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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 19.8899945Formalized record→≤ 14.797074Open frontier
6 provers on it3 of 7 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 89Formalized record
3 provers on it3 of 3 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 85Formalized record→≤ 5Open frontier
35 provers on it10 of 12 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.37134Formalized record→≤ 2.371177Open frontier
16 provers on it7 of 8 missions formalized

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Markov ChainOperations ResearchStochastic Systems·Captain: naimengye

Stochastic Networks III: Loss Networks and the Erlang Fixed PointTextbook

Motivation

Erlang's formula, the subject of mission I of this series, sizes a single telephone link. Real networks are not single links: a call occupies a circuit on every link of its route simultaneously, and it is lost unless every one of those links has a free circuit. That is the loss network, the model of Chapter 3 of Frank Kelly and Elena Yudovina's Stochastic Networks (Cambridge University Press, 2014), and it describes not only circuit-switched telephony but any system in which a request must acquire several resources at once or be refused: wavelength assignment in optical networks, radio channel allocation under interference constraints, slot booking, and admission control generally. The term used in those application areas is circuit-switched: before a request is accepted it is checked that enough resource is available for each stage of it.

The exact equilibrium distribution of a loss network is known and has product form. It is also useless for computation — its normalizing constant is a sum over the feasible states, and for a general resource matrix computing it is NP-hard. What practitioners use instead is the Erlang fixed point: pretend the links block independently, so that the traffic offered to link jjj is the traffic on the routes through it thinned by the blocking probability of every other link on each route, and then apply Erlang's formula link by link. The result is a system of coupled copies of Erlang's formula. The chapter's aim, in its own words, is to give insight into why that approximation works as well as it does; the first step is to show that it is well posed at all.

Setting

The links are J={1,…,J}\mathcal{J} = \{1,\dots,J\}J={1,…,J}, link jjj carrying CjC_jCj​ circuits. A route rrr belongs to a set R\mathcal{R}R of RRR routes, and the link-route incidence matrix AAA records how much of each link a route needs: a call on route rrr requires AjrA_{jr}Ajr​ circuits from link jjj and is lost if any link has fewer than AjrA_{jr}Ajr​ free. (The classical case is AAA a 000–111 matrix and Ajr=1A_{jr}=1Ajr​=1 exactly when j∈rj\in rj∈r; from section 3.3 the book allows any non-negative integers.)

Calls requesting route rrr arrive as a Poisson process of rate νr\nu_rνr​, independently across routes, and hold their circuits for an exponentially distributed time of unit mean. Writing nrn_rnr​ for the number of calls in progress on route rrr, the process n=(nr)n=(n_r)n=(nr​) is Markov on

S(C)={n∈Z+R:An≤C},S(C)=\{n\in\mathbb{Z}_+^{R} : An\le C\},S(C)={n∈Z+R​:An≤C},

and is called a loss network with fixed routing.

Write E(ν,C)E(\nu,C)E(ν,C) for Erlang's formula, E(ν,C)=νC/C!∑j=0Cνj/j!E(\nu,C)=\dfrac{\nu^{C}/C!}{\sum_{j=0}^{C}\nu^{j}/j!}E(ν,C)=∑j=0C​νj/j!νC/C!​, published in mission I of this series. The Erlang fixed point equations are

Ej  =  E ⁣((1−Ej)−1∑rAjr νr∏i(1−Ei)Air,  Cj),j=1,…,J.(3.7)E_j \;=\; E\!\left((1-E_j)^{-1}\sum_r A_{jr}\,\nu_r\prod_i (1-E_i)^{A_{ir}},\; C_j\right), \qquad j=1,\dots,J. \tag{3.7}Ej​=E((1−Ej​)−1r∑​Ajr​νr​i∏​(1−Ei​)Air​,Cj​),j=1,…,J.(3.7)

The factor (1−Ej)−1(1-E_j)^{-1}(1−Ej​)−1 removes link jjj's own thinning from the product, so in the 000–111 case the argument is ∑r∋jνr∏i∈r∖{j}(1−Ei)\sum_{r\ni j}\nu_r\prod_{i\in r\setminus\{j\}}(1-E_i)∑r∋j​νr​∏i∈r∖{j}​(1−Ei​), the reduced load offered to link jjj.

Formalization targets

Goal — Theorem 3.20, existence and uniqueness of the Erlang fixed point

∃! (E1,…,EJ)∈[0,1]J satisfying (3.7).\exists!\,(E_1,\dots,E_J)\in[0,1]^J \text{ satisfying } (3.7).∃!(E1​,…,EJ​)∈[0,1]J satisfying (3.7).

The goal fixes no formula for EEE and no rate of convergence: it asserts only that the approximation the field has used since the 1960s names a single, well-defined object. Existence alone is a short argument from Brouwer's theorem, since (3.7) defines a continuous self-map of the compact convex cube [0,1]J[0,1]^J[0,1]J; uniqueness is the substance.

Supporting levels

The exact theory that the fixed point approximates: Lemma 3.4 on truncating a reversible process; the uncapacitated network as an instance of the open migration product form of mission II; equation (3.3), the exact equilibrium distribution π(n)=G(C)∏rνrnr/nr!\pi(n)=G(C)\prod_r \nu_r^{n_r}/n_r!π(n)=G(C)∏r​νrnr​​/nr​! on S(C)S(C)S(C); and the acceptance probability 1−Lr=G(C)/G(C−Aer)1-L_r=G(C)/G(C-Ae_r)1−Lr​=G(C)/G(C−Aer​). Then the optimization side: that E(ν,C)E(\nu,C)E(ν,C) and the utilization ν(1−E(ν,C))\nu(1-E(\nu,C))ν(1−E(ν,C)) are strictly increasing in ν\nuν, which is what makes the revised dual objective strictly convex; and Theorem 3.10, that a minimizer of the Dual problem (3.5) over the positive orthant satisfies the conditions on BBB, equation (3.6).

Significance

The result itself. Without Theorem 3.20 the phrase "the Erlang fixed point" is not well formed, and neither is any engineering procedure that computes one — repeated substitution converges to a solution, and damped iteration is guaranteed to converge to one, but "the blocking probabilities predicted by the reduced-load approximation" names a unique vector only because of this theorem. The proof is also the interesting part: the fixed point equations are re-read as the stationary conditions of a strictly convex minimization, the revised dual (3.8), which is the Dual problem (3.5) of the maximum-probability analysis with its linear term replaced by ∫0yjU(z,Cj) dz\int_0^{y_j}U(z,C_j)\,dz∫0yj​​U(z,Cj​)dz. That connection is what later lets the book prove the approximation asymptotically exact in a limiting regime: Corollary 3.22 says the Erlang fixed point converges to the vector BBB coming from the maximum-probability problem.

Formalizing it. Nothing here is open. What the mission produces is the loss network model in Lean — state space, truncated rates, normalizing constant, incidence matrix — and a machine-checked statement of the object the reduced-load approximation computes. It is also where this series' earlier missions pay off: the uncapacitated network is literally the open migration process of mission II with λ≡0\lambda\equiv 0λ≡0, μ≡1\mu\equiv 1μ≡1, φj(n)=n\varphi_j(n)=nφj​(n)=n, and the exact distribution (3.3) is its truncation by Lemma 3.4 to the feasible set, using the DetailedBalance layer of mission I. Mathlib has no loss network theory and no Erlang formula beyond what mission I published.

Difficulty

Existence of a fixed point is easy and is not where the difficulty lies. Uniqueness resists every direct attack: the map defined by (3.7) is not a contraction in any obvious metric, its monotonicity structure is not the kind that forces a unique fixed point, and iterating it undamped can cycle. The book's route is indirect — exhibit a strictly convex function whose stationary conditions are exactly (3.7) — and finding that function is the whole content. Its strict convexity comes from a monotonicity fact about Erlang's formula, that the utilization ν(1−E(ν,C))\nu\bigl(1-E(\nu,C)\bigr)ν(1−E(ν,C)) is strictly increasing in ν\nuν, which is itself a milestone here.

A second, formal difficulty: the equations involve (1−Ej)−1(1-E_j)^{-1}(1−Ej​)−1, so a solution with Ej=1E_j=1Ej​=1 would be meaningless. It is worth checking before starting that no such solution exists for Cj≥1C_j\ge 1Cj​≥1, rather than assuming it.

Formalization scope

Routes and links are indexed by finite types, the incidence matrix has natural-number entries (the general case of section 3.3, not only 000–111), capacities are natural numbers, and arrival rates are positive reals. The feasible set S(C)S(C)S(C) is a subset of the state space, and a truncated process is the rate matrix restricted to that subset — which is exactly the book's truncation, since a transition leaving the set simply has no target.

Conventions: holding times have unit mean throughout, matching the book, so the departure rate from route rrr is nrn_rnr​ and no separate service-rate parameter appears. Normalizing constants are introduced through summability hypotheses that assert convergence and the value together, rather than as possibly-infinite quantities; G(C)G(C)G(C) is the reciprocal of the sum in the book's notation. Capacities are assumed at least 111 in the goal: a link with no circuits blocks everything, E(ν,0)=1E(\nu,0)=1E(ν,0)=1 identically, and the factor (1−Ej)−1(1-E_j)^{-1}(1−Ej​)−1 would then be undefined rather than merely large.

The goal cannot be satisfied trivially: it is a uniqueness statement, so a vacuous or degenerate reading would have to produce no solution, and existence is half of what is asserted.

Contributions welcome beyond the listed items: the Brouwer argument for existence of a solution to the 000–111 equations (3.1) of section 3.2; the utilization function U(y,C)U(y,C)U(y,C) and the revised dual (3.8); the central limit theorem 3.14 and Corollary 3.17; Lemma 3.21 and Corollary 3.22 on the limiting regime; and the diverse-routing models of section 3.7.

Selected references

  • Frank Kelly and Elena Yudovina, Stochastic Networks, Cambridge University Press, 2014, Chapter 3 (pp. 49–82); Lemma 3.4, equation (3.3), Theorems 3.10 and 3.20, equations (3.1), (3.5)–(3.9). DOI 10.1017/cbo9781139565363
  • F. P. Kelly, Loss networks, Annals of Applied Probability 1 (1991), 319–378. DOI 10.1214/aoap/1177005872
  • F. P. Kelly, Blocking probabilities in large circuit-switched networks, Advances in Applied Probability 18 (1986), 473–505. DOI 10.2307/1427303
  • R. B. Cooper and S. Katz, Analysis of alternate routing networks with account taken of the nonrandomness of overflow traffic, Bell Telephone Laboratories memorandum, 1964.
  • Frank Kelly, Reversibility and Stochastic Networks, Cambridge University Press, 2011 (reissue of the 1979 edition), Chapter 1 on truncation.
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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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Convex OptimizationLinear OptimizationOperations Research+2·Captain: mikedeng1

Introduction to Stochastic Programming I: Convexity, Attainment and Optimality of the Two-Stage Recourse ProblemTextbook

Motivation

Two-stage stochastic linear programming with recourse models a decision made before uncertainty resolves (the first-stage variables xxx) followed by a corrective decision made after (the second-stage, or recourse, variables yyy). Solving such a program means minimizing cTx+Q(x)c^{\mathsf T}x + Q(x)cTx+Q(x), where Q(x)Q(x)Q(x) is the expected cost of the best recourse action given xxx -- an object defined only implicitly, as the value of an embedded linear program that must be solved (or bounded) for every realization of the uncertain data. Before any algorithm for this problem can be justified -- the L-shaped method, stochastic decomposition, scenario decomposition, all developed in later chapters of Birge & Louveaux, Introduction to Stochastic Programming (Springer, 2011) -- one needs to know that QQQ is well-behaved enough to optimize over at all: that the feasible region is closed and convex, that QQQ itself is a finite, Lipschitz, convex function on it, that an optimal solution is actually attained rather than only approached in the limit, and finally what an optimality condition for the resulting nonsmooth convex program even looks like. This mission formalizes exactly that foundational layer, Chapter 3, Section 3.1 of the book.

