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Algorithmic Game TheoryOperations ResearchOptimization·Captain: mikedeng1

Supermodularity and Complementarity V: Existence of Equilibrium in Supermodular GamesTextbook

Motivation

Existence of equilibrium is the first question any model of strategic interaction must answer, and the classical answer — Nash's theorem via Kakutani's fixed point theorem — asks for a convex, compact strategy space and continuous payoffs. Many of the models economists actually use do not have that: a firm's technology set can be discrete or irregular, and a payoff need only be upper semicontinuous, not continuous. Topkis [1979] showed that when a game's structure is instead order-theoretic — each player's strategies form a lattice, and the players' incentives reinforce each other in a precise sense — an equilibrium exists without any convexity or continuity assumption at all, and the proof method delivers something Kakutani's theorem cannot: a greatest and a least equilibrium point, with the whole equilibrium set forming a complete lattice. Zhou [1994] later showed the completeness of the equilibrium lattice in full generality; this mission formalizes the resulting theorem (Topkis's Theorem 4.2.1) together with its parametric extension (Theorem 4.2.2, established independently by Milgrom and Roberts [1990a] and Sobel [1988]), which shows how the greatest and least equilibria move as a parameter of the game — its technology, its cost structure — changes. This machinery underlies monotone comparative statics for games throughout economics: oligopoly models with strategic complements, coordination games, and search and matching models with increasing returns.

Setting

A noncooperative game (N,S,{fi:i∈N})(N, S, \{f_i : i \in N\})(N,S,{fi​:i∈N}) consists of a finite player set NNN, a set S⊆RmS \subseteq \mathbb{R}^mS⊆Rm of feasible joint strategies x=(xi)i∈Nx = (x_i)_{i \in N}x=(xi​)i∈N​ (allowing the set of strategies feasible for one player to depend on the others' choices, so SSS need not be a product set), and a payoff function fif_ifi​ for each player iii. Write x−ix_{-i}x−i​ for the strategies of every player but iii, Si(x−i)S_i(x_{-i})Si​(x−i​) for the section of SSS at x−ix_{-i}x−i​ — player iii's feasible strategies given the others' choice — and Yi(x−i)=argmax⁡yi∈Si(x−i)fi(yi,x−i)Y_i(x_{-i}) = \operatorname{argmax}_{y_i \in S_i(x_{-i})} f_i(y_i, x_{-i})Yi​(x−i​)=argmaxyi​∈Si​(x−i​)​fi​(yi​,x−i​) for player iii's best-response set. The best joint response correspondence is Y(x)=∏i∈NYi(x−i)Y(x) = \prod_{i \in N} Y_i(x_{-i})Y(x)=∏i∈N​Yi​(x−i​). A feasible x′x'x′ is an equilibrium point if fi(yi,x−i′)≤fi(x′)f_i(y_i, x'_{-i}) \le f_i(x')fi​(yi​,x−i′​)≤fi​(x′) for every player iii and every feasible deviation yi∈Si(x−i′)y_i \in S_i(x'_{-i})yi​∈Si​(x−i′​) — no player can unilaterally improve.

A lattice is a partially ordered set in which every pair of elements has a join ∨\vee∨ and a meet ∧\wedge∧. A function ggg is supermodular on a subset if g(x)+g(y)≤g(x∨y)+g(x∧y)g(x) + g(y) \le g(x \vee y) + g(x \wedge y)g(x)+g(y)≤g(x∨y)+g(x∧y) for all x,yx, yx,y in it, and has increasing differences in two of its arguments (y,t)(y,t)(y,t) if y↦g(y,t′′)−g(y,t′)y \mapsto g(y, t'') - g(y, t')y↦g(y,t′′)−g(y,t′) is monotone whenever t′≺t′′t' \prec t''t′≺t′′. A game (N,S,{fi})(N, S, \{f_i\})(N,S,{fi​}) is a supermodular game if SSS is a sublattice, fi(yi,x−i)f_i(y_i, x_{-i})fi​(yi​,x−i​) is supermodular in yiy_iyi​ for every fixed x−ix_{-i}x−i​ and every iii, and fi(yi,x−i)f_i(y_i, x_{-i})fi​(yi​,x−i​) has increasing differences in (yi,x−i)(y_i, x_{-i})(yi​,x−i​) for every iii — jointly, the conditions under which each player's own strategy components are complements and complementary to the other players' strategies (Theorem 2.6.1 of chunk 01-lattices/02-monotonicity's book).

Formalization targets

Goal — Theorem 4.2.1

If (N,S,{fi})(N, S, \{f_i\})(N,S,{fi​}) is a supermodular game, SSS is nonempty and compact, and each fi(yi,x−i)f_i(y_i, x_{-i})fi​(yi​,x−i​) is upper semicontinuous in yiy_iyi​ on Si(x−i)S_i(x_{-i})Si​(x−i​) for every x−ix_{-i}x−i​ and every iii, then

{equilibrium points of (N,S,{fi})}\{\text{equilibrium points of } (N, S, \{f_i\})\}{equilibrium points of (N,S,{fi​})}

is nonempty, has a greatest and a least element, and, under the order it inherits from Rm\mathbb{R}^mRm, is itself a nonempty complete lattice.

Theorem 4.2.2 (the parametric extension)

Let TTT be a partially ordered set and, for each t∈Tt \in Tt∈T, (N,St,{fit})(N, S^t, \{f_i^t\})(N,St,{fit​}) a supermodular game with StS^tSt nonempty, compact, and increasing in ttt; suppose each fit(yi,x−i)f_i^t(y_i, x_{-i})fit​(yi​,x−i​) is upper semicontinuous in yiy_iyi​ and has increasing differences in (yi,t)(y_i, t)(yi​,t). Then for every ttt there exist a greatest and a least equilibrium point of game ttt, and both are increasing functions of ttt on TTT — the equilibrium set moves monotonically as the parameter increases.

Two supporting results are formalized as milestones because Theorem 4.2.1's own proof uses them directly: Lemma 4.2.1 (equilibrium points are exactly the fixed points of the best joint response correspondence) and Lemma 4.2.2, parts (b) and (f) (the best joint response set is a nonempty compact sublattice for every feasible xxx, and the correspondence is increasing in xxx).

Significance

The result itself. Theorem 4.2.1 is the lattice-theoretic alternative to Nash/Kakutani existence: it needs no convexity of SSS and no continuity of fif_ifi​ (upper semicontinuity suffices), and in exchange it delivers a greatest and a least equilibrium — with an explicit order-theoretic characterization via Theorem 2.5.1 of chunk 01-lattices — and the guarantee that the entire equilibrium set is a complete lattice, not merely nonempty. Theorem 4.2.2 gives this existence result teeth for applied comparative statics: it says that if a firm's cost structure, a market's demand parameter, or any other feature of the game increases (in the sense of the induced set order on StS^tSt and increasing differences in the payoffs), the extremal equilibria increase too — the qualitative content behind results such as "more competition leads to lower prices" in supermodular oligopoly models.

Formalizing it. The platform's existing Nash-equilibrium theorem (AGT.nash_existence, Theorem 1.8 of Algorithmic Game Theory) is a Brouwer/Kakutani argument for finite games with mixed strategies: it needs finiteness of every player's strategy set (so that mixed strategies form a compact convex simplex) and gives no lattice structure on the equilibrium set at all. Theorem 4.2.1 is a different technique entirely — it needs no finiteness, no mixing, and no convexity, and its conclusion (a complete lattice of equilibria) is exactly the content Brouwer/Kakutani cannot give. This mission is therefore not a restatement of Nash's theorem in different notation, but a second, independent existence technique with a strictly different structural payoff, formalized here for the first time on the platform. It builds directly on chunk 01-lattices's Theorem 2.5.1 (Zhou's fixed point theorem for increasing correspondences) and chunk 02-monotonicity's supermodularity/increasing differences definitions, both formalized earlier in this series.

Difficulty

The natural first idea for existence — "the best joint response correspondence has a fixed point by some general fixed-point theorem for correspondences" — needs the correspondence to be convex-valued and upper hemicontinuous for a Kakutani argument, neither of which supermodularity or upper semicontinuity alone supply: a best-response set under only upper semicontinuity can be a disconnected, non-convex set (e.g. the maximizers of a supermodular but non-quasiconcave function). The actual route goes through order instead of topology: Lemma 4.2.2 shows the best joint response set is a compact sublattice (hence subcomplete, by Theorem 2.3.1) and that the correspondence is increasing under the induced set order, which is exactly the hypothesis Theorem 2.5.1's non-constructive supremum/infimum construction needs — no convexity anywhere. A second subtlety, which the mission is careful not to elide: the equilibrium set of a supermodular game need be neither compact nor a sublattice of Rm\mathbb{R}^mRm when there are more than one player (Topkis's Examples 4.2.1 and 4.2.2 exhibit both failures); only the weaker claim — a complete lattice under the inherited order — is true in general, and that is what Theorem 2.5.1(b) supplies.

Formalization scope

A joint strategy is represented as a dependent function ∀ i, Fin (m i) → ℝ over a finite player type ι, with a player's own strategy accessed and overwritten via Function.update, so that x−ix_{-i}x−i​ is never reified as a separate object — every statement about fi(yi,x−i)f_i(y_i, x_{-i})fi​(yi​,x−i​) or membership in Si(x−i)S_i(x_{-i})Si​(x−i​) substitutes y for x's own i-th coordinate directly. IsSupermodularGame reuses chunk 02-monotonicity's SupermodularOn and IncreasingDifferencesOn verbatim, applied to each player's own payoff, rather than restating the supermodularity/increasing- differences conditions from scratch — a formalization that inlined a weaker, ad hoc notion here (e.g. supermodularity of the joint payoff vector rather than each player's own payoff in their own strategy) would trivialize the connection to chunk 02-monotonicity's theorems that the book's own proof relies on. Theorem 4.2.1's "nonempty complete lattice" conclusion is formalized, as in chunk 01-lattices, via IsLUB/IsGLB on the subtype of equilibrium points — never as membership of the ambient Rm\mathbb{R}^mRm supremum/infimum in the equilibrium set, which the book's own Examples 4.2.1–4.2.2 refute; a solution that instead proved the equilibrium set compact or a sublattice of Rm\mathbb{R}^mRm would be proving a strictly stronger and false claim. Only parts (b) and (f) of Lemma 4.2.2 are formalized, since those are the only two of its eight parts the proof of Theorem 4.2.1 uses; a complete development still needs chunk 01-lattices's Theorem 2.3.1 (subcomplete iff compact) and Theorem 2.5.1/2.5.2, and chunk 02-monotonicity's Theorem 2.8.1 and Corollary 2.7.1, none of which are restated here.

Selected references

  • Topkis, D. M., Equilibrium points in nonzero-sum n-person submodular games, SIAM Journal on Control and Optimization 17(6), 1979, pp. 773–787. https://doi.org/10.1137/0317054
  • Zhou, L., The set of Nash equilibria of a supermodular game is a complete lattice, Games and Economic Behavior 7(2), 1994, pp. 295–300. https://doi.org/10.1006/game.1994.1051
  • 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
  • Sobel, M. J., Isotone comparative statics for supermodular games, unpublished manuscript, 1988 (cited by Topkis [2011], Theorem 4.2.2).
  • Topkis, D. M., Supermodularity and Complementarity, Princeton University Press, 2011 (DOI 10.1515/9781400822539), Chapter 4, §4.1–4.2.
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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Introduction to Online Convex Optimization III: Online Gradient DescentTextbook

Motivation

Online convex optimization (OCO) models a repeated decision process: at each round a learner picks a point in a convex set, an adversary (or the world) reveals a convex cost function, the learner pays that cost at its own point, and the process repeats. No statistical assumption on the sequence of costs is made. This model, introduced by Zinkevich [Zinkevich, Online Convex Programming and Generalized Infinitesimal Gradient Ascent, ICML 2003], underlies most of modern online learning: portfolio selection, online routing, and — through its special case of stochastic optimization — the training of essentially every large machine-learning model in current use, since stochastic gradient descent (the subject of §3.4 of this chapter) is exactly an application of the regret bounds proved here.

The algorithm this chapter introduces, online gradient descent (OGD), is the field's default answer: take a gradient step against the most recently observed cost, project back onto the feasible set. It predates OCO itself as a heuristic, but Zinkevich's contribution — and this chapter's — is the regret analysis: a guarantee that holds against every sequence of costs, adversarially chosen, with an explicit, small constant. Precursors for less general settings appear in Kivinen and Warmuth [1997]; logarithmic-regret algorithms for OCO, the subject of §3.3 here, are due to Hazan, Agarwal and Kale [2007].

The online convex optimization protocol

Fix a convex set KKK in a real inner product space, playing the role of the decision (or "action") space, and a sequence of cost functions f1,f2,⋯:K→Rf_1, f_2, \dots : K \to \mathbb{R}f1​,f2​,⋯:K→R, each convex. At round ttt, the learner (not knowing ftf_tft​) plays a point xt∈Kx_t \in Kxt​∈K, then observes ftf_tft​ and pays ft(xt)f_t(x_t)ft​(xt​). Regret after TTT rounds compares the learner's cumulative cost to that of the single best fixed decision made with hindsight of the whole sequence:

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 learner with regret o(T)o(T)o(T) is, on average, eventually as good as the best fixed point in KKK, even though it never knew the cost sequence in advance.

Two chapter-wide parameters bound how hard an instance can be: DDD, the diameter of KKK (dist⁡(x,y)≤D\operatorname{dist}(x,y) \le Ddist(x,y)≤D for all x,y∈Kx, y \in Kx,y∈K), and GGG, a common bound on the gradient norm of every ftf_tft​ over KKK (∥∇ft(x)∥≤G\|\nabla f_t(x)\| \le G∥∇ft​(x)∥≤G for all x∈Kx \in Kx∈K), which implies but is strictly stronger than GGG-Lipschitzness on KKK. Online gradient descent (Algorithm 8) plays x1∈Kx_1 \in Kx1​∈K arbitrarily, then at every round sets yt+1=xt−ηt∇ft(xt)y_{t+1} = x_t - \eta_t \nabla f_t(x_t)yt+1​=xt​−ηt​∇ft​(xt​) and projects, xt+1=ΠK(yt+1)x_{t+1} = \Pi_K(y_{t+1})xt+1​=ΠK​(yt+1​), for a sequence of step sizes ηt\eta_tηt​ chosen in advance.

Formalization targets

Goal: Theorem 3.1 (online gradient descent regret)

RegretT≤32GDTfor all T≥1,\mathrm{Regret}_T \le \frac{3}{2} G D \sqrt{T} \quad \text{for all } T \ge 1,RegretT​≤23​GDT​for all T≥1,

using step sizes ηt=D/(Gt)\eta_t = D / (G\sqrt{t})ηt​=D/(Gt​). This is the chapter's — and arguably the book's — central result: the simplest algorithm for the fully general OCO protocol already attains O(T)O(\sqrt{T})O(T​) regret, with an explicit small constant, against convex Lipschitz costs with no further structure.

Milestone: Theorem 3.2 (matching lower bound)

Any algorithm for OCO incurs Ω(DGT)\Omega(DG\sqrt{T})Ω(DGT​) regret in the worst case: no algorithm, however clever, can improve asymptotically on Theorem 3.1's rate. This is the weaker, worst-case-existence half of the theorem (see Formalization scope).

Milestone: Theorem 3.3 (logarithmic regret under strong convexity)

If every ftf_tft​ is additionally α\alphaα-strongly convex, the same algorithm — with only the step sizes changed to ηt=1/(αt)\eta_t = 1/(\alpha t)ηt​=1/(αt) — achieves

RegretT≤G22α(1+log⁡T).\mathrm{Regret}_T \le \frac{G^2}{2\alpha}(1 + \log T).RegretT​≤2αG2​(1+logT).

Strong convexity is a strictly stronger hypothesis than convexity, so this target does not subsume the goal; it sits alongside it as the chapter's second, sharper regime.

Significance

Theorem 3.1 is the reference point against which every later algorithm and every later chapter's improvement (Online Newton Step, RFTL, adaptive-regret methods) is measured: any new algorithm for OCO is judged first by whether it matches this O(T)O(\sqrt{T})O(T​) rate, then by what extra structure lets it do better. Theorem 3.2 closes the question for the general convex-Lipschitz class: O(T)O(\sqrt{T})O(T​) is not an artifact of a loose analysis, it is information-theoretically necessary. Theorem 3.3 identifies the one extra hypothesis (strong convexity) that buys an exponential improvement in the horizon dependence, from T\sqrt{T}T​ to log⁡T\log TlogT, without any other change to the algorithm — the same phenomenon that in the book's Chapter 2 separated well-conditioned from general convex offline optimization, now transplanted to the online, adversarial setting.

None of these three statements has a machine-checked proof on the platform prior to this mission (see Formalization scope below for what was checked). Formalizing them establishes the regret protocol and the OGD algorithm as reusable definitions for the rest of this thirteen-chapter series, several chapters of which (Online Newton Step, RFTL, bandit convex optimization) build directly on Algorithm 8 or its regret guarantee.

Difficulty

The regret bound's proof (Theorem 3.1) is short but not naive: bounding ∇t⊤(xt−x⋆)\nabla_t^\top(x_t - x^\star)∇t⊤​(xt​−x⋆) by convexity alone gives no telescoping structure, so the argument instead bounds it using the projection step — the Pythagorean inequality ∥ΠK(z)−x⋆∥≤∥z−x⋆∥\|\Pi_K(z) - x^\star\| \le \|z - x^\star\|∥ΠK​(z)−x⋆∥≤∥z−x⋆∥ for x⋆∈Kx^\star \in Kx⋆∈K — applied to the specific point z=xt−ηt∇tz = x_t - \eta_t \nabla_tz=xt​−ηt​∇t​. This turns the per-round convexity bound into a telescoping sum in ∥xt−x⋆∥2\|x_t - x^\star\|^2∥xt​−x⋆∥2, and only the resulting sum, evaluated with the specific step-size schedule ηt=D/(Gt)\eta_t = D/(G\sqrt{t})ηt​=D/(Gt​), produces the T\sqrt{T}T​ rate; a constant or linearly growing step size does not. The same projection argument is reused for Theorem 3.3, where the strong-convexity inequality is engineered to make the ∥x⋆−xt∥2\|x^\star - x_t\|^2∥x⋆−xt​∥2 terms cancel exactly against the projection telescoping, leaving a harmonic sum. Theorem 3.2's difficulty is of a different kind: it is a lower bound over every algorithm, proved by exhibiting a randomized hard instance (the hypercube with 2n2^n2n sign-vector linear costs) on which no algorithm can do better than random guessing in expectation.

Formalization scope

KKK is formalized as a subset of an arbitrary real, complete inner product space (not fixed to Rn\mathbb{R}^nRn), since the chapter's argument uses only Hilbert-space structure. Rounds are 0-indexed (Finset.range T) rather than the book's 1-indexed rounds, so a step size stated here at round ttt is the book's step size at round t+1t+1t+1. D and G are carried as shared section hypotheses (the chapter-wide diameter and gradient-norm bounds), not re-derived or re-stated per theorem; G is formalized exactly as the book defines it (p. 20: a bound on ∥∇ft(x)∥\|\nabla f_t(x)\|∥∇ft​(x)∥ over KKK, via Mathlib's HasGradientAt), not as the weaker two-point Lipschitz condition it implies — an earlier draft used the weaker Lipschitz hypothesis and was corrected during moderation, since it made the drafted theorems strictly stronger than the book's own (true by an added argument the book does not give, but not faithful to the stated proof). The projection step is formalized relationally (IsMetricProjection, an arbitrary closest point) rather than as a canonical function, since a general convex set need not come with one built into Mathlib.

For Theorem 3.2, this mission formalizes the theorem's main sentence — the worst-case existence claim — quantifying over "any algorithm" as a non-anticipating map from the full cost sequence to the play sequence, with the hard cost sequence existentially quantified after the algorithm and the horizon: for every algorithm and every horizon there is a cost sequence forcing Ω(DGT)\Omega(DG\sqrt{T})Ω(DGT​) regret against it. (An earlier draft quantified the cost sequence first — one fixed sequence defeating every algorithm — which is false: a constant algorithm playing a minimizer of that one sequence has zero regret against it; this was corrected during moderation.) It does not formalize the theorem's parenthetical strengthening, that the same Ω(DGT)\Omega(DG\sqrt{T})Ω(DGT​) bound holds even when costs are drawn from a fixed stationary distribution; that claim is about expected regret of a deterministic algorithm against a random cost sequence, and would need a probability-space formalization of the OCO protocol that this mission's definitions do not build. A formalization limited to the deterministic worst case does not trivialize the theorem: it is exactly the inequality "O(T)O(\sqrt{T})O(T​) cannot be improved," stated without the randomization machinery of its proof.

Theorem 3.4 (the stochastic gradient descent corollary, via a noisy gradient oracle with bounded second moment) is not included: it needs an expectation over a random oracle applied at a random, round-dependent point, which is a substantially heavier probabilistic object than the deterministic protocol built here, and is left for a future mission or an extension of this one.

Selected references

  • Zinkevich, M. Online Convex Programming and Generalized Infinitesimal Gradient Ascent. ICML 2003. https://www.aaai.org/Papers/ICML/2003/ICML03-120.pdf
  • Kivinen, J. and Warmuth, M. K. Exponentiated Gradient Versus Gradient Descent for Linear Predictors. Information and Computation, 1997. https://doi.org/10.1006/inco.1996.2612
  • Hazan, E., Agarwal, A. and Kale, S. Logarithmic Regret Algorithms for Online Convex Optimization. Machine Learning 69, 2007. https://doi.org/10.1007/s10994-007-5016-8
  • Hazan, E. Introduction to Online Convex Optimization, 2nd ed. arXiv:1909.05207v3, Chapter 3. https://arxiv.org/abs/1909.05207
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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Introduction to Online Convex Optimization I: Learning from Expert Advice and the Hedge AlgorithmTextbook

Motivation

Consider a decision maker who must choose, at each of TTT rounds, between two actions on the advice of NNN "experts," none of which is known in advance to be reliable. This is the prediction-from-expert-advice problem, introduced by Littlestone and Warmuth [Littlestone & Warmuth, The Weighted Majority Algorithm, FOCS 1989/Inf. Comput. 1994] and generalized to real-valued losses by Freund and Schapire's Hedge algorithm [Freund & Schapire, A decision-theoretic generalization of on-line learning and an application to boosting, JCSS 1997]. It is one of the two founding problems of online learning (the other being universal portfolio selection, also introduced in this book's first chapter) and the historical origin of the multiplicative-weights update method, later recognized as a single algorithmic idea underlying results across game theory, optimization, and computational complexity [Arora, Hazan & Kale, The Multiplicative Weights Update Method: a Meta-Algorithm and Applications, Theory of Computing 2012]. This mission formalizes the chapter's three central guarantees: a matching deterministic lower bound, the Weighted Majority mistake bound, and Hedge's loss bound — the earliest instance, in the book's own development, of the "online convex optimization" phenomenon that its later chapters generalize to arbitrary convex losses.

Setting

At each round t=1,…,Tt = 1, \dots, Tt=1,…,T, a decision maker chooses one of two actions, AAA or BBB. After the choice, the true outcome for that round is revealed, and any action that disagrees with it is charged a mistake. NNN experts also each commit to a prediction every round, and the decision maker may consult their record.

The Weighted Majority (WM) algorithm maintains a weight Wt(i)W_t(i)Wt​(i) for each expert iii, initialized to W1(i)=1W_1(i) = 1W1​(i)=1. It predicts whichever action currently carries at least half the total weight, and after seeing the outcome, multiplies the weight of every expert who erred by (1−ε)(1-\varepsilon)(1−ε) for a fixed parameter ε∈(0,1/2)\varepsilon \in (0, 1/2)ε∈(0,1/2), leaving correct experts' weights unchanged. MTM_TMT​ denotes the algorithm's own mistake count through round TTT, and MT(i)M_T(i)MT​(i) expert iii's.

The Randomized Weighted Majority (RWM) algorithm uses the same weights, but instead of following the majority it samples an expert with probability proportional to its weight, pt(i)=Wt(i)/∑jWt(j)p_t(i) = W_t(i) / \sum_j W_t(j)pt​(i)=Wt​(i)/∑j​Wt​(j), and follows that expert's prediction; E[MT]\mathbb E[M_T]E[MT​] is its expected mistake count.

Hedge generalizes further, from binary mistakes to arbitrary non-negative real-valued losses ℓt(i)≥0\ell_t(i) \ge 0ℓt​(i)≥0 suffered by expert iii at round ttt. It samples expert iti_tit​ with probability xt(i)=Wt(i)/∑jWt(j)x_t(i) = W_t(i)/\sum_j W_t(j)xt​(i)=Wt​(i)/∑j​Wt​(j) from weights updated multiplicatively in the loss, Wt+1(i)=Wt(i) e−εℓt(i)W_{t+1}(i) = W_t(i) \, e^{-\varepsilon \ell_t(i)}Wt+1​(i)=Wt​(i)e−εℓt​(i). Writing losses and the mixed strategy as vectors, the algorithm's expected loss at round ttt is xt⊤ℓtx_t^\top \ell_txt⊤​ℓt​.

Formalization targets

Goal — Theorem 1.5 (Hedge's loss bound)

∑t=1Txt⊤ℓt  ≤  ∑t=1Tℓt(i⋆)  +  ε∑t=1Txt⊤ℓt2  +  log⁡Nε,∀ i⋆∈[N],\sum_{t=1}^T x_t^\top \ell_t \;\le\; \sum_{t=1}^T \ell_t(i^\star) \;+\; \varepsilon \sum_{t=1}^T x_t^\top \ell_t^2 \;+\; \frac{\log N}{\varepsilon}, \qquad \forall\, i^\star \in [N],t=1∑T​xt⊤​ℓt​≤t=1∑T​ℓt​(i⋆)+εt=1∑T​xt⊤​ℓt2​+εlogN​,∀i⋆∈[N],

where ℓt2(i):=ℓt(i)2\ell_t^2(i) := \ell_t(i)^2ℓt2​(i):=ℓt​(i)2. This is the chapter's most general result and the one the book reuses later on; it leaves ε\varepsilonε free (no asymptotic tuning), so it survives whatever later chapters do with ε\varepsilonε.

Milestones

  • Theorem 1.1 (deterministic lower bound). With L≤T/2L \le T/2L≤T/2 the best expert's mistake count, no deterministic algorithm can guarantee fewer than 2L2L2L mistakes on every instance.
  • Lemma 1.3 (Weighted Majority): MT≤2(1+ε)MT(i)+2log⁡N/εM_T \le 2(1+\varepsilon) M_T(i) + 2\log N/\varepsilonMT​≤2(1+ε)MT​(i)+2logN/ε for every expert iii.
  • Lemma 1.4 (Randomized Weighted Majority): E[MT]≤(1+ε)MT(i)+log⁡N/ε\mathbb E[M_T] \le (1+\varepsilon) M_T(i) + \log N /\varepsilonE[MT​]≤(1+ε)MT​(i)+logN/ε for every expert iii.

Significance

Theorem 1.1 shows the mistake-bound question has no trivial answer: even against only two maximally simple experts, any deterministic strategy is beaten by a factor of 222 by an adversary who knows its code. Lemmas 1.3 and 1.4 show this factor is essentially removable — first by relaxing "guarantee" to "guarantee in expectation" (RWM halves the deterministic penalty from 2(1+ε)2(1+\varepsilon)2(1+ε) to (1+ε)(1+\varepsilon)(1+ε)), then Theorem 1.5 removes the binary-mistake restriction altogether, replacing it with an explicit second-moment correction term ε∑txt⊤ℓt2\varepsilon \sum_t x_t^\top \ell_t^2ε∑t​xt⊤​ℓt2​ that vanishes as losses shrink. Together they trace the chapter's own narrative arc from "no algorithm beats 2L2L2L" to "an explicit, parameter-free family of algorithms gets within (1+ε)(1+\varepsilon)(1+ε) of the best expert for any ε\varepsilonε." All four results are proved by the book via the same device — a potential function Φt=∑iWt(i)\Phi_t = \sum_i W_t(i)Φt​=∑i​Wt​(i) — one of the first instances of the potential-function method that recurs throughout the rest of the book (e.g. Online Gradient Descent's regret proof) and throughout online learning generally. None of these four statements, in this exact form, has a formalized proof on Prove2Me or (to the extent searchable) elsewhere: the platform's closest existing result, BanditAlgorithm.ftrl_simplex_exp_weights_regret (see Formalization scope below), proves an asymptotically similar bound by an entirely different route and under a different loss model.

Difficulty

The natural first attempt at any of these bounds is to track MTM_TMT​ (or E[MT]\mathbb E[M_T]E[MT​], or ∑txt⊤ℓt\sum_t x_t^\top \ell_t∑t​xt⊤​ℓt​) directly and induct on TTT; this fails because the quantity itself has no useful recursive structure — knowing the algorithm's mistake count through round ttt says nothing about round t+1t+1t+1's outcome, which the adversary chooses to inflict maximum damage. The proofs instead introduce an auxiliary potential Φt=∑iWt(i)\Phi_t = \sum_i W_t(i)Φt​=∑i​Wt​(i) that is not the quantity being bounded, track it in two directions — an upper bound in terms of the algorithm's own performance (using 1+x≤ex1+x \le e^x1+x≤ex, or, for Hedge, e−x≤1−x+x2e^{-x} \le 1-x+x^2e−x≤1−x+x2 for x≥0x \ge 0x≥0) and a lower bound via the single best expert's weight, WT(i⋆)≤ΦTW_T(i^\star) \le \Phi_TWT​(i⋆)≤ΦT​ — and only convert back to the mistake/loss bound at the very end via one logarithm. Getting the direction of every inequality right (each of the four proofs chains four or five inequalities, each valid only in the stated parameter range) is the entire difficulty; there is no shortcut that avoids introducing Φt\Phi_tΦt​.

Formalization scope

Each algorithm is represented as a Prop-valued run predicate parametrizing over the weight sequence, the input (expert predictions/losses and true outcomes), and the algorithm's own output (predictions or mixed strategy), rather than as an executable program: IsHedgeRun fixes W 0 i = 1, the update W (t+1) i = W t i * exp(-ε * ℓ t i), and x t i = W t i / ∑ j, W t j; IsWeightedMajorityRun additionally fixes the majority-vote prediction rule explicitly (per the triage rubric, the algorithm is part of the audited statement here, not a black box the proof is free to instantiate). Randomization in RWM and Hedge is captured exactly as the book itself does — as a deterministic expectation, i.e. the inner product of the probability vector with the {0,1}-mistake or loss vector — rather than as a measure-theoretic random variable; the book's own Section 1.3.3 makes this identification explicit ("denote in vector notation the expected loss of the algorithm by E[ℓt(it)]=xt⊤ℓt\mathbb E[\ell_t(i_t)] = x_t^\top \ell_tE[ℓt​(it​)]=xt⊤​ℓt​"), so no probability space is introduced. Theorem 1.1's "deterministic algorithm" is a causal map from an outcome history to a prediction (prediction at round ttt depends only on outcomes before ttt), instantiated at the book's own two-expert construction (one expert always predicts AAA, the other always BBB) rather than a fully general NNN-expert adversary argument — a strictly weaker instance of the general claim, but the exact one the book's proof establishes, so no scope is lost relative to what is proved. ε\varepsilonε is kept as an explicit free parameter throughout, per the book's own presentation (no substitution of the corollary's optimized ε⋆=log⁡N/MT(i⋆)\varepsilon^\star = \sqrt{\log N / M_T(i^\star)}ε⋆=logN/MT​(i⋆)​ into the milestone statements).

A trivializing formalization to rule out: fixing N=1N = 1N=1 (a single expert) would make Lemmas 1.3–1.5 hold vacuously with MT=MT(i)M_T = M_T(i)MT​=MT​(i) regardless of the potential-function argument; every formal statement here quantifies over an unconstrained N:NN : \mathbb NN:N with N>0N > 0N>0, not a hard-coded small case.

