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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.

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

NoneFormalized record→≤ 2.99942Open frontier
Be the first prover0 of 1 missions formalized

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.

≤ 7.606309Formalized record
6 provers on it7 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.
≤ 87Formalized record
3 provers on it5 of 5 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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CombinatoricsMachine LearningProbability·Captain: naimengye

Understanding Machine Learning XXI: Covering NumbersTextbook

Motivation

Chapter 26 bounded the rate of uniform convergence by the Rademacher complexity; Chapter 27 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), introduces a second, metric measure of the size of a set of vectors, its covering numbers N(r,A)N(r, A)N(r,A), the smallest number of Euclidean balls of radius rrr needed to cover AAA, and connects the two through Dudley's chaining. Covering numbers behave well under scaling and under coordinatewise Lipschitz maps (Lemmas 27.2–27.3), they are easily bounded for sets lying in a low-dimensional subspace (Example 27.1), and the chaining lemma turns a bound on log⁡N(r,A)\log N(r, A)logN(r,A) at all scales r=c2−kr = c2^{-k}r=c2−k into a bound on R(A)R(A)R(A) (Lemma 27.4), with the clean corollary R(A)≤6cm(α+2β)R(A) \le \frac{6c}{m}(\alpha + 2\beta)R(A)≤m6c​(α+2β) when log⁡N(c2−k,A)≤α+βk\sqrt{\log N(c2^{-k}, A)} \le \alpha + \beta klogN(c2−k,A)​≤α+βk (Lemma 27.5). The chapter's example recovers R(A)=O(cdlog⁡d/m)R(A) = O(c\sqrt{d\log d}/m)R(A)=O(cdlogd​/m) for sets in a ddd-dimensional subspace, the technique that the book says would sharpen the fundamental theorem's sample complexity from dlog⁡(d/ϵ)/ϵ2d\log(d/\epsilon)/\epsilon^2dlog(d/ϵ)/ϵ2 to d/ϵ2d/\epsilon^2d/ϵ2.

Setting

For A⊆RmA \subseteq \mathbb{R}^mA⊆Rm with the Euclidean metric, A′A'A′ is an rrr-cover of AAA if every a∈Aa \in Aa∈A is within distance rrr of some a′∈A′a' \in A'a′∈A′, and N(r,A)N(r, A)N(r,A) is the cardinality of the smallest rrr-cover (Definition 27.1). The Rademacher complexity R(A)=1mEσsup⁡a∈A⟨σ,a⟩R(A) = \frac1m\mathbb{E}_\sigma\sup_{a \in A}\langle\sigma, a\rangleR(A)=m1​Eσ​supa∈A​⟨σ,a⟩ is Mission XX's. Chaining is run at the scales c2−kc2^{-k}c2−k, k=1,…,Mk = 1, \dots, Mk=1,…,M, where ccc is a radius of a ball containing AAA, the book's c=min⁡aˉmax⁡a∈A∥a−aˉ∥c = \min_{\bar a}\max_{a \in A}\|a - \bar a\|c=minaˉ​maxa∈A​∥a−aˉ∥ being the smallest such radius.

Formalization targets

Goal: Lemma 27.4

For a nonempty A⊆RmA \subseteq \mathbb{R}^mA⊆Rm, m≥1m \ge 1m≥1, contained in the ball of radius ccc about some aˉ\bar aaˉ, and every integer M>0M > 0M>0,

R(A)≤c 2−Mm+6cm∑k=1M2−klog⁡N(c 2−k,A).R(A) \le \frac{c\,2^{-M}}{\sqrt m} + \frac{6c}{m}\sum_{k=1}^M 2^{-k}\sqrt{\log N(c\,2^{-k}, A)}.R(A)≤m​c2−M​+m6c​k=1∑M​2−klogN(c2−k,A)​.

Milestones

Example 27.1 (the grid rrr-cover of a set of norm at most ccc in a ddd-dimensional subspace, of size (2cd/r+1)d(2c\sqrt d/r + 1)^d(2cd​/r+1)d); Lemma 27.2 (scaling and translation); Lemma 27.3 (the contraction principle); Lemma 27.5 (the corollary of chaining). Further item: Example 27.2 (R(A)=O(cdlog⁡d/m)R(A) = O(c\sqrt{d\log d}/m)R(A)=O(cdlogd​/m) for sets in a ddd-dimensional subspace).

Significance

Chaining is the standard way to get sharp uniform convergence rates: a single-scale union bound (Massart's lemma at one resolution) loses a logarithmic factor, and summing Massart bounds over a geometric sequence of scales, applied to the increments between successive nearest cover points, recovers it. Lemma 27.4 is the discrete Dudley integral, and Lemma 27.5 is the form in which it is used: any polynomial-in-1/r1/r1/r covering number gives R(A)=O(clog⁡N/m)R(A) = O(c\sqrt{\log N}/m)R(A)=O(clogN​/m)-type bounds without the extra logarithm. On the platform these items complete the complexity toolbox begun in Mission XX and provide covering numbers as a reusable notion; the contraction and scaling lemmas mirror their Rademacher counterparts.

Difficulty

Lemmas 27.2 and 27.3 are immediate: the image of an rrr-cover under the affine map is an rcrcrc-cover, and under a coordinatewise ρ\rhoρ-Lipschitz map a ρr\rho rρr-cover, since ∥φ(a)−φ(a′)∥2=∑i(φi(ai)−φi(ai′))2≤ρ2∥a−a′∥2\|\varphi(a) - \varphi(a')\|^2 = \sum_i(\varphi_i(a_i) - \varphi_i(a'_i))^2 \le \rho^2\|a - a'\|^2∥φ(a)−φ(a′)∥2=∑i​(φi​(ai​)−φi​(ai′​))2≤ρ2∥a−a′∥2; formally they are manipulations of the infimum in N∪{∞}\mathbb{N} \cup \{\infty\}N∪{∞}. Example 27.1 needs an orthonormal basis of the subspace (Gram–Schmidt, or Mathlib's orthonormal bases of finite-dimensional inner product subspaces of Rm\mathbb{R}^mRm with the Euclidean structure) and the rounding of coordinates to a grid. Lemma 27.4 is the real work: after centering, take minimal c2−kc2^{-k}c2−k-covers BkB_kBk​, the near-maximizer a∗a^*a∗ of ⟨σ,a⟩\langle\sigma, a\rangle⟨σ,a⟩ (which depends on σ\sigmaσ), its nearest points b(k)∈Bkb^{(k)} \in B_kb(k)∈Bk​, the telescoping a∗=(a∗−b(M))+∑k(b(k)−b(k−1))a^* = (a^* - b^{(M)}) + \sum_k(b^{(k)} - b^{(k-1)})a∗=(a∗−b(M))+∑k​(b(k)−b(k−1)), the bound ∥b(k)−b(k−1)∥≤3c2−k\|b^{(k)} - b^{(k-1)}\| \le 3c2^{-k}∥b(k)−b(k−1)∥≤3c2−k, and Massart's lemma (Mission XX) on the sets B^k\hat B_kB^k​ of increments, of cardinality at most N(c2−k,A)2N(c2^{-k}, A)^2N(c2−k,A)2; a formal proof must handle the supremum not being attained (approximate maximizers) and the dependence of all choices on σ\sigmaσ inside the finite average. Lemma 27.5 lets M→∞M \to \inftyM→∞ using ∑k2−k=1\sum_k 2^{-k} = 1∑k​2−k=1 and ∑kk2−k=2\sum_k k2^{-k} = 2∑k​k2−k=2. Example 27.2 combines Example 27.1 at the scales c2−kc2^{-k}c2−k with Lemma 27.5, with the book's constant log⁡(2d)\log(2\sqrt d)log(2d​). The book's derivation uses the count without +1+1+1, so a proof needs the volumetric covering bound (1+2c/r)d(1 + 2c/r)^d(1+2c/r)d for d≥2d \ge 2d≥2 and a direct count for d=1d = 1d=1.

Formalization scope

Vectors are Fin m → ℝ with an explicit Euclidean norm, because Mathlib's norm on that type is the sup norm; covers are arbitrary finsets of Rm\mathbb{R}^mRm and N(r,A)N(r, A)N(r,A) is an infimum in N∪{∞}\mathbb{N} \cup \{\infty\}N∪{∞}, so no junk value arises when no finite cover exists, and the chaining statements read NNN through ENat.toNat for the bounded sets they concern, where it is finite. Subspaces are Mathlib Submodules with finrank = d. Two statements are given with the constants their proofs support, and the item texts say so. Example 27.1's grid has 2c/ϵ+12c/\epsilon + 12c/ϵ+1 points per coordinate, so the cover has size (2cd/r+1)d(2c\sqrt d/r + 1)^d(2cd​/r+1)d, not (2cd/r)d(2c\sqrt d/r)^d(2cd​/r)d, which is less than 111 for r>2cdr > 2c\sqrt dr>2cd​ and cannot bound a covering number of a nonempty set; Example 27.2 correspondingly has log⁡(4d)\log(4\sqrt d)log(4d​) in place of log⁡(2d)\log(2\sqrt d)log(2d​). Lemma 27.4 is stated for any enclosing radius ccc about any center, since the proof only uses that {aˉ}\{\bar a\}{aˉ} is a ccc-cover of AAA; the book's minimal radius is the special case, and this is the form Example 27.2 needs (with aˉ=0\bar a = 0aˉ=0 and c=max⁡∥a∥c = \max\|a\|c=max∥a∥). Lemma 27.5 keeps the book's α,β>0\alpha, \beta > 0α,β>0.

Not stated: nothing else is in the chapter beyond the bibliographic remarks.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 27. doi:10.1017/CBO9781107298019
  • R. M. Dudley, Universal Donsker classes and metric entropy, Annals of Probability 15(4), 1987. doi:10.1214/aop/1176991978
  • M. Anthony, P. L. Bartlett, Neural Network Learning: Theoretical Foundations, Cambridge University Press, 1999. doi:10.1017/CBO9780511624216
  • M. Talagrand, Upper and Lower Bounds for Stochastic Processes, Springer, 2014. doi:10.1007/978-3-642-54075-2
  • R. Vershynin, High-Dimensional Probability, Cambridge University Press, 2018. doi:10.1017/9781108231596
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Machine LearningProbabilityStatistics·Captain: naimengye

Understanding Machine Learning XIX: Generative ModelsTextbook

Motivation

The book is discriminative almost throughout: it learns predictors, not distributions, following Vapnik's advice not to solve a more general problem as an intermediate step. Chapter 24 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), presents the generative alternative: assume a parametric form for the data distribution and estimate its parameters. The maximum likelihood principle is introduced on Bernoulli and Gaussian samples, shown to be empirical risk minimization for the log-loss, and analyzed through the decomposition of the true log-loss risk into a relative entropy plus an entropy (24.5), which explains both its consistency under a correct model and its overfitting on small samples. Naive Bayes and linear discriminant analysis show how generative assumptions reduce the number of parameters and make the Bayes classifier linear (24.8). The chapter's main theorem concerns the Expectation-Maximization algorithm of Dempster, Laird and Rubin for latent-variable models such as Gaussian mixtures: EM never decreases the log-likelihood (Theorem 24.3), because it is an alternate maximization of a lower bound G(Q,θ)G(Q, \theta)G(Q,θ) that touches the likelihood at the posterior (Lemma 24.2). The chapter ends with Bayesian reasoning and the rule of succession.

Setting

A Bernoulli sample S=(x1,…,xm)S = (x_1, \dots, x_m)S=(x1​,…,xm​) has log-likelihood L(S;θ)=log⁡(θ)∑ixi+log⁡(1−θ)∑i(1−xi)L(S;\theta) = \log(\theta)\sum_i x_i + \log(1-\theta)\sum_i(1-x_i)L(S;θ)=log(θ)∑i​xi​+log(1−θ)∑i​(1−xi​) and estimator θ^=1m∑ixi\hat\theta = \frac1m\sum_i x_iθ^=m1​∑i​xi​ (24.1); a Gaussian sample has L(S;(μ,σ))=−12σ2∑i(xi−μ)2−mlog⁡(σ2π)L(S;(\mu,\sigma)) = -\frac1{2\sigma^2}\sum_i(x_i-\mu)^2 - m\log(\sigma\sqrt{2\pi})L(S;(μ,σ))=−2σ21​∑i​(xi​−μ)2−mlog(σ2π​). The log-loss is ℓ(θ,x)=−log⁡Pθ[x]\ell(\theta, x) = -\log P_\theta[x]ℓ(θ,x)=−logPθ​[x] (24.4); on a finite domain, DRE[P∥Q]=∑xP[x]log⁡(P[x]/Q[x])D_{RE}[P\|Q] = \sum_x P[x]\log(P[x]/Q[x])DRE​[P∥Q]=∑x​P[x]log(P[x]/Q[x]) and H(P)=∑xP[x]log⁡(1/P[x])H(P) = \sum_x P[x]\log(1/P[x])H(P)=∑x​P[x]log(1/P[x]). A latent-variable model is a parametric joint Pθ[X=x,Y=y]P_\theta[X = x, Y = y]Pθ​[X=x,Y=y], y∈[k]y \in [k]y∈[k], with L(θ)=∑ilog⁡∑yPθ[X=xi,Y=y]L(\theta) = \sum_i\log\sum_y P_\theta[X = x_i, Y = y]L(θ)=∑i​log∑y​Pθ​[X=xi​,Y=y]; F(Q,θ)=∑i∑yQi,ylog⁡Pθ[X=xi,Y=y]F(Q,\theta) = \sum_i\sum_y Q_{i,y}\log P_\theta[X = x_i, Y = y]F(Q,θ)=∑i​∑y​Qi,y​logPθ​[X=xi​,Y=y], G(Q,θ)=F(Q,θ)−∑i∑yQi,ylog⁡Qi,yG(Q,\theta) = F(Q,\theta) - \sum_i\sum_y Q_{i,y}\log Q_{i,y}G(Q,θ)=F(Q,θ)−∑i​∑y​Qi,y​logQi,y​ over the set Q\mathcal{Q}Q of row-stochastic matrices, and EM alternates the E-step Qi,y(t+1)=Pθ(t)[Y=y∣X=xi]Q^{(t+1)}_{i,y} = P_{\theta^{(t)}}[Y = y \mid X = x_i]Qi,y(t+1)​=Pθ(t)​[Y=y∣X=xi​] (24.10) with the M-step θ(t+1)∈argmax⁡θF(Q(t+1),θ)\theta^{(t+1)} \in \operatorname{argmax}_\theta F(Q^{(t+1)}, \theta)θ(t+1)∈argmaxθ​F(Q(t+1),θ) (24.11).

Formalization targets

Goal: Theorem 24.3

For a positive parametric joint Pθ[X=x,Y=y]P_\theta[X = x, Y = y]Pθ​[X=x,Y=y], a sample x1,…,xmx_1, \dots, x_mx1​,…,xm​, and any run θ(0),θ(1),…\theta^{(0)}, \theta^{(1)}, \dotsθ(0),θ(1),… of EM (each M-step returning some maximizer of F(Q(t+1),⋅)F(Q^{(t+1)}, \cdot)F(Q(t+1),⋅)), the log-likelihood never decreases:

L(θ(t+1))≥L(θ(t))for all t.L(\theta^{(t+1)}) \ge L(\theta^{(t)}) \quad\text{for all } t.L(θ(t+1))≥L(θ(t))for all t.

Milestones

Equation (24.2) (Hoeffding for the Bernoulli estimator); the Gaussian maximum likelihood estimates of §24.1.1; Equation (24.5) (the risk decomposition DRE[P∥Pθ]+H(P)D_{RE}[P\|P_\theta] + H(P)DRE​[P∥Pθ​]+H(P)); Equation (24.8) (the LDA log-likelihood ratio is affine); Lemma 24.2 (EM as alternate maximization of GGG, with G(Q,θ)≤L(θ)G(Q, \theta) \le L(\theta)G(Q,θ)≤L(θ) and equality at the posterior). Further items: Gibbs' inequality, the Bernoulli maximum likelihood estimator (24.1)/(24.3), Exercise 1 (the biased variance estimate), Equation (24.6), the overfitting example of §24.1.3, Exercise 3 / (24.14), the weighted-centroid M-step (24.13), and the rule of succession of §24.5.

Significance

Theorem 24.3 is the guarantee that makes EM a sensible algorithm: it does not find the maximum likelihood estimate, but it climbs monotonically, and Lemma 24.2 identifies why, the E-step chooses the tightest lower bound G(Q,⋅)G(Q, \cdot)G(Q,⋅) at the current parameter and the M-step maximizes it. This variational view underlies a large part of modern latent-variable inference. Equation (24.5) is the information-theoretic content of maximum likelihood: the true risk is the entropy of the data plus the relative entropy to the model, so the best parameter is a projection of the data distribution onto the model class, and Gibbs' inequality is what makes that projection meaningful. The Bernoulli and Gaussian computations are the standard first examples, and Equation (24.8) is the reason linear classifiers appear in generative modeling. On the platform, the mission adds the relative entropy on finite domains, the EM objects, and Gaussian-integral identities that later probabilistic work can reuse.

Difficulty

The Bernoulli and Gaussian maximum likelihood facts are calculus, but as global maximization statements they need the concavity of log⁡\loglog and an explicit completion of squares rather than the book's stationary-point argument; the Gaussian case reduces to minimizing σ↦mσ^22σ2+mlog⁡σ\sigma \mapsto \frac{m\hat\sigma^2}{2\sigma^2} + m\log\sigmaσ↦2σ2mσ^2​+mlogσ. Equation (24.5) is a finite-sum identity; Gibbs' inequality is Jensen for log⁡\loglog with the equality case, or the elementary log⁡t≤t−1\log t \le t - 1logt≤t−1. Lemma 24.2 is Jensen's inequality applied row by row to ∑yQi,ylog⁡(Pθ[X=xi,Y=y]/Qi,y)\sum_y Q_{i,y}\log(P_\theta[X = x_i, Y = y]/Q_{i,y})∑y​Qi,y​log(Pθ​[X=xi​,Y=y]/Qi,y​), with care at entries Qi,y=0Q_{i,y} = 0Qi,y​=0, where the convention 0log⁡0=00\log 0 = 00log0=0 is exactly Lean's junk value; Theorem 24.3 chains the lemma's three parts as the book does. The Gaussian expectation identities (Exercise 1 and (24.6)) require the moments of gaussianReal and Fubini over the product law. Hoeffding's inequality (24.2) is Mission II's Theorem for Bernoulli variables; the overfitting example is the inequality log⁡(1−θ)≥−2θ\log(1-\theta) \ge -2\thetalog(1−θ)≥−2θ on [0,1/2][0, 1/2][0,1/2]. The rule of succession is a Beta-function identity provable by integration by parts.

Formalization scope

Parametric families are functions from a parameter type to real-valued probabilities or densities, following the book's convention (p. 344) that P[X=x]P[X = x]P[X=x] denotes either; no measure-theoretic densities are needed except in the two Gaussian-integral items, which use gaussianReal and the i.i.d. law of Mission I, and in the two Bernoulli probability items, which use the Bernoulli law of Mission XIV. Lean's log 0 = 0 is handled explicitly: the EM items assume a positive joint, since with junk logarithms Theorem 24.3 is false (the M-step could pick a parameter with a zero component and inflated FFF), while the entropy terms Qlog⁡QQ\log QQlogQ use the convention 0log⁡0=00\log 0 = 00log0=0 that the book intends; the Bernoulli maximum likelihood statement ranges over θ∈(0,1)\theta \in (0,1)θ∈(0,1); the log-loss decomposition and Gibbs' inequality take the second distribution positive. The M-step is a predicate ("some maximizer"), so Assumption 24.1 is not modeled, and an EM run is any sequence of such steps. The Gaussian maximum likelihood statement requires a nonconstant sample, without which the likelihood is unbounded; the overfitting example is stated for θ⋆≤1/2\theta^\star \le 1/2θ⋆≤1/2, the range on which the book's inequality (1−θ)m≥e−2θm(1-\theta)^m \ge e^{-2\theta m}(1−θ)m≥e−2θm holds. Equation (24.8) is stated as a matrix identity for any symmetric MMM in place of Σ−1\Sigma^{-1}Σ−1; the soft k-means M-step is stated as the weighted-centroid minimization it amounts to.

Not stated: Naive Bayes (24.7), which is a rewriting of Bayes' rule; the mixture density itself and the E-step formula (24.12); the Bayesian derivations (24.16) and maximum a posteriori estimation; Exercise 2.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 24. doi:10.1017/CBO9781107298019
  • A. P. Dempster, N. M. Laird, D. B. Rubin, Maximum likelihood from incomplete data via the EM algorithm, Journal of the Royal Statistical Society B 39(1), 1977. doi:10.1111/j.2517-6161.1977.tb01600.x
  • C. F. J. Wu, On the convergence properties of the EM algorithm, Annals of Statistics 11(1), 1983. doi:10.1214/aos/1176346060
  • T. M. Cover, J. A. Thomas, Elements of Information Theory, 2nd ed., Wiley, 2006. doi:10.1002/047174882X
  • C. M. Bishop, Pattern Recognition and Machine Learning, Springer, 2006.
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Machine LearningOptimizationProbability·Captain: naimengye

Understanding Machine Learning XVIII: Dimensionality ReductionTextbook

Motivation

Dimensionality reduction maps data in Rd\mathbb{R}^dRd to Rn\mathbb{R}^nRn, n≪dn \ll dn≪d, by a linear map x↦Wxx \mapsto Wxx↦Wx, for computational reasons, for generalization (Chapter 19's curse of dimensionality) and for interpretability. Chapter 23 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), studies three ways to choose WWW. Principal Component Analysis chooses the pair of compression and recovery matrices that minimizes the total squared reconstruction error, and the answer is the eigenvectors of ∑ixixi⊤\sum_i x_ix_i^\top∑i​xi​xi⊤​ for the largest eigenvalues (Theorem 23.2). Random projections choose WWW with independent Gaussian entries, and the Johnson–Lindenstrauss lemma says that the norms of any finite set of vectors are then preserved up to 1±ϵ1 \pm \epsilon1±ϵ with n=O(ϵ−2log⁡∣Q∣)n = O(\epsilon^{-2}\log|Q|)n=O(ϵ−2log∣Q∣) (Lemma 23.4). Compressed sensing exploits sparsity: a matrix with the restricted isometry property compresses every sss-sparse vector losslessly (Theorem 23.6), the reconstruction can be done by ℓ1\ell_1ℓ1​ minimization, a linear program, with an error bound that degrades gracefully for approximately sparse inputs (Theorem 23.8, due to Candès), and Gaussian random matrices with n=O(slog⁡d)n = O(s\log d)n=O(slogd) rows are RIP with high probability (Theorem 23.9).

Setting

Vectors are functions Rd\mathbb{R}^dRd with ∥v∥22=∑ivi2\|v\|_2^2 = \sum_i v_i^2∥v∥22​=∑i​vi2​, ∥v∥1=∑i∣vi∣\|v\|_1 = \sum_i|v_i|∥v∥1​=∑i​∣vi​∣ and ∥v∥0=∣{i:vi≠0}∣\|v\|_0 = |\{i : v_i \ne 0\}|∥v∥0​=∣{i:vi​=0}∣. The PCA problem (23.1) is argmin⁡W∈Rn×d,U∈Rd×n∑i=1m∥xi−UWxi∥22\operatorname{argmin}_{W \in \mathbb{R}^{n \times d}, U \in \mathbb{R}^{d \times n}}\sum_{i=1}^m\|x_i - UWx_i\|_2^2argminW∈Rn×d,U∈Rd×n​∑i=1m​∥xi​−UWxi​∥22​, and A=∑ixixi⊤A = \sum_i x_ix_i^\topA=∑i​xi​xi⊤​. A random matrix has independent N(0,v)N(0, v)N(0,v) entries, v=1v = 1v=1 in Lemma 23.3 and v=1/nv = 1/nv=1/n afterwards. WWW is (ϵ,s)(\epsilon, s)(ϵ,s)-RIP if ∣∥Wx∥22/∥x∥22−1∣≤ϵ\big|\|Wx\|_2^2/\|x\|_2^2 - 1\big| \le \epsilon​∥Wx∥22​/∥x∥22​−1​≤ϵ for every x≠0x \ne 0x=0 with ∥x∥0≤s\|x\|_0 \le s∥x∥0​≤s (Definition 23.5); vIv_IvI​ is vvv restricted to an index set III.

Formalization targets

Goal: Theorem 23.2

Let x1,…,xm∈Rdx_1, \dots, x_m \in \mathbb{R}^dx1​,…,xm​∈Rd, A=∑ixixi⊤A = \sum_i x_ix_i^\topA=∑i​xi​xi⊤​, and let u1,…,unu_1, \dots, u_nu1​,…,un​ be eigenvectors of AAA for its nnn largest eigenvalues, formalized as the first nnn columns of a spectral decomposition A=Vdiag⁡(D)V⊤A = V\operatorname{diag}(D)V^\topA=Vdiag(D)V⊤ with V⊤V=IV^\top V = IV⊤V=I and DDD nonincreasing. Then U=[u1⋯un]U = [u_1 \cdots u_n]U=[u1​⋯un​] with W=U⊤W = U^\topW=U⊤ minimizes (23.1): for every U′,W′U', W'U′,W′,

∑i∥xi−UU⊤xi∥2≤∑i∥xi−U′W′xi∥2.\sum_i\|x_i - UU^\top x_i\|^2 \le \sum_i\|x_i - U'W'x_i\|^2.i∑​∥xi​−UU⊤xi​∥2≤i∑​∥xi​−U′W′xi​∥2.

Milestones

Lemma 23.1 (the reduction of (23.1) to orthonormal UUU and W=U⊤W = U^\topW=U⊤); Lemma 23.4 (Johnson–Lindenstrauss); Theorem 23.6 (exact ℓ0\ell_0ℓ0​ recovery under RIP); Theorem 23.8 (Candès' ℓ1\ell_1ℓ1​ recovery bound); Theorem 23.9 (Gaussian matrices are RIP). Further items: Equation (23.3), Exercise 2, Remark 23.1 (the optimal value ∑i>nDi,i\sum_{i>n}D_{i,i}∑i>n​Di,i​), the eigenvector transfer of §23.1.1, Lemma 23.3, Theorem 23.7, Lemma 23.10, Lemma 23.11 and Lemma 23.12.

Significance

Theorem 23.2 is the Eckart–Young–Mirsky theorem in the form the book states it: PCA is the optimal linear compression-and-recovery scheme in the least-squares sense, and its solution is spectral. The Johnson–Lindenstrauss lemma is the basic tool of randomized dimensionality reduction, with a bound independent of ddd, and the book's variant with explicit constants is what later chapters and the compressed-sensing proofs use. Theorems 23.6–23.9 together are the three "surprising results" of compressed sensing: information-theoretic recoverability from RIP, efficient recovery by convex relaxation, and the existence of RIP matrices by randomness; their proofs, Candès' cone argument and Baraniuk–Davenport–DeVore–Wakin's net-plus-union-bound, are among the cleanest in applied mathematics and are natural formalization targets. On the platform, the mission introduces Gaussian random matrices as product measures and the RIP predicate, usable by later work on sparse recovery.

Difficulty

Lemma 23.1 requires building an orthonormal basis of the range of UWUWUW, padded to nnn vectors when the range has smaller dimension, and the identity ∥x−Vy∥2=∥x∥2+∥y∥2−2y⊤V⊤x\|x - Vy\|^2 = \|x\|^2 + \|y\|^2 - 2y^\top V^\top x∥x−Vy∥2=∥x∥2+∥y∥2−2y⊤V⊤x; Equation (23.3) is a trace computation. Theorem 23.2 combines (23.3), the change of basis B=V⊤UB = V^\top UB=V⊤U with B⊤B=IB^\top B = IB⊤B=I, the bound ∑iBj,i2≤1\sum_i B_{j,i}^2 \le 1∑i​Bj,i2​≤1 from extending BBB to an orthogonal matrix, and Exercise 2, a rearrangement inequality; Remark 23.1 adds trace⁡(A)=∑jDj,j\operatorname{trace}(A) = \sum_j D_{j,j}trace(A)=∑j​Dj,j​. Lemma 23.3 is the concentration of a χn2\chi^2_nχn2​ variable (Lemma B.12), which must itself be established from the Gaussian moment generating function; the Johnson–Lindenstrauss lemma is then a union bound. Theorem 23.6 is a two-line contradiction with RIP applied to x−x~x - \tilde xx−x~. Theorem 23.8 is the substantial one: the partition of [d][d][d] into blocks of sss largest remaining entries, the bound ∥hTj∥2≤s−1/2∥hTj−1∥1\|h_{T_j}\|_2 \le s^{-1/2}\|h_{T_{j-1}}\|_1∥hTj​​∥2​≤s−1/2∥hTj−1​​∥1​, the ℓ1\ell_1ℓ1​-minimality inequality (23.8), Lemma 23.10, and the two claims combined through (23.5); a formal proof must handle the last, possibly shorter block, which the book's "assume d/sd/sd/s is an integer" sidesteps. Lemma 23.11 is a volumetric net bound; Lemma 23.12 applies the Johnson–Lindenstrauss lemma to the image of an ϵ/4\epsilon/4ϵ/4-net of the unit sphere of Rs\mathbb{R}^sRs and closes the gap by the "smallest aaa" argument, and Theorem 23.9 is a union bound over index sets.

Formalization scope

Vectors are plain functions Fin d → ℝ with explicit norms, and matrices are Mathlib matrices, so the objectives are finite sums with no coercions between normed spaces. Random matrices are functions Fin n → Fin d → ℝ with the product of Gaussian laws gaussianReal 0 v, applied through Matrix.of; probability statements bound the outer measure of the failure event, and the failure events of Lemmas 23.4 and 23.12 are written with ≥ϵ\ge \epsilon≥ϵ so that the book's strict conclusions follow. "Eigenvectors corresponding to the nnn largest eigenvalues" is formalized as the first nnn columns of a spectral decomposition with nonincreasing diagonal, which is exactly the set of such systems and avoids Mathlib's eigenvalue ordering conventions. Minimizers (x~\tilde xx~, x⋆x^\starx⋆, xsx_sxs​) are arbitrary elements of the argmin.

Five statements are given as their proofs support them, and the item texts say so. Lemma 23.3 and the Johnson–Lindenstrauss lemma are stated for ϵ≤3/4\epsilon \le 3/4ϵ≤3/4: the printed range ϵ∈(0,3)\epsilon \in (0, 3)ϵ∈(0,3) (and ϵ≤3\epsilon \le 3ϵ≤3) is false, since the χn2\chi^2_nχn2​ upper tail decays like e−n(ϵ−ln⁡(1+ϵ))/2e^{-n(\epsilon - \ln(1+\epsilon))/2}e−n(ϵ−ln(1+ϵ))/2, slower than e−ϵ2n/6e^{-\epsilon^2 n/6}e−ϵ2n/6 for ϵ>0.785\epsilon > 0.785ϵ>0.785 (at ϵ=2.9\epsilon = 2.9ϵ=2.9 it fails for n=10n = 10n=10); the audit found this. Lemma 23.1 as printed, "every solution has orthonormal columns and W=U⊤W = U^\topW=U⊤", is false, since (cU,W/c)(cU, W/c)(cU,W/c) has the same objective as (U,W)(U, W)(U,W); the item states what the proof shows, that every (U,W)(U, W)(U,W) is dominated by some (V,V⊤)(V, V^\top)(V,V⊤) with V⊤V=IV^\top V = IV⊤V=I, which is all that (23.2) needs. Theorem 23.9 is stated with n≥216 slog⁡(72d/(δϵ))/ϵ2n \ge 216\,s\log(72d/(\delta\epsilon))/\epsilon^2n≥216slog(72d/(δϵ))/ϵ2: Lemma 23.12 with ϵ/3\epsilon/3ϵ/3 (so that (1±ϵ/3)2(1 \pm \epsilon/3)^2(1±ϵ/3)2 lies within 1±ϵ1 \pm \epsilon1±ϵ) and δ/ds\delta/d^sδ/ds, followed by a union bound over the at most dsd^sds index sets, gives these constants, and the printed 100100100 and 404040 are not reached by the argument. Theorem 23.8's proof assumes d/sd/sd/s is an integer for simplicity; the statement is given without that assumption, since only the last block of the partition can be short and the block inequality still holds. Lemma 23.3 has x≠0x \ne 0x=0, and the Johnson–Lindenstrauss lemma n≥1n \ge 1n≥1, since for n=0n = 0n=0 its ϵ\epsilonϵ is 000 and the conclusion fails.

Not stated: §23.1.2 (implementation), Remarks 23.2–23.3, §23.4 (the comparison of PCA and compressed sensing), Exercises 1 and 3–6.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 23. doi:10.1017/CBO9781107298019
  • W. B. Johnson, J. Lindenstrauss, Extensions of Lipschitz mappings into a Hilbert space, Contemporary Mathematics 26, 1984. doi:10.1090/conm/026/737400
  • E. J. Candès, The restricted isometry property and its implications for compressed sensing, Comptes Rendus Mathématique 346(9–10), 2008. doi:10.1016/j.crma.2008.03.014
  • R. Baraniuk, M. Davenport, R. DeVore, M. Wakin, A simple proof of the restricted isometry property for random matrices, Constructive Approximation 28, 2008. doi:10.1007/s00365-007-9003-x
  • D. L. Donoho, Compressed sensing, IEEE Transactions on Information Theory 52(4), 2006. doi:10.1109/TIT.2006.871582
  • E. J. Candès, T. Tao, Decoding by linear programming, IEEE Transactions on Information Theory 51(12), 2005. doi:10.1109/TIT.2005.858979
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CombinatoricsMachine LearningOptimization·Captain: naimengye

Understanding Machine Learning XVII: ClusteringTextbook

Motivation

Clustering is the most widely used tool of exploratory data analysis and, at the same time, the least well defined: similar points should share a cluster and dissimilar points should not, but similarity is not transitive while cluster membership is, and without labels there is no ground truth against which to evaluate a proposed grouping. Chapter 22 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), surveys the main paradigms, linkage-based algorithms, cost minimization with the k-means family, spectral relaxations of graph cuts, and the information bottleneck, and then returns to the question of what clustering is through Kleinberg's axioms. Its one theorem about that question is negative: no clustering function is simultaneously scale invariant, rich and consistent (Theorem 22.4). The mission formalizes this impossibility together with the chapter's positive facts: an iteration of the k-means algorithm never increases the k-means objective (Lemma 22.1), the RatioCut objective is the trace of a quadratic form of the graph Laplacian over cluster indicator vectors (Lemma 22.3), and the farthest-first traversal is a 2-approximation for the k-diam objective (Exercise 3).

