijk\Gamma^k_{ij}Γijk​ obtained pointwise from linear algebra are differentiable in the parameters; and carrying out the coefficient comparison in a basis that is not orthonormal, where one must use that EG−F2≠0EG - F^2 \neq 0EG−F2=0 rather than take inner products with an orthonormal frame.

The naive route to the Theorema Egregium — "solve the system (2) for the Γijk\Gamma^k_{ij}Γijk​, then quote the Gauss formula" — is the right one, but the first step must actually be carried out: the system (2) determines the symbols only because each of its three 2×22 \times 22×2 blocks has determinant EG−F2≠0EG - F^2 \neq 0EG−F2=0, and that is where the regularity hypothesis is used.

Formalization scope

A patch is a curried map x : ℝ → ℝ → EuclideanSpace ℝ (Fin 3), so that the partial derivatives xux_uxu​ and xvx_vxv​ are ordinary one-variable derivatives, and the domain is an open set U : Set (ℝ × ℝ); smoothness is ContDiffOn ℝ (⊤ : ℕ∞) of the uncurried map on U, matching do Carmo's use of "differentiable" for C∞C^\inftyC∞. Regularity is stated as xu∧xv≠0x_u \wedge x_v \neq 0xu​∧xv​=0 on U, with the vector product defined componentwise. All quantities (NNN, EEE, FFF, GGG, eee, fff, ggg, KKK) are total functions of the parameters, taking junk values off U; every statement restricts to points of U.

Christoffel symbols are not defined by a formula: a statement that mentions them quantifies over functions Γijk\Gamma^k_{ij}Γijk​ assumed to satisfy do Carmo's decomposition (1) on U, and a separate milestone asserts that such functions exist and are unique on U. The symmetry Γ12k=Γ21k\Gamma^k_{12} = \Gamma^k_{21}Γ12k​=Γ21k​ is built into the notation, as in the book.

Isometry is formalized as equality of EEE, FFF, GGG over a common parameter domain rather than as a map between surfaces; together with the milestone on invariance under change of parameters, this recovers do Carmo's statement that KKK is invariant under local isometries. The formalization deliberately keeps the surface concrete (a patch, not an abstract manifold), which is what makes the compatibility equations expressible as identities between explicit derivatives.

This mission's definition file builds on the vector-product definition introduced in mission I of this series (Fundamental Theorem of the Local Theory of Curves), so mission I must be submitted first: its definitions have to be published before the definition file of this mission can compile.

There is no vacuous reading: the hypotheses are satisfiable — every regular patch, for instance a graph or a surface of revolution, satisfies them — and the conclusion compares two curvature functions pointwise.

Selected references

  • Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition, Dover, 2016, §2-5, §3-3 and §4-3 (Theorema Egregium on p. 237; Gauss formula, eq. (5); Mainardi–Codazzi, eqs. (6), (6a)).
  • C. F. Gauss, Disquisitiones generales circa superficies curvas, Commentationes Societatis Regiae Scientiarum Gottingensis Recentiores 6 (1827), 99–146.
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Differential GeometryGeometry & Topology·Captain: Lucas

Differential Geometry of Curves and Surfaces I: Fundamental Theorem of the Local Theory of CurvesTextbook

Motivation

The differential geometry of curves in R3\mathbb{R}^3R3 is the entry point of every course and every textbook in the subject, and it is the first place where a geometric object is shown to be completely determined by a small list of numerical invariants. A space curve traced out by a particle moving at unit speed bends (curvature) and twists (torsion); the assertion that these two scalar functions determine the curve completely, up to a motion of space, is the prototype of every later "fundamental theorem" of the subject — for surfaces (Bonnet), for Riemannian metrics, and for submanifolds in general.

The reference for this mission is Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition (Dover, 2016), Chapter 1, Sections 1-4 and 1-5. The statement targeted here is the one printed on page 19 under the heading Fundamental Theorem of the Local Theory of Curves; the uniqueness half is proved on pages 20–22, and the existence half is deferred by do Carmo to the appendix of Chapter 4, where it is obtained from the existence and uniqueness theorem for linear systems of ordinary differential equations.

This is the first mission of a series formalizing do Carmo's book. The series shares one Lean namespace, DoCarmoDG, so that later missions on regular surfaces, the Gauss map, and Gauss–Bonnet build on the vocabulary fixed here.

Setting

Let I=(a,b)⊆RI = (a,b) \subseteq \mathbb{R}I=(a,b)⊆R be an open interval and let α:I→R3\alpha : I \to \mathbb{R}^3α:I→R3 be a smooth map. The curve α\alphaα is parametrized by arc length if ∣α′(s)∣=1|\alpha'(s)| = 1∣α′(s)∣=1 for every s∈Is \in Is∈I; the parameter sss is then the arc length measured along the curve.

For such a curve one sets

t(s)=α′(s),k(s)=∣α′′(s)∣.t(s) = \alpha'(s), \qquad k(s) = |\alpha''(s)| .t(s)=α′(s),k(s)=∣α′′(s)∣.

The vector t(s)t(s)t(s) is the unit tangent and the scalar k(s)≥0k(s) \ge 0k(s)≥0 is the curvature at sss. Differentiating α′⋅α′=1\alpha'\cdot\alpha' = 1α′⋅α′=1 gives α′′⋅α′=0\alpha''\cdot\alpha' = 0α′′⋅α′=0, so α′′(s)\alpha''(s)α′′(s) is orthogonal to t(s)t(s)t(s). At a point where k(s)≠0k(s) \neq 0k(s)=0 one defines the normal vector and the binormal vector

n(s)=α′′(s)k(s),b(s)=t(s)∧n(s),n(s) = \frac{\alpha''(s)}{k(s)}, \qquad b(s) = t(s) \wedge n(s),n(s)=k(s)α′′(s)​,b(s)=t(s)∧n(s),

where ∧\wedge∧ is the vector product of R3\mathbb{R}^3R3 (do Carmo §1-4). The triple {t(s),n(s),b(s)}\{t(s), n(s), b(s)\}{t(s),n(s),b(s)} is a positively oriented orthonormal basis, the Frenet trihedron. Since bbb has constant length and b′=t∧n′b' = t \wedge n'b′=t∧n′ is orthogonal to ttt, the derivative b′(s)b'(s)b′(s) is a multiple of n(s)n(s)n(s), and the torsion τ(s)\tau(s)τ(s) is defined by

b′(s)=τ(s) n(s).b'(s) = \tau(s)\, n(s).b′(s)=τ(s)n(s).

This is do Carmo's sign convention; many authors write −τ-\tau−τ for the same quantity, and the mission is committed to do Carmo's. With these conventions the Frenet formulas read

t′=k n,n′=−k t−τ b,b′=τ n.t' = k\,n, \qquad n' = -k\,t - \tau\, b, \qquad b' = \tau\, n .t′=kn,n′=−kt−τb,b′=τn.

A rigid motion of R3\mathbb{R}^3R3 is a map p↦ρ(p)+cp \mapsto \rho(p) + cp↦ρ(p)+c where ρ\rhoρ is an orthogonal linear map with positive determinant and c∈R3c \in \mathbb{R}^3c∈R3 (do Carmo §1-5, Exercise 6).

Formalization targets

Goal — Fundamental theorem of the local theory of curves (do Carmo, p. 19)

Given smooth functions k,τ:(a,b)→Rk, \tau : (a,b) \to \mathbb{R}k,τ:(a,b)→R with k(s)>0k(s) > 0k(s)>0:

∃ α:(a,b)→R3 parametrized by arc length with curvature k and torsion τ,\exists\, \alpha : (a,b) \to \mathbb{R}^3 \ \text{parametrized by arc length with curvature } k \text{ and torsion } \tau,∃α:(a,b)→R3 parametrized by arc length with curvature k and torsion τ, and any two such curves α,αˉ satisfy αˉ=ρ∘α+c for an orthogonal ρ with det⁡ρ>0.\text{and any two such curves } \alpha, \bar\alpha \text{ satisfy } \bar\alpha = \rho \circ \alpha + c \text{ for an orthogonal } \rho \text{ with } \det \rho > 0 .and any two such curves α,αˉ satisfy αˉ=ρ∘α+c for an orthogonal ρ with detρ>0.

The two halves are also stated separately as milestones, since they are proved by entirely different means: uniqueness by a Gronwall-free energy argument on the Frenet trihedron, existence by solving a linear ODE system.

Supporting statements

The orthonormality of the Frenet trihedron, the Frenet formulas themselves, the characterization of straight lines by k≡0k \equiv 0k≡0 and of plane curves by τ≡0\tau \equiv 0τ≡0, the closed formula τ=− (α′∧α′′)⋅α′′′/k2\tau = -\,(\alpha' \wedge \alpha'')\cdot\alpha''' / k^2τ=−(α′∧α′′)⋅α′′′/k2, and the invariance of arc length, curvature and torsion under rigid motions.

Significance

The theorem is the model case of a classification result: a geometric object modulo a symmetry group is faithfully encoded by a complete set of local invariants. Downstream it is what licenses the standard practice of "prescribing curvature and torsion" — constructing curves with specified geometric behaviour, computing with the Frenet apparatus rather than with the curve itself, and recognizing that any identity among kkk, τ\tauτ and their derivatives is a genuine statement about the curve and not about its parametrization. In do Carmo's own development the local canonical form (§1-6) and the global results of §1-7 both rest on the Frenet apparatus fixed here.

Mathlib contains the analytic ingredients — the Picard–Lindelöf theorem, existence and uniqueness for linear ODE systems, orthonormal bases and the orthogonal group of a real inner product space — but it does not contain the Frenet trihedron of a space curve, the torsion of a space curve, or this theorem. What this mission produces is therefore a reusable formal vocabulary for the local theory of space curves, plus machine-checked proofs of the classical statements about it. The mathematics is completely classical and has been known since Frenet (1847) and Serret (1851); what is open here is the formalization, not the mathematics.

