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Machine LearningProbabilityStatistics·Captain: naimengye

Understanding Machine Learning XXV: PAC-BayesTextbook

Motivation

The MDL and Occam principles of Chapter 7 rank hypotheses by description length and pay for a hypothesis according to its rank. Chapter 31 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), generalizes this to the PAC-Bayesian approach of McAllester: prior knowledge is a prior distribution PPP over the class, the learner outputs a posterior QQQ, read as the randomized predictor that draws h∼Qh \sim Qh∼Q, and the price of QQQ is its Kullback–Leibler divergence from PPP. The PAC-Bayes theorem (Theorem 31.1) says that with probability 1−δ1 - \delta1−δ, simultaneously for every posterior, the generalization loss exceeds the training loss by at most (D(Q∥P)+ln⁡(m/δ))/(2(m−1))\sqrt{(D(Q\|P) + \ln(m/\delta))/(2(m-1))}(D(Q∥P)+ln(m/δ))/(2(m−1))​. Its proof is a compact and elegant argument: Markov's inequality for an exponential moment, a change of measure from QQQ to PPP by Jensen's inequality, an exchange of expectations that is possible because the prior does not depend on the sample, and a moment bound for the deviation of a single hypothesis. The bound suggests the learning rule of Remark 31.1, minimize LS(Q)L_S(Q)LS​(Q) plus the divergence penalty, which is regularized risk minimization in disguise, and for a finite class with a uniform prior it recovers an Occam-type bound (Exercise 2).

Setting

HHH is a measurable space of hypotheses, ℓ:H×Z→[0,1]\ell : H \times Z \to [0,1]ℓ:H×Z→[0,1] a jointly measurable loss, DDD a distribution over ZZZ, and PPP a prior probability measure on HHH. For a posterior QQQ, ℓ(Q,z)=Eh∼Q[ℓ(h,z)]\ell(Q, z) = \mathbb{E}_{h \sim Q}[\ell(h, z)]ℓ(Q,z)=Eh∼Q​[ℓ(h,z)], LD(Q)=Eh∼Q[LD(h)]L_D(Q) = \mathbb{E}_{h \sim Q}[L_D(h)]LD​(Q)=Eh∼Q​[LD​(h)] and LS(Q)=Eh∼Q[LS(h)]L_S(Q) = \mathbb{E}_{h \sim Q}[L_S(h)]LS​(Q)=Eh∼Q​[LS​(h)], and D(Q∥P)=Eh∼Q[ln⁡(dQ/dP)]D(Q\|P) = \mathbb{E}_{h \sim Q}[\ln(dQ/dP)]D(Q∥P)=Eh∼Q​[ln(dQ/dP)] is the Kullback–Leibler divergence, a real number when Q≪PQ \ll PQ≪P and the log-density is QQQ-integrable.

Formalization targets

Goal: Theorem 31.1

For m≥2m \ge 2m≥2 and δ∈(0,1)\delta \in (0,1)δ∈(0,1), with probability at least 1−δ1 - \delta1−δ over S∼DmS \sim D^mS∼Dm, every probability measure Q≪PQ \ll PQ≪P with finite divergence satisfies

LD(Q)≤LS(Q)+D(Q∥P)+ln⁡(m/δ)2(m−1).L_D(Q) \le L_S(Q) + \sqrt{\frac{D(Q\|P) + \ln(m/\delta)}{2(m-1)}}.LD​(Q)≤LS​(Q)+2(m−1)D(Q∥P)+ln(m/δ)​​.

Milestones

The identity Ez∼D[ℓ(Q,z)]=LD(Q)\mathbb{E}_{z \sim D}[\ell(Q, z)] = L_D(Q)Ez∼D​[ℓ(Q,z)]=LD​(Q) (§31.1); the moment bound ES[e2(m−1)Δ(h)2]≤m\mathbb{E}_S[e^{2(m-1)\Delta(h)^2}] \le mES​[e2(m−1)Δ(h)2]≤m of the proof (p. 417); Exercise 2, the bound for a finite class with the uniform prior.

Significance

PAC-Bayes bounds are among the tightest generalization bounds known in practice, and the reason is visible in Theorem 31.1: the complexity term is not a property of the class but of the posterior actually chosen, measured against a prior, so a learner that stays close to its prior generalizes even in a huge class. The theorem is the ancestor of a large literature (Seeger, Langford, Catoni, Maurer) and of modern nonvacuous bounds for neural networks. Formally it is a pleasant target: the change-of-measure inequality Eh∼Q[f(h)]−D(Q∥P)≤ln⁡Eh∼P[ef(h)]\mathbb{E}_{h \sim Q}[f(h)] - D(Q\|P) \le \ln\mathbb{E}_{h \sim P}[e^{f(h)}]Eh∼Q​[f(h)]−D(Q∥P)≤lnEh∼P​[ef(h)] is the Donsker–Varadhan inequality, of independent value, and the moment bound is a sharp sub-Gaussian fact. On the platform, the mission introduces Gibbs risks and the Kullback–Leibler divergence between measures on a class, ending the book's series with its last learning principle.

Difficulty

The Gibbs risk identity is Fubini for a bounded jointly measurable function. The moment bound is the delicate step: the book derives it from Hoeffding's tail bound through Exercise 1, whose one-sided hypothesis is not enough (a constant negative variable satisfies it with an unbounded moment), and even the two-sided tail integrates only to 2m−12m - 12m−1; the claim ≤m\le m≤m is nevertheless true, for instance by writing eaΔ2=Eg[e2a gΔ]e^{a\Delta^2} = \mathbb{E}_g[e^{\sqrt{2a}\,g\Delta}]eaΔ2=Eg​[e2a​gΔ] for a standard Gaussian ggg and applying Hoeffding's lemma to the sample mean, which gives ES[e2(m−1)Δ2]≤(1−(m−1)/m)−1/2=m\mathbb{E}_S[e^{2(m-1)\Delta^2}] \le (1 - (m-1)/m)^{-1/2} = \sqrt mES​[e2(m−1)Δ2]≤(1−(m−1)/m)−1/2=m​. Theorem 31.1 then follows the book: Markov's inequality on ef(S)e^{f(S)}ef(S) with f(S)=sup⁡Q(2(m−1)Eh∼QΔ(h)2−D(Q∥P))f(S) = \sup_Q(2(m-1)\mathbb{E}_{h \sim Q}\Delta(h)^2 - D(Q\|P))f(S)=supQ​(2(m−1)Eh∼Q​Δ(h)2−D(Q∥P)), the change of measure (31.2) by Jensen's inequality for ln⁡\lnln applied to the density dQ/dPdQ/dPdQ/dP (the Donsker–Varadhan inequality, which needs Q≪PQ \ll PQ≪P and an integrable log-density), the exchange of expectations (31.4) by Fubini, the moment bound, and finally Jensen for x2x^2x2 in (31.6); formally the supremum over all posteriors is handled by proving the bound for each QQQ on the event {S:Eh∼P[e2(m−1)Δ(h)2]≤m/δ}\{S : \mathbb{E}_{h \sim P}[e^{2(m-1)\Delta(h)^2}] \le m/\delta\}{S:Eh∼P​[e2(m−1)Δ(h)2]≤m/δ}, whose complement has probability at most δ\deltaδ by Markov, which sidesteps any measurability question about fff. Exercise 2 is the theorem with Q=δhQ = \delta_hQ=δh​, for which D(Q∥P)=ln⁡∣H∣D(Q\|P) = \ln|H|D(Q∥P)=ln∣H∣.

Formalization scope

The class is an arbitrary measurable space, priors and posteriors are probability measures on it, and Q(h)/P(h)Q(h)/P(h)Q(h)/P(h) is Mathlib's Radon–Nikodym derivative; the divergence is a Bochner integral, so the theorem quantifies over posteriors Q≪PQ \ll PQ≪P whose log-density is QQQ-integrable, exactly the posteriors with a finite divergence, for which the bound has content, and no junk value can make a case false. Posteriors may depend on the sample: the statement bounds the outer measure of the set of samples for which some admissible QQQ violates the bound. The loss is jointly measurable so that h↦LD(h)h \mapsto L_D(h)h↦LD​(h) and (S,h)↦LS(h)(S, h) \mapsto L_S(h)(S,h)↦LS​(h) are measurable and the Gibbs risks are genuine integrals; m≥2m \ge 2m≥2 is forced by the denominator 2(m−1)2(m-1)2(m−1). The moment bound is stated as the claim the proof needs rather than as Exercise 1, whose printed hypothesis is insufficient; the item text records this. Exercise 2 is stated as a simultaneous bound over the finite class, the form in which the theorem delivers it.

Not stated: Remark 31.1 (a learning rule, not a theorem), Exercise 1 as printed, and the second part of Exercise 2.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 31. doi:10.1017/CBO9781107298019
  • D. A. McAllester, Some PAC-Bayesian theorems, Machine Learning 37, 1999. doi:10.1023/A:1007618624809
  • D. A. McAllester, PAC-Bayesian stochastic model selection, Machine Learning 51, 2003. doi:10.1023/A:1021840411064
  • A. Maurer, A note on the PAC Bayesian theorem, arXiv:cs/0411099, 2004.
  • M. Seeger, PAC-Bayesian generalisation error bounds for Gaussian process classification, Journal of Machine Learning Research 3, 2002.
  • J. Langford, J. Shawe-Taylor, PAC-Bayes and margins, NIPS 2002.
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CombinatoricsMachine LearningOptimization·Captain: naimengye

Understanding Machine Learning XV: Neural NetworksTextbook

Motivation

A feedforward neural network is a directed acyclic graph of neurons, each computing a fixed scalar activation of a weighted sum of its inputs; fixing the graph and the activation and letting the weights vary gives a hypothesis class. Chapter 20 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), studies these classes through the book's three lenses. Approximation: every Boolean function is implemented by a network of depth 2 (Claim 20.1), but only at exponential size (Theorem 20.2), while a sign neuron implements conjunctions and disjunctions (Lemma 20.4), the bridge to Boolean circuits and hence to everything computable in bounded time. Estimation: the VC dimension of the class of sign networks over a graph with ∣E∣|E|∣E∣ edges is O(∣E∣log⁡∣E∣)O(|E|\log|E|)O(∣E∣log∣E∣) (Theorem 20.6), so the sample complexity is governed by the number of weights. Optimization: training is NP-hard even for tiny networks, and the practical answer is SGD with the gradient computed by backpropagation, whose correctness the chapter derives from the chain rule.

Setting

A layered graph has layers V0,…,VTV_0, \dots, V_TV0​,…,VT​, every edge joining Vt−1V_{t-1}Vt−1​ to VtV_tVt​; V0V_0V0​ holds the nnn inputs and a constant neuron outputting 111. With weights w:E→Rw : E \to \mathbb{R}w:E→R and an activation σ\sigmaσ, the outputs are computed layer by layer, at+1,i=∑j:(vt,j,vt+1,i)∈Ewt,i,j ot,ja_{t+1,i} = \sum_{j : (v_{t,j}, v_{t+1,i}) \in E} w_{t,i,j}\,o_{t,j}at+1,i​=∑j:(vt,j​,vt+1,i​)∈E​wt,i,j​ot,j​ and ot+1,i=σ(at+1,i)o_{t+1,i} = \sigma(a_{t+1,i})ot+1,i​=σ(at+1,i​). The class HV,E,σ={hV,E,σ,w:w:E→R}H_{V,E,\sigma} = \{h_{V,E,\sigma,w} : w : E \to \mathbb{R}\}HV,E,σ​={hV,E,σ,w​:w:E→R} (20.1); for binary classification the output layer is a single neuron and σ\sigmaσ is the sign function, so HV,E,sign⁡H_{V,E,\operatorname{sign}}HV,E,sign​ is a set of {±1}\{\pm1\}{±1}-valued predictors on Rn\mathbb{R}^nRn. The size of the network is ∣V∣|V|∣V∣, its depth TTT. The growth function τH(m)=max⁡∣C∣≤m∣HC∣\tau_H(m) = \max_{|C| \le m}|H_C|τH​(m)=max∣C∣≤m​∣HC​∣ extends to classes with any finite codomain (p. 275), and the proof of Theorem 20.6 uses two of its properties, stated as Exercises 3 and 4: the growth function of a product class is at most the product of the growth functions, and likewise for a composition class. For backpropagation the activation is any differentiable σ\sigmaσ and the loss is 12∥oT−y∥2\frac12\|o_T - y\|^221​∥oT​−y∥2; the backward pass sets δT=oT−y\delta_T = o_T - yδT​=oT​−y and δt=δt+1diag⁡(σ′(at+1))Wt\delta_t = \delta_{t+1}\operatorname{diag}(\sigma'(a_{t+1}))W_tδt​=δt+1​diag(σ′(at+1​))Wt​.

Formalization targets

Goal: Theorem 20.6

The VC dimension of HV,E,sign⁡H_{V,E,\operatorname{sign}}HV,E,sign​ is O(∣E∣log⁡∣E∣)O(|E|\log|E|)O(∣E∣log∣E∣). Explicitly, for a layered graph of depth at least 111 with a single output neuron,

VCdim⁡(HV,E,sign⁡)≤2∣E∣log⁡2(16∣E∣),\operatorname{VCdim}(H_{V,E,\operatorname{sign}}) \le 2|E|\log_2(16|E|),VCdim(HV,E,sign​)≤2∣E∣log2​(16∣E∣),

stated as: every m≤VCdim⁡m \le \operatorname{VCdim}m≤VCdim satisfies this bound (so the VC dimension is finite).

Milestones

Claim 20.1 (the depth-2 graph with ∣V1∣=2n+1|V_1| = 2^n + 1∣V1​∣=2n+1 whose sign class contains every function {±1}n→{±1}\{\pm1\}^n \to \{\pm1\}{±1}n→{±1}); Theorem 20.2 (every sign network implementing all functions {0,1}n→{0,1}\{0,1\}^n \to \{0,1\}{0,1}n→{0,1} has 2n/3≤2∣V∣2^{n/3} \le 2|V|2n/3≤2∣V∣); Lemma 20.4 (conjunction and disjunction as sign neurons); Exercise 4 (growth function of a composition); the correctness of backpropagation (§20.6: the partial derivative for the edge (vt,j,vt+1,i)(v_{t,j}, v_{t+1,i})(vt,j​,vt+1,i​) is δt+1,iσ′(at+1,i)ot,j\delta_{t+1,i}\sigma'(a_{t+1,i})o_{t,j}δt+1,i​σ′(at+1,i​)ot,j​). Further items: Exercise 3 (growth function of a product) and the intermediate bound τH(m)≤(em)∣E∣\tau_H(m) \le (em)^{|E|}τH​(m)≤(em)∣E∣ of the proof of Theorem 20.6.

Significance

Theorem 20.6 is the reason networks are learnable at all in the book's sense: by the fundamental theorem, a class with finite VC dimension is agnostic PAC learnable with sample complexity linear in that dimension, and here the dimension is essentially the number of tunable parameters. The proof technique, due to Kakade and Tewari's lecture notes, is a composition-and-product argument on growth functions that applies to any layered class of threshold units and is reusable well beyond this chapter. Theorem 20.2 is the matching negative fact on expressive power, and it is a corollary of the same bound: a class that shatters 2n2^n2n points needs Ω(2n)\Omega(2^n)Ω(2n) edges. Backpropagation's correctness is the one theorem about training the chapter can offer, given the hardness results, and it is the algorithm every practitioner runs.

Difficulty

Claim 20.1 and Lemma 20.4 are explicit constructions: the neuron gi(x)=sign⁡(⟨x,ui⟩−n+1)g_i(x) = \operatorname{sign}(\langle x, u_i\rangle - n + 1)gi​(x)=sign(⟨x,ui​⟩−n+1) detects x=uix = u_ix=ui​ because ⟨x,ui⟩≤n−2\langle x, u_i\rangle \le n - 2⟨x,ui​⟩≤n−2 otherwise, and the output neuron takes the disjunction; formally one must build the weight function and evaluate the forward pass on the 2n2^n2n inputs. Exercises 3 and 4 are counting: a restricted product is determined by its two restricted factors, and a restricted composition f2∘f1f_2 \circ f_1f2​∘f1​ on CCC is determined by f1∣Cf_1|_Cf1​∣C​ and f2∣f1(C)f_2|_{f_1(C)}f2​∣f1​(C)​, with ∣f1(C)∣≤∣C∣|f_1(C)| \le |C|∣f1​(C)∣≤∣C∣. Theorem 20.6 then needs: the class of one neuron is the class of homogenous halfspaces on its dt,id_{t,i}dt,i​ incoming coordinates, of VC dimension at most dt,id_{t,i}dt,i​ (Mission VI), Sauer's lemma in the form τ(m)≤(em)d\tau(m) \le (em)^{d}τ(m)≤(em)d for every m≥1m \ge 1m≥1 (Mission IV; for m≤dm \le dm≤d use 2m≤(em)m2^m \le (em)^m2m≤(em)m), the layer class as a product and the network as a composition of layer classes, and finally the arithmetic 2m≤(em)∣E∣⇒m≤2∣E∣log⁡2(16∣E∣)2^m \le (em)^{|E|} \Rightarrow m \le 2|E|\log_2(16|E|)2m≤(em)∣E∣⇒m≤2∣E∣log2​(16∣E∣), which replaces the book's appeal to Lemma A.2 (for m≥8∣E∣m \ge 8|E|m≥8∣E∣ one has ln⁡m≤mln⁡22∣E∣\ln m \le \frac{m\ln 2}{2|E|}lnm≤2∣E∣mln2​). Theorem 20.2 follows from the goal with ∣E∣≤∣V∣2|E| \le |V|^2∣E∣≤∣V∣2. Backpropagation is a chain-rule computation in a single real variable: the loss as a function of one weight is a composition of finitely many differentiable maps, and the derivative unwinds to the backward recursion; the formal effort is in the induction along layers with the natural-number indexing of the model.

Formalization scope

Layers and neurons are indexed by natural numbers: a LayeredGraph records the depth, the layer widths and, for each t<Tt < Tt<T, the finite set of edges (vt,j,vt+1,i)(v_{t,j}, v_{t+1,i})(vt,j​,vt+1,i​) as pairs (i,j)(i, j)(i,j) within the layer widths. Weights are functions on all index triples, and only those on edges are used, so the class is the image of all weight functions, as in (20.1). The forward computation netOutput is a recursion on the layer index; netInput is at+1,ia_{t+1,i}at+1,i​. The sign activation returns ±1\pm1±1 with sign⁡(0)=−1\operatorname{sign}(0) = -1sign(0)=−1, the book's convention elsewhere, and a neuron with no incoming edges outputs σ(0)\sigma(0)σ(0) (p. 270). The binary class signNetClass n G is Bool-valued, true iff the output neuron's input is positive, and is stated for graphs of depth at least 111 (for depth 000 the edges out of the input layer would be used but not counted in ∣E∣|E|∣E∣). Growth functions with finite codomain are growthY, an sSup over restriction sizes, well defined because the codomains are finite; the Bool case is Mission IV's growth, and VC dimension and shattering are Mission IV's. Theorem 20.6 and Theorem 20.2 are given with explicit constants derived from the proof, since O(⋅)O(\cdot)O(⋅) statements have no formal content; the drafter verified max⁡{m:2m≤(em)∣E∣}≤2∣E∣log⁡2(16∣E∣)\max\{m : 2^m \le (em)^{|E|}\} \le 2|E|\log_2(16|E|)max{m:2m≤(em)∣E∣}≤2∣E∣log2​(16∣E∣) numerically for ∣E∣|E|∣E∣ up to 300030003000 and at 104,…,10710^4, \dots, 10^7104,…,107, and 2n≤2∣V∣2log⁡2(16∣V∣2)≤8∣V∣32^n \le 2|V|^2\log_2(16|V|^2) \le 8|V|^32n≤2∣V∣2log2​(16∣V∣2)≤8∣V∣3. Backpropagation is stated for an arbitrary layered graph (phantom edges have weight 000, p. 279), any differentiable activation, and one edge at a time as a HasDerivAt of the loss in that weight; δt\delta_tδt​ is defined by recursion on T−tT - tT−t. The book's layer indices in (20.3) are shifted by one in the statement.

Not stated: Theorem 20.3 (Turing machines), Theorem 20.5 and Exercise 1 (sigmoid approximation, which needs a convention for outputs in [−1,1][-1,1][−1,1] that the chapter leaves open), Theorem 20.7 and Exercise 6 (NP-hardness), Exercise 5 (the Ω(∣E∣2)\Omega(|E|^2)Ω(∣E∣2) sigmoid lower bound, which assumes an exact threshold), the sigmoid half of Theorem 20.2, and the SGD pseudocode of §20.6, which is a heuristic without a stated guarantee.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 20. doi:10.1017/CBO9781107298019
  • M. Anthony, P. L. Bartlett, Neural Network Learning: Theoretical Foundations, Cambridge University Press, 1999. doi:10.1017/CBO9780511624216
  • D. E. Rumelhart, G. E. Hinton, R. J. Williams, Learning representations by back-propagating errors, Nature 323, 1986. doi:10.1038/323533a0
  • I. Parberry, Circuit Complexity and Neural Networks, MIT Press, 1994.
  • E. B. Baum, D. Haussler, What size net gives valid generalization?, Neural Computation 1(1), 1989. doi:10.1162/neco.1989.1.1.151
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Mathematical PhysicsQuantum Information·Captain: Lucas

Albers–Kiefer–Reginatto 2008: Measurement Analysis and Quantum GravityResearch Paper

Motivation

Whether the gravitational field must be quantized is a long-standing foundational question. A well-known family of arguments tries to settle it by consistency alone: if a classical field were coupled to a quantum system, some basic principle — momentum conservation, the uncertainty relations, or the impossibility of superluminal signalling — would allegedly be violated. The two best-known versions are the gedanken experiment of Eppley and Hannah (1977) and the measurement-theoretic argument of DeWitt (1962).

Albers, Kiefer and Reginatto (Phys. Rev. D 78, 064051 (2008)) re-examine both arguments. Their paper is largely conceptual, but several of its steps are precise, checkable mathematical claims. This mission collects those claims and makes them machine-checkable.

Timeline.

  • 1962 — DeWitt's measurement analysis of the gravitational field, using Peierls brackets and a "universal principle" for apparatus uncertainties.
  • 1977 — Eppley and Hannah's gedanken experiment: a classical gravitational wave scattered off a quantum particle would imply momentum non-conservation, a violation of the uncertainty principle, or superluminal signalling.
  • 2008 — Albers, Kiefer and Reginatto argue that neither gedanken experiment forces quantization, and exhibit a consistent hybrid classical–quantum model.

Setting

Photon pair and detector (Sec. II). Each photon carries a polarization qubit with orthonormal basis ∣↑⟩|\uparrow\rangle∣↑⟩ (horizontal) and ∣↓⟩|\downarrow\rangle∣↓⟩ (vertical). A detector with state space H\mathcal HH (an arbitrary complex inner-product space) is coupled to photon 1. Before the measurement the joint state of photon 1, photon 2 and the detector is

∣Ψ0⟩=12(∣↑⟩1∣↓⟩2−∣↓⟩1∣↑⟩2)∣Φ0⟩,(1)|\Psi_0\rangle = \tfrac{1}{\sqrt2}\bigl(|\uparrow\rangle_1|\downarrow\rangle_2 - |\downarrow\rangle_1|\uparrow\rangle_2\bigr)|\Phi_0\rangle, \qquad (1)∣Ψ0​⟩=2​1​(∣↑⟩1​∣↓⟩2​−∣↓⟩1​∣↑⟩2​)∣Φ0​⟩,(1)

and after the detector has measured photon 1 it is

∣Ψ⟩=12(∣↑⟩1∣↓⟩2∣Φ↑⟩−∣↓⟩1∣↑⟩2∣Φ↓⟩).(2)|\Psi\rangle = \tfrac{1}{\sqrt2}\bigl(|\uparrow\rangle_1|\downarrow\rangle_2|\Phi_\uparrow\rangle - |\downarrow\rangle_1|\uparrow\rangle_2|\Phi_\downarrow\rangle\bigr). \qquad (2)∣Ψ⟩=2​1​(∣↑⟩1​∣↓⟩2​∣Φ↑​⟩−∣↓⟩1​∣↑⟩2​∣Φ↓​⟩).(2)

The reduced density operator of photon 2 is obtained from ∣Ψ⟩⟨Ψ∣|\Psi\rangle\langle\Psi|∣Ψ⟩⟨Ψ∣ by tracing out photon 1 and the detector; the paper asserts that for both states it equals

ρ^=12(∣↑⟩2⟨↑∣2+∣↓⟩2⟨↓∣2).(3)\hat\rho = \tfrac12\bigl(|\uparrow\rangle_2\langle\uparrow|_2 + |\downarrow\rangle_2\langle\downarrow|_2\bigr). \qquad (3)ρ^​=21​(∣↑⟩2​⟨↑∣2​+∣↓⟩2​⟨↓∣2​).(3)

Mass cube and gravitational wave (Sec. III B). The disturbance δT00GW\delta T^{\mathrm{GW}}_{00}δT00GW​ of the averaged energy density of the scattered wave depends on the cube's edge length aaa and speed vvv, with sensitivities Ta=∂ δT00GW/∂aT_a = \partial\,\delta T^{\mathrm{GW}}_{00}/\partial aTa​=∂δT00GW​/∂a and Tv=∂ δT00GW/∂vT_v = \partial\,\delta T^{\mathrm{GW}}_{00}/\partial vTv​=∂δT00GW​/∂v. With Δa≈Δx\Delta a \approx \Delta xΔa≈Δx and Δv≳ℏ/(2mΔx)\Delta v \gtrsim \hbar/(2m\Delta x)Δv≳ℏ/(2mΔx) the uncertainty ΔT00GW=(TaΔa)2+(TvΔv)2\Delta T^{\mathrm{GW}}_{00} = \sqrt{(T_a\Delta a)^2 + (T_v\Delta v)^2}ΔT00GW​=(Ta​Δa)2+(Tv​Δv)2​ has a strictly positive lower bound.

DeWitt's argument (Sec. V). A system observable sss reconstructed from apparatus data has uncertainty Δs2=ΔA2/g2+g2(ΔDΩs)2\Delta s^2 = \Delta A^2/g^2 + g^2(\Delta D_\Omega s)^2Δs2=ΔA2/g2+g2(ΔDΩ​s)2, where ggg is the coupling constant.

Formalization targets

Goal — no signalling through photon 2 (Eq. (3))

For all unit vectors Φ0,Φ↑,Φ↓∈H\Phi_0, \Phi_\uparrow, \Phi_\downarrow \in \mathcal HΦ0​,Φ↑​,Φ↓​∈H,

ρ2(Ψ0)=ρ^andρ2(Ψ)=ρ^.\rho_2(\Psi_0) = \hat\rho \quad\text{and}\quad \rho_2(\Psi) = \hat\rho .ρ2​(Ψ0​)=ρ^​andρ2​(Ψ)=ρ^​.

Milestones

  1. Eq. (1) ⇒ (3): ρ2(Ψ0)=ρ^\rho_2(\Psi_0) = \hat\rhoρ2​(Ψ0​)=ρ^​.
  2. Eq. (2) ⇒ (3): ρ2(Ψ)=ρ^\rho_2(\Psi) = \hat\rhoρ2​(Ψ)=ρ^​.
  3. Sec. III B lower bound: ΔT00GW≥ℏmTvTa\Delta T^{\mathrm{GW}}_{00} \ge \sqrt{\tfrac{\hbar}{m} T_v T_a}ΔT00GW​≥mℏ​Tv​Ta​​ whenever Δx>0\Delta x > 0Δx>0 and Δv≥ℏ/(2mΔx)\Delta v \ge \hbar/(2m\Delta x)Δv≥ℏ/(2mΔx).
  4. Sec. III B optimum: the function Δx↦(TaΔx)2+(Tvℏ/(2mΔx))2\Delta x \mapsto \sqrt{(T_a\Delta x)^2 + (T_v\hbar/(2m\Delta x))^2}Δx↦(Ta​Δx)2+(Tv​ℏ/(2mΔx))2​ attains its minimum over Δx>0\Delta x>0Δx>0 at Δxmin⁡=ℏ2mTvTa\Delta x_{\min} = \sqrt{\tfrac{\hbar}{2m}\tfrac{T_v}{T_a}}Δxmin​=2mℏ​Ta​Tv​​​, with value ℏmTvTa\sqrt{\tfrac{\hbar}{m}T_vT_a}mℏ​Tv​Ta​​.
  5. Eq. (61): min⁡g≠0ΔA2/g2+g2ΔD2=2 ΔA ΔD\min_{g\ne0}\sqrt{\Delta A^2/g^2 + g^2\Delta D^2} = \sqrt{2\,\Delta A\,\Delta D}ming=0​ΔA2/g2+g2ΔD2​=2ΔAΔD​.
  6. Eq. (64): if ΔA ΔC≥ℏ/2\Delta A\,\Delta C \ge \hbar/2ΔAΔC≥ℏ/2 then ℏ ∣Dss∣≤2 ΔA ΔC ∣Dss∣\sqrt{\hbar\,|D_s s|} \le \sqrt{2\,\Delta A\,\Delta C\,|D_s s|}ℏ∣Ds​s∣​≤2ΔAΔC∣Ds​s∣​.

Significance

The goal is the precise content of the paper's rebuttal of the superluminal-signalling branch of the Eppley–Hannah argument: the state of photon 2 accessible to a probe (such as a classical gravitational wave) is the same whether or not photon 1 has been measured, so a probe of photon 2 alone cannot tell whether photon 1 was measured. Milestones 3–6 are the quantitative estimates the paper uses in Sec. III B (a coupling to a test body obeying the uncertainty principle transfers a minimum uncertainty to the classical wave) and Sec. V (DeWitt's limitation on a single observable, Eq. (64)).

The results are elementary once stated; the value of the mission is to pin the paper's claims down exactly, including the hypotheses under which they hold. None of the statements has, to our knowledge, a machine-checked proof on the platform.

Difficulty

The goal and Milestones 1–2 need a workable representation of the partial trace over a factor that is an arbitrary (possibly infinite-dimensional) inner-product space; the cross terms between the two branches vanish because the two branches are orthogonal on photon 1, not because of any property of the detector states. Milestones 3–6 are single-variable optimization statements; the main care is in the side conditions (positivity, excluding g=0g=0g=0 and Δx=0\Delta x = 0Δx=0).

Formalization scope

  • The joint space C2⊗C2⊗H\mathbb C^2\otimes\mathbb C^2\otimes\mathcal HC2⊗C2⊗H is represented by functions {0,1}×{0,1}→H\{0,1\}\times\{0,1\}\to\mathcal H{0,1}×{0,1}→H (component Ψij\Psi_{ij}Ψij​ along ∣i⟩1∣j⟩2|i\rangle_1|j\rangle_2∣i⟩1​∣j⟩2​; index 0=↑0 = \uparrow0=↑, 1=↓1 = \downarrow1=↓). The reduced density matrix of photon 2 has entries ρ2(j,j′)=∑i⟨Ψij′,Ψij⟩H\rho_2(j,j') = \sum_i \langle \Psi_{ij'}, \Psi_{ij}\rangle_{\mathcal H}ρ2​(j,j′)=∑i​⟨Ψij′​,Ψij​⟩H​, and ρ^\hat\rhoρ^​ is a 2×22\times22×2 complex matrix.
  • The detector states are only assumed to be unit vectors. Orthogonality of ∣Φ↑⟩|\Phi_\uparrow\rangle∣Φ↑​⟩ and ∣Φ↓⟩|\Phi_\downarrow\rangle∣Φ↓​⟩ (a physical property of a detector that records the outcome) is not assumed, because Eq. (3) does not depend on it.
  • In Sec. III B the sensitivities Ta,TvT_a, T_vTa​,Tv​, the mass mmm and ℏ\hbarℏ are positive reals; the paper's approximate relations Δa≈Δx\Delta a\approx\Delta xΔa≈Δx and Δp≳ℏ/Δx\Delta p\gtrsim\hbar/\Delta xΔp≳ℏ/Δx are encoded as Δa=Δx\Delta a = \Delta xΔa=Δx and the hypothesis Δv≥ℏ/(2mΔx)\Delta v \ge \hbar/(2m\Delta x)Δv≥ℏ/(2mΔx).
  • In Eq. (61) the coupling constant ranges over all non-zero reals.
  • Sections IV (hybrid classical–quantum ensembles for Nordström gravity) and the appendices are out of scope for this mission.

Selected references

  • M. Albers, C. Kiefer, M. Reginatto, Measurement analysis and quantum gravity, Phys. Rev. D 78, 064051, 2008. https://doi.org/10.1103/PhysRevD.78.064051
  • K. Eppley, E. Hannah, The necessity of quantizing the gravitational field, Found. Phys. 7, 51–68, 1977. https://doi.org/10.1007/BF00715241
  • B. S. DeWitt, Definition of commutators via the uncertainty principle, J. Math. Phys. 3, 619, 1962. https://doi.org/10.1063/1.1724265
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Machine LearningProbability·Captain: Lucas

The Principles of Deep Learning Theory I: Wick's Theorem for Gaussian IntegralsTextbook

Motivation

The book The Principles of Deep Learning Theory by D. A. Roberts and S. Yaida (arXiv:2106.10165) develops a perturbative, physics-style theory of wide deep neural networks. Every later computation in the book, from the statistics of preactivations at initialization to the neural tangent kernel, reduces to Gaussian expectations of polynomials. The single tool that evaluates these expectations is Wick's theorem (eq. 1.45), which the authors ask the reader to "put a box around". This mission formalizes Chapter 1, §1.1 (Gaussian Integrals), culminating in that theorem. It is the first mission of a series formalizing the book, all in the Lean namespace DeepLearningTheory.