Setting

A clustering of a finite set XXX is a partition C=(C1,…,Ck)C = (C_1, \dots, C_k)C=(C1​,…,Ck​). For X⊆RnX \subseteq \mathbb{R}^nX⊆Rn the k-means objective is G(C)=∑i∑x∈Ci∥x−μ(Ci)∥2G(C) = \sum_i\sum_{x \in C_i}\|x - \mu(C_i)\|^2G(C)=∑i​∑x∈Ci​​∥x−μ(Ci​)∥2 with μ(Ci)\mu(C_i)μ(Ci​) the centroid of CiC_iCi​, equivalently min⁡μ1,…,μk∑i∑x∈Ci∥x−μi∥2\min_{\mu_1, \dots, \mu_k}\sum_i\sum_{x \in C_i}\|x - \mu_i\|^2minμ1​,…,μk​​∑i​∑x∈Ci​​∥x−μi​∥2 (22.1); the k-means algorithm alternately reassigns each point to a nearest centroid and recomputes the centroids. For a similarity matrix W∈Rm×mW \in \mathbb{R}^{m \times m}W∈Rm×m, the degree matrix is D=diag⁡(∑jWi,j)D = \operatorname{diag}(\sum_j W_{i,j})D=diag(∑j​Wi,j​), the unnormalized graph Laplacian is L=D−WL = D - WL=D−W (Definition 22.2), and RatioCut⁡(C)=∑i1∣Ci∣∑r∈Ci,s∉CiWr,s\operatorname{RatioCut}(C) = \sum_i \frac1{|C_i|}\sum_{r \in C_i, s \notin C_i}W_{r,s}RatioCut(C)=∑i​∣Ci​∣1​∑r∈Ci​,s∈/Ci​​Wr,s​. Kleinberg's setting is a clustering function FFF that takes a dissimilarity ddd over XXX, symmetric, zero on the diagonal and positive off it, and returns a partition; the three axioms are Scale Invariance (F(αd)=F(d)F(\alpha d) = F(d)F(αd)=F(d)), Richness (every partition is some F(d)F(d)F(d)) and Consistency (shrinking within-cluster and expanding between-cluster dissimilarities leaves FFF unchanged). The k-diam objective is max⁡jdiam⁡(Cj)\max_j\operatorname{diam}(C_j)maxj​diam(Cj​), and the farthest-first traversal picks μ1\mu_1μ1​ arbitrarily and μj\mu_jμj​ maximizing min⁡i<jd(x,μi)\min_{i<j}d(x, \mu_i)mini<j​d(x,μi​), then clusters by nearest center.

Formalization targets

Goal: Theorem 22.4

For a finite domain XXX with at least two points, there is no function FFF from dissimilarities over XXX to partitions of XXX satisfying Scale Invariance, Richness and Consistency.

Milestones

Lemma 22.1 (a k-means iteration does not increase GGG); the Laplacian identity v⊤Lv=12∑r,sWr,s(vr−vs)2v^\top L v = \frac12\sum_{r,s}W_{r,s}(v_r - v_s)^2v⊤Lv=21​∑r,s​Wr,s​(vr​−vs​)2 from the proof of Lemma 22.3; Lemma 22.3 (H⊤H=IH^\top H = IH⊤H=I and RatioCut⁡(C)=trace⁡(H⊤LH)\operatorname{RatioCut}(C) = \operatorname{trace}(H^\top L H)RatioCut(C)=trace(H⊤LH) for Hi,j=∣Cj∣−1/21[i∈Cj]H_{i,j} = |C_j|^{-1/2}\mathbb{1}[i \in C_j]Hi,j​=∣Cj​∣−1/21[i∈Cj​]); Exercise 3 (farthest-first traversal is a 2-approximation for k-diam). Further item: the centroid minimizes ∑x∈C∥x−μ∥2\sum_{x \in C}\|x - \mu\|^2∑x∈C​∥x−μ∥2, the content of (22.1)–(22.3).

Significance

Kleinberg's theorem is the chapter's conceptual center: it says there is no ideal clustering function, only trade-offs, and the choice of a method must encode prior knowledge about the task, the unsupervised analogue of the No-Free-Lunch theorem. Its proof is short but delicate about what a dissimilarity is, and formalizing it fixes the exact hypotheses. Lemma 22.1 is the only guarantee the book offers for Lloyd's algorithm, and it is the reason the algorithm terminates on finite data. Lemma 22.3 is the bridge from a combinatorial cut objective to the spectrum of the Laplacian, the starting point of spectral clustering and of the PCA-type argument used in Chapter 23. The farthest-first result of Exercise 3 is Gonzalez's classical 2-approximation for k-center-type objectives, stated here for the diameter objective, and it is tight in the sense that no better constant is possible unless P = NP.

Difficulty

Theorem 22.4 follows the book: Richness gives d1d_1d1​ with all-singleton output and d2d_2d2​ with a different output; positivity lets one scale d2d_2d2​ above d1d_1d1​ pointwise, and Scale Invariance and Consistency then force two different values for F(αd2)F(\alpha d_2)F(αd2​). Formally the work is in building the scaled dissimilarity and in comparing Setoids. Lemma 22.1 is two inequalities: the nearest-centroid reassignment does not increase ∑i∑x∈Ci∥x−μi∥2\sum_i\sum_{x \in C_i}\|x - \mu_i\|^2∑i​∑x∈Ci​​∥x−μi​∥2 for the old centroids, because it minimizes it pointwise over assignments, and recomputing centroids does not increase it either, because the centroid minimizes the within-cluster sum of squares; the latter is the separate centroid item, a completing-the-square computation in an inner product space. The Laplacian identity is a finite double-sum manipulation that uses the symmetry of WWW; Lemma 22.3 applies it to the columns of HHH and computes H⊤HH^\top HH⊤H from the partition structure. Exercise 3 is the hint's argument: let rrr be the distance from the next farthest-first point μk+1\mu_{k+1}μk+1​ to the chosen centers; every point is within rrr of its center, so every cluster of the algorithm has diameter at most 2r2r2r, while the k+1k+1k+1 points μ1,…,μk+1\mu_1, \dots, \mu_{k+1}μ1​,…,μk+1​ are pairwise at distance at least rrr, so two of them share a cluster of any kkk-clustering, whose diameter is then at least rrr. When ∣X∣≤k|X| \le k∣X∣≤k the argument degenerates but the statement stays trivially true.

Formalization scope

Partitions are Fin k\mathrm{Fin}\ kFin k-indexed families of finsets covering each point of the data exactly once, and nearest-center assignments and farthest-first centers are predicates rather than functions, so every tie-breaking rule is covered. The k-means items live in Rn\mathbb{R}^nRn as EuclideanSpace; the centroid of an empty cluster is 000, which never enters any sum. The spectral items use Mathlib matrices over Fin m, Matrix.diagonal, Matrix.trace, the root-namespace dotProduct, and require WWW symmetric, which the identity needs and which every similarity matrix satisfies; Lemma 22.3 requires nonempty clusters, without which HHH has a zero column. Kleinberg's function is formalized on a fixed finite domain, as a map from Dissimilarity X to Setoid X, dissimilarities being positive on distinct points as in Kleinberg (2003): the book's model of p. 309 only asks for d≥0d \ge 0d≥0, but the scaling step of the proof of Theorem 22.4 requires positivity, and the theorem is stated for domains with at least two points, since the proof uses two partitions only. The k-diam theorem is stated without a maximum: every cluster of the algorithm has diameter at most twice the diameter of some cluster of the competitor, which is Gk-diam(C^)≤2Gk-diam(C∗)G_{k\text{-diam}}(\hat C) \le 2G_{k\text{-diam}}(C^*)Gk-diam​(C^)≤2Gk-diam​(C∗) without conventions for empty index sets, and Metric.diam gives 000 on sets of fewer than two points, the exercise's convention.

Not stated: the linkage-based algorithms and dendrograms of §22.1 (no theorem is stated about them), the k-medoids and k-median objectives, the spectral clustering algorithm itself, the information bottleneck of §22.4, Exercises 1, 2 and 4–6.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 22. doi:10.1017/CBO9781107298019
  • J. Kleinberg, An impossibility theorem for clustering, NIPS 2002.
  • S. P. Lloyd, Least squares quantization in PCM, IEEE Transactions on Information Theory 28(2), 1982. doi:10.1109/TIT.1982.1056489
  • U. von Luxburg, A tutorial on spectral clustering, Statistics and Computing 17, 2007. doi:10.1007/s11222-007-9033-z
  • T. F. Gonzalez, Clustering to minimize the maximum intercluster distance, Theoretical Computer Science 38, 1985. doi:10.1016/0304-3975(85)90224-5
  • M. Ackerman, S. Ben-David, Measures of clustering quality: a working set of axioms for clustering, NIPS 2008.
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AnalysisMathematical Physics·Captain: Lucas

Weinberg 1965: Infrared Photons and Gravitons — the soft exponents A and BResearch Paper

Motivation

When a charged particle scatters, it can radiate photons of arbitrarily low energy. In perturbative quantum electrodynamics this shows up as infrared divergences: loop integrals over very soft virtual photons diverge logarithmically, and so do the rates for emitting soft real photons. The standard resolution, due to Bloch and Nordsieck and systematized by Yennie, Frautschi and Suura, is that the divergences cancel in any rate that sums over undetectable soft emissions below an energy resolution EEE.

S. Weinberg's paper Infrared Photons and Gravitons (Phys. Rev. 140, B516 (1965)) shows that the same mechanism works for gravitons, derives explicit formulas for the exponents that control the soft factors, and proves that the extra "collinear" divergences produced by massless hard particles cancel for gravitons but not for photons. The soft-graviton factor (2.5)–(2.7) used there is the factor that appears in Weinberg's soft graviton theorem, and the spectrum formula is used in the paper to estimate the gravitational radiation from thermal collisions in the sun.

Timeline.

  • 1937 — Bloch and Nordsieck: soft-photon divergences cancel between virtual and real emission.
  • 1961 — Yennie, Frautschi and Suura: all-orders exponentiation of soft-photon factors in QED.
  • 1965 — Weinberg: the analogous treatment for gravitons, closed forms (2.16) and (2.26) for the exponents AAA and BBB, cancellation of collinear divergences for gravitons (Sec. III), and the Coulomb-phase result conjectured by Dalitz (Sec. V).

Setting

Work in units ℏ=c=1\hbar=c=1ℏ=c=1 with the paper's metric: for four-vectors p=(p,p0)p=(\mathbf p,p^0)p=(p,p0) and q=(q,q0)q=(\mathbf q,q^0)q=(q,q0), p⋅q=p⋅q−p0q0p\cdot q=\mathbf p\cdot\mathbf q-p^0q^0p⋅q=p⋅q−p0q0. A process α→β\alpha\to\betaα→β has finitely many external lines nnn; line nnn has mass mnm_nmn​, three-momentum pn∈R3\mathbf p_n\in\mathbb R^3pn​∈R3, on-shell energy En=∣pn∣2+mn2E_n=\sqrt{|\mathbf p_n|^2+m_n^2}En​=∣pn​∣2+mn2​​, charge ene_nen​, and sign ηn=+1\eta_n=+1ηn​=+1 (outgoing) or −1-1−1 (incoming). The relative velocity of lines n,mn,mn,m is

βnm=[1−mn2mm2(pn⋅pm)2]1/2.\beta_{nm}=\Bigl[1-\frac{m_n^2m_m^2}{(p_n\cdot p_m)^2}\Bigr]^{1/2}.βnm​=[1−(pn​⋅pm​)2mn2​mm2​​]1/2.

For a unit vector q^\hat qq^​ (the direction of a soft quantum) define the photon and graviton angular functions

A(q^)=12(2π)3∑n,menemηnηm(pn⋅pm)[En−pn⋅q^][Em−pm⋅q^],B(q^)=8πG2(2π)3∑n,mηnηm{(pn⋅pm)2−12mn2mm2}[En−pn⋅q^][Em−pm⋅q^],A(\hat q)=\frac{1}{2(2\pi)^3}\sum_{n,m}\frac{e_ne_m\eta_n\eta_m(p_n\cdot p_m)}{[E_n-\mathbf p_n\cdot\hat q][E_m-\mathbf p_m\cdot\hat q]},\qquad B(\hat q)=\frac{8\pi G}{2(2\pi)^3}\sum_{n,m}\frac{\eta_n\eta_m\{(p_n\cdot p_m)^2-\frac12m_n^2m_m^2\}}{[E_n-\mathbf p_n\cdot\hat q][E_m-\mathbf p_m\cdot\hat q]},A(q^​)=2(2π)31​n,m∑​[En​−pn​⋅q^​][Em​−pm​⋅q^​]en​em​ηn​ηm​(pn​⋅pm​)​,B(q^​)=2(2π)38πG​n,m∑​[En​−pn​⋅q^​][Em​−pm​⋅q^​]ηn​ηm​{(pn​⋅pm​)2−21​mn2​mm2​}​,

and the infrared exponents A=∫d2Ω A(q^)A=\int d^2\Omega\,A(\hat q)A=∫d2ΩA(q^​) and B=∫d2Ω B(q^)B=\int d^2\Omega\,B(\hat q)B=∫d2ΩB(q^​), integrals over the unit sphere against surface measure. With infrared cutoff λ\lambdaλ and dividing point Λ\LambdaΛ, virtual soft quanta multiply a rate by (λ/Λ)A(\lambda/\Lambda)^A(λ/Λ)A or (λ/Λ)B(\lambda/\Lambda)^B(λ/Λ)B, and summing over real soft emission of total energy at most EEE gives the cutoff-free factors (E/Λ)Ab(A)(E/\Lambda)^Ab(A)(E/Λ)Ab(A) and (E/Λ)Bb(B)(E/\Lambda)^Bb(B)(E/Λ)Bb(B) of Eqs. (2.51)–(2.52).

Formalization targets

Goal — Eq. (2.26)

For masses mn>0m_n>0mn​>0,

B=G2π∑n,mηnηmmnmm1+βnm2βnm(1−βnm2)1/2ln⁡(1+βnm1−βnm)=Gπ∑n,mηnmnηmmmf(βnm),B=\frac{G}{2\pi}\sum_{n,m}\eta_n\eta_mm_nm_m\frac{1+\beta_{nm}^2}{\beta_{nm}(1-\beta_{nm}^2)^{1/2}}\ln\Bigl(\frac{1+\beta_{nm}}{1-\beta_{nm}}\Bigr)=\frac{G}{\pi}\sum_{n,m}\eta_nm_n\eta_mm_mf(\beta_{nm}),B=2πG​n,m∑​ηn​ηm​mn​mm​βnm​(1−βnm2​)1/21+βnm2​​ln(1−βnm​1+βnm​​)=πG​n,m∑​ηn​mn​ηm​mm​f(βnm​),

with f(0)=1f(0)=1f(0)=1 for the diagonal terms. This is the formula for graviton bremsstrahlung in an arbitrary collision.

Milestones

  1. Sec. II.2 — summed over the N!N!N! orderings, the multiple pole factors of NNN soft emissions from one line factorize into single-emission factors.
  2. Eq. (2.13) — the real part of the virtual-photon exponent equals −Aln⁡(Λ/λ)-A\ln(\Lambda/\lambda)−Aln(Λ/λ).
  3. Eq. (2.16) — A=−18π2∑n,mηnηmenemβnm−1ln⁡1+βnm1−βnmA=-\frac{1}{8\pi^2}\sum_{n,m}\eta_n\eta_me_ne_m\beta_{nm}^{-1}\ln\frac{1+\beta_{nm}}{1-\beta_{nm}}A=−8π21​∑n,m​ηn​ηm​en​em​βnm−1​ln1−βnm​1+βnm​​.
  4. Eq. (2.14) — A≥0A\ge0A≥0 under charge conservation.
  5. Eq. (2.24) — B≥0B\ge0B≥0 under energy–momentum conservation.
  6. Eqs. (3.4)–(3.5) — if one line becomes massless, BBB stays finite (the ln⁡m1\ln m_1lnm1​ terms cancel by energy–momentum conservation).
  7. Eq. (3.3) — for photons the corresponding limit is A→+∞A\to+\inftyA→+∞ when the massless line is charged.
  8. Eq. (4.9) — f(β)=1+116β2+6340β4+O(β6)f(\beta)=1+\frac{11}{6}\beta^2+\frac{63}{40}\beta^4+O(\beta^6)f(β)=1+611​β2+4063​β4+O(β6).

Significance

The exponents AAA and BBB are the only process-dependent quantities in the soft factors: once they are known in closed form, the infrared behaviour of any rate, the shape EAE^AEA or EBE^BEB of the soft spectrum, and the soft power spectrum E dΓ=B Γ0 dEE\,d\Gamma=B\,\Gamma^0\,dEEdΓ=BΓ0dE (2.53) follow. The Sec. III cancellation is the statement that gravitation, unlike massless electrodynamics or Yang–Mills theory, is free of unremovable collinear divergences at this level; the paper uses the contrast to argue that charged massless particles are problematic. The expansion (4.9) feeds the nonrelativistic quadrupole formula (4.13) behind the solar estimate.

The paper's arguments are informal physics derivations. This mission makes the mathematical content of those derivations precise and machine-checkable: the angular integrals, the sign statements, the limiting behaviour as a mass goes to zero, and the combinatorial factorization.

Difficulty

The closed forms need the solid-angle integral of a product of two denominators [En−pn⋅q^]−1[Em−pm⋅q^]−1[E_n-\mathbf p_n\cdot\hat q]^{-1}[E_m-\mathbf p_m\cdot\hat q]^{-1}[En​−pn​⋅q^​]−1[Em​−pm​⋅q^​]−1 for two arbitrary, non-collinear momenta; the one-denominator case is a textbook integral in polar coordinates, but the two-denominator case does not reduce to it by an obvious choice of axis. The positivity statements are false without the conservation laws, so any proof must use them in an essential way. The massless-limit statements concern the interplay of a logarithmically divergent term with a coefficient that vanishes only at the limiting configuration, so a termwise limit fails.

Formalization scope

Three-momenta live in EuclideanSpace ℝ (Fin 3); energies are the on-shell values ∣p∣2+m2\sqrt{|\mathbf p|^2+m^2}∣p∣2+m2​ and are not free variables. Solid-angle integrals are Bochner integrals on the unit sphere against Mathlib's volume.toSphere (total mass 4π4\pi4π). External lines are indexed by an arbitrary Fintype; the signs ηn\eta_nηn​ are real numbers constrained to ±1\pm1±1 by hypothesis. Sums over n,mn,mn,m run over all ordered pairs, including n=mn=mn=m, where βnn=0\beta_{nn}=0βnn​=0; the kernels β−1ln⁡1+β1−β\beta^{-1}\ln\frac{1+\beta}{1-\beta}β−1ln1−β1+β​ and fff are extended by their limits 222 and 111 at β=0\beta=0β=0, so the formulas are not trivialized by Lean's convention x/0=0x/0=0x/0=0. The printed Eq. (4.6) has an exponent 1/21/21/2 on the logarithm's argument that contradicts (2.26), (4.5) and (4.9); the definition of fff drops it. The −iηϵ-i\eta\epsilon−iηϵ prescriptions are suppressed. The δ(q2)\delta(q^2)δ(q2) integration in (2.13) is carried out, leaving an integral over the shell λ≤∣q∣≤Λ\lambda\le|\mathbf q|\le\Lambdaλ≤∣q∣≤Λ. Positivity is stated as ≥0\ge0≥0, because A=B=0A=B=0A=B=0 in degenerate configurations. Sec. IV beyond (4.9) (the velocity expansion (4.8), the quadrupole formula (4.13), the solar estimate) and the Coulomb phases of Sec. V are out of scope for this mission.

A complete development needs solid-angle integration on S2S^2S2 (a spherical-coordinates change of variables for volume.toSphere), integration in polar coordinates on R3\mathbb R^3R3, and elementary inequalities for Minkowski products of timelike and null vectors. These are reusable beyond this mission, and contributions of them as separate lemmas are welcome.

Selected references

  • S. Weinberg, Infrared Photons and Gravitons, Phys. Rev. 140, B516 (1965). https://doi.org/10.1103/PhysRev.140.B516
  • F. Bloch and A. Nordsieck, Note on the Radiation Field of the Electron, Phys. Rev. 52, 54 (1937). https://doi.org/10.1103/PhysRev.52.54
  • D. R. Yennie, S. C. Frautschi and H. Suura, The infrared divergence phenomena and high-energy processes, Ann. Phys. 13, 379 (1961). https://doi.org/10.1016/0003-4916(61)90151-8
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Mathematical Physics·Captain: Lucas

Monopoles, Instantons and Confinement I: Kink Solitons and the Bogomol'nyi BoundTextbook

Motivation

Solitons (localized, finite-energy, non-dissipating solutions of classical field equations) are the simplest examples of the topological objects that dominate the non-perturbative physics of gauge theories: vortices, magnetic monopoles and instantons. G. 't Hooft's lecture notes Monopoles, Instantons and Confinement (arXiv:hep-th/0010225) open with the two textbook examples in one space and one time dimension, the φ⁴ kink and the sine-Gordon soliton, because every later construction in the notes (the Abrikosov–Nielsen–Olesen vortex, the 't Hooft–Polyakov monopole, the BPST instanton) repeats the same pattern: a degenerate vacuum, a static solution interpolating between two vacua, and an energy (or action) bounded below by a topological quantity — the Bogomol'nyi bound — which the soliton saturates.

This mission formalizes that pattern in its cleanest setting, Chapter 1 (Sections 1.1–1.2) together with Exercise (i) of the notes.

Setting

A static real scalar field is a function φ:R→R\varphi : \mathbb R \to \mathbb Rφ:R→R. Its energy (eq. (1.5)) for a potential VVV is

EV[φ]=∫−∞∞(12(∂xφ)2+V(φ)) dx∈[0,∞].E_V[\varphi] = \int_{-\infty}^{\infty} \Big(\tfrac12 (\partial_x\varphi)^2 + V(\varphi)\Big)\,dx \in [0,\infty].EV​[φ]=∫−∞∞​(21​(∂x​φ)2+V(φ))dx∈[0,∞].

Two potentials are considered, with parameters λ,A,F>0\lambda, A, F > 0λ,A,F>0:

  1. Case (a), the "Mexican hat" (eq. (1.2)): Va(φ)=λ4!(φ2−F2)2V_a(\varphi) = \frac{\lambda}{4!}(\varphi^2 - F^2)^2Va​(φ)=4!λ​(φ2−F2)2, with the two vacua φ=±F\varphi = \pm Fφ=±F and particle mass mmm given by m2=λF2/3m^2 = \lambda F^2/3m2=λF2/3.
  2. Case (b), sine-Gordon (eq. (1.3)): Vb(φ)=A(1−cos⁡(2πφ/F))V_b(\varphi) = A\big(1 - \cos(2\pi\varphi/F)\big)Vb​(φ)=A(1−cos(2πφ/F)), with vacua φ=nF\varphi = nFφ=nF, n∈Zn \in \mathbb Zn∈Z, particle mass m=2πA/Fm = 2\pi\sqrt A/Fm=2πA​/F and quartic coupling λ=16π4A/F4\lambda = 16\pi^4 A/F^4λ=16π4A/F4.

The static field equation is ∂x2φ=V′(φ)\partial_x^2\varphi = V'(\varphi)∂x2​φ=V′(φ). The notes give the explicit solutions

φa(x)=Ftanh⁡(12m(x−x0)),φb(x)=2Fπarctan⁡(em(x−x0)),\varphi_a(x) = F\tanh\big(\tfrac12 m(x-x_0)\big), \qquad \varphi_b(x) = \frac{2F}{\pi}\arctan\big(e^{m(x-x_0)}\big),φa​(x)=Ftanh(21​m(x−x0​)),φb​(x)=π2F​arctan(em(x−x0​)),

which interpolate between −F-F−F and FFF (case (a)) and between 000 and FFF (case (b)).

Formalization targets

Goal

For every x0x_0x0​: in case (a) the kink has energy 2m3/λ2m^3/\lambda2m3/λ and no differentiable configuration with φ(−∞)=−F\varphi(-\infty) = -Fφ(−∞)=−F, φ(+∞)=F\varphi(+\infty) = Fφ(+∞)=F has smaller energy; in case (b) the soliton has energy 8m3/λ8m^3/\lambda8m3/λ and no differentiable configuration with φ(−∞)=0\varphi(-\infty) = 0φ(−∞)=0, φ(+∞)=F\varphi(+\infty) = Fφ(+∞)=F has smaller energy:

EVa[φa]=2m3λ≤EVa[φ],EVb[φb]=8m3λ≤EVb[φ].E_{V_a}[\varphi_a] = \frac{2m^3}{\lambda} \le E_{V_a}[\varphi], \qquad E_{V_b}[\varphi_b] = \frac{8m^3}{\lambda} \le E_{V_b}[\varphi].EVa​​[φa​]=λ2m3​≤EVa​​[φ],EVb​​[φb​]=λ8m3​≤EVb​​[φ].

Milestones

  1. First integral of the static equation, eq. (1.4).
  2. The φ⁴ kink solves the static equation with the stated boundary values.
  3. The sine-Gordon soliton solves the static equation with the stated boundary values.
  4. The φ⁴ kink mass 2m3/λ2m^3/\lambda2m3/λ (p. 5).
  5. The sine-Gordon soliton mass 8m3/λ8m^3/\lambda8m3/λ (p. 5).
  6. Bogomol'nyi bound, case (a) (eq. (1.7), Exercise (i)).
  7. Bogomol'nyi bound, case (b) (eq. (1.7), Exercise (i)).

Significance

The result identifies the soliton mass with a boundary term, E=W(φ)∣φ−∞φ+∞E = W(\varphi)\big|_{\varphi_{-\infty}}^{\varphi_{+\infty}}E=W(φ)​φ−∞​φ+∞​​ with W′=2VW' = \sqrt{2V}W′=2V​, so the mass depends only on the pair of vacua joined, and shows the kink is a global energy minimizer in its topological sector — the classical stability statement behind treating the kink as a particle of mass ∝m3/λ\propto m^3/\lambda∝m3/λ, heavy in the weak-coupling regime.

The physics is classical and fully known. What this mission adds is a machine-checked account: explicit verification of the closed-form solutions, exact evaluation of improper energy integrals, and a rigorous Bogomol'nyi argument for configurations that are merely differentiable, with limits at ±∞\pm\infty±∞ rather than compact support. No existing platform theorem matching these statements was found by a library search at drafting time.

Difficulty

The pointwise inequality 12φ′2+V(φ)≥φ′2V(φ)\tfrac12\varphi'^2 + V(\varphi) \ge \varphi'\sqrt{2V(\varphi)}21​φ′2+V(φ)≥φ′2V(φ)​ is elementary; the difficulty lies in turning it into a statement about improper integrals over R\mathbb RR for arbitrary differentiable fields. One must handle configurations of infinite energy, pass from integrals over [a,b][a,b][a,b] to R\mathbb RR using only the boundary limits, and deal with 2V\sqrt{2V}2V​ being non-smooth at the vacua of VaV_aVa​ and at every vacuum of VbV_bVb​ (a configuration may overshoot a vacuum). The explicit energy computations require exact evaluation of ∫sech4\int \mathrm{sech}^4∫sech4 and ∫sech2\int \mathrm{sech}^2∫sech2 type integrals as Lebesgue integrals.

Formalization scope

  • Fields are functions R→R\mathbb R \to \mathbb RR→R; derivatives are Mathlib's deriv. Every competitor in the bounds is assumed differentiable everywhere, and boundary values are expressed as limits at −∞-\infty−∞ and +∞+\infty+∞.
  • The energy is a lower Lebesgue integral valued in [0,∞][0,\infty][0,∞] of the (nonnegative) energy density, so configurations with infinite energy are allowed and satisfy the bounds trivially; no integrability hypothesis is imposed.
  • The parameters are strictly positive: λ>0\lambda > 0λ>0, A>0A > 0A>0, F>0F > 0F>0. The masses mmm and the sine-Gordon coupling are defined from λ,A,F\lambda, A, Fλ,A,F by the relations of Section 1.1, not left as free parameters.
  • The statements do not assume the competitor solves the field equation, and do not assume finite energy — assuming either would weaken the bound.
  • All declarations live in the namespace MonopolesInstantonsConfinement, intended to be shared by later missions drawn from the same notes.

Selected references

  • G. 't Hooft, Monopoles, Instantons and Confinement, lecture notes (Saalburg 1999) written by F. Bruckmann, 2000. arXiv:hep-th/0010225
  • E. B. Bogomol'nyi, The stability of classical solutions, Sov. J. Nucl. Phys. 24 (1976) 449.
  • R. Rajaraman, Solitons and Instantons, North-Holland, 1982.
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Machine LearningProbability·Captain: Lucas

Les Houches Lectures on Deep Learning at Large & Infinite Width III: Input–Output Jacobian of Random ReLU NetworksTextbook

Motivation

Lecture 5 of the Les Houches lectures on deep learning at large and infinite width (arXiv:2309.01592, Section 5, lectures by B. Hanin) shows that a random ReLU network evaluated at a single input can be solved exactly. The statistics of the network depend on depth LLL and width nnn through the inverse temperature β=5∑ℓ=1L1/nℓ≈5L/n\beta = 5\sum_{\ell=1}^{L} 1/n_\ell \approx 5L/nβ=5∑ℓ=1L​1/nℓ​≈5L/n. The input–output Jacobian is the simplest quantity where this can be seen. Its second moment does not depend on depth or width. Its fourth moment grows like eβe^{\beta}eβ, which gives a quantitative sense in which the regime where both LLL and nnn are large is controlled by L/nL/nL/n rather than by LLL or nnn alone. The lectures derive this through a combinatorial sum-over-paths formalism developed in Hanin's earlier papers (references [20–22] of the notes).

Setting

Fix a depth L≥1L\ge 1L≥1 and widths n0,…,nL+1≥1n_0,\dots,n_{L+1}\ge 1n0​,…,nL+1​≥1. Let μ\muμ be a probability measure on R\mathbb RR that has a density with respect to Lebesgue measure, is symmetric (μ(−A)=μ(A)\mu(-A)=\mu(A)μ(−A)=μ(A)), and has variance ∫t2 dμ=1\int t^2\,d\mu=1∫t2dμ=1. The weights are

Wij(ℓ)=(2nℓ−1)1/2W^ij(ℓ),W^ij(ℓ) i.i.d.∼μ,1≤ℓ≤L+1,W^{(\ell)}_{ij}=\Big(\tfrac{2}{n_{\ell-1}}\Big)^{1/2}\widehat W^{(\ell)}_{ij},\qquad \widehat W^{(\ell)}_{ij}\ \text{i.i.d.}\sim\mu,\qquad 1\le\ell\le L+1,Wij(ℓ)​=(nℓ−1​2​)1/2Wij(ℓ)​,Wij(ℓ)​ i.i.d.∼μ,1≤ℓ≤L+1,

all biases are 000, and the preactivations at an input x∈Rn0x\in\mathbb R^{n_0}x∈Rn0​ are

z(1)=W(1)x,z(ℓ+1)=W(ℓ+1) ReLU(z(ℓ))(1≤ℓ≤L),ReLU(t)=max⁡(t,0).z^{(1)}=W^{(1)}x,\qquad z^{(\ell+1)}=W^{(\ell+1)}\,\mathrm{ReLU}\big(z^{(\ell)}\big)\quad(1\le\ell\le L),\qquad \mathrm{ReLU}(t)=\max(t,0).z(1)=W(1)x,z(ℓ+1)=W(ℓ+1)ReLU(z(ℓ))(1≤ℓ≤L),ReLU(t)=max(t,0).

The network output is z(L+1)(x)∈RnL+1z^{(L+1)}(x)\in\mathbb R^{n_{L+1}}z(L+1)(x)∈RnL+1​. The input–output Jacobian has entries ∂zq(L+1)/∂xp\partial z^{(L+1)}_q/\partial x_p∂zq(L+1)​/∂xp​. A path is a tuple γ=(γ(0),…,γ(L+1))\gamma=(\gamma(0),\dots,\gamma(L+1))γ=(γ(0),…,γ(L+1)) with γ(ℓ)∈{1,…,nℓ}\gamma(\ell)\in\{1,\dots,n_\ell\}γ(ℓ)∈{1,…,nℓ​}, and Γp,q\Gamma_{p,q}Γp,q​ is the set of paths with γ(0)=p\gamma(0)=pγ(0)=p and γ(L+1)=q\gamma(L+1)=qγ(L+1)=q. Along a path, Wγ(ℓ)=Wγ(ℓ)γ(ℓ−1)(ℓ)W^{(\ell)}_\gamma=W^{(\ell)}_{\gamma(\ell)\gamma(\ell-1)}Wγ(ℓ)​=Wγ(ℓ)γ(ℓ−1)(ℓ)​ and ξγ(ℓ)=1{zγ(ℓ)(ℓ)(x)>0}\xi^{(\ell)}_{\gamma}=\mathbf 1\{z^{(\ell)}_{\gamma(\ell)}(x)>0\}ξγ(ℓ)​=1{zγ(ℓ)(ℓ)​(x)>0}.

Formalization targets

Goal: second moment of the Jacobian (eq. (124))

For every fixed input x≠0x\neq0x=0 and all p,qp,qp,q,

E[(∂zq(L+1)∂xp)2]=2n0.\mathbb E\Big[\Big(\frac{\partial z^{(L+1)}_q}{\partial x_p}\Big)^2\Big]=\frac{2}{n_0}.E[(∂xp​∂zq(L+1)​​)2]=n0​2​.

