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Machine LearningOperations ResearchOptimization·Captain: mikedeng1

Wasserstein Distributionally Robust Optimization I: Kantorovich Duality and Strong Duality for the Worst-Case RiskTextbook

Motivation

Every data-driven decision problem faces the same trap. A decision-maker estimates a risk functional R(P,ℓ)=EP[ℓ(ξ)]R(P,\ell) = \mathbb{E}_P[\ell(\xi)]R(P,ℓ)=EP​[ℓ(ξ)] from a nominal distribution P^N\hat P_NP^N​ built from NNN training samples, then optimizes a loss function ℓ\ellℓ against P^N\hat P_NP^N​ instead of the unknown true distribution PPP. Because the optimizer adapts to the noise in P^N\hat P_NP^N​, the in-sample risk of the optimizer systematically understates its true, out-of-sample risk — a phenomenon Smith and Winkler named the optimizer's curse (Smith & Winkler, Management Science, 2006). The remedy explored here is to hedge against a whole neighborhood of plausible distributions around P^N\hat P_NP^N​, rather than trusting the point estimate. Kuhn, Mohajerin Esfahani, Nguyen and Shafieezadeh-Abadeh's INFORMS TutORials chapter (2019) develops this neighborhood using the Wasserstein distance, and the present mission formalizes its foundational duality theory: the machinery every later result in the chapter (finite-sample guarantees, elliptical tractability, regularization) builds on.

Setting

Fix a norm ∥⋅∥\|\cdot\|∥⋅∥ on a finite-dimensional real vector space EEE (representing Rm\mathbb{R}^mRm). For p∈[1,∞)p \in [1,\infty)p∈[1,∞), the type-ppp Wasserstein distance between two Borel probability measures Q,Q′Q, Q'Q,Q′ on EEE is

Wp(Q,Q′)=(inf⁡π∈Π(Q,Q′)∫E×E∥ξ−ξ′∥p π(dξ,dξ′))1/p,W_p(Q,Q') = \left(\inf_{\pi \in \Pi(Q,Q')} \int_{E\times E} \|\xi-\xi'\|^p\, \pi(d\xi,d\xi')\right)^{1/p},Wp​(Q,Q′)=(π∈Π(Q,Q′)inf​∫E×E​∥ξ−ξ′∥pπ(dξ,dξ′))1/p,

where Π(Q,Q′)\Pi(Q,Q')Π(Q,Q′) is the set of couplings of QQQ and Q′Q'Q′ — joint probability measures on E×EE \times EE×E whose marginals are QQQ and Q′Q'Q′. The optimal π\piπ can be read as a transportation plan moving one pile of dirt (QQQ) into another (Q′Q'Q′) at minimum cost, which is why WpW_pWp​ is also called the earth mover's distance; the underlying linear program was formalized by Kantorovich (1942) after Monge's 1781 original.

Given NNN training samples ξ^1,…,ξ^N\hat\xi_1,\dots,\hat\xi_Nξ^​1​,…,ξ^​N​, the empirical distribution is P^N=1N∑i=1Nδξ^i\hat P_N = \frac1N\sum_{i=1}^N \delta_{\hat\xi_i}P^N​=N1​∑i=1N​δξ^​i​​. Centered at P^N\hat P_NP^N​, the Wasserstein ambiguity set of radius ε≥0\varepsilon \ge 0ε≥0 is

Bε,p(P^N)={Q∈P(Ξ):Wp(Q,P^N)≤ε},B_{\varepsilon,p}(\hat P_N) = \{Q \in \mathcal{P}(\Xi) : W_p(Q,\hat P_N) \le \varepsilon\},Bε,p​(P^N​)={Q∈P(Ξ):Wp​(Q,P^N​)≤ε},

where Ξ⊆E\Xi \subseteq EΞ⊆E is a closed set known to contain the support of the true distribution. The worst-case risk of a loss function ℓ\ellℓ 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)} \mathbb{E}_Q[\ell(\xi)],Rε,p​(P^N​,ℓ)=Q∈Bε,p​(P^N​)sup​EQ​[ℓ(ξ)],

and minimizing it over a class of admissible loss functions L\mathcal{L}L is a distributionally robust optimization problem. ε\varepsilonε measures the estimation error one insures against; a larger ambiguity set gives a more conservative (and more expensive) guarantee.

Formalization targets

Goal — Theorem 7, strong duality

Rε,p(P^N,ℓ)=inf⁡γ≥0 EP^N[ℓγ(ξ)]+γεp,ℓγ(ξ)=sup⁡z∈Ξℓ(z)−γ∥z−ξ∥p.R_{\varepsilon,p}(\hat P_N,\ell) = \inf_{\gamma \ge 0}\ \mathbb{E}_{\hat P_N}[\ell_\gamma(\xi)] + \gamma\varepsilon^p,\qquad \ell_\gamma(\xi) = \sup_{z\in\Xi} \ell(z) - \gamma\|z-\xi\|^p.Rε,p​(P^N​,ℓ)=γ≥0inf​ EP^N​​[ℓγ​(ξ)]+γεp,ℓγ​(ξ)=z∈Ξsup​ℓ(z)−γ∥z−ξ∥p.

This is the Lagrangian dual of the worst-case risk evaluation problem, with γ\gammaγ the multiplier of the Wasserstein constraint Wp(Q,P^N)≤εW_p(Q,\hat P_N)\le\varepsilonWp​(Q,P^N​)≤ε: it converts a supremum over an infinite-dimensional space of measures into a one-dimensional minimization of the Moreau-Yosida regularization ℓγ\ell_\gammaℓγ​. Every tractability result later in the chapter (finite convex reformulations, SDP relaxations) specializes this duality by choosing a loss class for which ℓγ\ell_\gammaℓγ​ is computable.

Supporting dual representations of WpW_pWp​ — Theorems 1 and 2

Wpp(Q,Q′)=sup⁡{∫ψ dQ′−∫φ dQ:φ,ψ bounded continuous, ψ(ξ)−φ(ξ′)≤∥ξ−ξ′∥p}W_p^p(Q,Q') = \sup\left\{\int \psi\,dQ' - \int \varphi\,dQ : \varphi,\psi \text{ bounded continuous},\ \psi(\xi)-\varphi(\xi') \le \|\xi-\xi'\|^p\right\}Wpp​(Q,Q′)=sup{∫ψdQ′−∫φdQ:φ,ψ bounded continuous, ψ(ξ)−φ(ξ′)≤∥ξ−ξ′∥p} W1(Q,Q′)=sup⁡Lip(φ)≤1∫φ dQ−∫φ dQ′W_1(Q,Q') = \sup_{\mathrm{Lip}(\varphi)\le 1} \int \varphi\,dQ - \int \varphi\,dQ'W1​(Q,Q′)=Lip(φ)≤1sup​∫φdQ−∫φdQ′

These identify WpW_pWp​ as a linear program's strong dual (Theorem 1) and, for p=1p=1p=1, specialize it to the Kantorovich-Rubinstein form (Theorem 2), which is what lets the worst-case-risk analysis reason about Lipschitz loss functions directly.

Upper and lower bounds — Theorems 5 and 6

Rε,p(P^N,ℓ)≤R(P^N,ℓ)+ε⋅Lip(ℓ)R_{\varepsilon,p}(\hat P_N,\ell) \le R(\hat P_N,\ell) + \varepsilon\cdot\mathrm{Lip}(\ell)Rε,p​(P^N​,ℓ)≤R(P^N​,ℓ)+ε⋅Lip(ℓ) Rε,p(P^N,ℓ)≥sup⁡{1N∑iℓ(ξ^i+θi):ξ^i+θi∈Ξ, 1N∑i∥θi∥p≤εp}R_{\varepsilon,p}(\hat P_N,\ell) \ge \sup\left\{\tfrac1N\textstyle\sum_i \ell(\hat\xi_i+\theta_i) : \hat\xi_i+\theta_i\in\Xi,\ \tfrac1N\textstyle\sum_i\|\theta_i\|^p\le\varepsilon^p\right\}Rε,p​(P^N​,ℓ)≥sup{N1​∑i​ℓ(ξ^​i​+θi​):ξ^​i​+θi​∈Ξ, N1​∑i​∥θi​∥p≤εp}

These are the tractable, easily-computed bracket that Theorems 7 and 10 later show is tight in important special cases.

Exact case — Theorem 10

Ξ=Rm, ℓ convex, p=1  ⟹  Rε,1(P^N,ℓ)=R(P^N,ℓ)+ε Lip(ℓ)\Xi = \mathbb{R}^m,\ \ell \text{ convex},\ p=1 \implies R_{\varepsilon,1}(\hat P_N,\ell) = R(\hat P_N,\ell) + \varepsilon\,\mathrm{Lip}(\ell)Ξ=Rm, ℓ convex, p=1⟹Rε,1​(P^N​,ℓ)=R(P^N​,ℓ)+εLip(ℓ)

Theorem 5's inequality becomes exact under convexity — the cleanest closing corollary of the duality theory, obtained from Theorem 7 by evaluating the Moreau-Yosida regularization of a convex function explicitly.

Significance

Theorem 7 is the hinge on which the entire computational program of Wasserstein distributionally robust optimization turns: every tractable reformulation in the source chapter (piecewise-concave losses via conic duality, quadratic losses via semidefinite programming, the shrinkage-estimator connection) is obtained by substituting a specific loss class into the right-hand side of Theorem 7 and showing the resulting Moreau-Yosida regularization is computable. Kuhn et al. themselves derive it as a corollary of Blanchet & Murthy (2019) and Gao & Kleywegt (2016) for the empirical case, generalized to Polish spaces by Blanchet & Murthy and Gao & Kleywegt independently — the paper cites [12] and [37] for the general statement. Formalizing it is what makes every later, more computational result in the chapter — the ones a solver is more likely to reach for next — rest on a mechanically verified foundation rather than a citation chain.

Status. The mathematical result is well established (multiple independent published proofs cited above); nothing here is open research. What this mission contributes is the first machine-checked formal statement of the duality theorem and its supporting dual representations (Theorems 1, 2, 5, 6, 10) on the Prove2Me platform — none of Wp's dual representation, the Wasserstein ambiguity set, or the worst-case risk functional exist there prior to this mission (see Formalization scope).

Difficulty

The obvious proof strategy — write down the Lagrangian of the semi-infinite program (6), swap the order of the outer supremum over QQQ and the inner minimization over the multiplier γ\gammaγ, and invoke ordinary Lagrangian strong duality — fails because (6) is an infinite- dimensional linear program over measures, not a finite convex program: there is no compact feasible set or Slater point in a form that ordinary finite-dimensional duality applies to directly. The actual proof goes through the dual representation of the Wasserstein distance itself (Theorem 1, which is why it is a prerequisite milestone), reformulating the constraint Wp(Q,P^N)≤εW_p(Q,\hat P_N)\le\varepsilonWp​(Q,P^N​)≤ε via its own dual variables and swapping the resulting sup-inf using minimax theorems for semi-infinite programs, not ordinary Lagrangian duality for finite programs.

Formalization scope

EEE is a generic finite-dimensional real normed space (NormedAddCommGroup, NormedSpace ℝ, Borel-measurable), representing Rm\mathbb{R}^mRm with the paper's arbitrary fixed norm as a parameter rather than fixing the Euclidean norm. A coupling is formalized directly via MeasureTheory.Measure.map: π.map Prod.fst = Q ∧ π.map Prod.snd = Q'. Constrained infima/suprema (over couplings, over the ambiguity set, over Lipschitz test functions, over perturbation matrices) use Mathlib's guarded-binder idiom ⨅ x (_ : P x), f x, which correctly returns ⊤\top⊤ (resp. ⊥\bot⊥) outside the feasible set rather than a finite junk value.

Two deliberate, disclosed conventions keep the extremal-value definitions faithful without extended-real integration machinery, both recorded in MODERATION_NOTES.md:

  1. worstCaseRisk and the dual representations (Theorems 1, 2) are valued in EReal, not ℝ, so an unbounded supremum is recorded as +∞+\infty+∞ rather than collapsed to Mathlib's real-valued junk value 0 on an unbounded family.
  2. The goal theorem (7) and its Moreau-Yosida regularization restrict the loss function to bounded continuous ℓ\ellℓ (BoundedContinuousFunction E ℝ), narrower than the paper's general upper-semicontinuous, P^N\hat P_NP^N​-integrable loss class L\mathcal{L}L (Assumption 1). This keeps ℓγ(ξ)=sup⁡z∈Ξℓ(z)−γ∥z−ξ∥p\ell_\gamma(\xi) = \sup_{z\in\Xi}\ell(z)-\gamma\|z-\xi\|^pℓγ​(ξ)=supz∈Ξ​ℓ(z)−γ∥z−ξ∥p a finite real number for every nonempty Ξ\XiΞ, so the right-hand side's Bochner integral is well-posed; the milestones (Theorems 5, 6, 10) keep the more general real-valued (not necessarily bounded) loss class, since their statements do not require evaluating a pointwise supremum over Ξ\XiΞ.
  3. Ξ is required closed in Theorems 5, 6 and 7, matching the paper's own standing assumption (p. 6: "we let Ξ⊆Rm\Xi\subseteq\mathbb{R}^mΞ⊆Rm be a closed set that is known to contain the support of PPP") for the whole worst-case-risk framework, which is used silently in the paper wherever a theorem takes Ξ\XiΞ as an argument but was not carried into these theorems' own hypothesis lists in an earlier draft.
  4. The goal theorem (7) additionally requires P^N\hat P_NP^N​ itself supported on Ξ\XiΞ (P^N(Ξc)=0\hat P_N(\Xi^c)=0P^N​(Ξc)=0, the same "supported on Ξ\XiΞ" convention ambiguitySet uses for Q∈P(Ξ)Q\in\mathcal P(\Xi)Q∈P(Ξ)), which the paper's framework presupposes for the nominal distribution throughout §2. Combined with ℓ\ellℓ bounded, this makes ℓγ\ell_\gammaℓγ​ bounded on the full-measure set Ξ\XiΞ (above by sup⁡ℓ\sup\ellsupℓ unconditionally, below by ℓ(ξ)\ell(\xi)ℓ(ξ) itself via z=ξz=\xiz=ξ for ξ∈Ξ\xi\in\Xiξ∈Ξ), which is what makes the right-hand side's integral genuinely well-posed rather than liable to Mathlib's non-integrable junk value 000.

There is no trivializing formalization risk from a vacuous hypothesis: Ξ.Nonempty and 0 < N are both required exactly where the paper's own indexing and support assumptions require them, and every extremal value uses the extended-real convention above rather than a convention that would make an inequality vacuously true.

No definition in this mission exists on the platform prior to this series (GET /theorems?q=Wasserstein, q=Kantorovich, q=optimal transport, q=coupling return only unrelated discrete/finite-type constructions); all seven definitions and six theorems are drafted fresh. WassersteinDRO.Duality.wassersteinDistance, .ambiguitySet and .worstCaseRisk are the substrate every later mission in this five-part series (Gelbrich tractability, finite-sample guarantees, regularization, shrinkage estimation) either imports directly or redefines locally per the series' reuse rule.

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, 130–166. https://doi.org/10.1287/educ.2019.0198
  • Villani, C. (2009). Optimal Transport: Old and New. Springer. (Cited as [108] for Theorems 1 and 2.)
  • Smith, J. E., & Winkler, R. L. (2006). The optimizer's curse: Skepticism and postdecision surprise in decision analysis. Management Science, 52(3), 311–322. https://doi.org/10.1287/mnsc.1050.0451
  • Gao, R., & Kleywegt, A. J. (2016). Distributionally Robust Stochastic Optimization with Wasserstein Distance. arXiv:1604.02199.
  • Blanchet, J., & Murthy, K. (2019). Quantifying Distributional Model Risk via Optimal Transport. Mathematics of Operations Research, 44(2), 565–600. https://doi.org/10.1287/moor.2018.0936
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Machine LearningStatistics·Captain: mikedeng1

High-Dimensional Statistics II: Talagrand's Convex Concentration InequalityTextbook

Motivation

Chapter 2's tail bounds mostly rest on moment-generating-function control, obtained either directly (sub-Gaussianity) or through explicit combinatorial arguments (Hoeffding, bounded differences). The entropic method offers a different, more structural route: bound a specific information-theoretic quantity — the φ\varphiφ-entropy of eλXe^{\lambda X}eλX — and convert that bound mechanically into a tail bound via a short ODE argument (the Herbst argument). This method's real payoff appears once it is combined with the tensorization property of entropy across independent coordinates, which is what lets it handle Lipschitz functions of many independent variables — including cases, such as separately convex functions, that elude the purely martingale-based techniques of Chapter 2. This mission formalizes the entropic method's two foundational entropy-to-tail conversions and its central Lipschitz-concentration application, following Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 3.

Setting

For φ(u):=ulog⁡u\varphi(u):=u\log uφ(u):=ulogu (u>0u>0u>0), φ(0):=0\varphi(0):=0φ(0):=0, the φ\varphiφ-entropy of a nonnegative random variable ZZZ is H(Z):=E[Zlog⁡Z]−E[Z]log⁡E[Z]H(Z):=\mathbb E[Z\log Z]-\mathbb E[Z]\log\mathbb E[Z]H(Z):=E[ZlogZ]−E[Z]logE[Z] (Eqs. (3.1)-(3.2)). Writing φX(λ):=E[eλX]\varphi_X(\lambda):=\mathbb E[e^{\lambda X}]φX​(λ):=E[eλX] for the moment generating function of XXX, the entropy of eλXe^{\lambda X}eλX has the explicit form H(eλX)=λφX′(λ)−φX(λ)log⁡φX(λ)H(e^{\lambda X}) = \lambda\varphi_X'(\lambda) -\varphi_X(\lambda)\log\varphi_X(\lambda)H(eλX)=λφX′​(λ)−φX​(λ)logφX​(λ) (Eq. (3.3)).

A function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R is separately convex if, for each coordinate kkk, the univariate function obtained by fixing every coordinate but the kkk-th is convex — strictly weaker than joint convexity of fff itself. fff is LLL-Lipschitz with respect to the Euclidean norm if ∣f(x)−f(x′)∣≤L∥x−x′∥2|f(x)-f(x')|\le L\|x-x'\|_2∣f(x)−f(x′)∣≤L∥x−x′∥2​ for all x,x′x,x'x,x′.

Formalization targets

Goal — Theorem 3.4 (separately convex Lipschitz concentration)

Let {Xi}i=1n\{X_i\}_{i=1}^n{Xi​}i=1n​ be independent, each supported on [a,b][a,b][a,b], and fff separately convex and LLL-Lipschitz. Then for all δ>0\delta>0δ>0,

P[f(X)≥E[f(X)]+δ]  ≤  exp⁡(−δ24L2(b−a)2).\mathbb P[f(X)\ge\mathbb E[f(X)]+\delta] \;\le\; \exp\Big(-\frac{\delta^2}{4L^2(b-a)^2}\Big).P[f(X)≥E[f(X)]+δ]≤exp(−4L2(b−a)2δ2​).

Milestone — Proposition 3.2 (the Herbst argument)

If H(eλX)≤12σ2λ2φX(λ)H(e^{\lambda X})\le\tfrac12\sigma^2\lambda^2\varphi_X(\lambda)H(eλX)≤21​σ2λ2φX​(λ) for all λ∈I\lambda\in Iλ∈I (I=[0,∞)I=[0,\infty)I=[0,∞) or R\mathbb RR), then log⁡E[eλ(X−E[X])]≤12λ2σ2\log\mathbb E[e^{\lambda(X-\mathbb E[X])}]\le \tfrac12\lambda^2\sigma^2logE[eλ(X−E[X])]≤21​λ2σ2 for all λ∈I\lambda\in Iλ∈I — the basic entropy-to-sub-Gaussian-tail conversion.

Milestone — Proposition 3.3 (the Bernstein entropy bound)

The sub-exponential analogue: if H(eλX)≤λ2{bφX′(λ)+φX(λ)(σ2−bE[X])}H(e^{\lambda X})\le\lambda^2\{b\varphi_X'(\lambda)+ \varphi_X(\lambda)(\sigma^2-b\mathbb E[X])\}H(eλX)≤λ2{bφX′​(λ)+φX​(λ)(σ2−bE[X])} for λ∈[0,1/b)\lambda\in[0,1/b)λ∈[0,1/b), then log⁡E[eλ(X−E[X])]≤σ2λ2(1−bλ)−1\log\mathbb E[e^{\lambda(X-\mathbb E[X])}]\le\sigma^2\lambda^2(1-b\lambda)^{-1}logE[eλ(X−E[X])]≤σ2λ2(1−bλ)−1 on the same range.

Significance

Propositions 3.2 and 3.3 are the two basic entropy-to-tail conversions the entire chapter's entropic method rests on — every subsequent Lipschitz-concentration result in the chapter (including Theorem 3.4 and the more advanced Theorem 3.24) is obtained by first establishing an entropy bound of one of these two forms and then invoking the corresponding proposition. Theorem 3.4 is itself the direct analogue, for independent bounded variables, of Chapter 2's Gaussian Lipschitz concentration (Theorem 2.26) — but crucially requires the extra hypothesis of separate convexity, which the Gaussian case does not need and which cannot be dropped in general.

Formalizing it. No faithful prior art exists on the platform. The one candidate flagged in BRIEF.md, Talagrand.lipschitz_concentration, was read in full: it is a weighted-Hamming- distance concentration bound for functions on a finite-alphabet product space Fin n → α, proved via Talagrand's convex-distance method — a different underlying space (finite alphabet vs. real-valued bounded coordinates) and a different Lipschitz norm (weighted Hamming vs. Euclidean) from Theorem 3.4, and not reused here. A search for "log-Sobolev" and "Herbst" turned up bousquet_herbst_cgf_le_phi_via_herbst/bousquet_herbst_cgf_le_phi_double_integration: these are abstract calculus lemmas about a generic function GGG satisfying an ODE-type growth condition (G′′≤vexG''\le ve^xG′′≤vex), concluding G(L)≤v(eL−1−L)G(L)\le v(e^L-1-L)G(L)≤v(eL−1−L) — a genuinely different statement shape from Proposition 3.2/3.3's entropy-to-CGF conversions (which conclude a quadratic, not exponential, bound on log⁡E[eλ(X−EX)]\log\mathbb E[e^{\lambda(X-\mathbb EX)}]logE[eλ(X−EX)]), and not a faithful match. All three theorems here are drafted as open goals (:= by sorry).

Difficulty

The naive approach to Theorem 3.4 — try to adapt the bounded-differences (martingale) method of Chapter 2 directly — fails, because the bounded-differences method needs fff to have small coordinatewise oscillation in an absolute sense, while separate convexity alone gives no such uniform bound (a separately convex function can vary arbitrarily fast within the interior of its domain, only its slope is controlled by the Lipschitz condition). The entropic method sidesteps this by working with the φ\varphiφ-entropy of eλf(X)e^{\lambda f(X)}eλf(X) directly: entropy has a tensorization property across independent coordinates (not itself part of this mission, but what the entropic method's proof of Theorem 3.4 uses) that reduces a multivariate entropy bound to a sum of "one coordinate at a time" contributions, each of which convexity and the Lipschitz condition jointly control — a route with no analogue in the bounded-differences approach.

Formalization scope

Separate convexity and Euclidean-Lipschitzness are both restated locally in this chapter's own sub-namespace (HighDimStat.Concentration), per this book series' rule against importing another chapter's draft definitions, even though Chapter 2 already defines an IsLLipschitz for the same Euclidean condition. φ_X'(\lambda)$ (Proposition 3.3) is realized via Mathlib's deriv, a legitimate way to state a hypothesis on a derivative without separately proving differentiability, appropriate at the draft-statement stage. Explicit Integrable` hypotheses guard the Bochner integral's junk value on non-integrable functions throughout (trap 2), not literal in the book's own propositions but implied by what "the entropy H(eλX)H(e^{\lambda X})H(eλX) exists" (an explicit qualifier the book itself makes when introducing Eq. (3.2)) means.

Goal substitution, disclosed. BRIEF.md recommends Theorem 3.24 (the two-sided, jointly convex analogue) as the primary goal, but explicitly names Theorem 3.4 as a fallback "if 3.24's dependence on the unnumbered transportation-cost inequality (Eq. 3.73, attributed to Samson) proves too heavy to state faithfully in the time available." Theorem 3.24's proof route depends on Theorem 3.19 (a general "transportation cost implies concentration" result for an abstract metric measure space, itself needing a from-scratch formalization of the transportation-cost inequality (3.58) and the concentration function αP,(X,ρ)\alpha_{P,(\mathcal X,\rho)}αP,(X,ρ)​) plus the unproven-in-chapter Eq. (3.73). Building this full stack faithfully was judged to exceed this chunk's time budget; Theorem 3.4 is drafted instead, using this mission's own budget on Propositions 3.2 and 3.3 (the two most load-bearing entropy-to-tail conversions of the chapter) rather than the heavier transportation-cost machinery. Theorem 3.19, Theorem 3.24, and Eq. (3.73) are all out of scope for this mission and named here as natural follow-on work.

Selected references

  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019. DOI: 10.1017/9781108627771. Chapter 3.
  • M. Ledoux, The Concentration of Measure Phenomenon, American Mathematical Society, 2001.
  • I. Herbst, unpublished (the argument bearing his name is attributed in Ledoux (2001) and standard references on log-Sobolev inequalities).
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Machine LearningStatistics·Captain: mikedeng1

High-Dimensional Statistics IX: Nuclear-Norm Regularization for Low-Rank Matrix RegressionTextbook

Motivation

Many estimation problems are naturally posed over matrices rather than vectors: recommender systems (Netflix-style matrix completion), multivariate regression with correlated responses, vector autoregressive time series, and phase retrieval all reduce to estimating an unknown matrix Θ∗\Theta^*Θ∗ that is low-rank, or well approximated by one. A rank constraint alone makes the natural least-squares estimator non-convex and generally intractable; replacing it with the nuclear norm — the sum of the matrix's singular values, the tightest convex surrogate for rank — yields a tractable semidefinite program. Wainwright's High-Dimensional Statistics (2019), Chapter 10, shows that this substitution costs nothing statistically: nuclear-norm-regularized least squares achieves error rates matching what one could hope for even knowing the rank in advance, by specializing Chapter 9's general decomposable-regularizer framework (mission 09-decomposability) directly to the nuclear norm.

Setting

For matrices A,B∈Rd1×d2A,B\in\mathbb R^{d_1\times d_2}A,B∈Rd1​×d2​, the trace inner product is ⟨ ⁣⟨A,B⟩ ⁣⟩:=trace(ATB)=∑j1,j2Aj1j2Bj1j2\langle\!\langle A,B\rangle\!\rangle := \mathrm{trace}(A^TB) = \sum_{j_1,j_2}A_{j_1j_2}B_{j_1j_2}⟨⟨A,B⟩⟩:=trace(ATB)=∑j1​,j2​​Aj1​j2​​Bj1​j2​​ (Eq. 10.1), inducing the Frobenius norm ∥ ⁣∣A∣ ⁣∥F\|\!|A|\!\|_F∥∣A∣∥F​. Given design matrices X1,…,Xn∈Rd1×d2X_1,\dots,X_n\in\mathbb R^{d_1\times d_2}X1​,…,Xn​∈Rd1​×d2​ and responses yi=⟨ ⁣⟨Xi,Θ∗⟩ ⁣⟩+wiy_i=\langle\!\langle X_i,\Theta^*\rangle\!\rangle+w_iyi​=⟨⟨Xi​,Θ∗⟩⟩+wi​, the observation operator Xn(Θ):=(⟨ ⁣⟨Xi,Θ⟩ ⁣⟩)i=1n\mathcal X_n(\Theta):=(\langle\!\langle X_i,\Theta\rangle\!\rangle)_{i=1}^nXn​(Θ):=(⟨⟨Xi​,Θ⟩⟩)i=1n​ and its adjoint Xn∗(u):=∑iuiXi\mathcal X_n^*(u):=\sum_iu_iX_iXn∗​(u):=∑i​ui​Xi​ (Eqs. 10.2-10.3) are the matrix analogs of a vector design matrix and its transpose. The nuclear norm ∥ ⁣∣Θ∣ ⁣∥nuc:=∑jσj(Θ)\|\!|\Theta|\!\|_{\mathrm{nuc}}:=\sum_j\sigma_j(\Theta)∥∣Θ∣∥nuc​:=∑j​σj​(Θ) (Eq. 10.5) — the sum of singular values — is a decomposable regularizer (in the sense of Chapter 9) with respect to the subspace pair spanned by the top singular vectors of any target matrix, and its dual norm (Table 9.1) is the ℓ2\ell_2ℓ2​-operator (spectral) norm ∥ ⁣∣⋅∣ ⁣∥2\|\!|\cdot|\!\|_2∥∣⋅∣∥2​. The estimator under study is nuclear-norm-regularized least squares,

Θ^∈arg min⁡Θ∈Rd1×d2{12n∥y−Xn(Θ)∥22+λn∥ ⁣∣Θ∣ ⁣∥nuc}(10.16)\hat\Theta \in \operatorname*{arg\,min}_{\Theta\in\mathbb R^{d_1\times d_2}} \left\{ \frac{1}{2n}\|y-\mathcal X_n(\Theta)\|_2^2 + \lambda_n\|\!|\Theta|\!\|_{\mathrm{nuc}} \right\} \tag{10.16}Θ^∈Θ∈Rd1​×d2​argmin​{2n1​∥y−Xn​(Θ)∥22​+λn​∥∣Θ∣∥nuc​}(10.16)

with λn>0\lambda_n>0λn​>0 user-chosen.

Formalization targets

Goal (Proposition 10.6)

Suppose Xn\mathcal X_nXn​ satisfies the restricted strong convexity condition (10.17), ∥Xn(Δ)∥22/(2n)≥κ/2∥ ⁣∣Δ∣ ⁣∥F2−c0d1+d2n∥ ⁣∣Δ∣ ⁣∥nuc2\|\mathcal X_n(\Delta)\|_2^2/(2n) \ge \kappa/2\|\!|\Delta|\!\|_F^2 - c_0\frac{d_1+d_2}{n}\|\!|\Delta|\!\|_{\mathrm{nuc}}^2∥Xn​(Δ)∥22​/(2n)≥κ/2∥∣Δ∣∥F2​−c0​nd1​+d2​​∥∣Δ∣∥nuc2​ for all Δ\DeltaΔ, with κ>0\kappa>0κ>0, c0≥0c_0\ge 0c0​≥0. Conditioned on the good event G(λn)={∥ ⁣∣1n∑iwiXi∣ ⁣∥2≤λn/2}\mathcal G(\lambda_n)=\{\|\!|\frac1n\sum_iw_iX_i|\!\|_2 \le\lambda_n/2\}G(λn​)={∥∣n1​∑i​wi​Xi​∣∥2​≤λn​/2}, any optimal Θ^\hat\ThetaΘ^ satisfies, for any r∈{1,…,d′}r\in\{1,\dots,d'\}r∈{1,…,d′} with r≤κn/(128c0(d1+d2))r\le\kappa n/(128c_0(d_1+d_2))r≤κn/(128c0​(d1​+d2​)),

∥ ⁣∣Θ^−Θ∗∣ ⁣∥F2≤92λn2κ2r+1κ{2λn∑j=r+1d′σj(Θ∗)+32c0(d1+d2)n(∑j=r+1d′σj(Θ∗))2}.\|\!|\hat\Theta-\Theta^*|\!\|_F^2 \le \frac{9}{2}\frac{\lambda_n^2}{\kappa^2}r + \frac{1}{\kappa}\left\{2\lambda_n\sum_{j=r+1}^{d'}\sigma_j(\Theta^*) + \frac{32c_0(d_1+d_2)}{n}\left(\sum_{j=r+1}^{d'}\sigma_j(\Theta^*)\right)^2\right\}.∥∣Θ^−Θ∗∣∥F2​≤29​κ2λn2​​r+κ1​⎩⎨⎧​2λn​j=r+1∑d′​σj​(Θ∗)+n32c0​(d1​+d2​)​​j=r+1∑d′​σj​(Θ∗)​2⎭⎬⎫​.

Milestone (Proposition 10.7)

Under the alternative Φ∗\Phi^*Φ∗-curvature condition (10.20) (a curvature bound on the gradient map rather than the Taylor error), with rank(Θ∗)<κ/(64τn)\mathrm{rank}(\Theta^*)<\kappa/(64\tau_n)rank(Θ∗)<κ/(64τn​): conditioned on G(λn)={∥ ⁣∣1nXn∗(w)∣ ⁣∥2≤λn/2}\mathcal G(\lambda_n)=\{\|\!|\frac1n\mathcal X_n^*(w)|\!\|_2\le\lambda_n/2\}G(λn​)={∥∣n1​Xn∗​(w)∣∥2​≤λn​/2}, any optimal Θ^\hat\ThetaΘ^ satisfies ∥ ⁣∣Θ^−Θ∗∣ ⁣∥2≤32 λn/κ\|\!|\hat\Theta-\Theta^*|\!\|_2 \le 3\sqrt2\,\lambda_n/\kappa∥∣Θ^−Θ∗∣∥2​≤32​λn​/κ — an operator-norm bound the book notes is, in conjunction with the cone-like constraint (10.15), strictly stronger than Proposition 10.6's Frobenius-norm bound.

Significance

Proposition 10.6 is this chapter's direct payoff from Chapter 9's general machinery: it shows that the deterministic backbone of the Lasso's guarantee (mission 07-sparse-linear) extends essentially verbatim to the matrix setting, with the sparsity level sss replaced by the target rank rrr and the ambient dimension ddd replaced by d1+d2d_1+d_2d1​+d2​ — exactly the "degrees of freedom" scaling one would predict by counting the parameters needed to specify a rank-rrr matrix. Every one of the chapter's later corollaries (matrix compressed sensing, multivariate regression, matrix completion) is obtained by verifying the restricted strong convexity condition (10.17) holds with high probability for a specific random design, then reading the rate directly off Proposition 10.6 — the same two-step recipe Chapter 9's own Theorem 9.19 established abstractly. Proposition 10.7's operator-norm bound is what subsequently controls the individual singular values of the estimation error, needed for exact-rank-recovery guarantees.