Setting

Fix N≥0N \ge 0N≥0 and a symmetric positive-definite real N×NN\times NN×N matrix K=(Kμν)K = (K_{\mu\nu})K=(Kμν​), the covariance. Write Kμν=(K−1)μνK^{\mu\nu} = (K^{-1})_{\mu\nu}Kμν=(K−1)μν​ for its inverse. The zero-mean multivariable Gaussian distribution with covariance KKK (eq. 1.31) has density on RN\mathbb{R}^NRN

p(z)=1∣2πK∣exp⁡(−12∑μ,ν=1NzμKμνzν),∣2πK∣=det⁡(2πK)=(2π)Ndet⁡K,p(z) = \frac{1}{\sqrt{|2\pi K|}} \exp\Big(-\tfrac12 \sum_{\mu,\nu=1}^N z_\mu K^{\mu\nu} z_\nu\Big), \qquad |2\pi K| = \det(2\pi K) = (2\pi)^N \det K,p(z)=∣2πK∣​1​exp(−21​μ,ν=1∑N​zμ​Kμνzν​),∣2πK∣=det(2πK)=(2π)NdetK,

and the expectation of an observable FFF is E[F(z)]=∫dNz p(z)F(z)\mathbb{E}[F(z)] = \int d^N z\, p(z) F(z)E[F(z)]=∫dNzp(z)F(z) (eqs. 1.36, 1.46), an integral against Lebesgue measure. A pairing of the labels 1,…,2m1,\dots,2m1,…,2m is a partition into mmm unordered pairs; equivalently, a fixed-point-free involution σ\sigmaσ of {1,…,2m}\{1,\dots,2m\}{1,…,2m} pairing aaa with σ(a)\sigma(a)σ(a). There are (2m−1)!!(2m-1)!!(2m−1)!! pairings.

Formalization targets

Goal: Wick's theorem (eq. 1.45)

For all indices μ1,…,μ2m∈{1,…,N}\mu_1,\dots,\mu_{2m} \in \{1,\dots,N\}μ1​,…,μ2m​∈{1,…,N} (repetitions allowed),

E[zμ1⋯zμ2m]=∑pairings σ ∏a<σ(a)Kμaμσ(a).\mathbb{E}[z_{\mu_1}\cdots z_{\mu_{2m}}] = \sum_{\text{pairings } \sigma}\ \prod_{a<\sigma(a)} K_{\mu_a \mu_{\sigma(a)}}.E[zμ1​​⋯zμ2m​​]=pairings σ∑​ a<σ(a)∏​Kμa​μσ(a)​​.

Milestones

  1. Eq. (1.30) — the normalization ∫dNz e−12z⊤K−1z=∣2πK∣\int d^N z\, e^{-\frac12 z^\top K^{-1} z} = \sqrt{|2\pi K|}∫dNze−21​z⊤K−1z=∣2πK∣​.
  2. Eq. (1.41) — the generating function ∫dNz e−12z⊤K−1z+J⋅z=∣2πK∣ e12J⊤KJ\int d^N z\, e^{-\frac12 z^\top K^{-1} z + J\cdot z} = \sqrt{|2\pi K|}\, e^{\frac12 J^\top K J}∫dNze−21​z⊤K−1z+J⋅z=∣2πK∣​e21​J⊤KJ for every source J∈RNJ \in \mathbb{R}^NJ∈RN.
  3. Odd moments vanish (p. 22, discussion after eq. 1.42).
  4. Eq. (1.43) — E[zμ1zμ2]=Kμ1μ2\mathbb{E}[z_{\mu_1} z_{\mu_2}] = K_{\mu_1\mu_2}E[zμ1​​zμ2​​]=Kμ1​μ2​​.
  5. Eq. (1.44) — E[zμ1zμ2zμ3zμ4]=Kμ1μ2Kμ3μ4+Kμ1μ3Kμ2μ4+Kμ1μ4Kμ2μ3\mathbb{E}[z_{\mu_1}z_{\mu_2}z_{\mu_3}z_{\mu_4}] = K_{\mu_1\mu_2}K_{\mu_3\mu_4} + K_{\mu_1\mu_3}K_{\mu_2\mu_4} + K_{\mu_1\mu_4}K_{\mu_2\mu_3}E[zμ1​​zμ2​​zμ3​​zμ4​​]=Kμ1​μ2​​Kμ3​μ4​​+Kμ1​μ3​​Kμ2​μ4​​+Kμ1​μ4​​Kμ2​μ3​​.

Significance

Wick's theorem (also known as Isserlis' theorem, 1918) is used throughout the book: the Gaussianity of the first layer (Chapter 4), the four-point correlators of deep linear networks (Chapter 3), and all perturbative expansions around the infinite-width limit are evaluated by Wick contractions. A machine-checked version stated in the book's own density-based conventions gives later missions of this series a dependable foundation. The result is classical; the work remaining is its formalization in exactly this form. A related statement for general (possibly degenerate) Gaussian measures already exists on the platform as FeynmanWick.wick_theorem_gaussian; the present mission keeps the book's formulation via the explicit density and a positive-definite covariance.

Difficulty

The book's derivation differentiates the generating function (1.41) 2m2m2m times at J=0J=0J=0, which requires justifying differentiation under the integral sign and organizing the combinatorics of the product rule into pairings. Both the analytic step (dominated convergence for Gaussian tails, in NNN dimensions) and the combinatorial step (a bijection between surviving terms and pairings, with the 1/(2mm!)1/(2^m m!)1/(2mm!) normalization) are routine on paper but need care in Lean. Computing the normalization (1.30) itself requires diagonalizing KKK and a linear change of variables.

Formalization scope

  • Vectors are functions Fin N → ℝ with Lebesgue measure; KKK is a Matrix (Fin N) (Fin N) ℝ with K.PosDef (which includes symmetry). The inverse is Mathlib's K⁻¹.
  • gaussianDensity K z and gaussExpect K F are exactly the book's p(z)p(z)p(z) and E[F]\mathbb{E}[F]E[F]; gaussQuadForm K z is ∑zμKμνzν\sum z_\mu K^{\mu\nu} z_\nu∑zμ​Kμνzν​.
  • pairings (2m) is the finite set of fixed-point-free involutions of Fin (2m); the product is over labels aaa with a<σ(a)a<\sigma(a)a<σ(a), so each pair contributes once.
  • Positive definiteness is assumed exactly as in the book; no statement is vacuous since, e.g., K=IK = IK=I satisfies every hypothesis.

Selected references

  • D. A. Roberts, S. Yaida (with B. Hanin), The Principles of Deep Learning Theory, Cambridge University Press, 2022. arXiv:2106.10165
  • L. Isserlis, On a formula for the product-moment coefficient of any order of a normal frequency distribution in any number of variables, Biometrika 12 (1918). doi:10.1093/biomet/12.1-2.134
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Mathematical PhysicsPartial Differential Equations·Captain: Lucas

Analytic toroidal 3D MHD equilibria with nested flux surfaces (Landreman 2026)Research Paper

Motivation

A magnetohydrodynamic (MHD) equilibrium is a magnetic field BBB and a scalar pressure ppp on a region of R3\mathbb R^3R3 satisfying

(∇×B)×B=∇p,∇⋅B=0.(\nabla\times B)\times B=\nabla p,\qquad \nabla\cdot B=0 .(∇×B)×B=∇p,∇⋅B=0.

Under the substitution B↦uB\mapsto uB↦u these are exactly the equations of a steady incompressible Euler flow, with ppp replaced by the Bernoulli function, so every statement in this mission is simultaneously a statement about stationary solutions of the 3D Euler equations. Magnetic confinement of a fusion plasma requires equilibria whose pressure surfaces are nested tori, because B⋅∇p=0B\cdot\nabla p=0B⋅∇p=0 forces ppp to be constant on the surfaces swept out by field lines.

Whether such equilibria exist without a continuous symmetry has been open since Grad, who conjectured in 1967 that smooth toroidal equilibria with non-constant pressure do not exist unless the configuration is symmetric (for instance axisymmetric), and restated the claim in 1985 as the assertion that, apart from the symmetric exceptions, there are no families of solutions depending smoothly on a parameter. Modern formulations of the conjecture appear in the work of Constantin–Drivas–Ginsberg (2021), Enciso–Luque–Peralta-Salas (2025) and Cardona–Duignan–Perrella (2025, Conjecture 2.5). Partial results have always relaxed something: Lortz (1970) obtained non-symmetric toroidal equilibria only with mirror symmetry and vanishing rotational transform; Bruno–Laurence (1996) and Enciso–Luque–Peralta-Salas (2025) allow discontinuous pressure and current sheets; Weitzner–Sengupta (2020) work in a topological torus rather than true toroidal geometry; near-axis and high-aspect-ratio expansions (Mercier 1964, Garren–Boozer 1991) give only approximate solutions.

Landreman (2026) exhibits explicit, fully non-axisymmetric, smooth analytic solutions on a genuine solid torus, with exact nested flux surfaces, finite aspect ratio and non-zero rotational transform. This mission formalizes the first of the two families presented there — the family with uniform rotational transform ι=2\iota=2ι=2 — in Lean 4.

Setting

Fix a parameter 0<ϵ<10<\epsilon<10<ϵ<1 and set a=1+ϵa=\sqrt{1+\epsilon}a=1+ϵ​, b=1−ϵb=\sqrt{1-\epsilon}b=1−ϵ​. For a Cartesian point x=(x0,x1,x2)x=(x_0,x_1,x_2)x=(x0​,x1​,x2​) (written (x,y,z)(x,y,z)(x,y,z) in the paper) define

s=x02a2+x12b2,F=1−(1−s)2−4x22,s=\frac{x_0^2}{a^2}+\frac{x_1^2}{b^2},\qquad F=\sqrt{1-(1-s)^2-4x_2^2},s=a2x02​​+b2x12​​,F=1−(1−s)2−4x22​​,

and the vector field

B=(2x2x0−(a/b)Fx1s, 2x2x1+(b/a)Fx0s, 1−s).B=\left(\frac{2x_2x_0-(a/b)Fx_1}{s},\ \frac{2x_2x_1+(b/a)Fx_0}{s},\ 1-s\right).B=(s2x2​x0​−(a/b)Fx1​​, s2x2​x1​+(b/a)Fx0​​, 1−s).

The natural domain is the open set Uϵ={x:1−(1−s)2−4x22>0}U_\epsilon=\{x: 1-(1-s)^2-4x_2^2>0\}Uϵ​={x:1−(1−s)2−4x22​>0}, on which s>0s>0s>0 and all the expressions above are smooth. With

Q=x02+x12+4x222,H=Q+∣B∣22,Q=\frac{x_0^2+x_1^2+4x_2^2}{2},\qquad H=Q+\frac{|B|^2}{2},Q=2x02​+x12​+4x22​​,H=Q+2∣B∣2​,

the flux label and the pressure are

ψ=H−1+ϵ2/22,p=pa−2ψ,\psi=\frac{H-1+\epsilon^2/2}{2},\qquad p=p_a-2\psi ,ψ=2H−1+ϵ2/2​,p=pa​−2ψ,

where pap_apa​ is an arbitrary constant. The level sets of ψ\psiψ are the pressure surfaces. For 0<δ<(1−ϵ)2/40<\delta<(1-\epsilon)^2/40<δ<(1−ϵ)2/4 the region Ωδ={x∈Uϵ:ψ≤δ}\Omega_\delta=\{x\in U_\epsilon:\psi\le\delta\}Ωδ​={x∈Uϵ​:ψ≤δ} is a solid torus bounded by a ψ\psiψ-surface, and this is the plasma domain.

Field lines are described by a second coordinate system. For labels (u,v)(u,v)(u,v) with u2+v2<1/4u^2+v^2<1/4u2+v2<1/4, putting q2=u2+v2q^2=u^2+v^2q2=u2+v2 and L=((1+1−4q2)/2)1/2L=\big((1+\sqrt{1-4q^2})/2\big)^{1/2}L=((1+1−4q2​)/2)1/2, the position map is

r(u,v,ζ)=(a[Lcos⁡ζ+ucos⁡ζ+vsin⁡ζL], b[Lsin⁡ζ+vcos⁡ζ−usin⁡ζL], vcos⁡2ζ−usin⁡2ζ).r(u,v,\zeta)=\Big(a\big[L\cos\zeta+\tfrac{u\cos\zeta+v\sin\zeta}{L}\big],\ b\big[L\sin\zeta+\tfrac{v\cos\zeta-u\sin\zeta}{L}\big],\ v\cos2\zeta-u\sin2\zeta\Big).r(u,v,ζ)=(a[Lcosζ+Lucosζ+vsinζ​], b[Lsinζ+Lvcosζ−usinζ​], vcos2ζ−usin2ζ).

The curve ζ↦r(u,v,ζ)\zeta\mapsto r(u,v,\zeta)ζ↦r(u,v,ζ) is an integral curve of BBB, the pair (u,v)(u,v)(u,v) labels the field line, and ζ\zetaζ acts as a toroidal angle of period 2π2\pi2π. The magnetic axis is the field line u=−ϵ/2u=-\epsilon/2u=−ϵ/2, v=0v=0v=0, on which ψ=0\psi=0ψ=0; it is the non-planar closed curve γ(ζ)=(1−ϵ2cos⁡ζ, 1−ϵ2sin⁡ζ, ϵ2sin⁡2ζ)\gamma(\zeta)=(\sqrt{1-\epsilon^2}\cos\zeta,\ \sqrt{1-\epsilon^2}\sin\zeta,\ \tfrac{\epsilon}{2}\sin 2\zeta)γ(ζ)=(1−ϵ2​cosζ, 1−ϵ2​sinζ, 2ϵ​sin2ζ).

Target

The goal theorem asserts that for every 0<ϵ<10<\epsilon<10<ϵ<1, every 0<δ<(1−ϵ)2/40<\delta<(1-\epsilon)^2/40<δ<(1−ϵ)2/4 and every constant pap_apa​, the pair (B,p)(B,p)(B,p) above is a smooth equilibrium on UϵU_\epsilonUϵ​ that is genuinely three-dimensional:

∇⋅B=0,(∇×B)×B=∇p,B⋅∇p=0on Uϵ,\nabla\cdot B=0,\qquad (\nabla\times B)\times B=\nabla p,\qquad B\cdot\nabla p=0 \quad\text{on } U_\epsilon,∇⋅B=0,(∇×B)×B=∇p,B⋅∇p=0on Uϵ​, ∇p(x)=0  ⟺  ψ(x)=0for x∈Ωδ,\nabla p(x)=0 \iff \psi(x)=0 \quad\text{for } x\in\Omega_\delta ,∇p(x)=0⟺ψ(x)=0for x∈Ωδ​,

together with smoothness of BBB and ppp on UϵU_\epsilonUϵ​ and the failure of axisymmetry: there is a rotation about the zzz axis and a point of Ωδ\Omega_\deltaΩδ​ whose image lies in Ωδ\Omega_\deltaΩδ​ and carries a different pressure.

The milestones are the individual equations of Section 2 of the paper: divergence-freedom, the tension identity (B⋅∇)B=−∇Q(B\cdot\nabla)B=-\nabla Q(B⋅∇)B=−∇Q, force balance, invariance of ψ\psiψ along BBB, the field-line position map and its Jacobian −ab-ab−ab, the expressions H=1+2ϵu+2(u2+v2)H=1+2\epsilon u+2(u^2+v^2)H=1+2ϵu+2(u2+v2) and ψ=(u+ϵ/2)2+v2\psi=(u+\epsilon/2)^2+v^2ψ=(u+ϵ/2)2+v2 in field-line labels, the magnetic axis, the enclosed volume V=2π2ab ψV=2\pi^2ab\,\psiV=2π2abψ, the uniform rotational transform ι=2\iota=2ι=2, and the averages 12π∫02π∣B∣2 dζ=1−ϵ2/2+2ψ\frac{1}{2\pi}\int_0^{2\pi}|B|^2\,d\zeta=1-\epsilon^2/2+2\psi2π1​∫02π​∣B∣2dζ=1−ϵ2/2+2ψ and ⟨∣B∣2⟩V=1−ϵ2/2+δ\langle|B|^2\rangle_V=1-\epsilon^2/2+\delta⟨∣B∣2⟩V​=1−ϵ2/2+δ.

Significance

The solutions contradict the strict formulation of Grad's conjecture used in the recent literature (for example Conjecture 2.5 of Cardona–Duignan–Perrella), since they are smooth, have non-constant pressure, exact nested toroidal flux surfaces, no continuous Euclidean symmetry, finite aspect ratio and non-zero rotational transform, and they form continuous families parameterized by ϵ\epsilonϵ and δ\deltaδ. Because MHD equilibrium is isomorphic to steady Euler flow, the same objects are explicit non-symmetric stationary Euler flows with invariant tori. They also serve as exact benchmarks for numerical equilibrium codes, where analytic three-dimensional solutions with known flux surfaces are otherwise unavailable.

The paper's derivations are elementary but long: they are algebraic identities among square roots and rational functions, verified in the paper by hand and by supporting numerical scripts. A machine-checked development removes the remaining doubt about sign conventions and domains, which is precisely what a counterexample to a conjecture requires. Nothing in this development is currently formalized in Mathlib: there is no curl, no divergence, and no notion of MHD equilibrium, so the mission also produces a small reusable vector-calculus layer on R3\mathbb R^3R3.

Difficulty

Force balance is an identity between derivatives of expressions containing 1−(1−s)2−4z2\sqrt{1-(1-s)^2-4z^2}1−(1−s)2−4z2​ and division by sss; differentiating it directly produces large expressions whose simplification needs the domain hypotheses (s>0s>0s>0 and positive radicand) at every step, so field_simp-style automation must be driven with those side conditions in hand. The statements about field-line coordinates require knowing that the position map is a diffeomorphism onto its image, which the paper establishes by a covering argument rather than by computation. The transform ι=2\iota=2ι=2 is the hardest milestone: it is a winding-number statement about the poloidal displacement of a field line relative to the magnetic axis, and the paper's proof is a continuity-in-ϵ\epsilonϵ argument, which in Lean needs an honest treatment of continuous angle lifts. The volume and average identities need the change of variables theorem with the constant Jacobian −ab-ab−ab over a solid torus.

Formalization scope

Points of space are Fin 3 → ℝ; partial derivatives are fderiv applied to the standard basis vector, and gradient, divergence, curl, cross product, the directional derivative B⋅∇fB\cdot\nabla fB⋅∇f and the tension (B⋅∇)B(B\cdot\nabla)B(B⋅∇)B are defined from it in the first definition file. Squared length is ∑iui2\sum_i u_i^2∑i​ui2​, so the Pi-type norm is never used. All the paper's objects — aaa, bbb, sss, FFF, BBB, UϵU_\epsilonUϵ​, QQQ, HHH, ψ\psiψ, ppp, Ωδ\Omega_\deltaΩδ​, LLL, r(u,v,ζ)r(u,v,\zeta)r(u,v,ζ), γ\gammaγ, rotation about the zzz axis, and the complex poloidal displacement used for the transform — are given in the second definition file, in the same notation as this description. Smoothness is ContDiffOn ℝ ⊤; volumes are the Lebesgue measure on Fin 3 → ℝ; integrals are Bochner integrals.

Everything is stated with the explicit field of Section 2 rather than an abstract existence claim, so no statement can be satisfied by a degenerate or symmetric configuration. The equilibrium conditions are asserted pointwise on UϵU_\epsilonUϵ​, which is open and non-empty for 0<ϵ<10<\epsilon<10<ϵ<1, so no milestone is vacuous. Contributions of the auxiliary calculus lemmas (differentiability of sss, FFF and BBB on UϵU_\epsilonUϵ​, and the product and quotient rules in this partialD formulation) are welcome and reusable by the companion family of Section 3, which is not part of this mission.

Selected references

  • M. Landreman, Analytic toroidal 3D MHD equilibria and steady Euler flows with invariant surfaces, J. Plasma Phys. (submitted), arXiv:2609.26742 (2026). https://arxiv.org/abs/2609.26742
  • H. Grad, Toroidal containment of a plasma, Phys. Fluids 10 (1967) 137–154. https://doi.org/10.1063/1.1761965
  • R. Cardona, N. Duignan, D. Perrella, Asymmetry of MHD equilibria for generic adapted metrics, Arch. Ration. Mech. Anal. 249 (2025) 1. https://doi.org/10.1007/s00205-024-02072-x
  • A. Enciso, A. Luque, D. Peralta-Salas, MHD equilibria with nonconstant pressure in nondegenerate toroidal domains, J. Eur. Math. Soc. 27 (2025) 2251–2291. https://doi.org/10.4171/JEMS/1328
  • P. Constantin, T. D. Drivas, D. Ginsberg, Flexibility and rigidity in steady fluid motion, Comm. Math. Phys. 385 (2021) 521–563. https://doi.org/10.1007/s00220-021-04048-4
  • O. P. Bruno, P. Laurence, Existence of three-dimensional toroidal MHD equilibria with nonconstant pressure, Comm. Pure Appl. Math. 49 (1996) 717–764. https://doi.org/10.1002/(SICI)1097-0312(199607)49:7<717::AID-CPA3>3.0.CO;2-C
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CombinatoricsMachine LearningProbability+1·Captain: naimengye

An Introduction to Computational Learning Theory III: The Vapnik-Chervonenkis Dimension, ε-Nets and Sample ComplexityTextbook

Motivation

Chapter 3 of Kearns and Vazirani, An Introduction to Computational Learning Theory (MIT Press, 1994, doi:10.7551/mitpress/3897.001.0001), asks how many random examples suffice to learn a concept from an infinite class. The cardinality bound of Occam's Razor is useless there, yet the rectangle game of Chapter 1 shows that some infinite classes are learnable from a finite sample. The answer is the Vapnik–Chervonenkis dimension: the size of the largest set on which the class realizes every labeling. Sauer's lemma says that a class of VC dimension ddd realizes only Φd(m)=∑i≤d(mi)≤(em/d)d\Phi_d(m) = \sum_{i \le d}\binom{m}{i} \le (em/d)^dΦd​(m)=∑i≤d​(im​)≤(em/d)d labelings on any mmm points, polynomially many rather than 2m2^m2m, and the ε-net theorem of Blumer, Ehrenfeucht, Haussler and Warmuth turns this into a sample bound: a consistent hypothesis from a class of VC dimension ddd is probably approximately correct once mmm is of order (1/ϵ)(log⁡(1/δ)+dlog⁡(1/ϵ))(1/\epsilon)(\log(1/\delta) + d\log(1/\epsilon))(1/ϵ)(log(1/δ)+dlog(1/ϵ)). A matching lower bound shows that Ω(d/ϵ)\Omega(d/\epsilon)Ω(d/ϵ) examples are necessary. The chapter thus gives a single combinatorial parameter that characterizes, up to a logarithmic factor, the sample complexity of learning any class in the distribution-free model.

Setting

For a class CCC of concepts X→{0,1}X \to \{0,1\}X→{0,1} and a finite S⊆XS \subseteq XS⊆X, ΠC(S)\Pi_C(S)ΠC​(S) is the set of dichotomies of SSS realized by CCC; SSS is shattered if all 2∣S∣2^{|S|}2∣S∣ are realized; VCD(C)\mathrm{VCD}(C)VCD(C) is the supremum of the sizes of shattered sets, possibly ∞\infty∞; ΠC(m)\Pi_C(m)ΠC​(m) is the largest ∣ΠC(S)∣|\Pi_C(S)|∣ΠC​(S)∣ over ∣S∣=m|S| = m∣S∣=m; and Φd(m)\Phi_d(m)Φd​(m) is defined by Φd(m)=Φd(m−1)+Φd−1(m−1)\Phi_d(m) = \Phi_d(m-1) + \Phi_{d-1}(m-1)Φd​(m)=Φd​(m−1)+Φd−1​(m−1), Φd(0)=Φ0(m)=1\Phi_d(0) = \Phi_0(m) = 1Φd​(0)=Φ0​(m)=1. For a target ccc the error regions are c Δ hc \,\Delta\, hcΔh for hhh in the hypothesis class, and a set of points is an ε-net if it meets every error region of weight at least ϵ\epsilonϵ under the target distribution DDD. Samples, their product law, consistency and the error of a hypothesis are those of Mission I.

Formalization targets

Goal: Theorems 3.3 and 3.4

Let HHH be a class of VC dimension at most ddd, well-behaved for the target ccc (the double-sample event of the proof is null-measurable), and m≥8/ϵm \ge 8/\epsilonm≥8/ϵ. The points of a random sample of mmm examples of a target ccc fail to be an ε-net for the error regions {c Δ h:h∈H}\{c \,\Delta\, h : h \in H\}{cΔh:h∈H} with probability at most

2 Φd(2m) 2−ϵm/2,2\,\Phi_d(2m)\,2^{-\epsilon m/2},2Φd​(2m)2−ϵm/2,

so any algorithm that outputs a hypothesis in HHH consistent with its sample has error greater than ϵ\epsilonϵ with at most that probability; with m≥(4/ϵ)log⁡2(2/δ)m \ge (4/\epsilon)\log_2(2/\delta)m≥(4/ϵ)log2​(2/δ) and m≥(8d/ϵ)log⁡2(13/ϵ)m \ge (8d/\epsilon)\log_2(13/\epsilon)m≥(8d/ϵ)log2​(13/ϵ) the probability is at most δ\deltaδ; and, if HHH is nonempty, every class contained in HHH for whose targets HHH is well-behaved is PAC learnable using HHH.

Milestones

Lemma 3.1 (Sauer's lemma, ΠC(m)≤Φd(m)\Pi_C(m) \le \Phi_d(m)ΠC​(m)≤Φd​(m)); Lemma 3.2 (Φd(m)=∑i≤d(mi)\Phi_d(m) = \sum_{i \le d}\binom{m}{i}Φd​(m)=∑i≤d​(im​)); the polynomial bound Φd(m)≤(em/d)d\Phi_d(m) \le (em/d)^dΦd​(m)≤(em/d)d of p. 57; Theorem 3.5 (the Ω(d/ϵ)\Omega(d/\epsilon)Ω(d/ϵ) lower bound, in the two explicit forms of its proof).

Significance

Theorem 3.3 is the fundamental theorem of PAC learning: it replaces log⁡∣H∣\log|H|log∣H∣ in Occam's Razor by the VC dimension and thereby covers rectangles, halfspaces, polygons, neural networks with a fixed architecture, and every class whose dichotomies grow polynomially. Its proof, the double sample and random partition argument, is the origin of symmetrization in empirical process theory. Sauer's lemma is a cornerstone of extremal combinatorics with independent proofs by Sauer, Shelah and Vapnik–Chervonenkis, and the lower bound of Theorem 3.5 shows that the upper bound is tight to within log⁡(1/ϵ)\log(1/\epsilon)log(1/ϵ), so the VC dimension genuinely characterizes sample complexity. None of these is machine-checked. Formalizing them puts on the platform the VC dimension, the growth function and the ε-net theorem with explicit constants, stated on the same sample law as the rest of this series, and the first information-theoretic lower bound for learning.

Difficulty

Sauer's lemma is a double induction on ddd and mmm through the auxiliary class C′C'C′ of dichotomies whose two extensions to a distinguished point are both realized, which needs care with the identification of dichotomies of SSS and of S∖{x}S \setminus \{x\}S∖{x}. The ε-net theorem needs: the reduction Pr⁡[A]≤2Pr⁡[B]\Pr[A] \le 2\Pr[B]Pr[A]≤2Pr[B] from a failed ε-net on the first half to a region hit at least ϵm/2\epsilon m/2ϵm/2 times by the second half, which is a Chebyshev bound on a binomial variable and is where m≥8/ϵm \ge 8/\epsilonm≥8/ϵ enters; the exchangeability of the 2m2m2m draws with a random partition into two halves; the counting bound (mℓ)/(2mℓ)≤2−ℓ\binom{m}{\ell}/\binom{2m}{\ell} \le 2^{-\ell}(ℓm​)/(ℓ2m​)≤2−ℓ; and Sauer's lemma applied to the error regions, whose growth function equals that of HHH. The explicit constants require the numerical inequality 2(2em/d)d2−ϵm/2≤δ2(2em/d)^d 2^{-\epsilon m/2} \le \delta2(2em/d)d2−ϵm/2≤δ under the two stated conditions. The lower bound is a probabilistic argument with a random target: conditional on the sample, the labels of unseen points are fair coins, so the number of errors on them is binomial and exceeds half its range with probability at least 1/21/21/2; the refined bound scales this construction to a region of weight 16ϵ16\epsilon16ϵ and uses Markov's inequality to bound the number of draws landing in it. Measurability of the failure sets is avoided by stating outer-measure bounds, except for the double-sample event, which the proof integrates: it is assumed null-measurable (the well-behavedness of Blumer et al., without which the theorem is false for a class of VC dimension 111 on ω1\omega_1ω1​). For the lower bound it is avoided by working over a finitely supported distribution on a space with measurable singletons.

Formalization scope

The VC dimension is a supremum in N∪{∞}\mathbb{N} \cup \{\infty\}N∪{∞}, the growth function a supremum in N\mathbb{N}N (bounded by 2m2^m2m), and Φd\Phi_dΦd​ the book's recurrence, with its closed form and polynomial bound stated as separate theorems. The goal is stated for a hypothesis class HHH (Theorem 3.4), Theorem 3.3 being the case C=HC = HC=H; it carries the exact bound of the proof, the explicit constants of Blumer et al. in place of the book's c0c_0c0​, the requirement m≥8/ϵm \ge 8/\epsilonm≥8/ϵ of the proof's Chebyshev step, measurability of the hypotheses and the target, well-behavedness of HHH for the target, and 0<ϵ,δ<10 < \epsilon, \delta < 10<ϵ,δ<1. PAC learnability of the subclasses of HHH needs HHH nonempty, since no algorithm outputs hypotheses in the empty class. The lower bound is stated for every deterministic learning function, on an instance space with measurable singletons, for a class shattering some set of d≥1d \ge 1d≥1 points, with the explicit constants derived in the proof sketch (m≤d/2m \le d/2m≤d/2: error ≥1/8\ge 1/8≥1/8 with probability ≥1/2\ge 1/2≥1/2; ϵ≤1/16\epsilon \le 1/16ϵ≤1/16 and m≤(d−1)/(64ϵ)m \le (d-1)/(64\epsilon)m≤(d−1)/(64ϵ): error >ϵ> \epsilon>ϵ with probability ≥1/4\ge 1/4≥1/4). Running time is not modelled. The composition bound for layered networks (Theorems 3.6 and 3.7) is not stated.

Trivializing readings are excluded: the ε-net event ranges over every hypothesis of HHH, the failure bounds are uniform over all consistent learners, and the lower bound holds for every learning function. Welcome contributions: Sauer's lemma, the closed form and the (em/d)d(em/d)^d(em/d)d bound, the random-partition counting lemma, and the binomial median inequality used in the lower bound.

Selected references

  • M. J. Kearns, U. V. Vazirani, An Introduction to Computational Learning Theory, MIT Press, 1994, Chapter 3. doi:10.7551/mitpress/3897.001.0001
  • A. Blumer, A. Ehrenfeucht, D. Haussler, M. K. Warmuth, Learnability and the Vapnik–Chervonenkis dimension, Journal of the ACM 36(4), 1989. doi:10.1145/76359.76371
  • V. N. Vapnik, A. Ya. Chervonenkis, On the uniform convergence of relative frequencies of events to their probabilities, Theory of Probability and its Applications 16(2), 1971. doi:10.1137/1116025
  • N. Sauer, On the density of families of sets, Journal of Combinatorial Theory, Series A 13(1), 1972. doi:10.1016/0097-3165(72)90019-2
  • A. Ehrenfeucht, D. Haussler, M. Kearns, L. Valiant, A general lower bound on the number of examples needed for learning, Information and Computation 82(3), 1989. doi:10.1016/0890-5401(89)90002-3
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Bandit AlgorithmsOperations ResearchOptimization+1·Captain: naimengye

Multi-armed Bandit Allocation Indices I: The Gittins Index, Optimal Stopping and MonotonicityTextbook

Motivation

A decision-maker has nnn projects, each a Markov reward process, and at every decision time may advance exactly one of them; the others stay frozen. Which project to advance so as to maximize the expected total discounted reward? Posed as a dynamic program the problem has a state space that is the product of the nnn state spaces, and the size of that product defeats every general method. The index theorem of Gittins and Jones (1974) says the dynamic program is solved exactly by an index policy: there is a real number ν(B,x)\nu(B, x)ν(B,x), computable for each bandit process BBB from its own data and its own current state xxx, such that always advancing a process of greatest index is optimal. Chapter 2 of Gittins, Glazebrook and Weber, Multi-armed Bandit Allocation Indices (2nd ed., doi:10.1002/9780470980033), introduces the index, proves the theorem three times, and works out the properties of the index that the rest of the book, from jobs and superprocesses to restless bandits, is built on: which stopping time attains it, how it is computed, how it moves with the discount factor, and when it collapses to the myopic rule.

The index theorem itself is already on the platform, proved, as BanditAlgorithm.gittins_index_theorem in the Bandit Algorithms series (Lattimore and Szepesvári, Theorem 35.9). This mission cites it and formalizes what Chapter 2 establishes around it.