Milestones

  1. Eq. (123): the output is a sum over paths, zq(L+1)=∑pxp∑γ∈Γp,q∏ℓ=1L+1Wγ(ℓ)∏ℓ=1Lξγ(ℓ)z^{(L+1)}_q=\sum_p x_p\sum_{\gamma\in\Gamma_{p,q}}\prod_{\ell=1}^{L+1}W^{(\ell)}_\gamma\prod_{\ell=1}^{L}\xi^{(\ell)}_\gammazq(L+1)​=∑p​xp​∑γ∈Γp,q​​∏ℓ=1L+1​Wγ(ℓ)​∏ℓ=1L​ξγ(ℓ)​.
  2. Proposition 5.2: at a fixed input x≠0x\neq 0x=0, the output has the same law as the output W(L+1)D(L)W(L)⋯D(1)W(1)xW^{(L+1)}D^{(L)}W^{(L)}\cdots D^{(1)}W^{(1)}xW(L+1)D(L)W(L)⋯D(1)W(1)x of a deep linear network with dropout. Here the D(ℓ)D^{(\ell)}D(ℓ) are diagonal with i.i.d. Bernoulli(1/2)(1/2)(1/2) entries, independent of the weights.
  3. Section 5.4, first exercise: almost surely, ∂zq(L+1)/∂xp=∑γ∈Γp,q∏ℓWγ(ℓ)∏ℓξγ(ℓ)\partial z^{(L+1)}_q/\partial x_p=\sum_{\gamma\in\Gamma_{p,q}}\prod_\ell W^{(\ell)}_\gamma\prod_\ell\xi^{(\ell)}_\gamma∂zq(L+1)​/∂xp​=∑γ∈Γp,q​​∏ℓ​Wγ(ℓ)​∏ℓ​ξγ(ℓ)​.
  4. Section 5.4, first exercise (conclusion): the law of ∂zq(L+1)/∂xp\partial z^{(L+1)}_q/\partial x_p∂zq(L+1)​/∂xp​ is the same for all x≠0x\neq0x=0.
  5. Section 5.5, fourth moment: E[(∂zq(L+1)/∂xp)4]=cn02exp⁡(5∑ℓ=1L1nℓ+O(L/n2))\mathbb E[(\partial z^{(L+1)}_q/\partial x_p)^4]=\frac{c}{n_0^2}\exp\big(5\sum_{\ell=1}^L\frac1{n_\ell}+O(L/n^2)\big)E[(∂zq(L+1)​/∂xp​)4]=n02​c​exp(5∑ℓ=1L​nℓ​1​+O(L/n2)). This is stated under the extra hypothesis ∫t4 dμ=3\int t^4\,d\mu=3∫t4dμ=3 (see Formalization scope).

Significance

Identity (124) says that, with the initialization CW=2C_W=2CW​=2 and zero biases, the typical size of the input–output Jacobian does not depend on depth or width. This is the exact form of the "criticality" of ReLU at CW=2C_W=2CW​=2. The fourth-moment statement shows that the fluctuations are not controlled in this way: they grow exponentially in β≈5L/n\beta\approx 5L/nβ≈5L/n. Together with Proposition 5.2, these results turn questions about deep random ReLU networks at one input into questions about products of random matrices with dropout. As far as the drafter knows, these statements have not been machine-checked before. The mission asks for formal proofs of the lecture's exact identities.

Difficulty

The ReLU network is not a linear function of the weights. Its activation pattern ξ(ℓ)\xi^{(\ell)}ξ(ℓ) depends on the weights of all earlier layers, so the path sum cannot be averaged term by term without first showing that the activation pattern is, in distribution, independent of the weights. That is the content of Proposition 5.2, which is argued only in sketch form in the notes. On top of that, the Jacobian must be identified with the path sum almost surely: at inputs where a preactivation vanishes the network is not differentiable. This requires the density assumption on μ\muμ and a separate treatment of layers in which every neuron is inactive.

Formalization scope

  • Widths form a sequence n : ℕ → ℕ; only n0,…,nL+1n_0,\dots,n_{L+1}n0​,…,nL+1​ are used. The normalized weights are coordinates of the product measure μ⊗\mu^{\otimes}μ⊗ on a finite index set (weightLaw). The Bernoulli masks are coordinates of the uniform product measure on Bool (maskLaw).
  • The Jacobian entry is the Fréchet derivative (fderiv) of y↦zq(L+1)(y)y\mapsto z^{(L+1)}_q(y)y↦zq(L+1)​(y) at xxx applied to the ppp-th basis vector. Mathlib returns 000 at points of non-differentiability, which form a null event for x≠0x\neq0x=0.
  • The notes write Wγ(ℓ)=Wγ(ℓ−1)γ(ℓ)(ℓ)W^{(\ell)}_\gamma=W^{(\ell)}_{\gamma(\ell-1)\gamma(\ell)}Wγ(ℓ)​=Wγ(ℓ−1)γ(ℓ)(ℓ)​. The formalization uses the orientation Wγ(ℓ)γ(ℓ−1)(ℓ)W^{(\ell)}_{\gamma(\ell)\gamma(\ell-1)}Wγ(ℓ)γ(ℓ−1)(ℓ)​, which matches the row/column convention of the network recursion.
  • Fourth moment. For a general μ\muμ the claim in §5.5 appears to need a correction. An informal computation (not part of this draft's verified content) gives a boundary term 2(μ4−3)(1/n1+1/nL)2(\mu_4-3)(1/n_1+1/n_L)2(μ4​−3)(1/n1​+1/nL​) in the exponent, which is of order 1/n1/n1/n rather than L/n2L/n^2L/n2 unless μ4=∫t4dμ=3\mu_4=\int t^4d\mu=3μ4​=∫t4dμ=3 (for example Gaussian μ\muμ). The milestone is therefore stated under the extra hypothesis μ4=3\mu_4=3μ4​=3. The constant c>0c>0c>0 and the O(⋅)O(\cdot)O(⋅) constant may depend on μ\muμ only.
  • An integral of a non-integrable function is 000 in Mathlib. The goal therefore also asserts integrability of the squared Jacobian, because 2/n0≠02/n_0\neq02/n0​=0.

Selected references

  • Y. Bahri, B. Hanin, A. Brossollet, V. Erba, C. Keup, R. Pacelli, J. B. Simon, Les Houches Lectures on Deep Learning at Large & Infinite Width, 2023. arXiv:2309.01592
  • B. Hanin, M. Nica, Products of Many Large Random Matrices and Gradients in Deep Neural Networks, Comm. Math. Phys., 2020. arXiv:1812.05994
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Machine LearningProbability·Captain: Lucas

Les Houches Lectures on Deep Learning at Large & Infinite Width II: Finite-Width Four-Point Function RecursionTextbook

Motivation

At infinite width a randomly initialized network is a Gaussian process (Mission I of this series). Real networks have finite width nnn, and the leading departure from Gaussianity is measured by the connected four-point function κ4\kappa_4κ4​. It captures both correlations between neurons and non-Gaussian fluctuations. Lecture 4 of the Les Houches lectures (arXiv:2309.01592, lectures by B. Hanin) states the central finite-width result, Theorem 4.2: κ4\kappa_4κ4​ is of order 1/n1/n1/n and obeys an explicit layer-to-layer recursion up to O(n−2)O(n^{-2})O(n−2). At criticality this gives the effective depth L/nL/nL/n as the parameter controlling finite-width effects. The result was first derived at a physics level of rigor by Yaida (2020) and in Roberts–Yaida–Hanin (2022), and later derived more mathematically by Hanin (reference [19] of the notes).

Setting

A network of depth LLL with widths n0,…,nL+1n_0,\dots,n_{L+1}n0​,…,nL+1​ and nonlinearity σ\sigmaσ has preactivations z(1)=b(1)+W(1)xz^{(1)}=b^{(1)}+W^{(1)}xz(1)=b(1)+W(1)x and z(ℓ+1)=b(ℓ+1)+W(ℓ+1)σ(z(ℓ))z^{(\ell+1)}=b^{(\ell+1)}+W^{(\ell+1)}\sigma(z^{(\ell)})z(ℓ+1)=b(ℓ+1)+W(ℓ+1)σ(z(ℓ)). The parameters are independent, with Wij(ℓ)∼N(0,CW/nℓ−1)W^{(\ell)}_{ij}\sim\mathcal N(0,C_W/n_{\ell-1})Wij(ℓ)​∼N(0,CW​/nℓ−1​) and bi(ℓ)∼N(0,Cb)b^{(\ell)}_i\sim\mathcal N(0,C_b)bi(ℓ)​∼N(0,Cb​), where Cb≥0C_b\ge0Cb​≥0 and CW>0C_W>0CW​>0 (eqs. (118)–(119)). At a single input xxx, write ⟨f⟩K\langle f\rangle_K⟨f⟩K​ for the average of fff against N(0,K)\mathcal N(0,K)N(0,K). The infinite-width kernel is K(1)=Cb+CW∣x∣2/n0K^{(1)}=C_b+C_W|x|^2/n_0K(1)=Cb​+CW​∣x∣2/n0​ and K(ℓ+1)=Cb+CW⟨σ2⟩K(ℓ)K^{(\ell+1)}=C_b+C_W\langle\sigma^2\rangle_{K^{(\ell)}}K(ℓ+1)=Cb​+CW​⟨σ2⟩K(ℓ)​ (eq. (120)). The parallel susceptibility is χ∥(ℓ)=CW ∂K⟨σ2⟩K∣K=K(ℓ)\chi_\parallel^{(\ell)}=C_W\,\partial_K\langle\sigma^2\rangle_K|_{K=K^{(\ell)}}χ∥(ℓ)​=CW​∂K​⟨σ2⟩K​∣K=K(ℓ)​. The normalized connected four-point function is

κ4(ℓ)=13(E[(zi(ℓ))4]−3 E[(zi(ℓ))2]2).\kappa^{(\ell)}_4=\tfrac13\Big(\mathbb E\big[(z^{(\ell)}_i)^4\big]-3\,\mathbb E\big[(z^{(\ell)}_i)^2\big]^2\Big).κ4(ℓ)​=31​(E[(zi(ℓ)​)4]−3E[(zi(ℓ)​)2]2).

Formalization targets

Goal: Theorem 4.2, recursion for κ4\kappa_4κ4​

If the hidden widths satisfy n≤nℓ≤Ann\le n_\ell\le Ann≤nℓ​≤An, then κ4(ℓ)=O(n−1)\kappa^{(\ell)}_4=O(n^{-1})κ4(ℓ)​=O(n−1) and

κ4(ℓ+1)=CW2nℓ VarK(ℓ)[σ2]+(χ∥(ℓ))2κ4(ℓ)+O(n−2),\kappa^{(\ell+1)}_4=\frac{C_W^2}{n_\ell}\,\mathrm{Var}_{K^{(\ell)}}\big[\sigma^2\big]+\big(\chi^{(\ell)}_\parallel\big)^2\kappa^{(\ell)}_4+O(n^{-2}),κ4(ℓ+1)​=nℓ​CW2​​VarK(ℓ)​[σ2]+(χ∥(ℓ)​)2κ4(ℓ)​+O(n−2),

with constants independent of the widths.

Milestones

  1. Proposition 4.3: AW∼N(Aμ,AΣAT)AW\sim\mathcal N(A\mu,A\Sigma A^{T})AW∼N(Aμ,AΣAT) for W∼N(μ,Σ)W\sim\mathcal N(\mu,\Sigma)W∼N(μ,Σ).
  2. Lemma 4.4: conditional on z(ℓ)z^{(\ell)}z(ℓ), the vector z(ℓ+1)z^{(\ell+1)}z(ℓ+1) is Gaussian with covariance Σ(ℓ)I\Sigma^{(\ell)}IΣ(ℓ)I, where Σ(ℓ)=Cb+CWnℓ∑jσ(zj(ℓ))2\Sigma^{(\ell)}=C_b+\frac{C_W}{n_\ell}\sum_j\sigma(z^{(\ell)}_j)^2Σ(ℓ)=Cb​+nℓ​CW​​∑j​σ(zj(ℓ)​)2; moreover κ4(ℓ+1)=Var[Σ(ℓ)]\kappa^{(\ell+1)}_4=\mathrm{Var}[\Sigma^{(\ell)}]κ4(ℓ+1)​=Var[Σ(ℓ)].
  3. Section 4.8, exercise: κ4(ℓ)=Cov((zi(ℓ))2,(zj(ℓ))2)\kappa^{(\ell)}_4=\mathrm{Cov}\big((z^{(\ell)}_i)^2,(z^{(\ell)}_j)^2\big)κ4(ℓ)​=Cov((zi(ℓ)​)2,(zj(ℓ)​)2) for i≠ji\neq ji=j.
  4. Theorem 4.2, criticality (ReLU, Cb=0C_b=0Cb​=0, CW=2C_W=2CW​=2, uniform width): κ4(L+1)/(K(L+1))2=CσL/n+OL(n−2)\kappa^{(L+1)}_4/(K^{(L+1)})^2=C_\sigma L/n+O_L(n^{-2})κ4(L+1)​/(K(L+1))2=Cσ​L/n+OL​(n−2).
  5. Theorem 4.2, expansion of observables: Ef(z1(ℓ),…,zm(ℓ))=⟨f⟩G(ℓ)+κ4(ℓ)8⟨(∑j∂j4+∑j1≠j2∂j12∂j22)f⟩K(ℓ)+O(n−2)\mathbb E f(z^{(\ell)}_1,\dots,z^{(\ell)}_m)=\langle f\rangle_{G^{(\ell)}}+\frac{\kappa^{(\ell)}_4}{8}\big\langle\big(\sum_j\partial_j^4+\sum_{j_1\neq j_2}\partial_{j_1}^2\partial_{j_2}^2\big)f\big\rangle_{K^{(\ell)}}+O(n^{-2})Ef(z1(ℓ)​,…,zm(ℓ)​)=⟨f⟩G(ℓ)​+8κ4(ℓ)​​⟨(∑j​∂j4​+∑j1​=j2​​∂j1​2​∂j2​2​)f⟩K(ℓ)​+O(n−2).

Significance

Theorem 4.2 is the first quantitative statement that finite-width networks at initialization are not Gaussian processes. The size of the deviation is 1/n1/n1/n per layer, and it accumulates linearly in depth at criticality. This is the basis for the claim of Lecture 4 that L/nL/nL/n controls correlations between neurons, fluctuations and, in later lectures, feature learning. As far as the drafter knows these statements have not been machine-checked. Lemma 4.4 and the covariance exercise are exact finite-width identities and are natural first targets.

Difficulty

The next layer is Gaussian only conditionally, with a random variance Σ(ℓ)\Sigma^{(\ell)}Σ(ℓ) that is an average over nℓn_\ellnℓ​ dependent neurons. Establishing the recursion to order n−2n^{-2}n−2 requires expanding Gaussian averages around the mean of Σ(ℓ)\Sigma^{(\ell)}Σ(ℓ) and controlling all higher cumulants of this collective observable uniformly in the widths. The nonlinearity is only assumed polynomially bounded, so smoothness must come from Gaussian averaging, not from σ\sigmaσ.

Formalization scope

  • Mission I's definitions (LesHouchesWidth_GaussianMLP: the network mlpZ, stdGaussianParams, nngpKernel, uniformWidths) are reused. Mission I must be launched first, and its definition then added to this proposal as a reference item.
  • New definitions (LesHouchesWidth_FiniteWidth): gaussAvg, gaussAvgVec, gaussVarSq, chiParallel, PolyBounded, kappa4, dressedTwoPoint, collectiveSigma.
  • "n1,…,nL≃nn_1,\dots,n_L\simeq nn1​,…,nL​≃n" is encoded as n≤nℓ≤Ann\le n_\ell\le Ann≤nℓ​≤An for a fixed A≥1A\ge1A≥1. The O(⋅)O(\cdot)O(⋅) constants may depend on all fixed data (Cb,CW,σ,L,n0,nL+1,x,AC_b,C_W,\sigma,L,n_0,n_{L+1},x,ACb​,CW​,σ,L,n0​,nL+1​,x,A, and m,fm,fm,f where relevant) but not on nnn or on the widths.
  • "Reasonable" σ\sigmaσ is taken to mean measurable and polynomially bounded, and the kernel is assumed nondegenerate: K(ℓ)>0K^{(\ell)}>0K(ℓ)>0 for 1≤ℓ≤L+11\le\ell\le L+11≤ℓ≤L+1, as the density-based definition of ⟨⋅⟩K\langle\cdot\rangle_K⟨⋅⟩K​ in Section 4.2 requires. "Reasonable" test functions fff are taken to be smooth with polynomially bounded derivatives of all orders.
  • The expansion of observables is stated with κ4(ℓ)\kappa^{(\ell)}_4κ4(ℓ)​ in front of the correction. The printed κ4(ℓ+1)\kappa^{(\ell+1)}_4κ4(ℓ+1)​ appears to be an index slip: with κ4(ℓ)\kappa^{(\ell)}_4κ4(ℓ)​ the formula reproduces E[z4]=3G2+3κ4\mathbb E[z^4]=3G^2+3\kappa_4E[z4]=3G2+3κ4​ and E[z12z22]=G2+κ4\mathbb E[z_1^2z_2^2]=G^2+\kappa_4E[z12​z22​]=G2+κ4​ exactly.
  • The criticality statement is formalized for ReLU at Cb=0C_b=0Cb​=0, CW=2C_W=2CW​=2, the one critical example in the notes where K(ℓ)K^{(\ell)}K(ℓ) is constant. For σ=tanh⁡\sigma=\tanhσ=tanh the notes' "≃\simeq≃" is asymptotic in depth and is not formalized here.

Selected references

  • Y. Bahri, B. Hanin, A. Brossollet, V. Erba, C. Keup, R. Pacelli, J. B. Simon, Les Houches Lectures on Deep Learning at Large & Infinite Width, 2023. arXiv:2309.01592
  • S. Yaida, Non-Gaussian processes and neural networks at finite widths, MSML 2020. arXiv:1910.00019
  • D. A. Roberts, S. Yaida, B. Hanin, The Principles of Deep Learning Theory, Cambridge University Press, 2022. arXiv:2106.10165
  • B. Hanin, Random Fully Connected Neural Networks as Perturbatively Solvable Hierarchies, 2022. arXiv:2204.01058
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Machine LearningProbability·Captain: Lucas

Les Houches Lectures on Deep Learning at Large & Infinite Width I: Gaussian-Process Limit of Wide Networks and Wick's TheoremTextbook

Motivation

A fully connected neural network with random Gaussian weights defines a random function of its input. Lecture 1 of the Les Houches lectures on deep learning at large and infinite width (arXiv:2309.01592, lectures by Y. Bahri) explains that, when the hidden layers become infinitely wide, this random function becomes a Gaussian process (the "neural network Gaussian process", NNGP). Its covariance kernel is computed by an explicit layer-to-layer recursion. The observation goes back to Neal (1996) for one hidden layer. It was extended to deep networks by Matthews et al. and Lee et al. (2018). It underlies Bayesian inference with infinitely wide networks (Section 1.6) and the analysis of signal propagation at large depth (Section 1.7). Lecture 2 introduces Wick's theorem, the tool for computing moments of Gaussian vectors that the lectures then use for finite-width corrections.

Setting

A network of depth LLL with widths n0,…,nL+1n_0,\dots,n_{L+1}n0​,…,nL+1​ and nonlinearity φ\varphiφ maps an input x∈Rn0x\in\mathbb R^{n_0}x∈Rn0​ to preactivations

zi(1)=bi(1)+∑jWij(1)xj,zi(ℓ+1)=bi(ℓ+1)+∑jWij(ℓ+1) φ(zj(ℓ)),z^{(1)}_i=b^{(1)}_i+\sum_{j}W^{(1)}_{ij}x_j,\qquad z^{(\ell+1)}_i=b^{(\ell+1)}_i+\sum_{j}W^{(\ell+1)}_{ij}\,\varphi\big(z^{(\ell)}_j\big),zi(1)​=bi(1)​+j∑​Wij(1)​xj​,zi(ℓ+1)​=bi(ℓ+1)​+j∑​Wij(ℓ+1)​φ(zj(ℓ)​),

with independent bi(ℓ)∼N(0,σb2)b^{(\ell)}_i\sim\mathcal N(0,\sigma_b^2)bi(ℓ)​∼N(0,σb2​) and Wij(ℓ)∼N(0,σw2/nℓ−1)W^{(\ell)}_{ij}\sim\mathcal N(0,\sigma_w^2/n_{\ell-1})Wij(ℓ)​∼N(0,σw2​/nℓ−1​) (eqs. (1)–(3) and (5); layers are indexed as in Lectures 4–5, so zlz^{l}zl of Lecture 1 is z(l+1)z^{(l+1)}z(l+1) here). For a 2×22\times22×2 covariance Σ\SigmaΣ write Fφ(Σ11,Σ12,Σ22)=E(u1,u2)∼N(0,Σ)[φ(u1)φ(u2)]F_\varphi(\Sigma_{11},\Sigma_{12},\Sigma_{22})=\mathbb E_{(u_1,u_2)\sim\mathcal N(0,\Sigma)}[\varphi(u_1)\varphi(u_2)]Fφ​(Σ11​,Σ12​,Σ22​)=E(u1​,u2​)∼N(0,Σ)​[φ(u1​)φ(u2​)] (eq. (15)). The NNGP kernel is

K(1)(x,x′)=σb2+σw2 x⋅x′n0,K(ℓ+1)(x,x′)=σb2+σw2Fφ(K(ℓ)(x,x),K(ℓ)(x,x′),K(ℓ)(x′,x′)).K^{(1)}(x,x')=\sigma_b^2+\sigma_w^2\,\frac{x\cdot x'}{n_0},\qquad K^{(\ell+1)}(x,x')=\sigma_b^2+\sigma_w^2F_\varphi\big(K^{(\ell)}(x,x),K^{(\ell)}(x,x'),K^{(\ell)}(x',x')\big).K(1)(x,x′)=σb2​+σw2​n0​x⋅x′​,K(ℓ+1)(x,x′)=σb2​+σw2​Fφ​(K(ℓ)(x,x),K(ℓ)(x,x′),K(ℓ)(x′,x′)).

A pairing of {1,…,2m}\{1,\dots,2m\}{1,…,2m} is a partition into mmm two-element blocks.

Formalization targets

Goal: Result 1 (single hidden layer)

For a network with one hidden layer of width nnn, fixed inputs x1,…,xmx_1,\dots,x_mx1​,…,xm​ and output width n2n_2n2​, as n→∞n\to\inftyn→∞ the vector (zi(2)(xa))i≤n2, a≤m(z^{(2)}_i(x_a))_{i\le n_2,\,a\le m}(zi(2)​(xa​))i≤n2​,a≤m​ converges in distribution to a centered Gaussian with covariance

E[zi(2)(xa)zj(2)(xb)]→δijK(2)(xa,xb).\mathbb E\big[z^{(2)}_i(x_a)z^{(2)}_j(x_b)\big]\to\delta_{ij}K^{(2)}(x_a,x_b).E[zi(2)​(xa​)zj(2)​(xb​)]→δij​K(2)(xa​,xb​).

Milestones

  1. Eq. (10): E[zi(1)(x)zi(1)(x′)]=K(1)(x,x′)\mathbb E[z^{(1)}_i(x)z^{(1)}_i(x')]=K^{(1)}(x,x')E[zi(1)​(x)zi(1)​(x′)]=K(1)(x,x′).
  2. Eqs. (9), (11): E[zi(2)(x)zi(2)(x′)]=K(2)(x,x′)\mathbb E[z^{(2)}_i(x)z^{(2)}_i(x')]=K^{(2)}(x,x')E[zi(2)​(x)zi(2)​(x′)]=K(2)(x,x′) at every finite width.
  3. Eq. (16): closed form of FReLUF_{\mathrm{ReLU}}FReLU​ (the arc-cosine kernel).
  4. Result 2 (Wick's theorem): E[zμ1⋯zμ2m]=∑pairings∏Kμkμk′\mathbb E[z_{\mu_1}\cdots z_{\mu_{2m}}]=\sum_{\text{pairings}}\prod K_{\mu_k\mu_{k'}}E[zμ1​​⋯zμ2m​​]=∑pairings​∏Kμk​μk′​​ for z∼N(0,K)z\sim\mathcal N(0,K)z∼N(0,K), and odd moments vanish.

A further item states the deep version of the limit, eqs. (13)–(14), in the simultaneous-width limit. It is included as a supporting theorem rather than a milestone.

Significance

Result 1 and its deep extension identify the prior over functions induced by random initialization. They also make the NNGP kernel the central computational object of the infinite-width theory. The finite-width covariance identities (9)–(11) are exact and explain where the recursion comes from. Formula (16) makes the recursion explicit for ReLU. Wick's theorem is the basic tool of the finite-width perturbation theory of later lectures. These are classical results. The mission asks for their formal proofs against a single shared model of random networks that the later missions of this series reuse.

Difficulty

Result 1 is a multivariate central limit theorem for sums of nnn i.i.d. vectors whose entries are products of a Gaussian weight and a nonlinear function of Gaussian first-layer preactivations. No assumption beyond square-integrability of φ\varphiφ against the relevant Gaussians is imposed, so the CLT must be applied in its L2L^2L2 form. The deep limit is harder: for L≥2L\ge2L≥2 the hidden preactivations are not Gaussian at finite width, and one must control a triangular array in which the widths of all layers grow together. The ReLU formula (16) is an explicit but delicate Gaussian integral over a cone.

Formalization scope

  • The parameters are coordinates of i.i.d. standard Gaussians (stdGaussianParams), scaled by σb\sigma_bσb​ and σw/nℓ−1\sigma_w/\sqrt{n_{\ell-1}}σw​/nℓ−1​​ (mlpBias, mlpWeight). This is equality in law with the prior (5).
  • Bivariate Gaussian averages use Mathlib's multivariateGaussian. Convergence in distribution is stated with bounded continuous test functions: E g(Zn)→∫g dN(0,C)\mathbb E\,g(Z_n)\to\int g\,d\mathcal N(0,C)Eg(Zn​)→∫gdN(0,C) for every bounded continuous ggg.
  • The one-hidden-layer goal assumes only that φ\varphiφ is measurable and that φ2\varphi^2φ2 is integrable against N(0,K(1)(xa,xa))\mathcal N(0,K^{(1)}(x_a,x_a))N(0,K(1)(xa​,xa​)) for each input. The deep statement assumes φ\varphiφ continuous with a linear envelope ∣φ(u)∣≤c+M∣u∣|\varphi(u)|\le c+M|u|∣φ(u)∣≤c+M∣u∣, the condition used by Matthews et al. (2018). The notes defer to the references for these conditions.
  • Pairings are fixed-point-free involutions of {0,…,2m−1}\{0,\dots,2m-1\}{0,…,2m−1}.

Selected references

  • Y. Bahri, B. Hanin, A. Brossollet, V. Erba, C. Keup, R. Pacelli, J. B. Simon, Les Houches Lectures on Deep Learning at Large & Infinite Width, 2023. arXiv:2309.01592
  • R. M. Neal, Bayesian Learning for Neural Networks, Springer, 1996. doi:10.1007/978-1-4612-0745-0
  • A. G. de G. Matthews, M. Rowland, J. Hron, R. E. Turner, Z. Ghahramani, Gaussian Process Behaviour in Wide Deep Neural Networks, ICLR 2018. arXiv:1804.11271
  • Y. Cho, L. K. Saul, Kernel Methods for Deep Learning, NeurIPS 2009.
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AnalysisMathematical Physics·Captain: Lucas

Missing baryons from stacked SZ filaments: the model and statistics of de Graaff et al. (2019)Research Paper

Motivation

Big-bang nucleosynthesis and the acoustic peaks of the cosmic microwave background fix the baryon density of the universe to about 5% of its total energy density, but in the low-redshift universe only some 10% of those baryons are seen in galaxies, with another 10% in the circumgalactic and intracluster medium. Simulations place the remainder — the missing baryons — in a diffuse warm-hot intergalactic medium (WHIM) at 10510^5105–10710^7107 K, spread along the filaments of the cosmic web. Absorption-line studies and X-ray emission from individual filaments probe the cool and the hot ends of that range respectively, leaving the bulk poorly constrained.

de Graaff, Cai, Heymans & Peacock (2019) attack the problem statistically, by stacking the Planck Compton-yyy map over 1 020 3341\,020\,3341020334 pairs of CMASS galaxies and measuring the residual signal in the bridge between each pair. Interpreting that residual requires an analytic model of a filament, and that model — a cylinder with a Gaussian cross-section, convolved with the instrument beam — is what this mission formalizes. The same model, applied to the CMB lensing convergence map, converts the measured signals into a gas density and temperature, and hence into a baryon fraction.

Setting

A filament is modelled as an infinite cylinder seen side-on. In the plane perpendicular to the filament axis, write ℓ\ellℓ for the line-of-sight coordinate and r⊥r_\perpr⊥​ for the transverse coordinate on the sky. The electron density is taken to be a two-dimensional Gaussian

ne(ℓ,r⊥)=n0exp⁡ ⁣(−ℓ22σ2)exp⁡ ⁣(−r⊥22(σ2+σB2)),n_e(\ell, r_\perp) = n_0 \exp\!\left(-\frac{\ell^2}{2\sigma^2}\right)\exp\!\left(-\frac{r_\perp^2}{2(\sigma^2+\sigma_B^2)}\right),ne​(ℓ,r⊥​)=n0​exp(−2σ2ℓ2​)exp(−2(σ2+σB2​)r⊥2​​),

with central density n0n_0n0​, intrinsic width σ\sigmaσ and beam width σB\sigma_BσB​; the transverse direction, unlike the line of sight, is smoothed by the instrument beam, which is why σB\sigma_BσB​ appears only there.

The Compton yyy parameter of a line of sight is the optical-depth-weighted temperature of the scattering electrons,

y=kBTeσTmec2∫ne dℓ,y = \frac{k_B T_e \sigma_T}{m_e c^2}\int n_e \, d\ell,y=me​c2kB​Te​σT​​∫ne​dℓ,

with kBk_BkB​ the Boltzmann constant, σT\sigma_TσT​ the Thomson cross-section, mec2m_e c^2me​c2 the electron rest energy and TeT_eTe​ the electron temperature, assumed constant across the filament. The convergence κ\kappaκ of CMB lensing is the analogous projection of the total matter density contrast δ=ρ/ρˉ−1\delta = \rho/\bar\rho - 1δ=ρ/ρˉ​−1,

κ=3H02Ωm2c2∫0DSDL(DS−DL)DS δa dDL,\kappa = \frac{3H_0^2\Omega_m}{2c^2}\int_0^{D_S} \frac{D_L(D_S-D_L)}{D_S}\,\frac{\delta}{a}\, dD_L,κ=2c23H02​Ωm​​∫0DS​​DS​DL​(DS​−DL​)​aδ​dDL​,

with H0H_0H0​ the Hubble constant, Ωm\Omega_mΩm​ the matter density parameter, aaa the scale factor and DL,DSD_L, D_SDL​,DS​ the comoving distances of lens and source. For a structure thin compared with the lensing kernel, the geometric factor is constant across it and κ\kappaκ reduces to a line-of-sight integral of δ\deltaδ against a fixed prefactor.

The significance of the measurement is assessed with a second, statistical layer. A stack of NNN binned profiles yiky^k_iyik​ (kkk the map index, iii the bin index) has mean profile yˉi=1N∑kyik\bar y_i = \frac1N\sum_k y^k_iyˉ​i​=N1​∑k​yik​ and covariance estimator Ci,j=1N∑k(yik−yˉi)(yjk−yˉj)C_{i,j} = \frac1N\sum_k (y^k_i-\bar y_i)(y^k_j-\bar y_j)Ci,j​=N1​∑k​(yik​−yˉ​i​)(yjk​−yˉ​j​); the deviation of the mean profile from zero is measured by χ2=∑i,jyˉi(C−1)i,jyˉj\chi^2 = \sum_{i,j}\bar y_i (C^{-1})_{i,j}\bar y_jχ2=∑i,j​yˉ​i​(C−1)i,j​yˉ​j​. Because the stacked maps overlap on the sky, the paper replaces CCC by a jackknife covariance built from NsubN_{\mathrm{sub}}Nsub​ sky sub-samples, Ci,jJK=Nsub−1Nsub∑k(yik−yˉi)(yjk−yˉj)C^{JK}_{i,j} = \frac{N_{\mathrm{sub}}-1}{N_{\mathrm{sub}}}\sum_k (y^k_i-\bar y_i)(y^k_j-\bar y_j)Ci,jJK​=Nsub​Nsub​−1​∑k​(yik​−yˉ​i​)(yjk​−yˉ​j​), and multiplies the inverse by the Hartlap factor (Nsub−n−2)/(Nsub−1)(N_{\mathrm{sub}}-n-2)/(N_{\mathrm{sub}}-1)(Nsub​−n−2)/(Nsub​−1), with nnn the number of bins.

Measurements enter through two numbers: the mean Compton parameter yˉ\bar{y}yˉ​ and the mean convergence κˉ\bar{\kappa}κˉ over the boxed filament region, together with the empirical observation that the peak of each profile is close to 1/0.91/0.91/0.9 times its mean. Every statement in this mission imposes that calibration as a hypothesis on the model.

Formalization targets

Goal — total electron content, Eq. (A.4)

Ne  =  L∬ne dℓ dr⊥  =  yˉ0.9 mec2kBTeσT 2π L σ2+σB2.N_e \;=\; L \iint n_e\, d\ell\, dr_\perp \;=\; \frac{\bar y}{0.9}\,\frac{m_e c^2}{k_B T_e \sigma_T}\,\sqrt{2\pi}\, L\, \sqrt{\sigma^2+\sigma_B^2}.Ne​=L∬ne​dℓdr⊥​=0.9yˉ​​kB​Te​σT​me​c2​2π​Lσ2+σB2​​.

This is the quantity the paper's baryon budget is computed from: given the measured yˉ\bar yyˉ​, an assumed temperature TeT_eTe​ and the beam width, it fixes the number of electrons in a filament of length LLL.

Milestone — projected profile, Eq. (A.2)

y(r⊥)=2π n0σ kBTeσTmec2exp⁡ ⁣(−r⊥22(σ2+σB2)).y(r_\perp) = \sqrt{2\pi}\, n_0\sigma\,\frac{k_B T_e \sigma_T}{m_e c^2}\exp\!\left(-\frac{r_\perp^2}{2(\sigma^2+\sigma_B^2)}\right).y(r⊥​)=2π​n0​σme​c2kB​Te​σT​​exp(−2(σ2+σB2​)r⊥2​​).

Milestone — central density, Eq. (A.3)

n0=yˉ/0.92π σ⋅mec2kBTeσT.n_0 = \frac{\bar y/0.9}{\sqrt{2\pi}\,\sigma}\cdot\frac{m_e c^2}{k_B T_e \sigma_T}.n0​=2π​σyˉ​/0.9​⋅kB​Te​σT​me​c2​.

