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Functional Analysis·Captain: mikedeng1

Markov Processes: Characterization and Convergence 19: Countable exclusion systemsTextbook

Why countable exclusion systems need a generation theorem

An exclusion system models particles moving among sites under the rule that each site is either vacant or occupied. A move exchanges the occupation variables at two sites, so particle number is conserved. On a countably infinite site set, however, the formal sum of all possible exchanges need not automatically determine a well-defined Markov evolution. Individual rates can be continuous and bounded while infinitely many potential exchanges remain active. Chapter 8, Section 3 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, gives conditions under which this formal operator closes to the generator of a conservative Feller semigroup Ethier--Kurtz, Theorem 3.6.

This mission states that theorem with its complete weighted two-site domain and its finite-coordinate core. It does not replace the countable system by a finite Markov chain, collapse the ordered-pair generator sum, or substitute the neighboring spin-flip theorem. Spin flips change particle number one coordinate at a time; exclusion moves exchange two coordinates and conserve it.

Configuration space, exchanges, and variations

Let S be a countable type of sites. A configuration is a function η : S → Bool, where false and true relabel vacancy and occupation. The product topology is induced by the discrete topology on Bool. The Lean space C(S → Bool, ℝ) consists of continuous real-valued observables on this compact configuration space and carries the uniform norm.

For sites i and j, exclusionExchange i j η swaps η i and η j and leaves every other coordinate unchanged. When i = j, the exchange is the identity. For an observable f, its two-site exchange variation is

var⁡ij(f)=sup⁡η∣f(exchange⁡ijη)−f(η)∣.\operatorname{var}_{ij}(f)=\sup_{\eta} \left|f(\operatorname{exchange}_{ij}\eta)-f(\eta)\right|.varij​(f)=ηsup​​f(exchangeij​η)−f(η)​.

The theorem assigns a continuous nonnegative rate c i j to every ordered pair and a nonnegative real dominating weight γ i j. Both families are symmetric, the diagonal rates vanish, and c i j η ≤ γ i j. The rows of γ are summable with one uniform upper bound, which is the Lean form of equation (3.27).

Rate dependence on the configuration is controlled through a different operation. spinFlip k η toggles the single coordinate k, and spinVariation (c i j) k measures the resulting uniform change in the rate. Equation (3.28) requires these single-site influences to be summable and bounded by K * γ i j, with one constant K for all pairs. The influence condition therefore deliberately uses single-site flips even though the dynamics itself uses two-site exchanges.

Formalization target

The pre-generator graph implements equation (3.29). Its domain is exactly the continuous observables satisfying

∑(i,j)∈S×Sγijvar⁡ij(f)<∞,\sum_{(i,j)\in S\times S}\gamma_{ij}\operatorname{var}_{ij}(f)<\infty,(i,j)∈S×S∑​γij​varij​(f)<∞,

where the sum is over ordered pairs and has no factor of one half. For (f,g) in the graph, the continuous output satisfies

g(η)=∑(i,j)∈S×Scij(η)(f(exchange⁡ijη)−f(η)).g(\eta)=\sum_{(i,j)\in S\times S}c_{ij}(\eta) \bigl(f(\operatorname{exchange}_{ij}\eta)-f(\eta)\bigr).g(η)=(i,j)∈S×S∑​cij​(η)(f(exchangeij​η)−f(η)).

The goal is Theorem 3.6 in full. Every observable in the weighted domain has a continuous image in the graph. The graph closure in the product uniform-norm topology is single-valued and equals the derivative graph of a strongly continuous contraction semigroup. The semigroup preserves nonnegative functions and the constant function one, expressing the conservative Feller conclusion.

The last clause retains the source's cylinder core. Restrict the initial graph to observables determined by finitely many coordinates: there is a finite set F such that configurations agreeing on F receive the same value. The closure of that restricted graph equals the entire closed generator graph. Generation, the full weighted domain, and the core remain one target because they are conclusions of the same source theorem.

Significance of the result

The theorem turns an infinite formal exchange sum into a closed Markov generator on continuous observables. The conclusion is stronger than pointwise convergence of the series: it identifies the whole generator domain through a derivative biconditional, provides positivity and conservativity, and establishes a finite-coordinate class from which the closed graph can be recovered.

The result is proved in the textbook. The formalization target is its precise Lean statement, including symmetry, zero diagonal, domination, the uniform row bound, the single-site influence bound, the weighted ordered-pair domain, graph closure, Feller generation, and cylinder core. Reusable infrastructure consists of the book-wide contraction-semigroup predicate and the already shared single-site flip and variation definitions; the exchange, exchange variation, and weighted graph are specific to this model.

Where the analytic difficulty lies

A naive finite-state jump-process argument does not apply. Countability and a uniform row bound do not turn the full ordered-pair collection into a finite set of moves. Pointwise notation for the exchange series also does not by itself prove that the result is continuous, that the graph closure is single-valued, or that finite-coordinate observables form a core. The weighted two-site domain and the configuration-influence condition are therefore essential parts of the theorem rather than optional regularity assumptions.

The spin-flip and exclusion models cannot be interchanged. A coordinate flip creates or removes occupation and is measured by a one-site domain. An exclusion move conserves occupation by swapping two coordinates and requires the γ-weighted two-site variation domain. Only the rate-influence hypothesis uses the shared one-site variation.

Formalization scope

The Lean statement allows empty, finite, and countably infinite S, matching the source's countability assumption without adding nonemptiness. Bool is an exact two-state encoding of {0,1}. Real suprema define both one-site and two-site uniform variations over the nonempty compact configuration space. Explicit Summable hypotheses prevent divergent real tsum expressions from being silently totalized.

The graph records a continuous output equal to the actual pointwise ordered-pair series. Its first conclusion ensures that this representation does not shrink the stated weighted domain. Closure is taken in C(S → Bool, ℝ) × C(S → Bool, ℝ). The semigroup is real-time indexed, while its laws and bounds are imposed for nonnegative times. No finite-site restriction, finite-total-rate replacement, factor of one half, exchange-based substitute for the influence bound, or weakened core statement is admitted.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 1, Section 3; Chapter 4; Chapter 8, Section 3, Theorem 3.6, equations (3.26)--(3.29), printed p. 381. Wiley DOI
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Machine LearningOperations ResearchOptimization·Captain: mikedeng1

Wasserstein Distributionally Robust Optimization V: The Wasserstein Shrinkage Estimator and Robust MMSE EstimationTextbook

Motivation

Minimum mean square error (MMSE) estimation — predicting a signal xxx from a noisy observation yyy by minimizing expected squared prediction error — underlies linear systems theory, linear regression, Kalman filtering, and multiple-input multiple-output signal processing. Its classical solution assumes the joint distribution of (x,y)(x,y)(x,y) is known exactly; in practice it is estimated from data, and the estimator inherits sampling error and model risk. Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter shows that hedging the MMSE objective against every distribution in a Wasserstein ball around the empirical distribution — an infinite-dimensional worst case over an intractable set of measures, a priori — collapses to a tractable, finite-dimensional convex semidefinite program (Theorem 25, p. 29), building on the Gelbrich-hull machinery of Section 2.3. This mission formalizes that reduction.

Setting

Fix mx,my∈Nm_x, m_y \in \mathbb{N}mx​,my​∈N and let ξ=(x,y)∈Rmx×Rmy\xi = (x,y) \in \mathbb{R}^{m_x} \times \mathbb{R}^{m_y}ξ=(x,y)∈Rmx​×Rmy​ be a random vector: xxx the signal to be estimated, yyy the observation. An estimator is a measurable function ψ:Rmy→Rmx\psi : \mathbb{R}^{m_y} \to \mathbb{R}^{m_x}ψ:Rmy​→Rmx​; write Ψ\PsiΨ for the family of all estimators. The distribution of ξ\xiξ is only known to lie in a type-2 Wasserstein ball Bε,2(P^N)B_{\varepsilon,2}(\hat P_N)Bε,2​(P^N​) centered at an elliptical nominal distribution P^N=Eg(μ^,Σ^)\hat P_N = E_g(\hat\mu,\hat\Sigma)P^N​=Eg​(μ^​,Σ^) with nominal mean μ^∈Rm\hat\mu \in \mathbb{R}^mμ^​∈Rm (m=mx+mym=m_x+m_ym=mx​+my​), nominal covariance Σ^∈S+m\hat\Sigma \in S^m_+Σ^∈S+m​, and density generator ggg. The distributionally robust MMSE estimation problem is

inf⁡ψ∈Ψsup⁡Q∈Bε,2(P^N)EQ[∥x−ψ(y)∥22].(35)\inf_{\psi \in \Psi} \sup_{Q \in B_{\varepsilon,2}(\hat P_N)} E_Q\big[\|x-\psi(y)\|_2^2\big]. \tag{35}ψ∈Ψinf​Q∈Bε,2​(P^N​)sup​EQ​[∥x−ψ(y)∥22​].(35)

Writing Σ^=(Σ^xxΣ^xyΣ^yxΣ^yy)\hat\Sigma = \begin{pmatrix}\hat\Sigma_{xx}&\hat\Sigma_{xy}\\\hat\Sigma_{yx}& \hat\Sigma_{yy}\end{pmatrix}Σ^=(Σ^xx​Σ^yx​​Σ^xy​Σ^yy​​) blockwise, the nonlinear convex SDP

max⁡Sf(S)=Tr[Sxx−SxySyy−1Syx]s.t.S=(SxxSxySyxSyy)⪰0,  Sxx⪰0,  Syy⪰0,  Tr[S+Σ^−2(Σ^1/2SΣ^1/2)1/2]≤ε2,  S⪰λmin⁡(Σ^)I(36)\max_S f(S) = \mathrm{Tr}[S_{xx} - S_{xy}S_{yy}^{-1}S_{yx}] \quad \text{s.t.} \quad S = \begin{pmatrix}S_{xx}&S_{xy}\\S_{yx}&S_{yy}\end{pmatrix} \succeq 0,\; S_{xx} \succeq 0,\; S_{yy} \succeq 0,\; \mathrm{Tr}[S+\hat\Sigma-2(\hat\Sigma^{1/2}S\hat\Sigma^{1/2})^{1/2}] \le \varepsilon^2,\; S \succeq \lambda_{\min}(\hat\Sigma) I \tag{36}Smax​f(S)=Tr[Sxx​−Sxy​Syy−1​Syx​]s.t.S=(Sxx​Syx​​Sxy​Syy​​)⪰0,Sxx​⪰0,Syy​⪰0,Tr[S+Σ^−2(Σ^1/2SΣ^1/2)1/2]≤ε2,S⪰λmin​(Σ^)I(36)

is the finite-dimensional relaxation the chapter builds toward.

Formalization targets

Goal (Theorem 25, distributionally robust MMSE estimator). If Σ^≻0\hat\Sigma \succ 0Σ^≻0, then the optimal value of problem (35) equals the optimal value of SDP (36). Moreover, if S⋆S^\starS⋆ is optimal in (36) with Syy⋆S^\star_{yy}Syy⋆​ invertible, then the affine function

ψ⋆(y)=Sxy⋆(Syy⋆)−1(y−μ^y)+μ^x\psi^\star(y) = S^\star_{xy}(S^\star_{yy})^{-1}(y-\hat\mu_y) + \hat\mu_xψ⋆(y)=Sxy⋆​(Syy⋆​)−1(y−μ^​y​)+μ^​x​

attains the outer infimum of (35) — it is a distributionally robust MMSE estimator, exhibited in closed form from an SDP optimizer.

Significance

Theorem 25 reduces an a priori infinite-dimensional, worst-case functional optimization problem (an infimum over all measurable estimators of a supremum over all distributions within a Wasserstein ball) to a finite convex program with one linear matrix inequality, one Loewner-order lower bound, and one trace/matrix-square-root constraint — solvable in polynomial time, with the optimal estimator recovered in closed form from the SDP's optimal block matrix. It shows that robustifying MMSE estimation against distributional ambiguity does not sacrifice tractability: the resulting estimator remains affine, the same functional form as the classical (non-robust) best linear unbiased estimator, only with its coefficients drawn from a regularized covariance estimate rather than the raw sample covariance. Formalizing it fixes, machine-checkably, the exact shape of that regularization — which SDP constraints are load-bearing (the Loewner lower bound in particular rules out a numerically unstable near-singular SyyS_{yy}Syy​) and which conditions (Σ^≻0\hat\Sigma \succ 0Σ^≻0, Syy⋆S^\star_{yy}Syy⋆​ invertible) the closed-form estimator formula actually needs.

Difficulty

The paper's own remark (p. 29) names the two nontrivial steps: first, "establishing a minimax theorem for (35) and exploiting the properties of elliptical distributions" to show the outer infimum is attained by an affine estimator — a priori (35) ranges over all measurable ψ\psiψ, and there is no obvious reason the worst case forces linearity. Second, "combining this structural insight with Theorem 16" (the SDP-representability result for indefinite quadratic losses under an elliptical nominal distribution, itself a nontrivial closed-form reduction of an infinite-dimensional worst-case risk) to convert the now-restricted problem over affine estimators into the finite SDP (36). Neither step is a routine consequence of the ambiguity-set definitions alone; each requires structural facts about elliptical distributions and quadratic losses proved earlier in the chapter.

Formalization scope

The signal-observation space is EuclideanSpace ℝ (Fin mx ⊕ Fin my), with xxx and yyy recovered as the two summand projections; the block matrix SSS is Matrix (Fin mx ⊕ Fin my) (Fin mx ⊕ Fin my) ℝ, and Matrix.toBlocks₁₁/toBlocks₁₂/toBlocks₂₁/toBlocks₂₂ give its four blocks. The constraint "Sxy=Syx⊤S_{xy}=S_{yx}^\topSxy​=Syx⊤​" is not stated as a separate hypothesis: it follows automatically once SSS is symmetric (implied by S.PosSemidef), so encoding the feasible set from a single symmetric S rather than four independently-quantified blocks makes it structurally impossible to drop — see pitfall 4 of BRIEF.md. The outer infimum of problem (35) ranges only over measurable ψ\psiψ (Measurable ψ on the binder), matching the paper's own definition of Ψ\PsiΨ as "the family of all possible measurable estimators" (p. 29) exactly. λ_min(Σ̂) is taken as a hypothesis parameter characterized by the two properties that make it the minimum ("≤ every eigenvalue of Σ̂, and attained by some eigenvalue"), rather than invoking a specific Mathlib min-eigenvalue API by name. S_{yy}⁻¹ uses the ordinary matrix inverse (junk zero matrix when singular), matching the paper's literal notation; S^\star_{yy} invertible is stated as an added hypothesis, not present verbatim on the page, because the paper leaves the formula's well-definedness implicit — disclosed per pitfall 5 rather than silently assumed away. The paper's own "which is always solvable" clause is not asserted: Theorem 25 states, as part of itself, that SDP (36) attains its maximum (an unconditional existence claim for an optimal S⋆S^\starS⋆); this formalization states only the conditional consequences of such an S⋆S^\starS⋆ existing, not that one does — proving or asserting solvability is out of this mission's scope, so the Lean statement is strictly weaker than Theorem 25's own conclusion on this point, disclosed rather than silently dropped. All risk-style suprema are EReal-valued and Integrable-guarded, matching the series' convention. No milestone theorem is included: the paper's own proof sketch derives (33)'s and by extension (36)'s SDP "via Theorem 16", but Theorem 16 (indefinite quadratic loss and p=2p=2p=2, eq. 23) was itself judged too heavy to state faithfully in 02-gelbrich's time budget and is not redefined here either — see STATUS.md. Theorem 24 (the Wasserstein shrinkage estimator, this chapter's originally recommended goal) is out of scope: its closed-form eigenvalue transformation (eq. 34a/34b) requires transcribing nested square roots from a rendered PDF page that this session's time budget did not allow verifying to the standard the brief demands (pitfall 1); the brief's own documented fallback to Theorem 25 was taken instead.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Nguyen, V. A., Shafieezadeh-Abadeh, S., Yue, M.-C., Kuhn, D., & Wiesemann, W. (2021). Optimistic distributionally robust optimization for nonparametric likelihood approximation. Advances in Neural Information Processing Systems, 32.
  • Shafieezadeh-Abadeh, S., Nguyen, V. A., Kuhn, D., & Mohajerin Esfahani, P. (2018). Wasserstein distributionally robust Kalman filtering. Advances in Neural Information Processing Systems, 31.
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Wasserstein Distributionally Robust Optimization II: The Gelbrich Ambiguity Set and Elliptical TractabilityTextbook

Motivation

Distributionally robust optimization (DRO) hedges a decision against every distribution within some ambiguity set around an estimated (nominal) distribution, rather than trusting the estimate exactly. When the ambiguity set is a ball of radius ε\varepsilonε around the empirical distribution P^N\hat P_NP^N​ in the type-ppp Wasserstein metric, the resulting worst-case risk problem inherits attractive statistical guarantees (Mohajerin Esfahani & Kuhn 2018) but is, in general, an optimization problem over an infinite-dimensional space of measures. Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter surveys when this problem becomes computationally tractable. One route — the subject of this mission — discards everything about the nominal distribution except its mean vector and covariance matrix and replaces the Wasserstein ball with a set built only from these two moments, the Gelbrich hull. The construction is due to Gelbrich (1990), who first bounded the Wasserstein distance between two distributions using only their means and covariances.

Setting

Fix Ξ⊆Rm\Xi \subseteq \mathbb{R}^mΞ⊆Rm, a nominal distribution P^N∈P(Ξ)\hat P_N \in \mathcal{P}(\Xi)P^N​∈P(Ξ), a radius ε>0\varepsilon > 0ε>0 and an exponent p≥1p \ge 1p≥1. The type-ppp Wasserstein distance between two probability measures Q,Q′Q, Q'Q,Q′ on Rm\mathbb{R}^mRm is

Wp(Q,Q′)=(inf⁡π∈Π(Q,Q′)∫∥ξ−ξ′∥p dπ(ξ,ξ′))1/p,W_p(Q,Q') = \Big(\inf_{\pi \in \Pi(Q,Q')} \int \|\xi-\xi'\|^p \, d\pi(\xi,\xi')\Big)^{1/p},Wp​(Q,Q′)=(π∈Π(Q,Q′)inf​∫∥ξ−ξ′∥pdπ(ξ,ξ′))1/p,

the infimum over couplings π\piπ (probability measures on Rm×Rm\mathbb{R}^m \times \mathbb{R}^mRm×Rm with marginals QQQ and Q′Q'Q′) of the ppp-th root of the expected ppp-th power of Euclidean distance. The Wasserstein ambiguity set 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}, and 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)} E_Q[\ell(\xi)]Rε,p​(P^N​,ℓ)=supQ∈Bε,p​(P^N​)​EQ​[ℓ(ξ)].

Suppose P^N\hat P_NP^N​ has mean vector μ^\hat\muμ^​ and covariance matrix Σ^∈S+m\hat\Sigma \in S^m_+Σ^∈S+m​ (the positive semidefinite m×mm\times mm×m matrices). The mean-covariance uncertainty set is

Uε(μ^,Σ^)={(μ,Σ)∈Rm×S+m:∥μ^−μ∥22+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2},U_\varepsilon(\hat\mu,\hat\Sigma) = \Big\{(\mu,\Sigma) \in \mathbb{R}^m \times S^m_+ : \|\hat\mu-\mu\|_2^2 + \mathrm{Tr}\big[\hat\Sigma+\Sigma-2(\hat\Sigma^{1/2}\Sigma\hat\Sigma^{1/2})^{1/2}\big] \le \varepsilon^2\Big\},Uε​(μ^​,Σ^)={(μ,Σ)∈Rm×S+m​:∥μ^​−μ∥22​+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2},

where Σ1/2\Sigma^{1/2}Σ1/2 is the positive-semidefinite square root. The Gelbrich hull is Gε(μ^,Σ^)={Q∈P(Ξ):(EQ[ξ],CovQ[ξ])∈Uε(μ^,Σ^)}G_\varepsilon(\hat\mu,\hat\Sigma) = \{Q \in \mathcal{P}(\Xi) : (E_Q[\xi],\mathrm{Cov}_Q[\xi]) \in U_\varepsilon(\hat\mu,\hat\Sigma)\}Gε​(μ^​,Σ^)={Q∈P(Ξ):(EQ​[ξ],CovQ​[ξ])∈Uε​(μ^​,Σ^)}: the distributions on Ξ\XiΞ whose own mean and covariance lie in Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^). An elliptical distribution Eg(μ,Σ)E_g(\mu,\Sigma)Eg​(μ,Σ) has density f(ξ)=C⋅det⁡(Σ)−1g((ξ−μ)⊤Σ−1(ξ−μ))f(\xi) = C \cdot \det(\Sigma)^{-1} g\big((\xi-\mu)^\top\Sigma^{-1}(\xi-\mu)\big)f(ξ)=C⋅det(Σ)−1g((ξ−μ)⊤Σ−1(ξ−μ)) for a density generator ggg and normalizing constant CCC; two elliptical distributions "have the same density generator" when their ggg coincide (e.g. both Gaussian, both Student-tνt_\nutν​ for the same ν\nuν).

Formalization targets

Goal (Theorem 13, Gelbrich hull). For every p≥2p \ge 2p≥2,

Bε,p(P^N)⊆Gε(μ^,Σ^).B_{\varepsilon,p}(\hat P_N) \subseteq G_\varepsilon(\hat\mu,\hat\Sigma).Bε,p​(P^N​)⊆Gε​(μ^​,Σ^).

This is an outer approximation: every distribution within ε\varepsilonε of P^N\hat P_NP^N​ in Wasserstein distance has a mean and covariance inside Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^), so optimizing over the Gelbrich hull instead of the Wasserstein ball can only enlarge the feasible set, never shrink it below the truth.

Supporting results. Theorem 4 (Gelbrich bound) gives the moment-only lower bound on W2W_2W2​ that Theorem 13 is built from, with equality for elliptical distributions sharing a generator. Proposition 1 sharpens the goal's containment to an equality on the mean-covariance projection itself, under the same two conditions (Ξ=Rm\Xi = \mathbb{R}^mΞ=Rm, P^N\hat P_NP^N​ elliptical). Corollary 1 propagates the goal's set containment to the risk level: Rε,p(P^N,ℓ)≤Rε(μ^,Σ^,ℓ)R_{\varepsilon,p}(\hat P_N,\ell) \le R_\varepsilon(\hat\mu,\hat\Sigma,\ell)Rε,p​(P^N​,ℓ)≤Rε​(μ^​,Σ^,ℓ) for every ℓ\ellℓ, where Rε(μ^,Σ^,ℓ)=sup⁡Q∈Gε(μ^,Σ^)EQ[ℓ(ξ)]R_\varepsilon(\hat\mu,\hat\Sigma,\ell) = \sup_{Q \in G_\varepsilon(\hat\mu,\hat\Sigma)} E_Q[\ell(\xi)]Rε​(μ^​,Σ^,ℓ)=supQ∈Gε​(μ^​,Σ^)​EQ​[ℓ(ξ)] is the Gelbrich risk.

Significance

Theorem 13 is the hinge between an intractable infinite-dimensional worst-case-risk problem and a tractable one: the paper goes on (Theorem 16, outside this mission's scope) to show that for quadratic loss functions and elliptical nominal distributions the Gelbrich risk itself equals the optimal value of a semidefinite program with two linear matrix inequality constraints — and that, under those same conditions, the Wasserstein worst-case risk, the Gelbrich risk and the SDP value all coincide. Corollary 1 is what makes the Gelbrich risk usable as a conservative surrogate even outside that special case: it upper-bounds the true worst-case risk for any loss function and any p≥2p \ge 2p≥2, at the cost of discarding all but first- and second-order information about the nominal distribution. Formalizing the goal and Corollary 1 gives the exact scope in which this moment-relaxation is licensed — the p≥2p \ge 2p≥2 restriction and the outer-approximation direction are both easy to get backwards, and this mission's Lean encoding fixes both irreversibly.

Difficulty

The obvious first argument is to prove containment pointwise: fix Q∈Bε,p(P^N)Q \in B_{\varepsilon,p}(\hat P_N)Q∈Bε,p​(P^N​) and show its mean and covariance land in Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^). That reduces Theorem 13 to Proposition 1's containment half, which in turn reduces to the Gelbrich bound (Theorem 4) applied to the pair (Q,P^N)(Q,\hat P_N)(Q,P^N​) — the inequality direction of Theorem 4 suffices for containment; only the sharper equality direction (needed for Proposition 1's own equality clause) requires the elliptical hypothesis. The non-obvious step is Theorem 4 itself: bounding W2(Q,Q′)W_2(Q,Q')W2​(Q,Q′) below by a closed-form expression in the two distributions' first two moments only, for arbitrary Q,Q′Q,Q'Q,Q′ with those moments, requires an argument that survives every coupling π\piπ — the paper's proof goes through a lower bound on the coupling's cross-covariance term via the eigenvalues of Σ1/2Σ′Σ1/2\Sigma^{1/2}\Sigma'\Sigma^{1/2}Σ1/2Σ′Σ1/2, not a direct manipulation of W2W_2W2​'s definition.

Formalization scope

Rm\mathbb{R}^mRm is EuclideanSpace ℝ (Fin m); a "distribution" is a MeasureTheory.Measure on it constrained by Q Set.univ = 1 (probability) and Q Ξᶜ = 0 (support in Ξ). The Wasserstein distance is ENNReal-valued (Definition 1's infimum over couplings, matching 01-duality's convention); the worst-case and Gelbrich risks are EReal-valued suprema restricted to loss functions integrable under the candidate distribution, avoiding Mathlib's junk value for a non-integrable Bochner integral. Σ1/2\Sigma^{1/2}Σ1/2 is the positive-semidefinite matrix square root, picked by choice from its defining existential and applied in this mission only to matrices hypothesized (or, per Section 2.3's standing assumption, given) positive semidefinite. Elliptical distributions (IsElliptical) are represented by the paper's own density formula (a measure equal to volume.withDensity of C·det(Σ)⁻¹·g((ξ-μ)ᵀΣ⁻¹(ξ-μ)) for some C>0), together with the mean/covariance facts every theorem in this chunk reads off directly; an earlier draft kept only the latter, under which "same density generator" held vacuously for any moment-matched pair — corrected after moderation flagged it (see STATUS.md). Because 01-duality (Wasserstein distance, ambiguity set, worst-case risk) is not yet a published mission, this chunk redefines those objects locally in its own namespace rather than importing an unpublished draft, per the series' definition-reuse policy; a future upload can retire the duplication once 01-duality is live. A formalization that dropped Theorem 4's "same density generator" condition from its equality clause, or that stated the goal's containment for all p≥1p\ge 1p≥1 rather than p≥2p \ge 2p≥2, would be trivializing or simply false — both are explicit hypotheses in the Lean statements. Matrix.PosSemidef and its Loewner order carry the S+mS^m_+S+m​ constraints; no elliptical-distribution or Gelbrich-hull infrastructure exists elsewhere on the platform, so this mission's definitions are original contributions reusable by any later extension (Theorem 16/17, Lemma 1/2's SDP representations) of this series.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Gelbrich, M. (1990). On a formula for the L2 Wasserstein metric between measures on Euclidean and Hilbert spaces. Mathematische Nachrichten, 147(1), 185–203.
  • Mohajerin Esfahani, P., & Kuhn, D. (2018). Data-driven distributionally robust optimization using the Wasserstein metric: performance guarantees and tractable reformulations. Mathematical Programming, 171(1), 115–166.
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Foundations of Machine Learning XIII: The Johnson-Lindenstrauss LemmaTextbook

Motivation

High-dimensional data is often computationally expensive to work with and hard to visualize. The Johnson-Lindenstrauss lemma answers a striking question in this setting: can any finite set of points, no matter how high-dimensional the ambient space, be squeezed into a space of dimension depending only on the number of points (logarithmically) and the desired accuracy, while barely disturbing the distances between them? The answer is yes, and — remarkably — a single, data-independent random construction (a random Gaussian matrix) achieves it with positive probability for any point set. This mission formalizes the lemma and the two probabilistic results its proof is built from.