Difficulty

The uniqueness half is a short argument on paper — the function ∣t−tˉ∣2+∣n−nˉ∣2+∣b−bˉ∣2|t - \bar t|^2 + |n - \bar n|^2 + |b - \bar b|^2∣t−tˉ∣2+∣n−nˉ∣2+∣b−bˉ∣2 has vanishing derivative by the Frenet formulas — but formally it requires first establishing that the Frenet frame is differentiable and satisfies those formulas, which needs k>0k > 0k>0 and the smoothness of s↦α′′(s)s \mapsto \alpha''(s)s↦α′′(s) away from its zeros, and then a connectedness argument on the interval.

The existence half cannot be done by exhibiting a formula: the curve is produced by solving the linear system F′=A(s)FF' = A(s) FF′=A(s)F for the 3×33 \times 33×3 frame FFF, checking that the solution stays orthogonal (this is where the skew-symmetry of AAA enters), and then integrating the first row. Recovering that the resulting curve has exactly the prescribed curvature and torsion, as computed by the definitions rather than as postulated by the ODE, is the step where most of the formal work sits.

The obvious shortcut — defining torsion by the closed formula −(α′∧α′′)⋅α′′′/k2-(\alpha' \wedge \alpha'') \cdot \alpha''' / k^2−(α′∧α′′)⋅α′′′/k2 — is not taken here: the definition is the book's, b′=τnb' = \tau nb′=τn, and the closed formula is a milestone to be proved.

Formalization scope

Curves are total functions ℝ → EuclideanSpace ℝ (Fin 3) that are assumed smooth only on the open interval Set.Ioo a b; smoothness is ContDiffOn ℝ (⊤ : ℕ∞), matching do Carmo's use of "differentiable" to mean C∞C^\inftyC∞. Because the interval is open, the ordinary deriv agrees with the derivative along the interval at every interior point, and all derivatives in the statements are plain iterated deriv. Curvature, normal, binormal and torsion are defined exactly as above; at points where k=0k = 0k=0 the normal vector takes the junk value 000, so every statement that mentions nnn, bbb or τ\tauτ carries the hypothesis k≠0k \neq 0k=0 explicitly.

The vector product is defined componentwise on EuclideanSpace ℝ (Fin 3), and a rigid motion is a LinearIsometryEquiv of EuclideanSpace ℝ (Fin 3) with positive determinant followed by a translation.

Degenerate intervals are not excluded: if b≤ab \le ab≤a the interval is empty and the statements hold vacuously, which is why the goal is not formulated as a statement about a single point but as a statement about all of (a,b)(a,b)(a,b) — no hypothesis is vacuous for a<ba < ba<b, and the existence clause is a genuine construction.

Contributions welcome: the Frenet apparatus and the ODE construction are the reusable parts, and both are prerequisites for the later missions of this series.

Selected references

  • Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition, Dover, 2016, Chapter 1, §1-4 and §1-5 (statement on p. 19, uniqueness proof pp. 20–22, existence in the appendix to Chapter 4).
  • F. Frenet, Sur les courbes à double courbure, Journal de Mathématiques Pures et Appliquées 17 (1852), 437–447.
  • J. A. Serret, Sur quelques formules relatives à la théorie des courbes à double courbure, Journal de Mathématiques Pures et Appliquées 16 (1851), 193–207.
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Mathematical PhysicsQuantum InformationTheoretical Computer Science·Captain: Lucas

Undecidability of the Spectral GapResearch Paper

Motivation

The spectral gap of a quantum many-body Hamiltonian is the difference between the energy of its ground state and the energy of its first excited state, in the limit of infinitely many particles. Whether a given microscopic interaction produces a gapped or a gapless system decides much of the macroscopic physics: gapped systems have exponentially decaying correlations and well-defined quantum phases, gapless systems sit at critical points and can display algebraically decaying correlations. Several long-standing questions — the Haldane conjecture for antiferromagnetic spin chains, the existence of gapped topological spin liquids, and the Yang–Mills mass gap — are instances of the question "given the interaction, is the system gapped?".

Cubitt, Pérez-García and Wolf proved that this question, posed for families of two-dimensional translationally invariant nearest-neighbour spin models, admits no algorithmic answer: the spectral gap problem is undecidable (Nature 528, 207–211 (2015); full version: Forum of Mathematics, Pi 10:e14 (2022), also arXiv:1502.04573).

Timeline of the ingredients the proof rests on: Turing's undecidability of the halting problem (1936); Berger's undecidability of the domino problem (1966) and Robinson's aperiodic tile set (Inventiones 12, 177–209 (1971)); Feynman's and Kitaev's circuit-to-Hamiltonian constructions, which turn a computation into a ground state; Gottesman and Irani's translationally invariant one-dimensional Hamiltonians encoding computation (FOCS 2009); and Bitansky–Vadhan-style quantum Turing machine engineering from Bernstein and Vazirani (SIAM J. Comput. 26, 1411–1473 (1997)). The 2015 result was later sharpened to one-dimensional chains by Bausch, Cubitt, Lucia and Pérez-García (PRX 10, 031038 (2020)).

Setting

Fix a local dimension ddd and, for each side length LLL, the square lattice Λ(L)={1,…,L}2\Lambda(L)=\{1,\dots,L\}^2Λ(L)={1,…,L}2 with open boundary conditions. Each site carries a copy of Cd\mathbb{C}^dCd, so the state space of the lattice has the standard product basis indexed by assignments of a level in {1,…,d}\{1,\dots,d\}{1,…,d} to each site. A model is specified by three Hermitian matrices: an on-site term h1h_1h1​ of size d×dd\times dd×d, and two interactions hrow,hcolh_{\mathrm{row}},h_{\mathrm{col}}hrow​,hcol​ of size d2×d2d^2\times d^2d2×d2 acting on horizontally and vertically adjacent pairs. The Hamiltonian of the finite lattice is

HΛ(L)  =  ∑horizontal edgeshrow(i,j)  +  ∑vertical edgeshcol(i,j)  +  ∑k∈Λ(L)h1(k),H^{\Lambda(L)} \;=\; \sum_{\text{horizontal edges}} h_{\mathrm{row}}^{(i,j)} \;+\; \sum_{\text{vertical edges}} h_{\mathrm{col}}^{(i,j)} \;+\; \sum_{k\in\Lambda(L)} h_1^{(k)},HΛ(L)=horizontal edges∑​hrow(i,j)​+vertical edges∑​hcol(i,j)​+k∈Λ(L)∑​h1(k)​,

the same three matrices being used at every edge and every site, which is what translational invariance means here. The quantity max⁡{∥h1∥,∥hrow∥,∥hcol∥}\max\{\|h_1\|,\|h_{\mathrm{row}}\|,\|h_{\mathrm{col}}\|\}max{∥h1​∥,∥hrow​∥,∥hcol​∥} is the local interaction strength.

Write λ0(HΛ(L))≤λ1(HΛ(L))≤⋯\lambda_0(H^{\Lambda(L)})\le\lambda_1(H^{\Lambda(L)})\le\cdotsλ0​(HΛ(L))≤λ1​(HΛ(L))≤⋯ for the eigenvalues and Δ(HΛ(L))=λ1−λ0\Delta(H^{\Lambda(L)})=\lambda_1-\lambda_0Δ(HΛ(L))=λ1​−λ0​ for the finite-size gap. The family {HΛ(L)}L\{H^{\Lambda(L)}\}_L{HΛ(L)}L​ is

  • gapped (Definition 1 of the source) if there are γ>0\gamma>0γ>0 and L0L_0L0​ such that for all L>L0L>L_0L>L0​ the ground state of HΛ(L)H^{\Lambda(L)}HΛ(L) is non-degenerate and Δ(HΛ(L))≥γ\Delta(H^{\Lambda(L)})\ge\gammaΔ(HΛ(L))≥γ;
  • gapless (Definition 2 of the source) if there is c>0c>0c>0 such that for every ε>0\varepsilon>0ε>0 there is an L0L_0L0​ with: for all L>L0L>L_0L>L0​, every point of [λ0,λ0+c][\lambda_0,\lambda_0+c][λ0​,λ0​+c] lies within ε\varepsilonε of the spectrum of HΛ(L)H^{\Lambda(L)}HΛ(L).

These two conditions are not negations of each other; the construction guarantees that every instance falls into one of them. The ground state energy density is Eρ=lim⁡L→∞λ0(HΛ(L))/L2E_\rho=\lim_{L\to\infty}\lambda_0(H^{\Lambda(L)})/L^2Eρ​=limL→∞​λ0​(HΛ(L))/L2.

Formalization targets

Goal — Theorem 3 of the source

For a fixed universal machine and every nnn, one explicit family of interactions, built from fixed integer-valued matrices A,A′,B,C,D,D′A,A',B,C,D,D'A,A′,B,C,D,D′, a diagonal projector Π\PiΠ, a rational β>0\beta>0β>0 that may be taken arbitrarily small, and an algebraic α(n)≤2β\alpha(n)\le 2\betaα(n)≤2β,

h1(n)=α(n)Π,hcol(n)=D+βD′,h_1(n)=\alpha(n)\Pi,\qquad h_{\mathrm{col}}(n)=D+\beta D',h1​(n)=α(n)Π,hcol​(n)=D+βD′, hrow(n)=A+β(A′+eiπφB+e−iπφB†+eiπ2−∣φ∣C+e−iπ2−∣φ∣C†),h_{\mathrm{row}}(n)=A+\beta\Bigl(A'+e^{i\pi\varphi}B+e^{-i\pi\varphi}B^{\dagger}+e^{i\pi 2^{-|\varphi|}}C+e^{-i\pi 2^{-|\varphi|}}C^{\dagger}\Bigr),hrow​(n)=A+β(A′+eiπφB+e−iπφB†+eiπ2−∣φ∣C+e−iπ2−∣φ∣C†),

with φ=φ(n)\varphi=\varphi(n)φ=φ(n) the rational whose binary expansion after the point is the binary expansion of nnn reversed, satisfies: the local interaction strength is at most 111; if the machine halts on input nnn the family is gapped with gap at least 111; and if it does not halt the family is gapless. Since halting is undecidable, no algorithm decides gappedness, even with the promise that exactly one of the two alternatives holds and even at fixed local dimension ddd.