Milestone — lensing counterpart, Eq. (A.5)

δ0=κˉ/0.92π σ⋅2ac23H02Ωm⋅DSDL(DS−DL).\delta_0 = \frac{\bar\kappa/0.9}{\sqrt{2\pi}\,\sigma}\cdot\frac{2ac^2}{3H_0^2\Omega_m}\cdot\frac{D_S}{D_L(D_S-D_L)}.δ0​=2π​σκˉ/0.9​⋅3H02​Ωm​2ac2​⋅DL​(DS​−DL​)DS​​.

Milestone — beam dominance, the remark after Eq. (A.4)

σB≤σ2+σB2≤σB(1+σ22σB2).\sigma_B \le \sqrt{\sigma^2+\sigma_B^2}\le \sigma_B\left(1+\frac{\sigma^2}{2\sigma_B^2}\right).σB​≤σ2+σB2​​≤σB​(1+2σB2​σ2​).

Milestone — the covariance estimators, Eqs. (3) and (5)-(6)

Both CCC and CJKC^{JK}CJK are symmetric and positive semidefinite, for every data set and every sample size.

Milestone — the significance statistic, Eq. (4)

C positive definite  ⟹  χ2=∑i,jyˉi(C−1)i,jyˉj≥0.C \text{ positive definite} \implies \chi^2 = \sum_{i,j}\bar y_i (C^{-1})_{i,j}\bar y_j \ge 0.C positive definite⟹χ2=i,j∑​yˉ​i​(C−1)i,j​yˉ​j​≥0.

Milestone — the Hartlap correction, Eq. (7)

∑i,jyˉi[Nsub−n−2Nsub−1C−1]i,jyˉj=Nsub−n−2Nsub−1∑i,jyˉi(C−1)i,jyˉj.\sum_{i,j}\bar y_i\left[\frac{N_{\mathrm{sub}}-n-2}{N_{\mathrm{sub}}-1}C^{-1}\right]_{i,j}\bar y_j = \frac{N_{\mathrm{sub}}-n-2}{N_{\mathrm{sub}}-1}\sum_{i,j}\bar y_i (C^{-1})_{i,j}\bar y_j.i,j∑​yˉ​i​[Nsub​−1Nsub​−n−2​C−1]i,j​yˉ​j​=Nsub​−1Nsub​−n−2​i,j∑​yˉ​i​(C−1)i,j​yˉ​j​.

Significance

The four displayed identities are the entire inferential chain from two stacked maps to a baryon fraction. Eq. (A.2) says what the model predicts for the observable; Eq. (A.3) inverts it at the filament axis; Eq. (A.4) turns the inversion into a total electron count, from which the paper obtains gas at (5.5±2.9) ρˉb(5.5\pm2.9)\,\bar\rho_b(5.5±2.9)ρˉ​b​ and T=(2.7±1.7)×106T=(2.7\pm1.7)\times10^6T=(2.7±1.7)×106 K, accounting for 11±7%11\pm7\%11±7% of the cosmic baryon budget; Eq. (A.5) supplies the independent lensing constraint that breaks the density–temperature degeneracy of the SZ measurement alone. The statistical milestones cover the other half of the analysis: the covariance estimators of Eqs. (3) and (5)-(6) that turn a stack into an error bar, the nonnegativity of the χ2\chi^2χ2 of Eq. (4) that is converted into the quoted 2.9σ2.9\sigma2.9σ, and the Hartlap rescaling of Eq. (7). The beam-dominance milestone quantifies the paper's claim that the result barely depends on the one free shape parameter, the intrinsic width σ\sigmaσ, which is taken from simulations rather than measured.

Formalizing them contributes a machine-checked derivation layer for a widely used observational technique: the projection of a Gaussian cylinder onto a Compton-yyy or convergence map, and the inversion of that projection, recur throughout stacked-SZ and stacked-lensing analyses. What this mission adds over the paper is a statement of each identity with all its hypotheses exposed — which positivity conditions are needed, which parameters genuinely drop out — rather than a new physical result. The physics is not re-derived and the measurement is not re-analysed; the empirical inputs yˉ\bar yyˉ​, κˉ\bar\kappaκˉ and the peak-to-mean ratio 1/0.91/0.91/0.9 enter as hypotheses, not as claims.

Difficulty

The identities are Gaussian integrals, so the mathematical depth is modest; the difficulty is bookkeeping and faithfulness. Three specific traps. First, the line-of-sight and transverse directions have different widths — σ\sigmaσ against σ2+σB2\sqrt{\sigma^2+\sigma_B^2}σ2+σB2​​ — and the asymmetry is what makes the final answer depend on the beam; a formalization that symmetrizes them is a different theorem. Second, the paper's n0n_0n0​ is not free: it is pinned by the calibration ypeak=yˉ/0.9y_{\text{peak}} = \bar y/0.9ypeak​=yˉ​/0.9, so the goal must carry that equation as a hypothesis rather than substituting a closed form for n0n_0n0​ silently. Third, the total electron count is an iterated integral over the plane, and the inner and outer variables must be kept in the paper's order.

Formalization scope

Everything is stated over R\mathbb{R}R with no units, so every physical constant is an explicit real variable; integrals are Bochner integrals over the whole real line with Lebesgue measure, which return 000 on a non-integrable integrand. The definition bundle fixes the model once — the SZ prefactor, the Gaussian cylinder profile, the Compton parameter, the thin-lens convergence prefactor, the convergence and the total electron content — and every statement is phrased against it. The convergence definition is the thin-lens specialization of Eq. (2): the geometric kernel is a constant prefactor, not an integral over lens distance, and the mission does not claim the reduction from the full Eq. (2) to that form.

Degenerate readings are ruled out as follows. The calibration hypotheses are satisfiable for every admissible choice of constants, so no statement is vacuous; conversely they genuinely constrain the central amplitude, so no statement holds for a trivial reason. The positivity hypotheses are the minimal ones that make the denominators nonzero, and the widths enter as σ>0\sigma > 0σ>0 with σB\sigma_BσB​ unrestricted, so the beam-free case σB=0\sigma_B = 0σB​=0 is included rather than excluded. The statistical layer is finite-dimensional: profiles are real arrays indexed by a finite bin type, covariances are real matrices, and matrix inversion is the nonsingular inverse, which returns the zero matrix on a singular argument — hence the positive-definiteness hypothesis in the χ2\chi^2χ2 milestone. Counts are natural numbers but all arithmetic in the prefactors is performed after casting to the reals, so Nsub−n−2N_{\mathrm{sub}} - n - 2Nsub​−n−2 is a genuine real subtraction and may be negative. The statistical statements assert the structural properties of the estimators as written; they do not assert unbiasedness, nor the reduction C→C/NC \to C/NC→C/N for the covariance of a mean, nor any property of the resampling scheme. Only Mathlib's Gaussian-integral, measure-theory and positive-semidefinite-matrix API is needed; no new infrastructure is required, and the resulting projection lemmas are reusable for any other stacked-profile analysis.

Selected references

  • A. de Graaff, Y.-C. Cai, C. Heymans, J. A. Peacock, Probing the missing baryons with the Sunyaev-Zel'dovich effect from filaments, Astronomy & Astrophysics 624, A48 (2019). doi:10.1051/0004-6361/201935159
  • R. A. Sunyaev, Y. B. Zeldovich, The Observations of Relic Radiation as a Test of the Nature of X-Ray Radiation from the Clusters of Galaxies, Comments on Astrophysics and Space Physics 4, 173 (1972).
  • Planck Collaboration XXII, Planck 2015 results. XXII. A map of the thermal Sunyaev-Zeldovich effect, A&A 594, A22 (2016). doi:10.1051/0004-6361/201525826
  • Planck Collaboration XV, Planck 2015 results. XV. Gravitational lensing, A&A 594, A15 (2016). doi:10.1051/0004-6361/201525941
  • J. Hartlap, P. Simon, P. Schneider, Why your model parameter confidences might be too optimistic: unbiased estimation of the inverse covariance matrix, A&A 464, 399 (2007). doi:10.1051/0004-6361:20066170
  • H. Tanimura et al., A search for warm/hot gas filaments between pairs of SDSS Luminous Red Galaxies, MNRAS 483, 223 (2019). doi:10.1093/mnras/sty3118
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Rydberg constant: Bohr-model derivation of the Rydberg formulaTextbook

Motivation

The Rydberg constant R∞R_\inftyR∞​ is the constant of spectroscopy that sets the scale of the hydrogen spectrum. It first appeared as an empirical fitting parameter in J. Rydberg's formula for the hydrogen spectral series; N. Bohr later showed that its value can be computed from more fundamental constants within his model of the atom. Before the 2019 revision of the SI it was, together with the electron spin ggg-factor, among the most accurately measured physical constants (relative standard uncertainty about 1.1×10−121.1\times 10^{-12}1.1×10−12, CODATA 2022). This mission formalizes the algebraic content of the standard account of R∞R_\inftyR∞​ as presented in the Wikipedia article Rydberg constant: its closed form, its reduced-mass correction, its alternative expressions through the fine-structure constant, and the Bohr-model derivation of the Rydberg formula.

Setting

Fix five strictly positive real numbers: the electron rest mass mem_eme​, the elementary charge eee, the vacuum permittivity ε0\varepsilon_0ε0​, the Planck constant hhh and the speed of light ccc. From them define

R∞=mee48ε02h3c,ℏ=h2π,α=14πε0e2ℏc,R_\infty=\frac{m_e e^4}{8\varepsilon_0^2h^3c},\qquad \hbar=\frac{h}{2\pi},\qquad \alpha=\frac{1}{4\pi\varepsilon_0}\frac{e^2}{\hbar c},R∞​=8ε02​h3cme​e4​,ℏ=2πh​,α=4πε0​1​ℏce2​,

the Compton wavelength λe=h/(mec)\lambda_e=h/(m_ec)λe​=h/(me​c), Compton frequency fC=mec2/hf_C=m_ec^2/hfC​=me​c2/h, Compton angular frequency ωC=2πfC\omega_C=2\pi f_CωC​=2πfC​, Bohr radius a0=4πε0ℏ2/(e2me)a_0=4\pi\varepsilon_0\hbar^2/(e^2m_e)a0​=4πε0​ℏ2/(e2me​), classical electron radius re=14πε0e2mec2r_e=\frac{1}{4\pi\varepsilon_0}\frac{e^2}{m_ec^2}re​=4πε0​1​me​c2e2​, and the Rydberg unit of energy Ry=hcR∞\mathrm{Ry}=hcR_\inftyRy=hcR∞​.

For a nucleus of mass M>0M>0M>0 the reduced mass is μ=1/(1/me+1/M)\mu=1/(1/m_e+1/M)μ=1/(1/me​+1/M) and the corrected Rydberg constant is RM=(μ/me)R∞R_M=(\mu/m_e)R_\inftyRM​=(μ/me​)R∞​; for hydrogen M=mpM=m_pM=mp​ and RM=RHR_M=R_{\mathrm H}RM​=RH​.

A Bohr orbit with principal quantum number nnn of a particle of mass mmm and charge −e-e−e about a fixed charge +e+e+e is a circular orbit of radius r>0r>0r>0 and speed v>0v>0v>0 such that the Coulomb force supplies the centripetal force and the angular momentum is quantized:

mv2r=e24πε0r2,mvr=nℏ.\frac{mv^2}{r}=\frac{e^2}{4\pi\varepsilon_0r^2},\qquad mvr=n\hbar .rmv2​=4πε0​r2e2​,mvr=nℏ.

Its energy is E=12mv2−e24πε0rE=\tfrac12mv^2-\dfrac{e^2}{4\pi\varepsilon_0 r}E=21​mv2−4πε0​re2​. The infinite-nuclear-mass model uses m=mem=m_em=me​; the reduced-mass model uses m=μm=\mum=μ.

Formalization targets

Goal: the Rydberg formula with reduced mass

For distinct positive integers n1,n2n_1,n_2n1​,n2​ and Bohr orbits of mass μ\muμ with quantum numbers n1,n2n_1,n_2n1​,n2​, the wavenumber 1/λ=(En2−En1)/(hc)1/\lambda=(E_{n_2}-E_{n_1})/(hc)1/λ=(En2​​−En1​​)/(hc) of the photon emitted in the transition satisfies

1λ=RM(1n12−1n22).\frac1\lambda=R_M\left(\frac1{n_1^2}-\frac1{n_2^2}\right).λ1​=RM​(n12​1​−n22​1​).

Milestones

  1. Equivalent forms of the reduced-mass correction: RM=μmeR∞=R∞1+me/M=Mme+MR∞R_M=\frac{\mu}{m_e}R_\infty=\frac{R_\infty}{1+m_e/M}=\frac{M}{m_e+M}R_\inftyRM​=me​μ​R∞​=1+me​/MR∞​​=me​+MM​R∞​.
  2. Isotopic shift: RMR_MRM​ is strictly increasing in MMM and stays below R∞R_\inftyR∞​.
  3. Rydberg unit of energy: hcR∞=α2mec2/2hcR_\infty=\alpha^2m_ec^2/2hcR∞​=α2me​c2/2.
  4. Alternative expressions: R∞=α2mec2h=α22λe=α4πa0R_\infty=\frac{\alpha^2m_ec}{2h}=\frac{\alpha^2}{2\lambda_e}=\frac{\alpha}{4\pi a_0}R∞​=2hα2me​c​=2λe​α2​=4πa0​α​, and 1/R∞=(4π/α)a01/R_\infty=(4\pi/\alpha)a_01/R∞​=(4π/α)a0​.
  5. Energy-unit expressions: Ry=12mec2α2=12e4me(4πε0)2ℏ2=12mec2rea0=12hcα2λe=12hfCα2=12ℏωCα2\mathrm{Ry}=\tfrac12m_ec^2\alpha^2=\tfrac12\frac{e^4m_e}{(4\pi\varepsilon_0)^2\hbar^2}=\tfrac12\frac{m_ec^2r_e}{a_0}=\tfrac12\frac{hc\alpha^2}{\lambda_e}=\tfrac12hf_C\alpha^2=\tfrac12\hbar\omega_C\alpha^2Ry=21​me​c2α2=21​(4πε0​)2ℏ2e4me​​=21​a0​me​c2re​​=21​λe​hcα2​=21​hfC​α2=21​ℏωC​α2.
  6. Bohr energy levels (infinite nuclear mass): En=−hcR∞/n2E_n=-hcR_\infty/n^2En​=−hcR∞​/n2.
  7. Rydberg formula (infinite nuclear mass): 1λ=Ry⋅1hc(1n12−1n22)=mee48ε02h3c(1n12−1n22)\frac1\lambda=\mathrm{Ry}\cdot\frac1{hc}\left(\frac1{n_1^2}-\frac1{n_2^2}\right)=\frac{m_ee^4}{8\varepsilon_0^2h^3c}\left(\frac1{n_1^2}-\frac1{n_2^2}\right)λ1​=Ry⋅hc1​(n12​1​−n22​1​)=8ε02​h3cme​e4​(n12​1​−n22​1​).
  8. Bohr energy levels with reduced mass: En=−hcRM/n2E_n=-hcR_M/n^2En​=−hcRM​/n2.

Significance

These identities are the standard bridge between the empirical Rydberg formula and the constants me,e,ε0,h,cm_e,e,\varepsilon_0,h,cme​,e,ε0​,h,c: they explain why a single constant governs all hydrogen series, why isotopes such as deuterium show shifted lines (the shift led to the discovery of deuterium), and how R∞R_\inftyR∞​ relates to α\alphaα, a0a_0a0​ and the Compton scales. The results are classical and not open; the mission's contribution is a machine-checked, reusable layer of definitions (Bohr orbits, reduced mass, the named atomic length and energy scales) on which later atomic-physics formalizations can build.

Difficulty

The content is elementary algebra with positivity side conditions. The main point to handle carefully is that the Bohr-orbit conditions determine vvv and rrr only implicitly; the energy must be computed from the two defining equations rather than from explicit formulas, and every division must be justified by positivity of the constants.

Formalization scope

All constants are real numbers bundled in a structure with strict positivity fields; no SI numerical values (CODATA figures, 1.09678×107 m−11.09678\times10^7\,\mathrm m^{-1}1.09678×107m−1, etc.) are formalized, and the precision-measurement and QED discussion of the source is out of scope. The Bohr model is formalized for a single particle of mass mmm orbiting a fixed charge +e+e+e (hydrogen-like, Z=1Z=1Z=1); the reduced-mass correction is modelled, as in the source, by substituting μ\muμ for mem_eme​. The photon wavenumber is taken to be the orbital energy difference divided by hchchc. The Bohr-orbit hypotheses are satisfiable for every n≥1n\ge1n≥1 and every m>0m>0m>0, so the Bohr-model statements are not vacuous. Contributions of alternative proofs and of generalizations (nuclear charge ZZZ, explicit orbit radii and speeds) are welcome.

Selected references

  • Wikipedia contributors, Rydberg constant, revision 1341645811. https://en.wikipedia.org/w/index.php?title=Rydberg_constant&oldid=1341645811
  • CODATA 2022 value of the Rydberg constant, NIST Reference on Constants, Units, and Uncertainty. https://physics.nist.gov/cgi-bin/cuu/Value?ryd
  • B. H. Bransden, C. J. Joachain, Quantum Mechanics, 2nd ed., Prentice Hall, 2000.
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Mathematical Physics·Captain: Lucas

Elementary Charge: the SI defining relations and charge quantizationTextbook

Motivation

Since the 2019 revision of the International System of Units (SI), the elementary charge eee is no longer a measured quantity: it is one of the seven defining constants of the SI and is fixed by definition at

e=1.602 176 634×10−19 C.e = 1.602\,176\,634 \times 10^{-19}\ \mathrm{C}.e=1.602176634×10−19 C.

Before that revision, eee had to be extracted from experiment, and the metrology literature accumulated several independent routes to it: Faraday's laws of electrolysis combined with the Avogadro constant, Millikan and Fletcher's oil-drop experiment (1909), shot-noise analysis, and — since the 1980s — the combination of the Josephson effect and the quantum Hall effect. Each route is a short algebraic recipe that turns other measured constants into eee. The 2019 redefinition did not delete those recipes; it inverted their role. With eee, the Planck constant hhh, the Avogadro constant NAN_\mathrm{A}NA​ and the speed of light ccc all fixed exactly, the recipes become exact arithmetic identities between defining constants, and the residual measurement uncertainty migrates to the constants that are no longer fixed (the vacuum magnetic permeability μ0\mu_0μ0​, equivalently the fine-structure constant α\alphaα).

This mission formalizes exactly those identities, as they are stated in the source article, together with the two quantization statements the same article records: Dirac's 1931 argument that a magnetic monopole forces charge quantization, and the closure property behind the observation that although quarks carry charges in multiples of e/3e/3e/3, isolatable particles carry integer multiples of eee.

Setting

All quantities are real numbers carrying SI units implicitly; the Lean development works in ℝ and fixes the numerical values as exact rationals, never as floating-point approximations.

The defining constants used here are e=1.602 176 634×10−19e = 1.602\,176\,634\times10^{-19}e=1.602176634×10−19 (coulomb), NA=6.022 140 76×1023N_\mathrm{A} = 6.022\,140\,76\times10^{23}NA​=6.02214076×1023 (per mole), h=6.626 070 15×10−34h = 6.626\,070\,15\times10^{-34}h=6.62607015×10−34 (joule second) and c=299 792 458c = 299\,792\,458c=299792458 (metre per second).

From these the article builds four derived constants, each of which is a definition in this mission rather than an axiom:

  • the Faraday constant F=NAeF = N_\mathrm{A} eF=NA​e, the charge of one mole of electrons;
  • the Josephson constant KJ=2e/hK_\mathrm{J} = 2e/hKJ​=2e/h, measurable through the Josephson effect;
  • the von Klitzing constant RK=h/e2R_\mathrm{K} = h/e^{2}RK​=h/e2, measurable through the quantum Hall effect;
  • the fine-structure constant in the form used by CODATA, α=μ0ce2/(2h)\alpha = \mu_0 c e^{2}/(2h)α=μ0​ce2/(2h), with μ0\mu_0μ0​ the vacuum magnetic permeability.

A fifth definition captures the natural unit of charge q0=4πε0ℏcq_0 = \sqrt{4\pi\varepsilon_0\hbar c}q0​=4πε0​ℏc​ of those natural unit systems in which e=q0αe = q_0\sqrt{\alpha}e=q0​α​, with ε0\varepsilon_0ε0​ the electric constant and ℏ\hbarℏ the reduced Planck constant.

Target

The goal theorem asserts that the three determination routes recorded in the source return one and the same number, the fixed SI value of eee, and that the electrolysis route's intermediate constant has its exact SI value:

F=NAe=96 485.332 123 310 018 4,FNA=e,F = N_\mathrm{A} e = 96\,485.332\,123\,310\,018\,4,\qquad \frac{F}{N_\mathrm{A}} = e,F=NA​e=96485.3321233100184,NA​F​=e, 2KJRK=e,2hαμ0c=ewheneverα=μ0ce22h.\frac{2}{K_\mathrm{J} R_\mathrm{K}} = e, \qquad \sqrt{\frac{2h\alpha}{\mu_0 c}} = e \quad\text{whenever}\quad \alpha = \frac{\mu_0 c e^{2}}{2h}.KJ​RK​2​=e,μ0​c2hα​​=ewheneverα=2hμ0​ce2​.

The milestones are the individual identities, each stated for arbitrary positive values of the constants rather than only at the SI values, plus the two quantization statements:

  1. F/NA=eF/N_\mathrm{A} = eF/NA​=e for any NA≠0N_\mathrm{A} \neq 0NA​=0;
  2. the exact value of FFF at the SI values of NAN_\mathrm{A}NA​ and eee;
  3. 2/(KJRK)=e2/(K_\mathrm{J}R_\mathrm{K}) = e2/(KJ​RK​)=e for e≠0e \neq 0e=0, h≠0h \neq 0h=0;
  4. the CODATA relation e=2hα/(μ0c)e = \sqrt{2h\alpha/(\mu_0 c)}e=2hα/(μ0​c)​;
  5. e=q0αe = q_0\sqrt{\alpha}e=q0​α​ for q0=4πε0ℏcq_0 = \sqrt{4\pi\varepsilon_0\hbar c}q0​=4πε0​ℏc​ and α=e2/(4πε0ℏc)\alpha = e^{2}/(4\pi\varepsilon_0\hbar c)α=e2/(4πε0​ℏc);
  6. Dirac quantization: if a monopole charge g≠0g \neq 0g=0 satisfies qg∈ℏ2Zqg \in \tfrac{\hbar}{2}\mathbb{Z}qg∈2ℏ​Z for every charge qqq in a collection, then every such qqq is an integer multiple of the fixed quantum ℏ/(2g)\hbar/(2g)ℏ/(2g);
  7. if every charge in a collection SSS is an integer multiple of a quantum q0q_0q0​, then so is every charge in the additive subgroup of R\mathbb{R}R generated by SSS.

Significance

The result itself. The content is the coherence of the SI's electrical sector: the same eee comes out of an electrochemical measurement chain, a quantum-electrical one and the CODATA relation, and the arithmetic that links them is exact. Milestones 6 and 7 record the two quantization statements in the source: the Dirac argument is a genuine implication (a monopole forces the charge spectrum into a discrete subgroup), while milestone 7 isolates the algebraic half of "stable groupings of quarks carry integer charge" — closure of a quantized spectrum under composition.

Formalizing it. What this mission produces is a small, faithful, reusable encoding of the 2019 SI defining constants and of the standard derived constants, with the exact rational values rather than floating-point ones, and with the degenerate cases made explicit. Nothing here is an open problem, and the mission should not be read as one: the value is a checked reference layer for physics-flavoured formalization, not a research advance.

Difficulty

Low, and stated as such deliberately. Milestones 1–3 are field arithmetic; 4 and 5 are field arithmetic plus Real.sqrt of a square, which needs the positivity hypotheses that are carried explicitly; 6 and 7 are elementary manipulations of ℤ-multiples and of AddSubgroup.closure. The only places a solver can go wrong are the degenerate ones: division by a constant that has not been assumed nonzero, and Real.sqrt of a quantity not known to be nonnegative — which is why every statement carries positivity or nonvanishing hypotheses rather than leaving Lean's junk values to decide the outcome.

Formalization scope

Conventions this mission commits to:

  • Units are implicit; every constant is a bare real number in the SI unit named in its docstring.
  • The fixed values are exact rationals (for example eSI = 1602176634 / 10 ^ 28), so the numeric milestone is an exact identity, provable by norm_num, not a floating-point comparison.
  • The derived constants are functions of their arguments, so that each identity can be stated for general positive values and then instantiated at the SI values. This rules out a trivializing reading in which a "relation" holds only because both sides are the same closed numeral.
  • Every division carries a nonvanishing hypothesis and every Real.sqrt a nonnegativity or positivity hypothesis, so no statement is discharged by a Lean junk value.
  • Dirac's condition is stated as membership of qgqgqg in ℏ2Z\tfrac{\hbar}{2}\mathbb{Z}2ℏ​Z for each charge in a given set, and its conclusion as membership of qqq in ℏ2gZ\tfrac{\hbar}{2g}\mathbb{Z}2gℏ​Z; the physical derivation of the condition is not part of the mission.
  • No physics is assumed as an axiom: everything is a definition plus arithmetic over ℝ, using only Mathlib.

Contributions welcome beyond the current list: the shot-noise and oil-drop routes, which the source describes qualitatively rather than by a formula, would need a probabilistic or mechanical model before they can be stated, and that model would be a worthwhile addition.

Selected references

  • "Elementary charge", Wikipedia, the revision supplied as the mission source: https://en.wikipedia.org/wiki/Elementary_charge
  • D. B. Newell and E. Tiesinga, The International System of Units (SI), NIST Special Publication 330 (2019). DOI: 10.6028/NIST.SP.330-2019
  • Bureau International des Poids et Mesures, The International System of Units (SI Brochure), 9th ed. https://www.bipm.org/documents/20126/41483022/SI-Brochure-9-EN.pdf
  • R. A. Millikan, "The isolation of an ion, a precision measurement of its charge, and the correction of Stokes's law", Science 32 (822), 436–448 (1910). DOI: 10.1126/science.32.822.436
  • J. Preskill, "Magnetic Monopoles", Annual Review of Nuclear and Particle Science 34, 461–530 (1984). DOI: 10.1146/annurev.ns.34.120184.002333
  • CODATA 2022 value of the elementary charge, NIST: https://physics.nist.gov/cgi-bin/cuu/Value?e
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Information TheoryMathematical Physics·Captain: Lucas

Boltzmann Constant: Kinetic Theory, Boltzmann Factors and EntropyTextbook

Motivation

The Boltzmann constant kBk_BkB​ is the proportionality factor relating the average thermal energy of the particles of a system to its thermodynamic temperature. It appears wherever a microscopic energy has to be compared with a macroscopic temperature: in the ideal gas law written per molecule, in the equipartition theorem, in the Boltzmann factor e−E/kBTe^{-E/k_BT}e−E/kB​T that governs equilibrium occupation probabilities, in Boltzmann's entropy formula S=klog⁡WS = k\log WS=klogW, in the thermal voltage of a ppp–nnn junction, and in the Johnson noise of a resistor.

The constant also has an unusual documentary history. Boltzmann linked entropy and probability in 1877 but never introduced a constant; Max Planck first wrote kkk, and gave the first numerical value (1.346×10−231.346\times10^{-23}1.346×10−23 J/K, about 2.5% below the modern figure), in his 1900–1901 derivation of the black-body law — the terse S=klog⁡WS = k\log WS=klogW on Boltzmann's tombstone is Planck's formulation. For most of the twentieth century kBk_BkB​ was a measured quantity; the 2017 acoustic gas thermometry campaign reached a relative uncertainty of 0.2 ppm, and as part of the 2019 revision of the SI the constant was defined to the exact value 1.380649×10−231.380649\times10^{-23}1.380649×10−23 J·K⁻¹, which is now what fixes the kelvin.

This mission formalizes the elementary quantitative content of that picture: the identities that make kBk_BkB​ a conversion factor, and the exact arithmetic that the 2019 SI definitions make possible.

Setting

Work throughout with real numbers; units are carried in the prose, not in the types. Fix the exact post-2019 SI values

kB=1.380649×10−23 J K−1,NA=6.02214076×1023 mol−1,q=1.602176634×10−19 C,k_B = 1.380649\times10^{-23}\ \mathrm{J\,K^{-1}}, \qquad N_A = 6.02214076\times10^{23}\ \mathrm{mol^{-1}}, \qquad q = 1.602176634\times10^{-19}\ \mathrm{C},kB​=1.380649×10−23 JK−1,NA​=6.02214076×1023 mol−1,q=1.602176634×10−19 C,

and define the molar gas constant as the product R=kBNAR = k_B N_AR=kB​NA​.

A gas sample is described by its pressure ppp, volume VVV, absolute temperature TTT, amount of substance nnn, molecule count N=nNAN = nN_AN=nNA​, particle mass mmm, and mean square particle speed ⟨v2⟩\langle v^2\rangle⟨v2⟩. A system with a finite set sss of microstates is described by an energy function E:s→RE : s \to \mathbb{R}E:s→R; its partition function is Z=∑i∈se−Ei/(kBT)Z = \sum_{i\in s} e^{-E_i/(k_BT)}Z=∑i∈s​e−Ei​/(kB​T) and its Boltzmann probabilities are Pi=e−Ei/(kBT)/ZP_i = e^{-E_i/(k_BT)}/ZPi​=e−Ei​/(kB​T)/Z. For a distribution ppp on sss, the Gibbs entropy is S=−kB∑ipilog⁡piS = -k_B\sum_i p_i\log p_iS=−kB​∑i​pi​logpi​, the Shannon entropy (in nats) is −∑ipilog⁡pi-\sum_i p_i\log p_i−∑i​pi​logpi​, and for WWW equiprobable microstates Boltzmann's entropy is kBlog⁡Wk_B \log WkB​logW. The thermal voltage is VT(T)=kBT/qV_T(T) = k_BT/qVT​(T)=kB​T/q. All logarithms are natural.

Target

The goal theorem is the statement that fixes the physical meaning of kBk_BkB​: kinetic theory plus the per-molecule gas law determine the mean translational kinetic energy. From

pV=13Nm⟨v2⟩andpV=NkBTpV = \tfrac{1}{3}Nm\langle v^2\rangle \qquad\text{and}\qquad pV = Nk_BTpV=31​Nm⟨v2⟩andpV=NkB​T

conclude

12m⟨v2⟩=32kBT,vrms=3kBT/m.\tfrac{1}{2}m\langle v^2\rangle = \tfrac{3}{2}k_BT, \qquad v_{\mathrm{rms}} = \sqrt{3k_BT/m}.21​m⟨v2⟩=23​kB​T,vrms​=3kB​T/m​.

The milestones are the surrounding identities, in the order of the source: the equivalence pV=nRT  ⟺  pV=NkBTpV = nRT \iff pV = Nk_BTpV=nRT⟺pV=NkB​T; equipartition, 12m⟨vx2⟩=12kBT\tfrac{1}{2}m\langle v_x^2\rangle = \tfrac{1}{2}k_BT21​m⟨vx2​⟩=21​kB​T per degree of freedom; the ratio law vrms(m1)/vrms(m2)=m2/m1v_{\mathrm{rms}}(m_1)/v_{\mathrm{rms}}(m_2) = \sqrt{m_2/m_1}vrms​(m1​)/vrms​(m2​)=m2​/m1​​; normalisation of the Boltzmann factors, ∑iPi=1\sum_i P_i = 1∑i​Pi​=1; the reduction of the Gibbs entropy on the uniform distribution to S=kBlog⁡WS = k_B\log WS=kB​logW; the identification S/kB=S/k_B = S/kB​= Shannon entropy; the energy kBTk_BTkB​T of one nat of rescaled entropy; and three numerical facts — VT(300 K)≈25.85V_T(300\ \mathrm{K}) \approx 25.85VT​(300 K)≈25.85 mV, kB≈8.617333262×10−5k_B \approx 8.617333262\times10^{-5}kB​≈8.617333262×10−5 eV/K, and the exact value R=8.31446261815324R = 8.31446261815324R=8.31446261815324 J·K⁻¹·mol⁻¹.

Significance

The results. Individually these are the standard first facts of kinetic theory and statistical mechanics; together they pin down what the constant does. The equipartition chain converts a temperature into a velocity distribution scale and explains the measured room-temperature rms speeds from helium (about 1370 m/s) to xenon (about 240 m/s). The entropy statements make precise the claim that thermodynamic entropy is Shannon entropy in energy units, with kBk_BkB​ as the exchange rate — the statement behind the natural-unit convention kB=1k_B = 1kB​=1. The numerical milestones exercise the consequence of the 2019 SI revision that unit conversions involving kBk_BkB​ are now exact rational arithmetic rather than propagated measurement uncertainty.

Formalizing them. All of these are settled physics; nothing here is open. What the mission produces is a small, reusable Lean development of the SI defining constants and of the elementary statistical-mechanical vocabulary (Boltzmann weights, partition function, Gibbs/Shannon/Boltzmann entropies), with each textbook identity stated against that shared model rather than re-derived ad hoc. It is a suitable entry-level mission and a foundation other physics missions can import.

Difficulty

The mathematics is elementary; the difficulty is entirely one of faithful modelling, and solvers should expect the friction to be there rather than in the proofs. Three specific points. First, Lean's division and logarithm are total: e−E/(kBT)e^{-E/(k_BT)}e−E/(kB​T) is defined at T=0T = 0T=0 and evaluates to 111, and log⁡x=0\log x = 0logx=0 for x≤0x \le 0x≤0, so statements must carry the positivity hypotheses that keep them physically meaningful rather than relying on the definitions to exclude bad inputs. Second, the entropy definitions are stated for an arbitrary real-valued weight function, not for a distribution; normalisation is a hypothesis where it is needed, never an assumption baked into the type. Third, the numerical milestones are claims about specific decimal numerals, and the tolerance in each is part of the statement: two of them are genuine approximations and one, the value of RRR, is an exact identity, which is only true because both factors are exact SI numerals.

Formalization scope

Quantities are real numbers (ℝ); no dimensional-analysis layer is used, and unit correctness is a convention of the prose. Finite state spaces are Finsets over an arbitrary index type, with nonemptiness stated as a hypothesis where the partition function must be nonzero. Entropies use the natural logarithm, so they are measured in nats, and the Shannon entropy is the Gibbs entropy divided by kBk_BkB​ by construction. Temperatures, masses, volumes and particle counts are positive reals where the physics requires it. The mean square speed is a free real variable constrained only by the stated equations; it is not built from a velocity distribution, and extending the development to an actual Maxwell–Boltzmann distribution is out of scope here and a natural follow-up mission.