Difficulty

Both results are direct specializations of Chapter 9's general oracle inequalities (Theorem 9.19 and Theorem 9.24 respectively) to the nuclear norm as regularizer and the Frobenius/operator norm pair, so their formalization difficulty lies almost entirely in getting the matrix-specific objects right rather than in new proof machinery: the nuclear norm requires an actual notion of singular values (realized via the eigenvalues of the Gram matrix ΘTΘ\Theta^T\ThetaΘTΘ, using Mathlib's Hermitian-matrix spectral theorem), the operator norm requires the correct rectangular generalization of the symmetric-matrix Rayleigh-quotient characterization used in mission 08-pca, and the restricted-strong-convexity and curvature conditions must be instantiated against the correctly-adjointed observation operator Xn∗\mathcal X_n^*Xn∗​. A further subtlety is keeping Proposition 10.6's Frobenius-norm conclusion and Proposition 10.7's operator-norm conclusion cleanly distinct — the book itself warns against conflating the norms used across different chapters of Part II (the vector ℓ2\ell_2ℓ2​-norm of chunks 07-sparse-linear/08-pca versus the matrix Frobenius and operator norms here).

Formalization scope

Scope cut, disclosed here and in STATUS.md. BRIEF.md recommends Corollary 10.10 (the sample-complexity bound for the Σ\SigmaΣ-Gaussian random matrix ensemble) as the goal theorem. Corollary 10.10 is a genuinely probabilistic statement — it asserts a bound holding "with probability at least 1−2e−2nδ21-2e^{-2n\delta^2}1−2e−2nδ2" over nnn i.i.d. draws of design matrices from a Σ\SigmaΣ-Gaussian ensemble (Theorem 10.8's own high-probability restricted-strong-convexity certification for that ensemble) — and formalizing it faithfully would require a genuine multivariate-Gaussian-measure infrastructure on matrix space (a probability space, an i.i.d. sequence of Σ\SigmaΣ-covariance-structured Gaussian matrices, and Mathlib's measure-theoretic probability API) that is disproportionate to this mission's time budget, and orthogonal to what Chapter 10 itself contributes (the chapter's own text stresses that Propositions 10.6 and 10.7 are the chapter's deterministic core, with probability entering only in Section 10.3's ensemble-specific certification — precisely mirroring chunk 09-decomposability's own "Theorem 9.19 is actually a deterministic result" framing). This mission instead takes Proposition 10.6 as its goal — explicitly named in BRIEF.md's own candidate list as "the nuclear-norm oracle inequality, an explicit corollary of Theorem 9.19" — the natural, tractable, still highly citable deterministic title result of Section 10.2, together with its companion Proposition 10.7. Theorem 10.8 (the Σ\SigmaΣ-Gaussian ensemble's RSC certification), Corollary 10.9 (noiseless exact recovery) and Corollary 10.10 itself are left for a future mission with a dedicated probability-theory budget. The cone-like constraint (Eq. 10.15) — whose own faithful statement requires the same explicit subspace-pair machinery (M(Ur,Vr),Mˉ(Ur,Vr)\mathcal M(U_r,V_r),\bar{\mathcal M}(U_r,V_r)M(Ur​,Vr​),Mˉ(Ur​,Vr​)) chunk 09-decomposability built for the general theory — is similarly left out, since Propositions 10.6 and 10.7's own numbered statements never expose these subspaces directly (only their proofs do, via instantiating Theorem 9.19/9.24). singularValues and nuclearNorm are noncomputable, defined via Mathlib's Hermitian-matrix eigenvalue spectral theorem; c0 ≥ 0 and λn > 0 are made explicit, matching this book's running conventions for RSC tolerance constants and regularization weights (see MODERATION_NOTES.md).

Selected references

  • Wainwright, M. J. High-Dimensional Statistics: A Non-Asymptotic Viewpoint. Cambridge University Press, 2019. Chapter 10. DOI: 10.1017/9781108627771.
  • Negahban, S., Wainwright, M. J. "Estimation of (near) low-rank matrices with noise and high-dimensional scaling." Annals of Statistics, 39(2), 2011, 1069–1097.
  • Recht, B., Fazel, M., Parrilo, P. A. "Guaranteed minimum-rank solutions of linear matrix equations via nuclear norm minimization." SIAM Review, 52(3), 2010, 471–501.
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Machine LearningStatisticsTheoretical Computer Science·Captain: mikedeng1

Foundations of Machine Learning V: Kernel Methods and the Representer TheoremTextbook

Motivation

Linear methods like SVMs work only when the classes are linearly separable, but most real data is not. Chapter 6 shows how to get non-linear decision boundaries for free: replace the input space's inner product with a kernel KKK that implicitly computes an inner product in a (possibly very high- or infinite-dimensional) feature space, without ever explicitly computing the feature mapping. This works for any positive definite symmetric (PDS) kernel — and the chapter's central theorem shows that such a kernel always induces a genuine Hilbert space (the reproducing kernel Hilbert space, RKHS) in which the kernel is literally an inner product. The chapter's capstone, the representer theorem, then shows that a broad class of optimization problems over this (possibly infinite-dimensional) Hilbert space always has a solution expressible as a finite linear combination of kernel evaluations at the training points — turning an infinite-dimensional problem into a finite, mmm-dimensional one.

Setting

A kernel K:X×X→RK:X\times X\to\mathbb RK:X×X→R is PDS (Definition 6.3) if for every finite sample {x1,…,xm}⊆X\{x_1,\dots,x_m\}\subseteq X{x1​,…,xm​}⊆X, the Gram matrix [K(xi,xj)][K(x_i,x_j)][K(xi​,xj​)] is symmetric positive semidefinite. Theorem 6.8 shows every PDS kernel is an inner product K(x,x′)=⟨Φ(x),Φ(x′)⟩K(x,x')=\langle \Phi(x),\Phi(x')\rangleK(x,x′)=⟨Φ(x),Φ(x′)⟩ in some Hilbert space HHH (the RKHS), which further has the reproducing property h(x)=⟨h,K(x,⋅)⟩h(x)=\langle h,K(x,\cdot)\rangleh(x)=⟨h,K(x,⋅)⟩ for every h∈Hh\in Hh∈H — evaluating hhh at a point is itself an inner product with the kernel section at that point. Theorem 6.10 shows PDS kernels are closed under sum, product, tensor product, pointwise limit, and power-series composition, letting complex kernels (Gaussian, and many others) be built from simple ones (polynomial kernels) without re-verifying positive-semidefiniteness from scratch. Section 6.3's representer theorem (Theorem 6.11) then considers minimizing, over h∈Hh\in Hh∈H, an objective F(h)=G(∥h∥H)+L(h(x1),…,h(xm))F(h)=G(\|h\|_H)+L(h(x_1),\dots,h(x_m))F(h)=G(∥h∥H​)+L(h(x1​),…,h(xm​)) that depends on hhh only through its norm and its values at mmm fixed points.

Formalization targets

Theorem 6.8 (RKHS existence, milestone). For a PDS kernel KKK, there exist a Hilbert space HHH and Φ:X→H\Phi:X\to HΦ:X→H with K(x,x′)=⟨Φ(x),Φ(x′)⟩K(x,x')=\langle\Phi(x),\Phi(x')\rangleK(x,x′)=⟨Φ(x),Φ(x′)⟩, and HHH has the reproducing property h(x)=⟨h,K(x,⋅)⟩h(x)=\langle h,K(x,\cdot)\rangleh(x)=⟨h,K(x,⋅)⟩ for all h∈Hh\in Hh∈H, x∈Xx\in Xx∈X.

Theorem 6.10 (closure properties, milestone). PDS kernels are closed under sum, product, tensor product, pointwise limit, and power-series composition with non-negative coefficients.

Theorem 6.11 — the mission's goal. For any non-decreasing G:R→RG:\mathbb R\to\mathbb RG:R→R and any loss L:Rm→R∪{+∞}L:\mathbb R^m\to\mathbb R\cup\{+\infty\}L:Rm→R∪{+∞}, argminh∈HG(∥h∥H)+L(h(x1),…,h(xm))\mathrm{argmin}_{h\in H} G(\|h\|_H)+ L(h(x_1),\dots,h(x_m))argminh∈H​G(∥h∥H​)+L(h(x1​),…,h(xm​)) admits a solution h⋆=∑i=1mαiK(xi,⋅)h^\star=\sum_{i=1}^m\alpha_i K(x_i,\cdot)h⋆=∑i=1m​αi​K(xi​,⋅); if GGG is increasing, every solution has this form.

Significance

Theorem 6.11 is the chapter's payoff and one of the most widely used structural results in kernel methods: it explains, in one general statement covering SVMs, kernel ridge regression, Gaussian process MAP estimation and many other algorithms simultaneously, why the dual (finite, mmm-coefficient) formulation always suffices — the RKHS's infinite dimensionality never has to be confronted directly. Theorem 6.8 is the structural fact the whole chapter (and every later kernelized algorithm in the book, chapters 9-11, 15) depends on: without it, "PDS kernel" would be a purely combinatorial condition on Gram matrices with no guarantee it corresponds to any actual inner product. No prior art on the Prove2Me platform is faithful to any of this chapter's content: GET /theorems?q=Representer theorem and q=reproducing kernel return no faithful match (one unrelated hit concerns a Gaussian-measure reproducing kernel in a different, probabilistic context, not this chapter's PDS-kernel/RKHS construction). All six items are drafted fresh.

Difficulty

Theorem 6.8's proof is a genuine construction: define H0H_0H0​ as finite linear combinations of kernel sections Φ(x)=K(x,⋅)\Phi(x)=K(x,\cdot)Φ(x)=K(x,⋅), define an inner product on H0H_0H0​ using KKK itself, verify it is well-defined (independent of the representation), positive semidefinite (via the PDS hypothesis), and — via the Cauchy-Schwarz-for-PDS-kernels lemma (Lemma 6.7) — actually positive definite, then complete H0H_0H0​ to a genuine Hilbert space HHH in which it is dense, and finally extend the reproducing property from the dense subspace H0H_0H0​ to all of HHH by a continuity argument. This is substantial analysis, not a restatement. Theorem 6.11's proof uses the orthogonal decomposition H=H1⊕H1⊥H=H_1\oplus H_1^\perpH=H1​⊕H1⊥​ (where H1=span{K(xi,⋅)}H_1=\mathrm{span}\{K(x_i, \cdot)\}H1​=span{K(xi​,⋅)}) and the reproducing property to show the orthogonal component h⊥h^\perph⊥ never helps and, when GGG is strictly increasing, strictly hurts — a short argument, but one that depends essentially on Theorem 6.8's reproducing property holding for the specific HHH constructed, not just any Hilbert space with the kernel as its inner product.

Formalization scope

IsPDS uses the book's own second SPSD characterization (c^T K c ≥ 0 for every finite sample and coefficient vector c) rather than the non-negative-eigenvalues characterization, avoiding spectral theory for a Prop-valued definition; the book states the two are equivalent. IsRKHSOf and IsMinimizer are formalization scaffolding, not book-numbered definitions: IsRKHSOf packages Theorem 6.8's own two displayed equations (6.8, 6.9) as a reusable predicate shared between Theorem 6.8 (its conclusion) and Theorem 6.11 (its "H its corresponding RKHS" hypothesis), using an explicit evaluation map ev : H → X → ℝ to stand in for "elements of H are functions on X," since Mathlib's abstract Hilbert spaces are not themselves spaces of functions; IsMinimizer packages argmin. Both X in Theorem 6.8's existential and Theorem 6.11's ambient type are plain Type rather than Type*, avoiding universe-polymorphic quantification over the constructed Hilbert space's own type — a harmless simplification, since every application in this book instantiates X at a concrete, small type (typically RN\mathbb R^NRN or a finite set). Theorem 6.11's loss codomain ℝ ∪ {+∞} is WithTop ℝ, not EReal (which would also admit -∞, an unstated generalization the book's own display does not license, since EReal's ⊤+⊥=⊥ collapse is a genuine faithfulness risk the book's own L:\mathbb R^m\to\mathbb R\cup\{+\infty\} avoids by construction). WithTop ℝ on its own does not avoid every collapse, though: an unconstrained L may be the constant function ⊤ (a legal instance of ℝ∪\{+\infty\}), forcing the objective identically ⊤ and every point to vacuously minimize it, which would make the theorem's second conjunct false. An added hypothesis, ∃ h₀, F h₀ ≠ ⊤, makes explicit the book's own implicit assumption that the objective is finite somewhere — see the Formalization scope note below. Theorem 6.11's two clauses are otherwise kept exactly as distinct as the book states them: existence needs only Monotone G (non-decreasing); "any solution has this form" needs StrictMono G (increasing) as an added hypothesis on the second conjunct only — per this chunk's own BRIEF.md, the crux of the theorem, and the trap this mission is most careful to avoid collapsing. Theorem 6.10's five closure clauses are stated as one conjunction (matching the book's single theorem, not five separate items); the power-series clause keeps the book's own radius-of-convergence domain restriction and adds an explicit summability hypothesis guarding the ∑' term.

Not formalized: Theorem 6.2 (Mercer's condition) — not needed by the goal's own proof chain (it is an equivalent characterization of PDS mentioned before the RKHS construction, not a premise Theorem 6.8's or 6.11's proof invokes) and its own hypotheses (compact X⊂RNX\subset \mathbb R^NX⊂RN, continuous KKK, an eigenfunction expansion of a compact self-adjoint integral operator) are real analytic content this mission's budget does not include; Lemma 6.7 (Cauchy-Schwarz for PDS kernels) and Lemma 6.9 (normalized PDS kernels) — supporting lemmas for Theorem 6.8's proof, not independently numbered results the goal cites; Theorem 6.12/Corollary 6.13 (Rademacher complexity/margin bounds for kernel-based hypotheses) — the chapter's optional further milestone, connecting to chunks 03/05's machinery, cut for budget; §6.5-6.8 (sequence kernels, weighted transducers, rational kernels, Bochner's theorem, approximate feature maps) — explicitly out of scope per this chunk's own BRIEF.md, a distinct, applications-heavy topic.

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 6, §6.1-6.4.
  • B. Schölkopf, R. Herbrich, A. J. Smola, "A generalized representer theorem," COLT 2001, Lecture Notes in Computer Science 2111, 2001, 416-426.
  • N. Aronszajn, "Theory of reproducing kernels," Transactions of the American Mathematical Society 68(3), 1950, 337-404.
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Machine LearningRandom Matrix TheoryStatistics·Captain: mikedeng1

High-Dimensional Probability IV: Norms of Random Matrices with Sub-gaussian EntriesTextbook

Motivation

Random matrices with independent entries appear whenever a system is measured through many noisy, roughly independent channels: shot noise in a sensor array, edges in an Erdős–Rényi-type random graph, or the design matrix of a linear model with independent covariates. A basic question about any such matrix AAA is how far it can stretch a vector — its operator norm ∥A∥\|A\|∥A∥ — since this single number controls the stability of every linear statistic computed from AAA: least-squares estimates, spectral clustering, covariance estimation, and random projections all reduce, at some point, to bounding ∥A∥\|A\|∥A∥.

The theory traces to Marchenko and Pastur's 1967 asymptotic law for the spectrum of large random matrices, and to Bai and Yin's 1988 almost-sure limit ∥A∥/n→2\|A\|/\sqrt n \to 2∥A∥/n​→2 for n×nn \times nn×n matrices with i.i.d. mean-zero, unit-variance entries. Those results are asymptotic: they say what happens as the dimension n→∞n \to \inftyn→∞, for a fixed matrix shape. The result formalized here, Theorem 4.4.5 of Vershynin's High-Dimensional Probability (2018) (DOI 10.1017/9781108231596), belongs to the more recent non-asymptotic strand of the theory: it gives an explicit, dimension-free bound that holds at every fixed m,nm, nm,n, with an explicit failure probability — the form of statement needed for finite-sample guarantees in statistics and data science, rather than limiting behavior.

Setting

Let AAA be an m×nm \times nm×n real matrix. Equip Rn\mathbb R^nRn and Rm\mathbb R^mRm with the Euclidean norm ∥⋅∥2\|\cdot\|_2∥⋅∥2​; AAA acts as a linear map ℓ2n→ℓ2m\ell_2^n \to \ell_2^mℓ2n​→ℓ2m​. Its operator norm (§4.1.2) is

∥A∥  :=  max⁡x∈Sn−1∥Ax∥2,\|A\| \;:=\; \max_{x \in S^{n-1}} \|Ax\|_2 ,∥A∥:=x∈Sn−1max​∥Ax∥2​,

the largest factor by which AAA can stretch a unit vector; equivalently, the largest singular value of AAA.

A real random variable XXX is sub-gaussian with the mission's own convention (matching the Orlicz ψ2\psi_2ψ2​ norm this series already carries as a published definition, HighDimProb.Concentration.subgaussianNorm) if

∥X∥ψ2  :=  inf⁡{t>0:Eexp⁡(X2/t2)≤2}  <  ∞.\|X\|_{\psi_2} \;:=\; \inf\{t > 0 : \mathbb E \exp(X^2/t^2) \le 2\} \;<\; \infty .∥X∥ψ2​​:=inf{t>0:Eexp(X2/t2)≤2}<∞.

Bounded random variables and Gaussians are sub-gaussian; a Bernoulli(ppp) variable and a ±1\pm 1±1-valued coin flip both qualify, which is why the theorem below directly covers random matrices with i.i.d. Rademacher or Gaussian entries as special cases.

The mission's proof technique is the ε-net argument, developed in §4.2 and used nowhere before this chapter of the book: a metric space (T,d)(T,d)(T,d), a subset K⊆TK \subseteq TK⊆T, and ε>0\varepsilon > 0ε>0 give rise to an ε-net N⊆KN \subseteq KN⊆K — a finite set such that every point of KKK is within ε\varepsilonε of some point of NNN — and a covering number N(K,d,ε)N(K, d, \varepsilon)N(K,d,ε), the smallest cardinality of such a net. The technique reduces a statement that must hold uniformly over an infinite (compact) set to a statement about finitely many points, paid for by a union bound whose cost is controlled by the covering number.

Formalization targets

Goal (Theorem 4.4.5)

∃ C>0  such that  ∀ t>0,Prob{ ∥A∥≤CK(m+n+t) }  ≥  1−2exp⁡(−t2),\exists\, C > 0 \;\text{such that}\; \forall\, t > 0,\quad \mathrm{Prob}\bigl\{\, \|A\| \le CK(\sqrt m + \sqrt n + t) \,\bigr\} \;\ge\; 1 - 2\exp(-t^2),∃C>0such that∀t>0,Prob{∥A∥≤CK(m​+n​+t)}≥1−2exp(−t2),

for any m×nm \times nm×n random matrix AAA with independent, mean-zero, sub-gaussian entries AijA_{ij}Aij​ and K=max⁡i,j∥Aij∥ψ2K = \max_{i,j} \|A_{ij}\|_{\psi_2}K=maxi,j​∥Aij​∥ψ2​​. This is the weakest stable form of the bound — it fixes no numerical value for CCC, only its existence and absoluteness (independence from mmm, nnn, AAA, ttt), so later refinements of the constant do not invalidate it.

Significance

The result itself. The bound ∥A∥≲m+n\|A\| \lesssim \sqrt m + \sqrt n∥A∥≲m​+n​ is sharp up to the constant: for entries of unit variance, E∥A∥≥14(m+n)\mathbb E\|A\| \ge \tfrac14(\sqrt m + \sqrt n)E∥A∥≥41​(m​+n​) for large m,nm, nm,n (the book's Exercise 4.4.7), so no non-asymptotic bound of this shape can be improved beyond constants. It is the entry point to the rest of the book's random matrix theory: Corollary 4.4.8 specializes it to symmetric matrices, and it underlies the community-detection (§4.5) and covariance-estimation (§4.7) applications later in the same chapter, neither of which is part of this mission.

Formalizing it. The theorem is a classical, fully proved result; nothing about its truth is open. What this mission contributes is a machine-checked formal statement — together with the two pieces of chapter infrastructure its own textbook proof names by number (Corollary 4.2.13, Exercise 4.4.3(a)) — and a third, self-contained application of the same covering-number machinery (Theorem 4.3.5) that exercises the shared IsEpsNet/coveringNumber definitions on a different metric space (the Hamming cube), independently of the Euclidean case. Mathlib and the Prove2Me platform currently have no ε-net, covering-number, or packing-number infrastructure (checked by q=random matrix, q=operator norm, q=covering number, q=net on the platform, and by filename search in Mathlib): this mission is the first to introduce it, restated inside its own namespace since it is not otherwise available to build on.

Difficulty

The obvious first approach is to bound ∥A∥=max⁡x∈Sn−1∥Ax∥2\|A\| = \max_{x \in S^{n-1}} \|Ax\|_2∥A∥=maxx∈Sn−1​∥Ax∥2​ directly by union-bounding a concentration inequality over the sphere Sn−1S^{n-1}Sn−1. This fails outright: Sn−1S^{n-1}Sn−1 is infinite (indeed uncountable) for n≥2n \ge 2n≥2, so no union bound over its points can converge — the naive approach gives ∞⋅(tail probability)\infty \cdot (\text{tail probability})∞⋅(tail probability). The ε-net argument is the fix, but it is not just "discretize and hope": the reduction from the sphere to a finite net (quadratic_form_on_net, Exercise 4.4.3(a)) loses a multiplicative factor 1/(1−2ε)1/(1-2\varepsilon)1/(1−2ε) that must be tracked, and the net's cardinality (covering_numbers_of_euclidean_ball_and_sphere, Corollary 4.2.13) is exponential in the dimension (9n9^n9n at ε=1/4\varepsilon = 1/4ε=1/4) — so the per-point tail probability from Hoeffding-type concentration must itself decay fast enough (quadratically in the exponent) to survive multiplying by 9m+n9^{m+n}9m+n many points. Getting the union bound to close requires choosing the threshold uuu in the tail bound proportionally to m+n+t\sqrt m + \sqrt n + tm​+n​+t, not to ttt alone — the m+n\sqrt m + \sqrt nm​+n​ term is exactly what pays for the net's exponential size.

Formalization scope

AAA is represented as Ω → Matrix (Fin m) (Fin n) ℝ; its entries A ω i j are the individual real random variables. Independence of the mnmnmn entries is iIndepFun over the index type Fin m × Fin n; mean-zero is the vanishing of each entry's Bochner integral. The operator norm is the norm of the associated continuous linear map between EuclideanSpace ℝ (Fin n) and EuclideanSpace ℝ (Fin m) (matrixOpNorm, every linear map between finite-dimensional normed spaces being automatically continuous), matching the book's maxₓ∈Sⁿ⁻¹ ‖Ax‖₂ exactly. The sub-gaussian norm KKK reuses this series' own published definition, HighDimProb.Concentration.subgaussianNorm, rather than a re-derivation. Covering numbers (coveringNumber) are restricted to finite (Finset) ε-nets, the only kind this chapter uses; this is a deliberate restriction, not a general-purpose covering-number formalization, and is disclosed as such. A hard-coded numeral for CCC, or an unquantified "with high probability" in place of the explicit failure probability 2exp⁡(−t2)2\exp(-t^2)2exp(−t2), would each trivialize the statement and is ruled out: CCC is existentially bound ahead of every other quantifier, and t>0t > 0t>0 is a free parameter with its own explicit bound, exactly as the book states it.

Definitions reusable beyond this mission: IsEpsNet and coveringNumber are stated for a general PseudoMetricSpace and apply unchanged to any later chapter's covering-number needs (e.g. Chapter 8's VC-dimension covering numbers), though per this series' rule that drafts cannot import drafts, a later chunk would restate rather than import them until this mission is published. matrixOpNorm is likewise chapter-agnostic. Contributions completing the sorry proofs of any of the four theorem items are welcome and independent of one another; the covering number and net-reduction items (covering_numbers_of_euclidean_ball_and_sphere, quadratic_form_on_net) are the standard prerequisites for the goal's own volumetric/ε-net proof.

Selected references

  • Vershynin, R. High-Dimensional Probability: An Introduction with Applications in Data Science. Cambridge University Press, 2018. DOI 10.1017/9781108231596
  • Bai, Z. D., Yin, Y. Q. "Necessary and sufficient conditions for almost sure convergence of the largest eigenvalue of a Wigner matrix." Annals of Probability 16 (1988), 1729–1741.
  • Marchenko, V. A., Pastur, L. A. "Distribution of eigenvalues for some sets of random matrices." Mathematics of the USSR-Sbornik 1 (1967), 457–483.
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Convex OptimizationLinear OptimizationOperations Research+1·Captain: mikedeng1

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

Motivation

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

Setting

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

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

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

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

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

Formalization targets

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

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

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

Supporting milestones

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

Significance

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

Difficulty

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

Formalization scope

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

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

Selected references

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

Markov Chains and Mixing Times XII: Continuous Time and Countable State SpacesTextbook

Motivation

The whole series so far lived in discrete time on finite state spaces. Chapters 20–21 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) lift both restrictions. Running the jumps of a chain at the arrivals of a rate-one Poisson clock produces the continuous-time chain, whose transition semigroup — the heat kernel — converges to stationarity for every irreducible chain, with no aperiodicity hypothesis: continuous time washes out periodicity. On countable state spaces, existence of a stationary distribution is no longer automatic, and the trichotomy of transience, null recurrence, and positive recurrence replaces it; the convergence theorem survives exactly on the positive-recurrent class. The chapter's crown jewel — and this mission's goal — is Pólya's theorem: simple random walk on the lattice Zd\mathbb Z^dZd is recurrent in dimensions one and two and transient in dimension three and higher. "A drunk man will find his way home, but a drunk bird may get lost forever."

Setting

Continuous time (Ch. 20). For a finite chain PPP, the heat kernel at time t≥0t\ge0t≥0 is defined by Poissonization,

Ht(x,y)=∑k=0∞e−ttkk! Pk(x,y),H_t(x,y)=\sum_{k=0}^{\infty}e^{-t}\frac{t^k}{k!}\,P^k(x,y),Ht​(x,y)=k=0∑∞​e−tk!tk​Pk(x,y),

the law at time ttt of a walk taking PPP-steps at Poisson arrival times (=et(P−I)=e^{t(P-I)}=et(P−I) as a matrix exponential). With ∥μ−ν∥TV=max⁡A∣μ(A)−ν(A)∣\|\mu-\nu\|_{TV}=\max_A|\mu(A)-\nu(A)|∥μ−ν∥TV​=maxA​∣μ(A)−ν(A)∣, the continuous distance and mixing time are dcont(t)=max⁡x∥Ht(x,⋅)−π∥TVd^{\mathrm{cont}}(t)=\max_x\|H_t(x,\cdot)-\pi\|_{TV}dcont(t)=maxx​∥Ht​(x,⋅)−π∥TV​ and tmixcont(ε)=inf⁡{t≥0:dcont(t)≤ε}t^{\mathrm{cont}}_{\mathrm{mix}}(\varepsilon)=\inf\{t\ge0:d^{\mathrm{cont}}(t)\le\varepsilon\}tmixcont​(ε)=inf{t≥0:dcont(t)≤ε}. The lazy version of a discrete chain is 12(I+P)\tfrac12(I+P)21​(I+P); from Mission VII, the spectral gap γ\gammaγ is 1−λ21-\lambda_21−λ2​ with λ2\lambda_2λ2​ the largest eigenvalue ≠1\ne1=1. The product chain on a product of nnn coordinate spaces picks a uniform coordinate and updates it by that coordinate's chain.

Countable state spaces (Ch. 21). A chain on a countable state space VVV is a function PPP with nonnegative entries and rows summing to one (as convergent series); ttt-step probabilities Pt(x,y)P^t(x,y)Pt(x,y) are defined recursively, and trajectory probabilities are countable sums of path weights. The first return time to xxx is τx+=min⁡{t≥1:Xt=x}\tau_x^+=\min\{t\ge1:X_t=x\}τx+​=min{t≥1:Xt​=x}; a state is recurrent when Px{τx+<∞}=1\mathbb P_x\{\tau_x^+<\infty\}=1Px​{τx+​<∞}=1 (tails tend to zero), positive recurrent when moreover Ex(τx+)<∞\mathbb E_x(\tau_x^+)<\inftyEx​(τx+​)<∞ (tails summable), and null recurrent when recurrent but not positive recurrent. A stationary distribution is a nonnegative π\piπ summing to one with πP=π\pi P=\piπP=π (as convergent series). Simple random walk on Zd\mathbb Z^dZd steps from xxx to one of its 2d2d2d nearest neighbours uniformly at random.

Formalization targets

Goal

Pólya's theorem (§21.2, Examples 21.8–21.9), the capstone of Chapters 20–21:

  1. for d≤2d\le2d≤2, simple random walk on Zd\mathbb Z^dZd is recurrent — it returns to its starting point with probability one;
  2. for d≥3d\ge3d≥3, it is transient — with positive probability it never returns.

Milestones

  • Theorem 20.1 — for any irreducible finite chain, aperiodic or not, the heat kernel converges: dcont(t)→0d^{\mathrm{cont}}(t)\to0dcont(t)→0 as t→∞t\to\inftyt→∞.
  • Theorem 20.3 — the two-way comparison between lazy discrete and continuous mixing: eventual ε\varepsilonε-mixing of the lazy chain at time kkk gives 2ε2\varepsilon2ε-mixing of the heat kernel at time kkk, and ε\varepsilonε-mixing of the heat kernel at time mmm gives 2ε2\varepsilon2ε-mixing of the lazy chain at time 4m4m4m.
  • Theorem 20.6 — the spectral bound for reversible chains: ∣Ht(x,y)−π(y)∣≤π(y)/π(x)  e−γt\bigl|H_t(x,y)-\pi(y)\bigr|\le\sqrt{\pi(y)/\pi(x)}\;e^{-\gamma t}​Ht​(x,y)−π(y)​≤π(y)/π(x)​e−γt.
  • Theorem 20.7 — mixing of continuous-time product chains: with all coordinate gaps ≥γ\ge\gamma≥γ and coordinate stationary masses bounded below, tmixcont(ε)≤(2γ)−1nlog⁡n+γ−1nlog⁡(1/(c0ε))t^{\mathrm{cont}}_{\mathrm{mix}}(\varepsilon)\le(2\gamma)^{-1}n\log n+\gamma^{-1}n\log(1/(c_0\varepsilon))tmixcont​(ε)≤(2γ)−1nlogn+γ−1nlog(1/(c0​ε)), with a matching n2γlog⁡n\tfrac{n}{2\gamma}\log n2γn​logn lower bound when the gaps are equal — the nlog⁡nn\log nnlogn product-chain phenomenon.
  • Proposition 21.3 — the recurrence dichotomy on countable spaces: a state is recurrent exactly when its Green's function ∑tPt(x,x)\sum_tP^t(x,x)∑t​Pt(x,x) diverges, and for an irreducible chain one recurrent state makes all states recurrent.
  • Theorem 21.12 — an irreducible countable chain is positive recurrent if and only if it has a stationary distribution.
  • Lemma 21.13 (Kac) — for an irreducible chain with stationary distribution π\piπ and any nonempty set SSS: ∑x∈Sπ(x) Ex(τS+)=1\sum_{x\in S}\pi(x)\,\mathbb E_x(\tau_S^+)=1∑x∈S​π(x)Ex​(τS+​)=1; in particular Ex(τx+)=1/π(x)\mathbb E_x(\tau_x^+)=1/\pi(x)Ex​(τx+​)=1/π(x).
  • Theorem 21.14 — the convergence theorem on countable spaces: an irreducible, aperiodic, positive recurrent chain has a unique stationary distribution π\piπ, and ∥Pt(x,⋅)−π∥TV→0\|P^t(x,\cdot)-\pi\|_{TV}\to0∥Pt(x,⋅)−π∥TV​→0 from every start.
  • Theorem 21.17 — in the null recurrent case, Pt(x,y)→0P^t(x,y)\to0Pt(x,y)→0 for all pairs of states: no stationary profile is approached.

Significance

The results. Theorem 20.1 explains why laziness and aperiodicity pervade the discrete theory — periodicity is an artifact of the discrete clock. The product-chain theorem 20.7 is the cleanest instance of the nlog⁡nn\log nnlogn paradigm (independent coordinates mix in relaxation time ×log⁡(number of coordinates)\times\log(\text{number of coordinates})×log(number of coordinates)) and the template for the hypercube cutoff of Mission XI. Chapter 21's trichotomy is the backbone of applied Markov chain theory — queueing, branching, renewal — and Kac's lemma with the convergence theorem 21.14 is the standard equipment of any probability course. Pólya's theorem is one of the most celebrated results of twentieth-century probability, the birth of the random-walk-in-dimension-ddd paradigm.

Formalizing them. Mathlib has no continuous-time Markov chains, no Poissonization, and no recurrence/transience theory (its PMF random walks stop far short). The countable-state layer built here — summable stationary equations, tail-sum return times, the recurrence dichotomy — is the missing infrastructure for formalized applied probability; Pólya's theorem is a famous target in its own right, and the d≥3d\ge3d≥3 half has never been formalized in any assistant to our knowledge.

Difficulty

The heat kernel is an infinite series of matrices: convergence (dominated by the Poisson weights), the semigroup property, and the interchange of the series with matrix products and limits must all be established by hand over tsum. Theorem 20.1 avoids aperiodicity by the number-theoretic fact that the Poisson distribution smears over residue classes — formally, the continuous chain is automatically aperiodic because Ht(x,x)>0H_t(x,x)>0Ht​(x,x)>0 for t>0t>0t>0. The product-chain bounds need the ℓ2\ell^2ℓ2 machinery of Mission VII applied coordinatewise and a careful union bound; the lower bound is a Gaussian-free second-moment argument. On the countable side, everything is series bookkeeping in the absence of Fintype: the recurrence dichotomy is a generating-function (renewal) identity G(x,x)=1/Px{τx+=∞}G(x,x)=1/\mathbb P_x\{\tau_x^+=\infty\}G(x,x)=1/Px​{τx+​=∞} handled through partial sums; Kac's lemma is a mass-transport double-count over trajectories; and Theorem 21.14 needs an aperiodicity-based coupling on a countable product space, the technical summit of the mission. Pólya's theorem itself combines a local central-limit-type estimate for the return probabilities (P2t(0,0)≍t−d/2P^{2t}(0,0)\asymp t^{-d/2}P2t(0,0)≍t−d/2, obtained by Stirling in d=1,2d=1,2d=1,2 and by a comparison argument in higher dimension) with the dichotomy of Proposition 21.3.