Setting

Fix natural numbers n1,n2,m1,m2n_1, n_2, m_1, m_2n1​,n2​,m1​,m2​ and a finite scenario count KKK. A two-stage recourse instance consists of first-stage data A∈Rm1×n1A \in \mathbb{R}^{m_1 \times n_1}A∈Rm1​×n1​, b∈Rm1b \in \mathbb{R}^{m_1}b∈Rm1​, c∈Rn1c \in \mathbb{R}^{n_1}c∈Rn1​, a fixed recourse matrix W∈Rm2×n2W \in \mathbb{R}^{m_2 \times n_2}W∈Rm2​×n2​, and, for each scenario k=1,…,Kk = 1,\dots,Kk=1,…,K, a cost vector qk∈Rn2q_k \in \mathbb{R}^{n_2}qk​∈Rn2​, a right-hand side hk∈Rm2h_k \in \mathbb{R}^{m_2}hk​∈Rm2​, a technology matrix Tk∈Rm2×n1T_k \in \mathbb{R}^{m_2 \times n_1}Tk​∈Rm2​×n1​, and a probability pk≥0p_k \ge 0pk​≥0 with ∑kpk=1\sum_k p_k = 1∑k​pk​=1 (Eq. (1.1)). The first-stage feasible region is K1={x∣Ax=b, x≥0}K_1 = \{x \mid Ax = b,\ x \ge 0\}K1​={x∣Ax=b, x≥0}.

For a fixed xxx and scenario kkk, the second-stage value is

Q(x,ξk)=min⁡y{qkTy∣Wy=hk−Tkx, y≥0}Q(x,\xi_k) = \min_{y}\{q_k^{\mathsf T}y \mid Wy = h_k - T_k x,\ y \ge 0\}Q(x,ξk​)=ymin​{qkT​y∣Wy=hk​−Tk​x, y≥0}

(Eq. (1.6)), taken as an extended real: +∞+\infty+∞ if no feasible yyy exists, −∞-\infty−∞ if the inner program is unbounded below. The expected recourse value is Q(x)=∑kpk Q(x,ξk)Q(x) = \sum_k p_k\, Q(x,\xi_k)Q(x)=∑k​pk​Q(x,ξk​) (Eq. (1.3)), combined so that +∞+(−∞)=+∞+\infty + (-\infty) = +\infty+∞+(−∞)=+∞ -- the book's own convention (p. 109): infeasibility in one scenario is treated as fatal even if another scenario is unboundedly favorable. The second-stage feasibility set is K2={x∣Q(x)<∞}K_2 = \{x \mid Q(x) < \infty\}K2​={x∣Q(x)<∞}, and the deterministic-equivalent objective is z(x)=cTx+Q(x)z(x) = c^{\mathsf T}x + Q(x)z(x)=cTx+Q(x) (Eq. (1.2)). For xxx with Q(x)Q(x)Q(x) finite, the subdifferential ∂Q(x)\partial Q(x)∂Q(x) is the set of η\etaη satisfying Q(x)+ηT(y−x)≤Q(y)Q(x) + \eta^{\mathsf T}(y-x) \le Q(y)Q(x)+ηT(y−x)≤Q(y) for every yyy (p. 115).

A simple-recourse instance is the special case W=[I,−I]W = [I,-I]W=[I,−I]: the recourse cost splits as q=(q+,q−)q = (q^+,q^-)q=(q+,q−), and Q(x)Q(x)Q(x) decomposes componentwise via the closed form of Eq. (1.9)-(1.10) using the (left- and right-limit) distribution functions Fi−,Fi+F_i^-, F_i^+Fi−​,Fi+​ of each hih_ihi​.

Formalization targets

Goal -- Chapter 3, Theorem 9 (p. 116)

x∗∈K1 is optimal in (1.2)  ⟺  ∃ λ∗∈Rm1, μ∗∈R≥0n1, (μ∗)Tx∗=0,  s.t. −c+ATλ∗+μ∗∈∂Q(x∗),x^* \in K_1 \text{ is optimal in (1.2)} \iff \exists\, \lambda^* \in \mathbb{R}^{m_1},\ \mu^* \in \mathbb{R}^{n_1}_{\ge 0},\ (\mu^*)^{\mathsf T}x^* = 0,\ \text{ s.t. } -c + A^{\mathsf T}\lambda^* + \mu^* \in \partial Q(x^*),x∗∈K1​ is optimal in (1.2)⟺∃λ∗∈Rm1​, μ∗∈R≥0n1​​, (μ∗)Tx∗=0,  s.t. −c+ATλ∗+μ∗∈∂Q(x∗),

given that (1.2) has a finite optimal value. This is the KKT-style necessary and sufficient optimality condition for the two-stage recourse LP, and the weakest of the mission's targets in the sense that everything else supports it: convexity and finiteness of QQQ (Theorem 6) are what make the left-to-right implication meaningful, closedness/convexity of K2K_2K2​ (Theorem 5) makes the feasible region well-posed, and attainment (Theorem 8) is what makes "x∗x^*x∗ is optimal" a statement about a point that exists rather than an infimum that may not be reached.

Supporting milestones

  • Theorem 5(a) (p. 111): K2K_2K2​ is closed and convex.
  • Theorem 6(a) (p. 112): QQQ is finite on K2K_2K2​, and Lipschitzian and convex there.
  • Theorem 8 (p. 115): under boundedness of K1∩K2K_1 \cap K_2K1​∩K2​ or eventual linearity of QQQ along recession directions, a finite optimal value is attained.
  • Corollary 10 (p. 116): Theorem 9 specialized to simple recourse, with ∂Q(x∗)\partial Q(x^*)∂Q(x∗) replaced by its explicit componentwise description.

Significance

Theorem 9 is the hinge on which the rest of the book's algorithmic chapters turn. The L-shaped method (Chapter 5) is a cutting-plane scheme whose cuts are literally elements of ∂Q(x)\partial Q(x)∂Q(x); stochastic decomposition and sampling-based methods use the same subdifferential structure with estimated cuts; the differentiable specialization (Eq. (1.14), c+∇Q(x∗)=ATλ∗+μ∗c + \nabla Q(x^*) = A^{\mathsf T}\lambda^* + \mu^*c+∇Q(x∗)=ATλ∗+μ∗) underlies nonlinear-programming approaches to the smooth case. None of this is meaningful without first knowing QQQ is convex, finite where it needs to be, and that a minimizer exists to characterize. Formalizing this mission's four milestones from the actual definition of QQQ as an embedded linear program's value -- rather than assuming these properties -- is exactly the content the book itself proves (or, for Theorem 6, explicitly cites to Wets [1972] and Kall [1976] rather than proving); this mission asks for genuine Lean proofs of Theorems 5, 8, 9 and Corollary 10 from the LP structure of QQQ, and records Theorem 6 as a stated (not re-derived) input, matching the book's own presentation.

Difficulty

The obvious shortcut is to treat QQQ as an opaque convex function and apply a textbook convex-KKT theorem off the shelf. This fails to capture what Theorem 9 actually is: a statement about the specific function Q(x)=∑kpkmin⁡y{qkTy∣Wy=hk−Tkx, y≥0}Q(x) = \sum_k p_k \min_y\{q_k^{\mathsf T}y \mid Wy = h_k - T_k x,\ y \ge 0\}Q(x)=∑k​pk​miny​{qkT​y∣Wy=hk​−Tk​x, y≥0}, built from finitely many parametric linear programs, each of which can be infeasible (Q(x,ξk)=+∞Q(x,\xi_k) = +\inftyQ(x,ξk​)=+∞) or unbounded (Q(x,ξk)=−∞Q(x,\xi_k) = -\inftyQ(x,ξk​)=−∞) depending on xxx. Convexity of QQQ must come from convexity of the value function of a parametric LP in its right-hand side (the book's Theorem 2 argument: a convex combination of optimal solutions at two right-hand sides is feasible, hence suboptimal, at the combined right-hand side) -- not from an assumed hypothesis. Handling ±∞\pm\infty±∞ correctly is a second, easy-to-miss source of error: the book fixes an explicit, non-default convention (+∞+\infty+∞ dominates −∞-\infty−∞) for combining per-scenario values, the opposite of the convention Mathlib's own extended-real arithmetic uses, so any formalization that reaches for EReal's built-in addition to aggregate QQQ silently states a different theorem. Theorem 8's attainment condition is a genuine existence result, not an automatic consequence of convexity: continuity alone does not give attainment on an unbounded feasible region, and the book's own counterexample (Eq. (1.11), a negative-exponential tail with infimum 000 attained by no finite xxx) shows the boundedness/recession hypotheses are load-bearing.

Formalization scope

The scenario set is modeled as Fin K, a finite discrete random variable, matching Section 3.1b's development; under this model "ξ\xiξ has finite second moments" (the standing hypothesis of Theorems 4-11 in the general, possibly-continuous case) holds automatically and so does not appear as a separate hypothesis anywhere in this mission. Q(x,\xi_k) is defined as an EReal via sInf of the second-stage LP's feasible objective values -- sInf of the empty set is ⊤, and of a set unbounded below is ⊥ -- and is genuinely derived from that inner minimization rather than assumed convex; this rules out the chapter's trivializing formalization, which the paper-level triage explicitly warns against: taking Q(x) as an opaque convex-function hypothesis instead of deriving its properties from the inner LP's structure. Aggregating the KKK per-scenario values into Q(x)Q(x)Q(x) uses a bespoke bookAdd operation implementing the book's stated convention +∞+(−∞)=+∞+\infty+(-\infty)=+\infty+∞+(−∞)=+∞, since Mathlib's EReal addition is defined with the opposite convention (⊥+⊤=⊤+⊥=⊥\bot+\top=\top+\bot=\bot⊥+⊤=⊤+⊥=⊥). ∂Q(x)\partial Q(x)∂Q(x) is the ordinary subgradient-inequality set for this extended-real-valued function.