The statements are deliberately non-vacuous: every hypothesis set in the mission is satisfiable (positive temperature, positive mass, nonempty state space), and the numerical items admit no trivializing reading since they are closed claims about fixed numerals. Only Mathlib is required — Real.exp, Real.log, Real.sqrt, and Finset.sum. The definition file is intended to be reusable: any later mission about thermodynamics, black-body radiation, or the Shockley diode equation can import the SI constants and entropy vocabulary unchanged.

Selected references

  • Wikipedia, Boltzmann constant — the source text this mission formalizes: https://en.wikipedia.org/wiki/Boltzmann_constant
  • D. B. Newell and E. Tiesinga (eds.), The International System of Units (SI), NIST Special Publication 330 (2019). DOI: https://doi.org/10.6028/NIST.SP.330-2019 — the exact defining values of kBk_BkB​, NAN_ANA​ and qqq.
  • M. Planck, "Ueber das Gesetz der Energieverteilung im Normalspectrum", Annalen der Physik 309(3):553–563 (1901). DOI: https://doi.org/10.1002/andp.19013090310 — the first introduction of kkk and of S=klog⁡WS = k\log WS=klogW.
  • R. P. Feynman, R. B. Leighton and M. Sands, The Feynman Lectures on Physics, Vol. I, ch. 39 (kinetic theory of gases): https://www.feynmanlectures.caltech.edu/I_39.html
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Mathematical Logic·Captain: Lucas

Jech Set Theory I: Silver's Theorem on Singular CardinalsTextbook

Motivation

How large can the power set of an infinite set be? For a regular cardinal κ\kappaκ (one that is not the supremum of fewer than κ\kappaκ smaller ordinals) the answer is: almost anything. Easton's theorem (1970) shows that the function κ↦2κ\kappa \mapsto 2^{\kappa}κ↦2κ on regular cardinals can be prescribed arbitrarily in any model of ZFC, subject only to monotonicity and König's inequality cf⁡(2κ)>κ\operatorname{cf}(2^{\kappa}) > \kappacf(2κ)>κ. For a long time it was expected that singular cardinals — those that are such a supremum, like ℵω\aleph_{\omega}ℵω​ — would behave the same way.

They do not. In 1974 Jack Silver proved that the Generalized Continuum Hypothesis cannot fail for the first time at a singular cardinal of uncountable cofinality: if 2α=α+2^{\alpha} = \alpha^{+}2α=α+ for every infinite α<κ\alpha < \kappaα<κ and cf⁡κ>ω\operatorname{cf}\kappa > \omegacfκ>ω, then 2κ=κ+2^{\kappa} = \kappa^{+}2κ=κ+. This was the first ZFC theorem constraining the continuum function at singular cardinals, and it opened the area now called the singular cardinal problem.

A short timeline:

  • 1970 — Easton: the continuum function on regular cardinals is essentially arbitrary.
  • 1974 — Silver (ICM Vancouver): GCH cannot first fail at a singular cardinal of uncountable cofinality; more generally the Singular Cardinal Hypothesis is decided at cofinality ω\omegaω.
  • 1975 — Galvin and Hajnal: elementary inequalities for cardinal powers at singular cardinals of uncountable cofinality.
  • 1976–77 — Baumgartner and Prikry, and independently Jensen, give elementary (non-forcing, non-ultrapower) proofs of Silver's theorem; the proof reproduced in Jech's Chapter 8 is of this kind.
  • 1977 — Magidor: it is consistent, relative to large cardinals, that GCH holds below ℵω\aleph_{\omega}ℵω​ while 2ℵω>ℵω+12^{\aleph_{\omega}} > \aleph_{\omega+1}2ℵω​>ℵω+1​ — so Silver's restriction to uncountable cofinality is necessary.
  • 1980s onwards — Shelah's pcf theory, whose flagship result ℵωℵ0<ℵω4\aleph_{\omega}^{\aleph_0} < \aleph_{\omega_4}ℵωℵ0​​<ℵω4​​ (when ℵω\aleph_\omegaℵω​ is a strong limit) grows out of exactly the stationary-set machinery assembled here.

This mission is the first in a series formalizing Thomas Jech, Set Theory (Third Millennium Edition, Springer 2003). It covers Chapter 8, "Stationary Sets" (pp. 91–98).

Setting

Fix a regular uncountable cardinal κ\kappaκ and regard it as the well-ordered set of ordinals below it. A set C⊆κC \subseteq \kappaC⊆κ is closed unbounded, or a club, if it is unbounded in κ\kappaκ and contains all of its limit points below κ\kappaκ (an ordinal α>0\alpha > 0α>0 is a limit point of CCC when sup⁡(C∩α)=α\sup(C \cap \alpha) = \alphasup(C∩α)=α). A set S⊆κS \subseteq \kappaS⊆κ is stationary if S∩C≠∅S \cap C \neq \emptysetS∩C=∅ for every club CCC. Clubs are closed under intersections of fewer than κ\kappaκ of them, so they generate a κ\kappaκ-complete filter, the club filter; its dual is the nonstationary ideal.

The club filter has a second closure property with no analogue for ordinary filters. The diagonal intersection of a κ\kappaκ-indexed family is

△α<κXα  =  {ξ<κ  :  ξ∈⋂α<ξXα},\mathop{\triangle}_{\alpha<\kappa} X_\alpha \;=\; \Bigl\{ \xi < \kappa \;:\; \xi \in \bigcap_{\alpha<\xi} X_\alpha \Bigr\},△α<κ​Xα​={ξ<κ:ξ∈α<ξ⋂​Xα​},

and a filter closed under diagonal intersections is called normal. A function fff defined on S⊆κS \subseteq \kappaS⊆κ is regressive if f(α)<αf(\alpha) < \alphaf(α)<α for all nonzero α∈S\alpha \in Sα∈S.

For cardinal arithmetic, cf⁡κ\operatorname{cf}\kappacfκ denotes the cofinality of κ\kappaκ (the least length of an unbounded sequence in κ\kappaκ), κ+\kappa^{+}κ+ the cardinal successor, and κ\kappaκ is singular when cf⁡κ<κ\operatorname{cf}\kappa < \kappacfκ<κ. The Singular Cardinal Hypothesis (SCH) is the assertion that κcf⁡κ=κ+\kappa^{\operatorname{cf}\kappa} = \kappa^{+}κcfκ=κ+ for every singular κ\kappaκ with 2cf⁡κ<κ2^{\operatorname{cf}\kappa} < \kappa2cfκ<κ. A sequence of cardinals is normal if it is strictly increasing and continuous at limits.

Formalization targets

Goal — Silver's theorem (Jech 8.12)

κ singular, cf⁡κ>ω, (∀α ℵ0≤α<κ⇒2α=α+)  ⟹  2κ=κ+.\kappa \text{ singular},\ \operatorname{cf}\kappa > \omega,\ \bigl(\forall \alpha \ \aleph_0 \le \alpha < \kappa \Rightarrow 2^{\alpha} = \alpha^{+}\bigr) \;\Longrightarrow\; 2^{\kappa} = \kappa^{+}.κ singular, cfκ>ω, (∀α ℵ0​≤α<κ⇒2α=α+)⟹2κ=κ+.

This is the weakest statement of the chapter that still needs the full machinery: it fixes no particular κ\kappaκ and no particular cofinality, and it stays correct no matter how the singular cardinal problem develops above it.

Milestones, in dependency order

  1. Lemma 8.4 — the diagonal intersection of κ\kappaκ clubs is a club; equivalently the club filter is normal.
  2. Theorem 8.7 (Fodor) — a regressive function on a stationary set is constant on a stationary subset.
  3. Theorem 8.10 (Solovay) — every stationary subset of κ\kappaκ is the union of κ\kappaκ pairwise disjoint stationary sets.
  4. Lemma 8.14 — if ⟨κα⟩\langle \kappa_\alpha\rangle⟨κα​⟩ is normal with limit κ\kappaκ, λcf⁡κ<κ\lambda^{\operatorname{cf}\kappa} < \kappaλcfκ<κ for λ<κ\lambda < \kappaλ<κ, and {α:καcf⁡κα=κα+}\{\alpha : \kappa_\alpha^{\operatorname{cf}\kappa_\alpha} = \kappa_\alpha^{+}\}{α:καcfκα​​=κα+​} is stationary in cf⁡κ\operatorname{cf}\kappacfκ, then κcf⁡κ=κ+\kappa^{\operatorname{cf}\kappa} = \kappa^{+}κcfκ=κ+.
  5. Theorem 8.13 (Silver) — SCH at every cardinal of cofinality ω\omegaω implies SCH everywhere.

Significance

Silver's theorem is the boundary between the two halves of cardinal arithmetic. Above it sit the ZFC theorems of pcf theory; below it sit the consistency results (Magidor, Prikry, Radin forcing) that show how much freedom is left, and they are confined to cofinality ω\omegaω precisely because Theorems 8.12 and 8.13 close off everything else. Its proof also packages tools used throughout set theory: the normality of the club filter, Fodor's pressing-down lemma, and the technique of bounding almost disjoint families of functions by a stationary-set argument.

Formalization status: Mathlib already has clubs and stationary sets in an arbitrary well-ordered type (IsClub, IsStationary), with the finite and <κ<\kappa<κ-indexed intersection lemmas — Jech's Lemma 8.2 and Theorem 8.3. It does not have diagonal intersections, Fodor's theorem, Solovay's splitting theorem, or any singular cardinal arithmetic beyond the definitions of regular and singular cardinals. Each milestone below is therefore a genuine addition, and the first three are reusable well outside this mission.

Difficulty

The naive route to the goal — induct on α<κ\alpha < \kappaα<κ and pass to the limit — fails immediately: 2κ2^{\kappa}2κ for singular κ\kappaκ is not determined by the values 2α2^{\alpha}2α for α<κ\alpha < \kappaα<κ in any elementary way; that is exactly the content of the independence results. What the proof must do instead is bound the number of functions on cf⁡κ\operatorname{cf}\kappacfκ, and it gets that bound from a stationary set rather than from a club: uncountable cofinality is what makes the set of relevant stages stationary, and stationarity is what survives the diagonal argument. Cofinality ω\omegaω breaks this at the first step, since every subset of ω\omegaω that is unbounded is already a club and Fodor's theorem is empty.

The two hard pieces are Lemma 8.14 and, inside it, Lemma 8.16: given an almost disjoint family FFF of functions with f(α)∈Aαf(\alpha) \in A_\alphaf(α)∈Aα​ and ∣Aα∣≤ℵα|A_\alpha| \le \aleph_\alpha∣Aα​∣≤ℵα​ on a stationary set of α\alphaα, one must show ∣F∣≤ℵω1|F| \le \aleph_{\omega_1}∣F∣≤ℵω1​​ by assigning to each fff a pair (stationary set, bounded restriction) and checking the assignment is injective. That argument uses Fodor's theorem on a set of functions, and the bookkeeping does not simplify.

Formalization scope

The ambient order is Mathlib's type of ordinals below a cardinal, k.ord.ToType (written Below k in the mission's definition bundle); clubs and stationary sets are Mathlib's IsClub and IsStationary on that type, so a set is closed in the sense of being closed under suprema of directed subsets — equivalent, for a well-order with the order topology, to Jech's "contains its limit points". Families indexed by "α<κ\alpha < \kappaα<κ" are functions out of that same type, which is what makes the diagonal intersection typecheck without a side condition. Cardinal exponentiation, cofinality (Ordinal.cof of k.ord) and the successor cardinal (Order.succ) are Mathlib's.

One trivializing formalization is ruled out explicitly: the GCH hypothesis of the goal is stated for infinite cardinals α<κ\alpha < \kappaα<κ only. Quantified over all cardinals it would be unsatisfiable — 22=4≠3=2+2^{2} = 4 \neq 3 = 2^{+}22=4=3=2+ — and Silver's theorem would become vacuous.

A complete development needs: diagonal intersections and the normality of the club filter; Fodor's theorem; the sets Eλκ={α<κ:cf⁡α=λ}E^{\kappa}_{\lambda} = \{\alpha < \kappa : \operatorname{cf}\alpha = \lambda\}Eλκ​={α<κ:cfα=λ} and their stationarity; Solovay's splitting theorem via Lemmas 8.8 and 8.9; almost disjoint families of ordinal functions and the counting Lemmas 8.15 and 8.16; and Theorem 5.22(ii) on cardinal powers, which Jech's proof of Theorem 8.13 cites. Contributions of any of these as separate reductions are welcome, as are alternative proofs of the goal (for instance via a generic elementary embedding) that bypass some of the chain.

Selected references

  • Thomas Jech, Set Theory, The Third Millennium Edition, revised and expanded. Springer Monographs in Mathematics, Springer, 2003 (ISBN 3-540-44085-2). Chapter 8, "Stationary Sets", pp. 91–98 — the source of every statement in this mission.
  • Jack Silver, On the singular cardinals problem. Proceedings of the International Congress of Mathematicians (Vancouver, 1974), vol. 1, pp. 265–268.
  • William B. Easton, Powers of regular cardinals. Annals of Mathematical Logic 1 (1970), pp. 139–178.
  • Fred Galvin and András Hajnal, Inequalities for cardinal powers. Annals of Mathematics 101 (1975), pp. 491–498.
  • James E. Baumgartner and Karel Prikry, Singular cardinals and the generalized continuum hypothesis. American Mathematical Monthly 84 (1977), pp. 108–113.
  • Menachem Magidor, On the singular cardinals problem I. Israel Journal of Mathematics 28 (1977), pp. 1–31.
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CombinatoricsMachine LearningProbability+1·Captain: naimengye

An Introduction to Computational Learning Theory V: Classification Noise and Statistical QueriesTextbook

Motivation

Chapter 5 of Kearns and Vazirani, An Introduction to Computational Learning Theory (MIT Press, 1994, doi:10.7551/mitpress/3897.001.0001), asks what happens to PAC learning when the labels are unreliable. In the classification noise model of Angluin and Laird, each label returned by the oracle is flipped independently with a fixed probability η<1/2\eta < 1/2η<1/2. The algorithms of Chapter 1 collapse at once: the elimination algorithm deletes a correct literal on the strength of a single mislabeled example, and the tightest-fit rectangle may not exist. The chapter's remedy is to learn from statistics: an algorithm that forms its hypothesis only from estimates of probabilities of simple events is insensitive to occasional wrong labels. Kearns's statistical query model makes this precise, replacing the example oracle by an oracle that returns the probability of any predicate of a labeled example to within a tolerance, and the main theorem (5.3) shows that every class learnable from statistical queries is PAC learnable in the presence of classification noise. The proof rests on a single identity, Equation (5.2), that expresses the true value of a statistical query in terms of three quantities that can each be estimated from noisy examples, and on the observation that a hypothesis's disagreement with the noisy label is an affine function of its true error, which lets the best of several candidate hypotheses be recognized without clean data.

Setting

The framework is that of Mission I. The noisy example law is that of (x,b)(x, b)(x,b) with x∼Dx \sim Dx∼D and b=c(x)b = c(x)b=c(x) flipped with probability η\etaη. A statistical query is a predicate χ\chiχ of a labeled example with value Pχ=Pr⁡x∼D[χ(x,c(x))=1]P_\chi = \Pr_{x \sim D}[\chi(x, c(x)) = 1]Pχ​=Prx∼D​[χ(x,c(x))=1]. The inputs split into X1X_1X1​, where the label matters to χ\chiχ, and X2X_2X2​, where it does not; p1=D(X1)p_1 = D(X_1)p1​=D(X1​) and D1D_1D1​ is DDD conditioned on X1X_1X1​. For conjunctions over {0,1}n\{0,1\}^n{0,1}n, p0(z)p_0(z)p0​(z) is the probability that a literal zzz is set to 000 and p01(z)p_{01}(z)p01​(z) the probability that it is 000 on a positive example; zzz is significant if p0(z)≥ϵ/8np_0(z) \ge \epsilon/8np0​(z)≥ϵ/8n and harmful if p01(z)≥ϵ/8np_{01}(z) \ge \epsilon/8np01​(z)≥ϵ/8n.

Formalization targets

Goal: Equation (5.2)

For 0≤η<1/20 \le \eta < 1/20≤η<1/2 and every statistical query χ\chiχ,

Pχ=p1⋅Pr⁡EXCNη(c,D1)[χ=1]−η1−2η+Pr⁡EXCNη(c,D)[χ=1∧x∈X2],P_\chi = p_1 \cdot \frac{\Pr_{EX^\eta_{CN}(c, D_1)}[\chi = 1] - \eta}{1 - 2\eta} + \Pr_{EX^\eta_{CN}(c, D)}[\chi = 1 \wedge x \in X_2],Pχ​=p1​⋅1−2ηPrEXCNη​(c,D1​)​[χ=1]−η​+EXCNη​(c,D)Pr​[χ=1∧x∈X2​],

the probabilities on the right being taken under the noisy oracle.

Milestones

The §5.2 analysis behind Theorem 5.2 (the conjunction of all significant, non-harmful literals has error at most ϵ/2\epsilon/2ϵ/2); the product estimate bound of p. 115 (AB−2τ′≤A^B^≤AB+3τ′AB - 2\tau' \le \hat A\hat B \le AB + 3\tau'AB−2τ′≤A^B^≤AB+3τ′); the identity of p. 117 (γh=η+(1−2η) error(h)\gamma_h = \eta + (1 - 2\eta)\,\mathrm{error}(h)γh​=η+(1−2η)error(h)).

Significance

Equation (5.2) is the entire mechanism of noise-tolerant learning in the statistical query model: the noisy oracle cannot be de-noised example by example, but the probability of any predicate can be recovered exactly from noisy probabilities, because on the inputs where the label matters the noise acts as a known affine contraction and on the others it acts not at all. Together with the p. 117 identity, which turns hypothesis selection into a comparison of noisy disagreement rates, and the Chernoff bounds of Mission IV, it yields Theorem 5.3 and hence noise-tolerant algorithms for every class the book has learned so far (conjunctions, decision lists, kkk-CNF). The §5.2 analysis is the first statistical-query algorithm and shows the pattern: a hypothesis defined by thresholds on a few probabilities, with enough slack between the thresholds that estimates suffice. None of this is machine-checked. The formalization fixes the noisy example law on the platform's sample framework and proves the exact identities on which the noise-tolerant simulation depends.

Difficulty

Equation (5.2) is a computation with the pushforward of a product measure: one must express the noisy law on X1X_1X1​ as a mixture of the clean law and its label-flipped image, solve the affine relation for the clean probability, and combine with the restriction to X2X_2X2​, where the flipped and unflipped labels give the same value of χ\chiχ; the degenerate case D(X1)=0D(X_1) = 0D(X1​)=0, in which the conditional measure is zero and the first term vanishes, must be handled separately. The p. 117 identity is the same computation without the split. The §5.2 analysis is two union bounds over the 2n2n2n literals after the observation that a literal of the target is never harmful and that a literal of the hypothesis is never insignificant. The product lemma is elementary arithmetic with a case split at A<τ′A < \tau'A<τ′.

Formalization scope

The noisy oracle is a measure on labeled examples obtained by mapping the product of DDD and a Bernoulli(η\etaη) coin; the conditional D1D_1D1​ is Mathlib's conditional measure; queries are arbitrary measurable predicates of a labeled example, with no tolerance or query-count bookkeeping. Theorem 5.3 itself, the definitions of efficient learnability from statistical queries (Definition 14) and of efficient noisy PAC learnability (Definition 13), Theorem 5.1, Theorem 5.2 as a statement about an algorithm with oracle access, and Corollary 5.4 are not stated: they quantify over query algorithms and their running times, for which this series has no model; the mission carries their exact probabilistic content. The error-propagation analysis of §5.4.2–5.4.3 with tolerance τ/27\tau/27τ/27 and the guessing resolution Δ\DeltaΔ is not stated beyond the product lemma, since the factor 1/(1−2η)1/(1-2\eta)1/(1−2η) is not in [0,1][0,1][0,1] and the book's constant does not account for it. Hypotheses: 0≤η<1/20 \le \eta < 1/20≤η<1/2 for the decomposition, 0≤η≤10 \le \eta \le 10≤η≤1 for the disagreement identity, ϵ>0\epsilon > 0ϵ>0 for the conjunction analysis, all reals in [0,1][0,1][0,1] for the product lemma.

Trivializing readings are excluded: the decomposition is an exact identity for every measurable query, and the conjunction bound is for the exact thresholds ϵ/8n\epsilon/8nϵ/8n with the union bound's ϵ/2\epsilon/2ϵ/2. Welcome contributions: the mixture representation of the noisy law, the restriction of a pushforward to X2X_2X2​, and the two union bounds.

Selected references

  • M. J. Kearns, U. V. Vazirani, An Introduction to Computational Learning Theory, MIT Press, 1994, Chapter 5. doi:10.7551/mitpress/3897.001.0001
  • D. Angluin, P. Laird, Learning from noisy examples, Machine Learning 2(4), 1988. doi:10.1007/BF00116829
  • M. Kearns, Efficient noise-tolerant learning from statistical queries, Journal of the ACM 45(6), 1998. doi:10.1145/293347.293351
  • M. Kearns, M. Li, Learning in the presence of malicious errors, SIAM Journal on Computing 22(4), 1993. doi:10.1137/0222052
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An Introduction to Computational Learning Theory IV: Weak and Strong Learning, Boosting and Chernoff BoundsTextbook

Motivation

Chapter 4 of Kearns and Vazirani, An Introduction to Computational Learning Theory (MIT Press, 1994, doi:10.7551/mitpress/3897.001.0001), asks whether the PAC model's demand for arbitrarily small error and confidence is essential. A weak learning algorithm need only, with some fixed positive probability, output a hypothesis that beats random guessing by a fixed margin. Schapire's theorem, the chapter's main result, says that this apparently much weaker requirement is equivalent to the original one: any weak learner can be converted, by running it on carefully filtered distributions and combining its hypotheses by majority votes, into a strong learner. The construction is boosting, which became one of the most influential ideas in machine learning. The chapter proves the equivalence in two steps. Boosting the confidence is elementary: run the learner several times and validate. Boosting the accuracy is the substance: a modest procedure that combines three hypotheses, each with error at most β\betaβ on its own distribution, into a majority with error at most g(β)=3β2−2β3<βg(\beta) = 3\beta^2 - 2\beta^3 < \betag(β)=3β2−2β3<β, applied recursively until the error is driven below the target. The Chernoff bounds of the Appendix, the book's workhorse for estimating probabilities from samples, are what makes the validation steps rigorous.

Setting

The framework is that of Mission I. A class CCC is weakly learnable using HHH if for some advantage γ>0\gamma > 0γ>0, confidence δ0>0\delta_0 > 0δ0​>0 and sample size mmm, an algorithm outputs hypotheses in HHH that, for every target in CCC and every distribution, have error at most 1/2−γ1/2 - \gamma1/2−γ with probability at least δ0\delta_0δ0​; the algorithm's prediction L(S)(x)L(S)(x)L(S)(x) is a measurable function of the sample and the instance together, as it is for every algorithm. Given a hypothesis h1h_1h1​, the filtered distribution D2D_2D2​ gives weight 1/21/21/2 to the instances on which h1h_1h1​ errs and 1/21/21/2 to those on which it is correct, preserving relative weights within each part, and D3D_3D3​ is DDD conditioned on h1≠h2h_1 \ne h_2h1​=h2​; the modest procedure outputs majority(h1,h2,h3)\mathrm{majority}(h_1, h_2, h_3)majority(h1​,h2​,h3​). Ternary majority trees over HHH are the closure of HHH under the majority of three. For confidence boosting, kkk independent samples yield kkk hypotheses, and a fresh sample selects the one with the fewest mistakes. Bernoulli trials are mmm independent coin flips with success probability ppp.

Formalization targets

Goal: Theorem 4.9

If CCC is weakly PAC learnable using measurable hypotheses in HHH, then CCC is PAC learnable using the class of ternary majority trees with leaves from HHH: for all ϵ,δ∈(0,1/2)\epsilon, \delta \in (0, 1/2)ϵ,δ∈(0,1/2) some sample size and some algorithm outputting majority trees achieve error at most ϵ\epsilonϵ with probability at least 1−δ1 - \delta1−δ, for every target in CCC and every distribution.

Milestones

Theorem 9.2 (the additive and multiplicative Chernoff bounds); the two facts of §4.2 behind confidence boosting (independent runs all fail with probability at most (1−δ0)k(1 - \delta_0)^k(1−δ0​)k; the fewest-mistakes selection loses at most γ\gammaγ with probability at least 1−2ke−mγ2/21 - 2k e^{-m\gamma^2/2}1−2ke−mγ2/2); Lemma 4.1 (the modest procedure: error at most g(β)g(\beta)g(β)).

Significance

Theorem 4.9 is one of the landmark results of learning theory: it shows that the PAC model has no intermediate strength, that Occam learning, weak learning and strong learning coincide, and that the resources of a strong learner can be bounded polylogarithmically in 1/ϵ1/\epsilon1/ϵ in memory and hypothesis size. Its constructive proof is the first boosting algorithm, ancestor of AdaBoost and of gradient boosting. Lemma 4.1 is the analytic core, a clean inequality about three hypotheses and three distributions in which the filtered distribution is exactly calibrated so that h1h_1h1​ has no advantage on it. The Chernoff bounds are the concentration inequalities invoked throughout the book, and their formalization on the product law of Bernoulli trials makes every later "estimate to within γ\gammaγ with confidence 1−δ1 - \delta1−δ" step reusable. None of these is machine-checked in this form; the boosting theorem in the sample-complexity sense is, to our knowledge, not formalized anywhere.

Difficulty

Lemma 4.1 is a computation with conditional measures: writing errorD\mathrm{error}_DerrorD​ of the majority as the weight of the instances on which h1h_1h1​ and h2h_2h2​ both err plus β3\beta_3β3​ times the weight of their disagreement, mapping weights under D2D_2D2​ back to DDD by the factors 2(1−β1)2(1 - \beta_1)2(1−β1​) and 2β12\beta_12β1​ (Equation (4.1)), and maximizing the resulting polynomial in β1,β2,β3,γ1,γ2\beta_1, \beta_2, \beta_3, \gamma_1, \gamma_2β1​,β2​,β3​,γ1​,γ2​; the degenerate cases where a conditioning event is null must be handled separately. The Chernoff bounds require the exponential moment method on a finite product measure. The confidence-boosting facts are the product bound for independent blocks and Hoeffding plus a union bound. The goal is a genuine construction: from a large sample of DDD one must simulate the recursive algorithm Strong-Learn, whose calls to the weak learner on filtered distributions are served by rejection sampling from the remaining examples, bound the depth of the recursion by the growth of g−1g^{-1}g−1 iterates (Lemma 4.2), bound the number of examples consumed at each node (Lemmas 4.3–4.7) and allocate the confidence over all the places the simulation can fail; then package the result as a deterministic function of a sample of fixed size. An alternative route is available: weak learnability with a fixed sample size forces a finite VC dimension (a class shattering a large set defeats any fixed-size learner on the uniform distribution over it), after which Theorem 3.3 gives a consistent strong learner; but its hypotheses lie in CCC, not in the majority trees over HHH, so it does not prove the stated conclusion.

Formalization scope

The weak-learning hypothesis is the book's with constants γ,δ0\gamma, \delta_0γ,δ0​ in place of the inverse polynomials, which is what the definition says for a fixed class; hypotheses in HHH are required to be measurable, and the weak learner jointly measurable in the sample and the instance, because Strong-Learn runs it on distributions filtered through its own earlier outputs and the analysis integrates over the earlier samples (for an arbitrary function the combined failure event need not be measurable, and outer-measure bounds on separate runs do not combine); the conclusion is the book's hypothesis class, the majority trees over HHH, built as an inductive predicate. Filtered distributions use Mathlib's conditional measure, so that a null conditioning event yields the zero measure; Lemma 4.1 is stated for 0≤β≤1/20 \le \beta \le 1/20≤β≤1/2 and holds in those degenerate cases too. The confidence-boosting milestone states the two probabilistic facts rather than the composite algorithm, whose sample indexing across runs and validation is bookkeeping; the selection rule is any rule minimizing mistakes. Chernoff's bounds are stated with non-strict inequalities in the events, for 0≤p≤10 \le p \le 10≤p≤1 and 0<γ≤10 < \gamma \le 10<γ≤1. Running time, the recursion-depth and sample-size lemmas with unspecified constants (4.2–4.8), and Exercises 4.1–4.3 are not stated.

Trivializing readings are excluded: the weak-learning guarantee is uniform over all targets and distributions with an advantage strictly positive, the strong conclusion is for every ϵ,δ\epsilon, \deltaϵ,δ, and Lemma 4.1 requires all three error bounds on their respective distributions. Welcome contributions: Lemma 4.1 itself, the Hoeffding bound on the product law, and the rejection-sampling lemma that turns a sample of DDD into a sample of a filtered distribution.

Selected references

  • M. J. Kearns, U. V. Vazirani, An Introduction to Computational Learning Theory, MIT Press, 1994, Chapter 4 and Chapter 9. doi:10.7551/mitpress/3897.001.0001
  • R. E. Schapire, The strength of weak learnability, Machine Learning 5(2), 1990. doi:10.1007/BF00116037
  • Y. Freund, Boosting a weak learning algorithm by majority, Information and Computation 121(2), 1995. doi:10.1006/inco.1995.1136
  • W. Hoeffding, Probability inequalities for sums of bounded random variables, Journal of the American Statistical Association 58(301), 1963. doi:10.1080/01621459.1963.10500830
  • H. Chernoff, A measure of asymptotic efficiency for tests of a hypothesis based on the sum of observations, Annals of Mathematical Statistics 23(4), 1952. doi:10.1214/aoms/1177729330
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Multi-armed Bandit Allocation Indices VI: Bandit Sampling Processes, Favourable Priors and Invariance of the IndexTextbook

Motivation

The bandit processes that motivated the index theorem are sampling processes: an arm is a population from which one draws i.i.d. observations whose distribution has an unknown parameter, and each draw both earns something and teaches something. Chapter 7 of Gittins, Glazebrook and Weber, Multi-armed Bandit Allocation Indices (2nd ed., doi:10.1002/9780470980033), develops the theory of such processes in the Bayesian setting: the state of the process is the current posterior for the parameter, continuing it samples the next value from the predictive distribution and moves to the new posterior. When the observations are themselves the rewards one has a reward process, the classical Bayesian multi-armed bandit; when the aim is to find as quickly as possible an individual whose measurement reaches a target TTT (a compound active enough to warrant further testing, in the drug-screening problem from which the index theorem came) one has a target process, which is a job that completes when the target is reached. Two questions organize the chapter. When can the index be written down without any optimization, and when do symmetries of the model reduce the index to a function of fewer variables? The first is answered by the notion of a favourable prior (Section 7.3): if no run of observations below the target can raise the current probability of success, then the index is that probability, exactly, by Proposition 2.7. The second is answered by the invariance theorems of Section 7.4: a location parameter with a conjugate prior gives ν(xˉ,n)=xˉ+ν(0,n)\nu(\bar x, n) = \bar x + \nu(0, n)ν(xˉ,n)=xˉ+ν(0,n), a scale parameter gives ν(xˉ,n)=xˉ ν(1,n)\nu(\bar x, n) = \bar x\,\nu(1, n)ν(xˉ,n)=xˉν(1,n), and for target processes the target can be absorbed into the state, ν(xˉ,n,T)=ν(xˉ−T,n,0)\nu(\bar x, n, T) = \nu(\bar x - T, n, 0)ν(xˉ,n,T)=ν(xˉ−T,n,0). These identities are what make the tables of Chapter 8 one-dimensional.

Setting

A sampling model consists of a likelihood f(⋅∣θ)f(\cdot \mid \theta)f(⋅∣θ), a family of priors π(⋅∣p)\pi(\cdot \mid p)π(⋅∣p) on the parameter indexed by the parameters ppp of a conjugate family, and the Bayes update p↦pxp \mapsto p_xp↦px​ of those parameters after observing xxx; the family is conjugate if the posterior of π(⋅∣p)\pi(\cdot \mid p)π(⋅∣p) given X=xX = xX=x is π(⋅∣px)\pi(\cdot \mid p_x)π(⋅∣px​). The predictive distribution is f(⋅∣p)=∫f(⋅∣θ)π(dθ∣p)f(\cdot \mid p) = \int f(\cdot \mid \theta)\pi(d\theta \mid p)f(⋅∣p)=∫f(⋅∣θ)π(dθ∣p). The reward process moves from ppp to pxp_xpx​ with x∼f(⋅∣p)x \sim f(\cdot \mid p)x∼f(⋅∣p) and earns r(p)=∫xf(x∣p)dxr(p) = \int x f(x \mid p)dxr(p)=∫xf(x∣p)dx. The target process with target TTT moves to the completion state CCC if x≥Tx \ge Tx≥T and to pxp_xpx​ otherwise, earning the current probability of success r(p)=f([T,∞)∣p)r(p) = f([T, \infty) \mid p)r(p)=f([T,∞)∣p), and 000 in CCC. A state ppp is favourable if r(px1⋯xm)≤r(p)r(p_{x_1 \cdots x_m}) \le r(p)r(px1​⋯xm​​)≤r(p) for every finite sequence of observations xi<Tx_i < Txi​<T. For the invariance theorems the parameters are (xˉ,n)(\bar x, n)(xˉ,n) with the update ((nxˉ+x)/(n+1),n+1)((n\bar x + x)/(n+1), n+1)((nxˉ+x)/(n+1),n+1); μ\muμ is a location parameter of the likelihood if f(⋅∣μ+c)f(\cdot \mid \mu + c)f(⋅∣μ+c) is f(⋅∣μ)f(\cdot \mid \mu)f(⋅∣μ) shifted by ccc, and xˉ\bar xxˉ is a location parameter of the prior family if π(⋅∣xˉ+c,n)\pi(\cdot \mid \bar x + c, n)π(⋅∣xˉ+c,n) is π(⋅∣xˉ,n)\pi(\cdot \mid \bar x, n)π(⋅∣xˉ,n) shifted by ccc; scale parameters are defined with x↦bxx \mapsto bxx↦bx, b>0b > 0b>0. The Gittins index is that of the Bandit Algorithms model on these chains.