Setting

A bandit process BBB (§2.3–2.4) is a Markov reward process on a countable state space EEE: transition probabilities P(y∣x)P(y \mid x)P(y∣x), a bounded reward r(x)r(x)r(x) received each time the continuation control is applied in state xxx, and a discount factor a∈(0,1)a \in (0, 1)a∈(0,1); the freeze control leaves the state unchanged and yields nothing. The law of the process started at xxx is Px\mathbb{P}_xPx​ and x(t)x(t)x(t) is its state at process time t=0,1,2,…t = 0, 1, 2, \dotst=0,1,2,…. A stopping time τ\tauτ is a past-measurable rule for switching from continuation to freezing, taking values in {1,2,… }∪{∞}\{1, 2, \dots\} \cup \{\infty\}{1,2,…}∪{∞}. For such τ\tauτ, Rτ(B,x)=Ex[∑t<τatr(x(t))]R_\tau(B, x) = \mathbb{E}_x[\sum_{t < \tau} a^t r(x(t))]Rτ​(B,x)=Ex​[∑t<τ​atr(x(t))] is the expected discounted reward and Wτ(B,x)=Ex[∑t<τat]W_\tau(B, x) = \mathbb{E}_x[\sum_{t < \tau} a^t]Wτ​(B,x)=Ex​[∑t<τ​at] the expected discounted time; their ratio ντ(B,x)\nu_\tau(B, x)ντ​(B,x) (2.7) is the equivalent constant reward rate of that portion of BBB. The Gittins index is

ν(B,x)=sup⁡τ>0Rτ(B,x)Wτ(B,x)(2.6)\nu(B, x) = \sup_{\tau > 0} \frac{R_\tau(B, x)}{W_\tau(B, x)} \tag{2.6}ν(B,x)=τ>0sup​Wτ​(B,x)Rτ​(B,x)​(2.6)

and, equivalently, the fair charge (2.5): the greatest rent λ\lambdaλ per period for which continuing BBB for one or more periods, paying λ\lambdaλ each period, can be done without expected loss. A simple family of alternative bandit processes (SFABP) is nnn such processes with a common discount factor, one of which is continued at each decision time; an index policy continues a process of greatest index. In the Lean development the single-arm model is the platform's (GittinsIndex): the chain law is built by the Ionescu–Tulcea construction, stopping times are adapted N∪{∞}\mathbb{N}\cup\{\infty\}N∪{∞}-valued maps on trajectories, and gittinsIndex P r a x is (2.6).

Formalization targets

Goal: Lemma 2.2, the optimal stopping set

The supremum in (2.6) is attained. For the initial state ξ\xiξ, the attaining stopping rule may be taken to be "stop at the first time t≥1t \ge 1t≥1 at which the state lies in Σ0\Sigma_0Σ0​" for any set Σ0\Sigma_0Σ0​ with

{x:ν(B,x)<ν(B,ξ)}⊆Σ0⊆{x:ν(B,x)≤ν(B,ξ)},\{x : \nu(B, x) < \nu(B, \xi)\} \subseteq \Sigma_0 \subseteq \{x : \nu(B, x) \le \nu(B, \xi)\},{x:ν(B,x)<ν(B,ξ)}⊆Σ0​⊆{x:ν(B,x)≤ν(B,ξ)},

and every such rule has ντ(B,ξ)=ν(B,ξ)\nu_\tau(B, \xi) = \nu(B, \xi)ντ​(B,ξ)=ν(B,ξ).

Milestones

Theorem 2.1 as a reference to the proved platform theorem; Eq. (2.5), the fair-charge characterization of the index; the restart-in-state formulation of §2.6.4 as the convergence of the Katehakis–Veinott value iteration; Theorem 2.3, monotonicity in the discount factor; Lemma 2.4, the interchange of two bandit portions; Propositions 2.5–2.8, the monotone-index cases in which the index is the immediate reward, or is attained only after the first step, or only at τ=∞\tau = \inftyτ=∞.

Significance

Lemma 2.2 is the working form of the index: it turns the supremum over all stopping times into a specific rule, the first time the index falls below its starting value, and it is what the interchange proof of §2.7, the modified-forwards-induction policies of §2.6.6, the monotone-index propositions of §2.11 and the treatment of jobs in Chapter 3 all use. The fair-charge form (2.5) is the prevailing-charge proof of the theorem (Weber 1992) and the interpretation that carries over to superprocesses and restless bandits. The restart formulation is how indices are computed in practice (Katehakis and Veinott 1987), and Theorem 2.3 is the first of the comparative statics used throughout Chapters 7 and 8. Lemma 2.4 is the elementary inequality behind the original proof of Gittins and Jones.

Of these, only the index theorem has a machine-checked proof today. Formalizing the rest gives the platform the index as a usable object: a characterization of the optimal stopping rule, a convergent algorithm for it, and the monotonicity facts, all stated against the existing model so that every later mission of this series and every future use of the L&S model can build on them.

Difficulty

The obvious first move for Lemma 2.2, "take the stopping time that achieves the supremum", is what has to be proved: the supremum is over an uncountable family, and attainment comes from the optimal stopping problem with charge λ=ν(B,ξ)\lambda = \nu(B, \xi)λ=ν(B,ξ), whose value function satisfies φ(x)=max⁡{0,r(x)−λ+aE[φ(x(1))∣x(0)=x]}\varphi(x) = \max\{0, r(x) - \lambda + a\mathbb{E}[\varphi(x(1)) \mid x(0) = x]\}φ(x)=max{0,r(x)−λ+aE[φ(x(1))∣x(0)=x]}, together with the fact that its optimal stopping set is characterized by the strict and non-strict inequalities λ>ν(B,x)\lambda > \nu(B, x)λ>ν(B,x) and λ≥ν(B,x)\lambda \ge \nu(B, x)λ≥ν(B,x). That last step is the content: it identifies the local decision "stop or continue" with a comparison of indices, which is why any set between the two level sets works. On the platform's model this requires the dynamic-programming theory of discounted optimal stopping on a countable space (Theorem 2.10 of the book), the identification of fairChargeProfit with that value function, and the strong Markov property of markovChainMeasure at a trajectory stopping time. Theorem 2.3 needs randomized stopping times (a geometric kill) and the fact that they do not enlarge the supremum. The restart iteration is monotone and bounded but its operator is not a contraction in the restart value, so its limit has to be identified with the restart problem's value directly; that value is max⁡(0,ν/(1−a))\max(0, \nu/(1-a))max(0,ν/(1−a)), not ν/(1−a)\nu/(1-a)ν/(1−a), because restarting forever is free.

Formalization scope

The state space is a countable type with measurable singletons, so every subset is measurable; rewards are bounded; a∈(0,1)a \in (0, 1)a∈(0,1). The chain law, stopping times, the discounted stopped sums and the index are the platform's, unchanged. Expectations are Bochner integrals; with bounded rewards they are finite and no total-function default value enters. IsPositiveStoppingTime fixes τ≥1\tau \ge 1τ≥1 everywhere, so Wτ≥1W_\tau \ge 1Wτ​≥1 and the ratio (2.7) is a genuine quotient. The stopping rule of Lemma 2.2 is the hitting time from time 111 of a set, with ∞\infty∞ when the set is never hit. The fair-charge profit is a real supremum over the nonempty bounded family of positive stopping times, and (2.5) is stated with the outer supremum over {λ:profit(λ)≥0}\{\lambda : \text{profit}(\lambda) \ge 0\}{λ:profit(λ)≥0}, a nonempty set bounded above. The restart iteration is stated as a limit, with the value max⁡(0,ν(B,ξ)/(1−a))\max(0, \nu(B, \xi)/(1-a))max(0,ν(B,ξ)/(1−a)): for a nonnegative index this is the book's ν/(1−a)\nu/(1-a)ν/(1−a), and the maximum is forced by a one-state example with negative reward. The propositions' hypotheses are almost-sure events under Px\mathbb{P}_xPx​, written as events of measure one.

Two trivializing readings are excluded: the index is never taken over all N∪{∞}\mathbb{N}\cup\{\infty\}N∪{∞}-valued maps but over adapted stopping times, and the stopping set of the goal is not restricted to the two extreme level sets. Contributions welcome: the optimal-stopping dynamic program on markovChainMeasure (value iteration, the strong Markov property at a stopping time), the equivalence of randomized and non-randomized stopping times for the supremum, and the monotone convergence of the restart iteration.

Selected references

  • J. Gittins, K. Glazebrook, R. Weber, Multi-armed Bandit Allocation Indices, 2nd ed., Wiley, 2011, Chapter 2. doi:10.1002/9780470980033
  • J. C. Gittins, D. M. Jones, A dynamic allocation index for the sequential design of experiments, in Progress in Statistics (Gani, ed.), North-Holland, 1974.
  • R. Weber, On the Gittins index for multiarmed bandits, Annals of Applied Probability 2(4), 1992. doi:10.1214/aoap/1177005588
  • M. N. Katehakis, A. F. Veinott, The multi-armed bandit problem: decomposition and computation, Mathematics of Operations Research 12(2), 1987. doi:10.1287/moor.12.2.262
  • T. Lattimore, C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020, Chapter 35. doi:10.1017/9781108571401
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Operations ResearchOptimization·Captain: naimengye

The Theory and Practice of Revenue Management I: Single-Resource Capacity ControlTextbook

Which fares to open, and when to close them

An airline sells one flight, a hotel one night, a car-rental firm one day of one car: a fixed capacity, perishable at a deadline, sold to customers who arrive over time and are willing to pay different amounts. Chapter 2 of Talluri and van Ryzin's The Theory and Practice of Revenue Management (2004) is the theory of that single resource. Its three models answer the same question with increasing generality: Littlewood's two-class rule, the nnn-class static model and its dynamic-arrival version give the seller a protection level per class, a booking limit or a bid price, all three equivalent; the discrete-choice model, in which customers buy down when a cheaper fare is open, replaces classes by offer sets and shows that only the efficient sets, ordered by their purchase probability, are ever offered, with a higher set the more capacity or the less time remains. This mission formalizes that last result, Theorem 2.3, together with the structural results of the two earlier models that it generalizes.

Setting

Static model. Classes 1,…,n1, \dots, n1,…,n with prices p1≥⋯≥pn≥0p_1 \ge \dots \ge p_n \ge 0p1​≥⋯≥pn​≥0 arrive in stages, lowest class first, with demands DjD_jDj​ distributed on N\mathbb NN. With xxx units left at stage jjj the seller observes DjD_jDj​ and accepts u≤min⁡{Dj,x}u \le \min\{D_j, x\}u≤min{Dj​,x} units; the value function is the Bellman equation (2.3), Vj(x)=E[max⁡u{pju+Vj−1(x−u)}]V_j(x) = \mathbb E[\max_u \{p_j u + V_{j-1}(x-u)\}]Vj​(x)=E[maxu​{pj​u+Vj−1​(x−u)}], V0=0V_0 = 0V0​=0 (staticValue), and ΔVj(x)=Vj(x)−Vj(x−1)\Delta V_j(x) = V_j(x) - V_j(x-1)ΔVj​(x)=Vj​(x)−Vj​(x−1) is the marginal value of capacity. The protection level yj∗=max⁡{x:pj+1<ΔVj(x)}y_j^* = \max\{x : p_{j+1} < \Delta V_j(x)\}yj∗​=max{x:pj+1​<ΔVj​(x)} (protLevel), the booking limit bj∗=C−yj−1∗b_j^* = C - y_{j-1}^*bj∗​=C−yj−1∗​ (bookLimit) and the bid price πj+1(x)=ΔVj(x)\pi_{j+1}(x) = \Delta V_j(x)πj+1​(x)=ΔVj​(x) (bidPrice) define the three controls of Theorem 2.1.

Dynamic model. Over TTT periods at most one request arrives per period, of class jjj with probability λj(t)\lambda_j(t)λj​(t); the value function (2.17) is Vt(x)=Vt+1(x)+E[max⁡u∈{0,1}(R(t)−ΔVt+1(x))u]V_t(x) = V_{t+1}(x) + \mathbb E[\max_{u \in \{0,1\}} (R(t) - \Delta V_{t+1}(x))u]Vt​(x)=Vt+1​(x)+E[maxu∈{0,1}​(R(t)−ΔVt+1​(x))u] (dynValue), with time-dependent protection levels (2.19), booking limits (2.20) and bid prices (2.18).

Choice model. When the set SSS of classes is open an arriving customer buys class j∈Sj \in Sj∈S with probability Pj(S)P_j(S)Pj​(S); Q(S)=∑j∈SPj(S)Q(S) = \sum_{j \in S} P_j(S)Q(S)=∑j∈S​Pj​(S) is the purchase probability and R(S)=∑j∈SPj(S)pjR(S) = \sum_{j \in S} P_j(S) p_jR(S)=∑j∈S​Pj​(S)pj​ the expected revenue (purchaseProb, expRevenue). The value function (2.26) is Vt(x)=max⁡Sλt(R(S)−Q(S)ΔVt+1(x))+Vt+1(x)V_t(x) = \max_{S} \lambda_t (R(S) - Q(S)\Delta V_{t+1}(x)) + V_{t+1}(x)Vt​(x)=maxS​λt​(R(S)−Q(S)ΔVt+1​(x))+Vt+1​(x) (choiceValue). A set TTT is inefficient (Definition 2.1, IsInefficient) if a randomization α\alphaα over the subsets has ∑Sα(S)Q(S)≤Q(T)\sum_S \alpha(S) Q(S) \le Q(T)∑S​α(S)Q(S)≤Q(T) and ∑Sα(S)R(S)>R(T)\sum_S \alpha(S) R(S) > R(T)∑S​α(S)R(S)>R(T), and efficient otherwise.

Formalization targets

Goal: Theorem 2.3

In every period with capacity left, some efficient set maximizes (2.26); and, the efficient sets being ordered by QQQ, the largest optimal set is nondecreasing in the remaining capacity xxx and nondecreasing in the period ttt: choice_optimal_policy. Monotonicity is stated as "every efficient optimal set at (t,x)(t, x)(t,x) is matched by one at (t,x′)(t, x')(t,x′), x′≥xx' \ge xx′≥x, with at least as large a purchase probability", and likewise in ttt.

Supporting targets

Littlewood's rule (2.1), ΔV1(x)=p1P(D1≥x)\Delta V_1(x) = p_1 \mathbb P(D_1 \ge x)ΔV1​(x)=p1​P(D1​≥x) and the acceptance criterion; Proposition 2.1, the marginal values of the static model are decreasing in xxx and increasing in the stages remaining; Theorem 2.1, nested protection levels, nested booking limits and bid-price tables each attain the Bellman maximum at every stage; Proposition 2.2 and Theorem 2.2, the same two results for the dynamic model, with marginal values now decreasing in time; Proposition 2-2.A.4 of the appendix, the marginal values of the choice model are decreasing in xxx and in ttt; Proposition 2.3, an inefficient set is never optimal; and the ordering of efficient sets, Q(S)≤Q(S′)Q(S) \le Q(S')Q(S)≤Q(S′) implies R(S)≤R(S′)R(S) \le R(S')R(S)≤R(S′) when S′S'S′ is efficient.

The continuous-demand optimality conditions (2.9) of Sect. 2.2.2.3, stated without proof, the computational and heuristic methods of Sects. 2.2.3-2.2.4, the overbooking models of Sect. 2.7 and the nested-policy characterization of Sect. 2.6.2.5 are not targets.

Significance

Theorem 2.3 is the structural result behind choice-based revenue management: it reduces the 2n2^n2n offer sets to the efficient frontier of (Q(S),R(S))(Q(S), R(S))(Q(S),R(S)), orders that frontier, and shows the optimal policy walks up it as capacity grows or the deadline nears. It was the analytical core of Talluri and van Ryzin's (2004) choice-model paper and is the reason the efficient sets, not the fare classes, are the unit of control when customers substitute between fares. The static and dynamic results, from Littlewood (1972) and Brumelle and McGill (1993) to Lee and Hersh (1993), are the foundation of every airline seat inventory control system; the equivalence of protection levels, booking limits and bid prices is what lets the same optimal policy be implemented on any of the three kinds of reservation system. None of these results has a machine-checked proof.

Difficulty

The two marginal-value propositions are inductions in which the inductive step is the discrete concavity of a max-plus convolution, Lemma 2-2.A.1 of the appendix: x↦max⁡0≤a≤m{ap+g(x−a)}x \mapsto \max_{0 \le a \le m}\{ap + g(x-a)\}x↦max0≤a≤m​{ap+g(x−a)} is concave when ggg is, which in Lean requires reasoning about the argmax on N\mathbb NN and the truncated subtraction. The static model's expectation is a tsum against a pmf, so every step also needs summability of a bounded family. The protection-level theorems then need the down-set structure of {x:pj+1<ΔVj(x)}\{x : p_{j+1} < \Delta V_j(x)\}{x:pj+1​<ΔVj​(x)} under monotonicity of ΔVj\Delta V_jΔVj​, and the three controls have to be shown to coincide unit by unit. For the choice model, Proposition 2.3 is a one-line convexity argument once ΔV≥0\Delta V \ge 0ΔV≥0 is known, and the monotonicity in Theorem 2.3 is a monotone comparative-statics argument on the objective R(S)−Q(S)ΔR(S) - Q(S)\DeltaR(S)−Q(S)Δ, which is easy in Δ\DeltaΔ but must be combined with Proposition 2-2.A.4 in both xxx and ttt; the existence of an efficient maximizer uses Proposition 2.3 and the finiteness of the subsets.

Formalization scope

Capacities, stages and periods are natural numbers, the value functions recurse on the stage or on the number of periods to go, and the book's ranges (x≤Cx \le Cx≤C, t≤Tt \le Tt≤T, j≤nj \le nj≤n) are hypotheses of the theorems. Demand in the static model is a pmf on N\mathbb NN rather than a random variable, so the expectation in (2.3) is a tsum; the dynamic model's expectation over R(t)R(t)R(t) is written out, including the no-arrival term, which vanishes under nonnegative prices. The choice model is defined by its compact form (2.26), and the maximization includes the empty offer set. Optimality of a control means attaining the inner maximum of the Bellman equation at every state, which is what the book's proofs establish. The bid-price control is formalized with the bid price πj+1(x+1−z)\pi_{j+1}(x + 1 - z)πj+1​(x+1−z) of the zzz-th unit allocated; the book prints x−zx - zx−z, which is one unit off from (2.5). The appendix's Proposition 2-2.A.4 prints its time monotonicity in the reverse direction; the formal statement is the direction consistent with Proposition 2.2 and Theorem 2.3. The ordering of efficient sets is stated with non-strict inequalities, since Definition 2.1 admits ties in revenue.

Selected references

  • K. T. Talluri and G. J. van Ryzin, The Theory and Practice of Revenue Management, Kluwer/Springer, 2004, Chapter 2. https://doi.org/10.1007/b139000
  • K. Littlewood, Forecasting and control of passenger bookings, AGIFORS Symposium Proceedings 12, 1972; reprinted in Journal of Revenue and Pricing Management 4(2), 2005. https://doi.org/10.1057/palgrave.rpm.5170134
  • S. L. Brumelle and J. I. McGill, Airline seat allocation with multiple nested fare classes, Operations Research 41(1), 1993. https://doi.org/10.1287/opre.41.1.127
  • T. C. Lee and M. Hersh, A model for dynamic airline seat inventory control with multiple seat bookings, Transportation Science 27(3), 1993. https://doi.org/10.1287/trsc.27.3.252
  • K. T. Talluri and G. J. van Ryzin, Revenue management under a general discrete choice model of consumer behavior, Management Science 50(1), 2004. https://doi.org/10.1287/mnsc.1030.0147
  • C. J. Lautenbacher and S. Stidham, The underlying Markov decision process in the single-leg airline yield-management problem, Transportation Science 33(2), 1999. https://doi.org/10.1287/trsc.33.2.136
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Fundamentals of Supply Chain Theory VII: Multiechelon Inventory ModelsTextbook

One stage at a time

A serial supply chain is the simplest multiechelon system: a retailer orders from a warehouse, which orders from a plant, which orders from an outside supplier with unlimited stock. Only the retailer sees customer demand, only the retailer pays a stockout penalty, and every stage pays to hold inventory. Choosing how much each stage should hold looks like a joint optimization over all stages at once, because an upstream stockout delays every downstream replenishment. Clark and Scarf (1960) showed that it is not: measured in echelon terms, the optimal policy is a base-stock policy at every stage, and the optimal levels can be found one stage at a time from the customer upward, each step a single-variable convex minimization. Chapter 6 of Snyder and Shen's Fundamentals of Supply Chain Theory (2019) presents the infinite-horizon form of that result as its Theorem 6.3, the bounds of Shang and Song (2003) that make the levels cheap to approximate, and the contrasting guaranteed-service model of Graves and Willems (2000), in which stages quote delivery times rather than fill rates and the optimal safety stocks are all-or-nothing. This mission formalizes the chapter's numbered results, with Theorem 6.3 as its goal.

Setting

Stages are numbered 1,…,N1, \dots, N1,…,N from the customer upward. Stage jjj has a local holding cost hj′h'_jhj′​ per unit per period; its echelon holding cost is hj=hj′−hj+1′h_j = h'_j - h'_{j+1}hj​=hj′​−hj+1′​ with hN+1′=0h'_{N+1} = 0hN+1′​=0, so that hj′=∑i≥jhih'_j = \sum_{i \ge j} h_ihj′​=∑i≥j​hi​ (localHolding, echelonHolding). Stage jjj's echelon consists of stages j,j−1,…,1j, j-1, \dots, 1j,j−1,…,1, and its echelon on-hand inventory IjI_jIj​ (echelonOnHand) is all on-hand and in-transit stock in that echelon. Stage 1 pays a stockout cost ppp per unit per period. Orders placed by stage jjj arrive after a lead time LjL_jLj​ if stage j+1j+1j+1 can ship them; DjD_jDj​ denotes the lead-time demand at stage jjj.

An echelon base-stock policy gives each stage a level SjS_jSj​ and orders to keep its echelon inventory position at SjS_jSj​. The chapter derives, from conservation of flow, a recursion that evaluates the expected cost of any echelon base-stock vector SSS (csBar, csHat, csG):

gˉ0(x)=(p+h1′)x−,g^j(x)=hjx+gˉj−1(x),gj(y)=E[g^j(y−Dj)],gˉj(x)=gj(min⁡{Sj,x}),\bar g_0(x) = (p + h'_1)x^-, \qquad \hat g_j(x) = h_j x + \bar g_{j-1}(x), \qquad g_j(y) = \mathbb{E}[\hat g_j(y - D_j)], \qquad \bar g_j(x) = g_j(\min\{S_j, x\}),gˉ​0​(x)=(p+h1′​)x−,g^​j​(x)=hj​x+gˉ​j−1​(x),gj​(y)=E[g^​j​(y−Dj​)],gˉ​j​(x)=gj​(min{Sj​,x}),

and the expected cost of the system under SSS is gN(SN)g_N(S_N)gN​(SN​). The term gˉj\bar g_jgˉ​j​ is the implicit penalty function: it charges stage j+1j+1j+1 for the downstream consequences of running short. A vector is sequentially optimal (CSSequential) when each SjS_jSj​ minimizes gjg_jgj​, which depends only on S1,…,Sj−1S_1, \dots, S_{j-1}S1​,…,Sj−1​.

The Shang-Song bounds compare gjg_jgj​ with the cost of the jjj-stage truncated system when all its local holding costs are set to one value, hjh_jhj​ for the lower bound and ∑k≤jhk\sum_{k \le j} h_k∑k≤j​hk​ for the upper (ssLower, ssUpper). With equal holding costs all stock is held at stage 1, so each bound is a single-stage newsvendor cost for the demand D~j=D1+⋯+Dj\tilde D_j = D_1 + \dots + D_jD~j​=D1​+⋯+Dj​ over the cumulative lead time (tildeLaw) with stockout cost p+hj+1′p + h'_{j+1}p+hj+1′​, plus the holding cost of the stock in transit to stages 1,…,j−11, \dots, j-11,…,j−1, whose mean is E[D1]+⋯+E[Dj−1]\mathbb{E}[D_1] + \dots + \mathbb{E}[D_{j-1}]E[D1​]+⋯+E[Dj−1​] (pipelineMean).

In the guaranteed-service model each stage iii has a processing time TiT_iTi​, quotes a committed service time SiS_iSi​ to its customer, and receives an inbound time SIi=Si+1SI_i = S_{i+1}SIi​=Si+1​ from its supplier (gsInbound), SINSI_NSIN​ being external. Demand is bounded, so the stage can meet every order within SiS_iSi​ by holding safety stock kSIi+Ti−Sik\sqrt{SI_i + T_i - S_i}kSIi​+Ti​−Si​​ with k=zασk = z_\alpha\sigmak=zα​σ, and the holding cost is g(S)=∑ihikSIi+Ti−Sig(S) = \sum_i h_i k \sqrt{SI_i + T_i - S_i}g(S)=∑i​hi​kSIi​+Ti​−Si​​ (gsCost) over the feasible times 0≤Si≤SIi+Ti0 \le S_i \le SI_i + T_i0≤Si​≤SIi​+Ti​ (GSFeasible).

Formalization targets

Goal: Theorem 6.3

For echelon holding costs hj≥0h_j \ge 0hj​≥0, stockout cost p≥0p \ge 0p≥0 and lead-time demands of finite mean, if S∗S^*S∗ is sequentially optimal then for every echelon base-stock vector SSS,

gN(SN∗∣S∗)  ≤  gN(SN∣S),g_N(S^*_N \mid S^*) \;\le\; g_N(S_N \mid S),gN​(SN∗​∣S∗)≤gN​(SN​∣S),

and gN(SN∗∣S∗)g_N(S^*_N \mid S^*)gN​(SN∗​∣S∗) is the optimal cost. This is clark_scarf_sequential.

Supporting targets

Proposition 6.1, ∑jhjIj=∑jhj′(Ij′+ITj−1)\sum_j h_j I_j = \sum_j h'_j (I'_j + IT_{j-1})∑j​hj​Ij​=∑j​hj′​(Ij′​+ITj−1​); the stage-1 identities (6.29) and (6.30), that g1g_1g1​ is a newsvendor cost with penalty p+h2′p + h'_2p+h2′​ and its minimizer solves F1(S1∗)=(p+h2′)/(h1+p+h2′)F_1(S^*_1) = (p + h'_2)/(h_1 + p + h'_2)F1​(S1∗​)=(p+h2′​)/(h1​+p+h2′​); convexity of every gjg_jgj​ under sequential optimality; existence of a sequentially optimal vector when hj>0h_j > 0hj​>0 and p>0p > 0p>0; Theorem 6.4, gjl≤gj≤gjug^l_j \le g_j \le g^u_jgjl​≤gj​≤gju​, and Sjl≤Sj∗≤SjuS^l_j \le S^*_j \le S^u_jSjl​≤Sj∗​≤Sju​ where SjuS^u_jSju​ minimizes gjlg^l_jgjl​ and SjlS^l_jSjl​ minimizes gjug^u_jgju​ (the book's pairing, p. 200); and Theorem 6.5, that in the guaranteed-service serial system with s1=0s_1 = 0s1​=0 every optimal Si∗S^*_iSi∗​ is 000 or Si+1∗+TiS^*_{i+1} + T_iSi+1∗​+Ti​.

Theorem 6.2, the optimality of echelon base-stock policies among all policies, is stated in the book without a model of the policy space and is not a target here; Theorem 6.3 is the optimization it licenses.

Significance

Theorem 6.3 is what Zipkin calls the fundamental equations of supply chain theory. It reduces a joint optimization over NNN coupled levels to NNN one-dimensional convex problems, and every exact method and most heuristics for serial and assembly systems, Rosling's reduction of assembly systems to serial ones included, run through it. Theorem 6.4 turns the recursion into closed-form bounds and the Shang-Song heuristic, which the book reports as accurate to within a fraction of a percent. Theorem 6.5 explains the shape of optimal safety stock placement under guaranteed service and why its dynamic program only needs to examine endpoints.

None of these results has a machine-checked proof. The book proves none of them in full: Theorem 6.3 is asserted after an informal derivation, Theorem 6.4 is cited, and Proposition 6.1 and Theorem 6.5 are left as exercises. Formalizing the recursion's convexity and the exchange argument behind Theorem 6.3 produces a reusable treatment of the implicit penalty function; the concavity-on-a-polytope argument for Theorem 6.5 is reusable for the tree systems of Sect. 6.3.5.

Difficulty

The obvious attack on Theorem 6.3, differentiating the system cost in each SjS_jSj​, fails immediately: the cost depends on SjS_jSj​ through min⁡{Sj,x}\min\{S_j, x\}min{Sj​,x} inside nested expectations and is not convex in SSS jointly. The argument that works is an induction along the recursion, comparing gj(⋅∣S)g_j(\cdot \mid S)gj​(⋅∣S) with gj(⋅∣S∗)g_j(\cdot \mid S^*)gj​(⋅∣S∗) pointwise. Its key step is that, for the convex gj(⋅∣S∗)g_j(\cdot \mid S^*)gj​(⋅∣S∗) minimized at Sj∗S^*_jSj∗​, the value gj(min⁡{Sj∗,x})g_j(\min\{S^*_j, x\})gj​(min{Sj∗​,x}) is the least value of gjg_jgj​ on (−∞,x](-\infty, x](−∞,x], so that any other truncation point can only cost more. That step needs convexity of gj(⋅∣S∗)g_j(\cdot \mid S^*)gj​(⋅∣S∗), which needs gˉj−1(⋅∣S∗)\bar g_{j-1}(\cdot \mid S^*)gˉ​j−1​(⋅∣S∗) convex, which needs Sj−1∗S^*_{j-1}Sj−1∗​ to be a minimizer; for an arbitrary SSS the functions gˉj(⋅∣S)\bar g_j(\cdot \mid S)gˉ​j​(⋅∣S) are not convex, and the induction must carry both vectors at once.

Integrability is a second, silent obstacle. Each gjg_jgj​ is an expectation of translates of g^j\hat g_jg^​j​; the recursion preserves Lipschitz continuity with a constant growing with the costs, and finite means are exactly what make every integral in the recursion a genuine expectation rather than Lean's default value zero.

Theorem 6.4 requires relating the recursion, in which demands enter one stage at a time, to a single newsvendor cost in the sum D~j\tilde D_jD~j​, which is a convolution; the inequalities come from the structure of (6.31) in the two extreme holding-cost profiles and are not obvious from the recursion's formulas. Theorem 6.5 is a statement about every minimizer, not the existence of an extreme one, so the proof must show the cost is strictly concave along every feasible direction that changes a net lead time and then classify the vertices of the feasible region.

Formalization scope

Stages are indexed by natural numbers 1,…,N1, \dots, N1,…,N; the cost functions take total functions on N\mathbb{N}N and never read values outside that range. The recursion is defined for every vector SSS, so the theorem compares values of one family of functions rather than a separately defined system cost; the identification of gN(SN∣S)g_N(S_N \mid S)gN​(SN​∣S) with the steady-state expected cost of the physical system is the book's derivation and is not restated. Expectations are Lebesgue integrals under the lead-time demand laws, assumed to be probability measures on R\mathbb{R}R with finite means. Sequential optimality is a hypothesis of the goal; a separate target shows it is satisfiable when hj>0h_j > 0hj​>0 and p>0p > 0p>0, so the goal is not vacuous.

The bounding functions of Theorem 6.4 keep the holding cost of pipeline stock that the truncated cost (6.31) charges. The book omits that constant when it writes their minimizers, which it does not affect, but part (a) compares values, and without the constant the upper bound fails already in the book's own Example 6.1. For part (b) the minimizers of the bounding functions are asserted to exist and to bracket Sj∗S^*_jSj∗​; when the fractiles of D~j\tilde D_jD~j​ are unique these are the book's quantile values. Theorem 6.5 is stated over real service times; because the feasible region's vertices are integral when the data are, every integer-optimal vector is optimal over the reals, so the real statement contains the book's integer program (6.38) to (6.42). Proposition 6.1 is stated with IT0=0IT_0 = 0IT0​=0 built into the echelon sum.

The definition module is shared by all nine items. The dynamic program (6.43) to (6.44) for guaranteed-service serial systems and the tree-system algorithm of Sect. 6.3.6 are natural extensions on the same definitions.

Selected references

  • L. V. Snyder and Z.-J. M. Shen, Fundamentals of Supply Chain Theory, 2nd ed., Wiley, 2019, Chapter 6. https://doi.org/10.1002/9781119584445
  • A. J. Clark and H. Scarf, Optimal policies for a multi-echelon inventory problem, Management Science 6(4), 1960. https://doi.org/10.1287/mnsc.6.4.475
  • F. Chen and Y.-S. Zheng, Lower bounds for multi-echelon stochastic inventory systems, Management Science 40(11), 1994. https://doi.org/10.1287/mnsc.40.11.1426
  • K. H. Shang and J.-S. Song, Newsvendor bounds and heuristic for optimal policies in serial supply chains, Management Science 49(5), 2003. https://doi.org/10.1287/mnsc.49.5.618.15147
  • S. C. Graves and S. P. Willems, Optimizing strategic safety stock placement in supply chains, Manufacturing & Service Operations Management 2(1), 2000. https://doi.org/10.1287/msom.2.1.68.23267
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Multistage Stochastic Optimization III: Distortion Risk Functionals and Their Dual RepresentationTextbook

Motivation

A decision maker who does not want to be judged by expected loss alone needs a functional that weighs the bad outcomes more heavily than the good ones and still behaves well under optimization: monotone, convex, unchanged by shifting the loss, and scaling with it. Kusuoka's theorem (mission II) says every such law-invariant functional on an atomless space is a supremum of mixtures of Average Values-at-Risk. The mixtures themselves are the distortion risk functionals of Denneberg (Distorted probabilities and insurance premiums, Methods of Operations Research 63, 1990) and Acerbi (Spectral measures of risk: A coherent representation of subjective risk aversion, Journal of Banking and Finance 26, 2002, doi:10.1016/S0378-4266(02)00281-9), also called spectral risk measures: integrals of the quantile function against a nondecreasing density σ\sigmaσ. They are the risk functionals used throughout Pflug and Pichler's book (doi:10.1007/978-3-319-08843-3) in the multistage objectives of Chapters 5 and 6, and the three representations proved in Sections 3.2 to 3.4 — as a supremum over densities ZZZ, as a maximum over uniform variables, and as an infimum over convex-conjugate constraints — are what make them computable inside an optimization model. This mission formalizes those representations.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P). A random variable Y:Ω→RY:\Omega\to\mathbb RY:Ω→R is a loss, and the functionals act on L∞L^\inftyL∞, the bounded measurable ones. The Value-at-Risk at level u∈(0,1]u\in(0,1]u∈(0,1] is the lower quantile V@Ru(Y)=inf⁡{y:P(Y≤y)≥u}\mathsf{V@R}_u(Y)=\inf\{y:P(Y\le y)\ge u\}V@Ru​(Y)=inf{y:P(Y≤y)≥u} and the Average Value-at-Risk at level α∈[0,1)\alpha\in[0,1)α∈[0,1) is AV@Rα(Y)=11−α∫α1V@Ru(Y) du\mathsf{AV@R}_\alpha(Y)=\frac{1}{1-\alpha}\int_\alpha^1\mathsf{V@R}_u(Y)\,duAV@Rα​(Y)=1−α1​∫α1​V@Ru​(Y)du, extended to α=1\alpha=1α=1 by the essential supremum (mission II). A risk functional satisfies the four axioms (M), (C), (T), (H) of Definition 3.2.