Milestones

The milestone list follows the numbering of the full version: Lemma 8 and Theorem 9 (reduction of halting to ground state energy and to arbitrary low-energy properties), Corollary 7 (the same undecidability for unconstrained local dimension, with rational interactions), Proposition 53 and Corollary 54 (the diverging ground state energy and its promise version), and Theorem 5 (undecidability of the ground state energy density).

Significance

The result rules out a general algorithm — and therefore any complete general method — for deciding gappedness from the interaction matrices, however much computing power is available; the property genuinely depends on arbitrarily large system sizes. It also implies, via the standard link between undecidability and independence, that there are concrete finite-dimensional models whose gap is independent of the axioms of any consistent recursively axiomatized formal system (Corollary 4 of the source), and it transfers to other low-energy properties such as the existence of algebraically decaying ground-state correlations.

The theorem is proved; none of it is formalized. This mission produces the machine-checked version. The reusable infrastructure it forces into existence is substantial on its own: a formal model of translationally invariant lattice Hamiltonians and their thermodynamic-limit spectral behaviour, the tiling layer, and computational-history-state Hamiltonians. Each milestone is a self-contained statement that can be attacked without the others.

Difficulty

The obvious approach — encode a halting computation as an energy penalty — gives the ground state energy of a finite lattice, not a property of the limit; this is exactly what Lemma 8 achieves, and it is not enough, because a gap is a statement about the sequence of spectra as L→∞L\to\inftyL→∞ and is insensitive to any single lattice size. The construction must make the halting information visible at all sufficiently large sizes at once while a fixed finite local dimension carries every instance nnn. That forces three separate difficulties: an aperiodic (Robinson) tiling to create squares of every size 2n2^n2n inside one translationally invariant model; a quantum phase-estimation Turing machine whose transition amplitudes encode nnn in a single phase eiπφ(n)e^{i\pi\varphi(n)}eiπφ(n), so that the instance index does not inflate the local dimension; and a history-state Hamiltonian whose low-energy spectrum can be controlled well enough that a positive energy density in the halting case turns into a genuine spectral gap, and a vanishing one into a dense spectrum above the ground state.

Formalization scope

The development commits to the following conventions, all of which are visible in the definition items of this mission.

  1. Lattices are finite: sites are pairs of indices in {0,…,L−1}\{0,\dots,L-1\}{0,…,L−1}, edges are consecutive pairs within a row or a column (open boundary conditions; the periodic case of Section 6.3 of the source is out of scope).
  2. Operators are complex matrices indexed by product-basis configurations; the interactions are embedded by acting as the given matrix on the two sites of an edge and as the identity elsewhere.
  3. The spectrum is taken as the set of real numbers in the matrix spectrum, and λ0\lambda_0λ0​ is its infimum; every statement carries the Hermiticity hypotheses that make this the usual spectrum. Multiplicities are dimensions of eigenspaces, which is how the "identity of spectra as multisets" of Theorem 9 is expressed.
  4. Gapped, gapless and the energy density are properties of the whole family {HΛ(L)}L\{H^{\Lambda(L)}\}_L{HΛ(L)}L​ generated by a fixed triple of matrices, exactly as in Definitions 1 and 2.
  5. Operator norms are ℓ2\ell_2ℓ2​ operator norms; the local interaction strength is the maximum of the three.
  6. Machines are represented by partial recursive codes: "halts on input nnn" is definedness of the evaluation, and "has not halted after LLL steps" is the step-bounded evaluation returning nothing. The explicit local-dimension bounds of Lemma 8 and Theorem 9, which are stated in the source in terms of the number of internal states and the alphabet size of a Turing machine, are replaced by the existence of a finite local dimension.

Degenerate readings are excluded: a zero local dimension satisfies none of the statements, since a non-degenerate ground state requires a one-dimensional eigenspace and the gapless condition requires a non-empty spectrum; and every existential statement fixes the matrices before quantifying over all instances nnn and all lattice sizes LLL.

Contributions are welcome at any milestone, and also on the infrastructure the milestones need — Wang tilings and the Robinson tile set, Gottesman–Irani history-state Hamiltonians, and quantum Turing machines in the Bernstein–Vazirani sense — which are needed for Theorem 6 and Lemma 47 of the source and are not yet part of this mission's item list.

Selected references

  • T. S. Cubitt, D. Pérez-García, M. M. Wolf, Undecidability of the Spectral Gap (full version), Forum of Mathematics, Pi 10:e14, 1–102 (2022). https://doi.org/10.1017/fmp.2021.15 — the version all statements of this mission are formalized against; preprint: https://arxiv.org/abs/1502.04573
  • T. S. Cubitt, D. Pérez-García, M. M. Wolf, Undecidability of the spectral gap, Nature 528, 207–211 (2015). https://doi.org/10.1038/nature16059
  • R. M. Robinson, Undecidability and nonperiodicity for tilings of the plane, Inventiones Mathematicae 12, 177–209 (1971). https://doi.org/10.1007/BF01418780
  • D. Gottesman, S. Irani, The quantum and classical complexity of translationally invariant tiling and Hamiltonian problems, FOCS 2009. https://arxiv.org/abs/0905.2419
  • E. Bernstein, U. Vazirani, Quantum complexity theory, SIAM J. Comput. 26, 1411–1473 (1997). https://doi.org/10.1137/S0097539796300921
  • J. Bausch, T. S. Cubitt, A. Lucia, D. Pérez-García, Undecidability of the spectral gap in one dimension, Phys. Rev. X 10, 031038 (2020). https://doi.org/10.1103/PhysRevX.10.031038
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Mathematical PhysicsPure Mathematics·Captain: Lucas

The Gribov Region: Geometry of the Landau-Gauge Faddeev--Popov OperatorResearch Paper

Motivation

Quantizing a Yang–Mills theory by the Faddeev–Popov procedure requires a gauge condition that picks one representative from each gauge orbit. In the Landau gauge the condition is ∂μAμa=0\partial_\mu A_\mu^a = 0∂μ​Aμa​=0. Gribov showed in 1978 that this condition is not ideal: a gauge orbit can meet the surface ∂μAμ=0\partial_\mu A_\mu = 0∂μ​Aμ​=0 more than once, so gauge-equivalent configurations — Gribov copies — are still being integrated over (V. N. Gribov, Quantization of non-Abelian gauge theories, Nucl. Phys. B139 (1978) 1). Infinitesimally, a copy of a transverse field AAA corresponds to a zero mode of the Faddeev–Popov operator Mab(A)=−∂μDμab(A)M^{ab}(A) = -\partial_\mu D_\mu^{ab}(A)Mab(A)=−∂μ​Dμab​(A), which is Hermitian on transverse configurations.

Gribov's proposed remedy is to restrict the functional integral to the Gribov region Ω\OmegaΩ, the set of transverse configurations at which M(A)M(A)M(A) is positive definite. The interest of Ω\OmegaΩ is not only that it removes infinitesimal copies: the fact that it is a bounded region of field space is the geometric input of Gribov's confinement scenario, because restricting the integration to a bounded region deforms the gluon propagator in the infrared and produces a mass scale. Whether the restriction to Ω\OmegaΩ is the physically correct prescription is still debated; the geometric properties of Ω\OmegaΩ themselves are not — they are consequences of the algebraic structure of M(A)M(A)M(A), and they are what this mission formalizes.

Timeline of the properties at issue, as recorded in §2.2.1 (pp. 188–189) of the review by N. Vandersickel and D. Zwanziger, The Gribov problem and QCD dynamics, Phys. Rep. 520 (2012) 175–251 (doi:10.1016/j.physrep.2012.07.003):

  • 1978, Gribov: existence of copies infinitesimally across the horizon ∂Ω\partial\Omega∂Ω (Nucl. Phys. B139 (1978) 1).
  • 1982, D. Zwanziger: Ω\OmegaΩ is convex and bounded in every direction (Nucl. Phys. B209 (1982) 336).
  • 1982, M. Semenov-Tyan-Shanskii and V. Franke: the variational characterization of Ω\OmegaΩ by relative minima of ∥AU∥2\|A^U\|^2∥AU∥2, and the fact that Ω\OmegaΩ still contains copies.
  • 1989, G. Dell'Antonio and D. Zwanziger: Ω\OmegaΩ is contained in an ellipsoid (Nucl. Phys. B326 (1989) 333).
  • 1991, G. Dell'Antonio and D. Zwanziger: every gauge orbit passes inside Ω\OmegaΩ (Comm. Math. Phys. 138 (1991) 291–299).

Setting

Fix a real vector space VVV of gauge-field configurations (in the physical situation, the transverse fields AμaA_\mu^aAμa​) and a finite index set {1,…,n}\{1,\dots,n\}{1,…,n} on which the Faddeev–Popov operator acts (colour index times a finite basis of fluctuation modes ω\omegaω). The formalization works with the algebraic structure that the Faddeev–Popov operator has, and nothing else:

M(A)  =  M0  +  M2(A),M(A) \;=\; M_0 \;+\; M_2(A),M(A)=M0​+M2​(A),

where

  • M0M_0M0​ is the field-independent part, M0=−∂2M_0 = -\partial^2M0​=−∂2 in the physical setting, taken here to be a fixed symmetric positive definite n×nn \times nn×n real matrix;
  • A↦M2(A)A \mapsto M_2(A)A↦M2​(A) is linear in AAA, and each M2(A)M_2(A)M2​(A) is a symmetric traceless real n×nn \times nn×n matrix. In the physical setting M2(A)ab=∂μfabcAμcM_2(A)^{ab} = \partial_\mu f^{abc} A_\mu^cM2​(A)ab=∂μ​fabcAμc​, which is traceless already in the colour indices.

The Gribov region is

Ω  =  { A∈V  :  M(A) is positive definite },M(A) positive definite  ⟺  ∀ w≠0, wTM(A) w>0.\Omega \;=\; \{\, A \in V \;:\; M(A) \text{ is positive definite} \,\}, \qquad M(A) \text{ positive definite} \iff \forall\, w \neq 0,\ w^{\mathsf T} M(A)\, w > 0 .Ω={A∈V:M(A) is positive definite},M(A) positive definite⟺∀w=0, wTM(A)w>0.