The mission needs no Mathlib infrastructure beyond finite sums, Real.log, and Real.exp; the book's own OCO protocol and regret definition (§1.1) are not needed, since this chapter's proofs work directly with mistake/loss counts (per the chunk brief). BanditAlgorithm.ftrl_simplex_exp_weights_regret (Bandit Algorithms XII, Prop. 28.7, arXiv:2003.05963 §28) proves Rn≤2nlog⁡dR_n \le \sqrt{2n\log d}Rn​≤2nlogd​ for exponential weights on the simplex against [0,1][0,1][0,1]-valued losses, via an FTRL/mirror-descent instantiation — the same asymptotic phenomenon as Theorem 1.5, but a different proof technique, a different (bounded, not merely non-negative) loss assumption, and stated for simplex-comparator regret rather than the per-expert loss comparator here; it is listed as a reference/comparison point, not reused.

Selected references

  • N. Littlestone, M. Warmuth, The Weighted Majority Algorithm, FOCS 1989 / Information and Computation 108(2), 1994. https://doi.org/10.1006/inco.1994.1009
  • Y. Freund, R. Schapire, A Decision-Theoretic Generalization of On-Line Learning and an Application to Boosting, Journal of Computer and System Sciences 55(1), 1997. https://doi.org/10.1006/jcss.1997.1504
  • S. Arora, E. Hazan, S. Kale, The Multiplicative Weights Update Method: a Meta-Algorithm and Applications, Theory of Computing 8(1), 2012. https://doi.org/10.4086/toc.2012.v008a006
  • E. Hazan, Introduction to Online Convex Optimization, 2nd ed., arXiv:1909.05207v3, Chapter
    1. https://arxiv.org/abs/1909.05207
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Dynamic ProgrammingMachine LearningReinforcement Learning·Captain: mikedeng1

Foundations of Reinforcement Learning IV: Reinforcement Learning Basics and the UCB-VI AlgorithmTextbook

Motivation

Reinforcement learning (RL) formalizes sequential decision-making under uncertainty: an agent repeatedly observes a state, takes an action, receives a reward, and transitions to a new state, with the goal of maximizing cumulative reward over an unknown environment. It underlies applications from game-playing agents to robotics and adaptive medical treatment. What separates RL from the bandit and contextual bandit problems of earlier chapters in this series is state: the environment carries information forward across time steps, so a good action now can pay off many steps later, and a poor exploration strategy can take exponentially long to discover it. This mission formalizes the foundational results of finite-horizon episodic RL — the Markov Decision Process (MDP) model, the Bellman-optimality principle that makes dynamic programming possible, and the analytical toolkit (the performance-difference and Bellman-residual-decomposition lemmas) used throughout the field's regret analyses — culminating in a polynomial regret guarantee for UCB-VI, the canonical optimism-based algorithm for tabular RL introduced by Azar, Osband, and Munos (Minimax Regret Bounds for Reinforcement Learning, ICML 2017, arXiv:1703.05449).

Setting

A finite-horizon episodic Markov Decision Process M=(S,A,{PhM}h=1H,{RhM}h=1H,d1)M = (S, A, \{P^M_h\}_{h=1}^H, \{R^M_h\}_{h=1}^H, d_1)M=(S,A,{PhM​}h=1H​,{RhM​}h=1H​,d1​) consists of a finite state space SSS, a finite action space AAA, a horizon HHH, per-layer transition kernels PhM:S×A→Δ(S)P^M_h : S\times A \to \Delta(S)PhM​:S×A→Δ(S) and reward distributions RhM:S×A→Δ(R)R^M_h : S\times A \to \Delta(\mathbb R)RhM​:S×A→Δ(R), and an initial state distribution d1∈Δ(S)d_1 \in \Delta(S)d1​∈Δ(S). An episode unrolls for h=1,…,Hh=1,\dots,Hh=1,…,H: the learner selects an action ah∼πh(sh)a_h \sim \pi_h(s_h)ah​∼πh​(sh​) under a randomized non-stationary policy π=(π1,…,πH)∈Πrns\pi = (\pi_1,\dots,\pi_H) \in \Pi^{\mathrm{rns}}π=(π1​,…,πH​)∈Πrns (each πh:S→Δ(A)\pi_h : S \to \Delta(A)πh​:S→Δ(A)), receives reward rh∼RhM(sh,ah)r_h \sim R^M_h(s_h,a_h)rh​∼RhM​(sh​,ah​), and transitions to sh+1∼PhM(sh,ah)s_{h+1}\sim P^M_h(s_h,a_h)sh+1​∼PhM​(sh​,ah​). The value of π\piπ is fM(π):=EM,π[∑hrh]f^M(\pi) := \mathbb E^{M,\pi}[\sum_h r_h]fM(π):=EM,π[∑h​rh​], and the state-action and state value functions QhM,π(s,a)Q^{M,\pi}_h(s,a)QhM,π​(s,a), VhM,π(s)V^{M,\pi}_h(s)VhM,π​(s) are the analogous reward-to-go quantities from layer hhh onward. In the online RL problem, M⋆M^\starM⋆ is unknown, the learner interacts with it for TTT episodes, and the goal is to minimize the regret Reg=∑t=1T(fM⋆(πM⋆)−fM⋆(πt))\mathrm{Reg} = \sum_{t=1}^T \big(f^{M^\star} (\pi^{M^\star}) - f^{M^\star}(\pi^t)\big)Reg=∑t=1T​(fM⋆(πM⋆)−fM⋆(πt)) against the best policy πM⋆∈arg⁡max⁡π∈ΠrnsfM⋆(π)\pi^{M^\star} \in \arg\max_{\pi\in\Pi^{\mathrm{rns}}} f^{M^\star}(\pi)πM⋆∈argmaxπ∈Πrns​fM⋆(π).

Formalization targets

Goal — Theorem 1 (UCB-VI regret)

∃ C>0, ∀ δ∈(0,1],Pr⁡[Reg≤C⋅H⋅S⋅A T⋅log⁡(SAHT/δ)]≥1−δ,\exists\, C>0,\ \forall\, \delta\in(0,1],\quad \Pr\Big[\mathrm{Reg} \le C\cdot H\cdot S\cdot\sqrt{A\,T}\cdot\sqrt{\log(SAHT/\delta)}\Big] \ge 1-\delta,∃C>0, ∀δ∈(0,1],Pr[Reg≤C⋅H⋅S⋅AT​⋅log(SAHT/δ)​]≥1−δ,

for the UCB-VI algorithm run with the explicit bonus bh,δt(s,a)=2log⁡(2SAHT/δ)/nht(s,a)b^t_{h,\delta}(s,a) = 2\sqrt{\log(2SAHT/\delta)/n^t_h(s,a)}bh,δt​(s,a)=2log(2SAHT/δ)/nht​(s,a)​, under Assumption 6 (deterministic, known, [0,1][0,1][0,1]-bounded rewards). This is the weakest stable form of the guarantee: it fixes only the shape of the bound (polynomial in S,A,H,TS,A,H,TS,A,H,T, logarithmic in 1/δ1/\delta1/δ), leaving the exact leading constant — which the book itself does not pin down on this page — outside the formal claim.

Reaching it rests on three structural facts, each formalized as a milestone in attack order:

  • Proposition 25 (Bellman optimality): existence of a single deterministic policy simultaneously optimal at every state, computable by backward induction — the reason dynamic programming solves planning at all.
  • Lemma 13 (Performance difference) and Lemma 14 (Bellman residual decomposition): two "credit assignment" identities decomposing a value gap (between two policies, or one policy under two models) into a sum of per-layer, on-roll-in terms.
  • Lemma 15 (Error decomposition for optimistic policies): the fact that a greedy policy driven by any optimistic value estimate suffers sub-optimality controlled additively — not exponentially — by that estimate's own Bellman residuals, evaluated on-policy.

Significance

The result itself. Theorem 1 is the chapter's headline result: the first guarantee, in this development, that a learning algorithm — one that does not know the environment's transitions in advance — can achieve regret growing only polynomially in the size of the state space, the action space, and the horizon, and only as T\sqrt TT​ in the number of episodes. The chapter's own "combination lock" example (Figure 8) shows this is not automatic: naive exploration strategies (such as ε\varepsilonε-greedy, which suffices for ordinary bandits) incur regret exponential in the horizon on some MDPs with as few as H+2H+2H+2 states. UCB-VI's guarantee is the sample-complexity foundation on which essentially every subsequent result on tabular, linear, and general function-approximation RL in the book is built.

Formalizing it. No part of this chapter's mathematical content already has a faithful counterpart on the platform (see Difficulty, below, and Formalization scope). This mission contributes: (i) a from-scratch Lean formalization of the finite-horizon episodic MDP model and its value functions, faithful to the book's 000/111-indexing and reward-distribution conventions; (ii) faithful statements (drafted with sorry, not yet proved) of Proposition 25 and Lemmas 13–15; and (iii) a faithful statement of Theorem 1 itself, including a from-scratch construction of the finite TTT-episode adaptive interaction process needed to make sense of a high-probability regret guarantee. Proving these — Proposition 25 by backward induction, Lemmas 13–15 by telescoping, and Theorem 1 by combining Lemma 15's optimism bound with a concentration argument bounding the estimation-error and martingale terms of Eqs. (5.30)–(5.33) (omitted here; see Difficulty) — is open work for solvers.

Difficulty

The obvious approach to Theorem 1 — bound the regret episode-by-episode using only the fact that QtQ^tQt is close to QM⋆,⋆Q^{M^\star,\star}QM⋆,⋆ in some fixed sense — fails because QtQ^tQt's error is itself random (it depends on the transitions observed so far) and compounds across HHH layers of dynamic programming. Lemma 15 defuses the compounding: it shows the sub-optimality gap is additive in the per-layer Bellman residuals rather than multiplicative, provided QtQ^tQt is optimistic. Making QtQ^tQt optimistic with high probability, in turn, requires a concentration argument for the empirical transition estimates P^ht\widehat P^t_hPht​ (an application of Freedman's or the Azuma–Hoeffding inequality, not included among this mission's milestones) and a union bound over all (s,a,h,t)(s,a,h,t)(s,a,h,t) — accounting for the SAHTSAHTSAHT inside the bonus's logarithm. The final regret sum further requires bounding ∑t∑h1/nht(sht,aht)\sum_t \sum_h 1/\sqrt{n^t_h(s^t_h,a^t_h)}∑t​∑h​1/nht​(sht​,aht​)​ by a pigeonhole/potential-function argument over the visitation counts, which is where the SATS\sqrt{AT}SAT​ scaling — rather than a naive SATSA\sqrt{T}SAT​ — originates. None of this concentration or counting machinery is included in the current milestones; a solver attempting Theorem 1 needs it as prerequisite lemmas.

Formalization scope

MDP and value functions. States and actions are finite types (Fintype); layers are represented 000-indexed throughout the Lean development (the book's layer hhh is h - 1), with the terminal convention V _ _ H _ = 0 matching VH+1≡0V_{H+1}\equiv 0VH+1​≡0. Since every value/expectation formula in this chapter uses the reward distribution Rh(s,a)∈Δ(R)R_h(s,a)\in\Delta(\mathbb R)Rh​(s,a)∈Δ(R) only through its mean, EpisodicMDP.R records that mean directly — equivalent, by linearity of expectation, to carrying the full distribution, and changing no theorem's content. Transition kernels and policies are represented as plain real-valued functions (S → A → ℝ-style) rather than as Mathlib's PMF, with IsPolicy/the EpisodicMDP structure's own proof fields asserting the probability-distribution properties (nonnegativity, summing to 111) where the book requires membership in Πrns\Pi^{\mathrm{rns}}Πrns or a well-formed kernel; this keeps every expectation a finite Finset.sum, needing no measure theory. The optimal value functions Qstar/Vstar are defined as literal suprema over the entire (uncountable, since ∣A∣≥2|A|\ge2∣A∣≥2) policy type — not via a recursive shortcut — which is what rules out the trivializing formalization of Proposition 25: defining Vstar by the very recursion the proposition asserts would make the proposition a tautology, whereas here it is a genuine claim about a supremum over an enormous space of competitor policies.

UCB-VI and Theorem 1. Because SSS, AAA, HHH, and TTT are all finite, the TTT-episode adaptive interaction (in which round ttt's policy is a function of the realized history of the first t−1t-1t−1 episodes) is modeled as a finite probability space: the outcome type Fin T → Trajectory S A H is a Fintype, "probability" is a finite sum over it, and "with probability ≥1−δ\ge 1-\delta≥1−δ" is a plain inequality between two real numbers — no MeasureTheory is used anywhere in this mission. The universal constant CCC in Theorem 1 is existentially quantified (∃ C > 0, …) rather than given as a literal numeral, since its value is not pinned down by the book on this page and this mission does not carry out the (non-milestoned) concentration argument that would derive it; this is the convention adopted throughout for the book's own "≲\lesssim≲" notation. The empirical-transition estimator inside QhtQ^t_hQht​ is defined to be 000 when nht(s,a)=0n^t_h(s,a)=0nht​(s,a)=0 (no data yet collected for that pair) — a boundary case Eq. (5.25) does not address, resolved here by convention rather than proof.

Prior art. The platform's existing BanditAlgorithm.UCRL2Algorithm mission formalizes UCRL2 for the average-reward, infinite-horizon MDP setting with a diameter parameter, and its Bellman-optimality statement is the average-cost optimality equation — genuinely different from this chapter's finite-horizon episodic Bellman recursion, even though both go by the name "Bellman optimality." No reference item was reused; every definition and theorem in this mission is drafted from scratch. Both missions bound regret via optimism over a confidence set of models, but for different objectives (average reward vs. finite-horizon cumulative reward) and different MDP classes.

Reusable infrastructure and open contributions. EpisodicMDP, Policy, V/Q/Qstar/Vstar, and stateDist/stateExp are reusable by any future mission on finite-horizon episodic RL in this book's later chapters. Contributions welcome: proofs of the four milestone lemmas (by backward induction and telescoping, respectively); the concentration lemmas underlying Theorem 1's optimism guarantee (Eqs. (5.30)–(5.33) of the source, not milestoned here); and the final regret proof combining them.

Selected references

  • Foster, D. J. and Rakhlin, A., Foundations of Reinforcement Learning and Interactive Decision Making, 2023. arXiv:2312.16730v1
  • Azar, M. G., Osband, I., and Munos, R., Minimax Regret Bounds for Reinforcement Learning, ICML 2017. arXiv:1703.05449
  • Jaksch, T., Ortner, R., and Auer, P., Near-optimal Regret Bounds for Reinforcement Learning, JMLR 11 (2010).
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CombinatoricsNumber Theory·Captain: aarontcao

Shao's three units theorem: density 5/8 forces a three-fold additive basisResearch Paper

Let mmm be an odd squarefree positive integer and let AAA be a set of units modulo mmm with ∣A∣>58φ(m)|A| > \frac{5}{8}\varphi(m)∣A∣>85​φ(m). Then A+A+A=Z/mZA + A + A = \mathbb{Z}/m\mathbb{Z}A+A+A=Z/mZ: every residue class, unit or not, is a sum of three elements of AAA.

This is Corollary 1.5 of Xuancheng Shao, A density version of the Vinogradov three primes theorem, Duke Math. J. 163 (2014) 489-512, arXiv:1206.6139v2. It is the local input to Shao's density version of the three primes theorem, and it is a clean finite statement in its own right.

The constant is sharp and the inequality is strict

At m=15m = 15m=15 the set {2,8,11,13,14}\{2, 8, 11, 13, 14\}{2,8,11,13,14} has five elements, so 5φ(15)=8⋅55\varphi(15) = 8 \cdot 55φ(15)=8⋅5 exactly, and 111 is not a sum of three of its elements. The hypothesis therefore fails by nothing at all and the conclusion already fails. If <<< is weakened to ≤\le≤, the statement is false.

Where the proof comes from

The corollary cannot be proved by induction on sets. Passing from mmm to a prime factor ppp splits AAA into fibers of different densities, and a set is the wrong object to carry through that split. The induction has to run on functions f:Z/mZ→[0,1]f : \mathbb{Z}/m\mathbb{Z} \to [0,1]f:Z/mZ→[0,1], and the corollary is the case f=1Af = 1_Af=1A​ of a weighted statement, Proposition 1.4. That is the one step from which the rest follows.

The weighted statement then splits at the primes 3 and 5. For mmm coprime to 30 the induction runs on the prime factors, using Cauchy-Davenport-Chowla for three sets modulo a prime, and it produces the stronger bilinear conclusion f(a)f(b)+f(b)f(c)+f(c)f(a)>58(f(a)+f(b)+f(c))f(a)f(b) + f(b)f(c) + f(c)f(a) > \frac{5}{8}(f(a) + f(b) + f(c))f(a)f(b)+f(b)f(c)+f(c)f(a)>85​(f(a)+f(b)+f(c)). The modulus 15 is handled separately by a linear program over the eight units. Two averaging inequalities, one symmetric and one asymmetric, are what turn a density above 5/85/85/8 into a single good triple in both halves.

What the milestones are

The nine milestones follow Shao's own numbering: the two averaging inequalities of Section 2 (Lemmas 2.1 and 2.2), the finite check at m=15m = 15m=15 (Lemma 2.3), the three-set Cauchy-Davenport-Chowla bound, the divisor reduction that lets the proof assume 15∣m15 \mid m15∣m, the induction away from 3 and 5 (Proposition 3.1), the modulus-15 case (Proposition 3.2), the weighted local result (Proposition 1.4), and the counting bridge that the units modulo mmm number φ(m)\varphi(m)φ(m).

Notes on the formalization

Every item is stated in Mathlib primitives alone, so the mission needs no definition items: IsUnit, Nat.totient, Odd, Squarefree, Finset, and Antitone. The set of units modulo mmm is written Finset.univ.filter (fun x => IsUnit x) at each use rather than through a defined abbreviation, so a reader auditing a statement has to trust only Mathlib. That is also why open scoped Classical appears in the preamble.

The density hypothesis is written 5 * Nat.totient m < 8 * A.card, which is ∣A∣>58φ(m)|A| > \frac{5}{8}\varphi(m)∣A∣>85​φ(m) cleared of division so the whole statement stays in N\mathbb{N}N with no rounding.

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Linear OptimizationOptimizationTheoretical Computer Science·Captain: moutei

Primal-Dual Online Algorithms II: Finite LP Duality and Complementary SlacknessTextbook

Motivation

Almost every competitive online algorithm built by the primal-dual method rests on the same two facts about a pair of linear programs. The first is weak duality: any feasible solution of the dual is a lower bound on any feasible solution of the primal. The second is complementary slackness: if a feasible primal-dual pair satisfies a local, per-coordinate tightness condition, the pair is optimal — and if it satisfies that condition only up to factors α\alphaα and β\betaβ, the primal is within αβ\alpha\betaαβ of optimal.

The second fact in its approximate form is the engine of the whole method. An online algorithm cannot compute an optimum; what it can do is maintain a primal solution and a dual solution side by side so that each new request preserves an approximate tightness invariant. The approximate complementary slackness theorem then converts that local invariant into a global competitive ratio, with no reference to the optimum at all. Chapter 2 of Buchbinder's thesis states it as the background result on which the rest of the work is built.

Setting

Fix finite index types III (primal variables) and JJJ (primal constraints), a matrix A:I×J→RA : I \times J \to \mathbb{R}A:I×J→R, a cost vector c:I→Rc : I \to \mathbb{R}c:I→R and a right-hand side b:J→Rb : J \to \mathbb{R}b:J→R. The covering primal and packing dual are

(P)min⁡∑icixi  s.t.  ∑iAijxi ≥ bj  (∀j),x≥0,(P)\quad \min \sum_{i} c_i x_i \ \text{ s.t. } \ \sum_{i} A_{ij} x_i \ \ge\ b_j \ \ (\forall j), \qquad x \ge 0,(P)mini∑​ci​xi​  s.t.  i∑​Aij​xi​ ≥ bj​  (∀j),x≥0, (D)max⁡∑jbjyj  s.t.  ∑jAijyj ≤ ci  (∀i),y≥0.(D)\quad \max \sum_{j} b_j y_j \ \text{ s.t. } \ \sum_{j} A_{ij} y_j \ \le\ c_i \ \ (\forall i), \qquad y \ge 0.(D)maxj∑​bj​yj​  s.t.  j∑​Aij​yj​ ≤ ci​  (∀i),y≥0.

Note the index convention: AijA_{ij}Aij​ carries the primal-variable index first, so the primal constraint indexed by jjj sums over iii and the dual constraint indexed by iii sums over jjj.

Given α,β≥1\alpha, \beta \ge 1α,β≥1, the pair (x,y)(x,y)(x,y) satisfies approximate complementary slackness when

  • primal side: for every iii with xi>0x_i > 0xi​>0, ci/α ≤ ∑jAijyj ≤ ci\quad c_i/\alpha \ \le\ \sum_j A_{ij} y_j \ \le\ c_ici​/α ≤ ∑j​Aij​yj​ ≤ ci​;
  • dual side: for every jjj with yj>0y_j > 0yj​>0, bj ≤ ∑iAijxi ≤ β bj\quad b_j \ \le\ \sum_i A_{ij} x_i \ \le\ \beta\, b_jbj​ ≤ ∑i​Aij​xi​ ≤ βbj​.

Formalization targets

Goal — approximate complementary slackness

For a primal-feasible xxx, a dual-feasible yyy, and α,β≥1\alpha,\beta \ge 1α,β≥1 satisfying the two conditions above,

∑icixi ≤ αβ∑jbjyj.\sum_{i} c_i x_i \ \le\ \alpha\beta \sum_{j} b_j y_j .i∑​ci​xi​ ≤ αβj∑​bj​yj​.

Taking α=β=1\alpha = \beta = 1α=β=1 recovers exact complementary slackness and hence optimality of both members of the pair. The goal is stated with the source's hypotheses, including the two-sided bounds, rather than the weakest hypotheses that make the inequality go through; a separate item records the minimal-hypothesis strengthening.

Weak duality

∑jbjyj ≤ ∑icixifor every feasible x and y,\sum_j b_j y_j \ \le\ \sum_i c_i x_i \quad \text{for every feasible } x \text{ and } y,j∑​bj​yj​ ≤ i∑​ci​xi​for every feasible x and y,

with no nonnegativity assumption on AAA, bbb or ccc beyond feasibility itself.

Strong duality — imported, not reproved

Strong duality is not proved in this mission. The platform already carries LinearOptimization.lp_strong_duality, proved in this exact environment, for linear programs in Bertsimas–Tsitsiklis general form over Fin-indexed data. This mission's contribution is an adapter: from a primal optimum of (P)(P)(P), produce a dual optimum of (D)(D)(D) of equal value, for Fin-indexed instances. Reference items point at the imported theorem, its dual construction, and the dual-of-dual identity.

The biconditional — a dual optimum exists if and only if a primal optimum does — is deliberately left open. Weak duality does not derive the existence of a primal optimum from the existence of a dual one; the reverse implication needs strong duality applied to the dual program together with the dual-of-dual identity, and that reduction is not yet compiled. It is offered as a parallel target rather than claimed as established.

Significance

This mission is the foundation of the series. Every later mission — set cover, ski rental, and the online covering and packing problems that follow — states its approximation or competitiveness result as an instance of approximate complementary slackness. Formalizing it once, over arbitrary finite index types, is what makes the later missions short.

It also fills a real gap. Mathlib currently has no linear-programming duality: four separate attempts were closed unmerged. Approximate (α,β)(\alpha,\beta)(α,β) complementary slackness appears not to be formalized in any public library, so the goal theorem is, as far as we can determine, first of its kind.

Difficulty

The goal is a summation argument, not a deep theorem: the work is in handling the per-coordinate case split on xi>0x_i > 0xi​>0 versus xi=0x_i = 0xi​=0 and in interchanging a double sum. Three mechanical milestones isolate exactly those steps. The strong-duality adapter is the hard item, because it must reconcile two different presentations of the same program — index types, matrix orientation, and bundling all differ between our definitions and the imported theorem's.

Formalization scope

Definitions cover §2.1 of the source. Four distinct notions of "the program has a finite optimum" are separated on purpose — attained optimum, nonempty feasible set, bounded objective, and the conjunction — because the source's informal word "bounded" conflates them. The definitions are stated over arbitrary finite index types; the strong-duality items are stated only for Fin, because that is the only index type for which the imported dependency path exists.

Selected references

  • Niv Buchbinder, Designing Competitive Online Algorithms via a Primal-Dual Approach, PhD thesis, Tel Aviv University, 2008, §2.1, pp. 7–9. https://www.tau.ac.il/~nivb/download/phd-thsis.pdf
  • Dimitris Bertsimas and John N. Tsitsiklis, Introduction to Linear Optimization, Athena Scientific, 1997 — the general form used by the imported strong-duality theorem.
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Differential GeometryMathematical Physics·Captain: Lucas

Mirror Symmetry is T-Duality: the D-brane moduli space (Strominger-Yau-Zaslow)Research Paper

Motivation

Mirror symmetry began as an empirical observation in string theory: certain pairs (X,Y)(X,Y)(X,Y) of Calabi–Yau threefolds, with no evident geometric relation, give rise to the same physical theory, and invariants that are hard to compute on XXX (counts of holomorphic curves) turn into easy computations on YYY (variations of complex structure). The paper Mirror symmetry is T-duality by A. Strominger, S.-T. Yau and E. Zaslow, Nucl. Phys. B 479 (1996) 243–259, proposed the first structural explanation: XXX should carry a fibration by special Lagrangian 3-tori, the mirror YYY should be obtained by replacing each fibre with its dual torus, and the mirror map should be fibrewise T-duality. This proposal is now called the SYZ conjecture, and it organises most later geometric work on mirror symmetry.

The string-theoretic argument of Sections 1–2 of the paper is heuristic and is not formalizable as stated. Section 3 is different: it is a self-contained piece of differential geometry about the moduli space of a special Lagrangian submanifold together with a flat U(1)U(1)U(1) connection on it. This mission formalizes Section 3.

A short timeline of the mathematics the section rests on:

  • Harvey and Lawson, Calibrated geometries (Acta Math. 148, 1982), introduced special Lagrangian submanifolds as a calibrated geometry in a Calabi–Yau manifold.
  • R. McLean, Deformations of calibrated submanifolds (Duke preprint 96-01, 1996; Comm. Anal. Geom. 6 (1998) 705–747), proved that the space of deformations of a compact special Lagrangian submanifold LLL is a smooth manifold of dimension b1(L)b_1(L)b1​(L), whose tangent space at LLL is the space of harmonic 111-forms on LLL. The paper cites this as its reference [7].
  • SYZ (1996), Section 3, add the moduli of flat U(1)U(1)U(1) connections, exhibit an L2L^2L2 metric gabg_{ab}gab​ and a compatible almost complex structure J\mathcal JJ on the resulting 2b12b_12b1​-dimensional moduli space M\mathcal MM, derive the identity ∂agbc=∂bgac\partial_a g_{bc} = \partial_b g_{ac}∂a​gbc​=∂b​gac​ (their Eq. (3.4)), and conclude that M\mathcal MM is Kähler. They also exhibit a natural nnn-form Θ\ThetaΘ on M\mathcal MM, holomorphic when the brane is a torus.
  • N. Hitchin, The moduli space of special Lagrangian submanifolds (Ann. Scuola Norm. Sup. Pisa 25, 1997), gave a rigorous treatment in which the McLean metric is Hessian with respect to natural affine structures — the coordinate-free counterpart of Eq. (3.4).

Setting

Fix n≥1n \ge 1n≥1. The ambient Calabi–Yau manifold is modelled by Cn\mathbb C^nCn, carrying

  • the Riemannian metric g(u,v)=Re⁡⟨u,v⟩g(u,v) = \operatorname{Re}\langle u, v\rangleg(u,v)=Re⟨u,v⟩,
  • the complex structure Ju=iuJ u = i uJu=iu,
  • the Kähler form ω(u,v)=Im⁡⟨u,v⟩\omega(u,v) = \operatorname{Im}\langle u,v\rangleω(u,v)=Im⟨u,v⟩, which equals g(Ju,v)g(Ju, v)g(Ju,v),
  • the holomorphic volume form Ω=dz1∧⋯∧dzn\Omega = dz^1 \wedge \cdots \wedge dz^nΩ=dz1∧⋯∧dzn, evaluated on nnn vectors as the complex determinant of the matrix they span, and its imaginary part κ=Im⁡Ω\kappa = \operatorname{Im}\Omegaκ=ImΩ.

Here ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ is the standard Hermitian product of Cn\mathbb C^nCn, conjugate-linear in its first argument.

The brane LLL is an nnn-torus. It is presented by its universal cover: a map f:Rn→Cnf : \mathbb R^n \to \mathbb C^nf:Rn→Cn that is periodic up to translation,

f(x+ea)=f(x)+λa,a=1,…,n,f(x + e_a) = f(x) + \lambda_a, \qquad a = 1,\dots,n,f(x+ea​)=f(x)+λa​,a=1,…,n,

for a fixed family of periods λ1,…,λn∈Cn\lambda_1,\dots,\lambda_n \in \mathbb C^nλ1​,…,λn​∈Cn. Such an fff is exactly a map of the torus Rn/Zn\mathbb R^n/\mathbb Z^nRn/Zn into the complex torus Cn/Λ\mathbb C^n/\LambdaCn/Λ, and integration over LLL is integration over the unit cube [0,1]n[0,1]^n[0,1]n.

Write ∂if\partial_i f∂i​f for the partial derivatives of fff. The map fff is Lagrangian at xxx if ω(∂if,∂jf)=0\omega(\partial_i f, \partial_j f) = 0ω(∂i​f,∂j​f)=0 for all i,ji,ji,j, i.e. f∗ω=0f^{*}\omega = 0f∗ω=0; it is special Lagrangian if in addition κ(∂1f,…,∂nf)=0\kappa(\partial_1 f, \dots, \partial_n f) = 0κ(∂1​f,…,∂n​f)=0, i.e. f∗κ=0f^{*}\kappa = 0f∗κ=0. This is the supersymmetry condition of the paper (Section 2, conditions (ii) and (iii)). The induced metric is gij=g(∂if,∂jf)g_{ij} = g(\partial_i f, \partial_j f)gij​=g(∂i​f,∂j​f), the volume density is det⁡g\sqrt{\det g}detg​, and the second fundamental form of a Lagrangian immersion is the totally symmetric tensor

hijk=ω(∂i∂jf,∂kf).h_{ijk} = \omega(\partial_i \partial_j f, \partial_k f).hijk​=ω(∂i​∂j​f,∂k​f).

Given a family ftf_tft​ of such maps, its deformation 111-form is

θi=ω ⁣(∂f∂t,∂if),\theta_i = \omega\!\left(\tfrac{\partial f}{\partial t}, \partial_i f\right),θi​=ω(∂t∂f​,∂i​f),

the 111-form obtained by contracting the velocity into the Kähler form. For an mmm-parameter family F:Rm→(Rn→Cn)F : \mathbb R^m \to (\mathbb R^n \to \mathbb C^n)F:Rm→(Rn→Cn), t↦ftt \mapsto f_tt↦ft​, one gets mmm such forms θa\theta^aθa, a=1,…,ma = 1,\dots,ma=1,…,m, one per moduli direction.

The moduli data of Section 3 is a smooth mmm-parameter family FFF of special Lagrangian tori, all with the same periods, subject to two normalizations taken from the paper: each θa(t)\theta^a(t)θa(t) is harmonic for the induced metric g(t)g(t)g(t) (closed and co-closed), and the cohomology class of each θa\theta^aθa is constant along the family. The L2L^2L2 (McLean) metric on the moduli parameters is

gab(t)  =  ∫Lgij θia θjb  det⁡g  dnx.g_{ab}(t) \;=\; \int_{L} g^{ij}\,\theta^a_i\,\theta^b_j \; \sqrt{\det g}\; d^n x .gab​(t)=∫L​gijθia​θjb​detg​dnx.

The full moduli space M\mathcal MM of the paper also records the flat U(1)U(1)U(1) connection; its moduli form a torus of the same dimension, with coordinates sas^asa. On M\mathcal MM, modelled by Rm×Rm\mathbb R^m \times \mathbb R^mRm×Rm with coordinates (ta,sa)(t^a, s^a)(ta,sa), the paper puts the block-diagonal metric G=gab(dtadtb+dsadsb)G = g_{ab}(dt^a dt^b + ds^a ds^b)G=gab​(dtadtb+dsadsb) and the constant almost complex structure J(∂ta)=∂sa\mathcal J(\partial_{t^a}) = \partial_{s^a}J(∂ta​)=∂sa​, J(∂sa)=−∂ta\mathcal J(\partial_{s^a}) = -\partial_{t^a}J(∂sa​)=−∂ta​, with fundamental 222-form ωM(X,Y)=G(JX,Y)\omega_{\mathcal M}(X,Y) = G(\mathcal J X, Y)ωM​(X,Y)=G(JX,Y).