A distortion function is a nonnegative, nondecreasing σ:[0,1)→[0,∞)\sigma:[0,1)\to[0,\infty)σ:[0,1)→[0,∞) with ∫01σ=1\int_0^1\sigma=1∫01​σ=1, and the distortion risk functional with density σ\sigmaσ is

Rσ(Y)  =  ∫01σ(u) V@Ru(Y) du.\mathcal R_\sigma(Y)\;=\;\int_0^1\sigma(u)\,\mathsf{V@R}_u(Y)\,du .Rσ​(Y)=∫01​σ(u)V@Ru​(Y)du.

The Average Value-at-Risk is the case σα=(1−α)−11[α,1)\sigma_\alpha=(1-\alpha)^{-1}\mathbf 1_{[\alpha,1)}σα​=(1−α)−11[α,1)​. A random variable ZZZ is dominated by σ\sigmaσ, Z≼σZ\preccurlyeq\sigmaZ≼σ, when Z∈L1Z\in L^1Z∈L1, E(Z)=1\mathbb E(Z)=1E(Z)=1 and AV@Rα(Z)≤11−α∫α1σ\mathsf{AV@R}_\alpha(Z)\le\frac{1}{1-\alpha}\int_\alpha^1\sigmaAV@Rα​(Z)≤1−α1​∫α1​σ for every α∈[0,1)\alpha\in[0,1)α∈[0,1). A variable UUU is uniformly distributed when P(U≤u)=uP(U\le u)=uP(U≤u)=u on [0,1][0,1][0,1]. For h:R→Rh:\mathbb R\to\mathbb Rh:R→R the conjugate is h∗(s)=sup⁡y(s y−h(y))∈(−∞,+∞]h^*(s)=\sup_y(s\,y-h(y))\in(-\infty,+\infty]h∗(s)=supy​(sy−h(y))∈(−∞,+∞].

Formalization targets

Goal — Theorem 3.16 (printed pp. 105–106)

Rσ(Y)  =  sup⁡{E(Y⋅Z) : Z≼σ}(Y∈L∞).\mathcal R_\sigma(Y)\;=\;\sup\bigl\{\mathbb E(Y\cdot Z)\ :\ Z\preccurlyeq\sigma\bigr\} \qquad(Y\in L^\infty).Rσ​(Y)=sup{E(Y⋅Z) : Z≼σ}(Y∈L∞).

The distortion functional is a risk functional (printed p. 99)

Rσ\mathcal R_\sigmaRσ​ satisfies (M), (C), (T) and (H).

Representation (3.11) (printed p. 100)

There is a probability measure μ\muμ on [0,1][0,1][0,1] with Rσ(Y)=∫01AV@Rα(Y) μ(dα)\mathcal R_\sigma(Y)=\int_0^1\mathsf{AV@R}_\alpha(Y)\,\mu(d\alpha)Rσ​(Y)=∫01​AV@Rα​(Y)μ(dα) for all Y∈L∞Y\in L^\inftyY∈L∞.

Corollary 3.18 (printed pp. 107–108)

For α<1\alpha<1α<1, AV@Rα(Y)=sup⁡{E(YZ):EZ=1, AV@Rp(Z)≤11−α ∀p∈[α,1]}=sup⁡{E(YZ):EZ=1, 0≤Z≤11−α}\mathsf{AV@R}_\alpha(Y)=\sup\{\mathbb E(YZ):\mathbb EZ=1,\ \mathsf{AV@R}_p(Z)\le\frac1{1-\alpha}\ \forall p\in[\alpha,1]\} =\sup\{\mathbb E(YZ):\mathbb EZ=1,\ 0\le Z\le\frac1{1-\alpha}\}AV@Rα​(Y)=sup{E(YZ):EZ=1, AV@Rp​(Z)≤1−α1​ ∀p∈[α,1]}=sup{E(YZ):EZ=1, 0≤Z≤1−α1​}; for α=1\alpha=1α=1 the latter with the upper bound dropped.

Corollary 3.19 (printed p. 108)

On an atomless space, Rσ(Y)=max⁡{E(Y⋅σ(U)):U uniform}\mathcal R_\sigma(Y)=\max\{\mathbb E(Y\cdot\sigma(U)):U\text{ uniform}\}Rσ​(Y)=max{E(Y⋅σ(U)):U uniform}, the maximum attained.

Theorem 3.22 (printed p. 111)

Rσ(Y)=inf⁡{E(h(Y)):∫01h∗(σ(u)) du≤0}\mathcal R_\sigma(Y)=\inf\{\mathbb E(h(Y)):\int_0^1h^*(\sigma(u))\,du\le 0\}Rσ​(Y)=inf{E(h(Y)):∫01​h∗(σ(u))du≤0} over measurable h:R→Rh:\mathbb R\to\mathbb Rh:R→R.

Significance

Theorem 3.16 identifies the conjugate of a distortion functional: Rσ∗(Z)\mathcal R_\sigma^*(Z)Rσ∗​(Z) is 000 when Z≼σZ\preccurlyeq\sigmaZ≼σ and +∞+\infty+∞ otherwise, so Rσ\mathcal R_\sigmaRσ​ is the support function of an explicit convex set of densities. Everything else follows from that. Corollary 3.18 recovers the classical dual of the Average Value-at-Risk and shows that its constraints can be relaxed to the levels in [α,1][\alpha,1][α,1]; Corollary 3.19 turns the supremum into a maximum over couplings and identifies the maximizer, the co-monotone one, which is how distortion functionals are evaluated on scenario trees; Corollary 3.21, not stated here, combines the theorem with Kusuoka's representation to give the dual of every version independent risk functional. Theorem 3.22 goes the other way and writes Rσ\mathcal R_\sigmaRσ​ as an infimum, which is what converts a minimax problem — minimize a supremum over ZZZ — into a plain minimization over the decision and an auxiliary function hhh, the form in which the book solves risk-averse programs in Chapters 5 and 6.

Everything here is proved in the source and in the cited papers; the platform has the finite-scenario Artzner–Delbaen representation of coherent risk measures but nothing on distortion functionals, and Mathlib has no risk-measure material and no quantile-based representation theory. The definitions of this mission sit on those of mission II and are reused as such.

Difficulty

The obvious route to Theorem 3.16 is Fenchel–Moreau duality: Rσ\mathcal R_\sigmaRσ​ is convex and lower semicontinuous on L∞L^\inftyL∞, so it equals its biconjugate, and the task is to compute Rσ∗(Z)=sup⁡Y E(YZ)−Rσ(Y)\mathcal R_\sigma^*(Z)=\sup_Y\,\mathbb E(YZ)-\mathcal R_\sigma(Y)Rσ∗​(Z)=supY​E(YZ)−Rσ​(Y). The step where the naive computation stalls is bounding E(YZ)\mathbb E(YZ)E(YZ) by a quantity that depends only on the distributions of YYY and ZZZ: this is the rearrangement (Chebyshev, Hardy–Littlewood) inequality E(YZ)≤∫01GY−1(u)GZ−1(u) du\mathbb E(YZ)\le\int_0^1G_Y^{-1}(u)G_Z^{-1}(u)\,duE(YZ)≤∫01​GY−1​(u)GZ−1​(u)du, with equality for co-monotone couplings. Given it, Rσ∗(Z)=sup⁡Y∫01GY−1(GZ−1−σ)\mathcal R_\sigma^*(Z)=\sup_Y\int_0^1G_Y^{-1}(G_Z^{-1}-\sigma)Rσ∗​(Z)=supY​∫01​GY−1​(GZ−1​−σ), and testing with indicator-type YYY shows the supremum is 000 exactly when the upper-tail averages of ZZZ are dominated by those of σ\sigmaσ, which is the constraint Z≼σZ\preccurlyeq\sigmaZ≼σ. Neither the rearrangement inequality nor the identification of the conjugate is available in Mathlib.

For the corollaries the difficulties are concrete. Corollary 3.18 needs Z≥0Z\ge 0Z≥0 to be deduced from the constraints, which the source does by contradiction through the value p=P(Z<0)p=P(Z<0)p=P(Z<0). Corollary 3.19 needs the co-monotone coupling to exist, which is where the atomless hypothesis enters, and needs σ(U)\sigma(U)σ(U) to be feasible for (3.15), which uses Gσ(U)−1=σG_{\sigma(U)}^{-1}=\sigmaGσ(U)−1​=σ. Theorem 3.22 needs, besides the inequality E(h(Y))≥Rσ(Y)\mathbb E(h(Y))\ge\mathcal R_\sigma(Y)E(h(Y))≥Rσ​(Y) from Fenchel–Young, an admissible hhh that nearly attains it; the source builds it from σ\sigmaσ and GY−1G_Y^{-1}GY−1​ via Corollary 3.23.

Formalization scope

Random variables are functions Ω→R\Omega\to\mathbb RΩ→R on an arbitrary measurable space with a probability measure, exactly as in mission II, whose MemLinfty, valueAtRisk, averageValueAtRisk, IsRiskFunctional, Atomless and IsKusuokaMeasure are imported and not redefined. The distortion density is a function on R\mathbb RR constrained on [0,1)[0,1)[0,1); its integrability on (0,1)(0,1)(0,1) is part of the definition, and both ∫01σ\int_0^1\sigma∫01​σ and Rσ\mathcal R_\sigmaRσ​ integrate over the open interval, which excludes the level 000 where the quantile formula is not meaningful and changes no value.

Every supremum and infimum is over a subtype of functions satisfying the constraints, and the prose of each item records why the family is nonempty and bounded, so that no real supremum takes its junk value. Pointwise constraints on ZZZ are almost sure. The constraint of (3.15) is stated for α∈[0,1)\alpha\in[0,1)α∈[0,1): at α=1\alpha=1α=1 the source's expression is 0/00/00/0 and means the limit, and the constraint there is implied by the others; (3.19) at α=1\alpha=1α=1 is stated separately with the upper bound dropped. The conjugate takes values in the extended reals, and admissibility in Theorem 3.22 requires h∗(σ(u))h^*(\sigma(u))h∗(σ(u)) finite almost everywhere, integrable, with integral at most 000, and h(Y)h(Y)h(Y) integrable — the conditions under which the expectations in (3.24) are the integrals the source means.

Two hypotheses are added beyond the printed statements and are flagged in the items: atomless for Corollary 3.19, because otherwise no uniform variable need exist and the maximum would be over an empty set; and integrability of h(Y)h(Y)h(Y) in Theorem 3.22, without which Lean's integral of a non-integrable h(Y)h(Y)h(Y) is 000. Theorem 3.16 itself carries no atomless hypothesis, and the mission notes check the identity on two-point spaces by hand. A trivializing formalization — a constraint set that is empty or unbounded, so that the supremum is 000 — is excluded by the constant density Z≡1Z\equiv 1Z≡1, feasible for every σ\sigmaσ, and by Z≥0Z\ge 0Z≥0.

Welcome contributions beyond the milestones: Corollary 3.15 (the representation through the distribution function for Y≥0Y\ge 0Y≥0), Corollary 3.21 (the dual of a version independent risk functional through its Kusuoka set), Corollary 3.23, and the explicit mixing measure (3.12).

Selected references

  • Georg Ch. Pflug and Alois Pichler, Multistage Stochastic Optimization, Springer, 2014, Sections 3.2–3.4. doi:10.1007/978-3-319-08843-3
  • Carlo Acerbi, Spectral measures of risk: A coherent representation of subjective risk aversion, Journal of Banking and Finance 26 (2002). doi:10.1016/S0378-4266(02)00281-9
  • Shigeo Kusuoka, On law invariant coherent risk measures, Advances in Mathematical Economics 3 (2001). doi:10.1007/978-4-431-67891-5_4
  • Alois Pichler, The natural Banach space for version independent risk measures, Insurance: Mathematics and Economics 53 (2013). doi:10.1016/j.insmatheco.2013.07.005
  • Georg Ch. Pflug and Werner Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. doi:10.1142/6478
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Dynamical SystemsMathematical Physics·Captain: Lucas

Dynamics and Relativity I: Kepler's Laws from the Inverse-Square LawTextbook

Motivation

The derivation of Kepler's three laws from Newton's inverse-square law of gravitation is the calculation with which mathematical physics begins. Kepler published the laws in 1609 and 1619 as empirical regularities distilled from Tycho Brahe's naked-eye astrometry: planets travel on ellipses with the Sun at a focus, the Sun–planet segment sweeps equal areas in equal times, and the square of the orbital period scales as the cube of the orbit's size. That an attractive force falling off as 1/r21/r^21/r2 forces exactly these three regularities was established by Newton in the Principia (1687); as David Tong remarks in the source notes, the third law was within reach of several of Newton's contemporaries, but the derivation of the first — that the orbit is a conic section with the centre of attraction at a focus — was Newton's alone.

This mission formalizes that derivation as it is presented in §4 (Central Forces) of David Tong's Dynamics and Relativity, the Cambridge Part IA Mathematical Tripos lecture notes (Lent 2013). It is the first mission in a series covering those notes, and it targets the chapter's capstone, Kepler's first law.

Setting

A point particle of mass m>0m>0m>0 moves in Euclidean 333-space along a trajectory x:R→R3x:\mathbb R\to\mathbb R^3x:R→R3, assumed twice continuously differentiable and never passing through the origin, where the field below is singular. Write r(t)=∥x(t)∥r(t)=\lVert x(t)\rVertr(t)=∥x(t)∥ and r^=x/r\hat r = x/rr^=x/r.

The particle moves in a central force field when it obeys Tong's equation of motion (4.1),

m x¨(t)  =  F(r(t)) r^(t),m\,\ddot x(t) \;=\; F\big(r(t)\big)\,\hat r(t),mx¨(t)=F(r(t))r^(t),

where F:R→RF:\mathbb R\to\mathbb RF:R→R gives the radial component of the force at distance rrr; for a force derived from a central potential V(r)V(r)V(r) one has F=− dV/drF=-\,dV/drF=−dV/dr. The Kepler problem (Tong §4.3.1) is the inverse-square special case, potential (4.12)

V(r)=−k mr,F(r)=−k mr2,V(r) = -\frac{k\,m}{r}, \qquad F(r) = -\frac{k\,m}{r^{2}},V(r)=−rkm​,F(r)=−r2km​,

with k=GM>0k=GM>0k=GM>0 for gravitational attraction by a mass MMM fixed at the origin. (The same equations govern the Coulomb problem, with k=−qQ/4πϵ0mk=-qQ/4\pi\epsilon_0 mk=−qQ/4πϵ0​m, which is repulsive when k<0k<0k<0; this mission fixes k>0k>0k>0.)

Two conserved quantities organize the problem. The angular momentum is the vector

L(t)  =  m x(t)×x˙(t),L(t) \;=\; m\,x(t)\times\dot x(t),L(t)=mx(t)×x˙(t),

and we write l=∥L∥/ml=\lVert L\rVert/ml=∥L∥/m for the angular momentum per unit mass, which in the plane polar coordinates of Tong (4.5) is l=r2θ˙l=r^{2}\dot\thetal=r2θ˙. The total energy of the Kepler problem is

E(t)  =  12m∥x˙(t)∥2  −  k mr(t).E(t) \;=\; \tfrac12 m\lVert \dot x(t)\rVert^{2} \;-\; \frac{k\,m}{r(t)} .E(t)=21​m∥x˙(t)∥2−r(t)km​.

Tong's solution (4.14) of the orbit equation states that the trajectory lies on a conic section with a focus at the origin. Coordinate-free, this says that there is a fixed eccentricity vector A∈R3A\in\mathbb R^3A∈R3, pointing towards the point of closest approach, with

r(t)+⟨A,x(t)⟩  =  r0for all t,r0=l2k,r(t) + \langle A, x(t)\rangle \;=\; r_0 \qquad\text{for all } t, \qquad r_0 = \frac{l^{2}}{k},r(t)+⟨A,x(t)⟩=r0​for all t,r0​=kl2​,

which is Tong's r=r0/(1+ecos⁡θ)r = r_0/(1+e\cos\theta)r=r0​/(1+ecosθ) with e=∥A∥e=\lVert A\rVerte=∥A∥ the eccentricity and θ\thetaθ measured from the direction of AAA, and r0r_0r0​ the semi-latus rectum.

Finally, a set S⊆R3S\subseteq\mathbb R^3S⊆R3 is an ellipse with a focus at the origin when there are a nonzero normal vector nnn, a second focus ccc with ⟨n,c⟩=0\langle n,c\rangle=0⟨n,c⟩=0, and a real number aaa with ∥c∥<2a\lVert c\rVert<2a∥c∥<2a, such that SSS is exactly the set of points yyy of the plane {y:⟨n,y⟩=0}\{y : \langle n,y\rangle = 0\}{y:⟨n,y⟩=0} satisfying the two-foci (string) property

∥y∥+∥y−c∥  =  2a.\lVert y\rVert + \lVert y - c\rVert \;=\; 2a .∥y∥+∥y−c∥=2a.

The inequality ∥c∥<2a\lVert c\rVert<2a∥c∥<2a forces a>0a>0a>0 and rules out the degenerate loci; c=0c=0c=0 gives a circle.

Target

The goal theorem is Kepler's first law, K1 of Tong §4.3.2: each planet moves in an ellipse, with the Sun at one focus. Formally, for a trajectory xxx of the attractive inverse-square problem with nonvanishing angular momentum and negative total energy,

k>0,L≠0,E<0  ⟹  ∃ S an ellipse with a focus at the origin such that x(t)∈S for all t.k>0,\quad L\neq 0,\quad E<0 \;\Longrightarrow\; \exists\,S \text{ an ellipse with a focus at the origin such that } x(t)\in S \text{ for all } t.k>0,L=0,E<0⟹∃S an ellipse with a focus at the origin such that x(t)∈S for all t.

The hypothesis L≠0L\neq0L=0 excludes purely radial free-fall, whose trajectory is a segment rather than an ellipse, and E<0E<0E<0 is the bounded regime, which by Tong (4.16) is exactly e<1e<1e<1.

The milestones follow the source in order: conservation of angular momentum and the resulting planarity of the motion (§4, p. 48); Kepler's second law (K2), which holds for any central force; conservation of energy; the conic orbit (4.14); the identification of a conic of eccentricity e<1e<1e<1 as an ellipse with a focus at the origin (4.15); the energy–eccentricity relation (4.16); and Kepler's third law (K3, p. 62),

T  =  2π R3/2GM,R=12(rmin⁡+rmax⁡).T \;=\; \frac{2\pi\,R^{3/2}}{\sqrt{GM}}, \qquad R = \tfrac12\big(r_{\min}+r_{\max}\big).T=GM​2πR3/2​,R=21​(rmin​+rmax​).

Significance

The result. K1 is the statement that fixes the inverse-square law among all central force laws: K2 holds for every central force, and dimensional analysis alone gives the shape of K3, but closed orbits that are exact ellipses with the attracting centre at a focus are special to the 1/r21/r^21/r2 force (and to the harmonic force, with the centre at the centre of the ellipse). Everything quantitative in classical celestial mechanics — orbit determination, the mass–period relation used to weigh binary stars, and the perturbative treatment of precession that eventually exposed the anomaly in Mercury's orbit — is built on the Kepler solution.

Formalizing it. The mathematics has been settled for three centuries; what this mission produces is a machine-checked treatment of the Newtonian derivation, starting from the differential equation rather than from a prescribed orbit. Mathlib has no central-force or two-body library, so the definitions here — central force motion, angular momentum, conserved energy, swept area, and the two-foci characterization of an ellipse — are new and reusable across the rest of the series and by any later mission in classical mechanics. The existing platform mission Celestial Mechanics I: Binary Star Systems runs the complementary direction, verifying that a prescribed conic orbit satisfies the equations of motion and reducing the two-body problem to a one-body problem; the present mission asks for the converse, which is the harder half and the one Newton is credited with.

Difficulty

The derivation in the source changes the independent variable from time ttt to the polar angle θ\thetaθ, substitutes u=1/ru=1/ru=1/r, and solves the resulting linear oscillator equation (4.11). Each of those steps needs infrastructure that does not exist in Mathlib. There is no polar-angle function attached to a curve in the plane: one has to produce a continuously differentiable angle θ(t)\theta(t)θ(t) lifting the trajectory, show θ˙=l/r2\dot\theta = l/r^{2}θ˙=l/r2 never vanishes so that θ\thetaθ is a legitimate change of variable, and then transport a second-order ODE through that reparametrization. Solving (4.11) then requires a uniqueness theorem for the inhomogeneous harmonic oscillator, and reading the conic back into Cartesian form requires the algebra of (4.15).

Kepler's third law carries an extra burden beyond the formula: the statement quantifies over the least period of the motion, so a solution must establish that a negative-energy orbit is periodic at all, and must identify inf⁡tr(t)\inf_t r(t)inft​r(t) and sup⁡tr(t)\sup_t r(t)supt​r(t) as the periapsis and apoapsis distances r0/(1±e)r_0/(1\pm e)r0​/(1±e).

Formalization scope

Trajectories are maps ℝ → EuclideanSpace ℝ (Fin 3), with ContDiff ℝ 2 smoothness and the standing hypothesis x(t)≠0x(t)\neq0x(t)=0 for all ttt built into the definition of central force motion, together with m>0m>0m>0. Time is all of R\mathbb RR: the trajectories considered are globally defined, so collision orbits are excluded by hypothesis rather than by a maximal-interval argument. Derivatives are Mathlib's deriv, so velocity and acceleration are the first and second derivatives of the trajectory.

Three conventions are worth flagging. First, the force is given by its radial profile FFF rather than by a potential, avoiding any appeal to the junk value of a derivative at 000; the Kepler case is the instance F(r)=−km/r2F(r)=-km/r^{2}F(r)=−km/r2. Second, the swept area of K2 is the integral 12∫∥x×x˙∥ dt\tfrac12\int\lVert x\times\dot x\rVert\,dt21​∫∥x×x˙∥dt, which is the standard area element 12r2 dθ\tfrac12 r^2\,d\theta21​r2dθ of the source written invariantly; the content of K2 is that this integrand is constant in time, so that the area depends on t1−t0t_1-t_0t1​−t0​ alone. Third, K1 asserts that the trajectory is contained in an ellipse; it does not assert that the particle traverses the whole ellipse, which is a separate (true) statement about periodic orbits.

The degenerate readings are ruled out explicitly. The eccentricity vector formulation of the conic is an equation holding at every time, not an existence claim at one time; the ellipse predicate carries ∥c∥<2a\lVert c\rVert<2a∥c∥<2a, so a point or a segment does not qualify; and the hypothesis L≠0L\neq0L=0 in K1 and in the conic milestone is necessary, since a radial trajectory satisfies every other hypothesis but lies on no ellipse.

Contributions of independent interest are welcome: a plane polar coordinate API for curves, uniqueness for the forced harmonic oscillator, and the classification of the loci r+⟨A,x⟩=r0r+\langle A,x\rangle = r_0r+⟨A,x⟩=r0​ into ellipse, parabola and hyperbola according to ∥A∥<1\lVert A\rVert<1∥A∥<1, =1=1=1, >1>1>1 (this mission needs only the first case) would all be reusable well beyond this series.

Selected references

  • David Tong, Dynamics and Relativity, University of Cambridge Part IA Mathematical Tripos lecture notes, Lent 2013, §4 (Central Forces), pp. 48–62. http://www.damtp.cam.ac.uk/user/tong/relativity.html
  • Isaac Newton, Philosophiæ Naturalis Principia Mathematica, 1687, Book I, Propositions XI–XVII.
  • S. Chandrasekhar, Newton's Principia for the Common Reader, Oxford University Press, 1995.
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Control TheoryLinear OptimizationOperations Research+2·Captain: mikedeng1

Resource Allocation and Cross-Layer Control in Wireless Networks I: The Network Layer Capacity RegionTextbook

Motivation

Every wireless network control algorithm — routing, scheduling, power control, admission control — is ultimately judged against one question: which traffic loads can it keep stable? Answering that question requires a precise, algorithm-independent notion of queueing stability under random arrivals and a randomly time-varying, possibly non-ergodic-looking channel. Tassiulas & Ephremides (1992) and Neely, Modiano & Rohrs (2005) developed the framework used throughout Georgiadis, Neely & Tassiulas's survey Resource Allocation and Cross-Layer Control in Wireless Networks (Foundations and Trends in Networking, 2006): "strong stability" of a queue backlog process, defined purely through the time-averaged expected backlog, with no assumption that the arrival or service process is stationary, Markov, or even has a well-defined long-run average. The present mission formalizes the chapter's foundational single-queue results — the two structural facts every later network-wide capacity and control result in the book is built from.

Setting

A queue is described by three processes on slots t=0,1,2,…t=0,1,2,\dotst=0,1,2,…: an arrival process A(t)A(t)A(t) (new bits admitted at the end of slot ttt), a service process svc(t)\mathrm{svc}(t)svc(t) (the transmission rate offered during slot ttt), and the backlog U(t)U(t)U(t), evolving by the queueing law

U(t+1)=max⁡[U(t)−svc(t),0]+A(t).U(t+1)=\max[U(t)-\mathrm{svc}(t),0]+A(t).U(t+1)=max[U(t)−svc(t),0]+A(t).

The queue is strongly stable if its expected backlog has a bounded time average, lim sup⁡t→∞1t∑τ=0t−1E{U(τ)}<∞\limsup_{t\to\infty}\frac1t\sum_{\tau=0}^{t-1}\mathbb E\{U(\tau)\}<\inftylimsupt→∞​t1​∑τ=0t−1​E{U(τ)}<∞. An arrival process is admissible with rate λ\lambdaλ if (i) its time-average expected rate is λ\lambdaλ, (ii) its second moment conditioned on the history is uniformly bounded, and (iii) for every δ>0\delta>0δ>0 there is an averaging window over which the conditional average rate exceeds λ\lambdaλ by at most δ\deltaδ, uniformly in the starting time — a robust substitute for "the rate is exactly λ\lambdaλ" that holds for i.i.d., Markov-modulated, and burstiness-constrained arrivals alike. A service process is admissible with rate μ\muμ analogously, with a deterministic pointwise upper bound in place of the second-moment condition. Both notions are formalized here on a filtered probability space (Ω,P,F)(\Omega,P,\mathcal F)(Ω,P,F), with F(t)\mathcal F(t)F(t) the history of slots 0,…,t−10,\dots,t-10,…,t−1 exactly as the book's own H(t)\mathcal H(t)H(t).

Formalization targets

Goal — Lemma 3.6 (Stability Conditions under Admissibility)

(a) λ≤μ is necessary for strong stability;(b) λ<μ is sufficient for it.\text{(a) } \lambda\le\mu \text{ is necessary for strong stability;}\qquad \text{(b) } \lambda<\mu \text{ is sufficient for it.}(a) λ≤μ is necessary for strong stability;(b) λ<μ is sufficient for it.

This is the chapter's central single-queue result: it converts the purely structural notion of strong stability into the one comparison — arrival rate versus service rate — that every later capacity-region and control-algorithm argument in the book reduces to.

Milestone — Lemma 3.3 (Necessary Condition for Strong Stability)

if U is strongly stable and E{A(t)}≤Amax⁡ ∀t (or E{svc(t)−A(t)}≤Dmax⁡ ∀t), then lim⁡t→∞E{U(t)}/t=0.\text{if } U \text{ is strongly stable and } \mathbb E\{A(t)\}\le A_{\max}\ \forall t \text{ (or } \mathbb E\{\mathrm{svc}(t)-A(t)\}\le D_{\max}\ \forall t\text{), then } \lim_{t\to\infty}\mathbb E\{U(t)\}/t=0.if U is strongly stable and E{A(t)}≤Amax​ ∀t (or E{svc(t)−A(t)}≤Dmax​ ∀t), then t→∞lim​E{U(t)}/t=0.

This is the elementary real-analysis fact — no admissibility, no probability beyond an already-given expectation sequence — that underlies the necessity half of Lemma 3.6's proof.

Significance

Strong stability and the admissibility framework are the load-bearing definitions of the entire book: every later chapter's algorithm-performance theorem (Chapter 4's backpressure throughput optimality, Chapter 5's utility-optimal Lyapunov drift bound, Chapter 6's energy-constrained control) is a theorem about when its induced queues are strongly stable, and every one of those proofs cites Lemma 3.6 (or its network generalization, Theorem 3.8's capacity region) as the final step converting a drift bound into a stability conclusion. Formalizing it fixes, once for the whole series, the precise real-analysis and conditional-expectation content of "arrival rate below service rate implies stability" that a Prove2Me solver would otherwise have to reconstruct from scratch for each downstream chapter.

Formalizing it. No result in this mission has a machine-checked proof anywhere; nothing adjacent exists on the platform (searched for strong stability, admissible arrival process, Lyapunov drift, network capacity region — the one hit, a Foster–Lyapunov hitting-time bound for a finite-state MDP, is a scalar drift-to-a-target-state object, not a queue-backlog vector with no absorbing state, and is not reused). This mission is the first formalization of either result.

Difficulty

The obvious first idea for the sufficiency half (b) is to try to bound E{U(t)}\mathbb E\{U(t)\}E{U(t)} directly by unrolling the queueing recursion and taking expectations termwise. This fails immediately: expectation does not commute with max⁡(⋅,0)\max(\cdot,0)max(⋅,0), so E{U(t+1)}≠max⁡[E{U(t)}−E{svc(t)},0]+E{A(t)}\mathbb E\{U(t+1)\}\ne\max[\mathbb E\{U(t)\}-\mathbb E\{\mathrm{svc}(t)\},0]+\mathbb E\{A(t)\}E{U(t+1)}=max[E{U(t)}−E{svc(t)},0]+E{A(t)} in general — the whole reason admissibility's second-moment and TTT-slot averaging clauses exist is to control exactly this gap between the pathwise recursion and its expectation, via a genuine (non-elementary) drift argument. The necessity half (a) has the opposite trap: it is tempting to prove λ≤μ\lambda\le\muλ≤μ from a single-slot expectation inequality, but a queue can be strongly stable while E{U(t)}\mathbb E\{U(t)\}E{U(t)} oscillates on any finite window, so the argument has to go through the time-averaged (Lemma 3.3) quantity, not a slot-by-slot one.

Formalization scope

Admissibility's conditional-expectation clauses are stated with Mathlib's Filtration ℕ and condExp (P[f | 𝓕 t]), following this platform's established idiom for martingale-difference hypotheses. Every conditional or plain expectation in a defining clause carries an explicit Integrable guard, because Mathlib's Bochner integral and condExp both silently default to 0 on a non-integrable function — without the guard, a process with an undefined or infinite second moment would satisfy admissibility vacuously, which is not the book's assumption (the book assumes these moments are finite; it never derives it). Lemma 3.3 is formalized directly on the real sequences representing E{U(t)}\mathbb E\{U(t)\}E{U(t)}, E{A(t)}\mathbb E\{A(t)\}E{A(t)}, E{svc(t)}\mathbb E\{\mathrm{svc}(t)\}E{svc(t)} — exactly the content the book's own statement and proof use, with no further probabilistic structure, since the lemma's hypotheses and conclusion never mention anything but these expectations. Out of scope for this mission: the network-wide capacity region (Definition 3.7, Theorem 3.8, Corollaries 3.9-3.10) and the graph-family construction Γ\GammaΓ/Cl{Γ}\mathrm{Cl}\{\Gamma\}Cl{Γ} of §3.2-3.3. Faithfully formalizing "λ\lambdaλ is stably supportable by the network" requires embedding admissible-process realizations into a full multi-queue routing model, which is substantially heavier than either result formalized here and was left out entirely — per this series' faithfulness-over-coverage rule — rather than approximated by, e.g., dropping the second-moment or TTT-slot clauses of admissibility, which would silently change what "admissible" means. A trivializing formalization to rule out: defining AdmissibleArrival/AdmissibleService without the Integrable guards above would make Lemma 3.6 provable by choosing a non-integrable process, which is not the book's theorem.

Selected references

  • Georgiadis, Neely & Tassiulas, Resource Allocation and Cross-Layer Control in Wireless Networks, Foundations and Trends in Networking, Vol. 1, No. 1 (2006), pp. 1-144. https://doi.org/10.1561/1300000001
  • Tassiulas & Ephremides, "Stability properties of constrained queueing systems and scheduling policies for maximum throughput in multihop radio networks", IEEE Transactions on Automatic Control, 37(12), 1992. https://doi.org/10.1109/9.182479
  • Neely, Modiano & Rohrs, "Dynamic power allocation and routing for time-varying wireless networks", IEEE Journal on Selected Areas in Communications, 23(1), 2005. https://doi.org/10.1109/JSAC.2004.837349
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Graph TheoryOperations ResearchTheoretical Computer Science·Captain: mikedeng1

The Design of Competitive Online Algorithms via a Primal-Dual Approach VII: Online Group Steiner TreesTextbook

Motivation

The group Steiner tree problem generalizes the ordinary Steiner tree problem: given a rooted tree and several groups of vertices, find a minimum-cost subtree that connects at least one vertex of each group to the root. It is a canonical instance of the generalized-connectivity family this survey studies in Chapter 11 — a family that also contains the online set-cover problem (Chapter 5 of this series) as a special case. Buchbinder and Naor's chapter shows how to convert the celebrated offline randomized-rounding algorithm of Garg, Konjevod and Ravi [56] into an online one, by imitating its per-edge coupling structure one iteration at a time as the online fractional solution (obtained from this survey's own Chapter 4 framework) evolves. This mission formalizes that online rounding scheme's three defining probabilistic guarantees and the resulting competitive-ratio theorem.