Setting

For a set VVV of mmm points in RN\mathbb R^NRN, a map f:RN→Rkf:\mathbb R^N\to\mathbb R^kf:RN→Rk is a (1±ϵ)(1\pm\epsilon)(1±ϵ)-distance-preserving embedding of VVV if (1−ϵ)∥u−v∥2≤∥f(u)−f(v)∥2≤(1+ϵ)∥u−v∥2(1-\epsilon)\|u-v\|^2\le\|f(u)-f(v)\|^2\le(1+\epsilon)\|u-v\|^2(1−ϵ)∥u−v∥2≤∥f(u)−f(v)∥2≤(1+ϵ)∥u−v∥2 for every u,v∈Vu,v\in Vu,v∈V. The book's proof constructs f=A/kf=A/\sqrt kf=A/k​ from a random matrix A∈Rk×NA\in\mathbb R^{k\times N}A∈Rk×N with i.i.d. standard normal (N(0,1)N(0,1)N(0,1)) entries, and argues by the probabilistic method: for a fixed pair of points, Lemma 15.3 shows fff preserves their squared distance up to (1±ϵ)(1\pm\epsilon)(1±ϵ) with probability at least 1−2e−(ϵ2−ϵ3)k/41-2e^{-(\epsilon^2-\epsilon^3)k/4}1−2e−(ϵ2−ϵ3)k/4, because the ratio ∥f(x)∥2/∥x∥2\|f(x)\|^2/\|x\|^2∥f(x)∥2/∥x∥2 (for xxx the difference of the two points) is exactly a χk2\chi^2_kχk2​ random variable, whose two-sided concentration around its mean kkk is Lemma 15.2. A union bound over the O(m2)O(m^2)O(m2) pairs in VVV then shows the probability that every pair is simultaneously preserved is still strictly positive — so a map with the desired property must exist, even though no single fixed matrix is exhibited.

Formalization targets

Lemma 15.2 (Chi-squared concentration, milestone). If Q∼χk2Q\sim\chi^2_kQ∼χk2​, then for 0<ϵ<1/20<\epsilon<1/20<ϵ<1/2, P[(1−ϵ)k≤Q≤(1+ϵ)k]≥1−2e−(ϵ2−ϵ3)k/4P[(1-\epsilon)k\le Q\le(1+\epsilon)k]\ge1-2e^{-(\epsilon^2-\epsilon^3)k/4}P[(1−ϵ)k≤Q≤(1+ϵ)k]≥1−2e−(ϵ2−ϵ3)k/4.

Lemma 15.3 (Gaussian random projection distortion, milestone). For x∈RNx\in\mathbb R^Nx∈RN, k<Nk<Nk<N, and A∈Rk×NA\in\mathbb R^{k\times N}A∈Rk×N with i.i.d. N(0,1)N(0,1)N(0,1) entries,

P[(1−ϵ)∥x∥2≤∥1kAx∥2≤(1+ϵ)∥x∥2]≥1−2e−(ϵ2−ϵ3)k/4.P\Big[(1-\epsilon)\|x\|^2\le\big\|\tfrac1{\sqrt k}Ax\big\|^2\le(1+\epsilon)\|x\|^2\Big] \ge1-2e^{-(\epsilon^2-\epsilon^3)k/4}.P[(1−ϵ)∥x∥2≤​k​1​Ax​2≤(1+ϵ)∥x∥2]≥1−2e−(ϵ2−ϵ3)k/4.

Lemma 15.4 — the mission's goal (Johnson-Lindenstrauss). For 0<ϵ<1/20<\epsilon<1/20<ϵ<1/2, integer m>4m>4m>4, and k=20log⁡(m)/ϵ2k=20\log(m)/\epsilon^2k=20log(m)/ϵ2, any set VVV of mmm points in RN\mathbb R^NRN admits a map f:RN→Rkf:\mathbb R^N\to\mathbb R^kf:RN→Rk with (1−ϵ)∥u−v∥2≤∥f(u)−f(v)∥2≤(1+ϵ)∥u−v∥2(1-\epsilon)\|u-v\|^2\le\|f(u)-f(v)\|^2\le(1+\epsilon) \|u-v\|^2(1−ϵ)∥u−v∥2≤∥f(u)−f(v)∥2≤(1+ϵ)∥u−v∥2 for all u,v∈Vu,v\in Vu,v∈V.

Significance

This is one of the cleanest instances in the book of the probabilistic method: existence is proved without exhibiting the object, by showing a random construction succeeds with positive probability. The target dimension k=O(log⁡m/ϵ2)k=O(\log m/\epsilon^2)k=O(logm/ϵ2) is independent of the ambient dimension NNN — the embedding works no matter how large the original feature space is, which is exactly why the lemma has inspired random-projection methods throughout dimensionality reduction, streaming algorithms, and compressed sensing. Prior art on the Prove2Me platform is not faithful here: HighDimProb.Isoperimetry.johnson_lindenstrauss (Vershynin series) proves a Johnson-Lindenstrauss-type bound, but via a uniformly-random mmm-dimensional subspace and its orthogonal projection, rescaled by n/m\sqrt{n/m}n/m​ — a genuinely different construction from this book's explicit i.i.d.-Gaussian-matrix map f=A/kf=A/\sqrt kf=A/k​, and with different (existentially quantified, unspecified) constants rather than this book's explicit k=20log⁡(m)/ϵ2k=20\log(m)/\epsilon^2k=20log(m)/ϵ2. The two are classically known to give essentially the same qualitative guarantee, but showing them equivalent would require an independent equivalence proof neither platform item nor this mission undertakes; per the chunk's own brief, the Vershynin theorem is cited here only as related work, not reused as a kind: reference item.

Not formalized here: Theorem 15.1 (the PCA solution), the chapter's other headline result. BRIEF.md explicitly flags PCA and JL as the chapter's two independent capstones, not a proof chain, and recommends dropping PCA if the mission focuses purely on JL. Theorem 15.1's proof is an Eckart-Young-type Frobenius-norm optimization argument over the set of rank-kkk orthogonal projection matrices — sharing no definitions, hypotheses, or proof technique with the probabilistic-method argument this mission's three items are built from. Formalizing it would mean standing up a second, unrelated piece of mathematics (constrained matrix optimization, singular value decomposition) from scratch for a single additional item; per the captain brief's guidance to leave out, rather than approximate, material disproportionate to the time budget, it is omitted. §15.2 (kernel PCA) and §15.3 (Isomap, LLE, Laplacian eigenmaps) are likewise out of scope, per BRIEF.md's own page-range restriction — applications- heavy manifold-learning material with no numbered result feeding Lemma 15.4's proof.

Difficulty

Lemma 15.2's proof is a genuine Chernoff-bound argument: apply Markov's inequality to exp⁡(λQ)\exp(\lambda Q)exp(λQ), substitute the chi-squared distribution's own moment-generating function (1−2λ)−k/2(1-2\lambda)^{-k/2}(1−2λ)−k/2, and optimize the resulting bound over λ∈(0,1/2)\lambda\in(0,1/2)λ∈(0,1/2) by calculus (the book's own choice λ=ϵ/(2(1+ϵ))\lambda=\epsilon/(2(1+\epsilon))λ=ϵ/(2(1+ϵ)) is exactly the minimizer) — not a one-line union of tail bounds, and the same argument must be repeated (with a sign flip) for the lower tail before combining via a union bound. Lemma 15.3's proof needs the non-obvious observation that Tj=x^j/∥x∥T_j=\widehat x_j/\|x\|Tj​=xj​/∥x∥ (for x^=Ax\widehat x=Axx=Ax) are themselves i.i.d. standard normal — a consequence of AAA's i.i.d. Gaussian entries and E[x^j2]=∥x∥2\mathbb E[\widehat x_j^2]=\|x\|^2E[xj2​]=∥x∥2, not immediate from the definitions alone — before the sum of their squares can be recognized as exactly a χk2\chi^2_kχk2​ variable and Lemma 15.2 applied. Lemma 15.4's own proof, while conceptually simple (a single union bound), needs the specific numerical accounting 2m2e−(ϵ2−ϵ3)k/4=2m5ϵ−3<2m−1/22m^2e^{-(\epsilon^2-\epsilon^3)k/4}=2m^{5\epsilon-3}<2m^{-1/2}2m2e−(ϵ2−ϵ3)k/4=2m5ϵ−3<2m−1/2 at the chosen k=20log⁡(m)/ϵ2k=20\log(m)/\epsilon^2k=20log(m)/ϵ2 and ϵ≤1/2\epsilon\le1/2ϵ≤1/2 to conclude the success probability is strictly positive — a formalization that merely asserted "the union bound gives a positive probability" without this exact accounting would not establish the book's specific, tight constant k=20log⁡(m)/ϵ2k=20\log(m)/\epsilon^2k=20log(m)/ϵ2.

Formalization scope

SqNorm is the coordinate-wise squared Euclidean norm (∑ᵢ vᵢ²), used in place of Mathlib's EuclideanSpace/PiLp norm typeclass machinery to keep the statements close to the book's own concrete ℝ^N/ℝ^k-coordinate notation. IsChiSquaredMGF states the moment-generating-function characterization of a chi-squared distribution that the proof of Lemma 15.2 itself cites (Eq. C.25), rather than restating the book's own Definition C.7, which sits in an out-of-chapter appendix not read for this mission; this is checked (in SELF_REVIEW.md) to be a faithful, uniquely-determining substitute, since a real random variable's law is determined by its MGF wherever it is finite near 0. IsIIDStandardGaussianMatrix states "i.i.d. standard normal entries" via Mathlib's gaussianReal 0 1 (marginal law) together with iIndepFun (joint independence). The goal theorem's target dimension k is taken as ⌈20 log(m)/ε²⌉ (Nat.ceil) rather than the book's real-valued 20 log(m)/ε², since a map's codomain dimension must be a natural number; this rounding only strengthens (never weakens) the existential conclusion, since the union-bound success probability is monotonically increasing in k. No numerical constant in any of the three items is otherwise altered from the book's own displayed form. A trivializing formalization this mission avoids: stating Lemma 15.4 with an unspecified k = O(log m/ε²) (an asymptotic, not an explicit constant) — per BRIEF.md's own naming of this as one of the series' "explicit-constant" results, k's exact formula 20 log(m)/ε² (up to the ceiling needed for well-typedness) is stated directly.

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 15, §15.4.
  • W. B. Johnson, J. Lindenstrauss, "Extensions of Lipschitz mappings into a Hilbert space," Contemporary Mathematics 26, 1984, 189-206.
  • S. Vempala, The Random Projection Method, DIMACS Series in Discrete Mathematics and Theoretical Computer Science, 2004.
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Machine LearningStatistics·Captain: mikedeng1

Support Vector Machines VII: Consistency of Support Vector Machines for RegressionTextbook

Motivation

Chapter 9 asks whether the support vector machine — a regularized empirical risk minimizer fD,λf_{D,\lambda}fD,λ​ over an RKHS HHH — is a statistically consistent estimator for regression: does RL,P(fD,λn)→RL,P∗R_{L,P}(f_{D,\lambda_n}) \to R^*_{L,P}RL,P​(fD,λn​​)→RL,P∗​ as the sample size n→∞n \to \inftyn→∞, for a suitable regularization schedule λn→0\lambda_n \to 0λn​→0? The chapter's main theorem (Theorem 9.1) answers yes, under an explicit polynomial rate condition on λn\lambda_nλn​. Its proof reduces the question to bounding how far the empirical regularized solution can be from the population regularized solution, and that reduction bottoms out in a single concentration-of-measure fact: how tightly does an empirical mean of i.i.d. Hilbert-space-valued random variables concentrate around its true mean, given only a bound on one qqq-th moment (no exponential-moment assumption at all)? That fact is Lemma 9.2, "the following lemma to bound the probability of ∣RL,P(fD,λ)−RL,P(fP,λ)∣≤ε|R_{L,P}(f_{D,\lambda}) - R_{L,P}(f_{P,\lambda})| \le \varepsilon∣RL,P​(fD,λ​)−RL,P​(fP,λ​)∣≤ε for ∣D∣→∞|D| \to \infty∣D∣→∞" — the technical core the whole chapter's consistency argument rests on, and this mission's goal.

Setting

Fix a measurable space ZZZ, a distribution PPP on ZZZ, a separable Hilbert space HHH, and a measurable g:Z→Hg : Z \to Hg:Z→H. Its qqq-th moment norm, for q∈(1,∞)q \in (1,\infty)q∈(1,∞), is ∥g∥q:=(EP∥g∥Hq)1/q\|g\|_q := (\mathbb E_P\|g\|_H^q)^{1/q}∥g∥q​:=(EP​∥g∥Hq​)1/q — the direct Hilbert-space analogue of an ordinary LqL^qLq norm. The proof machinery behind concentration results of this kind is symmetrization: replacing a centered i.i.d. sum 1n∑i(ξi−EPξi)\frac1n\sum_i(\xi_i - \mathbb E_P\xi_i)n1​∑i​(ξi​−EP​ξi​) by a Rademacher-randomized sum 1n∑iεiξi\frac1n\sum_i \varepsilon_i \xi_in1​∑i​εi​ξi​, where a Rademacher sequence ε1,…,εn\varepsilon_1,\dots,\varepsilon_nε1​,…,εn​ is a family of independent ±1\pm1±1-valued random variables, each taking each sign with probability 1/21/21/2. Once randomized, the sum's LpL^pLp-norms (for different ppp) become comparable to each other via Kahane's inequality, with a universal constant depending only on the two exponents involved — never on the sample size or the ambient Banach space.

Formalization targets

Goal: Lemma 9.2 (concentration of Hilbert-space-valued sample means)

Pn ⁣({(z1,…,zn)∈Zn:∥1n∑i=1ng(zi)−EPg∥H≥ε})≤cq(∥g∥qε nq∗)q,q∗:=min⁡{1/2, 1−1/q}P^n\!\left(\left\{(z_1,\dots,z_n) \in Z^n : \left\|\frac1n\sum_{i=1}^n g(z_i) - \mathbb E_P g\right\|_H \ge \varepsilon\right\}\right) \le c_q\left(\frac{\|g\|_q}{\varepsilon\, n^{q^*}}\right)^{q}, \qquad q^* := \min\{1/2,\,1-1/q\}Pn({(z1​,…,zn​)∈Zn:​n1​i=1∑n​g(zi​)−EP​g​H​≥ε})≤cq​(εnq∗∥g∥q​​)q,q∗:=min{1/2,1−1/q}

for a universal constant cq>0c_q>0cq​>0 depending only on qqq, every ε>0\varepsilon>0ε>0 and every n≥1n \ge 1n≥1. This is a genuine generalization of Chebyshev's inequality to Hilbert-space-valued means, sharp enough (via the explicit rate n−q∗n^{-q^*}n−q∗) to drive Theorem 9.1's own polynomial regularization condition λnp∗n→∞\lambda_n^{p^*} n \to \inftyλnp∗​n→∞.

Milestones (attack order)

  1. Theorem A.8.1 (Symmetrization) — EPΨ(∥1n∑i(ξi−EPξi)∥)≤EPEνΨ(2∥1n∑iεiξi∥)\mathbb E_P\Psi(\|\frac1n\sum_i(\xi_i-\mathbb E_P\xi_i)\|) \le \mathbb E_P\mathbb E_\nu\Psi(2\|\frac1n\sum_i\varepsilon_i\xi_i\|)EP​Ψ(∥n1​∑i​(ξi​−EP​ξi​)∥)≤EP​Eν​Ψ(2∥n1​∑i​εi​ξi​∥) for convex non-decreasing Ψ\PsiΨ, i.i.d. PPP-integrable ξi\xi_iξi​ valued in a separable Banach space, and a Rademacher sequence εi\varepsilon_iεi​. Directly cited in Lemma 9.2's proof ("Using the symmetrization argument given in Theorem A.8.1...").
  2. Theorem A.8.3 (Kahane's inequality) — for a Rademacher sequence, every two Lp(ν)L^p(\nu)Lp(ν) and Lq(ν)L^q(\nu)Lq(ν) norms of ∥∑iεixi∥\|\sum_i\varepsilon_ix_i\|∥∑i​εi​xi​∥ are comparable via a universal constant Kp,qK_{p,q}Kp,q​, independent of nnn and the Banach space EEE. Directly cited in Lemma 9.2's proof ("If q∈(1,2]q\in(1,2]q∈(1,2], we obtain with Kahane's inequality, see Theorem A.8.3, that...").

Theorem 9.1 itself (BRIEF.md's recommended goal — the full SVM-regression consistency theorem) was not attempted this session; see STATUS.md for the reason and the fallback taken instead.

Significance

Lemma 9.2 is stated and proved once, in the Appendix's general Rademacher-sequence toolkit and this chapter, and then used directly to obtain Theorem 9.1's consistency guarantee: substituting g:=g := g:= the pointwise SVM "difference process" into Lemma 9.2 converts a purely probabilistic concentration fact into a statement about how close the empirical SVM solution's risk is to the population solution's risk, for every sample size. Because the bound depends on nothing but a single moment ∥g∥q\|g\|_q∥g∥q​ — no boundedness, no sub-Gaussian tail — it is what lets Theorem 9.1 avoid assuming the loss or the label distribution has any exponential tail control, which is essential for regression (where Y⊂RY \subset \mathbb RY⊂R need not be bounded, unlike the classification setting of this series' earlier chapters). Symmetrization and Kahane's inequality are themselves standard, reusable tools of empirical process theory (used throughout Chapter 7's entropy-number program, excluded from this series, and Chapter 6's classification oracle inequality).

Difficulty

The published proof of Lemma 9.2 is a short but dense computation: Markov's inequality reduces the tail bound to bounding EPn∥h∥Hq\mathbb E_{P^n}\|h\|_H^qEPn​∥h∥Hq​ for the centered mean hhh; Theorem A.8.1 symmetrizes; for q∈(1,2]q \in (1,2]q∈(1,2], Theorem A.8.3 (Kahane) converts the qqq-th moment of the Rademacher sum to its second moment, which an explicit orthogonality computation (the book's Eq. (9.4), Eνn∥∑iεixi∥2=∑i∥xi∥2\mathbb E_{\nu^n}\|\sum_i\varepsilon_ix_i\|^2 = \sum_i\|x_i\|^2Eνn​∥∑i​εi​xi​∥2=∑i​∥xi​∥2 for any fixed x1,…,xnx_1,\dots,x_nx1​,…,xn​, an immediate consequence of the Rademacher signs' independence and the Hilbert space's parallelogram identity) reduces to a sum of individual second moments; the case q>2q>2q>2 argues analogously with a different exponent split. None of this computation is captured by this mission's two milestones alone — they supply the two cited theorems, not the connecting algebra — so a complete proof of the goal from the milestones as stated still requires reconstructing this argument, exactly as the captain brief's milestones are meant to be (the book's own attack path, not a fully mechanized proof outline).

Formalization scope

ZZZ and Θ\ThetaΘ (the Rademacher sequence's own probability space) are arbitrary measurable spaces; HHH is [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [MeasurableSpace H] [BorelSpace H] [SeparableSpace H] (a separable real Hilbert space with its Borel σ\sigmaσ-algebra), matching "HHH be a separable Hilbert space" without narrowing to a concrete space (e.g. ℓ2\ell^2ℓ2) the book itself does not assume. IsRademacherSequence states independence via Mathlib's iIndepFun and the ±1\pm1±1-probability-1/21/21/2 condition directly, since no ready-made "Rademacher distribution" object exists in this Mathlib revision (checked by search). q∗:=min⁡{1/2,1−1/q}q^* := \min\{1/2, 1-1/q\}q∗:=min{1/2,1−1/q} is substituted algebraically rather than introducing a separate conjugate exponent q′q'q′, since 1/q+1/q′=11/q+1/q'=11/q+1/q′=1 pins q′q'q′ down uniquely — not a change of content. In Theorem A.8.3, "for all Banach spaces EEE" quantifies over E : Type (the Type 0 universe) rather than every universe Type*, a disclosed minor restriction with no effect on this mission's own use of the theorem (with EEE instantiated to a Type* Hilbert space HHH that is, in every actual application, itself at the Type level).

A trivializing formalization here would drop the "independent" half of IsRademacherSequence (leaving only the marginal ±1\pm1±1-probability-1/21/21/2 condition, true even for perfectly correlated signs) or drop the "i.i.d." qualifier on ξ1,…,ξn\xi_1,\dots,\xi_nξ1​,…,ξn​ in Theorem A.8.1 (both symmetrization and Kahane's inequality are false, or at least unproven by the book's own argument, without independence) — both are ruled out here by stating iIndepFun explicitly rather than only the marginal distribution conditions.

IsRademacherSequence is reusable beyond this mission: any future formalization of Chapter 7's entropy-number/Rademacher-complexity program, or of Chapter 6's oracle inequality's own use of Rademacher averages, would restate it locally (per Hard Rule 9) from the same book definition. Contributions completing the three sorrys are welcome; Theorem 9.1 itself remains a natural, substantially larger follow-up mission built on top of this one's two milestones together with the RKHS/regularized-risk-minimizer apparatus already available in this series' 04-representer mission (restated locally, per Hard Rule 9).

Selected references

  • I. Steinwart & A. Christmann, Support Vector Machines, Springer, Information Science and Statistics, 2008. https://doi.org/10.1007/978-0-387-77242-4 (Chapter 9, §§9.1-9.2, pp. 333-337, and Appendix §A.8, pp. 535-537).
  • J.-P. Kahane, Some Random Series of Functions, 2nd ed., Cambridge University Press, 1985 (Kahane's inequality, Theorem A.8.3's original source).
  • A. W. van der Vaart & J. A. Wellner, Weak Convergence and Empirical Processes, Springer, 1996 (Lemma 2.3.1, the source of Theorem A.8.1's proof technique).
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Operations ResearchStochastic Systems·Captain: mikedeng1

Stochastic Orders VIII: Closure of the Convexity Orders Under Random SumsTextbook

Counting terms and comparing the resulting sums

Chapters III and IV formalize what it means for one random variable to be "more spread out" or "larger and more spread out" than another. Chapter VIII asks a different kind of question: if the number of terms in a sum of i.i.d. random variables is itself random, and one count is larger than another in one of these orders, does the resulting random sum inherit the comparison? This mission formalizes the chapter's own answer — Theorem 8.A.13 — a clean, self-contained closure result that needs only the icx/icv/cx orders from Chunks 03/04 (restated locally) and one nonnegative-integer-valued index, without the heavier parametric-family apparatus (SICX, SICV, SIL, and the stochastic-convexity-of-a-family notions) that occupies most of the rest of the chapter.

The icx/icv/cx orders, restated for this chapter

This chapter restates the univariate increasing convex, increasing concave and convex orders (Chunks 04 and 03's own subjects) locally, since drafts cannot import another mission's definitions: for random variables X,YX,YX,Y, X≤icxYX\le_{icx}YX≤icx​Y [X≤icvYX\le_{icv}YX≤icv​Y] if E[φ(X)]≤E[φ(Y)]E[\varphi(X)]\le E[\varphi(Y)]E[φ(X)]≤E[φ(Y)] for every increasing convex [concave] φ:R→R\varphi:\mathbb{R}\to\mathbb{R}φ:R→R for which the expectations exist, and X≤cxYX\le_{cx}YX≤cx​Y if the same holds for every convex φ\varphiφ (dropping "increasing"). Theorem 8.A.13 applies these same three orders to nonnegative-integer-valued random variables M,NM,NM,N — a special case of the real-valued order (after the coercion N→R\mathbb{N}\to\mathbb{R}N→R), not a separate discrete order, per this chapter's own pitfall 1.

Formalization target

Goal: closure of the icx/icv/cx orders under random sums (Theorem 8.A.13)

Let {Yk,k∈N++}\{Y_k, k\in\mathbb{N}_{++}\}{Yk​,k∈N++​} be i.i.d. nonnegative random variables, independent of the two nonnegative discrete random variables MMM and NNN. Then

M≤icx[≤icv] N  ⟹  ∑k=1MYk≤icx[≤icv]∑k=1NYk,M≤cxN  ⟹  ∑k=1MYk≤cx∑k=1NYk.M\le_{icx}[\le_{icv}]\,N \implies \sum_{k=1}^{M}Y_k \le_{icx}[\le_{icv}]\sum_{k=1}^{N}Y_k, \qquad M\le_{cx}N \implies \sum_{k=1}^{M}Y_k \le_{cx}\sum_{k=1}^{N}Y_k.M≤icx​[≤icv​]N⟹k=1∑M​Yk​≤icx​[≤icv​]k=1∑N​Yk​,M≤cx​N⟹k=1∑M​Yk​≤cx​k=1∑N​Yk​.

Comparing the number of terms propagates to a comparison of the resulting random sums. This is "an application of these notions in establishing a stochastic inequality," in the book's own words right before the theorem — the formal content behind Example 8.A.2's claim that a homogeneous Poisson process is SIL, via the semigroup property of Example 8.A.7 (neither a numbered theorem, so neither is drafted as a milestone here — cited as background only, per CAPTAIN_BRIEF.md rule 5).

The book's proof defines ψ(n)=E[φ(∑k=1nYk)]\psi(n) = E[\varphi(\sum_{k=1}^n Y_k)]ψ(n)=E[φ(∑k=1n​Yk​)] for an increasing convex [concave] φ\varphiφ and observes (via the unnumbered Example 8.A.4) that ψ\psiψ is itself increasing and convex [concave] in nnn; the icx/icv order on M,NM,NM,N then transfers directly to ψ(M)\psi(M)ψ(M) vs. ψ(N)\psi(N)ψ(N), giving part (a). Part (b) follows from part (a) together with the equal-means fact E[∑k=1MYk]=E[∑k=1NYk]E[\sum_{k=1}^M Y_k]=E[\sum_{k=1}^N Y_k]E[∑k=1M​Yk​]=E[∑k=1N​Yk​] under M≤cxNM\le_{cx}NM≤cx​N (Theorem 4.A.35, a Chapter 4 result not restated in this mission).