This is Eq. (2.52) of the review, with positivity as in Eq. (2.54). The boundary ∂Ω\partial\Omega∂Ω is the first Gribov horizon, where the lowest non-trivial eigenvalue of M(A)M(A)M(A) vanishes.

Formalization targets

Goal — Ω\OmegaΩ is a bounded convex set containing the origin

0∈Ω,Ω convex,∀A≠0 ∃λ0>0 ∀λ≥λ0: λA∉Ω,Ω bounded.0 \in \Omega, \qquad \Omega \text{ convex}, \qquad \forall A \neq 0\ \exists \lambda_0 > 0\ \forall \lambda \ge \lambda_0:\ \lambda A \notin \Omega, \qquad \Omega \text{ bounded}.0∈Ω,Ω convex,∀A=0 ∃λ0​>0 ∀λ≥λ0​: λA∈/Ω,Ω bounded.

The last two clauses are stated under the assumption that A↦M2(A)A \mapsto M_2(A)A↦M2​(A) is injective, i.e. that distinct configurations give distinct field-dependent parts; without it Ω\OmegaΩ contains the whole kernel of M2M_2M2​ as a linear subspace and no boundedness statement can hold.

Supporting statements

M(αA1+βA2)=αM(A1)+βM(A2)(α+β=1),M(\alpha A_1 + \beta A_2) = \alpha M(A_1) + \beta M(A_2) \quad (\alpha + \beta = 1),M(αA1​+βA2​)=αM(A1​)+βM(A2​)(α+β=1), M symmetric, tr⁡M=0, M≠0  ⟹  ∃w: wTMw<0.M \text{ symmetric},\ \operatorname{tr} M = 0,\ M \neq 0 \;\Longrightarrow\; \exists w:\ w^{\mathsf T} M w < 0 .M symmetric, trM=0, M=0⟹∃w: wTMw<0.

These are Eq. (2.53) and Eq. (2.58) of the review; they are the two ingredients from which convexity and directional boundedness follow.

Significance

What the result gives: Ω\OmegaΩ is the region to which Gribov's improved gauge fixing restricts the functional integral, and every subsequent construction in this line of work — the no-pole condition, the horizon function and the local Gribov–Zwanziger action — presupposes that the restriction is to a bounded convex region containing the perturbative point A=0A = 0A=0. Convexity is what makes the horizon condition a single well-posed constraint; boundedness in every direction is the property from which the infrared suppression of the gluon propagator, and hence Gribov's mass scale, is read off. Without boundedness there is no geometric mechanism for a mass gap in this scenario.

Status honesty: these statements are proved mathematics, not open problems; the arguments in §2.2.1 of the review are short. What is missing is a machine-checked account. No formalization of the Gribov region in Lean is known to the drafter of this proposal; the platform's existing Gribov material concerns Singer's topological obstruction to continuous gauge fixing, which is a different theorem about a different object.

Difficulty

The statements are elementary once the correct hypotheses are isolated, and the mission is calibrated accordingly: it is a faithfulness exercise rather than a depth exercise. The two places where a naive attempt fails are worth naming. First, directional boundedness does not follow from positivity alone: it needs the tracelessness of M2(A)M_2(A)M2​(A), which is what forces a direction www with wTM2(A)w<0w^{\mathsf T} M_2(A) w < 0wTM2​(A)w<0; a positive semidefinite perturbation would give a region unbounded along that ray. Second, "bounded in every direction" does not imply "bounded" for a general set, and the implication used here rests on convexity together with injectivity of M2M_2M2​ — the argument goes through a limit of rescaled configurations and a closure of the positivity condition, not through a uniform bound extracted directly from the ray statement.

Formalization scope

The mission commits to a finite-dimensional linear-algebra model of the Faddeev–Popov operator, packaged as a structure carrying: the matrix M0M_0M0​ together with a proof that it is positive definite; the linear map A↦M2(A)A \mapsto M_2(A)A↦M2​(A) together with proofs that each M2(A)M_2(A)M2​(A) is symmetric and traceless. Configurations live in an arbitrary real vector space VVV, which carries a norm and finite-dimensionality only in the two statements where boundedness is asserted. Positive definiteness is Mathlib's notion for real matrices, which includes symmetry; the region is the set of configurations where it holds strictly, so Ω\OmegaΩ is the open region and the horizon is not part of it.

This is a model, not the field-theoretic object: it replaces the operator −∂μDμ-\partial_\mu D_\mu−∂μ​Dμ​ acting on transverse fields by its finite-dimensional algebraic shadow, and the reviewer should audit it as such. The properties targeted here are exactly those whose proofs in §2.2.1 use only linearity in AAA, symmetry, tracelessness, and positivity of −∂2-\partial^2−∂2; results that genuinely need the infinite-dimensional setting — that every gauge orbit passes inside Ω\OmegaΩ, and that Ω\OmegaΩ still contains copies on its boundary — are deliberately out of scope, since they cannot be stated in this model.

The model is not vacuous: an instance exists already for V=RV = \mathbb{R}V=R, n=2n = 2n=2, M0=IM_0 = IM0​=I and M2(t)=t diag(1,−1)M_2(t) = t\,\mathrm{diag}(1,-1)M2​(t)=tdiag(1,−1), with M2M_2M2​ injective, so none of the statements is satisfied vacuously. Nor is any target trivially true: Ω\OmegaΩ is a proper nonempty subset of VVV in that instance.

Infrastructure needed: Mathlib's positive-definiteness API for matrices, the spectral theorem for real symmetric matrices (for the traceless lemma), and basic convexity and boundedness in finite-dimensional normed spaces. The traceless lemma — a nonzero symmetric traceless matrix has a direction of negative quadratic form — is reusable well beyond this mission. Contributions extending the model towards the infinite-dimensional setting, or supplying the explicit ellipsoidal bound of Dell'Antonio–Zwanziger in place of plain boundedness, are welcome.

Selected references

  • N. Vandersickel, D. Zwanziger, The Gribov problem and QCD dynamics, Physics Reports 520 (2012) 175–251. https://doi.org/10.1016/j.physrep.2012.07.003
  • V. N. Gribov, Quantization of non-Abelian gauge theories, Nuclear Physics B139 (1978) 1.
  • D. Zwanziger, Nonperturbative modification of the Faddeev–Popov formula and banishment of the naive vacuum, Nuclear Physics B209 (1982) 336.
  • M. Semenov-Tyan-Shanskii, V. Franke, A variational principle for the Lorentz condition and restriction of the domain of path integration in non-abelian gauge theory, 1982.
  • G. Dell'Antonio, D. Zwanziger, Ellipsoidal bound on the Gribov horizon contradicts the perturbative renormalization group, Nuclear Physics B326 (1989) 333.
  • G. Dell'Antonio, D. Zwanziger, Every gauge orbit passes inside the Gribov horizon, Communications in Mathematical Physics 138 (1991) 291–299.
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AnalysisNumber Theory·Captain: Lucas

The de Bruijn–Newman Constant is Non-negativeResearch Paper

Motivation

The Riemann hypothesis asserts that all nontrivial zeros of the Riemann zeta function lie on the critical line. A classical way to measure how far the hypothesis is from failing runs through a one-parameter deformation of the Riemann ξ\xiξ function by the backward heat flow. De Bruijn (1950) introduced a family of entire functions HtH_tHt​, t∈Rt \in \mathbb{R}t∈R, with H0H_0H0​ essentially the ξ\xiξ function, and showed that HtH_tHt​ has only real zeros for t≥1/2t \ge 1/2t≥1/2. Newman (1976) proved that there is a finite constant Λ\LambdaΛ, now called the de Bruijn–Newman constant, such that HtH_tHt​ has only real zeros precisely when t≥Λt \ge \Lambdat≥Λ. The Riemann hypothesis is exactly the statement Λ≤0\Lambda \le 0Λ≤0, and Newman conjectured the complementary bound Λ≥0\Lambda \ge 0Λ≥0 — in his phrase, that if the Riemann hypothesis is true, then it is only barely so.

Timeline of lower bounds on Λ\LambdaΛ, all obtained before 2018 by exhibiting Lehmer pairs, that is, pairs of adjacent zeros of ζ\zetaζ that are unusually close together: Λ>−∞\Lambda > -\inftyΛ>−∞ (Newman 1976), Λ≥−50\Lambda \ge -50Λ≥−50 (Csordas–Norfolk–Varga 1988), Λ≥−5\Lambda \ge -5Λ≥−5 (te Riele 1991), Λ≥−0.385\Lambda \ge -0.385Λ≥−0.385 (Norfolk–Ruttan–Varga 1992), Λ≥−0.0991\Lambda \ge -0.0991Λ≥−0.0991 (Csordas–Ruttan–Varga 1991), Λ≥−4.379×10−6\Lambda \ge -4.379 \times 10^{-6}Λ≥−4.379×10−6 (Csordas–Smith–Varga 1994), Λ≥−5.895×10−9\Lambda \ge -5.895 \times 10^{-9}Λ≥−5.895×10−9 (Csordas–Odlyzko–Smith–Varga 1993), Λ≥−2.63×10−9\Lambda \ge -2.63 \times 10^{-9}Λ≥−2.63×10−9 (Odlyzko 2000), Λ≥−1.15×10−11\Lambda \ge -1.15 \times 10^{-11}Λ≥−1.15×10−11 (Saouter–Gourdon–Demichel 2011). Rodgers and Tao closed the gap in 2020 by proving Λ≥0\Lambda \ge 0Λ≥0. In the other direction, de Bruijn's bound Λ≤1/2\Lambda \le 1/2Λ≤1/2 was sharpened to Λ<1/2\Lambda < 1/2Λ<1/2 by Ki–Kim–Lee (2009) and to Λ≤0.22\Lambda \le 0.22Λ≤0.22 by the Polymath 15 project (2019).