Formalization targets

Goal: Theorem 7.9 (in the form of Corollary 7.10)

If μ\muμ is a location parameter of a reward process with a conjugate prior family in which xˉ\bar xxˉ is a location parameter and the parameters update as the sample mean and count, then for every n>0n > 0n>0

r(xˉ+c,n)=r(xˉ,n)+candν(xˉ,n)=xˉ+ν(0,n),r(\bar x + c, n) = r(\bar x, n) + c \quad\text{and}\quad \nu(\bar x, n) = \bar x + \nu(0, n),r(xˉ+c,n)=r(xˉ,n)+candν(xˉ,n)=xˉ+ν(0,n),

under the standing assumptions that the observations have a mean and the discounted rewards of the chain are integrable.

Milestones

Proposition 7.4 (favourable state: ν=r\nu = rν=r); Example 7.5 (Bernoulli target process, ν(α,β)=α/(α+β)\nu(\alpha, \beta) = \alpha/(\alpha + \beta)ν(α,β)=α/(α+β)); Example 7.6 (normal target process with known variance, ν(xˉ,n)=Φ(xˉ(1+n−1)−1/2)\nu(\bar x, n) = \Phi(\bar x (1 + n^{-1})^{-1/2})ν(xˉ,n)=Φ(xˉ(1+n−1)−1/2) for xˉ≥0\bar x \ge 0xˉ≥0); Theorem 7.11 (scale parameter: ν(xˉ,n)=xˉ ν(1,n)\nu(\bar x, n) = \bar x\,\nu(1, n)ν(xˉ,n)=xˉν(1,n)); Theorem 7.17 (target process with a location parameter: ν(xˉ,n,T)=ν(xˉ−T,n,0)\nu(\bar x, n, T) = \nu(\bar x - T, n, 0)ν(xˉ,n,T)=ν(xˉ−T,n,0)).

Significance

Theorem 7.9 and its companions are the reason the Gittins index of the normal reward process is tabulated as a function of nnn alone and that of the exponential process as a function of nnn and one ratio; every computational method of Chapter 8 starts by reducing the state space with them. Proposition 7.4 is the source of every closed-form index in the book: it identifies the states in which sampling for information is worthless, so that the index collapses to the immediate expected reward, and Examples 7.5 and 7.6 show that for the Bernoulli target process this is every state and for the normal target process every state with a nonnegative posterior mean. The formalization gives the platform its first Bayesian sampling-process model, in which the state is a posterior and conjugacy is stated through the posterior kernel of the likelihood, and its first index identities on unbounded-reward chains, which is where the integrability assumptions of the Bandit Algorithms model do real work.

None of this is machine-checked. The invariance theorems are stated in the proper-prior form of the corollaries, with the model's symmetry as hypotheses, so that they apply to any conjugate family with the stated structure rather than to a particular density.

Difficulty

The invariance theorems require showing that the chain of parameters from the shifted (scaled) state is the image of the chain from the original state under the shift (scaling) of trajectories, which is an equivariance of the Ionescu–Tulcea construction with respect to a measurable bijection commuting with the kernel; that stopping times are carried to stopping times; that the discounted reward of a stopping time shifts by ccc times the discounted time; and that the supremum of a nonempty bounded set of reals shifts and scales accordingly. Boundedness of the set of ratios is where the integrability assumption enters. Proposition 7.4 is the chain-level statement that all rewards along every trajectory from a favourable state are at most r(p)r(p)r(p), which needs an induction on the trajectory law of the target chain, followed by the argument of Proposition 2.7. Example 7.6 needs the monotonicity of xˉm(1+1/(n+m))−1/2\bar x_m (1 + 1/(n+m))^{-1/2}xˉm​(1+1/(n+m))−1/2 in the observations below the target, a small inequality, plus the Gaussian probability of a half-line as the current probability of success; Example 7.5 needs only that α/(α+β+m)\alpha/(\alpha + \beta + m)α/(α+β+m) decreases.

Formalization scope

The sampling model is a structure with Markov likelihood and prior kernels and a jointly measurable update; the predictive distribution is the kernel composition; conjugacy is an almost-everywhere identity between Mathlib's posterior of the likelihood with respect to the prior and the prior at the updated parameters, and is carried as a hypothesis of the invariance theorems and of Proposition 7.4 so that their subject is the Bayesian process. For the parameters (xˉ,n)(\bar x, n)(xˉ,n) it is required on n>0n > 0n>0 only (IsConjugateOn): a proper prior has n>0n > 0n>0, and conjugacy at every (xˉ,n)∈R2(\bar x, n) \in \mathbb{R}^2(xˉ,n)∈R2 is impossible with a location parameter, since at n=−1n = -1n=−1 the update divides by zero and sends every observation to one state, which made the first draft's location theorems vacuous. The chains are built with Kernel.map of product kernels, so their measurability is structural, and the target process lives on P ⊕ Unit with the completion state absorbing. The book's improper priors are replaced by proper conjugate families with the location or scale structure of Corollaries 7.10 and 7.12, as those corollaries do; the discrete-time correction factor of Section 2.8 is not applied since it cancels in every identity stated. The two examples are built directly from a uniform or Gaussian seed with the transition probabilities the book computes (the beta and normal posterior computations of Exercise 7.1 are not formalized). Hypotheses: a∈(0,1)a \in (0, 1)a∈(0,1); integrable observations and L&S Assumption 35.6 for the reward processes; n>0n > 0n>0 for the invariance theorems and xˉ>0\bar x > 0xˉ>0 for the scale theorem; α,β>0\alpha, \beta > 0α,β>0; xˉ≥0\bar x \ge 0xˉ≥0 and n>0n > 0n>0 for the normal example.

Trivializing readings are excluded: the indices are the genuine suprema of the Bandit Algorithms definition with integrable rewards, the update rule is the book's and not a free parameter, and the favourability condition ranges over all finite observation sequences. Welcome contributions: the equivariance of the trajectory measure under a state bijection commuting with the kernel, the transport of stopping times, and the reward bound along the target chain from a favourable state.

Selected references

  • J. Gittins, K. Glazebrook, R. Weber, Multi-armed Bandit Allocation Indices, 2nd ed., Wiley, 2011, Chapter 7. doi:10.1002/9780470980033
  • J. C. Gittins, D. M. Jones, A dynamic allocation index for the sequential design of experiments, in Progress in Statistics (J. Gani, ed.), North-Holland, 1974.
  • D. M. Jones, Search Procedures for Industrial Chemical Research, PhD thesis, University of Wales, 1975.
  • H. Raiffa, R. Schlaifer, Applied Statistical Decision Theory, Harvard University Press, 1961.
  • T. S. Ferguson, Mathematical Statistics: A Decision Theoretic Approach, Academic Press, 1967.
  • T. Lattimore, C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020, Chapters 34–35. doi:10.1017/9781108571401
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Multi-armed Bandit Allocation Indices V: Restless Bandits, Indexability and Whittle Indices for Monotone ModelsTextbook

Motivation

Every proof of the index theorem in Gittins, Glazebrook and Weber, Multi-armed Bandit Allocation Indices (2nd ed., doi:10.1002/9780470980033), uses the fact that a bandit not being processed is frozen. Chapter 6 drops that: Whittle's restless bandits evolve under the passive action too, by a different law, and mmm of nnn must be active at every time. The problem is PSPACE-hard in general, so Whittle proposed a heuristic built from a Lagrangian relaxation: replace the hard constraint by a subsidy WWW paid whenever a bandit is passive, solve the resulting single-bandit average-reward problem, and read off, for each state, the least subsidy W(x)W(x)W(x) at which the passive action becomes optimal. When the set of states where passivity is optimal grows monotonically with WWW, the bandit is indexable and W(x)W(x)W(x) is its Whittle index; the Whittle index policy activates the mmm bandits of largest index. It reduces to the Gittins index policy when the passive action freezes, it is asymptotically optimal as nnn grows under a fluid-stability condition (Weber and Weiss), and it has become the standard heuristic for sensor management, opportunistic channel access, maintenance and queueing control. The price is that indexability must be established model by model. Section 6.5 shows how easy this is when the single-bandit problem is solved by a monotone policy, on two bi-directional models: the spinning plates asset, which improves under investment and deteriorates when neglected, and the vigour bandit of Whittle's Ehrenfest project, which tires when worked and recovers when rested.

Setting

A restless bandit is a Markov decision process with two actions, active (u=1u = 1u=1) and passive (u=0u = 0u=0), each with its own transition kernel and reward. Under a deterministic stationary Markov policy ggg with passive subsidy WWW the reward in state xxx is r(x,g(x))+W(1−g(x))r(x, g(x)) + W(1 - g(x))r(x,g(x))+W(1−g(x)), and the average reward from xxx is the Cesàro limit of the expected rewards. The optimal average reward g(W)g(W)g(W) is the supremum over such policies and initial states; a policy is optimal if it attains g(W)g(W)g(W) from every initial state; E0(W)E_0(W)E0​(W) is the set of states in which some optimal policy is passive; the bandit is indexable if E0(W)E_0(W)E0​(W) is nondecreasing in WWW; and W(x)=inf⁡{W:x∈E0(W)}W(x) = \inf\{W : x \in E_0(W)\}W(x)=inf{W:x∈E0​(W)}.

The spinning plates asset lives on {1,…,k}\{1, \dots, k\}{1,…,k}: active moves x→x+1x \to x + 1x→x+1 at rate λ(x)\lambda(x)λ(x), passive moves x→x−1x \to x - 1x→x−1 at rate μ(x)\mu(x)μ(x), λ(k)=μ(1)=0\lambda(k) = \mu(1) = 0λ(k)=μ(1)=0, and r(x)r(x)r(x) is earned under both actions, rrr increasing. Uniformized so that rates are at most one, it is a discrete-time bandit whose kernels move with the rate's probability and otherwise stay. The monotone policy (y)(y)(y) is passive exactly on {x≥y}\{x \ge y\}{x≥y}; under it the asset alternates between y−1y - 1y−1 and yyy, spending the fraction ϕ(y)=λ(y−1)/(λ(y−1)+μ(y))\phi(y) = \lambda(y-1)/(\lambda(y-1) + \mu(y))ϕ(y)=λ(y−1)/(λ(y−1)+μ(y)) of its time at yyy, so its average reward is Wϕ(y)+R(y)W\phi(y) + R(y)Wϕ(y)+R(y) with R(y)=r(y)ϕ(y)+r(y−1)(1−ϕ(y))R(y) = r(y)\phi(y) + r(y-1)(1 - \phi(y))R(y)=r(y)ϕ(y)+r(y−1)(1−ϕ(y)), and W∗(x)=(R(x+1)−R(x))/(ϕ(x)−ϕ(x+1))W^*(x) = (R(x+1) - R(x))/(\phi(x) - \phi(x+1))W∗(x)=(R(x+1)−R(x))/(ϕ(x)−ϕ(x+1)). The vigour bandit is the mirror image: active moves down at rate ν(x)\nu(x)ν(x) and earns r(x)r(x)r(x), passive moves up at rate ρ(x)\rho(x)ρ(x) and earns nothing, ψ(y)=ν(y)/(ν(y)+ρ(y−1))\psi(y) = \nu(y)/(\nu(y) + \rho(y-1))ψ(y)=ν(y)/(ν(y)+ρ(y−1)), and W∗∗(x)=(r(x)(1−ψ(x))−r(x+1)(1−ψ(x+1)))/(ψ(x+1)−ψ(x))W^{**}(x) = (r(x)(1 - \psi(x)) - r(x+1)(1 - \psi(x+1)))/(\psi(x+1) - \psi(x))W∗∗(x)=(r(x)(1−ψ(x))−r(x+1)(1−ψ(x+1)))/(ψ(x+1)−ψ(x)).

Formalization targets

Goal: Theorem 6.4

For the spinning plates asset: (i) if ϕ\phiϕ is strictly decreasing over the thresholds 1≤y≤k+11 \le y \le k + 11≤y≤k+1, the asset is indexable; (ii) if additionally W∗W^*W∗ is strictly decreasing over the states, the Whittle index is

W(x)=W∗(x)=R(x+1)−R(x)ϕ(x)−ϕ(x+1),1≤x≤k.W(x) = W^*(x) = \frac{R(x+1) - R(x)}{\phi(x) - \phi(x+1)}, \qquad 1 \le x \le k.W(x)=W∗(x)=ϕ(x)−ϕ(x+1)R(x+1)−R(x)​,1≤x≤k.

Milestones

Eqs. (6.9)–(6.10): the monotone policy (y)(y)(y) earns Wϕ(y)+R(y)W\phi(y) + R(y)Wϕ(y)+R(y) from every initial state and g(W)=max⁡y[Wϕ(y)+R(y)]g(W) = \max_y [W\phi(y) + R(y)]g(W)=maxy​[Wϕ(y)+R(y)], because a monotone policy always achieves g(W)g(W)g(W); Theorem 6.5, the same two statements for the vigour bandit with ψ\psiψ increasing and W∗∗W^{**}W∗∗ increasing.

Significance

Theorem 6.4 is the chapter's template for proving indexability: the single-bandit value g(W)g(W)g(W) is the upper envelope of finitely many lines Wϕ(y)+R(y)W\phi(y) + R(y)Wϕ(y)+R(y) whose slopes decrease in the threshold, so the optimal threshold moves monotonically with the subsidy and the hinge points of the envelope are the indices. The same argument gives Theorem 6.5, the admission-control indices of Section 6.7, and the marginal productivity indices of Niño-Mora; it is the reason Whittle indices are computable in closed form for bi-directional models. Its formalization establishes, on the platform, the first restless-bandit model with a proved index, and the general notions of passive set, indexability and Whittle index that every later restless-bandit statement will use.

None of this is machine-checked. The average-reward optimality notion is stated without the DP equation (6.6), through optimality from every initial state, which is what the equation's solution encodes on a finite state space and avoids the relative value function altogether.

Difficulty

The proof in the book is two paragraphs, but it stands on the reduction to monotone policies, which is only sketched: every deterministic stationary policy, from every initial state, drives the asset into an absorbing endpoint or a two-state cycle {z−1,z}\{z - 1, z\}{z−1,z} whose average reward is that of the monotone policy (z)(z)(z), so no policy beats the best monotone one and the passive set under an optimal-from-everywhere policy is exactly {x≥x(W)}\{x \ge x(W)\}{x≥x(W)} for the smallest maximizing threshold. Formalizing this needs the average reward of a finite Markov chain as a limit determined by the stationary distribution of the recurrent class reached, for the two-point kernels of the model, and a case analysis of policies as {0,1}\{0,1\}{0,1}-strings. The envelope argument then needs that the smallest maximizer of max⁡y[Wϕ(y)+R(y)]\max_y [W\phi(y) + R(y)]maxy​[Wϕ(y)+R(y)] is nonincreasing in WWW when ϕ\phiϕ is strictly decreasing, and that with W∗W^*W∗ strictly decreasing the maximizer is ≤x\le x≤x exactly when W≥W∗(x)W \ge W^*(x)W≥W∗(x). Theorem 6.5 is the same with the roles of up and down exchanged. Nothing in Mathlib computes Cesàro limits of finite Markov chains.

Formalization scope

Restless bandits are the two-action DecisionProcesses of the superprocess module; average reward is a real limsup of Cesàro means of Bochner integrals over the chain law of the Bandit Algorithms model under the stationary kernel; the optimal average reward is a supremum over the finite type of deterministic stationary Markov policies and the finite state space, bounded by the reward bound. Both models are on Fin k with the book's states shifted down by one, kernels driftKernel p f that move to f x with probability p x, and the boundary conventions of ϕ\phiϕ and ψ\psiψ (the book's "convenient positive values") replaced by their values 1,01, 01,0 and 0,10, 10,1 at the two extreme thresholds; the model assumptions λ(k)=μ(1)=0\lambda(k) = \mu(1) = 0λ(k)=μ(1)=0, ν(1)=ρ(k)=0\nu(1) = \rho(k) = 0ν(1)=ρ(k)=0, rates in [0,1][0, 1][0,1], and rrr increasing and nonnegative are hypotheses. Theorem 6.5's "increasing" is read as strictly increasing, as in Theorem 6.4, since a nonstrict ψ\psiψ admits zero interior rates for which the monotone reduction fails. The milestone (6.9) requires k≥1k \ge 1k≥1 and positive interior rates, which Theorem 6.4's hypothesis (i) implies.

Trivializing readings are excluded: indexability is monotonicity of the passive set over all real subsidies, the passive set is defined through policies optimal from every initial state, and the index identity is for every state. Welcome contributions: the average reward of a two-state cycle, the reduction of an arbitrary {0,1}\{0,1\}{0,1}-policy to a monotone one, and the envelope lemma for lines with decreasing slopes.

Selected references

  • J. Gittins, K. Glazebrook, R. Weber, Multi-armed Bandit Allocation Indices, 2nd ed., Wiley, 2011, Chapter 6. doi:10.1002/9780470980033
  • P. Whittle, Restless bandits: activity allocation in a changing world, Journal of Applied Probability 25(A), 1988. doi:10.2307/3214163
  • R. R. Weber, G. Weiss, On an index policy for restless bandits, Journal of Applied Probability 27(3), 1990. doi:10.2307/3214547
  • K. D. Glazebrook, C. Kirkbride, D. Ruiz-Hernandez, Spinning plates and squad systems: policies for bi-directional restless bandits, Advances in Applied Probability 38(1), 2006. doi:10.1239/aap/1143936141
  • J. Niño-Mora, Restless bandits, partial conservation laws and indexability, Advances in Applied Probability 33(1), 2001. doi:10.1017/S0001867800010661
  • C. H. Papadimitriou, J. N. Tsitsiklis, The complexity of optimal queueing network control, Mathematics of Operations Research 24(2), 1999. doi:10.1287/moor.24.2.293
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Bandit AlgorithmsLinear OptimizationOperations Research+2·Captain: naimengye

Multi-armed Bandit Allocation Indices IV: The Achievable Region, Generalized Conservation Laws and the Adaptive Greedy AlgorithmTextbook

Motivation

Chapter 5 of Gittins, Glazebrook and Weber, Multi-armed Bandit Allocation Indices (2nd ed., doi:10.1002/9780470980033), presents the achievable region methodology of Tsoucas, Bertsimas and Niño-Mora, Glazebrook and Garbe, and Dacre, Glazebrook and Niño-Mora: instead of arguing about policies, one argues about the set of performance vectors they can produce. For a multi-armed bandit the natural performance of a policy is the vector of discounted numbers of times each state is continued; the expected return is linear in it; and the set of achievable performances turns out to be a polytope cut out by conservation laws, one inequality per subset of states, with equality exactly for the priority policies that put that subset last. Optimizing a linear objective over a polytope is a linear program, its dual is solved by an adaptive greedy algorithm, and the primal solution is the performance of a priority policy whose priorities are the algorithm's outputs, the Gittins indices. This gives yet another proof of the index theorem (Section 5.3) and, more importantly, a definition, generalized conservation laws (Section 5.4), of the class of systems for which the same argument works: branching bandits, multi-class queues, job scheduling with discounted rewards, systems with imposed priority classes. The chapter's main result, Theorem 5.5, is the statement that every such system is solved by an index policy.

Setting

There are NNN job types E={1,…,N}E = \{1, \dots, N\}E={1,…,N}. A policy π\piπ has a performance xπ∈R+Nx^\pi \in \mathbb{R}^N_+xπ∈R+N​, a vector of expectations; a permutation σ\sigmaσ of EEE defines the permutation policy giving σN\sigma_NσN​ highest and σ1\sigma_1σ1​ lowest priority, and Sk={σ1,…,σk}S_k = \{\sigma_1, \dots, \sigma_k\}Sk​={σ1​,…,σk​} is the set of the kkk lowest-priority types. The system satisfies GCL(1) if there are a base function b:2E→R+b : 2^E \to \mathbb{R}_+b:2E→R+​ and a matrix A=(AiS)A = (A_i^S)A=(AiS​), positive on SSS and zero off it, such that for every policy

∑i∈SAiSxiπ≥b(S)(S⊆E),∑i∈EAiExiπ=b(E),\sum_{i \in S} A_i^S x_i^\pi \ge b(S) \quad (S \subseteq E), \qquad \sum_{i \in E} A_i^E x_i^\pi = b(E),i∈S∑​AiS​xiπ​≥b(S)(S⊆E),i∈E∑​AiE​xiπ​=b(E),

with equality in the first for every permutation policy whose ∣S∣|S|∣S∣ lowest-priority types are SSS. GCL(2) reverses the inequality. The adaptive greedy algorithm AG(A,r)AG(A, r)AG(A,r) picks iNi_NiN​ maximizing ri/AiEr_i/A_i^Eri​/AiE​, sets yˉE\bar y_Eyˉ​E​ to the maximum, removes iNi_NiN​, and repeats with the adjusted rewards ri−∑j≥kAiSjyˉSjr_i - \sum_{j \ge k} A_i^{S_j}\bar y_{S_j}ri​−∑j≥k​AiSj​​yˉ​Sj​​ divided by AiSk−1A_i^{S_{k-1}}AiSk−1​​; its outputs are the order i1,…,iNi_1, \dots, i_Ni1​,…,iN​, the dual variables yˉSk\bar y_{S_k}yˉ​Sk​​ and the indices νik=∑j≥kyˉSj\nu_{i_k} = \sum_{j \ge k} \bar y_{S_j}νik​​=∑j≥k​yˉ​Sj​​.

For the SFABP of Section 5.3, nnn identical bandit processes on EEE with kernel PPP and discount factor aaa in the model of the Bandit Algorithms series, xiπ=Eπ∑tatIi(t)x_i^\pi = \mathbb{E}^\pi \sum_t a^t I_i(t)xiπ​=Eπ∑t​atIi​(t) is the discounted number of continuations of a bandit in state iii, AiS=E[1+a+⋯+aTiS−1]A_i^S = \mathbb{E}[1 + a + \cdots + a^{T_i^S - 1}]AiS​=E[1+a+⋯+aTiS​−1] is the discounted return time to SSS from i∈Si \in Si∈S, and b(S)b(S)b(S) is the minimal cost ∑i∈SAiSxiπ\sum_{i \in S} A_i^S x_i^\pi∑i∈S​AiS​xiπ​, namely (1−a)−1E[aτ](1-a)^{-1}\mathbb{E}[a^\tau](1−a)−1E[aτ] with τ\tauτ the number of continuations needed to bring every bandit into SSS.

Formalization targets

Goal: Theorem 5.5

For a GCL(1) system whose achievable region is convex, and any reward vector rrr: the achievable region is the polytope

P(A,b)={x∈R+N:∑i∈SAiSxi≥b(S), S⊂E, ∑i∈EAiExi=b(E)};P(A, b) = \Big\{x \in \mathbb{R}_+^N : \sum_{i \in S} A_i^S x_i \ge b(S),\ S \subset E,\ \sum_{i \in E} A_i^E x_i = b(E)\Big\};P(A,b)={x∈R+N​:i∈S∑​AiS​xi​≥b(S), S⊂E, i∈E∑​AiE​xi​=b(E)};

its extreme points are performances of permutation policies; AG(A,r)AG(A, r)AG(A,r) has an output; and for every output the permutation policy in the order it finds, the Gittins index policy, maximizes ∑irixiπ\sum_i r_i x_i^\pi∑i​ri​xiπ​ over all policies.

Milestones

Lemma 5.1 (the SFABP satisfies the conservation laws, with equality for policies giving priority to states outside SSS); the identification on p. 123 of the adaptive greedy indices of a SFABP with the Gittins indices, together with their monotonicity along the order found; Theorem 5.10, the GCL(2) counterpart of the goal for cost minimization.

Significance

Theorem 5.5 is the index theorem in its most general form of this kind: it says nothing about Markov chains, only that performances are expectations, objectives are linear and conservation laws hold, and it delivers both the optimal policy and the algorithm that computes its priorities in polynomial time in the number of job types. It is the theorem behind the index results for branching bandits and Klimov's multi-class queue and behind the suboptimality bounds of Sections 5.5 and 5.7, all of which are calculations on the polytope. Lemma 5.1 and the p. 123 identification are what tie the abstract theorem to the Gittins index: they show that the multi-armed bandit is a GCL(1) system and that the priorities the algorithm produces are the same indices as Chapters 2 to 4 define through stopping times.

None of these is machine-checked. Formalizing Theorem 5.5 puts an LP-duality index theorem on the platform in a form any system can instantiate by verifying its conservation laws; formalizing Lemma 5.1 relates the Bandit Algorithms run law to the single-chain return times, which is the first conservation law on that model; and the p. 123 theorem gives an algorithmic characterization of the Gittins index on finite chains, distinct from the restart and largest-remaining-index characterizations of Chapter 2.

Difficulty

The goal's optimality clause is weak LP duality once one shows that the greedy dual variables are nonpositive except yˉE\bar y_Eyˉ​E​ and satisfy the dual constraints with equality, which is a finite induction on the stages; the extreme-point clause needs that every vertex of a polyhedron is the unique maximizer of some linear functional, and the region clause that a compact convex set is the convex hull of its extreme points (Krein–Milman in finite dimension, or the polyhedral fact directly). None of this is in Mathlib in the required form. Lemma 5.1 is probabilistic: the lower bound requires the strong Markov property of the continued bandit under an arbitrary past-measurable policy, a pathwise accounting of the discounted periods paid for by each continuation from SSS, and the observation that at most τ\tauτ slots can be spent on bandits that have never been in SSS; the equality for priority policies requires that these policies use exactly those slots first and then tile the future with return excursions, and the product form of b(S)b(S)b(S) requires independence of the bandits' process-time trajectories under the run law, which is built decision time by decision time rather than as a product. The p. 123 theorem is the computation (5.13) to (5.14) combined with the optimal-stopping characterization of Chapter 2 for the stop sets {i1,…,ik−2}\{i_1, \dots, i_{k-2}\}{i1​,…,ik−2​}, which lie between {ν<ν(ik−1)}\{\nu < \nu(i_{k-1})\}{ν<ν(ik−1​)} and {ν≤ν(ik−1)}\{\nu \le \nu(i_{k-1})\}{ν≤ν(ik−1​)}; ties make the induction delicate, and the statement is claimed for every tie-breaking.

Formalization scope

GCL(1) and GCL(2) systems are structures over an arbitrary policy type: performance, base function, matrix, permutation policies and the three laws are fields, so the theorems are statements about finite-dimensional data and the platform's proof needs no probability. The adaptive greedy algorithm is specified relationally, as the set of its possible outputs with arbitrary tie-breaking, and the conclusion holds for each of them; existence of an output is asserted separately. The optimality clause is stated as a comparison with every policy rather than as a real supremum. The hypothesis that the achievable region is convex is explicit: the book's argument from extreme points to the whole polytope uses randomization of policies, and without it the region of a system with only its permutation policies is finite. The SFABP items use nnn identical bandits on Fin N in the Bandit Algorithms model, the coefficients AiSA_i^SAiS​ through Mission I's stoppedTime at the return time, and b(S)b(S)b(S) in the product form (1−a)−1∏j:kj∉SE[aTkjS](1-a)^{-1}\prod_{j : k_j \notin S}\mathbb{E}[a^{T^S_{k_j}}](1−a)−1∏j:kj​∈/S​E[aTkj​S​], which is the minimal cost the argument on p. 120 establishes; the book prints a sum, which is 000 when all bandits start in SSS where the minimal cost is 1/(1−a)1/(1-a)1/(1−a). Discount factors are in (0,1)(0, 1)(0,1) throughout.

Trivializing readings are excluded: AiS>0A_i^S > 0AiS​>0 for i∈Si \in Si∈S is part of the structure and of Lemma 5.1's conclusion, the polytope equations are over all subsets, and the index clause quantifies over every greedy output. Welcome contributions: the nonpositivity and dual feasibility of the greedy variables, the vertex-exposure lemma for polyhedra, and the product decomposition of the run law of identical bandits.

Selected references

  • J. Gittins, K. Glazebrook, R. Weber, Multi-armed Bandit Allocation Indices, 2nd ed., Wiley, 2011, Chapter 5. doi:10.1002/9780470980033
  • D. Bertsimas, J. Niño-Mora, Conservation laws, extended polymatroids and multiarmed bandit problems; a polyhedral approach to indexable systems, Mathematics of Operations Research 21(2), 1996. doi:10.1287/moor.21.2.257
  • P. Tsoucas, The region of achievable performance in a model of Klimov, IBM Research Report RC16543, 1991.
  • E. G. Coffman, I. Mitrani, A characterization of waiting time performance realizable by single-server queues, Operations Research 28(3), 1980. doi:10.1287/opre.28.3.810
  • K. D. Glazebrook, R. Garbe, Almost optimal policies for stochastic systems which almost satisfy conservation laws, Annals of Operations Research 92, 1999. doi:10.1023/A:1018992306696
  • T. Lattimore, C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020, Chapter 35. doi:10.1017/9781108571401
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Algorithmic Game TheoryBandit AlgorithmsMachine Learning+2·Captain: naimengye

Introduction to Multi-Armed Bandits XI: Bandits and Agents, Incentivized Exploration via Hidden ExplorationTextbook

Motivation

A recommendation system learns from the users it serves: the diner who tries a restaurant produces the review the next diner reads. Each user would rather exploit what is already known than explore for the benefit of those who come later, so a population of self-interested agents under-explores, and an alternative that looks bad on sparse early evidence may never be tried again even when it is the best. Chapter 11 of Slivkins, Introduction to Multi-Armed Bandits (arXiv:1904.07272), treats incentivized exploration: a principal who cannot force the agents but can recommend, and who, because it aggregates what earlier agents observed, knows more than any one of them. The question is whether recommendations alone can induce enough exploration to learn as fast as an ordinary bandit algorithm. The model is that of Kremer, Mansour and Perry (JPE 2014) and the results are those of Mansour, Slivkins and Syrgkanis (EC 2015, Operations Research 2020), specialized to two arms; the single-round problem is Bayesian persuasion in the sense of Kamenica and Gentzkow (AER 2011).

Setting

There are KKK arms and TTT rounds. A mean reward vector μ∈[0,1]K\mu \in [0,1]^Kμ∈[0,1]K is drawn from a known prior PPP, and each pull of arm aaa yields a reward drawn from a known family DμaD_{\mu_a}Dμa​​ with mean μa\mu_aμa​. In round ttt the principal recommends an arm rect\mathrm{rec}_trect​; agent ttt, who knows the prior, the family, the algorithm and the round but not the past, sees only rect\mathrm{rec}_trect​, chooses ata_tat​, collects rt∼Dμatr_t \sim D_{\mu_{a_t}}rt​∼Dμat​​​ and leaves; the principal observes (at,rt)(a_t, r_t)(at​,rt​). The chapter works with two arms, ordered so that the prior means satisfy μ10≥μ20\mu^0_1 \ge \mu^0_2μ10​≥μ20​, with a prior of finite support and finitely many reward values.

An algorithm is Bayesian incentive-compatible (BIC, Definition 11.4) if following its recommendation is in every agent's interest given what the agent knows: for every round ttt and arms a≠a′a \ne a'a=a′ with Pr⁡[rect=a,Et−1]>0\Pr[\mathrm{rec}_t = a, E_{t-1}] > 0Pr[rect​=a,Et−1​]>0,

E[μa−μa′∣rect=a, Et−1]≥0,(11.1)\mathbb{E}[\mu_a - \mu_{a'} \mid \mathrm{rec}_t = a,\ E_{t-1}] \ge 0, \tag{11.1}E[μa​−μa′​∣rect​=a, Et−1​]≥0,(11.1)

where Et−1E_{t-1}Et−1​ is the event that all previous agents complied. A BIC algorithm is then an ordinary bandit algorithm whose recommendations are followed, and the run has the law of the Bayesian bandit of Chapter 3. Two contrasting policies frame the chapter. GREEDY reveals the history and lets agents exploit, at∈arg⁡max⁡aE[μa∣Ht]a_t \in \arg\max_a \mathbb{E}[\mu_a \mid H_t]at​∈argmaxa​E[μa​∣Ht​] (11.2); it is BIC and it fails. HiddenExploration (Algorithm 11.1) hides a little exploration in a lot of exploitation: on a signal sig\mathrm{sig}sig, with probability ε\varepsilonε it recommends a target arm atrg(sig)a_{\mathrm{trg}}(\mathrm{sig})atrg​(sig), otherwise the arm maximizing E[μa∣sig]\mathbb{E}[\mu_a \mid \mathrm{sig}]E[μa​∣sig], ties to arm 1. Its posterior gap is G=E[μ2−μ1∣sig]G = \mathbb{E}[\mu_2 - \mu_1 \mid \mathrm{sig}]G=E[μ2​−μ1​∣sig]. RepeatedHE (Algorithm 11.2) runs it round after round with an arbitrary bandit algorithm ALG\mathrm{ALG}ALG as the target: N0N_0N0​ initial rounds recommend arm 1; afterwards, with probability ε\varepsilonε the round is an exploration round in which ALG\mathrm{ALG}ALG chooses (and is fed the reward), and otherwise the exploitation branch recommends min⁡arg⁡max⁡aE[μa∣St]\min\arg\max_a \mathbb{E}[\mu_a \mid S_t]minargmaxa​E[μa​∣St​], where StS_tSt​ is the data of all exploration rounds so far (11.10). The quantity that governs everything is G1,n=E[μ2−μ1∣S1,n]G_{1,n} = \mathbb{E}[\mu_2 - \mu_1 \mid S_{1,n}]G1,n​=E[μ2​−μ1​∣S1,n​] (11.11), the posterior gap after nnn samples of arm 1, and Property (11.12), that Pr⁡[G1,n>0]>0\Pr[G_{1,n} > 0] > 0Pr[G1,n​>0]>0 for some nnn: arm 2 can appear better after enough samples of arm 1.

Formalization targets

Goal: Theorem 11.15

RepeatedHE with exploration probability ε>0\varepsilon > 0ε>0 and N0N_0N0​ initial samples of arm 1 is BIC as long as

ε<13 E[G⋅1{G>0}],G=GN0+1=E[μ2−μ1∣S1,N0],\varepsilon < \tfrac13\,\mathbb{E}\big[G \cdot \mathbf 1\{G > 0\}\big], \qquad G = G_{N_0+1} = \mathbb{E}[\mu_2 - \mu_1 \mid S_{1,N_0}],ε<31​E[G⋅1{G>0}],G=GN0​+1​=E[μ2​−μ1​∣S1,N0​​],

for any bandit algorithm ALG\mathrm{ALG}ALG and any horizon. The threshold depends on the prior alone.