Significance

Random sums are the natural model for aggregate risk, total service time, or total demand when the number of contributing terms is itself uncertain — the number of claims in an insurance period, the number of customers served, the number of jobs in a batch. Theorem 8.A.13 is the tool that lets an analyst reduce a comparison of two such aggregates to a comparison of the (often much simpler) counting processes that generate them, without having to reason about the joint distribution of the sums directly. It is also the concrete instance, stripped of the rest of the chapter's parametric-family machinery, of a pattern that recurs throughout the book: an order on an index set (here, the count MMM vs. NNN) transferring through a monotone/convex construction (here, summation) to an order on the resulting random variables — the same shape Chunk 06's Theorem 6.B.16(b) and Chunk 07's Theorem 7.A.9 each illustrate in their own settings.

No platform prior art exists: GET /theorems?q=random+sum, q=compound+distribution, q=Poisson+process, and q=renewal return nothing usable (the last returns only MarkovMixing/CLT-adjacent hits, not classical renewal or compound-sum results, confirmed at triage time and re-checked this session). This mission restates the icx/icv/cx orders and their random-sum closure as a self-contained result, independently drafted since drafts cannot import Chunks 03/04's Lean.

Difficulty

The chief formalization risk is treating M≤icxNM\le_{icx}NM≤icx​N as a separate "discrete" order rather than the same real-valued order applied to N\mathbb{N}N-valued random variables after coercion — this chapter's own pitfall 1. A second risk is drafting ∑k=1MYk\sum_{k=1}^{M}Y_k∑k=1M​Yk​ as a fixed-length sum with MMM substituted in afterward, rather than a genuine random (randomly-stopped) sum where MMM is itself random and independent of the {Yk}\{Y_k\}{Yk​} sequence — this chapter's own pitfall 2; the independence hypothesis has to be carried explicitly, not left as an unstated convention. A third risk, common to every bracketed theorem in this series, is conflating the icx and icv cases of part (a) into a single Or-joined statement rather than two clearly distinguished conjuncts — this chapter's own pitfall 3.

A different kind of risk, specific to this chapter, is scope creep into the parametric-family apparatus (SI, SCX, SICX, SIL, and the "family indexed by θ∈Θ\theta\in\Thetaθ∈Θ" definitions) that occupies most of Chapter 8: as BRIEF.md's own Setup note observes, that apparatus is heavier than the rest of the book (a family, a parameter set, and several bracketed cases per definition), and a trivializing risk specific to it — flagged in this chapter's pitfall 4 — is a family predicate that is vacuously true for a degenerate parametrization (e.g. Θ\ThetaΘ a singleton). This mission avoids that risk entirely by choosing the one clean, self-contained closure theorem in the chapter that needs none of it.

Formalization scope

The icx/icv/cx orders are restated locally (IcxOrder, IcvOrder, ConvexOrder, univariate, real-valued), exactly matching Chunks 04 and 03's own shapes, since drafts cannot import another mission's definitions. M,N:Ω→NM,N:\Omega\to\mathbb{N}M,N:Ω→N are nonnegative-integer-valued; the orders are applied to them via the coercion fun ω => (M ω : ℝ) (resp. N), matching pitfall 1 exactly — no separate discrete-order predicate is introduced. The i.i.d. sequence is drafted as Y : ℕ → Ω → ℝ (indexing Y 0, Y 1, … for the book's Y_1, Y_2, …, a one-step reindexing noted explicitly rather than left implicit), with iIndepFun Y μ for mutual independence and IdentDistrib (Y j) (Y k) μ μ for every j, k for identical distribution, plus 0 ≤ᵐ[μ] Y k for nonnegativity. The random sum itself is ∑ k ∈ Finset.range (M ω), Y k ω — a genuine randomly-stopped sum, per pitfall 2 — and independence of {Yk}\{Y_k\}{Yk​} from (M,N)(M,N)(M,N) jointly is IndepFun (fun ω => (M ω, N ω)) (fun ω k => Y k ω) μ, treating the whole sequence as one ℕ → ℝ-valued random element, stated as an explicit hypothesis rather than an implicit convention. The theorem's three conjuncts (icx, icv, cx) mirror the book's own single Theorem 8.A.13, whose part (a) bundles the icx/icv brackets and whose part (b) states the cx case separately, per pitfall 3.

A trivializing formalization this mission rules out: substituting M into a fixed-length Finset.range n sum after the fact (erasing the random-stopping structure that makes this a random-sum theorem at all) rather than genuinely summing over Finset.range (M ω), and treating M ≤icx N as anything other than the same real-valued order Chunks 03/04 define, applied after coercion. This mission draws on no platform prior art (searches for "random sum", "compound distribution", "Poisson process" and "renewal" as of 2026-09-18 return nothing usable). Unlike every other chapter in this series so far, this mission has no milestone theorems: every other numbered result near the goal in this chapter needs the parametric-family apparatus this mission deliberately avoids, and the un-numbered facts the goal's own proof cites (Example 8.A.4's potential-function monotonicity, Example 8.A.7's semigroup property) cannot be milestones per CAPTAIN_BRIEF.md rule 5 — see STATUS.md for the full accounting.

Selected references

  • M. Shaked and J. G. Shanthikumar, Stochastic Orders, Springer Series in Statistics, Springer, 2007, Chapter 8 (Stochastic Convexity and Concavity), §8.A.1–8.A.2. https://doi.org/10.1007/978-0-387-34675-5
  • This series' Chunk 03 (StochasticOrders.Convex) and Chunk 04 (StochasticOrders.MonotoneConvex), for the univariate convex and increasing convex/concave orders this chapter restates locally.
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High-Dimensional Probability X: Exact Sparse RecoveryTextbook

Motivation

Compressed sensing asks a question that looks impossible at first: can a signal x∈Rnx\in\mathbb R^nx∈Rn be reconstructed exactly from far fewer than nnn linear measurements y=Ax∈Rmy=Ax\in\mathbb R^my=Ax∈Rm, m≪nm\ll nm≪n? Classical linear algebra says no — an underdetermined system has infinitely many solutions. But if xxx is known in advance to be sparse (most of its coordinates are zero), the extra structure makes recovery possible: solving the convex program that minimizes the ℓ1\ell_1ℓ1​ norm of a candidate solution, subject to matching the measurements, recovers xxx exactly, for a measurement matrix AAA with a suitable geometric property. This idea, developed by Candès, Romberg, Tao and Donoho in the mid-2000s, underlies modern MRI acceleration, single-pixel cameras, and sparse signal processing generally.

The chapter isolates the exact geometric property a measurement matrix needs — the restricted isometry property (RIP) — and proves, purely by linear algebra with no probability involved, that RIP alone is sufficient for exact recovery by ℓ1\ell_1ℓ1​ minimization. (A companion result, outside this mission, shows random sub-gaussian matrices satisfy RIP with high probability once mmm is large enough, which is what makes the deterministic guarantee here practically useful; this mission formalizes the deterministic half.)

Setting

For a vector vvv indexed by a finite set, write ∥v∥0\|v\|_0∥v∥0​ for its number of non-zero coordinates (so vvv is sss-sparse if ∥v∥0≤s\|v\|_0\le s∥v∥0​≤s), ∥v∥1:=∑i∣vi∣\|v\|_1:=\sum_i|v_i|∥v∥1​:=∑i​∣vi​∣ for its ℓ1\ell_1ℓ1​ norm, and ∥v∥2:=∑ivi2\|v\|_2:=\sqrt{\sum_i v_i^2}∥v∥2​:=∑i​vi2​​ for its Euclidean norm.

An m×nm\times nm×n matrix AAA satisfies the restricted isometry property (RIP) with parameters α,β,s\alpha,\beta,sα,β,s if

α∥v∥2  ≤  ∥Av∥2  ≤  β∥v∥2for every s-sparse v∈Rn,\alpha\|v\|_2 \;\le\; \|Av\|_2 \;\le\; \beta\|v\|_2 \qquad\text{for every } s\text{-sparse } v\in\mathbb R^n,α∥v∥2​≤∥Av∥2​≤β∥v∥2​for every s-sparse v∈Rn,

i.e. AAA acts as an approximate isometry on every sss-sparse vector — equivalently (the book's own Exercise 10.5.9), the singular values of every m×sm\times sm×s column-submatrix of AAA lie in [α,β][\alpha,\beta][α,β].

Given a matrix AAA and measurements y=Axy=Axy=Ax for an unknown sparse xxx, the exact-recovery program is

minimize ∥x′∥1subject toy=Ax′.\text{minimize } \|x'\|_1 \quad\text{subject to}\quad y = Ax'.minimize ∥x′∥1​subject toy=Ax′.

Formalization targets

Goal (Theorem 10.5.10, RIP implies exact recovery)

∃ x^=xwheneverx^ solves the exact-recovery program for y=Ax,\exists\,\hat x = x \quad\text{whenever}\quad \hat x \text{ solves the exact-recovery program for } y=Ax,∃x^=xwheneverx^ solves the exact-recovery program for y=Ax,

precisely: suppose AAA satisfies RIP with parameters α,β,(1+λ)s\alpha,\beta,(1+\lambda)sα,β,(1+λ)s where λ>(β/α)2\lambda>(\beta/\alpha)^2λ>(β/α)2; then for every sss-sparse xxx, every x^\hat xx^ that is feasible (Ax^=AxA\hat x=AxAx^=Ax) and ℓ1\ell_1ℓ1​-optimal among feasible vectors satisfies x^=x\hat x=xx^=x. No constant here is hard-coded beyond the book's own explicit threshold λ>(β/α)2\lambda>(\beta/\alpha)^2λ>(β/α)2 — the weakest stable form of the claim.

Significance

RIP isolates exactly the geometric mechanism that makes ℓ1\ell_1ℓ1​-minimization work for sparse recovery: once a matrix is known to satisfy it, exact recovery is a deterministic, provable consequence with no appeal to randomness, no failure probability, and no measurement-count formula to verify beyond the RIP parameters themselves. This clean separation — a purely geometric sufficient condition (RIP), proved separately (in the book's Theorem 10.5.11, outside this mission) to hold with high probability for random sub-gaussian matrices — is the template compressed sensing theory follows throughout: geometric/deterministic guarantee first, probabilistic verification that random constructions meet it second. The theorem is one of the two standard routes (with the direct probabilistic argument of Theorem 10.5.1) to the chapter's central claim that m=O(slog⁡n)m=O(s\log n)m=O(slogn) measurements suffice to recover any sss-sparse signal in Rn\mathbb R^nRn — exponentially fewer than the nnn measurements a naive linear-algebraic argument would need.

The result itself, and the RIP framework, are classical and well-established (Candès-Tao 2005). This mission formalizes the deterministic linear-algebra core of the argument — the statement infrastructure (RIP, sparsity, the exact-recovery program stated as an explicit optimization problem) and the goal theorem — for a solver to close with a proof.

Difficulty

The natural first idea for showing x^=x\hat x=xx^=x is to try to bound the recovery error h:=x^−xh:=\hat x-xh:=x^−x directly using ∥Ah∥2\|Ah\|_2∥Ah∥2​ (which vanishes, since both xxx and x^\hat xx^ are feasible) together with RIP applied to hhh itself — but hhh need not be sparse at all: it is the difference of two sparse-ish vectors and can have full support. The actual argument decomposes hhh's support into blocks by descending magnitude (the support I0I_0I0​ of xxx, then the λs\lambda sλs largest remaining coordinates I1I_1I1​, then the next λs\lambda sλs, and so on), applies RIP only to the leading block I0,1=I0∪I1I_{0,1}=I_0\cup I_1I0,1​=I0​∪I1​ (which genuinely has bounded sparsity ≤(1+λ)s\le(1+\lambda)s≤(1+λ)s), and separately bounds the contribution of every later block using the fact that x^\hat xx^ is ℓ1\ell_1ℓ1​-optimal (so ∥hI0c∥1≤∥hI0∥1\|h_{I_0^c}\|_1\le\|h_{I_0}\|_1∥hI0c​​∥1​≤∥hI0​​∥1​, the "cone constraint"): each later block's ℓ2\ell_2ℓ2​ norm is controlled by the ℓ1\ell_1ℓ1​ mass of the previous block divided by its size. This is a genuinely multi-step argument combining a purely geometric fact (RIP on one bounded-sparsity block) with a purely combinatorial one (the magnitude-sorted decomposition), and the "obvious" idea of applying RIP to hhh as a whole does not typecheck, since RIP says nothing about vectors with more than (1+λ)s(1+\lambda)s(1+λ)s non-zero entries.

Formalization scope

Vectors are plain functions ι → ℝ on a finite index type, not EuclideanSpace ℝ ι: the latter's fixed ℓ2\ell_2ℓ2​ norm instance cannot also host the ℓ1\ell_1ℓ1​ norm the program's objective needs, so both norms (L2Norm, L1Norm) are defined directly by their defining sums on the same underlying type. Sparsity (Sparsity) takes a real-valued threshold s : ℝ, matching that the RIP parameter (1+λ)s(1+\lambda)s(1+λ)s used by the goal theorem is a real number even at integer base sparsity. A solution x^\hat xx^ "of the program" is formalized as an explicit argmin membership — feasibility (A.mulVec xhat = A.mulVec x) conjoined with optimality over the exact feasible set (∀ x', A.mulVec x' = A.mulVec x → l1Norm xhat ≤ l1Norm x') — never "there exists an estimator such that", the trivialization risk this chapter's own triage brief flags explicitly (shared with Chapter 3's Max-Cut): an existential reading would prove a different, strictly weaker statement. The conclusion is stated for every such x^\hat xx^, not one witness, matching that RIP forces uniqueness.

This mission covers Theorem 10.5.10 only, as the sole item; the probabilistic goal Theorem 10.5.1 (exact recovery for random sub-gaussian measurement matrices, which needs Theorem 10.5.10 together with a separate probabilistic argument, Theorem 10.5.11, that random matrices satisfy RIP), and the Lasso guarantee (Theorem 10.6.1), are both left out for lack of session time: each would need a fresh probabilistic apparatus (independent isotropic sub-gaussian random rows, a failure-probability bound) built from scratch in this chapter's own sub-namespace, with no reusable published definition from an earlier chunk. L2Norm, L1Norm, Sparsity and RIP are reusable by any later chapter or mission needing sparse vectors or the restricted isometry property; solvers' contributions are welcome on completing the proof of Theorem 10.5.10 itself (the magnitude-sorted support decomposition sketched under Difficulty above), and, beyond this mission's current scope, on Theorem 10.5.11 and Theorem 10.5.1.

Selected references

  • E. J. Candès, T. Tao, Decoding by linear programming, IEEE Transactions on Information Theory 51 (2005), 4203–4215. https://doi.org/10.1109/TIT.2005.858979
  • D. L. Donoho, Compressed sensing, IEEE Transactions on Information Theory 52 (2006), 1289–1306. https://doi.org/10.1109/TIT.2006.871582
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 10. https://doi.org/10.1017/9781108231596
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High-Dimensional Statistics IV: Dudley's Entropy Integral BoundTextbook

Motivation

Many of the central questions of high-dimensional statistics reduce to bounding the expected supremum of a stochastic process: the maximum correlation of noise with a family of candidate signals, the operator norm of a random matrix, the uniform deviation of an empirical process from its mean. Whenever the index set of the process is infinite or exponentially large, a naive union bound over "all" indices is either vacuous or requires re-deriving a tail bound from scratch for every new problem. Chaining is the general-purpose technique that removes this need: it bounds the expected supremum of a process purely in terms of the geometry of its index set, measured by how many balls of a given radius are needed to cover it. The classical form of this bound is due to Dudley (1967), building on ideas that trace to Kolmogorov; the exposition here follows Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 5.

Setting

Fix an index set TTT and a collection of zero-mean random variables {Xθ,θ∈T}\{X_\theta,\theta\in T\}{Xθ​,θ∈T}. Say this collection is a sub-Gaussian process with respect to a (pseudo)metric ρX\rho_XρX​ on TTT (Definition 5.16) if

E[eλ(Xθ−Xθ′)]  ≤  eλ2ρX(θ,θ′)2/2for all θ,θ′∈T, λ∈R.\mathbb E\big[e^{\lambda(X_\theta-X_{\theta'})}\big] \;\le\; e^{\lambda^2\rho_X(\theta,\theta')^2/2} \qquad \text{for all } \theta,\theta'\in T,\ \lambda\in\mathbb R.E[eλ(Xθ​−Xθ′​)]≤eλ2ρX​(θ,θ′)2/2for all θ,θ′∈T, λ∈R.

This single condition covers, as special cases, the canonical Gaussian process Xθ=⟨θ,w⟩X_\theta = \langle\theta, w\rangleXθ​=⟨θ,w⟩ for www a standard Gaussian vector (with ρX\rho_XρX​ the Euclidean metric) and the Rademacher process built from i.i.d. Rademacher signs.

A δ\deltaδ-cover of TTT with respect to a metric ρ\rhoρ is a finite set {θ1,…,θN}⊂T\{\theta_1,\dots,\theta_N\}\subset T{θ1​,…,θN​}⊂T such that every θ∈T\theta\in Tθ∈T lies within ρ\rhoρ-distance δ\deltaδ of some θi\theta_iθi​; the δ\deltaδ-covering number N(δ;T,ρ)N(\delta;T,\rho)N(δ;T,ρ) is the size of the smallest such cover (Definition 5.1). The quantity log⁡N(δ;T,ρ)\log N(\delta;T,\rho)logN(δ;T,ρ) is the metric entropy of TTT at scale δ\deltaδ. Writing D:=sup⁡θ,θ′∈TρX(θ,θ′)D:=\sup_{\theta,\theta'\in T}\rho_X(\theta,\theta')D:=supθ,θ′∈T​ρX​(θ,θ′) for the diameter of TTT, the δ\deltaδ-truncated Dudley entropy integral is

J(δ;D)  :=  ∫δDlog⁡N(u;T) du.J(\delta; D) \;:=\; \int_\delta^D \sqrt{\log N(u;T)}\,du.J(δ;D):=∫δD​logN(u;T)​du.

Formalization targets

Goal — Theorem 5.22 (Dudley's entropy integral bound)

E[sup⁡θ,θ′∈T(Xθ−Xθ′)]  ≤  2 E[sup⁡γ,γ′∈TρX(γ,γ′)≤δ(Xγ−Xγ′)]+32 J(δ/4;D),for any δ∈[0,D].\mathbb E\Big[\sup_{\theta,\theta'\in T}(X_\theta-X_{\theta'})\Big] \;\le\; 2\,\mathbb E\Big[\sup_{\substack{\gamma,\gamma'\in T\\\rho_X(\gamma,\gamma')\le\delta}}(X_\gamma-X_{\gamma'})\Big] + 32\,J(\delta/4; D), \qquad \text{for any } \delta\in[0,D].E[θ,θ′∈Tsup​(Xθ​−Xθ′​)]≤2E[γ,γ′∈TρX​(γ,γ′)≤δ​sup​(Xγ​−Xγ′​)]+32J(δ/4;D),for any δ∈[0,D].

The bound holds for every zero-mean sub-Gaussian process, with no further structure on TTT beyond its metric entropy — this is what makes it a general-purpose tool rather than a bound tailored to one model.

Milestone — Proposition 5.17 (one-step discretization bound)

The same conclusion with 32 J(δ/4;D)32\,J(\delta/4;D)32J(δ/4;D) replaced by the cruder single-scale term 4D2log⁡N(δ;T)4\sqrt{D^2\log N(\delta;T)}4D2logN(δ;T)​, under the extra technical hypothesis N(δ;T)≥10N(\delta;T)\ge 10N(δ;T)≥10. This is the one-step precursor whose refinement — iterating the discretization over a geometric sequence of scales instead of applying it once — is exactly what chaining improves.

Milestone — Theorem 5.25 (the Gaussian comparison principle)

A general comparison principle for pairs of centered Gaussian random vectors whose pairwise covariances are ordered coordinatewise and tested against a function with matching sign conditions on its mixed second partial derivatives: E[F(X)]≤E[F(Y)]\mathbb E[F(X)]\le\mathbb E[F(Y)]E[F(X)]≤E[F(Y)]. This is the source, by specializing FFF and the covariance-ordering sets, of both Slepian's inequality and the Sudakov–Fernique comparison, the two workhorse tools of Gaussian process theory used elsewhere in the chapter to obtain sharper, Gaussian-specific bounds than the sub-Gaussian chaining bound above.

Significance

Dudley's bound is the single most-used tool for controlling suprema of stochastic processes in high-dimensional statistics and empirical process theory: Gaussian complexity bounds for convex bodies, operator-norm bounds for random matrices, and uniform laws of large numbers for function classes are all obtained by computing a covering-number bound for the relevant index set and substituting it into Theorem 5.22 (see, for instance, Examples 5.18–5.21 later in the same chapter, and Chapters 13–14 of the book). Its significance is exactly its generality: it converts a purely geometric quantity — how "big" a set is under a metric — into a probabilistic bound, uniformly over every sub-Gaussian process on that set.

Formalizing it. The mathematical proof (interpolation-free, based on chaining and repeated union bounds) is well understood and not itself in question; what this mission produces is a faithful Lean statement of the theorem, its immediate one-step precursor, and the general Gaussian comparison principle that underlies the chapter's complementary (Gaussian-specific) results, each against Mathlib's own measure-theoretic and Gaussian-process infrastructure. All three theorems are currently stated as open goals (:= by sorry); no claim is made here that they are already formalized elsewhere on the platform (a fresh prior-art search for "Dudley," "chaining," "Slepian," "Sudakov," and "Gaussian comparison" returned no faithful matches).

Difficulty

The naive approach — apply Proposition 5.17's one-step discretization once, at whatever scale δ\deltaδ seems best — cannot see improvement past the cruder D2log⁡N(δ;T)\sqrt{D^2\log N(\delta;T)}D2logN(δ;T)​ scaling of the metric entropy at a single resolution. The chaining argument that proves Theorem 5.22 instead telescopes the supremum across a geometric ladder of covers at scales D2−1,D2−2,…D2^{-1},D2^{-2},\dotsD2−1,D2−2,…, paying for each scale's approximation with a union bound over its own (much smaller, for a small δ\deltaδ) covering number, and only then summing the resulting terms into an integral. The difficulty is not any single step of this argument — each step is an elementary sub-Gaussian tail bound — but bookkeeping the composition correctly: the recursive "best approximation at level mmm of the best approximation at level m+1m+1m+1" chain (Eq. (5.47)) must be built explicitly, and the telescoping sum of LLL union bounds, each over a set that itself depends on the level mmm, is what converts into an integral only in the L→∞L\to\inftyL→∞ limit as the covers refine to TTT itself.

Formalization scope

The index set TTT is formalized as a nonempty Fintype, rather than the book's general totally bounded metric space: this keeps every covering number, diameter, and supremum in this mission a genuine maximum over a finite, nonempty family (realized via ⨆/sInf over finite index types), rather than requiring the full apparatus of totally bounded infinite metric spaces to state the covering-number definition (Definition 5.1) faithfully without risking a vacuous or ill-defined infimum. This is a genuine narrowing of the book's stated generality, disclosed here rather than left implicit — the underlying mathematics of the proof does not depend on finiteness, but a faithful formalization of a general totally bounded space's covering number was judged out of scope for this mission's budget.

The constant 323232 in the goal theorem is kept exactly as stated; the book's own remark that "there is no particular significance to the constant 32, which could be improved with a more careful analysis" is not license to substitute a sharper constant, since doing so would no longer match what this particular proof establishes. Expectations are Bochner integrals against an explicit probability measure Prob, with integrability required as an explicit hypothesis in the sub-Gaussian process definition (SubGaussianProcess) rather than left implicit, since Mathlib's Bochner integral silently returns 000 for a non-integrable function — a trivializing formalization this mission's definitions and hypotheses rule out.

Theorem 5.25's "centered Gaussian random vector" is formalized using Mathlib's own ProbabilityTheory.HasGaussianLaw predicate (a genuine multivariate Gaussian law, not merely Gaussian marginals) together with an explicit coordinatewise mean-zero hypothesis, and its mixed second partial derivative condition is formalized via iteratedFDeriv ℝ 2 F applied to the relevant pair of standard basis vectors, keeping the sign pattern over the disjoint index sets AAA and BBB exact rather than collapsing it to a global convexity assumption on FFF.

Out of scope for this mission: Sudakov's minoration (the complementary lower bound on the expected supremum of a genuinely Gaussian process, Theorem 5.30, misidentified as "Theorem 5.36" in this mission's planning brief — the correct Sudakov minoration statement is Theorem 5.30, p. 148; Theorem 5.36 is instead a tail-bound generalization of Dudley's bound to ψq\psi_qψq​-Orlicz processes) and the Slepian/Sudakov–Fernique corollaries of Theorem 5.25 (Corollary 5.26, Theorem 5.27) — both natural follow-on work for a later contribution, once the Gaussian comparison principle formalized here is in place.

Selected references

  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019. DOI: 10.1017/9781108627771. Chapter 5.
  • R. M. Dudley, "The sizes of compact subsets of Hilbert space and continuity of Gaussian processes," Journal of Functional Analysis, 1(3):290–330, 1967.
  • M. Ledoux and M. Talagrand, Probability in Banach Spaces: Isoperimetry and Processes, Springer, 1991.
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High-Dimensional Probability VII: Slepian's Inequality for Gaussian ProcessesTextbook

Motivation

A Gaussian process is a family (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ of jointly Gaussian real random variables indexed by an arbitrary set TTT — not necessarily time. The canonical example is Xt=⟨g,t⟩X_t = \langle g, t\rangleXt​=⟨g,t⟩ for ttt ranging over a subset T⊆RnT\subseteq\mathbb R^nT⊆Rn and ggg a standard Gaussian vector in Rn\mathbb R^nRn; this single family already encodes questions as varied as the operator norm of a random matrix, the size of a random projection, and the metric complexity of a convex body. In every one of these applications the object of interest reduces to the same quantity: Esup⁡t∈TXtE\sup_{t\in T} X_tEsupt∈T​Xt​, the expected supremum of the process.

Bounding Esup⁡t∈TXtE\sup_{t\in T} X_tEsupt∈T​Xt​ directly is hard — computing it exactly is possible only in special cases, such as the reflection principle for Brownian motion. Slepian's inequality (David Slepian, 1962) sidesteps this by comparison: if a second Gaussian process (Yt)t∈T(Y_t)_{t\in T}(Yt​)t∈T​ has matching variances and at-least-as-large pairwise increments as (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​, then YYY's supremum stochastically dominates XXX's. This turns a hard direct estimate into a search for a simpler comparison process — the technique that Sudakov and Fernique later sharpened by dropping the equal-variance hypothesis (Theorem 7.2.11), and that Sudakov used to derive a purely geometric lower bound on Esup⁡t∈TXtE\sup_{t\in T}X_tEsupt∈T​Xt​ from the covering numbers of (T,d)(T,d)(T,d) (Theorem 7.4.1, Sudakov's minoration inequality). Together these results are the entry point to the theory of Gaussian width and generic chaining that occupies the rest of the book (Chapters 7–9, 11), and they underlie sharp bounds on random matrices (Section 7.3), random projections (Chapter 9), and high-dimensional geometry more broadly (Adler and Taylor, Random Fields and Geometry, Springer, 2007; Talagrand, Upper and Lower Bounds for Stochastic Processes, Springer, 2014).