Theorem 8's condition (b) is stated with the book's own quantifier structure: the threshold λˉ\bar\lambdaλˉ and the recession value depend on the point xxx and direction vvv exactly as written, with no strengthening. Theorem 6(a)'s Lipschitz bound is stated, not derived -- the book itself cites it to Wets [1972] and Kall [1976] without proof -- so a faithful Lean proof of that milestone is expected to remain out of scope for this mission. Corollary 10 similarly takes the closed form of ∂Qi(x)\partial Q_i(x)∂Qi​(x) from Eq. (1.10) as a hypothesis on an abstract QQQ, matching how the book itself uses (1.10) as an already-established fact rather than re-deriving it from the second-stage LP in the corollary's own proof. Theorem 11's subdifferential-decomposition result (∂Q(x)=Eω[∂Q(x,ξ(ω))]+N(K2,x)\partial Q(x) = E_\omega[\partial Q(x,\xi(\omega))] + N(K_2,x)∂Q(x)=Eω​[∂Q(x,ξ(ω))]+N(K2​,x)) is deliberately left out of this mission's scope: it is not needed by Theorem 9's own proof, and its normal-cone term would require relatively-complete-recourse machinery this mission does not otherwise need. No prior-art match was found on the platform: VectorSpaceOpt.fenchel_duality and the Luenberger-derived VectorSpaceOpt.generalized_kuhn_tucker / kkt_complementary_slackness family use a differentiable (Gateaux-derivative) or conjugate-function KKT model over general normed spaces, not this chapter's finite-dimensional, possibly-nondifferentiable subgradient formulation over the specific polyhedral set K1K_1K1​, so none is a faithful match and all items here are original drafts.

Selected references

  • J.R. Birge and F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer Series in Operations Research and Financial Engineering, Springer, 2011. https://doi.org/10.1007/978-1-4614-0237-4
  • R.J-B. Wets, "Programming Under Uncertainty: The Equivalent Convex Program," SIAM Journal on Applied Mathematics 14 (1966), 89-105 (Lipschitz continuity of the recourse function, cited by the book as Wets [1972] for the closely related result used in Theorem 6). https://doi.org/10.1137/0114008
  • D.P. Walkup and R.J-B. Wets, "Stochastic Programs with Recourse," SIAM Journal on Applied Mathematics 15 (1967), 1299-1314 (finiteness of the recourse function and coincidence of the possibility and expectation feasibility sets, underlying Proposition 3 and Theorem 4). https://doi.org/10.1137/0115113
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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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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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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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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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Control TheoryDynamic ProgrammingOperations Research+1·Captain: Shuze Chen

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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Graph TheoryOperations Research·Captain: Shuze Chen

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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Algebraic TopologyPure Mathematics·Captain: korbonits

Hatcher Algebraic Topology I: The Fundamental Group of the CircleTextbook

Motivation

The fundamental group π1(X,x0)\pi_1(X, x_0)π1​(X,x0​) is the first algebraic invariant a student of topology meets, and π1(S1)≅Z\pi_1(S^1)\cong\mathbb{Z}π1​(S1)≅Z is the first computation of it that carries real content. Allen Hatcher's Algebraic Topology (Cambridge University Press, 2002; freely available at pi.math.cornell.edu/~hatcher/AT/AT.pdf) is the standard text on the subject. Its Chapter 1 opens with exactly this computation (Theorem 1.7, p. 29) and immediately draws three classical consequences from it: the Fundamental Theorem of Algebra (Theorem 1.8), the Brouwer fixed point theorem for the disk (Theorem 1.9), and the Borsuk–Ulam theorem for the sphere (Theorem 1.10).

This mission is the opening entry in a series that formalizes Hatcher's book capstone by capstone. It covers the subsection "The Fundamental Group of the Circle" of Section 1.1 (pp. 29–33): the covering-space lifting properties that drive the proof, the theorem itself, and its three applications. Later entries in the series (van Kampen's theorem, the classification of covering spaces, simplicial and singular homology) will build on the declarations introduced here, which all live in the shared Lean namespace Hatcher.

Setting

A path in a topological space XXX is a continuous map f:I→Xf : I \to Xf:I→X, where I=[0,1]I = [0,1]I=[0,1]. A homotopy of paths is a family ft:I→Xf_t : I \to Xft​:I→X, 0≤t≤10 \le t \le 10≤t≤1, such that the endpoints ft(0)=x0f_t(0) = x_0ft​(0)=x0​ and ft(1)=x1f_t(1) = x_1ft​(1)=x1​ are independent of ttt and the associated map F:I×I→XF : I \times I \to XF:I×I→X, F(s,t)=ft(s)F(s,t) = f_t(s)F(s,t)=ft​(s), is continuous. A loop at a basepoint x0x_0x0​ is a path with f(0)=f(1)=x0f(0) = f(1) = x_0f(0)=f(1)=x0​. The set of homotopy classes [f][f][f] of loops at x0x_0x0​ is the fundamental group π1(X,x0)\pi_1(X, x_0)π1​(X,x0​); its product is [f][g]=[f⋅g][f][g] = [f\cdot g][f][g]=[f⋅g], where f⋅gf\cdot gf⋅g traverses fff and then ggg, each at double speed (Hatcher, Proposition 1.3).

The circle S1⊂R2S^1 \subset \mathbb{R}^2S1⊂R2 is realised as the unit circle of C\mathbb{C}C, so the point (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta)(cosθ,sinθ) is eiθe^{i\theta}eiθ and the basepoint (1,0)(1,0)(1,0) is 111. Hatcher's map

p:R→S1,p(s)=(cos⁡2πs,sin⁡2πs)=e2πisp : \mathbb{R} \to S^1, \qquad p(s) = (\cos 2\pi s, \sin 2\pi s) = e^{2\pi i s}p:R→S1,p(s)=(cos2πs,sin2πs)=e2πis

is Hatcher.circleCover. The loops

ωn(s)=(cos⁡2πns,sin⁡2πns)=p(ns),n∈Z,\omega_n(s) = (\cos 2\pi n s, \sin 2\pi n s) = p(ns), \qquad n \in \mathbb{Z},ωn​(s)=(cos2πns,sin2πns)=p(ns),n∈Z,

based at (1,0)(1,0)(1,0) are Hatcher.omegaLoopN n, and ω=ω1\omega = \omega_1ω=ω1​ is Hatcher.omegaLoop; its class [ω]∈π1(S1,1)[\omega] \in \pi_1(S^1, 1)[ω]∈π1​(S1,1) is Hatcher.omegaClass.

A covering space of XXX is a space X~\tilde XX~ together with a map p:X~→Xp : \tilde X \to Xp:X~→X such that every x∈Xx \in Xx∈X has an open neighbourhood UUU for which p−1(U)p^{-1}(U)p−1(U) is a disjoint union of open sets each mapped homeomorphically onto UUU by ppp (Hatcher's condition (∗)(\ast)(∗), p. 29; such a UUU is evenly covered). A lift of a map f:Y→Xf : Y \to Xf:Y→X is a map f~:Y→X~\tilde f : Y \to \tilde Xf~​:Y→X~ with p∘f~=fp \circ \tilde f = fp∘f~​=f.

Formalization targets

Goal (Theorem 1.7)

π1(S1,1)\pi_1(S^1, 1)π1​(S1,1) is an infinite cyclic group generated by [ω][\omega][ω]. In the form stated in Lean:

∀ g∈π1(S1,1)∃! n∈Z:[ω]n=g.\forall\, g \in \pi_1(S^1, 1)\quad \exists!\, n \in \mathbb{Z}:\quad [\omega]^n = g.∀g∈π1​(S1,1)∃!n∈Z:[ω]n=g.

Surjectivity of n↦[ω]nn \mapsto [\omega]^nn↦[ω]n says [ω][\omega][ω] generates; uniqueness of nnn says the group is infinite cyclic rather than finite.

Milestones on the road to the goal

  1. p(s)=e2πisp(s) = e^{2\pi i s}p(s)=e2πis is a covering space of S1S^1S1 (Hatcher, p. 29).
  2. Homotopy lifting property (c): for a covering space p:X~→Xp : \tilde X \to Xp:X~→X, a map F:Y×I→XF : Y \times I \to XF:Y×I→X and a lift of F∣Y×{0}F|_{Y \times \{0\}}F∣Y×{0}​ extend uniquely to a lift of FFF (p. 30).
  3. Path lifting property (a): a path fff starting at x0x_0x0​ and a point x~0∈p−1(x0)\tilde x_0 \in p^{-1}(x_0)x~0​∈p−1(x0​) determine a unique lift f~\tilde ff~​ starting at x~0\tilde x_0x~0​ (p. 29).
  4. Lifting homotopies of paths (b): a homotopy of paths ftf_tft​ starting at x0x_0x0​ lifts uniquely to a homotopy of paths f~t\tilde f_tf~​t​ starting at x~0\tilde x_0x~0​ (p. 29).
  5. Every loop in S1S^1S1 at (1,0)(1,0)(1,0) is homotopic to ωn\omega_nωn​ for a unique n∈Zn \in \mathbb{Z}n∈Z (the reformulation of Theorem 1.7 that Hatcher actually proves, p. 29).
  6. [ω]n=[ωn][\omega]^n = [\omega_n][ω]n=[ωn​] for every n∈Zn \in \mathbb{Z}n∈Z (Hatcher's remark after Theorem 1.7, p. 29).

Applications (Theorems 1.8–1.10)

Every nonconstant f∈C[z] has a root in C.\text{Every nonconstant } f \in \mathbb{C}[z] \text{ has a root in } \mathbb{C}.Every nonconstant f∈C[z] has a root in C. Every continuous h:D2→D2 has a fixed point.\text{Every continuous } h : D^2 \to D^2 \text{ has a fixed point.}Every continuous h:D2→D2 has a fixed point. Every continuous f:S2→R2 satisfies f(x)=f(−x) for some x∈S2.\text{Every continuous } f : S^2 \to \mathbb{R}^2 \text{ satisfies } f(x) = f(-x) \text{ for some } x \in S^2.Every continuous f:S2→R2 satisfies f(x)=f(−x) for some x∈S2.

Significance

The result itself. The computation π1(S1)≅Z\pi_1(S^1) \cong \mathbb{Z}π1​(S1)≅Z assigns to every loop in the circle an integer, its winding number, and shows that this integer is the only homotopy invariant of the loop. It is the seed of degree theory, and in Hatcher's text it is the starting point for every later computation of fundamental groups (products, van Kampen, covering spaces). The three applications are the standard demonstration that a single algebraic invariant can settle purely geometric or algebraic existence questions.

Formalizing it. Mathlib (revision 0df444a) already contains the covering-space infrastructure: IsCoveringMap, path lifting (IsCoveringMap.liftPath, eq_liftPath_iff'), homotopy lifting (IsCoveringMap.liftHomotopy, eq_liftHomotopy_iff'), monodromy, and the fact that Circle.exp is a covering map (Circle.isCoveringMap_exp). It also has FundamentalGroup X x as the endomorphism group of the fundamental groupoid. It does not contain the computation π1(S1)≅Z\pi_1(S^1) \cong \mathbb{Z}π1​(S1)≅Z, nor the two-dimensional Brouwer and Borsuk–Ulam theorems. The Fundamental Theorem of Algebra is in Mathlib as Complex.exists_root (proved by Liouville's theorem rather than by Hatcher's argument); it is kept as a milestone because it is one of the section's stated theorems, and a solver may close it directly from Mathlib. Milestones 2–4 are also within reach of the existing lifting API, but they are the lemmas Hatcher states and uses, and a faithful record of them in the mission's own namespace is what later entries in the series will import.