Target

The goal theorem is the conclusion of Section 3: for every such family, the fundamental 222-form of the moduli space is closed,

d ωM=0,d\,\omega_{\mathcal M} = 0,dωM​=0,

and since J\mathcal JJ is constant in these coordinates it is integrable, so (M,G,J)(\mathcal M, G, \mathcal J)(M,G,J) is Kähler.

The milestones are the numbered intermediate results of the paper, in the paper's own order:

Prop. 1:ddtft∗ω=dθ.\textbf{Prop. 1:}\quad \frac{d}{dt} f_t^{*}\omega = d\theta .Prop. 1:dtd​ft∗​ω=dθ. Prop. 2:ddtft∗κ=− d(∗θ),soddtft∗κ=0  ⟺  d†θ=0.\textbf{Prop. 2:}\quad \frac{d}{dt} f_t^{*}\kappa = -\,d(\ast\theta), \quad\text{so}\quad \frac{d}{dt} f_t^{*}\kappa = 0 \iff d^{\dagger}\theta = 0 .Prop. 2:dtd​ft∗​κ=−d(∗θ),sodtd​ft∗​κ=0⟺d†θ=0. Prop. 4:ddtgij=2 hijk wkfor the flow f˙=Jf∗w.\textbf{Prop. 4:}\quad \frac{d}{dt} g_{ij} = 2\,h_{ijk}\,w^{k}\quad\text{for the flow } \dot f = J f_{*} w .Prop. 4:dtd​gij​=2hijk​wkfor the flow f˙​=Jf∗​w. Eq. (A.2):∂aθb is exact.\textbf{Eq. (A.2):}\quad \partial_a \theta^b \text{ is exact.}Eq. (A.2):∂a​θb is exact. Eq. (3.4):∂agbc=∂bgac.\textbf{Eq. (3.4):}\quad \partial_a g_{bc} = \partial_b g_{ac}.Eq. (3.4):∂a​gbc​=∂b​gac​.

$$\textbf{Θ\ThetaΘ closed:}\quad \partial_c \int_L \theta^{a_1}\wedge\cdots\wedge\theta^{a_n} = 0 .

\textbf{Hessian} \Rightarrow \textbf{Kähler:}\quad \partial_a g_{bc} = \partial_b g_{ac} ;\Longrightarrow; d,\omega_{\mathcal M} = 0 .$$

Together, Propositions 1 and 2 are the statement that the tangent space to the moduli space consists of harmonic 111-forms — McLean's theorem in the form the paper uses it. Eq. (3.4) is the technical heart, and the last milestone is the step from it to the goal.

Significance

The result. Section 3 supplies the only rigorous mathematics in the paper. It says that the object the physics predicts to be a Calabi–Yau manifold — the moduli space of a supersymmetric brane — does carry the first piece of that structure, a Kähler metric, and that it carries a natural nnn-form which, for toroidal branes, is a holomorphic b1b_1b1​-form and hence a candidate for the Calabi–Yau form of the mirror. Eq. (3.4) says the McLean metric is locally the Hessian of a potential; this affine-Hessian structure of the SYZ base is the starting point of the later large-complex-structure-limit programme.

Formalizing it. The Section 3 results have rigorous published proofs (McLean for the tangent space, Hitchin for the Hessian property), but no machine-checked proof exists for any of them, and Mathlib currently has no special Lagrangian geometry, no Hodge theory, and no differential forms on manifolds. The mission therefore also produces reusable infrastructure: a workable coordinate model of calibrated submanifold geometry, the variation formulas for the induced metric and for the pullbacks of ω\omegaω and κ\kappaκ, and the Hessian-metric criterion for a Kähler structure, which is independent of the rest and reusable wherever affine-Kähler geometry appears.

Difficulty

The obvious approach to the goal — "the metric is Hessian, so take the potential and write down the Kähler form" — is not available: the potential is not part of the data, and producing it requires the symmetry ∂agbc=∂bgac\partial_a g_{bc} = \partial_b g_{ac}∂a​gbc​=∂b​gac​ first. That symmetry is the hard step, and it is hard for a specific reason: differentiating gbc(t)=∫Lgijθibθjcdet⁡gg_{bc}(t) = \int_L g^{ij}\theta^b_i\theta^c_j \sqrt{\det g}gbc​(t)=∫L​gijθib​θjc​detg​ in the direction tat^ata produces four terms — from θb\theta^bθb, from θc\theta^cθc, from the inverse metric gijg^{ij}gij, and from the volume density — and only their sum is symmetric in (a,b)(a,b)(a,b). Two of them are killed by an integration by parts that needs both harmonicity of θ\thetaθ and compactness of LLL (this is where the torus, and not a coordinate patch, is essential); one is killed because a special Lagrangian submanifold is minimal, so the mean curvature term in ∂adet⁡g\partial_a \sqrt{\det g}∂a​detg​ vanishes; what survives is −2∫Lhijkwaiwbjwck-2\int_L h_{ijk} w_a^i w_b^j w_c^k−2∫L​hijk​wai​wbj​wck​, which is symmetric because hhh is a symmetric 333-tensor. Every one of those four cancellations has to be carried out.

Proposition 2 carries a separate difficulty: it is an identity between the variation of a determinant and a divergence, and it is false without the hypothesis that ftf_tft​ is special Lagrangian at the point in question — for a merely Lagrangian fff there is a further term proportional to the Lagrangian angle.

Formalization scope

The formalization commits to the following, all of which are visible in the definition item and none of which are silent:

  • The ambient Calabi–Yau is flat. Sections 2 and 3 of the paper work with a general Calabi–Yau; here the ambient space is Cn\mathbb C^nCn (equivalently, after imposing periodicity, a flat complex torus Cn/Λ\mathbb C^n/\LambdaCn/Λ). This is the semi-flat/large-complex-structure regime in which the paper's own Section 2 check is carried out, and it is the price of Mathlib having no differential forms on manifolds. Propositions 1, 2 and 4 are stated for arbitrary smooth maps Rn→Cn\mathbb R^n \to \mathbb C^nRn→Cn and are genuinely local, so for them the restriction only removes the ambient curvature terms that the paper also drops by working in normal coordinates. The moduli-level statements do use the flat ambient.
  • The brane is a torus, presented by periodicity up to a fixed period lattice; L2L^2L2 pairings are integrals over [0,1]n[0,1]^n[0,1]n against Lebesgue measure. Compactness is used, and cannot be dropped.
  • Derivatives are Fréchet derivatives of maps on Rk\mathbb R^kRk contracted with a standard basis vector. Lean's fderiv returns 000 at a point of non-differentiability, so a statement about derivatives of a non-smooth map is a statement about zeros; every item therefore carries an explicit smoothness hypothesis, and the moduli-level items carry it inside the family structure.
  • Matrix inversion and square roots are total. The inverse of a singular matrix is 000 and the square root of a negative real is 000 in Lean. The items that use gijg^{ij}gij or det⁡g\sqrt{\det g}detg​ therefore carry an explicit immersion hypothesis det⁡g≠0\det g \ne 0detg=0.
  • Closedness of a 222-form is the Palais formula on constant vector fields, dω(X,Y,Z)=X ω(Y,Z)+Y ω(Z,X)+Z ω(X,Y)d\omega(X,Y,Z) = X\,\omega(Y,Z) + Y\,\omega(Z,X) + Z\,\omega(X,Y)dω(X,Y,Z)=Xω(Y,Z)+Yω(Z,X)+Zω(X,Y), which is the exterior derivative because the fields are constant. Closedness is asserted for all triples of tangent vectors at all points.
  • Non-triviality. The hypotheses are satisfiable: for λa\lambda_aλa​ the standard real basis vectors of Cn\mathbb C^nCn, the family F(t)(x)=x+itF(t)(x) = x + i tF(t)(x)=x+it of flat real subtori of Cn/Λ\mathbb C^n/\LambdaCn/Λ meets every condition of the family structure, with θia=−δia\theta^a_i = -\delta^a_iθia​=−δia​ and gab=δabg_{ab} = \delta_{ab}gab​=δab​. The goal is therefore not vacuous, and it is also not trivially true: J\mathcal{J}J is constant but gabg_{ab}gab​ is not, so dωM=0d\omega_{\mathcal M}=0dωM​=0 is a genuine condition on the family.

A complete development needs, beyond the definition item: the chain and product rules for fderiv on Rk\mathbb R^kRk, symmetry of second derivatives, differentiation under the integral sign on a compact box, integration by parts for periodic functions on [0,1]n[0,1]^n[0,1]n, and the derivative of det⁡\detdet and of matrix inversion. The last two, and the Hessian-implies-Kähler milestone, are reusable outside this mission. Contributions that replace the flat ambient by a general Kähler ambient chart, or that lift the model to Mathlib manifolds once differential forms exist there, are welcome and would supersede parts of this development.

Selected references

  • A. Strominger, S.-T. Yau, E. Zaslow, Mirror symmetry is T-duality, Nuclear Physics B 479 (1996) 243–259. doi:10.1016/0550-3213(96)00434-8, arXiv:hep-th/9606040
  • R. Harvey, H. B. Lawson, Calibrated geometries, Acta Mathematica 148 (1982) 47–157. doi:10.1007/BF02392726
  • R. C. McLean, Deformations of calibrated submanifolds, Communications in Analysis and Geometry 6 (1998) 705–747. doi:10.4310/CAG.1998.v6.n4.a4
  • N. J. Hitchin, The moduli space of special Lagrangian submanifolds, Annali della Scuola Normale Superiore di Pisa 25 (1997) 503–515. arXiv:dg-ga/9711002
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Differential GeometryGeometry & Topology·Captain: Lucas

Differential Geometry of Curves and Surfaces III: Global Properties of Plane CurvesTextbook

Motivation

The local theory of curves describes what happens near one point; the global theory asks what a curve must satisfy because it closes up. Two classical statements make the difference visible. The isoperimetric inequality says that among all simple closed plane curves of a given length, the circle encloses the largest area — a question already settled in intent by the Greeks, but given a satisfactory proof only in the nineteenth century, and the short proof reproduced by do Carmo is E. Schmidt's from 1939. The four-vertex theorem says that the curvature of a simple closed convex curve has at least four critical points, so no convex oval has the curvature profile of a curve that just rises and falls once.

The reference for this mission is Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition (Dover, 2016), §1-7, "Global Properties of Plane Curves" (pp. 31–46): the area formula, equation (1) on p. 33; the isoperimetric inequality, Theorem 1 on p. 34; the theorem of turning tangents on p. 37; the lemma, equation (5) on p. 38; and the four-vertex theorem, Theorem 2 on p. 37.

This is the third mission of a series formalizing do Carmo's book, and shares the namespace DoCarmoDG with the earlier ones.

Setting

A closed plane curve of length lll is a regular map α:[0,l]→R2\alpha : [0,l] \to \mathbb{R}^2α:[0,l]→R2 whose derivatives of all orders agree at the two endpoints; equivalently, and as used here, a smooth lll-periodic map α:R→R2\alpha : \mathbb{R} \to \mathbb{R}^2α:R→R2. It is parametrized by arc length when ∣α′(s)∣=1|\alpha'(s)| = 1∣α′(s)∣=1 for all sss, in which case lll is its length. It is simple when it has no self-intersection: α(t1)≠α(t2)\alpha(t_1) \neq \alpha(t_2)α(t1​)=α(t2​) for distinct t1,t2∈[0,l)t_1, t_2 \in [0,l)t1​,t2​∈[0,l).

Write JJJ for rotation by +π/2+\pi/2+π/2, J(a,b)=(−b,a)J(a,b) = (-b,a)J(a,b)=(−b,a). For a curve parametrized by arc length the signed curvature is

k(s)=⟨α′′(s), Jα′(s)⟩,k(s) = \bigl\langle \alpha''(s),\, J\alpha'(s) \bigr\rangle,k(s)=⟨α′′(s),Jα′(s)⟩,

which is do Carmo's convention of §1-5, Remark 1: the normal is chosen so that {α′,Jα′}\{\alpha', J\alpha'\}{α′,Jα′} has the orientation of the natural basis, and then α′′=k Jα′\alpha'' = k\,J\alpha'α′′=kJα′. A vertex is a parameter ttt with k′(t)=0k'(t) = 0k′(t)=0. The curve is convex when, for every parameter ttt, the whole trace lies in one of the two closed half-planes bounded by the tangent line at ttt.

An angle function for α\alphaα is a smooth θ\thetaθ with α′(s)=(cos⁡θ(s),sin⁡θ(s))\alpha'(s) = (\cos\theta(s), \sin\theta(s))α′(s)=(cosθ(s),sinθ(s)); the rotation index is (θ(l)−θ(0))/2π(\theta(l) - \theta(0))/2\pi(θ(l)−θ(0))/2π. The area bounded by a positively oriented simple closed curve is given by do Carmo's equation (1),

A=12∫0l(x y′−y x′) dt,α=(x,y).A = \frac{1}{2}\int_0^l \bigl(x\,y' - y\,x'\bigr)\,dt, \qquad \alpha = (x,y).A=21​∫0l​(xy′−yx′)dt,α=(x,y).

Formalization targets

Goal — Four-vertex theorem (do Carmo, Theorem 2, p. 37)

α simple closed convex⟹#{ t∈[0,l):k′(t)=0 }≥4.\alpha \ \text{simple closed convex} \quad \Longrightarrow \quad \#\{\,t \in [0,l) : k'(t) = 0\,\} \ge 4 .α simple closed convex⟹#{t∈[0,l):k′(t)=0}≥4.

Supporting statements

The three equivalent forms of the area formula (1); the existence of a smooth angle function; the identity k=θ′k = \theta'k=θ′; the theorem of turning tangents (the rotation index of a simple closed curve is ±1\pm 1±1); the isoperimetric inequality l2≥4πAl^2 \ge 4\pi Al2≥4πA with equality exactly for circles; and do Carmo's lemma (5), ∫0l(Ax+By+C) k′(s) ds=0\int_0^l (Ax + By + C)\,k'(s)\,ds = 0∫0l​(Ax+By+C)k′(s)ds=0, which drives the proof of the goal.

Significance

The isoperimetric inequality is the ancestor of a large family of geometric inequalities, and its sharp case characterizes the circle — the first instance of the pattern "extremal configuration is the round one" that recurs throughout geometry. The four-vertex theorem is a genuinely global statement with no local counterpart: locally, the curvature of a convex arc may be strictly monotone, and it is only the requirement that the curve close up convexly that forces four critical points. Its converse, for strictly positive curvature, was proved by H. Gluck in 1971; do Carmo notes that the theorem also holds for simple closed curves that are not convex, by a harder argument.

Mathlib contains integration, the winding number of a loop in the complex plane and the Jordan curve theorem, but it does not contain the signed curvature of a plane curve, the theorem of turning tangents in this form, the isoperimetric inequality for curves with its equality case, or the four-vertex theorem. What this mission adds is that vocabulary and machine-checked proofs of the four classical statements.

Difficulty

Each target fails for a different reason under the naive approach.

For the area formula, the identification of 12∮(x dy−y dx)\frac12\oint(x\,dy - y\,dx)21​∮(xdy−ydx) with the area of the interior is exactly the Jordan-curve input that do Carmo declares he is assuming; the formalization avoids that dependency by defining the bounded area through the integral, so a solver has to prove only the integration-by-parts identities among the three forms of (1).

For the theorem of turning tangents, the difficulty is that a smooth lift θ\thetaθ of the tangent indicatrix must be produced and then shown to increase by exactly ±2π\pm 2\pi±2π over one period — a degree-theoretic statement about a loop in the circle, where simplicity of the curve is what excludes the values 0,±2,±3,…0, \pm 2, \pm 3, \dots0,±2,±3,….

For the isoperimetric inequality, Schmidt's proof compares the curve with a circle tangent to two parallel supporting lines and uses the arithmetic–geometric mean inequality; the equality discussion, which is where the characterization of the circle lives, is the delicate part.

For the four-vertex theorem, the obvious argument — "curvature on a compact interval attains a maximum and a minimum, so there are two vertices" — gives only two, and the whole content is the step from two to four. The lemma (5) supplies the contradiction: if k′k'k′ changed sign only at the maximum and the minimum, a suitable line Ax+By+C=0Ax + By + C = 0Ax+By+C=0 through those two points would make the integrand of (5) of one sign and not identically zero.

Formalization scope

Curves are smooth maps ℝ → EuclideanSpace ℝ (Fin 2), closedness being lll-periodicity with l>0l > 0l>0, which is do Carmo's condition that the curve and all its derivatives agree at the endpoints. Unit speed is imposed globally, so the parameter is arc length and lll is the length. Simplicity is injectivity on the half-open period [0,l)[0,l)[0,l). Convexity is stated per parameter: for each ttt the trace lies in one closed half-plane of the tangent line at ttt, the choice of side being allowed to depend on ttt, as in the book's phrasing.

The area is defined by do Carmo's integral (1) rather than as the measure of the interior of the curve, so no Jordan curve theorem is presupposed; consequently the isoperimetric statement is formulated with the absolute value ∣A∣|A|∣A∣, which makes it independent of the curve's orientation and equal to the enclosed area for a positively oriented simple curve. The equality case asserts that the trace lies on a circle of positive radius.

"At least four vertices" is formalized as the existence of four pairwise distinct parameters in [0,l)[0,l)[0,l) at which k′k'k′ vanishes, which rules out the degenerate reading in which one vertex is counted several times.

Selected references

  • Manfredo P. do Carmo, Differential Geometry of Curves and Surfaces, 2nd edition, Dover, 2016, §1-7 (area formula, eq. (1), p. 33; isoperimetric inequality, Theorem 1, p. 34; theorem of turning tangents, p. 37; lemma, eq. (5), p. 38; four-vertex theorem, Theorem 2, p. 37).
  • E. Schmidt, Über das isoperimetrische Problem im Raum von n Dimensionen, Mathematische Zeitschrift 44 (1939), 689–788.
  • H. Gluck, The converse to the four-vertex theorem, L'Enseignement Mathématique 17 (1971), 295–309.
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AlgebraNumber Theory·Captain: Lucas

Grothendieck-Teichmüller: the graded Lie algebra grt_1 and the Deligne-Drinfeld-Ihara conjectureOpen Problem

Motivation

The Grothendieck-Teichmüller group organises a family of symmetries that act on braided monoidal categories, on quantised universal enveloping algebras, on the little-discs operad, and on the ring of periods of the projective line minus three points. Three versions exist: a profinite one GT^\widehat{GT}GT, introduced by Grothendieck and Drinfeld and containing the absolute Galois group Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q); a pro-ℓ\ellℓ one; and a pro-unipotent one GTGTGT, together with its graded companion GRTGRTGRT. This mission is about the graded, pro-unipotent side, which is the version that governs the homological-algebra and deformation-quantisation applications, and which is closest to a concrete, computable object: a Lie algebra of Lie polynomials in two variables, cut out by three explicit equations.

Its Lie algebra grt1\mathfrak{grt}_1grt1​ carries a distinguished family of elements σ3,σ5,σ7,…\sigma_3, \sigma_5, \sigma_7, \dotsσ3​,σ5​,σ7​,…, one in each odd degree at least 333, produced from the Knizhnik-Zamolodchikov associator. Deligne, Drinfeld and Ihara conjectured that grt1\mathfrak{grt}_1grt1​ is the free Lie algebra on such a family. A timeline of what is actually known:

  • 1990 - V. Drinfeld, On quasitriangular quasi-Hopf algebras and a group closely connected with Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q), introduces GTGTGT, GRTGRTGRT, associators, and the defining equations of grt1\mathfrak{grt}_1grt1​; the Knizhnik-Zamolodchikov associator shows the set of associators is non-empty, hence σ3,σ5,…\sigma_3, \sigma_5, \dotsσ3​,σ5​,… exist and are non-zero.
  • 2012 - F. Brown, Mixed Tate motives over Z\mathbb ZZ (Annals of Mathematics 175, 949-976, doi:10.4007/annals.2012.175.2.10), proves that the ζf(r1,…,rn)\zeta^{\mathfrak f}(r_1,\dots,r_n)ζf(r1​,…,rn​) with rj∈{2,3}r_j \in \{2,3\}rj​∈{2,3} form a basis of the algebra of motivic multiple zeta values. One half of the conjecture follows: the Lie subalgebra of grt1\mathfrak{grt}_1grt1​ generated by the σ2p+1\sigma_{2p+1}σ2p+1​ is free on them.
  • The converse half - that these elements generate all of grt1\mathfrak{grt}_1grt1​ - is open.

Setting

Let F(x,y)\mathbb{F}(x,y)F(x,y) be the free Lie algebra over Q\mathbb QQ on two generators xxx and yyy, graded by total word length. For a Lie algebra AAA over Q\mathbb QQ and a,b∈Aa, b \in Aa,b∈A, write ψ(a,b)\psi(a,b)ψ(a,b) for the image of ψ∈F(x,y)\psi \in \mathbb{F}(x,y)ψ∈F(x,y) under the unique Lie algebra morphism sending x↦ax \mapsto ax↦a and y↦by \mapsto by↦b.

For n≥1n \ge 1n≥1, the Drinfeld-Kohno Lie algebra tn\mathfrak t_ntn​ is generated over Q\mathbb QQ by symbols tijt_{ij}tij​, 1≤i,j≤n1 \le i, j \le n1≤i,j≤n, subject to

tii=0,tij=tji,[tij,tkl]=0,[tij,tik+tjk]=0,t_{ii} = 0, \qquad t_{ij} = t_{ji}, \qquad [t_{ij}, t_{kl}] = 0, \qquad [t_{ij}, t_{ik} + t_{jk}] = 0,tii​=0,tij​=tji​,[tij​,tkl​]=0,[tij​,tik​+tjk​]=0,

the third relation for i,j,k,li,j,k,li,j,k,l pairwise distinct and the fourth for i,j,ki,j,ki,j,k pairwise distinct. It is the Lie algebra of infinitesimal braid relations: the associated graded of the pure braid Lie algebra, and the coefficient algebra of the Knizhnik-Zamolodchikov connection.

The graded Grothendieck-Teichmüller Lie algebra grt1\mathfrak{grt}_1grt1​ is the set of ψ∈F(x,y)\psi \in \mathbb{F}(x,y)ψ∈F(x,y) satisfying three equations:

ψ(x,y)=−ψ(y,x),\psi(x,y) = -\psi(y,x),ψ(x,y)=−ψ(y,x), ψ(x,y)+ψ(y,z)+ψ(z,x)=0where x+y+z=0,\psi(x,y) + \psi(y,z) + \psi(z,x) = 0 \quad \text{where } x + y + z = 0,ψ(x,y)+ψ(y,z)+ψ(z,x)=0where x+y+z=0, ψ(t12,t23)−ψ(t12,t23+t24)+ψ(t12+t13,t24+t34)−ψ(t13+t23,t34)+ψ(t23,t34)=0  in t4.\psi(t_{12},t_{23}) - \psi(t_{12},t_{23}+t_{24}) + \psi(t_{12}+t_{13},t_{24}+t_{34}) - \psi(t_{13}+t_{23},t_{34}) + \psi(t_{23},t_{34}) = 0 \ \text{ in } \mathfrak t_4 .ψ(t12​,t23​)−ψ(t12​,t23​+t24​)+ψ(t12​+t13​,t24​+t34​)−ψ(t13​+t23​,t34​)+ψ(t23​,t34​)=0  in t4​.

All three are linear in ψ\psiψ and degree preserving, so grt1\mathfrak{grt}_1grt1​ is a graded Q\mathbb QQ-subspace.

grt1\mathfrak{grt}_1grt1​ is not closed under the bracket of F(x,y)\mathbb{F}(x,y)F(x,y); it is closed under the Ihara (Poisson) bracket

{f,g}=[f,g]+Dfg−Dgf,\{f,g\} = [f,g] + D_f g - D_g f,{f,g}=[f,g]+Df​g−Dg​f,

where DfD_fDf​ is the derivation of F(x,y)\mathbb{F}(x,y)F(x,y) determined by Dfx=0D_f x = 0Df​x=0 and Dfy=[y,f]D_f y = [y,f]Df​y=[y,f]. Writing Der\mathrm{Der}Der for the Lie algebra of derivations of F(x,y)\mathbb{F}(x,y)F(x,y) under the commutator, the assignment f↦Dff \mapsto D_ff↦Df​ satisfies [Df,Dg]=D{f,g}[D_f, D_g] = D_{\{f,g\}}[Df​,Dg​]=D{f,g}​, and it is injective on grt1\mathfrak{grt}_1grt1​; this is the form in which the Lie structure of grt1\mathfrak{grt}_1grt1​ is expressed in the formal statements below.

Finally, for n1≥2n_1 \ge 2n1​≥2 and n2,…,nk≥1n_2,\dots,n_k \ge 1n2​,…,nk​≥1 the multiple zeta value is

ζ(n1,…,nk)=∑j1>j2>⋯>jk≥11j1n1j2n2⋯jknk.\zeta(n_1,\dots,n_k) = \sum_{j_1 > j_2 > \cdots > j_k \ge 1} \frac{1}{j_1^{n_1} j_2^{n_2} \cdots j_k^{n_k}} .ζ(n1​,…,nk​)=j1​>j2​>⋯>jk​≥1∑​j1n1​​j2n2​​⋯jknk​​1​.

These numbers are the coefficients of the Knizhnik-Zamolodchikov associator, which is why they enter a mission about grt1\mathfrak{grt}_1grt1​; they satisfy the stuffle and shuffle relations, whose common refinement (the double shuffle relations) is the arithmetic side of the same story.

Formalization targets

Goal - Deligne-Drinfeld-Ihara

∃ σ0,σ1,σ2,⋯∈grt1,deg⁡σp=2p+3,such that grt1 is the free Lie algebra on (σp)p≥0 for { ,}.\exists\, \sigma_0, \sigma_1, \sigma_2, \dots \in \mathfrak{grt}_1, \quad \deg \sigma_p = 2p+3, \quad \text{such that } \mathfrak{grt}_1 \text{ is the free Lie algebra} \text{ on } (\sigma_p)_{p \ge 0} \text{ for } \{\,,\}.∃σ0​,σ1​,σ2​,⋯∈grt1​,degσp​=2p+3,such that grt1​ is the free Lie algebra on (σp​)p≥0​ for {,}.

Concretely: the Lie algebra morphism from the free Lie algebra on countably many generators to Der\mathrm{Der}Der sending the ppp-th generator to DσpD_{\sigma_p}Dσp​​ is injective, and its image is exactly D(grt1)D(\mathfrak{grt}_1)D(grt1​). The statement fixes the degrees of the generators but not the generators themselves, which is the weakest form that still carries the content of the conjecture.

Milestone level - Brown's half

The same family exists with the morphism merely injective: the σ2p+1\sigma_{2p+1}σ2p+1​ generate a free Lie subalgebra. This is a theorem (Brown 2012); the open part of the goal is surjectivity.

Supporting levels

The Ihara bracket is a Lie bracket; grt1\mathfrak{grt}_1grt1​ is closed under it; the degree-333 element [x+y,[x,y]][x+y,[x,y]][x+y,[x,y]] lies in grt1\mathfrak{grt}_1grt1​; every odd degree ≥3\ge 3≥3 contains a non-zero element of grt1\mathfrak{grt}_1grt1​; multiple zeta values satisfy the stuffle and shuffle relations; and ζ(2,1)=ζ(3)\zeta(2,1) = \zeta(3)ζ(2,1)=ζ(3).

Significance

A positive answer would determine grt1\mathfrak{grt}_1grt1​ completely and, through the GTGTGT-GRTGRTGRT-associator torsor, describe the pro-unipotent Grothendieck-Teichmüller group by generators without relations. Downstream it would pin down the homotopy automorphisms of the rationalised little-discs operad and the Lie algebra of the motivic Galois group of mixed Tate motives over Z\mathbb ZZ up to the same freeness statement. Without it, even the dimension of grt1\mathfrak{grt}_1grt1​ in a given degree is only known to be bounded above by the Broadhurst-Kreimer style count, with equality unproved.

Formalizing this mission produces a machine-checked definition of tn\mathfrak t_ntn​, grt1\mathfrak{grt}_1grt1​ and the Ihara bracket - objects that have no Mathlib counterpart at present - and machine-checked proofs of the Lie-theoretic facts around them. Brown's theorem itself is proved in the literature but not formalized; the goal statement is genuinely open, and no part of this mission is closed by an existing Lean development known to the proposal.

Difficulty

The obvious approach to the goal - exhibit the generators and count dimensions degree by degree - fails in both directions. Upwards, no closed formula for σ2p+1\sigma_{2p+1}σ2p+1​ is known: they are extracted from the Knizhnik-Zamolodchikov associator, whose coefficients are regularised iterated integrals, and only their leading coefficients are controlled. Downwards, freeness of the subalgebra they generate is not an algebraic manipulation of the three defining equations: Brown derives it from the motivic theory of multiple zeta values, where the missing input is a basis theorem for a period algebra, not an identity in F(x,y)\mathbb{F}(x,y)F(x,y). Even the milestone "grt1\mathfrak{grt}_1grt1​ is closed under the Ihara bracket" is not a formality: the pentagon equation lives in t4\mathfrak t_4t4​ and must be transported through substitutions into a quotient Lie algebra.

Formalization scope

The formalization commits to the following conventions, all visible in the definition files.

  1. The base field is Q\mathbb QQ. The source works over a field KKK of characteristic zero; every statement here is over Q\mathbb QQ.
  2. grt1\mathfrak{grt}_1grt1​ is modelled inside the free Lie algebra FreeLieAlgebra ℚ (Fin 2), i.e. by Lie polynomials, not the completed Lie algebra F^(x,y)\widehat{\mathbb{F}}(x,y)F(x,y) of the source. The three defining equations are homogeneous, so the graded object determines the completed one; solvers should be aware that no topology or completion appears anywhere.
  3. tn\mathfrak t_ntn​ is the quotient of the free Lie algebra on ordered pairs of indices in Fin n by the Lie ideal generated by the four relation families above, so dkGen i j is ti+1,j+1t_{i+1,j+1}ti+1,j+1​ under the shift Fin 4 = {0,1,2,3} versus indices 1,2,3,41,2,3,41,2,3,4.
  4. Homogeneity is expressed by the rescaling characterisation: ψ\psiψ has degree nnn if ψ(cx,cy)=cnψ(x,y)\psi(cx,cy) = c^n \psi(x,y)ψ(cx,cy)=cnψ(x,y) for all c∈Qc \in \mathbb Qc∈Q. Over an infinite field this is equivalent to homogeneity for the word-length grading.
  5. The Ihara derivation uses Dfx=0D_f x = 0Df​x=0. The source writes Dfx=xD_f x = xDf​x=x in Remark 4.4 and in Section 7.3, but that convention contradicts Lemma 7.2 of the same notes and the computation {x,y}=[x,y]+[y,x]=0\{x,y\} = [x,y] + [y,x] = 0{x,y}=[x,y]+[y,x]=0 in Remark 7.2; Dfx=0D_f x = 0Df​x=0 is the convention under which both hold, and is the standard one.
  6. The Lie structure on grt1\mathfrak{grt}_1grt1​ is carried by the injection f↦Dff \mapsto D_ff↦Df​ into LieDerivation ℚ (FreeLieAlgebra ℚ (Fin 2)) (FreeLieAlgebra ℚ (Fin 2)), so that freeness can be stated as injectivity of a morphism out of a free Lie algebra without first installing a new Lie algebra structure. Note f↦Dff \mapsto D_ff↦Df​ is injective on grt1\mathfrak{grt}_1grt1​ but not on all of F(x,y)\mathbb{F}(x,y)F(x,y), where Dy=0D_y = 0Dy​=0; a supporting item records the injectivity actually used.
  7. Multiple zeta values are real numbers defined by an iterated tsum; for non-admissible words the series diverges and the definition returns Mathlib's junk value. Every statement about them therefore carries an admissibility hypothesis: all letters ≥1\ge 1≥1 and first letter ≥2\ge 2≥2. The stuffle and shuffle products are multisets of words, so no free module on words is needed.
  8. Nothing here is vacuous by construction: the defining equations of grt1\mathfrak{grt}_1grt1​ are linear conditions on a non-zero graded space, t4≠0\mathfrak t_4 \ne 0t4​=0, and the milestone [x+y,[x,y]]∈grt1[x+y,[x,y]] \in \mathfrak{grt}_1[x+y,[x,y]]∈grt1​, [x+y,[x,y]]≠0[x+y,[x,y]] \ne 0[x+y,[x,y]]=0 exhibits a non-zero element.