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P). A random process indexed by a set TTT is a family (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ of real random variables on Ω\OmegaΩ. It is a Gaussian process if every finite linear combination ∑t∈T0atXt\sum_{t\in T_0} a_t X_t∑t∈T0​​at​Xt​ (T0⊆TT_0\subseteq TT0​⊆T finite, at∈Ra_t\in \mathbb Rat​∈R) is a (possibly degenerate) normal random variable — equivalently, every finite marginal (Xt)t∈T0(X_t)_{t\in T_0}(Xt​)t∈T0​​ is a multivariate Gaussian vector. A process is mean zero if EXt=0EX_t = 0EXt​=0 for every ttt.

For a mean zero process, the increments d(t,s):=∥Xt−Xs∥L2=(E(Xt−Xs)2)1/2d(t,s) := \lVert X_t - X_s\rVert_{L^2} = (E(X_t - X_s)^2)^{1/2}d(t,s):=∥Xt​−Xs​∥L2​=(E(Xt​−Xs​)2)1/2 always define a (pseudo)metric on TTT — the canonical metric — turning the otherwise unstructured index set into a metric space. For a metric space (T,d)(T,d)(T,d) and $\varepsilon

0,the∗∗coveringnumber∗∗, the **covering number** ,the∗∗coveringnumber∗∗N(T,d,\varepsilon)isthesmallestcardinalityofafinitesubsetis the smallest cardinality of a finite subsetisthesmallestcardinalityofafinitesubsetN\subseteq Tsuchthateverypointofsuch that every point ofsuchthateverypointofTiswithinis withiniswithin\varepsilonofsomepointofof some point ofofsomepointofN(an(an(an\varepsilon−net);-net); −net);N(T,d,\varepsilon) := \infty$ if no finite net exists.

Because TTT need not be countable, sup⁡t∈TXt(ω)\sup_{t\in T} X_t(\omega)supt∈T​Xt​(ω) need not be a measurable function of ω\omegaω. Following the book's own convention, every quantity built from this supremum — Esup⁡t∈TXtE\sup_{t\in T}X_tEsupt∈T​Xt​ and P{sup⁡t∈TXt≥τ}P\{\sup_{t\in T}X_t\ge\tau\}P{supt∈T​Xt​≥τ} — is instead defined through the process's finite-dimensional marginals: as the supremum, over finite nonempty T0⊆TT_0\subseteq TT0​⊆T, of Emax⁡t∈T0XtE\max_{t\in T_0}X_tEmaxt∈T0​​Xt​ (respectively P{max⁡t∈T0Xt≥τ}P\{\max_{t\in T_0}X_t\ge\tau\}P{maxt∈T0​​Xt​≥τ}). This sidesteps the measurability question entirely, at the cost of the quantity possibly being +∞+\infty+∞.

Formalization targets

Slepian's inequality (Theorem 7.2.1, goal)

Let (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ and (Yt)t∈T(Y_t)_{t\in T}(Yt​)t∈T​ be mean zero Gaussian processes with EXt2=EYt2EX_t^2 = EY_t^2EXt2​=EYt2​ and E(Xt−Xs)2≤E(Yt−Ys)2E(X_t-X_s)^2 \le E(Y_t-Y_s)^2E(Xt​−Xs​)2≤E(Yt​−Ys​)2 for all t,s∈Tt,s\in Tt,s∈T. Then for every τ∈R\tau\in\mathbb Rτ∈R,

P{sup⁡t∈TXt≥τ}≤P{sup⁡t∈TYt≥τ},P\{\sup_{t\in T} X_t \ge \tau\} \le P\{\sup_{t\in T} Y_t \ge \tau\},P{t∈Tsup​Xt​≥τ}≤P{t∈Tsup​Yt​≥τ},

and consequently Esup⁡t∈TXt≤Esup⁡t∈TYtE\sup_{t\in T} X_t \le E\sup_{t\in T} Y_tEsupt∈T​Xt​≤Esupt∈T​Yt​.

Sudakov-Fernique's inequality (Theorem 7.2.11, milestone)

Under only the increment hypothesis E(Xt−Xs)2≤E(Yt−Ys)2E(X_t-X_s)^2 \le E(Y_t-Y_s)^2E(Xt​−Xs​)2≤E(Yt​−Ys​)2 (no equal-variance hypothesis),

Esup⁡t∈TXt≤Esup⁡t∈TYt.E\sup_{t\in T} X_t \le E\sup_{t\in T} Y_t.Et∈Tsup​Xt​≤Et∈Tsup​Yt​.

This is the weaker-hypothesis, strictly more applicable form: it is what Sudakov's minoration inequality and the sharp Gaussian random matrix bound of Section 7.3 both invoke.

Sudakov's minoration inequality (Theorem 7.4.1, milestone)

Let (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ be a mean zero Gaussian process with canonical metric ddd. For every ε≥0\varepsilon\ge 0ε≥0 at which N(T,d,ε)=:NN(T,d,\varepsilon)=:NN(T,d,ε)=:N is finite,

Esup⁡t∈TXt≥c ε log⁡NE\sup_{t\in T} X_t \ge c\,\varepsilon\,\sqrt{\log N}Et∈Tsup​Xt​≥cεlogN​

for an absolute constant c>0c>0c>0. This is the weakest, most stable form of the bound: it names no numerical value for ccc, so it survives any later sharpening of the constant.

Slepian's inequality, finite-dimensional case (Theorem 7.2.9, milestone)

The vector-indexed special case of Theorem 7.2.1 (TTT finite), proved first by Gaussian interpolation and then extended to the general index set.

Significance

The results themselves. Slepian's inequality is the founding comparison theorem for Gaussian processes; Sudakov-Fernique's inequality is its practically indispensable generalization, used routinely to bound suprema of Gaussian processes without needing to track variances explicitly. Sudakov's minoration inequality is the first bridge from the probability of a Gaussian process to the metric geometry of its index set, complementing Dudley's upper bound (Chapter 8) and together giving matching bounds — up to a logarithmic factor, and exactly in many cases of interest — on Esup⁡t∈TXtE\sup_{t\in T}X_tEsupt∈T​Xt​ purely from the covering numbers of (T,d)(T,d)(T,d). Downstream, this machinery gives the sharp bound E∥A∥≤m+nE\lVert A\rVert \le \sqrt m + \sqrt nE∥A∥≤m​+n​ on Gaussian random matrices (Section 7.3), underlies the Gaussian width used throughout convex geometry and compressed sensing (Chapters 9, 11), and bounds the covering numbers of polytopes and other convex sets (Corollary 7.4.4).

Formalizing it. All three inequalities are proved by the book (Gaussian interpolation and integration by parts for Slepian/Sudakov-Fernique; a direct application of Sudakov-Fernique to a well-chosen comparison process for Sudakov's minoration), so this mission's work is formalizing the statements faithfully and precisely — including the finite-marginal convention needed to make Esup⁡t∈TXtE\sup_{t\in T}X_tEsupt∈T​Xt​ and P{sup⁡t∈TXt≥τ}P\{\sup_{t\in T}X_t\ge\tau\}P{supt∈T​Xt​≥τ} meaningful for an uncountable index set without begging the underlying measurability question. The Gaussian interpolation technique itself (Lemmas 7.2.3, 7.2.5, 7.2.7) is not part of this mission's formalization scope; it is the proof method for the milestones and belongs to solvers closing them.

Difficulty

The obvious first idea — bound Esup⁡tXtE\sup_t X_tEsupt​Xt​ by controlling each XtX_tXt​ separately, e.g. via a union bound over a net — throws away exactly the structure Slepian-type comparisons exploit: the joint Gaussianity across ttt, not marginal tail behavior at each fixed ttt. A union bound needs a net and a modulus of continuity to begin with; Slepian's and Sudakov-Fernique's inequalities need neither — they compare two processes directly through their covariance structure, which is what makes the technique (Gaussian interpolation: continuously deform the covariance of one process into the other's, and track how a smooth, nearly-indicator functional behaves along the path) work with no assumption on TTT beyond the two hypotheses stated. The genuine difficulty is the smooth-interpolation argument itself — showing that Ef(Z(u))E f(Z(u))Ef(Z(u)) is monotone in uuu for the right choice of test function fff — which is exactly the part left as a milestone for solvers to formalize, not sketched here per the mission format's own rule against proof ideas.

Formalization scope

Esup⁡t∈TXtE\sup_{t\in T}X_tEsupt∈T​Xt​ (ProcessESup) is valued in EReal, not ℝ: the finite-marginal supremum a real-valued definition would silently default to the junk value 000 when the set of finite-marginal expectations is unbounded above — exactly the case the book itself records as Esup⁡t∈TXt=∞E\sup_{t\in T}X_t=\inftyEsupt∈T​Xt​=∞ (Exercise 7.4.2, a non-relatively-compact index set). P\{\sup_{t\in T}X_t\ge\tau\} (ProcessTailProb) stays real-valued, since it is always bounded in [0,1][0,1][0,1] and so carries no such risk. Both are defined through finite nonempty subsets of TTT, per the book's own footnote to Section 7.2; no separability, continuity, or countability assumption is placed on TTT itself.

Gaussianity is Mathlib's ProbabilityTheory.IsGaussianProcess — every finite restriction of the process has a Gaussian law — which is definitionally the book's Definition 7.1.10 ("every finite linear combination is Gaussian"); mean-zero is stated as an explicit hypothesis alongside it. Integrability of every quantity appearing under an expectation is not stated as a separate hypothesis: Fernique's theorem (already in Mathlib for general Gaussian measures) guarantees a Gaussian process has finite moments of every order, exactly as the book takes for granted.

Sudakov's minoration inequality (Theorem 7.4.1) is formalized for the case the book's own proof actually covers — N(T,d,ε)N(T,d,\varepsilon)N(T,d,ε) finite, taken as a hypothesis = (N : ℕ) rather than as a case split inside the conclusion — since the book itself defers the infinite-covering-number case to a separate, unproved exercise (7.4.2). This keeps TTT fully general (still possibly uncountable) at every fixed ε\varepsilonε where the net is finite, which rules out a trivializing reading of the theorem: nothing here forces TTT itself to be finite or countable, only the covering number at the scale ε\varepsilonε in play, which is the book's own hypothesis.

Definitions reusable beyond this mission: ProcessESup, ProcessTailProb, CanonicalMetric, and CoveringNumber are exactly the substrate Chapters 8 ("Dudley's Integral Inequality"), 9 ("The Matrix Deviation Inequality"), and 11 ("Dvoretzky-Milman's Theorem") need for Gaussian width and generic chaining; per this series' plan those missions restate them locally (drafts cannot import another draft's definitions), using this chunk's forms as the faithful reference. Contributions closing the Gaussian-interpolation machinery (Lemmas 7.2.3–7.2.8) as a reusable definitions layer, beyond what any one milestone needs, are welcome.

Selected references

  • Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018. https://www.math.uci.edu/~rvershyn/papers/HDP-book/HDP-book.pdf
  • D. Slepian, "The one-sided barrier problem for Gaussian noise", Bell System Technical Journal 41 (1962), 463–501.
  • V. N. Sudakov, "Gaussian random processes and measures of solid angles in Hilbert space", Soviet Mathematics Doklady 12 (1971), 412–415.
  • X. Fernique, "Regularité des trajectoires des fonctions aléatoires gaussiennes", in École d'Été de Probabilités de Saint-Flour IV-1974, Springer Lecture Notes in Mathematics 480 (1975), 1–96.
  • M. Talagrand, Upper and Lower Bounds for Stochastic Processes: Modern Methods and Classical Problems, Springer, 2014.
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Introduction to Stochastic Programming VII: Convergence Rates for Sample Average ApproximationTextbook

Motivation

Most stochastic programs cannot be solved exactly: the expectation defining the objective is an integral over a continuous or high-dimensional random parameter, and evaluating it exactly is as hard as the optimization itself. The standard remedy is Monte Carlo: draw a sample of size ν from the random parameter, replace the true expectation by the sample average, and solve the resulting finite-dimensional "sample average approximation" (SAA) instead. This only helps if the SAA's optimal value and optimal solution actually converge to the true problem's as ν → ∞, and if that convergence is fast enough to be useful with a sample size one can actually draw and solve. Birge & Louveaux's Chapter 9, §9.5, states the two central asymptotic results that justify this approach for a general (not necessarily linear, not necessarily two-stage) stochastic program: a central limit theorem describing the SAA optimal value's fluctuations around the truth (Theorem 6, after Shapiro [1991]), and an exponential-rate large-deviation bound on how quickly both the SAA value and the SAA solution concentrate near their true counterparts as the sample grows (Theorem 7, after Dai, Chen & Birge [2000]). This mission formalizes both statements.

Setting

Fix a feasible set X ⊆ ℝⁿ of first-stage decisions and an outcome space Ξ carrying a σ-algebra. The book considers the general stochastic program

z* = inf_{x ∈ X} ∫_Ξ g(x,ξ) P(dξ),                                                        (5.1)

with g : ℝⁿ × Ξ → ℝ an abstract integrand — no longer specialized to the two-stage recourse cost Q(x,ξ) of Chapters 3–7, matching the book's own level of generality at this point in §9.5 — and ξ a random element of (Ξ, 𝓑, P). Given an i.i.d. sample ξ₁, ξ₂, … from P, the sample average approximation of size ν is

zν = inf_{x ∈ X} (1/ν) Σᵢ₌₁^ν g(x,ξᵢ) .                                                    (5.2)

Both z* and zν are attained (an optimal solution x* of (5.1); a random optimal solution xν(ω) of (5.2) at each sample outcome ω). The two chapter results describe, in different regimes, how (zν, xν) relates to (z*, x*) as ν → ∞.

Formalized in this mission: X sits in EuclideanSpace ℝ (Fin n); the sample is a sequence ξ : ℕ → Ω → Ξ on an ambient probability space (Ω, P), independent and identically distributed (Mathlib's iIndepFun/IdentDistrib); z*, x*, zν, xν are given as hypotheses that pin them down as the optimal value and an optimal point of (5.1)/(5.2) (a lower bound over X plus attainment at the named point), rather than computed via sInf/sSup of an image set — Real's extended-real infimum returns the junk value 0 on an unbounded-below or empty set, which would silently misstate the theorems if X, g are only assumed as loosely as the book states them.

Formalization targets

Goal — Chapter 9, Theorem 7 (p. 412)

∀ ε>0, ∃ α>0, ∃ β>0,
  (∀ ν>0, P[|zν − z*| ≥ ε] ≤ α·e^{−βν})
  ∧ (x* the unique optimal solution of (5.1) → ∀ ν≥1, P[‖xν − x*‖ ≥ ε] ≤ α·e^{−βν})

under the moment hypothesis: there exist a>0, θ₀>0, η : Ξ → ℝ with |g(x,ξ)| ≤ a·η(ξ) for all x ∈ X, and E[e^{θ·η(ξ)}] < ∞ for every θ ∈ [0,θ₀]. This is the mission's goal because it is a clean, self-contained existential-constants statement — no algorithm to define, unlike most of the chapter's other convergence results — and because, like Chunk 03's Theorem 6(a), the book's own proof cites an external paper (Dai, Chen & Birge [2000], Theorems 3.1–3.2) and gives no in-text derivation: the statement itself, not a derivation from a preceding numbered result of this book, is the mission's content.

Milestone — Chapter 9, Theorem 6 (p. 411)

X compact, g(x,·) measurable ∀x∈X, g Lipschitz in x with an L²(μ) envelope a,
x0 the unique minimizer of x ↦ E g(x) over X
  ⟹ √ν·[zν − E g(x0)] converges in distribution to N(0, Var g(x0))

Included as a milestone (not used in Theorem 7's proof, which the book does not give — see above) because it is the chapter's other general SAA convergence result, standing on the same setup (5.1)–(5.2), and because Mathlib's MeasureTheory.Function.ConvergenceInDistribution (the TendstoInDistribution predicate) plus Probability.Distributions.Gaussian.Real (gaussianReal) and Mathlib's own i.i.d. central limit theorem (ProbabilityTheory.tendstoInDistribution_inv_sqrt_mul_sum_sub) supply exactly the vocabulary needed to state — not prove — a faithful weak-convergence-to-Gaussian conclusion. Chunk 09's BRIEF.md flagged this as a milestone to attempt "only if your workspace has enough of a weak-convergence/CLT toolkit in Mathlib to state it faithfully"; the toolkit is present (verified directly, not assumed from substrate.md, which predates this rev's addition of ConvergenceInDistribution.lean), so it is included.

Significance

Every practical Monte Carlo solution method for stochastic programming — every discretization, every scenario-reduction heuristic, every "solve on a sample and hope" approach used throughout the rest of the book and the wider literature — rests on exactly these two results: that the SAA converges at all (Theorem 6's CLT gives the asymptotic distribution of the error) and that it converges fast enough to bound the error at a finite, computable sample size (Theorem 7's exponential rate). Formalizing them gives Prove2Me a first foothold in convergence-rate theory for stochastic optimization under sampling, a genre distinct from the concentration-of-measure results already reachable via Mathlib's sub-Gaussian machinery (Probability/Moments/SubGaussian.lean): sub-Gaussian concentration bounds a fixed-size sample's deviation from its own mean, not the rate-in-ν convergence of a nested sequence of optimization problems' values and solutions to a limiting problem's — the object Theorem 7 is actually about.

Difficulty

Theorem 6 needs a functional/uniform argument over the whole feasible set X (not the plain i.i.d. CLT at the single point x0) to control the interaction between sampling noise and the optimization over x; the book states it without proof, citing Shapiro [1991]. Theorem 7's constants α, β are produced by a large-deviation argument specific to the exponential-moment condition, again cited rather than derived in the book. Both are left as sorry; the value of this mission is the faithful statement, matching the difficulty pattern already established for Chunk 03's Theorem 6(a) (a result the book itself only cites).

Formalization scope

  • Existential constants left abstract, never sharpened or weakened. Theorem 7's α, β are ∃-bound exactly as the book leaves them (trap 8 of reference/FAITHFULNESS_TRAPS.md: the existentials sit outside every quantifier they must be uniform over — in particular outside the ∀ ν). No closed form for α, β in terms of a, θ0, ε is invented.
  • The book's own typo is corrected, and the correction is flagged. The printed (5.8) reads P[E[zν − z*)] ≥ ε] ≤ αe^{−βν} — an unmatched parenthesis and a stray E[·] around a quantity that is already deterministic. milestones.yaml/MODERATION_NOTES.md quote the typo verbatim; the Lean and natural_language_statement use the unambiguous P[|zν − z*| ≥ ε] the surrounding prose (and every other occurrence of this quantity in the section) plainly intends.
  • g is left fully abstract, not specialized to the two-stage recourse cost Q(x,ξ) of Chunks 03–07, matching §9.5's own generality and keeping this mission independent of every other chunk's namespace (no cross-chunk import, per missions/README.md's "Prior art" column for this chunk: "none expected").
  • z*, x*, zν, xν are hypothesis-characterized, not sInf/sSup-defined, to avoid the real extended-value junk-value trap (trap 5) discussed under Setting above.
  • Measurability of zν, xν is an added hypothesis (hzSAA_meas/hxSAA_meas/hzSAA_meas in Theorem 6), not derivable from the other hypotheses since g is abstract; the book is silent on this technical point, standard for an applied convergence theorem, but Lean's P {ω | …} needs it for the displayed probability to be the actual measure of the event rather than an outer-measure value on a possibly non-measurable set.
  • Convergence in distribution (Theorem 6) is formalized via Mathlib's TendstoInDistribution, with the limiting Gaussian supplied as an explicit random variable Y on a separate probability space with HasLaw Y (gaussianReal 0 σ²) P' — the same pattern Mathlib's own CLT (tendstoInDistribution_inv_sqrt_mul_sum_sub) uses for its own conclusion.
  • Trivialization risk (this chapter's own, beyond paper.md's book-wide list item 5). A formalization that quantifies α, β universally, or with an invented closed form, would assert something the book's proof (cited, not given) does not establish; a formalization of Theorem 7 that used a computable sInf-defined zν on a set that is not shown bounded below would let the conclusion hold vacuously via the junk value 0, independent of the genuine large-deviation content — both are excluded by the choices above.

Selected references

  • Birge, J.R., Louveaux, F. Introduction to Stochastic Programming, 2nd ed., Springer 2011, Chapter 9, §9.5 (pp. 409–412).
  • Shapiro, A. "Asymptotic properties of statistical estimators in stochastic programming." Annals of Statistics 19 (1991), 1463–1466 — proof of Theorem 6 (their Theorem 3.3).
  • Dai, L., Chen, C.-H., Birge, J.R. "Convergence properties of two-stage stochastic programming." Journal of Optimization Theory and Applications 106 (2000), 489–509 — proof of Theorem 7 (their Theorems 3.1–3.2).
  • King, A.J., Rockafellar, R.T. "Asymptotic theory for solutions in statistical estimation and stochastic programming." Mathematics of Operations Research 18 (1993), 148–162 — the general theory of §9.5's opening (Theorem 5), the chapter's third general result, not formalized here (see STATUS.md for why it is out of scope).
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Introduction to Stochastic Programming IV: Nested Decomposition for Multistage ProgramsTextbook

Motivation

Sequential planning problems — inventory replenishment, hydro-thermal power scheduling, asset-liability management — routinely span more than two decision epochs, with information about the future revealed gradually as each period unfolds. A two-stage recourse model (decide now, observe once, recourse once) is too coarse for these: it either collapses the whole horizon into a single "wait and see" observation or forces an ad-hoc rolling-horizon heuristic with no optimality guarantee. The multistage stochastic program is the natural model that keeps the full sequence of decisions and observations, and Benders (L-shaped) decomposition is the workhorse algorithm the field has used to solve it since Van Slyke and Wets [1969] introduced it for the two-stage case. Ho and Manne [1974] and Glassey [1973] first proposed nested decomposition for deterministic multistage models; Louveaux [1980] extended it to multistage quadratic stochastic programs, and Birge [1985] gave the linear multistage generalization this mission formalizes, later implemented at scale by Pereira and Pinto [1985] and Gassmann [1990] and still the basis of production stochastic-programming solvers today.

Setting

A multistage stochastic linear program unfolds over HHH stages t=1,…,Ht = 1,\dots,Ht=1,…,H. At each stage, uncertainty resolves into one of finitely many realizations, so the whole process of realizations forms a scenario tree: a single scenario at t=1t=1t=1 (the root), branching into finitely many scenarios at t=2t=2t=2, each of those again branching at t=3t=3t=3, and so on. Write kkk for a scenario (a tree node) and a(k)a(k)a(k) for its ancestor, the scenario at stage t−1t-1t−1 that kkk descends from; Dt+1(j)D^{t+1}(j)Dt+1(j) is the set of scenario jjj's descendants at the next stage. Each scenario kkk at stage ttt carries its own decision vector xkt≥0x^t_k \ge 0xkt​≥0, bounded above (xkt≤uktx^t_k \le u^t_kxkt​≤ukt​, coordinatewise), subject to the linear constraint

Wtxkt=hkt−Tkt−1xa(k)t−1,W^t x^t_k = h^t_k - T^{t-1}_k x^{t-1}_{a(k)},Wtxkt​=hkt​−Tkt−1​xa(k)t−1​,

where the recourse matrix WtW^tWt depends only on the stage (fixed recourse) while the transition matrix Tkt−1T^{t-1}_kTkt−1​ and right-hand side hkth^t_khkt​ may vary scenario by scenario. Stacking every scenario's constraint over the whole tree gives the deterministic equivalent linear program, minimizing the probability-weighted total cost ∑kpk(ckt)⊤xkt\sum_k p_k (c^t_k)^\top x^t_k∑k​pk​(ckt​)⊤xkt​ over this feasible region — problem (3.4.1) in the source.

The nested L-shaped method solves (3.4.1) by decomposition rather than forming this (typically enormous) single LP directly. Each scenario kkk owns a small subproblem, NLDS(t,k)\mathrm{NLDS}(t,k)NLDS(t,k), that looks exactly like a two-stage L-shaped subproblem: it has kkk's own constraint and bound, plus a running set of feasibility cuts and optimality cuts accumulated so far, plus, if kkk has descendants, an approximation variable θkt\theta^t_kθkt​ standing in for the (unknown, convex, piecewise-linear) future cost Qkt+1Q^{t+1}_kQkt+1​ of everything downstream of kkk. Solving NLDS(t,k)\mathrm{NLDS}(t,k)NLDS(t,k) either finds it infeasible — in which case a feasibility cut is derived from the infeasibility certificate and sent up to kkk's parent — or finds an optimal dual solution, whose aggregate over all of jjj's children (weighted by conditional probability) becomes a candidate optimality cut for j=a(k)j = a(k)j=a(k). The method sweeps forward and backward across the tree, feasibility and optimality cuts accumulating at every internal node, until no node's subproblem produces a fresh cut.

Formalization targets

Goal (Chapter 6, Theorem 1)

if every Ξt is finite and every xt has a finite upper bound, then the nested L-shaped method\text{if every }\Xi_t\text{ is finite and every }x_t\text{ has a finite upper bound, then the nested L-shaped method}if every Ξt​ is finite and every xt​ has a finite upper bound, then the nested L-shaped method converges finitely to an optimal solution of the deterministic equivalent (3.4.1), or correctly certifies its infeasibility.\text{converges finitely to an optimal solution of the deterministic equivalent (3.4.1), or correctly certifies its infeasibility.}converges finitely to an optimal solution of the deterministic equivalent (3.4.1), or correctly certifies its infeasibility.

This is the chapter's only numbered result and the weakest faithful statement of "the method works": it makes no claim about the number of iterations beyond finiteness, and none about which sequencing protocol (forward-forward-back, or any other) is used to choose which subproblem to solve next.

Significance

Finite convergence is what separates an algorithm from a heuristic: without it, nothing rules out an infinite sequence of ever-finer cuts that never certifies optimality or infeasibility. Birge's 1985 result is the reason nested Benders decomposition can be used as an exact method rather than an approximation, and every later refinement (bunching, sifting, multicuts, parallel implementations, all mentioned in the source text) modifies how cuts are generated or which subproblem is solved next without touching this finiteness guarantee — they are all still instances of the same cut-generation mechanism this mission formalizes. The two-stage case (Chapter 5, Theorem 2) is the H=2H=2H=2 special case of this theorem; the mission's tree-indexed state and transition relation are written to specialize to the two-stage development directly when the tree has one branching level, though the two developments are not connected by an import (see Formalization scope). No machine-checked proof of either the two-stage or multistage case appears to exist prior to this series; formalizing it here produces the first Lean statement of the mechanism nested Benders decomposition rests on.