Difficulty

The obvious first idea for the goal is to define the winding number of a loop through the complex argument. That fails because arg⁡\argarg is discontinuous on S1S^1S1; the integer has to be produced by lifting the loop through ppp and reading off the endpoint of the lift, which is only well defined because of the uniqueness in the path lifting property. The second difficulty is uniqueness of nnn: this needs lifting of homotopies (milestone 4), not just of paths, together with the observation that a lifted homotopy of paths has constant endpoints.

Connecting the concrete loops to Mathlib's abstract π1\pi_1π1​ is its own obstacle. FundamentalGroup Circle 1 multiplies by composing morphisms of the fundamental groupoid, so identifying [ω]n[\omega]^n[ω]n with the class of the explicit loop ωn\omega_nωn​ (milestone 6) requires reparametrization arguments for concatenated paths, for negative nnn as well as positive.

For Theorem 1.9 the difficulty is the construction and continuity of the retraction r:D2→S1r : D^2 \to S^1r:D2→S1 from a fixed-point-free map, and then the non-existence of a retraction, which uses that π1(S1)≠0\pi_1(S^1) \neq 0π1​(S1)=0. For Theorem 1.10 Hatcher's proof lifts a loop g(s)=f(cos⁡2πs,sin⁡2πs)/∣⋯∣g(s) = f(\cos 2\pi s, \sin 2\pi s)/\lvert \cdots \rvertg(s)=f(cos2πs,sin2πs)/∣⋯∣ through ppp and shows the lift changes by an odd integer over half a turn; making that parity argument rigorous in Lean is the substance of the milestone.

Formalization scope

  • S1S^1S1 is Circle (the unit circle in C\mathbb{C}C) with basepoint 1; D2D^2D2 is Metric.closedBall (0 : EuclideanSpace ℝ (Fin 2)) 1; S2S^2S2 is Metric.sphere (0 : EuclideanSpace ℝ (Fin 3)) 1, with −x-x−x the antipodal point.
  • A covering space is Mathlib's IsCoveringMap p. This agrees with Hatcher's condition (∗)(\ast)(∗); neither requires ppp to be surjective.
  • Paths are continuous maps C(I, X) or Mathlib Paths; for homotopies of paths, the square is written I × I with Hatcher's coordinate order F(s,t)=ft(s)F(s,t) = f_t(s)F(s,t)=ft​(s): the first coordinate is the path parameter, the second the homotopy parameter. In the general homotopy lifting property the domain is Y × I with YYY an arbitrary topological space, as in Hatcher.
  • π1(S1,1)\pi_1(S^1, 1)π1​(S1,1) is Mathlib's FundamentalGroup Circle 1, and [ω][\omega][ω] is FundamentalGroup.fromPath ⟦omegaLoop⟧. Because the goal quantifies over integer powers of a single element, the order of multiplication in FundamentalGroup is immaterial to its truth.
  • The goal is stated as ∀g ∃!n, [ω]n=g\forall g\, \exists! n,\ [\omega]^n = g∀g∃!n, [ω]n=g rather than as an abstract isomorphism with Z\mathbb{Z}Z, so that the generator is pinned to Hatcher's explicit loop; an isomorphism FundamentalGroup Circle 1 ≃* Multiplicative ℤ sending [ω][\omega][ω] to 111 is an immediate corollary and a welcome contribution.
  • "Nonconstant polynomial" is 0 < f.degree, which excludes both the zero polynomial and nonzero constants.

Contributions welcome: proofs of the milestones from Mathlib's lifting API, a degree homomorphism π1(S1,1)→Z\pi_1(S^1,1) \to \mathbb{Z}π1​(S1,1)→Z packaged for reuse, and any lemma about concatenation and reparametrization of loops in Circle that later chapters of the series can import.

Selected references

  • A. Hatcher, Algebraic Topology, Cambridge University Press, 2002. Section 1.1, "The Fundamental Group of the Circle", pp. 29–33. https://pi.math.cornell.edu/~hatcher/AT/AT.pdf
  • L. E. J. Brouwer, Über Abbildung von Mannigfaltigkeiten, Mathematische Annalen 71 (1911), 97–115. https://doi.org/10.1007/BF01456931
  • K. Borsuk, Drei Sätze über die n-dimensionale euklidische Sphäre, Fundamenta Mathematicae 20 (1933), 177–190. https://doi.org/10.4064/fm-20-1-177-190
  • Mathlib, Mathlib/Topology/Homotopy/Lifting.lean (path and homotopy lifting for covering maps). https://github.com/leanprover-community/mathlib4/blob/0df444a360eaa60ab8c11dca51a86af692955474/Mathlib/Topology/Homotopy/Lifting.lean
  • Mathlib, Mathlib/AlgebraicTopology/FundamentalGroupoid/FundamentalGroup.lean (the fundamental group). https://github.com/leanprover-community/mathlib4/blob/0df444a360eaa60ab8c11dca51a86af692955474/Mathlib/AlgebraicTopology/FundamentalGroupoid/FundamentalGroup.lean
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Algorithmic Game TheoryTheoretical Computer Science·Captain: Shuze Chen

Algorithmic Game Theory I: Existence of Nash EquilibriumTextbook

Motivation

The strategic-form game is the basic object of noncooperative game theory, and the Nash equilibrium — a profile of randomized strategies from which no player benefits by deviating unilaterally — is its central solution concept. Nash proved in 1951 that every game with finitely many players and finite strategy sets has such an equilibrium (Nash, Non-cooperative games, Ann. Math. 54 (1951)); this single existence theorem is the reason the concept organizes the rest of the field, from the computational complexity of finding equilibria to the price of anarchy. The theorem is stated as Theorem 1.8 of Nisan–Roughgarden–Tardos–Vazirani (eds.), Algorithmic Game Theory (Cambridge, 2007), the source text of this mission series, whose first chapter (Tardos–Vazirani) also treats the two special cases that admit direct algorithmic proofs: two-person zero-sum games, where equilibria are exactly the optimal solutions of a dual pair of linear programs (von Neumann 1928; Theorem 1.11), and a simple linear market, where equilibrium prices are computed by an ascending tight-set algorithm (Theorem 1.17).

A timeline of the existence theorem: von Neumann (1928) proved the minimax theorem for two-person zero-sum games; Nash (1950, 1951) extended existence to arbitrary finite games, first via Kakutani's fixed-point theorem and then via Brouwer's. All known proofs of the general theorem pass through a fixed-point principle, and this is not an artifact: computing a Nash equilibrium is PPAD-complete (Daskalakis–Goldberg–Papadimitriou 2009; Chen–Deng–Teng 2009), and PPAD is precisely the complexity class of the fixed-point arguments.

Setting

A finite strategic-form game consists of a finite set ι\iotaι of players, for each player iii a finite nonempty set SiS_iSi​ of pure strategies, and for each player a payoff function ui:∏jSj→Ru_i : \prod_j S_j \to \mathbb{R}ui​:∏j​Sj​→R; all players are utility maximizers. A mixed strategy for player iii is a probability distribution on SiS_iSi​, represented as a weight function σi:Si→R\sigma_i : S_i \to \mathbb{R}σi​:Si​→R with σi≥0\sigma_i \ge 0σi​≥0 and ∑sσi(s)=1\sum_{s} \sigma_i(s) = 1∑s​σi​(s)=1 (a lottery). Players randomize independently, so a mixed profile σ=(σi)i\sigma = (\sigma_i)_{i}σ=(σi​)i​ induces the product distribution on pure strategy vectors, and player iii's expected payoff is

Ui(σ)  =  ∑s∈∏jSj(∏jσj(sj)) ui(s).U_i(\sigma) \;=\; \sum_{s \in \prod_j S_j} \Big(\prod_j \sigma_j(s_j)\Big)\, u_i(s).Ui​(σ)=s∈∏j​Sj​∑​(j∏​σj​(sj​))ui​(s).

A mixed profile σ\sigmaσ is a (mixed) Nash equilibrium if for every player iii and every lottery τ\tauτ on SiS_iSi​, replacing σi\sigma_iσi​ by τ\tauτ does not increase UiU_iUi​.

A two-person zero-sum game is given by a matrix A∈Rm×nA \in \mathbb{R}^{m \times n}A∈Rm×n: the row player picks a row distribution ppp, the column player a column distribution qqq, and the column player pays the row player pTAqp^{\mathsf T} A qpTAq in expectation.

The market of §1.8.1 of the source has finitely many divisible goods, good aaa in sas_asa​ units, and finitely many buyers, buyer jjj bringing budget mj>0m_j > 0mj​>0 and interested in a nonempty set of goods; utilities are linear 0/1, so a buyer wants any goods from her interest set and none other. Market-clearing prices are positive prices under which each buyer can spend her whole budget on cheapest goods in her interest set while every good sells out exactly.

Formalization targets

Goal (capstone) — Theorem 1.8

Every finite strategic-form game has a mixed Nash equilibrium.\text{Every finite strategic-form game has a mixed Nash equilibrium.}Every finite strategic-form game has a mixed Nash equilibrium.

Stated for an arbitrary finite family of finite nonempty strategy types; no bound on the number of players, no genericity assumptions.

Supporting — Brouwer fixed-point theorem

K⊆E nonempty compact convex, E finite-dimensional, f:K→K continuous  ⟹  ∃x, f(x)=x.K \subseteq E \text{ nonempty compact convex},\ E \text{ finite-dimensional},\ f : K \to K \text{ continuous} \implies \exists x,\ f(x) = x.K⊆E nonempty compact convex, E finite-dimensional, f:K→K continuous⟹∃x, f(x)=x.

Mathlib currently has no form of Brouwer's theorem; every known proof of Theorem 1.8 needs it (or an equivalent), so it enters the mission as an explicit milestone rather than an assumed library fact.

Theorem 1.11 — zero-sum games

∃ p∗,q∗:∀p, pTAq∗≤p∗TAq∗,∀q, p∗TAq∗≤p∗TAq,and(p∗,q∗) is a mixed Nash equilibrium\exists\, p^\ast, q^\ast:\quad \forall p,\ p^{\mathsf T} A q^\ast \le {p^\ast}^{\mathsf T} A q^\ast, \quad \forall q,\ {p^\ast}^{\mathsf T} A q^\ast \le {p^\ast}^{\mathsf T} A q, \quad\text{and}\quad (p^\ast, q^\ast) \text{ is a mixed Nash equilibrium}∃p∗,q∗:∀p, pTAq∗≤p∗TAq∗,∀q, p∗TAq∗≤p∗TAq,and(p∗,q∗) is a mixed Nash equilibrium

of the explicit two-player game with payoffs AxyA_{xy}Axy​ to the row player and −Axy-A_{xy}−Axy​ to the column player. The source states the result as: optimal solutions of a dual pair of LPs form a Nash equilibrium of the zero-sum game; the first two conjuncts are the saddle point that LP optimality amounts to, and the third states the Nash-equilibrium clause against the mission's own game vocabulary, so "zero-sum" is formal (the two payoffs sum to zero) rather than implicit in the shape of the statement.