Milestones

Theorem 11.7 (GREEDY never chooses arm 2 with probability at least μ10−μ20\mu^0_1 - \mu^0_2μ10​−μ20​) and Corollary 11.8 (linear Bayesian regret of GREEDY under independent priors); Lemma 11.10 (HiddenExploration is BIC when ε≤13E[G1{G>0}]\varepsilon \le \frac13\mathbb{E}[G\mathbf 1\{G > 0\}]ε≤31​E[G1{G>0}]) with Claim 11.12 (the arm-2 side of the constraint suffices); Corollary 11.14 (RepeatedHE is BIC under the round-by-round condition); Theorem 11.19 (without Property (11.12) no BIC algorithm ever plays arm 2, ties to arm 1).

Significance

The results say when exploration can be incentivized at all and how. Theorem 11.7 shows that revealing everything is not a solution: the greedy dynamics gets stuck on arm 1 with a probability that does not shrink with TTT, and Corollary 11.8 turns that into Ω(T)\Omega(T)Ω(T) Bayesian regret. Theorem 11.15 shows that a recommendation-only principal can induce any amount of exploration it wants, with ALG\mathrm{ALG}ALG arbitrary, at a per-round rate ε\varepsilonε fixed by the prior; Theorem 11.17 (stated with a proof sketch, and omitted here) then transfers ALG\mathrm{ALG}ALG's regret to RepeatedHE up to the prior-dependent factors N0N_0N0​ and 1/ε1/\varepsilon1/ε, so O~(T)\tilde O(\sqrt T)O~(T​) regret is attainable subject to incentives. Theorem 11.19 closes the picture: Property (11.12) is necessary as well as sufficient. Together they characterize which priors admit incentivized exploration and give an algorithm that works for all of them.

Nothing of this is machine-checked. The mission adds to the Bayesian layer of mission III (prior, posterior by Bayes' rule, Bayesian regret) the BIC constraint on a joint law, GREEDY as a policy, the single-round HiddenExploration on an abstract finite signal, and the law of RepeatedHE; all of it is reusable for the KKK-arm and the "explore all explorable arms" extensions of the literature review.

Difficulty

Theorem 11.7 is a martingale argument: the posterior gap along the history is a Doob martingale, the first round in which arm 2 is chosen is a bounded stopping time, and optional stopping gives E[Zτ]=μ10−μ20\mathbb{E}[Z_\tau] = \mu^0_1 - \mu^0_2E[Zτ​]=μ10​−μ20​; all of this has to be set up on the joint law of (μ,HT)(\mu, H_T)(μ,HT​) of mission III, where the posterior is defined by Bayes' rule and the identification with a conditional expectation is itself a theorem (posterior_eq_condProb). Lemma 11.10 is the heart of the chapter and is not a computation about rec\mathrm{rec}rec: it works with F(E)=E[G1E]F(E) = \mathbb{E}[G\mathbf 1_E]F(E)=E[G1E​], splits along the two branches, uses that the exploitation branch recommends arm 2 exactly when G>0G > 0G>0, and closes with F(G>0)+F(G<0)=E[μ2−μ1]≤0F(G > 0) + F(G < 0) = \mathbb{E}[\mu_2 - \mu_1] \le 0F(G>0)+F(G<0)=E[μ2​−μ1​]≤0; the only place where the analysis uses that both branches are functions of the signal is the step E[μ2−μ1∣rec=2]=E[G∣rec=2]\mathbb{E}[\mu_2 - \mu_1 \mid \mathrm{rec} = 2] = \mathbb{E}[G \mid \mathrm{rec} = 2]E[μ2​−μ1​∣rec=2]=E[G∣rec=2], and a formalization has to make that step explicit. Theorem 11.15 requires seeing each later round of RepeatedHE as a HiddenExploration with signal StS_tSt​, where ALG\mathrm{ALG}ALG's choice is a randomized function of StS_tSt​, and then the monotonicity of E[Gt1{Gt>0}]\mathbb{E}[G_t\mathbf 1\{G_t > 0\}]E[Gt​1{Gt​>0}] in ttt, a two-line consequence of St+1S_{t+1}St+1​ determining StS_tSt​ that presupposes the posterior given StS_tSt​ is the Bayes posterior of the exploration data alone, which is true because the exploration decisions do not depend on μ\muμ given that data. Corollary 11.8 needs the independence of the event "μ1<1−2α\mu_1 < 1 - 2\alphaμ1​<1−2α and arm 2 is never chosen" from μ2\mu_2μ2​. Theorem 11.19 is an induction in which the inductive hypothesis is a probability-zero statement about all earlier rounds.

Formalization scope

Arms are Fin 2, the book's arm 1 being index 0; rounds are Fin T. The prior is a probability measure on mean vectors supported on a finite set F⊆[0,1]2F \subseteq [0,1]^2F⊆[0,1]2, with μ10≥μ20\mu^0_1 \ge \mu^0_2μ10​≥μ20​ as a hypothesis; the reward family is mission III's RewardFamily (finitely many values, mean ν\nuν for ν∈[0,1]\nu \in [0,1]ν∈[0,1]). BIC is defined on a joint law of (μ,record)(\mu, \text{record})(μ,record) of the run in which every agent complies, with the recommendation of each round read off the record; the compliance event Et−1E_{t-1}Et−1​ of (11.1) is the sure event of that law, which is the standard reading of "the agents believe all previous agents complied". For a bandit policy the law is mission III's jointMeasure. Conditional expectations are written as finite sums over FFF, so there are no integrals and no integrability side conditions; a posterior mean off the support is a junk 000 that never enters a theorem. GREEDY allows arbitrary tie-breaking; HiddenExploration's exploitation branch breaks ties toward arm 1 as Algorithm 11.1 does; the tie convention of Theorem 11.19 is the strict form of BIC for arm 2. The law of RepeatedHE is an explicit finitely supported measure, μ\muμ and record weighted by the prior times the product of the round probabilities (initial rounds forced to arm 1, then the ε\varepsilonε-coin, ALG\mathrm{ALG}ALG's kernel on its own history, or the exploitation arm, then DμatD_{\mu_{a_t}}Dμat​​​); it is written this way because ALG\mathrm{ALG}ALG is fed a history of variable length. Two conditions are stated exactly as printed: Lemma 11.10 with ε≤13E[G1{G>0}]\varepsilon \le \frac13\mathbb{E}[G\mathbf 1\{G > 0\}]ε≤31​E[G1{G>0}] (non-strict, checked at equality) and Theorem 11.15 with the strict inequality.

Trivializations are excluded: ε>0\varepsilon > 0ε>0 throughout; the BIC condition is asserted only where the recommendation has positive probability, and the sums in it are over the finite support, so an unsatisfiable hypothesis cannot hide in a measure-zero set. Welcome contributions: the optional-stopping argument on jointMeasure, the identification of explPostMean with the conditional expectation given the exploration data, the Bayes-rule algebra behind Lemma 11.10, and the counting lemmas on heRecords.

Selected references

  • A. Slivkins, Introduction to Multi-Armed Bandits, Foundations and Trends in Machine Learning 12(1-2), 2019, Chapter 11. arXiv:1904.07272, doi:10.1561/2200000068
  • I. Kremer, Y. Mansour, M. Perry, Implementing the "Wisdom of the Crowd", Journal of Political Economy 122(5), 2014. doi:10.1086/676597
  • Y. Mansour, A. Slivkins, V. Syrgkanis, Bayesian Incentive-Compatible Bandit Exploration, Operations Research 68(4), 2020 (EC 2015). doi:10.1287/opre.2019.1919
  • E. Kamenica, M. Gentzkow, Bayesian Persuasion, American Economic Review 101(6), 2011. doi:10.1257/aer.101.6.2590
  • M. Sellke, A. Slivkins, The Price of Incentivizing Exploration: A Characterization via Thompson Sampling and Sample Complexity, Operations Research 71(5), 2023. doi:10.1287/opre.2022.2401
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Mechanism DesignOperations Research·Captain: naimengye

The Theory and Practice of Revenue Management IV: AuctionsTextbook

Why a reserve price, and why it does not matter which auction

Airlines selling last seats, Priceline's name-your-own-price, procurement of supply contracts: Chapter 6 of Talluri and van Ryzin's The Theory and Practice of Revenue Management (2004) treats auctions as pricing mechanisms and asks what revenue they earn and how to design them. Its centre is Myerson's (1981) theory for independent private values: whatever the mechanism, so long as bidders with higher valuations are more likely to win and the lowest type gains nothing, the firm's expected revenue is the expected virtual value ∑iJ(vi)yi(v)\sum_i J(v_i) y_i(v)∑i​J(vi​)yi​(v) of the winners, with J(v)=v−(1−F(v))/f(v)J(v) = v - (1 - F(v))/f(v)J(v)=v−(1−F(v))/f(v) (Theorem 6.1, the revenue equivalence theorem). Maximizing that expression pointwise gives the optimal auction: the standard first- or second-price auction with a reserve price v∗v^*v∗ at the zero of JJJ (Theorem 6.2). This mission formalizes the second-price form of Theorem 6.2 as its goal, with the dominant-strategy and first-price equilibria of the informal analysis, Theorem 6.1, the optimal allocation and Proposition 6.1 on list prices as supporting results.

Setting

NNN customers have i.i.d. valuations on [0,vˉ][0, \bar v][0,vˉ] with a continuously differentiable, strictly increasing distribution FFF and positive density fff (PrivateValues, IsRegular); the joint law is the product measure (joint). A direct-revelation mechanism (Mechanism) maps reported valuations to allocations yi(v)∈{0,1}y_i(v) \in \{0, 1\}yi​(v)∈{0,1}, at most CCC units in total, and payments pi(v)p_i(v)pi​(v). For a report www by customer iii, Pi(w)P_i(w)Pi​(w) is the win probability, Ri(w)R_i(w)Ri​(w) the expected payment and Si(w)=wPi(w)−Ri(w)S_i(w) = w P_i(w) - R_i(w)Si​(w)=wPi​(w)−Ri​(w) the surplus (winProb, expPayment, expSurplus); incentive compatibility, Si(w)≥wPi(w′)−Ri(w′)S_i(w) \ge w P_i(w') - R_i(w')Si​(w)≥wPi​(w′)−Ri​(w′), is the equilibrium condition of the direct mechanism (IsIncentiveCompatible). The chapter's mechanisms are the CCC-unit second-price auction with reserve price rrr (secondPriceReserve: the CCC highest valuations above rrr win and pay the larger of rrr and the highest losing valuation), the list-price mechanism for N≤CN \le CN≤C (listPrice), and the single-unit first-price auction with its equilibrium bid b∗(v)=v−∫0vP(s) ds/P(v)b^*(v) = v - \int_0^v P(s)\,ds / P(v)b∗(v)=v−∫0v​P(s)ds/P(v), P=FN−1P = F^{N-1}P=FN−1 (firstPriceBid).

Formalization targets

Goal: Theorem 6.2

With JJJ strictly increasing (Assumption 7.2) and v∗v^*v∗ its zero, the CCC-unit second-price auction with reserve price v∗v^*v∗ is a feasible, incentive-compatible mechanism with monotone allocations and zero surplus at zero, and its expected revenue is at least that of every such mechanism: reserve_price_auction_optimal.

Supporting targets

Bidding one's valuation is dominant in the second-price auction (Sect. 6.2.2.1); the bid (6.4) solves the first-order condition (6.3), is a symmetric equilibrium of the first-price auction and shades below the valuation (Sect. 6.2.2.2); Theorem 6.1, revenue equals expected virtual surplus and each expected payment is wPi(w)−∫0wPiw P_i(w) - \int_0^w P_iwPi​(w)−∫0w​Pi​; the pointwise optimal allocation of Sect. 6.2.5; and Proposition 6.1, a list price at v∗v^*v∗ is optimal when N≤CN \le CN≤C.

Proposition 6.2 (asymptotic optimality of list prices, a law-of-large-numbers statement about scaled auctions), the first-price form of Theorem 6.2 with its equilibrium (6.9) stated without proof, and the dynamic, replenishment and network auctions of Sects. 6.3-6.5 (Propositions 6.3-6.11, from Vulcano, van Ryzin and Maglaras and from Cooper and Menich) are not targets of this mission.

Significance

Theorem 6.1 is the tool that lets revenue be computed from allocations alone, which is why the first- and second-price auctions of Examples 6.1-6.3 earn the same (N−1)/(N+1)(N-1)/(N+1)(N−1)/(N+1) and why any dynamic pricing scheme that ends with the same winners earns the same as the optimal auction (Sect. 6.2.6.3). Theorem 6.2 says a firm with private-value customers cannot do better than a standard auction with the right reserve price, and Proposition 6.1 that with enough capacity a list price already does it: auctions are a small-numbers phenomenon. These are the foundations on which the chapter's dynamic auctions and the list-price comparisons of Sects. 6.3-6.4 rest, and Myerson's optimal auction has no machine-checked proof in its multi-unit form.

Difficulty

Theorem 6.1 is an envelope argument in measure-theoretic clothing: incentive compatibility gives the two-sided inequalities of Appendix 6.A, monotonicity of PiP_iPi​ makes SiS_iSi​ convex with derivative PiP_iPi​ almost everywhere, so Si(w)=∫0wPiS_i(w) = \int_0^w P_iSi​(w)=∫0w​Pi​, and then an integration by parts against the density converts ∫(wPi(w)−Si(w))f(w) dw\int (w P_i(w) - S_i(w)) f(w)\,dw∫(wPi​(w)−Si​(w))f(w)dw into ∫J(w)Pi(w)f(w) dw\int J(w) P_i(w) f(w)\,dw∫J(w)Pi​(w)f(w)dw; the win probabilities are integrals over a product measure with one coordinate replaced, and Fubini is needed to return to E[J(vi)yi(v)]\mathbb E[J(v_i) y_i(v)]E[J(vi​)yi​(v)]. The goal then needs the reserve-price auction shown incentive compatible (a dominant-strategy argument on the threshold payment), measurable, monotone and with zero surplus at zero, and the pointwise optimal allocation integrated. The first-price item is calculus on an interval integral with a vanishing denominator at 000 and a monotone comparative-statics argument for the equilibrium inequality.

Formalization scope

Mechanisms are direct-revelation mechanisms on [0,vˉ]N[0, \bar v]^N[0,vˉ]N, as the book reduces to in Sect. 6.2.3.1; expectations over the other customers are integrals over the joint law with customer iii's coordinate overwritten by the report. Payments are assumed bounded on reports in [0,vˉ]N[0, \bar v]^N[0,vˉ]N (not on all of RN\mathbb R^NRN, where the second-price payment is unbounded) and the rules measurable. Ties in the second-price auction are broken by index, a null event, and when every customer wins the losing supremum is 000 so the winner pays the reserve. Theorem 6.2 is stated for the second-price auction; the first-price version with reserve price, whose equilibrium (6.9) the book asserts without proof, is left out and noted. Optimality is over mechanisms satisfying conditions (i) and (ii) of Theorem 6.1 and incentive compatibility, which is the class the book compares against. The virtual value's zero v∗v^*v∗ is a parameter with J(v∗)=0J(v^*) = 0J(v∗)=0 rather than the maximum of (6.8), which under strict monotonicity is the same point.

Selected references

  • K. T. Talluri and G. J. van Ryzin, The Theory and Practice of Revenue Management, Kluwer/Springer, 2004, Chapter 6. https://doi.org/10.1007/b139000
  • R. B. Myerson, Optimal auction design, Mathematics of Operations Research 6(1), 1981. https://doi.org/10.1287/moor.6.1.58
  • J. G. Riley and W. F. Samuelson, Optimal auctions, American Economic Review 71(3), 1981. https://www.jstor.org/stable/1802786
  • P. Klemperer, Auction theory: a guide to the literature, Journal of Economic Surveys 13(3), 1999. https://doi.org/10.1111/1467-6419.00083
  • W. Vickrey, Counterspeculation, auctions, and competitive sealed tenders, Journal of Finance 16(1), 1961. https://doi.org/10.1111/j.1540-6261.1961.tb02789.x
  • E. Maskin and J. Riley, Optimal multi-unit auctions, in The Economics of Missing Markets, Information, and Games, Oxford University Press, 1989.
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Inventory Control VIII: The Clark-Scarf Decomposition for a Serial SystemTextbook

Safety stock in a chain

Chapter 10 of Axsäter's Inventory Control turns to reorder points and safety stocks in multi-echelon systems, where the installations cannot be treated separately: a large stock downstream lets an upstream site run lean, and a long upstream lead-time argues for stock at the top. The best-known exact technique for serial systems is the decomposition of Clark and Scarf (1960), which the book presents in the infinite-horizon form of Federgruen and Zipkin (1984). It is also where the echelon stock measure comes from. The section's argument is short and self-contained, and its conclusion is a complete description of the optimal policy for a two-level serial system: order-up-to levels at both installations, one of them a newsboy solution, the other the minimizer of a convex function in which upstream shortages appear as an induced cost. It is the capstone of Chapter 10.

Setting

Installation 1 faces normally distributed period demand with mean μ\muμ and standard deviation σ\sigmaσ, independent across periods, so the demand over nnn periods, D(n)D(n)D(n), is normal with mean nμn\munμ and standard deviation n σ\sqrt n\,\sigman​σ. Installation 1 replenishes from installation 2 with lead-time L1L_1L1​ periods; installation 2 replenishes from an outside supplier with infinite supply and lead-time L2L_2L2​. Demand that cannot be met is backordered. Costs per unit and period are echelon holding costs e1,e2≥0e_1, e_2 \ge 0e1​,e2​≥0, so the installation holding costs are h1=e1+e2h_1 = e_1 + e_2h1​=e1​+e2​ and h2=e2h_2 = e_2h2​=e2​, and a shortage cost b1b_1b1​ at installation 1; there are no ordering costs. Events in a period occur in the order: installation 2 orders, its delivery arrives, installation 1 orders, its delivery arrives, demand, cost evaluation.

Consider an arbitrary period ttt. After ordering, installation 2 has an echelon inventory position y2y_2y2​, and by the standard argument its echelon stock in period t+L2t + L_2t+L2​ is y2−D(L2)y_2 - D(L_2)y2​−D(L2​). Installation 1 then orders, realizing an echelon position y1y_1y1​ that cannot exceed what is available: y1≤y2−D(L2)y_1 \le y_2 - D(L_2)y1​≤y2​−D(L2​) (Eq. 10.1). Its inventory level after the demand in period t+L2+L1t + L_2 + L_1t+L2​+L1​ is y1−D(L1+1)y_1 - D(L_1+1)y1​−D(L1​+1). The expected period costs are C2=h2 E(y2−D(L2)−y1)C_2 = h_2\,\mathbb{E}(y_2 - D(L_2) - y_1)C2​=h2​E(y2​−D(L2​)−y1​) at installation 2 and C1=h1 E(y1−D(L1+1))++b1 E(y1−D(L1+1))−C_1 = h_1\,\mathbb{E}(y_1 - D(L_1+1))^{+} + b_1\,\mathbb{E}(y_1 - D(L_1+1))^{-}C1​=h1​E(y1​−D(L1​+1))++b1​E(y1​−D(L1​+1))− at installation 1, and the book reallocates the term −h2y1-h_2y_1−h2​y1​ to obtain

C~2(y2)=h2(y2−μ2′),C~1(y1)=e1y1−h1μ1′′+(h1+b1) E(y1−D(L1+1))−,\tilde C_2(y_2) = h_2(y_2 - \mu_2'), \qquad \tilde C_1(y_1) = e_1y_1 - h_1\mu_1'' + (h_1 + b_1)\,\mathbb{E}\big(y_1 - D(L_1+1)\big)^{-},C~2​(y2​)=h2​(y2​−μ2′​),C~1​(y1​)=e1​y1​−h1​μ1′′​+(h1​+b1​)E(y1​−D(L1​+1))−,

with μ2′=L2μ\mu_2' = L_2\muμ2′​=L2​μ and μ1′′=(L1+1)μ\mu_1'' = (L_1+1)\muμ1′′​=(L1​+1)μ. As a function of a free y^1\hat y_1y^​1​, C~1\tilde C_1C~1​ is the newsboy-type function C^1\hat C_1C^1​ of Eq. (10.6), minimized at the level S1=y^1∗S_1 = \hat y_1^{*}S1​=y^​1∗​ given by the fractile equation (10.8). Passing everything available up to S1S_1S1​ to installation 1, y1=min⁡{S1,y2−D(L2)}y_1 = \min\{S_1, y_2 - D(L_2)\}y1​=min{S1​,y2​−D(L2​)}, gives the total cost C^2(y2)\hat C_2(y_2)C^2​(y2​) of Eq. (10.9), whose minimizer S2=y2∗S_2 = y_2^{*}S2​=y2∗​ is the order-up-to level of installation 2.

Formalization targets

Goal — the decomposition

With S1S_1S1​ from (10.8) and S2S_2S2​ a minimizer of C^2\hat C_2C^2​: for every y2y_2y2​ and every allocation rule aaa with a(u)≤y2−ua(u) \le y_2 - ua(u)≤y2​−u and finite expected cost,

C^2(S2)  ≤  E[C~2(y2)+C~1(a(D(L2)))],\hat C_2(S_2) \;\le\; \mathbb{E}\big[\tilde C_2(y_2) + \tilde C_1(a(D(L_2)))\big],C^2​(S2​)≤E[C~2​(y2​)+C~1​(a(D(L2​)))],

and the order-up-to policy (S1,S2)(S_1, S_2)(S1​,S2​) attains C^2(S2)\hat C_2(S_2)C^2​(S2​).

Supporting targets

Eq. (10.3), the stage-1 period cost through the expected backorders; the reallocation (10.4)-(10.5), which leaves the total unchanged; the closed form (10.6) of C^1\hat C_1C^1​ through the loss function GGG; the convexity of C^1\hat C_1C^1​, its derivative (10.7), and the fractile characterization (10.8) of its minimizers; the pointwise rule that min⁡{S1,y2−u}\min\{S_1, y_2 - u\}min{S1​,y2​−u} is the cheapest feasible y1y_1y1​; the identity (10.9); and the convexity of C^2\hat C_2C^2​ (Problem 10.1) with the existence of its minimizer when e2>0e_2 > 0e2​>0.

Significance

The result itself. The decomposition reduces a two-dimensional stochastic control problem to two one-dimensional convex problems solved in sequence, from downstream to upstream, and it identifies the optimal policy class. The downstream level S1S_1S1​ is a newsboy solution with overage cost e1e_1e1​, the value added, and underage cost e2+b1e_2 + b_1e2​+b1​, and it is independent of the upstream installation altogether; the upstream level S2S_2S2​ sees the downstream installation only through the induced shortage cost, the last term of (10.9). The book notes the extensions the argument admits, to more echelons, to batch ordering at the top, and, via Rosling's equivalence, to assembly systems, and its Sect. 10.1.2 adapts it, now only approximately, to distribution systems under the balance assumption. Example 10.1 shows the typical outcome: the optimal average stock at the upstream installation is slightly negative.

Formalizing it. The section's mathematics is a chain of expectations under Gaussian laws and two convexity arguments. Formalizing it fixes what "optimal" means, a per-period comparison against every allocation rule, and separates the two convexity claims the book makes in one clause each. Nothing here is open; no statement has a machine-checked proof yet.

Difficulty

The pointwise allocation rule and the newsboy fractile are the same arguments as in the newsboy mission. The two places where work is needed are the identity (10.9), an expectation of a piecewise function split at u=y2−S1u = y_2 - S_1u=y2​−S1​, and the convexity of C^2\hat C_2C^2​, which requires seeing that x↦C^1(min⁡{S1,x})x \mapsto \hat C_1(\min\{S_1, x\})x↦C^1​(min{S1​,x}) is convex precisely because S1S_1S1​ is a minimizer of the convex C^1\hat C_1C^1​ (for any other cut-off the function is not convex), and that convexity is preserved by integrating against the law of D(L2)D(L_2)D(L2​), which needs the integrability of the linearly growing C^1\hat C_1C^1​. Existence of S2S_2S2​ then follows from the growth of C^2\hat C_2C^2​ at both ends, which comes from the asymptotics of the loss function: G(z)→0G(z) \to 0G(z)→0 as z→∞z \to \inftyz→∞ and G(z)+z→0G(z) + z \to 0G(z)+z→0 as z→−∞z \to -\inftyz→−∞.

Formalization scope

D(n)D(n)D(n) is csDemand mu sigma n, the Gaussian law newsboyDemand (n μ) (√n σ) from the newsboy mission, so the loss function GGG and its closed form are reused as references. The costs are parametrized by e1,e2,b1e_1, e_2, b_1e1​,e2​,b1​ with h1=e1+e2h_1 = e_1 + e_2h1​=e1​+e2​ and h2=e2h_2 = e_2h2​=e2​ written out; C~1\tilde C_1C~1​, C~2\tilde C_2C~2​, the pre-reallocation period cost and C^2\hat C_2C^2​ are Bochner integrals against these laws. Every statement assumes σ>0\sigma > 0σ>0; the goal and the convexity statements assume e1,e2≥0e_1, e_2 \ge 0e1​,e2​≥0 and b1>0b_1 > 0b1​>0, the book's cost signs. L2=0L_2 = 0L2​=0 is allowed and makes D(L2)D(L_2)D(L2​) a point mass, which is the setting of the book's Problem 10.2.

S1S_1S1​ enters as any solution of the fractile equation (10.8) and S2S_2S2​ as any minimizer of C^2\hat C_2C^2​; the other items show that both exist when e1,e2>0e_1, e_2 > 0e1​,e2​>0. When e1=0e_1 = 0e1​=0 the fractile is 111, no S1S_1S1​ exists, and the goal is vacuous, which is faithful: the book observes that then S1→∞S_1 \to \inftyS1​→∞ and installation 2 never carries stock. Symmetrically, when e2=0e_2 = 0e2​=0 and L2≥1L_2 \ge 1L2​≥1, C^2\hat C_2C^2​ decreases towards its infimum without attaining it, so no S2S_2S2​ exists and the goal is again vacuous: with free upstream holding the optimal y2y_2y2​ is unbounded. Allocation rules are arbitrary functions of the realized D(L2)D(L_2)D(L2​) with an integrability hypothesis; without it Lean's integral of a non-integrable cost would be 000 and could undercut C^2(S2)\hat C_2(S_2)C^2​(S2​), which is negative in Example 10.1's stage-1 term.

What is not modelled is the infinite-horizon dynamic problem: the book's optimality claim is made period by period, and the passage to the stationary policy rests on the remark that the outside supplier has infinite supply, so the same y2y_2y2​ can be chosen in every period. The definitions are reusable for the three-echelon extension and for the distribution system of Sect. 10.1.2; contributions formalizing Problem 10.2 (L2=0L_2 = 0L2​=0) as a first step are welcome.

Selected references

  • Sven Axsäter, Inventory Control, 3rd edition, International Series in Operations Research & Management Science 225, Springer, 2015, Sect. 10.1.1. DOI 10.1007/978-3-319-15729-0
  • Andrew J. Clark and Herbert Scarf, Optimal Policies for a Multi-Echelon Inventory Problem, Management Science 6(4), 1960, pp. 475-490. DOI 10.1287/mnsc.6.4.475
  • Awi Federgruen and Paul Zipkin, Computational Issues in an Infinite-Horizon, Multiechelon Inventory Model, Operations Research 32(4), 1984, pp. 818-836. DOI 10.1287/opre.32.4.818
  • Kaj Rosling, Optimal Inventory Policies for Assembly Systems under Random Demands, Operations Research 37(4), 1989, pp. 565-579. DOI 10.1287/opre.37.4.565
  • Geert-Jan van Houtum, Karl Inderfurth and Willem H. M. Zijm, Materials Coordination in Stochastic Multi-Echelon Systems, European Journal of Operational Research 95(1), 1996, pp. 1-23. DOI 10.1016/0377-2217(96)00080-8
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Fundamentals of Supply Chain Theory VI: Pooling and FlexibilityTextbook

Pooling as a design principle

A firm that holds inventory in five warehouses needs more safety stock than one that holds the same inventory in one warehouse, because the demands of five regions do not all run high at once. Eppen (1979) made this precise for a multi-location newsvendor and gave it its name, the risk-pooling effect. Chapter 7 of Snyder and Shen's Fundamentals of Supply Chain Theory (2019) follows the same idea through three settings in which pooling happens without physical consolidation: two retailers who ship stock to each other after seeing demand (transshipments, after Tagaras 1989), and plants that can each make more than one product (process flexibility, after Jordan and Graves 1995). The chapter's capstone is the theorem of Simchi-Levi and Wei (2012) that, among designs in which every plant makes two products and every product is made at two plants, a single long chain through all of them is best. This mission formalizes the chapter's numbered results, with that theorem as its goal.

Setting

Risk pooling. NNN distribution centers face normally distributed per-period demands Di∼N(μi,σi2)D_i \sim N(\mu_i, \sigma_i^2)Di​∼N(μi​,σi2​) with correlation coefficients ρij\rho_{ij}ρij​, and each runs a base-stock policy with holding cost hhh and backorder cost ppp per unit per period, so its optimal expected cost is the optimal newsvendor cost optNvCost h p D, the infimum over base-stock levels SSS of E[h(S−D)++p(D−S)+]\mathbb{E}[h(S - D)^+ + p(D - S)^+]E[h(S−D)++p(D−S)+]. Merging the centers gives one facing the total demand, normal with mean ∑iμi\sum_i \mu_i∑i​μi​ and variance σ02=∑i∑jσiσjρij\sigma_0^2 = \sum_i \sum_j \sigma_i \sigma_j \rho_{ij}σ02​=∑i​∑j​σi​σj​ρij​ (pooledVariance).

Transshipments. Two retailers i,ji, ji,j with base-stock levels Si,SjS_i, S_jSi​,Sj​ face independent demands. After demand is observed, under complete pooling the retailer with a surplus sends the retailer with a shortage Yji=min⁡{Sj−Dj, Di−Si}Y_{ji} = \min\{S_j - D_j,\ D_i - S_i\}Yji​=min{Sj​−Dj​, Di​−Si​} units (transship), and nothing moves otherwise. The type-1 service level is the probability of no stockout, αi0=Pr⁡[Di≤Si]\alpha^0_i = \Pr[D_i \le S_i]αi0​=Pr[Di​≤Si​] without and αi=Pr⁡[Di−Si≤Yji]\alpha_i = \Pr[D_i - S_i \le Y_{ji}]αi​=Pr[Di​−Si​≤Yji​] with transshipments; the type-2 service level is the fill rate, one minus expected unmet demand over expected demand, βi0\beta^0_iβi0​ and βi\beta_iβi​ likewise.

Process flexibility. A flexibility design on nnn products and nnn plants is a set EEE of (product, plant) pairs, an edge (i,j)(i, j)(i,j) meaning plant jjj can make product iii. Given a demand realization ddd and a common plant capacity CCC, the performance P(d,E)P(d, E)P(d,E) (perf) is the maximum sales obtainable by assigning production along the edges of EEE without exceeding any capacity or demand, the linear program (7.22) to (7.26). A balanced system (BalancedSystem) has equal capacities and an exchangeable demand vector, one whose joint law is invariant under permutations of the products, and [E]=E[P(D,E)][E] = \mathbb{E}[P(D, E)][E]=E[P(D,E)] is the expected performance (expPerf). The named designs are the dedicated design Dn={(i,i)}D_n = \{(i, i)\}Dn​={(i,i)}, the long chain CnC_nCn​ in which plant jjj also makes product j+1j + 1j+1 (and plant nnn makes product 111), the open chain LkL_kLk​ obtained from CkC_kCk​ by deleting the edge (1,k)(1, k)(1,k), and LknL^n_kLkn​, the open chain on the first kkk pairs together with the dedicated edges of the rest. A 2-flexibility design (TwoFlex) is one in which every product has exactly two plants and every plant exactly two products; CnC_nCn​ is one, and so is any union of disjoint shorter chains.

Formalization targets

Goal: Theorem 7.9

For a balanced system of size n≥2n \ge 2n≥2 with exchangeable demand,

Cn∈arg⁡max⁡A∈F2[A],C_n \in \arg\max_{A \in \mathcal{F}_2} [A],Cn​∈argA∈F2​max​[A],

that is, CnC_nCn​ is a 2-flexibility design and [A]≤[Cn][A] \le [C_n][A]≤[Cn​] for every 2-flexibility design AAA. This is long_chain_optimal.

Supporting targets

The chapter's route to the goal: Lemma 7.5, supermodularity of sales in the flexible edges of the long chain for every realization, P(d,E)+P(d,E∖{α,β})≥P(d,E∖{α})+P(d,E∖{β})P(d, E) + P(d, E \setminus \{\alpha, \beta\}) \ge P(d, E \setminus \{\alpha\}) + P(d, E \setminus \{\beta\})P(d,E)+P(d,E∖{α,β})≥P(d,E∖{α})+P(d,E∖{β}) for E⊆CnE \subseteq C_nE⊆Cn​; Corollary 7.6, the same in expectation; Lemma 7.7, the increments [Lk+1n]−[Lkn][L^n_{k+1}] - [L^n_k][Lk+1n​]−[Lkn​] are nondecreasing in kkk, ending with [Cn]−[Lnn][C_n] - [L^n_n][Cn​]−[Lnn​]; and Lemma 7.8, [Cn]=n([Ln]−[Ln−1])[C_n] = n([L_n] - [L_{n-1}])[Cn​]=n([Ln​]−[Ln−1​]).

Risk pooling, Theorem 7.1: gC∗≤gD∗g^*_C \le g^*_DgC∗​≤gD∗​, the optimal cost of the merged center is at most the sum of the optimal costs of the separate ones, with the covariance inequality ∑i∑jσiσjρij≤∑iσi\sqrt{\sum_i\sum_j \sigma_i\sigma_j\rho_{ij}} \le \sum_i \sigma_i∑i​∑j​σi​σj​ρij​​≤∑i​σi​ as a separate lemma.

Transshipments, Theorems 7.2 to 7.4: αi=αi0+∣∂E[Yji]/∂Si∣\alpha_i = \alpha^0_i + |\partial\mathbb{E}[Y_{ji}]/\partial S_i|αi​=αi0​+∣∂E[Yji​]/∂Si​∣, βi=βi0+E[Yji]/E[Di]\beta_i = \beta^0_i + \mathbb{E}[Y_{ji}]/\mathbb{E}[D_i]βi​=βi0​+E[Yji​]/E[Di​], and all four post-transshipment service levels are nondecreasing in SiS_iSi​.