Setting

Fix a rooted tree T = (V, E, r) with non-negative edge costs c : E → ℝ, and k groups g₁, …, g_k ⊆ V, each request (r, gᵢ) arriving online. An online covering algorithm (from Chapter 4's framework, applied to the LP relaxation of this connectivity problem) maintains a monotonically increasing fractional weight w : E → ℝ on the edges, reinterpreted so that wₑ is the maximum flow that can be routed through e to any vertex of its subtree — a technical substitution needed so weights are monotone non-increasing along any root-to-leaf path, the property the rounding algorithm requires. At the end of each iteration in which some weights are augmented from w to w' = w + δ, the rounding algorithm processes every edge e with δₑ > 0, in topological order starting from the root, and randomly decides whether to add it to a growing random edge-cover C ⊆ E: deterministically, if w'ₑ > 1; via a single coin flip, if e is incident to the root or its parent edge's inclusion in C is already certain; via a coin flip conditional on the parent edge already being in C, otherwise. Because a coin is only ever flipped for a child once its parent is (or is already known to be) in C, C always induces a connected subtree containing the root.

Formalization targets

Theorem 11.4 (the goal, p. 231): there is a randomized online algorithm for the group Steiner problem in trees with competitive ratio O(log²n log k), where n is the number of leaves. It is built by running T independent trials of the rounding scheme in parallel and taking the union of the resulting covers, for T chosen (this mission's own explicit derivation — the book gives only the narrative "we run O(log k log N) independent trials... using simple probabilistic analysis") so that every group fails to be covered with probability at most 1/(2k), while the union's expected cost stays at T · log(n) · OPT.

Three milestones, in attack order, each stated exactly as the book states it (p. 230-231), with the book's own caveat "we state the main lemmas and omit the proofs" preserved — no in-source proof exists for any of the three beyond the algorithm's own description, so each is left sorry with no invented proof strategy:

  • Lemma 11.1: at the end of an iteration, ℙ[e ∈ C] = w'ₑ for every edge, and ℙ[e ∈ C] = 1 whenever wₑ > 1 already.
  • Lemma 11.2: the expected cost of C is at most ∑_{e∈T} cₑ w'ₑ (linearity of expectation applied to Lemma 11.1).
  • Lemma 11.3: for a group g of size at most N with total routable flow wg ≥ 1, the probability some vertex of g is covered is Ω(1/log N).

Significance

This is the survey's most involved application of the primal-dual framework: unlike Chapters 5, 9, 10 and 13, which round a single scalar decision per online step, the group Steiner algorithm must couple an entire iteration's worth of edge decisions so that the resulting random set stays a connected subtree — the coin-flip probabilities in the Algorithm box are exactly the minimal adjustment needed to keep marginal probabilities matching the fractional solution while preserving this connectivity invariant online. No formal development of the group Steiner problem (online or offline) was found on the platform as of 2026-09-20; this mission is the first.

Difficulty

Two distinct obstacles. First, faithfully representing "the probability that e ∈ C" for an online, coupled random process without assuming its proof: the mission represents the algorithm's random cover as an abstract finite probability distribution RandomCover E and states each lemma as an implication from the Algorithm box's three coupling rules (transcribed as hypotheses on marginal and conditional probabilities) to the claimed marginal or expected-value conclusion — capturing exactly what the book asserts without proof, rather than either assuming the conclusion trivially or constructing a full multi-iteration coupled process (which the source's own "we omit the proofs" indicates is genuinely nontrivial, citing [56]). Second, Theorem 11.4's own competitive ratio is stated in the book only asymptotically, with a purely narrative derivation ("we run O(log k log N) independent trials... we get a competitive ratio of O(log n log k log N)... probability at least 1 − 1/k") and no displayed formula anywhere in the chapter. Per this series' explicit-constants rule, this mission supplies its own explicit closed form for the number of trials T and the resulting bounds via a standard Chernoff/union-bound argument applied to Lemma 11.3's constant α; this derivation is the mission's own (documented below), not a transcription, since none exists in the source to transcribe.

Formalization scope

RandomCover E is a finite pmf p : Finset E → ℝ (Finset E itself finite since E is Fintype), with marg, condProb and expectedCost/probHits derived from it by ordinary Finset sums — no measure theory, since the sample space is always finite. RoundedTree E bundles parent : E → Option E (e(p)) and a non-negative cost. Lemma 11.3's wg (the flow routable to a group's vertices simultaneously) is left as hypothesis-supplied data rather than defined via an explicit max-flow formalization, which this mission's scope does not require (welcome contribution). Theorem 11.4's number of trials is the explicit closed form T = ⌈(log N · log(2k)) / α⌉, α the (existentially quantified, uniform) constant from Lemma 11.3; its coverage guarantee is 1 − 1/(2k) per group (this mission's own union-bound derivation), not the book's stated 1 − 1/k — the book reaches the stronger bound via an additional shortest-path fallback mechanism for any group the trials miss, which is out of scope here (welcome contribution, along with completing any of the four sorrys and formalizing Theorem 11.5's extension to general graphs via HST embedding, out of scope since it depends on an external embedding result not proved in this book).

Selected references

  • N. Buchbinder, J. Naor. The Design of Competitive Online Algorithms via a Primal-Dual Approach. Foundations and Trends in Theoretical Computer Science, 3(2-3):93-263, 2009. https://doi.org/10.1561/0400000024
  • N. Garg, G. Konjevod, R. Ravi. A polylogarithmic approximation algorithm for the group Steiner tree problem. Journal of Algorithms, 37(1):66-84, 2000 (cited as [56] in the survey).
  • N. Alon, B. Awerbuch, Y. Azar, N. Buchbinder, J. Naor. A general approach to online network optimization problems. ACM Transactions on Algorithms, 2(4):640-660, 2006 (cited as [4], the source of this chapter's results per the Notes, p. 231).
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The Design of Competitive Online Algorithms via a Primal-Dual Approach II: The Online Set-Cover ProblemTextbook

Motivation

Section 4 of this survey derives a simple randomized O(log⁡mlog⁡n)O(\log m \log n)O(logmlogn)-competitive algorithm for the online set-cover problem, by rounding the fractional solution the online packing-covering framework produces. An intriguing question the survey poses next: can the same guarantee be achieved deterministically? The standard tool for removing randomness, the method of conditional expectations, requires finding a pessimistic estimator — a potential function whose value the algorithm can track and whose behavior certifies the randomized algorithm's guarantee step by step. Chapter 5 constructs exactly this potential function for the weighted online set-cover problem, and shows that greedily minimizing it online reproduces the randomized algorithm's competitive ratio with no randomness at all. This mission formalizes that construction: the potential function itself (Lemma 5.1) and the correctness guarantee it buys (Theorem 5.2).

Setting

Fix a finite universe of elements EEE and a finite family of sets TTT with positive costs csc_scs​, both known to the algorithm in advance (only which elements will actually need covering, and in what order, is unknown). A monotonically increasing assignment w:T→Rw : T \to \mathbb{R}w:T→R of fractional weights to sets is produced online by a fractional subroutine (any O(log⁡m)O(\log m)O(logm)- competitive online fractional algorithm — the survey's own Section 4.2 supplies one). An element's weight is we:=∑s∣e∈swsw_e := \sum_{s \mid e \in s} w_swe​:=∑s∣e∈s​ws​. Given a target α≥c(COPT)\alpha \ge c(C_{OPT})α≥c(COPT​) (a guessed upper bound on the optimal integral cover's cost — the survey handles an unknown optimum by doubling this guess across phases, outside this chapter's own scope), the algorithm maintains a chosen cover C⊆TC \subseteq TC⊆T and the potential

Φ  =  ∑e∉Cˉn2we  +  n⋅exp⁡ ⁣(12α∑s(csχC(s)−3wscslog⁡n)),\Phi \;=\; \sum_{e \notin \bar C} n^{2w_e} \;+\; n \cdot \exp\!\Big(\tfrac{1}{2\alpha} \sum_{s} \big(c_s \chi_C(s) - 3 w_s c_s \log n\big)\Big),Φ=e∈/Cˉ∑​n2we​+n⋅exp(2α1​s∑​(cs​χC​(s)−3ws​cs​logn)),

where n=∣E∣n = |E|n=∣E∣ and χC\chi_CχC​ is CCC's characteristic function. Whenever a set sss's weight increases, the algorithm computes Φ\PhiΦ both with and without adding sss to CCC and chooses whichever keeps Φ\PhiΦ from exceeding its value before the step (failing only if neither does, which Lemma 5.1 shows cannot happen when α≥c(COPT)\alpha \ge c(C_{OPT})α≥c(COPT​)).

Formalization targets

Theorem 5.2 (goal, p. 139): given the invariant Φ<n2\Phi < n^2Φ<n2 that Lemma 5.1 maintains throughout a run, (i) every element of weight ≥1\ge 1≥1 is covered, and (ii) the chosen cover costs at most α⋅O(log⁡mlog⁡n)\alpha \cdot O(\log m \log n)α⋅O(logmlogn).

Lemma 5.1 (milestone, p. 137): the potential function never increases in expectation across a weight-augmenting step, under the algorithm's own randomized choice of whether to add the augmented set to the cover (the internal argument — via the method of conditional expectations — that certifies the deterministic algorithm's choice rule never fails).

Significance

This chapter answers, for the online set-cover problem specifically, a question that recurs throughout online algorithm design: when can a randomized guarantee be derandomized online? The potential-function technique here is the survey's own template for the answer (it recurs, per the chapter's Notes section, in the routing algorithm of Chapter 9 and the ad-auctions algorithm of Chapter 10, both formalized as separate missions in this series) — a self-contained, reusable instance of "derandomization via an explicit pessimistic estimator" in the online setting, distinct from the offline set-cover primal-dual and dual-fitting algorithms of this book's own Chapter 2, already on the platform (PrimalDualOnline.SetCover.*, checked below: a static instance with no arrival order and no potential function, a genuinely different model).

Difficulty

The central formalization challenge is that Lemma 5.1's own statement, "Φend≤Φstart\Phi_{end} \le \Phi_{start}Φend​≤Φstart​", denotes the potential's value in expectation under the algorithm's randomized choice — not a single deterministic before/after pair — since the lemma is proved via a probabilistic argument (adding sss to the cover with probability 1−n−2δs1 - n^{-2\delta_s}1−n−2δs​) whose role is purely internal to justifying the deterministic algorithm's rule (choose whichever of the two options controls Φ\PhiΦ). Stating the lemma as a bare inequality between two potential values, without the mixture, would either be false (the "add sss" branch alone can increase Φ\PhiΦ) or would silently smuggle in the derandomized choice as a hypothesis rather than proving it is always available. This mission states the expectation explicitly as a probability-weighted average of the two branch potentials, matching the actual analytic content of the book's proof (equations 5.1-5.6) rather than its final one-line restatement.

Formalization scope

SetCoverInstance E T bundles elemSets : E → Finset T (the sets containing an element) and positive costs c. elementWeight and coveredBy are literal transcriptions of wew_ewe​ and "e∈Cˉe \in \bar Ce∈Cˉ". potential transcribes Φ\PhiΦ's displayed formula verbatim, with n cast from Fintype.card E. potential_nonincreasing (Lemma 5.1) is the expectation inequality described above. algorithm_correctness (Theorem 5.2) takes the potential invariant Φ < n² as a hypothesis (the state Lemma 5.1, applied repeatedly from the initial value Φ<n2\Phi < n^2Φ<n2, is what the book's own proof shows every reachable state satisfies) together with an explicit ratio β standing for "the fractional solution is O(log m)-competitive" (∑ wₛcₛ ≤ βα) — the book imports this fact from Section 4 as a black-box subroutine rather than re-deriving a specific numeric constant in this chapter, and this mission does the same rather than re-deriving Chapter 4's own constant under the (different) d→md \to md→m substitution the book's prose glosses over. The conclusion is then the fully explicit α · log n · (3β + 2), matching the book's own derivation (displayed inequality, p. 139-140) with O(log m) replaced by the parameter β. This correctly rules out the trivializing formalization in which the O(log m log n) bound is left as an unquantified existential constant, or in which Φ's invariant is assumed directly as an unmotivated free hypothesis rather than the fact Lemma 5.1 is what actually establishes. Reals throughout; Real.log, Real.exp, Real.rpow (via the ^ notation on reals) for the book's own log, exp and n^{2w_e}. Nothing here is reused from 04-framework (concurrent draft; per this series' own rule, drafts do not import drafts) even though this chapter's fractional subroutine is conceptually the same online covering framework — restated here only as the abstract ratio β, not as a Lean dependency. Welcome contributions: completing the two sorrys, and formalizing the doubling-across-phases wrapper (Section 5.1's "Obtaining a Deterministic Algorithm" discussion) that removes the need to know α ≥ c(C_OPT) in advance.

Selected references

  • N. Buchbinder, J. Naor. The Design of Competitive Online Algorithms via a Primal-Dual Approach. Foundations and Trends in Theoretical Computer Science, 3(2-3):93-263, 2009. https://doi.org/10.1561/0400000024
  • N. Alon, B. Awerbuch, Y. Azar, N. Buchbinder, J. Naor. The online set cover problem. STOC 2003 / SIAM J. Comput. 39(2), 2009 (cited by this book's Chapter 5 Notes as [3]).
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Ablowitz–Chakravarty–Halburd: the Chazy–Ramanujan correspondence and the Darboux–Halphen reduction of self-dual Yang–MillsResearch Paper

Motivation

In 1985 R. S. Ward conjectured that "many (and perhaps all?) of the ordinary and partial differential equations that are regarded as being integrable or solvable may be obtained from the self-dual gauge field equations (or its generalizations) by reduction". The self-dual Yang–Mills (SDYM) equations are therefore often called the master integrable system: choosing a gauge algebra and a symmetry group to reduce by produces, on the one hand, the classical soliton equations and the Painlevé transcendents, and on the other — once infinite-dimensional gauge algebras are allowed — a family of third-order equations whose solutions have movable natural barriers and are therefore not of Painlevé type.

This mission formalizes the endpoint of one such reduction chain, as surveyed by Ablowitz, Chakravarty and Halburd, Integrable systems and reductions of the self-dual Yang–Mills equations, J. Math. Phys. 44 (2003) 3147–3173, Section V. Reducing SDYM to functions of a single variable gives the Nahm equations; taking the gauge algebra to be the divergence-free vector fields on S3S^3S3 turns them into a matrix flow which, after diagonalizing the symmetric part, becomes the generalized Darboux–Halphen system. Its trace is governed by the Chazy equation, written down by Chazy in 1909, and — this is the paper's historical observation — the Chazy equation is equivalent to the differential system Ramanujan derived in 1916 for the Eisenstein series P=E2P = E_2P=E2​, Q=E4Q = E_4Q=E4​, R=E6R = E_6R=E6​. Chazy and Ramanujan worked on the same equation at nearly the same time and apparently did not know it.

Setting

Throughout, ttt and qqq are complex variables and all functions are complex-valued; a "solution on sss" means the stated derivative identities hold at every point of a set s⊆Cs \subseteq \mathbb{C}s⊆C.

The classical Chazy equation is the third-order equation

d3ydt3=2y d2ydt2−3(dydt)2.\frac{d^3y}{dt^3} = 2y\,\frac{d^2y}{dt^2} - 3\left(\frac{dy}{dt}\right)^2 .dt3d3y​=2ydt2d2y​−3(dtdy​)2.

The classical Darboux–Halphen system is the first-order system for ω1,ω2,ω3\omega_1,\omega_2,\omega_3ω1​,ω2​,ω3​

ω˙1=ω2ω3−ω1(ω2+ω3),\dot\omega_1 = \omega_2\omega_3 - \omega_1(\omega_2+\omega_3),ω˙1​=ω2​ω3​−ω1​(ω2​+ω3​),

together with its two cyclic images. It arose in Darboux's study of triply orthogonal surfaces and was solved by Halphen. Its generalized form adds a term τ2=τ12+τ22+τ32\tau^2 = \tau_1^2+\tau_2^2+\tau_3^2τ2=τ12​+τ22​+τ32​ to each right-hand side, where τ˙1=−τ1(ω2+ω3)\dot\tau_1 = -\tau_1(\omega_2+\omega_3)τ˙1​=−τ1​(ω2​+ω3​) and cyclically.

Ramanujan's system is

qdPdq=P2−Q12,qdQdq=PQ−R3,qdRdq=PR−Q22,q\frac{dP}{dq} = \frac{P^2-Q}{12},\qquad q\frac{dQ}{dq} = \frac{PQ-R}{3},\qquad q\frac{dR}{dq} = \frac{PR-Q^2}{2},qdqdP​=12P2−Q​,qdqdQ​=3PQ−R​,qdqdR​=2PR−Q2​,

satisfied by P(q)=1−24∑n≥1σ1(n)qnP(q) = 1-24\sum_{n\ge1}\sigma_1(n)q^nP(q)=1−24∑n≥1​σ1​(n)qn, Q(q)=1+240∑n≥1σ3(n)qnQ(q) = 1+240\sum_{n\ge1}\sigma_3(n)q^nQ(q)=1+240∑n≥1​σ3​(n)qn, R(q)=1−504∑n≥1σ5(n)qnR(q) = 1-504\sum_{n\ge1}\sigma_5(n)q^nR(q)=1−504∑n≥1​σ5​(n)qn, where σk(n)=∑d∣ndk\sigma_k(n)=\sum_{d\mid n}d^kσk​(n)=∑d∣n​dk.

Finally, the 3×33\times33×3 matrix flow obtained from the Nahm equations with the diff(S3)\mathrm{diff}(S^3)diff(S3) gauge algebra is

M˙=(Adj⁡M)T+MTM−(Tr⁡M)M,Adj⁡M=(det⁡M)M−1,\dot M = (\operatorname{Adj} M)^{T} + M^{T}M - (\operatorname{Tr} M)M,\qquad \operatorname{Adj}M = (\det M)M^{-1},M˙=(AdjM)T+MTM−(TrM)M,AdjM=(detM)M−1,

and the generalized Chazy equation with parameter nnn is

d3ydt3−2yd2ydt2+3(dydt)2=436−n2(6dydt−y2)2.\frac{d^3y}{dt^3} - 2y\frac{d^2y}{dt^2} + 3\left(\frac{dy}{dt}\right)^2 = \frac{4}{36-n^2}\left(6\frac{dy}{dt}-y^2\right)^2 .dt3d3y​−2ydt2d2y​+3(dtdy​)2=36−n24​(6dtdy​−y2)2.

Formalization targets

Goal — the Chazy–Ramanujan correspondence (eqs. (78) and (71))

If P,Q,RP,Q,RP,Q,R satisfy Ramanujan's system on a region of the punctured qqq-plane, then

y(t):=iπP ⁣(e2πit)y(t) := i\pi P\!\left(e^{2\pi i t}\right)y(t):=iπP(e2πit)

satisfies the classical Chazy equation on the preimage region. In particular y(t)=iπE2(t)y(t)=i\pi E_2(t)y(t)=iπE2​(t) is a solution of the Chazy equation, and knowing the general solution of Chazy gives the general solution of Ramanujan's system.

Supporting targets

The milestone list covers the reduction chain in both directions: the matrix flow M˙=(Adj⁡M)T+MTM−(Tr⁡M)M\dot M = (\operatorname{Adj}M)^T + M^TM-(\operatorname{Tr}M)MM˙=(AdjM)T+MTM−(TrM)M and its reduction to the Darboux–Halphen system (eqs. (51)–(54)), the first integrals (55), the passage y=−2(ω1+ω2+ω3)y = -2(\omega_1+\omega_2+\omega_3)y=−2(ω1​+ω2​+ω3​) from Darboux–Halphen to Chazy and back through the roots of a cubic, the SL(2)\mathrm{SL}(2)SL(2) symmetry (73) of the Chazy equation, Rankin's fourth-order equation for the discriminant cusp form, the change of variable q=e2iτq=e^{2i\tau}q=e2iτ between the two forms of Ramanujan's system, and the generalized Chazy equation (81).

Significance

The Chazy equation is the bridge between integrable systems and the theory of modular forms. Its particular solution y=iπE2y = i\pi E_2y=iπE2​ makes the quasi-modularity of the second Eisenstein series an ODE statement; via y=12(log⁡Δ)′y = \tfrac12 (\log\Delta)'y=21​(logΔ)′ it turns into Rankin's homogeneous fourth-order equation for the discriminant cusp form Δ\DeltaΔ, whose Fourier coefficients are the Ramanujan τ\tauτ-function. The SL(2,Z)\mathrm{SL}(2,\mathbb{Z})SL(2,Z) action on solutions is exactly the weight-2 quasi-modular transformation law. In the other direction, the general solution of Chazy is a ratio of hypergeometric functions with a movable natural barrier, which is why these reductions are used as the standard counterexample to the identification of integrability with the Painlevé property.

None of this material is currently in Mathlib: there is no Chazy equation, no Darboux–Halphen system, no Ramanujan differential system, and no Eisenstein-series ODE. The mission builds that layer from scratch. Each statement is a closed-form differential identity, so the development is self-contained: it needs no analytic continuation theory, no modular-forms library, and no existence theory for ODEs. What a solver must supply is careful derivative bookkeeping and polynomial algebra.

Status honesty: every statement in this mission is a classical, published result — Darboux, Halphen, Chazy (1909–1911), Ramanujan (1916), Rankin (1956), and Ablowitz–Chakravarty–Halburd (1990s–2003). Nothing here is open mathematics. What is open is the machine-checked proof; to the captain's knowledge no formalization of these identities exists.

Difficulty

The obvious approach — "differentiate three times and call ring" — fails for two reasons. First, the statements are about functions, not about polynomials: each differentiation step requires producing the derivative of a product, a quotient, or a composition from the hypotheses, and only then is the resulting algebraic identity a ring problem. Second, two of the targets go against the flow of the hypotheses. Recovering the Darboux–Halphen system from a Chazy solution means recovering ω˙i\dot\omega_iω˙i​ from the derivatives of the three elementary symmetric functions of the ωi\omega_iωi​: this is a linear system whose matrix is a Vandermonde matrix in ω1,ω2,ω3\omega_1,\omega_2,\omega_3ω1​,ω2​,ω3​, invertible precisely because the roots are assumed distinct — which is why the distinctness hypothesis is not decoration. Similarly, the matrix milestone needs the conjugation-equivariance of M↦(Adj⁡M)T+MTM−(Tr⁡M)MM \mapsto (\operatorname{Adj}M)^T + M^TM - (\operatorname{Tr}M)MM↦(AdjM)T+MTM−(TrM)M, which holds for the transpose only because the conjugating matrix is complex orthogonal.

Formalization scope

Everything is over C\mathbb{C}C, matching the paper. Solutions are represented pointwise on an arbitrary set s⊆Cs \subseteq \mathbb{C}s⊆C rather than on all of C\mathbb{C}C, because the solutions of interest have movable singularities and natural barriers; no openness, holomorphy or connectivity is assumed unless a statement needs it.

Higher derivatives are carried as explicit extra function arguments joined by HasDerivAt hypotheses rather than through iterated deriv. This avoids junk values entirely: a statement never asserts anything about the value of a derivative that does not exist. The same convention is used for the matrix flow, where the derivative is imposed entrywise, so that no norm or normed-space structure on the space of matrices needs to be chosen.

Divisions are arranged so that no denominator can vanish under the stated hypotheses: Ramanujan's system is written in the form q dP/dq=(P2−Q)/12q\,dP/dq = (P^2-Q)/12qdP/dq=(P2−Q)/12, with no division by qqq; the generalized Chazy equation carries the hypothesis n2≠36n^2 \ne 36n2=36; and the first-integral and discriminant statements carry explicit nonvanishing hypotheses.

There is no trivializing formalization available here. Every statement is an implication between two systems of differential equations whose hypotheses are satisfied by the classical explicit solutions (P=E2P=E_2P=E2​, Q=E4Q=E_4Q=E4​, R=E6R=E_6R=E6​ for the Ramanujan system; Halphen's solutions for Darboux–Halphen), so none of them is vacuous, and none is an identity that holds for arbitrary functions.

A complete development needs only Mathlib's derivative calculus (HasDerivAt and its product, quotient and composition rules), Complex.exp, and Matrix.adjugate with the basic adjugate identities. Contributions of reusable pieces are welcome: in particular a clean statement of the derivative of the elementary symmetric functions of a triple of functions, and the Vandermonde inversion step, would both be of use beyond this mission.

Selected references

  • M. J. Ablowitz, S. Chakravarty, R. G. Halburd, Integrable systems and reductions of the self-dual Yang–Mills equations, J. Math. Phys. 44 (2003) 3147–3173. doi:10.1063/1.1586967
  • J. Chazy, Sur les équations différentielles du troisième ordre et d'ordre supérieur dont l'intégrale générale a ses points critiques fixes, Acta Math. 34 (1911) 317–385. doi:10.1007/BF02393131
  • S. Ramanujan, On certain arithmetical functions, Trans. Cambridge Philos. Soc. 22 (1916) 159–184.
  • G. Halphen, Sur un système d'équations différentielles, C. R. Acad. Sci. Paris 92 (1881) 1101–1103.
  • R. A. Rankin, The construction of automorphic forms from the derivatives of a given form, J. Indian Math. Soc. 20 (1956) 103–116.
  • M. J. Ablowitz, S. Chakravarty, R. G. Halburd, The generalized Chazy equation and Schwarzian triangle functions, Asian J. Math. 2 (1998) 619–624. doi:10.4310/AJM.1998.v2.n4.a1
  • R. S. Ward, Integrable and solvable systems, and relations among them, Philos. Trans. R. Soc. London A 315 (1985) 451–457. doi:10.1098/rsta.1985.0051
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Machine LearningOperations ResearchOptimization+1·Captain: mikedeng1

Wasserstein Distributionally Robust Optimization IV: Regularization by Robustification in Classification and RegressionTextbook

Motivation

Regularization — adding a penalty on model complexity to an empirical risk minimization objective — is one of the oldest and most reliably effective tools in statistical learning: ridge regression, LASSO, and margin-based support vector machines all fit this template. For decades the regularization weight and penalty function were chosen heuristically or by cross-validation, with only asymptotic or worst-case generalization bounds explaining why they help. Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter on Wasserstein distributionally robust optimization (DRO) gives regularization a different, non-asymptotic justification: a decision rule that is robust to adversarial perturbations of its training data, measured in Wasserstein distance, is exactly a regularized empirical risk minimizer — no approximation, no asymptotics. This mission formalizes the general form of that equivalence, Theorem 10 (p. 14), which underlies every regularization-by-robustification result the chapter derives for classification and regression alike.

Setting

Fix a normed space Ξ=Rm\Xi = \mathbb{R}^mΞ=Rm, a convex loss function ℓ:Ξ→R\ell : \Xi \to \mathbb{R}ℓ:Ξ→R, a radius ε≥0\varepsilon \ge 0ε≥0, and NNN training samples ξ^1,…,ξ^N∈Ξ\hat\xi_1,\dots,\hat\xi_N \in \Xiξ^​1​,…,ξ^​N​∈Ξ (N≥1N \ge 1N≥1). The empirical distribution is P^N=1N∑i=1Nδξ^i\hat P_N = \frac{1}{N}\sum_{i=1}^N \delta_{\hat\xi_i}P^N​=N1​∑i=1N​δξ^​i​​. The worst-case risk of ℓ\ellℓ at radius ε\varepsilonε (eq. (6), p. 6) is

Rε,p(P^N,ℓ)=sup⁡Q∈Bε,p(P^N)EQ[ℓ(ξ)],R_{\varepsilon,p}(\hat P_N,\ell) = \sup_{Q \in B_{\varepsilon,p}(\hat P_N)} E_Q[\ell(\xi)],Rε,p​(P^N​,ℓ)=Q∈Bε,p​(P^N​)sup​EQ​[ℓ(ξ)],

where Bε,p(P^N)B_{\varepsilon,p}(\hat P_N)Bε,p​(P^N​) is the type-ppp Wasserstein ball of radius ε\varepsilonε around P^N\hat P_NP^N​ (Definition 1, p. 3) — the set of probability measures on Ξ\XiΞ within Wasserstein distance ε\varepsilonε of the empirical distribution, under a norm ∥⋅∥\|\cdot\|∥⋅∥ on Ξ\XiΞ and its transportation exponent ppp. The Lipschitz modulus Lip(ℓ)=sup⁡ξ≠ξ′∣ℓ(ξ)−ℓ(ξ′)∣∥ξ−ξ′∥\mathrm{Lip}(\ell) = \sup_{\xi\ne\xi'} \frac{|\ell(\xi)-\ell(\xi')|}{\|\xi-\xi'\|}Lip(ℓ)=supξ=ξ′​∥ξ−ξ′∥∣ℓ(ξ)−ℓ(ξ′)∣​ (possibly +∞+\infty+∞) measures how fast ℓ\ellℓ can grow.

Formalization targets

Goal (Theorem 10, convex loss and p=1p=1p=1). If ℓ\ellℓ is convex and p=1p=1p=1, then the worst-case risk of ℓ\ellℓ over the type-1 Wasserstein ball around the empirical distribution coincides with the Lipschitz-regularized empirical loss:

Rε,1(P^N,ℓ)=R(P^N,ℓ)+ε⋅Lip(ℓ),R_{\varepsilon,1}(\hat P_N,\ell) = R(\hat P_N,\ell) + \varepsilon \cdot \mathrm{Lip}(\ell),Rε,1​(P^N​,ℓ)=R(P^N​,ℓ)+ε⋅Lip(ℓ),

where R(P^N,ℓ)=1N∑i=1Nℓ(ξ^i)R(\hat P_N,\ell) = \frac{1}{N}\sum_{i=1}^N \ell(\hat\xi_i)R(P^N​,ℓ)=N1​∑i=1N​ℓ(ξ^​i​) is the ordinary empirical risk. The left side is the worst-case expected loss under adversarial perturbations of the training data of bounded aggregate Wasserstein cost; the right side is the ordinary empirical risk plus a regularization term proportional to the perturbation radius ε\varepsilonε and the loss's own Lipschitz modulus — no approximation, an exact equality for every convex ℓ\ellℓ.

Significance

This is the single result underlying every specific regularization-by-robustification corollary the chapter derives — the ℓ2\ell_2ℓ2​-regularized SVM and its ℓ1\ell_1ℓ1​/ℓ∞\ell_\inftyℓ∞​ variants, regularized logistic regression, and the regression analogue with a Lipschitz loss (Proposition 3) — because each of those is obtained by substituting a specific convex, Lipschitz loss (hinge, logloss, a linear-model margin loss) for the general ℓ\ellℓ here and reading off Lip(ℓ)\mathrm{Lip}(\ell)Lip(ℓ) in closed form. Theorem 10 is exact (p=1p=1p=1, Ξ = R^m) precisely because a type-1 transportation cost is dual to the Lipschitz modulus (a consequence of the Kantorovich- Rubinstein duality this book's earlier duality theorems establish), whereas the corresponding statement for p≥2p \ge 2p≥2 (Theorem 11 elsewhere in the chapter) needs a strictly stronger hypothesis on ℓ\ellℓ. Formalizing Theorem 10 fixes, machine-checkably, the exact scope of the equivalence — which losses qualify (convex, no boundedness or smoothness needed), which transportation exponent is required (p=1p=1p=1, not any p≥1p\ge1p≥1), and that the equality is exact, not an upper or lower bound — the single fact every classification- and regression-specific robustification corollary in the chapter cites without re-deriving.

Difficulty

The natural first attempt treats the worst-case risk as an instance of the general finite convex reduction (Theorem 8, which needs ℓ\ellℓ or a related concave/convex-conjugate structure and applies for a general norm exponent p,qp,qp,q with 1/p+1/q=11/p+1/q=11/p+1/q=1) and specializes it to p=1p=1p=1. This is not the paper's own route for Theorem 10: at p=1p=1p=1 the dual exponent q=∞q=\inftyq=∞, and the general finite-convex-program reduction (11) degenerates in a way that is more naturally derived directly from the type-1 Wasserstein distance's own dual (Kantorovich-Rubinstein) representation — a Lipschitz test function pairs exactly with a type-1 transportation cost, which is why the answer is Lipschitz-regularization and not some other penalty. The Lean statement records only the final equality (the proof itself, via Theorem 8 or the direct Kantorovich-Rubinstein route, is left as sorry, as required for a draft item), but the choice of which milestones would support that proof is exactly this: the type-1/Lipschitz-modulus duality is a structurally different argument from the finite-convex-program machinery Theorem 8 needs for other ppp, which is why this chapter's earlier draft mistakenly tried to reach a specialization of Theorem 10 (Proposition 2, restated for a labeled, κ=∞\kappa=\inftyκ=∞ ambiguity set) through a finite-atom shortcut that does not actually capture the general type-1 ball Theorem 10's own proof needs — see Formalization scope.