Theorem 1.17 (existence form)

The 0/1-utilities linear market admits market-clearing prices and allocations.\text{The 0/1-utilities linear market admits market-clearing prices and allocations.}The 0/1-utilities linear market admits market-clearing prices and allocations.

The source proves this by an ascending-price algorithm and also bounds its running time; the complexity half has no formal counterpart in this mission.

Significance

The capstone is the foundation of the whole mission series: correlated equilibria, price-of-anarchy bounds, and mechanism-design characterizations in later missions all quantify over or compare against Nash equilibria, and the series inherits its game vocabulary (IsLottery, IsMixedProfile, expectedPayoff, IsMixedNash) from this mission.

Formalizing it produces the first Brouwer fixed-point theorem in this environment — a well-known gap in mathlib with reuse value far beyond game theory (every degree-theoretic and equilibrium-existence argument needs it). The zero-sum milestone yields the minimax theorem, reusable for the learning-dynamics mission that follows. All results here are classical and proved on paper; the work requested is machine-checked proof, not new mathematics.

Difficulty

The central difficulty is Brouwer. The standard routes are (i) Sperner's lemma plus a limit argument, which needs a formal theory of simplicial subdivisions that does not exist in mathlib; (ii) algebraic topology (no retraction of the ball onto the sphere), for which mathlib has singular homology but not yet the homology of spheres in usable form; (iii) analytic proofs (Milnor–Rogers). None is short; the milestone is deliberately stated for a general nonempty compact convex set in a finite-dimensional normed space so that any route serves, and so the lemma lands in reusable generality.

Given Brouwer, Theorem 1.8 still requires Nash's gain-function construction on the product of simplices and the verification that fixed points are equilibria — bookkeeping-heavy but standard. Theorem 1.11 does not need Brouwer: mathlib's Sion minimax theorem (Mathlib.Topology.Sion) applies to the bilinear payoff on the product of standard simplices, or one can argue by LP duality directly. Theorem 1.17 needs the tight-set/max-flow argument of Lemmas 1.15–1.16 or any direct construction of the equilibrium.

Formalization scope

Games are presented concretely: players form a finite index type, strategies a finite type per player, payoffs are functions into R\mathbb{R}R; mixed strategies are weight functions with a IsLottery predicate, not measure-theoretic distributions. Deviations in the equilibrium definition range over all lotteries (not only pure strategies): the pure-deviation reduction is a lemma a solver may prove, not part of the definition. Strategy sets are assumed nonempty in the capstone; the player set need not be. In the zero-sum milestone both dimensions are positive (Fin (m+1), Fin (n+1)), payoffs flow from the column player to the row player, stdSimplex plays the role of the mixed-strategy space, and the Nash-equilibrium conjunct is stated for the Boolean-indexed two-player game built by matrixGameStrat/zeroSumPayoff/matrixGameProfile from the definitions bundle. In the market milestone all supplies and budgets are positive, every buyer's interest set is nonempty, and every good has an interested buyer, matching the standing assumptions of §1.8.1; allocations are recorded as money spent, so the clearing condition is ∑jxja=pasa\sum_j x_{ja} = p_a s_a∑j​xja​=pa​sa​ with no division anywhere.

Trivializing readings are ruled out: the empty simplex has no lotteries, so nonemptiness hypotheses appear exactly where their absence would make an existence claim false (Brouwer on the empty set, games with an empty strategy set, zero-dimensional matrix games).

Selected references

  • J. F. Nash, Non-cooperative games, Annals of Mathematics 54 (1951), 286–295. DOI
  • J. von Neumann, Zur Theorie der Gesellschaftsspiele, Mathematische Annalen 100 (1928), 295–320. DOI
  • N. Nisan, T. Roughgarden, É. Tardos, V. V. Vazirani (eds.), Algorithmic Game Theory, Cambridge University Press, 2007, Chapter 1. DOI
  • C. Daskalakis, P. W. Goldberg, C. H. Papadimitriou, The complexity of computing a Nash equilibrium, SIAM J. Computing 39 (2009), 195–259. DOI
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Theoretical Computer Science·Captain: marwahaha

Schönhage–Pan–Winograd Bound: omega < 2.522Research Paper

Motivation

The matrix-multiplication exponent measures the asymptotic arithmetic cost of multiplying square matrices. An upper bound ω<c\omega<cω<c means that, over the field under consideration, N×NN\times NN×N matrices can be multiplied using O(Nc+ε)O(N^{c+\varepsilon})O(Nc+ε) arithmetic operations for every ε>0\varepsilon>0ε>0. Improvements to ω\omegaω are a central benchmark in algebraic complexity because matrix multiplication is also a basic subroutine in linear algebra, graph algorithms, and symbolic computation.

The existing Prove2Me mission formalizes Schönhage's bound ω<2.55\omega<2.55ω<2.55 from a concrete two-summand tensor degeneration. The present mission advances the same formal development to the next clean historical construction. Pan and Winograd found a simultaneous approximate algorithm for three matrix products; Romani recorded its tensor form and the parameter choice n=11n=11n=11, k=5k=5k=5, which gives ω≤2.5218127…\omega\le 2.5218127\ldotsω≤2.5218127…. Schönhage's 1981 paper reports the equivalent bound 3log⁡52/log⁡1103\log 52/\log 1103log52/log110 in the arbitrary-field setting. The exact formal target here is the slightly weaker rational inequality ω<1261/500=2.522\omega<1261/500=2.522ω<1261/500=2.522.

Setting

For a field KKK, the matrix-multiplication tensor ⟨a,b,c⟩K\langle a,b,c\rangle_K⟨a,b,c⟩K​ encodes multiplication of an a×ba\times ba×b matrix by a b×cb\times cb×c matrix:

⟨a,b,c⟩K=∑i<a∑j<b∑ℓ<ceij⊗ejℓ⊗eℓi.\langle a,b,c\rangle_K =\sum_{i<a}\sum_{j<b}\sum_{\ell<c} e_{ij}\otimes e_{j\ell}\otimes e_{\ell i}.⟨a,b,c⟩K​=i<a∑​j<b∑​ℓ<c∑​eij​⊗ejℓ​⊗eℓi​.

A direct sum places several such tensors in disjoint coordinate blocks. A tensor TTT has border rank at most rrr when it is a polynomial degeneration of the diagonal tensor Ir=∑s<res⊗es⊗esI_r=\sum_{s<r}e_s\otimes e_s\otimes e_sIr​=∑s<r​es​⊗es​⊗es​. In the Lean development this relation is Degenerates T (TensorObj.diagObj K 3 r). The argument order matters: the first tensor is the target and the diagonal tensor is the source.

The platform already defines ordinary tensor rank, asymptotic tensor rank, the tensor-rank exponent matMulExp K, the equivalent Strassen-preorder exponent matMulExp_strassen K, and Schönhage's asymptotic sum inequality. This mission reuses those declarations. No alternative definition of ω\omegaω is introduced.

Formalization targets

The goal has exactly the same quantified proposition as the existing 2.552.552.55 mission, with only the rational endpoint changed:

∀K  [Field(K)],matMulExp⁡(K)<1261500.\forall K\;[\mathrm{Field}(K)],\qquad \operatorname{matMulExp}(K)<\frac{1261}{500}.∀K[Field(K)],matMulExp(K)<5001261​.

The source construction to be formalized is

R‾ ⁣(⟨1,5,22⟩K⊕⟨11,2,5⟩K⊕⟨10,11,1⟩K)≤156.\underline R\!\left( \langle1,5,22\rangle_K\oplus \langle11,2,5\rangle_K\oplus \langle10,11,1\rangle_K \right)\le156.R​(⟨1,5,22⟩K​⊕⟨11,2,5⟩K​⊕⟨10,11,1⟩K​)≤156.

Each summand has volume 110110110:

1⋅5⋅22=11⋅2⋅5=10⋅11⋅1=110.1\cdot5\cdot22=11\cdot2\cdot5=10\cdot11\cdot1=110.1⋅5⋅22=11⋅2⋅5=10⋅11⋅1=110.

The milestone chain records the degeneration, its asymptotic-rank consequence, the exact numerical implication

3⋅110ωKStr/3≤156⟹ωKStr<1261500,3\cdot110^{\omega^{\mathrm{Str}}_K/3}\le156 \quad\Longrightarrow\quad \omega^{\mathrm{Str}}_K<\frac{1261}{500},3⋅110ωKStr​/3≤156⟹ωKStr​<5001261​,

and the resulting Strassen-form exponent bound. The public goal then transfers the bound to matMulExp K through the already established equality of the two exponent definitions.

Significance

Mathematically, this construction improves the concrete exponent certified by the existing mission from 2.552.552.55 to 2.5222.5222.522 without changing the surrounding theory. It isolates the first genuinely new ingredient after the accepted Schönhage example: a larger simultaneous tensor degeneration rather than a sharper numerical estimate for the old witness.

For formalization, the mission tests whether the current polynomial-degeneration API can express a historically important trilinear aggregation at realistic scale. Once the explicit witness is available, the remaining declarations form a reusable template for later bounds: a source tensor degeneration, an asymptotic-rank bound, a specialization of the asymptotic sum inequality, and a final exponent transfer. This creates a trustworthy stepping stone toward the Coppersmith--Winograd tensor and later laser-method analyses.

The 2.5222.5222.522 theorem is known mathematically; the open work is its machine-checked Lean formalization. The exact numerical endpoint and every downstream bridge from the degeneration have already been checked locally. The explicit Pan--Winograd degeneration remains the substantive open milestone.

Difficulty

The central difficulty is not the logarithmic comparison. It is constructing and verifying the polynomial family whose leading nonzero coefficient is exactly the tagged direct sum of the three matrix-multiplication tensors and whose earlier coefficients vanish. The family has 156156156 diagonal source slots and many indexed target coordinates. A proof must account for all mixed-coordinate terms and all cancellations uniformly over an arbitrary field.

Romani's published summary states the approximate-rank inequality but does not spell out a Lean-ready map between its trilinear forms and the platform's TensorObj.bigAdd coordinate spaces. A solver must therefore recover the source indexing carefully and prove that the resulting modewise linear maps have the required coefficients. Reversing the degeneration direction, conflating tensor rank with asymptotic rank, or silently assuming a characteristic-zero scalar identity would invalidate the result.

Formalization scope

All theorems quantify over an arbitrary type KKK with [Field K], matching the existing Schönhage goal and the arbitrary-field statement of the source bound. Tensor spaces are finite-dimensional function spaces already packaged by MMObj; the three products are combined with TensorObj.bigAdd. Border rank is represented by the existing finitely supported polynomial-family predicate Degenerates. Because the source summary specifies approximate rank but not a leading order, the main degeneration milestone existentially quantifies that order instead of hard-coding one.