Difficulty

The obvious first idea — prove finiteness by bounding the total number of cuts a node can ever receive, the way a flat scenario set bounds the two-stage method's cut count by its number of LP bases — fails because a node's own subproblem is not a fixed-size LP: every cut recorded at node kkk becomes a new row of kkk's own constraint set, so the "number of possible bases" at kkk keeps changing as the algorithm runs, and the bound at kkk depends recursively on how many cuts kkk's own children could ever produce. The book's actual argument (p. 290) is a genuine induction on the stage index, from the last stage backward: assume the bound holds for every node at stage t+1t+1t+1, then combinatorially bound the finite number of extended bases at stage ttt that this permits, then take the finite union over every possible extension size. This mission's Lean development commits to a scope that keeps a node's basis a fixed-size object (see below) rather than re-deriving that combinatorial bound.

Formalization scope

Every stage shares one decision dimension nnn and one constraint dimension mmm (Fin n, Fin m); the book allows these to vary by stage but nothing in Theorem 1's statement needs that generality. Scenario probabilities p are the unconditional probability of reaching a node, required strictly positive and summing to 111 within each stage (Instance.hp_pos, Instance.hp_sum); the aggregation formulas use only the ratio pk/pjp_k/p_jpk​/pj​ for kkk a child of jjj, which reads the same whether p is unconditional or conditional, so this is a normalization choice, not a substantive restriction. The upper bound ub is ℝ-valued rather than extended-real-valued, which is Theorem 1's own hypothesis ("finite upper bounds"), not an added convention.

The one deliberate scope-narrowing choice, flagged here and in MODERATION_NOTES.md, and strengthened in this revision after moderator review (2026-09-19, CHANGES_REQUESTED.md #2): a node kkk's dual witness (Basis, FeasBasis) is read off kkk's original constraint (1.2) alone — the fixed-size recourse matrix Wstage(k)W^{\mathrm{stage}(k)}Wstage(k) — never off the extended constraint set (1.2)-(1.4). The gap this leaves is broader than "accumulated cuts are ignored": kkk's own continuation variable θk\theta_kθk​ — present in (1.1)'s objective, and fixed to 000 from Step 0 onward, not merely absent until cuts accumulate — has no representation at all in Basis, multiplier, basisValue, or the optimality-cut coefficients optCutCoeffs computes for a parent jjj of kkk. Consequently, whenever a child kkk used in an optimality cut is itself an interior node (kkk has children of its own, i.e. stage(k)<H−1\mathrm{stage}(k) < H-1stage(k)<H−1, which happens for every H≥3H \geq 3H≥3 tree), the mechanized cut coefficients are not the book's (Ejt−1,ejt−1)(E^{t-1}_j, e^{t-1}_j)(Ejt−1​,ejt−1​) of Eq. (1.1) and are not the printed algorithm's mechanism at that node — they are the dual of kkk's plain sub-LP alone, omitting kkk's own contribution to the recourse value entirely, not only the portion contributed by kkk's accumulated cuts. This gap is inert exactly when every child aggregated in a cut is a last-stage node (H≤2H \le 2H≤2, where the mechanism coincides with the already-published two-stage sibling 05-two-stage-methods) and active for every deeper cut, which is most of what a general Tree H actually exercises. Concretely: as mechanized, the optimality-cut half of Step (Bases.optCutCoeffs, Step.opt) is faithful to the printed nested L-shaped method's cut-generation step only when every child it aggregates over is a last-stage node; for an interior child it computes a value that omits that child's own θ\thetaθ term rather than the book's recursive one. The feasibility-cut half (Bases.feasCutCoeffs, Step.feas) has no such gap — feasibility does not involve θ\thetaθ at any stage — and the tree/instance layer (Tree, Instance) and the goal theorem's own outer shape are unaffected: thm1_finite_convergence's statement (existence of a finite, Step-reachable state that is infeasible-certified or globally optimal) is not weakened, but the reader should treat the mechanized Step relation itself, for H ≥ 3, as a documented variant of Steps 1-2 rather than a literal transcription of them at every node — see STATUS.md's Revision section for the moderator exchange this responds to. Reworking cut generation to consume each child's own current (xk,θk)(x_k, \theta_k)(xk​,θk​) witness directly, so that an interior child's continuation value is no longer dropped, is left to a future revision; it is a materially larger change (the child's local optimum is then piecewise-linear rather than linear in its own parent's decision, so the duality argument needs a genuinely different — not merely extended — basis notion) than this session's time budget allows. This keeps every basis type a fixed-size Fin m → Fin n object, exactly as in the two-stage method, and keeps the algorithm's finite-step bound an explicit, provable cardinality (|Node × FeasBasis| + |Node → Basis|) rather than the book's own implicit, recursively-defined one. The trivializing formalization this scope choice must not fall into — declaring victory by proving the plain two-stage case is what convergence "reduces to" without ever quantifying over the tree — is avoided because every definition and the goal statement itself are stated for a general Tree H with unrestricted branching, not merely H=2H = 2H=2; what is disclosed above is a gap in how faithfully Step models the book's own cut-generation mechanism at depth, not a restriction of the statement to H=2H = 2H=2.

Reusable beyond this mission: Def_StochasticProg_Multistage_Tree (the finite scenario tree) is a natural building block for 07-integer-programs (an integer restriction of the same two-stage subproblem) and 10-multistage-approximations (multistage Jensen bounds, which need the same tree). Contributions welcome: a faithful account of the extended-basis induction sketched above, and a formalization of Chapter 6, Theorem 3 (finite termination of the quadratic nested decomposition of Section 6.2), which this mission omits for time (see STATUS.md).

Selected references

  • J.R. Birge, "Decomposition and Partitioning Methods for Multistage Stochastic Linear Programs", Operations Research 33(5), 1985.
  • R.M. Van Slyke, R. Wets, "L-Shaped Linear Programs with Applications to Optimal Control and Stochastic Programming", SIAM Journal on Applied Mathematics 17(4), 1969. https://doi.org/10.1137/0117061
  • H.I. Gassmann, "MSLiP: A Computer Code for the Multistage Stochastic Linear Programming Problem", Mathematical Programming 47, 1990. https://doi.org/10.1007/BF01580858
  • M.V.F. Pereira, L.M.V.G. Pinto, "Stochastic Optimization of a Multireservoir Hydroelectric System: A Decomposition Approach", Water Resources Research 21(6), 1985. https://doi.org/10.1029/WR021i006p00779
  • J.R. Birge, F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer Series in Operations Research and Financial Engineering, 2011. https://doi.org/10.1007/978-1-4614-0237-4
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Mathematical Physics·Captain: Lucas

Langevin Dynamics in a Harmonic Trap: the Mean-Squared Displacement EquationTextbook

Motivation

A micron-sized bead suspended in water and held by an optical tweezer is one of the standard measuring instruments of soft-matter physics: the bead's fluctuating position reports on the viscosity of the medium, on the stiffness of the trap, and on the forces exerted by whatever is attached to the bead. The quantity that experiments record is the mean-squared displacement (MSD) ⟨r2⟩(t)\langle r^2 \rangle (t)⟨r2⟩(t) of the bead. Interpreting such data rests on a single classical calculation, due to Paul Langevin (1908): write Newton's second law for the bead including the drag of the fluid, the trap force and the fluctuating force of the molecular environment, multiply the equation by the position, and average over realizations. What comes out is a closed, deterministic, second-order ordinary differential equation for ⟨r2⟩\langle r^2 \rangle⟨r2⟩ — no stochastic calculus required. This mission formalizes exactly that derivation, and the solution of the resulting equation, for a particle in a harmonic trap.

Setting

A particle of mass m>0m > 0m>0 moves in ddd Cartesian dimensions. Its position at time t∈Rt \in \mathbb{R}t∈R is the vector r(t)r(t)r(t) with components xi(t)x_i(t)xi​(t), i=1,…,di = 1,\dots,di=1,…,d; its velocity components are vi(t)=x˙i(t)v_i(t) = \dot{x}_i(t)vi​(t)=x˙i​(t) and its acceleration components ai(t)=v˙i(t)a_i(t) = \dot{v}_i(t)ai​(t)=v˙i​(t). The particle feels three forces: a hydrodynamic drag −ζr˙-\zeta \dot{r}−ζr˙ with drag coefficient ζ\zetaζ; a harmonic trap force −kr-k r−kr with spring constant kkk; and a random force f(t)f(t)f(t) exerted by the surrounding medium, which is held at temperature TTT. Newton's second law then reads

mr¨(t)=−ζr˙(t)−k r(t)+f(t).m \ddot{r}(t) = -\zeta \dot{r}(t) - k\, r(t) + f(t).mr¨(t)=−ζr˙(t)−kr(t)+f(t).

A single solution of this equation, for one realization of the random force, is called a path. An ensemble is a probability space (Ω,μ)(\Omega,\mu)(Ω,μ) of such paths, and the ensemble average of a quantity AAA is ⟨A⟩=∫ΩA dμ\langle A \rangle = \int_\Omega A \, d\mu⟨A⟩=∫Ω​Adμ. Two physical inputs single out a thermal environment: the random force is uncorrelated with the instantaneous position, ⟨r⋅f⟩=0\langle r \cdot f \rangle = 0⟨r⋅f⟩=0, and the velocity obeys equipartition, m⟨r˙2⟩=d kBTm \langle \dot{r}^2 \rangle = d\, k_B Tm⟨r˙2⟩=dkB​T with kBk_BkB​ Boltzmann's constant. The mean-squared displacement is M(t)=⟨r(t)2⟩M(t) = \langle r(t)^2 \rangleM(t)=⟨r(t)2⟩.

Formalization targets

Goal — the MSD equation

mM¨(t)+ζM˙(t)+2k M(t)=2d kBT,M(t)=⟨r(t)2⟩.m \ddot{M}(t) + \zeta \dot{M}(t) + 2 k\, M(t) = 2 d\, k_B T , \qquad M(t) = \langle r(t)^2 \rangle .mM¨(t)+ζM˙(t)+2kM(t)=2dkB​T,M(t)=⟨r(t)2⟩.

This is the weakest stable form of the result: it fixes no initial condition, no sign convention on the roots, and no regime (inertial or overdamped), and every later statement about the MSD of a trapped Brownian particle is a consequence of it.

Milestone level — the pathwise identity

For each realization, with S=r2S = r^2S=r2,

m2S¨+ζ2S˙+k S=m r˙2+r⋅f,\tfrac{m}{2} \ddot{S} + \tfrac{\zeta}{2} \dot{S} + k\, S = m\, \dot{r}^2 + r \cdot f ,2m​S¨+2ζ​S˙+kS=mr˙2+r⋅f,

which is Newton's equation contracted with rrr and rewritten using r⋅r˙=12S˙r \cdot \dot r = \tfrac12 \dot Sr⋅r˙=21​S˙ and r⋅r¨=12S¨−r˙2r \cdot \ddot r = \tfrac12 \ddot S - \dot r^2r⋅r¨=21​S¨−r˙2.

Milestone level — the explicit solution

With λ±\lambda_\pmλ±​ the two distinct roots of mλ2+ζλ+2k=0m\lambda^2 + \zeta\lambda + 2k = 0mλ2+ζλ+2k=0,

M(t)=d kBTk[1+λ−eλ+t−λ+eλ−tλ+−λ−]M(t) = \frac{d\,k_B T}{k} \left[ 1 + \frac{\lambda_- e^{\lambda_+ t} - \lambda_+ e^{\lambda_- t}} {\lambda_+ - \lambda_-} \right]M(t)=kdkB​T​[1+λ+​−λ−​λ−​eλ+​t−λ+​eλ−​t​]

solves the goal equation with M(0)=M˙(0)=0M(0) = \dot M(0) = 0M(0)=M˙(0)=0, and in the inertialess (overdamped) case the solution reduces to M(t)=dkBTk(1−e−2kt/ζ)M(t) = \frac{d k_B T}{k}\left(1 - e^{-2kt/\zeta}\right)M(t)=kdkB​T​(1−e−2kt/ζ), which grows as 2d(kBT/ζ)t2 d (k_B T/\zeta) t2d(kB​T/ζ)t at short times and saturates at the equipartition plateau dkBT/kd k_B T / kdkB​T/k.

Significance

The MSD equation is what converts a measured displacement trace into physical numbers: its plateau dkBT/kd k_B T/kdkB​T/k calibrates trap stiffness, its short-time slope gives the diffusion coefficient D=kBT/ζD = k_B T/\zetaD=kB​T/ζ, and the crossover between the two identifies the relaxation time ζ/(2k)\zeta/(2k)ζ/(2k). The derivation is also the historical template for treating noisy dynamics without a theory of stochastic integrals: Langevin's move of averaging the equation multiplied by rrr is what makes the noise term drop out.

Formalizing it produces a machine-checked statement of the classical calculation together with the assumptions it actually needs, each of which is carried explicitly as a hypothesis rather than left implicit in the prose: interchange of ensemble averaging with time differentiation, integrability of the averaged quantities, decorrelation of the random force from the position, and equipartition. The pathwise identity and the solution-verification statements are elementary calculus; the substance of the mission is that the physical derivation is faithful once those hypotheses are written down.

Difficulty

The obvious route — solve the stochastic equation for r(t)r(t)r(t) and then square and average — requires a theory of stochastic integration against the random force, whose statistics the problem never specifies beyond the two averaged facts above. Langevin's derivation avoids this entirely, but the step "average the equation" hides two real assumptions: that ⟨⋅⟩\langle \cdot \rangle⟨⋅⟩ commutes with d/dtd/dtd/dt (so that ⟨S¨⟩\langle \ddot{S}\rangle⟨S¨⟩ is the second derivative of MMM), and that ⟨r⋅f⟩\langle r \cdot f \rangle⟨r⋅f⟩ vanishes at every time. Neither follows from the equation of motion; both must be hypotheses, and stating them precisely without weakening the theorem into vacuity is the formalization problem.

Formalization scope

Paths are represented in components: position, velocity, acceleration and force are families x,v,a,f:Fin d→R→Rx, v, a, f : \mathrm{Fin}\ d \to \mathbb{R} \to \mathbb{R}x,v,a,f:Fin d→R→R, and the model predicate records that vvv is the derivative of xxx, that aaa is the derivative of vvv, and that Newton's law holds at every time, so no differentiability is smuggled in. Euclidean contractions are the single helper dotSum d u w t=∑iui(t)wi(t)\mathrm{dotSum}\ d\ u\ w\ t = \sum_i u_i(t) w_i(t)dotSum d u w t=∑i​ui​(t)wi​(t), so that r2r^2r2, r⋅r˙r\cdot\dot rr⋅r˙, r˙2\dot r^2r˙2 and r⋅fr \cdot fr⋅f are all instances of one definition. Ensembles are an arbitrary probability space with the integral as average, and paths are indexed by the sample point; the averaging assumptions appear as hypotheses relating MMM and its derivatives to integrals of the pathwise quantities. Dimension ddd is arbitrary, the source's d=3d = 3d=3 being a special case.

No hypothesis of the goal is vacuous: a deterministic ensemble (one path, a Dirac measure) with f≡0f \equiv 0f≡0 and a particle at rest satisfies all of them when kBT=0k_B T = 0kB​T=0, and nondegenerate instances exist for every choice of parameters, so the statement is not satisfied only in an empty context. All statements target real-valued time and real coefficients; no positivity of mmm, ζ\zetaζ, kkk is assumed except where a milestone needs it for an asymptotic claim.

Selected references

  • P. Langevin, Sur la théorie du mouvement brownien, C. R. Acad. Sci. Paris 146 (1908), 530–533. English translation: D. S. Lemons and A. Gythiel, Paul Langevin's 1908 paper "On the Theory of Brownian Motion", American Journal of Physics 65 (1997), 1079–1081. https://doi.org/10.1119/1.18725
  • Nonequilibrium Statistical Physics, Honour School of Mathematical and Theoretical Physics Part C, Trinity Term 2018 examination paper A15282W1, Question 1.
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Mathematical Physics·Captain: lisamegawatts

Finite Reflection Positivity Methods II: Split-Gibbs Normalization and ClosureTextbook

Motivation

Reflection positivity turns a factorized weight across a reflection plane into a positive-semidefinite kernel of observables. The first mission in this series certified that finite split-weight mechanism and its two-observable chessboard inequality. A physical finite-volume Gibbs model needs one more layer before it can consume those results: its unnormalized weight must have a strictly positive partition function, normalization must preserve the split representation, and the hypotheses used for probability normalization must not be confused with those used for reflection positivity.

This mission isolates that finite algebraic layer. It does not present the results as new mathematics; its purpose is to make the interfaces and their failure modes explicit enough for later clock and XY consumers.

Setting

Let XXX be a finite half-configuration space and let a full configuration be (x,y)∈X×X(x,y)\in X\times X(x,y)∈X×X. A split weight is

W(x,y)=∑a∈Acaϕa(x)ϕa(y),W(x,y)=\sum_{a\in A}c_a\phi_a(x)\phi_a(y),W(x,y)=a∈A∑​ca​ϕa​(x)ϕa​(y),

where AAA is finite, ca∈Rc_a\in\mathbb Rca​∈R, and ϕa:X→R\phi_a:X\to\mathbb Rϕa​:X→R. Its partition function and normalized weight are

Z=∑x,y∈XW(x,y),W^(x,y)=W(x,y)Z.Z=\sum_{x,y\in X}W(x,y),\qquad \widehat W(x,y)=\frac{W(x,y)}{Z}.Z=x,y∈X∑​W(x,y),W(x,y)=ZW(x,y)​.

For observables Fi:X→RF_i:X\to\mathbb RFi​:X→R, define the reflected kernel

Kij=∑x,y∈XW^(x,y)Fi(x)Fj(y).K_{ij}=\sum_{x,y\in X}\widehat W(x,y)F_i(x)F_j(y).Kij​=x,y∈X∑​W(x,y)Fi​(x)Fj​(y).

Positive semidefiniteness means symmetry together with nonnegativity of every real quadratic form.

Formalization targets

The mission keeps two logically independent requirements visible. Nonnegative split coefficients ca≥0c_a\ge0ca​≥0 give reflection positivity through a weighted Gram factorization. Pointwise nonnegativity W(x,y)≥0W(x,y)\ge0W(x,y)≥0, together with one strictly positive value, gives Z>0Z>0Z>0 and probability normalization. Neither requirement is silently substituted for the other.

The positive targets prove:

  1. finite normalization of a nonnegative, nonzero weight;
  2. closure of split data under common half-factors;
  3. closure of split data under pointwise products;
  4. preservation of reflection positivity under division by Z>0Z>0Z>0; and
  5. the combined probability, PSD-kernel, and chessboard conclusions
Kij2≤KiiKjj.K_{ij}^{2}\le K_{ii}K_{jj}.Kij2​≤Kii​Kjj​.

Two controls freeze the boundary. The symmetric two-point matrix with diagonal 111 and off-diagonal 222 is pointwise positive and normalizes to a probability weight, but its raw and normalized delta-observable kernels are not PSD. Conversely, zero split data have nonnegative coefficients and PSD raw kernels, but Z=0Z=0Z=0 and their formally normalized weight is not a probability weight.

Significance

The result is a reusable adapter between an unnormalized finite Gibbs factorization and the previously certified reflection-positive kernel API. It prevents a later model proof from treating pointwise positivity as if it were a Gram representation, or treating reflection positivity as if it guaranteed a nonzero normalizer. The next physical consumer can therefore focus on proving an explicit nonnegative factorization of its cross-plane Boltzmann weight.

Scope

All types and sums used for normalization and kernels are finite, and all weights, coefficients, features, observables, and matrices are real. The mission proves no clock- or XY-specific Gibbs factorization, no spectral or Gaussian-domination theorem, no thermodynamic limit, and no Kosterlitz--Thouless conclusion. Those require separate missions. Physical R1R1R1 and G1G1G1 are not conclusions here.

References

  • J. Fröhlich, R. Israel, E. H. Lieb, and B. Simon, Phase transitions and reflection positivity. I. General theory and long range lattice models, Communications in Mathematical Physics 62 (1978), 1--34. https://doi.org/10.1007/BF01940327
  • Prove2Me mission Finite Reflection Positivity Methods I: Split Weights and Infrared Modes, mission db962332-7a71-4d34-a01c-e85cdee243ce.
  • LeanProofs, ReflectionPositivityInfraredBound.lean, repository snapshot dbf503b2909cc17787d40a21eb75a0c9354cc6ef: https://github.com/MonumentalSystems/LeanProofs/blob/dbf503b2909cc17787d40a21eb75a0c9354cc6ef/LeanProofs/StatMech/ReflectionPositivityInfraredBound.lean
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Markov ChainStochastic Systems·Captain: naimengye

Introduction to Stochastic Networks II: Kolmogorov's Criterion for ReversibilityTextbook

Motivation

A Markov process is reversible when, in equilibrium, transitions from xxx to yyy occur at the same average rate as transitions from yyy to xxx. Algebraically this is the detailed balance condition π(x)q(x,y)=π(y)q(y,x)\pi(x)q(x,y)=\pi(y)q(y,x)π(x)q(x,y)=π(y)q(y,x), and it is the single most useful structural property a network process can have: it replaces a global linear system by one equation per pair of states, and it hands you the equilibrium measure as a product of rate ratios rather than as the solution of anything.

The catch is that detailed balance mentions π\piπ, which is exactly what one is trying to find. Chapter 2 of Richard Serfozo's Introduction to Stochastic Networks (Springer, 1999) removes the circularity. Kolmogorov's criterion characterizes reversibility by a condition on the rates alone: around every closed path, the product of the forward rates equals the product of the backward rates. And the proof is constructive — once the criterion holds, the invariant measure is

π(x)=∏i=1nq(xi−1,xi)q(xi,xi−1)\pi(x)=\prod_{i=1}^{n}\frac{q(x_{i-1},x_i)}{q(x_i,x_{i-1})}π(x)=i=1∏n​q(xi​,xi−1​)q(xi−1​,xi​)​

along any path from a fixed origin x0x^0x0 to xxx, the criterion being precisely what makes the answer independent of the path chosen.

Setting

q(x,y)q(x,y)q(x,y) is a non-negative rate function on a state space E\mathbb EE, with the two-way communication property that q(x,y)q(x,y)q(x,y) and q(y,x)q(y,x)q(y,x) are positive together — a process failing this is visibly not reversible, since some transition would be possible but its reverse would not. A path x0,…,xnx_0,\dots,x_nx0​,…,xn​ is a sequence with q(xi−1,xi)>0q(x_{i-1},x_i)>0q(xi−1​,xi​)>0 throughout, and qqq is assumed irreducible: every state is reachable from every other along a path. Write ρ(x,y)=q(x,y)/q(y,x)\rho(x,y)=q(x,y)/q(y,x)ρ(x,y)=q(x,y)/q(y,x) for the rate ratio.

qqq is reversible when some positive π\piπ satisfies the detailed balance equations. Such a π\piπ is automatically an invariant measure, the total balance equations being the sum of the detailed ones.

Formalization targets

Goal — Theorem 2.8, Kolmogorov's criterion and the canonical measure

Three statements are equivalent:

  1. qqq is reversible;
  2. (Kolmogorov's criterion) for every closed sequence x0,…,xn=x0x_0,\dots,x_n=x_0x0​,…,xn​=x0​,
∏i=1nq(xi−1,xi)=∏i=1nq(xi,xi−1);\prod_{i=1}^{n}q(x_{i-1},x_i)=\prod_{i=1}^{n}q(x_i,x_{i-1});i=1∏n​q(xi−1​,xi​)=i=1∏n​q(xi​,xi−1​);
  1. for every path, ∏i=1nρ(xi−1,xi)\prod_{i=1}^n\rho(x_{i-1},x_i)∏i=1n​ρ(xi−1​,xi​) depends on the path only through its endpoints.

And when they hold, fixing any origin x0x^0x0 there is a positive π\piπ with π(x0)=1\pi(x^0)=1π(x0)=1 satisfying detailed balance and given at every state by the product of ratios along any path from x0x^0x0.

Supporting levels

The canonical form (2.2), that qqq is reversible with respect to π\piπ exactly when q(x,y)=γ(x,y)/π(x)q(x,y)=\gamma(x,y)/\pi(x)q(x,y)=γ(x,y)/π(x) for a symmetric non-negative γ\gammaγ; Example 2.1, the birth–death process with π(x)=∏n=1xλ(n−1)/μ(n)\pi(x)=\prod_{n=1}^{x}\lambda(n-1)/\mu(n)π(x)=∏n=1x​λ(n−1)/μ(n); Theorem 2.2, that a process whose communication graph is a tree is reversible; and Theorem 2.5, the time-reversal criterion, which identifies a stationary distribution from a candidate reversed rate function without mentioning reversibility at all.

Significance

The results themselves. Kolmogorov's criterion is the working test. It is how one checks that a birth–death process, a random walk on a tree, a reversible Jackson network or a Whittle network with reversible routing is reversible, and it is a finite check on cycles rather than a search for an unknown measure. The ratio form (iii) is what gets used in practice: it says the product of ratios along a path is a well-defined function of the endpoints, which is exactly what licenses defining π\piπ by that product.

Theorem 2.2 is the structural special case with no computation at all — a tree has no cycles, so the criterion is vacuous and reversibility is automatic. Theorem 2.5 points in a different direction: it identifies a stationary distribution from a guess at the time-reversed rates, and it is the tool Serfozo uses later to prove the Whittle equilibrium theorem a second way and to establish that departure processes from networks are Poisson.

Formalizing them. Mathlib has no reversibility theory for Markov processes: no detailed balance, no Kolmogorov criterion, no time reversal of a rate function. It has SimpleGraph.IsTree, which the tree item uses, and nothing else that bears on this chapter. The whole apparatus is contributed here.

Difficulty

The goal is a genuine equivalence with a constructive core, and the three implications are of quite different character.

(i) ⇒\Rightarrow⇒ (ii) is the easy one: multiply the detailed balance equations around the closed path and cancel the π\piπ's, which is legitimate because the π\piπ values are positive. Note the criterion is asserted for arbitrary closed sequences, not only for paths; the two-way property is what makes both sides vanish together when some rate is zero.

(ii) ⇔\Leftrightarrow⇔ (iii) is a cycle-splicing argument: two paths with the same endpoints concatenate, one reversed, into a closed path, and the criterion says its forward and backward products agree, which is the equality of ratio products.

(ii) ⇒\Rightarrow⇒ (i) is where the construction lives. Fix an origin x0x^0x0; irreducibility gives a path to every state; define π\piπ by the ratio product; (iii) makes it well defined; and then detailed balance at an edge follows by extending a path by that edge. Serfozo's Remark 2.9 gives the same construction as a recursion over the sets En\mathbb E_nEn​ of states reachable in nnn steps, which may be the easier route to organize.