Formalization scope

Chapter 20 lives on finite state spaces: the heat kernel is a tsum over kkk of Poisson weights times matrix powers (summability is provable, not assumed), continuous distance is a supremum over states, and the continuous mixing time is an sInf over nonnegative reals (junk 000 if the set were empty — excluded under the theorems' hypotheses). Discrete-vs-continuous comparison (Theorem 20.3) is stated with eventual thresholds (∃K,∀k≥K\exists K,\forall k\ge K∃K,∀k≥K), matching the book's asymptotic phrasing. Chapter 21 lives on a Countable type: stochasticity and stationarity are HasSum statements, ttt-step powers are defined recursively with tsum convolutions, return-time tails are countable sums of path weights over finite horizons, and recurrence/positive recurrence are the tail-limit and tail-summability conditions above — measure theory never enters. Pólya's theorem is stated for the origin of Zd\mathbb Z^dZd with the walk defined by nearest-neighbour steps; the d≤2d\le2d≤2 and d≥3d\ge3d≥3 halves are separate conjuncts of one statement.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • G. Pólya, Über eine Aufgabe der Wahrscheinlichkeitsrechnung betreffend die Irrfahrt im Straßennetz, Math. Ann. 84 (1921). https://doi.org/10.1007/BF01458701
  • W. Feller, An Introduction to Probability Theory and Its Applications, Vol. I, 3rd ed., Wiley, 1968.
  • D. Aldous, J. A. Fill, Reversible Markov Chains and Random Walks on Graphs, 2002. https://www.stat.berkeley.edu/~aldous/RWG/book.html
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Markov ChainStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times VII: Eigenvalues and the Cheeger InequalityTextbook

Motivation

How fast does a Markov chain forget its starting point? For a reversible chain the complete answer is coded in the eigenvalues of its transition matrix: the largest eigenvalue is always 111, and the size of the gap between 111 and the rest of the spectrum is the chain's fundamental time constant — a large gap means fast mixing, a small gap means slow mixing. Chapters 12–13 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) develop this spectral theory and culminate in the discrete Cheeger inequality of Jerrum–Sinclair and Lawler–Sokal, which says that the spectral gap γ\gammaγ (an analytic quantity, defined below) and the bottleneck constant Φ⋆\Phi_\starΦ⋆​ (a geometric quantity from Mission IV, also recalled below) control each other:

Φ⋆22  ≤  γ  ≤  2 Φ⋆.\frac{\Phi_\star^2}{2}\;\le\;\gamma\;\le\;2\,\Phi_\star.2Φ⋆2​​≤γ≤2Φ⋆​.

A chain mixes rapidly exactly when its state space has no bottleneck. This inequality is the backbone of the Markov-chain approach to approximate counting and of spectral graph theory at large; alongside it the chapters provide Wilson's method — the sharpest general technique for mixing-time lower bounds — and the comparison machinery that transfers spectral estimates between chains.

Setting

All chains live on a finite state space VVV. A chain with transition matrix PPP and stationary distribution π\piπ is reversible when the detailed balance equations π(x)P(x,y)=π(y)P(y,x)\pi(x)P(x,y)=\pi(y)P(y,x)π(x)P(x,y)=π(y)P(y,x) hold; reversibility is the standing assumption of both chapters. The yardsticks of the series are the total variation distance ∥μ−ν∥TV=max⁡A⊆V∣μ(A)−ν(A)∣\|\mu-\nu\|_{TV}=\max_{A\subseteq V}|\mu(A)-\nu(A)|∥μ−ν∥TV​=maxA⊆V​∣μ(A)−ν(A)∣, the worst-case distance to stationarity d(t)=max⁡x∥Pt(x,⋅)−π∥TVd(t)=\max_x\|P^t(x,\cdot)-\pi\|_{TV}d(t)=maxx​∥Pt(x,⋅)−π∥TV​, and the mixing time tmix(ε)=min⁡{t:d(t)≤ε}t_{\mathrm{mix}}(\varepsilon)=\min\{t: d(t)\le\varepsilon\}tmix​(ε)=min{t:d(t)≤ε}, with tmix=tmix(1/4)t_{\mathrm{mix}}=t_{\mathrm{mix}}(1/4)tmix​=tmix​(1/4); we write πmin⁡=min⁡xπ(x)\pi_{\min}=\min_x\pi(x)πmin​=minx​π(x).

The spectral vocabulary: an eigenfunction of PPP is a nonzero f:V→Rf:V\to\mathbb Rf:V→R with Pf=λfPf=\lambda fPf=λf, where (Pf)(x)=∑yP(x,y)f(y)(Pf)(x)=\sum_yP(x,y)f(y)(Pf)(x)=∑y​P(x,y)f(y); the number λ\lambdaλ is then an eigenvalue. Out of the spectrum one forms

  • λ2\lambda_2λ2​, the largest eigenvalue different from 111, and the spectral gap γ=1−λ2\gamma=1-\lambda_2γ=1−λ2​;
  • λ⋆\lambda_\starλ⋆​, the largest absolute value of an eigenvalue different from 111, the absolute gap γ⋆=1−λ⋆\gamma_\star=1-\lambda_\starγ⋆​=1−λ⋆​, and the relaxation time trel=1/γ⋆t_{\mathrm{rel}}=1/\gamma_\startrel​=1/γ⋆​.

Functions on VVV carry the weighted inner product ⟨f,g⟩π=∑xf(x)g(x)π(x)\langle f,g\rangle_\pi=\sum_xf(x)g(x)\pi(x)⟨f,g⟩π​=∑x​f(x)g(x)π(x) — the geometry, denoted ℓ2(π)\ell^2(\pi)ℓ2(π), in which a reversible PPP is self-adjoint — and the Dirichlet form

E(f)=12∑x,y[f(x)−f(y)]2 π(x)P(x,y),\mathcal E(f)=\tfrac12\sum_{x,y}\bigl[f(x)-f(y)\bigr]^2\,\pi(x)P(x,y),E(f)=21​x,y∑​[f(x)−f(y)]2π(x)P(x,y),

the average squared variation of fff along the chain's transitions. Finally, from Mission IV: the bottleneck ratio of a set SSS of states is Φ(S)=∑x∈S, y∉Sπ(x)P(x,y) / π(S)\Phi(S)=\sum_{x\in S,\,y\notin S}\pi(x)P(x,y)\,/\,\pi(S)Φ(S)=∑x∈S,y∈/S​π(x)P(x,y)/π(S), the conditional probability at stationarity of escaping SSS in one step, and the bottleneck constant is Φ⋆=min⁡{Φ(S):∅≠S, π(S)≤12}\Phi_\star=\min\{\Phi(S):\varnothing\ne S,\ \pi(S)\le\tfrac12\}Φ⋆​=min{Φ(S):∅=S, π(S)≤21​}.

Formalization targets

Goal

Theorem 13.14, the discrete Cheeger inequality: for a reversible irreducible chain,

Φ⋆22  ≤  γ  ≤  2 Φ⋆.\frac{\Phi_\star^2}{2}\;\le\;\gamma\;\le\;2\,\Phi_\star.2Φ⋆2​​≤γ≤2Φ⋆​.

Milestones

  • Lemma 12.1 — every eigenvalue satisfies ∣λ∣≤1|\lambda|\le1∣λ∣≤1; for an irreducible chain the eigenfunctions of the eigenvalue 111 are the constant functions; an irreducible aperiodic chain does not have −1-1−1 as an eigenvalue.
  • Lemma 12.2 — the spectral representation: a reversible chain admits eigenfunctions f1,…,f∣V∣f_1,\dots,f_{|V|}f1​,…,f∣V∣​, orthonormal with respect to ⟨⋅,⋅⟩π\langle\cdot,\cdot\rangle_\pi⟨⋅,⋅⟩π​, with eigenvalues λj\lambda_jλj​, such that Pt(x,y)/π(y)=∑jfj(x)fj(y)λjtP^t(x,y)/\pi(y)=\sum_jf_j(x)f_j(y)\lambda_j^tPt(x,y)/π(y)=∑j​fj​(x)fj​(y)λjt​ for all t,x,yt,x,yt,x,y.
  • Theorem 12.3 — mixing is at most relaxation times a log factor: tmix(ε)≤log⁡(1/(ε πmin⁡)) trel+1t_{\mathrm{mix}}(\varepsilon)\le\log\bigl(1/(\varepsilon\,\pi_{\min})\bigr)\,t_{\mathrm{rel}}+1tmix​(ε)≤log(1/(επmin​))trel​+1.
  • Theorem 12.4 — mixing is at least the relaxation time: tmix(ε)≥(trel−1)log⁡(1/(2ε))t_{\mathrm{mix}}(\varepsilon)\ge(t_{\mathrm{rel}}-1)\log\bigl(1/(2\varepsilon)\bigr)tmix​(ε)≥(trel​−1)log(1/(2ε)).
  • §12.3.1 — the model computation: simple random walk on the nnn-cycle has the numbers cos⁡(2πj/n)\cos(2\pi j/n)cos(2πj/n), j=0,…,n−1j=0,\dots,n-1j=0,…,n−1, among its eigenvalues.
  • Theorem 13.1 — if every pair of states admits a coupling of the two one-step distributions that contracts some metric ρ\rhoρ on VVV by a factor θ\thetaθ in expectation, then λ⋆≤θ\lambda_\star\le\thetaλ⋆​≤θ.
  • Theorem 13.5, Wilson's method — an eigenfunction Φ\PhiΦ with eigenvalue λ∈(12,1)\lambda\in(\tfrac12,1)λ∈(21​,1) whose one-step increments have second moment at most RRR yields the explicit lower bound tmix(ε)≥[2log⁡(1/λ)]−1[log⁡((1−λ)Φ(x)2/(2R))+log⁡((1−ε)/ε)]t_{\mathrm{mix}}(\varepsilon)\ge\bigl[2\log(1/\lambda)\bigr]^{-1}\bigl[\log\bigl((1-\lambda)\Phi(x)^2/(2R)\bigr)+\log\bigl((1-\varepsilon)/\varepsilon\bigr)\bigr]tmix​(ε)≥[2log(1/λ)]−1[log((1−λ)Φ(x)2/(2R))+log((1−ε)/ε)].
  • Lemmas 13.11–13.12 — the variational characterization: γ\gammaγ is the minimum of E(f)\mathcal E(f)E(f) over functions with mean zero (∑xf(x)π(x)=0\sum_xf(x)\pi(x)=0∑x​f(x)π(x)=0) and unit norm (⟨f,f⟩π=1\langle f,f\rangle_\pi=1⟨f,f⟩π​=1), and the minimum is attained.
  • Lemma 13.22 — the comparison method: if a second reversible chain P~\tilde PP~ on the same space, with stationary distribution π~\tilde\piπ~, Dirichlet form E~\tilde{\mathcal E}E~, and gap γ~\tilde\gammaγ~​, satisfies E~(f)≤B E(f)\tilde{\mathcal E}(f)\le B\,\mathcal E(f)E~(f)≤BE(f) for every fff, then γ~≤[max⁡xπ(x)/π~(x)]B γ\tilde\gamma\le\bigl[\max_x\pi(x)/\tilde\pi(x)\bigr]B\,\gammaγ~​≤[maxx​π(x)/π~(x)]Bγ.

Significance

The results. Theorems 12.3–12.4 sandwich the mixing time between trelt_{\mathrm{rel}}trel​ and trellog⁡(1/πmin⁡)t_{\mathrm{rel}}\log(1/\pi_{\min})trel​log(1/πmin​) — the fundamental equivalence of spectral and mixing estimates for reversible chains, prerequisite for the cutoff criterion of Mission XI. The Cheeger inequality converts isoperimetry into spectral bounds; it is the mathematical core of the Jerrum–Sinclair program of polynomial-time approximate counting, and its graph version underlies expander theory. Wilson's method produced the sharp lower bounds for adjacent transpositions and hypercube-type chains; the comparison lemma is the engine behind the shuffle bounds cited in Mission V (§16.1).

Formalizing them. Mathlib has the spectral theorem for symmetric matrices but nothing connecting spectra to Markov chains: no spectral gap, no relaxation time, no Dirichlet forms, no Cheeger inequality in any form. A formalized discrete Cheeger inequality would be a landmark reusable well outside this series (spectral graph theory, expanders); the eigenvalue and Rayleigh-quotient layer built here is what Missions IX (tree relaxation, block dynamics) and XI (cutoff criterion) consume.

Difficulty

Everything routes through one change of basis: conjugating PPP by the diagonal matrix with entries π(x)\sqrt{\pi(x)}π(x)​ produces a matrix that is symmetric precisely because the chain is reversible, so Mathlib's spectral theorem applies — but transporting the resulting eigenbasis back to ℓ2(π)\ell^2(\pi)ℓ2(π), keeping track of orthonormality with respect to the weighted inner product, is a genuine formal-linear-algebra project; nothing about it is deep, all of it is fussy. The definitions of λ2\lambda_2λ2​ and λ⋆\lambda_\starλ⋆​ as suprema over the set of non-unit eigenvalues (finite, and nonempty once ∣V∣≥2|V|\ge2∣V∣≥2) must be reconciled with the eigenbasis enumeration before any variational argument runs. The upper half of Cheeger is direct from the variational characterization — test it on the indicator function of a bottleneck set SSS, recentred to have mean zero; the lower half is the hard half: the standard proof takes an optimal fff, decomposes it over its level sets {f>c}\{f>c\}{f>c}, and applies Cauchy–Schwarz twice, and formalizing that level-set sweep is the main effort of the mission. Wilson's method needs a supermartingale-style iteration of the eigenfunction estimate; its constants are exact, so the inequalities cannot be rounded.

Formalization scope

Eigenvalues are defined by real eigenvectors (∃f≠0, Pf=λf\exists f\ne0,\ Pf=\lambda f∃f=0, Pf=λf); for reversible chains this captures the whole spectrum, and all statements assume reversibility wherever the book does. λ2\lambda_2λ2​ and λ⋆\lambda_\starλ⋆​ are suprema of explicit sets of reals; on a one-point space these sets are empty and the supremum takes a junk value, so the affected statements carry the explicit hypothesis ∣V∣≥2|V|\ge2∣V∣≥2, matching the book's implicit assumption of a non-degenerate chain. trel=(1−λ⋆)−1t_{\mathrm{rel}}=(1-\lambda_\star)^{-1}trel​=(1−λ⋆​)−1 with total inverse. Theorem 12.3 carries an explicit +1+1+1 absorbing the rounding of a real-valued bound to an integer time. The cycle eigenvalue statement exhibits eigenvalues (existence of eigenfunctions); completeness of that list is not asserted. The variational characterization asserts both the minimization identity and its attainment, so it can be used in either direction.

Welcome contributions: the symmetrization API (conjugation by diag(π)\mathrm{diag}(\sqrt{\pi})diag(π​)), Rayleigh-quotient lemmas, level-set (layer-cake) infrastructure — all reused by Missions IX and XI.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • M. Jerrum, A. Sinclair, Approximating the permanent, SIAM J. Comput. 18 (1989). https://doi.org/10.1137/0218077
  • G. F. Lawler, A. D. Sokal, Bounds on the L² spectrum for Markov chains and Markov processes, Trans. Amer. Math. Soc. 309 (1988). https://doi.org/10.1090/S0002-9947-1988-0930082-9
  • D. B. Wilson, Mixing times of lozenge tiling and card shuffling Markov chains, Ann. Appl. Probab. 14 (2004). https://doi.org/10.1214/aoap/1042765669
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Markov ChainStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times IV: Lower Bounds on Mixing TimesTextbook

Motivation

Missions II–III produce upper bounds on mixing times. Whether such a bound is sharp is a different question: an O(n2)O(n^2)O(n2) bound on a chain that actually mixes in nlog⁡nn\log nnlogn steps hides the truth. Chapter 7 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) develops the standard toolkit of lower bounds: the counting and diameter bounds (a chain cannot spread faster than its transition graph allows), the bottleneck ratio (a chain cannot mix faster than it crosses its worst cut), and distinguishing statistics (a chain is far from stationarity as long as some statistic separates Pt(x,⋅)P^t(x,\cdot)Pt(x,⋅) from π\piπ by several standard deviations). The bottleneck bound — closely related to the conductance of the chain and, via Mission VII, to the Cheeger inequality — is the single most important obstruction result in the subject: it is how slow mixing (torpid mixing of Ising at low temperature, in Mission IX) is proved.

Setting

For a chain PPP with stationary distribution π\piπ, the edge measure is Q(x,y)=π(x)P(x,y)Q(x,y)=\pi(x)P(x,y)Q(x,y)=π(x)P(x,y), the bottleneck ratio of a set SSS of states is

Φ(S)=Q(S,Sc)π(S),Q(S,Sc)=∑x∈S, y∉Sπ(x)P(x,y),\Phi(S)=\frac{Q(S,S^{c})}{\pi(S)},\qquad Q(S,S^c)=\sum_{x\in S,\,y\notin S}\pi(x)P(x,y),Φ(S)=π(S)Q(S,Sc)​,Q(S,Sc)=x∈S,y∈/S∑​π(x)P(x,y),

and the bottleneck ratio of the chain is Φ⋆=min⁡{Φ(S):π(S)≤12, S≠∅}\Phi_\star=\min\{\Phi(S):\pi(S)\le\tfrac12,\ S\neq\varnothing\}Φ⋆​=min{Φ(S):π(S)≤21​, S=∅}. The maximal one-step out-degree is Δ=max⁡x∣{y:P(x,y)>0}∣\Delta=\max_x|\{y:P(x,y)>0\}|Δ=maxx​∣{y:P(x,y)>0}∣; the diameter is measured in the graph joining x≠yx\ne yx=y when P(x,y)+P(y,x)>0P(x,y)+P(y,x)>0P(x,y)+P(y,x)>0. For a statistic f:V→Rf:V\to\mathbb Rf:V→R and distribution μ\muμ, Eμ(f)\mathbb E_\mu(f)Eμ​(f) and Var⁡μ(f)\operatorname{Var}_\mu(f)Varμ​(f) are the finite-sum expectation and variance, and μf−1\mu f^{-1}μf−1 denotes the pushforward of μ\muμ under fff.

Formalization targets

Goal

tmix  ≥  14Φ⋆.t_{\mathrm{mix}}\;\ge\;\frac{1}{4\Phi_\star}.tmix​≥4Φ⋆​1​.

This is Theorem 7.3, the bottleneck-ratio lower bound, the chapter's central theorem.

Milestones

The counting bound tmix(ε)≥log⁡(∣V∣(1−ε))/log⁡Δt_{\mathrm{mix}}(\varepsilon)\ge\log\bigl(|V|(1-\varepsilon)\bigr)/\log\Deltatmix​(ε)≥log(∣V∣(1−ε))/logΔ for chains with uniform stationary distribution (§7.1.1, display (7.2)); the diameter bound: any two states satisfy dist(x0,y0)≤2 tmix(ε)\mathrm{dist}(x_0,y_0)\le 2\,t_{\mathrm{mix}}(\varepsilon)dist(x0​,y0​)≤2tmix​(ε) for ε<1/2\varepsilon<1/2ε<1/2 (§7.1.2, display (7.3)); Proposition 7.8 (a statistic separating means by rrr standard deviations forces ∥μ−ν∥TV≥1−4/(4+r2)\|\mu-\nu\|_{\mathrm{TV}}\ge1-4/(4+r^2)∥μ−ν∥TV​≥1−4/(4+r2)); Lemma 7.9 (projection under a statistic does not increase TV distance); Proposition 7.13 (the lazy hypercube walk satisfies d(12nlog⁡n−αn)≥1−8e1−2αd(\tfrac12 n\log n-\alpha n)\ge 1-8e^{1-2\alpha}d(21​nlogn−αn)≥1−8e1−2α); and Proposition 7.14 (the top-to-random shuffle needs nlog⁡n−O(n)n\log n-O(n)nlogn−O(n) shuffles, matching the upper bound of Mission III).

Significance

The results. Together with Mission III this pins the top-to-random shuffle at nlog⁡n±O(n)n\log n\pm O(n)nlogn±O(n) — the first sharp mixing result of the series, and the prototype of the cutoff phenomenon formalized in Mission XI. Proposition 7.13 similarly matches the hypercube upper bound and feeds the cutoff analysis. The bottleneck bound is used in Mission IX to prove exponentially slow mixing of the mean-field Ising model at low temperature, and its two-sided refinement is the Cheeger inequality of Mission VII.

Formalizing them. Mathlib has no notion of conductance/bottleneck ratio of a chain, no distinguishing-statistic method, and no mixing-time lower bound of any kind. The pushforward and variance infrastructure over finitely supported distributions is elementary but new, and reusable wherever second-moment methods appear (Wilson's method in Mission VII).

Difficulty

The bottleneck theorem's proof is short but exact: it hinges on the identity π(S)∥μSP−μS∥TV=Q(S,Sc)\pi(S)\|\mu_S P-\mu_S\|_{\mathrm{TV}}=Q(S,S^c)π(S)∥μS​P−μS​∥TV​=Q(S,Sc) for π\piπ conditioned on SSS, followed by a telescoping estimate of ∥μSPt−μS∥TV\|\mu_S P^t-\mu_S\|_{\mathrm{TV}}∥μS​Pt−μS​∥TV​; the formal cost is manipulating conditioned measures and one-sided TV sums (Remark 4.3 from Mission II). For Proposition 7.8, the second-moment argument runs through Chebyshev on both distributions plus optimization of a threshold — the constants 4/(4+r2)4/(4+r^2)4/(4+r2) are exact, not asymptotic, so the formal inequalities must be done carefully. Proposition 7.13 requires the binomial mean/variance computation for Hamming weight under both π\piπ and Pt(1,⋅)P^t(\mathbf 1,\cdot)Pt(1,⋅), including the negative-correlation bound for unrefreshed coordinates. The naive route to a lower bound — "the chain has not left a small set, so it is far from π\piπ" — is precisely the counting bound and is too weak for the sharp results; the statistics method is what closes the gap.

Formalization scope

Φ⋆\Phi_\starΦ⋆​ is an infimum over the subtype of nonempty sets with π(S)≤12\pi(S)\le\tfrac12π(S)≤21​; on a one-point space this subtype is empty and the infimum takes a junk value, making the goal trivially true there (the bound carries content only for ∣V∣≥2|V|\ge2∣V∣≥2, as in the book). The counting bound divides by log⁡Δ\log\DeltalogΔ with total division (Δ≤1\Delta\le1Δ≤1 gives a trivially true statement). The diameter bound is stated for arbitrary pairs of states through SimpleGraph.dist of the transition graph, which subsumes the book's diameter formulation. Propositions 7.13 and 7.14 are stated for all integer times t≤12nlog⁡n−αnt\le\frac12 n\log n-\alpha nt≤21​nlogn−αn (resp. t≤nlog⁡n−αnt\le n\log n-\alpha nt≤nlogn−αn), using monotonicity of ddd instead of evaluating at a real-valued time — this avoids floor artifacts while keeping the book's content. Proposition 7.14 quantifies "α\alphaα large, then nnn large" exactly as the book's iterated limit.

Welcome contributions: monotonicity of d(t)d(t)d(t) in ttt; conditioned-measure lemmas; variance API for distExp/distVar.

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • M. Jerrum, A. Sinclair, Approximating the permanent, SIAM J. Comput. 18 (1989). https://doi.org/10.1137/0218077
  • D. Aldous, P. Diaconis, Shuffling cards and stopping times, Amer. Math. Monthly 93 (1986). https://doi.org/10.1080/00029890.1986.11971821
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Markov ChainStochastic Systems·Captain: Shuze Chen

Markov Chains and Mixing Times III: Coupling and Strong Stationary TimesTextbook

Motivation

The Convergence Theorem of Mission II says an irreducible aperiodic chain mixes geometrically, but with constants coming from a crude Doeblin decomposition — useless for actual chains, whose state spaces are exponentially large. Chapters 5–6 of Levin–Peres–Wilmer, Markov Chains and Mixing Times (AMS, 2009) develop the two classic probabilistic techniques that give useful upper bounds: coupling — run two copies of the chain jointly so that they meet quickly, and read a TV bound off the meeting time — and strong stationary times — random times at which the chain is exactly stationary, independent of the time. The flagship application is the top-to-random shuffle: repeatedly take the top card of a deck of nnn cards and reinsert it at a uniform position; the deck is well mixed after nlog⁡n+cnn\log n + cnnlogn+cn shuffles, with error at most e−ce^{-c}e−c.

Setting

A Markovian coupling of a chain PPP (with the stay-together convention (5.2)) is a chain QQQ on pairs whose coordinate marginals are both PPP and which moves diagonal states to diagonal states. The coupling time τcouple\tau_{\mathrm{couple}}τcouple​ is the hitting time of the diagonal; its tails are expressed with the trajectory calculus of Mission I.

A randomized stopping time is presented by its stopping rule: for each time ttt and trajectory prefix ω\omegaω, a number st(ω)∈[0,1]s_t(\omega)\in[0,1]st​(ω)∈[0,1], the conditional probability of stopping at ttt given the trajectory so far and no earlier stop. A strong stationary time for the chain started at xxx is an almost surely finite such τ\tauτ with

Px{τ=t, Xτ=y}=Px{τ=t} π(y),\mathbb P_x\{\tau=t,\ X_\tau=y\}=\mathbb P_x\{\tau=t\}\,\pi(y),Px​{τ=t, Xτ​=y}=Px​{τ=t}π(y),

i.e. Xτ∼πX_\tau\sim\piXτ​∼π independent of τ\tauτ. The separation distance is sx(t)=max⁡y [1−Pt(x,y)/π(y)]s_x(t)=\max_y\,[1-P^t(x,y)/\pi(y)]sx​(t)=maxy​[1−Pt(x,y)/π(y)].

The mission also fixes the concrete chains it bounds: the lazy walk on the discrete torus Znd\mathbb Z_n^dZnd​, the Metropolis chain on proper qqq-colorings of a graph, the Glauber dynamics of the hardcore model with fugacity λ\lambdaλ, and the top-to-random shuffle on decks of nnn cards (states are arrangements, i.e. permutations; position 000 is the top).

Formalization targets

Goal

Let d(t)=max⁡x∥Pt(x,⋅)−π∥TVd(t)= \max_x\|P^t (x,\cdot)−\pi\|_{TV}d(t)=maxx​∥Pt(x,⋅)−π∥TV​,

d(⌈nlog⁡n+αn⌉)  ≤  e−α(α>0)d\bigl(\lceil n\log n+\alpha n\rceil\bigr)\;\le\;e^{-\alpha}\qquad(\alpha>0)d(⌈nlogn+αn⌉)≤e−α(α>0)

for the top-to-random shuffle on n≥2n\ge2n≥2 cards — display (6.16) of the book, the chapter's flagship bound, proved by combining the strong stationary time τtop\tau_{\mathrm{top}}τtop​ with the coupon collector tail of Mission I.

Milestones

Theorem 5.2 and Corollary 5.3 (the coupling bound: ∥Pt(x,⋅)−Pt(y,⋅)∥TV≤Px,y{τcouple>t}\|P^t(x,\cdot)-P^t(y,\cdot)\|_{\mathrm{TV}}\le\mathbb P_{x,y}\{\tau_{\mathrm{couple}}>t\}∥Pt(x,⋅)−Pt(y,⋅)∥TV​≤Px,y​{τcouple​>t}, hence d(t)≤max⁡x,yPx,y{τcouple>t}d(t)\le\max_{x,y}\mathbb P_{x,y}\{\tau_{\mathrm{couple}}>t\}d(t)≤maxx,y​Px,y​{τcouple​>t}); Theorem 5.5 (tmix(ε)≤c(d) n2log⁡2ε−1t_{\mathrm{mix}}(\varepsilon)\le c(d)\,n^2\log_2\varepsilon^{-1}tmix​(ε)≤c(d)n2log2​ε−1 for the lazy torus walk); Theorem 5.7 (Metropolis colorings, q>3Δq>3\Deltaq>3Δ: mixing in O(nlog⁡n)O(n\log n)O(nlogn)); Theorem 5.8 (hardcore Glauber, λ<(Δ−1)−1\lambda<(\Delta-1)^{-1}λ<(Δ−1)−1: mixing in O(nlog⁡n)O(n\log n)O(nlogn)); Proposition 6.1 with Example 6.7 (τtop\tau_{\mathrm{top}}τtop​ is a strong stationary time); Lemma 6.11 (sx(t)≤Px{τ>t}s_x(t)\le\mathbb P_x\{\tau>t\}sx​(t)≤Px​{τ>t}); Lemma 6.13 (∥Pt(x,⋅)−π∥TV≤sx(t)\|P^t(x,\cdot)-\pi\|_{\mathrm{TV}}\le s_x(t)∥Pt(x,⋅)−π∥TV​≤sx​(t)); Proposition 6.10 (d(t)≤max⁡xPx{τ>t}d(t)\le\max_x\mathbb P_x\{\tau>t\}d(t)≤maxx​Px​{τ>t}).

Significance

The results. The coupling bound is the single most used upper-bound technique in the subject: Missions VIII (path coupling), IX (Ising) and XI (cutoff examples) all instantiate it. Strong stationary times and separation distance return in Mission XI (separation cutoff) and underlie perfect sampling in Mission XIII. The three concrete bounds (torus, colorings, hardcore) are the standard first applications and give the first polynomial mixing results of the series; the colorings and hardcore chains are the objects of intense ongoing research on sampling thresholds.

Formalizing them. Nothing here exists in Mathlib. The novel infrastructure is the stopping-rule formalization of randomized stopping times over trajectory prefixes — measure-theory-free, but expressive enough for the strong stationarity identity — and the Markovian-coupling predicate on pair chains. Both are reused later in the series (Matthews method, cutoff, CFTP).

Difficulty

The coupling bound itself is short once Proposition 4.7 (Mission II) is available; the work is in the applications. For the torus, the coordinatewise coupling requires assembling ddd one-dimensional couplings and bounding the coupling time by a sum of one-dimensional meeting times — the formal bookkeeping of "couple coordinate by coordinate" is the real cost, and the constant c(d)c(d)c(d) absorbs it. For Theorem 5.7 and 5.8 the argument is a grand coupling over all colorings/configurations simultaneously; the formal statements quantify only over the resulting bound, but a solver must build the coupling. For Proposition 6.1, the crux is the induction "given kkk cards under the original bottom card, all k!k!k! orders are equally likely" — an exchangeability argument that must be carried through the stopping-rule encoding. Lemma 6.11 is where the definition of strong stationarity does its work; the naive attempt to prove Proposition 6.10 directly from the coupling characterization fails, which is exactly why separation distance is introduced.

Formalization scope

Couplings of chains are transition matrices on V×VV\times VV×V with marginal conditions stated row by row; the stay-together convention is part of the predicate, matching (5.2). Stopping rules take the trajectory prefix (which includes the starting state), so times "depending on the starting position" are covered; strong stationarity packages the stopping rule bounds, almost-sure finiteness (∑tPx{τ=t}=1\sum_t\mathbb P_x\{\tau=t\}=1∑t​Px​{τ=t}=1), and the product identity. The colorings chain lives on the subtype of proper colorings; the hardcore chain is the Glauber dynamics of Mission II restricted to the subtype of hardcore configurations (transitions never leave it). Mixing-time upper bounds carry an explicit +1+1+1 for integer rounding where the book's real-valued display would otherwise be false for the integer-valued tmixt_{\mathrm{mix}}tmix​. The torus statement fixes ε≤1/2\varepsilon\le 1/2ε≤1/2; for ε\varepsilonε near 111 the display is false as stated in the book.

Welcome contributions: interface lemmas between setAvoidTailProb of the pair chain and the two coordinates; the taboo-matrix form of coupling-time tails; exchangeability infrastructure for the deck chains (reused in Mission V).

Selected references

  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009. https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf
  • D. Aldous, P. Diaconis, Shuffling cards and stopping times, Amer. Math. Monthly 93 (1986). https://doi.org/10.1080/00029890.1986.11971821
  • P. Diaconis, J. A. Fill, Strong stationary times via a new form of duality, Ann. Probab. 18 (1990). https://doi.org/10.1214/aop/1176990628
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Bandit AlgorithmsMachine LearningReinforcement Learning·Captain: mikedeng1

Provably Efficient Reinforcement Learning with Linear Function Approximation 1: LSVI-UCB Has Regret O(√(d³H³Tι²)) with Probability 1 − p on Linear MDPsResearch Paper

Motivation

Reinforcement learning with large or continuous state spaces is done in practice with function approximation: the agent represents value functions in a low-dimensional parametric family instead of a table indexed by states. For tabular Markov decision processes, regret bounds of order H2SAT\sqrt{H^2SAT}H2SAT​ have been known since the work on UCRL and UCBVI, but they scale with the number of states SSS and actions AAA and say nothing when SSS is infinite. Before 2019, provable guarantees for function approximation either needed a simulator, assumed deterministic transitions, or had regret exponential in the horizon.

Jin, Yang, Wang and Jordan, Provably Efficient Reinforcement Learning with Linear Function Approximation (arXiv:1907.05388, COLT 2020), identified a model, the linear MDP, in which an optimistic version of least-squares value iteration has regret polynomial in the feature dimension ddd and the horizon HHH and independent of SSS and AAA. The model and the algorithm, LSVI-UCB, became a standard reference point for the theory of RL with function approximation.

Timeline:

  • 2017–2018: Azar, Osband, Munos (arXiv:1703.05449) and Jin, Allen-Zhu, Bubeck, Jordan (arXiv:1807.03765) give near-optimal T\sqrt TT​ regret for tabular episodic MDPs.
  • 2019: Yang and Wang (arXiv:1902.04779) study linear transition models with a simulator; Jin, Yang, Wang, Jordan prove Theorem 3.1 below without a simulator.
  • 2020: Zanette, Lazaric, Kochenderfer, Brunskill (arXiv:2003.00153) improve the dependence on ddd under a low inherent Bellman error assumption.