The mission includes no placeholder laser-value definition and makes no claim about the later 2.3762.3762.376 analysis. It also excludes Schönhage's additional microscopic symmetrization improvement beyond 3log⁡52/log⁡1103\log52/\log1103log52/log110. A valid solution must construct the stated degeneration itself; a vacuous hypothesis or a redefinition of matMulExp is outside scope.

Reusable contributions include coefficient lemmas for polynomial tensor families, finite-index equivalences for direct sums, and generic aggregation identities that specialize to the n=11n=11n=11, k=5k=5k=5 witness. Contributions that merely restate the target under stronger field hypotheses do not close the arbitrary-field milestone.

Selected references

  • A. Schönhage, Partial and Total Matrix Multiplication, SIAM Journal on Computing 10(3), 1981, pp. 434--455. DOI 10.1137/0210032.
  • Francesco Romani, Some Properties of Disjoint Sums of Tensors Related to Matrix Multiplication, CNR Nota Interna B80-4, February 1980, printed p. 6; journal version, SIAM Journal on Computing 11(2), 1982. Archived preprint and DOI 10.1137/0211020.
  • Avi Wigderson and Jeroen Zuiddam, Asymptotic Spectra: Theory, Applications and Extensions, 2023, for the tensor-preorder and asymptotic-rank framework reused by the Lean development. Author manuscript.
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Markov ChainProbabilityStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times VIII: Path Coupling and Approximate CountingTextbook

Motivation

The coupling method of Mission III asks for a coupling of two copies of a chain from every pair of starting states — often painful to construct globally. Chapter 14 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) replaces that global demand by a local one. The path coupling technique of Bubley and Dyer says: put a connected graph structure on the state space, and couple one step of the chain only across edges; if each edge contracts in expectation, contraction propagates automatically along paths to arbitrary pairs of distributions. The bookkeeping runs through the transportation metric (Kantorovich distance) between distributions, whose theory — attainment by an optimal coupling, the triangle inequality — is developed on the way. The chapter's payoff is the sharpest elementary bound for sampling proper colorings (Theorem 14.8: the Glauber dynamics mixes in O(nlog⁡n)O(n\log n)O(nlogn) steps once q>2Δq>2\Deltaq>2Δ), and, through the sampling-to-counting reduction of Jerrum–Valiant–Vazirani, a polynomial-time approximation algorithm for counting colorings — the paradigm of the Markov chain Monte Carlo method as an algorithmic tool.

Setting

All chains live on a finite state space VVV with a transition matrix PPP; Pt(x,⋅)P^t(x,\cdot)Pt(x,⋅) is the time-ttt distribution from xxx, ∥μ−ν∥TV=max⁡A⊆V∣μ(A)−ν(A)∣\|\mu-\nu\|_{TV}=\max_{A\subseteq V}|\mu(A)-\nu(A)|∥μ−ν∥TV​=maxA⊆V​∣μ(A)−ν(A)∣ the total variation distance, d(t)=max⁡x∥Pt(x,⋅)−π∥TVd(t)=\max_x\|P^t(x,\cdot)-\pi\|_{TV}d(t)=maxx​∥Pt(x,⋅)−π∥TV​ the worst-case distance to the stationary distribution π\piπ, and tmix(ε)=min⁡{t:d(t)≤ε}t_{\mathrm{mix}}(\varepsilon)=\min\{t:d(t)\le\varepsilon\}tmix​(ε)=min{t:d(t)≤ε} the mixing time. A coupling of distributions μ,ν\mu,\nuμ,ν is a distribution qqq on V×VV\times VV×V with marginals μ\muμ and ν\nuν.

Given a metric-like cost ρ\rhoρ on pairs of states, the transportation metric between two distributions is the cheapest expected cost of moving one onto the other:

ρK(μ,ν)=min⁡{∑x,yρ(x,y) q(x,y)  :  q a coupling of μ,ν}.\rho_K(\mu,\nu)=\min\Bigl\{\sum_{x,y}\rho(x,y)\,q(x,y)\;:\;q\ \text{a coupling of}\ \mu,\nu\Bigr\}.ρK​(μ,ν)=min{x,y∑​ρ(x,y)q(x,y):q a coupling of μ,ν}.

Given a connected graph structure GGG on the state space with edge lengths ℓ≥1\ell\ge1ℓ≥1, the path metric ρ(x,y)\rho(x,y)ρ(x,y) is the least total length of a GGG-path from xxx to yyy.

For the colorings application: a qqq-coloring of the vertices of a graph is proper when adjacent vertices receive distinct colors, and the Glauber dynamics on proper colorings picks a uniform vertex and re-samples its color uniformly among the colors legal there; its stationary distribution is uniform on the proper colorings. Throughout, nnn is the number of vertices and Δ\DeltaΔ the maximum degree of the graph being colored.

Formalization targets

Goal

Theorem 14.8, the capstone of Chapter 14: for the Glauber dynamics on proper qqq-colorings, if q>2Δq>2\Deltaq>2Δ then

tmix(ε)  ≤  ⌈q−Δq−2Δ  n (log⁡n−log⁡ε)⌉.t_{\mathrm{mix}}(\varepsilon)\;\le\;\Bigl\lceil\frac{q-\Delta}{q-2\Delta}\;n\,\bigl(\log n-\log\varepsilon\bigr)\Bigr\rceil.tmix​(ε)≤⌈q−2Δq−Δ​n(logn−logε)⌉.

Milestones

  • Lemma 14.3 and Remark 14.2 — the transportation distance is attained by an optimal coupling, and satisfies the triangle inequality (so it is a genuine metric on distributions).
  • Theorem 14.6, path coupling (Bubley–Dyer) — if for every edge {x,y}\{x,y\}{x,y} of a connected graph structure there is a coupling of the one-step distributions P(x,⋅),P(y,⋅)P(x,\cdot),P(y,\cdot)P(x,⋅),P(y,⋅) contracting the path metric by e−αe^{-\alpha}e−α in expectation, then one step of the chain contracts the transportation metric of arbitrary distribution pairs by e−αe^{-\alpha}e−α.
  • Corollary 14.7 — under the same hypotheses, d(t)≤e−αt diam(V)d(t)\le e^{-\alpha t}\,\mathrm{diam}(V)d(t)≤e−αtdiam(V) and tmix(ε)≤⌈(log⁡diam(V)−log⁡ε)/α⌉t_{\mathrm{mix}}(\varepsilon)\le\lceil(\log\mathrm{diam}(V)-\log\varepsilon)/\alpha\rceiltmix​(ε)≤⌈(logdiam(V)−logε)/α⌉, where diam(V)\mathrm{diam}(V)diam(V) is the largest path-metric distance between two states.
  • Theorem 14.12, approximate counting — for q>2Δq>2\Deltaq>2Δ there is a randomized estimator, computed from an explicit polynomial number of independent uniform random seeds, which with probability at least 1−η1-\eta1−η estimates the number of proper qqq-colorings within a (1±ε)(1\pm\varepsilon)(1±ε) factor: rapid sampling yields rapid approximate counting.

Significance

The results. Path coupling converted the coupling method from an art into a calculus: one bounds a single-edge contraction constant, and the machinery does the rest. It is the standard tool for Glauber dynamics on colorings, independent sets, and other constraint-satisfaction models, and the q>2Δq>2\Deltaq>2Δ colorings bound is its flagship application. Theorem 14.12 is the discrete embodiment of the Jerrum–Valiant–Vazirani equivalence between approximate counting and sampling — the conceptual foundation of the entire MCMC approach to #P\#\mathrm P#P-hard counting problems.

Formalizing them. Mathlib has no transportation/Kantorovich metric in the finite setting, no path coupling, and nothing on approximate counting. The transportation-metric layer (optimal couplings, triangle inequality) is reusable far beyond this mission — it is the finite Wasserstein distance. The path-coupling theorem feeds directly into Mission IX (Ising) and is quoted throughout modern mixing literature.

Difficulty

The transportation metric asks for minimization over the (compact) polytope of couplings: attainment is a finite-dimensional compactness argument, and the triangle inequality requires gluing two optimal couplings along their common marginal — the classic construction that must be carried out with explicit finite sums here. Path coupling itself is an induction along geodesics of the path metric, with the subtlety that the composite coupling produced along a path need not be optimal, only admissible; the bookkeeping of the contraction constant through the induction is exactly the kind of argument Lean keeps honest. Theorem 14.8 instantiates the machinery: the single-edge coupling for colorings needs a careful case analysis of the proposed recolorings at the two endpoints (matching legal colors bijectively), and the contraction constant (q−2Δ)/(q−Δ)(q-2\Delta)/(q-\Delta)(q−2Δ)/(q−Δ) emerges from counting disagreeing proposals. Theorem 14.12 layers a probabilistic-amplification argument (medians of means over independent runs) on top of the mixing bound; its combinatorial core — expressing ∣Ω∣−1|\Omega|^{-1}∣Ω∣−1 as a telescoping product of marginal probabilities — is elementary but notation-heavy, and the formal statement quantifies over explicit seed spaces, so the whole estimator is a finite object.

Formalization scope

The transportation metric is an sInf over coupling costs (the coupling polytope is nonempty for genuine distributions, and attainment is part of the milestone, so the junk value never propagates); the path metric is an sInf over walk lengths in a connected graph. The Glauber dynamics on colorings is the restriction to proper colorings of the single-site heat-bath chain of Mission II, matching §3.3 of the book; its state space is the subtype of proper colorings, nonempty whenever q>2Δq>2\Deltaq>2Δ (a fact the hypotheses of the goal supply). Mixing-time upper bounds are stated with the book's explicit ceilings, so no rounding slack is hidden. In Theorem 14.12 the estimator is presented concretely as a function of finitely many uniform seeds, and "with probability ≥1−η\ge1-\eta≥1−η" is a counting inequality over the seed space — no measure theory enters. Contributions of intermediate lemmas (optimal-coupling gluing, geodesic decompositions, colorings edge-coupling) are welcome and will be reused by Mission IX.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • R. Bubley, M. Dyer, Path coupling: a technique for proving rapid mixing in Markov chains, FOCS 1997. https://doi.org/10.1109/SFCS.1997.646111
  • M. Jerrum, A very simple algorithm for estimating the number of k-colorings of a low-degree graph, Random Structures Algorithms 7 (1995). https://doi.org/10.1002/rsa.3240070205
  • M. Jerrum, L. Valiant, V. Vazirani, Random generation of combinatorial structures from a uniform distribution, Theoret. Comput. Sci. 43 (1986). https://doi.org/10.1016/0304-3975(86)90174-X
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Markov ChainProbabilityStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times VI: Networks, Hitting Times, and Cover TimesTextbook

Motivation

A reversible Markov chain is an electrical network: states are nodes, and the conductance c(x,y)=π(x)P(x,y)c(x,y)=\pi(x)P(x,y)c(x,y)=π(x)P(x,y) turns hitting probabilities into voltages and hitting times into resistances. This dictionary, going back to Kakutani and popularized by Doyle and Snell, converts probabilistic estimates into the physical laws of circuits — series/parallel reduction, energy minimization, monotonicity under edge removal. Chapters 9–11 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) develop the dictionary and its two crown results: the commute time identity of Chandra–Raghavan–Ruzzo–Smolensky–Tiwari, Ea(τb)+Eb(τa)=cG R(a↔b)\mathbb E_a(\tau_b)+\mathbb E_b(\tau_a)=c_G\,R(a\leftrightarrow b)Ea​(τb​)+Eb​(τa​)=cG​R(a↔b), and the Matthews method bounding cover times by hitting times with harmonic-number precision.