Formalization scope

Ξ\XiΞ is EuclideanSpace ℝ (Fin m) (fixed to Set.univ, matching the theorem's own "Ξ = R^m" hypothesis) with an arbitrary fixed norm as a type-class parameter, not specialized to Euclidean. The worst-case risk, Wasserstein distance, ambiguity set, nominal risk, empirical distribution and Lipschitz modulus are all redefined locally in this chapter's own namespace, verbatim restatements of 01-duality's own drafts of the same objects (identical EReal/ENNReal/Integrable conventions), because 01-duality is not yet a published mission (CAPTAIN_ADDENDUM_WAVE2.md rule 5); a later upload can retire the duplication once it is live. hN : 0 < N excludes the empty-sample case the paper's own "N training samples" presupposes; hℓ : Integrable ℓ (empiricalDistribution ξhat) guards the empirical risk's Bochner integral (automatically satisfied under any real-valued ℓ since the empirical distribution is a finite convex combination of Dirac masses, but stated explicitly rather than assumed silently). No constant is pinned to a numeral. This mission originally targeted Proposition 2 (regularization by robustification for classification, p. 25), a specialization of Theorem 10 to a labeled, κ=∞ input-output ambiguity set — but that draft's κ=∞ ambiguity set restricted admissible perturbations to a finite family of exactly N atoms, each sample's entire mass moving as one indivisible unit, which is a strict, non-faithful subset of the true κ=∞ Wasserstein ball (splitting a sample's mass across several destinations is a legitimate, and for a convex loss strictly more powerful, perturbation by Jensen's inequality). This made the goal theorem false for at least one of the three loss functions (Table 1) the mission itself certified as covered (logloss), not merely narrower than the paper's claim — moderation caught this and required either a faithful general-ambiguity-set reformulation or retargeting the goal. This mission takes the latter: Theorem 10 itself, already correctly and generally stated using the unrestricted Wasserstein ball throughout, is now the goal, with no further milestone (no other numbered result in this chunk's scope is needed for Theorem 10's own statement beyond the shared definitions above). A future mission in this series can revisit Proposition 2/3 with a properly general labeled ambiguity set once that construction (label-pinned marginal plus an aggregate coupling condition on the input coordinate, rather than a finite atom family) is built.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Shafieezadeh-Abadeh, S., Esfahani, P. M., & Kuhn, D. (2015). Distributionally robust logistic regression. Advances in Neural Information Processing Systems, 28.
  • Blanchet, J., Kang, Y., & Murthy, K. (2019). Robust Wasserstein profile inference and applications to machine learning. Journal of Applied Probability, 56(3), 830–857.
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Wasserstein Distributionally Robust Optimization III: Finite-Sample and Asymptotic Performance GuaranteesTextbook

Motivation

A decision maker who solves a distributionally robust optimization (DRO) problem over a Wasserstein ball chooses a radius ε\varepsilonε by hand, and it is natural to ask what guarantee that choice actually buys: how large must ε\varepsilonε be, as a function of the sample size NNN and a desired confidence level, before the resulting worst-case risk is provably not an underestimate of the true (unknown-distribution) risk? Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter answers this for the mean-covariance relaxation of Wasserstein DRO introduced via the Gelbrich hull (Section 2.3): Theorem 21 gives a concentration inequality for how fast the sample mean and covariance approach the true mean and covariance, and Theorem 22 turns that concentration bound into a finite-sample statistical guarantee for the Gelbrich risk itself. This mission formalizes both.

Setting

Fix m∈Nm \in \mathbb{N}m∈N. Let PPP be the unknown true distribution on Rm\mathbb{R}^mRm with mean vector μ\muμ and covariance matrix Σ∈S+m\Sigma \in S^m_+Σ∈S+m​, and suppose PPP is light-tailed: there exist α>2\alpha > 2α>2 and A>0A > 0A>0 with EP[exp⁡(∥ξ∥2α)]≤AE_P[\exp(\|\xi\|_2^\alpha)] \le AEP​[exp(∥ξ∥2α​)]≤A. Let ξ^1,…,ξ^N\hat\xi_1,\dots,\hat \xi_Nξ^​1​,…,ξ^​N​ be NNN independent, identically distributed samples from PPP; write PNP^NPN for their joint law (the NNN-fold product measure) and μ^,Σ^\hat\mu, \hat\Sigmaμ^​,Σ^ for the resulting sample mean and sample covariance, i.e. the mean and covariance of the empirical distribution P^N=1N∑iδξ^i\hat P_N = \frac{1}{N}\sum_i \delta_{\hat\xi_i}P^N​=N1​∑i​δξ^​i​​. Recall from the Gelbrich construction the mean-covariance uncertainty set Uε(μ^,Σ^)={(μ,Σ)∈Rm×S+m:∥μ^−μ∥22+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2}U_\varepsilon(\hat\mu,\hat\Sigma) = \{(\mu,\Sigma) \in \mathbb{R}^m \times S^m_+ : \|\hat\mu-\mu\|_2^2 + \mathrm{Tr}[\hat\Sigma+\Sigma-2(\hat\Sigma^{1/2} \Sigma\hat\Sigma^{1/2})^{1/2}] \le \varepsilon^2\}Uε​(μ^​,Σ^)={(μ,Σ)∈Rm×S+m​:∥μ^​−μ∥22​+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2}, and the Gelbrich risk Rε(μ^,Σ^,ℓ)=sup⁡Q∈Gε(μ^,Σ^)EQ[ℓ(ξ)]R_\varepsilon(\hat\mu,\hat\Sigma,\ell) = \sup_{Q \in G_\varepsilon(\hat\mu,\hat\Sigma)} E_Q[\ell(\xi)]Rε​(μ^​,Σ^,ℓ)=supQ∈Gε​(μ^​,Σ^)​EQ​[ℓ(ξ)] of a loss function ℓ\ellℓ over the Gelbrich hull Gε(μ^,Σ^)G_\varepsilon(\hat\mu,\hat \Sigma)Gε​(μ^​,Σ^).

Formalization targets

Milestone (Theorem 21, concentration inequalities II). There is c>1c > 1c>1, depending on PPP only through μ,Σ,α,A,m\mu,\Sigma,\alpha,A,mμ,Σ,α,A,m (not on any finer feature of PPP), such that for every η∈(0,1]\eta \in (0,1]η∈(0,1],

PN[(μ,Σ)∈Uε(μ^,Σ^)]≥1−ηwheneverε≥εN(η):=log⁡(c/η)N.P^N\big[(\mu,\Sigma) \in U_\varepsilon(\hat\mu,\hat\Sigma)\big] \ge 1-\eta \quad \text{whenever} \quad \varepsilon \ge \varepsilon_N(\eta) := \frac{\log(c/\eta)}{\sqrt N}.PN[(μ,Σ)∈Uε​(μ^​,Σ^)]≥1−ηwheneverε≥εN​(η):=N​log(c/η)​.

Goal (Theorem 22(a), finite sample guarantees II). Under the same hypotheses, for every η∈(0,1)\eta \in (0,1)η∈(0,1) and ε≥εN(η)\varepsilon \ge \varepsilon_N(\eta)ε≥εN​(η),

PN{R(P,ℓ)≤Rε(μ^,Σ^,ℓ)    ∀ℓ∈L}≥1−η.P^N\Big\{R(P,\ell) \le R_\varepsilon(\hat\mu,\hat\Sigma,\ell) \;\; \forall \ell \in L\Big\} \ge 1-\eta.PN{R(P,ℓ)≤Rε​(μ^​,Σ^,ℓ)∀ℓ∈L}≥1−η.

With probability at least 1−η1-\eta1−η over the draw of the training sample, the Gelbrich risk computed from that sample upper-bounds the true risk of every admissible loss function simultaneously — not just of one fixed ℓ\ellℓ chosen in advance. (The paper's part (b), the analogous guarantee $P^N\{R(P,\ell^\star) \le R_\varepsilon(\hat\mu,\hat\Sigma,\ell^\star)\} \ge 1-\eta$ for the specific optimizer ℓ⋆\ell^\starℓ⋆ of the Gelbrich risk minimization problem, is not formalized in this mission — see Formalization scope.)

Significance

Theorem 22 is what makes the Gelbrich-risk relaxation of Wasserstein DRO more than a computational convenience: it certifies that solving the tractable Gelbrich risk minimization problem gives a decision whose true out-of-sample risk is, with high probability, no worse than the value the solver reports — a genuine confidence guarantee, not merely an approximation of the Wasserstein worst-case risk. Theorem 21's rate, εN(η)=O(N−1/2)\varepsilon_N(\eta) = O(N^{-1/2})εN​(η)=O(N−1/2), is also of independent interest: it is dimension-free (no curse of dimensionality), in contrast to the paper's earlier general-distribution concentration result (Theorem 18, out of scope for this mission) whose rate degrades with mmm. Formalizing Theorem 21 fixes, machine-checkably, the exact functional form of εN(η)\varepsilon_N(\eta)εN​(η) and the precise sense in which ccc is "distribution-free" given (μ,Σ,α,A,m)(\mu,\Sigma,\alpha,A,m)(μ,Σ,α,A,m) — a subtlety easy to state informally but easy to get wrong formally (see Difficulty).

Difficulty

The central formalization difficulty is not proving the theorems (both are left as sorry in this draft) but stating the existential constant ccc correctly. The paper says ccc "depends on PPP only through μ,Σ,α,A,m\mu,\Sigma,\alpha,A,mμ,Σ,α,A,m" — informally, a promise that ccc is uniform across every distribution PPP sharing those five parameters, not merely that some ccc exists for each PPP separately (a vacuously true, much weaker statement obtained by naively quantifying ccc after PPP). The correct encoding places ∃c\exists c∃c before the universal quantifier over PPP: for fixed (μ,Σ,α,A,m)(\mu,\Sigma,\alpha,A,m)(μ,Σ,α,A,m), one ccc must work for every PPP with that mean, covariance, and tail bound. Getting this quantifier order backwards silently converts a genuine finite-sample guarantee into a triviality (FAITHFULNESS_TRAPS.md trap 8).

Formalization scope

Distributions live on EuclideanSpace ℝ (Fin m); PNP^NPN, the law of NNN iid samples, is the NNN-fold product measure MeasureTheory.Measure.pi (fun _ => P) on Fin N → EuclideanSpace ℝ (Fin m) — an event about the random sample sequence is a set of such tuples, and "PN[event]≥1−ηP^N[\text{event}] \ge 1-\etaPN[event]≥1−η" is that product measure's mass on the event set. All risk and uncertainty-set definitions (meanVector, covarianceMatrix, meanCovarianceUncertaintySet, gelbrichHull, gelbrichRisk, nominalRisk, empiricalDistribution) are redefined locally in this chapter's own namespace, matching 02-gelbrich's conventions exactly, since neither 01-duality nor 02-gelbrich is yet a published mission (CAPTAIN_ADDENDUM_WAVE2.md rule 5); a later upload can retire the duplication once those missions are live. The existential constant c is placed before the universal quantifier over P in both theorems, exactly capturing "depends on P only through µ,Σ,α,A,m" — see Difficulty. Only Theorem 22's part (a) (the uniform bound over a loss class L) is formalized; part (b) — the bound for the specific optimizer ℓ* of the Gelbrich risk minimization problem (19) — is left out, because it requires first formalizing "ℓ* is an optimizer of problem (19)" as an object (an infimum-attaining selection over a data-dependent optimization problem), which is additional infrastructure this mission's time budget did not cover; formalizing it as an unconditional bound over an arbitrary data-dependent ℓ* (dropping the optimality hypothesis) would be unfaithful — the guarantee genuinely depends on ℓ* being an optimizer, not an arbitrary measurable function of the sample. The goal theorem also carries hΞ, stating Ξ contains the support of P (the paper's own standing assumption, p. 6, for every later use of Ξ), and hLInt, an Integrable ℓ P guard for every ℓ ∈ L, matching Assumption 1 (p. 9); both were added after moderation found the goal's original statement, without them, admitted a counter-instance (Ξ = ∅ collapses the Gelbrich hull to empty and the risk supremum to ⊥, making the guarantee provably false rather than merely undisclosed). Theorem 18 (the general, dimension- dependent concentration inequality with its piecewise ε_N(η) formula) and Theorems 19/20/23 (its downstream guarantees and the asymptotic-consistency results) are out of scope for this mission, which targets the Gelbrich-risk branch (Theorems 21/22) specifically.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Fournier, N., & Guillin, A. (2015). On the rate of convergence in Wasserstein distance of the empirical measure. Probability Theory and Related Fields, 162(3), 707–738.
  • Gao, R., & Kleywegt, A. J. (2023). Distributionally robust stochastic optimization with Wasserstein distance. Mathematics of Operations Research, 48(2), 603–655.
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Machine LearningProbabilityStatistics+1·Captain: mikedeng1

Foundations of Machine Learning XII: Algorithmic StabilityTextbook

Motivation

Every generalization bound in Chapters 2-11 depends only on the complexity of a fixed hypothesis set HHH — Rademacher complexity, VC-dimension, growth function — and holds regardless of which algorithm within HHH actually returns the hypothesis. This is both a strength (broad applicability) and a limitation: it throws away everything specific to how an algorithm searches HHH, and can be uninformative when HHH itself is large or unbounded (e.g. a regularized objective that implicitly restricts the search without shrinking HHH as a set). Chapter 14 introduces a fundamentally different route to a generalization bound — a property of the algorithm rather than the hypothesis class — first used by Devroye, Rogers and Wagner for kkk-nearest-neighbor rules and given its modern general form by Bousquet and Elisseeff (2002), whose treatment this chapter follows and (for non-differentiable convex losses) extends.

Setting

A labeled example is z=(x,y)∈X×Yz=(x,y)\in X\times Yz=(x,y)∈X×Y; for a loss function L:Y′×Y→R+L:Y'\times Y\to\mathbb R_+L:Y′×Y→R+​ (where Y′Y'Y′ may differ from YYY, e.g. Y={−1,+1}Y=\{-1,+1\}Y={−1,+1} but Y′=RY'=\mathbb RY′=R for a real-valued hypothesis), the loss of a hypothesis hhh at zzz is Lz(h)=L(h(x),y)L_z(h)=L(h(x),y)Lz​(h)=L(h(x),y). Given a learning algorithm AAA that maps a sample SSS of size mmm to a hypothesis hS∈Hh_S\in HhS​∈H, the empirical error and generalization error are R^S(h)=1m∑iLzi(h)\hat R_S(h)=\frac1m\sum_iL_{z_i}(h)R^S​(h)=m1​∑i​Lzi​​(h) and R(h)=Ez∼D[Lz(h)]R(h)=\mathbb E_{z\sim D}[L_z(h)]R(h)=Ez∼D​[Lz​(h)]. Uniform β\betaβ-stability (Definition 14.1) says: for any two samples SSS, S′S'S′ differing by a single point, the algorithm's returned hypotheses satisfy ∣Lz(hS)−Lz(hS′)∣≤β|L_z(h_S)-L_z(h_{S'})|\le\beta∣Lz​(hS​)−Lz​(hS′​)∣≤β for every zzz — replacing one training point can change the algorithm's loss on any point by at most β\betaβ. For the regularized algorithms studied in §14.3, a kernel-based regularization algorithm minimizes FS(h)=R^S(h)+λ∥h∥K2F_S(h)=\hat R_S(h)+ \lambda\|h\|_K^2FS​(h)=R^S​(h)+λ∥h∥K2​ over the RKHS HHH of a positive-definite kernel KKK, and a loss LLL is σ\sigmaσ-admissible (Definition 14.3) if ∣L(h′(x),y)−L(h(x),y)∣≤σ∣h′(x)−h(x)∣|L(h'(x),y)-L(h(x),y)|\le\sigma|h'(x)-h(x)|∣L(h′(x),y)−L(h(x),y)∣≤σ∣h′(x)−h(x)∣ for all hypotheses h,h′h,h'h,h′ — a Lipschitz-like smoothness condition satisfied by the standard regression and classification losses.

Formalization targets

Proposition 14.4 (milestone). For a PDS kernel KKK with K(x,x)≤r2K(x,x)\le r^2K(x,x)≤r2 and a convex, σ\sigmaσ-admissible loss LLL, the kernel-based regularization algorithm is β\betaβ-stable with

β≤σ2r2mλ.\beta \le \frac{\sigma^2r^2}{m\lambda}.β≤mλσ2r2​.

Corollary 14.5 (milestone). For SVR (the ϵ\epsilonϵ-insensitive loss LϵL_\epsilonLϵ​, bounded by MMM), with probability at least 1−δ1-\delta1−δ:

R(hS)≤R^S(hS)+r2mλ+(2r2λ+M)log⁡(1/δ)2m.R(h_S) \le \hat R_S(h_S) + \frac{r^2}{m\lambda} + \Big(\frac{2r^2}\lambda+M\Big)\sqrt{\frac{\log(1/\delta)}{2m}}.R(hS​)≤R^S​(hS​)+mλr2​+(λ2r2​+M)2mlog(1/δ)​​.

Theorem 14.2 — the mission's goal. For a loss bounded by MMM and a β\betaβ-stable algorithm AAA, with probability at least 1−δ1-\delta1−δ over a sample SSS of size mmm:

R(hS)≤R^S(hS)+β+(2mβ+M)log⁡(1/δ)2m.R(h_S) \le \hat R_S(h_S) + \beta + (2m\beta+M)\sqrt{\frac{\log(1/\delta)}{2m}}.R(hS​)≤R^S​(hS​)+β+(2mβ+M)2mlog(1/δ)​​.

Significance

Theorem 14.2 is the book's demonstration that algorithm-dependent analysis is not merely a special-case curiosity: it is broad enough to cover an entire family (every kernel-based regularization algorithm — KRR, SVR, SVMs, and beyond) uniformly, via a single stability coefficient computation (Proposition 14.4) that is then specialized per algorithm just by plugging in that loss's admissibility constant σ\sigmaσ. Corollary 14.5's SVR bound is the concrete payoff: a fully explicit, dimension-free generalization guarantee for a widely used regression algorithm, with every constant (rrr, λ\lambdaλ, mmm) traceable to the algorithm's own hyperparameters, no VC-dimension or Rademacher-complexity computation required. Unlike Chapters 3-11, whose bounds are oblivious to how HHH is searched, algorithmic stability is the first tool in the book that can, in principle, certify generalization for a hypothesis class too large or poorly understood for a complexity-based bound to be informative, provided the algorithm itself is stable. No prior art on the Prove2Me platform is faithful: GET /theorems?q=algorithmic+stability, q=uniform+stability return no hits; q=McDiarmid returns only bounded_diff_martingale_two_sided (Boucheron-Lugosi-Massart's own two-sided bounded-differences martingale inequality), which is McDiarmid's inequality's own proof engine (the background result Theorem 14.2's proof applies), not any result of this chapter — a different mathematical object entirely, not reused. All eleven items are drafted fresh.

Not formalized here: Corollary 14.6 (KRR bound), Lemma 14.7 (boundedness of kernel-regularization hypotheses) and Corollary 14.8 (SVM bound). Corollary 14.6 is structurally identical to Corollary 14.5 (a different loss function's admissibility constant plugged into the same Proposition 14.4 + Theorem 14.2 chain) and adds no new formalization content beyond Corollary 14.5, already drafted; Lemma 14.7 and Corollary 14.8 are omitted together, since 14.8's own statement needs 14.7's bound on ∣hS(x)∣|h_S(x)|∣hS​(x)∣ to compute its explicit MMM (unlike Corollary 14.5, which is given MMM as a hypothesis) — a genuine additional formalization layer (the reproducing-kernel norm bound ∣hS(x)∣≤rB/λ|h_S(x)|\le r\sqrt{B/\lambda}∣hS​(x)∣≤rB/λ​) disproportionate to a single further corollary within this mission's budget.

Difficulty

The chapter's central technical step is recognizing that β\betaβ-stability plus the loss bound MMM together give exactly the bounded-difference property McDiarmid's inequality needs, applied to Φ(S)=R(hS)−R^S(hS)\Phi(S)=R(h_S)-\hat R_S(h_S)Φ(S)=R(hS​)−R^S​(hS​) as a function of the sample: replacing one point of SSS changes R(hS)R(h_S)R(hS​) by at most β\betaβ (stability applied to the population loss, an expectation over zzz) and changes R^S(hS)\hat R_S(h_S)R^S​(hS​) by at most β+M/m\beta+M/mβ+M/m (stability on the m−1m-1m−1 shared points, plus the full loss bound M/mM/mM/m on the one point that actually changed) — two different, asymmetric arguments that must be combined correctly to get ∣Φ(S)−Φ(S′)∣≤2β+M/m|\Phi(S)-\Phi(S')|\le 2\beta+M/m∣Φ(S)−Φ(S′)∣≤2β+M/m, not merely "stability implies boundedness" asserted directly. Proposition 14.4's own proof (not formalized here beyond its statement) needs a generalized Bregman divergence to handle a possibly non-differentiable convex loss — an extension of Bousquet-Elisseeff's original argument the book credits to itself as novel — via the reproducing-kernel property and Cauchy-Schwarz to convert a divergence bound into a bound on ∥h−h′∥K\|h-h'\|_K∥h−h′∥K​, then back into a pointwise loss bound.

Formalization scope

IsRKHSOf/IsMinimizer are restated locally in Stability, byte-identical to chunk 06-kernels's own copies (a draft item cannot import another chunk's draft module); H is an abstract real inner-product space with an evaluation map ev : H → X → ℝ standing for "elements of H are functions on X", the same device chunk 06's own RKHS formalization uses, since Mathlib's abstract Hilbert spaces are not themselves spaces of functions. UniformlyStable fixes the sample size m as part of the algorithm's type (A : (Fin m → X × Y) → (X → Y')), matching the book's own standing convention of a fixed sample size m throughout the chapter. Proposition 14.4 is stated pairwise — for any two samples differing by one point and any minimizers of their respective regularized objectives, the pointwise loss bound holds — rather than fixing a global choice-function algorithm A, since the book's own proof picks an arbitrary minimizer of each objective without asserting uniqueness; Corollary 14.5 does fix a choice function A (one minimizer per sample), since Theorem 14.2's own statement needs a single algorithm evaluated across the whole product-measure sample space. No numerical constant in any of the three theorems is altered from the book's own displayed form. A trivializing formalization this mission avoids: stating Theorem 14.2 only for the strict per-hypothesis loss bound (∀ h ∈ H, ∀ z, L_z(h) ≤ M) rather than the book's own weaker, algorithm-specific condition (hbound, ∀ S, ∀ z, L_z(A S) ≤ M) — the weaker hypothesis is kept, exactly matching the book's explicit statement that "a weaker condition suffices."

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 14.
  • O. Bousquet, A. Elisseeff, "Stability and generalization," Journal of Machine Learning Research 2, 2002, 499-526.
  • M. Kearns, D. Ron, "Algorithmic stability and sanity-check bounds for leave-one-out cross-validation," Neural Computation 11(6), 1999, 1427-1453.
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High-Dimensional Statistics V: Thresholding-Based Covariance EstimationTextbook

Motivation

Estimating a d×dd\times dd×d covariance matrix Σ\SigmaΣ from nnn samples is a canonical high-dimensional problem: the natural estimator, the sample covariance Σ^\hat\SigmaΣ^, is consistent in operator norm only when n≳dn\gtrsim dn≳d, which fails outright in the regime d≫nd\gg nd≫n common to modern applications. When Σ\SigmaΣ is additionally known to be sparse — few nonzero entries per row — a simple fix restores consistency even when d≫nd\gg nd≫n: threshold every entry of Σ^\hat\SigmaΣ^ below a data-dependent level to zero. This mission formalizes the matrix concentration machinery behind that fix and the resulting guarantee, following Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 6.

Setting

For a random matrix QQQ, the matrix variance is var(Q):=E[Q2]−(E[Q])2\mathrm{var}(Q):=\mathbb E[Q^2]-(\mathbb E[Q])^2var(Q):=E[Q2]−(E[Q])2, and the Loewner order A⪯BA\preceq BA⪯B on symmetric matrices means B−AB-AB−A is positive semidefinite. A zero-mean symmetric random matrix QQQ satisfies Bernstein's condition (Definition 6.10) with parameter b>0b>0b>0 if E[Qj]⪯12j! bj−2var(Q)\mathbb E[Q^j]\preceq\tfrac12 j!\,b^{j-2}\mathrm{var}(Q)E[Qj]⪯21​j!bj−2var(Q) for j=3,4,…j=3,4,\dotsj=3,4,… — the matrix analogue of the scalar Bernstein condition of Chapter 2. The operator (spectral) norm ∣ ⁣∣ ⁣∣M∣ ⁣∣ ⁣∣2|\!|\!|M|\!|\!|_2∣∣∣M∣∣∣2​ is MMM's largest singular value.

Given a threshold λ>0\lambda>0λ>0, the hard-thresholding operator is Tλ(u):=u⋅1[∣u∣>λ]T_\lambda(u):=u\cdot \mathbb 1[|u|>\lambda]Tλ​(u):=u⋅1[∣u∣>λ], extended entrywise to matrices (Eq. (6.52)). A covariance matrix Σ\SigmaΣ's sparsity pattern is captured by its adjacency matrix Ajℓ:=1[Σjℓ≠0]A_{j\ell}:=\mathbb 1[\Sigma_{j\ell}\neq0]Ajℓ​:=1[Σjℓ​=0] (p. 181); ∣ ⁣∣ ⁣∣A∣ ⁣∣ ⁣∣2≤d|\!|\!|A|\!|\!|_2\le d∣∣∣A∣∣∣2​≤d always, with equality only when Σ\SigmaΣ has no zero entries, and ∣ ⁣∣ ⁣∣A∣ ⁣∣ ⁣∣2≤s|\!|\!|A|\!|\!|_2\le s∣∣∣A∣∣∣2​≤s whenever Σ\SigmaΣ has at most sss nonzero entries per row.

Formalization targets

Goal — Theorem 6.23 (thresholding-based covariance estimation)

Let {xi}i=1n\{x_i\}_{i=1}^n{xi​}i=1n​ be i.i.d. zero-mean random vectors with covariance Σ\SigmaΣ, each coordinate sub-Gaussian with parameter at most σ\sigmaσ. If n>log⁡dn>\log dn>logd, then for any δ>0\delta>0δ>0, the thresholded sample covariance Tλn(Σ^)T_{\lambda_n}(\hat\Sigma)Tλn​​(Σ^) with λn/σ2=8log⁡d/n+δ\lambda_n/\sigma^2 = 8\sqrt{\log d/n}+\deltaλn​/σ2=8logd/n​+δ satisfies

P[ ∣ ⁣∣ ⁣∣Tλn(Σ^)−Σ∣ ⁣∣ ⁣∣2≥2∣ ⁣∣ ⁣∣A∣ ⁣∣ ⁣∣2λn ]  ≤  8e−n16min⁡{δ,δ2}.\mathbb P\big[\,|\!|\!|T_{\lambda_n}(\hat\Sigma)-\Sigma|\!|\!|_2 \ge 2|\!|\!|A|\!|\!|_2\lambda_n\,\big] \;\le\; 8e^{-\frac{n}{16}\min\{\delta,\delta^2\}}.P[∣∣∣Tλn​​(Σ^)−Σ∣∣∣2​≥2∣∣∣A∣∣∣2​λn​]≤8e−16n​min{δ,δ2}.

The error scales with the graph sparsity ∣ ⁣∣ ⁣∣A∣ ⁣∣ ⁣∣2|\!|\!|A|\!|\!|_2∣∣∣A∣∣∣2​, not with ddd directly — the whole point of thresholding when the ambient dimension is much larger than the sample size.

Milestone — Theorem 6.17 (the matrix Bernstein bound)

For independent, zero-mean, symmetric random matrices {Qi}\{Q_i\}{Qi​} satisfying Bernstein's condition with parameter bbb,

P[1n∣ ⁣∣ ⁣∣∑i=1nQi∣ ⁣∣ ⁣∣2≥δ]  ≤  2 rank(∑i=1nvar(Qi))exp⁡(−nδ22(σ2+bδ)).\mathbb P\Big[\frac1n\Big|\!\Big|\!\Big|\sum_{i=1}^n Q_i\Big|\!\Big|\!\Big|_2 \ge \delta\Big] \;\le\; 2\,\mathrm{rank}\Big(\sum_{i=1}^n\mathrm{var}(Q_i)\Big)\exp\Big(-\frac{n\delta^2}{2(\sigma^2+b\delta)}\Big).P[n1​​​​i=1∑n​Qi​​​​2​≥δ]≤2rank(i=1∑n​var(Qi​))exp(−2(σ2+bδ)nδ2​).

This is the general matrix concentration tool the whole chapter builds toward; Theorem 6.23 is one of its corollaries.

Milestone — Eq. (6.54) (the deterministic thresholding bound)

For any λn\lambda_nλn​ with ∥Σ^−Σ∥max⁡≤λn\|\hat\Sigma-\Sigma\|_{\max}\le\lambda_n∥Σ^−Σ∥max​≤λn​, ∣ ⁣∣ ⁣∣Tλn(Σ^)−Σ∣ ⁣∣ ⁣∣2≤2∣ ⁣∣ ⁣∣A∣ ⁣∣ ⁣∣2λn|\!|\!|T_{\lambda_n}(\hat\Sigma)-\Sigma|\!|\!|_2\le2|\!|\!|A|\!|\!|_2\lambda_n∣∣∣Tλn​​(Σ^)−Σ∣∣∣2​≤2∣∣∣A∣∣∣2​λn​ — a purely deterministic fact, with no probability involved, that reduces Theorem 6.23's proof to a single probabilistic input: controlling ∥Σ^−Σ∥max⁡\|\hat\Sigma-\Sigma\|_{\max}∥Σ^−Σ∥max​.

Significance

Theorem 6.17 is the workhorse of the whole chapter: besides Theorem 6.23, it also underlies Corollary 6.20's operator-norm bound for the unstructured sample covariance matrix (used in turn for the two example ensembles in Section 6.4.5), by taking Qi:=xixiT−ΣQ_i:=x_ix_i^T-\SigmaQi​:=xi​xiT​−Σ. Theorem 6.23 itself is the standard justification for thresholding-based covariance estimators used throughout high-dimensional statistics whenever the sparsity pattern of Σ\SigmaΣ, though unknown, is believed to be structured.

Formalizing it. No faithful prior art exists on the platform for the matrix Bernstein bound or covariance thresholding (a fresh search for "matrix Bernstein," "Bernstein condition matrix," "thresholding covariance," and "sparse covariance" returned no hits). The existing RademacherWigner.* items formalize spectral-edge and empirical-spectral-distribution bounds for the Wigner ensemble specifically (a symmetric matrix with i.i.d. entries) — a narrower, different random-matrix model from the general Bernstein-condition matrices this chapter treats, and not reused here. All three theorems are drafted as open goals (:= by sorry).

Difficulty

The naive approach to a matrix tail bound — apply the scalar Chernoff/Bernstein technique directly to the operator norm — fails because the operator norm is not a linear functional of QQQ, so the scalar moment generating function bound does not translate directly. The resolution (Lemma 6.13, not itself part of this mission) instead bounds the trace of the matrix exponential of the sum, which is linear-algebraically tractable via the Golden–Thompson-type inequality and the union bound over the (at most rank(Vˉ)\mathrm{rank}(\bar V)rank(Vˉ)) nonzero eigenvalue directions of the aggregate variance Vˉ=∑ivar(Qi)\bar V=\sum_i\mathrm{var}(Q_i)Vˉ=∑i​var(Qi​) — this is exactly why the bound's prefactor is rank(Vˉ)\mathrm{rank}(\bar V)rank(Vˉ), not the ambient dimension ddd: a low-rank aggregate variance (e.g. from a highly structured collection of matrices) yields a much tighter bound than a naive union bound over all ddd eigen-directions would. Theorem 6.23's own difficulty is entirely in the reduction to Theorem 6.17 plus Eq. (6.54): checking that Qi:=xixiT−ΣQ_i:=x_ix_i^T-\SigmaQi​:=xi​xiT​−Σ satisfies the Bernstein condition with the stated parameters, and that ∥Σ^−Σ∥max⁡\|\hat\Sigma-\Sigma\|_{\max}∥Σ^−Σ∥max​ concentrates at the stated rate via a union bound over the O(d2)O(d^2)O(d2) matrix entries.

Formalization scope

"Symmetric" is realized via Mathlib's Matrix.IsSymm; the Loewner order via (B-A).PosSemidef. The matrix moment generating function itself (ΨQ(λ):=E[e^{λQ}]) is not formalized, since none of this mission's three theorem statements need it directly — Bernstein's condition (Definition 6.10) is stated purely in terms of polynomial moments E[Qj]\mathbb E[Q^j]E[Qj], avoiding the substantial extra machinery (Mathlib's NormedSpace.exp for matrices) that a faithful matrix-exponential definition would require, at no cost to faithfulness for the three statements actually drafted.

Independence of {Qi}\{Q_i\}{Qi​}/{xi}\{x_i\}{xi​} is realized via Mathlib's iIndepFun; this required adding a local MeasurableSpace (Matrix (Fin d) (Fin d) ℝ) instance in the workspace, since Matrix is a def, not an abbrev, over the underlying Pi type, so Lean's instance search does not automatically find the Pi-type MeasurableSpace instance for it. "Identically distributed" is realized via Mathlib's IdentDistrib against a fixed reference index. "Each component sub-Gaussian" is restated locally as an explicit MGF bound at the reference index, per this book's cross-chapter rule against importing another chapter's draft definitions.

If a statement admits a trivializing formalization: the rank(...) prefactor of Theorem 6.17 is kept exactly, not replaced by the ambient dimension ddd (which would be a strictly weaker, non-trivializing but unfaithful simplification, since the bound's whole point is that rank(...) ≤ d can be much smaller). ‖·‖_max and opNorm at d=0 return Mathlib's junk value 0 (harmless: no matrix entries or singular values exist at that degenerate size either).

Out of scope for this mission: Theorem 6.15 (the sub-Gaussian-tail matrix concentration result that precedes Theorem 6.17 in the same section) and Corollary 6.20 (the unstructured covariance-estimation corollary) — both natural follow-on work, cut for this chunk's time budget; see STATUS.md.