Setting

An episodic MDP MDP(S,A,H,P,r)\mathrm{MDP}(\mathcal S,\mathcal A,H,\mathbb P,r)MDP(S,A,H,P,r) has a measurable state space S\mathcal SS, a finite action set A\mathcal AA, a horizon HHH, transition kernels Ph(⋅∣x,a)\mathbb P_h(\cdot\mid x,a)Ph​(⋅∣x,a) and deterministic rewards rh(x,a)∈[0,1]r_h(x,a)\in[0,1]rh​(x,a)∈[0,1] for steps h=1,…,Hh=1,\dots,Hh=1,…,H. A policy π(x,h)\pi(x,h)π(x,h) chooses an action at each state and step. Its value functions satisfy the Bellman equation Qhπ=rh+PhVh+1πQ^\pi_h=r_h+\mathbb P_hV^\pi_{h+1}Qhπ​=rh​+Ph​Vh+1π​, Vhπ(x)=Qhπ(x,π(x,h))V^\pi_h(x)=Q^\pi_h(x,\pi(x,h))Vhπ​(x)=Qhπ​(x,π(x,h)), VH+1π=0V^\pi_{H+1}=0VH+1π​=0, where PhV(x,a)=∫V dPh(⋅∣x,a)\mathbb P_hV(x,a)=\int V\,d\mathbb P_h(\cdot\mid x,a)Ph​V(x,a)=∫VdPh​(⋅∣x,a); the optimal values Vh⋆V^\star_hVh⋆​, Qh⋆Q^\star_hQh⋆​ satisfy the same recursion with a maximum over actions.

The MDP is linear (Assumption A) with feature map ϕ:S×A→Rd\phi:\mathcal S\times\mathcal A\to\mathbb R^dϕ:S×A→Rd if ∥ϕ∥≤1\|\phi\|\le1∥ϕ∥≤1 and for each step there are signed measures μh=(μh(1),…,μh(d))\boldsymbol\mu_h=(\mu_h^{(1)},\dots,\mu_h^{(d)})μh​=(μh(1)​,…,μh(d)​) and a vector θh\theta_hθh​ with

Ph(⋅∣x,a)=⟨ϕ(x,a),μh(⋅)⟩,rh(x,a)=⟨ϕ(x,a),θh⟩,\mathbb P_h(\cdot\mid x,a)=\langle\phi(x,a),\boldsymbol\mu_h(\cdot)\rangle,\qquad r_h(x,a)=\langle\phi(x,a),\theta_h\rangle,Ph​(⋅∣x,a)=⟨ϕ(x,a),μh​(⋅)⟩,rh​(x,a)=⟨ϕ(x,a),θh​⟩,

and ∥θh∥≤d\|\theta_h\|\le\sqrt d∥θh​∥≤d​, ∥(∣μh(1)∣(S),…,∣μh(d)∣(S))∥≤d\|(|\mu_h^{(1)}|(\mathcal S),\dots,|\mu_h^{(d)}|(\mathcal S))\|\le\sqrt d∥(∣μh(1)​∣(S),…,∣μh(d)​∣(S))∥≤d​.

In each episode k=1,…,Kk=1,\dots,Kk=1,…,K an adversary chooses the initial state x1kx^k_1x1k​; the agent then plays HHH steps, the next state xh+1kx^k_{h+1}xh+1k​ being drawn from Ph(⋅∣xhk,ahk)\mathbb P_h(\cdot\mid x^k_h,a^k_h)Ph​(⋅∣xhk​,ahk​). LSVI-UCB (Algorithm 1) computes, backwards over hhh, the Gram matrix Λhk=∑τ<kϕhτ(ϕhτ)⊤+λI\Lambda^k_h=\sum_{\tau<k}\phi^\tau_h(\phi^\tau_h)^\top+\lambda IΛhk​=∑τ<k​ϕhτ​(ϕhτ​)⊤+λI of the past features ϕhτ=ϕ(xhτ,ahτ)\phi^\tau_h=\phi(x^\tau_h,a^\tau_h)ϕhτ​=ϕ(xhτ​,ahτ​), the ridge-regression weight whkw^k_hwhk​ for the targets rh+max⁡aQh+1kr_h+\max_aQ^k_{h+1}rh​+maxa​Qh+1k​, and the optimistic estimate

Qhk(x,a)=min⁡{(whk)⊤ϕ(x,a)+βϕ(x,a)⊤(Λhk)−1ϕ(x,a), H},Q^k_h(x,a)=\min\Big\{(w^k_h)^\top\phi(x,a)+\beta\sqrt{\phi(x,a)^\top(\Lambda^k_h)^{-1}\phi(x,a)},\ H\Big\},Qhk​(x,a)=min{(whk​)⊤ϕ(x,a)+βϕ(x,a)⊤(Λhk​)−1ϕ(x,a)​, H},

and then plays greedily with respect to QhkQ^k_hQhk​. Its policy in episode kkk is πk\pi_kπk​, and the regret is

Regret(K)=∑k=1K[V1⋆(x1k)−V1πk(x1k)],T=KH.\mathrm{Regret}(K)=\sum_{k=1}^K\big[V^\star_1(x^k_1)-V^{\pi_k}_1(x^k_1)\big],\qquad T=KH.Regret(K)=k=1∑K​[V1⋆​(x1k​)−V1πk​​(x1k​)],T=KH.

Formalization targets

Goal: Theorem 3.1

There are absolute constants c,C>0c,C>0c,C>0 such that for every linear MDP, every p∈(0,1)p\in(0,1)p∈(0,1) and every run of LSVI-UCB with λ=1\lambda=1λ=1 and β=c⋅dHι\beta=c\cdot dH\sqrt\iotaβ=c⋅dHι​, ι=log⁡(2dT/p)\iota=\log(2dT/p)ι=log(2dT/p),

P(Regret(K)≤Cd3H3Tι2)≥1−p.\mathbb P\Big(\mathrm{Regret}(K)\le C\sqrt{d^3H^3T\iota^2}\Big)\ge1-p .P(Regret(K)≤Cd3H3Tι2​)≥1−p.

Milestones

The milestones follow Appendix B of the paper: linearity of QπQ^\piQπ (Proposition 2.3) and the weight bounds (Lemmas B.1, B.2, with Lemma D.1); the covering bound for the value class (Lemma D.6, with the Euclidean-ball covering of Lemma D.5); the uniform self-normalized concentration (Lemma D.4, with Theorem D.3) and the good event (Lemma B.3); the error propagation (Lemma B.4), optimism (Lemma B.5) and the recursion (Lemma B.6); and the bonus-sum bound (17)–(18), with Lemma D.2. Lemma D.2, Theorem D.3 and Lemma D.5 are already on the platform and are referenced.

A companion statement, not a milestone, formalizes Proposition 5.1 (§5): on a finite state space with non-degenerate features, if the Bellman operators Thπ\mathbb T^\pi_hThπ​ of (8) map linear action-value functions to linear ones for every policy, then Ph\mathbb P_hPh​ is linear in ϕ\phiϕ.

Significance

The theorem shows that exploration with function approximation can be sample-efficient without a simulator: the regret depends on the intrinsic dimension ddd of the features and polynomially on HHH, not on the size of the state space. Its analysis, a uniform concentration bound over a data-dependent class of value functions combined with optimism, is the template for a large later literature: misspecified and low-rank MDPs, kernel and neural function approximation, and reward-free exploration.

The result has a published proof, but no machine-checked one. A formalization supplies the measure-theoretic episodic MDP on a general state space, an interaction protocol with adaptive initial states, the LSVI-UCB algorithm, and a checked chain from self-normalized martingale bounds to the regret theorem. The formal statements also record two points where the printed paper is imprecise: the normalization of the measures μh\boldsymbol\mu_hμh​ (see Formalization scope) and the existential reading of the weights in Lemma B.1.

Difficulty

The regression targets rh+max⁡aQh+1k(xh+1τ,⋅)r_h+\max_aQ^k_{h+1}(x^\tau_{h+1},\cdot)rh​+maxa​Qh+1k​(xh+1τ​,⋅) depend on all past data through Qh+1kQ^k_{h+1}Qh+1k​. The self-normalized bound for vector-valued martingales (Theorem D.3) therefore cannot be applied to them directly: the natural first idea, conditioning on the past and treating Vh+1kV^k_{h+1}Vh+1k​ as fixed, fails because Vh+1kV^k_{h+1}Vh+1k​ is not measurable with respect to the past at the time xh+1τx^\tau_{h+1}xh+1τ​ is drawn. The concentration must hold uniformly over a function class, which requires a covering-number bound for a class parametrized by vectors and matrices (Lemma D.6) and a union bound in the right scale.

A second difficulty is formal: the probabilistic protocol mixes an adversary, a learning algorithm reading its own past outputs, and transition kernels on a general measurable space, and the martingale argument (Azuma–Hoeffding over the KHKHKH steps) needs every object to be measurable with respect to the right σ-algebra.

Formalization scope

  • Model. S\mathcal SS is any measurable space; A\mathcal AA is a finite nonempty type with its discrete σ-algebra and a linear order used only to break ties in the argmax. Steps and episodes are 1-based. VπV^\piVπ, QπQ^\piQπ, V⋆V^\starV⋆, Q⋆Q^\starQ⋆ are defined by the Bellman recursions (1) and (2), with value 000 outside 1≤h≤H1\le h\le H1≤h≤H; theorems about general policies assume them measurable.
  • Assumption A is stated with the total-variation normalization ∥(∣μh(i)∣(S))i∥≤d\|(|\mu_h^{(i)}|(\mathcal S))_i\|\le\sqrt d∥(∣μh(i)​∣(S))i​∥≤d​ instead of the printed ∥μh(S)∥≤d\|\boldsymbol\mu_h(\mathcal S)\|\le\sqrt d∥μh​(S)∥≤d​; under the printed condition Lemma B.1 is false. The feature map is assumed measurable.
  • Runs. A run is a process on a probability space with a filtration over the flattened time (k−1)(H+1)+(h−1)(k-1)(H+1)+(h-1)(k−1)(H+1)+(h−1): states are adapted, actions are those of Algorithm 1, and the conditional law of xh+1kx^k_{h+1}xh+1k​ given the past is Ph(⋅∣xhk,ahk)\mathbb P_h(\cdot\mid x^k_h,a^k_h)Ph​(⋅∣xhk​,ahk​). The initial states are otherwise unrestricted.
  • Constants. ccc and CCC are quantified before the spaces, ddd, HHH, KKK, ppp, the MDP and the run; d,H,K≥1d,H,K\ge1d,H,K≥1 and p∈(0,1)p\in(0,1)p∈(0,1). "With probability 1−p1-p1−p" is an upper bound on the outer measure of the failure event.
  • Ruling out trivializations. The goal does not assume the good event, optimism, or any milestone conclusion; β\betaβ is fixed by the existentially quantified ccc, not free; the regret uses the model value of the greedy policy, not a realized return. A sorry-free check exhibits a linear MDP and a run satisfying all hypotheses.
  • Known gap. Algorithm 1 clips QhkQ^k_hQhk​ only from above, so the bound ∣Vh+1k∣≤H|V^k_{h+1}|\le H∣Vh+1k​∣≤H that Lemma B.3's proof needs (and the target bound in Lemma B.2's proof, here an explicit hypothesis) is not automatic off the good event. Lemma B.3 is stated as printed, for every cβ>0c_\beta>0cβ​>0; a solver who finds it unprovable should report this in the discussion.
  • Infrastructure needed: covering numbers of norm balls, the self-normalized martingale bound, Azuma–Hoeffding (in Mathlib), integration against signed measures, and measurability of the algorithm's outputs. The MDP and run definitions are reusable for other episodic RL results; contributions of general lemmas about them are welcome.

Selected references

  • C. Jin, Z. Yang, Z. Wang, M. I. Jordan, Provably Efficient Reinforcement Learning with Linear Function Approximation, COLT 2020; arXiv:1907.05388v2, 2019. https://arxiv.org/abs/1907.05388
  • Y. Abbasi-Yadkori, D. Pál, Cs. Szepesvári, Improved Algorithms for Linear Stochastic Bandits, NeurIPS 2011. https://papers.nips.cc/paper/2011/hash/e1d5be1c7f2f456670de3d53c7b54f4a-Abstract.html
  • M. G. Azar, I. Osband, R. Munos, Minimax Regret Bounds for Reinforcement Learning, ICML 2017. https://arxiv.org/abs/1703.05449
  • C. Jin, Z. Allen-Zhu, S. Bubeck, M. I. Jordan, Is Q-learning Provably Efficient?, NeurIPS 2018. https://arxiv.org/abs/1807.03765
  • L. F. Yang, M. Wang, Sample-Optimal Parametric Q-Learning Using Linearly Additive Features, ICML 2019. https://arxiv.org/abs/1902.04779
  • A. Zanette, A. Lazaric, M. Kochenderfer, E. Brunskill, Learning Near Optimal Policies with Low Inherent Bellman Error, ICML 2020. https://arxiv.org/abs/2003.00153
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Operations ResearchOptimizationStatistics·Captain: mikedeng1

Recovering Best Statistical Guarantees via the Empirical Divergence-Based Distributionally Robust Optimization 2: Empirical Burg-Ball DRO Bounds Converge Almost Surely to E[h(x;ξ)]Research Paper

Motivation

Many stochastic optimization models contain an expected-value constraint

Z0(x)=E0[h(x;ξ)]≤0,Z_0(x)=E_0[h(x;\xi)]\le 0,Z0​(x)=E0​[h(x;ξ)]≤0,

where ξ\xiξ is a random object with unknown law P0P_0P0​, xxx is a decision and hhh is a known loss. When P0P_0P0​ is known only through an i.i.d. sample ξ1,…,ξn\xi_1,\dots,\xi_nξ1​,…,ξn​, data-driven distributionally robust optimization (DRO) replaces E0E_0E0​ by the worst case over a ball of distributions around the data. H. Lam, Recovering Best Statistical Guarantees via the Empirical Divergence-Based Distributionally Robust Optimization (arXiv:1605.09349v1, 2016; Operations Research 67(4), 2019), studies a ball of reweightings of the sample itself, measured by the Burg entropy, and links its radius to empirical likelihood (Owen 2001).

Lam's Theorem 2 shows that, for a fixed decision xxx, the minimum and maximum of Ew[h(x;ξ)]E_w[h(x;\xi)]Ew​[h(x;ξ)] over this ball bracket Z0(x)Z_0(x)Z0​(x) with probability tending to 1−α1-\alpha1−α when the radius is χ1,1−α2/(2n)\chi^2_{1,1-\alpha}/(2n)χ1,1−α2​/(2n). Theorem 3, the goal of this mission, complements it: the two bounds also converge almost surely to Z0(x)Z_0(x)Z0​(x). A confidence statement says the robust bounds are rarely wrong; consistency says they are eventually tight, so that the robust constraint does not stay conservative as data accumulate.

This mission is the second of a three-mission series on the pointwise theory of the paper (1: coverage, Theorem 2; 3: reduction to a Burg ball on a finite support, Proposition 1).

Setting

Let ξ1,ξ2,…\xi_1,\xi_2,\dotsξ1​,ξ2​,… be i.i.d. random elements of a measurable space Ξ\XiΞ with law P0P_0P0​. Fix a decision x∈Rmx\in\mathbb R^mx∈Rm and write Z0(x)=E0[h(x;ξ)]Z_0(x)=E_0[h(x;\xi)]Z0​(x)=E0​[h(x;ξ)].

The Burg generator is ϕ(t)=−log⁡t+t−1\phi(t)=-\log t+t-1ϕ(t)=−logt+t−1 for t>0t>0t>0 and ϕ(t)=+∞\phi(t)=+\inftyϕ(t)=+∞ for t≤0t\le0t≤0. The empirical Burg-entropy divergence ball of radius η\etaη is the set of weight vectors

Un(η)={w∈Rn: −1n∑i=1nlog⁡(nwi)≤η, ∑i=1nwi=1, wi≥0}.\mathcal U_n(\eta)=\Big\{w\in\mathbb R^n:\ -\frac1n\sum_{i=1}^n\log(nw_i)\le\eta,\ \sum_{i=1}^nw_i=1,\ w_i\ge0\Big\}.Un​(η)={w∈Rn: −n1​i=1∑n​log(nwi​)≤η, i=1∑n​wi​=1, wi​≥0}.

On the simplex, −1n∑ilog⁡(nwi)=1n∑iϕ(nwi)-\frac1n\sum_i\log(nw_i)=\frac1n\sum_i\phi(nw_i)−n1​∑i​log(nwi​)=n1​∑i​ϕ(nwi​), the ϕ\phiϕ-divergence of www from the uniform weights.

Let 0<α<10<\alpha<10<α<1 and let q=χ1,1−α2q=\chi^2_{1,1-\alpha}q=χ1,1−α2​ be the (1−α)(1-\alpha)(1−α)-quantile of the χ12\chi^2_1χ12​ distribution. The lower and upper empirical DRO values are

Z‾n(x)=min⁡w∈Un(q/(2n))∑i=1nh(x;ξi)wi,Z‾n(x)=max⁡w∈Un(q/(2n))∑i=1nh(x;ξi)wi.\underline Z_n(x)=\min_{w\in\mathcal U_n(q/(2n))}\sum_{i=1}^nh(x;\xi_i)w_i,\qquad \overline Z_n(x)=\max_{w\in\mathcal U_n(q/(2n))}\sum_{i=1}^nh(x;\xi_i)w_i.Z​n​(x)=w∈Un​(q/(2n))min​i=1∑n​h(x;ξi​)wi​,Zn​(x)=w∈Un​(q/(2n))max​i=1∑n​h(x;ξi​)wi​.

The proof works with the centred observations h~i=h(x;ξi)−Z0(x)\tilde h_i=h(x;\xi_i)-Z_0(x)h~i​=h(x;ξi​)−Z0​(x).

Formalization targets

Goal: Theorem 3 (p. 12)

Under the conditions of Theorem 2 (0<Var0(h(x;ξ))<∞0<\mathrm{Var}_0(h(x;\xi))<\infty0<Var0​(h(x;ξ))<∞, Z0(x)Z_0(x)Z0​(x) finite),

Z‾n(x)→a.s.Z0(x)andZ‾n(x)→a.s.Z0(x)(n→∞).\underline Z_n(x)\xrightarrow{a.s.}Z_0(x)\quad\text{and}\quad\overline Z_n(x)\xrightarrow{a.s.}Z_0(x)\qquad(n\to\infty).Z​n​(x)a.s.​Z0​(x)andZn​(x)a.s.​Z0​(x)(n→∞).

Milestones (the steps of the printed proof, at a single decision)

  1. Lemma 3 (p. 38, Owen's Lemma 11.2): for i.i.d. YiY_iYi​ with EYi2<∞EY_i^2<\inftyEYi2​<∞, max⁡1≤i≤n∣Yi∣=o(n1/2)\max_{1\le i\le n}|Y_i|=o(n^{1/2})max1≤i≤n​∣Yi​∣=o(n1/2) a.s.
  2. (75)–(76) (p. 33): the Lagrangian dual
Z‾n(x)−Z0(x)=min⁡λ≥0,γ −∑i=1nλnlog⁡(1−h~i+γλ)+λq2n−γ,\overline Z_n(x)-Z_0(x)=\min_{\lambda\ge0,\gamma}\ -\sum_{i=1}^n\frac{\lambda}{n}\log\Big(1-\frac{\tilde h_i+\gamma}{\lambda}\Big)+\lambda\frac{q}{2n}-\gamma ,Zn​(x)−Z0​(x)=λ≥0,γmin​ −i=1∑n​nλ​log(1−λh~i​+γ​)+λ2nq​−γ,

with the printed conventions at λ=0\lambda=0λ=0 and for arguments outside the domain of the logarithm. 3. The elementary inequality (p. 34): −log⁡(1−t)≤t+2t2-\log(1-t)\le t+2t^2−log(1−t)≤t+2t2 for ∣t∣≤1/2|t|\le1/2∣t∣≤1/2. 4. (77) (p. 34): if max⁡i∣h~i∣≤λ/2\max_i|\tilde h_i|\le\lambda/2maxi​∣h~i​∣≤λ/2 with λ>0\lambda>0λ>0, then

Z‾n(x)−Z0(x)≤1n∑i=1nh~i+2(1/n)∑ih~i2λ+λq2n.\overline Z_n(x)-Z_0(x)\le\frac1n\sum_{i=1}^n\tilde h_i+2\frac{(1/n)\sum_i\tilde h_i^2}{\lambda}+\lambda\frac{q}{2n}.Zn​(x)−Z0​(x)≤n1​i=1∑n​h~i​+2λ(1/n)∑i​h~i2​​+λ2nq​.
  1. The uniform-weight lower bound (p. 34): Z‾n(x)−Z0(x)≥1n∑ih~i\overline Z_n(x)-Z_0(x)\ge\frac1n\sum_i\tilde h_iZn​(x)−Z0​(x)≥n1​∑i​h~i​.

Milestones 2, 4 and 5 are deterministic statements about an arbitrary data vector; only Lemma 3 and the goal are probabilistic.

Significance

The result. Theorem 3 shows that the empirical DRO with the χ12\chi^2_1χ12​ calibration is a consistent estimator of the constraint function at every fixed decision, not only a confidence bound. Together with Theorem 2 it places the empirical Burg-ball DRO on the same footing as the classical normal-approximation confidence interval: correct asymptotic coverage and shrinkage to the truth. The deterministic bounds (76)–(77) are also reusable on their own: they control the worst-case reweighting of any finite sample by its first two empirical moments.

Formalizing it. The theorem is proved in the paper; no machine-checked proof is known. The mission asks for a formal proof of the printed argument, specialized to one decision. A closely related open target exists on the platform: GenEmpLik.Expansion.lemma_1 (Duchi, Glynn and Namkoong) states the expansion of the robust mean, sample mean plus ρsn2/n+o(n−1/2)\sqrt{\rho s_n^2/n}+o(n^{-1/2})ρsn2​/n​+o(n−1/2), for a smooth generator class under stationary ergodic data. Combined with the strong law it would give the upper half of Theorem 3, but it is a different statement with different hypotheses and is itself unproved, so it is not used as a milestone here.

Difficulty

The tempting argument, "the ball shrinks to the empirical distribution and the empirical mean converges", does not close by itself: h(x;ξ)h(x;\xi)h(x;ξ) is only square integrable, not bounded, and the maximizing weight shifts mass towards the largest observations, so the gap Z‾n(x)−1n∑ih(x;ξi)\overline Z_n(x)-\frac1n\sum_ih(x;\xi_i)Zn​(x)−n1​∑i​h(x;ξi​) has to be controlled against the extremes of the sample rather than by the size of the ball alone. The printed proof routes this through the convex dual (76). That step needs a constraint qualification, the conjugate of the Burg generator with its boundary conventions (an infinite value outside the domain of the logarithm, and the degenerate multiplier λ=0\lambda=0λ=0), and a choice of multiplier that dominates every centred observation while still letting all three terms of (77) vanish. The almost-sure statement then combines Lemma 3 with two strong laws on one event of full probability.

Formalization scope

  • Data. The sample ξ1,…,ξn\xi_1,\dots,\xi_nξ1​,…,ξn​ is ξ 0, …, ξ (n-1): a sequence of measurable maps that is independent (iIndepFun) and identically distributed (IdentDistrib with ξ 0). Z0(x)Z_0(x)Z0​(x) is the Bochner integral of h x ∘ ξ 0, and the moment conditions are MemLp (h x ∘ ξ 0) 2 (finite mean and variance) together with positive variance, which makes the integral the true mean.
  • Decision. The paper's x∈Θ⊂Rmx\in\Theta\subset\mathbb R^mx∈Θ⊂Rm is an arbitrary point of EuclideanSpace ℝ (Fin m); Θ\ThetaΘ plays no role in a pointwise statement and is dropped.
  • Quantile. qqq is pinned by N(0,1){y:y2≤q}=1−α\mathcal N(0,1)\{y:y^2\le q\}=1-\alphaN(0,1){y:y2≤q}=1−α, which determines it uniquely. The radius q/(2n)q/(2n)q/(2n) is passed as ρ=q/2\rho=q/2ρ=q/2 to the published GenEmpLik.Expansion.robustMean, whose ball has radius ρ/n\rho/nρ/n.
  • Values. Z‾n\overline Z_nZn​ is robustMean burg (q/2); Z‾n\underline Z_nZ​n​ is robustLower burg (q/2) from the frozen shared EmpiricalDRO.Coverage.Setting module, a real infimum over the same published ball (PhiDivRobust.Counterpart.probUncertaintySet). For n≥1n\ge1n≥1 the value sets are nonempty and bounded, so the real sSup/sInf are the attained maximum and minimum.
  • Divergence. burg is valued in EReal with +∞+\infty+∞ for t≤0t\le0t≤0, so a zero weight is excluded from the ball by an infinite divergence and never by a junk value of Real.log. The dual summand dualTerm is EReal-valued with the printed conventions: +∞+\infty+∞ for t≥λ>0t\ge\lambda>0t≥λ>0; 000 or +∞+\infty+∞ at λ=0\lambda=0λ=0.
  • Generalizations, disclosed. The deterministic milestones hold for every data vector; (76) is stated for every q>0q>0q>0 (the Slater point needs q>0q>0q>0), (77) for every λ>0\lambda>0λ>0 satisfying the hypothesis, and the uniform-weight bound for every radius ρ≥0\rho\ge0ρ≥0. In the goal, positive variance and the value of α\alphaα are kept as printed although the conclusion does not need them.
  • Ruled out. Junk logarithms at zero weights, a junk sSup/sInf of an empty value set, a free radius detached from the χ12\chi^2_1χ12​ quantile, and a dropped variance condition are all excluded by the encoding above. The paper's printed (75) writes Z‾n(x)\overline Z_n(x)Zn​(x) where its radius qn/(2n)q_n/(2n)qn​/(2n) makes it Z‾n∗(x)\overline Z^*_n(x)Zn∗​(x); at a single decision the two coincide.
  • Not posed. The paper's headline result, Theorem 4 (uniform coverage over Θ\ThetaΘ with a χ2\chi^2χ2-process quantile qnq_nqn​), and the uniform statements Theorems 5–7 need Donsker and Glivenko–Cantelli classes, weak convergence in ℓ∞(Θ)\ell^\infty(\Theta)ℓ∞(Θ) and conditional quantiles of Gaussian-process suprema, none of which has library support yet; they are left out.
  • Reuse. Lemma 3 for nonnegative variables is the proved platform theorem NumStochOpt.ListScheduling.lemma_8_1_i_max_over_sqrt_ae, included as a reference. Mathlib's ProbabilityTheory.strong_law_ae supplies the laws of large numbers. Contributions welcome: the duality (76) for general ϕ\phiϕ-divergence balls, and the deterministic bound (77).

Selected references

  • H. Lam, Recovering Best Statistical Guarantees via the Empirical Divergence-Based Distributionally Robust Optimization, arXiv:1605.09349v1, 2016; Operations Research 67(4), 2019. https://arxiv.org/abs/1605.09349v1 , https://doi.org/10.1287/opre.2018.1786
  • A. B. Owen, Empirical Likelihood, Chapman & Hall/CRC, 2001. https://doi.org/10.1201/9781420036152
  • A. Ben-Tal, D. den Hertog, A. De Waegenaere, B. Melenberg, G. Rennen, Robust solutions of optimization problems affected by uncertain probabilities, Management Science 59(2), 2013. https://doi.org/10.1287/mnsc.1120.1641
  • J. C. Duchi, P. W. Glynn, H. Namkoong, Statistics of robust optimization: a generalized empirical likelihood approach, Mathematics of Operations Research 46(3), 2021. https://arxiv.org/abs/1610.03425
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Mathematical PhysicsQuantum Information·Captain: Lucas

Hardy 2001 I: Five Reasonable Axioms — Degrees of Freedom K = N^rResearch Paper

Motivation

In the usual textbook presentation, quantum theory starts from postulates that have no obvious operational meaning: states are density operators on a complex Hilbert space, measurements are positive operators, and probabilities are given by the trace formula p=tr(A^ρ^)p=\mathrm{tr}(\hat A\hat\rho)p=tr(A^ρ^​). In Quantum Theory From Five Reasonable Axioms (Hardy 2001), Lucien Hardy asks whether this structure can instead be derived from simple statements about preparations, transformations and measurements, in the same way that classical probability theory can be set up by pure thought. He proposes five axioms (probabilities, simplicity, subspaces, composite systems, continuity) and argues that they single out finite- and countably-infinite-dimensional quantum theory. Dropping a single word, "continuous" in Axiom 5, leaves classical probability theory instead.

The paper is one of the starting points of the operational or generalized probabilistic theory (GPT) approach to the foundations of quantum mechanics. It was followed by reconstructions that replace the simplicity axiom, e.g. Dakić–Brukner 2009, Masanes–Müller 2011 and Chiribella–D'Ariano–Perinotti 2011.

Setting

A system is described by two integers. The dimension NNN is the maximum number of states that can be distinguished in a single-shot measurement. The number of degrees of freedom KKK is the minimum number of probability measurements needed to determine the state. The state is the vector p=(p1,…,pK)∈RKp=(p^1,\dots,p^K)\in\mathbb R^Kp=(p1,…,pK)∈RK of the probabilities of KKK fiducial measurements. States are not assumed normalized: the null state p=0p=0p=0 (no system present) is allowed. The set SSS of allowed states is convex, and its pure states are its extremal points other than 000.

The five axioms are:

  1. Probabilities. Relative frequencies converge to the same limit for every ensemble prepared by a given preparation.
  2. Simplicity. K=K(N)K=K(N)K=K(N) is a function of N=1,2,…N=1,2,\dotsN=1,2,…, and for each NNN it takes the minimum value consistent with the axioms.
  3. Subspaces. A system whose state is constrained to an MMM-dimensional subspace behaves like a system of dimension MMM.
  4. Composite systems. A composite of systems AAA and BBB has N=NANBN=N_AN_BN=NA​NB​ and K=KAKBK=K_AK_BK=KA​KB​.
  5. Continuity. Between any two pure states there is a continuous reversible transformation.

A probability theory can be summarized by its signature x=(x1,x2,… )x=(x_1,x_2,\dots)x=(x1​,x2​,…), defined through

K=Nx1+12!N(N−1)x2+13!N(N−1)(N−2)x3+⋯=∑k≥1(Nk)xk.K=Nx_1+\tfrac1{2!}N(N-1)x_2+\tfrac1{3!}N(N-1)(N-2)x_3+\cdots=\sum_{k\ge1}\binom Nk x_k .K=Nx1​+2!1​N(N−1)x2​+3!1​N(N−1)(N−2)x3​+⋯=k≥1∑​(kN​)xk​.

Classical probability theory has x=(1,0,0,… )x=(1,0,0,\dots)x=(1,0,0,…) and K=NK=NK=N. Complex quantum theory has x=(1,2,0,… )x=(1,2,0,\dots)x=(1,2,0,…) and K=N2K=N^2K=N2. Real and quaternionic quantum theory have x=(1,1,0,… )x=(1,1,0,\dots)x=(1,1,0,…) and x=(1,4,0,… )x=(1,4,0,\dots)x=(1,4,0,…).

Formalization targets

Goal: K(N)=NrK(N)=N^rK(N)=Nr

Section 8.1 shows that Axiom 3 forces K(N+1)≥K(N)+1K(N+1)\ge K(N)+1K(N+1)≥K(N)+1, and Axiom 4 forces K(NANB)=K(NA)K(NB)K(N_AN_B)=K(N_A)K(N_B)K(NA​NB​)=K(NA​)K(NB​). The goal theorem is the purely arithmetic consequence (Eq. (57)):

K(N+1)≥K(N)+1  and  K(NANB)=K(NA)K(NB)  (N,NA,NB≥1)⟹∃r∈{1,2,3,… }: K(N)=Nr  ∀N≥1.K(N+1)\ge K(N)+1\ \text{ and }\ K(N_AN_B)=K(N_A)K(N_B)\ \ (N,N_A,N_B\ge1)\quad\Longrightarrow\quad \exists r\in\{1,2,3,\dots\}:\ K(N)=N^r\ \ \forall N\ge1 .K(N+1)≥K(N)+1  and  K(NA​NB​)=K(NA​)K(NB​)  (N,NA​,NB​≥1)⟹∃r∈{1,2,3,…}: K(N)=Nr  ∀N≥1.

Milestones

The milestones follow the paper's own steps, in the paper's numbering:

  • Appendix 2: a strictly increasing, completely multiplicative KKK on the positive integers satisfies K(n)=nαK(n)=n^\alphaK(n)=nα. Section 8.1: if every nαn^\alphanα is an integer, then α\alphaα is a positive integer.
  • Section 6.6 / Appendix 1: measured probabilities are linear in the state, pmeas=r⋅pp_{\rm meas}=r\cdot ppmeas​=r⋅p. Section 6.7: transformations act as matrices, p↦Zpp\mapsto Zpp↦Zp. Section 7: reversible transformations send pure states to pure states.
  • Section 4 / 8.5: in classical probability theory the pure states are exactly the NNN basis states, and no continuous path of pure states joins two distinct ones. The equations ∑k(pk)2=1\sum_k(p^k)^2=1∑k​(pk)2=1, 0≤pk≤10\le p^k\le10≤pk≤1, ∑kpk=1\sum_kp^k=1∑k​pk=1 force a basis vector.
  • Sections 5 and 8.1: the signatures of the classical, quantum, real, quaternionic and K=N3K=N^3K=N3 theories, and the failure of K=KAKBK=K_AK_BK=KA​KB​ for real (too many) and quaternionic (too few) composites.
  • Section 5: the N2N^2N2 projectors ∣n⟩⟨n∣|n\rangle\langle n|∣n⟩⟨n∣, ∣mn⟩x⟨mn∣|mn\rangle_x\langle mn|∣mn⟩x​⟨mn∣, ∣mn⟩y⟨mn∣|mn\rangle_y\langle mn|∣mn⟩y​⟨mn∣ are linearly independent over R\mathbb RR and span the Hermitian operators.
  • Sections 5 and 8.6 (N=2N=2N=2): the overlap formula (35) for ccc; det⁡D>0  ⟺  c−<c<c+\det D>0 \iff c_-<c<c_+detD>0⟺c−​<c<c+​; the decomposition rTDr′=v⃗ TAv⃗′+μμ′/2r^TDr'=\vec v^{\,T}A\vec v'+\mu\mu'/2rTDr′=vTAv′+μμ′/2; AAA positive definite   ⟺  c−<c<c+\iff c_-<c<c_+⟺c−​<c<c+​; the Bloch matrix (87).
  • Section 8.7 (N=3N=3N=3): the 9×99\times99×9 matrix Dij=tr(P^iP^j)D_{ij}=\mathrm{tr}(\hat P_i\hat P_j)Dij​=tr(P^i​P^j​) with h=1/2h=1/2h=1/2, q=1/4q=1/4q=1/4.