The birth–death item is a telescoping recursion, π(x+1)μ(x+1)=π(x)λ(x)\pi(x+1)\mu(x+1)=\pi(x)\lambda(x)π(x+1)μ(x+1)=π(x)λ(x), and the observation that the two families of detailed balance equations — for y=x+1y=x+1y=x+1 and for y=x−1y=x-1y=x−1 — are the same family. Theorem 2.2 is a cut argument: removing an edge of a tree splits the state space into two pieces joined by that edge alone, so the flow balance across the cut is the detailed balance equation for that edge. Theorem 2.5 is two lines of rearrangement once the sums are known to converge.

Formalization scope

The state space is an arbitrary type and qqq is an arbitrary non-negative real rate function; nothing here needs a process, a measure space or even countability, because reversibility as Serfozo defines it "applies to any nonnegative rates or probabilities as an algebraic property, not necessarily associated with a stochastic process". The same statements therefore cover discrete-time chains with qqq read as transition probabilities, which is what the book points out.

Paths are functions {0,…,n}→E\{0,\dots,n\}\to\mathbb E{0,…,n}→E with positive consecutive rates. A path of length zero is a single state and its ratio product is the empty product 111, which is consistent with π(x0)=1\pi(x^0)=1π(x0)=1.

Kolmogorov's criterion is stated for arbitrary closed sequences, exactly as the book states it, not only for closed paths. Under two-way communication the two readings agree — if one rate in the sequence vanishes then so does its reverse and both products are zero — but the book's form is the one that is directly checkable.

The canonical measure is not defined by a choice function. Instead the conclusion asserts the existence of a positive π\piπ with π(x0)=1\pi(x^0)=1π(x0)=1 satisfying detailed balance and agreeing with the ratio product along every path from the origin. That is the content of (2.9) without needing to pick a path for each state.

Theorem 2.2 is stated for a finite state space. Serfozo assumes the process is ergodic, and the cut-flow argument then sums the balance equations over one side of the cut; on an infinite state space that summation needs an integrability condition that the book leaves implicit in "ergodic". Finiteness makes the rearrangement unconditional and the statement clearly true; the general case is listed under contributions.

Theorem 2.5 is stated as the conclusion that π\piπ satisfies the balance equations, with explicit summability hypotheses for the three families of sums involved. That π\piπ is the stationary distribution additionally requires it to be normalized and the process to be ergodic, neither of which is part of the algebraic content.

Contributions welcome beyond the listed items: Theorem 2.4, the characterization of reversibility by invariance of the finite-dimensional distributions under time reversal; Remark 2.9's recursive construction of the canonical measure; Theorem 2.22 on reversible network processes with batch movements; Theorem 2.31 and the partition-reversible processes of Sections 2.8 and 2.9; and the reversibility criteria for Jackson and Whittle networks in Examples 2.24 and 2.25.

Selected references

  • Richard Serfozo, Introduction to Stochastic Networks, Applications of Mathematics 44, Springer, 1999, chapter 2, pp. 44–51; (2.1), (2.2), Example 2.1, Theorems 2.2, 2.5 and 2.8, Remark 2.9. DOI 10.1007/978-1-4612-1482-3
  • A. N. Kolmogoroff, Zur Theorie der Markoffschen Ketten, Mathematische Annalen 112 (1936), 155–160. DOI 10.1007/BF01565412
  • F. P. Kelly, Reversibility and Stochastic Networks, Wiley, 1979; reissued Cambridge University Press, 2011, chapter 1. DOI 10.1017/CBO9781139226424
  • P. Whittle, Systems in Stochastic Equilibrium, Wiley, 1986, chapters 1 and 10.
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AnalysisStochastic Systems·Captain: naimengye

Probability Theory and Examples V: Blumenthal's 0-1 Law and the Local Behaviour of Brownian PathsTextbook

Motivation

A Brownian path is continuous, and that is essentially all it is. It has no derivative anywhere, it crosses zero infinitely often in every interval (0,ϵ)(0,\epsilon)(0,ϵ), and it becomes positive and negative immediately after time zero. None of this is visible from the finite-dimensional distributions; it is a statement about the germ of the path at a point, and the tool that unlocks it is a zero-one law.

Chapter 7 of Rick Durrett's Probability: Theory and Examples (Version 5, 2019) develops that tool. The natural filtration Fs0=σ(Br:r≤s)\mathcal F^{0}_{s}=\sigma(B_r:r\le s)Fs0​=σ(Br​:r≤s) is enlarged to Fs+=⋂t>sFt0\mathcal F^{+}_{s}=\bigcap_{t>s}\mathcal F^{0}_{t}Fs+​=⋂t>s​Ft0​, which allows "an infinitesimal peek at the future" — a quantity like lim sup⁡t↓s(Bt−Bs)/f(t−s)\limsup_{t\downarrow s}(B_t-B_s)/f(t-s)limsupt↓s​(Bt​−Bs​)/f(t−s) is Fs+\mathcal F^{+}_{s}Fs+​-measurable but not Fs0\mathcal F^{0}_{s}Fs0​-measurable. Blumenthal's 0-1 law (Theorem 7.2.3) says that at s=0s=0s=0 this enlargement buys nothing probabilistically: the germ σ\sigmaσ-field F0+\mathcal F^{+}_{0}F0+​ is trivial.

Everything local follows. If the path had any chance of staying non-positive on some interval (0,ϵ)(0,\epsilon)(0,ϵ), that would be a germ event of probability at least 1/21/21/2 by symmetry, so it has probability one — and the path enters (0,∞)(0,\infty)(0,∞) immediately. Continuity then forces it to return to zero immediately as well. Combined with the time inversion Xt=tB(1/t)X_t=tB(1/t)Xt​=tB(1/t), which turns the germ at 000 into the tail at ∞\infty∞, the same law gives lim sup⁡t→∞Bt/t=∞\limsup_{t\to\infty}B_t/\sqrt t=\inftylimsupt→∞​Bt​/t​=∞ and the recurrence of one-dimensional Brownian motion.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and B:R≥0→Ω→RB:\mathbb R_{\ge0}\to\Omega\to\mathbb RB:R≥0​→Ω→R a Brownian motion: its finite-dimensional laws are centred Gaussian with covariance cov⁡(Bs,Bt)=s∧t\operatorname{cov}(B_s,B_t)=s\wedge tcov(Bs​,Bt​)=s∧t, and almost every path is continuous. In particular B0=0B_0=0B0​=0 almost surely, so this is Durrett's P0\mathbb P_0P0​.

Three σ\sigmaσ-fields organize the chapter:

Ft0=σ(Bs:s≤t),F0+=⋂t>0Ft0,T=⋂t≥0σ(Bs:s≥t).\mathcal F^{0}_{t}=\sigma(B_s:s\le t),\qquad \mathcal F^{+}_{0}=\bigcap_{t>0}\mathcal F^{0}_{t},\qquad \mathcal T=\bigcap_{t\ge0}\sigma(B_s:s\ge t).Ft0​=σ(Bs​:s≤t),F0+​=t>0⋂​Ft0​,T=t≥0⋂​σ(Bs​:s≥t).

The first is the past, the second the germ at time zero, the third the tail at infinity.

A path fff is Lipschitz at the point sss with constant CCC when ∣f(t)−f(s)∣≤C∣t−s∣|f(t)-f(s)|\le C|t-s|∣f(t)−f(s)∣≤C∣t−s∣ for all ttt within some positive distance of sss. A path differentiable at sss is Lipschitz at sss, so failing this at every point and for every constant is a strong form of nowhere differentiability.

Formalization targets

Goal — Theorem 7.2.3, Blumenthal's 0-1 law

A∈F0+⟹P(A)∈{0,1}.A\in\mathcal F^{+}_{0}\quad\Longrightarrow\quad \mathbb P(A)\in\{0,1\}.A∈F0+​⟹P(A)∈{0,1}.

In words: the germ σ\sigmaσ-field is trivial. Nothing about the path in an arbitrarily short initial interval is genuinely random.

Supporting levels

Theorem 7.1.5, that Brownian paths are Hölder continuous of every exponent γ<1/2\gamma<1/2γ<1/2 on every bounded interval; Theorem 7.1.6, that with probability one they are not Lipschitz at any point, hence nowhere differentiable — the Paley–Wiener–Zygmund theorem in the proof of Dvoretsky, Erdős and Kakutani; Theorem 7.2.4, that the path enters (0,∞)(0,\infty)(0,∞) immediately; Theorem 7.2.5, that its zero set accumulates at 000; and Theorem 7.2.8, that lim sup⁡t→∞Bt/t=+∞\limsup_{t\to\infty}B_t/\sqrt t=+\inftylimsupt→∞​Bt​/t​=+∞ and lim inf⁡t→∞Bt/t=−∞\liminf_{t\to\infty}B_t/\sqrt t=-\inftyliminft→∞​Bt​/t​=−∞.

Significance

The results themselves. Blumenthal's law is the gateway to every local path property of Brownian motion, and Durrett uses it immediately for exactly that. Theorems 7.2.4 and 7.2.5 together say the path oscillates across zero infinitely often in every initial interval — the reason the zero set is an uncountable closed set of Lebesgue measure zero, and the reason the "first return to zero" is not a useful notion at time 000. Theorem 7.2.8 is the same law pushed to t→∞t\to\inftyt→∞ by time inversion, and it is what makes one-dimensional Brownian motion recurrent (Theorem 7.2.9).

The Hölder pair is the sharp description of path regularity. Exponent γ<1/2\gamma<1/2γ<1/2 always works, γ>1/2\gamma>1/2γ>1/2 never does, and the borderline 1/21/21/2 is subtle: P(t∈H1/2)=0\mathbb P(t\in H_{1/2})=0P(t∈H1/2​)=0 for each fixed ttt, but Davis (1983) showed P(H1/2≠∅)=1\mathbb P(H_{1/2}\ne\emptyset)=1P(H1/2​=∅)=1. Nowhere differentiability is the historical headline — Paley, Wiener and Zygmund (1933) — and the proof given here is a short covering argument rather than a series construction.

Formalizing them. Mathlib has the object but almost none of the theory. It defines IsPreBrownianReal and IsBrownianReal, proves that a centred Gaussian process with covariance s∧ts\wedge ts∧t is pre-Brownian, and supplies the invariances — negation, scaling t↦c−1/2B(ct)t\mapsto c^{-1/2}B(ct)t↦c−1/2B(ct), the shift t↦B(t0+t)−B(t0)t\mapsto B(t_0+t)-B(t_0)t↦B(t0​+t)−B(t0​), and the time inversion t↦tB(1/t)t\mapsto tB(1/t)t↦tB(1/t) — together with the weak Markov property IsPreBrownianReal.indepFun_shift. It does not have the germ or tail σ\sigmaσ-fields, Blumenthal's law, the strong Markov property, any path-regularity result, or the Kolmogorov–Chentsov continuity theorem: Probability/Process/Kolmogorov.lean defines IsKolmogorovProcess, the hypothesis, and stops there. So this mission supplies the σ\sigmaσ-fields and then everything Durrett proves with them.

Difficulty

The goal reduces to Durrett's Theorem 7.2.2, that E(Z∣Fs+)=E(Z∣Fs0)\mathbb E(Z\mid\mathcal F^{+}_{s})=\mathbb E(Z\mid\mathcal F^{0}_{s})E(Z∣Fs+​)=E(Z∣Fs0​) for bounded path-measurable ZZZ; at s=0s=0s=0, F00=σ(B0)\mathcal F^{0}_{0}=\sigma(B_0)F00​=σ(B0​) is trivial because B0=0B_0=0B0​=0 almost surely, so 1A=E(1A∣F0+)=P(A)\mathbf 1_A=\mathbb E(\mathbf 1_A\mid\mathcal F^{+}_{0})=\mathbb P(A)1A​=E(1A​∣F0+​)=P(A) almost surely, and an indicator almost surely equal to a constant forces that constant to be 000 or 111. Theorem 7.2.2 itself is a monotone class argument on top of the Markov property, and the Markov property in this setting is Mathlib's indepFun_shift plus the observation that the conditional expectation of a product ∏mfm(Btm)\prod_m f_m(B_{t_m})∏m​fm​(Btm​​) over Fs+\mathcal F^{+}_{s}Fs+​ lands in Fs0\mathcal F^{0}_{s}Fs0​. Assembling that is the work.

Theorem 7.2.4 is then three lines — P0(τ≤t)≥P0(Bt>0)=1/2\mathbb P_0(\tau\le t)\ge\mathbb P_0(B_t>0)=1/2P0​(τ≤t)≥P0​(Bt​>0)=1/2 by symmetry of the Gaussian, let t↓0t\downarrow0t↓0, apply the goal — provided the event has been shown to lie in the germ field, which is where continuity of paths enters. Theorem 7.2.5 follows from 7.2.4 applied to BBB and −B-B−B together with the intermediate value theorem.

Theorem 7.1.5 needs the Kolmogorov–Chentsov continuity theorem, which has to be built: from E∣Bt−Bs∣2m=Cm∣t−s∣m\mathbb E|B_t-B_s|^{2m}=C_m|t-s|^mE∣Bt​−Bs​∣2m=Cm​∣t−s∣m one gets Hölder-γ\gammaγ control for γ<(m−1)/2m\gamma<(m-1)/2mγ<(m−1)/2m, and m→∞m\to\inftym→∞ gives every γ<1/2\gamma<1/2γ<1/2. The dyadic chaining and Borel–Cantelli step is the substance, and it is worth building as a general theorem about IsKolmogorovProcess rather than only for Brownian motion.

Theorem 7.1.6 is self-contained and short: fix CCC, let AnA_nAn​ be the event that some s∈[0,1]s\in[0,1]s∈[0,1] has ∣Bt−Bs∣≤C∣t−s∣|B_t-B_s|\le C|t-s|∣Bt​−Bs​∣≤C∣t−s∣ whenever ∣t−s∣≤3/n|t-s|\le3/n∣t−s∣≤3/n, and bound P(An)≤n P(∣B1∣≤5Cn−1/2)3≤n{10Cn−1/2(2π)−1/2}3→0\mathbb P(A_n)\le n\,\mathbb P(|B_1|\le5Cn^{-1/2})^3\le n\{10Cn^{-1/2}(2\pi)^{-1/2}\}^3\to0P(An​)≤nP(∣B1​∣≤5Cn−1/2)3≤n{10Cn−1/2(2π)−1/2}3→0; since AnA_nAn​ increases, every P(An)=0\mathbb P(A_n)=0P(An​)=0.

Theorem 7.2.8 needs the tail 0-1 law, Theorem 7.2.7, which is the goal transported through the time inversion Xt=tB(1/t)X_t=tB(1/t)Xt​=tB(1/t) — Mathlib's IsPreBrownianReal.inv — because the tail field of BBB is the germ field of XXX. With that, P0(Bn/n≥K i.o.)≥P0(B1≥K)>0\mathbb P_0(B_n/\sqrt n\ge K\ \text{i.o.})\ge\mathbb P_0(B_1\ge K)>0P0​(Bn​/n​≥K i.o.)≥P0​(B1​≥K)>0 by scaling, so the probability is one, and KKK is arbitrary.

Formalization scope

The process is Mathlib's IsBrownianReal, indexed by ℝ≥0, on an abstract probability space — not the canonical path space C[0,∞)C[0,\infty)C[0,∞) that Durrett uses. This is why the shift operators θs\theta_sθs​ and the family {Px}\{\mathbb P_x\}{Px​} do not appear: there is one measure, the process starts at 000 almost surely, and each statement is about that process. Theorem 7.2.7 as Durrett states it quantifies over all starting points and has no direct analogue here; the tail 0-1 law for the process started at 000 does, and is listed under contributions as the route to Theorem 7.2.8.

The three σ\sigmaσ-fields are built as suprema and infima in the lattice of σ\sigmaσ-algebras on Ω\OmegaΩ: pastSigma B t is the supremum of the pullbacks of the Borel field along BsB_sBs​ for s≤ts\le ts≤t, and germSigma B, tailSigma B are the corresponding infima. The goal carries the hypothesis that each BtB_tBt​ is measurable, not merely almost-everywhere measurable, which is what IsPreBrownianReal gives and what puts these σ\sigmaσ-fields below the ambient one; the canonical construction satisfies it, and without it "P(A)\mathbb P(A)P(A)" for a germ event would be an outer measure.

Hölder continuity is stated locally — for almost every path, every TTT admits a constant — since global Hölder continuity on [0,∞)[0,\infty)[0,∞) is false. The order of quantifiers puts the null set first, so a single path works for every TTT at once.

The hitting statements avoid an infimum over a possibly empty set. "τ=0\tau=0τ=0 almost surely" is written as: almost surely, for every ϵ>0\epsilon>0ϵ>0 there is t∈(0,ϵ)t\in(0,\epsilon)t∈(0,ϵ) with Bt>0B_t>0Bt​>0; and "T0=0T_0=0T0​=0 almost surely" as the same with Bt=0B_t=0Bt​=0. These are equivalent to Durrett's statements and say what the infimum is there to say. Similarly Theorem 7.2.8 is written with ∃ᶠ … in atTop rather than as an extended-real lim sup⁡\limsuplimsup, which is what "lim sup⁡=+∞\limsup=+\inftylimsup=+∞" means and avoids a coercion.

LipschitzAtPoint f s C is "there is a scale δ>0\delta>0δ>0 on which ∣f(t)−f(s)∣≤C∣t−s∣|f(t)-f(s)|\le C|t-s|∣f(t)−f(s)∣≤C∣t−s∣". Its negation for every sss and every CCC is Theorem 7.1.6, and it has content in both directions: the identity path is Lipschitz at every point with C=1C=1C=1, while t↦tt\mapsto\sqrt tt↦t​ is not Lipschitz at 000 with C=1C=1C=1 — both checked in Lean before publishing.

Existence is not part of this mission. Mathlib proves nothing of the form "a Brownian motion exists", and nothing here needs it: every item takes a Brownian motion as a hypothesis. That the hypothesis is satisfiable is a theorem — Durrett's 7.1.1, via Kolmogorov extension and the continuity theorem — and it is listed under contributions, where it belongs, since building it is a project of its own.

Contributions welcome beyond the listed items: Kolmogorov–Chentsov as a general statement about IsKolmogorovProcess; Theorem 7.1.1, the existence of Brownian motion; Theorem 7.2.2 in full, for every sss; the tail 0-1 law and Theorem 7.2.9, recurrence; the strong Markov property and the reflection principle of section 7.3; and Exercise 7.1.5, that no path is Hölder of any exponent γ>1/2\gamma>1/2γ>1/2.

Selected references

  • Rick Durrett, Probability: Theory and Examples, Version 5 (11 January 2019), chapter 7, sections 7.1 and 7.2 (pp. 353–365); Theorems 7.1.5, 7.1.6, 7.2.3, 7.2.4, 7.2.5, 7.2.8. Published as the 5th edition, Cambridge University Press, 2019, DOI 10.1017/9781108591034
  • R. M. Blumenthal, An extended Markov property, Transactions of the American Mathematical Society 85 (1957), 52–72. DOI 10.1090/S0002-9947-1957-0088102-2
  • R. E. A. C. Paley, N. Wiener and A. Zygmund, Notes on random functions, Mathematische Zeitschrift 37 (1933), 647–668. DOI 10.1007/BF01474606
  • A. Dvoretzky, P. Erdős and S. Kakutani, Nonincrease everywhere of the Brownian motion process, Proceedings of the Fourth Berkeley Symposium II (1961), 103–116.
  • N. Wiener, Differential space, Journal of Mathematics and Physics 2 (1923), 131–174. DOI 10.1002/sapm192321131
  • I. Karatzas and S. E. Shreve, Brownian Motion and Stochastic Calculus, 2nd ed., Springer, 1991, chapter 2. DOI 10.1007/978-1-4612-0949-2
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Markov ChainStochastic Systems·Captain: naimengye

Probability Theory and Examples III: The Markov Chain Convergence TheoremTextbook

Motivation

A Markov chain forgets. Run it long enough and the distribution of its position stops depending on where it started — that is the intuition behind shuffling a deck, behind Markov chain Monte Carlo, behind PageRank, and behind the stationary analyses of every queueing model. Chapter 5 of Rick Durrett's Probability: Theory and Examples (Version 5, 2019) makes it a theorem, and identifies exactly what can go wrong.

Two things can. The chain may fail to reach parts of the state space, and the answer is irreducibility. Or it may reach them only on a lattice of times — a chain alternating between two halves of its state space never forgets whether the clock is even or odd — and the answer is aperiodicity. Theorem 5.6.6 says that is the complete list: an irreducible, aperiodic chain with a stationary distribution has pn(x,y)→π(y)p^n(x,y)\to\pi(y)pn(x,y)→π(y), for every pair of states, whatever the starting point.

Setting

Let SSS be a countable state space and p(x,y)p(x,y)p(x,y) a transition probability: non-negative, with each row summing to one. The nnn-step transition probabilities are the matrix powers, p0(x,y)=δxyp^0(x,y)=\delta_{xy}p0(x,y)=δxy​ and pn+1(x,y)=∑zp(x,z)pn(z,y)p^{n+1}(x,y)=\sum_z p(x,z)p^n(z,y)pn+1(x,y)=∑z​p(x,z)pn(z,y).

Hitting is described by the first-passage probabilities fn(x,y)=Px(Ty=n)f^n(x,y)=\mathbb{P}_x(T_y=n)fn(x,y)=Px​(Ty​=n), given by f1(x,y)=p(x,y)f^1(x,y)=p(x,y)f1(x,y)=p(x,y) and fn+1(x,y)=∑z≠yp(x,z)fn(z,y)f^{n+1}(x,y)=\sum_{z\ne y}p(x,z)f^n(z,y)fn+1(x,y)=∑z=y​p(x,z)fn(z,y) — the chain moves once and then reaches yyy for the first time, having avoided it meanwhile. Summing them gives

ρxy=Px(Ty<∞)=∑n≥1fn(x,y),EyTy=∑n≥1n fn(y,y).\rho_{xy}=\mathbb{P}_x(T_y<\infty)=\sum_{n\ge1}f^n(x,y),\qquad \mathbb{E}_yT_y=\sum_{n\ge1}n\,f^n(y,y).ρxy​=Px​(Ty​<∞)=n≥1∑​fn(x,y),Ey​Ty​=n≥1∑​nfn(y,y).

A state is recurrent when ρyy=1\rho_{yy}=1ρyy​=1, the chain is irreducible when ρxy>0\rho_{xy}>0ρxy​>0 for all x,yx,yx,y, and a state xxx is aperiodic when the greatest common divisor of Ix={n≥1:pn(x,x)>0}I_x=\{n\ge1:p^n(x,x)>0\}Ix​={n≥1:pn(x,x)>0} is 111. A stationary distribution is a probability vector π\piπ with ∑xπ(x)p(x,y)=π(y)\sum_x\pi(x)p(x,y)=\pi(y)∑x​π(x)p(x,y)=π(y).

Formalization targets

Goal — Theorem 5.6.6, the convergence theorem

p irreducible, aperiodic, with stationary distribution π⟹pn(x,y)⟶π(y)  for all x,y.p \text{ irreducible},\ \text{aperiodic},\ \text{with stationary distribution } \pi \quad\Longrightarrow\quad p^n(x,y)\longrightarrow\pi(y)\ \text{ for all } x,y .p irreducible, aperiodic, with stationary distribution π⟹pn(x,y)⟶π(y)  for all x,y.

The goal asserts pointwise convergence of the transition probabilities, not convergence in total variation and not a rate; those are strengthenings, and stating the weakest useful form is what keeps the theorem stable.

Supporting levels

Theorem 5.3.1, that a state is recurrent exactly when ∑npn(y,y)\sum_n p^n(y,y)∑n​pn(y,y) diverges — the bridge between the hitting picture and the matrix picture; Theorem 5.3.2, that recurrence is contagious; Theorem 5.5.10, that every state in the support of a stationary distribution is recurrent; and Theorem 5.5.11, that for an irreducible chain with a stationary distribution π(x)=1/ExTx\pi(x)=1/\mathbb{E}_xT_xπ(x)=1/Ex​Tx​.

Significance

The result itself. Theorem 5.6.6 is what licenses reading a stationary distribution as a long-run frequency. Without it, π\piπ is merely a fixed point of a linear map; with it, π(y)\pi(y)π(y) is the limiting probability of being at yyy, from any start. Theorem 5.5.11 then gives the quantity a second, purely local meaning — π(x)\pi(x)π(x) is the reciprocal of the mean return time to xxx — which is the identity behind every renewal-reward computation in applied probability and behind the "expected time between visits" estimates that Monte Carlo methods rely on. The two necessary hypotheses are sharp: a periodic chain has pn(x,y)p^n(x,y)pn(x,y) oscillating rather than converging, and Durrett's Theorem 5.7.2 gives the corrected statement in that case.

Formalizing it. Mathlib has no countable-state Markov chain theory. It has ProbabilityTheory.Kernel and an Irreducible notion for kernels, but nothing about recurrence, transience, first-passage decompositions, stationary measures or the convergence theorem, and nothing that specializes to a transition matrix on a countable set. The mission therefore contributes the whole apparatus of sections 5.3, 5.5 and 5.6 — the nnn-step and first-passage probabilities, ρxy\rho_{xy}ρxy​, the mean return time, recurrence, irreducibility, aperiodicity and stationarity — together with the results that make it usable.

Difficulty

The usual proof of the goal is a coupling argument, and it is short but not obvious: run two independent copies of the chain, one from xxx and one from π\piπ, on the product space S×SS\times SS×S with transition probability pˉ((x1,x2),(y1,y2))=p(x1,y1)p(x2,y2)\bar p((x_1,x_2),(y_1,y_2))=p(x_1,y_1)p(x_2,y_2)pˉ​((x1​,x2​),(y1​,y2​))=p(x1​,y1​)p(x2​,y2​); aperiodicity plus irreducibility make the product chain irreducible, π×π\pi\times\piπ×π is stationary for it, so it is recurrent and the two copies meet almost surely; after they meet they can be exchanged. Each step of that is a separate obligation, and the one that consumes aperiodicity is the irreducibility of the product chain — for a periodic chain it fails, which is exactly why the theorem does.

The number-theoretic ingredient is worth flagging: irreducibility of the product needs that Ix={n:pn(x,x)>0}I_x=\{n:p^n(x,x)>0\}Ix​={n:pn(x,x)>0}, being closed under addition with gcd⁡1\gcd 1gcd1, contains every sufficiently large integer. That is the numerical semigroup fact, and it is where aperiodicity is actually used.

Formalization scope

The state space is any countable type with decidable equality, and the transition probability is a plain function S×S→RS\times S\to\mathbb{R}S×S→R constrained by IsTransition: non-negative entries, summable rows, rows summing to one. Sums over the state space are unconditional sums, so no finiteness is assumed anywhere.