Selected references

  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019. DOI: 10.1017/9781108627771. Chapter 6.
  • J. A. Tropp, "User-friendly tail bounds for sums of random matrices," Foundations of Computational Mathematics, 12(4):389–434, 2012.
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Foundations of Machine Learning XI: Maximum Entropy Models and DualityTextbook

Motivation

Maximum entropy (Maxent) models are a widely used family of density-estimation algorithms: given a sample and a set of features, they select the distribution that matches the empirical feature averages while being otherwise as "agnostic" (close to a prior, usually uniform) as possible — a principle that, notably, never requires specifying a parametric family of distributions to search over. This mission formalizes the theorem that explains why this works in practice: Maxent's primal optimization (over distributions, subject to feature-matching constraints) is exactly dual to an unconstrained maximum-likelihood problem over a specific, rich parametric family — the Gibbs distributions — even though the Maxent principle never mentions that family at all.

Setting

For a sample S=(x1,…,xm)S=(x_1,\dots,x_m)S=(x1​,…,xm​) drawn i.i.d. from DDD over a finite set XXX, and a feature map Φ:X→RN\Phi:X\to\mathbb R^NΦ:X→RN with ∥Φ∥∞≤r\|\Phi\|_\infty\le r∥Φ∥∞​≤r, the Maxent principle seeks p∈Δp\in\Deltap∈Δ (the simplex of distributions over XXX) minimizing the relative entropy D(p∥p0)D(p\|p_0)D(p∥p0​) to a prior p0p_0p0​, subject to ∥Ex∼p[Φ(x)]−Ex∼D^[Φ(x)]∥∞≤λ\|E_{x\sim p}[\Phi(x)]-E_{x\sim\hat D}[\Phi(x)]\|_\infty\le\lambda∥Ex∼p​[Φ(x)]−Ex∼D^​[Φ(x)]∥∞​≤λ (problem 12.7). Introducing the indicator function IKI_KIK​ (000 on KKK, +∞+\infty+∞ elsewhere) turns this into the unconstrained primal objective F(p)=D~(p∥p0)+IC(Ep[Φ])F(p)=\tilde D(p\|p_0)+I_C(E_p[\Phi])F(p)=D~(p∥p0​)+IC​(Ep​[Φ]) (Eq. 12.8), with CCC the feature-constraint set. A Gibbs distribution with parameter w∈RNw\in\mathbb R^Nw∈RN is pw(x)=p0(x)ew⋅Φ(x)/Z(w)p_w(x)=p_0(x)e^{w\cdot\Phi(x)}/Z(w)pw​(x)=p0​(x)ew⋅Φ(x)/Z(w), Z(w)Z(w)Z(w) the partition function (Eq. 12.9); its associated dual objective is G(w)=1m∑ilog⁡pw(xi)p0(xi)−λ∥w∥1G(w)=\frac1m\sum_i\log\frac{p_w(x_i)}{p_0(x_i)}-\lambda\|w\|_1G(w)=m1​∑i​logp0​(xi​)pw​(xi​)​−λ∥w∥1​ (Eq. 12.10) — note −1m∑ilog⁡pw(xi)-\frac1m\sum_i\log p_w(x_i)−m1​∑i​logpw​(xi​) is exactly the empirical log-loss LS(w)L_S(w)LS​(w), so maximizing GGG is minimizing an L1-regularized log-loss over the Gibbs family.

Formalization targets

Theorem 12.2 — the mission's goal (Maxent duality). sup⁡w∈RNG(w)=min⁡pF(p)\sup_{w\in\mathbb R^N}G(w)=\min_pF(p)supw∈RN​G(w)=minp​F(p). Furthermore, letting p∗=arg⁡min⁡pF(p)p^*=\arg\min_pF(p)p∗=argminp​F(p) and d∗=sup⁡wG(w)d^*=\sup_wG(w)d∗=supw​G(w): for any ϵ>0\epsilon>0ϵ>0 and any www with ∣G(w)−d∗∣<ϵ|G(w)-d^*|<\epsilon∣G(w)−d∗∣<ϵ, D(p∗∥pw)≤ϵD(p^*\|p_w)\le\epsilonD(p∗∥pw​)≤ϵ.

Theorem 12.3 (Maxent L1-regularization generalization bound, milestone). Fix δ>0\delta>0δ>0. Let w^\hat ww^ solve the L1-regularized dual (12.12) with λ=2Rm(H)+rlog⁡(2/δ)/(2m)\lambda=2R_m(H)+r\sqrt{\log(2/\delta)/(2m)}λ=2Rm​(H)+rlog(2/δ)/(2m)​. Then, with probability at least 1−δ1-\delta1−δ,

LD(w^)≤inf⁡wLD(w)+2∥w^∥1[2Rm(H)+rlog⁡(2/δ)/(2m)].L_D(\hat w) \le \inf_wL_D(w) + 2\|\hat w\|_1\Big[2R_m(H)+r\sqrt{\log(2/\delta)/(2m)}\Big].LD​(w^)≤winf​LD​(w)+2∥w^∥1​[2Rm​(H)+rlog(2/δ)/(2m)​].

Significance

Theorem 12.2 is one of the most striking dualities in the book: the Maxent principle, phrased purely in terms of closeness to a prior distribution, turns out to always produce a solution in the Gibbs family — not because that family was ever specified, but because relative entropy is the specific measure of closeness whose Fenchel conjugate is the log-partition function. This explains a whole zoo of models (log-linear models, exponential families, Gaussian and bimodal Gibbs distributions from quadratic features) as instances of a single duality theorem, and gives a computationally friendlier route to the (constrained, infinite-if-XXX-is-large) primal problem via the (unconstrained, NNN-dimensional) dual. The theorem's proof is a genuine application of conditional (Fenchel) strong duality, not an unconditional fact — this is, per the chapter's own brief, the sharpest trivialization risk in the entire mission series, since "strong duality always holds for convex problems" is false in general, and a formalization skipping the book's own qualification condition (λ>0\lambda>0λ>0, placing u0u_0u0​ in the interior of the constraint set) would prove a different, potentially-false statement. No prior art on the platform is faithful: GET /theorems?q=maximum+entropy returns no hits, and Mathlib's generic Fenchel-conjugate machinery (Analysis/Convex/Conjugate) does not package the book's own specific qualification conditions as a single reusable theorem matching Theorem B.39 — reusing it inside a proof (not the audited statement) remains available to whoever proves this theorem later.

Not formalized here: Theorem 12.4 (a Bregman-divergence generalization of Theorem 12.2) and Theorem 12.5 (its L2-regularized concrete special case). BRIEF.md itself flags Theorem 12.4 as possibly too heavy and offers Theorem 12.5 as an easier alternative; this mission omits both, since even Theorem 12.5 requires a second, structurally parallel dual-objective-and-minimizer formalization (for L2 rather than L1 regularization) — disproportionate to this mission's budget once Theorem 12.2's own qualification-condition bookkeeping (the heaviest single item in this mission series) is accounted for. §12.1 (density estimation without features: ML/MAP), §12.7 (coordinate descent), and §12.8-12.9 (Bregman-divergence extensions, L2-regularization in general) are likewise out of scope, per BRIEF.md's own page-range restriction.

Difficulty

Theorem 12.2's proof is the book's own explicit application of the Fenchel duality theorem (Theorem B.39, Appendix B) to the specific triple f(p)=D~(p∥p0)f(p)=\tilde D(p\|p_0)f(p)=D~(p∥p0​), g(u)=IC(u)g(u)=I_C(u)g(u)=IC​(u), Ap=∑xp(x)Φ(x)Ap=\sum_xp(x)\Phi(x)Ap=∑x​p(x)Φ(x) — every qualification condition (A a bounded linear map, u_0\in A(\mathrm{dom}f)\cap\mathrm{cont}(g), needing \lambda>0 to place u_0 in int(C)) must be checked for this triple, not assumed generically; the conjugate computations themselves (f^*(q)=\log\sum_xp_0(x)e^{q(x)}$ via Lemma B.37, g^(w)=E_{\hat D}[w\cdot\Phi]+\lambda|w|_1 via the dual-norm identity) are specific algebraic derivations, not immediate from abstract duality alone. The second clause's proof needs a further, non-obvious algebraic identity (G(w)-D(p^|p_0)+D(p^|p_w)expanding, via Hölder's inequality applied to the primal feasibility ofp^, to something \le0) that is not a restatement of the first clause but a separate argument built on top of it. Theorem 12.3's proof structurally mirrors chunk 04's SRM bound (bounding L_D(\hat w)-L_S(\hat w)via Hölder's inequality and the Rademacher-complexity feature-concentration bound of Eq. 12.5, then using\hat w`'s optimality twice), but is applied to the log-loss of a Gibbs distribution rather than a generic bounded loss.

Formalization scope

MaxEntPrimalObjective uses EReal (the extended reals) so that the book's own +\infty values (from I_K, \tilde D) are represented exactly, matching the chapter's own explicit use of an extended-real-valued indicator function rather than a soft penalty — a trivializing formalization this mission avoids is silently replacing +\infty with a large real sentinel, which would misstate a convex-analysis object whose entire role in the proof is its infinite value outside the feasible/simplex set. hlam : 0 < lam is a genuine load-bearing hypothesis in the goal theorem, matching the book's own use of \lambda>0 to invoke Theorem B.39's qualification condition — not a free convexity assumption; this is the mission's central faithfulness guard against the chapter's own named trivialization risk. EmpiricalRademacherComplexity/ RademacherComplexity are restated locally, byte-identical to chunks 05-svm/07-boosting's own copies (a draft item cannot import another chunk's draft module). p^* in the goal theorem and \hat w in Theorem 12.3 are both quantified via explicit hypotheses (IsLeast, a minimizer inequality) rather than assumed to exist unconditionally, matching the book's own "let p^*=..."/"let \hat w be a solution of..." phrasing without asserting existence or uniqueness beyond what the book itself asserts. No numerical constant in either theorem is altered from the book's own displayed form.

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 12, §12.1-12.6.
  • E. T. Jaynes, "Information theory and statistical mechanics," Physical Review 106(4), 1957, 620-630.
  • S. Della Pietra, V. Della Pietra, J. Lafferty, "Inducing features of random fields," IEEE Transactions on Pattern Analysis and Machine Intelligence 19(4), 1997, 380-393.
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Algorithmic Game TheoryOperations ResearchProbability+1·Captain: mikedeng1

Stochastic Orders IX: The PQD and Supermodular OrdersTextbook

Ordering how strongly two variables move together

The first eight chapters of Shaked and Shanthikumar's Stochastic Orders (Springer, 2007) compare single random variables — location, variability, convexity. Chapter IX turns to a different question: given two coordinates of a random vector, how strongly do they tend to move together? "Large values of X1X_1X1​ go with large values of X2X_2X2​" is a qualitative property (positive dependence); comparing how much two bivariate distributions exhibit it, holding their individual marginals fixed, is what this chapter's positive dependence orders make precise. This mission formalizes the two central ones — the PQD order and the supermodular order — and the supermodular order's closure properties, the chapter's own capstone result.

The PQD and supermodular orders

Let X=(X1,…,Xn)X=(X_1,\dots,X_n)X=(X1​,…,Xn​) and Y=(Y1,…,Yn)Y=(Y_1,\dots,Y_n)Y=(Y1​,…,Yn​) be two random vectors, with joint survival function Fˉ(x)=P{X1>x1,…,Xn>xn}\bar F(x)=P\{X_1>x_1,\dots,X_n>x_n\}Fˉ(x)=P{X1​>x1​,…,Xn​>xn​} and joint distribution function F(x)=P{X1≤x1,…,Xn≤xn}F(x)=P\{X_1\le x_1,\dots,X_n\le x_n\}F(x)=P{X1​≤x1​,…,Xn​≤xn​} (similarly Gˉ,G\bar G, GGˉ,G for YYY). XXX is smaller than YYY in the PQD order, written X≤PQDYX\le_{PQD}YX≤PQD​Y, if

Fˉ(x)≤Gˉ(x)  and  F(x)≤G(x)for every x∈Rn.\bar F(x)\le\bar G(x)\ \text{ and }\ F(x)\le G(x) \quad\text{for every }x\in\mathbb{R}^n.Fˉ(x)≤Gˉ(x)  and  F(x)≤G(x)for every x∈Rn.

(It follows, though it need not be assumed, that XXX and YYY then share the same univariate marginals — the two inequalities together pin the marginals down, unlike a single one alone.) This is Lehmann's positive-quadrant-dependence order in its general multivariate form: YYY's coordinates cluster together, in both the upper and lower "quadrants," at least as strongly as XXX's.

A function φ:Rn→R\varphi:\mathbb{R}^n\to\mathbb{R}φ:Rn→R is supermodular if φ(x)+φ(y)≤φ(x∧y)+φ(x∨y)\varphi(x)+\varphi(y)\le\varphi(x\wedge y)+\varphi(x\vee y)φ(x)+φ(y)≤φ(x∧y)+φ(x∨y) for the coordinatewise meet/join — the function-level notion the platform's Topkis/Supermodularity series already formalizes for games and lattices, reused here directly. XXX is smaller than YYY in the supermodular order, written X≤smYX\le_{sm}YX≤sm​Y, if E[φ(X)]≤E[φ(Y)]E[\varphi(X)]\le E[\varphi(Y)]E[φ(X)]≤E[φ(Y)] for every supermodular φ\varphiφ for which the two expectations exist. Because the indicator of any upper or lower orthant is itself supermodular, X≤smY  ⟹  X≤PQDYX\le_{sm}Y\implies X\le_{PQD}YX≤sm​Y⟹X≤PQD​Y (Eq. 9.A.17): the supermodular order is strictly finer than the PQD order, and for n=2n=2n=2 the two coincide.

Formalization targets

Goal: closure properties of the supermodular order (Theorem 9.A.9(a),(c))

(X1,…,Xn)≤sm(Y1,…,Yn)  ⟹  (g1(X1),…,gn(Xn))≤sm(g1(Y1),…,gn(Yn))(X_1,\dots,X_n)\le_{sm}(Y_1,\dots,Y_n) \implies (g_1(X_1),\dots,g_n(X_n))\le_{sm}(g_1(Y_1),\dots,g_n(Y_n))(X1​,…,Xn​)≤sm​(Y1​,…,Yn​)⟹(g1​(X1​),…,gn​(Xn​))≤sm​(g1​(Y1​),…,gn​(Yn​))

whenever every gig_igi​ is increasing, or every gig_igi​ is decreasing (part a); and

X≤smY  ⟹  XI≤smYIfor every I⊆{1,…,n}X\le_{sm}Y \implies X_I\le_{sm}Y_I \quad\text{for every } I\subseteq\{1,\dots,n\}X≤sm​Y⟹XI​≤sm​YI​for every I⊆{1,…,n}

(part c, closure under marginalization). These are two of Theorem 9.A.9's five closure properties — the theorem the brief for this mission recommends as its goal — chosen as the ones that need no further definitional machinery beyond the orders themselves (composition and a coordinate projection, both plain pushforwards of the vector's law).

Supporting milestone

  • Theorem 9.A.4, the general multivariate closure of the PQD order under independent pairing: if X≤PQDYX\le_{PQD}YX≤PQD​Y, U≤PQDVU\le_{PQD}VU≤PQD​V, with X,UX,UX,U independent and Y,VY,VY,V independent, then (φ1(X1,U1),…,φn(Xn,Un))≤PQD(φ1(Y1,V1),…,φn(Yn,Vn))(\varphi_1(X_1,U_1),\dots,\varphi_n(X_n,U_n))\le_{PQD}(\varphi_1(Y_1,V_1),\dots,\varphi_n(Y_n,V_n))(φ1​(X1​,U1​),…,φn​(Xn​,Un​))≤PQD​(φ1​(Y1​,V1​),…,φn​(Yn​,Vn​)) for all increasing φi\varphi_iφi​ — the closure property the chapter opens with (as Theorem 9.A.1, the bivariate case), generalized to nnn dimensions.

Significance

Positive dependence orders formalize a comparison operations research and risk management need constantly but rarely state precisely: two portfolios, insurance lines, or queueing networks with identical individual risk profiles can still differ sharply in how their components co-move, and that co-movement — not the marginals — is often what drives tail risk, correlated failures, or aggregate variability. The supermodular order is the standard tool for comparing this directly: Theorem 9.A.9's closure properties are what let a comparison established for primitive components survive the operations a model actually performs on them — relabeling by a monotone transform (part a), reading off a subset of coordinates (part c), combining independent sub-vectors (part b), conditioning on a covariate (part d), or passing to a distributional limit (part e). Chapter VI's multivariate stochastic order and Chapter VII's multivariate convex order are the two other multivariate orders in the book; the supermodular order is the one built specifically to compare dependence structure rather than location or spread, and it connects directly to the platform's existing Topkis/Supermodularity series, whose function-level predicate this mission reuses rather than restates.

Formalizing Theorem 9.A.9 fixes the exact shape a supermodular-order closure claim takes when built as a pushforward of the vector's law — the natural Mathlib-idiomatic rendering once the order is stated on laws rather than on variables tied to a fixed ambient space — for any future mission in this series or elsewhere that needs to state a closure property of a vector-valued stochastic order. No proof is attempted; both drafted parts of Theorem 9.A.9 have short book proofs (part (a) from the fact that composing a supermodular function with all-increasing or all-decreasing coordinate maps is again supermodular; part (c) the book calls "easy to prove"), making them plausible future proof targets.

Difficulty

The chapter's central definitional trap is that the PQD order's defining condition — even in its general multivariate form — determines the marginals as a consequence of the two joint inequalities holding together, not as a separate hypothesis to add; adding same-marginals as an extra explicit condition on top of Eqs. (9.A.13)-(9.A.14) would not be false, but it would present as a hypothesis something the theorem's own two conditions already force. A second trap is specific to Theorem 9.A.9(a): the gig_igi​ must be uniformly increasing or uniformly decreasing across all coordinates, not an arbitrary per-coordinate mix — a mixed-monotonicity version is a materially different, unproven claim, since it is exactly the all-same-direction condition that keeps a composition with a supermodular function supermodular. A third, more basic trap common to every function-class order in this book: "for every supermodular φ\varphiφ" must be a genuine universal quantifier with the two expectations' existence stated as an explicit hypothesis, not a global assumption or a specific test function standing in for the whole class.

Formalization scope

Unlike the univariate orders formalized elsewhere in this series (which take random variables X:Ω→RX:\Omega\to\mathbb{R}X:Ω→R, Y:Ω′→RY:\Omega'\to\mathbb{R}Y:Ω′→R on two possibly-different probability spaces), PQDOrder and SupermodularOrder here are stated directly on the two vectors' laws — measures P,QP,QP,Q on ι→R\iota\to\mathbb{R}ι→R for a finite index type ι\iotaι — since the book's own comparisons never reference a joint law of XXX and YYY together, only their separate distributions. This is also what lets Theorem 9.A.9(a)'s coordinatewise composition and (c)'s marginalization be stated as plain pushforwards (Measure.map) of one law, without carrying an ambient sample space through the statement. The index type is left an arbitrary finite type (Fintype ι, not fixed to Fin n) so the same two declarations serve both a full nnn-vector and any marginal sub-vector obtained by restricting to a subset III of coordinates — the shape Theorem 9.A.9(c) itself needs. Supermodularity reuses the platform's own Supermodularity.Monotonicity.SupermodularOn (from the Topkis series, via a kind: reference item) with its relativizing set argument fixed to Set.univ, its plain unrelativized form — checked to match the book's φ(x)+φ(y)≤φ(x∧y)+φ(x∨y) on ι → ℝ's own coordinatewise lattice structure exactly, not a games- or player-scoped variant. Independence in Theorem 9.A.4 is formalized by taking the joint law of the two independent vectors to be the product measure of their marginals — the standard way to construct an independent coupling with prescribed marginals — rather than adding a separate independence hypothesis about pre-existing random variables. Measurable hypotheses are added on every map a Measure.map is taken along, guarding against the pushforward's junk-zero-measure convention for a non-measurable map; none narrows what the book's own theorems claim, since every map used (a monotone/antitone composition, a coordinate projection) is genuinely measurable. A trivializing formalization is ruled out explicitly: the supermodular quantifier ranges over the reused, already-audited Topkis predicate rather than a hand-rolled or restricted one, and the "for all increasing φi\varphi_iφi​" of Theorem 9.A.4 is a genuine universal over jointly-monotone functions of two arguments, not a fixed example.

This mission draws on the platform's own Topkis/Supermodularity series for its supermodular function-level building block (Supermodularity.Monotonicity.SupermodularOn, reused as a reference item — the strongest prior-art connection of the whole nine-chapter series, per the series plan) but on no prior art for the orders themselves (repeated searches for "PQD", "positive dependence", "Fréchet bound" and "supermodular" returned nothing on-topic beyond the Topkis series as of 2026-09-18). Reusable beyond this mission: the laws-only, arbitrary-Fintype- index formalization pattern is available to any later mission in this series needing a multivariate order (Chapter VI's multivariate stochastic order, Chapter VII's multivariate convex order) that wants marginalization or coordinatewise composition stated as plain pushforwards.

Selected references

  • M. Shaked and J. G. Shanthikumar, Stochastic Orders, Springer Series in Statistics, Springer, 2007. https://doi.org/10.1007/978-0-387-34675-5
  • E. L. Lehmann, "Some concepts of dependence", Annals of Mathematical Statistics, 37(5), 1966, 1137–1153. https://doi.org/10.1214/aoms/1177699260
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High-Dimensional Statistics VII: Eigenvector Perturbation for High-Dimensional PCATextbook

Motivation

Principal component analysis (PCA) is one of the oldest and most widely used tools in multivariate statistics: given data with covariance matrix Σ\SigmaΣ, project onto the top eigenvector(s) of Σ\SigmaΣ to find the directions of maximal variance. In practice one never observes Σ\SigmaΣ itself, only a perturbed version — a sample covariance matrix Σ^=Σ+P\hat\Sigma = \Sigma + PΣ^=Σ+P, with PPP the (random) estimation error. The natural question, asked since at least Davis and Kahan (1970) and Wedin (1972), is: how close is the top eigenvector of Σ^\hat\SigmaΣ^ to that of Σ\SigmaΣ? Wainwright's High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 8, gives a self-contained, sharp, non-asymptotic answer, phrased entirely in terms of two deterministic quantities: the eigengap of Σ\SigmaΣ, and a single scalar summarizing how the perturbation PPP couples to the top eigendirection.

Unlike most of the results in this book series, this one is a statement of pure linear algebra: no probability, no concentration inequality, no sample size is needed to state or prove it. Randomness enters only afterward, when PPP is instantiated as an actual sampling error and bounded using the machinery of earlier chapters (Corollary 8.7, out of this mission's scope).

Setting

Let Σ∈Rd×d\Sigma \in \mathbb R^{d\times d}Σ∈Rd×d be a symmetric positive semidefinite matrix. Say θ∈Rd\theta \in \mathbb R^dθ∈Rd is a maximal unit eigenvector of Σ\SigmaΣ if ∥θ∥2=1\|\theta\|_2=1∥θ∥2​=1 and θ\thetaθ maximizes the Rayleigh quotient ⟨θ,Σθ⟩\langle\theta,\Sigma\theta\rangle⟨θ,Σθ⟩ over the whole unit sphere Sd−1\mathcal S^{d-1}Sd−1 — the variational characterization of the top eigenvector/eigenvalue pair, matching Eq. (8.14) of the book. Write γ1(Σ):=⟨θ∗,Σθ∗⟩\gamma_1(\Sigma) := \langle\theta^*,\Sigma\theta^*\rangleγ1​(Σ):=⟨θ∗,Σθ∗⟩ for the corresponding top eigenvalue. Say Σ\SigmaΣ has eigengap ν>0\nu>0ν>0 at θ∗\theta^*θ∗ if every unit vector vvv orthogonal to θ∗\theta^*θ∗ satisfies ⟨v,Σv⟩≤γ1(Σ)−ν\langle v,\Sigma v\rangle \le \gamma_1(\Sigma) - \nu⟨v,Σv⟩≤γ1​(Σ)−ν — the Courant-Fischer variational form of the book's ν:=γ1(Σ)−γ2(Σ)\nu := \gamma_1(\Sigma)-\gamma_2(\Sigma)ν:=γ1​(Σ)−γ2​(Σ).

For a symmetric perturbation matrix P∈Rd×dP \in \mathbb R^{d\times d}P∈Rd×d, write ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2:=sup⁡∥v∥2=1∣⟨v,Pv⟩∣|\!|\!|P|\!|\!|_2 := \sup_{\|v\|_2=1}|\langle v,Pv\rangle|∣∣∣P∣∣∣2​:=sup∥v∥2​=1​∣⟨v,Pv⟩∣ for its ℓ2\ell_2ℓ2​-operator norm, and

p~  :=  Pθ∗−⟨Pθ∗,θ∗⟩ θ∗\tilde p \;:=\; P\theta^* - \langle P\theta^*,\theta^*\rangle\,\theta^*p~​:=Pθ∗−⟨Pθ∗,θ∗⟩θ∗

for the component of Pθ∗P\theta^*Pθ∗ orthogonal to θ∗\theta^*θ∗ — the piece of the perturbation that actually couples the top eigendirection to the rest of the space (Eq. (8.11)). Note ∥p~∥2\|\tilde p\|_2∥p~​∥2​ can be far smaller than ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2|\!|\!|P|\!|\!|_2∣∣∣P∣∣∣2​: a perturbation can be large in every direction yet barely move the top eigenvector, if its interaction with θ∗\theta^*θ∗ specifically is small.

Formalization targets

Goal (Theorem 8.5)

Let Σ\SigmaΣ be symmetric positive semidefinite with maximal unit eigenvector θ∗\theta^*θ∗ and eigengap ν>0\nu>0ν>0. For any symmetric PPP with ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2<ν/2|\!|\!|P|\!|\!|_2 < \nu/2∣∣∣P∣∣∣2​<ν/2, and any maximal unit eigenvector θ^\hat\thetaθ^ of Σ^:=Σ+P\hat\Sigma := \Sigma+PΣ^:=Σ+P with ⟨θ^,θ∗⟩≥0\langle\hat\theta,\theta^*\rangle \ge 0⟨θ^,θ∗⟩≥0,

∥θ^−θ∗∥2  ≤  2∥p~∥2ν−2∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2.\|\hat\theta - \theta^*\|_2 \;\le\; \frac{2\|\tilde p\|_2}{\nu - 2|\!|\!|P|\!|\!|_2}.∥θ^−θ∗∥2​≤ν−2∣∣∣P∣∣∣2​2∥p~​∥2​​.

Milestone (Lemma 8.6, the PCA basic inequality)

Under the same eigengap hypothesis, with $\Psi(\Delta;P) := \langle\Delta,P\Delta\rangle

  • 2\langle\Delta,P\theta^\rangleandandand\Delta := \hat\theta-\theta^$,
ν(1−⟨θ^,θ∗⟩2)  ≤  ∣Ψ(Δ;P)∣.\nu\bigl(1-\langle\hat\theta,\theta^*\rangle^2\bigr) \;\le\; |\Psi(\Delta;P)|.ν(1−⟨θ^,θ∗⟩2)≤∣Ψ(Δ;P)∣.

Significance

The bound isolates exactly what drives eigenvector instability: not the raw size of the perturbation but its projection onto the top eigendirection, rescaled by the inverse eigengap. This explains, in one inequality, the qualitative phenomenon Example 8.4 illustrates numerically (a tiny perturbation can move the eigenvector far when the eigengap is small) and quantifies exactly how far. It is the deterministic engine behind every consistency result for PCA in the rest of the chapter: Corollary 8.7 (rates for the spiked covariance model) and the sparse-PCA guarantee (Theorem 8.10) both specialize this same bound, after bounding ∥p~∥2\|\tilde p\|_2∥p~​∥2​ and ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2|\!|\!|P|\!|\!|_2∣∣∣P∣∣∣2​ using concentration for a specific random design. It is also a sharp instance of the general Davis-Kahan-type perturbation theory for symmetric matrices, phrased with an explicit, non-asymptotic constant rather than an O(⋅)O(\cdot)O(⋅).

The theorem is already proved in the source; this mission's contribution is a machine-checked formal statement (and, eventually, proof) of the bound and its supporting basic inequality, composing with any future formalization of the chapter's probabilistic corollaries.

Difficulty

The proof is genuinely variational, not spectral: it never diagonalizes Σ\SigmaΣ or Σ^\hat\SigmaΣ^, only uses that θ∗\theta^*θ∗ and θ^\hat\thetaθ^ are optimal for their respective Rayleigh-quotient maximizations. The one place a naive argument fails is in bounding ∣Ψ(Δ;P)∣|\Psi(\Delta;P)|∣Ψ(Δ;P)∣ itself (the proof of Lemma 8.6): a direct Cauchy-Schwarz bound on ⟨Δ,PΔ⟩\langle\Delta,P\Delta\rangle⟨Δ,PΔ⟩ using ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2|\!|\!|P|\!|\!|_2∣∣∣P∣∣∣2​ alone would produce a bound in terms of ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2|\!|\!|P|\!|\!|_2∣∣∣P∣∣∣2​ throughout, not the sharper ∥p~∥2\|\tilde p\|_2∥p~​∥2​ the theorem actually delivers; getting the sharper dependence requires decomposing Δ\DeltaΔ along θ∗\theta^*θ∗ and its orthogonal complement and tracking the two pieces separately (the ϱ\varrhoϱ, zzz decomposition on p. 244). The sharpness of the threshold ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2<ν/2|\!|\!|P|\!|\!|_2 < \nu/2∣∣∣P∣∣∣2​<ν/2 is also not a proof artifact: the book's own 2×22\times 22×2 example (Σ=diag(2,1)\Sigma=\mathrm{diag}(2,1)Σ=diag(2,1), P=diag(−1/2,1/2)P=\mathrm{diag}(-1/2,1/2)P=diag(−1/2,1/2)) shows the perturbed matrix can lose a unique maximal eigenvector exactly at ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2=ν/2|\!|\!|P|\!|\!|_2 = \nu/2∣∣∣P∣∣∣2​=ν/2.

Formalization scope

Σ\SigmaΣ, PPP, Σ^=Σ+P\hat\Sigma=\Sigma+PΣ^=Σ+P are Matrix (Fin d) (Fin d) ℝ; "symmetric" is M.transpose = M; "positive semidefinite" is the quadratic-form condition ⟨v,Σv⟩≥0\langle v, \Sigma v\rangle \ge 0⟨v,Σv⟩≥0 for all vvv, stated directly rather than via a Mathlib PosSemidef typeclass. "Maximal unit eigenvector" and "eigengap" are both given their variational (Rayleigh-quotient) characterizations rather than defined through Mathlib's enumerated matrix-eigenvalue API — mathematically equivalent to the book's spectral definitions by the Courant-Fischer theorem, and the same characterization the book's own proof works with throughout (Eq. (8.14)). The operator norm ∣ ⁣∣ ⁣∣⋅∣ ⁣∣ ⁣∣2|\!|\!|\cdot|\!|\!|_2∣∣∣⋅∣∣∣2​ is likewise realized variationally, valid because this mission only ever applies it to symmetric matrices, exactly as the book does in this chapter. p~\tilde pp~​ is realized as a basis-independent vector in Rd\mathbb R^dRd (the component of Pθ∗P\theta^*Pθ∗ orthogonal to θ∗\theta^*θ∗) rather than the book's basis-dependent Rd−1\mathbb R^{d-1}Rd−1 representative; its ℓ2\ell_2ℓ2​-norm — the only quantity the theorem's conclusion uses — is identical either way.

Deliberate scope decision, disclosed here rather than silently: the book's own Theorem 8.5 concludes that Σ^\hat\SigmaΣ^ "has a unique maximal eigenvector θ^\hat\thetaθ^" satisfying the bound — asserting both existence and uniqueness as part of the theorem, on top of the quantitative bound. This mission formalizes only the quantitative bound, for an arbitrary maximal unit eigenvector θ^\hat\thetaθ^ of Σ^\hat\SigmaΣ^ satisfying the sign condition ⟨θ^,θ∗⟩≥0\langle\hat\theta,\theta^*\rangle\ge0⟨θ^,θ∗⟩≥0 — exactly what the book's own proof establishes (the proof never separately argues existence or uniqueness; both are consequences that could be derived from the bound together with a compactness argument for existence, left to a future extension) and exactly what every downstream use in the chapter (Examples, Corollary 8.7) actually invokes. A trivializing formalization would instead drop the sharp threshold ∣ ⁣∣ ⁣∣P∣ ⁣∣ ⁣∣2<ν/2|\!|\!|P|\!|\!|_2 < \nu/2∣∣∣P∣∣∣2​<ν/2 to ≤, or conflate the general operator norm with the symmetric-matrix Rayleigh-quotient characterization for a non-symmetric PPP; this mission does neither. Corollary 8.7 (spiked covariance rates) and Theorem 8.10 (sparse PCA, needing the uniform deviation condition of Eq. (8.26)) are out of this mission's scope; a companion mission formalizing them on top of this one's pca_eigenvector_perturbation_bound is natural future work, together with a proof of existence of a maximal unit eigenvector via compactness of the sphere.

Selected references

  • Wainwright, M. J. High-Dimensional Statistics: A Non-Asymptotic Viewpoint. Cambridge University Press, 2019. Chapter 8. DOI: 10.1017/9781108627771.
  • Davis, C., Kahan, W. M. "The rotation of eigenvectors by a perturbation. III." SIAM Journal on Numerical Analysis, 7(1), 1970, 1–46.
  • Wedin, P.-Å. "Perturbation bounds in connection with singular value decomposition." BIT Numerical Mathematics, 12(1), 1972, 99–111.
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High-Dimensional Statistics VI: The Lasso's l2-Error Bound under Restricted EigenvalueTextbook

Motivation

Modern regression problems routinely have far more candidate predictors than observations: genomics with tens of thousands of genes and a few hundred patients, signal recovery from far fewer measurements than the signal's ambient dimension, image reconstruction from an undersampled set of linear projections. In every such setting the classical least-squares estimator is either undetermined or hopelessly noisy, and the ordinary theory of linear regression, built for n≫dn \gg dn≫d, has nothing to say.