Significance

The goal is the step at which the two structural axioms (subspaces and composites) cut the space of possible theories down to a single integer parameter rrr. Combined with Section 8.5, which rules out r=1r=1r=1 by continuity, and with the simplicity axiom, it gives K=N2K=N^2K=N2. Everything after that in the paper (the Bloch sphere, general NNN, the trace formula, complete positivity) is carried out inside the K=N2K=N^2K=N2 case. The milestones on signatures make precise in which sense real and quaternionic quantum theory are excluded: their degree-of-freedom counts are not multiplicative under composition.

The paper's argument is informal physics. This mission isolates the mathematically precise statements that the argument relies on, so that they can be proved independently of the physical interpretation. It does not formalize the axioms themselves as a single Lean structure.

Difficulty

The arithmetic goal is an instance of a classical question about monotone completely multiplicative functions. Complete multiplicativity alone fixes KKK only through its values at the primes, which are a priori unrelated to one another, and monotonicity is the only link between different primes. The step from a real exponent α\alphaα to an integer exponent is a separate integrality argument that the paper does not spell out. The linearity milestones need care because the hypotheses hold only on a convex set containing 000, not on all of RK\mathbb R^KRK. The N=2N=2N=2 milestones are explicit but delicate algebra with square roots and boundary cases a,b∈{0,1}a,b\in\{0,1\}a,b∈{0,1}.

Formalization scope

  • All theorems live in the namespace HardyFiveAxioms. State vectors are functions Fin K → ℝ. Indices are 000-based, so the paper's fiducial vector kkk is index k−1k-1k−1.
  • K(N)K(N)K(N) is a function ℕ → ℕ (goal) or ℕ → ℝ (Appendix 2), constrained only at arguments ≥1\ge1≥1. The value at 000 is irrelevant.
  • The signature is a finite list [x₁, …, x_L], and 1k!N(N−1)⋯(N−k+1)\frac1{k!}N(N-1)\cdots(N-k+1)k!1​N(N−1)⋯(N−k+1) is written as the binomial coefficient (Nk)\binom Nk(kN​).
  • Pure states are Set.extremePoints ℝ S \ {0}. The classical state space is {p≥0, ∑npn≤1}\{p\ge0,\ \sum_np_n\le1\}{p≥0, ∑n​pn​≤1}.
  • The quantum projectors are explicit matrices vecMulVec v (star v) over ℂ, and the qubit matrices DDD, CCC, AAA and the roots c±c_\pmc±​ are explicit definitions.
  • Axiom 5's "continuous reversible transformation" enters only through the classical milestone, as a continuous path unitInterval → ℝᴺ that stays inside the pure states.
  • The goal does not assume the conclusion in disguise. Its hypotheses are the two consequences of Axioms 3 and 4 derived in Section 8.1. It is not vacuous: K(N)=NrK(N)=N^rK(N)=Nr satisfies both hypotheses for every r≥1r\ge1r≥1.

Contributions are welcome on any milestone. The linearity, extreme-point and positive-definiteness lemmas are reusable beyond this mission.

Selected references

  • L. Hardy, Quantum Theory From Five Reasonable Axioms, arXiv:quant-ph/0101012v4, 2001. https://arxiv.org/abs/quant-ph/0101012
  • B. Dakić, Č. Brukner, Quantum Theory and Beyond: Is Entanglement Special?, 2009. https://arxiv.org/abs/0911.0695
  • Ll. Masanes, M. P. Müller, A derivation of quantum theory from physical requirements, New J. Phys. 13, 063001, 2011. https://arxiv.org/abs/1004.1483
  • G. Chiribella, G. M. D'Ariano, P. Perinotti, Informational derivation of quantum theory, Phys. Rev. A 84, 012311, 2011. https://arxiv.org/abs/1011.6451
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Operations ResearchOptimization·Captain: mikedeng1

Consumer Returns Policies and Supply Chain Performance 1: With Valuations Learned after Purchase, the Seller's Optimal Policy Is p* = E max(V, s), F̄(q*) = (c − s)/(p* − s), r* = sResearch Paper

Motivation

Retailers accept large volumes of returned merchandise, and a common default is the full refund: a buyer who is unhappy with a product brings it back and gets the whole price back. Many consumers only learn how much they value a product after they have it at home — clothes that do not fit, a gadget that does not suit the buyer's needs. A returns policy therefore plays two roles at once. It raises the buyer's willingness to pay before purchase, and after purchase it decides which units stay with consumers and which go back to the seller to be salvaged.

Xuanming Su's paper Consumer Returns Policies and Supply Chain Performance (SSRN 1020451; published in Manufacturing & Service Operations Management 11(4), 2009, doi:10.1287/msom.1080.0240) puts this effect into a newsvendor model with random demand. The earlier literature it builds on, notably Che (1996) and Davis, Gerstner and Hagerty (1995), asked whether a seller should offer full refunds or no returns at all. Su's model makes the refund amount a separate decision variable. The answer it gives is closed-form and sharp: the optimal refund equals the salvage value. This mission formalizes Sections 3–4 of the paper: the single-seller model, the full-refund benchmark, and the optimal partial refund.

Setting

A seller stocks a quantity q≥0q \ge 0q≥0 before a selling season at unit cost ccc. Unsold and returned units are salvaged at value sss. Market demand is a nonnegative random variable XXX with law DDD, distribution function FFF and Fˉ=1−F\bar F = 1 - FFˉ=1−F. Each consumer who buys learns a valuation VVV after purchase. Valuations are i.i.d. with law ν\nuν and finite mean μ=EV\mu = EVμ=EV, and the standing assumption is μ>c>s≥0\mu > c > s \ge 0μ>c>s≥0.

The seller chooses a price ppp, a quantity qqq and a refund rrr. Once a consumer has bought, they keep the product if V≥rV \ge rV≥r and return it otherwise. The keep and return probabilities are

Gˉ(r)=P(V≥r),G(r)=P(V<r).\bar G(r) = \mathbb P(V \ge r), \qquad G(r) = \mathbb P(V < r).Gˉ(r)=P(V≥r),G(r)=P(V<r).

Before purchase a consumer's expected utility from buying is Emax⁡(V,r)E\max(V, r)Emax(V,r), so this is the reservation price. Every consumer buys if p≤Emax⁡(V,r)p \le E\max(V, r)p≤Emax(V,r) and nobody buys otherwise (the demand rule (6)). With Emin⁡(X,q)E\min(X, q)Emin(X,q) the expected sales of a stock qqq, the seller's expected profit (7)–(8) is

Π(p,q,r)=[(p−s)Gˉ(r)+(p−r)G(r)] Emin⁡(X,q)−(c−s)qif p≤Emax⁡(V,r),\Pi(p,q,r) = \big[(p-s)\bar G(r) + (p-r)G(r)\big]\,E\min(X,q) - (c-s)q \quad\text{if } p \le E\max(V,r),Π(p,q,r)=[(p−s)Gˉ(r)+(p−r)G(r)]Emin(X,q)−(c−s)qif p≤Emax(V,r),

and −(c−s)q-(c-s)q−(c−s)q otherwise. Two special cases serve as benchmarks. Under full refunds (r=pr = pr=p) every consumer buys and the profit is Πfull(p,q)=(p−s)Gˉ(p)Emin⁡(X,q)−(c−s)q\Pi_{\text{full}}(p,q) = (p-s)\bar G(p)E\min(X,q) - (c-s)qΠfull​(p,q)=(p−s)Gˉ(p)Emin(X,q)−(c−s)q, from (1)–(2). Under no returns the price is μ\muμ and the profit is Πno(q)=(μ−s)Emin⁡(X,q)−(c−s)q\Pi_{\text{no}}(q) = (\mu - s)E\min(X,q) - (c-s)qΠno​(q)=(μ−s)Emin(X,q)−(c−s)q, from (3). Social welfare (12)–(13) is the sum of consumer surplus and seller profit, SW(p,q,r)=∫[r,∞)(v−s) dν(v)⋅Emin⁡(X,q)−(c−s)qSW(p,q,r) = \int_{[r,\infty)}(v-s)\,d\nu(v)\cdot E\min(X,q) - (c-s)qSW(p,q,r)=∫[r,∞)​(v−s)dν(v)⋅Emin(X,q)−(c−s)q, again subject to the demand rule.

Formalization targets

Goal: Proposition 2 (p. 11)

With p∗=Emax⁡(V,s)p^* = E\max(V,s)p∗=Emax(V,s), r∗=sr^* = sr∗=s and any q∗q^*q∗ satisfying

Fˉ(q∗)=c−sEmax⁡(V,s)−s,\bar F(q^*) = \frac{c-s}{E\max(V,s) - s},Fˉ(q∗)=Emax(V,s)−sc−s​,

the triple (p∗,q∗,r∗)(p^*, q^*, r^*)(p∗,q∗,r∗) maximizes Π\PiΠ over all prices, all refunds and all quantities q≥0q \ge 0q≥0:

Π(p,q,r)≤Π(p∗,q∗,r∗).\Pi(p,q,r) \le \Pi(p^*, q^*, r^*).Π(p,q,r)≤Π(p∗,q∗,r∗).

Milestones

  1. The reservation price splits as Emax⁡(V,r)=rG(r)+∫[r,∞)v dνE\max(V,r) = rG(r) + \int_{[r,\infty)} v\,d\nuEmax(V,r)=rG(r)+∫[r,∞)​vdν, which is the step (28)→(29) of the proof (p. 26).
  2. At p=Emax⁡(V,r)p = E\max(V,r)p=Emax(V,r) the per-unit margin (p−s)Gˉ(r)+(p−r)G(r)(p-s)\bar G(r) + (p-r)G(r)(p−s)Gˉ(r)+(p−r)G(r) equals ∫[r,∞)(v−s) dν\int_{[r,\infty)}(v-s)\,d\nu∫[r,∞)​(v−s)dν, displays (27)–(30), p. 26.
  3. This integral is maximized at r=sr = sr=s (p. 26).
  4. Hence (Emax⁡(V,s),s)(E\max(V,s), s)(Emax(V,s),s) maximizes the margin subject to p≤Emax⁡(V,r)p \le E\max(V,r)p≤Emax(V,r), the first step of the proof (p. 26).
  5. The newsvendor critical fractile, a reference to a proved platform theorem (p. 26).
  6. Proposition 1(i) (p. 9): under full refunds, p∗∈arg⁡max⁡p(p−s)Gˉ(p)p^* \in \arg\max_p (p-s)\bar G(p)p∗∈argmaxp​(p−s)Gˉ(p) with Fˉ(q∗)=(c−s)/((p∗−s)Gˉ(p∗))\bar F(q^*) = (c-s)/((p^*-s)\bar G(p^*))Fˉ(q∗)=(c−s)/((p∗−s)Gˉ(p∗)) is optimal.
  7. Proposition 1(ii) at s=0s = 0s=0 (p. 26): with nonnegative valuations, no returns beats every full-refund policy.
  8. Corollary 1 (p. 12): the inequality (p−s)Gˉ(p)≤Emax⁡(V,s)−s(p-s)\bar G(p) \le E\max(V,s) - s(p−s)Gˉ(p)≤Emax(V,s)−s (p. 26), and its consequence that partial refunds earn at least the full-refund profit and, for strictly increasing FFF, stock at least as much.
  9. Corollary 2 (p. 13): the triple of Proposition 2 also maximizes social welfare.

Significance

The result separates two things that a full refund ties together: the price and the refund. Setting r=sr = sr=s sends every unit back to its more valuable use. Consumers who value the product above its salvage value keep it, and the rest return it to be salvaged. The price Emax⁡(V,s)E\max(V,s)Emax(V,s) then extracts the whole expected surplus. Consequences follow directly. Partial refunds dominate both full refunds and no returns (Corollary 1). They raise the stocking quantity, which benefits an upstream manufacturer paid per unit ordered. With valuation uncertainty resolved only after purchase, the monopoly outcome is welfare-maximizing (Corollary 2). Section 5 of the paper, formalized in the companion mission, uses Proposition 2's triple as the first-best target that supply chain contracts must implement.

The results are proved on paper with short arguments in Appendix A of the paper. None of them has a machine-checked proof. The mission's contribution is a formal model of consumer returns with the demand rule built in, plus checked versions of Propositions 1–2 and Corollaries 1–2 for general valuation laws (with atoms), not only densities.

Difficulty

The paper's proof treats the problem as separable: first maximize the margin over (p,r)(p, r)(p,r), then solve a newsvendor problem in qqq. Two steps that are routine on paper need care. First, the margin bound must hold over the whole constrained region p≤Emax⁡(V,r)p \le E\max(V, r)p≤Emax(V,r), including refunds above the price and negative prices. It rests on comparing ∫[r,∞)(v−s) dν\int_{[r,\infty)}(v-s)\,d\nu∫[r,∞)​(v−s)dν with ∫[s,∞)(v−s) dν\int_{[s,\infty)}(v-s)\,d\nu∫[s,∞)​(v−s)dν, which needs the closed half-line convention to hold up at atoms of ν\nuν. Second, the newsvendor step must be done for a demand law that may have atoms, where Fˉ\bar FFˉ has no inverse. Without the demand rule the problem is not separable at all: formula (8) alone is unbounded in ppp. Without nonnegativity of demand and quantity it is unbounded in the other direction.

Formalization scope

Lean represents all prices, refunds, costs, quantities and profits as real numbers. The valuation law is a probability measure ν on ℝ with integrable identity, so a density is not required. The demand law is a probability measure D on ℝ with D (Set.Iio 0) = 0. Gˉ(r)\bar G(r)Gˉ(r) is (ν (Set.Ici r)).toReal and G(r)G(r)G(r) is (ν (Set.Iio r)).toReal, following the page's tie rule (keep iff V≥rV \ge rV≥r). Emin⁡(X,q)E\min(X,q)Emin(X,q) is SupplyChainTheory.expSales D q from the published module SupplyChainTheory_contracts, and Fˉ\bar FFˉ is 1 - ProbabilityTheory.cdf D. Printed page numbers equal PDF page numbers throughout the source.

Committed conventions and readings:

  • Demand rule inside the objectives. Profit and welfare are zero-demand cash flows when p>Emax⁡(V,r)p > E\max(V,r)p>Emax(V,r).
  • Nonnegativity. Stocking quantities range over q≥0q \ge 0q≥0 and demand is nonnegative. Both are the page's words ("stocking quantity", "a mass of infinitesimal consumers"), and without them the profit is unbounded.
  • Salvage value. 0≤s0 \le s0≤s, as on p. 26.
  • Optimality, not uniqueness. Every optimum is stated as optimality of the page's closed-form triple. Uniqueness fails when ν\nuν has gaps: if ν\nuν puts no mass on [s,r)[s, r)[s,r), the refund rrr is optimal too.
  • No continuity of FFF for the goal. The goal assumes no continuity of FFF. Existence of q∗q^*q∗ is not claimed.
  • Corollary 1, quantity part. The quantity comparison assumes FFF strictly increasing on [0,∞)[0,\infty)[0,∞), which the proof's Fˉ−1\bar F^{-1}Fˉ−1 presumes. Without it the statement is false.
  • Proposition 1(ii) at s=0s = 0s=0. This case assumes nonnegative valuations. The "sufficiently low" form of Proposition 1(ii) is not formalized.

A trivializing formalization is ruled out: p∗p^*p∗ and r∗r^*r∗ are the explicit values Emax⁡(V,s)E\max(V,s)Emax(V,s) and sss, not an argmax chosen by Classical.choose. The maximization ranges over all (p,r)(p, r)(p,r) and all q≥0q \ge 0q≥0, not a set restricted to r=sr = sr=s. The returned-units cash flow (p−r+s)G(r)(p - r + s)G(r)(p−r+s)G(r) appears in the profit.

The newsvendor step reuses the proved platform theorem SupplyChainTheory.chain_optimal_fractile. The other pieces needed are elementary lemmas on integrals over half-lines and the concavity of q↦Emin⁡(X,q)q \mapsto E\min(X,q)q↦Emin(X,q). They are reusable for any newsvendor-type model. Proofs of any milestone, and a general-law newsvendor optimality lemma that does not need a continuous FFF, are welcome.

Selected references

  • X. Su, Consumer Returns Policies and Supply Chain Performance, SSRN working paper 1020451, version of August 2008. https://ssrn.com/abstract=1020451 — published in Manufacturing & Service Operations Management 11(4), 2009. https://doi.org/10.1287/msom.1080.0240
  • Y.-K. Che, Customer Return Policies for Experience Goods, Journal of Industrial Economics 44(1), 1996. https://doi.org/10.2307/2950560
  • S. Davis, E. Gerstner, M. Hagerty, Money Back Guarantees in Retailing: Matching Products to Consumer Tastes, Journal of Retailing 71(1), 1995. https://doi.org/10.1016/0022-4359(95)90010-1
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Algorithmic Game TheoryOperations Research·Captain: mikedeng1

Worst-Case Equilibria I: On Two Identical Parallel Links Every Mixed Nash Equilibrium Has Expected Makespan at Most 3/2 Times the OptimumResearch Paper

Motivation

When many users share a network and each routes its own traffic selfishly, the outcome is a Nash equilibrium rather than a centrally optimized assignment. Koutsoupias and Papadimitriou, in Worst-case equilibria (STACS 1999; journal version 2009), proposed to measure the loss caused by this lack of coordination by the worst-case ratio between the social cost of an equilibrium and the social optimum. The ratio, first called the coordination ratio and now the price of anarchy, became a central quantity of algorithmic game theory, studied for routing, scheduling, congestion games, auctions and network design.

The paper analyses the simplest setting in which the question is nontrivial: agents sending traffic over parallel links, which is the same as scheduling independent jobs on parallel machines with the jobs choosing their machines. For two identical links it determines the price of anarchy exactly.

Timeline.

  • 1999: Koutsoupias and Papadimitriou introduce the model and the measure; on two identical links the price of anarchy is 3/23/23/2, and on mmm identical links it is Ω(log⁡m/log⁡log⁡m)\Omega(\log m/\log\log m)Ω(logm/loglogm), with a nonmatching upper bound in the conference version.
  • 2002: Czumaj and Vöcking, and independently Koutsoupias, Mavronicolas and Spirakis, show that this lower bound is tight for mmm identical links, Θ(log⁡m/log⁡log⁡m)\Theta(\log m/\log\log m)Θ(logm/loglogm); Czumaj and Vöcking also give tight bounds for links of different speeds.

Setting

There are nnn agents and mmm identical parallel links. Agent iii has an amount of traffic wi>0w_i>0wi​>0 to send over one link. A pure profile s=(j1,…,jn)∈{1,…,m}ns=(j_1,\dots,j_n)\in\{1,\dots,m\}^ns=(j1​,…,jn​)∈{1,…,m}n assigns a link to each agent; the load of link jjj is ℓj(s)=∑k: jk=jwk\ell_j(s)=\sum_{k:\,j_k=j}w_kℓj​(s)=∑k:jk​=j​wk​, and the cost of agent iii is ℓji(s)\ell_{j_i}(s)ℓji​​(s), the traffic on its own link.

A mixed strategy of agent iii is a probability distribution (pi1,…,pim)(p_i^1,\dots,p_i^m)(pi1​,…,pim​) on the links; the agents randomize independently, so sss occurs with probability ∏ipiji\prod_i p_i^{j_i}∏i​piji​​. The cost to agent iii of a mixed profile ppp is its expected cost cic_ici​. The profile ppp is a Nash equilibrium if no agent can lower its expected cost by changing its own distribution while the others keep theirs.

The expected traffic on link jjj is Mj=∑ipijwiM^j=\sum_i p_i^jw_iMj=∑i​pij​wi​, and the cost of agent iii when its traffic is assigned to link jjj is cij=wi+∑k≠ipkjwk=Mj+(1−pij)wic_i^j=w_i+\sum_{k\ne i}p_k^jw_k=M^j+(1-p_i^j)w_icij​=wi​+∑k=i​pkj​wk​=Mj+(1−pij​)wi​.

The social cost of ppp is the expected maximum load,

cost=∑j1=1m⋯∑jn=1m∏i=1npiji max⁡j∑k: jk=jwk,\mathrm{cost}=\sum_{j_1=1}^m\cdots\sum_{j_n=1}^m\prod_{i=1}^n p_i^{j_i}\,\max_{j}\sum_{k:\,j_k=j}w_k ,cost=j1​=1∑m​⋯jn​=1∑m​i=1∏n​piji​​jmax​k:jk​=j∑​wk​,

and the social optimum opt\mathrm{opt}opt is the least maximum load over all pure assignments, the optimum of the mmm-way partition problem for w1,…,wnw_1,\dots,w_nw1​,…,wn​.

The proof of the main theorem uses two further quantities: the contribution probability qiq_iqi​, the probability that agent iii is on the (lexicographically first) link of maximum load, and the collision probability tik=∑jpijpkjt_{ik}=\sum_jp_i^jp_k^jtik​=∑j​pij​pkj​ of agents iii and kkk.

Formalization targets

Goal: Theorem 3

For any number nnn of agents with positive traffics and m=2m=2m=2 identical links, every Nash equilibrium ppp satisfies

cost(p) ≤ 32 opt.\mathrm{cost}(p)\ \le\ \frac32\,\mathrm{opt}.cost(p) ≤ 23​opt.

Milestones

In the order the proof of Theorem 3 uses them:

  1. Equation (2): cij=wi+∑k≠ipkjwk=Mj+(1−pij)wic_i^j=w_i+\sum_{k\ne i}p_k^jw_k=M^j+(1-p_i^j)w_icij​=wi​+∑k=i​pkj​wk​=Mj+(1−pij​)wi​ for every mixed profile.
  2. The support property: at an equilibrium agent iii uses only links minimizing cijc_i^jcij​, and ci=min⁡jcijc_i=\min_jc_i^jci​=minj​cij​.
  3. The lower bounds opt≥max⁡{wi, ∑kwk/m}\mathrm{opt}\ge\max\{w_i,\ \sum_kw_k/m\}opt≥max{wi​, ∑k​wk​/m}.
  4. Theorem 2 with (6): at every equilibrium on mmm identical links,
ci ≤ ∑kwkm+m−1m wi ≤ (2−1m)opt.c_i\ \le\ \frac{\sum_kw_k}{m}+\frac{m-1}{m}\,w_i\ \le\ \Big(2-\frac1m\Big)\mathrm{opt}.ci​ ≤ m∑k​wk​​+mm−1​wi​ ≤ (2−m1​)opt.
  1. cost=∑iqiwi\mathrm{cost}=\sum_iq_iw_icost=∑i​qi​wi​.
  2. Inequality (7): qi+qk≤1+tikq_i+q_k\le1+t_{ik}qi​+qk​≤1+tik​ for distinct agents i,ki,ki,k.
  3. ci=wi+∑k≠itikwkc_i=w_i+\sum_{k\ne i}t_{ik}w_kci​=wi​+∑k=i​tik​wk​.
  4. On two links, at every equilibrium, ∑k≠iqkwk≤(32−qi)∑k≠iwk\sum_{k\ne i}q_kw_k\le\big(\tfrac32-q_i\big)\sum_{k\ne i}w_k∑k=i​qk​wk​≤(23​−qi​)∑k=i​wk​.

Companion items

The second sentence of Theorem 1 (on two links some equilibrium has cost=32 opt>0\mathrm{cost}=\tfrac32\,\mathrm{opt}>0cost=23​opt>0), which shows the goal is tight, and the fact from its proof that the uniform profile pij=1/mp_i^j=1/mpij​=1/m of mmm unit agents on mmm links is an equilibrium.

Significance

Theorem 3 and the instance of Theorem 1 show that on two identical links selfish randomized routing never costs more than 50%50\%50% above the optimum, whatever the number of agents and their traffics, and that this factor is attained. Theorem 2 gives a per-agent guarantee for any number of links: the expected cost an individual agent experiences at any equilibrium is within 2−1/m2-1/m2−1/m of the optimum, the same factor as Graham's list-scheduling bound. Together they separate the individual and the social view: individual costs stay within a constant, while the expected maximum load, the social cost, can be a factor Ω(log⁡m/log⁡log⁡m)\Omega(\log m/\log\log m)Ω(logm/loglogm) above the optimum.

The results are proved in the paper. As far as is known they have not been machine-checked. Formalizing them produces a verified model of mixed equilibria in load balancing games, with the social cost as an expected maximum over the product distribution, which is the starting point of the later literature on links with speeds, on general congestion games and on smoothness arguments. The intermediate identities (the contribution and collision probabilities) are reusable for any expected-maximum bound over independent random assignments.

Difficulty

The social cost is an expectation of a maximum over mnm^nmn outcomes, and the equilibrium probabilities are given only implicitly, as the solution of a linear system determined by the agents' supports. The natural first idea, to bound the expected maximum load by the maximum expected load max⁡jMj\max_jM^jmaxj​Mj, fails: the expected maximum can be much larger, and bounding it is exactly what makes the problem hard (for mmm links it grows like the maximum occupancy of mmm balls in mmm bins). Computing the equilibrium probabilities explicitly does not help either; the paper gives them for two links and notes it does not see how to use them to bound the social cost. The argument has to relate the per-agent expected costs, which the equilibrium condition controls, to the expected maximum, which it does not control directly.

Formalization scope

Agents are Fin n and links Fin m (the goal uses Fin 2); the paper's agent iii and link jjj are indices i−1i-1i−1, j−1j-1j−1. A mixed profile is p : Fin n → Fin m → ℝ with p i j =pij=p_i^j=pij​. The game is built on the published definitions agt_games (AGT.IsMixedNash, AGT.expectedPayoff, AGT.profileProb). That vocabulary maximizes payoffs, so the payoff of an agent is minus the load of its link, and the expected cost is minus the expected payoff. The equilibrium is the full mixed Nash condition, including that each pip_ipi​ is a probability distribution; the support description is a milestone, not the definition. The social cost is the expected maximum load over the product distribution, never the maximum expected load. opt\mathrm{opt}opt is a minimum over pure assignments, with the number of links an explicit argument. The lexicographically first maximum link is the lowest-indexed link of maximum load.

Traffics are positive, as in the paper's model; some milestones need only nonnegative traffics or no sign condition, and say so. Statements over mmm links assume m≥1m\ge1m≥1. Price-of-anarchy statements are inequalities cost≤c⋅opt\mathrm{cost}\le c\cdot\mathrm{opt}cost≤c⋅opt for every equilibrium, never a quotient cost/opt\mathrm{cost}/\mathrm{opt}cost/opt, whose value at opt=0\mathrm{opt}=0opt=0 would be a junk 000. A formalization in which the social cost is max⁡jMj\max_jM^jmaxj​Mj, or in which the equilibrium is only a support condition without the requirement that the pip_ipi​ be distributions, would trivialize or falsify the goal and is ruled out by these definitions.

A complete development needs finite sums over the mnm^nmn pure profiles, marginalization of product distributions, and the case analysis of the final step. The marginalization lemmas (summing out the other agents, collision probabilities of independent choices) are reusable beyond this mission. Proofs of the milestones, alternative arguments for Theorem 3, and a proof of Theorem 2 for its own sake are all welcome.

Page numbers are those of the PDF file of the journal version; it prints a page number only on its first page.

Selected references

  • E. Koutsoupias and C. Papadimitriou, Worst-case equilibria, STACS 1999, LNCS 1563, pp. 404–413. https://doi.org/10.1007/3-540-49116-3_38 (this mission cites the authors' journal version of 2009, Computer Science Review 3(2), 65–69, https://doi.org/10.1016/j.cosrev.2009.04.003)
  • A. Czumaj and B. Vöcking, Tight bounds for worst-case equilibria, SODA 2002, pp. 413–420; ACM Transactions on Algorithms 3(1), 2007. https://doi.org/10.1145/1186810.1186814
  • E. Koutsoupias, M. Mavronicolas and P. Spirakis, Approximate equilibria and ball fusion, Theory of Computing Systems 36, 683–693, 2003. https://doi.org/10.1007/s00224-003-1131-5
  • R. L. Graham, Bounds on multiprocessing timing anomalies, SIAM Journal on Applied Mathematics 17(2), 416–429, 1969. https://doi.org/10.1137/0117039
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AnalysisHarmonic Analysis·Captain: mikedeng1

Distribution Function Inequalities for Martingales 4: For Convex Φ of Moderate Growth, EΦ(f*) and EΦ(S(f)) Are Comparable for Every MartingaleResearch Paper

Motivation

Martingale inequalities compare what a fluctuating process does along a path with how large its successive increments are. Such estimates are used in probability and harmonic analysis because a martingale can represent information revealed step by step, while its square function measures accumulated fluctuation. In his 1973 Wald Memorial Lectures, Burkholder developed distribution function inequalities that cover many choices of size measure at once, extending the power norm comparisons treated earlier in the paper. Burkholder, 1973

The target of this mission is Theorem 15.1 of that paper: a two sided comparison for every convex function of moderate growth. The paper attributes the decomposition of a martingale into small and large jumps to Davis, and cites a convex comparison lemma introduced in earlier work and subsequently treated by Garsia and Neveu. These attributions matter to the scope of the mission: the decomposition and lemma are separate, named milestones, while Burkholder's printed two sided inequality is the goal. Burkholder, 1973, §§14–16

Setting

Work on a probability space (Ω,A,P)(\Omega,\mathcal A,P)(Ω,A,P) with an increasing sequence of sub sigma fields A0,A1,…\mathcal A_0,\mathcal A_1,\ldotsA0​,A1​,…. A real martingale f=(f1,f2,…)f=(f_1,f_2,\ldots)f=(f1​,f2​,…) is observed from time 111 onward. Following the paper, put f0=0f_0=0f0​=0 in the formulas for its differences: d1=f1d_1=f_1d1​=f1​ and dk=fk−fk−1d_k=f_k-f_{k-1}dk​=fk​−fk−1​ for k≥2k\ge2k≥2. This convention differs from the index zero value required for a Lean martingale, which is discussed below.

The square function S(f)S(f)S(f) and maximal function f∗f^*f∗ are pathwise quantities:

S(f)=(∑k=1∞dk2)1/2,f∗=sup⁡k≥1∣fk∣.S(f)=\left(\sum_{k=1}^{\infty}d_k^2\right)^{1/2}, \qquad f^*=\sup_{k\ge1}|f_k|.S(f)=(k=1∑∞​dk2​)1/2,f∗=k≥1sup​∣fk​∣.

Either quantity can be infinite. Their finite versions stop at nnn: Sn(f)S_n(f)Sn​(f) sums the first nnn squared differences, and fn∗f_n^*fn∗​ takes the maximum through time nnn. For a positive exponent ppp, the paper writes ∥f∥p=sup⁡n≥1(E∣fn∣p)1/p\|f\|_p=\sup_{n\ge1}(E|f_n|^p)^{1/p}∥f∥p​=supn≥1​(E∣fn​∣p)1/p. The notation EΦ(Y)E\Phi(Y)EΦ(Y) means the expectation of a nonnegative transform of a nonnegative random variable YYY.

A function of moderate growth is a nondecreasing continuous Φ:[0,∞]→[0,∞]\Phi:[0,\infty]\to[0,\infty]Φ:[0,∞]→[0,∞] with Φ(0)=0\Phi(0)=0Φ(0)=0 and

Φ(2x)≤c(6.1)Φ(x)(x>0)\Phi(2x)\le c_{(6.1)}\Phi(x)\qquad(x>0)Φ(2x)≤c(6.1)​Φ(x)(x>0)

for some nonnegative growth constant c(6.1)c_{(6.1)}c(6.1)​. The target adds convexity on finite nonnegative arguments. The examples Φ(x)=x\Phi(x)=xΦ(x)=x and Φ(x)=xp\Phi(x)=x^pΦ(x)=xp for p≥1p\ge1p≥1 satisfy these conditions. The paper sets aside Φ≡0\Phi\equiv0Φ≡0 as trivial; the Lean statements allow it because every displayed comparison still holds.

Formalization targets

The two sided convex comparison

The goal is precisely the form printed as Theorem 15.1:

C1EΦ(S(f))≤EΦ(f∗)≤C2EΦ(S(f)),C1,C2>0.C_1 E\Phi(S(f))\le E\Phi(f^*)\le C_2 E\Phi(S(f)), \qquad C_1,C_2>0.C1​EΦ(S(f))≤EΦ(f∗)≤C2​EΦ(S(f)),C1​,C2​>0.

The constants depend only on c(6.1)c_{(6.1)}c(6.1)​, and are uniform over the probability space, filtration, martingale, and particular choice of Φ\PhiΦ with that growth bound. The statement includes both sides; the paper writes a proof for the right side and says the left side follows by the same pattern. No integrability or boundedness is imposed on fff or on the two expectations. Burkholder, 1973, Theorem 15.1, pp. 33–34

Supporting statements

The milestones record the paper's good λ\lambdaλ lemma, Doob's cited maximal estimate, the predictable jump inequalities of §12, the quasi subadditivity of Φ\PhiΦ, Davis's decomposition and its jump bounds, and the convexity lemma of §16. The latter compares a sum of nonnegative random variables with the sum of their conditional expectations. Its two Neveu statements are retained as cited intermediate targets. These results identify distinct mathematical interfaces that a solver can formalize and reuse; the milestone text is transcribed from the indicated pages of the article.