Contributions welcome: the Lie-theoretic milestones (Lemma 7.2, Corollary 7.1, closure of grt1\mathfrak{grt}_1grt1​, the degree-333 element) are self-contained and need no motivic input; the multiple zeta milestones need summability infrastructure for iterated series; Brown's theorem and the goal need a substantial development that does not yet exist in Lean.

Selected references

  • V. G. Drinfeld, On quasitriangular quasi-Hopf algebras and a group closely connected with Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q), Leningrad Math. J. 2 (1991), 829-860.
  • F. Brown, Mixed Tate motives over Z\mathbb ZZ, Annals of Mathematics 175 (2012), 949-976, doi:10.4007/annals.2012.175.2.10.
  • T. Willwacher, The Grothendieck-Teichmüller Group, ETH Zürich lecture notes, 27 February 2014 (the source text for this mission).
  • T. Willwacher, M. Kontsevich's graph complex and the Grothendieck-Teichmüller Lie algebra, Invent. Math. 200 (2015), 671-760, doi:10.1007/s00222-014-0528-x.
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AlgebraNumber TheoryRepresentation Theory·Captain: Lucas

Ngo's Fundamental Lemma II: Isogenies of Root Data and Paired GroupsResearch Paper

Motivation

Waldspurger's non-standard fundamental lemma is an identity between stable orbital integrals on the Lie algebras of two reductive groups that are not isomorphic, and not even isogenous as algebraic groups, but whose root data become identified after tensoring with Q\mathbb{Q}Q. The basic example is the pair (Sp2n,SO2n+1)(\mathrm{Sp}_{2n}, \mathrm{SO}_{2n+1})(Sp2n​,SO2n+1​), whose root systems CnC_nCn​ and BnB_nBn​ are exchanged by Langlands duality; the identity is what allows the twisted fundamental lemma to be deduced from the ordinary one. Waldspurger formulated the conjecture in L'endoscopie tordue n'est pas si tordue (2008); it is Theorem 1.12.7 of Bao Chau Ngo, Le lemme fondamental pour les algebres de Lie, Publ. Math. IHES 111 (2010), 1-169 (DOI), proved there in equal characteristic by the same Hitchin-fibration argument that gives the ordinary fundamental lemma.

Before any of that geometry can start, the two sides have to be compared: one needs a single Cartan subalgebra, a single Weyl group and a single space of characteristic polynomials serving both groups at once. Producing that comparison is a self-contained piece of linear algebra over the root data, carried out in Ngo's §1.12, and it is what this mission asks for.

Setting

Let G1G_1G1​ and G2G_2G2​ be split reductive groups over a field, pinned, with maximal tori T1T_1T1​ and T2T_2T2​. Each is determined by its root datum (X∗(Ti),X∗(Ti),Φi,Φi∨,Δi)(X^*(T_i), X_*(T_i), \Phi_i, \Phi_i^\vee, \Delta_i)(X∗(Ti​),X∗​(Ti​),Φi​,Φi∨​,Δi​), where Φi\Phi_iΦi​ is the set of roots, Φi∨\Phi_i^\veeΦi∨​ the set of coroots and Δi\Delta_iΔi​ the set of simple roots singled out by the pinning.

An isogeny of root data between G1G_1G1​ and G2G_2G2​ (Ngo, Definition 1.12.1) is a pair of isomorphisms of Q\mathbb{Q}Q-vector spaces

ψ∗:X∗(T2)⊗Q⟶X∗(T1)⊗Q,ψ∗:X∗(T1)⊗Q⟶X∗(T2)⊗Q\psi^* : X^*(T_2)\otimes\mathbb{Q} \longrightarrow X^*(T_1)\otimes\mathbb{Q}, \qquad \psi_* : X_*(T_1)\otimes\mathbb{Q} \longrightarrow X_*(T_2)\otimes\mathbb{Q}ψ∗:X∗(T2​)⊗Q⟶X∗(T1​)⊗Q,ψ∗​:X∗​(T1​)⊗Q⟶X∗​(T2​)⊗Q

which are transposes of one another, such that ψ∗\psi^*ψ∗ carries the set of lines Qα2\mathbb{Q}\alpha_2Qα2​ (α2∈Φ2\alpha_2 \in \Phi_2α2​∈Φ2​) bijectively onto the set of lines Qα1\mathbb{Q}\alpha_1Qα1​ (α1∈Φ1\alpha_1\in\Phi_1α1​∈Φ1​), matching lines of simple roots with lines of simple roots, and such that ψ∗\psi_*ψ∗​ has the same property for the lines spanned by coroots. Two semisimple groups with the same adjoint group are isogenous in this sense; so are a group and its Langlands dual, the interesting cases being Bn↔CnB_n \leftrightarrow C_nBn​↔Cn​, F4F_4F4​ and G2G_2G2​, where a short root α\alphaα is sent to αˇ\check\alphaαˇ and a long root to nαˇn\check\alphanαˇ with n=∣αlong∣2/∣αshort∣2n = |\alpha_{\mathrm{long}}|^2/|\alpha_{\mathrm{short}}|^2n=∣αlong​∣2/∣αshort​∣2. Groups obtained by twisting a pair of isogenous pinned groups by a common torsor are called paired.

A prime ppp is good with respect to ψ∗\psi^*ψ∗ when it divides neither of the indices

∣X∗(T1)/(X∗(T1)∩X∗(T2))∣and∣X∗(T2)/(X∗(T1)∩X∗(T2))∣,\bigl|X_*(T_1)/(X_*(T_1)\cap X_*(T_2))\bigr| \quad\text{and}\quad \bigl|X_*(T_2)/(X_*(T_1)\cap X_*(T_2))\bigr|,​X∗​(T1​)/(X∗​(T1​)∩X∗​(T2​))​and​X∗​(T2​)/(X∗​(T1​)∩X∗​(T2​))​,

the two lattices being compared inside the single Q\mathbb{Q}Q-vector space identified by ψ∗\psi_*ψ∗​.

Formalization targets

Goal (1.12.4 and 1.12.6): the Weyl groups are identified compatibly

ψ∗ w ψ∗−1∈W2for all w∈W1,and conversely,\psi_* \, w \, \psi_*^{-1} \in W_2 \quad \text{for all } w \in W_1, \qquad\text{and conversely,}ψ∗​wψ∗−1​∈W2​for all w∈W1​,and conversely,

i.e. conjugation by ψ∗\psi_*ψ∗​ carries the Weyl group W1W_1W1​ acting on X∗(T1)⊗QX_*(T_1)\otimes\mathbb{Q}X∗​(T1​)⊗Q onto the Weyl group W2W_2W2​ acting on X∗(T2)⊗QX_*(T_2)\otimes\mathbb{Q}X∗​(T2​)⊗Q. Ngo's reason is that the reflection attached to a root depends only on the line through that root, so the bijection of root lines transports reflections to reflections. This equivariance is what makes the induced isomorphism t1→t2\mathfrak{t}_1 \to \mathfrak{t}_2t1​→t2​ descend to an isomorphism ν:cG1→cG2\nu : \mathfrak{c}_{G_1} \to \mathfrak{c}_{G_2}ν:cG1​​→cG2​​ of the spaces of characteristic polynomials, which is Lemme 1.12.6 and which is what allows two points a1a_1a1​ and a2a_2a2​ with ν(a1)=a2\nu(a_1) = a_2ν(a1​)=a2​ to be compared at all.

Milestones

Two steps lead there: the reflection computation that makes a matched pair of root lines give a matched pair of reflections, and the integral statement behind Ngo's good-characteristic hypothesis — that when the two indices above are invertible in the base ring, the two lattices become identified after base change.

Significance

Theorem 1.12.7, the non-standard fundamental lemma, asserts that for two paired groups over Ov=k[[ϖ]]O_v = k[[\varpi]]Ov​=k[[ϖ]] with residue characteristic exceeding twice the Coxeter numbers, and for points a1a_1a1​ and a2a_2a2​ corresponding under ν\nuν, the stable orbital integrals of the characteristic functions of g1(Ov)\mathfrak{g}_1(O_v)g1​(Ov​) and g2(Ov)\mathfrak{g}_2(O_v)g2​(Ov​) agree. Waldspurger showed that this identity, together with the ordinary fundamental lemma, implies the twisted fundamental lemma. None of the objects in that statement — reductive group schemes over a discrete valuation ring, orbital integrals, Haar measures on the centralizer tori — exists in Mathlib today. The comparison of §1.12 does not need any of them: it is a statement about lattices, root systems and Weyl groups, and it is a strict prerequisite, since without the isomorphism ν\nuν the two sides of Theorem 1.12.7 cannot even be matched up.

Beyond this paper, the notion of an isogeny of root data and the good-characteristic base change of a pair of lattices are reusable: they are the standard bookkeeping behind Langlands duality for split groups, and neither is currently available.

Difficulty

The reflection step looks like a one-line computation and is one — but only once the two proportionality constants are known to agree. If ψ∗(α2)=c α1\psi^*(\alpha_2) = c\,\alpha_1ψ∗(α2​)=cα1​ and ψ∗(α1∨)=c′ α2∨\psi_*(\alpha_1^\vee) = c'\,\alpha_2^\veeψ∗​(α1∨​)=c′α2∨​, the conjugate of sα1s_{\alpha_1}sα1​​ is sα2s_{\alpha_2}sα2​​ exactly when c=c′c = c'c=c′, and that is forced by transposition together with ⟨α,α∨⟩=2\langle\alpha,\alpha^\vee\rangle = 2⟨α,α∨⟩=2. The genuine difficulty in the goal is different: the definition only says that ψ∗\psi^*ψ∗ and ψ∗\psi_*ψ∗​ permute lines, so one has to show that the bijection induced on root lines and the bijection induced on coroot lines are the same bijection. A solver who assumes this without proof has assumed the substance of 1.12.4.

The lattice milestone has its own trap: the quotient Λ1/(Λ1∩Λ2)\Lambda_1/(\Lambda_1\cap\Lambda_2)Λ1​/(Λ1​∩Λ2​) must be shown to have vanishing Tor\mathrm{Tor}Tor after base change, not merely to vanish, or the inclusion becomes only surjective.

Formalization scope

Root data are modelled by Mathlib's RootPairing ι ℚ M N, with MMM the character space, NNN the cocharacter space, and rational coefficients throughout, so that "tensoring with Q\mathbb{Q}Q" is built into the ambient objects rather than performed explicitly. A choice of simple roots is recorded as a subset of the index type rather than as a RootPairing.Base; nothing in the statements depends on that subset beyond its role in the definition of an isogeny. The Weyl group is the subgroup of linear automorphisms of the cocharacter space generated by the coreflections, which is the form in which it acts on the Cartan.

The goal is stated as a two-sided intertwining property rather than as an equality of subgroups: every element of W1W_1W1​ is intertwined by ψ∗\psi_*ψ∗​ with some element of W2W_2W2​ and conversely. This avoids introducing a conjugation homomorphism, and it is the form in which the statement is used. Both root pairings in the goal are required to be finite, reduced root systems, matching Ngo's hypothesis that G1G_1G1​ and G2G_2G2​ are reductive groups.

The good-characteristic condition is formalized exactly as Ngo writes it, by the invertibility in the base ring of the two indices, each expressed as the cardinality of an explicit quotient group; the conclusion is the bijectivity of the map induced on the tensor product by the inclusion of the intersection. If a quotient were infinite its cardinality is reported as 000, and invertibility of 000 then forces the base ring to be trivial, so no false statement hides in that corner.

No statement here is vacuous: any pair consisting of a root system and itself, with ψ∗\psi^*ψ∗ and ψ∗\psi_*ψ∗​ the identity, satisfies every hypothesis, and the pair (Bn,Cn)(B_n, C_n)(Bn​,Cn​) gives the intended non-trivial instances.

Selected references

  • Bao Chau Ngo, Le lemme fondamental pour les algebres de Lie, Publ. Math. IHES 111 (2010), 1-169. https://doi.org/10.1007/s10240-010-0026-7
  • J.-L. Waldspurger, L'endoscopie tordue n'est pas si tordue, Mem. Amer. Math. Soc. 908 (2008). https://doi.org/10.1090/memo/0908
  • J.-L. Waldspurger, Le lemme fondamental implique le transfert, Compositio Math. 105 (1997), 153-236. https://doi.org/10.1023/A:1000103112268
  • T. A. Springer, Reductive groups, in Automorphic Forms, Representations and L-functions, Proc. Sympos. Pure Math. 33 (1979), 3-27. https://doi.org/10.1090/pspum/033.1
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Functional AnalysisProbability·Captain: Lucas

An Introduction to Stochastic PDEs I: The Cameron–Martin TheoremTextbook

Motivation

A stochastic partial differential equation is driven by noise that lives on an infinite-dimensional function space, and the first object one has to control is the law of that noise: a Gaussian measure on a separable Banach space. Martin Hairer's lecture notes An Introduction to Stochastic PDEs (arXiv:0907.4178) devote their first technical chapter (Section 4) to exactly this, because every later construction — stochastic convolutions, invariant measures for semilinear equations, the ergodic theory of the stochastic Navier–Stokes equations — is phrased against it.

The single structural fact that chapter produces is the Cameron–Martin theorem (Theorem 4.44, p. 31). It answers the question: in which directions may one translate an infinite-dimensional Gaussian measure without destroying its null sets? In finite dimensions the answer is "all of them", because Lebesgue measure is translation invariant. In infinite dimensions the admissible directions form a proper, and typically much smaller, Hilbert subspace Hμ⊂BH_\mu \subset BHμ​⊂B — the Cameron–Martin space — and the translated measure is either equivalent to μ\muμ or mutually singular with it, with nothing in between. This dichotomy is the reason Girsanov-type changes of measure, Schilder-type large deviation rate functions, support theorems and Malliavin calculus all take the form they do.

Setting

Throughout, BBB is a separable Banach space, B∗B^{*}B∗ its topological dual, and μ\muμ a Borel probability measure on BBB.

μ\muμ is Gaussian (Definition 4.4, p. 19) if for every continuous linear functional ℓ∈B∗\ell \in B^{*}ℓ∈B∗ the push-forward ℓ∗μ\ell_{*}\muℓ∗​μ is a Gaussian measure on R\mathbb RR in the sense of Definition 4.1, i.e. has characteristic function exp⁡(−σ2ℓ2+iℓm)\exp(-\tfrac{\sigma}{2}\ell^{2} + i\ell m)exp(−2σ​ℓ2+iℓm); the degenerate case σ=0\sigma = 0σ=0, a Dirac mass, is included. It is centred if all these one-dimensional laws have mean zero, which is expressed here as ∫Bx μ(dx)=0\int_B x \, \mu(dx) = 0∫B​xμ(dx)=0.

For a centred Gaussian μ\muμ the covariance form (4.2, p. 20) is

Cμ(ℓ,ℓ′)  =  ∫Bℓ(x) ℓ′(x) μ(dx),ℓ,ℓ′∈B∗.C_\mu(\ell, \ell') \;=\; \int_B \ell(x)\,\ell'(x)\, \mu(dx), \qquad \ell, \ell' \in B^{*} .Cμ​(ℓ,ℓ′)=∫B​ℓ(x)ℓ′(x)μ(dx),ℓ,ℓ′∈B∗.

It is well defined because ∥x∥2\|x\|^{2}∥x∥2 is μ\muμ-integrable, and it is a bounded bilinear form (Corollary 4.14, p. 22).

The Cameron–Martin space (Definition 4.26, p. 27) is classically built as the completion of

H˚μ  =  { h∈B:∃ h∗∈B∗ with Cμ(h∗,ℓ)=ℓ(h)  ∀ℓ∈B∗ }\mathring H_\mu \;=\; \{\, h \in B : \exists\, h^{*} \in B^{*} \text{ with } C_\mu(h^{*}, \ell) = \ell(h) \ \ \forall \ell \in B^{*} \,\}H˚μ​={h∈B:∃h∗∈B∗ with Cμ​(h∗,ℓ)=ℓ(h)  ∀ℓ∈B∗}

under ∥h∥μ2=Cμ(h∗,h∗)\|h\|_\mu^{2} = C_\mu(h^{*}, h^{*})∥h∥μ2​=Cμ​(h∗,h∗). This mission uses the equivalent intrinsic description of Exercise 4.38 (p. 29), which avoids the completion:

∥h∥μ  =  sup⁡{ ℓ(h)  :  ℓ∈B∗, Cμ(ℓ,ℓ)≤1 },Hμ={ h∈B:∥h∥μ<∞ }.\|h\|_\mu \;=\; \sup\{\, \ell(h) \;:\; \ell \in B^{*},\ C_\mu(\ell, \ell) \le 1 \,\}, \qquad H_\mu = \{\, h \in B : \|h\|_\mu < \infty \,\} .∥h∥μ​=sup{ℓ(h):ℓ∈B∗, Cμ​(ℓ,ℓ)≤1},Hμ​={h∈B:∥h∥μ​<∞}.

The supremum is taken in [0,∞][0, \infty][0,∞]; since −ℓ-\ell−ℓ is admissible whenever ℓ\ellℓ is, it equals sup⁡∣ℓ(h)∣\sup |\ell(h)|sup∣ℓ(h)∣ over the same set. For h∈Bh \in Bh∈B write Th:B→BT_h : B \to BTh​:B→B, Th(x)=x+hT_h(x) = x + hTh​(x)=x+h.

Formalization targets

Goal — Theorem 4.44 (Cameron–Martin)

For a centred Gaussian measure μ\muμ on a separable Banach space BBB and h∈Bh \in Bh∈B,

(Th)∗μ ≪ μ⟺h∈Hμ.(T_h)_{*}\mu \ \ll \ \mu \qquad \Longleftrightarrow \qquad h \in H_\mu .(Th​)∗​μ ≪ μ⟺h∈Hμ​.

Both implications are asserted: translation along a Cameron–Martin direction produces an absolutely continuous measure, and translation along any other direction does not (in fact it produces a mutually singular measure).

Milestones

The milestone list follows the route of Section 4.2:

  1. Exercise 4.38 — the supremum description agrees with Definition 4.26 on H˚μ\mathring H_\muH˚μ​.
  2. Proposition 4.32 — Hμ⊂BH_\mu \subset BHμ​⊂B with ∥h∥2≤∥Cμ∥ ∥h∥μ2\|h\|^{2} \le \|C_\mu\| \, \|h\|_\mu^{2}∥h∥2≤∥Cμ​∥∥h∥μ2​.
  3. Proposition 4.40 — every L2(μ)L^{2}(\mu)L2(μ)-limit of elements of B∗B^{*}B∗ has a centred Gaussian law whose variance is its own L2L^2L2 norm squared.
  4. Equation (4.14) — the explicit density Dh(x)=exp⁡(h∗(x)−12∥h∥μ2)D_h(x) = \exp(h^{*}(x) - \tfrac12\|h\|_\mu^{2})Dh​(x)=exp(h∗(x)−21​∥h∥μ2​) of the shifted measure, for h∈H˚μh \in \mathring H_\muh∈H˚μ​.
  5. The total-variation separation bound ∥N(0,1)−N(m,1)∥TV≥2−2e−m2/8\|\mathcal N(0,1) - \mathcal N(m,1)\|_{\mathrm{TV}} \ge 2 - 2e^{-m^{2}/8}∥N(0,1)−N(m,1)∥TV​≥2−2e−m2/8 used in the converse half of Theorem 4.44.
  6. Proposition 4.45 — HμH_\muHμ​ is exactly the intersection of all measurable linear subspaces of full measure.

Significance

The Cameron–Martin theorem is what makes the Cameron–Martin space a canonical object rather than a formal construction: HμH_\muHμ​ is simultaneously the set of admissible shifts, the intersection of all full-measure linear subspaces (Proposition 4.45), and the space whose unit ball governs Gaussian isoperimetry (Theorem 4.53, Borell–Sudakov–Cirel'son). Downstream in the notes it is used to identify invariant measures of linear SPDEs and to compare them; outside the notes it is the starting point of Malliavin calculus and of large deviation theory for Gaussian measures.

Status, precisely. The Mathlib library pinned by this mission already contains a substantial part of Section 4: the predicate IsGaussian (Definition 4.4), uniqueness of measures with equal characteristic functionals on a separable Banach space (Propositions 4.8 and 4.11), invariance of μ⊗μ\mu \otimes \muμ⊗μ under rotations (Proposition 4.12), Fernique's theorem (Theorem 4.13), and the covariance form of (4.2) together with its boundedness (Corollary 4.14) as a continuous bilinear form on the dual. Those results are therefore not milestones here; they are the assumed foundation. What is absent, and what this mission asks for, is everything from the Cameron–Martin space onwards: its definition, its elementary properties, and Theorem 4.44 itself. No machine-checked proof of the infinite-dimensional Cameron–Martin theorem is known to the captain in any Lean library.

Difficulty

The naive route — write down the two densities and take their ratio — is unavailable: there is no translation-invariant reference measure on an infinite-dimensional Banach space, so "the density of μ\muμ" does not exist and the Radon–Nikodym derivative of (Th)∗μ(T_h)_{*}\mu(Th​)∗​μ with respect to μ\muμ must be produced directly, as the exponential of a random variable.

That random variable is the obstruction. For h∈H˚μh \in \mathring H_\muh∈H˚μ​ the functional h∗h^{*}h∗ is continuous and the computation is a characteristic-function identity. But H˚μ\mathring H_\muH˚μ​ is in general strictly smaller than HμH_\muHμ​: a general h∈Hμh \in H_\muh∈Hμ​ has an associated h∗h^{*}h∗ that exists only as an L2(μ)L^{2}(\mu)L2(μ)-limit of continuous functionals, defined μ\muμ-almost everywhere and linear only on a measurable subspace of full measure (Propositions 4.34 and 4.39). Establishing that these limits are Gaussian with the expected variance (Proposition 4.40) is the technical bridge, and it is why milestone 3 is stated as a statement about L2L^{2}L2-limits rather than about elements of B∗B^{*}B∗.

The converse half has a different shape. One must produce, for h∉Hμh \notin H_\muh∈/Hμ​, a single one-dimensional projection that separates μ\muμ from (Th)∗μ(T_h)_{*}\mu(Th​)∗​μ arbitrarily well; unboundedness of ℓ(h)\ell(h)ℓ(h) over the covariance unit ball supplies ℓ\ellℓ with Cμ(ℓ,ℓ)=1C_\mu(\ell,\ell) = 1Cμ​(ℓ,ℓ)=1 and ℓ(h)\ell(h)ℓ(h) as large as desired, and the quantitative Gaussian total-variation bound of milestone 5 converts this into total variation distance 222, i.e. mutual singularity.

Formalization scope

The development is in Lean 4 with Mathlib, in the namespace HairerSPDE, shared by the whole series drawn from these notes. The conventions it commits to:

  1. BBB carries NormedAddCommGroup, NormedSpace ℝ, its Borel σ-algebra, CompleteSpace and SecondCountableTopology — the last two encode "separable Banach space".
  2. Gaussianity is Mathlib's IsGaussian, which is Definition 4.4 verbatim; centredness is the extra hypothesis ∫x dμ=0\int x \, d\mu = 0∫xdμ=0, needed because IsGaussian permits a non-zero mean.
  3. The covariance form is Mathlib's covarianceBilinDual, which equals (4.2) for centred measures with finite second moment and is set to zero otherwise; Fernique's theorem rules the degenerate branch out for Gaussian measures.
  4. The Cameron–Martin norm is the [0,∞][0,\infty][0,∞]-valued supremum above, so membership in HμH_\muHμ​ is finiteness of that supremum; this is the only new definition the mission publishes.
  5. Translation is fun x ↦ x + h, absolute continuity is Mathlib's ≪, and "measurable linear subspace" is a Submodule ℝ B whose carrier is a measurable set.

The goal is an equivalence, so neither half can be discharged vacuously: the direction h∈Hμ⇒(Th)∗μ≪μh \in H_\mu \Rightarrow (T_h)_*\mu \ll \muh∈Hμ​⇒(Th​)∗​μ≪μ is non-trivial already for h≠0h \ne 0h=0 in finite dimensions, and the converse has content precisely when Hμ≠BH_\mu \ne BHμ​=B. Note that ∥0∥μ=0\|0\|_\mu = 0∥0∥μ​=0 always, and that for μ\muμ a Dirac mass the covariance form vanishes and Hμ={0}H_\mu = \{0\}Hμ​={0}; both degenerate cases are inside the statement rather than excluded by hypothesis.

Contributions welcome beyond the milestones: the reproducing kernel space RμR_\muRμ​ and the isomorphism of Proposition 4.34, measurable linear extensions (Proposition 4.39), the dilation singularity of Proposition 4.43, and μ(Hμ)=0\mu(H_\mu) = 0μ(Hμ​)=0 in the infinite-dimensional case (second half of Proposition 4.45). All of these are reusable outside this mission.

Selected references

  • M. Hairer, An Introduction to Stochastic PDEs, lecture notes, 2009/2023. arXiv:0907.4178
  • V. I. Bogachev, Gaussian Measures, Mathematical Surveys and Monographs 62, American Mathematical Society, 1998. DOI:10.1090/surv/062
  • X. Fernique, Intégrabilité des vecteurs gaussiens, C. R. Acad. Sci. Paris Sér. A-B 270 (1970), A1698–A1699.
  • G. Da Prato, J. Zabczyk, Stochastic Equations in Infinite Dimensions, Cambridge University Press, 1992. DOI:10.1017/CBO9780511666223
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AnalysisDynamical SystemsTopology·Captain: Lucas

Local Connectivity of the Mandelbrot Set (MLC)Open Problem

The set

For a complex parameter ccc, iterate the quadratic map

fc(z)=z2+cf_c(z) = z^2 + cfc​(z)=z2+c

starting at the critical point z=0z = 0z=0. The Mandelbrot set is the set of parameters for which this orbit stays bounded:

M={ c∈C : sup⁡k∈N∣fc k(0)∣<∞ }.M = \{\, c \in \mathbb{C} \ : \ \sup_{k \in \mathbb{N}} \left| f_c^{\,k}(0) \right| < \infty \,\}.M={c∈C : k∈Nsup​​fck​(0)​<∞}.

Equivalently -- and this is the first milestone of the mission -- c∈Mc \in Mc∈M if and only if ∣fc k(0)∣≤2|f_c^{\,k}(0)| \le 2∣fck​(0)∣≤2 for every kkk, which exhibits MMM as a compact subset of the plane.

MMM is the parameter-space picture of the simplest non-trivial family in complex dynamics, and it acts as a dictionary: the shape of MMM near a parameter ccc encodes the dynamics of fcf_cfc​ on its Julia set, so structural questions about MMM are questions about the whole quadratic family at once. Douady and Hubbard proved in 1982 that MMM is connected, by exhibiting a conformal isomorphism

Φ:C∖M⟶C∖D‾\Phi : \mathbb{C} \setminus M \longrightarrow \mathbb{C} \setminus \overline{\mathbb{D}}Φ:C∖M⟶C∖D

between the complement of MMM and the exterior of the closed unit disk.

The question

MLC conjecture. MMM is locally connected: every point of MMM has a neighbourhood basis, in the subspace topology, consisting of connected sets.

By Caratheodory's theorem, MLC is equivalent to the statement that Φ−1\Phi^{-1}Φ−1 extends continuously to the unit circle. That extension would deliver a complete combinatorial description of MMM -- the pinched disk model of Douady and Thurston -- in which every boundary point is labelled by the external rays landing on it. Two headline consequences follow: the density of hyperbolicity in the quadratic family (Fatou's conjecture: every quadratic polynomial can be perturbed to one with an attracting cycle), and zero area for ∂M\partial M∂M.

MLC has been open since the early 1980s and is regarded as the central problem of one-dimensional complex dynamics.

Timeline

  • 1982 -- Douady and Hubbard prove that MMM is connected, via the Boettcher uniformisation of its complement, and formulate MLC.
  • 1984/85 -- The Orsay notes develop the combinatorics of external rays and the pinched-disk model, and show that MLC implies the density of hyperbolicity in the quadratic family.
  • 1990 -- Yoccoz proves MLC at every finitely renormalizable parameter without an indifferent periodic point, introducing the Yoccoz puzzle and the rigidity techniques that dominate later work.
  • 1997 -- Lyubich extends local connectivity to infinitely renormalizable parameters of bounded type, using complex bounds for quadratic-like renormalization.
  • 1997 -- Graczyk-Swiatek and Lyubich prove density of hyperbolicity in the real quadratic family.
  • 1998 -- Shishikura proves that ∂M\partial M∂M has Hausdorff dimension 222, by parabolic implosion. Whether ∂M\partial M∂M has positive area remains open.
  • 2005 -- Buff and Cheritat construct quadratic Julia sets of positive area, showing that the analogous area question in the dynamical plane has a negative answer.
  • Today -- MLC is known at large classes of parameters, but the general case, and with it the density of hyperbolicity, remain open.

What this mission asks for

The goal theorem is MLC itself, in the form "the Mandelbrot set, as a topological subspace of C\mathbb{C}C, is a locally connected space".

The milestones are of three kinds, and are ordered accordingly:

  1. Foundations provable today -- the escape criterion (in the quadratic and the general unicritical degree) and compactness. These make the filter-theoretic definition usable and are the natural entry point for a solver new to the mission.
  2. Known theorems from the literature -- connectedness of MMM (Douady-Hubbard), the implication MLC ⇒\Rightarrow⇒ density of hyperbolicity (Douady-Hubbard), and dim⁡H(∂M)=2\dim_H(\partial M) = 2dimH​(∂M)=2 (Shishikura). These are hard but settled, and formalizing them builds the infrastructure -- Boettcher coordinates, external rays, parabolic implosion -- that any attack on the goal will need.
  3. The open companions -- density of hyperbolicity in the quadratic and unicritical families, zero area of ∂M\partial M∂M, and MLC for all Multibrot sets MnM_nMn​, the parameter sets of z↦zn+cz \mapsto z^n + cz↦zn+c.

All statements are phrased against a single shared definition file, so a solver can move between milestones without re-fixing conventions.

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Analysis·Captain: Lucas

Rudin PMA XI: The Lebesgue TheoryTextbook

Motivation

Chapter 11 of Walter Rudin's Principles of Mathematical Analysis (3rd edition, McGraw-Hill, 1976) replaces the Riemann integral of Chapter 6 with the Lebesgue integral, and the reward is a theory of integration whose limit theorems have no superfluous hypotheses and whose space of square-integrable functions is complete. The chapter runs from set functions and outer measures, through the Carathéodory construction of Lebesgue measure, measurable functions and the integral, to the convergence theorems (monotone convergence, Fatou, dominated convergence) and finally to the space L2(μ)\mathscr{L}^2(\mu)L2(μ) and the Riesz–Fischer theorem (Theorem 11.42):

every Cauchy sequence in L2(μ) converges in the mean to an element of L2(μ).\text{every Cauchy sequence in } \mathscr{L}^2(\mu) \text{ converges in the mean to an element of } \mathscr{L}^2(\mu).every Cauchy sequence in L2(μ) converges in the mean to an element of L2(μ).

That completeness is what makes L2\mathscr{L}^2L2 a Hilbert space, and it is the reason the Fourier series of Chapter 8 converge in the mean to the functions they represent.

This mission is the eleventh and last in a series formalizing Rudin Chapters 1–11. It uses the Riemann–Stieltjes integral of Mission VI (for Theorem 11.33, comparing the two integrals) and the trigonometric Fourier series of Mission VIII (for the L2\mathscr{L}^2L2 reading of Parseval's theorem).