Setting

For a real number uuu put

Φ(u):=∑n=1∞(2π2n4e9u−3πn2e5u)exp⁡(−πn2e4u),\Phi(u) := \sum_{n=1}^{\infty}\bigl(2\pi^2 n^4 e^{9u} - 3\pi n^2 e^{5u}\bigr)\exp\bigl(-\pi n^2 e^{4u}\bigr),Φ(u):=n=1∑∞​(2π2n4e9u−3πn2e5u)exp(−πn2e4u),

a function that decays super-exponentially as ∣u∣→∞|u| \to \infty∣u∣→∞ and satisfies Φ(u)=Φ(−u)\Phi(u) = \Phi(-u)Φ(u)=Φ(−u). For each t∈Rt \in \mathbb{R}t∈R define the entire function

Ht(z):=∫0∞etu2 Φ(u) cos⁡(zu) du.H_t(z) := \int_0^{\infty} e^{t u^2}\,\Phi(u)\,\cos(z u)\,du .Ht​(z):=∫0∞​etu2Φ(u)cos(zu)du.

Each HtH_tHt​ is even and satisfies Ht(zˉ)=Ht(z)‾H_t(\bar z) = \overline{H_t(z)}Ht​(zˉ)=Ht​(z)​; the function H0H_0H0​ is 18ξ(12+iz2)\tfrac18 \xi\bigl(\tfrac12 + \tfrac{iz}{2}\bigr)81​ξ(21​+2iz​), so the Riemann hypothesis says exactly that every zero of H0H_0H0​ is real. Write

S:={ t∈R:every zero of Ht is real },Λ:=inf⁡S.S := \{\, t \in \mathbb{R} : \text{every zero of } H_t \text{ is real} \,\},\qquad \Lambda := \inf S .S:={t∈R:every zero of Ht​ is real},Λ:=infS.

By Pólya and Newman, SSS is the ray [Λ,∞)[\Lambda, \infty)[Λ,∞) with −∞<Λ≤1/2-\infty < \Lambda \le 1/2−∞<Λ≤1/2.

When Λ<t≤0\Lambda < t \le 0Λ<t≤0 the zeros of HtH_tHt​ are real, simple, symmetric about the origin and avoid the origin, so they can be listed as (xj(t))j∈Z∗(x_j(t))_{j \in \mathbb{Z}^*}(xj​(t))j∈Z∗​, indexed by the nonzero integers, with 0<x1(t)<x2(t)<⋯0 < x_1(t) < x_2(t) < \cdots0<x1​(t)<x2​(t)<⋯ and x−j(t)=−xj(t)x_{-j}(t) = -x_j(t)x−j​(t)=−xj​(t). The classical locations ξj\xi_jξj​ are defined for j≥1j \ge 1j≥1 by Ψ(ξj)=j\Psi(\xi_j) = jΨ(ξj​)=j with

Ψ(T):=T4πlog⁡T4π−T4π,\Psi(T) := \frac{T}{4\pi}\log\frac{T}{4\pi} - \frac{T}{4\pi},Ψ(T):=4πT​log4πT​−4πT​,

extended by ξ−j=−ξj\xi_{-j} = -\xi_jξ−j​=−ξj​; they are the positions the zeros would occupy if the Riemann–von Mangoldt counting formula were exact. Throughout, log⁡+x:=log⁡(2+∣x∣)\log_+ x := \log(2 + |x|)log+​x:=log(2+∣x∣).

Formalization targets

Goal — Newman's conjecture

Λ≥0,equivalentlyevery t with Ht having only real zeros satisfies t≥0.\Lambda \ge 0, \qquad\text{equivalently}\qquad \text{every } t \text{ with } H_t \text{ having only real zeros satisfies } t \ge 0 .Λ≥0,equivalentlyevery t with Ht​ having only real zeros satisfies t≥0.

The goal is stated in both forms simultaneously, so that it does not depend on any convention for the infimum of a set that might be empty or unbounded below.

Milestones

The milestone list follows the architecture of Rodgers–Tao, which is a proof by contradiction: every milestone is stated under the standing hypothesis Λ<0\Lambda < 0Λ<0 of that paper, in the time ranges the paper uses (Λ<t≤0\Lambda < t \le 0Λ<t≤0, then Λ/2≤t≤0\Lambda/2 \le t \le 0Λ/2≤t≤0, then Λ/4≤t≤0\Lambda/4 \le t \le 0Λ/4≤t≤0). In order: an upper bound for HtH_tHt​ near the real axis (Lemma 4); Riemann–von Mangoldt type counting formulae for the zeros of HtH_tHt​ (Theorem 9); the resulting macroscopic description of the zeros (Corollary 10); the equations of motion ∂txk=2∑j≠k(xk−xj)−1\partial_t x_k = 2\sum_{j \ne k} (x_k - x_j)^{-1}∂t​xk​=2∑j=k​(xk​−xj​)−1 (Theorem 11); a quantitative lower bound on gaps between zeros (Proposition 13); a bound on the time-integrated renormalized energy (Theorem 17); and a bound on that energy at time t=0t = 0t=0 (Proposition 26). The last of these says that at time zero the zeros are, on average, locally in the equilibrium configuration of an arithmetic progression, which contradicts known results on the local distribution of zeros of ζ\zetaζ.

Significance

Λ≥0\Lambda \ge 0Λ≥0 settles Newman's conjecture, and together with the Riemann hypothesis it would force Λ=0\Lambda = 0Λ=0. Unconditionally, it says that the zeros of ξ\xiξ are not in local equilibrium: infinitely often, gaps between consecutive zeros deviate from the mean spacing, which is what makes the pair correlation phenomenology of Montgomery and of Conrey–Ghosh–Goldston–Gonek–Heath-Brown incompatible with Λ<0\Lambda < 0Λ<0. Any proof of the Riemann hypothesis must therefore be compatible with the hypothesis being tight in this sense.

The theorem has a complete published proof (Rodgers–Tao, Forum of Mathematics, Pi, 2020); it is not an open problem. What is missing is a machine-checked proof. To the extent the material has been formalized at all, the underlying objects — the ξ\xiξ function, the heat flow HtH_tHt​, the counting function for zeros, the zero dynamics, the renormalized energies — are not available in Mathlib, so the mission produces reusable analytic infrastructure: bounds for a Fourier–Laplace type integral by the saddle point method, a Riemann–von Mangoldt counting argument via the argument principle, and a gradient-flow monotonicity framework for an infinite particle system with logarithmic interaction.

Difficulty

The obvious route to Λ≥0\Lambda \ge 0Λ≥0 is the one used for every previous lower bound: exhibit Lehmer pairs of ever higher quality, since if Λ\LambdaΛ were very negative the zeros of H0H_0H0​ would repel each other and unusually close pairs of zeta zeros could not exist. Producing an infinite sequence of Lehmer pairs of arbitrarily high quality is possible under the GUE hypothesis, but the known unconditional upper bounds for small gaps between zeta zeros are too weak, even assuming the Riemann hypothesis. The proof instead upgrades repulsion to relaxation to local equilibrium: it must control the zeros of HtH_tHt​ uniformly for Λ<t≤0\Lambda < t \le 0Λ<t≤0 at length scales as fine as log⁡T\log TlogT, with only the weaker counting formulae available for negative ttt (an error term O(log⁡+2T)O(\log_+^2 T)O(log+2​T) rather than O(log⁡+T)O(\log_+ T)O(log+​T)), and must make sense of a Hamiltonian and an energy that are given by divergent series, which requires truncation, renormalization, and careful control of all the resulting boundary terms.

Formalization scope

The Lean development commits to the following conventions. Φ\PhiΦ is a tsum over the positive integers and Ht(z)H_t(z)Ht​(z) is the Bochner integral over (0,∞)(0, \infty)(0,∞) of etu2Φ(u)cos⁡(zu)e^{tu^2}\Phi(u)\cos(zu)etu2Φ(u)cos(zu); no convergence or entireness statement is built into the definition. Λ\LambdaΛ is sInf of the set of admissible times, and the goal theorem also states the quantifier form "every admissible ttt is nonnegative", so it cannot be satisfied by a junk value of the infimum. The zero families (xj(t))(x_j(t))(xj​(t)) and the classical locations (ξj)(\xi_j)(ξj​) are not defined by choice functions: they enter the milestones as universally quantified functions Z→R\mathbb{Z} \to \mathbb{R}Z→R subject to explicit predicates saying exactly which sequences they are, so a milestone asserts something about every valid enumeration. Asymptotic notation is unfolded: O(⋅)O(\cdot)O(⋅) becomes an explicit existential constant, oT→∞(⋅)o_{T \to \infty}(\cdot)oT→∞​(⋅) an explicit ε\varepsilonε–T0T_0T0​ statement, and a principal value sum a limit of symmetric partial sums. Where a statement asserts the value of a time integral, absolute integrability is part of the conclusion, so the statement cannot be satisfied by the convention that a non-integrable function has integral zero.

One degeneracy is inherent to the source and is stated here explicitly: since the paper argues by contradiction, each milestone carries the hypothesis Λ<0\Lambda < 0Λ<0 (directly, or through a time range such as Λ<t≤0\Lambda < t \le 0Λ<t≤0). Once the goal theorem is proved, those hypotheses are unsatisfiable and the milestones become vacuously true. They are the intended attack path on the goal, not independent targets, and a solver who derives one of them from the goal theorem contributes nothing.

Contributions welcome: the analytic estimates for HtH_tHt​ (Lemma 4) and the counting formulae (Theorem 9) are independent of the dynamical part and are the natural entry points; Mathlib-level infrastructure on the argument principle, the saddle point method, and Stirling asymptotics for Γ\GammaΓ in vertical strips is reusable well beyond this mission.