Significance

The theorem lets one replace the expected convex transform of a path's maximum by the expected transform of its quadratic fluctuation, up to constants controlled by a single growth parameter. Choosing Φ(x)=x\Phi(x)=xΦ(x)=x recovers the L1L^1L1 comparison displayed after Davis's decomposition; choosing a convex power gives the p≥1p\ge1p≥1 power cases. The assertion is useful even when one or both expectations are infinite, because it gives a uniform relation across the whole class of admissible martingales and functions. Burkholder, 1973, §§14–15

The result is proved in the paper. This mission asks for a machine checked Lean proof of the known theorem and of the selected statements that support it. The definitions for square and maximal functions, moderate growth, and nonnegative conditional projections can be reused in other martingale comparisons. A previously posed platform theorem about Robbins–Monro noise sums has the shape of one power function instance, but its process and time window differ; it does not supply this general result.

Difficulty

The size of a single martingale increment can dominate both a maximum and a square function. A direct comparison of the two pathwise expressions therefore gives no uniform expectation bound for arbitrary martingales and convex Φ\PhiΦ. The §12 estimates require predictable control of jumps, while the target has no such hypothesis. Davis's decomposition exposes the small and large jump contributions as different objects, and the §16 convexity lemma is needed to compare the conditional terms arising from large jumps. Convexity is essential for that lemma and for Theorem 15.1; the §12 good λ\lambdaλ statements themselves assume only moderate growth. Burkholder, 1973, §§12, 14–16

Formalization scope

Lean uses Mathlib's Martingale f ℱ P for a process indexed by natural numbers. The article begins at 111 and uses f0=0f_0=0f0​=0 only in its difference formulas. The definitions of dkd_kdk​, S(f)S(f)S(f), f∗f^*f∗, and ∥f∥p\|f\|_p∥f∥p​ therefore read positive indices and insert zero in the article's formulas; Lean's actual f(0)f(0)f(0) is the compatible conditional expectation extension needed by Mathlib. Davis's partial sums also begin at 111, and the decomposition theorem specifies the index zero extensions for its two martingales.

The square function, maximal function, LpL^pLp norm, and all nonnegative expectations take values in [0,∞][0,\infty][0,∞]. This retains unbounded sample paths and nonintegrable expectations. For a nonnegative variable zkz_kzk​, E(zk∣Ak−1)E(z_k\mid\mathcal A_{k-1})E(zk​∣Ak−1​) is the extended conditional expectation condLExp, so a nonintegrable zkz_kzk​ cannot silently become zero. Davis's signed yky_kyk​ is integrable, so its real conditional expectation uses Mathlib's ordinary conditional expectation. Predictable bounds such as ∣dk∣≤wk|d_k|\le w_k∣dk​∣≤wk​ and the resulting claims are stated almost everywhere at each positive index.

The Lean predicate for moderate growth states the doubling law at zero and infinity as well as positive finite xxx; zero is automatic from Φ(0)=0\Phi(0)=0Φ(0)=0, and the endpoint at infinity follows by continuity in the nontrivial case. Convexity is read from finite real arguments. The zero function is included. A valid formalization must retain both inequalities in the goal and choose its constants before the martingale and Φ\PhiΦ; choosing constants after the data would make the goal much weaker.

The development needs finite and infinite square function sums, maximal functions, stopping and tail events, Mathlib martingales, conditional expectations, and convexity on the nonnegative reals. Contributions proving or improving any of the named milestones are welcome, including independent proofs of the cited Doob and Neveu statements. No extra boundedness or integrability assumption should be inserted into the goal to simplify a proof.

Selected references

  • D. L. Burkholder, Distribution Function Inequalities for Martingales, The Annals of Probability 1(1), 1973, pp. 19–42. DOI.
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Graph TheoryMarkov Chain·Captain: mikedeng1

Geometric Bounds for Eigenvalues of Markov Chains 1: Poincaré Inequality β₁ ≤ 1 − 1/κ for Reversible Chains via Path Lengths |γ_xy|_QResearch Paper

Motivation

The rate at which a finite Markov chain approaches equilibrium depends on its eigenvalues. For a reversible chain, an upper bound on the second largest eigenvalue gives a lower bound on the spectral gap, which is one of the quantities used to study relaxation toward stationarity. Diaconis and Stroock asked how to estimate this eigenvalue using the geometry of transitions rather than computing the whole spectrum. Their 1991 paper gives an answer in terms of paths through the graph of positive transitions, and compares it with other geometric estimates Diaconis and Stroock, 1991.

This mission covers the first estimate in that paper, Proposition 1, together with the alternative parameter of Proposition 1′ and the random-walk specialization in Corollary 1. These results are known mathematical theorems. The work here is to state their exact finite, reversible setting in Lean and make their formal proofs available as reusable spectral estimates. The paper's examples show why the path selection matters: two choices for the same chain can give substantially different bounds Diaconis and Stroock, 1991, §2.

Setting

Let XXX be a finite state space and let P(x,y)P(x,y)P(x,y) be the transition probability from xxx to yyy. Assume that PPP is irreducible and reversible with respect to a stationary probability distribution π\piπ. The edge measure is Q(x,y)=π(x)P(x,y)=π(y)P(y,x)Q(x,y)=\pi(x)P(x,y)=\pi(y)P(y,x)Q(x,y)=π(x)P(x,y)=π(y)P(y,x). Thus Q(x,y)>0Q(x,y)>0Q(x,y)>0 identifies an available edge of the transition graph. Because the chain is irreducible, every state has positive stationary mass and distinct states can be connected by such edges Diaconis and Stroock, 1991, §1A–B.

For each ordered pair of distinct states x,yx,yx,y, choose a path γxy\gamma_{xy}γxy​ from xxx to yyy. A path may revisit a vertex, but cannot use an unordered edge twice. Write Γ\GammaΓ for the whole choice of paths. The weighted path length is ∣γxy∣Q=∑e∈γxyQ(e)−1|\gamma_{xy}|_Q=\sum_{e\in\gamma_{xy}}Q(e)^{-1}∣γxy​∣Q​=∑e∈γxy​​Q(e)−1. Here a traversal has an orientation, and e∈γxye\in\gamma_{xy}e∈γxy​ in the congestion formula means that the path traverses the directed edge eee in that orientation. The congestion parameter of (1.5) is

κ(Γ)=max⁡e∑γxy∋e∣γxy∣Q π(x)π(y),\kappa(\Gamma)=\max_{e}\sum_{\gamma_{xy}\ni e}|\gamma_{xy}|_Q\,\pi(x)\pi(y),κ(Γ)=emax​γxy​∋e∑​∣γxy​∣Q​π(x)π(y),

with the maximum over directed edges for which Q(e)>0Q(e)>0Q(e)>0. The paper also defines K(Γ)=max⁡eQ(e)−1∑γxy∋e∣γxy∣π(x)π(y)K(\Gamma)=\max_e Q(e)^{-1}\sum_{\gamma_{xy}\ni e}|\gamma_{xy}|\pi(x)\pi(y)K(Γ)=maxe​Q(e)−1∑γxy​∋e​∣γxy​∣π(x)π(y), where ∣γxy∣|\gamma_{xy}|∣γxy​∣ is the ordinary number of edges Diaconis and Stroock, 1991, pp. 37–38.

The variance of a real function ϕ\phiϕ is Var⁡π(ϕ)=∑x(ϕ(x)−∑zϕ(z)π(z))2π(x)\operatorname{Var}_\pi(\phi)=\sum_x(\phi(x)-\sum_z\phi(z)\pi(z))^2\pi(x)Varπ​(ϕ)=∑x​(ϕ(x)−∑z​ϕ(z)π(z))2π(x). Its Dirichlet energy is EP(ϕ,ϕ)=12∑x,y(ϕ(x)−ϕ(y))2Q(x,y)\mathcal E_P(\phi,\phi)=\frac12\sum_{x,y}(\phi(x)-\phi(y))^2Q(x,y)EP​(ϕ,ϕ)=21​∑x,y​(ϕ(x)−ϕ(y))2Q(x,y). If ∣X∣≥2|X|\ge2∣X∣≥2, let β1\beta_1β1​ denote the second largest real eigenvalue of PPP, below the simple eigenvalue 111 Diaconis and Stroock, 1991, pp. 36–37.

Formalization targets

Proposition 1: the path bound

For every admissible path system Γ\GammaΓ,

β1≤1−1κ(Γ).\beta_1\le 1-\frac{1}{\kappa(\Gamma)}.β1​≤1−κ(Γ)1​.

The mission's milestones are the pairwise expression for variance, the paper's per-path Cauchy–Schwarz inequality, the resulting Var⁡π(ϕ)≤κ(Γ)EP(ϕ,ϕ)\operatorname{Var}_\pi(\phi)\le\kappa(\Gamma)\mathcal E_P(\phi,\phi)Varπ​(ϕ)≤κ(Γ)EP​(ϕ,ϕ), and the variational characterization (1.2) of the spectral gap. The last is the proved theorem MarkovMixing.dirichlet_gap, which states (1.2) for centered functions of unit squared norm, a normalization under which the ratio in (1.2) is unchanged, and adds that the infimum is attained Diaconis and Stroock, 1991, pp. 37–38.

Companion estimates

Proposition 1′ states β1≤1−1/K(Γ)\beta_1\le1-1/K(\Gamma)β1​≤1−1/K(Γ) using the alternative congestion parameter. For a connected simple graph G=(X,E)G=(X,E)G=(X,E), Corollary 1 specializes Proposition 1 to simple random walk, with stationary distribution π(x)=d(x)/(2∣E∣)\pi(x)=d(x)/(2|E|)π(x)=d(x)/(2∣E∣). If d∗=max⁡xd(x)d_*=\max_x d(x)d∗​=maxx​d(x), γ∗\gamma_*γ∗​ is the maximum number of edges in a chosen path, and bbb is the maximum number of selected paths traversing a directed edge, its bound is

β1≤1−2∣E∣d∗2γ∗b.\beta_1\le1-\frac{2|E|}{d_*^2\gamma_*b}.β1​≤1−d∗2​γ∗​b2∣E∣​.

The paper states Proposition 1′ without a separate proof and derives Corollary 1 from the graph's transition probabilities Diaconis and Stroock, 1991, pp. 38–39.

Significance

The result converts information about a path family into a numerical spectral-gap estimate. This lets a solver analyze a chain through its transition graph when an exact diagonalization is inconvenient. The graph corollary makes the quantities especially concrete: number of edges, maximum degree, longest selected path, and how many selected paths share an edge. Such estimates are one ingredient in quantitative convergence bounds for reversible chains Diaconis and Stroock, 1991, §§1D, 2.

The finite-chain vocabulary for stochasticity, stationarity, reversibility, eigenvalues, variance, and Dirichlet energy is already published in the MarkovMixing layer. The mission adds the paper's edge-simple path system and its two congestion parameters, then formalizes the source's statements against that vocabulary. The path definitions and pairwise variance identity can be reused in other canonical-path arguments; the three claims from pp. 37–39 still need machine-checked proofs in this mission. The variational spectral-gap theorem used as a milestone is already proved on Prove2Me Levin, Peres and Wilmer, 2009, §13.3.

Difficulty

The challenge is to account for each selected path without changing the congestion constant. Paths are indexed by ordered endpoints, edges in the maximum are directed, and the paper permits repeated vertices while forbidding repeated edges. Counting traversals with the wrong orientation, or allowing an edge to repeat, changes the parameter that appears in the final bound. The graph case also depends on keeping the number of paths through an edge separate from path length; replacing either with a coarser graph quantity would give a different theorem Diaconis and Stroock, 1991, §1B.

Formalization scope

The state space is a finite Lean type, PPP is a real matrix, and π\piπ is a real-valued probability vector. A path is a list of vertices. Its traversed directed edges are successive vertex pairs; the edge-simple rule compares those pairs as unordered edges. One path is chosen for each ordered pair x≠yx\ne yx=y, and values of Γ(x,x)\Gamma(x,x)Γ(x,x) never enter the formulas. The maximum over positive directed edges is implemented as a real supremum over a finite subtype. On an empty index set that expression has Lean's default value zero; irreducibility and ∣X∣≥2|X|\ge2∣X∣≥2 exclude this case in the eigenvalue results.

The standing assumptions are stochasticity, irreducibility, stationarity, and detailed balance. The goal and its companion eigenvalue estimates also require ∣X∣≥2|X|\ge2∣X∣≥2 because the second largest eigenvalue is undefined for a one-state chain. The variance identity needs only a probability distribution, while the per-path estimate uses only a positive-edge walk. The graph corollary assumes connectedness and at least two vertices; it derives the chain properties from the graph as the paper does. The mission does not assume the desired Poincaré inequality or the spectral conclusion as hypotheses.

The main proof obligations concern the pathwise inequality, the finite reindexing that produces the paper's exact κ\kappaκ, and the eigenvalue bound. Contributions that establish those claims, the graph specialization, or the alternative KKK estimate fit the stated scope. The shared Markov-chain definitions and the path vocabulary are intended to support later results of the same paper.

Selected references

  • Persi Diaconis and Daniel Stroock, Geometric Bounds for Eigenvalues of Markov Chains, Annals of Applied Probability 1(1), 1991, pp. 36–61. DOI.
  • David A. Levin, Yuval Peres and Elizabeth L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2009, Chapters 12–13. Text.
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Functional AnalysisMarkov Chain·Captain: mikedeng1

Logarithmic Sobolev Inequalities for Finite Markov Chains 1: Chi-Square Distance ‖h_t^x − 1‖₂ ≤ e^{1−c} at t = (2α)⁻¹ log log(1/π(x)) + c/λResearch Paper

Motivation

A finite Markov chain repeatedly applies a transition rule to move among a finite set of states. Its stationary distribution is a probability law that the transition rule leaves unchanged. For algorithms that sample from a target distribution, and for random walks used to model a system, a central question is how long a chain started from one state takes to resemble its stationary law. Diaconis and Saloff-Coste study how a logarithmic Sobolev inequality controls this approach to equilibrium. Their paper develops finite-chain functional inequalities and applies them to mixing bounds, product chains, and concrete walks. Diaconis and Saloff-Coste, 1996.

Theorem 3.7 gives a starting-state bound in a weighted quadratic distance. Its dependence on the initial state's stationary mass is a double logarithm, while the final convergence term is governed by the spectral gap. This separates two effects: reaching a distribution that is no longer sharply concentrated, and then reducing its remaining deviation from stationarity. The paper also distinguishes general chains from reversible ones, with different constants in the first time scale. Diaconis and Saloff-Coste, 1996, pp. 719 and 723–724.

Setting

Let VVV be a finite state space. A transition matrix KKK assigns nonnegative numbers K(x,y)K(x,y)K(x,y) whose sum over yyy is one for every xxx. A probability vector π\piπ is stationary when ∑xπ(x)K(x,y)=π(y)\sum_x\pi(x)K(x,y)=\pi(y)∑x​π(x)K(x,y)=π(y) for every yyy; here every π(y)\pi(y)π(y) is strictly positive. The chain is irreducible when every state can reach every other state in some finite number of steps. It is reversible when π(x)K(x,y)=π(y)K(y,x)\pi(x)K(x,y)=\pi(y)K(y,x)π(x)K(x,y)=π(y)K(y,x) for all states x,yx,yx,y. These conditions are the paper's standing finite-chain setting. Diaconis and Saloff-Coste, 1996, pp. 700–702 and 714.

For a real function fff on VVV, write Eπf=∑xf(x)π(x)E_\pi f=\sum_x f(x)\pi(x)Eπ​f=∑x​f(x)π(x) and Var⁡π(f)=∑x(f(x)−Eπf)2π(x)\operatorname{Var}_\pi(f)=\sum_x(f(x)-E_\pi f)^2\pi(x)Varπ​(f)=∑x​(f(x)−Eπ​f)2π(x). Its weighted ppp-norm is ∥f∥p=(∑x∣f(x)∣pπ(x))1/p\|f\|_p=(\sum_x|f(x)|^p\pi(x))^{1/p}∥f∥p​=(∑x​∣f(x)∣pπ(x))1/p. The Dirichlet form used here is the ordered bilinear expression E(f,g)=∑x(f(x)−(Kf)(x))g(x)π(x)\mathcal E(f,g)=\sum_x(f(x)-(Kf)(x))g(x)\pi(x)E(f,g)=∑x​(f(x)−(Kf)(x))g(x)π(x). It is generally not symmetric for a nonreversible chain. The spectral gap is the variational quantity λ=inf⁡Var⁡π(f)≠0E(f,f)/Var⁡π(f)\lambda=\inf_{\operatorname{Var}_\pi(f)\ne0}\mathcal E(f,f)/\operatorname{Var}_\pi(f)λ=infVarπ​(f)=0​E(f,f)/Varπ​(f). The log-Sobolev constant is α=inf⁡L(f)≠0E(f,f)/L(f)\alpha=\inf_{\mathcal L(f)\ne0}\mathcal E(f,f)/\mathcal L(f)α=infL(f)=0​E(f,f)/L(f), where L(f)=∑x∣f(x)∣2log⁡(∣f(x)∣2/∥f∥22)π(x)\mathcal L(f)=\sum_x |f(x)|^2\log(|f(x)|^2/\|f\|_2^2)\pi(x)L(f)=∑x​∣f(x)∣2log(∣f(x)∣2/∥f∥22​)π(x). Diaconis and Saloff-Coste, 1996, pp. 701, 705–706, 714.

The continuous-time heat kernel Ht=e−t(I−K)H_t=e^{-t(I-K)}Ht​=e−t(I−K) averages all discrete step counts with Poisson weights. If the chain starts at xxx, then Ht(x,y)H_t(x,y)Ht​(x,y) is the probability of being at yyy at time ttt. Its density relative to stationarity is htx(y)=Ht(x,y)/π(y)h_t^x(y)=H_t(x,y)/\pi(y)htx​(y)=Ht​(x,y)/π(y). Thus ∥htx−1∥2\|h_t^x-1\|_2∥htx​−1∥2​ measures the weighted quadratic deviation of the time-ttt law from π\piπ. Diaconis and Saloff-Coste, 1996, p. 702.

Formalization targets

Spectral decay and hypercontractivity

The milestones include the L2L^2L2 spectral-gap decay of Lemma 2.4, the heat-flow moment identity of Lemma 2.5, the power inequalities of Lemma 2.6, and the derivative formula (3.2). The two hypercontractivity clauses of Theorem 3.5 state that ∥Htf∥q≤∥f∥2\|H_t f\|_q\le\|f\|_2∥Ht​f∥q​≤∥f∥2​ when q−1≤e2αtq-1\le e^{2\alpha t}q−1≤e2αt for a general chain, or when q−1≤e4αtq-1\le e^{4\alpha t}q−1≤e4αt for a reversible chain, with q≥2q\ge2q≥2 and t>0t>0t>0. These are separate source statements and remain separate milestones. Diaconis and Saloff-Coste, 1996, pp. 706–707, 719–721.

Chi-square convergence

The goal is Theorem 3.7. For a state xxx with π(x)≤e−1\pi(x)\le e^{-1}π(x)≤e−1 and any c>0c>0c>0, it asserts

∥htx−1∥2≤e1−catt=12αlog⁡log⁡1π(x)+cλ.\|h_t^x-1\|_2\le e^{1-c} \quad\text{at}\quad t=\frac{1}{2\alpha}\log\log\frac1{\pi(x)}+\frac c\lambda.∥htx​−1∥2​≤e1−catt=2α1​loglogπ(x)1​+λc​.

For a reversible chain, the same bound holds with 1/(4α)1/(4\alpha)1/(4α) in place of 1/(2α)1/(2\alpha)1/(2α). The theorem specifies these times exactly; no broader range of times is built into the goal. Diaconis and Saloff-Coste, 1996, p. 723, Theorem 3.7.

Significance

The goal turns two chain constants into an explicit convergence estimate for every eligible starting state. It provides a way to assess a chain whose initial law is a point mass, where the initial density can be large when π(x)\pi(x)π(x) is small. The reversible clause records the paper's stronger time bound under detailed balance. The preceding milestones expose the general spectral and hypercontractive results as reusable statements for other mixing questions. Diaconis and Saloff-Coste, 1996, pp. 719 and 723–724.

These statements are proved in the 1996 paper; this mission asks for machine-checked proofs of the specified formal statements. Published finite-chain definitions for stochasticity, stationarity, irreducibility, detailed balance, weighted expectation and variance, and the heat kernel are already available. The variational gap, log-Sobolev constant, entropy functionals, and this theorem family are the remaining local formalization work. Their individual proof status on the platform can evolve independently after the proposal is launched.

Difficulty

The immediate spectral-gap estimate reduces the L2L^2L2 deviation exponentially, but by itself retains a factor tied to the size of the initial point-mass density. That gives a dependence on log⁡(1/π(x))\log(1/\pi(x))log(1/π(x)), rather than the double logarithm in Theorem 3.7. The stronger bound requires control of how the heat operator changes norms, including the distinction between reversible and nonreversible chains. A formal proof must keep the bilinear Dirichlet arguments in their printed order and handle a real exponent that varies with time. Diaconis and Saloff-Coste, 1996, pp. 706–707, 719–724.

Formalization scope

The Lean state space is a finite type, KKK is a real matrix, and π\piπ is a real-valued stationary probability vector positive at every state. Irreducibility is explicit in the Section 3 statements; reversibility is an additional premise only for the corresponding clauses. The heat kernel is the published Poissonized semigroup. The local λ\lambdaλ and α\alphaα are variational real infima, and operator norm claims are expressed as inequalities for every function. Discrete eigenvalue-based gap definitions are not substituted for the paper's λ\lambdaλ.

The goal's condition π(x)≤e−1\pi(x)\le e^{-1}π(x)≤e−1 gives a meaningful double logarithm, and irreducibility in this finite setting gives positive gap and log-Sobolev constants on every state space where the goal is applicable. The positive stationary mass makes the density quotient meaningful. Nonnegative or positive function premises follow the source's power and derivative statements; no arbitrary sign-changing real powers are used. The Lean conventions for zero logarithm terms and for real infima are documented with the definitions. This excludes trivial conclusions from totalized logarithms, division by zero, or empty variational sets.

The development invites proofs of the seven target theorems and reusable finite-state lemmas about the semigroup, weighted norms, entropy, and variational constants. The definitions remain local to this paper's mission series because the published Markov-chain substrate provides the general finite-chain model, while the variational quantities and normalization here are tied to these source statements.

Selected references

  • Persi Diaconis and Laurent Saloff-Coste, Logarithmic Sobolev inequalities for finite Markov chains, Annals of Applied Probability 6(3):695–750, 1996. DOI: 10.1214/aoap/1034968224.
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Functional Analysis·Captain: mikedeng1

Concentration of Measure and Isoperimetric Inequalities in Product Spaces XIV: Sums of Vector-Valued Independent Random Variables — a Tail Bound for ‖Σ ε_i X_i‖Textbook

Motivation

Many limit theorems of probability in Banach spaces, among them the strong law of large numbers and the law of the iterated logarithm for vector-valued random variables, reduce to sharp estimates of the tail probability

P(∥∑i≤NXi∥≥t)P\Big(\Big\|\sum_{i\le N}X_i\Big\|\ge t\Big)P(​i≤N∑​Xi​​≥t)

for independent random variables XiX_iXi​ with values in a Banach space WWW. For many years these estimates were obtained with martingale methods, and they were not optimal. Chapter 13 of M. Talagrand, Concentration of measure and isoperimetric inequalities in product spaces (Publ. Math. IHÉS 81, 1995), explains how the isoperimetric inequalities of the earlier chapters, in particular control by qqq points (Theorem 3.1.1), give such estimates with explicit constants.

Timeline. M. Ledoux observed (unpublished note on Gaussian randomization, reference [L] of the paper) that for Gaussian sums ∑giXi\sum g_iX_i∑gi​Xi​ one may split ∥∑giXi∥\|\sum g_iX_i\|∥∑gi​Xi​∥ into its conditional mean given (Xi)(X_i)(Xi​) plus a deviation, and that the conditional mean has a monotonicity property that replaces positivity arguments ([L], Eq. (13.1)–(13.2) of the paper). Ledoux and Talagrand used this to characterize the Banach-valued random variables satisfying the law of the iterated logarithm (1988). The resulting conviction that an isoperimetric principle was at work led to Talagrand's 1989 isoperimetric theorem (Ann. Probab. 17), superseded in the 1995 paper by Theorem 3.1.1. Ledoux–Talagrand, Probability in Banach Spaces (1991), Theorem 6.17, proves a variant of the bound formalized here that also allows truncation of the variables.

Setting

Let WWW be a real Banach space with dual W∗W^*W∗, and let X1,…,XNX_1,\dots,X_NX1​,…,XN​ be independent (not necessarily identically distributed) WWW-valued random variables. Let ε1,…,εN\varepsilon_1,\dots,\varepsilon_Nε1​,…,εN​ be Rademacher signs: independent, independent of (Xi)(X_i)(Xi​), with P(εi=1)=P(εi=−1)=1/2P(\varepsilon_i=1)=P(\varepsilon_i=-1)=1/2P(εi​=1)=P(εi​=−1)=1/2. Following the paper, write

∥∑i≤NεiXi∥=Eε∥∑i≤NεiXi∥+(∥∑i≤NεiXi∥−Eε∥∑i≤NεiXi∥),\Big\|\sum_{i\le N}\varepsilon_iX_i\Big\|=E_\varepsilon\Big\|\sum_{i\le N}\varepsilon_iX_i\Big\|+\Big(\Big\|\sum_{i\le N}\varepsilon_iX_i\Big\|-E_\varepsilon\Big\|\sum_{i\le N}\varepsilon_iX_i\Big\|\Big),​i≤N∑​εi​Xi​​=Eε​​i≤N∑​εi​Xi​​+(​i≤N∑​εi​Xi​​−Eε​​i≤N∑​εi​Xi​​),

where EεE_\varepsilonEε​ is expectation in the signs only. The conditional mean is Z=Eε∥∑iεiXi∥Z=E_\varepsilon\|\sum_i\varepsilon_iX_i\|Z=Eε​∥∑i​εi​Xi​∥. The weak variance of a point x=(xi)∈WNx=(x_i)\in W^Nx=(xi​)∈WN is

σ2(x)=sup⁡{∑i≤Nw∗(xi)2: w∗∈W∗, ∥w∗∥≤1}.\sigma^2(x)=\sup\Big\{\sum_{i\le N}w^*(x_i)^2:\ w^*\in W^*,\ \|w^*\|\le1\Big\}.σ2(x)=sup{i≤N∑​w∗(xi​)2: w∗∈W∗, ∥w∗∥≤1}.

The decreasing rearrangement ∥xi∥∗=sup⁡{t: card⁡{j≤N:∥xj∥≥t}≥i}\|x_i\|^*=\sup\{t:\ \operatorname{card}\{j\le N:\|x_j\|\ge t\}\ge i\}∥xi​∥∗=sup{t: card{j≤N:∥xj​∥≥t}≥i} is the iii-th largest norm, and ∑i≤k∥xi∥∗\sum_{i\le k}\|x_i\|^*∑i≤k​∥xi​∥∗ is the sum of the kkk largest norms.

For sets A1,…,Aq⊆WNA_1,\dots,A_q\subseteq W^NA1​,…,Aq​⊆WN, the qqq-point distance of xxx is

f(A1,…,Aq,x)=inf⁡{card⁡{i≤N: xi∉{yi1,…,yiq}}: yl∈Al}.f(A_1,\dots,A_q,x)=\inf\big\{\operatorname{card}\{i\le N:\ x_i\notin\{y^1_i,\dots,y^q_i\}\}:\ y^l\in A_l\big\}.f(A1​,…,Aq​,x)=inf{card{i≤N: xi​∈/{yi1​,…,yiq​}}: yl∈Al​}.

For b>0b>0b>0 let B={σ≤b}B=\{\sigma\le b\}B={σ≤b} and k(x)=f(B,…,B,x)k(x)=f(B,\dots,B,x)k(x)=f(B,…,B,x) with qqq copies of BBB.

Formalization targets

Goal: Theorem 13.4 (p. 200)

With a=2E∥∑iεiXi∥a=2E\|\sum_i\varepsilon_iX_i\|a=2E∥∑i​εi​Xi​∥ and s2=E σ2(X)s^2=E\,\sigma^2(X)s2=Eσ2(X), for all integers q≥2q\ge2q≥2, k≥0k\ge0k≥0 and u,t>0u,t>0u,t>0,

P(∥∑i≤NεiXi∥≥2aq+3t+u)≤2q+1qk+1+4exp⁡(−u232qs2)+2P(∑i≤k∥Xi∥∗>t).P\Big(\Big\|\sum_{i\le N}\varepsilon_iX_i\Big\|\ge 2aq+3t+u\Big)\le\frac{2^{q+1}}{q^{k+1}}+4\exp\Big(-\frac{u^2}{32qs^2}\Big)+2P\Big(\sum_{i\le k}\|X_i\|^*>t\Big).P(​i≤N∑​εi​Xi​​≥2aq+3t+u)≤qk+12q+1​+4exp(−32qs2u2​)+2P(i≤k∑​∥Xi​∥∗>t).

Milestones

  1. Proposition 13.1 (p. 197): for a>0a>0a>0, P(Z≥qa+t)≤q−k−1P(Z≤a)−q+P(∑i≤k∥Xi∥∗≥t)P(Z\ge qa+t)\le q^{-k-1}P(Z\le a)^{-q}+P(\sum_{i\le k}\|X_i\|^*\ge t)P(Z≥qa+t)≤q−k−1P(Z≤a)−q+P(∑i≤k​∥Xi​∥∗≥t).
  2. Proposition 13.3 (p. 199): for fixed x∈WNx\in W^Nx∈WN and u>0u>0u>0,
Pε(∥∑iεixi∥≥2Eε∥∑iεixi∥+u+∑i≤k(x)∥xi∥∗)≤4exp⁡(−u216qb2).P_\varepsilon\Big(\Big\|\sum_i\varepsilon_ix_i\Big\|\ge2E_\varepsilon\Big\|\sum_i\varepsilon_ix_i\Big\|+u+\sum_{i\le k(x)}\|x_i\|^*\Big)\le4\exp\Big(-\frac{u^2}{16qb^2}\Big).Pε​(​i∑​εi​xi​​≥2Eε​​i∑​εi​xi​​+u+i≤k(x)∑​∥xi​∥∗)≤4exp(−16qb2u2​).
  1. Eq. (13.14) (p. 200): the joint bound at level 2v+u+t2v+u+t2v+u+t combining the two.

The goal keeps the paper's explicit constants.

Significance

The result. Theorem 13.4 bounds the tail of a Rademacher sum in an arbitrary Banach space using three quantities only: the mean E∥∑εiXi∥E\|\sum\varepsilon_iX_i\|E∥∑εi​Xi​∥, the weak variance s2s^2s2, and the law of the kkk largest summands. No moment assumption on the XiX_iXi​ beyond these is needed, and q,kq,kq,k are free parameters to optimize. By symmetrization, such bounds are the main input for the law of large numbers and the law of the iterated logarithm in Banach spaces, for the integrability of sums, and for comparison of moments.

Formalizing it. The result is proved in the paper (and in a different form in Ledoux–Talagrand 1991). It is not formalized: Mathlib has independence, product measures and the dual of a normed space, but no Rademacher sums in Banach spaces and none of Talagrand's isoperimetric inequalities. The mission yields a machine-checked statement of the vector-valued tail bound with explicit constants, connected to the qqq-point inequality (Theorem 3.1.1, posed in mission IV of this series) and to the concentration of ∥∑Yivi∥\|\sum Y_iv_i\|∥∑Yi​vi​∥ for bounded YiY_iYi​ (Theorem 13.2, posed in mission IX).

Difficulty

The obvious approach controls ∥∑iεiXi∥\|\sum_i\varepsilon_iX_i\|∥∑i​εi​Xi​∥ by its mean plus a concentration term. Bounded-difference (martingale) inequalities do not work here: the increments are ∥Xi∥\|X_i\|∥Xi​∥, which can be unbounded and heavy-tailed, so the resulting bound depends on ∑∥Xi∥2\sum\|X_i\|^2∑∥Xi​∥2 rather than on the much smaller weak variance σ2\sigma^2σ2. Concentration for the signs conditionally on (Xi)(X_i)(Xi​) (Theorem 13.2) gives the weak variance, but at scale σ(X)\sigma(X)σ(X), a random quantity. The difficulty is to make both the conditional mean ZZZ and σ(X)\sigma(X)σ(X) uniformly controlled on most of the space, at the cost of discarding only a few large summands; a single-point isoperimetric inequality does not supply this.

Formalization scope

  • WWW is a real normed space with CompleteSpace W, MeasurableSpace W and BorelSpace W; W∗W^*W∗ is W →L[ℝ] ℝ with the operator norm. σ2\sigma^2σ2 is a real ⨆ over the dual unit ball, which is nonempty and bounded above by ∑∥xi∥2\sum\|x_i\|^2∑∥xi​∥2.
  • The XiX_iXi​ are realized canonically on WNW^NWN = Fin N → W with PPP = Measure.pi μ for laws μ i (independent, not identically distributed). Signs are Fin N → Bool under the platform's uniform measure Komlos.spMeasure N (referenced). The joint law is the product of the two. Coordinates are 0-based; the rearrangement index is 1-based as in the paper.
  • EεE_\varepsilonEε​ is the finite average over 2N2^N2N sign patterns. aaa and s2s^2s2 are lower Lebesgue integrals (∫⁻) in [0,∞][0,\infty][0,∞], so they need no integrability hypothesis, and a=∞a=\inftya=∞ makes the goal hold with an empty event. Probabilities are in [0,∞][0,\infty][0,∞], so P(B)=0P(B)=0P(B)=0 or P(Z≤a)=0P(Z\le a)=0P(Z≤a)=0 makes the corresponding term +∞+\infty+∞.
  • The paper ignores measurability (pp. 81–82). Here measurability of x↦∥∑εixi∥x\mapsto\|\sum\varepsilon_ix_i\|x↦∥∑εi​xi​∥ (each sign pattern) and of σ2\sigma^2σ2 is an explicit hypothesis; it is automatic for separable WWW.
  • The paper writes q∈Nq\in\mathbf Nq∈N; statements take q≥2q\ge2q≥2, the range of Theorem 3.1.1, and all bounds are trivial for q≤1q\le1q≤1.
  • The paper calls ∥xi∥∗\|x_i\|^*∥xi​∥∗ the "non-decreasing rearrangement", but its formula gives the iii-th largest norm; the formula is formalized.
  • Trivializing formalizations are ruled out: σ2\sigma^2σ2 and EεE_\varepsilonEε​ cannot take junk values (bounded nonempty supremum, finite average), the qqq-point distance is ℕ∞-valued, and no Bochner integral of a possibly non-integrable function appears.