The chain's law is not constructed. Every quantity here — pnp^npn, fnf^nfn, ρxy\rho_{xy}ρxy​, EyTy\mathbb{E}_yT_yEy​Ty​ — is defined by an explicit recursion on the transition matrix, not as an expectation against a measure on path space. This is a deliberate choice: building the path measure is a substantial project of its own, and none of the statements in these sections need it. The recursions are the standard ones and they are the definitions the book's own computations use. The cost is that probabilistic statements about paths, such as Theorem 5.6.1 on the almost-sure limit of the visit counts Nn(y)/nN_n(y)/nNn​(y)/n, cannot be phrased in this language and are not part of the mission.

Conventions: p0p^0p0 is the identity matrix; fnf^nfn vanishes at n=0n=0n=0; ρxy\rho_{xy}ρxy​ and EyTy\mathbb{E}_yT_yEy​Ty​ are unconditional sums over n≥1n\ge1n≥1, so an infinite mean return time appears as a non-summable series rather than as an extended real. Theorem 5.5.11 is therefore stated as summability together with π(x)⋅ExTx=1\pi(x)\cdot\mathbb{E}_xT_x=1π(x)⋅Ex​Tx​=1, which asserts finiteness of the mean return time rather than silently relying on a division convention.

Aperiodicity is "the only natural number dividing every element of IxI_xIx​ is 111", which is gcd⁡Ix=1\gcd I_x=1gcdIx​=1 written without needing a gcd of a set; it is false when IxI_xIx​ is empty, which is correct, since the period of such a state is undefined.

The goal is not vacuous: the hypotheses are satisfiable by any strictly positive transition matrix on a finite set.

Contributions welcome beyond the listed items: Theorem 5.3.3 on finite closed sets; the decomposition theorem 5.3.5; existence of a stationary measure from a recurrent state (5.5.7) and its uniqueness (5.5.9); the equivalence of positive recurrence and the existence of a stationary distribution (5.5.12); Theorem 5.7.2 for the periodic case; and the path-level results of section 5.6, which need the chain's law on path space.

Selected references

  • Rick Durrett, Probability: Theory and Examples, Version 5 (11 January 2019), chapter 5, sections 5.3, 5.5 and 5.6 (pp. 281–320); Theorems 5.3.1, 5.3.2, 5.5.10, 5.5.11, 5.6.6. Published as the 5th edition, Cambridge University Press, 2019, DOI 10.1017/9781108591034
  • J. R. Norris, Markov Chains, Cambridge University Press, 1998, chapter 1. DOI 10.1017/CBO9780511810633
  • D. A. Levin and Y. Peres, Markov Chains and Mixing Times, 2nd ed., American Mathematical Society, 2017. DOI 10.1090/mbk/107
  • W. Doeblin, Exposé de la théorie des chaînes simples constantes de Markoff à un nombre fini d'états, Revue Mathématique de l'Union Interbalkanique 2 (1938), 77–105.
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Stochastic Networks V: Random Access and the Critical Rate of Backoff SchemesTextbook

Motivation

When many stations share one broadcast channel, something has to decide who transmits. A token passed around the stations works when there are few of them and none is silent for long, but it scales badly and breaks if the token is lost. The alternative is to let stations transmit whenever they like and use randomness to recover from the resulting collisions. That is the design of ALOHA, built in the 1970s to connect terminals across the Hawaiian islands, and of Ethernet, and of essentially every contention-based access protocol since.

Chapter 5 of Frank Kelly and Elena Yudovina's Stochastic Networks (Cambridge University Press, 2014) asks what such protocols can achieve, and the answers are largely negative. ALOHA with a fixed retransmission probability jams: with probability one there is a finite random time after which every slot contains a collision and no packet ever succeeds again, for every positive arrival rate. Ethernet's binary exponential backoff does better, but only just: it has a positive critical arrival rate, above which only finitely many packets are ever transmitted, and it is still not positive recurrent at rates where it does transmit infinitely many. The chapter's general statement is the one this mission targets: any backoff slower than exponential jams at every positive arrival rate.

Setting

Time is slotted, and a transmission attempt occupies exactly one slot. New packets arrive in a Poisson stream of rate ν\nuν, so the number arriving in a slot is Poisson with mean ν\nuν. A slot in which exactly one station transmits carries its packet successfully; a slot in which two or more transmit is a collision and carries nothing.

In an acknowledgement-based scheme a station learns nothing about the channel except whether its own transmissions succeeded. A packet arriving in slot ttt attempts transmission in slots t+x0,t+x1,…t+x_0, t+x_1, \dotst+x0​,t+x1​,… with 1=x0<x1<⋯1 = x_0 < x_1 < \cdots1=x0​<x1​<⋯, the sequence chosen independently for each packet, and

h(x)=P(x∈X),h(1)=1h(x) = \mathbb{P}(x \in X), \qquad h(1) = 1h(x)=P(x∈X),h(1)=1

is the retransmission function. For ALOHA, h(x)=fh(x) = fh(x)=f for every x>1x > 1x>1; for Ethernet's binary exponential backoff, ∑r≤th(r)∼log⁡2t\sum_{r \le t} h(r) \sim \log_2 t∑r≤t​h(r)∼log2​t.

Now imagine the channel externally jammed from time 000, so that every retransmission actually occurs. The attempts in slot ttt are then Poisson with mean ν∑r=1th(r)\nu\sum_{r=1}^{t}h(r)ν∑r=1t​h(r), and the probability that fewer than two attempts are made in slot ttt is

Pt=(1+ν∑r=1th(r))exp⁡(−ν∑r=1th(r)).P_t=\Bigl(1+\nu\sum_{r=1}^{t}h(r)\Bigr)\exp\Bigl(-\nu\sum_{r=1}^{t}h(r)\Bigr).Pt​=(1+νr=1∑t​h(r))exp(−νr=1∑t​h(r)).

The expected number of such slots is H(ν)=∑t≥1PtH(\nu)=\sum_{t\ge1}P_tH(ν)=∑t≥1​Pt​, which is decreasing in ν\nuν, and the critical rate is

νc=inf⁡{ν:H(ν)<∞}.\nu_c=\inf\{\nu : H(\nu)<\infty\}.νc​=inf{ν:H(ν)<∞}.

Theorem 5.11 of the book says νc\nu_cνc​ deserves its name: below it infinitely many packets are transmitted with probability one, above it only finitely many.

Formalization targets

Goal — condition (5.7): slower-than-exponential backoff has νc=0\nu_c=0νc​=0

1log⁡t∑x=1th(x)⟶∞⟹H(ν)=∑t≥1Pt<∞  for every ν>0.\frac{1}{\log t}\sum_{x=1}^{t}h(x)\longrightarrow\infty \quad\Longrightarrow\quad H(\nu)=\sum_{t\ge1}P_t<\infty \ \text{ for every } \nu>0 .logt1​x=1∑t​h(x)⟶∞⟹H(ν)=t≥1∑​Pt​<∞  for every ν>0.

Since H(ν)<∞H(\nu)<\inftyH(ν)<∞ for every positive ν\nuν, the critical rate is νc=0\nu_c=0νc​=0, and by Theorem 5.11 the expected number of successful transmissions is finite at every positive arrival rate. The goal fixes no constant and no rate: it says only that the dividing line between "jams always" and "has a positive capacity" sits at logarithmic growth of ∑x≤th(x)\sum_{x\le t}h(x)∑x≤t​h(x), which is exponential growth of the backoff.

Supporting levels

The ALOHA drift calculation of section 5.1 and its consequence that the drift is positive once the backlog is large enough; the summability ∑np(n)<∞\sum_n p(n)<\infty∑n​p(n)<∞ that combines with Borel–Cantelli to give Proposition 5.3; the monotonicity of PtP_tPt​ in ν\nuν; the opposite extreme, that a scheme with ∑xh(x)<∞\sum_x h(x)<\infty∑x​h(x)<∞ — one that gives up on a packet after finitely many attempts — has νc=∞\nu_c=\inftyνc​=∞; that ALOHA's own retransmission function satisfies condition (5.7); and the bound of Remark 5.14, that a positive recurrent acknowledgement-based scheme needs ν≤e−ν\nu\le e^{-\nu}ν≤e−ν and hence ν<0.5672\nu<0.5672ν<0.5672, which is strictly below Ethernet's νc=log⁡2\nu_c=\log 2νc​=log2.

Significance

The result itself. Condition (5.7) is the chapter's structural statement about random access, and it is a sharp one. Any retransmission rule under which a packet keeps trying at a rate that does not decay fast enough — a fixed probability, a polynomially growing backoff, anything short of exponential — has critical rate zero: the channel jams at every positive load. Exponential backoff is not a tuning choice, it is the minimum that makes the protocol work at all, and the log⁡b\log blogb formula for a backoff by factor bbb (Exercise 5.7) then says how much capacity each choice of bbb buys. The gap recorded in Remark 5.14 is the other half of the picture: even above the threshold, "infinitely many packets get through" is much weaker than "the backlog is stable", and between 0.5670.5670.567 and log⁡2≈0.693\log 2 \approx 0.693log2≈0.693 Ethernet does the first and provably not the second.

Formalizing it. None of this is open; the analysis is due to Kelly and MacPhee (1987) and Aldous (1987). What the mission contributes is a machine-checked account of the analytic core: the definitions of PtP_tPt​, H(ν)H(\nu)H(ν) and νc\nu_cνc​, the two extremes of the classification, and the ALOHA calculations. Mathlib has no protocol analysis and nothing about random access channels.

Difficulty

The obstacle is a modelling one and it is worth stating plainly rather than discovering halfway through. The chapter's headline results — Proposition 5.3 that ALOHA jams almost surely, Theorem 5.11 that νc\nu_cνc​ is the critical rate, Theorem 5.15 that geometric Ethernet is transient — are statements about sample paths of a Markov chain built on a Poisson arrival stream, and their proofs are coupling arguments comparing a system started empty with one started with a backlog. Nothing in Mathlib supports that construction, and building it is a research-scale project rather than a chapter. This mission therefore formalizes the analytic half and quotes the probabilistic half, which is the same division the book itself makes when it computes νc\nu_cνc​ for a scheme: Theorem 5.11 is proved once, and every subsequent statement about a protocol is a convergence question about ∑tPt\sum_t P_t∑t​Pt​.

Within that analytic half the difficulty is real but ordinary. The summand PtP_tPt​ is a product of a factor growing with ∑r≤th(r)\sum_{r\le t}h(r)∑r≤t​h(r) and one decaying exponentially in it, so the growth hypothesis has to be turned into a summable bound without assuming any regularity of hhh beyond non-negativity — in particular ∑r≤th(r)\sum_{r\le t}h(r)∑r≤t​h(r) need not be eventually monotone in any useful quantitative sense, only divergent faster than log⁡t\log tlogt.

Formalization scope

The retransmission function is any non-negative real sequence; the normalization h(1)=1h(1)=1h(1)=1 is not imposed, since none of the statements need it and imposing it would exclude the comparison schemes. PtP_tPt​ and the partial sums are real-valued, and "H(ν)<∞H(\nu)<\inftyH(ν)<∞" is stated as summability of the sequence rather than as a bound on an extended-real sum, so convergence is asserted rather than assumed. The goal is stated for each fixed ν>0\nu>0ν>0 separately, which is what makes νc=0\nu_c=0νc​=0; it is not stated as a claim about the infimum, because the infimum of the set {ν:H(ν)<∞}\{\nu : H(\nu)<\infty\}{ν:H(ν)<∞} adds nothing once the set is known to be all of (0,∞)(0,\infty)(0,∞).

The growth hypothesis is the book's condition (5.7) verbatim: (log⁡t)−1∑x≤th(x)→∞\bigl(\log t\bigr)^{-1}\sum_{x\le t}h(x)\to\infty(logt)−1∑x≤t​h(x)→∞. Note that at t=0t=0t=0 and t=1t=1t=1 the quotient involves log⁡t≤0\log t \le 0logt≤0 and is not meaningful; divergence to infinity is an eventual statement, so this costs nothing, but it is why the hypothesis is a limit rather than a pointwise bound.

The mission is not vacuous in either direction: the ALOHA milestone exhibits a retransmission function satisfying the hypothesis, and the ∑xh(x)<∞\sum_x h(x)<\infty∑x​h(x)<∞ milestone exhibits one that fails it as strongly as possible, with H(ν)=∞H(\nu)=\inftyH(ν)=∞ for every ν\nuν.

Contributions welcome beyond the listed items: Ethernet's ∑r≤th(r)∼log⁡2t\sum_{r\le t}h(r)\sim\log_2 t∑r≤t​h(r)∼log2​t and the resulting νc=log⁡2\nu_c=\log 2νc​=log2; the generalization νc=log⁡b\nu_c=\log bνc​=logb of Exercise 5.7; the scheme h(x)=1/(xlog⁡x)h(x)=1/(x\log x)h(x)=1/(xlogx) with νc=∞\nu_c=\inftyνc​=∞; the continuous-time halving νc=12log⁡b\nu_c=\frac12\log bνc​=21​logb of Kelly and MacPhee; and, for anyone willing to build the probabilistic layer, Proposition 5.3 and Theorem 5.11 themselves.

Selected references

  • Frank Kelly and Elena Yudovina, Stochastic Networks, Cambridge University Press, 2014, Chapter 5 (pp. 108–132); Definition 5.1, Proposition 5.3, Theorems 5.11 and 5.15, condition (5.7), Examples 5.8, 5.12 and 5.13, Remark 5.14. DOI 10.1017/cbo9781139565363
  • N. Abramson, The ALOHA system — another alternative for computer communications, AFIPS Conference Proceedings 37 (1970), 281–285. DOI 10.1145/1478462.1478502
  • F. P. Kelly and I. M. MacPhee, The number of packets transmitted by collision detect random access schemes, Annals of Probability 15 (1987), 1557–1568. DOI 10.1214/aop/1176991992
  • D. J. Aldous, Ultimate instability of exponential back-off protocol for acknowledgement-based transmission control of random access communication channels, IEEE Transactions on Information Theory 33 (1987), 219–223. DOI 10.1109/TIT.1987.1057295
  • R. M. Metcalfe and D. R. Boggs, Ethernet: distributed packet switching for local computer networks, Communications of the ACM 19 (1976), 395–404. DOI 10.1145/360248.360253
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High-Dimensional Probability II: Concentration Inequalities for Sums of Independent Random VariablesTextbook

Motivation

The central limit theorem tells us that a normalized sum of independent random variables converges in distribution to a Gaussian. For applications — bounding the failure probability of a randomized algorithm, controlling the error of a Monte Carlo estimator, proving a generalization bound in learning theory — a limiting distribution is not enough: what is needed is a single, explicit, non-asymptotic inequality that holds for every fixed sample size NNN, not merely as N→∞N \to \inftyN→∞. Hoeffding's inequality (Wassily Hoeffding, 1963) and Bernstein's inequality (Sergei Bernstein, 1920s–1940s, in the form used here due to Vadim Bennett and later authors) are the two archetypal answers: both give an explicit Gaussian-type tail bound for a weighted sum of independent random variables, valid for every NNN, with all constants made explicit. They are the workhorses behind concentration of measure, high-dimensional statistics, and the non-asymptotic analysis of randomized algorithms; a textbook trying to reach the Johnson–Lindenstrauss lemma, random matrix norms, or the restricted isometry property has to pass through this chapter first, because every one of those results is itself an application of a weighted-sum concentration inequality to a specific choice of random variables.

The central limit theorem's own error term is the obstruction that direct concentration inequalities are built to avoid: the Berry–Esseen theorem (Andrew C. Berry, 1941; Carl-Gustav Esseen, 1942) bounds the normal approximation's error at order 1/N1/\sqrt N1/N​, which is too slow to recover a genuinely exponential tail bound for finite NNN. Hoeffding's and Bernstein's inequalities are proved instead by a direct argument — bounding the moment generating function of the sum and optimizing a Markov/Chernoff exponential tilt — that never invokes the central limit theorem or its error term at all.

The sub-gaussian and sub-exponential norms

Fix a probability space (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P). For a real random variable XXX on (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P), define its sub-gaussian norm

∥X∥ψ2:=inf⁡{t>0:Eexp⁡(X2/t2) is finite and ≤2}\|X\|_{\psi_2} := \inf\{t > 0 : \mathbb E \exp(X^2/t^2) \text{ is finite and } \le 2\}∥X∥ψ2​​:=inf{t>0:Eexp(X2/t2) is finite and ≤2}

and its sub-exponential norm

∥X∥ψ1:=inf⁡{t>0:Eexp⁡(∣X∣/t) is finite and ≤2}.\|X\|_{\psi_1} := \inf\{t > 0 : \mathbb E \exp(|X|/t) \text{ is finite and } \le 2\}.∥X∥ψ1​​:=inf{t>0:Eexp(∣X∣/t) is finite and ≤2}.

In both definitions, the requirement that the exponential moment be finite (i.e. that the moment-generating integrand be integrable), and not merely satisfy "≤2\le 2≤2" as a bare inequality, is essential: without it a moment that is genuinely infinite for a given ttt would vacuously count as "≤2\le 2≤2" under the Bochner integral's convention that a non-integrable function integrates to 000, and every random variable — however heavy-tailed — would trivially have norm 000. XXX is called sub-gaussian (respectively sub-exponential) when this infimum is over a nonempty set, i.e. when some finite ttt makes the moment finite and at most 222. These are genuine norms (up to the identification of almost-surely-equal random variables) on the vector space of random variables for which they are finite, and they are the natural non-asymptotic yardsticks for tail heaviness: ∥X∥ψ2<∞\|X\|_{\psi_2} < \infty∥X∥ψ2​​<∞ characterizes a Gaussian-type tail P{∣X∣≥t}≤2exp⁡(−ct2/∥X∥ψ22)P\{|X| \ge t\} \le 2\exp(-ct^2/\|X\|_{\psi_2}^2)P{∣X∣≥t}≤2exp(−ct2/∥X∥ψ2​2​), while ∥X∥ψ1<∞\|X\|_{\psi_1} < \infty∥X∥ψ1​​<∞ characterizes an exponential-type tail P{∣X∣≥t}≤2exp⁡(−ct/∥X∥ψ1)P\{|X| \ge t\} \le 2\exp(-ct/\|X\|_{\psi_1})P{∣X∣≥t}≤2exp(−ct/∥X∥ψ1​​). Every bounded random variable — in particular every Bernoulli or Rademacher (symmetric Bernoulli) random variable — is sub-gaussian, and the square of a sub-gaussian random variable is sub-exponential; a genuinely sub-exponential (not sub-gaussian) example is the squared coordinate gi2g_i^2gi2​ of a standard Gaussian vector, or the exponential distribution itself.

Formalization targets

Goal — Theorem 2.8.2 (Bernstein's inequality, weighted sum). Let X1,…,XNX_1, \dots, X_NX1​,…,XN​ be independent, mean-zero, sub-exponential random variables on (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P), and let a=(a1,…,aN)∈RNa = (a_1, \dots, a_N) \in \mathbb R^Na=(a1​,…,aN​)∈RN. Then, for every t≥0t \ge 0t≥0,

P{∣∑i=1NaiXi∣≥t}  ≤  2exp⁡[−cmin⁡(t2K2∥a∥22,tK∥a∥∞)],P\Bigl\{\Bigl|\sum_{i=1}^N a_i X_i\Bigr| \ge t\Bigr\} \;\le\; 2\exp\left[-c\min\left(\frac{t^2}{K^2\|a\|_2^2}, \frac{t}{K\|a\|_\infty}\right)\right],P{​i=1∑N​ai​Xi​​≥t}≤2exp[−cmin(K2∥a∥22​t2​,K∥a∥∞​t​)],

where K=max⁡i∥Xi∥ψ1K = \max_i \|X_i\|_{\psi_1}K=maxi​∥Xi​∥ψ1​​ and c>0c > 0c>0 is an absolute constant that does not depend on NNN, the XiX_iXi​, aaa, or ttt.

The goal is deliberately the weighted and sub-exponential form, the weakest of the chapter's results that is still stable under the improvements a solver might find: it neither fixes ai≡1a_i \equiv 1ai​≡1 (the unweighted Theorem 2.8.1, a special case) nor restricts to the lighter sub-gaussian tail (Theorem 2.6.3, which follows from a strictly stronger hypothesis). Both weaker theorems, plus Hoeffding's and Chernoff's inequalities, are included as milestones because Bernstein's own proof is built directly from them.

Significance

The result itself. Bernstein's inequality is the two-tail-regime concentration bound: a sub-gaussian tail exp⁡(−ct2/(K∥a∥2)2)\exp(-ct^2/(K\|a\|_2)^2)exp(−ct2/(K∥a∥2​)2) near the mean, transitioning to a heavier sub-exponential tail exp⁡(−ct/(K∥a∥∞))\exp(-ct/(K\|a\|_\infty))exp(−ct/(K∥a∥∞​)) far from it, exactly the behavior one should expect from a mixture of light-tailed terms with one heavy-tailed outlier. It underlies the concentration of quadratic forms (Chapter 6's Hanson–Wright inequality controls ∑εiεj\sum \varepsilon_i \varepsilon_j∑εi​εj​-type terms, which are themselves products of sub-gaussians and hence sub-exponential by Lemma 2.7.7), and it is the standard tool for bounding empirical-process suprema whose summands are not bounded but merely light-tailed.

Formalizing it. No formalization of Bernstein's inequality — in either the weighted or unweighted, or sub-gaussian or sub-exponential form — exists yet on Prove2Me (GET /theorems?q=Bernstein and q=sub-exponential return no relevant hits, checked 2026-09-17). What this mission produces is not just the statement but the machinery underneath it: a working Orlicz-norm treatment of ψ1\psi_1ψ1​ and ψ2\psi_2ψ2​ that a later mission (the Hanson–Wright inequality, or any future chapter that needs sub-exponential concentration) can build on directly.

Difficulty

The obvious first idea — squaring both sides and applying Chebyshev, as one does to prove the weak law of large numbers — gives only a polynomial tail bound decaying like 1/N1/N1/N, far too weak to be useful (this is exactly the point made by the chapter's opening discussion of the coin-tossing example, comparing the linear decay from Chebyshev against the target exponential decay). The central limit theorem promises the right shape of tail asymptotically but, per Berry–Esseen, with an error of order 1/N1/\sqrt N1/N​ that swamps any exponential gain for large deviations — the CLT approximation is simply not valid in the tail regime the inequality needs. The actual argument instead controls the moment generating function of the full sum directly and optimizes an exponential (Chernoff) tilt; this is why the sub-gaussian and sub-exponential norms — MGF-control objects, not moment or tail objects per se — are the right technical vehicle, even though Proposition 2.5.2 and 2.7.1 show all these characterizations are equivalent up to constants. The min of two terms in Bernstein's exponent is not an artifact of a loose proof: it reflects a genuinely two-regime tail (Gaussian near the mean, exponential in the far tail), and collapsing it to a single term in either direction would either be false (dropping the exponential term) or needlessly weak (dropping the Gaussian term, which is what a naive union bound over the worst single term would give).

Formalization scope

Random variables are ℝ-valued functions on an explicit probability space (Ω, mΩ, P) (Ω : Type, MeasurableSpace Ω, P : Measure Ω, [IsProbabilityMeasure P]), matching the book's setup throughout. Independence is Mathlib's ProbabilityTheory.iIndepFun, and tail probabilities are stated with P.real, Mathlib's ℝ-valued measure evaluation, which corresponds directly to the book's P{⋅}P\{\cdot\}P{⋅}.

Both Orlicz norms are defined locally, as genuine infima matching Definitions 2.5.6 and 2.7.5 verbatim (subgaussianNorm, subexponentialNorm, each sInf {t > 0 : Integrable (fun ω => E[...]) P ∧ E[...] ≤ 2}), rather than reused from Mathlib's HasSubgaussianMGF (Mathlib.Probability.Moments.SubGaussian). The Integrable conjunct is not optional dressing: Mathlib's Bochner integral of a non-integrable function is 0 by convention, so a bare E[...] ≤ 2 (without asserting integrability) would be satisfied by every t for which the moment is actually infinite, collapsing the sub-gaussian norm of a standard Gaussian (and, symmetrically, the sub-exponential norm of any heavy-tailed variable) to 0 — a trivializing formalization the mission was moderated to rule out. The same Integrable conjunct appears in every moment hypothesis (general_hoeffding, bernstein_unweighted, bernstein_weighted): ∃ s > 0, Integrable (...) P ∧ ∫ ... ≤ 2, so that the hypothesis is not satisfied vacuously by non-integrable exponential moments either. HasSubgaussianMGF bounds the moment generating function directly with a variance-proxy parameter σ2\sigma^2σ2 (E exp(tX) ≤ exp(c t²/2)), which is a different object definitionally from the Orlicz ψ2\psi_2ψ2​ norm — equivalent up to a constant factor by the book's own Proposition 2.5.2, but not interchangeable without restating that equivalence — and Mathlib has no sub-exponential analogue at all. Since the goal theorem and two of its milestones need the sub-exponential norm, one consistent convention (the book's own Orlicz norms) is used for both ψ1\psi_1ψ1​ and ψ2\psi_2ψ2​ throughout the mission, rather than mixing Mathlib's MGF-based sub-gaussian convention with a locally defined sub-exponential one.

Every occurrence of the book's "ccc is an absolute constant" is formalized as a genuine existential quantifier fixed before the random variables, the vector a, and t are introduced: ∃ c : ℝ, 0 < c ∧ ∀ ..., P.real {...} ≤ 2 * Real.exp (-(c * ...)). No numeral is substituted for c anywhere; a solver's proof may use any positive constant it can establish, exactly mirroring the book's own non-constructive existence claims. The trivializing formalization this rules out is fixing c to a specific small numeral (which would be a strictly stronger, easier, and unfaithful claim) or, in the other direction, weakening the statement by allowing c to depend on N, the XiX_iXi​, a, or t (which would make the theorem vacuous, since any such bound trivially holds for a small enough ccc depending on the instance).

Chernoff's inequality (Theorem 2.3.1) needs no Orlicz norm — Bernoulli parameters pip_ipi​ are given directly via P.real {X i = 1} = p i ∧ P.real {X i = 0} = 1 - p i, and the conclusion uses Real.rpow (^ on ℝ → ℝ → ℝ) for the real exponent ttt in (eμ/t)t(e\mu/t)^t(eμ/t)t. Hoeffding's inequality for symmetric Bernoulli variables (Theorem 2.2.2) is likewise self-contained, needing only the two-point probability hypothesis defining the Rademacher distribution.