Selected references

  • B. Rodgers and T. Tao, The de Bruijn–Newman constant is non-negative, Forum of Mathematics, Pi 8 (2020), e6. https://doi.org/10.1017/fmp.2020.6
  • N. G. de Bruijn, The roots of trigonometric integrals, Duke Math. J. 17 (1950), 197–226. https://doi.org/10.1215/S0012-7094-50-01720-0
  • C. M. Newman, Fourier transforms with only real zeros, Proc. Amer. Math. Soc. 61 (1976), 246–251. https://doi.org/10.1090/S0002-9939-1976-0434982-5
  • G. Csordas, W. Smith and R. S. Varga, Lehmer pairs of zeros, the de Bruijn–Newman constant Λ\LambdaΛ, and the Riemann hypothesis, Constr. Approx. 10 (1994), 107–129. https://doi.org/10.1007/BF01205170
  • H. L. Montgomery, The pair correlation of zeros of the zeta function, Proc. Sympos. Pure Math. XXIV (1973), 181–193. https://doi.org/10.1090/pspum/024
  • J. B. Conrey, A. Ghosh, D. Goldston, S. M. Gonek and D. R. Heath-Brown, On the distribution of gaps between zeros of the zeta-function, Q. J. Math. 36 (1985), 43–51. https://doi.org/10.1093/qmath/36.1.43
  • D. H. J. Polymath, Effective approximation of heat flow evolution of the Riemann ξ\xiξ function, and a new upper bound for the de Bruijn–Newman constant, Res. Math. Sci. 6 (2019), 31. https://doi.org/10.1007/s40687-019-0193-1
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CombinatoricsMechanism Design·Captain: Shuze Chen

Algorithmic Game Theory V: Stable Matching and Trading without MoneyTextbook

Algorithmic Game Theory V: Stable Matching and Trading without Money

Motivation

When money is off the table and the Gibbard–Satterthwaite theorem (Mission III of this series) blocks general strategyproof choice, restricted preference domains reopen the door. The two great examples both come from allocation: Shapley–Scarf's housing market (1974), where Gale's Top Trading Cycle algorithm finds the unique core allocation and Roth (1982) showed the mechanism is strategy-proof; and the Gale–Shapley marriage market (1962), where deferred acceptance produces a stable matching, the men-optimal one, which Dubins–Freedman (1981) and Roth (1982) showed cannot be manipulated by any man. This machinery runs the US medical residency match and school choice systems worldwide, and the 2012 Nobel memorial prize to Roth and Shapley cites exactly the results of this mission. Chapter 10 (Schummer–Vohra, "Mechanism Design without Money") of Nisan–Roughgarden–Tardos–Vazirani (eds.), Algorithmic Game Theory (Cambridge, 2007) is the source text; its single-peaked §10.2 is left to a possible later mission, since it needs its own preference-domain machinery.

Setting

Marriage market (§10.4): finite sets MMM of men and WWW of women, each agent holding a strict preference ordering over the opposite side (the preference-profile vocabulary of Mission III; P i a bP\,i\,a\,bPiab reads "iii strictly prefers aaa to bbb"). Following the book's dummy-partner convention, ∣M∣=∣W∣|M| = |W|∣M∣=∣W∣ and a matching is a bijection μ:M≃W\mu : M \simeq Wμ:M≃W. A pair (m,w)(m, w)(m,w) blocks μ\muμ if each prefers the other to their assigned partner; μ\muμ is stable if no pair blocks it. A stable μ\muμ is male-optimal if every man weakly prefers it to every stable alternative. A coalition dominates μ\muμ if it can rematch within itself with every member strictly better off; the core is the set of undominated matchings.

Housing market (§10.3): a finite set NNN of agents, agent iii owning house iii, each with a strict preference over all houses; an allocation is a permutation of NNN. A coalition blocks an allocation if it can redistribute the houses its members own so that all are weakly and someone strictly better off.

Formalization targets

Goal (capstone) — Theorem 10.13

Any mechanism selecting the male-optimal stable matching is strategy-proof for the men: no man can misreport his ordering and obtain a wife he truly prefers.

Theorem 10.10 — existence

Every marriage market has a stable matching.

Theorem 10.11 / Gale–Shapley 1962 — male-optimality

Some stable matching is weakly best for every man simultaneously. This man-by-man form is Gale–Shapley's optimal assignment (1962, Theorem 2); the book's Theorem 10.11 phrases male-optimality as the absence of a stable alternative making every man weakly and some man strictly better off, which is equivalent for finite strict markets — the equivalence being a (short) theorem, the attribution follows Gale–Shapley.

Theorem 10.12 — the core

A matching is stable iff it is in the core of the matching game.

Theorems 10.6 and 10.7 — housing

The core of the housing market is a single allocation, and the mechanism selecting it is strategy-proof.

Significance

These are the foundational theorems of market design — the branch of mechanism design with the strongest record of deployed systems — and none of them exists in Lean. The mission also settles a methodological point for the series: algorithm-defined objects (deferred acceptance, top trading cycles) enter through the properties that characterize their outputs — male-optimality, core membership — so the theorems are statements about all mechanisms with the given property, and any construction of the algorithm proves the existence milestones. The matching vocabulary (bijections as matchings, blocking, stability, domination) is reusable for the college-admissions and roommates variants beyond this mission.

Difficulty

Existence (10.10) is the real formalization work: whether by formalizing deferred acceptance and its termination or by another route (e.g. Adachi's fixed-point formulation, which the book sketches as Theorem 10.14 via Tarski), the solver must build the proposal machinery. Male-optimality (10.11) rides on the same construction with the "no man is ever rejected by an achievable wife" invariant. The core equivalence (10.12) is deliberately light — a transposition embeds a blocking pair as a two-agent coalition. Housing uniqueness (10.6) needs the cycle-peeling induction of TTC. The two strategyproofness results are the subtle ones: both known proof routes (Dubins–Freedman's combinatorial argument, or Roth's via the blocking lemma) require careful bookkeeping of which coalitions can improve under a misreport, and the mechanism is pinned only by its defining property, so proofs must use optimality/core facts rather than algorithm internals.

Formalization scope

Preferences are strict total orders as in Mission III (IsPrefProfile), oriented "first argument preferred". Matchings are Equivs; the book's ∣M∣=∣W∣|M| = |W|∣M∣=∣W∣ convention enters the existence statements as the hypothesis Nonempty (M ≃ W) and nothing else about cardinalities is assumed. Domination and house-blocking quantify a rematching Equiv together with the improving coalition, coalitions being sets closed under the rematching — single-agent and pair coalitions are special cases, so no separate pair-blocking clause is needed in the core theorems. Mechanisms in the strategyproofness results are arbitrary functions constrained only by their defining property (male-optimal selection; core selection), quantified before the misreport — nothing may be chosen with hindsight. Both sides keep finiteness only where used: the core equivalence (10.12) holds for arbitrary types and carries no Fintype.

Selected references

  • D. Gale, L. S. Shapley, College admissions and the stability of marriage, Amer. Math. Monthly 69 (1962), 9–15. DOI
  • L. Shapley, H. Scarf, On cores and indivisibility, J. Math. Econ. 1 (1974), 23–37. DOI
  • L. E. Dubins, D. A. Freedman, Machiavelli and the Gale–Shapley algorithm, Amer. Math. Monthly 88 (1981), 485–494. DOI
  • A. E. Roth, The economics of matching: stability and incentives, Math. Oper. Res. 7 (1982), 617–628. DOI
  • A. E. Roth, Incentive compatibility in a market with indivisible goods, Econ. Letters 9 (1982), 127–132. DOI
  • N. Nisan, T. Roughgarden, É. Tardos, V. V. Vazirani (eds.), Algorithmic Game Theory, Cambridge University Press, 2007, Chapter 10. DOI
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Mechanism DesignTheoretical Computer Science·Captain: Shuze Chen

Algorithmic Game Theory IV: VCG and the Limits of TruthfulnessTextbook

Motivation

Mission III of this series ends at an impossibility: without money, incentive compatibility over three or more alternatives means dictatorship. This mission formalizes the classical escape route — quasilinear utilities and payments — and the exact price of it. Vickrey (1961) discovered that a second-price auction makes truth-telling dominant; Clarke (1971) and Groves (1973) generalized the idea to arbitrary social choice: welfare-maximizing rules can always be made truthful by the right payments. The converse program — which choice rules are implementable at all — runs through Rochet (1987) and Myerson (1981) to Saks–Yu (2005): weak monotonicity characterizes implementability on convex domains, and on single-parameter domains the characterization is complete and elementary — monotone rules with critical-value payments. Chapter 9, §§9.3 and 9.5 of Nisan–Roughgarden–Tardos–Vazirani (eds.), Algorithmic Game Theory (Cambridge, 2007), written by Nisan, is the source text.

Setting

A set AAA of alternatives and a finite set ι\iotaι of players. Player iii holds a private valuation vi:A→Rv_i : A \to \mathbb{R}vi​:A→R from a publicly known domain Vi⊆RAV_i \subseteq \mathbb{R}^AVi​⊆RA; utilities are quasilinear: choosing aaa and charging pip_ipi​ gives iii utility vi(a)−piv_i(a) - p_ivi​(a)−pi​. A (direct revelation) mechanism is a social choice function fff from valuation profiles to AAA together with payment functions pip_ipi​ (Definition 9.14). The mechanism is incentive compatible if no unilateral misreport from the domain ever beats the truth (Definition 9.15).

A VCG mechanism (Definition 9.16) has fff maximizing social welfare ∑ivi(a)\sum_i v_i(a)∑i​vi​(a) and payments of the Groves form pi=hi(v−i)−∑j≠ivj(f(v))p_i = h_i(v_{-i}) - \sum_{j\ne i} v_j(f(v))pi​=hi​(v−i​)−∑j=i​vj​(f(v)); the Clarke pivot rule takes hi(v−i)=max⁡b∑j≠ivj(b)h_i(v_{-i}) = \max_b \sum_{j \ne i} v_j(b)hi​(v−i​)=maxb​∑j=i​vj​(b). A rule is weakly monotone (Definition 9.28) if a unilateral change of valuation that moves the outcome from aaa to bbb satisfies vi′(b)−vi′(a)≥vi(b)−vi(a)v_i'(b) - v_i'(a) \ge v_i(b) - v_i(a)vi′​(b)−vi′​(a)≥vi​(b)−vi​(a). A single-parameter domain (Definition 9.33) is given by a win set Wi⊆AW_i \subseteq AWi​⊆A per player and bids t∈[t0,t1]t \in [t_0, t_1]t∈[t0​,t1​]: the valuation is ttt on WiW_iWi​ and 000 elsewhere.