Needed infrastructure: Rademacher sums in Banach spaces, order statistics of finitely many reals, the qqq-point inequality on general product spaces, and Theorem 13.2 for Bernoulli variables. The rearrangement and the qqq-point distance can be reused elsewhere. Contributions are welcome on any milestone, and on proving Proposition 13.3 from a stated form of Theorem 13.2.

Selected references

  • M. Talagrand, Concentration of measure and isoperimetric inequalities in product spaces, Publ. Math. IHÉS 81 (1995), 73–205. https://doi.org/10.1007/BF02699376
  • M. Ledoux, M. Talagrand, Characterization of the law of the iterated logarithm in Banach spaces, Ann. Probab. 16 (1988), 1242–1264. https://doi.org/10.1214/aop/1176991688
  • M. Ledoux, M. Talagrand, Probability in Banach Spaces: Isoperimetry and Processes, Springer, 1991. https://doi.org/10.1007/978-3-642-20212-4
  • M. Talagrand, Isoperimetry and integrability of the sum of independent Banach-space valued random variables, Ann. Probab. 17 (1989), 1546–1570. https://doi.org/10.1214/aop/1176991174
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Stochastic Systems·Captain: mikedeng1

Random Walks in a Random Environment 4: For Z_n = σ_n(1 + Z_{n−1}) with i.i.d. σ_n ≥ 0, (Z_1 + ⋯ + Z_n)/n → Eσ/(1 − Eσ) a.s. if Eσ < 1, and → ∞ if Eσ ≥ 1Research Paper

Motivation

A random walk in a random environment on Z\mathbb ZZ moves one step right with probability αx\alpha_xαx​ and one step left with probability 1−αx1-\alpha_x1−αx​ from site xxx, where the αx\alpha_xαx​ are themselves i.i.d. random variables. In his 1975 paper, F. Solomon (Ann. Probab. 3(1):1–31, DOI 10.1214/aop/1176996444) decided recurrence and transience of this walk and computed its speed. Section 4 of the paper isolates a piece of that analysis: the conditional mean time for the walk to cross one bond, given the environment.

Fix the environment, make 000 reflecting, and let μn\mu_nμn​ be the mean first-passage time from nnn to n+1n+1n+1. Conditioning on the first step gives μn=σnμn−1+(σn+1)\mu_n=\sigma_n\mu_{n-1}+(\sigma_n+1)μn​=σn​μn−1​+(σn​+1) with σn=(1−αn)/αn\sigma_n=(1-\alpha_n)/\alpha_nσn​=(1−αn​)/αn​, and Zn=12(μn−1)Z_n=\tfrac12(\mu_n-1)Zn​=21​(μn​−1) satisfies a linear recursion with random coefficients (p. 28). The sum Z1+⋯+ZnZ_1+\dots+Z_nZ1​+⋯+Zn​ is, up to an affine change, the expected time to reach level nnn in that environment. Recursions of the same form, Zn=AnZn−1+BnZ_n=A_nZ_{n-1}+B_nZn​=An​Zn−1​+Bn​ with i.i.d. coefficients, are the random difference equations studied by Kesten (Acta Math. 131, 1973) and Vervaat (Adv. Appl. Probab. 11, 1979); they recur in queueing (waiting-time recursions), insurance (discounted cash flows, "perpetuities") and the analysis of stochastic algorithms.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space and σ1,σ2,…\sigma_1,\sigma_2,\dotsσ1​,σ2​,… independent, identically distributed, nonnegative real random variables. The system of difference equations (4.1) is

Z0=0,Zn=σn (1+Zn−1),n≥1.Z_0=0,\qquad Z_n=\sigma_n\,(1+Z_{n-1}),\quad n\ge1 .Z0​=0,Zn​=σn​(1+Zn−1​),n≥1.

In the Lean development Z σ n ω is defined by this recursion (module SolomonRWRE.DiffEq.System), so it is a function of σ1,…,σn\sigma_1,\dots,\sigma_nσ1​,…,σn​ and needs no existence hypothesis. Unfolding gives the closed form (4.3), Zn=∑j=1nσj⋯σnZ_n=\sum_{j=1}^n\sigma_j\cdots\sigma_nZn​=∑j=1n​σj​⋯σn​.

The mean is ν=E(σ)=∫σ1 dP∈[0,∞]\nu=E(\sigma)=\int\sigma_1\,dP\in[0,\infty]ν=E(σ)=∫σ1​dP∈[0,∞] (nu P σ); σ\sigmaσ need not be integrable, and ν=∞\nu=\inftyν=∞ is allowed. The products are ρj=σ1⋯σj\rho_j=\sigma_1\cdots\sigma_jρj​=σ1​⋯σj​ (rho), and the block sums of the proof are

Ykn=∑j=1n−k+1 ∏i=jj+k−1σi(Y σ k n),Y_k^n=\sum_{j=1}^{n-k+1}\ \prod_{i=j}^{j+k-1}\sigma_i \qquad(\texttt{Y σ k n}),Ykn​=j=1∑n−k+1​ i=j∏j+k−1​σi​(Y σ k n),

the sums of the products of kkk consecutive σ\sigmaσ's inside σ1,…,σn\sigma_1,\dots,\sigma_nσ1​,…,σn​. For one step of the proof the sequence is extended to a two-sided i.i.d. family {σj}j∈Z\{\sigma_j\}_{j\in\mathbb Z}{σj​}j∈Z​ (module TwoSided), with Sn=∑j=−∞nσj⋯σn∈[0,∞]S_n=\sum_{j=-\infty}^n\sigma_j\cdots\sigma_n\in[0,\infty]Sn​=∑j=−∞n​σj​⋯σn​∈[0,∞].

Formalization targets

Goal: Theorem (4.4)

lim⁡n→∞Z1+⋯+Znn={ν1−ν,ν<1,∞,ν≥1,almost surely.\lim_{n\to\infty}\frac{Z_1+\dots+Z_n}{n}=\begin{cases}\dfrac{\nu}{1-\nu}, & \nu<1,\\[2mm] \infty, & \nu\ge1,\end{cases}\qquad\text{almost surely.}n→∞lim​nZ1​+⋯+Zn​​=⎩⎨⎧​1−νν​,∞,​ν<1,ν≥1,​almost surely.

The goal fixes nothing beyond the paper's hypotheses: any law on [0,∞)[0,\infty)[0,∞), integrable or not. Both cases are almost-sure limits.

Milestones, in the order of the proof (pp. 28–29)

  1. The closed form (4.3), Zn=∑j=1nσj⋯σnZ_n=\sum_{j=1}^n\sigma_j\cdots\sigma_nZn​=∑j=1n​σj​⋯σn​.
  2. The regrouping Z1+⋯+Zn=Y1n+⋯+YnnZ_1+\dots+Z_n=Y_1^n+\dots+Y_n^nZ1​+⋯+Zn​=Y1n​+⋯+Ynn​.
  3. For fixed k≥1k\ge1k≥1, Ykn/n→νkY_k^n/n\to\nu^kYkn​/n→νk almost surely, in [0,∞][0,\infty][0,∞].
  4. lim inf⁡n(Z1+⋯+Zn)/n≥∑k≥1νk\liminf_n (Z_1+\dots+Z_n)/n\ge\sum_{k\ge1}\nu^kliminfn​(Z1​+⋯+Zn​)/n≥∑k≥1​νk almost surely, which settles ν≥1\nu\ge1ν≥1.
  5. For a two-sided family, Zn≤SnZ_n\le S_nZn​≤Sn​ pathwise, and Sn<∞S_n<\inftySn​<∞ almost surely when ν<1\nu<1ν<1.
  6. For ν<1\nu<1ν<1, lim sup⁡n1n∑k=1nZk≤ν/(1−ν)\limsup_n\frac1n\sum_{k=1}^nZ_k\le\nu/(1-\nu)limsupn​n1​∑k=1n​Zk​≤ν/(1−ν) almost surely.

Companion: Lemma (4.2)(i)–(ii)

If ∑nn−1P(ρn>1)<∞\sum_n n^{-1}P(\rho_n>1)<\infty∑n​n−1P(ρn​>1)<∞ then ∑jρj<∞\sum_j\rho_j<\infty∑j​ρj​<∞ a.s. and ZnZ_nZn​ converges in law to ∑jρj\sum_j\rho_j∑j​ρj​; if the series diverges, Zn→∞Z_n\to\inftyZn​→∞ in probability; when E(ln⁡σ)E(\ln\sigma)E(lnσ) is defined, the two cases are E(ln⁡σ)<0E(\ln\sigma)<0E(lnσ)<0 and E(ln⁡σ)≥0E(\ln\sigma)\ge0E(lnσ)≥0.

Significance

The result. Theorem (4.4) gives the almost-sure growth rate of the cumulative mean passage time of a random walk in a random environment: linear with slope ν/(1−ν)\nu/(1-\nu)ν/(1−ν) when E(σ)<1E(\sigma)<1E(σ)<1, superlinear otherwise. This is the averaged counterpart of the speed law of §1 of the paper (Theorem (1.16)), where the limiting speed (1−Eσ)/(1+Eσ)(1-E\sigma)/(1+E\sigma)(1−Eσ)/(1+Eσ) is exactly the reciprocal of 1+2ν/(1−ν)1+2\nu/(1-\nu)1+2ν/(1−ν). The superlinear case ν≥1\nu\ge1ν≥1 is the starting point of the paper's §4 limit laws for f(n)(Z1+⋯+Zn)f(n)(Z_1+\dots+Z_n)f(n)(Z1​+⋯+Zn​) (Lemma (4.5) to Theorem (4.9)), which are stated without proof. Lemma (4.2) concerns the single variable ZnZ_nZn​, and its dichotomy is a statement about perpetuities ∑jσ1⋯σj\sum_j\sigma_1\cdots\sigma_j∑j​σ1​⋯σj​.

Formalizing it. The theorem has been proved since 1975; what this mission adds is a machine-checked proof. No result about random difference equations, random products, or this paper is on the platform. The proof needs, for a nonnegative stationary ergodic sequence with possibly infinite mean, the almost-sure convergence of averages in [0,∞][0,\infty][0,∞]. That convergence is not in Mathlib in this form (Mathlib has the i.i.d. strong law for integrable variables, ProbabilityTheory.strong_law_ae), and Birkhoff's pointwise ergodic theorem is posed on the platform as an open item (Birkhoff1931.tendsto_birkhoffAverage_condExp). A completed mission therefore leaves behind a nonnegative, infinite-mean ergodic theorem for block products of i.i.d. sequences, which is reusable well beyond this paper.

Difficulty

The obvious argument fails at independence. ZnZ_nZn​ is a sum of products sharing the factor σn\sigma_nσn​, so Z1,Z2,…Z_1,Z_2,\dotsZ1​,Z2​,… are neither independent nor stationary, and no law of large numbers applies to them directly. The regrouping into YknY_k^nYkn​ produces sums of kkk-dependent block products, which are stationary but not independent, so the i.i.d. strong law does not apply either. Moreover there are nnn such groups at time nnn, so letting kkk and nnn grow together needs a uniform argument: Fatou's lemma gives only the lower bound. The upper bound requires a different object, SnS_nSn​, which is stationary because it looks infinitely far into the past, and it exists only because ν<1\nu<1ν<1 makes the backward series converge. A second trap is the infinite-mean case: σ\sigmaσ may be non-integrable, and every integrability-based ergodic or strong-law statement must be adapted to nonnegative variables with values in [0,∞][0,\infty][0,∞].

Formalization scope

  • Driving sequence. σ : ℕ → Ω → ℝ; the hypotheses (IsIIDNonneg) are on σ1,σ2,…\sigma_1,\sigma_2,\dotsσ1​,σ2​,… (the shifted family n ↦ σ (n + 1)): measurable, pointwise nonnegative, mutually independent (iIndepFun), and identically distributed with σ1\sigma_1σ1​ (IdentDistrib). σ0\sigma_0σ0​ is unused and unconstrained.
  • Expectations are lower Lebesgue integrals in [0,∞][0,\infty][0,∞] (∫⁻). A Bochner integral would return 000 for a non-integrable σ\sigmaσ, which would put ν=0<1\nu=0<1ν=0<1 and make the goal false; this trivializing reading is excluded by the definition of nu.
  • Limits are taken in [0,∞][0,\infty][0,∞]: the averages are mapped there by ENNReal.ofReal, which loses nothing because Zk≥0Z_k\ge0Zk​≥0. In the case ν<1\nu<1ν<1, ν/(1−ν)\nu/(1-\nu)ν/(1−ν) is computed in [0,∞][0,\infty][0,∞] and is finite.
  • Indices. The sums start at k=1k=1k=1 (Finset.Icc 1 n); in YknY_k^nYkn​ the upper limit n+1−kn+1-kn+1−k uses natural-number subtraction, which gives the empty sum for k>nk>nk>n.
  • Two-sided family. Milestone 5 is stated for a separate predicate IsIIDNonnegZ on σ : ℤ → Ω → ℝ; ZnZ_nZn​ is computed from its restriction to N\mathbb NN. This mirrors the page's "without loss of generality"; the goal keeps the one-sided family.
  • Lemma (4.2). One hypothesis is added: σ1\sigma_1σ1​ is not almost surely 111. For σ≡1\sigma\equiv1σ≡1 the series ∑n−1P(ρn>1)\sum n^{-1}P(\rho_n>1)∑n−1P(ρn​>1) vanishes while ∑ρj=∞\sum\rho_j=\infty∑ρj​=∞, so clause (i) fails as printed; the paper's proof cites its Lemma (1.6), which assumes nondegeneracy. "Converges in law" is Mathlib's TendstoInDistribution; "p−lim⁡Zn=∞p-\lim Z_n=\inftyp−limZn​=∞" is P(Zn≤M)→0P(Z_n\le M)\to0P(Zn​≤M)→0 for every MMM; E(ln⁡σ)E(\ln\sigma)E(lnσ) is the difference of the [0,∞][0,\infty][0,∞]-valued expectations of its positive and negative parts, required not to be both infinite, with ln⁡0=−∞\ln0=-\inftyln0=−∞.

Contributions welcome beyond the milestones: an ergodic theorem for nonnegative stationary sequences with values in [0,∞][0,\infty][0,∞]; the identity E(S1)=ν/(1−ν)E(S_1)=\nu/(1-\nu)E(S1​)=ν/(1−ν); and the construction of a two-sided i.i.d. extension of a one-sided sequence, which turns milestone 5 into a statement about the goal's sequence.

Selected references

  • F. Solomon, Random walks in a random environment, The Annals of Probability 3(1):1–31, 1975. https://doi.org/10.1214/aop/1176996444
  • H. Kesten, Random difference equations and renewal theory for products of random matrices, Acta Mathematica 131:207–248, 1973. https://doi.org/10.1007/BF02392040
  • W. Vervaat, On a stochastic difference equation and a representation of non-negative infinitely divisible random variables, Advances in Applied Probability 11(4):750–783, 1979. https://doi.org/10.2307/1426858
  • G. D. Birkhoff, Proof of the ergodic theorem, Proceedings of the National Academy of Sciences 17(12):656–660, 1931. https://doi.org/10.1073/pnas.17.12.656
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Information TheoryOptimizationStatistics·Captain: mikedeng1

I-Divergence Geometry of Probability Distributions and Minimization Problems 1: Cyclic I-Projections onto Linear Sets of a Finite Space Converge to the I-Projection onto Their IntersectionResearch Paper

Motivation

Fitting a probability distribution to prescribed margins or moments is a basic task in statistics and information theory. Starting from a reference distribution, one can enforce one constraint at a time by choosing the closest distribution in I-divergence, then cycle through the constraints. In a contingency table this procedure is iterative proportional fitting. A single projection onto the intersection is the desired answer, but each step of the iteration sees only one constraint set. Csiszár's 1975 paper proves that cyclic I-projections converge to the joint I-projection when the underlying set is finite and the constraint sets are linear. This mission formalizes that result together with the geometric statements needed to identify its limit.

Setting

Let (X,X)(X,\mathcal X)(X,X) be a measurable space. A probability distribution (PD) is a probability measure on it. For PDs PPP and QQQ, the I-divergence I(P∥Q)I(P\|Q)I(P∥Q) is the Kullback–Leibler divergence: integrate the logarithm of the density of PPP relative to QQQ against PPP, with value +∞+\infty+∞ when PPP is not absolutely continuous with respect to QQQ or the integral diverges. It takes values in [0,+∞][0,+\infty][0,+∞] and vanishes exactly when P=QP=QP=Q. The logarithmic conventions are log⁡0=−∞\log0=-\inftylog0=−∞ and 0⋅(±∞)=00\cdot(\pm\infty)=00⋅(±∞)=0 (Csiszár 1975, (1.1)–(1.3)).

Given a PD RRR and a set E\mathcal EE of PDs that contains at least one PPP with finite I(P∥R)I(P\|R)I(P∥R), an I-projection QQQ of RRR onto E\mathcal EE minimizes I(P∥R)I(P\|R)I(P∥R) over P∈EP\in\mathcal EP∈E and itself has finite divergence. The variation distance is the L1L^1L1 distance between the densities of two PDs relative to a common dominating measure. A set of PDs is linear here when every real affine combination of two members that is still a PD also belongs to the set. This includes distributions satisfying fixed linear moment constraints (Csiszár 1975, pp. 147 and 150–151).

For the goal, XXX is finite. Choose k≥1k\ge1k≥1 linear sets E1,…,Ek\mathcal E_1,\ldots,\mathcal E_kE1​,…,Ek​, and write E=⋂i=1kEi\mathcal E=\bigcap_{i=1}^k\mathcal E_iE=⋂i=1k​Ei​. Beginning with Q0=RQ_0=RQ0​=R, let QnQ_nQn​ be the I-projection of Qn−1Q_{n-1}Qn−1​ onto Ei\mathcal E_iEi​ when n=mk+in=mk+in=mk+i and 1≤i≤k1\le i\le k1≤i≤k. The common feasible set is assumed nonempty and contains a PD absolutely continuous with respect to RRR. These assumptions ensure that the intended finite-divergence projection problem is present (Csiszár 1975, Theorem 3.2).

Formalization targets

The goal is the convergence statement of Theorem 3.2:

∀x∈X,Qn({x})⟶Q({x}),Q=proj⁡EI(R).\forall x\in X,\qquad Q_n(\{x\})\longrightarrow Q(\{x\}), \quad Q=\operatorname{proj}^{I}_{\mathcal E}(R).∀x∈X,Qn​({x})⟶Q({x}),Q=projEI​(R).

The goal also asserts existence of the cyclic sequence. On finite XXX, convergence of every point mass is equivalent to convergence in variation distance. The target fixes no rate. Its milestones include existence on variation-closed convex sets (Theorem 2.1), the identity (2.6) and the tangent-hyperplane Lemma 2.1, the Pythagorean characterization and transitivity of I-projections (Theorems 2.2–2.3), the density form under general linear constraints (Theorem 3.1) and the finite-moment exponential-density characterization (Corollary 3.1(A)), and the finite-space identity used in Theorem 3.2's proof. The two displayed identities in that proof are also targets:

I(Q∥R)=I(Q∥Qn)+∑i=1nI(Qi∥Qi−1),I(P∥Qn)=I(P∥Q)+I(Q∥Qn)(P∈E).I(Q\|R)=I(Q\|Q_n)+\sum_{i=1}^{n}I(Q_i\|Q_{i-1}),\qquad I(P\|Q_n)=I(P\|Q)+I(Q\|Q_n)\quad(P\in\mathcal E).I(Q∥R)=I(Q∥Qn​)+i=1∑n​I(Qi​∥Qi−1​),I(P∥Qn​)=I(P∥Q)+I(Q∥Qn​)(P∈E).

They specify the divergence relationships that the eventual convergence theorem must preserve (Csiszár 1975, (3.14)–(3.15)).

Significance

The theorem justifies enforcing finitely many linear distribution constraints one at a time while still obtaining the same I-projection as a simultaneous minimization. It gives a precise limit for the iterative proportional fitting procedure discussed by Csiszár, including cases in which the initial distribution has zero probabilities; strict positivity of RRR is not required (Csiszár 1975, p. 155). The accompanying identities make the relation between a partial iterate and the final solution explicit. The result was proved in 1975. The work here is to provide machine-checked proofs of that known result and its supporting geometry, while keeping the source's extended-value and boundary conventions visible.

Difficulty

Successive projections minimize divergence over different sets. Minimization for one set by itself does not identify the minimizer over their intersection, and ordinary metric projection facts do not directly apply because I-divergence is asymmetric and can be infinite. The paper's statements need to handle zero densities and feasible distributions at infinite divergence without turning extended-real expressions into default values. On the finite space, convergence of a subsequence is available, but the formal claim must still identify every possible limit as the joint I-projection. These are the mathematical and representation difficulties faced by a complete proof (Csiszár 1975, §§2–3).

Formalization scope

Lean uses Measure X and Mathlib's InformationTheory.klDiv : ℝ≥0∞ for I(P∥Q)I(P\|Q)I(P∥Q). A projection is a finite-divergence minimizer over the stated feasible set; no real-valued infimum or implicit arbitrary witness replaces it. Variation distance uses the densities relative to P+QP+QP+Q, which dominates both PDs and gives the value of (1.6). Variation closure is expressed by sequential convergence in this distance. The integral ∫log⁡qR dP\int\log q_R\,dP∫logqR​dP is represented in extended reals using positive and negative logarithmic parts and ENNReal.log; the theorem hypotheses keep the indeterminate +∞−(+∞)+\infty-(+\infty)+∞−(+∞) case out. Density equations are RRR-almost everywhere, and a claim that QQQ has an RRR-density explicitly includes Q≪RQ\ll RQ≪R.

For moment constraints, every integral is accompanied by integrability. Real affine combinations are tested through their values on measurable sets; the candidate combination must be a PD. The goal assumes a finite carrier with measurable singleton sets and k≥1k\ge1k≥1. Lean indexes the sets by Fin k from zero, so Qs (n+1) is projected onto the set at n % k; this is the paper's rule (3.13) shifted by one. The goal asserts existence of a recursive sequence before speaking about every such sequence, and the required feasible witness has P≪RP\ll RP≪R. These choices rule out an empty cyclic schedule, junk integrals, and a vacuous convergence assertion. Reusable contributions include the variation-distance and I-projection interfaces, their Pythagorean geometry, and the finite-moment density characterization; the mission's main closure remains Theorem 3.2.

Selected references

  • I. Csiszár, I-Divergence Geometry of Probability Distributions and Minimization Problems, The Annals of Probability 3(1), 146–158 (1975). DOI: 10.1214/aop/1176996454.
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CombinatoricsOperations ResearchTheoretical Computer Science·Captain: mikedeng1

An Optimal Algorithm for On-line Bipartite Matching 1: RANKING Finds a Matching of Expected Size at Least n(1 − 1/e) − o(n) on Every Graph with a Perfect MatchingResearch Paper

Motivation

Online matching describes allocation when requests must be answered as they arrive. A matching decision uses only the edges revealed so far and cannot be revised when later requests appear. In the bipartite setting studied by Karp, U. Vazirani, and V. Vazirani, the arriving vertices are girls and the possible partners are boys. Even when the full graph has a perfect matching, a fixed greedy priority can leave many girls unmatched. The paper introduced RANKING, which randomly chooses the boys' priority order once and then uses that order for every arrival.

The question is quantitative: how many pairs does RANKING guarantee in expectation against a graph and an arrival order chosen before its random ranking? The paper's target is a fraction approaching 1−1/e1-1/e1−1/e of the nnn pairs in a perfect matching. Its printed Theorem 1 concerns an auxiliary algorithm called EARLY; the RANKING statement follows the intended chain through Lemmas 3 and 5. The original EARLY analysis has a gap for general upper-triangular matrices, so this mission states the RANKING target and the earlier, unaffected lemmas separately. This distinction matters because an assertion about EARLY would be a different formalization target.

Setting

A bipartite graph has a boy side UUU and a girl side VVV, each with nnn vertices. An edge (u,v)(u,v)(u,v) means that boy uuu may be paired with girl vvv. A matching is a collection of edges in which no boy or girl occurs twice. The standing hypothesis for the performance guarantee is that the graph has a perfect matching: some bijection from boys to girls selects an edge for every boy. The graph is otherwise arbitrary.

Girls arrive in a predetermined order. When girl vvv arrives, only her incident edges are revealed. RANKING first chooses a uniformly random permutation π\piπ of the boys. For each arriving girl, it selects the highest-ranked adjacent boy who is still unmatched, if one exists. Write MR(G,π)M_{\mathrm R}(G,\pi)MR​(G,π) for the final matching. The expected size is the finite average over all n!n!n! rankings. The guarantee must hold for every graph and every predetermined arrival order; relabeling girls lets the formal statement fix their order to n,n−1,…,1n,n-1,\ldots,1n,n−1,…,1.

The paper also uses a dual rows-arrive view. Boys arrive in an order and choose among eligible girls, whose priority order is fixed. This is the same greedy rule with the sides exchanged. For its triangular reduction, the columns are numbered 1,…,n1,\ldots,n1,…,n and column nnn has highest priority. An upper-triangular matrix with unit diagonal is a graph with every edge (i,i)(i,i)(i,i) and with an edge (i,j)(i,j)(i,j) only when i≤ji\le ji≤j. On such a graph, the auxiliary algorithm EARLY declines to match row iii if column iii is already covered by EARLY's own matching. For any matching MMM, D(M)D(M)D(M) denotes the indices for which both row iii and column iii are covered.

Formalization targets

RANKING guarantee

For every ε>0\varepsilon>0ε>0, one threshold NNN must work for every size n≥Nn\ge Nn≥N and every graph GGG with a perfect matching:

Eπ∼Unif(Sn)∣MR(G,π)∣≥(1−e−1−ε)n.\mathbb E_{\pi\sim\mathrm{Unif}(S_n)}|M_{\mathrm R}(G,\pi)| \ge (1-e^{-1}-\varepsilon)n.Eπ∼Unif(Sn​)​∣MR​(G,π)∣≥(1−e−1−ε)n.

This is the uniform lower-bound reading of the paper's n(1−1/e)−o(n)n(1-1/e)-o(n)n(1−1/e)−o(n) target. It does not prescribe a finite-nnn additive constant. The mission goal is the RANKING assertion drawn from the paper's Theorem 1 and Lemmas 3 and 5. The six milestones formalize the paper's Lemmas 1–5 and the corollary to Lemma 4, in their source order. They cover the side-exchange identity, arbitrary refusal algorithms, the triangular reduction, the matching-count identity, its expected form, and the pointwise comparison with EARLY.

Significance

The guarantee gives a concrete worst-case floor for a simple randomized allocation rule: as the graph size grows, RANKING matches at least an asymptotic 1−1/e1-1/e1−1/e fraction of the pairs available in a perfect matching, in expectation. The order is selected before the random permutation, matching the paper's performance measure. The lower bound remains meaningful on sparse graphs and does not rely on a density assumption. The original paper also studies the limit on what any randomized online algorithm can guarantee; that upper-bound result is treated in a separate mission.

A formal development here would provide reusable finite definitions for online greedy matching, arbitrary state-dependent refusal, fixed-order duality, and uniform expectation over permutations. The goal is a theorem statement awaiting a machine-checked proof; compiling the draft declarations verifies their Lean syntax and types, not their truth. The local mission separates the valid early structural statements from later statements whose published EARLY argument does not justify them on general upper-triangular graphs.

Difficulty

The random permutation does not make the fate of different vertices independent. Matching one girl removes a boy who might be essential to a later girl, so a per-arrival probability estimate cannot simply be added across all arrivals. The dual and triangular views capture useful structure, but turning that structure into a uniform bound for every graph is the main obstacle. In particular, reasoning about EARLY as if its matched-column set had the same monotonicity as unrestricted RANKING fails on some upper-triangular matrices. A proof of the goal must establish the RANKING guarantee without treating those later EARLY statements as available facts.

Formalization scope

Boys and girls are both Fin n; an adjacency matrix is a relation between them. A published predicate represents a perfect matching as an edge-preserving bijection. The generic greedy run processes arrival times in increasing order and interprets a smaller priority index as higher rank. It makes a new matching decision only from the current matching and the arriving vertex. RANKING's returned edges are consistently ordered as (boy, girl), even though girls arrive. The dual run has rows arriving in an arbitrary permutation and takes column n−1n-1n−1 as highest priority in Lean's zero-based numbering. EARLY's refusal test consults the matching constructed by EARLY itself.

All expectations are finite averages over Equiv.Perm (Fin n), scaled by 1/n!1/n!1/n!. The formal o(n)o(n)o(n) claim is ∀ε>0, ∃N, ∀n≥N, ∀G\forall\varepsilon>0,\ \exists N,\ \forall n\ge N,\ \forall G∀ε>0, ∃N, ∀n≥N, ∀G with a perfect matching, the displayed lower bound. Placing NNN before GGG preserves the worst-case meaning. The perfect-matching condition is essential: the empty graph cannot satisfy a positive linear guarantee. The triangular matrix in Lemma 3 retains every diagonal edge, so a zero matrix cannot witness the reduction. These conventions rule out vacuous versions of the goal and reduction.

The definitions of partial matching, covered vertices, greedy run, RANKING, EARLY, and uniform average are part of the mission. A complete proof may build further finite counting and permutation machinery; such lemmas can be shared beyond this paper. Contributions toward the six milestone statements, the goal, and faithful supporting results are in scope. Lemmas 6–12 and the printed EARLY Theorem 1 are outside this mission because their analysis depends on claims that fail for some matrices allowed by their surrounding assumptions.

Selected references

  • Richard M. Karp, Umesh V. Vazirani, and Vijay V. Vazirani, An Optimal Algorithm for On-line Bipartite Matching, Proceedings of the 22nd Annual ACM Symposium on Theory of Computing, 1990, pp. 352–358. DOI: 10.1145/100216.100262.
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Supply Chain Coordination with Contracts IV: Competing Newsvendors with Proportional Allocation Have a Unique Equilibrium, and a Coordinating Buy-Back Gives the Supplier ((p(n − 1) + b)/(pn))Π(q°)Textbook

Why competing retailers change the contracting problem

A supplier who sells through a single newsvendor retailer faces double marginalization: the retailer bears the whole cost of leftover stock but earns only the retail margin, so under a plain wholesale-price contract he orders less than the integrated supply chain would. The literature reviewed in G. P. Cachon's chapter Supply Chain Coordination with Contracts (Handbooks in OR & MS, vol. 11, 2003) shows that buy-back, revenue-sharing and related contracts correct this distortion. Section 6.5 asks what happens when the supplier sells through several retailers who compete for the same customers.

Competition can push in the opposite direction. When customers buy wherever stock is available, a retailer who stocks more also takes demand from his rivals, and he does not count that loss as a cost. This demand-stealing effect pushes the retailers towards over-ordering, which offsets double marginalization. §6.5.1 makes this precise in the proportional allocation model, in which total demand is split among the retailers in proportion to their inventories. The model goes back to the deterministic version of Wang and Gerchak (2001); related allocation models are those of Lippman and McCardle (1997) and Anupindi and Bassok (1999), and Mahajan and van Ryzin (2001) observe the same mitigation of the need for coordinating contracts.

This mission formalizes §6.5.1 of the chapter's January 2003 third draft, pp. 48–53.

The proportional allocation model

There are n≥2n \ge 2n≥2 retailers and one supplier. Total retail demand D≥0D \ge 0D≥0 is random, with distribution function FFF that is differentiable on (0,∞)(0,\infty)(0,∞) with density fff, strictly increasing on [0,∞)[0,\infty)[0,∞), and satisfies F(0)=0F(0)=0F(0)=0. The retail price is ppp and the supplier's unit production cost is ccc, with 0<c<p0 < c < p0<c<p. Goodwill costs, the salvage value and the retailers' handling cost are zero.

Retailer iii orders qi≥0q_i \ge 0qi​≥0. Write q=∑jqjq = \sum_j q_jq=∑j​qj​ and q−i=q−qiq_{-i} = q - q_iq−i​=q−qi​. Retailer iii receives the demand Di=(qi/q)DD_i = (q_i/q)DDi​=(qi​/q)D. Under a buy-back contract (w,b)(w, b)(w,b) he pays www per unit ordered and is refunded bbb per unit left over; b=0b = 0b=0 is the wholesale-price contract. His expected profit is

πi(qi,q−i)=E[pmin⁡(qi,Di)+b(qi−Di)+]−wqi=(p−w)qi−(p−b)qiq∫0qF(x) dx.\pi_i(q_i, q_{-i}) = \mathbb E\big[p\min(q_i, D_i) + b(q_i - D_i)^+\big] - wq_i = (p-w)q_i - (p-b)\frac{q_i}{q}\int_0^q F(x)\,dx .πi​(qi​,q−i​)=E[pmin(qi​,Di​)+b(qi​−Di​)+]−wqi​=(p−w)qi​−(p−b)qqi​​∫0q​F(x)dx.

Because total sales min⁡(q,D)\min(q, D)min(q,D) depend only on the total stock, the integrated chain earns Π(q)=pS(q)−cq\Pi(q) = pS(q) - cqΠ(q)=pS(q)−cq with S(q)=E[min⁡(q,D)]S(q) = \mathbb E[\min(q,D)]S(q)=E[min(q,D)], and its optimal stock qoq^oqo solves the newsvendor equation F(qo)=(p−c)/pF(q^o) = (p-c)/pF(qo)=(p−c)/p, Eq. (20). A Nash equilibrium is a profile of orders in which each qi∗q^*_iqi∗​ maximizes πi(⋅,q−i∗)\pi_i(\cdot, q^*_{-i})πi​(⋅,q−i∗​) over all orders x≥0x \ge 0x≥0. A contract coordinates the chain when its equilibrium total order is qoq^oqo.