Setting

A set function on a ring R\mathscr{R}R of sets is countably additive if it takes the value ∑ϕ(An)\sum \phi(A_n)∑ϕ(An​) on a countable disjoint union. Rudin constructs an outer measure μ∗\mu^*μ∗ from such a ϕ\phiϕ by covering with elementary sets and taking an infimum, calls a set measurable when it is approximable by elementary sets in the metric d(A,B)=μ∗(A△B)d(A, B) = \mu^*(A \triangle B)d(A,B)=μ∗(A△B), and proves that the measurable sets form a σ\sigmaσ-algebra on which μ∗\mu^*μ∗ is countably additive (Theorem 11.10). A real function fff is measurable when {x:f(x)>a}\{x : f(x) > a\}{x:f(x)>a} is measurable for every aaa, and the integral ∫Ef dμ\int_E f\,d\mu∫E​fdμ is defined first for simple functions, then for nonnegative measurable functions as a supremum, and then for general fff by f=f+−f−f = f^+ - f^-f=f+−f−.

The space L2(μ)\mathscr{L}^2(\mu)L2(μ) consists of the measurable fff with ∫∣f∣2dμ<∞\int |f|^2 d\mu < \infty∫∣f∣2dμ<∞, normed by ∥f∥2=(∫∣f∣2dμ)1/2\|f\|_2 = (\int |f|^2 d\mu)^{1/2}∥f∥2​=(∫∣f∣2dμ)1/2; a sequence {fn}\{f_n\}{fn​} converges in the mean to fff if ∥fn−f∥2→0\|f_n - f\|_2 \to 0∥fn​−f∥2​→0.

Mathlib's measure theory is used wherever it is mathematically the same object: MeasureTheory.OuterMeasure and its Carathéodory σ\sigmaσ-algebra, MeasurableSet, Measurable, the lower Lebesgue integral ∫⁻ for nonnegative extended-real functions, the Bochner integral ∫ and Integrable for the general case. What is set up freshly is Rudin's L2\mathscr{L}^2L2 of functions — Rudin.MemL2, Rudin.L2Norm, Rudin.CauchyL2, Rudin.TendstoL2 — rather than Mathlib's quotient space Lp, because the Riesz–Fischer theorem as Rudin states it produces an honest limit function, and the ε-N phrasing of Cauchyness and of mean convergence is part of the statement.

Formalization targets

Goal — the Riesz–Fischer theorem (Theorem 11.42)

If {fn}\{f_n\}{fn​} is a Cauchy sequence in L2(μ)\mathscr{L}^2(\mu)L2(μ), then there exists f∈L2(μ)f \in \mathscr{L}^2(\mu)f∈L2(μ) with ∥fn−f∥2→0\|f_n - f\|_2 \to 0∥fn​−f∥2​→0: the space L2(μ)\mathscr{L}^2(\mu)L2(μ) is complete.

Rudin's proof extracts a subsequence with ∥fnk+1−fnk∥2<2−k\|f_{n_{k+1}} - f_{n_k}\|_2 < 2^{-k}∥fnk+1​​−fnk​​∥2​<2−k, sums the telescoping series, uses the monotone convergence theorem and the Schwarz inequality to show that the sum converges almost everywhere, and identifies the pointwise limit as the mean limit of the whole sequence. Every ingredient is a milestone of this mission.

Milestones

the measurable sets of an outer measure form a σ-algebra on which it is countably additive(11.10)\text{the measurable sets of an outer measure form a } \sigma\text{-algebra on which it is countably additive} \qquad (11.10)the measurable sets of an outer measure form a σ-algebra on which it is countably additive(11.10) sup⁡nfn and lim sup⁡nfn are measurable(11.17)\sup_n f_n \text{ and } \limsup_n f_n \text{ are measurable} \qquad (11.17)nsup​fn​ and nlimsup​fn​ are measurable(11.17) ∣f∣, f+g, fg are measurable(11.16, 11.18)|f|,\ f+g,\ fg \text{ are measurable} \qquad (11.16,\ 11.18)∣f∣, f+g, fg are measurable(11.16, 11.18) E↦∫Ef dμ is countably additive(11.24)E \mapsto \int_E f\,d\mu \text{ is countably additive} \qquad (11.24)E↦∫E​fdμ is countably additive(11.24) ∣∫f dμ∣≤∫∣f∣ dμ(11.26, 11.27)\left|\int f\,d\mu\right| \le \int |f|\,d\mu \qquad (11.26,\ 11.27)​∫fdμ​≤∫∣f∣dμ(11.26, 11.27) ∫lim⁡nfn dμ=lim⁡n∫fn dμ  for 0≤f1≤f2≤⋯(11.28)\int \lim_n f_n \,d\mu = \lim_n \int f_n\,d\mu \ \text{ for } 0 \le f_1 \le f_2 \le \cdots \qquad (11.28)∫nlim​fn​dμ=nlim​∫fn​dμ  for 0≤f1​≤f2​≤⋯(11.28) ∫∑nfn dμ=∑n∫fn dμ  for fn≥0(11.30)\int \sum_n f_n \,d\mu = \sum_n \int f_n\,d\mu \ \text{ for } f_n \ge 0 \qquad (11.30)∫n∑​fn​dμ=n∑​∫fn​dμ  for fn​≥0(11.30) ∫lim inf⁡nfn dμ≤lim inf⁡n∫fn dμ(11.31)\int \liminf_n f_n\,d\mu \le \liminf_n \int f_n\,d\mu \qquad (11.31)∫nliminf​fn​dμ≤nliminf​∫fn​dμ(11.31) dominated convergence(11.32)\text{dominated convergence} \qquad (11.32)dominated convergence(11.32) Riemann-integrable⇒Lebesgue-integrable, with the same integral(11.33)\text{Riemann-integrable} \Rightarrow \text{Lebesgue-integrable, with the same integral} \qquad (11.33)Riemann-integrable⇒Lebesgue-integrable, with the same integral(11.33) ∣∫fg dμ∣≤∥f∥2 ∥g∥2(11.35)\left|\int fg\,d\mu\right| \le \|f\|_2\,\|g\|_2 \qquad (11.35)​∫fgdμ​≤∥f∥2​∥g∥2​(11.35) continuous functions are dense in L2[a,b](11.38)\text{continuous functions are dense in } \mathscr{L}^2[a,b] \qquad (11.38)continuous functions are dense in L2[a,b](11.38) ∑ncn2=∫f2dμ for a complete orthonormal system(11.45)\sum_n c_n^2 = \int f^2 d\mu \text{ for a complete orthonormal system} \qquad (11.45)n∑​cn2​=∫f2dμ for a complete orthonormal system(11.45)

Significance

The Lebesgue theory is the point at which analysis acquires limit theorems that do not require uniform convergence. Monotone convergence, Fatou's lemma and dominated convergence are the three statements that make the integral usable in probability, in Fourier analysis and in the theory of partial differential equations, and the Riesz–Fischer theorem is what makes L2\mathscr{L}^2L2 a Hilbert space and therefore the natural home of Fourier expansions: Parseval's identity (11.45) is the assertion that the Fourier coefficient map is an isometry onto ℓ2\ell^2ℓ2.

Theorem 11.33 is the bridge back to the earlier chapters — every Riemann-integrable function is Lebesgue-integrable with the same integral, and a bounded function on [a,b][a, b][a,b] is Riemann-integrable exactly when it is continuous almost everywhere — so the two halves of the book agree wherever both apply.

Mathlib has an extensive measure theory and proves many of these results in considerable generality. This mission's contribution is to state them in Rudin's formulation, for Rudin's L2\mathscr{L}^2L2 of functions and with his explicit ε-N definitions, so that the chapter is available as a coherent, self-contained unit that matches the textbook line by line and links back to the Riemann–Stieltjes integral of Mission VI.

Difficulty

Individually, most milestones will reduce to Mathlib results after the correct dictionary is in place, and the interesting work is exactly in that translation: Rudin's measurability ({x : f(x) > a} measurable) versus Mathlib's Measurable, Rudin's integral of a nonnegative function versus ∫⁻ with values in ℝ≥0∞, Rudin's L2\mathscr{L}^2L2 of genuine functions versus Lp as a quotient by almost-everywhere equality. The last of these is what makes the goal theorem nontrivial to derive: Mathlib's completeness of Lp gives a limit class, and one must choose a measurable representative and verify Rudin's mean convergence with the concrete norm Rudin.L2Norm, which is Real.sqrt (∫ f²) and not an ENNReal quantity.

Theorem 11.33 (Riemann implies Lebesgue) and Theorem 11.38 (density of continuous functions) are the two other places where real work is required: the first has to connect the Chapter 6 definition of the Riemann integral with intervalIntegral, and the second is an approximation argument.

Formalization scope

Conventions fixed by this mission:

  • Measure-theoretic vocabulary is Mathlib's: MeasureTheory.Measure, MeasurableSet, Measurable, Integrable, ∫⁻ x, f x ∂μ for nonnegative ℝ≥0∞-valued integrands and ∫ x, f x ∂μ for the general real case. Rudin's Carathéodory construction is MeasureTheory.OuterMeasure.caratheodory.
  • Statements about suprema and upper limits of sequences of functions (11.17), and about term-by-term integration of series (11.30) and Fatou's theorem (11.31), use ℝ≥0∞-valued functions, matching Rudin's use of extended real values there.
  • Rudin.MemL2 μ f is "f is measurable and f² is integrable"; Rudin.L2Norm μ f is Real.sqrt (∫ x, (f x)^2 ∂μ); Rudin.CauchyL2 and Rudin.TendstoL2 are Rudin's ε-N Cauchy condition and mean convergence. No quotient is taken, so the goal theorem produces a function.
  • Theorem 11.33 is stated with Rudin.RiemannIntegrable and Rudin.RiemannIntegral from Mission VI, so the two integrals are literally compared.
  • Parseval (11.45) is stated for an arbitrary complete orthonormal system in L2(μ)\mathscr{L}^2(\mu)L2(μ), completeness being phrased as "a function orthogonal to every φn\varphi_nφn​ has norm zero"; the trigonometric case is Theorem 8.16 of Mission VIII.

Contributions of the convergence theorems (11.28, 11.31, 11.32) and of the Schwarz inequality (11.35) are especially useful, since the goal theorem consumes them directly.

Selected references

  • Walter Rudin, Principles of Mathematical Analysis, 3rd edition, McGraw-Hill, 1976, Chapter 11 (pp. 300–332).
  • Walter Rudin, Real and Complex Analysis, 3rd edition, McGraw-Hill, 1987, Chapters 1–3.
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Analysis·Captain: Lucas

Rudin PMA VIII: Some Special FunctionsTextbook

Motivation

Chapter 8 of Walter Rudin's Principles of Mathematical Analysis (3rd edition, McGraw-Hill, 1976) puts the general theory of the preceding chapters to work on concrete functions. Power series are differentiated term by term; the exponential function is defined by its series and the trigonometric functions and the number π\piπ are extracted from it; the fundamental theorem of algebra is proved; Fourier series are introduced through general orthonormal systems; and the Gamma function is characterized by log-convexity.

The chapter's capstone is Parseval's theorem (Theorem 8.16): for Riemann-integrable 2π2\pi2π-periodic functions, the Fourier series converges in the mean square sense and the L2L^2L2 inner product is computed by the (absolutely convergent) sum of products of Fourier coefficients. It is the statement that the trigonometric system is not merely orthonormal but complete, and it is the finite-dimensional Pythagorean theorem carried to infinite dimensions.

This mission is the eighth in a series formalizing Rudin Chapters 1–11; it uses the convergence tests of Mission III and the uniform-convergence and approximation theorems of Mission VII, and it is the analytic counterpart of the abstract L2L^2L2 theory of Mission XI.

Setting

A power series is ∑cnxn\sum c_n x^n∑cn​xn; by Chapter 3 it converges on an interval (−R,R)(-R,R)(−R,R). A sequence {φn}\{\varphi_n\}{φn​} of complex functions on [a,b][a,b][a,b] is an orthonormal system if ∫abφnφm‾=0\int_a^b \varphi_n \overline{\varphi_m} = 0∫ab​φn​φm​​=0 for n≠mn \ne mn=m and ∫ab∣φn∣2=1\int_a^b |\varphi_n|^2 = 1∫ab​∣φn​∣2=1; the Fourier coefficients of fff relative to it are cn=∫abfφn‾c_n = \int_a^b f \overline{\varphi_n}cn​=∫ab​fφn​​, and the Fourier series is ∑cnφn\sum c_n \varphi_n∑cn​φn​. For the trigonometric system on [−π,π][-\pi,\pi][−π,π] one writes

cn=12π∫−ππf(x)e−inx dx,sN(f;x)=∑n=−NNcneinx,∥h∥2=(12π∫−ππ∣h∣2)1/2.c_n = \frac{1}{2\pi}\int_{-\pi}^{\pi} f(x)e^{-inx}\,dx, \qquad s_N(f;x) = \sum_{n=-N}^{N} c_n e^{inx}, \qquad \|h\|_2 = \Big(\frac{1}{2\pi}\int_{-\pi}^{\pi}|h|^2\Big)^{1/2}.cn​=2π1​∫−ππ​f(x)e−inxdx,sN​(f;x)=n=−N∑N​cn​einx,∥h∥2​=(2π1​∫−ππ​∣h∣2)1/2.

A trigonometric polynomial is a finite sum ∑n=−NNcneinx\sum_{n=-N}^{N} c_n e^{inx}∑n=−NN​cn​einx. The Gamma function is Γ(x)=∫0∞tx−1e−t dt\Gamma(x) = \int_0^\infty t^{x-1}e^{-t}\,dtΓ(x)=∫0∞​tx−1e−tdt for x>0x > 0x>0.

Formalization targets

Goal — Parseval's theorem (Theorem 8.16)

For Riemann-integrable 2π2\pi2π-periodic fff and ggg with Fourier coefficients cnc_ncn​ and γn\gamma_nγn​:

lim⁡N→∞∥f−sN(f)∥2=0,12π∫−ππfgˉ=∑n=−∞∞cnγn‾,12π∫−ππ∣f∣2=∑n=−∞∞∣cn∣2.\lim_{N\to\infty}\|f - s_N(f)\|_2 = 0, \qquad \frac{1}{2\pi}\int_{-\pi}^{\pi} f\bar g = \sum_{n=-\infty}^{\infty} c_n \overline{\gamma_n}, \qquad \frac{1}{2\pi}\int_{-\pi}^{\pi} |f|^2 = \sum_{n=-\infty}^{\infty} |c_n|^2 .N→∞lim​∥f−sN​(f)∥2​=0,2π1​∫−ππ​fgˉ​=n=−∞∑∞​cn​γn​​,2π1​∫−ππ​∣f∣2=n=−∞∑∞​∣cn​∣2.

Milestones

term-by-term differentiation of a power series(8.1)\text{term-by-term differentiation of a power series} \qquad (8.1)term-by-term differentiation of a power series(8.1) ∑cn=C⇒∑cnxn→C as x→1−(8.2)\textstyle\sum c_n = C \Rightarrow \sum c_n x^n \to C \text{ as } x \to 1^- \qquad (8.2)∑cn​=C⇒∑cn​xn→C as x→1−(8.2) interchange of the order of summation in a double series(8.3)\text{interchange of the order of summation in a double series} \qquad (8.3)interchange of the order of summation in a double series(8.3) two power series agreeing on a set with a limit point have equal coefficients(8.5)\text{two power series agreeing on a set with a limit point have equal coefficients} \qquad (8.5)two power series agreeing on a set with a limit point have equal coefficients(8.5) E(z+w)=E(z)E(w), E′=E, growth of E(8.6)E(z+w) = E(z)E(w),\ E' = E,\ \text{growth of } E \qquad (8.6)E(z+w)=E(z)E(w), E′=E, growth of E(8.6) cos⁡(π/2)=0, cos⁡>0 on [0,π/2), ez+2πi=ez, ∣z∣=1⇒z=eit(8.7)\cos(\pi/2) = 0,\ \cos > 0 \text{ on } [0,\pi/2),\ e^{z+2\pi i} = e^z,\ |z| = 1 \Rightarrow z = e^{it} \qquad (8.7)cos(π/2)=0, cos>0 on [0,π/2), ez+2πi=ez, ∣z∣=1⇒z=eit(8.7) every nonconstant complex polynomial has a root(8.8)\text{every nonconstant complex polynomial has a root} \qquad (8.8)every nonconstant complex polynomial has a root(8.8) Fourier partial sums minimize the mean square error; Bessel’s inequality(8.11, 8.12)\text{Fourier partial sums minimize the mean square error; Bessel's inequality} \qquad (8.11,\ 8.12)Fourier partial sums minimize the mean square error; Bessel’s inequality(8.11, 8.12) a local Lipschitz condition at x forces sN(f;x)→f(x)(8.14)\text{a local Lipschitz condition at } x \text{ forces } s_N(f;x) \to f(x) \qquad (8.14)a local Lipschitz condition at x forces sN​(f;x)→f(x)(8.14) trigonometric polynomials approximate continuous periodic functions uniformly(8.15)\text{trigonometric polynomials approximate continuous periodic functions uniformly} \qquad (8.15)trigonometric polynomials approximate continuous periodic functions uniformly(8.15) Γ(x+1)=xΓ(x), Γ(n+1)=n!, log⁡Γ convex(8.18)\Gamma(x+1) = x\Gamma(x),\ \Gamma(n+1) = n!,\ \log\Gamma \text{ convex} \qquad (8.18)Γ(x+1)=xΓ(x), Γ(n+1)=n!, logΓ convex(8.18) Bohr–Mollerup: these three properties characterize Γ(8.19)\text{Bohr–Mollerup: these three properties characterize } \Gamma \qquad (8.19)Bohr–Mollerup: these three properties characterize Γ(8.19)

Significance

Parseval's theorem is the completeness statement for the trigonometric system: Bessel's inequality (8.12) holds for every orthonormal system, and equality for all fff is exactly what distinguishes a complete system. The proof shows how the pieces of the book fit together: it uses the approximation theorem 8.15 (itself a corollary of Stone–Weierstrass from Chapter 7), the minimizing property 8.11, and the Schwarz inequality of Chapter 1. Chapter 11 generalizes the conclusion to arbitrary complete orthonormal systems in L2L^2L2, where the Riemann-integrable hypothesis can be dropped.

The other milestones are where the elementary functions acquire their properties: the 2π2\pi2π-periodicity of the complex exponential, the definition of π\piπ as twice the first positive zero of the cosine, and the log-convexity characterization of the Gamma function are all established here rather than assumed.

Mathlib has the exponential and trigonometric functions, π\piπ, the fundamental theorem of algebra, the Gamma function with the Bohr–Mollerup theorem, and a Fourier theory on the additive circle. The work in this mission is to state Rudin's versions — 2π2\pi2π-periodic functions on R\mathbb{R}R, generic orthonormal systems on an interval, Riemann-integrable rather than square-integrable hypotheses — and connect them to that library.

Difficulty

Parseval's theorem is where an approximation argument in the uniform norm has to be converted into one in the mean square norm. The chain is: approximate fff in ∥⋅∥2\|\cdot\|_2∥⋅∥2​ by a continuous periodic hhh (a nontrivial step for a merely Riemann-integrable fff, and the place where the hypothesis is really used), approximate hhh uniformly by a trigonometric polynomial PPP, and then use the minimizing property of the partial sums to conclude ∥f−sN(f)∥2\|f - s_N(f)\|_2∥f−sN​(f)∥2​ is small. The first step has no analogue in the uniform theory and is the main obstacle; the third depends on sNs_NsN​ being an orthogonal projection, which is Theorem 8.11.

Formalization scope

Conventions fixed by this mission:

  • Integrals of complex-valued functions use Mathlib's interval integral ∫ x in a..b, f x, not the real-valued Riemann–Stieltjes integral built in Mission VI; for the Riemann-integrable integrands of this chapter the two agree. Integrability hypotheses are stated as IntervalIntegrable.
  • Fourier notions are Rudin.fourierCoeff, Rudin.fourierPartialSum, Rudin.L2Norm, Rudin.IsTrigPolynomial, Rudin.HasPeriodTwoPi, and, for general systems, Rudin.IsOrthonormalSystem and Rudin.genFourierCoeff, all following Rudin's normalizations (in particular the 1/2π1/2\pi1/2π in cnc_ncn​ and in ∥⋅∥2\|\cdot\|_2∥⋅∥2​).
  • Series of real numbers use Rudin.SeriesConvergesTo from Mission III, so that conditional convergence is expressible; the two-sided sums ∑n=−∞∞\sum_{n=-\infty}^{\infty}∑n=−∞∞​ of Parseval are stated as limits of the symmetric partial sums ∑∣n∣≤N\sum_{|n| \le N}∑∣n∣≤N​, as in Rudin.
  • exp⁡\expexp, cos⁡\coscos, π\piπ and Γ\GammaΓ are Mathlib's; Theorem 8.7 is therefore stated as the list of properties Rudin derives, not as a redefinition of π\piπ.

Selected references

  • Walter Rudin, Principles of Mathematical Analysis, 3rd edition, McGraw-Hill, 1976, Chapter 8 (pp. 172–201).
  • P. J. Davis, Leonhard Euler's integral: A historical profile of the Gamma function, American Mathematical Monthly 66 (1959), 849–869. https://doi.org/10.2307/2309786
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AnalysisDifferential Geometry·Captain: Lucas

Rudin PMA X: Integration of Differential FormsTextbook

Motivation

Chapter 10 of Walter Rudin's Principles of Mathematical Analysis (3rd edition, McGraw-Hill, 1976) builds the calculus of differential forms in Rn\mathbb{R}^nRn and proves the theorem that unifies the integral theorems of vector analysis. The fundamental theorem of calculus, the Green, divergence and classical Stokes theorems all say the same thing — that integrating a derivative over a region is the same as integrating the original object over the boundary of that region — and Stokes' theorem (Theorem 10.33),

∫Ψdω=∫∂Ψω,\int_\Psi d\omega = \int_{\partial \Psi} \omega ,∫Ψ​dω=∫∂Ψ​ω,

is that statement, once "region" is made precise as a chain of parametrized surfaces and "derivative" as the exterior derivative.

This mission is the tenth in a series formalizing Rudin Chapters 1–11; it uses the inverse function theorem and the several-variable calculus of Mission IX.

Setting

For an open E⊆RnE \subseteq \mathbb{R}^nE⊆Rn, a kkk-surface in EEE is a C′C'C′-mapping Φ\PhiΦ from a parameter domain D⊆RkD \subseteq \mathbb{R}^kD⊆Rk — a kkk-cell or the standard simplex Qk={u:ui≥0,∑ui≤1}Q^k = \{u : u_i \ge 0, \sum u_i \le 1\}Qk={u:ui​≥0,∑ui​≤1} — into EEE; surfaces are maps, not point sets. A kkk-form in EEE is a formal sum

ω=∑ai1⋯ik(x) dxi1∧⋯∧dxik\omega = \sum a_{i_1\cdots i_k}(\mathbf{x})\,dx_{i_1}\wedge\cdots\wedge dx_{i_k}ω=∑ai1​⋯ik​​(x)dxi1​​∧⋯∧dxik​​

with continuous coefficients, whose meaning is the rule assigning to each kkk-surface Φ\PhiΦ the number

∫Φω=∫D∑ai1⋯ik(Φ(u)) ∂(φi1,…,φik)∂(u1,…,uk) du.\int_\Phi \omega = \int_D \sum a_{i_1\cdots i_k}(\Phi(\mathbf{u}))\, \frac{\partial(\varphi_{i_1},\dots,\varphi_{i_k})}{\partial(u_1,\dots,u_k)}\,d\mathbf{u}.∫Φ​ω=∫D​∑ai1​⋯ik​​(Φ(u))∂(u1​,…,uk​)∂(φi1​​,…,φik​​)​du.

The exterior derivative of ω\omegaω is the (k+1)(k+1)(k+1)-form with coefficients DjaID_j a_IDj​aI​; the pullback ωT\omega_TωT​ along a differentiable TTT substitutes TTT into the coefficients and the differentials. A kkk-chain is a formal integer combination of kkk-surfaces with parameter domain QkQ^kQk, its integral is the corresponding combination of integrals, and its boundary ∂Ψ\partial\Psi∂Ψ is obtained from the alternating sum ∑j(−1)j\sum_j (-1)^j∑j​(−1)j of the faces of QkQ^kQk.

Formalization targets

Goal — Stokes' theorem (Theorem 10.33)

If Ψ\PsiΨ is a kkk-chain of class C′′C''C′′ in an open V⊆RnV \subseteq \mathbb{R}^nV⊆Rn and ω\omegaω is a (k−1)(k-1)(k−1)-form of class C′C'C′ in VVV, then

∫Ψdω=∫∂Ψω.\int_\Psi d\omega = \int_{\partial\Psi} \omega .∫Ψ​dω=∫∂Ψ​ω.

For k=n=1k = n = 1k=n=1 this is the fundamental theorem of calculus, for k=n=2k = n = 2k=n=2 Green's theorem, for k=n=3k = n = 3k=n=3 the divergence theorem, and for k=2k = 2k=2, n=3n = 3n=3 the theorem of Stokes.

Milestones

the iterated integrals of a continuous function on a cell agree(10.2)\text{the iterated integrals of a continuous function on a cell agree} \qquad (10.2)the iterated integrals of a continuous function on a cell agree(10.2) partitions of unity subordinate to an open cover of a compact set(10.8)\text{partitions of unity subordinate to an open cover of a compact set} \qquad (10.8)partitions of unity subordinate to an open cover of a compact set(10.8) ∫f(y) dy=∫f(T(x)) ∣JT(x)∣ dx(10.9)\int f(\mathbf{y})\,d\mathbf{y} = \int f(T(\mathbf{x}))\,|J_T(\mathbf{x})|\,d\mathbf{x} \qquad (10.9)∫f(y)dy=∫f(T(x))∣JT​(x)∣dx(10.9) d(dω)=0(10.20)d(d\omega) = 0 \qquad (10.20)d(dω)=0(10.20) (dω)T=d(ωT)(10.22c)(d\omega)_T = d(\omega_T) \qquad (10.22\mathrm{c})(dω)T​=d(ωT​)(10.22c) ∫T∘Φω=∫ΦωT(10.25)\int_{T\circ\Phi}\omega = \int_\Phi \omega_T \qquad (10.25)∫T∘Φ​ω=∫Φ​ωT​(10.25) reordering the vertices of a simplex multiplies the integral by the sign(10.27)\text{reordering the vertices of a simplex multiplies the integral by the sign} \qquad (10.27)reordering the vertices of a simplex multiplies the integral by the sign(10.27) Poincareˊ’s lemma: on a convex open set, closed forms are exact(10.39)\text{Poincaré's lemma: on a convex open set, closed forms are exact} \qquad (10.39)Poincareˊ’s lemma: on a convex open set, closed forms are exact(10.39)

Significance

Stokes' theorem is the organizing theorem of multivariable analysis; its formal content is that ddd and ∂\partial∂ are adjoint, which is also the starting point of de Rham cohomology. Poincaré's lemma is its local converse: on a convex set the only obstruction to a closed form being exact disappears, so the failure of exactness measures the shape of the domain. The change of variables theorem (10.9) is what makes integrals independent of the parametrization and is used in the proof of Stokes itself, and partitions of unity (10.8) are the standard device for passing from local to global statements.

Mathlib has a general change-of-variables theorem for the Lebesgue integral, smooth partitions of unity, and the theory of alternating forms and de Rham differentials on manifolds; it does not have Rudin's concrete apparatus of parametrized surfaces, affine chains, and their boundaries, nor a version of Stokes' theorem for such chains. This mission builds that apparatus and states the chapter's theorems for it; the definitions are reusable for any development that wants a hands-on, coordinate-based treatment of forms.

Difficulty

This is the most demanding mission of the series, for two reasons. First, the objects have to be set up before anything can be said: forms as coefficient families, their integrals as Jacobian integrals, chains, and the boundary operator with its signs. Second, Stokes' theorem is proved by reducing to a single oriented simplex, transporting along the parametrization by Theorem 10.25, and then computing the integral over QkQ^kQk by an iterated integral in which all but two terms of the boundary cancel; the cancellation is entirely a matter of getting the signs of the face maps right, and it is where a formalization will spend its time.

A further subtlety: with forms presented by coefficients indexed by all index tuples, the identity d(dω)=0d(d\omega) = 0d(dω)=0 is false coefficient-wise and true as an identity of forms. Since Rudin defines a form to be its integration functional, statements of the shape "this form vanishes" are formalized as "its integral over every surface vanishes", and that is how 10.20, 10.22(c) and 10.39 are stated here.

Formalization scope

Conventions fixed by this mission:

  • Points of Rn\mathbb{R}^nRn are Fin n → ℝ. A kkk-form is Rudin.KForm k n, a coefficient function indexed by all tuples Fin k → Fin n, following Rudin's equation (34).
  • Rudin.integralOverCell and Rudin.integralOverSimplex are Rudin's equation (35) for the two admissible parameter domains, with Rudin.jacobian the determinant of the matrix of partial derivatives. The integral over the parameter domain is the Lebesgue integral for the volume measure, which agrees with Rudin's Riemann integral for continuous integrands.
  • Rudin.extDeriv and Rudin.pullback are the exterior derivative and the pullback; Rudin.Chain, Rudin.Chain.integral and Rudin.Chain.boundary are chains with integer multiplicities, their integrals, and the boundary built from the faces of the standard simplex with Rudin's signs (−1)j(-1)^j(−1)j.
  • Regularity is ContDiff ℝ 1 and ContDiff ℝ 2 for Rudin's C′C'C′ and C′′C''C′′.
  • Equalities between forms are stated as equalities of their integrals over surfaces, as explained above; the goal theorem is an equality of two real numbers, so it is not vacuous.

Contributions of the supporting differential-form identities (10.20, 10.22, 10.25) are especially welcome, since they are exactly the lemmas the goal theorem consumes.

Selected references

  • Walter Rudin, Principles of Mathematical Analysis, 3rd edition, McGraw-Hill, 1976, Chapter 10 (pp. 245–299).
  • Michael Spivak, Calculus on Manifolds, W. A. Benjamin, 1965.
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Analysis·Captain: Lucas

Rudin PMA V: DifferentiationTextbook

Motivation

Chapter 5 of Walter Rudin's Principles of Mathematical Analysis (3rd edition, McGraw-Hill, 1976) is the differential calculus of one real variable, developed from the definition of the derivative as a limit of difference quotients. Its organizing result is the mean value theorem and the family of consequences that follow from it: monotonicity criteria, L'Hospital's rule, and — the chapter's capstone — Taylor's theorem (Theorem 5.15), which approximates a function by a polynomial of degree n−1n-1n−1 and expresses the error exactly as a single nnn-th derivative evaluated at an unspecified intermediate point.

Taylor's theorem is what makes differentiability quantitatively useful. It is the tool that turns local smoothness into explicit error bounds, and the estimates of Chapter 8 for the exponential, trigonometric and Gamma functions all rest on it.

This mission is the fifth in a series formalizing Rudin Chapters 1–11; it uses the continuity and compactness results of Mission IV.

Setting

Let fff be real-valued on [a,b][a,b][a,b]. For x∈[a,b]x \in [a,b]x∈[a,b] the derivative is

f′(x)=lim⁡t→xf(t)−f(x)t−x,f'(x) = \lim_{t \to x} \frac{f(t) - f(x)}{t - x},f′(x)=t→xlim​t−xf(t)−f(x)​,

whenever the limit exists. Higher derivatives f′,f′′,…,f(n)f', f'', \dots, f^{(n)}f′,f′′,…,f(n) are defined by iteration; f(n)f^{(n)}f(n) exists on a set only if f(n−1)f^{(n-1)}f(n−1) exists in a neighbourhood of each of its points. fff has a local maximum at xxx if f(t)≤f(x)f(t) \le f(x)f(t)≤f(x) for all ttt near xxx.

Given a positive integer nnn and a point α\alphaα, the Taylor polynomial of fff at α\alphaα of degree n−1n-1n−1 is

P(t)=∑k=0n−1f(k)(α)k! (t−α)k.P(t) = \sum_{k=0}^{n-1} \frac{f^{(k)}(\alpha)}{k!}\,(t-\alpha)^k .P(t)=k=0∑n−1​k!f(k)(α)​(t−α)k.