Formalization targets

Goal (capstone) — Theorem 9.36

A normalized mechanism (losers pay 0) on a single-parameter domain is incentive compatible iff the rule is monotone and every winning bid pays the critical value — the threshold below which the bid loses.

Theorem 9.17 — VCG is truthful

Every VCG mechanism is incentive compatible.

Lemma 9.20 — Clarke pivot

With Clarke pivot payments, a welfare-maximizing rule makes no positive transfers, and is individually rational when valuations are nonnegative.

Theorem 9.29 — weak monotonicity

Necessity: incentive compatibility forces WMON, on any domain. Sufficiency: on convex domains, WMON rules admit implementing payments (Saks–Yu).

Significance

These are the working theorems of every later mechanism-design mission: the approximation mechanisms of Chapter 12, the profit-maximization results of Chapter 13, and the sponsored-search analysis of Chapter 28 all argue through Theorem 9.36's monotonicity-plus-critical-value normal form, and VCG is the benchmark they approximate. Formalizing the cluster produces the platform's quasilinear-mechanism vocabulary — domains, truthfulness, Groves payments, weak monotonicity, single-parameter settings — on top of the social-choice layer of Mission III.

The capstone and Theorem 9.17 are textbook results with complete proofs in the source; the Saks–Yu half of Theorem 9.29 is stated but not proved in the book ("quite involved"), so that milestone carries a genuinely hard formalization with a published paper proof. None have prior Lean formalizations.

Difficulty

Theorem 9.17 is a three-line inequality chase once the Groves form is unfolded — a deliberate warm-up. Lemma 9.20 adds the attained maximum over a finite alternative set. The necessity half of 9.29 is a two-application argument; the sufficiency half is the hard point of the mission: the known proofs walk two-cycle inequalities into a path-integral construction of payments on a convex domain, and nothing of the kind exists in Mathlib. For the capstone, the delicate part is the critical value: the book defines it as a supremum that "is undefined" when the player always wins, and the honest formal rendering — a constant payment c that is a least upper bound of the losing bids whenever losing bids exist — makes the case split explicit; the equivalence proof must thread monotonicity, the threshold structure of the winning set, and normalization through both directions.

Formalization scope

Valuations are functions A → ℝ; domains are sets V i : Set (A → ℝ); mechanisms are total functions with every property quantified only over profiles from the domain, so behavior on invalid inputs carries no content. The Groves term hᵢ is a function of the full profile constrained to be invariant under changes of coordinate i — the standard rendering of "depends only on v−iv_{-i}v−i​". The Clarke payment uses a Finset.sup' over a finite nonempty A, so no junk supremum arises. In the single-parameter setting the valuation induced by a bid is Set.indicator, bids live in Set.Icc t0 t1 with t0 ≤ t1, and the critical value is characterized by IsLUB guarded by nonemptiness of the losing set — the book's "undefined" caveat made precise without a junk sSup. Weak monotonicity's sufficiency half carries Convex ℝ (V i) and finite A (the Saks–Yu setting); the necessity half deliberately carries no hypotheses beyond incentive compatibility itself.

Selected references

  • W. Vickrey, Counterspeculation, auctions, and competitive sealed tenders, J. Finance 16 (1961), 8–37. DOI
  • E. H. Clarke, Multipart pricing of public goods, Public Choice 11 (1971), 17–33. DOI
  • T. Groves, Incentives in teams, Econometrica 41 (1973), 617–631. DOI
  • M. Saks, L. Yu, Weak monotonicity suffices for truthfulness on convex domains, Proc. 6th ACM EC (2005), 286–293. DOI
  • N. Nisan, T. Roughgarden, É. Tardos, V. V. Vazirani (eds.), Algorithmic Game Theory, Cambridge University Press, 2007, Chapter 9, §§9.3, 9.5. DOI
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Analysis·Captain: Lucas

Rudin PMA VI: The Riemann-Stieltjes IntegralTextbook

Motivation

Chapter 6 of Walter Rudin's Principles of Mathematical Analysis (3rd edition, McGraw-Hill, 1976) constructs the Riemann–Stieltjes integral ∫abf dα\int_a^b f\,d\alpha∫ab​fdα: the Riemann integral with the increments Δxi\Delta x_iΔxi​ of the variable replaced by the increments Δαi=α(xi)−α(xi−1)\Delta \alpha_i = \alpha(x_i) - \alpha(x_{i-1})Δαi​=α(xi​)−α(xi−1​) of a monotonically increasing integrator α\alphaα. Taking α(x)=x\alpha(x) = xα(x)=x recovers the ordinary Riemann integral; taking α\alphaα a step function turns integrals into sums, so series and integrals become special cases of one construction. This is the reason Rudin develops the theory in this generality: it unifies Chapter 3's series with the integral, and it is the natural setting for the Fourier coefficients of Chapter 8.

The chapter's capstone is the fundamental theorem of calculus (Theorem 6.21): an integrable function which is the derivative of some FFF integrates to F(b)−F(a)F(b) - F(a)F(b)−F(a).

This mission is the sixth in a series formalizing Rudin Chapters 1–11; it uses the uniform continuity of Mission IV and the mean value theorem of Mission V.

Setting

A partition PPP of [a,b][a,b][a,b] is a finite set of points a=x0≤x1≤⋯≤xn=ba = x_0 \le x_1 \le \dots \le x_n = ba=x0​≤x1​≤⋯≤xn​=b, with increments Δαi=α(xi)−α(xi−1)\Delta \alpha_i = \alpha(x_i) - \alpha(x_{i-1})Δαi​=α(xi​)−α(xi−1​) for a monotonically increasing α\alphaα. For a bounded real fff put Mi=sup⁡[xi−1,xi]fM_i = \sup_{[x_{i-1},x_i]} fMi​=sup[xi−1​,xi​]​f, mi=inf⁡[xi−1,xi]fm_i = \inf_{[x_{i-1},x_i]} fmi​=inf[xi−1​,xi​]​f, and

U(P,f,α)=∑i=1nMi Δαi,L(P,f,α)=∑i=1nmi Δαi.U(P,f,\alpha) = \sum_{i=1}^n M_i\,\Delta\alpha_i, \qquad L(P,f,\alpha) = \sum_{i=1}^n m_i\,\Delta\alpha_i .U(P,f,α)=i=1∑n​Mi​Δαi​,L(P,f,α)=i=1∑n​mi​Δαi​.

The upper and lower integrals are inf⁡PU(P,f,α)\inf_P U(P,f,\alpha)infP​U(P,f,α) and sup⁡PL(P,f,α)\sup_P L(P,f,\alpha)supP​L(P,f,α); fff is integrable with respect to α\alphaα, written f∈R(α)f \in \mathcal{R}(\alpha)f∈R(α), when they agree, and the common value is ∫abf dα\int_a^b f\,d\alpha∫ab​fdα. P′P'P′ refines PPP when every division point of PPP is one of P′P'P′. Writing R\mathcal{R}R for R(α)\mathcal{R}(\alpha)R(α) with α(x)=x\alpha(x) = xα(x)=x gives the Riemann integral ∫abf dx\int_a^b f\,dx∫ab​fdx.

Formalization targets

Goal — the fundamental theorem of calculus (Theorem 6.21)

f∈R on [a,b],F′=f on [a,b]  ⟹  ∫abf(x) dx=F(b)−F(a).f \in \mathcal{R} \text{ on } [a,b], \quad F' = f \text{ on } [a,b] \;\Longrightarrow\; \int_a^b f(x)\,dx = F(b) - F(a).f∈R on [a,b],F′=f on [a,b]⟹∫ab​f(x)dx=F(b)−F(a).

Milestones

P′ refines P⇒L(P,f,α)≤L(P′,f,α), U(P′,f,α)≤U(P,f,α)(6.4)P' \text{ refines } P \Rightarrow L(P,f,\alpha) \le L(P',f,\alpha),\ U(P',f,\alpha) \le U(P,f,\alpha) \qquad (6.4)P′ refines P⇒L(P,f,α)≤L(P′,f,α), U(P′,f,α)≤U(P,f,α)(6.4) ∫‾f dα≤∫‾f dα(6.5)\underline{\int} f\,d\alpha \le \overline{\int} f\,d\alpha \qquad (6.5)∫​fdα≤∫​fdα(6.5) f∈R(α)  ⟺  ∀ε>0 ∃P, U(P,f,α)−L(P,f,α)<ε(6.6)f \in \mathcal{R}(\alpha) \iff \forall \varepsilon>0\ \exists P,\ U(P,f,\alpha) - L(P,f,\alpha) < \varepsilon \qquad (6.6)f∈R(α)⟺∀ε>0 ∃P, U(P,f,α)−L(P,f,α)<ε(6.6) f continuous⇒f∈R(α)(6.8)f \text{ continuous} \Rightarrow f \in \mathcal{R}(\alpha) \qquad (6.8)f continuous⇒f∈R(α)(6.8) f monotone, α continuous⇒f∈R(α)(6.9)f \text{ monotone},\ \alpha \text{ continuous} \Rightarrow f \in \mathcal{R}(\alpha) \qquad (6.9)f monotone, α continuous⇒f∈R(α)(6.9) linearity of the integral(6.12a)\text{linearity of the integral} \qquad (6.12\mathrm{a})linearity of the integral(6.12a) monotonicity, additivity in the interval, and ∣ ⁣∫f dα∣≤M(α(b)−α(a))(6.12b,c,d)\text{monotonicity, additivity in the interval, and } \big|\!\int f\,d\alpha\big| \le M(\alpha(b)-\alpha(a)) \qquad (6.12\mathrm{b,c,d})monotonicity, additivity in the interval, and ​∫fdα​≤M(α(b)−α(a))(6.12b,c,d) α′∈R⇒(f∈R(α)  ⟺  fα′∈R), ∫f dα=∫fα′ dx(6.17)\alpha' \in \mathcal{R} \Rightarrow \big(f \in \mathcal{R}(\alpha) \iff f\alpha' \in \mathcal{R}\big),\ \int f\,d\alpha = \int f\alpha'\,dx \qquad (6.17)α′∈R⇒(f∈R(α)⟺fα′∈R), ∫fdα=∫fα′dx(6.17) change of variable through a strictly increasing φ(6.19)\text{change of variable through a strictly increasing } \varphi \qquad (6.19)change of variable through a strictly increasing φ(6.19) F(x)=∫axf dt is continuous, and F′(x0)=f(x0) where f is continuous(6.20)F(x) = \int_a^x f\,dt \text{ is continuous, and } F'(x_0) = f(x_0) \text{ where } f \text{ is continuous} \qquad (6.20)F(x)=∫ax​fdt is continuous, and F′(x0​)=f(x0​) where f is continuous(6.20) integration by parts(6.22)\text{integration by parts} \qquad (6.22)integration by parts(6.22)

Significance

The fundamental theorem is what makes the integral computable: it reduces integration to antidifferentiation and so links Chapters 5 and 6. Theorem 6.20 is its companion — it says the integral of a continuous function is an antiderivative — and together they show the two operations are mutually inverse to the extent that the hypotheses allow. Theorem 6.17 explains when a Stieltjes integral collapses to a Riemann integral with the density α′\alpha'α′, and it is the computational tool for integrators that are differentiable; the step-function case at the other extreme (Rudin's 6.15–6.16) is what turns sums into integrals.