The Lasso — ℓ1\ell_1ℓ1​-penalized least squares, introduced by Tibshirani (1996) — is the workhorse response: penalize the least-squares objective by the ℓ1\ell_1ℓ1​-norm of the coefficient vector, which both drives many coordinates exactly to zero and remains a convex, tractable program. What is far from obvious a priori is that this convex relaxation is not just computationally convenient but statistically correct: under a condition on the design matrix, its estimation error is controlled at a rate matching what one could hope for even knowing the true support in advance. Wainwright's High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 7, gives the deterministic backbone of this guarantee — the part of the argument that holds for any noise vector and any design matrix satisfying a single geometric condition, before any probability is introduced.

Setting

Consider the linear model y=Xθ∗+wy = X\theta^* + wy=Xθ∗+w, where X∈Rn×dX \in \mathbb R^{n\times d}X∈Rn×d is a known design matrix, θ∗∈Rd\theta^* \in \mathbb R^dθ∗∈Rd is an unknown coefficient vector, and w∈Rnw \in \mathbb R^nw∈Rn is a noise vector, observed together with the response y∈Rny \in \mathbb R^ny∈Rn. Write ∥θ∥1:=∑j=1d∣θj∣\|\theta\|_1 := \sum_{j=1}^d|\theta_j|∥θ∥1​:=∑j=1d​∣θj​∣ and ∥v∥∞:=max⁡j∣vj∣\|v\|_\infty := \max_j |v_j|∥v∥∞​:=maxj​∣vj​∣. The Lagrangian Lasso is the convex program

θ^∈arg min⁡θ∈Rd{12n∥y−Xθ∥22+λn∥θ∥1},\hat\theta \in \operatorname*{arg\,min}_{\theta \in \mathbb R^d} \left\{ \frac{1}{2n}\|y - X\theta\|_2^2 + \lambda_n \|\theta\|_1 \right\},θ^∈θ∈Rdargmin​{2n1​∥y−Xθ∥22​+λn​∥θ∥1​},

with regularization parameter λn>0\lambda_n > 0λn​>0 chosen by the user.

Say θ∗\theta^*θ∗ is supported on S⊆{1,…,d}S \subseteq \{1,\dots,d\}S⊆{1,…,d} if θj∗=0\theta^*_j = 0θj∗​=0 for every j∉Sj \notin Sj∈/S, and write ∣S∣=s|S| = s∣S∣=s for its sparsity. For a subset SSS and a constant α≥1\alpha \ge 1α≥1, the cone

Cα(S):={Δ∈Rd∣∥ΔSc∥1≤α∥ΔS∥1}C_\alpha(S) := \{\Delta \in \mathbb R^d \mid \|\Delta_{S^c}\|_1 \le \alpha \|\Delta_S\|_1\}Cα​(S):={Δ∈Rd∣∥ΔSc​∥1​≤α∥ΔS​∥1​}

collects the directions in which an estimation error concentrated near the true support can plausibly point. The matrix XXX satisfies the restricted eigenvalue (RE) condition over SSS with parameters (κ,α)(\kappa,\alpha)(κ,α) if

1n∥XΔ∥22≥κ∥Δ∥22for all Δ∈Cα(S).\frac{1}{n}\|X\Delta\|_2^2 \ge \kappa \|\Delta\|_2^2 \qquad \text{for all } \Delta \in C_\alpha(S).n1​∥XΔ∥22​≥κ∥Δ∥22​for all Δ∈Cα​(S).

Ordinarily, when d>nd > nd>n, the quadratic cost's Hessian XTX/nX^TX/nXTX/n is rank-deficient and has a large flat subspace, so no uniform positive-curvature bound like this can hold over all of Rd\mathbb R^dRd; the RE condition asks for curvature only along the cone Cα(S)C_\alpha(S)Cα​(S) that the Lasso's own optimality actually forces its error into.

The companion notion — the restricted nullspace property, C1(S)∩null(X)={0}C_1(S) \cap \mathrm{null}(X) = \{0\}C1​(S)∩null(X)={0} — is the noiseless analogue: it is exactly the condition under which the ℓ1\ell_1ℓ1​-relaxed basis pursuit program min⁡θ∥θ∥1\min_\theta \|\theta\|_1minθ​∥θ∥1​ s.t. Xθ=yX\theta = yXθ=y exactly recovers every SSS-sparse θ∗\theta^*θ∗ from y=Xθ∗y = X\theta^*y=Xθ∗ (Theorem 7.8). A small pairwise incoherence δPW(X):=max⁡j,k∣⟨Xj,Xk⟩/n−1[j=k]∣\delta_{PW}(X) := \max_{j,k} |\langle X_j,X_k\rangle/n - \mathbb 1[j=k]|δPW​(X):=maxj,k​∣⟨Xj​,Xk​⟩/n−1[j=k]∣ is one simply-checked sufficient condition for it (Proposition 7.9).

Formalization targets

Goal (Theorem 7.13(a) and its final sentence)

Under (A1) θ∗\theta^*θ∗ supported on SSS, ∣S∣=s|S|=s∣S∣=s, and (A2) XXX satisfies the RE condition over SSS with parameters (κ,3)(\kappa,3)(κ,3): for any θ^\hat\thetaθ^ solving the Lagrangian Lasso with λn≥2∥XTw/n∥∞\lambda_n \ge 2\|X^Tw/n\|_\inftyλn​≥2∥XTw/n∥∞​,

∥θ^−θ∗∥2≤3κs λn,∥θ^−θ∗∥1≤4s ∥θ^−θ∗∥2.\|\hat\theta - \theta^*\|_2 \le \frac{3}{\kappa}\sqrt{s}\,\lambda_n, \qquad \|\hat\theta - \theta^*\|_1 \le 4\sqrt{s}\,\|\hat\theta-\theta^*\|_2.∥θ^−θ∗∥2​≤κ3​s​λn​,∥θ^−θ∗∥1​≤4s​∥θ^−θ∗∥2​.

Milestones

  • Theorem 7.8. The restricted nullspace property is equivalent to exact recovery by basis pursuit for every SSS-sparse vector.
  • Proposition 7.9. δPW(X)≤1/(3s)\delta_{PW}(X) \le 1/(3s)δPW​(X)≤1/(3s) implies the restricted nullspace property for every SSS with ∣S∣≤s|S|\le s∣S∣≤s.

Significance

The bound is the deterministic core underneath every high-dimensional consistency guarantee for the Lasso: once a statistician checks that a particular random design (Gaussian, sub-Gaussian, or otherwise) satisfies the RE condition with high probability, and bounds ∥XTw/n∥∞\|X^Tw/n\|_\infty∥XTw/n∥∞​ using concentration of the noise, this one inequality converts directly into a rate — Wainwright's own Examples 7.14–7.15 do exactly this for the classical Gaussian linear model and for compressed sensing. It also isolates why the Lasso is competitive with an oracle that already knows the support: the rate s/n\sqrt{s/n}s/n​ (up to log factors, once λn\lambda_nλn​ is instantiated) is the same order one would get regressing only on the sss true coordinates.

The theorem is already proved in the source; this mission's contribution is a machine-checked formal statement (and, eventually, proof) of the bound together with its two supporting structural results, in a form that composes with the rest of this book's formalized chapters and with any future formalization of the concentration arguments (Chapters 2–6) that supply λn\lambda_nλn​'s numerical value in specific models.

Difficulty

The proof is short but every step leans on getting the cone membership exactly right. The first hurdle is showing the error Δ:=θ^−θ∗\Delta := \hat\theta - \theta^*Δ:=θ^−θ∗ lands in C3(S)C_3(S)C3​(S) at all — this needs the Lagrangian basic inequality (from θ^\hat\thetaθ^'s optimality against θ∗\theta^*θ∗), not the simpler constrained-Lasso argument used for parts (b)/(c), and the constant 333 (not 111) comes precisely from the factor of 222 in the λn\lambda_nλn​ bound combined with Hölder's inequality on the noise term. A tempting shortcut is to assume the uniform curvature bound (7.24), ∥XΔ∥22/n≥κ∥Δ∥22\|X\Delta\|_2^2/n \ge \kappa\|\Delta\|_2^2∥XΔ∥22​/n≥κ∥Δ∥22​ for all Δ≠0\Delta \ne 0Δ=0 — but in the regime d>nd > nd>n this uniform bound is never satisfiable, since XTX/nX^TX/nXTX/n has a (d−n)(d-n)(d−n)-dimensional null space; the entire point of the restricted eigenvalue condition is to demand curvature only on the cone the optimality argument already produces.

Formalization scope

XXX, θ∗\theta^*θ∗, θ^\hat\thetaθ^, www are unconstrained vectors/matrices over Fin n/Fin d-indexed reals; SSS is a Finset (Fin d). The RE condition's constant κ\kappaκ is required positive, since the book divides by it throughout the discussion of Theorem 7.13 even though Definition 7.12 itself states the condition schematically; α=3\alpha=3α=3 is fixed to the book's own value, not a free parameter of the goal. The ℓ∞\ell_\inftyℓ∞​- and pairwise-incoherence suprema are real iSups over finite index types, which default to Mathlib's junk value 000 at dimension 000 — a degenerate corner with no vector to measure, not a trivializing case of the theorem's actual content. A trivializing formalization would drop the final-sentence ℓ1\ell_1ℓ1​-bound as "a trivial Cauchy–Schwarz corollary" or silently substitute the stronger, later-defined restricted isometry property for the restricted eigenvalue condition; this mission does neither. Parts (b) (constrained Lasso) and (c) (relaxed basis pursuit) of Theorem 7.13, and the primal–dual-witness support-recovery result (Theorem 7.21), are out of this mission's scope; a full-strength companion mission covering them, including the RIP-based Proposition 7.11 and the random-design certification Theorem 7.16, is natural future work.

Selected references

  • Wainwright, M. J. High-Dimensional Statistics: A Non-Asymptotic Viewpoint. Cambridge University Press, 2019. Chapter 7. DOI: 10.1017/9781108627771.
  • Tibshirani, R. "Regression shrinkage and selection via the Lasso." Journal of the Royal Statistical Society: Series B, 58(1), 1996, 267–288.
  • Chen, S. S., Donoho, D. L., Saunders, M. A. "Atomic decomposition by basis pursuit." SIAM Journal on Scientific Computing, 20(1), 1998, 33–61.
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Support Vector Machines IV: The Representer Theorem for Empirical SVM SolutionsTextbook

Motivation

Support vector machines (SVMs) are trained by solving a regularized empirical risk minimization problem over a reproducing kernel Hilbert space (RKHS) — a space that is typically infinite-dimensional. On its face, this looks computationally hopeless: how can a computer search an infinite-dimensional space for a minimizer? The representer theorem is the result that makes SVM training tractable at all: it shows that no matter how large the RKHS is, the minimizer of the SVM objective for a sample of size nnn always lies in the nnn-dimensional subspace spanned by the kernel evaluated at the nnn sample points. This turns an infinite- dimensional optimization problem into a finite-dimensional one before a single line of an optimization algorithm is written, and it is the reason every practical SVM solver (from the original sequential minimal optimization algorithm onward) searches only over nnn coefficients rather than over an abstract function space.

The theorem in this mission — Theorem 5.5 of Steinwart and Christmann, Support Vector Machines (Springer, 2008) — is stated for general convex losses and general kernels, subsuming the classification-SVM and regression-SVM special cases that appear throughout the machine learning literature. Its lineage traces to Kimeldorf and Wahba's 1971 representer theorem for spline-smoothing problems; the book's own version (attributed to a 1971 result, generalized here to arbitrary convex losses and RKHSs) is the general form used throughout the rest of the book.

Setting

Fix a nonempty set XXX (the input space) and a loss function L:X×R×R→[0,∞)L : X \times \mathbb R \times \mathbb R \to [0,\infty)L:X×R×R→[0,∞): a measurable map where L(x,y,t)L(x,y,t)L(x,y,t) is the cost of predicting label yyy by value ttt when the input is xxx. LLL is convex if L(x,y,⋅)L(x,y,\cdot)L(x,y,⋅) is convex for every fixed x,yx,yx,y.

A reproducing kernel Hilbert space (RKHS) over XXX is a real Hilbert space HHH of real-valued functions on XXX that carries a kernel k:X×X→Rk : X \times X \to \mathbb Rk:X×X→R with two properties: k(⋅,x)∈Hk(\cdot,x) \in Hk(⋅,x)∈H for every x∈Xx \in Xx∈X, and the reproducing property f(x)=⟨f,k(⋅,x)⟩Hf(x) = \langle f, k(\cdot,x)\rangle_Hf(x)=⟨f,k(⋅,x)⟩H​ holds for every f∈Hf \in Hf∈H and x∈Xx \in Xx∈X. Intuitively, kkk lets you evaluate any f∈Hf \in Hf∈H at a point xxx by taking an inner product with the fixed function k(⋅,x)k(\cdot,x)k(⋅,x) — this is what makes HHH a space of genuine, pointwise-evaluable functions rather than an abstract Hilbert space.

Given a finite sample D:=((x1,y1),…,(xn,yn))∈(X×R)nD := ((x_1,y_1),\dots,(x_n,y_n)) \in (X \times \mathbb R)^nD:=((x1​,y1​),…,(xn​,yn​))∈(X×R)n, the empirical LLL-risk of f:X→Rf : X \to \mathbb Rf:X→R is RL,D(f):=1n∑i=1nL(xi,yi,f(xi))R_{L,D}(f) := \tfrac1n\sum_{i=1}^n L(x_i,y_i,f(x_i))RL,D​(f):=n1​∑i=1n​L(xi​,yi​,f(xi​)). For a regularization parameter λ>0\lambda > 0λ>0, the SVM training problem asks for a minimizer of the regularized empirical risk

f↦λ∥f∥H2+RL,D(f)f \mapsto \lambda\|f\|_H^2 + R_{L,D}(f)f↦λ∥f∥H2​+RL,D​(f)

over all of HHH. A minimizer of this objective is called an empirical SVM solution fD,λf_{D,\lambda}fD,λ​.

Formalization targets

Goal — Theorem 5.5 (Representer theorem)

∃! fD,λ∈H:λ∥fD,λ∥H2+RL,D(fD,λ)=min⁡f∈H(λ∥f∥H2+RL,D(f)),fD,λ(x)=∑i=1nαi k(x,xi)   for some α1,…,αn∈R.\exists! \, f_{D,\lambda} \in H : \quad \lambda\|f_{D,\lambda}\|_H^2 + R_{L,D}(f_{D,\lambda}) = \min_{f \in H} \Bigl(\lambda\|f\|_H^2 + R_{L,D}(f)\Bigr), \qquad f_{D,\lambda}(x) = \sum_{i=1}^n \alpha_i\, k(x,x_i) \; \text{ for some } \alpha_1,\dots,\alpha_n \in \mathbb R.∃!fD,λ​∈H:λ∥fD,λ​∥H2​+RL,D​(fD,λ​)=f∈Hmin​(λ∥f∥H2​+RL,D​(f)),fD,λ​(x)=i=1∑n​αi​k(x,xi​) for some α1​,…,αn​∈R.

The theorem asserts both halves at once: the regularized empirical risk has a unique minimizer over the (possibly infinite-dimensional) HHH, and that unique minimizer is representable as a finite linear combination of the kernel functions at the sample points. Neither the coefficients αi\alpha_iαi​ nor the finite-dimensional subspace they live in are fixed in advance by the statement; only their existence is asserted, so a stronger claim (e.g. uniqueness or an explicit formula for the αi\alpha_iαi​) would be a different, harder theorem not proved here.

Supporting milestones (the general, population-level analogue)

The book develops the representer theorem's existence-and-uniqueness clause by first proving it for the corresponding population problem — minimizing f↦λ∥f∥H2+RL,P(f)f \mapsto \lambda\|f\|_H^2 + R_{L,P}(f)f↦λ∥f∥H2​+RL,P​(f) over a distribution PPP rather than a finite sample — and then adapting the same two arguments to the empirical case:

  • Lemma 5.1 (uniqueness): for a convex loss and an RKHS HHH with RL,P(f)<∞R_{L,P}(f) < \inftyRL,P​(f)<∞ for some f∈Hf \in Hf∈H, the regularized population risk has at most one minimizer over HHH, for every λ>0\lambda > 0λ>0.
  • Theorem 5.2 (existence): for a convex, PPP-integrable Nemitski loss and the RKHS of a bounded kernel, the regularized population risk has at least one minimizer, for every λ>0\lambda > 0λ>0.
  • Theorem 5.6 (non-triviality): under the same hypotheses as Theorem 5.2, if HHH can beat the risk of the zero function (inf⁡f∈HRL,P(f)<RL,P(0)\inf_{f \in H} R_{L,P}(f) < R_{L,P}(0)inff∈H​RL,P​(f)<RL,P​(0)), then every minimizer is nonzero, for every λ>0\lambda > 0λ>0.

Significance

The representer theorem is the single fact that turns kernel-based learning from a theoretical curiosity into a practical algorithm family: every popular SVM solver (SMO, coordinate descent, interior-point methods for the dual) is, at bottom, a method for finding the nnn coefficients α1,…,αn\alpha_1,\dots,\alpha_nα1​,…,αn​ the theorem guarantees exist, not for searching HHH directly. The representation also underlies the "kernel trick": since the objective and the solution both depend on HHH only through inner products ⟨k(⋅,xi),k(⋅,xj)⟩H=k(xi,xj)\langle k(\cdot,x_i), k(\cdot,x_j)\rangle_H = k(x_i,x_j)⟨k(⋅,xi​),k(⋅,xj​)⟩H​=k(xi​,xj​), an SVM can be trained and evaluated without ever computing with elements of HHH explicitly, using only the n×nn \times nn×n Gram matrix of kernel values.

Formalizing this theorem means formalizing the existence-and-uniqueness argument (Lemma 5.1's strict-convexity computation for the midpoint of two hypothetical minimizers, together with the weak-compactness argument used for existence) and the orthogonal-projection argument for the representation clause (projecting any candidate minimizer onto the finite-dimensional span of the kernel functions at the sample points strictly improves — or leaves unchanged — both the norm term and the risk term, so an optimal solution can always be chosen inside that span). No part of this argument has a machine-checked Lean proof in Mathlib or elsewhere at the time of writing; only the underlying general-purpose tools (Hilbert-space projections, convexity of norms) are already in Mathlib.

Difficulty

The natural first idea for the representation clause is to try to exhibit the coefficients αi\alpha_iαi​ directly, e.g. by writing down the dual optimization problem and reading off its KKT multipliers. This is exactly backwards: the book's proof (and any faithful one) derives the representation before knowing anything about a dual problem, purely from the orthogonal decomposition H=H∣X′⊕H∣X′⊥H = H|_{X'} \oplus H|_{X'}^\perpH=H∣X′​⊕H∣X′⊥​ of HHH into the span H∣X′H|_{X'}H∣X′​ of the sample's kernel functions and its orthogonal complement. The key insight — one that a solver who reaches for duality first will miss — is that projecting any f∈Hf \in Hf∈H onto H∣X′H|_{X'}H∣X′​ leaves the empirical risk exactly unchanged (since RL,DR_{L,D}RL,D​ only sees fff's values at the sample points, and the reproducing property shows those values are unaffected by throwing away the H∣X′⊥H|_{X'}^\perpH∣X′⊥​ component) while weakly decreasing the norm term, so the infimum over all of HHH is already attained inside the finite-dimensional H∣X′H|_{X'}H∣X′​.

For the existence-and-uniqueness clause, the difficulty is genuinely functional-analytic rather than algorithmic: existence needs a compactness argument in a space with no compact balls (Theorem 5.2 gets around this via lower semicontinuity and boundedness of the sublevel set, not via any finite-dimensional trick), and uniqueness needs the parallelogram-law strict convexity of the Hilbert norm, not merely convexity of the loss.

Formalization scope

HHH is represented as an arbitrary real Hilbert space together with an injective linear evaluation map into X→RX \to \mathbb RX→R (so that HHH is genuinely realized as a space of functions, not an abstract Hilbert space with no relation to XXX), and a kernel kkk satisfying the reproducing property with respect to that evaluation map (IsRKHSOfKernel). This is an equivalent, operative rendering of "HHH is the RKHS of the kernel kkk" (Definition 4.18 together with Lemma 4.19 of the book), chosen because it is exactly the form the chapter's own proofs use; it is restated inside this chunk's own InfiniteSample sub-namespace rather than imported from the Kernels chapter's mission, since drafts in this series cannot import one another.

The population risk RL,PR_{L,P}RL,P​ is formalized as a lower Lebesgue integral into [0,∞][0,\infty][0,∞] (ENNReal), which is always well-defined for a nonnegative integrand with no integrability hypothesis — matching the book's own remark that "the integral always exists, although it is not necessarily finite." The empirical risk RL,DR_{L,D}RL,D​, by contrast, is a manifestly finite average over the nnn sample points and is formalized as an ordinary real number. The sample size nnn is required positive (n≥1n \ge 1n≥1), matching the book's implicit convention that the empirical measure Dˉ:=1n∑iδ(xi,yi)\bar D := \tfrac1n\sum_i \delta_{(x_i,y_i)}Dˉ:=n1​∑i​δ(xi​,yi​)​ presupposes a nonempty sample.

A trivializing formalization of the representer theorem would state only the representation clause fD,λ(x)=∑iαik(x,xi)f_{D,\lambda}(x) = \sum_i \alpha_i k(x,x_i)fD,λ​(x)=∑i​αi​k(x,xi​) while assuming the existence of "the" solution fD,λf_{D,\lambda}fD,λ​ as a hypothesis; this begs the question, since the book's own proof establishes existence and uniqueness as part of the theorem, not as a standing assumption. This mission's goal keeps both clauses bundled into one ∃! statement for exactly this reason.

The infrastructure needed — a general convex loss, a Nemitski-loss integrability condition, and the RKHS/reproducing-kernel bundle — is restated locally here and is reusable, with the same caveat about not being importable across this series' independently drafted chapters, by any later mission (e.g. this book's own Chapters 6, 8 and 9) that needs the same objects. Contributed proofs are welcome for either the existence/uniqueness argument (Lemma 5.1/Theorem 5.2's techniques) or the orthogonal-projection representation argument; the two are largely independent and could be solved separately.

Selected references

  • I. Steinwart and A. Christmann, Support Vector Machines, Springer Series in Information Science and Statistics, Springer, 2008. https://doi.org/10.1007/978-0-387-77242-4
  • G. Kimeldorf and G. Wahba, "Some results on Tchebycheffian spline functions," Journal of Mathematical Analysis and Applications, 33(1):82–95, 1971. https://doi.org/10.1016/0022-247X(71)90184-3
  • B. Schölkopf, R. Herbrich, and A. J. Smola, "A generalized representer theorem," in Computational Learning Theory (COLT 2001), Lecture Notes in Computer Science, vol. 2111, Springer, 2001, pp. 416–426. https://doi.org/10.1007/3-540-44581-1_27
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Operations ResearchProbabilityStatistics+1·Captain: mikedeng1

Stochastic Orders V: The Laplace Transform OrderTextbook

Comparing distributions by their Laplace transforms

Many of the orders in Shaked and Shanthikumar's Stochastic Orders (Springer, 2007) are built by fixing a class of test functions φ\varphiφ and declaring X≤YX \le YX≤Y whenever E[φ(X)]≤E[φ(Y)]E[\varphi(X)] \le E[\varphi(Y)]E[φ(X)]≤E[φ(Y)] for every φ\varphiφ in that class: all increasing functions give the usual stochastic order, all convex functions give the convex order. This mission formalizes the order obtained from the single function φs(x)=−e−sx\varphi_s(x) = -e^{-sx}φs​(x)=−e−sx, s>0s > 0s>0 — the Laplace transform order — together with its principal alternative characterization and three of its closure properties. Unlike almost every other order in the book, this one has essentially no dependence on material from earlier chapters, which is why it is a natural standalone mission.

The Laplace transform order

Let XXX be a real-valued random variable on a probability space (Ω,μ)(\Omega,\mu)(Ω,μ), and let YYY be a real-valued random variable on a (possibly different) probability space (Ω′,ν)(\Omega',\nu)(Ω′,ν). XXX is smaller than YYY in the Laplace transform order, written X≤LtYX \le_{Lt} YX≤Lt​Y, if

E[e−sX]≥E[e−sY]for every s>0.E[e^{-sX}] \ge E[e^{-sY}] \quad \text{for every } s > 0.E[e−sX]≥E[e−sY]for every s>0.

The order is meant for nonnegative random variables: the book's own standing convention for the whole of §5.A is that every random variable mentioned is nonnegative, since otherwise E[e−sX]E[e^{-sX}]E[e−sX] need not even be finite. Every theorem below carries that hypothesis explicitly rather than folding it into the order's own definition, so the definition itself is stated exactly as broadly as the book's raw equation (5.A.1) is — a comparison of two expectations, for two random variables that need not share a probability space, since ≤Lt\le_{Lt}≤Lt​ is a comparison of distributions.

A second definition supports one of the milestones: a function φ:[0,∞)→R\varphi : [0,\infty) \to \mathbb{R}φ:[0,∞)→R is completely monotone if all its derivatives exist and (−1)nφ(n)(x)≥0(-1)^n\varphi^{(n)}(x) \ge 0(−1)nφ(n)(x)≥0 for every x>0x > 0x>0 and every n=0,1,2,…n = 0, 1, 2, \dotsn=0,1,2,…. Every φs(x)=e−sx\varphi_s(x) = e^{-sx}φs​(x)=e−sx, s>0s > 0s>0, is completely monotone, which is what connects the raw definition of ≤Lt\le_{Lt}≤Lt​ to its function-class characterization below.

Formalization targets

Goal: the integrated-survival-function characterization (Theorem 5.A.1)

X≤LtY  ⟺  ∫0∞e−sxFˉ(x) dx≤∫0∞e−sxGˉ(x) dxfor every s>0,X \le_{Lt} Y \iff \int_0^\infty e^{-sx}\bar F(x)\,dx \le \int_0^\infty e^{-sx}\bar G(x)\,dx \quad \text{for every } s > 0,X≤Lt​Y⟺∫0∞​e−sxFˉ(x)dx≤∫0∞​e−sxGˉ(x)dxfor every s>0,

where Fˉ(x)=P{X>x}\bar F(x) = P\{X>x\}Fˉ(x)=P{X>x} and Gˉ(x)=P{Y>x}\bar G(x) = P\{Y>x\}Gˉ(x)=P{Y>x} are the survival functions of XXX and YYY. This is the book's principal restatement of the order, obtained from the identity ∫0∞e−sxFˉ(x) dx=s−1(1−E[e−sX])\int_0^\infty e^{-sx}\bar F(x)\,dx = s^{-1}(1-E[e^{-sX}])∫0∞​e−sxFˉ(x)dx=s−1(1−E[e−sX]): instead of comparing the raw Laplace transforms of XXX and YYY themselves, it compares the Laplace transforms of their survival functions, weighted the same way. It is the natural goal for a standalone chapter mission: the chapter's own defining equation plus one elementary identity is exactly the book's own proof, and it is the form of the order that the chapter's closure properties are stated against.

Supporting milestones

  • Eq. (5.A.5), the mean inequality: X≤LtY  ⟹  E[X]≤E[Y]X \le_{Lt} Y \implies E[X] \le E[Y]X≤Lt​Y⟹E[X]≤E[Y], provided the expectations exist — obtained by dividing the defining inequality by sss and letting s↓0s \downarrow 0s↓0.
  • Theorem 5.A.3, the function-class characterization: X≤LtYX \le_{Lt} YX≤Lt​Y iff E[φ(X)]≥E[φ(Y)]E[\varphi(X)] \ge E[\varphi(Y)]E[φ(X)]≥E[φ(Y)] for every completely monotone φ\varphiφ, provided the expectations exist — the order's analogue of "all increasing functions" for ≤st\le_{st}≤st​ or "all convex functions" for ≤cx\le_{cx}≤cx​.
  • Theorem 5.A.7(a), closure under functions with a completely monotone derivative: X≤LtYX \le_{Lt} YX≤Lt​Y and ggg positive with g′g'g′ completely monotone gives g(X)≤Ltg(Y)g(X) \le_{Lt} g(Y)g(X)≤Lt​g(Y).
  • Theorem 5.A.7(d), the convolution corollary: independent Xi≤LtYiX_i \le_{Lt} Y_iXi​≤Lt​Yi​, i=1,…,mi=1,\dots,mi=1,…,m, gives ∑iXi≤Lt∑iYi\sum_i X_i \le_{Lt} \sum_i Y_i∑i​Xi​≤Lt​∑i​Yi​.

Significance

The Laplace transform order is the natural comparison for nonnegative quantities that arise as sums or mixtures of exponential-type random variables — waiting times, workloads, service completion times — precisely because it is preserved under convolution (Theorem 5.A.7(d)) and under the broad class of transformations with a completely monotone derivative (Theorem 5.A.7(a)), which includes every concave power xpx^pxp, 0<p≤10<p\le 10<p≤1. It sits strictly between the convex-type orders and weaker moment comparisons: Eq. (5.A.5) shows it implies ordered means, but (unlike ≤cx\le_{cx}≤cx​) it does not require equal means, and (unlike ≤icx\le_{icx}≤icx​) it is not implied by a pointwise comparison of integrated tails alone — it is its own, genuinely different order, useful whenever a modeler's comparison naturally arises through Laplace-transform (equivalently, moment-generating-function-at- negative-argument) calculations rather than through a coupling or a tail-probability argument. Theorem 5.A.3's function-class form is the bridge that lets the order be verified either way: by a single-parameter family of exponential test functions, or by the full class of completely monotone functions of which they are the extreme rays.

Difficulty

The chapter's own first warning applies directly: the order's every characterization requires X,Y≥0X,Y \ge 0X,Y≥0, and dropping that hypothesis anywhere — as opposed to carrying it explicitly on each theorem, per this mission's convention — would silently change which statements are even well-posed, since E[e−sX]E[e^{-sX}]E[e−sX] can diverge for XXX unbounded below. The quantifier "∀s>0\forall s > 0∀s>0" in both the raw definition and Theorem 5.A.1 ranges over the whole positive half-line, not a bounded or discretized set of test points; narrowing it would produce a strictly weaker order. In CompletelyMonotone, the phrase "all its derivatives exist" is a genuine hypothesis, not a formality: stating only the sign condition on iteratedDeriv n φ x without also requiring φ to be C^∞ would let the definition be satisfied vacuously wherever a derivative fails to exist (a classic junk-value trap), which is why the mission's definition bundles smoothness explicitly. Theorem 5.A.7(a)'s "ggg positive" is a hypothesis on ggg's values at the nonnegative reals that XXX and YYY actually take, not on all of R\mathbb{R}R, and must not be silently strengthened to "ggg everywhere positive" or weakened to "ggg nonnegative" (which would let ggg vanish and break the order's need for e−sg(X)e^{-sg(X)}e−sg(X) to be well-behaved).

Formalization scope

LaplaceOrder μ ν X Y takes X:Ω→RX : \Omega \to \mathbb{R}X:Ω→R on (Ω,μ)(\Omega,\mu)(Ω,μ) and Y:Ω′→RY : \Omega' \to \mathbb{R}Y:Ω′→R on a separate (Ω′,ν)(\Omega',\nu)(Ω′,ν), matching the series' convention (e.g. StochasticOrders.Usual.UsualOrder) that the order compares distributions, not jointly defined variables. Nonnegativity of XXX and YYY is an explicit hypothesis ∀ ω, 0 ≤ X ω / ∀ ω, 0 ≤ Y ω on every theorem, never built into LaplaceOrder itself. CompletelyMonotone φ is ContDiff ℝ ⊤ φ ∧ ∀ n x, 0 < x → 0 ≤ (-1)^n * iteratedDeriv n φ x — the smoothness conjunct guards the junk-value trap described above. The survival function Fˉ(x)=P{X>x}\bar F(x) = P\{X>x\}Fˉ(x)=P{X>x} in the goal theorem is formalized inline as (μ {ω | x < X ω}).toReal, valid since μ is a probability measure (so the underlying ENNReal value is finite and the conversion to ℝ loses no information); the integral ∫0∞\int_0^\infty∫0∞​ is Bochner integration over Set.Ici (0 : ℝ). "Provided the expectations exist" becomes explicit Integrable hypotheses per statement (on XXX, YYY themselves for Eq. 5.A.5; on φ∘X\varphi \circ Xφ∘X, φ∘Y\varphi \circ Yφ∘Y for each φ\varphiφ in Theorem 5.A.3), rather than a blanket integrability assumption that would understate which expectations the book actually needs. Independence in the convolution corollary is ProbabilityTheory.iIndepFun, one family per side, as in Chunk 01's own convolution corollary. A trivializing formalization is ruled out: ≤Lt\le_{Lt}≤Lt​ is not restated as a comparison of one moment or of the raw random variables' means, and the "universal function class" of Theorem 5.A.3 is exactly the completely monotone functions the book names, not a fixed finite subfamily or a narrowed subclass (e.g. only the exponentials themselves, which would make Theorem 5.A.3 a restatement of the definition rather than its own theorem).

This mission draws on no platform prior art: repeated searches for "Laplace transform" and "completely monotone" during this session return only unrelated analytic-number-theory formalizations (a Langlands–Tunnell Laplace–Mellin transform identity) and no hits at all, respectively — confirming BRIEF.md's expectation that this subarea is untouched on the platform. It is one of nine missions in a series covering the whole book; per the series' own convention, its definitions are not imported by any other chapter's mission, and it does not import any other chapter's definitions in turn (the chapter itself has essentially no cross-chapter dependence, the reason it was flagged as the series' most self-contained chunk).

Selected references

  • M. Shaked and J. G. Shanthikumar, Stochastic Orders, Springer Series in Statistics, Springer, 2007. https://doi.org/10.1007/978-0-387-34675-5
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