Formalization targets

Goal — Taylor's theorem (Theorem 5.15)

Let f(n−1)f^{(n-1)}f(n−1) be continuous on [a,b][a,b][a,b], let f(n)(t)f^{(n)}(t)f(n)(t) exist for t∈(a,b)t \in (a,b)t∈(a,b), and let α≠β\alpha \ne \betaα=β be points of [a,b][a,b][a,b]. Then there is a point xxx strictly between α\alphaα and β\betaβ such that

f(β)  =  ∑k=0n−1f(k)(α)k! (β−α)k  +  f(n)(x)n! (β−α)n.f(\beta) \;=\; \sum_{k=0}^{n-1} \frac{f^{(k)}(\alpha)}{k!}\,(\beta-\alpha)^k \;+\; \frac{f^{(n)}(x)}{n!}\,(\beta-\alpha)^n .f(β)=k=0∑n−1​k!f(k)(α)​(β−α)k+n!f(n)(x)​(β−α)n.

For n=1n = 1n=1 this is exactly the mean value theorem.

Milestones

f differentiable at x⇒f continuous at x(5.2)f \text{ differentiable at } x \Rightarrow f \text{ continuous at } x \qquad (5.2)f differentiable at x⇒f continuous at x(5.2) local maximum at an interior x, f′(x) exists⇒f′(x)=0(5.8)\text{local maximum at an interior } x,\ f'(x) \text{ exists} \Rightarrow f'(x) = 0 \qquad (5.8)local maximum at an interior x, f′(x) exists⇒f′(x)=0(5.8) (f(b)−f(a)) g′(x)=(g(b)−g(a)) f′(x) for some x∈(a,b)(5.9)(f(b)-f(a))\,g'(x) = (g(b)-g(a))\,f'(x) \text{ for some } x \in (a,b) \qquad (5.9)(f(b)−f(a))g′(x)=(g(b)−g(a))f′(x) for some x∈(a,b)(5.9) f(b)−f(a)=(b−a)f′(x) for some x∈(a,b)(5.10)f(b) - f(a) = (b-a) f'(x) \text{ for some } x \in (a,b) \qquad (5.10)f(b)−f(a)=(b−a)f′(x) for some x∈(a,b)(5.10) f′≥0⇒f increasing;f′=0⇒f constant;f′≤0⇒f decreasing(5.11)f' \ge 0 \Rightarrow f \text{ increasing}; \quad f' = 0 \Rightarrow f \text{ constant}; \quad f' \le 0 \Rightarrow f \text{ decreasing} \qquad (5.11)f′≥0⇒f increasing;f′=0⇒f constant;f′≤0⇒f decreasing(5.11) f′(a)<A<f′(b)⇒f′(x)=A for some x∈(a,b)(5.12)f'(a) < A < f'(b) \Rightarrow f'(x) = A \text{ for some } x \in (a,b) \qquad (5.12)f′(a)<A<f′(b)⇒f′(x)=A for some x∈(a,b)(5.12) f,g→0 and f′/g′→A⇒f/g→A(5.13)f, g \to 0 \text{ and } f'/g' \to A \Rightarrow f/g \to A \qquad (5.13)f,g→0 and f′/g′→A⇒f/g→A(5.13) ∥f(b)−f(a)∥≤(b−a) ∥f′(x)∥ for some x∈(a,b), f vector-valued(5.19)\|f(b) - f(a)\| \le (b-a)\,\|f'(x)\| \text{ for some } x \in (a,b),\ f \text{ vector-valued} \qquad (5.19)∥f(b)−f(a)∥≤(b−a)∥f′(x)∥ for some x∈(a,b), f vector-valued(5.19)

Significance

The mean value theorem converts a hypothesis about derivatives into a statement about increments, and everything in the chapter is an application of that conversion. Monotonicity criteria (5.11) are the basis of every "the function is increasing, hence injective" argument, including the change of variable in Chapter 6. Darboux's theorem (5.12) shows that derivatives, though not necessarily continuous, cannot have simple discontinuities — a fact that is easy to state and impossible to guess from the definition. Theorem 5.19 is the form of the mean value theorem that survives for vector-valued functions: the equality is lost (there need be no single point where the vector increment is proportional to the derivative), and only the inequality remains; the same phenomenon dictates the statements of Chapter 9.

Mathlib contains the mean value theorem, L'Hospital's rule, and a Taylor theorem with various remainder forms. The value of this mission is a statement of Taylor's theorem in Rudin's exact formulation — arbitrary distinct endpoints α,β\alpha, \betaα,β in [a,b][a,b][a,b], hypotheses only on f(n−1)f^{(n-1)}f(n−1) and f(n)f^{(n)}f(n), an intermediate point xxx strictly between them — and the derivation of the chapter's other results in a form the later missions can quote.

Difficulty

Taylor's theorem is proved by choosing the constant MMM so that f(β)=P(β)+M(β−α)nf(\beta) = P(\beta) + M(\beta-\alpha)^nf(β)=P(β)+M(β−α)n and applying Rolle's theorem nnn times to g(t)=f(t)−P(t)−M(t−α)ng(t) = f(t) - P(t) - M(t-\alpha)^ng(t)=f(t)−P(t)−M(t−α)n; the bookkeeping is in tracking that g(k)(α)=0g^{(k)}(\alpha) = 0g(k)(α)=0 for k<nk < nk<n and that each application produces a new intermediate point strictly inside the previous interval. In a proof assistant the iteration is the awkward part: the induction is on nnn with the interval shrinking, and the statement must be general enough in α\alphaα and β\betaβ (either order) for the inductive step to apply. The hypothesis that f(n)f^{(n)}f(n) exists only on the open interval, while f(n−1)f^{(n-1)}f(n−1) is merely continuous on the closed one, must be preserved — strengthening it to CnC^nCn on [a,b][a,b][a,b] would make the statement weaker than Rudin's.

Formalization scope

Conventions fixed by this mission:

  • Derivatives are Mathlib's deriv and iteratedDeriv, which are total functions returning 0 where the function is not differentiable; every statement therefore carries explicit differentiability hypotheses exactly where Rudin states them.
  • Intervals are Set.Icc a b and Set.Ioo a b, and "for some xxx between α\alphaα and β\betaβ" is stated as an explicit disjunction, since the goal does not assume α<β\alpha < \betaα<β.
  • Vector-valued functions in 5.19 take values in EuclideanSpace ℝ (Fin k), and the conclusion is the inequality, not an equality — the equality version is false, as Rudin notes.
  • L'Hospital's rule is formalized in the 0/00/00/0 case at a finite left endpoint, which is the first case of Rudin's Theorem 5.13; the ∞\infty∞ case and the limits at ±∞\pm\infty±∞ are not part of this mission.
  • Local maxima in 5.8 are stated with an explicit radius, matching Rudin's Definition 5.7.

Selected references

  • Walter Rudin, Principles of Mathematical Analysis, 3rd edition, McGraw-Hill, 1976, Chapter 5 (pp. 103–119).
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Control TheoryFunctional AnalysisMachine Learning·Captain: olivier

Universal Reservoir Computers from Non-Homogeneous State-Affine SystemsResearch Paper

Motivation

A reservoir computer learns a dynamical input/output relation with a recurrent network whose internal weights are fixed once and never trained; only a linear readout on the state is fitted. The method works in practice — it is a standard tool for learning chaotic dynamics — but its justification requires an approximation theorem: the family of reservoirs used must be rich enough to reach any reasonable target system.

The target class is fixed by fading memory, the continuity notion Boyd and Chua introduced in 1985 for the approximation of nonlinear operators: a filter has fading memory when inputs that agree on the recent past produce nearby present outputs, however much they differ long ago. The question is then which reservoir families are dense in that class.

Non-homogeneous state-affine systems are the family that answers it. They are affine in the state, with coefficients depending polynomially on the input, and the density result proved for them is what every later universality theorem for reservoir computing rests on — including the one for echo state networks, whose proof approximates a target filter by a state-affine system first and only then by a network.

Timeline.

  • 1985 — Boyd and Chua identify fading memory as the right continuity notion, and prove a universality result for Volterra series.
  • 2018 — Grigoryeva and Ortega prove that non-homogeneous state-affine systems with linear readouts are universal in the fading memory category, in discrete time and with uniformly bounded inputs.
  • 2018 — The same authors use that density result to prove that echo state networks are universal.

Setting

Time is indexed by the nonpositive integers, so an input has an infinite past and a present. Inputs are real-valued and bounded by one: the set IZ−I^{\mathbb{Z}_-}IZ−​ of sequences with zt∈[−1,1]z_t \in [-1,1]zt​∈[−1,1].

A non-homogeneous state-affine system is the reservoir

xt=p(zt) xt−1+q(zt),yt=W⊤xt,x_t = p(z_t)\,x_{t-1} + q(z_t), \qquad y_t = W^{\top} x_t ,xt​=p(zt​)xt−1​+q(zt​),yt​=W⊤xt​,

where ppp is a polynomial with N×NN \times NN×N matrix coefficients, qqq a polynomial with NNN-vector coefficients, and W∈RNW \in \mathbb{R}^NW∈RN the linear readout. Writing p(z)=∑jzjPjp(z) = \sum_j z^j P_jp(z)=∑j​zjPj​, the system is affine in the state and polynomial in the input.

Two constants govern it: Mp=max⁡z∈I∥p(z)∥2M_p = \max_{z \in I} \lVert p(z) \rVert_2Mp​=maxz∈I​∥p(z)∥2​ and Mq=max⁡z∈I∥q(z)∥2M_q = \max_{z \in I} \lVert q(z) \rVert_2Mq​=maxz∈I​∥q(z)∥2​. When Mp<1M_p < 1Mp​<1 the state map contracts, the system has the echo state property — exactly one bounded state sequence per input — and the states obey ∥xt∥≤Mq/(1−Mp)\lVert x_t \rVert \le M_q/(1 - M_p)∥xt​∥≤Mq​/(1−Mp​). The induced map from input history to present output is the SAS functional HWp,qH^{p,q}_WHWp,q​.

Formalization targets

Goal — state-affine systems are universal

∀ H with fading memory, ∀ε∈(0,1), ∃ p,q,W with Mp,Mq<1−ε:sup⁡z∣H(z)−HWp,q(z)∣<ε.\forall\, H \text{ with fading memory},\ \forall \varepsilon \in (0,1),\ \exists\, p,q,W \text{ with } M_p, M_q < 1-\varepsilon:\quad \sup_{z} \bigl| H(z) - H^{p,q}_W(z) \bigr| < \varepsilon .∀H with fading memory, ∀ε∈(0,1), ∃p,q,W with Mp​,Mq​<1−ε:zsup​​H(z)−HWp,q​(z)​<ε.

Any fading memory filter on uniformly bounded scalar inputs is approximated, uniformly over all such inputs, by a state-affine system read out linearly.

Supporting — the echo state property under a contracting polynomial

max⁡z∈I∥p(z)∥2<1  ⟹  exactly one bounded state sequence, with ∥xt∥≤Mq/(1−Mp).\max_{z \in I} \lVert p(z) \rVert_2 < 1 \;\Longrightarrow\; \text{exactly one bounded state sequence, with } \lVert x_t \rVert \le M_q/(1-M_p).z∈Imax​∥p(z)∥2​<1⟹exactly one bounded state sequence, with ∥xt​∥≤Mq​/(1−Mp​).

Significance

The result itself. It is the density theorem of reservoir computing. Without it, nothing guarantees that a reservoir family can represent the system one is trying to learn, and the practice of fitting only a linear readout has no theoretical backing. It is also the input to the universality theorem for echo state networks: that proof replaces the target filter by a state-affine system before replacing it by a network, so the present result is a prerequisite rather than a parallel statement.

Formalizing it. The supporting target is a specialization of a result already published on this platform: a state-affine system is a contracting reservoir map, so its echo state property follows from the abstract contraction theorem rather than from a new argument. What this mission adds beyond that is the density statement itself, which is of a different nature — an approximation theorem in a function space, not a fixed point argument.

Difficulty

The obvious approach to the goal is to exhibit an approximating system directly, and it fails: the target is an arbitrary fading memory filter, given by no formula, so no construction can be read off it. The proof is not constructive in that sense. It proceeds instead by showing that the family of SAS functionals is a polynomial algebra which separates points and contains the constants, and by applying a Stone-Weierstrass argument on a space of input sequences made compact by the weighted topology.

Two points resist. The compactness is not that of the supremum norm — the space of uniformly bounded sequences is not compact for it — but of the weighted norm, and it is that topology in which the approximation is obtained. And the algebra property is delicate: the product of two SAS functionals must again be one, which is what forces the non-homogeneous form. The corresponding statement fails for linear reservoirs, whose products leave the family.

Formalization scope

Time is indexed by N\mathbb{N}N, index kkk denoting the instant kkk steps into the past and k=0k = 0k=0 the present; the system equation reads xk=p(zk)xk+1+q(zk)x_k = p(z_k) x_{k+1} + q(z_k)xk​=p(zk​)xk+1​+q(zk​). This is a relabelling of the source's indexing, not a weakening.

Inputs are scalar, as in the source's Section 3, where the restriction is made explicit and the multidimensional extension deferred to a remark. Polynomials are given by their coefficient families, and evaluated as ∑jzjPj\sum_j z^j P_j∑j​zjPj​; the bounds MpM_pMp​ and MqM_qMq​ are stated as explicit operator and norm bounds valid on [−1,1][-1,1][−1,1] rather than through a maximum, so that any valid bound may be supplied.

The fading memory property of the target is the one already published on this platform, stated for a functional rather than a filter: the two are in linear bijection, so nothing is lost and causality and time-invariance need not be formalized separately.

One trivialization is ruled out. The goal quantifies over state sequences satisfying the system equation, and the supporting target is what guarantees such a sequence exists and is unique under the stated bounds; without it, the approximation claim could be read as vacuous.

A complete development needs the Stone-Weierstrass theorem, available in Mathlib, together with compactness of the weighted sequence space, which is not and has to be built. Contributions are welcome on both targets.

Selected references

  • L. Grigoryeva, J.-P. Ortega, Universal discrete-time reservoir computers with stochastic inputs and linear readouts using non-homogeneous state-affine systems, Journal of Machine Learning Research 19(24) (2018), 1–40. https://jmlr.org/papers/v19/18-020.html · https://arxiv.org/abs/1712.00754
  • L. Grigoryeva, J.-P. Ortega, Echo state networks are universal, Neural Networks 108 (2018), 495–508. https://doi.org/10.1016/j.neunet.2018.08.025 · https://arxiv.org/abs/1806.00797
  • S. Boyd, L. Chua, Fading memory and the problem of approximating nonlinear operators with Volterra series, IEEE Transactions on Circuits and Systems 32 (1985), 1150–1161. https://doi.org/10.1109/TCS.1985.1085649
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Algebra·Captain: mysticflounder

Equational Magmas: E677 → E255 (finite case)Open Problem

Motivation

An equation for a magma constrains a binary operation without assuming that it is associative, commutative, or has an identity. Which laws imply which others, over all magmas or over finite magmas only, is the question the Equational Theories Project studies at scale. Restricting the underlying set to be finite can change the answer: a structural argument may depend on the fact that a surjective self-map of a finite set is injective.

The project's December 2025 paper reports the finite implication from E677 to E255 as unresolved, while reporting a counterexample to the implication when infinite magmas are allowed. The paper also tentatively conjectures that a finite counterexample exists. This mission makes the affirmative implication its formal target and also accepts a rigorous refutation of the complete finite statement.

This mission treats the universal target as open. Supporting structural facts and conditional reductions are separately identified, so that progress on one does not assert completion of the target.

Setting

A magma here is a type α\alphaα with a total binary operation ⋄:α×α→α\diamond:\alpha\times\alpha\to\alpha⋄:α×α→α. Parentheses specify the order of evaluation throughout; no reassociation is permitted. The condition E677 means

∀x,y∈α,x=y⋄(x⋄((y⋄x)⋄y)).\forall x,y\in\alpha,\quad x=y\diamond\bigl(x\diamond((y\diamond x)\diamond y)\bigr).∀x,y∈α,x=y⋄(x⋄((y⋄x)⋄y)).

The condition E255 means

∀x∈α,x=((x⋄x)⋄x)⋄x.\forall x\in\alpha,\quad x=((x\diamond x)\diamond x)\diamond x.∀x∈α,x=((x⋄x)⋄x)⋄x.

These are the two laws used in Chapter 13 of the project blueprint. For a fixed element yyy, the left translation (left multiplication) map is Ly(x)=y⋄xL_y(x)=y\diamond xLy​(x)=y⋄x. A fixer of xxx is an element yyy with y⋄x=xy\diamond x=xy⋄x=x; it acts on xxx from the left. This definition concerns one element xxx; it does not require yyy to act as an identity on every element. The left orbit of xxx is the forward orbit x,Lx(x),Lx2(x),…x,L_x(x),L_x^2(x),\ldotsx,Lx​(x),Lx2​(x),… of xxx under its own left translation.

Formalization targets

The supporting targets expose the relevant distinction between a constraint on a possible fixer and the existence of a fixer. For every finite α\alphaα satisfying E677, the first supporting statement is

∀y∈α,Ly is bijective.\forall y\in\alpha,\quad L_y\text{ is bijective}.∀y∈α,Ly​ is bijective.

The second supporting statement determines any fixer:

∀x,y∈α,y⋄x=x ⟹ y=(x⋄x)⋄x.\forall x,y\in\alpha,\quad y\diamond x=x\ \Longrightarrow\ y=(x\diamond x)\diamond x.∀x,y∈α,y⋄x=x ⟹ y=(x⋄x)⋄x.

The third supporting statement is the backward recurrence

∀x,y∈α,x=(y⋄x)⋄((y⋄(y⋄x))⋄y).\forall x,y\in\alpha,\quad x=(y\diamond x)\diamond\bigl((y\diamond(y\diamond x))\diamond y\bigr).∀x,y∈α,x=(y⋄x)⋄((y⋄(y⋄x))⋄y).

These three statements are blueprint Lemma 13.1(i)–(iii) and are Proved on this platform. The following fixer-existence assertion is the same obligation as E255 under E677 and finiteness (blueprint Lemma 13.2); it is a reduction node, not a milestone:

∀x∈α,∃y∈α,y⋄x=x.\forall x\in\alpha,\quad\exists y\in\alpha,\quad y\diamond x=x.∀x∈α,∃y∈α,y⋄x=x.

The mission goal is

∀ finite magmas α,E677⁡(α) ⟹ E255⁡(α).\forall\text{ finite magmas }\alpha,\quad \operatorname{E677}(\alpha)\ \Longrightarrow\ \operatorname{E255}(\alpha).∀ finite magmas α,E677(α) ⟹ E255(α).

For finite E677 magmas, E255 at xxx supplies the fixer (x⋄x)⋄x(x\diamond x)\diamond x(x⋄x)⋄x; from any fixer yyy of xxx, Lemma 13.1(ii) gives y=(x⋄x)⋄xy=(x\diamond x)\diamond xy=(x⋄x)⋄x and hence E255 at xxx. Each direction is one line, so fixer existence is not a strictly weaker milestone.

Three open sub-goals come from the case split in the accepted reduction sketches for the fixer-existence node. Sub-goal 1 is orbit-local: for a fixed xxx, if two elements of the left orbit of xxx have equal right products by xxx, then they are equal or xxx has a fixer. Sub-goal 2 concerns the case of exactly one element AAA outside the left orbit of xxx, with xxx having no fixer: a right-translation collision c⋄x=A⋄xc\diamond x=A\diamond xc⋄x=A⋄x between an orbit point ccc and AAA must propagate to the orbit successor x⋄cx\diamond cx⋄c. Sub-goal 3 assumes x⋄x≠xx\diamond x\ne xx⋄x=x and at least two elements outside the left orbit: if right translation by xxx sends an orbit point outside the orbit, then xxx has a fixer. Sub-goal 3 is not a smaller case of the goal. If it holds for every finite E677 magma, the mission goal follows by a product construction (milestone "Sub-goal 3 support (a)"), and the mission goal gives Sub-goal 3 because E255 at xxx supplies the fixer (x⋄x)⋄x(x\diamond x)\diamond x(x⋄x)⋄x. So a proof of Sub-goal 3 alone proves the goal, and a route through Sub-goals 1 and 2 still needs Sub-goal 3. The D4 milestones specialize Sub-goal 1 to a left orbit of exact period four; D4.0, D4.1, D4.2 and D4.4a–e are Proved, and the series is open at D4.3 and its five branch closeouts D4.3a–e. One conditional result (E677 together with conjugacy-closed left translations implies E255; Padilla, 2026) is Proved on this platform. The milestone "Alternative resolution — a finite E677 counterexample to E255" (theorem finite_counterexample) is the disproof target. The sixteen milestones "Counterexample structure (a)–(p)" are constraints on a counterexample and rules for a counterexample search, all Proved; (h)–(j) take small-order facts as hypotheses. None of the sixteen is a disproof. None of the displayed statements restricts the cardinality to a tested range.

In the authors' repository, Sub-goal 1 is called Piece 1, the unique-outsider case containing Sub-goal 2 is called Gap 1, and the case of Sub-goal 3 is called Gap ≥ 2; those names appear in some theorem sources and file names.

Significance

A resolution determines whether this particular law gains E255 as a consequence upon restriction to finite carriers. An affirmative proof must cover every finite cardinality, every operation on each carrier, and every assignment of the universally quantified elements. A finite counterexample must supply an operation that satisfies every instance of E677 while failing E255 at some element.

The formal package provides small, reusable statements of the two laws, the left translation property, and the fixer constraint. Keeping these statements separate allows their precise hypotheses and conclusions to be checked individually. In particular, the second supporting result says what a fixer must be when one exists; the fixer-existence formulation records the additional mathematical content needed to ensure existence.

Difficulty

The left translation conclusion concerns maps with the left input fixed. The fixer-existence formulation instead asks about the image of the map y↦y⋄xy\mapsto y\diamond xy↦y⋄x, with its right input fixed. No assumption in the formal goal makes these two maps interchangeable. Bijectivity of every left translation map alone does not state that a fixer exists.

Because the implication fails for infinite magmas, E255 is not an equational consequence of E677, so any proof must use finiteness in an essential way. The blueprint's linear and linear-extension constructions cannot produce a finite counterexample (blueprint Lemmas 13.3 and 13.4); community members have formalized on this platform the scalar-coefficient case of the linear lemma, the Type I and Type II affine families, and the linear-extension lemma (see the discussion thread).

Likewise, checking a collection of finite operation tables does not quantify over arbitrary finite cardinalities. Such computation does not discharge the goal submitted here. Any proof must justify every use of finiteness and retain the displayed parenthesization of the laws.

Formalization scope

The representation uses an arbitrary universe-polymorphic type, an explicit binary operation, and a Fintype instance for finite targets. Passing the operation explicitly avoids importing a separate magma package or imposing algebraic typeclass laws. The predicates E677 and E255 themselves do not assume finiteness; each theorem states its own finite-carrier hypothesis.

Empty carriers are included. Both laws hold vacuously on them; the pointwise fixer statement is also vacuous because there is no element xxx. Consequently an empty carrier cannot refute the main goal. Nonempty carriers of every finite size are included without further assumptions. There is no associativity, commutativity, idempotence, identity element, or cancellation hypothesis hidden in the representation.

The definition bundle FiniteMagmaE677 provides E677, E255, HasFixerAt (existence of a fixer of xxx), InLeftOrbit (membership in the left orbit of xxx) and OrbitRightCollisionOrFixer. Three further bundles, FiniteMagmaE677_seventh_element_growth, FiniteMagmaE677_d4_first_return and FiniteMagmaE677_sswap_renewal, hold the period-four packet types used by the D4 milestones.

Status (2026-10-22 UTC). Proved on this platform: Lemma 13.1(i)–(iii), the Sub-goal 1, Sub-goal 2 and Sub-goal 3 support lemmas, D4.0, D4.1, D4.2, D4.4a–e, the conditional conjugacy-closure theorem, Counterexample structure (a)–(p), and three further conditional theorems by omegaestable (existential row transport, parametrized row transport, left-parameter transport; see the discussion thread). Open: Sub-goals 1–3, D4.3 with D4.3a–e, and the counterexample target. Community members have also formalized the blueprint's 496-element non-right-cancellative E677 magma (see the discussion thread).

Welcome contributions: a proof of any open sub-goal or D4.3 branch (a proof of Sub-goal 3 proves the goal; see the milestone "Sub-goal 3 support (a)"); a proof sketch that reduces an open leaf to new lemmas; a concrete operation table on Fin n proving finite_counterexample, which would make the main theorem false.

Results in the captain's private repository that are not on this platform

Results that are Proved on this platform are not repeated here. Readers cannot open the captain's private repository, so each statement is given in full. PROVEN means a complete proof, in the form stated. BOUNDED means a SAT-solver result for one encoded finite structure: each UNSAT result used here has a DRAT proof that drat-trim accepted (unverified C code, not a kernel-checked proof). EMPIRICAL means a computation over finite data, with no certificate.

Not ported

A port of these results to this platform is a long job.

1. The finite facts that Counterexample structure (h)–(j) take as hypotheses. BOUNDED. No E677 magma has order 2, 3, 4, 6 or 8, and every E677 magma of order 7 or 9 has an idempotent. Counterexample structure (h) and (j) give the earlier sources and the captain's check. These facts, except those for orders 2 and 3, are hypotheses of theorems that are Proved on this platform, so a port of them would make (h)–(j) unconditional; it needs kernel-checked proofs made from the DRAT certificates. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/idempotent-free-small-orders-2026-10-21/ and, for order 8, experiments/analysis/ti-groups-2026-10-19/ (section "Order 8").

2. Period-four refinements of D4.2. PROVEN (Lean; axioms propext, Classical.choice, Quot.sound). A repository theorem refines the five branches of the D4.2 first-return packet and keeps every case. Write q=c2⋄xq=c_2\diamond xq=c2​⋄x. In the R-through-one branch (the repository's name), each outcome is a fixer of xxx, a strict decrease of a finite contact budget, a new LxL_xLx​-cycle disjoint from the elements already accounted for (with its exact size), or a closed trace of Lq−1L_q^{-1}Lq−1​ that is reduced to two phase-contact families. In the two unswapped S branches, each outcome is a fixer of xxx, a decrease by one of the number of unmarked phases on the LxL_xLx​-cycle of qqq, or a new disjoint LxL_xLx​-cycle with its exact size. These results do not close D4.3 or any of D4.3a–e, because the outcomes are not yet combined into one state with a strictly decreasing well-founded measure. A port needs the repository's library of period-four packets. Source: the captain's private repository, revision 4100763b, lean/E677/Spine/Piece1D4RefinedFirstReturn.lean, e677_d4_q_refinedFirstReturnPacket_of_firstReturnPacket.

Not formalized

These results have only solver or computation evidence, and no Lean proof, and no milestone on this platform uses them as hypotheses.

3. A counterexample has at least 11 elements. BOUNDED. Every E677 magma with at most 10 elements satisfies E255. By item 1, no E677 magma has order 2, 3, 4, 6 or 8. Every E677 magma of order 5, 7 or 9 is right-cancellative; then each right translation y↦y⋄xy\mapsto y\diamond xy↦y⋄x is a bijection, so xxx has a fixer, and Lemma 13.1(ii) gives E255 at xxx. At order 10, a point xxx at which E255 fails has no fixer, so xxx is not in its own column {y⋄x}\{y\diamond x\}{y⋄x}; a search for such a table, split into 67 cases by the cycle type of LxL_xLx​ (the length l≥2l\ge 2l≥2 of the left orbit of xxx, and the cycle lengths of LxL_xLx​ on the other 10−l10-l10−l elements), is UNSAT in each case. Earlier reports: the sources listed in Counterexample structure (h)–(j) for the E677 magmas of orders 2–4 and 6–9, among them a Lean proof for order 6 by J. Hyun. Without certificates (ETP Zulip thread "FINITE: 677 -> 255"): J. Brox (Mace4) reports no counterexample of order 9 (2024-12-10), none of order at most 10 (2025-01-10), no E677 magma of order 10 (2025-01-12) and no counterexample of order 11 (2025-03-12); B. Le Floch (2024-12-22, Mace4) reports none of order at most 9; J. Hyun (2025-01-09, CaDiCaL) none of order 5 to 8; S. Chuks-Onah (2026-05-01, Z3) none of order 5 or 6; R. Schneider (2026-05-15, own search program) and B. Subercaseaux (2026-05-15, SAT) none of order at most 11. The new content here is the DRAT certificates. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/rc-small-orders-2026-10-19/ and experiments/analysis/rc-cubes-2026-10-19/.

4. Order 35 over the quotient x⋄y=4x+3yx\diamond y=4x+3yx⋄y=4x+3y on F7\mathbb{F}_7F7​. With the order-7 fact of item 1, Counterexample structure (i) gives: if a minimum counterexample MMM has order 35 and a non-universal congruence θ\thetaθ that relates zzz and q(z)q(z)q(z), then M/θM/\thetaM/θ has 7 elements and an idempotent, and the classes have 5 elements. By the classification of J. Brox (ETP Zulip thread "FINITE: 677 -> 255", 2025-03-26, Mace4, no certificate; not checked by the captain), M/θM/\thetaM/θ is then isomorphic to 4x+3y4x+3y4x+3y or to 4x+y4x+y4x+y on F7\mathbb{F}_7F7​. Take QQQ: x⋄y=4x+3yx\diamond y=4x+3yx⋄y=4x+3y on F7\mathbb{F}_7F7​ (0 is its only idempotent), write the elements of MMM as pairs (a,s)(a,s)(a,s) with a∈F7a\in\mathbb{F}_7a∈F7​ and s∈F5s\in\mathbb{F}_5s∈F5​, and call the map (s,t)↦(s,t)\mapsto(s,t)↦ (second coordinate of (a,s)⋄(b,t)(a,s)\diamond(b,t)(a,s)⋄(b,t)) the block over (a,b)(a,b)(a,b). Results, each for an E677 magma of this form:

  • If at most five blocks other than the block over (0,0)(0,0)(0,0) do not have the form (s,t)↦s+fab(t−s)(s,t)\mapsto s+f_{ab}(t-s)(s,t)↦s+fab​(t−s) with a permutation fabf_{ab}fab​ of F5\mathbb{F}_5F5​, then E255 holds. BOUNDED (two short paper lemmas reduce it to 48 patterns of non-cyclic blocks, each UNSAT). This includes the case where every block has this form.
  • If every block has the form (s,t)↦A t+B(s,t)\mapsto A\,t+B(s,t)↦At+B with A∈{1,4}A\in\{1,4\}A∈{1,4} (with AAA and BBB chosen for each block and each sss), then E255 holds. BOUNDED.
  • With all blocks free, the solver runs did not finish, so there is no result. The quotient 4x+y4x+y4x+y was not tested.

The only known E677 magma of order 35 with this quotient and classes of 5 elements is isomorphic to Q×M5Q\times M_5Q×M5​, where M5M_5M5​ is s⋄t=2s−ts\diamond t=2s-ts⋄t=2s−t on F5\mathbb{F}_5F5​ (EMPIRICAL). T. Tao (ETP Zulip thread "FINITE: 677 -> 255", 2024-12-13) proposed the extensions (x,s)⋄(y,t)=(4x+3y, s⋄x,yt)(x,s)\diamond(y,t)=(4x+3y,\ s\diamond_{x,y}t)(x,s)⋄(y,t)=(4x+3y, s⋄x,y​t), and (same thread, 2024-12-22) the fibre operations s+fx,y(t−s)s+f_{x,y}(t-s)s+fx,y​(t−s) of the first result. The second result is a case of the form (x⋄y, bx,y,st+cx,y,s)(x\diamond y,\ b_{x,y,s}t+c_{x,y,s})(x⋄y, bx,y,s​t+cx,y,s​) for which B. Reinke (same thread, 2026-06-11) expected E255 to lift, without a proof. Source: the captain's private repository, revision dd2ee3e5, docs/current/e677-coverage-matrix-2026-10-19.md (the rows for this quotient) and experiments/analysis/pro-counterexample-audit-2026-10-20/.