Significance

Theorem 7.9 is the analytical answer to a question that had been settled only by simulation: Jordan and Graves reported that one chain through all plants achieves nearly twice the sales benefit of three short chains with the same number of edges, and Simchi-Levi and Wei proved that no arrangement of the same edge budget does better. It is the justification for the chaining guideline used in automotive and semiconductor capacity planning, and Lemma 7.8, which expresses the long chain through open chains, is what makes the long chain's performance computable by a greedy pass. Theorem 7.1 is the quantitative basis for consolidation decisions and for postponement, since a generic product is pooled inventory. Theorems 7.2 to 7.4 quantify what transshipments buy in service, which is the argument for allowing them despite their cost.

None of these results has a machine-checked proof. The book proves Lemma 7.7, Lemma 7.8 and Theorem 7.9 in full given Lemma 7.5, which it cites to Simchi-Levi and Wei, and omits the proofs of Theorems 7.3 and 7.4 and the identity (7.30) behind Lemma 7.8. Formalizing Lemma 7.5 and (7.30) means formalizing the structure of maximum flows on a cycle, which is reusable for the later results of Simchi-Levi and Wei on the long chain's performance relative to full flexibility and for the multi-echelon flexibility models the chapter cites.

Difficulty

The obvious approach to Theorem 7.9 is to compare CnC_nCn​ with an arbitrary 2-flexibility design directly. Nothing in the definitions supports that: the two designs share no structure beyond their degree sequences. The book's argument instead routes everything through the long chain's own edges. Lemma 7.5 gives supermodularity only for subsets of CnC_nCn​, and the decomposition of an arbitrary 2-flexibility design into disjoint cycles, each a relabeled long chain on a subsystem, is what allows the comparison. A solver must therefore prove that a 2-regular bipartite graph is a disjoint union of even cycles, that exchangeability makes every relabeling of a cycle worth the same as CnjC_{n_j}Cnj​​ on its subsystem, and that the performance of a disjoint union is the sum of the performances of its parts.

Lemma 7.5 itself is where the combinatorics lives. It says that on the cycle CnC_nCn​ the maximum flow is supermodular in the flexible edges, and the proof in Simchi-Levi and Wei goes through the structure of augmenting paths on a cycle. The natural first idea, that supermodularity follows from some general property of maximum flows, is false: maximum flow is not supermodular in arbitrary edge sets, and the lemma is specific to subsets of a single cycle.

Lemma 7.7 is where exchangeability is used, and it is used in a way that is easy to state and tedious to formalize: removing the edge (2,1)(2, 1)(2,1) from Lk+1nL^n_{k+1}Lk+1n​ leaves a design that is LknL^n_kLkn​ only after the pair 111 is moved to the end, so the argument needs the invariance of [E][E][E] under relabeling the products and plants by a common permutation. The book notes that Lemma 7.7, unlike Lemma 7.5, is false realization by realization.

For the transshipment theorems, the book differentiates a density formula by Leibniz's rule. Under the weaker hypothesis stated here, laws without atoms and with finite means, the derivative of E[Yji]\mathbb{E}[Y_{ji}]E[Yji​] in SiS_iSi​ has to be obtained by dominated convergence from the pointwise derivative of a piecewise-linear function whose kinks lie on null sets.

Formalization scope

perf is a supremum over a set of reals, nonempty because y=0y = 0y=0 is feasible when d≥0d \ge 0d≥0 and C≥0C \ge 0C≥0, and bounded by ∑idi\sum_i d_i∑i​di​; the demand is nonnegative for every outcome and the capacity nonnegative in BalancedSystem, and Lemma 7.5 carries these as hypotheses. The supremum is attained, but the definition does not assert it. Expected performance is a Lebesgue integral; the demand is integrable by assumption and P(d,E)P(d, E)P(d,E) is 111-Lipschitz in ddd, so the integrand is integrable, and a solver must prove this measurability rather than assume it.

Exchangeability is the equality of the laws of (Dσ(i))i(D_{\sigma(i)})_i(Dσ(i)​)i​ and (Di)i(D_i)_i(Di​)i​ for every permutation σ\sigmaσ. Designs are finite sets of pairs of Fin n; the chains are defined with finRotate, so indices wrap modulo nnn and the closing edge of CnC_nCn​ is (1,n)(1, n)(1,n) in the book's numbering, which is the edge its proofs and Figure 7.3(c) use. Lemma 7.8 involves open chains on subsystems of sizes nnn and n−1n - 1n−1; these are designs on Fin k evaluated on the first kkk coordinates of the demand (subDemand, subPerf).

Theorem 7.1 states the optimal costs as infima of the newsvendor cost over all base-stock levels, on Mathlib's gaussianReal; a nonpositive pooled variance gives a degenerate law, for which the inequality still holds, so the statement is not trivialized by that convention. The transshipment theorems take the two demand laws as probability measures on R\mathbb{R}R with no atoms (Theorem 7.2) and finite, positive means; the quantity YjiY_{ji}Yji​ is defined for all outcomes and the service levels are probabilities and expectations under the product law.

The definition module is shared by all eleven items. Beyond the milestones, formalizing the identity (7.30) as its own lemma and the disjoint-union additivity of perf would be natural contributions.

Selected references

  • L. V. Snyder and Z.-J. M. Shen, Fundamentals of Supply Chain Theory, 2nd ed., Wiley, 2019, Chapter 7. https://doi.org/10.1002/9781119584445
  • G. D. Eppen, Effects of centralization on expected costs in a multi-location newsboy problem, Management Science 25(5), 1979. https://doi.org/10.1287/mnsc.25.5.498
  • G. Tagaras, Effects of pooling on the optimization and service levels of two-location inventory systems, IIE Transactions 21(3), 1989. https://doi.org/10.1080/07408178908966208
  • W. C. Jordan and S. C. Graves, Principles on the benefits of manufacturing process flexibility, Management Science 41(4), 1995. https://doi.org/10.1287/mnsc.41.4.577
  • D. Simchi-Levi and Y. Wei, Understanding the performance of the long chain and sparse designs in process flexibility, Operations Research 60(5), 2012. https://doi.org/10.1287/opre.1120.1082
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Fundamentals of Supply Chain Theory V: The Bullwhip EffectTextbook

Why orders swing more than sales

Procter & Gamble observed in the 1990s that the orders its distributors placed for diapers were far more variable than the retail sales of diapers, and that its own orders to suppliers were more variable still, although the end demand for diapers is about as stable as demand gets. The phenomenon, a growing amplification of variability as one moves upstream in a supply chain, is the bullwhip effect. Lee, Padmanabhan and Whang (1997) argued that it is not a symptom of irrational behaviour: four rational responses of an inventory manager to their own environment each produce it. Chapter 13 of Snyder and Shen's Fundamentals of Supply Chain Theory (2019) makes three of the four quantitative, following Chen, Drezner, Ryan and Simchi-Levi (2000) for demand signal processing, Lee et al. for the rationing game, and Cachon (1999) for order batching. This mission formalizes those three models and the theorems the chapter proves about them.

Setting

Demand signal processing. A retailer faces a demand process DtD_tDt​, t∈Zt \in \mathbb{Z}t∈Z, that follows the stationary first-order autoregressive model

Dt=d+ρDt−1+ϵt,D_t = d + \rho D_{t-1} + \epsilon_t,Dt​=d+ρDt−1​+ϵt​,

with a constant d≥0d \ge 0d≥0, a correlation constant −1<ρ<1-1 < \rho < 1−1<ρ<1, and errors ϵt\epsilon_tϵt​ that are independent N(0,σ2)N(0, \sigma^2)N(0,σ2) variables, each independent of the demands before period ttt. In steady state every DtD_tDt​ has the law N(d/(1−ρ), σ2/(1−ρ2))N\big(d/(1-\rho),\ \sigma^2/(1-\rho^2)\big)N(d/(1−ρ), σ2/(1−ρ2)). The retailer replenishes with a lead time of LLL periods under a base-stock policy but does not know the demand parameters, so it estimates the lead-time demand from a moving average of the previous m≥1m \ge 1m≥1 demands:

μ^tL=Lm∑i=1mDt−i,σ^etL=C1m∑i=1met−i2,et=Dt−μ^t1,\hat\mu^L_t = \frac{L}{m}\sum_{i=1}^m D_{t-i}, \qquad \hat\sigma^L_{et} = C\sqrt{\frac{1}{m}\sum_{i=1}^m e_{t-i}^2}, \qquad e_t = D_t - \hat\mu^1_t,μ^​tL​=mL​i=1∑m​Dt−i​,σ^etL​=Cm1​i=1∑m​et−i2​​,et​=Dt​−μ^​t1​,

and sets the base-stock level St=μ^tL+zασ^etLS_t = \hat\mu^L_t + z_\alpha \hat\sigma^L_{et}St​=μ^​tL​+zα​σ^etL​, where zαz_\alphazα​ is a safety factor. The book writes the constant in σ^etL\hat\sigma^L_{et}σ^etL​ as CLρC_{L\rho}CLρ​ and does not give its form; here it is a free parameter CCC. Each period the retailer orders Qt=St−St−1+Dt−1Q_t = S_t - S_{t-1} + D_{t-1}Qt​=St​−St−1​+Dt−1​, which may be negative. In Lean the process is the structure AR1Demand, whose fields are the parameters, the errors, the demands, the recursion, the independence properties and the stationary law; muHat, err, sigmaHat, baseStock and order are the five quantities above.

Order batching. NNN retailers face independent N(μ,σ2)N(\mu, \sigma^2)N(μ,σ2) demands in every period and each orders once every R≥1R \ge 1R≥1 periods, the order being its demand over the previous RRR periods. The supplier's order in a given period is the total ordered by the retailers whose ordering day falls in that period. Three patterns are compared: random ordering, in which each retailer's day is uniform over the RRR days, so the number XXX of retailers ordering on a given day is binomial(N,1/R)(N, 1/R)(N,1/R); positively correlated ordering, in which all retailers order on the same day, so X=NX = NX=N with probability 1/R1/R1/R and 000 otherwise; and balanced ordering, in which the retailers are spread as evenly as possible, so with N=MR+kN = MR + kN=MR+k, 0≤k<R0 \le k < R0≤k<R, XXX is M+1M+1M+1 with probability k/Rk/Rk/R and MMM otherwise. The structure BatchOrders P N R mu sigma carries the demands, the ordering count XXX independent of them, and supplierOrder, the sum of the last RRR demands of retailers 1,…,X1, \dots, X1,…,X; each pattern enters a theorem as a hypothesis on the law of XXX.

Rationing game. Two identical retailers face single-period demand with distribution function FFF, holding cost hhh and stockout penalty ppp, so the newsvendor quantity Q∗Q^*Q∗ satisfies F(Q∗)=p/(h+p)F(Q^*) = p/(h+p)F(Q∗)=p/(h+p). With probability rrr the supplier can deliver only A1<2Q∗A_1 < 2Q^*A1​<2Q∗ units in total and allocates them pro rata to the orders, retailer 1 receiving A1Q1/(Q1+Q2)A_1 Q_1/(Q_1 + Q_2)A1​Q1​/(Q1​+Q2​); with probability 1−r1 - r1−r supply is unlimited. Retailer 1's expected cost when the retailers order Q1Q_1Q1​ and Q2Q_2Q2​ is

g1(Q1)=(1−r) nv(Q1)+r nv ⁣(A1Q1Q1+Q2),g_1(Q_1) = (1-r)\,\mathrm{nv}(Q_1) + r\,\mathrm{nv}\!\Big(\frac{A_1 Q_1}{Q_1 + Q_2}\Big),g1​(Q1​)=(1−r)nv(Q1​)+rnv(Q1​+Q2​A1​Q1​​),

with nv\mathrm{nv}nv the newsvendor cost; this is rationingCost.

Formalization targets

Goal: Theorem 13.2, demand signal processing

Var[Qt]Var[Dt]  ≥  1+(2Lm+2L2m2)(1−ρm),\frac{\mathrm{Var}[Q_t]}{\mathrm{Var}[D_t]} \;\ge\; 1 + \Big(\frac{2L}{m} + \frac{2L^2}{m^2}\Big)(1 - \rho^m),Var[Dt​]Var[Qt​]​≥1+(m2L​+m22L2​)(1−ρm),

with equality when zα=0z_\alpha = 0zα​=0. This is bullwhip_signal_processing. The bound exceeds 111 whenever L>0L > 0L>0, whatever the value of ρ\rhoρ: a lead time and a moving-average forecast are enough to produce the effect.

Supporting targets

The chapter's own route to the goal, each a milestone: the steady-state moments (13.2) to (13.4), E[Dt]=d/(1−ρ)\mathbb{E}[D_t] = d/(1-\rho)E[Dt​]=d/(1−ρ), Var[Dt]=σ2/(1−ρ2)\mathrm{Var}[D_t] = \sigma^2/(1-\rho^2)Var[Dt​]=σ2/(1−ρ2) and Cov[Dt,Dt−k]=ρkVar[Dt]\mathrm{Cov}[D_t, D_{t-k}] = \rho^k \mathrm{Var}[D_t]Cov[Dt​,Dt−k​]=ρkVar[Dt​]; the identity Qt=(1+L/m)Dt−1−(L/m)Dt−m−1+zα(σ^etL−σ^e,t−1L)Q_t = (1 + L/m) D_{t-1} - (L/m) D_{t-m-1} + z_\alpha(\hat\sigma^L_{et} - \hat\sigma^L_{e,t-1})Qt​=(1+L/m)Dt−1​−(L/m)Dt−m−1​+zα​(σ^etL​−σ^e,t−1L​); Lemma 13.1, Cov[Dt−i,σ^etL]=0\mathrm{Cov}[D_{t-i}, \hat\sigma^L_{et}] = 0Cov[Dt−i​,σ^etL​]=0 for 1≤i≤m1 \le i \le m1≤i≤m; the vanishing of the cross term (13.12); and the variance of the demand part, (1+(2L/m+2L2/m2)(1−ρm))Var[Dt]\big(1 + (2L/m + 2L^2/m^2)(1 - \rho^m)\big)\mathrm{Var}[D_t](1+(2L/m+2L2/m2)(1−ρm))Var[Dt​].

Order batching, Theorem 13.4: under the three patterns the supplier's order has mean NμN\muNμ and

Var[Qtc]≥Var[Qtr]≥Var[Qtb]≥Nσ2,\mathrm{Var}[Q^c_t] \ge \mathrm{Var}[Q^r_t] \ge \mathrm{Var}[Q^b_t] \ge N\sigma^2,Var[Qtc​]≥Var[Qtr​]≥Var[Qtb​]≥Nσ2,

through the three variance formulas Nσ2+μ2N(R−1)N\sigma^2 + \mu^2 N(R-1)Nσ2+μ2N(R−1), Nσ2+μ2N2(R−1)N\sigma^2 + \mu^2 N^2 (R-1)Nσ2+μ2N2(R−1) and Nσ2+μ2k(R−k)N\sigma^2 + \mu^2 k(R-k)Nσ2+μ2k(R−k).

The rationing game, Theorem 13.3: if Q>0Q > 0Q>0 is a symmetric Nash equilibrium, that is, QQQ minimizes g1g_1g1​ over positive order quantities when the other retailer orders QQQ, then Q>Q∗Q > Q^*Q>Q∗.

Significance

The three theorems are the quantitative core of the chapter. Theorem 13.2 is the single-stage building block that Theorems 13.6 and 13.7 later iterate along a serial chain, giving the product-form and the exponential lower bounds on the amplification at stage kkk; its comparative statics, the bound decreasing in mmm and increasing in LLL, are the basis of the remedies the chapter recommends (shorter lead times, smoother forecasts, sharing point-of-sale data). Theorem 13.4 ranks the ordering patterns and justifies the advice to balance ordering days when batching cannot be avoided. Theorem 13.3 shows that pro-rata rationing alone inflates orders; the book is careful to note that inflated orders are not by themselves inflated variances, and that the variance statement for this model is due to Rong, Shen and Snyder (2017).

None of these results has a machine-checked proof. The book's proofs of Theorems 13.2 and 13.4 are complete but informal, and the proof of Lemma 13.1 is omitted with a citation to Ryan's 1997 thesis; formalizing it requires a self-contained argument. The variance decomposition of QtQ_tQt​ and the conditioning argument for Theorem 13.4 are reusable for the multistage results of Sect. 13.2.5, which are natural follow-up missions on the same definitions.

Difficulty

The obvious computation of Var[Qt]\mathrm{Var}[Q_t]Var[Qt​] expands the order into its demand part and its safety-stock part and hopes the cross term disappears. It does, but not for a reason visible in the formulas: σ^etL\hat\sigma^L_{et}σ^etL​ is a square root of a sum of squares of forecast errors, a nonlinear function of m+mm + mm+m demands, and its covariance with a single demand is zero only because the errors are jointly Gaussian with mean zero and σ^\hat\sigmaσ^ is an even function of them, so the covariance is the expectation of an odd function of a centred Gaussian vector. That is Lemma 13.1, and the vanishing of the cross term needs two further covariances, Cov[Dt−1,σ^e,t−1L]\mathrm{Cov}[D_{t-1}, \hat\sigma^L_{e,t-1}]Cov[Dt−1​,σ^e,t−1L​] and Cov[Dt−m−1,σ^etL]\mathrm{Cov}[D_{t-m-1}, \hat\sigma^L_{et}]Cov[Dt−m−1​,σ^etL​], which the book reduces to the lemma through the recursion (the second reduction divides by ρ\rhoρ) but which hold for every ρ\rhoρ by the same symmetry. A solver must set up the joint Gaussian structure of the demand vector and prove the odd-function argument; nothing in Mathlib does this directly.

The second obstacle is that the moments (13.2) to (13.4) are not assumed but derived: the structure carries the stationary law of each DtD_tDt​ and the independence of ϵt\epsilon_tϵt​ from the past, and the autocovariance ρkVar[Dt]\rho^k \mathrm{Var}[D_t]ρkVar[Dt​] has to be obtained from the recursion by induction on the lag, with integrability supplied by the Gaussian laws.

For Theorem 13.4 the work is the conditioning on XXX: given X=xX = xX=x the supplier's order is a sum of xRxRxR independent normals, so its conditional mean is xRμxR\muxRμ and conditional variance xRσ2xR\sigma^2xRσ2, and the total variance is E[Var[Q∣X]]+Var[E[Q∣X]]\mathbb{E}[\mathrm{Var}[Q \mid X]] + \mathrm{Var}[\mathbb{E}[Q \mid X]]E[Var[Q∣X]]+Var[E[Q∣X]]. The order is defined by a sum over retailers i<Xi < Xi<X, so the independence of XXX from the demands has to be used through the indicator structure rather than through a conditional-expectation library result.

For Theorem 13.3 the argument is a first-order condition. It requires that the newsvendor cost be differentiable with derivative (h+p)F(y)−p(h+p)F(y) - p(h+p)F(y)−p, which holds when FFF is continuous, and that the symmetric equilibrium be an interior minimizer, which is why Q>0Q > 0Q>0 and the minimization over Q1>0Q_1 > 0Q1​>0 are hypotheses.

Formalization scope

Time is indexed by Z\mathbb{Z}Z so that Dt−m−1D_{t-m-1}Dt−m−1​ exists for every ttt. AR1Demand asserts the recursion for every outcome, the independence of the whole error family, the independence of ϵt\epsilon_tϵt​ from (Ds)s<t(D_s)_{s < t}(Ds​)s<t​, and the stationary law of every DtD_tDt​; these are the "steady-state" assumptions the book makes in words. The structure is satisfiable: the stationary Gaussian AR(1) process on a full-measure set of error sequences has all these properties. The constant CLρC_{L\rho}CLρ​ is a free real parameter CCC; no theorem depends on its value.

The goal divides by Var[Dt]\mathrm{Var}[D_t]Var[Dt​], which is σ2/(1−ρ2)>0\sigma^2/(1-\rho^2) > 0σ2/(1−ρ2)>0 under the structure's hypotheses σ>0\sigma > 0σ>0 and ∣ρ∣<1|\rho| < 1∣ρ∣<1, so the ratio is a genuine quotient. Mathlib's ProbabilityTheory.variance and covariance are used; both are the ordinary real quantities for square-integrable variables, which every variable here is, σ^etL\hat\sigma^L_{et}σ^etL​ included.

In BatchOrders the demands are indexed by Fin N × Fin R, the count XXX is a natural-valued random variable bounded by NNN and independent of the demand family, and supplierOrder sums the RRR demands of retailers 1,…,X1, \dots, X1,…,X, the book's "without loss of generality" choice. The laws of XXX are hypotheses on point probabilities P.real {ω | X ω = j}; with R≥1R \ge 1R≥1 each of the three families of hypotheses is satisfiable by a structure with the corresponding law. The subtractions R−1R - 1R−1 and R−kR - kR−k are real.

In the rationing game the demand law is a probability measure on R\mathbb{R}R whose distribution function is continuous and strictly increasing on [0,∞)[0, \infty)[0,∞); the newsvendor loss is assumed integrable at every order quantity. The pro-rata allocation uses Lean's total division, which is never at 000 in the theorem since Q1+Q2>0Q_1 + Q_2 > 0Q1​+Q2​>0.

Beyond the ten milestones, the multistage Theorems 13.6 and 13.7 and the centralized-information bound of Theorem 13.5 are welcome as extensions on the same AR1Demand.

Selected references

  • L. V. Snyder and Z.-J. M. Shen, Fundamentals of Supply Chain Theory, 2nd ed., Wiley, 2019, Chapter 13. https://doi.org/10.1002/9781119584445
  • H. L. Lee, V. Padmanabhan and S. Whang, Information distortion in a supply chain: the bullwhip effect, Management Science 43(4), 1997. https://doi.org/10.1287/mnsc.43.4.546
  • F. Chen, Z. Drezner, J. K. Ryan and D. Simchi-Levi, Quantifying the bullwhip effect in a simple supply chain: the impact of forecasting, lead times, and information, Management Science 46(3), 2000. https://doi.org/10.1287/mnsc.46.3.436.12069
  • G. P. Cachon, Managing supply chain demand variability with scheduled ordering policies, Management Science 45(6), 1999. https://doi.org/10.1287/mnsc.45.6.843
  • Y. Rong, Z.-J. M. Shen and L. V. Snyder, The impact of ordering behavior on order-quantity variability: a study of forward and reverse bullwhip effects, Naval Research Logistics 64(1), 2017. https://doi.org/10.1002/nav.21757
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Markov Decision Processes III: The Average Reward Optimality Equation for Unichain ModelsTextbook

Motivation

When a system is controlled indefinitely and decisions are frequent — a router admitting packets, a queue accepting jobs, a machine being maintained — discounting future rewards is often unjustified, and what matters is the long-run average reward per period. Puterman's Chapter 8 (doi:10.1002/9780470316887) develops the theory of this criterion, and its central object is a single equation, the average reward optimality equation 0=max⁡a∈As{r(s,a)−g+∑jp(j∣s,a)h(j)−h(s)}0=\max_{a\in A_s}\{r(s,a)-g+\sum_jp(j\mid s,a)h(j)-h(s)\}0=maxa∈As​​{r(s,a)−g+∑j​p(j∣s,a)h(j)−h(s)}, whose unknowns are a scalar gain ggg and a bias function hhh. For unichain models, in which every stationary policy generates a Markov chain with one recurrent class, this equation determines the optimal gain and an optimal stationary policy. The results go back to Howard (Dynamic Programming and Markov Processes, MIT Press, 1960) for the recurrent case and to Blackwell (Discrete dynamic programming, Annals of Mathematical Statistics 33, 1962, doi:10.1214/aoms/1177704593) and Derman for the general finite case; Puterman's Section 8.4 proves them through the discounted theory of mission II, by letting the discount factor tend to one.

Setting

The model is stationary (Assumption 8.0.1): a finite set SSS of states, for each sss a finite nonempty set AsA_sAs​ of actions, a reward r(s,a)r(s,a)r(s,a) and transition probabilities p(j∣s,a)p(j\mid s,a)p(j∣s,a), none depending on the decision epoch. A policy π∈ΠHR\pi\in\Pi^{HR}π∈ΠHR may randomize and may depend on the whole history; the deterministic stationary policy d∞d^\inftyd∞ applies the decision rule d:S→Ad:S\to Ad:S→A at every epoch. Its transition matrix is Pd(i,j)=p(j∣i,d(i))P_d(i,j)=p(j\mid i,d(i))Pd​(i,j)=p(j∣i,d(i)).

For a policy π\piπ, vN+1π(s)=Esπ[∑t=1Nr(Xt,Yt)]v^\pi_{N+1}(s)=\mathbb E^\pi_s[\sum_{t=1}^Nr(X_t,Y_t)]vN+1π​(s)=Esπ​[∑t=1N​r(Xt​,Yt​)] is the expected reward over NNN epochs. Since the limit of N−1vN+1π(s)N^{-1}v^\pi_{N+1}(s)N−1vN+1π​(s) need not exist (Example 8.1.1), the chapter works with the lim sup and lim inf average rewards g+π(s)g^\pi_+(s)g+π​(s) and g−π(s)g^\pi_-(s)g−π​(s), and with g±∗(s)=sup⁡πg±π(s)g^*_\pm(s)=\sup_{\pi}g^\pi_\pm(s)g±∗​(s)=supπ​g±π​(s). A policy π∗\pi^*π∗ is average optimal when g−π∗(s)≥g+π(s)g^{\pi^*}_-(s)\ge g^\pi_+(s)g−π∗​(s)≥g+π​(s) for all sss and π\piπ, the strongest of the three criteria of Section 8.1.2.

The optimality residual is B(g,h)(s)=max⁡a∈As{r(s,a)−g+∑jp(j∣s,a)h(j)−h(s)}B(g,h)(s)=\max_{a\in A_s}\{r(s,a)-g+\sum_jp(j\mid s,a)h(j)-h(s)\}B(g,h)(s)=maxa∈As​​{r(s,a)−g+∑j​p(j∣s,a)h(j)−h(s)}, and the optimality equation is B(g,h)=0B(g,h)=0B(g,h)=0. A decision rule is hhh-improving when it attains max⁡a∈As{r(s,a)+∑jp(j∣s,a)h(j)}\max_{a\in A_s}\{r(s,a)+\sum_jp(j\mid s,a)h(j)\}maxa∈As​​{r(s,a)+∑j​p(j∣s,a)h(j)} at every state. A transition matrix is unichain when it consists of a single recurrent class plus a possibly empty set of transient states, and the MDP is unichain when PdP_dPd​ is unichain for every deterministic decision rule.

Formalization targets

Goal — Theorem 8.4.5 (printed p. 361)

For a finite unichain model: (a) some deterministic stationary policy is average optimal; (b) the optimality equation B(g∗,h∗)=0B(g^*,h^*)=0B(g∗,h∗)=0 has a solution, and (d) its scalar satisfies g+∗(s)=g−∗(s)=g∗g^*_+(s)=g^*_-(s)=g^*g+∗​(s)=g−∗​(s)=g∗ for every sss; (c) for every solution, every h∗h^*h∗-improving decision rule gives an average optimal stationary policy.

Theorem 8.4.1 (printed p. 356)

If B(g,h)≤0B(g,h)\le 0B(g,h)≤0 then g≥g+∗g\ge g^*_+g≥g+∗​; if B(g,h)≥0B(g,h)\ge 0B(g,h)≥0 then g≤sup⁡dg−d∞≤g−∗g\le\sup_{d}g^{d^\infty}_-\le g^*_-g≤supd​g−d∞​≤g−∗​; if B(g,h)=0B(g,h)=0B(g,h)=0 then g+∗=g−∗=gg^*_+=g^*_-=gg+∗​=g−∗​=g.

Theorem 8.4.3 (printed p. 358)

In a finite unichain model B(g,h)=0B(g,h)=0B(g,h)=0 has a solution, and every solution has the same ggg.

Theorem 8.4.4 (printed p. 361)

If B(g∗,h∗)=0B(g^*,h^*)=0B(g∗,h∗)=0 and d∗d^*d∗ is h∗h^*h∗-improving, then (d∗)∞(d^*)^\infty(d∗)∞ is average optimal.

Significance

Theorem 8.4.1(c) is what the source calls "one of the most important results for average reward models": a solution of the optimality equation with constant ggg pins down the optimal gain under every criterion at once, so that in finite unichain models the three optimality criteria of Section 8.1.2 coincide. Theorem 8.4.3 guarantees such a solution exists, and Theorem 8.4.4 reads an optimal policy off it. Together, Theorem 8.4.5 reduces the infinite-horizon average reward problem over all history-dependent randomized policies to a finite system of equations in (g,h)(g,h)(g,h), which is what policy iteration, value iteration and linear programming solve in Sections 8.5 to 8.8.

The results are classical and proved. Formalizing them fixes the chain-structure hypothesis in a checkable form and pins down which criterion "average optimal" means, two places where the literature is loose. The platform's MarkovDecisionProcesses series has the finite-horizon (mission I) and discounted (mission II) models; this mission adds the undiscounted stationary model, the gains, and the unichain classification, on which Chapter 9's multichain optimality equations and Chapter 10's sensitive discount optimality can be built.

Difficulty

The obvious argument for Theorem 8.4.3 is to take the discounted optimal value vλ∗v^*_\lambdavλ∗​ of mission II and let λ↑1\lambda\uparrow 1λ↑1. It fails as stated because vλ∗v^*_\lambdavλ∗​ blows up like (1−λ)−1(1-\lambda)^{-1}(1−λ)−1; what converges is the Laurent expansion vλd∞=(1−λ)−1ge+h+o(1)v^{d^\infty}_\lambda=(1-\lambda)^{-1}ge+h+o(1)vλd∞​=(1−λ)−1ge+h+o(1) of the value of a fixed stationary policy, Corollary 8.2.4, and that expansion needs the limiting matrix Pd∗P_d^*Pd∗​ and the deviation matrix HPdH_{P_d}HPd​​ of a unichain chain. So the proof must first develop the Markov chain theory of Section 8.2 and Appendix A, choose a subsequence of discount factors along which one policy is discount optimal (possible because DMDD^{MD}DMD is finite), and only then pass to the limit in the discounted optimality equation.

Theorem 8.4.1 looks elementary and hides the analytic step: iterating ge≥rd+(Pd−I)hge\ge r_d+(P_d-I)hge≥rd​+(Pd​−I)h along an arbitrary history-dependent policy and dividing by NNN requires the telescoping term N−1(PNπ−I)hN^{-1}(P^\pi_N-I)hN−1(PNπ​−I)h to vanish, which uses boundedness of hhh, and requires the reduction from history-dependent randomized to Markov randomized policies (Theorem 8.1.2). For Theorem 8.4.4 the step is Corollary 8.2.7, that rd−ge+(Pd−I)h=0r_d-ge+(P_d-I)h=0rd​−ge+(Pd​−I)h=0 forces the gain of d∞d^\inftyd∞ to be ggg, which is the multiplication by Pd∗P_d^*Pd∗​ that annihilates (Pd−I)(P_d-I)(Pd​−I).

The traps are in the definitions. Recurrence and the unichain property must be stated so that the source's Example 8.4.3 comes out as the book says — the policy using a1,1a_{1,1}a1,1​ has the absorbing state s2s_2s2​ as its single recurrent class — and the optimality residual must use the lim sup / lim inf gains, since a definition through a limit that need not exist would be a junk value on the policies of Example 8.1.1.

Formalization scope

State and action spaces are Fintypes and admissible actions are nonempty Finsets, as in missions I and II; the stationary model is a new structure because mission II's DiscountedMDP bundles a discount factor, and carries the same data otherwise. Policies are history-dependent and randomized, so "average optimal" has its full strength; a stationary policy is the deterministic one built from a decision rule. Expected total reward is defined by the policy evaluation recursion, as in the earlier missions, rather than through a measure on trajectories.

Gains are Filter.limsup and Filter.liminf of N−1vN+1π(s)N^{-1}v^\pi_{N+1}(s)N−1vN+1π​(s) on R\mathbb RR; these are the source's because the sequence is bounded by max⁡∣r∣\max|r|max∣r∣, and the suprema g±∗g^*_\pmg±∗​ over the nonempty family of policies are genuine real suprema for the same reason. The residual B(g,h)B(g,h)B(g,h) is a Finset.sup' over the admissible actions. Recurrence is "every state reachable from iii reaches iii" and unichain is "any two recurrent states communicate", the definitions of Appendix A for finite chains, applied to PdP_dPd​ for every admissible deterministic decision rule.

Restrictions relative to the printed text, all noted in the items: Theorem 8.4.1 is stated for finite SSS where the source says countable, since the chapter's standing assumption and the model are finite; the gain gd∞g^{d^\infty}gd∞ of a stationary policy in (8.4.5) is written as its lim inf gain, which equals it; and the chain ge=g∗=g+∗=g−∗ge=g^*=g^*_+=g^*_-ge=g∗=g+∗​=g−∗​ of (8.4.6) is stated through g+∗g^*_+g+∗​ and g−∗g^*_-g−∗​, since g∗g^*g∗ presupposes existing limits. Nothing is trivialized: the existential in Theorem 8.4.5(a) has to produce a decision rule, and B(g,h)=0B(g,h)=0B(g,h)=0 with a junk maximum is impossible since every AsA_sAs​ is nonempty. Welcome contributions beyond the milestones: Theorem 8.1.2 (reduction to Markov policies), Corollary 8.2.7 (the gain of a stationary policy from the evaluation equations), and the equivalence of the three optimality criteria in finite models.

Selected references

  • Martin L. Puterman, Markov Decision Processes: Discrete Stochastic Dynamic Programming, Wiley, 1994, Chapter 8. doi:10.1002/9780470316887
  • Ronald A. Howard, Dynamic Programming and Markov Processes, MIT Press, 1960.
  • David Blackwell, Discrete dynamic programming, Annals of Mathematical Statistics 33 (1962). doi:10.1214/aoms/1177704593
  • Cyrus Derman, Finite State Markovian Decision Processes, Academic Press, 1970.
  • Paul J. Schweitzer and Awi Federgruen, The functional equations of undiscounted Markov renewal programming, Mathematics of Operations Research 3 (1978). doi:10.1287/moor.3.4.308
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