Setting

A network is a symmetric nonnegative conductance function ccc on pairs of vertices; the associated walk moves with probabilities

P(x,y)=c(x,y)/c(x)P(x,y)=c(x,y)/c(x)P(x,y)=c(x,y)/c(x)

where c(x)=∑yc(x,y)c(x)=\sum_y c(x,y)c(x)=∑y​c(x,y), and cG=∑xc(x)c_G=\sum_x c(x)cG​=∑x​c(x). A function hhh is harmonic at xxx if h(x)=∑yP(x,y)h(y)h(x)=\sum_y P(x,y)h(y)h(x)=∑y​P(x,y)h(y). The voltage with boundary values 111 at aaa and 000 at zzz is W(x)=Px{τa<τz}W(x)=\mathbb P_x\{\tau_a<\tau_z\}W(x)=Px​{τa​<τz​}, the harmonic extension of its boundary data; the current flowing out of aaa has strength ∥I∥=∑yc(a,y) [W(a)−W(y)]\|I\|=\sum_y c(a,y)\,[W(a)-W(y)]∥I∥=∑y​c(a,y)[W(a)−W(y)], and the effective resistance is R(a↔z)=∥I∥−1R(a\leftrightarrow z)=\|I\|^{-1}R(a↔z)=∥I∥−1. A flow from aaa to zzz is an antisymmetric edge function obeying the node law off {a,z}\{a,z\}{a,z}; its energy is E(θ)=∑eθ(e)2/c(e)\mathcal E(\theta)=\sum_e\theta(e)^2/c(e)E(θ)=∑e​θ(e)2/c(e). Hitting times τS=min⁡{t≥0:Xt∈S}\tau_S=\min\{t\ge0:X_t\in S\}τS​=min{t≥0:Xt​∈S}, their expectations, the Green's function Gτz(a,x)G_{\tau_z}(a,x)Gτz​​(a,x), the maximal hitting time thitt_{\mathrm{hit}}thit​, and the cover time tcovt_{\mathrm{cov}}tcov​ (expected time to visit every state, maximized over starts) all use the trajectory calculus of Mission I.

Formalization targets

Goal

Ea(τb)+Eb(τa)  =  cG R(a↔b).\mathbb E_a(\tau_b)+\mathbb E_b(\tau_a)\;=\;c_G\,R(a\leftrightarrow b).Ea​(τb​)+Eb​(τa​)=cG​R(a↔b).

This is Proposition 10.6, the commute time identity — the exact bridge between the probabilistic and electrical sides, and the engine of the transience/recurrence theory of Mission XII.

Milestones

Reversibility and stationarity of the network walk with π(x)=c(x)/cG\pi(x)=c(x)/c_Gπ(x)=c(x)/cG​ (§9.1); Proposition 9.1 (existence and uniqueness of harmonic extensions with given boundary values, h(x)=Exf(XτB)h(x)=\mathbb E_x f(X_{\tau_B})h(x)=Ex​f(XτB​​)); Lemma 9.6 (the Green's function identity Gτz(a,a)=c(a)R(a↔z)G_{\tau_z}(a,a)=c(a)R(a\leftrightarrow z)Gτz​​(a,a)=c(a)R(a↔z)); Theorem 9.10 (Thomson's principle: R(a↔z)R(a\leftrightarrow z)R(a↔z) is the minimal energy of a unit flow, attained); Theorem 9.12 (Rayleigh monotonicity: lowering conductances raises effective resistance); Lemma 10.1 (the random target lemma: ∑yEa(τy)π(y)\sum_y\mathbb E_a(\tau_y)\pi(y)∑y​Ea​(τy​)π(y) does not depend on aaa); Corollary 10.8 (the resistance triangle inequality); Theorem 11.2 (Matthews: tcov≤thit (1+12+⋯+1n)t_{\mathrm{cov}}\le t_{\mathrm{hit}}\,(1+\tfrac12+\dots+\tfrac1n)tcov​≤thit​(1+21​+⋯+n1​)); Proposition 11.4 (the matching Matthews lower bound over subsets).

Significance

The results. The commute time identity computes hitting times from circuit reductions — this is how hitting times on trees, tori and glued graphs are actually evaluated — and, through Thomson and Rayleigh, makes them monotone under graph operations, something invisible probabilistically. The Matthews bounds pin cover times up to a log⁡n\log nlogn factor in complete generality; they are the tool behind cover-time results for lamplighter groups in Mission XI's sequel. Green's function identities feed Mission XII's recurrence theory, where R(a↔∞)R(a\leftrightarrow\infty)R(a↔∞) decides transience.

Formalizing them. Mathlib has graph Laplacians but no electrical network theory: no effective resistance, no flows, no energy, no Thomson/Rayleigh, no hitting or cover times. This mission publishes that layer over the trajectory calculus of Mission I. It is the most reusable single block of the series outside Missions I–II: effective resistance on finite networks is of independent interest to combinatorics (spanning trees, spectral sparsification) well beyond mixing times.

Difficulty

The identity chain behind the goal runs: Green's function of the stopped walk →\to→ escape probability Pa{τz<τa+}=(c(a)R(a↔z))−1\mathbb P_a\{\tau_z<\tau_a^+\}=\bigl(c(a)R(a\leftrightarrow z)\bigr)^{-1}Pa​{τz​<τa+​}=(c(a)R(a↔z))−1 (via harmonic uniqueness) →\to→ the Aldous–Fill occupation identity Gτ(a,x)=Ea(τ)π(x)G_\tau(a,x)=\mathbb E_a(\tau)\pi(x)Gτ​(a,x)=Ea​(τ)π(x) for stopping times with Xτ=aX_\tau=aXτ​=a — each step is a manipulation of infinite series of trajectory sums whose exchange steps (splitting a path at its first visit, last-exit decompositions) need summability from Mission I's Lemma 1.13. Thomson's principle is a finite-dimensional convex minimization: existence of the minimizer needs a compactness or completing-the-square argument, and the identification of the minimizer with the current flow needs the cycle law; the naive "differentiate the energy" route must be made exact. Matthews' method is a clean but genuinely clever argument — a uniformly random ordering of targets and the harmonic-number telescoping; the formal cost is the exchangeability of the randomized order against the chain, handled combinatorially.

Formalization scope

Networks are functions c:V×V→Rc:V\times V\to\mathbb Rc:V×V→R with a symmetry-and-nonnegativity predicate; loops are permitted; connectivity enters as irreducibility of the induced walk. The voltage is defined probabilistically as Px{τa<τz}\mathbb P_x\{\tau_a<\tau_z\}Px​{τa​<τz​} (the book's harmonic characterization is Proposition 9.1); R(a↔z)R(a\leftrightarrow z)R(a↔z) is the reciprocal of the explicit current strength, with total division junk when a,za,za,z are disconnected — statements carry irreducibility so this does not arise. Energy counts each undirected edge once, formalized as half the ordered double sum, and 02/0=00^2/0=002/0=0 handles absent edges. Cover times are tail sums of the explicit event "some state unvisited". The Matthews lower bound is stated with an arbitrary lower bound mmm for the pairwise hitting times of the subset AAA — equivalent to the book's min over pairs and easier to instantiate.

Welcome contributions: series/parallel reduction laws, the cycle and node law API for flows, escape-probability lemmas — all reused in Mission XII's infinite-network arguments.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • P. G. Doyle, J. L. Snell, Random Walks and Electric Networks, MAA, 1984. https://arxiv.org/abs/math/0001057
  • A. K. Chandra, P. Raghavan, W. L. Ruzzo, R. Smolensky, P. Tiwari, The electrical resistance of a graph captures its commute and cover times, STOC 1989. https://doi.org/10.1145/73007.73062
  • P. Matthews, Covering problems for Markov chains, Ann. Probab. 16 (1988). https://doi.org/10.1214/aop/1176991894
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Experimental DesignOperations ResearchProbability+2·Captain: Shuze Chen

Treatment Locality in A/B TestingResearch Paper

Modern A/B tests must infer lifetime treatment effects — e.g. customer lifetime value under a new feature — from short-horizon experiment data. Chen, Simchi-Levi and Wang (arXiv:2407.19618) model the experiment as a Markov decision process and exploit a structural fact of many practical interventions: the treatment is local, modifying the system at a single crucial state only. This mission formalizes the core asymptotic theory of the paper: for any differentiable estimator built from the experiment's transition and reward statistics, information sharing — pooling across test arms the samples collected away from the treated state — keeps the estimator asymptotically normal with the same asymptotic bias and never increases its asymptotic variance (Theorem 9), and is asymptotically efficient among unbiased estimators (Theorem 5). The route runs through a Markov chain central limit theorem with the asymptotic variance identified as the autocovariance series, and the linearization/delta method for functionals of chain statistics.

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Markov ChainProbabilityStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times I: Existence and Uniqueness of the Stationary DistributionTextbook

Markov Chains and Mixing Times I: Existence and Uniqueness of the Stationary Distribution

Motivation

Finite Markov chains are the basic model for memoryless random dynamics: card shuffles, random walks on graphs and groups, Monte Carlo samplers, and queueing systems are all chains on a finite state space. The single most used fact about them is that an irreducible chain has exactly one stationary distribution — a probability vector π\piπ with π=πP\pi = \pi Pπ=πP — and that this π\piπ is strictly positive and encodes the long-run behaviour of the chain through the return-time identity π(x)=1/Ex(τx+)\pi(x) = 1/\mathbb{E}_x(\tau_x^+)π(x)=1/Ex​(τx+​). Every later result in the theory of mixing times (convergence theorems, coupling bounds, spectral methods, cutoff) is a statement about the distance of the chain from this π\piπ, so nothing in the subject can be formalized before this mission is.

This mission is the first in a series formalizing D. A. Levin, Y. Peres and E. L. Wilmer, Markov Chains and Mixing Times (AMS, 2009), covering Chapters 1–2: the basic vocabulary of finite chains (stochastic matrices, irreducibility, period, reversibility, time reversal, random walks on graphs and groups) and the classical examples of Chapter 2 (gambler's ruin, coupon collecting, the reflection principle for simple random walk on Z\mathbb{Z}Z). Later missions in the series build on the definitions published here.

Setting

A chain on a finite state space Ω\OmegaΩ is presented by its transition matrix, a matrix P∈RΩ×ΩP \in \mathbb{R}^{\Omega\times\Omega}P∈RΩ×Ω with nonnegative entries whose rows sum to 111. A distribution is a row vector μ\muμ with nonnegative entries summing to 111; one step of the chain carries μ\muμ to μP\mu PμP, and the ttt-step transition probabilities are the entries of the matrix power PtP^tPt.