5. Extensions and row changes of the order-31 magma x⋄y=5x−4y+1x\diamond y=5x-4y+1x⋄y=5x−4y+1 on F31\mathbb{F}_{31}F31​. Call it Q31Q_{31}Q31​. It has no idempotent, and it is the smallest known E677 magma without an idempotent; every known E677 magma without an idempotent has order divisible by 31 (EMPIRICAL). So Q31Q_{31}Q31​ is the smallest known candidate quotient in Counterexample structure (j). BOUNDED results:

  • No E677 magma has a congruence with quotient Q31Q_{31}Q31​ and classes of 2 or 3 elements.
  • No E677 magma with a congruence with quotient Q31Q_{31}Q31​ and classes of 4 elements fails E255.
  • In the family (u,s)⋄(w,t)=(5u−4w+1, s+hw−u(t−s))(u,s)\diamond(w,t)=(5u-4w+1,\ s+h_{w-u}(t-s))(u,s)⋄(w,t)=(5u−4w+1, s+hw−u​(t−s)) on F31×F5\mathbb{F}_{31}\times\mathbb{F}_5F31​×F5​, with permutations hdh_dhd​ of F5\mathbb{F}_5F5​, no E677 member fails E255.
  • An E677 operation on F31\mathbb{F}_{31}F31​ that fails E255 differs from Q31Q_{31}Q31​ in at least 20 rows and at least 40 cells.

B. Le Floch (ETP Zulip thread "FINITE: 677 -> 255", 2024-12-13) found 5x−4y+c5x-4y+c5x−4y+c mod 31 as the one linear E677 model in which ccc cannot be removed, and R. Schneider (same thread, 2025-11-21) noted that Q31Q_{31}Q31​ has no idempotent. T. Tao (same thread, 2024-12-13) proposed the extensions (x,s)⋄(y,t)=(x⋄y, s⋄y−xt)(x,s)\diamond(y,t)=(x\diamond y,\ s\diamond_{y-x}t)(x,s)⋄(y,t)=(x⋄y, s⋄y−x​t) of Q31Q_{31}Q31​. B. Reinke (same thread, 2025-11-07) encoded them for z3 and wrote that he thought he could exclude classes of fewer than 4 elements (no certificate). The first result above covers all extensions with classes of 2 or 3 elements, not only these; the third result is the case of Tao's extensions with fibre operations s+h(t−s)s+h(t-s)s+h(t−s). Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/gap2-monolith-m3-2026-10-17/ (§2, §6), experiments/analysis/pro-counterexample-audit-2026-10-20/ (cyclic-section-19375/, construction-19350/) and experiments/analysis/idempotent-free-2026-10-19/.

6. Tables with an automorphism of prime order, orders 12–21. BOUNDED, incomplete. Let α\alphaα be an automorphism of prime order ppp of an E677 magma of order nnn, 12≤n≤2112\le n\le 2112≤n≤21, with fff fixed points, and let zzz be a point with no fixer. The fixed points of α\alphaα form a submagma, so an E677 magma of order fff; by item 1, f∉{2,3,4,6,8}f\notin\{2,3,4,6,8\}f∈/{2,3,4,6,8}. The search covers f∈{0,1,5,7,9,11}f\in\{0,1,5,7,9,11\}f∈{0,1,5,7,9,11}. If α\alphaα fixes zzz, the fixed points form an E677 magma of order fff that fails E255 at zzz; this is excluded for f≤9f\le 9f≤9 by item 3, and for f=11f=11f=11 4 shapes (n,p,f)(n,p,f)(n,p,f) are UNSAT and 7 were not run. If zzz is in a cycle of α\alphaα, 26 shapes are UNSAT (all 9 shapes with p≥11p\ge 11p≥11, and 17 shapes with p≤7p\le 7p≤7); 14 shapes are UNKNOWN after 3600 s, and 40 were not run. Not covered: the shapes with f=0f=0f=0 and one cycle (n=p∈{13,17,19}n=p\in\{13,17,19\}n=p∈{13,17,19}, translation-invariant tables on Zn\mathbb{Z}_nZn​), fixed-point count 10, and fixed-point counts of at least 12. Earlier searches without certificates (ETP Zulip thread "FINITE: 677 -> 255"): R. Schneider (2025-11-20 and 2025-11-21) searched the tables with the automorphism (0)(1 2 … n−1)(0)(1\,2\,\dots\,n-1)(0)(12…n−1) up to n=31n=31n=31 and found only right-cancellative ones (the shapes with f=1f=1f=1 and one cycle); B. Reinke (2025-11-21) noted that the fixed points form a submagma and found no table with one cycle and 5 fixed points of order at most 25 other than order 5 (the shapes with f=5f=5f=5 and one cycle), and (2025-11-26) noted that in a minimum counterexample only the identity automorphism fixes the failing point. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/symmetric-simple-2026-10-20/.

7. A refuted intermediate statement. EMPIRICAL (exhaustive check of one explicit table, run twice with independent encodings; not kernel-checked). Let S(x)S(x)S(x) be the closure of the left orbit of xxx under z↦z⋄xz\mapsto z\diamond xz↦z⋄x. The repository's gate CP asserted: in a finite E677 magma, if the hypotheses of Sub-goal 3 hold at xxx and z↦z⋄xz\mapsto z\diamond xz↦z⋄x is not injective on S(x)S(x)S(x), then the left orbit of xxx has minimal period 777. Let KKK be the 7-element E677 magma of Sub-goal 3 support (a) (file db/7/1 of the public collection memoryleak47/eq677), and let MMM be the E677 magma of order 777777 in file db/77/65 of the same collection. In M×KM\times KM×K (order 539539539; E677 checked on all 5392539^25392 pairs), the point (0,0)(0,0)(0,0) satisfies these hypotheses, and its left orbit has minimal period lcm⁡(7,6)=42\operatorname{lcm}(7,6)=42lcm(7,6)=42. The point (0,0)(0,0)(0,0) has the fixer (76,4)(76,4)(76,4), so this is not a counterexample to E255, and it refutes CP only in the form without a no-fixer hypothesis. Source: the captain's private repository, revision 4100763b, docs/current/dead-ends/gap-ge-2.md, entry D7-6.

8. Φ(x)=(x⋄x)⋄x\Phi(x)=(x\diamond x)\diamond xΦ(x)=(x⋄x)⋄x is not injective in general. EMPIRICAL. In the 2026-09-27 snapshot of the community database (4091 tables), every table satisfies E255, and Φ\PhiΦ is not injective in 1107 of them; the smallest such order is 777. In one table of order 7, row 6 is the identity row, so 666 is a fixer of every xxx and Lemma 13.1(ii) gives Φ(x)=6\Phi(x)=6Φ(x)=6 for every xxx. So global injectivity of Φ\PhiΦ is not a usable intermediate target. Source: the captain's private repository, revision 4100763b, docs/professor-phi-injectivity.md, correction of 2026-10-14.

Selected references

  • Matthew Bolan et al., The Equational Theories Project: Advancing Collaborative Mathematical Research at Scale, arXiv:2512.07087v2 (December 16, 2025), paper.
  • The Equational Theories Project contributors, Equational Theories, online proof blueprint, Chapter 13, equations (1)–(2) and Lemmas 13.1–13.4, chapter, accessed September 7, 2026 and October 13, 2026.
  • J. I. Padilla (GitHub: omegaestable), Prove E677 implies E255 under left translation conjugacy closure, Equational Theories Project pull request #1518, 2026 (closed without merge by its author on 2026-10-13; the theorem is Proved on this platform), pull request.
  • Lean Zulip, channel "Equational", thread "FINITE: 677 -> 255", thread.
54 thms4 active usersReviewed
Computational GeometryDiscrete GeometryGraph Theory·Captain: hao jia

Uniform Obstacle Bounds for Planar Graphs (OPG-37357)Open Problem

Motivation

An obstacle representation turns a graph into a visibility system: vertices are points in the plane, and nonedges are blocked by polygonal obstacles. The obstacle number asks for the minimum number of obstacles needed. OPG-37357 records two different questions for planar graphs. The first asks whether one obstacle can ever be insufficient. The second asks whether some universal constant bounds the ordinary obstacle number of every planar graph.

The status of the two parts is different. Berman, Chappell, Faudree, Gimbel, Hartman, and Williams proved in 2017 that explicit planar graphs, including the icosahedron and their graphs X4X_4X4​ and X6X_6X6​, have ordinary obstacle number two. Thus the first question has a published positive answer. The universal-constant question remains the research target here. A separate invariant called planar or plane obstacle number requires a crossing-free visibility drawing; results for that invariant must not be substituted for the ordinary obstacle number used by this mission.

Setting

A finite simple graph GGG has a kkk-obstacle drawing when its vertices are placed injectively as points in R2\mathbb R^2R2 and there are kkk pairwise disjoint closed connected polygonal obstacles such that

uv∈E(G)⟺[p(u),p(v)] meets no obstacle.uv\in E(G) \quad\Longleftrightarrow\quad [p(u),p(v)]\text{ meets no obstacle}.uv∈E(G)⟺[p(u),p(v)] meets no obstacle.

Graph vertices lie outside every obstacle. The ordinary obstacle number obs⁡(G)\operatorname{obs}(G)obs(G) is the least such kkk. The drawing itself may contain crossings between visible graph edges; planarity is a property of the abstract input graph, not an extra constraint on the obstacle drawing.

The Lean model represents a polygonal obstacle as a connected finite union of closed filled triangles. This gives a compact polygonal region with exact real-coordinate segment incidence. Straight-line planarity of the abstract graph is represented separately.

Formalization targets

The two-part OPG record

The source records both

∃ finite planar G, obs⁡(G)>1\exists\text{ finite planar }G,\ \operatorname{obs}(G)>1∃ finite planar G, obs(G)>1

and

∃k∈N ∀ finite planar H, obs⁡(H)≤k.\exists k\in\mathbb N\ \forall\text{ finite planar }H, \ \operatorname{obs}(H)\le k.∃k∈N ∀ finite planar H, obs(H)≤k.

The first assertion is known in the literature and appears as a published-result milestone. The second is open and is therefore the mission's main theorem. Together they preserve the two-part source without presenting the whole record as unresolved.

Published first part

A milestone formalizes the stronger published statement

∃ finite planar G,obs⁡(G)≤2andobs⁡(G)≰1.\exists\text{ finite planar }G, \qquad \operatorname{obs}(G)\le2 \quad\text{and}\quad \operatorname{obs}(G)\not\le1.∃ finite planar G,obs(G)≤2andobs(G)≤1.

This captures ordinary obstacle number exactly two without hard-coding one graph before its adjacency data and lower-bound certificate are formalized.

Universal bound

The open milestone asks for a single natural number kkk, chosen before the graph, that works for every finite planar graph. The number of obstacle corners is not bounded by this theorem; only the number of connected polygonal obstacles is.

Significance

The published first part establishes that planarity alone does not force a one-obstacle representation. The second part asks whether planar graphs nevertheless have uniformly bounded visibility complexity. A positive answer would produce a common finite obstacle budget independent of graph order; a negative answer would require a family of planar graphs with unbounded ordinary obstacle number.

Formalization is especially useful because several nearby notions differ by one word but have different known bounds: ordinary versus plane obstacle number, arbitrary polygonal versus convex obstacles, and fixed-placement versus freely chosen drawings. The mission's definitions make those choices explicit and provide reusable segment-obstacle semantics for later geometric graph formalizations.

Difficulty

A finite combinatorial graph does not come with a canonical visibility drawing. Even when one starts with an arbitrary connected blocking set, replacing it by one bounded simple polygon requires compactness, component, incidence, and polygonal-neighborhood arguments. Conversely, lower bounds must quantify over every possible placement and obstacle, not merely refute a selected coordinate drawing.

Counting results for unrestricted graphs do not automatically preserve planarity. Bounds for planar obstacle number impose a crossing-free drawing and therefore answer a different question. The known two-obstacle examples close only the existential first part and give no universal kkk.

Formalization scope

All graph vertex types are finite. Obstacles are closed connected polygonal regions represented by finite triangle unions; they are pairwise disjoint and avoid graph vertices. Visibility uses the full closed segment, so tangency or boundary contact blocks a nonedge. The planarity witness is independent of the obstacle drawing. Empty and one-vertex graphs remain in the universal quantifier and should be handled without division or nonemptiness assumptions.

The repository's fixed-placement polygonization argument and finite arrangement code are candidate_only. They may motivate supporting lemmas, but they neither prove the unrestricted obstacle-drawing completeness theorem nor settle the universal bound. Contributions are welcome on exact geometry primitives, the published two-obstacle construction and lower bound, conversions between connected blockers and polygonal obstacles, and the universal root. A proof for the plane invariant, convex invariant, one fixed drawing, or a finite order cutoff must be labeled at that narrower scope.

Selected references

  • L. W. Berman, G. G. Chappell, J. R. Faudree, J. Gimbel, C. Hartman, and G. I. Williams, Graphs with Obstacle Number Greater than One, JGAA 21(6), 2017. https://doi.org/10.7155/jgaa.00452
  • J. Gimbel, P. Ossona de Mendez, and P. Valtr, Obstacle Numbers of Planar Graphs, Graph Drawing 2017. https://arxiv.org/abs/1706.06992
  • M. Balko, S. Chaplick, R. Ganian, S. Gupta, M. Hoffmann, P. Valtr, and A. Wolff, Bounding and Computing Obstacle Numbers of Graphs, SIAM Journal on Discrete Mathematics 38(2), 2024. https://arxiv.org/abs/2206.15414
  • Open Problem Garden / UnsolvedMath, OPG-37357. https://www.unsolvedmath.com/problems/OPG-37357
6 thms4 active usersReviewed
CombinatoricsGraph TheoryOptimization·Captain: hao jia

Clique Partitions of Chordal Graphs (Erdos Problem 81)Open Problem

Motivation

An edge partition into cliques compresses the adjacency structure of a graph into complete pieces without allowing any edge to be counted twice. Erdős Problem 81 asks for the asymptotically sharp upper bound on the number of pieces needed when the graph is chordal. Chordal graphs have strong elimination structure, but that structure does not make the partition parameter additive under arbitrary edge deletion, and obtaining a linear error term remains substantially stronger than identifying the leading quadratic coefficient.

Erdős, Ordman, and Zalcstein studied clique partitions of chordal graphs in 1993. Their examples already exhibit the n2/6n^2/6n2/6 scale, while their general upper estimate had a larger quadratic coefficient. Later dense-packing results of Haxell–Rödl and Yuster compare fractional and integer triangle packings with an o(n2)o(n^2)o(n2) gap. The project candidate combines that interface with chordal elimination arguments to formulate a uniform n2/6+o(n2)n^2/6+o(n^2)n2/6+o(n2) milestone. It does not supply the O(n)O(n)O(n) remainder asked for by the root.

Setting

A finite simple graph is chordal when it has no induced cycle of length greater than three. The Lean definition uses the equivalent perfect-elimination form: vertices admit an injective ranking such that the later neighbors of every vertex form a clique.

An edge partition into cliques is a finite family P\mathcal PP of complete vertex sets such that every edge of GGG belongs to exactly one member of P\mathcal PP. Members may share vertices but may not share edges. Write cp⁡(G)\operatorname{cp}(G)cp(G) for the minimum possible number of pieces.

The asymptotic notation

n26+O(n)\frac{n^2}{6}+O(n)6n2​+O(n)

means that there are constants C>0C>0C>0 and n0≥1n_0\ge1n0​≥1, chosen independently of GGG and nnn, such that every chordal nnn-vertex graph with n≥n0n\ge n_0n≥n0​ has a clique partition with at most n2/6+Cnn^2/6+Cnn2/6+Cn pieces.

Formalization targets

Erdős Problem 81

The root theorem is

∃C>0 ∃n0≥1 ∀n≥n0 ∀G chordal on n vertices,cp⁡(G)≤n26+Cn.\exists C>0\ \exists n_0\ge1\ \forall n\ge n_0\ \forall G\text{ chordal on }n\text{ vertices}, \qquad \operatorname{cp}(G)\le \frac{n^2}{6}+Cn.∃C>0 ∃n0​≥1 ∀n≥n0​ ∀G chordal on n vertices,cp(G)≤6n2​+Cn.

The quantifier order is essential: CCC and n0n_0n0​ are universal and cannot depend on the graph.

Leading-coefficient milestone

The supporting target records the weaker uniform statement

∀ε>0 ∃n0 ∀n≥n0 ∀G chordal on n vertices,cp⁡(G)≤(16+ε)n2.\forall\varepsilon>0\ \exists n_0\ \forall n\ge n_0\ \forall G\text{ chordal on }n\text{ vertices}, \qquad \operatorname{cp}(G)\le \left(\frac16+\varepsilon\right)n^2.∀ε>0 ∃n0​ ∀n≥n0​ ∀G chordal on n vertices,cp(G)≤(61​+ε)n2.

This is the precise n2/6+o(n2)n^2/6+o(n^2)n2/6+o(n2) form. It is not equivalent to the root: choosing ε=1/n\varepsilon=1/nε=1/n is invalid because the cutoff may depend on the fixed value of ε\varepsilonε.

Significance

The root would determine the clique-partition extremum for chordal graphs up to a linear remainder, matching the scale of the complete-split examples that motivate the coefficient 1/61/61/6. It would refine a leading-order asymptotic theorem into a uniform estimate strong enough to distinguish second-order behavior.

Formalization creates a clean interface among perfect elimination orderings, exact edge partitions, fractional edge-and-triangle decompositions, and integer triangle packings. It also forces the proof to distinguish a partition from a cover and original graph order from the order of any auxiliary hypergraph. These definitions can support other decomposition problems on chordal and split graphs.

Difficulty

Perfect elimination does not by itself give the sharp partition count. Greedily taking maximal cliques may overlap in edges or accumulate too many singleton pieces. Similarly, a fractional edge-and-triangle partition can achieve the right leading coefficient while integer rounding loses o(n2)o(n^2)o(n2) pieces; the root requires that loss to be only O(n)O(n)O(n).

The dense-packing theorem has quantifiers of the form “for every fixed ε>0\varepsilon>0ε>0 there exists N(ε)N(\varepsilon)N(ε).” It therefore yields a uniform subquadratic error but no linear error. Any proof of the root must add a chordal-specific rounding or extremal reduction rather than treating the general packing theorem as if its ε\varepsilonε could vary with nnn.

Formalization scope

Graphs are finite and simple. Chordality is encoded by existence of a perfect-elimination ranking, including disconnected and edgeless graphs. A clique piece is a finite vertex set that spans a complete subgraph. Exactness means every actual edge occurs in exactly one piece; no nonedge can occur inside a piece. Bounds are compared in R\mathbb RR so the displayed asymptotic expressions retain their conventional form, while the number of parts remains a natural number.

The candidate derivation of the leading coefficient imports finite linear-programming duality and the Haxell–Rödl/Yuster fixed-triangle packing approximation. It is candidate_only, not an admitted result or kernel proof. Contributions may formalize the perfect-elimination lemmas, the fractional compression, the uniform packing interface, complete-split lower examples, or the root linear rounding theorem. A result for edge-and-triangle pieces only, a fractional partition, or one fixed order must not be presented as the unrestricted integer clique-partition theorem.

Selected references

  • P. Erdős, E. T. Ordman, and Y. Zalcstein, Clique Partitions of Chordal Graphs, Combinatorics, Probability and Computing 2(4), 1993. https://doi.org/10.1017/S0963548300000808
  • P. E. Haxell and V. Rödl, Integer and Fractional Packings in Dense Graphs, Combinatorica 21, 2001. https://doi.org/10.1007/s004930170003
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  • Erdős Problems, Problem 81. https://www.erdosproblems.com/81
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Partial Differential EquationsPure Mathematics·Captain: korbonits

Formalize Navier-StokesOpen Problem

Motivation

The incompressible Navier–Stokes equations are the standard model for the motion of a viscous fluid such as water or air, used daily in engineering, meteorology and oceanography. Yet the most basic mathematical question about them is open: starting from smooth initial data in three dimensions, does a smooth solution exist for all time? This is one of the seven Millennium Prize Problems of the Clay Mathematics Institute. Its official formulation is Charles Fefferman's problem description, Existence and smoothness of the Navier–Stokes equation (2000), which offers a prize for a proof of any one of four statements: global existence and smoothness on R3\mathbb{R}^3R3 (statement (A)) or on the torus R3/Z3\mathbb{R}^3/\mathbb{Z}^3R3/Z3 (statement (B)), or a counterexample to either (statements (C) and (D)). This mission formalizes statement (A), together with the classical partial results that Fefferman lists as known.

Timeline.

  • 1822–1845: Navier and Stokes write down the equations of a viscous incompressible fluid.
  • 1934: Jean Leray, Sur le mouvement d'un liquide visqueux emplissant l'espace (Acta Math. 63), proves on R3\mathbb{R}^3R3 that smooth solutions exist for a positive time depending on the data, that they exist for all time when the data is small compared with the viscosity, and that global weak solutions with finite energy always exist. Their smoothness and uniqueness are left open.
  • 1933–1969: the two-dimensional problem is settled (Leray for the plane; Olga Ladyzhenskaya's monograph The Mathematical Theory of Viscous Incompressible Flow, 2nd ed. 1969, for bounded domains): smooth solutions exist for all time and are unique.
  • 1984: Tosio Kato, Strong LpL^pLp-solutions of the Navier–Stokes equation in Rm\mathbb{R}^mRm (Math. Z. 187), gives global solutions for initial data small in L3(R3)L^3(\mathbb{R}^3)L3(R3).
  • 1976–1998: partial regularity. Scheffer, then Caffarelli, Kohn and Nirenberg (Comm. Pure Appl. Math. 35, 1982), show that the singular set of a suitable weak solution has one-dimensional parabolic Hausdorff measure zero.
  • 2000: the Clay Mathematics Institute adopts Fefferman's formulation as a Millennium Prize Problem. It remains open.

Setting

Fix a dimension n≥1n \ge 1n≥1 and write Rn\mathbb{R}^nRn for Euclidean nnn-space with its Euclidean norm ∣x∣|x|∣x∣; in Lean this is NavierStokes.Vec n. A velocity field assigns to each time t∈Rt \in \mathbb{R}t∈R and point x∈Rnx \in \mathbb{R}^nx∈Rn a vector u(x,t)∈Rnu(x,t) \in \mathbb{R}^nu(x,t)∈Rn; in Lean u tu\,tut is the field at time ttt and u t xu\,t\,xutx is Fefferman's u(x,t)u(x,t)u(x,t). A pressure is a real function p(x,t)p(x,t)p(x,t). The viscosity ν\nuν is a positive constant. The external force of Fefferman's equation (1) is identically zero throughout, as in statement (A).

For a vector field v:Rn→Rnv : \mathbb{R}^n \to \mathbb{R}^nv:Rn→Rn the divergence is

div⁡v=∑i=1n∂vi∂xi,\operatorname{div} v = \sum_{i=1}^n \frac{\partial v_i}{\partial x_i},divv=i=1∑n​∂xi​∂vi​​,

in Lean NavierStokes.div, computed from the Fréchet derivative Dv(x)Dv(x)Dv(x) as ∑i(Dv(x) ei)i\sum_i (Dv(x)\,e_i)_i∑i​(Dv(x)ei​)i​. The Laplacian Δv=∑i∂2v/∂xi2\Delta v = \sum_i \partial^2 v/\partial x_i^2Δv=∑i​∂2v/∂xi2​ acts componentwise (Mathlib's Laplacian on inner product spaces). The gradient ∇p\nabla p∇p is Mathlib's gradient. The convective term ∑juj ∂u/∂xj\sum_j u_j\,\partial u/\partial x_j∑j​uj​∂u/∂xj​ is the derivative of u(⋅,t)u(\cdot,t)u(⋅,t) at xxx in the direction u(x,t)u(x,t)u(x,t). Finally ∣∇v∣2=∑i,j(∂vi/∂xj)2|\nabla v|^2 = \sum_{i,j} (\partial v_i/\partial x_j)^2∣∇v∣2=∑i,j​(∂vi​/∂xj​)2 is NavierStokes.gradNormSq.

Admissible initial data (Fefferman's condition (4), NavierStokes.IsInitialData): a C∞C^\inftyC∞, divergence-free vector field u0u^0u0 that decays together with all its derivatives faster than any power,

∣∂xαu0(x)∣≤CαK (1+∣x∣)−Kon Rn, for every α and K.|\partial_x^\alpha u^0(x)| \le C_{\alpha K}\,(1+|x|)^{-K} \quad \text{on } \mathbb{R}^n, \text{ for every } \alpha \text{ and } K.∣∂xα​u0(x)∣≤CαK​(1+∣x∣)−Kon Rn, for every α and K.

In Lean the bound is (1+∣x∣)K ∥Dku0(x)∥≤CkK(1+|x|)^K\,\|D^k u^0(x)\| \le C_{kK}(1+∣x∣)K∥Dku0(x)∥≤CkK​ on the kkk-th Fréchet derivative, an equivalent family of conditions. These are exactly the divergence-free Schwartz functions.

A physically reasonable solution on a set SSS of times (NavierStokes.IsSolutionOn; S=[0,∞)S = [0,\infty)S=[0,∞) for NavierStokes.IsSolution) is a pair (u,p)(u,p)(u,p) such that

  1. (Fefferman (6)) uuu and ppp are C∞C^\inftyC∞ on S×RnS \times \mathbb{R}^nS×Rn, up to the boundary of SSS;
  2. (Fefferman (1), f≡0f \equiv 0f≡0) for every t∈St \in St∈S with t>0t > 0t>0 and every xxx,
∂u∂t+∑j=1nuj∂u∂xj=ν Δu−∇p;\frac{\partial u}{\partial t} + \sum_{j=1}^n u_j \frac{\partial u}{\partial x_j} = \nu\,\Delta u - \nabla p;∂t∂u​+j=1∑n​uj​∂xj​∂u​=νΔu−∇p;
  1. (Fefferman (2)) div⁡u(⋅,t)=0\operatorname{div} u(\cdot,t) = 0divu(⋅,t)=0 for every t∈St \in St∈S;
  2. (Fefferman (3)) u(x,0)=u0(x)u(x,0) = u^0(x)u(x,0)=u0(x);
  3. (Fefferman (7), bounded energy) ∫Rn∣u(x,t)∣2 dx<C\int_{\mathbb{R}^n} |u(x,t)|^2\,dx < C∫Rn​∣u(x,t)∣2dx<C for all t∈St \in St∈S, for some constant CCC.

Formalization targets

Goal: Fefferman's statement (A)

Take ν>0\nu > 0ν>0 and n=3n = 3n=3. For every admissible initial datum u0u^0u0 there exist a velocity field uuu and a pressure ppp forming a physically reasonable solution on R3×[0,∞)\mathbb{R}^3 \times [0,\infty)R3×[0,∞):

∀ ν>0, ∀ u0 satisfying (4), ∃ (u,p) satisfying (1), (2), (3), (6), (7) on R3×[0,∞).\forall\, \nu > 0,\ \forall\, u^0 \text{ satisfying (4)},\ \exists\, (u,p) \text{ satisfying (1), (2), (3), (6), (7) on } \mathbb{R}^3 \times [0,\infty).∀ν>0, ∀u0 satisfying (4), ∃(u,p) satisfying (1), (2), (3), (6), (7) on R3×[0,∞).

This is NavierStokes.existence_and_smoothness_R3. It is open; a proof would settle the Millennium Prize Problem in the affirmative.

Milestones: what Fefferman lists as known

  1. Local existence (NavierStokes.local_existence_R3): for n=3n = 3n=3 and every admissible u0u^0u0 there are T>0T > 0T>0 and a physically reasonable solution on R3×[0,T)\mathbb{R}^3 \times [0,T)R3×[0,T). Fefferman: "(A) and (B) hold ... if the time interval [0,∞)[0,\infty)[0,∞) is replaced by a small time interval [0,T)[0,T)[0,T), with TTT depending on the initial data."
  2. Global existence for small data (NavierStokes.small_data_global_existence_R3): there is an absolute constant c>0c > 0c>0 such that, for n=3n = 3n=3, (A) holds for every admissible u0u^0u0 with
∥u0∥L22 ∥∇u0∥L22≤c ν4.\|u^0\|_{L^2}^2\,\|\nabla u^0\|_{L^2}^2 \le c\,\nu^4.∥u0∥L22​∥∇u0∥L22​≤cν4.

Fefferman: "(A) and (B) hold provided the initial velocity u0u^0u0 satisfies a smallness condition." The scale-invariant product is Leray's form of the condition; it implies smallness of ∥u0∥L3/ν\|u^0\|_{L^3}/\nu∥u0∥L3​/ν, so Kato's theorem also applies. 3. The two-dimensional case (NavierStokes.existence_and_smoothness_R2): statement (A) with n=2n = 2n=2. Fefferman: "In two dimensions, the analogues of assertions (A) and (B) have been known for a long time (Ladyzhenskaya)."

A bridging lemma, NavierStokes.isInitialData_iff_schwartz, identifies the admissible data with the divergence-free elements of Mathlib's Schwartz space.

Significance

The result itself. Statement (A) asks whether the basic model of viscous flow is well posed in the classical sense, i.e. whether smooth finite-energy flows can develop singularities in finite time. A positive answer shows the equations never leave the classical regime; a negative one shows the model predicts its own breakdown. Fefferman: "since we don't even know whether these solutions exist, our understanding is at a very primitive level."

Formalizing it. None of the results in this mission has a machine-checked proof, and Mathlib contains no theory of the Navier–Stokes or Euler equations. The milestones are all proved in the literature; formalizing them requires building, on Mathlib's calculus, measure theory and Schwartz space, the heat semigroup on Rn\mathbb{R}^nRn, the pressure equation Δp=−∑i,j∂i∂j(uiuj)\Delta p = -\sum_{i,j} \partial_i\partial_j(u_i u_j)Δp=−∑i,j​∂i​∂j​(ui​uj​) or the Leray projection, energy estimates, and a fixed-point construction of solutions, most of which is reusable for other evolution equations. The goal is open and expected to remain so; its role is to fix in Lean the exact statement the prize asks for, so partial results are formalized against it.

Difficulty

The energy identity ddt∫∣u∣2=−2ν∫∣∇u∣2\frac{d}{dt}\int|u|^2 = -2\nu\int|\nabla u|^2dtd​∫∣u∣2=−2ν∫∣∇u∣2 controls uuu in L2L^2L2 and ∇u\nabla u∇u in Lt,x2L^2_{t,x}Lt,x2​, but in three dimensions this control is supercritical: under the scaling uλ(x,t)=λu(λx,λ2t)u_\lambda(x,t) = \lambda u(\lambda x, \lambda^2 t)uλ​(x,t)=λu(λx,λ2t) that preserves the equations, the energy of uλu_\lambdauλ​ shrinks as λ→∞\lambda \to \inftyλ→∞, so bounded energy does not prevent concentration at small scales. Every known continuation criterion (Leray, Prodi–Serrin, Beale–Kato–Majda, Escauriaza–Seregin–Šverák) needs a quantity at or above critical scaling, none of which the energy controls. The obvious first idea, an ordinary differential inequality for ∥∇u(t)∥L2\|\nabla u(t)\|_{L^2}∥∇u(t)∥L2​, gives ddt∥∇u∥L22≤Cν−3∥∇u∥L26\frac{d}{dt}\|\nabla u\|_{L^2}^2 \le C\nu^{-3}\|\nabla u\|_{L^2}^6dtd​∥∇u∥L22​≤Cν−3∥∇u∥L26​, which closes only for small data or short time. That is exactly why milestones 1 and 2 are theorems and the goal is not.

The formalization adds a second difficulty: the solutions of the literature live in Sobolev or Besov spaces, with pointwise smoothness of uuu and ppp recovered afterwards by regularity theory, and Mathlib has neither Sobolev spaces on Rn\mathbb{R}^nRn nor the heat semigroup in usable form.