Mathlib has no Riemann–Stieltjes integral: it has the Bochner integral, the interval integral, and a Lebesgue–Stieltjes measure, but the upper-and-lower-sum construction of Chapter 6 is absent. This mission therefore builds the object from Rudin's definitions and develops its basic theory; that development is reusable beyond this mission — Chapter 7's interchange theorem (7.16) and Chapter 8's Fourier coefficients are stated with respect to it.

Difficulty

Two obstacles are specific to formalizing this chapter. First, the upper and lower integrals are an infimum and a supremum over the set of all partitions, which is not a lattice-friendly index; every comparison between partitions goes through the common refinement, and Theorem 6.4 is the workhorse that makes such comparisons possible. Second, the fundamental theorem is proved by choosing a partition on which U−L<εU - L < \varepsilonU−L<ε and applying the mean value theorem on each subinterval, so the proof requires selecting an intermediate point per subinterval — a finite choice that is easy on paper and must be organized explicitly in Lean.

The integrator α\alphaα is only assumed monotone, so it may be discontinuous, and the theory must not assume otherwise: Theorem 6.9 needs continuity of α\alphaα precisely because it is not available in general.

Formalization scope

Conventions fixed by this mission:

  • A partition of [a, b] is Rudin.Partition a b: the number n of subintervals together with a monotone placement function x with x 0 = a and x n = b. Rudin allows xi−1=xix_{i-1} = x_ixi−1​=xi​, and so does this structure.
  • Rudin.upperSum, Rudin.lowerSum, Rudin.upperIntegral, Rudin.lowerIntegral, Rudin.RSIntegrable, Rudin.RSIntegral follow Definitions 6.1–6.2 literally, with sSup and sInf over the images f([xi−1,xi])f([x_{i-1},x_i])f([xi−1​,xi​]).
  • Since sSup/sInf on ℝ return 0 on unbounded sets, every statement carries Rudin's boundedness hypothesis for fff explicitly; likewise monotonicity of α\alphaα is assumed as MonotoneOn α (Set.Icc a b) rather than built into a type.
  • Rudin.RiemannIntegrable and Rudin.RiemannIntegral are the case α=id\alpha = \mathrm{id}α=id, in which the goal theorem and Theorems 6.20–6.22 are stated, matching Rudin.
  • Derivatives are HasDerivAt, so F' = f is stated pointwise on [a, b] with the value f x supplied, as in Rudin's hypothesis.

The goal is not vacuous, and not a restatement of a library lemma: the integral in it is the one defined in this mission, so a solution must connect the upper/lower sum construction to differentiation rather than quoting Mathlib's interval integral.

Selected references

  • Walter Rudin, Principles of Mathematical Analysis, 3rd edition, McGraw-Hill, 1976, Chapter 6 (pp. 120–142).
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Dynamic ProgrammingOperations ResearchOptimization+1·Captain: Shuze Chen

Dynamic Programming and Optimal Control VII: Infinite Horizon ProblemsTextbook

Motivation

Infinite-horizon dynamic programming is the mathematical core of Markov decision processes and reinforcement learning: Bellman equations, value iteration, policy iteration, and their guarantees. Chapter 7 of Bertsekas, Dynamic Programming and Optimal Control, Vol. I (3rd ed., 2005) develops the finite-state theory in its cleanest generality — stochastic shortest path (SSP) problems first (Prop. 7.2.1–7.2.2), with discounted problems (Prop. 7.3.1) and average-cost problems (Prop. 7.4.1–7.4.2) derived from the SSP analysis. These propositions are cited throughout the MDP/RL literature as the base case of the theory; none of them exists in Mathlib.

Setting

States 1,…,n1, \dots, n1,…,n plus an implicit cost-free absorbing termination state ttt; finite nonempty control sets U(i)U(i)U(i); costs g(i,u)g(i,u)g(i,u); sub-stochastic transitions pij(u)≥0p_{ij}(u) \ge 0pij​(u)≥0, ∑jpij(u)≤1\sum_j p_{ij}(u) \le 1∑j​pij​(u)≤1, the deficit being the termination probability (BertsekasSSPModel). Operators

(TμJ)(i)=g(i,μ(i))+∑jpij(μ(i))J(j),(TJ)(i)=min⁡u∈U(i)[g(i,u)+∑jpij(u)J(j)](T_\mu J)(i) = g(i,\mu(i)) + \sum_j p_{ij}(\mu(i)) J(j), \qquad (TJ)(i) = \min_{u \in U(i)}\Big[g(i,u) + \sum_j p_{ij}(u) J(j)\Big](Tμ​J)(i)=g(i,μ(i))+j∑​pij​(μ(i))J(j),(TJ)(i)=u∈U(i)min​[g(i,u)+j∑​pij​(u)J(j)]

(BertsekasSSPPolicyOp, BertsekasSSPBellmanOp), NNN-stage costs by backward recursion with policy shift (BertsekasSSPNCost), and the survival mass P{xm≠t}P\{x_m \ne t\}P{xm​=t} (BertsekasSSPSurvival). Assumption 7.2.1: for some m>0m > 0m>0, every admissible policy has survival mass <1< 1<1 from every state after mmm stages. The discounted setting reuses the same model with stochastic rows and 0<α<10 < \alpha < 10<α<1 (BertsekasDiscounted*); the average-cost setting adds a designated state sss with the avoidance probability of Assumption 7.4.1 (BertsekasSSPAvoidProb).

Target

Under Assumption 7.2.1, there is a vector J∗J^*J∗ with

TkJ0→J∗  ∀J0,J∗=TJ∗ uniquely,J∗(i)≤Jπ(i)=lim⁡NJπN(i)  ∀π admissible,T^k J_0 \to J^* \ \ \forall J_0, \qquad J^* = T J^* \text{ uniquely}, \qquad J^*(i) \le J_\pi(i) = \lim_N J^N_\pi(i) \ \ \forall \pi \text{ admissible},TkJ0​→J∗  ∀J0​,J∗=TJ∗ uniquely,J∗(i)≤Jπ​(i)=Nlim​JπN​(i)  ∀π admissible,

and a stationary policy attaining J∗J^*J∗ — BertsekasDP.ssp_main_theorem (goal, Prop. 7.2.1(a),(b)). Milestones: 7.2.1(c) policy evaluation, 7.2.1(d) optimality iff greediness, 7.2.2 policy iteration, 7.3.1 the full discounted counterpart, 7.4.1 the average-cost Bellman equation, 7.4.2 average-cost policy iteration.

Significance

These are the convergence guarantees behind value iteration and policy iteration — the two algorithms at the root of dynamic programming practice and of RL analyses (Q-learning's target operator is exactly TTT). The SSP form is the strongest of the three: the discounted theory is its special case (termination with probability 1−α1 - \alpha1−α per stage) and the average-cost theory reduces to it through cycles at the recurrent state. Formalized, the chapter yields a reusable finite-MDP theory: monotone operators, mmm-stage contractions, and the machinery for later Vol. II material. All results are proved in the book; the formalization is new.

Difficulty

TTT is not a one-stage contraction in the sup-norm under Assumption 7.2.1 — only an mmm-stage contraction, uniformly over the finitely many mmm-stage policy prefixes; extracting the uniform contraction factor ρ<1\rho < 1ρ<1 (via finiteness of the policy space) is the crux of the whole chapter. The limit of NNN-stage costs for nonstationary policies must be established, not assumed (tail-sum estimate ρ⌊N/m⌋\rho^{\lfloor N/m \rfloor}ρ⌊N/m⌋). For the average-cost results the associated-SSP construction (stop on reaching sss) must be built inside the proof. The liminf phrasing of average-cost optimality is deliberate: for arbitrary nonstationary policies the Cesàro limit need not exist.

Formalization scope

Finite states Fin n, finite control type, constraint sets as Finsets with attained minima; no termination state in the carrier — termination is the sub-stochastic deficit, exactly as the book treats it computationally. Policies are sequences of stage policies (Markov); costs of nonstationary policies via the shift recursion. Convergence is Tendsto in the product topology (equivalently sup-norm, nnn finite). Average cost uses real liminf and division with the N=0N = 0N=0 term junk-valued at 0 (irrelevant at infinity). The discounted theorem packages parts (a)–(e) in one statement mirroring Prop. 7.3.1.

Selected references

  • D. P. Bertsekas, Dynamic Programming and Optimal Control, Vol. I, 3rd ed., Athena Scientific, 2005. (§7.1–7.4.) http://www.athenasc.com/dpbook.html
  • D. P. Bertsekas, J. N. Tsitsiklis, An analysis of stochastic shortest path problems, Math. Oper. Res. 16 (1991), 580–595. https://doi.org/10.1287/moor.16.3.580
  • M. L. Puterman, Markov Decision Processes, Wiley, 1994. https://doi.org/10.1002/9780470316887
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