Two contract prices appear on p. 52: the wholesale price w^(q)=p(1−1nF(q)−n−1n⋅1q∫0qF)\widehat w(q) = p\big(1 - \tfrac1n F(q) - \tfrac{n-1}{n}\cdot\tfrac1q\int_0^qF\big)w(q)=p(1−n1​F(q)−nn−1​⋅q1​∫0q​F) that induces total stock qqq, and the buy-back wholesale price

wb(b)=p−(p−b)[1n⋅p−cp+n−1n⋅1qo∫0qoF(x) dx].w_b(b) = p - (p-b)\left[\frac1n\cdot\frac{p-c}{p} + \frac{n-1}{n}\cdot\frac{1}{q^o}\int_0^{q^o}F(x)\,dx\right].wb​(b)=p−(p−b)[n1​⋅pp−c​+nn−1​⋅qo1​∫0qo​F(x)dx].

Formalization targets

Goal: the coordinating buy-back contract (pp. 51–53)

For n≥2n \ge 2n≥2, b<pb < pb<p and qoq^oqo solving (20), with w=wb(b)w = w_b(b)w=wb​(b): qoq^oqo maximizes Π\PiΠ; b<wb(b)<pb < w_b(b) < pb<wb​(b)<p; the profile in which every retailer orders qo/nq^o/nqo/n is the unique Nash equilibrium; and at that equilibrium

πi=p−bpn2 Π(qo),πs=wqo−cqo−b E[(qo−D)+]=p(n−1)+bpn Π(qo).\pi_i = \frac{p-b}{pn^2}\,\Pi(q^o), \qquad \pi_s = wq^o - cq^o - b\,\mathbb E[(q^o-D)^+] = \frac{p(n-1)+b}{pn}\,\Pi(q^o).πi​=pn2p−b​Π(qo),πs​=wqo−cqo−bE[(qo−D)+]=pnp(n−1)+b​Π(qo).

Milestones

The milestones are the section's own claims, in attack order: the newsvendor characterization (20); the inequality 1q∫0qF<F(q)\frac1q\int_0^qF < F(q)q1​∫0q​F<F(q); the closed form of πi\pi_iπi​ and its strict concavity in the retailer's own order (p. 50); the first-order condition and Eq. (21); the monotonicity and limits of the left side LnL_nLn​ of Eq. (22), giving a unique root for b<w<pb < w < pb<w<p; the unique, symmetric Nash equilibrium for every b<w<pb < w < pb<w<p; the increase of the equilibrium total in nnn; that w^(q)\widehat w(q)w(q) induces qqq, that w^(qo)>c\widehat w(q^o) > cw(qo)>c, and that the supplier's profit under wholesale pricing has negative slope at qoq^oqo; the coordinating price wb(b)w_b(b)wb​(b) with wb(b)>w^(qo)w_b(b) > \widehat w(q^o)wb​(b)>w(qo) for b>0b > 0b>0; and the ratio πs(qo,wb(0),0)/Π(qo)=(n−1)/n\pi_s(q^o, w_b(0), 0)/\Pi(q^o) = (n-1)/nπs​(qo,wb​(0),0)/Π(qo)=(n−1)/n (p. 53). A companion item states the endpoint b=pb = pb=p, at which the supplier takes all of Π(qo)\Pi(q^o)Π(qo).

Significance

The section answers two questions. First, with competing retailers a plain wholesale-price contract can coordinate the chain and still leave the supplier a positive margin, which a single retailer never allows. Second, that contract is not the supplier's best wholesale price, and it fixes a single division of profit. Buy-back contracts remove both limitations: the family (wb(b),b)(w_b(b), b)(wb​(b),b) coordinates for every b<pb < pb<p and moves the supplier's share continuously from (n−1)/n(n-1)/n(n−1)/n to all of Π(qo)\Pi(q^o)Π(qo). The ratio (n−1)/n(n-1)/n(n−1)/n also measures how little a coordinating contract adds when many retailers compete (80% of the optimal profit at n=5n = 5n=5).

The results are proved in the chapter, mostly by short computations, and none of them has been machine-checked. The formalization makes explicit what the page leaves implicit: that no equilibrium has a retailer ordering zero, the limits behind "from 0 to 1", and the density condition behind the strict sign on p. 52. It also produces a reusable proportional-allocation game and a Nash-equilibrium predicate for nonnegative real strategies.

Difficulty

The algebraic identities (the profits at the coordinating contract, the ratio (n−1)/n(n-1)/n(n−1)/n, the derivative at qoq^oqo) are routine once πi\pi_iπi​ has its closed form. The closed form itself requires computing the expectation with proportional shares and identifying E[min⁡(q,D)]\mathbb E[\min(q,D)]E[min(q,D)] with q−∫0qFq - \int_0^q Fq−∫0q​F.

The real obstacle is the uniqueness of the equilibrium. The page argues from first-order conditions, which describe only interior best responses. A complete proof must show that each retailer's profit is strictly concave in his own order, that no retailer orders zero in equilibrium, and that the all-zero profile (where πi\pi_iπi​ has q=0q = 0q=0 in a denominator) is not an equilibrium. Strict concavity is the delicate step. The second derivative mixes the density with the term 2q−iq3(qF(q)−∫0qF)\frac{2q_{-i}}{q^3}\big(qF(q) - \int_0^qF\big)q32q−i​​(qF(q)−∫0q​F), and concavity has to be established on the closed half-line, including the boundary qi=0q_i = 0qi​=0.

Formalization scope

Retailers are indexed by Fin n with n≥2n \ge 2n≥2 (the page's n>1n > 1n>1). The comparison in nnn also allows a single retailer, as the page does. Orders are real numbers qi≥0q_i \ge 0qi​≥0, and best responses range over all x≥0x \ge 0x≥0. The demand law is a probability measure on R\mathbb RR carried by [0,∞)[0,\infty)[0,∞) with finite mean, FFF is its cdf, and fff is a field with HasDerivAt F (f y) y for y>0y > 0y>0. These are the chapter's standing assumptions (p. 7). The condition c>0c > 0c>0 is needed for (20) to have a solution. The integrated optimum qoq^oqo enters each theorem through the hypothesis F(qo)=(p−c)/pF(q^o) = (p-c)/pF(qo)=(p−c)/p, which determines it uniquely. Transfers run from the retailers to the supplier.

Added or made explicit relative to the page: b<pb < pb<p in the concavity claim (at b=pb = pb=p the profit is linear); f(qo)>0f(q^o) > 0f(qo)>0 for the strict sign of the supplier's marginal profit; positivity of the total order wherever 1q∫0qF\frac1q\int_0^qFq1​∫0q​F appears. The page's printed slips (the first-order condition rescaled by q∗/(p−b)q^*/(p-b)q∗/(p−b), "F(qo)=(p−c)/cF(q^o) = (p-c)/cF(qo)=(p−c)/c", "w(b)w(b)w(b)") are corrected in the statements and kept in the milestone quotes.

Ruled out as trivializing: w^\widehat ww and wbw_bwb​ are the printed formulas, not "the price at which qoq^oqo is an equilibrium"; the supplier's profit is computed from the transfers, not as Π\PiΠ minus the retailers' profits; the equilibrium statement quantifies over all nonnegative deviations, so restricting attention to interior or symmetric profiles is not an option.

A complete development needs interval integrals of a cdf, the fundamental theorem of calculus for q↦∫0qFq \mapsto \int_0^qFq↦∫0q​F, and strict concavity from a strictly decreasing derivative. The proportional-allocation game and the Nash predicate are reusable for the other allocation models of §6.5. No platform item is referenced: the competing-retailer game of Cachon and Lariviere (2005), RevShareCoord.Competing.*, uses deterministic revenue functions and is a different model.

Selected references

  • G. P. Cachon, Supply Chain Coordination with Contracts, in S. Graves and T. de Kok (eds.), Handbooks in Operations Research and Management Science, vol. 11, North-Holland, 2003; read in the author's 3rd draft (Jan. 2003), §6.5.1. https://doi.org/10.1016/S0927-0507(03)11006-7
  • Y. Wang and Y. Gerchak, Supply chain coordination when demand is shelf-space dependent, Manufacturing & Service Operations Management 3(1), 2001, 82–87. https://doi.org/10.1287/msom.3.1.82.9998
  • S. A. Lippman and K. F. McCardle, The competitive newsboy, Operations Research 45(1), 1997, 54–65. https://doi.org/10.1287/opre.45.1.54
  • S. Mahajan and G. van Ryzin, Inventory competition under dynamic consumer choice, Operations Research 49(5), 2001, 646–657. https://doi.org/10.1287/opre.49.5.646.10603
  • G. P. Cachon and M. A. Lariviere, Supply chain coordination with revenue-sharing contracts: strengths and limitations, Management Science 51(1), 2005, 30–44. https://doi.org/10.1287/mnsc.1040.0215
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CombinatoricsStatistics·Captain: mikedeng1

Two Moments Suffice for Poisson Approximations: The Chen-Stein Method 2: A Dependent Bernoulli Process Is Within 2(2b₁+2b₂+b₃) of a Poisson Process in Total VariationResearch Paper

Motivation

Many counting problems in probability, combinatorics and statistics ask for the law of the number of occurrences of rare, weakly dependent events: long head runs in coin tossing, matching segments between two DNA sequences, isolated vertices or small subgraphs in a random graph, clusters of points in a scan statistic. Chen's 1975 adaptation of Stein's method gives an explicit error bound for approximating such a count by a Poisson law. Arratia, Goldstein and Gordon (Ann. Probab. 17 (1989) 9–25) recast it in terms of a neighbourhood of dependence for each event. In this form the error bound needs only the first two moments of the indicators whenever each event is independent of the events outside its neighbourhood. The paper's examples (head runs, DNA sequence matching, birthday-type problems) made this form standard in applied probability.

The paper has two main results. Theorem 1 bounds the distance between the law of the total count and a Poisson law; it is essentially contained in Chen (1975). Theorem 2, which the authors describe as new, is a process version. It compares the joint law of all the indicators, that is, where the events occur, with a Poisson process. Theorem 3, a corollary, compares a dependent family of events with an independent family having the same marginal probabilities. This mission formalizes Theorem 2, the finite-dimensional bound it is derived from, the steps of its proof in §6, and Theorem 3.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space and III an index set. For α∈I\alpha\in Iα∈I let XαX_\alphaXα​ be a Bernoulli random variable, Xα∈{0,1}X_\alpha\in\{0,1\}Xα​∈{0,1}, with

pα=P(Xα=1)>0,λ=∑α∈Ipα∈(0,∞).p_\alpha=P(X_\alpha=1)>0,\qquad \lambda=\sum_{\alpha\in I}p_\alpha\in(0,\infty).pα​=P(Xα​=1)>0,λ=α∈I∑​pα​∈(0,∞).

For each α\alphaα fix a set Bα⊆IB_\alpha\subseteq IBα​⊆I with α∈Bα\alpha\in B_\alphaα∈Bα​, the neighbourhood of dependence of α\alphaα. Put pαβ=E(XαXβ)p_{\alpha\beta}=E(X_\alpha X_\beta)pαβ​=E(Xα​Xβ​) and

b1=∑α∈I∑β∈Bαpαpβ,b2=∑α∈I∑α≠β∈Bαpαβ,b3=∑α∈IE∣E{Xα−pα∣σ(Xβ:β∈I−Bα)}∣.b_1=\sum_{\alpha\in I}\sum_{\beta\in B_\alpha}p_\alpha p_\beta,\qquad b_2=\sum_{\alpha\in I}\sum_{\alpha\neq\beta\in B_\alpha}p_{\alpha\beta},\qquad b_3=\sum_{\alpha\in I}E\bigl|E\{X_\alpha-p_\alpha\mid\sigma(X_\beta:\beta\in I-B_\alpha)\}\bigr|.b1​=α∈I∑​β∈Bα​∑​pα​pβ​,b2​=α∈I∑​α=β∈Bα​∑​pαβ​,b3​=α∈I∑​E​E{Xα​−pα​∣σ(Xβ​:β∈I−Bα​)}​.

Roughly, b1b_1b1​ measures the size of the neighbourhoods, b2b_2b2​ the expected number of neighbours of an occurrence, and b3b_3b3​ the dependence between an event and the events outside its neighbourhood. In many applications XαX_\alphaXα​ is independent of σ(Xβ:β∉Bα)\sigma(X_\beta:\beta\notin B_\alpha)σ(Xβ​:β∈/Bα​), so b3=0b_3=0b3​=0.

The dependent Bernoulli process is X=(Xα)α∈I\mathbf X=(X_\alpha)_{\alpha\in I}X=(Xα​)α∈I​, a random element of Z+I\mathbb Z_+^IZ+I​. The Poisson process on III with intensity p(⋅)p_{(\cdot)}p(⋅)​ is Y=(Yα)α∈I\mathbf Y=(Y_\alpha)_{\alpha\in I}Y=(Yα​)α∈I​ with the YαY_\alphaYα​ mutually independent and YαY_\alphaYα​ Poisson with mean pαp_\alphapα​.

Distances are measured in the paper's total variation norm,

∥L(U)−L(V)∥=sup⁡∥h∥=1∣Eh(U)−Eh(V)∣=2sup⁡A∣P(U∈A)−P(V∈A)∣,\|\mathcal L(U)-\mathcal L(V)\|=\sup_{\|h\|=1}|Eh(U)-Eh(V)|=2\sup_A|P(U\in A)-P(V\in A)|,∥L(U)−L(V)∥=∥h∥=1sup​∣Eh(U)−Eh(V)∣=2Asup​∣P(U∈A)−P(V∈A)∣,

which is twice the usual total variation distance.

Formalization targets

Goal: Theorem 2

∥L(X)−L(Y)∥≤2(2b1+2b2+b3).\|\mathcal L(\mathbf X)-\mathcal L(\mathbf Y)\|\le2(2b_1+2b_2+b_3).∥L(X)−L(Y)∥≤2(2b1​+2b2​+b3​).

The bound has no dependence on λ\lambdaλ and no assumption on III beyond countability (which the setting forces).

Milestones, in attack order

  1. TiSih=hT_iS_ih=hTi​Si​h=h (§6, p. 22). For functions on Z+d\mathbb Z_+^dZ+d​, the coordinatewise Stein operators (Tif)(j)=jif(j)−λif(j+ei)(T_if)(j)=j_if(j)-\lambda_if(j+e_i)(Ti​f)(j)=ji​f(j)−λi​f(j+ei​) and (Sih)(j+ei)=−(λiP(Zi=ji))−1E{h(j1,…,Zi,…,jd)1(Zi≤ji)}(S_ih)(j+e_i)=-(\lambda_iP(Z_i=j_i))^{-1}E\{h(j_1,\dots,Z_i,\dots,j_d)1(Z_i\le j_i)\}(Si​h)(j+ei​)=−(λi​P(Zi​=ji​))−1E{h(j1​,…,Zi​,…,jd​)1(Zi​≤ji​)} satisfy TiSih=hT_iS_ih=hTi​Si​h=h.
  2. Bounds on fi=Si(h−Pih)f_i=S_i(h-P_ih)fi​=Si​(h−Pi​h) (§6, p. 22), where PihP_ihPi​h averages hhh over a Poisson(λi\lambda_iλi​) iii-th coordinate. For ∥h∥≤1\|h\|\le1∥h∥≤1, ∥fi∥<2(1∧1.4λi−1/2)\|f_i\|<2(1\wedge1.4\lambda_i^{-1/2})∥fi​∥<2(1∧1.4λi−1/2​) and ∥Δkfi∥<4(1∧1.4λi−1/2)\|\Delta_kf_i\|<4(1\wedge1.4\lambda_i^{-1/2})∥Δk​fi​∥<4(1∧1.4λi−1/2​).
  3. Display (15) (p. 24). E{(Xα−pα)(f(U+Xβek)−f(U))}≤2∥f∥(pαβ+pαpβ)E\{(X_\alpha-p_\alpha)(f(U+X_\beta e_k)-f(U))\}\le2\|f\|(p_{\alpha\beta}+p_\alpha p_\beta)E{(Xα​−pα​)(f(U+Xβ​ek​)−f(U))}≤2∥f∥(pαβ​+pα​pβ​) for any random UUU.
  4. Displays (13)–(14), the step i=1i=1i=1 (p. 23). With Wj=∑α∈I(j)XαW_j=\sum_{\alpha\in I(j)}X_\alphaWj​=∑α∈I(j)​Xα​ the block sums of a partition and Z1Z_1Z1​ an independent Poisson(λ1\lambda_1λ1​),
∣Eh(W1,…,Wd)−Eh(Z1,W2,…,Wd)∣≤2∥f1∥∑I(1)pα2+2∥f1∥∑I(1)∑α≠β∈Bα(pαβ+pαpβ)+∥f1∥∑I(1)sα.|Eh(W_1,\dots,W_d)-Eh(Z_1,W_2,\dots,W_d)|\le2\|f_1\|\sum_{I(1)}p_\alpha^2+2\|f_1\|\sum_{I(1)}\sum_{\alpha\ne\beta\in B_\alpha}(p_{\alpha\beta}+p_\alpha p_\beta)+\|f_1\|\sum_{I(1)}s_\alpha.∣Eh(W1​,…,Wd​)−Eh(Z1​,W2​,…,Wd​)∣≤2∥f1​∥I(1)∑​pα2​+2∥f1​∥I(1)∑​α=β∈Bα​∑​(pαβ​+pα​pβ​)+∥f1​∥I(1)∑​sα​.
  1. The finite-dimensional bound (Theorem 2, p. 11). For a partition of III into nonempty blocks I(1),…,I(d)I(1),\dots,I(d)I(1),…,I(d) with Wj=∑I(j)XαW_j=\sum_{I(j)}X_\alphaWj​=∑I(j)​Xα​, Zj=∑I(j)YαZ_j=\sum_{I(j)}Y_\alphaZj​=∑I(j)​Yα​ and λj=EWj\lambda_j=EW_jλj​=EWj​:
∥L((W1,…,Wd))−L((Z1,…,Zd))∥≤2(1∧1.4(min⁡iλi)−1/2)(2b1+2b2+b3).\|\mathcal L((W_1,\dots,W_d))-\mathcal L((Z_1,\dots,Z_d))\|\le2\bigl(1\wedge1.4(\min_i\lambda_i)^{-1/2}\bigr)(2b_1+2b_2+b_3).∥L((W1​,…,Wd​))−L((Z1​,…,Zd​))∥≤2(1∧1.4(imin​λi​)−1/2)(2b1​+2b2​+b3​).

Companion results

  • Theorem 3 (p. 12). For an independent Bernoulli process X′\mathbf X'X′ with the same marginals as X\mathbf XX, ∥L(X)−L(X′)∥≤2(2b1+2b2+b3)+4∑pα2\|\mathcal L(\mathbf X)-\mathcal L(\mathbf X')\|\le2(2b_1+2b_2+b_3)+4\sum p_\alpha^2∥L(X)−L(X′)∥≤2(2b1​+2b2​+b3​)+4∑pα2​.
  • The remark after Theorem 3. ∥L(X′)−L(Y)∥≤2∑pα2\|\mathcal L(\mathbf X')-\mathcal L(\mathbf Y)\|\le2\sum p_\alpha^2∥L(X′)−L(Y)∥≤2∑pα2​, so 4∑pα24\sum p_\alpha^24∑pα2​ in Theorem 3 can be replaced by 2∑pα22\sum p_\alpha^22∑pα2​.

Significance

The result. Theorem 2 says that when b1b_1b1​, b2b_2b2​, b3b_3b3​ are small, the set of indices at which the dependent events occur is close in law to a Poisson process with the same intensity. The bound covers every event about the locations, not just the total count. It is in the strong total variation norm and needs only moment information when b3=0b_3=0b3​=0. Theorem 3 turns this into a decoupling statement: a dependent family of rare events is almost indistinguishable from an independent family with the same marginals. The process bound is the form used when the positions of rare events matter, for example in the distribution of the location of the longest match in sequence comparison and in scan statistics.

Formalizing it. The results are proved in the paper; none is machine-checked. A formal development would give a Lean statement and proof of a Chen–Stein bound with explicit constants, for countable index sets and arbitrary dependence. It would also include the coordinatewise Stein operators on Z+d\mathbb Z_+^dZ+d​ and the bounds on their solutions, which are reusable for other multivariate Poisson approximations. A companion mission formalizes Theorem 1, including Lemma 1 (the bounds on the one-variable Stein solution) on which milestone 2 rests.

Difficulty

The total variation distance between two laws on Z+I\mathbb Z_+^IZ+I​ cannot be bounded coordinate by coordinate, because the XαX_\alphaXα​ are dependent. The one-variable Stein equation controls only the law of a single integer-valued statistic. The paper passes through finite-dimensional block sums and replaces the coordinates one at a time. At each replacement the error has to be charged to the terms of b1,b2,b3b_1,b_2,b_3b1​,b2​,b3​ indexed by the current block, so that the total over all blocks reproduces 2b1+2b2+b32b_1+2b_2+b_32b1​+2b2​+b3​ without a factor ddd. Two further points need care. First, the bound ∥Δkf1∥≤2∥f1∥\|\Delta_kf_1\|\le2\|f_1\|∥Δk​f1​∥≤2∥f1​∥ is the only one available for differences in a coordinate other than the one being replaced; this is why the constants are larger than in Theorem 1. Second, the infinite index set requires a limiting argument from finitely many blocks to the full process.

Formalization scope

  • The index set is a countable type. The page says "arbitrary index set", but pα>0p_\alpha>0pα​>0 and ∑pα<∞\sum p_\alpha<\infty∑pα​<∞ force countability; the assumption also makes X\mathbf XX measurable as a map into NI\mathbb N^INI with the product σ-algebra.
  • The XαX_\alphaXα​ are measurable, N\mathbb NN-valued and bounded by 111. pαp_\alphapα​ is P(Xα=1)P(X_\alpha=1)P(Xα​=1). The standing hypotheses pα>0p_\alpha>0pα​>0, ∑pα=λ\sum p_\alpha=\lambda∑pα​=λ and λ>0\lambda>0λ>0 are explicit.
  • b1,b2,b3b_1,b_2,b_3b1​,b2​,b3​ and sαs_\alphasα​ are [0,∞][0,\infty][0,∞]-valued, and every bound is an inequality in [0,∞][0,\infty][0,∞], so a divergent series is never read as 000. The conditional expectation in sαs_\alphasα​ is taken with respect to a σ-algebra generated by measurable maps, hence a genuine sub-σ-algebra.
  • The norm ∥L(U)−L(V)∥\|\mathcal L(U)-\mathcal L(V)\|∥L(U)−L(V)∥ is twice the published definition MarkovChainCLT.tvDist (supremum over measurable sets of ∣μ(A)−ν(A)∣|\mu(A)-\nu(A)|∣μ(A)−ν(A)∣). Dropping the factor 222 would make the goal twice as strong and false in general.
  • Y\mathbf YY (and X′\mathbf X'X′ in Theorem 3) lives on its own probability space. Mutual independence of the YαY_\alphaYα​ and of the Xα′X'_\alphaXα′​ is a hypothesis. Without it the law of the process is not determined by the marginals and the statements are false.
  • Block sums WjW_jWj​ are N\mathbb NN-valued tsums, equal to the true sums almost surely. A partition is a surjection I→{1,…,d}I\to\{1,\dots,d\}I→{1,…,d} (Fin d), so Lean's coordinate 0 is the paper's coordinate 111.
  • (Sih)(j)(S_ih)(j)(Si​h)(j) is set to 000 when ji=0j_i=0ji​=0, as for SSS in §4. The strict inequalities in milestone 2 use the actual sup norms over Z+d\mathbb Z_+^dZ+d​.

Needed infrastructure: product measures and independence on NI\mathbb N^INI, Poisson laws (Mathlib's poissonMeasure), conditional expectation, and a one-variable Stein bound (Lemma 1). Contributions of proofs of any milestone, of the general step iii of §6, and of the one-dimensional Lemma 1 are welcome.

Selected references

  • R. Arratia, L. Goldstein, L. Gordon, Two moments suffice for Poisson approximations: the Chen-Stein method, Ann. Probab. 17(1) (1989) 9–25. https://doi.org/10.1214/aop/1176991491
  • L. H. Y. Chen, Poisson approximation for dependent trials, Ann. Probab. 3(3) (1975) 534–545. https://doi.org/10.1214/aop/1176996359
  • A. D. Barbour, G. K. Eagleson, Poisson approximation for some statistics based on exchangeable trials, Adv. Appl. Probab. 15(3) (1983) 585–600. https://doi.org/10.2307/1426620
  • A. D. Barbour, L. Holst, S. Janson, Poisson Approximation, Oxford University Press, 1992. https://global.oup.com/academic/product/poisson-approximation-9780198522355
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CombinatoricsStatistics·Captain: mikedeng1

Two Moments Suffice for Poisson Approximations: The Chen-Stein Method 1: Total Variation Bound 2[(b₁+b₂)(1−e^{−λ})/λ + b₃′(1∧1.4λ^{−1/2})] for a Sum of Dependent IndicatorsResearch Paper

Motivation

Counts of rare events often look Poisson even when the events are dependent. For example, a local pattern in a random graph can overlap another copy of the pattern, so the corresponding occurrence indicators are not independent. The useful question is quantitative: how far is the distribution of the total count from a Poisson distribution with the same mean? Arratia, Goldstein and Gordon give a bound in terms of three quantities that can be estimated from neighbourhoods of dependence. Their 1989 paper applies the Chen–Stein method to the count and then to the full point process. This mission concerns the count bound, Theorem 1.

The authors explain that the result is essentially contained in Chen’s earlier work, while their one-variable proof prepares the process result in Theorem 2. The bound remains useful as a precise statement of the dependence conditions under which the Poisson approximation works. The process theorem belongs to the companion mission.

Setting

Let III index Bernoulli indicators XαX_\alphaXα​, each taking values in {0,1}\{0,1\}{0,1} on a probability space with law PPP. Write pα=P(Xα=1)>0p_\alpha=P(X_\alpha=1)>0pα​=P(Xα​=1)>0, and let

W=∑α∈IXα,λ=EW=∑α∈Ipα∈(0,∞).W=\sum_{\alpha\in I}X_\alpha,\qquad \lambda=E W=\sum_{\alpha\in I}p_\alpha\in(0,\infty).W=α∈I∑​Xα​,λ=EW=α∈I∑​pα​∈(0,∞).

For each α\alphaα, choose a dependence neighbourhood Bα⊆IB_\alpha\subseteq IBα​⊆I containing α\alphaα. The neighbourhoods need not be symmetric, and the theorem imposes no independence condition: dependence on indicators outside BαB_\alphaBα​ is measured directly. Define pαβ=E(XαXβ)p_{\alpha\beta}=E(X_\alpha X_\beta)pαβ​=E(Xα​Xβ​) and

b1=∑α∑β∈Bαpαpβ,b2=∑α∑β∈Bαβ≠αpαβ.\begin{aligned} b_1&=\sum_\alpha\sum_{\beta\in B_\alpha}p_\alpha p_\beta,\\ b_2&=\sum_\alpha\sum_{\substack{\beta\in B_\alpha\\\beta\ne\alpha}}p_{\alpha\beta}. \end{aligned}b1​b2​​=α∑​β∈Bα​∑​pα​pβ​,=α∑​β∈Bα​β=α​∑​pαβ​.​

The remaining quantities use conditional expectation. Let Vα=∑β∉BαXβV_\alpha=\sum_{\beta\notin B_\alpha}X_\betaVα​=∑β∈/Bα​​Xβ​, and let Fα\mathcal F_\alphaFα​ be the sigma algebra generated by all XβX_\betaXβ​ outside BαB_\alphaBα​. Put

sα′=E∣E[Xα−pα∣Vα]∣,b3′=∑αsα′,sα=E∣E[Xα−pα∣Fα]∣,b3=∑αsα.\begin{aligned} s'_\alpha&=E\left|E[X_\alpha-p_\alpha\mid V_\alpha]\right|, & b'_3&=\sum_\alpha s'_\alpha,\\ s_\alpha&=E\left|E[X_\alpha-p_\alpha\mid\mathcal F_\alpha]\right|, & b_3&=\sum_\alpha s_\alpha. \end{aligned}sα′​sα​​=E∣E[Xα​−pα​∣Vα​]∣,=E∣E[Xα​−pα​∣Fα​]∣,​b3′​b3​​=α∑​sα′​,=α∑​sα​.​

Conditioning on the count VαV_\alphaVα​ retains less information than conditioning on all far indicators, so sα′≤sαs'_\alpha\le s_\alphasα′​≤sα​. Let ZZZ have the Poisson law with mean λ\lambdaλ. The paper defines ∥L(W)−L(Z)∥\|\mathcal L(W)-\mathcal L(Z)\|∥L(W)−L(Z)∥ as twice the usual supremum over events: 2sup⁡A∣P(W∈A)−P(Z∈A)∣2\sup_A|P(W\in A)-P(Z\in A)|2supA​∣P(W∈A)−P(Z∈A)∣.

Formalization targets

Theorem 1: total variation and the zero-count event

The goal is the complete four-clause statement of Theorem 1, including its strict final inequality:

∥L(W)−L(Z)∥≤2[(b1+b2)1−e−λλ+b3′min⁡{1,1.4λ−1/2}]≤2(b1+b2+b3),∣P(W=0)−e−λ∣≤(b1+b2+b3′)1−e−λλ<min⁡{1,λ−1}(b1+b2+b3).\begin{aligned} \|\mathcal L(W)-\mathcal L(Z)\| &\le 2\left[(b_1+b_2)\frac{1-e^{-\lambda}}{\lambda} +b'_3\min\{1,1.4\lambda^{-1/2}\}\right]\\ &\le 2(b_1+b_2+b_3),\\ |P(W=0)-e^{-\lambda}| &\le (b_1+b_2+b'_3)\frac{1-e^{-\lambda}}{\lambda} <\min\{1,\lambda^{-1}\}(b_1+b_2+b_3). \end{aligned}∥L(W)−L(Z)∥∣P(W=0)−e−λ∣​≤2[(b1​+b2​)λ1−e−λ​+b3′​min{1,1.4λ−1/2}]≤2(b1​+b2​+b3​),≤(b1​+b2​+b3′​)λ1−e−λ​<min{1,λ−1}(b1​+b2​+b3​).​

The intermediate targets are the Stein-operator inverse identity, the bound on a telescoping term, display (11) relating the approximation error to b1,b2,b3′b_1,b_2,b'_3b1​,b2​,b3′​, and the two clauses of Lemma 1. The goal keeps the coefficients and both forms of b3b_3b3​ fixed, as the paper states them.

Significance

The result reduces a distributional approximation question to local sums of probabilities and conditional-dependence errors. When b1b_1b1​, b2b_2b2​ and b3b_3b3​ are small, the entire law of the count is close to its Poisson comparison law, and the probability of no occurrence has its own sharper bound. The latter is useful whenever a model asks whether at least one rare event occurs. The result applies without demanding exact independence outside the chosen neighbourhoods; the residual dependence appears in b3b_3b3​.

The paper proves these results. The formalization task is to give the known estimates machine-checked statements and proofs with the constants and probability conventions exposed. Mathlib supplies the Poisson measure and conditional expectation, while the mission adds the paper-specific neighbourhood sums and Stein operators. The formalized theorem can be reused for count approximations in other dependent-indicator models once those models supply bounds on the three error quantities. No machine-checked proof is claimed here: the theorem items are proposed targets with sorry bodies.

Difficulty

A first approximation based only on EWE WEW misses overlapping event pairs. Bounding pair dependence through b2b_2b2​ alone also misses dependence between one indicator and the aggregate of far indicators. The authors' third term measures that remaining effect by conditional expectation. The proof must control the Stein solution uniformly while preserving its precise constants; replacing that control with a qualitative bound would not recover Theorem 1. In the countably infinite setting, the sums and conditional expectations also require careful handling of convergence and measurability. The proof of Lemma 1 is attributed in the paper to Barbour and Eagleson; it is a substantive target here rather than an assumed bound.

Formalization scope

The Lean index type is countable. Under the paper's assumptions pα>0p_\alpha>0pα​>0 and ∑αpα<∞\sum_\alpha p_\alpha<\infty∑α​pα​<∞, only countably many indices can exist, so this representation retains the stated probabilistic setting. Indicators are measurable natural-number-valued functions with values at most one. The parameter λ\lambdaλ is a positive real equipped with the exact HasSum statement for the probabilities. The Poisson law is Mathlib's poissonMeasure at λ\lambdaλ converted to a nonnegative real parameter.

The sums defining b1,b2,b3,b3′b_1,b_2,b_3,b'_3b1​,b2​,b3​,b3′​ use extended nonnegative reals, so divergence becomes +∞+\infty+∞ rather than the real tsum default zero. The random counts WWW and VαV_\alphaVα​ use natural-number tsum; their divergent-input default can occur only on a null set under the finite-mean hypotheses and therefore does not change their laws. Measurability of these counts follows from countability and measurability of each indicator. The far-field sigma algebra is generated by the measurable indicators, and the formalization checks that it lies below the ambient sigma algebra, avoiding a default-zero conditional expectation. The paper's total variation norm is exactly 2 * MarkovChainCLT.tvDist, with the factor two retained.

The source writes a strict final inequality without discussing infinite error sums. The Lean statement conditions that single strict clause on b1+b2+b3<∞b_1+b_2+b_3<\inftyb1​+b2​+b3​<∞; otherwise both sides can be infinite and strict comparison is false. The other three clauses allow infinite bounds, as the source does. Lemma 1 fixes the Stein inverse at zero exactly as the paper chooses and uses explicit pointwise sup-norm bounds over all nonnegative integers. Display (11) allows ∣h(k)∣≤1|h(k)|\le1∣h(k)∣≤1, a strengthening of the displayed ∥h∥=1\|h\|=1∥h∥=1 case. These choices rule out loss of the norm's factor two, disappearing divergent sums, default-zero mapped measures or conditional expectations, and an unannounced independence assumption.

Selected references

  • Richard Arratia, Larry Goldstein and Louis Gordon, Two moments suffice for Poisson approximations: the Chen-Stein method, Annals of Probability 17(1), 9–25, 1989. DOI 10.1214/aop/1176991491.
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