Formalization scope

  • Rn\mathbb{R}^nRn is EuclideanSpace ℝ (Fin n) with Lebesgue measure; the dimension is a parameter, the goal fixes n=3n = 3n=3 and the 2D milestone n=2n = 2n=2.
  • A velocity field is a function of all real times, but every condition is imposed only on the time set SSS; values at negative times are unconstrained.
  • Smoothness on Rn×[0,∞)\mathbb{R}^n \times [0,\infty)Rn×[0,∞) is Mathlib's ContDiffOn of the uncurried map on the closed half-space, i.e. all derivatives extend continuously to t=0t = 0t=0. The momentum equation is imposed at interior times t>0t > 0t>0 with two-sided derivatives; by continuity of the derivatives this is equivalent to Fefferman's "t≥0t \ge 0t≥0".
  • Derivatives are Mathlib's total functions (fderiv, deriv, iteratedFDeriv, gradient, Laplacian) with junk value 000 at non-differentiable points; the smoothness hypotheses make every derivative in the statements honest.
  • The energy is a Lebesgue integral in [0,∞][0,\infty][0,∞], equal to ∞\infty∞ when u(⋅,t)∉L2u(\cdot,t) \notin L^2u(⋅,t)∈/L2, so bounded energy cannot hold vacuously. The L2L^2L2 norms in the small-data hypothesis are Bochner integrals, genuine for Schwartz data.
  • No normalization is imposed on the pressure, as in Fefferman's text.

No trivializing formalization. The zero field solves the equations only for u0=0u^0 = 0u0=0; for any other admissible u0u^0u0 the initial condition, smoothness, the equation on t>0t > 0t>0 and bounded energy must all hold.

Infrastructure needed and welcome contributions. The heat kernel on Rn\mathbb{R}^nRn with Schwartz bounds; the Riesz-transform representation of the pressure or the Leray projection; energy identities for smooth decaying solutions; local existence by Picard iteration; the two-dimensional vorticity equation and its maximum principle. Theorems in the NavierStokes namespace, decompositions of the milestones, and Mathlib lemmas about ContDiffOn on half-spaces are all welcome. Statements (B), (C), (D) and the Euler equations (ν=0\nu = 0ν=0) are out of scope.

Selected references

  • C. L. Fefferman, Existence and smoothness of the Navier–Stokes equation, Clay Mathematics Institute Millennium Prize Problem description, 2000. https://www.claymath.org/wp-content/uploads/2022/06/navierstokes.pdf
  • J. Leray, Sur le mouvement d'un liquide visqueux emplissant l'espace, Acta Mathematica 63 (1934), 193–248. https://doi.org/10.1007/BF02547354
  • O. A. Ladyzhenskaya, The Mathematical Theory of Viscous Incompressible Flow, 2nd ed., Gordon and Breach, 1969. https://archive.org/details/mathematicaltheo0000lady
  • T. Kato, Strong LpL^pLp-solutions of the Navier–Stokes equation in Rm\mathbb{R}^mRm, with applications to weak solutions, Mathematische Zeitschrift 187 (1984), 471–480. https://doi.org/10.1007/BF01174182
  • L. Caffarelli, R. Kohn, L. Nirenberg, Partial regularity of suitable weak solutions of the Navier–Stokes equations, Communications on Pure and Applied Mathematics 35 (1982), 771–831. https://doi.org/10.1002/cpa.3160350604
  • A. J. Majda, A. L. Bertozzi, Vorticity and Incompressible Flow, Cambridge University Press, 2002. https://doi.org/10.1017/CBO9780511613203
  • J. C. Robinson, J. L. Rodrigo, W. Sadowski, The Three-Dimensional Navier–Stokes Equations: Classical Theory, Cambridge University Press, 2016. https://doi.org/10.1017/CBO9781139095143
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🏆Completed
Information Theory·Captain: Elsie66

Shannon's Source Coding TheoremResearch Paper

Motivation

How short can a code for a data source be, if the code must still be uniquely decodable — if every string of concatenated codewords can be unambiguously split back into the original symbols? Shannon's 1948 source coding theorem answers this exactly: the entropy of the source is a hard lower bound on the average codeword length of any uniquely decodable code, and it is also achievable up to a one-symbol slack. Entropy is not just a measure of "average surprise" — it is the literal, tight answer to a combinatorial question about how densely symbols can be packed into strings without losing decodability. This is the theorem that gives Shannon's entropy its operational meaning, and it underlies every practical lossless compression scheme (Huffman coding, arithmetic coding, Lempel–Ziv) as the benchmark they approach.

Timeline.

  • 1948 — Claude Shannon, "A Mathematical Theory of Communication" (Bell System Technical Journal), introduces entropy and proves the source coding theorem.
  • 1949 — Leon Kraft's MIT master's thesis proves the combinatorial inequality (for prefix codes) that makes the theorem's achievability half constructive.
  • 1956 — Brockway McMillan extends Kraft's inequality's necessity direction from prefix codes to the strictly larger class of uniquely decodable codes, giving the theorem its full generality.

Setting

A source has a finite alphabet of symbols ι\iotaι, with at least two symbols, and probability distribution p:ι→Rp:\iota\to\mathbb Rp:ι→R (pi>0p_i>0pi​>0, ∑ipi=1\sum_i p_i=1∑i​pi​=1). A code assigns to each symbol iii a codeword c(i)c(i)c(i), a finite string over a DDD-ary code alphabet α\alphaα (D=∣α∣≥2D=|\alpha|\ge 2D=∣α∣≥2); the code is uniquely decodable if every finite sequence of codewords is determined by its concatenation. The entropy of ppp in base DDD is

HD(p)=−∑ipilog⁡Dpi.H_D(p) = -\sum_i p_i \log_D p_i.HD​(p)=−i∑​pi​logD​pi​.

The expected codeword length of ccc under ppp is L(c)=∑ipi ∣c(i)∣L(c) = \sum_i p_i \, |c(i)|L(c)=∑i​pi​∣c(i)∣.

Formalization targets

Goal — Shannon's source coding theorem

∀ injective, uniquely decodable c,HD(p)≤L(c),∃ such c,L(c)<HD(p)+1.\forall \text{ injective, uniquely decodable } c,\quad H_D(p) \le L(c), \qquad \exists \text{ such } c,\quad L(c) < H_D(p) + 1.∀ injective, uniquely decodable c,HD​(p)≤L(c),∃ such c,L(c)<HD​(p)+1.

(For a source with ∣ι∣≥2|\iota| \ge 2∣ι∣≥2 symbols — see Formalization scope for why the single-symbol case must be excluded.)

Significance

The result itself. This theorem is the reason entropy is called entropy in an information-theoretic sense at all: it converts a quantity defined by an abstract formula (−∑pilog⁡pi-\sum p_i\log p_i−∑pi​logpi​) into the exact answer to an operational question (minimum achievable expected code length), with a slack no worse than one symbol. It is the founding theorem of lossless source coding and the benchmark every practical compressor is measured against.

Formalizing it. Mathlib recently gained genuine information-theoretic coding content: InformationTheory.UniquelyDecodable and the necessity direction of the Kraft–McMillan inequality (McMillan's 1956 result: a uniquely decodable code's lengths satisfy ∑wD−∣w∣≤1\sum_w D^{-|w|}\le 1∑w​D−∣w∣≤1) are already proved, via a counting argument on concatenations of rrr codewords. This mission builds directly on that foundation rather than duplicating it. What Mathlib does not have — and what this mission's milestones supply — is Kraft's original 1949 sufficiency direction (existence of a uniquely decodable code realizing any length assignment satisfying the Kraft sum bound), any notion of Shannon entropy for a general finite distribution, and the source coding theorem itself.

Difficulty

The lower bound (HD(p)≤L(c)H_D(p)\le L(c)HD​(p)≤L(c)) is the easier half: it follows from the Kraft–McMillan inequality (already in Mathlib) via Gibbs'/Jensen's inequality applied to the two probability-like sequences pip_ipi​ and D−ℓi/KD^{-\ell_i}/KD−ℓi​/K (where K=∑jD−ℓj≤1K=\sum_j D^{-\ell_j}\le1K=∑j​D−ℓj​≤1 is the Kraft sum) — a short, self-contained convexity argument.

The achievability half is the genuine construction. Given the ideal (generally non-integer) lengths −log⁡Dpi-\log_D p_i−logD​pi​, one rounds up to ℓi=⌈−log⁡Dpi⌉\ell_i=\lceil -\log_D p_i\rceilℓi​=⌈−logD​pi​⌉ (Shannon–Fano–Elias lengths); a one-line estimate shows D−ℓi≤piD^{-\ell_i}\le p_iD−ℓi​≤pi​, so the Kraft sum of the rounded lengths is still ≤∑ipi=1\le\sum_i p_i=1≤∑i​pi​=1, and the bound ℓi<−log⁡Dpi+1\ell_i<-\log_D p_i+1ℓi​<−logD​pi​+1 gives L(c)<HD(p)+1L(c)<H_D(p)+1L(c)<HD​(p)+1 immediately once a code with exactly these lengths is shown to exist. Producing that code is Kraft's sufficiency direction, and it needs an explicit construction: order the lengths, and assign to symbol iii the first ℓi\ell_iℓi​ digits of the DDD-ary expansion of the cumulative sum ∑j<iD−ℓj\sum_{j<i} D^{-\ell_j}∑j<i​D−ℓj​. Verifying this assignment is injective, has the prescribed lengths, and is uniquely decodable (indeed prefix-free) is a careful but standard combinatorial argument — the main open piece of this mission.

Formalization scope

The source alphabet ι\iotaι must have at least two symbols (∣ι∣≥2|\iota|\ge 2∣ι∣≥2), not merely be nonempty. A single-symbol source forces p≡1p\equiv 1p≡1 and entropy HD(p)=0H_D(p)=0HD​(p)=0, so the achievability conjunct would demand a codeword of length 000 — but a uniquely decodable code can never contain the empty codeword (InformationTheory.UniquelyDecodable.epsilon_not_mem, provable from the definition: the empty string decodes ambiguously as zero or two copies of itself), so no admissible code exists and the theorem would be false, not merely hard, at ∣ι∣=1|\iota|=1∣ι∣=1. The same defect breaks Kraft's sufficiency direction (Milestone 2) whenever any prescribed length is 000, independent of ∣ι∣|\iota|∣ι∣; that milestone accordingly requires every length strictly positive. With ∣ι∣≥2|\iota|\ge2∣ι∣≥2 and full support, every pi<1p_i<1pi​<1 strictly, so the Shannon–Fano lengths ⌈−log⁡Dpi⌉\lceil-\log_D p_i\rceil⌈−logD​pi​⌉ are automatically all ≥1\ge1≥1, and the achievability construction only ever needs Milestone 2 at positive lengths. The code alphabet α\alphaα is likewise an arbitrary finite type (matching Mathlib's own Fintype/Nonempty conventions for the Kraft–McMillan file), with ∣α∣≥2|\alpha|\ge2∣α∣≥2 required to keep Real.logb non-degenerate. The source distribution is required strictly positive (pi>0p_i>0pi​>0) — the standard simplifying assumption (zero-probability symbols can always be dropped without loss). Unique decodability is stated exactly as Mathlib's InformationTheory.UniquelyDecodable, not re-derived from a "prefix code" definition, so the mission's results transport directly onto Mathlib's existing Kraft–McMillan file. A trivializing route to rule out: proving only the lower bound (citing Mathlib's inequality) while leaving the existential achievability half unaddressed would not be Shannon's theorem — the sandwich HD(p)≤L∗<HD(p)+1H_D(p)\le L^*<H_D(p)+1HD​(p)≤L∗<HD​(p)+1 is the theorem's actual content, and the lower bound alone (already essentially free from Mathlib) is not a novel contribution on its own.

Reusable output: the Kraft sufficiency construction (Milestone 2) is directly reusable for any future formalization of Huffman coding optimality, arithmetic coding, or the general "Kraft-inequality-achieving code exists" fact used throughout coding theory. Contributions are welcome starting from Milestone 2 (the open construction) or Milestone 3 (the Gibbs'-inequality lower bound, which only needs Milestone 1, already available via Mathlib).

Selected references

  • C. E. Shannon, "A Mathematical Theory of Communication," The Bell System Technical Journal 27 (1948), 379–423, 623–656.
  • T. M. Cover and J. A. Thomas, Elements of Information Theory, 2nd ed., Wiley, 2006, Chapter 5 ("Data Compression"), §5.2 ("Kraft Inequality") and §5.4 ("Bounds on the Optimal Code Length," Theorem 5.4.1).
  • L. G. Kraft, A Device for Quantizing, Grouping, and Coding Amplitude-Modulated Pulses, M.S. thesis, MIT, 1949.
  • B. McMillan, "Two Inequalities Implied by Unique Decipherability," IRE Transactions on Information Theory 2:4 (1956), 115–116.
  • Mathlib, Mathlib.InformationTheory.Coding.UniquelyDecodable and Mathlib.InformationTheory.Coding.KraftMcMillan (2026).
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Quantum InformationTheoretical Computer Science·Captain: Goku

Stabilizer Rank of Magic StatesOpen Problem

Motivation

Quantum circuits built from Clifford gates alone are classically simulable in polynomial time. Universality is recovered by adding copies of a magic state, and the fastest known classical simulators of such circuits work by writing the magic-state input as a short linear combination of stabilizer states. The length of the shortest such combination -- the stabilizer rank -- is therefore the exponent governing classical simulation of quantum computation in this model, and lower bounds on it are among the very few unconditional obstructions to classical simulation available at all.

A timeline of what is established for the standard magic state ∣H⟩|H\rangle∣H⟩:

  • 2016. Bravyi, Smith and Smolin exhibit a decomposition giving χ(∣H⊗6⟩)≤7\chi(|H^{\otimes 6}\rangle)\le 7χ(∣H⊗6⟩)≤7, hence χ(∣H⊗n⟩)≤7 n/6≤2 0.468n\chi(|H^{\otimes n}\rangle)\le 7^{\,n/6}\le 2^{\,0.468n}χ(∣H⊗n⟩)≤7n/6≤20.468n, and prove a lower bound of order n\sqrt{n}n​.
  • 2020. Huang, Newman and Szegedy show that hardness assumptions stronger than P≠NP\mathrm{P}\neq\mathrm{NP}P=NP, such as the exponential time hypothesis, imply χ(∣H⊗n⟩)=2Ω(n)\chi(|H^{\otimes n}\rangle)=2^{\Omega(n)}χ(∣H⊗n⟩)=2Ω(n) (arXiv link).
  • 2022. Peleg, Shpilka and Volk improve the unconditional lower bound to Ω(n)\Omega(n)Ω(n) and give the first non-trivial bound for the approximate rank (arXiv:2106.03214).
  • 2024. A quadratic lower bound is obtained for the approximate stabilizer rank (arXiv:2305.10277).

Between the linear unconditional lower bound and the 20.468n2^{0.468n}20.468n upper bound lies the open problem this mission targets.

Setting

Index the computational basis of an nnn-qubit system by bit strings x∈{0,1}nx\in\{0,1\}^nx∈{0,1}n, so a state is a vector ψ∈C2n\psi\in\mathbb{C}^{2^n}ψ∈C2n with coordinates ψ(x)\psi(x)ψ(x).

The Pauli operators are XaZbX^aZ^bXaZb for a,b∈{0,1}na,b\in\{0,1\}^na,b∈{0,1}n, acting by XaZb∣x⟩=(−1) b⋅x∣x⊕a⟩X^aZ^b|x\rangle=(-1)^{\,b\cdot x}|x\oplus a\rangleXaZb∣x⟩=(−1)b⋅x∣x⊕a⟩, where b⋅xb\cdot xb⋅x counts the coordinates on which both are 111 and ⊕\oplus⊕ is bitwise addition; the Pauli group is the set of 4⋅4n4\cdot 4^n4⋅4n operators icXaZbi^cX^aZ^bicXaZb. A unitary UUU is a Clifford unitary when UPU†UPU^\daggerUPU† lies in the Pauli group for every Pauli group element PPP, and a stabilizer state is a vector U∣0⋯0⟩U|0\cdots0\rangleU∣0⋯0⟩ for some Clifford UUU. There are 2n∏k=1n(2k+1)2^n\prod_{k=1}^{n}(2^k+1)2n∏k=1n​(2k+1) of them up to phase -- six for a single qubit.

The stabilizer rank χ(ψ)\chi(\psi)χ(ψ) is the least rrr admitting coefficients c1,…,cr∈Cc_1,\dots,c_r\in\mathbb{C}c1​,…,cr​∈C and stabilizer states φ1,…,φr\varphi_1,\dots,\varphi_rφ1​,…,φr​ with ψ=∑j≤rcjφj\psi=\sum_{j\le r}c_j\varphi_jψ=∑j≤r​cj​φj​.

The magic state is ∣H⟩=cos⁡(π/8)∣0⟩+sin⁡(π/8)∣1⟩|H\rangle=\cos(\pi/8)|0\rangle+\sin(\pi/8)|1\rangle∣H⟩=cos(π/8)∣0⟩+sin(π/8)∣1⟩, and ∣H⊗n⟩|H^{\otimes n}\rangle∣H⊗n⟩ its nnn-fold tensor power, with coordinates cos⁡(π/8) n−∣x∣sin⁡(π/8) ∣x∣\cos(\pi/8)^{\,n-|x|}\sin(\pi/8)^{\,|x|}cos(π/8)n−∣x∣sin(π/8)∣x∣ where ∣x∣|x|∣x∣ is the Hamming weight of xxx.

Target

The goal is a super-polynomial lower bound: for every exponent ddd and constant CCC there exists nnn with

χ(∣H⊗n⟩)  >  C nd,\chi\bigl(|H^{\otimes n}\rangle\bigr)\;>\;C\,n^{d},χ(∣H⊗n⟩)>Cnd,

equivalently, χ(∣H⊗n⟩)\chi(|H^{\otimes n}\rangle)χ(∣H⊗n⟩) is not O(nd)O(n^d)O(nd) for any fixed ddd.

Stronger statements are expected but are deliberately not the goal. An exponential bound χ=2Ω(n)\chi=2^{\Omega(n)}χ=2Ω(n) is believed and follows from hardness assumptions, but a goal naming a specific growth rate would be superseded by the next improvement; super-polynomiality is the weakest statement that settles the question of principle.

Significance

The result itself. A super-polynomial lower bound would unconditionally rule out efficient classical simulation of Clifford-plus-magic-state circuits by stabilizer decomposition, currently the leading such technique. The converse direction shows how much is at stake: a polynomial upper bound on χ(∣H⊗n⟩)\chi(|H^{\otimes n}\rangle)χ(∣H⊗n⟩) would imply BPP=BQP\mathrm{BPP}=\mathrm{BQP}BPP=BQP, and via postselection P=NP\mathrm{P}=\mathrm{NP}P=NP. There is also a purely classical payoff -- improving the known bound even to super-linear would produce a Boolean function computable in polynomial time requiring a super-linear number of summands in any decomposition into exponentials of quadratic forms over F2\mathbb{F}_2F2​, resolving a separate open question.

Formalizing it. The goal is open, so no known proof is being transcribed. What the mission produces is a machine-checked statement of the problem together with formalizations of the established bounds, none of which has a machine-checked proof anywhere. It also produces the first Pauli/Clifford/stabilizer layer in Lean: no existing Lean library contains the nnn-qubit Pauli group, the Clifford group, or stabilizer states, and that layer is reusable for stabilizer error correction, magic monotones, and Clifford simulation generally.

Difficulty

Counting settles the problem for random states: the stabilizer states are too few for short combinations to cover a generic state, so almost every state has exponential stabilizer rank. This says nothing about ∣H⊗n⟩|H^{\otimes n}\rangle∣H⊗n⟩, which is a single explicit, highly structured vector, and the entire difficulty is that lower bounds must be proved for that specific state rather than for a typical one. Every newcomer proposes the counting argument; it does not apply.

The known techniques reduce the question to statements about decompositions of explicit Boolean functions into quadratic-form exponentials, and the barrier is quantitative: the available arguments lose a factor that caps them at linear bounds. The source of the current record documents explicitly why its method cannot pass super-linear, and the fact that going beyond linear would resolve an independent open problem in Boolean function complexity indicates the obstruction is not merely technical.

Formalization scope

State vectors are functions {0,1}n→C\{0,1\}^n\to\mathbb{C}{0,1}n→C and are not required to be normalised; normalisation does not affect the rank, and stabilizer states are unit vectors automatically as Clifford images of ∣0⋯0⟩|0\cdots0\rangle∣0⋯0⟩. The Pauli group is given by the explicit parametrisation icXaZbi^cX^aZ^bicXaZb rather than an abstract presentation, and the Clifford group is characterised as its unitary normaliser, equivalent to the usual generated-by-H,S,CNOTH,S,\mathrm{CNOT}H,S,CNOT description. Because eiθUe^{i\theta}UeiθU normalises the Pauli group whenever UUU does, the stabilizer states are closed under global phase; this is harmless, as the coefficients are arbitrary complex numbers.

One trivialising reading must be excluded. The rank is defined as an infimum over a set of natural numbers, and Lean gives the empty infimum the value 000; if no decomposition existed the rank would be 000 for every state and the goal would be false rather than merely unproved. The milestone χ(ψ)≤2n\chi(\psi)\le 2^nχ(ψ)≤2n is what certifies the set is nonempty, making the rank a genuine minimum, and it should be proved first. Separately, the goal quantifies CCC over all reals including negative values, for which the inequality is trivially satisfiable; the content lies in large positive CCC.

A complete development needs, beyond the published definitions, the correspondence between stabilizer states and affine subspaces carrying quadratic phase functions, on which all known lower-bound arguments rest. Contributions of any milestone are welcome, as are function-level reformulations of the rank and the equivalent characterisation of stabilizer states via maximal abelian Pauli subgroups.

Selected references

  • S. Peleg, A. Shpilka, B. L. Volk, Lower Bounds on Stabilizer Rank, Quantum 6 (2022) 652; arXiv:2106.03214.
  • S. Bravyi, G. Smith, J. Smolin, Trading Classical and Quantum Computational Resources, Phys. Rev. X 6 (2016) 021043; arXiv:1506.01396.
  • C. Huang, M. Newman, M. Szegedy, Explicit Lower Bounds on Strong Quantum Simulation, IEEE Trans. Inf. Theory 66(9) (2020) 5585--5600.
  • Quadratic Lower Bounds on the Approximate Stabilizer Rank: A Probabilistic Approach, STOC 2024; arXiv:2305.10277.
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Dynamic Programming and Optimal Control V: LQG and Certainty EquivalenceTextbook

Motivation

The separation theorem — certainty equivalence for linear-quadratic control with imperfect state information — is one of the celebrated structural results of stochastic control: the optimal controller splits into a least-squares estimator and the deterministic LQR actuator, designed independently. It underlies every LQG autopilot and Kalman-filter-based regulator. Section 5.2 of Bertsekas, Dynamic Programming and Optimal Control, Vol. I (3rd ed., 2005) proves it from the DP algorithm over information vectors, with Lemma 5.2.1 supplying the key fact that the estimation error is beyond the controller's influence. No formal analogue exists in Mathlib.

Setting

Linear dynamics and measurements

xk+1=Akxk+Bkuk+wk,zk=Ckxk+vk,x_{k+1} = A_k x_k + B_k u_k + w_k, \qquad z_k = C_k x_k + v_k,xk+1​=Ak​xk​+Bk​uk​+wk​,zk​=Ck​xk​+vk​,

with quadratic cost E[xN⊤QNxN+∑k<N(xk⊤Qkxk+uk⊤Rkuk)]\mathbb{E}\big[x_N^\top Q_N x_N + \sum_{k<N}(x_k^\top Q_k x_k + u_k^\top R_k u_k)\big]E[xN⊤​QN​xN​+∑k<N​(xk⊤​Qk​xk​+uk⊤​Rk​uk​)], Qk⪰0Q_k \succeq 0Qk​⪰0, Rk≻0R_k \succ 0Rk​≻0. The initial state and the zero-mean disturbances/noises are independent with finite ranges; independence is structural — the sample space is the product of an initial-state coordinate and per-stage noise coordinates (BertsekasLQGModel, BertsekasLQGSample, BertsekasLQGProb). A policy maps the realized measurement history (z0,…,zk)(z_0,\dots,z_k)(z0​,…,zk​) to uku_kuk​; the closed-loop process is BertsekasLQGTraj, the expected cost BertsekasLQGCost. The estimator E[xk∣Ik]\mathbb{E}[x_k \mid I_k]E[xk​∣Ik​] is an explicit conditional average (BertsekasCondExpVec, BertsekasLQGEstimate); the gains LkL_kLk​ come from the time-varying Riccati recursion (BertsekasLQGRiccati, BertsekasLQGGain).

Target

π∗(Ik)=Lk E[xk∣Ik]  along its own trajectories⟹J(π∗)≤J(π)  ∀π,\pi^*(I_k) = L_k\, \mathbb{E}[x_k \mid I_k] \ \text{ along its own trajectories} \quad\Longrightarrow\quad J(\pi^*) \le J(\pi)\ \ \forall \pi,π∗(Ik​)=Lk​E[xk​∣Ik​]  along its own trajectories⟹J(π∗)≤J(π)  ∀π,

— BertsekasDP.lqg_certainty_equivalence (goal). Milestone: Lemma 5.2.1 in pointwise form — the error xk−E[xk∣Ik]x_k - \mathbb{E}[x_k \mid I_k]xk​−E[xk​∣Ik​] is the same under any two policies, outcome by outcome (lqg_estimation_error_policy_independent).

Significance

This is the theorem that justifies designing estimator and controller separately — remove it and the entire LQG methodology loses its warrant. The formalization also yields the first machine-checked instance of the informational decomposition (control-dependent part + policy-independent error) that recurs throughout imperfect-information control. Notably the result needs no Gaussian assumption — only zero mean and independence — and the finite-support model makes that generality exact. The result is classical (Joseph–Tou 1961, Gunckel–Franklin 1963; the book's §5.2); the formal proof is new.

Difficulty

The heart is Lemma 5.2.1: showing the estimation error coincides, sample by sample, with the error of the control-free system — which requires proving that the observation-history σ-events under any policy coincide with those of the control-free system (controls are determined by the history, so they shift observations by a known amount). Then the DP argument over information histories must carry the quadratic decomposition through the backward recursion. Bookkeeping over histories-as-lists is the main formal burden; probability theory stays finite.

Formalization scope

Finite-support randomness (all expectations are finite sums); conditional expectation with the explicit junk value 0 on zero-probability events — the goal's hypothesis is accordingly restricted to outcomes of positive probability. Policies are functions of the measurement list only (equivalent to the book's information vector for deterministic policies, since past controls are recoverable from past measurements). Matrices are time-varying; positive definiteness of RkR_kRk​ makes every matrix inverse in the gains genuine. Measurement noise covariance is not assumed positive definite — the estimator is the abstract conditional expectation, not the Kalman filter (whose recursive form, §5.2.1, would be a natural follow-up mission).

Selected references

  • D. P. Bertsekas, Dynamic Programming and Optimal Control, Vol. I, 3rd ed., Athena Scientific, 2005. (§5.2, Lemma 5.2.1.) http://www.athenasc.com/dpbook.html
  • P. D. Joseph, J. T. Tou, On linear control theory, Trans. AIEE 80 (1961), 193–196. https://doi.org/10.1109/TAI.1961.6371743
  • T. L. Gunckel, G. F. Franklin, A general solution for linear sampled-data control, J. Basic Eng. 85 (1963), 197–201. https://doi.org/10.1115/1.3656559
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Dynamic Programming and Optimal Control II: Label Correcting MethodsTextbook

Motivation

Label correcting methods are the workhorse family of shortest-path algorithms — Dijkstra's method, Bellman–Ford, SLF/LLL variants and A* all fit the template analyzed in §2.3.1 of Bertsekas, Dynamic Programming and Optimal Control, Vol. I (3rd ed., 2005), where shortest paths appear as the purely deterministic face of dynamic programming. The correctness proof (Prop. 2.3.1) is short on paper but genuinely nondeterministic — any node may be removed from the candidate list, children processed in any order — so a formal proof certifies a whole family of concrete algorithms at once.

Setting

A finite directed graph with arc set A\mathcal{A}A, real arc lengths aija_{ij}aij​, origin sss and destination t≠st \ne st=s (BertsekasSPGraph). Walks are nonempty node lists whose consecutive pairs are arcs (BertsekasIsWalkFrom), with length the sum of arc lengths (BertsekasWalkLength); the shortest distance is the infimum of walk lengths in the extended reals, +∞+\infty+∞ if no walk exists (BertsekasShortestDistance). The standing assumption of §2.3: every cycle has nonnegative length (negative arcs allowed).

The algorithm state (BertsekasLCState) carries labels dj∈R‾d_j \in \overline{\mathbb{R}}dj​∈R, the scalar UPPER, and the candidate list OPEN. Initially ds=0d_s = 0ds​=0, all other labels ∞\infty∞, UPPER =∞= \infty=∞, OPEN ={s}= \{s\}={s}. One iteration (BertsekasLCStep, nondeterministic): remove any iii from OPEN; for each child jjj of iii in any order, if di+aij<min⁡{dj,UPPER}d_i + a_{ij} < \min\{d_j, \text{UPPER}\}di​+aij​<min{dj​,UPPER} set dj:=di+aijd_j := d_i + a_{ij}dj​:=di​+aij​, and put jjj in OPEN if j≠tj \ne tj=t, or update UPPER if j=tj = tj=t. The algorithm terminates when OPEN is empty.

Target

OPEN=∅  ⟹  UPPER=dist⁡(s,t)∈R‾,\text{OPEN} = \varnothing \implies \text{UPPER} = \operatorname{dist}(s, t) \in \overline{\mathbb{R}},OPEN=∅⟹UPPER=dist(s,t)∈R,

for every execution, under the nonnegative arc length assumption of §2.3 (aij≥0a_{ij} \ge 0aij​≥0 for every arc) — BertsekasDP.label_correcting_correctness_of_nonneg_arcs (goal). Milestones: termination — no infinite execution exists, which needs only the weaker nonnegative-cycle assumption (label_correcting_terminates) — and the workhorse invariant that every finite label is the length of an actual walk from sss, which needs neither (label_correcting_invariant).

The nonnegative-arc hypothesis is essential and not a formalization artifact: the algorithm prunes with the test di+aij<min⁡{dj,UPPER}d_i + a_{ij} < \min\{d_j, \mathrm{UPPER}\}di​+aij​<min{dj​,UPPER}, and with a negative arc a longer prefix can still reach ttt more cheaply, so the pruned node is never entered into OPEN. An earlier version of this mission's goal carried only the nonnegative-cycle assumption of §2.1 and was disproved by the counterexample s=0s=0s=0, t=2t=2t=2, a02=1a_{02}=1a02​=1, a01=2a_{01}=2a01​=2, a12=−2a_{12}=-2a12​=−2 (a graph with no cycles at all), where the algorithm terminates with UPPER=1\mathrm{UPPER}=1UPPER=1 while the shortest distance is 000. Exercise 2.7 of the source treats the nonnegative-cycle case, which requires a modified algorithm.

Significance

Prop. 2.3.1 certifies simultaneously breadth-first search, Dijkstra (best-first), depth-first and small-label-first variants — every removal discipline is one refinement of the nondeterministic relation. Formally, the development contributes a reusable small-step framework for label-setting/correcting algorithms on which sharper results (Dijkstra's single-pass property, A* admissibility, §2.3.3) can later be built. The result is classical; the formal content is the induction along the nondeterministic step relation.

Difficulty

Termination is the subtle half: labels do not decrease monotonically along the run in an obvious well-founded way; the book's argument counts the finitely many distinct walk lengths below a bound — this needs the nonnegative-cycle assumption and a careful bound relating labels to simple-path lengths. The invariant proof must thread through the fold over children within a single step.

Formalization scope

Finite node type with decidable equality; arcs as a Finset of ordered pairs; lengths total on V×VV \times VV×V (only arc values matter). The step relation is fully nondeterministic in pivot choice and child order (a permutation quantifier); correctness quantifies over all reachable terminal states — there is no fixed schedule to exploit. Distances live in EReal, so the no-path case is the honest empty infimum, not a sentinel. The trivializing risk of restricting to nonnegative arcs is avoided: only cycles are constrained.

Selected references

  • D. P. Bertsekas, Dynamic Programming and Optimal Control, Vol. I, 3rd ed., Athena Scientific, 2005. (Prop. 2.3.1, §2.3.) http://www.athenasc.com/dpbook.html
  • E. W. Dijkstra, A note on two problems in connexion with graphs, Numer. Math. 1 (1959), 269–271. https://doi.org/10.1007/BF01386390
  • R. Bellman, On a routing problem, Quart. Appl. Math. 16 (1958), 87–90. https://doi.org/10.1090/qam/102435
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