The chain is irreducible if for all states x,yx, yx,y there is a ttt with Pt(x,y)>0P^t(x,y) > 0Pt(x,y)>0. The period of a state xxx is gcd⁡ T(x)\gcd\,\mathcal{T}(x)gcdT(x) where T(x)={t≥1:Pt(x,x)>0}\mathcal{T}(x) = \{t \ge 1 : P^t(x,x) > 0\}T(x)={t≥1:Pt(x,x)>0}, and the chain is aperiodic if every state has period 111. A distribution π\piπ is stationary if πP=π\pi P = \piπP=π, and π\piπ and PPP are in detailed balance (the chain is reversible) if π(x)P(x,y)=π(y)P(y,x)\pi(x)P(x,y) = \pi(y)P(y,x)π(x)P(x,y)=π(y)P(y,x) for all x,yx,yx,y.

Trajectory events over a finite horizon are finite sums of path weights: a length-ttt trajectory is a function ω:{0,…,t}→Ω\omega : \{0,\dots,t\} \to \Omegaω:{0,…,t}→Ω, with weight ∏i<tP(ωi,ωi+1)\prod_{i<t} P(\omega_i, \omega_{i+1})∏i<t​P(ωi​,ωi+1​) conditional on its starting state. The tail probability Px{τz+>t}\mathbb{P}_x\{\tau_z^+ > t\}Px​{τz+​>t} of the first hitting time τz+=min⁡{t≥1:Xt=z}\tau_z^+ = \min\{t \ge 1 : X_t = z\}τz+​=min{t≥1:Xt​=z} is the sum of the weights of the trajectories from xxx that avoid zzz at times 1,…,t1,\dots,t1,…,t, and expectations of hitting times are recovered by the tail-sum formula E(Y)=∑t≥0P{Y>t}\mathbb{E}(Y) = \sum_{t\ge0} \mathbb{P}\{Y > t\}E(Y)=∑t≥0​P{Y>t}, formalized as a tsum over ttt.

Formalization targets

Goal

P stochastic and irreducible on a finite nonempty Ω  ⟹  ∃! π, π=πP.\text{$P$ stochastic and irreducible on a finite nonempty $\Omega$} \;\Longrightarrow\; \exists!\, \pi,\ \pi = \pi P .P stochastic and irreducible on a finite nonempty Ω⟹∃!π, π=πP.

This is Corollary 1.17 of the book. It asserts only existence and uniqueness, leaving the finer structure of π\piπ to the milestones; it is the weakest statement on which the rest of the series can stand, which is why it is the goal.

Milestones toward and around the goal

The milestone list follows the book's own route: well-definedness of the period (Lemma 1.6), positivity of some matrix power for irreducible aperiodic chains (Proposition 1.7), finiteness of expected hitting times (Lemma 1.13), existence of a positive stationary distribution together with

π(x) Ex(τx+)=1\pi(x)\,\mathbb{E}_x(\tau_x^+) = 1π(x)Ex​(τx+​)=1

(Proposition 1.14), constancy of harmonic functions (Lemma 1.16), stationarity from detailed balance (Proposition 1.19), the stationary and reversible measure π(x)=deg⁡(x)/2∣E∣\pi(x) = \deg(x)/2|E|π(x)=deg(x)/2∣E∣ of simple random walk on a graph (Examples 1.12 and 1.20), the time reversal P^\hat PP^ and its path-reversal identity (Proposition 1.22), and the random walks on finite groups of Section 2.6 (Propositions 2.12–2.14). From Chapter 2 the list adds the gambler's ruin formulas Pk{Xτ=n}=k/n\mathbb{P}_k\{X_\tau = n\} = k/nPk​{Xτ​=n}=k/n and Ek(τ)=k(n−k)\mathbb{E}_k(\tau) = k(n-k)Ek​(τ)=k(n−k) (Proposition 2.1), the coupon collector expectation n∑k≤n1/kn\sum_{k\le n} 1/kn∑k≤n​1/k and tail bound e−ce^{-c}e−c (Propositions 2.3 and 2.4), and the reflection principle and the bound Pk{τ0>r}≤12k/r\mathbb{P}_k\{\tau_0 > r\} \le 12k/\sqrt{r}Pk​{τ0​>r}≤12k/r​ for simple random walk on Z\mathbb{Z}Z (Lemma 2.18 and Theorem 2.17).

Significance

The result itself. Existence and uniqueness of π\piπ is the pivot on which the entire quantitative theory turns: it defines the target of convergence, and the identity π(x) Ex(τx+)=1\pi(x)\,\mathbb{E}_x(\tau_x^+) = 1π(x)Ex​(τx+​)=1 ties the stationary measure to return times, which later missions use for hitting-time and cover-time results. Detailed balance is the practical tool by which stationary measures of graph and group walks are computed, and the Chapter 2 examples (gambler's ruin, coupon collecting, reflection) are the standard building blocks reused throughout the book — the coupon collector bound, for instance, is exactly the estimate behind the nlog⁡n+cnn \log n + cnnlogn+cn analysis of the top-to-random shuffle in a later mission of this series.

Formalizing it. Mathlib currently has no theory of finite Markov chains: no stochastic-matrix predicate, no stationary distribution, no periodicity, no hitting times. Everything proved in this mission is new formal mathematics, and the definition layer published here (mm_basic, mm_path, mm_classical) is the shared foundation that all twelve subsequent missions of the series import. All results are classical and have textbook proofs; none has a machine-checked proof.

Difficulty

The delicate point is the existence proof. The natural first idea — extract π\piπ from an eigenvector of PTP^{\mathsf T}PT for eigenvalue 111, or invoke a fixed-point theorem — either does not give positivity and nonnegativity without further work, or uses compactness machinery (Brouwer) that is unavailable. The book's proof instead builds π~(y)=Ez(visits to y before τz+)\tilde\pi(y) = \mathbb{E}_z(\text{visits to } y \text{ before } \tau_z^+)π~(y)=Ez​(visits to y before τz+​) and verifies π~P=π~\tilde\pi P = \tilde\piπ~P=π~ by reindexing trajectory sums; formalizing it requires managing infinite series of path sums (summability from the geometric tail bound of Lemma 1.13, exchanging tsum with finite sums, splitting a trajectory at its last step). The uniqueness half is linear algebra via constancy of harmonic functions (Lemma 1.16), which is elementary but requires a maximum-principle argument over a finite state space. The reflection principle and Theorem 2.17 are finite combinatorics on ±1\pm 1±1 paths — the bijection is easy to describe and fiddly to implement.

Formalization scope

States form a Fintype with decidable equality; chains are Matrix V V ℝ with the row-stochasticity predicate IsStochastic; distributions are functions V → ℝ with the predicate IsDist. Everything is distribution-side: no probability space or measure theory is used. The period is formalized as sup⁡{d:d∣t for all t∈T(x)}\sup\{d : d \mid t \text{ for all } t \in \mathcal{T}(x)\}sup{d:d∣t for all t∈T(x)}, which equals gcd⁡T(x)\gcd \mathcal{T}(x)gcdT(x) when T(x)≠∅\mathcal{T}(x) \neq \varnothingT(x)=∅ and takes the junk value 000 otherwise. Expectations of hitting times are tsums of tail probabilities, with the usual junk value 000 for non-summable families — the statements are arranged (e.g. multiplicatively, π(x)⋅Ex(τx+)=1\pi(x)\cdot\mathbb{E}_x(\tau_x^+) = 1π(x)⋅Ex​(τx+​)=1) so that junk values cannot make them vacuously true. Existence statements carry a Nonempty V hypothesis; irreducibility on the empty space is vacuous, and without nonemptiness the goal would be false, not trivial. The coupon collector and the walk on Z\mathbb{Z}Z are presented directly by their driving randomness (uniform draws Fin t → Fin n, uniform sign strings Fin r → Bool), so those probabilities are elementary counting; in particular the reflection principle is stated as an equality of cardinalities of sets of sign strings — this is equivalent to the probabilistic statement because all 2r2^r2r strings are equally likely.

Contributions welcome beyond the milestone list: simp lemmas for the definition layer, the taboo-matrix representation of avoidance probabilities (useful for Lemma 1.13), and any interface lemmas connecting pathWeight sums to matrix powers — these will be reused by every later mission in the series.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • J. R. Norris, Markov Chains, Cambridge University Press, 1998. https://doi.org/10.1017/CBO9780511810633
  • D. Aldous, J. A. Fill, Reversible Markov Chains and Random Walks on Graphs, 2002 (unfinished monograph). https://www.stat.berkeley.edu/~aldous/RWG/book.html
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Convex OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Convex Optimization V: Newton's MethodTextbook

The classical convergence theory of smooth convex minimization. For a function that is mmm-strongly convex and MMM-smooth (mI⪯∇2f(x)⪯MImI \preceq \nabla^2 f(x) \preceq MImI⪯∇2f(x)⪯MI), gradient descent converges linearly, while Newton's method exhibits its famous two phases: a damped phase in which every backtracking step decreases the objective by a fixed amount γ\gammaγ, and a quadratically convergent phase in which the scaled gradient norm squares at each step, L2m2∥∇f(x+)∥2≤(L2m2∥∇f(x)∥2)2\tfrac{L}{2m^2}\lVert \nabla f(x^{+})\rVert_2 \le \bigl(\tfrac{L}{2m^2}\lVert \nabla f(x)\rVert_2\bigr)^22m2L​∥∇f(x+)∥2​≤(2m2L​∥∇f(x)∥2​)2. Together they give the iteration count of B&V (9.36),

#iterations  ≤  f(x(0))−p⋆γ  +  log⁡2log⁡2(ε0/ε),γ=αβη2mM2,ε0=2m3L2,\#\text{iterations} \;\le\; \frac{f(x^{(0)}) - p^{\star}}{\gamma} \;+\; \log_2\log_2(\varepsilon_0/\varepsilon), \qquad \gamma = \frac{\alpha\beta\eta^2 m}{M^2}, \quad \varepsilon_0 = \frac{2m^3}{L^2},#iterations≤γf(x(0))−p⋆​+log2​log2​(ε0​/ε),γ=M2αβη2m​,ε0​=L22m3​,

with LLL the Lipschitz constant of the Hessian and α,β\alpha,\betaα,β the backtracking parameters. This mission formalizes Chapters 9–10 of Boyd & Vandenberghe with every constant exactly as printed — a quantitative theory entirely absent from Mathlib.

12 thms4 active usersReviewed
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Convex OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Convex Optimization II: KKT ConditionsTextbook

The Karush–Kuhn–Tucker conditions are the central result of convex optimization: for a convex differentiable problem satisfying Slater's condition, a point is optimal exactly when primal feasibility, dual feasibility, complementary slackness and Lagrangian stationarity hold. This mission formalizes Chapters 4–5 of Boyd & Vandenberghe end to end — the first-order optimality criterion, concavity of the Lagrange dual, weak duality, Slater's strong-duality theorem with dual attainment (via the separating-hyperplane argument of §5.3.2), the saddle-point characterization, sensitivity bounds and Pareto scalarization — culminating in the full KKT characterization.

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