Selected references

  • W. Hoeffding, Probability Inequalities for Sums of Bounded Random Variables, Journal of the American Statistical Association 58(301), 1963. https://doi.org/10.2307/2282952
  • S. Bernstein, The Theory of Probabilities, Gastehizdat Publishing House, Moscow, 1946 (Russian; the inequality is due to Bernstein's earlier 1920s–1930s work, this textbook states the modern sub-exponential form following later expositions).
  • A. C. Berry, The Accuracy of the Gaussian Approximation to the Sum of Independent Variates, Transactions of the American Mathematical Society 49(1), 1941. https://doi.org/10.2307/1990053
  • C.-G. Esseen, On the Liapunoff Limit of Error in the Theory of Probability, Arkiv för Matematik, Astronomi och Fysik A28, 1942.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 2. https://doi.org/10.1017/9781108231596
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High-Dimensional Probability I: Approximate Carathéodory's TheoremTextbook

Motivation

Many arguments in high-dimensional geometry, statistics and computer science need to approximate a point of a convex set by an average of a handful of extreme points, rather than represent it exactly. The classical Carathéodory theorem (1907) answers the exact question: every point of the convex hull of a set T⊆RnT \subseteq \mathbb{R}^nT⊆Rn is a convex combination of at most n+1n+1n+1 points of TTT. That bound is tight and grows with the dimension nnn, which makes it useless whenever nnn is large — exactly the regime of interest in high-dimensional probability.

B. Maurey's empirical method — an unpublished 1980–81 result reported by G. Pisier, "Remarques sur un résultat non publié de B. Maurey," Séminaire d'Analyse Fonctionnelle 1980–1981 — and later applied by B. Carl to bound covering numbers of operators between Banach spaces (Inequalities of Bernstein-Jackson-type and the degree of compactness of operators in Banach spaces, Ann. Inst. Fourier 35(3), 1985, 79–118), replaces the exact question with an approximate one and removes the dimension dependence entirely: to approximate xxx to accuracy ε\varepsilonε, the number of points needed depends only on ε\varepsilonε, never on nnn. Vershynin's High-Dimensional Probability opens with this result as its "Appetizer," using it to illustrate the book's central theme — that randomness is a tool for constructing deterministic combinatorial objects — before any probabilistic machinery has been introduced.

Setting

A convex combination of finitely many points z1,…,zm∈Rnz_1, \dots, z_m \in \mathbb{R}^nz1​,…,zm​∈Rn is a sum ∑i=1mλizi\sum_{i=1}^m \lambda_i z_i∑i=1m​λi​zi​ with λi≥0\lambda_i \ge 0λi​≥0 and ∑iλi=1\sum_i \lambda_i = 1∑i​λi​=1. The convex hull conv⁡(T)\operatorname{conv}(T)conv(T) of a set T⊆RnT \subseteq \mathbb{R}^nT⊆Rn is the set of all convex combinations of all finite collections of points of TTT. The diameter of TTT is diam⁡(T)=sup⁡{∥s−t∥2:s,t∈T}\operatorname{diam}(T) = \sup\{\|s-t\|_2 : s, t \in T\}diam(T)=sup{∥s−t∥2​:s,t∈T}, the Euclidean norm throughout.

The classical Carathéodory theorem states that every x∈conv⁡(T)x \in \operatorname{conv}(T)x∈conv(T) is a convex combination of at most n+1n+1n+1 points of TTT — with n+1n+1n+1 generally unavoidable, attained by a simplex. The question this mission answers is different: given that we are willing to approximate xxx rather than represent it exactly, and willing to use only combinations with equal coefficients 1/k1/k1/k (an average of kkk points, with repetition allowed), how large must kkk be as a function of the desired accuracy?

Formalization targets

Goal — Theorem 0.0.2, Approximate Carathéodory's theorem

diam(T)≤1, x∈conv⁡(T), k∈Z>0 ⟹ ∃ x1,…,xk∈T:∥x−1k∑j=1kxj∥2≤1k.\text{diam}(T) \le 1,\ x \in \operatorname{conv}(T),\ k \in \mathbb{Z}_{>0} \ \Longrightarrow\ \exists\, x_1,\dots,x_k \in T:\quad \left\| x - \frac{1}{k}\sum_{j=1}^{k} x_j \right\|_2 \le \frac{1}{\sqrt{k}}.diam(T)≤1, x∈conv(T), k∈Z>0​ ⟹ ∃x1​,…,xk​∈T:​x−k1​j=1∑k​xj​​2​≤k​1​.

The quantifiers are exactly this order: for every bounded TTT, every point of its convex hull, and every target kkk, such an averaging set exists. This is the weakest stable statement carrying the theorem's content — the number of points kkk does not depend on the dimension nnn, and the coefficients are forced to be uniform — and it is the form the corollary below invokes directly.

Milestone — Corollary 0.0.4, Covering polytopes by balls

P=conv⁡(T), ∣T∣=N, diam⁡(P)≤1, ε>0 ⟹ ∃ C, ∣C∣≤N⌈1/ε2⌉:P⊆⋃c∈CB‾(c,ε).P = \operatorname{conv}(T),\ |T| = N,\ \operatorname{diam}(P) \le 1,\ \varepsilon > 0 \ \Longrightarrow\ \exists\, C,\ |C| \le N^{\lceil 1/\varepsilon^2 \rceil}:\quad P \subseteq \bigcup_{c \in C} \overline{B}(c, \varepsilon).P=conv(T), ∣T∣=N, diam(P)≤1, ε>0 ⟹ ∃C, ∣C∣≤N⌈1/ε2⌉:P⊆c∈C⋃​B(c,ε).

This is a direct application of the goal to computational geometry's covering problem: how many balls of radius ε\varepsilonε are needed to cover a polytope, and where should they be centered.

Significance

The result itself. The approximate Carathéodory theorem is the prototype of a dimension-free approximation result: whenever a set is bounded, a fixed number of points (depending only on the target accuracy, not the ambient dimension) suffices to approximate any point of its convex hull. This is what makes possible dimension-independent covering-number bounds such as Corollary 0.0.4, which in turn are the starting point for the book's later treatment of entropy, packing and generic chaining (Chapters 4, 7–8). The technique generalizes far beyond Rn\mathbb{R}^nRn: it underlies covering-number bounds for operators between Banach spaces (Carl's original application) and is a recurring device in learning theory for bounding the size of an ε\varepsilonε-net of a hypothesis class.

Formalizing it. Both results are elementary and already fully proved in the literature; no open mathematical content remains. What this mission contributes is a machine-checked, faithful Lean statement of Maurey's construction and its corollary, phrased over Mathlib's existing convex-hull and metric-diameter machinery, so that later missions in this series (concentration inequalities, Johnson–Lindenstrauss, chaining) can build on a verified base case of "probability constructs a deterministic covering," and so that the empirical method itself becomes a reusable, linked component on the platform. The proof of the goal (via the probabilistic argument sketched by the book: interpret a convex combination as a probability distribution, average kkk i.i.d. samples, and bound the variance) is left open for solvers.

Difficulty

The identity that makes the proof work — averaging kkk independent copies of a random vector concentrates around its mean at rate 1/k1/\sqrt{k}1/k​ in mean-square — is a two-line computation once the convex combination is reinterpreted probabilistically. The step that is easy to miss is this reinterpretation itself: nothing in the statement mentions probability, so the "obvious" attack of manipulating the convex-combination weights directly, or trying to construct x1,…,xkx_1,\dots,x_kx1​,…,xk​ by some explicit combinatorial recipe, does not see a path to a bound independent of nnn. The probabilistic argument produces the points non-constructively, via an averaging/existence argument (the expected squared distance is small, so some realization achieves it) rather than an explicit formula — a solver has to introduce a probability space and a random vector that does not appear anywhere in the formal statement to be proved.

Formalization scope

Both results are stated over EuclideanSpace ℝ (Fin n) for an explicit dimension n : ℕ, so ‖·‖ is the Euclidean norm and Mathlib's Metric.diam is used directly for diam⁡(T)=sup⁡{∥s−t∥2}\operatorname{diam}(T) = \sup\{\|s-t\|_2\}diam(T)=sup{∥s−t∥2​}. The convex hull is Mathlib's convexHull ℝ T; by Mathlib's convexHull_eq, this already coincides with the book's own definition of a convex combination of finitely many points of TTT, so no bespoke convex-combination definition is introduced — this mission needs no supporting definitions of its own. In the corollary, "a polytope PPP with NNN vertices" is formalized, following the book's own proof, as P=conv⁡(T)P = \operatorname{conv}(T)P=conv(T) for a finite vertex set TTT with #T=N\#T = N#T=N, rather than via a separate Polytope structure (which Mathlib does not provide and the book's argument does not need). The covering bound N⌈1/ε2⌉N^{\lceil 1/\varepsilon^2\rceil}N⌈1/ε2⌉ is an exponent, not a product with NNN — matching the book's own proof, which counts the NkN^kNk ordered kkk-tuples of vertices with repetition, k:=⌈1/ε2⌉k := \lceil 1/\varepsilon^2\rceilk:=⌈1/ε2⌉; the typeset "N⌈1/ε2⌉N\lceil 1/\varepsilon^2\rceilN⌈1/ε2⌉" in the corollary statement is the same juxtaposition-as-exponent notation the proof uses for "NkN^kNk" one line earlier.

A trivializing formalization is ruled out explicitly: the goal must hold for every integer k>0k > 0k>0 and every x∈conv⁡(T)x \in \operatorname{conv}(T)x∈conv(T), not merely some convenient choice — e.g. k=1k = 1k=1 together with x∈Tx \in Tx∈T trivially satisfies the inequality but proves nothing about the theorem's actual content, that a fixed, dimension-independent kkk works uniformly over all points of the hull. The formal statement quantifies TTT, then xxx, then kkk, and only then asserts existence of the x1,…,xkx_1,\dots,x_kx1​,…,xk​, exactly in that order.

Classical Carathéodory (Theorem 0.0.1, stated for context in the source but not used by either formalized result's proof) is not drafted here: Mathlib already proves the corresponding statement via affine independence (Caratheodory.eq_pos_convex_span_of_mem_convexHull, Analysis/Convex/Caratheodory.lean), from which the book's "n+1n+1n+1 points" bound follows via AffineIndependent.card_le_finrank_succ. It is not added as a kind: reference milestone because no corresponding theorem is yet published on the Prove2Me platform to point at (checked 2026-09-17: GET /theorems?q=Caratheodory returns only unrelated tropical-convexity results), and re-drafting existing Mathlib content as a new platform theorem would duplicate rather than reuse it.

Selected references

  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, DOI 10.1017/9781108231596, Appetizer (pp. 1–5).
  • G. Pisier, "Remarques sur un résultat non publié de B. Maurey," Séminaire d'Analyse Fonctionnelle (Maurey–Schwartz), 1980–1981, exposé no. 5. numdam.org/item/SAF_1980-1981____A5_0
  • B. Carl, "Inequalities of Bernstein-Jackson-type and the degree of compactness of operators in Banach spaces," Annales de l'Institut Fourier, 35(3), 1985, 79–118. numdam.org/item/AIF_1985__35_3_79_0
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Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

Introduction to Stochastic Programming VI: Jensen and Edmundson-Madansky BoundsTextbook

Motivation

Two-stage stochastic programs with recourse require evaluating Q(x)=Eξ[Q(x,ξ)]Q(x) = \mathbb E_\xi[Q(x,\xi)]Q(x)=Eξ​[Q(x,ξ)], the expected value of a recourse function, at every candidate first-stage decision xxx. When ξ\xiξ is high-dimensional or continuously distributed, this expectation is a multivariate integral of a piecewise-linear, generally nondifferentiable integrand, and classical quadrature rules — built for smooth integrands in low dimension — do not apply (Birge & Louveaux, §8.1). What does apply is convexity: Q(x,⋅)Q(x,\cdot)Q(x,⋅) is convex whenever the recourse problem is a linear program in ξ\xiξ, and convexity alone is enough to sandwich Eξ[Q(x,ξ)]\mathbb E_\xi[Q(x,\xi)]Eξ​[Q(x,ξ)] between two computable discrete approximations. This chapter develops that sandwich, and it is the standard device used throughout the stochastic-programming literature to bound and iteratively refine the recourse function: the lower bound goes back to Jensen [1906]; the upper bound is due to Edmundson [1956] and Madansky [1959], with the mean-consistent LP refinement due to Madansky [1960] and Gassmann & Ziemba [1986]. Refinements of both bounds appear in Huang, Ziemba & Ben-Tal [1977], Kall & Stoyan [1982] and Frauendorfer [1988].

Setting

Fix a probability space (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P) and an integrand g:D×Ξ→Rg : D \times \Xi \to \mathbb Rg:D×Ξ→R, where Ξ⊆E\Xi \subseteq EΞ⊆E is the (convex, closed) support of a random vector ξ:Ω→Ξ\xi : \Omega \to \Xiξ:Ω→Ξ and EEE is a real vector space (in the recourse application, g(x,⋅)=Q(x,⋅)g(x,\cdot) = Q(x,\cdot)g(x,⋅)=Q(x,⋅) and DDD is the first-stage feasible region). Write E(g(x))=Eξ[g(x,ξ)]=∫Ξg(x,ξ) P(dξ)\mathbb E(g(x)) = \mathbb E_\xi[g(x,\xi)] = \int_\Xi g(x,\xi)\, P(d\xi)E(g(x))=Eξ​[g(x,ξ)]=∫Ξ​g(x,ξ)P(dξ).

A partition of Ξ\XiΞ into ν\nuν measurable blocks Sν={S1,…,Sν}S^\nu = \{S_1,\dots,S_\nu\}Sν={S1​,…,Sν​} determines, for each block, its probability pl=P[ξ∈Sl]p_l = P[\xi \in S_l]pl​=P[ξ∈Sl​] and its conditional mean ξl=E[ξ∣Sl]\xi^l = \mathbb E[\xi \mid S_l]ξl=E[ξ∣Sl​]. Equivalently — and this is the convention this mission's Lean development uses — the blocks may be taken directly on the sample space as the pulled-back sets Sl=ξ−1(regionl)⊆ΩS_l = \xi^{-1}(\text{region}_l) \subseteq \OmegaSl​=ξ−1(regionl​)⊆Ω, with pl=P(Sl)p_l = P(S_l)pl​=P(Sl​) and ξl=pl−1∫Slξ dP\xi^l = p_l^{-1}\int_{S_l}\xi\,dPξl=pl−1​∫Sl​​ξdP the Bochner integral average of ξ\xiξ over the block; the two descriptions coincide.

Formalization targets

Goal — Chapter 8, Theorem 1 (Jensen lower bound), p. 346

g(x,⋅) convex on Ξ ⟹ E(g(x)) ≥ ∑l=1νpl g(x,ξl).g(x,\cdot) \text{ convex on } \Xi \ \Longrightarrow\ \mathbb E(g(x)) \ \ge\ \sum_{l=1}^{\nu} p_l\, g(x,\xi^l).g(x,⋅) convex on Ξ ⟹ E(g(x)) ≥ l=1∑ν​pl​g(x,ξl).

This is the sharpest statement the chapter proves for the lower bound: it holds for every finite measurable partition, with no assumption beyond convexity of g(x,⋅)g(x,\cdot)g(x,⋅) and integrability.

Chapter 8, Theorem 2 (Edmundson-Madansky upper bound), pp. 347-348

For Ξ\XiΞ compact, let ext Ξ\mathrm{ext}\,\XiextΞ be the extreme points of co Ξ\mathrm{co}\,\XicoΞ, carrying the Borel field of all its subsets. If, for every ξ∈Ξ\xi \in \Xiξ∈Ξ, φ(ξ,⋅)\varphi(\xi,\cdot)φ(ξ,⋅) is a probability measure on ext Ξ\mathrm{ext}\,\XiextΞ with barycenter ξ\xiξ (i.e. ∫ext Ξe φ(ξ,de)=ξ\int_{\mathrm{ext}\,\Xi} e\,\varphi(\xi,de) = \xi∫extΞ​eφ(ξ,de)=ξ) and ω↦φ(ξ(ω),A)\omega \mapsto \varphi(\xi(\omega), A)ω↦φ(ξ(ω),A) is measurable for every AAA, then

E(g(x)) ≤ ∫ext Ξg(x,e) λ(de),λ(A)=∫Ωφ(ξ(ω),A) P(dω).\mathbb E(g(x)) \ \le\ \int_{\mathrm{ext}\,\Xi} g(x,e)\, \lambda(de), \qquad \lambda(A) = \int_\Omega \varphi(\xi(\omega), A)\, P(d\omega).E(g(x)) ≤ ∫extΞ​g(x,e)λ(de),λ(A)=∫Ω​φ(ξ(ω),A)P(dω).

Together the two targets give the chapter's headline sandwich: for convex g(x,⋅)g(x,\cdot)g(x,⋅), the finite-partition Jensen value and the Edmundson-Madansky value bracket the true expectation, and refining the partition (resp. the disintegration) tightens both sides toward it.

Significance

The Jensen bound is the workhorse of discrete-distribution approximation in stochastic programming: it is what makes Qν(x)=∑lplQ(x,ξl)Q^\nu(x) = \sum_l p_l Q(x,\xi^l)Qν(x)=∑l​pl​Q(x,ξl) a valid, refinable lower-approximation of the true recourse function, and it underlies the partition-refinement schemes (§8.2, following Birge & Wets [1986] and Frauendorfer & Kall [1988]) used inside the LLL-shaped method and separable-programming solvers described later in the chapter (§8.3). The Edmundson-Madansky bound is its indispensable upper counterpart: without it there is no certificate of how far a lower approximation can be from the truth, and the mean-consistent LP refinement (eq. 2.9, not part of this mission) reduces to a moment-problem computation over λ\lambdaλ. Both bounds are, to date, unformalized: the platform holds no theorem matching either a finite-partition conditional-Jensen inequality or an extreme-point disintegration bound (searched GET /theorems?q=... for "Jensen", "conditional expectation", "Edmundson Madansky", "partition convex" — no relevant hits), so this mission is a first formalization of both, not a reformulation of existing platform content. Mathlib supplies the raw convexity substrate this mission is built from — finite Jensen (Analysis/Convex/Jensen.lean) and, critically, the set-average integral Jensen inequality (ConvexOn.map_set_average_le in Analysis/Convex/Integral.lean), exactly the per-block step the book's proof of Theorem 1 performs — but no existing lemma assembles these into the partitioned, conditional-mean statement the book actually states.

Difficulty

The obvious shortcut is to prove "convex functions lie above their tangent line" and stop — this captures no partition structure at all and is not the theorem the book states (the theorem is about Σlplg(x,ξl)\Sigma_l p_l g(x,\xi^l)Σl​pl​g(x,ξl), a sum over blocks, not a single linearization). The real content is bookkeeping across the partition: writing E(g(x))\mathbb E(g(x))E(g(x)) as ∑lP(Sl) E[g(x,ξ)∣Sl]\sum_l P(S_l)\,\mathbb E[g(x,\xi)\mid S_l]∑l​P(Sl​)E[g(x,ξ)∣Sl​] (an exact identity, no convexity needed), then applying ordinary Jensen inside each block to replace E[g(x,ξ)∣Sl]\mathbb E[g(x,\xi)\mid S_l]E[g(x,ξ)∣Sl​] by g(x,ξl)g(x,\xi^l)g(x,ξl) from below — the inequality only enters at the second step, once per block. Proving this in Lean means correctly discharging, for every block, the side conditions Mathlib's integral-Jensen lemma needs (closedness of Ξ\XiΞ, continuity of g(x,⋅)g(x,\cdot)g(x,⋅) on Ξ\XiΞ, integrability on the block) and then summing the ν\nuν per-block inequalities against weights plp_lpl​ that themselves depend on the partition — an easy step to get wrong by, e.g., letting ξl\xi^lξl be an arbitrary point of SlS_lSl​ rather than exactly its conditional mean, which understates what Jensen actually forces. Theorem 2 additionally requires setting up the disintegration λ\lambdaλ correctly: λ\lambdaλ is a probability measure defined as an integral of the kernel-like family φ\varphiφ against P∘ξ−1P\circ\xi^{-1}P∘ξ−1, and both the barycenter condition on φ\varphiφ and the measurability of ω↦φ(ξ(ω),A)\omega \mapsto \varphi(\xi(\omega),A)ω↦φ(ξ(ω),A) are load-bearing — dropping either makes λ\lambdaλ ill-defined or the bound's proof inapplicable.

Formalization scope

Ξ⊆E\Xi \subseteq EΞ⊆E for EEE a complete real normed vector space (NormedAddCommGroup E, NormedSpace ℝ E, CompleteSpace E); no finite-dimensionality is assumed since neither theorem's proof needs it. The parameter xxx ranges over an arbitrary type α\alphaα with D⊆αD \subseteq \alphaD⊆α, and ggg is left as a bare function α → E → ℝ, matching the book's level of abstraction (the recourse LP's own data A,b,c,q,W,T,hA,b,c,q,W,T,hA,b,c,q,W,T,h is never used in either proof).

The partition is formalized directly on the sample space Ω\OmegaΩ (a Partition structure: pairwise-disjoint measurable blocks covering Ω\OmegaΩ, each of positive measure) rather than on Ξ\XiΞ, per the equivalence noted under Setting; ξl\xi^lξl is defined as the Bochner-integral average pl−1∫Slξ dPp_l^{-1}\int_{S_l}\xi\,dPpl−1​∫Sl​​ξdP, so it is forced to be the conditional mean and cannot be weakened to an arbitrary sample point of the block — the change the chunk brief flags as the main faithfulness trap for this chapter.

Two explicit hypotheses are added beyond the book's own statement of Theorem 1, both needed by Mathlib's integral-Jensen lemma rather than narrowings of the mathematical content: ContinuousOn (g x) Ξ (finite-dimensional convex functions are automatically continuous on the interior of their domain, which is what the book implicitly relies on; stated explicitly since EEE is not assumed finite-dimensional) and integrability of ξ\xiξ and of g(x,ξ(⋅))g(x,\xi(\cdot))g(x,ξ(⋅)) (needed for E(g(x))\mathbb E(g(x))E(g(x)) and each ξl\xi^lξl to be well-defined). For Theorem 2, the disintegrating family φ\varphiφ is E → Measure Ext for an abstract type Ext (standing for ext Ξ\mathrm{ext}\,\XiextΞ) with the discrete MeasurableSpace (every subset measurable, matching the book's "Borel field ... the collection of all subsets"), mapped into EEE by an embedding toE whose range is exactly (convexHull ℝ Ξ).extremePoints ℝ; the measure λ\lambdaλ (named μExt in the Lean code, since λ is a reserved keyword) is a hypothesis satisfying its defining equation (2.6) rather than constructed, since constructing a measure from a set function is a separate, book-external piece of measure theory the chapter's own proof does not perform either — it simply asserts λ\lambdaλ is the probability measure with that value on every set.

A trivializing formalization is ruled out explicitly: a version that lets ξl\xi^lξl range over an arbitrary point of SlS_lSl​, or that proves only the ordinary (unconditional) Jensen inequality without ever introducing the partition, states something strictly weaker than the book and is not what is formalized here.

Both draft theorems end in := by sorry; a full Lean proof of Theorem 1 combines Mathlib's ConvexOn.map_set_average_le applied per block with the exact decomposition of ∫Ω\int_\Omega∫Ω​ into ∑l∫Sl\sum_l \int_{S_l}∑l​∫Sl​​ over the partition's disjoint, covering blocks. Reusable beyond this mission: the Partition structure and its weight/condMean accessors generalize to any chapter needing a finite measurable partition with conditional means (this book's later approximation schemes, §8.2-8.5 and Chapter 10, all build on the same device). Contributions solving either theorem, or formalizing the partition-refinement monotonicity E(g(x))≥Eν+1(g(x))≥Eν(g(x))\mathbb E(g(x)) \ge \mathbb E^{\nu+1}(g(x)) \ge \mathbb E^\nu(g(x))E(g(x))≥Eν+1(g(x))≥Eν(g(x)) (eq. 2.3, not part of this mission's milestone list since it is not itself a numbered theorem) as a follow-up, are welcome.

Selected references

  • J.R. Birge, 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
  • J.L.W.V. Jensen, Sur les fonctions convexes et les inégalités entre les valeurs moyennes, Acta Mathematica 30 (1906), 175-193. https://doi.org/10.1007/BF02418571
  • H.P. Edmundson, Bounds on the expectation of a convex function of a random variable, The RAND Corporation, Paper 982, 1956.
  • A. Madansky, Bounds on the expectation of a convex function of a multivariate random variable, Annals of Mathematical Statistics 30 (1959), 743-746. https://doi.org/10.1214/aoms/1177706207
  • A. Madansky, Inequalities for stochastic linear programming problems, Management Science 6 (1960), 197-204. https://doi.org/10.1287/mnsc.6.2.197
  • H.I. Gassmann, W.T. Ziemba, A tight upper bound for the expectation of a convex function of a multivariate random variable, Mathematical Programming Study 27 (1986), 39-53. https://doi.org/10.1007/BFb0121114
  • J.R. Birge, R.J-B. Wets, Designing approximation schemes for stochastic optimization problems, in particular for stochastic programs with recourse, Mathematical Programming Study 27 (1986), 54-102. https://doi.org/10.1007/BFb0121122
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Operations ResearchOptimization·Captain: mikedeng1

Introduction to Stochastic Programming II: The Value of Perfect Information and of the Stochastic SolutionTextbook

Motivation

Every stochastic program is, in practice, compared against a shortcut. A decision maker facing genuine uncertainty is tempted either to replace the random data by its mean and solve one deterministic problem, or to imagine that perfect information about the future were available and solve a separate deterministic problem per scenario. Both temptations have precise answers: the expected value of perfect information (EVPI) measures how much a decision maker should be willing to pay for a perfect forecast, and the value of the stochastic solution (VSS) measures the cost of ignoring uncertainty altogether by solving the mean-value problem. Both concepts originate in decision analysis — EVPI traces to Raiffa and Schlaifer (1961) — and were brought into stochastic programming by Madansky (1960), who proved the first chain of inequalities relating the wait-and-see value, the recourse value and the expected-value-solution's cost. Birge and Louveaux, Introduction to Stochastic Programming, 2nd ed. (Springer, 2011), Chapter 4, gives the standard modern treatment, including a refined family of bounds — built from pairs subproblems against a chosen reference scenario — that sharpen VSS beyond the original mean-scenario comparison. This mission formalizes that chapter's capstone: the five-quantity, four-inequality chain that pins VSS between two computable optimal values.

Setting

Fix a two-stage stochastic program with fixed recourse: a finite family of K scenarios ξ1,…,ξK\xi_1,\dots,\xi_Kξ1​,…,ξK​ in Rd\mathbb R^dRd, each occurring with probability pk≥0p_k \ge 0pk​≥0, ∑kpk=1\sum_k p_k = 1∑k​pk​=1; a first-stage feasible set K1⊆Rn1K_1 \subseteq \mathbb R^{n_1}K1​⊆Rn1​; and, for every first-stage decision x∈Rn1x \in \mathbb R^{n_1}x∈Rn1​ and every scenario ξ∈Rd\xi \in \mathbb R^dξ∈Rd, a scenario cost z(x,ξ)z(x,\xi)z(x,ξ) — the optimal value of cTx+min⁡{qTy∣Wy=h(ξ)−Tx, y≥0}c^Tx + \min\{q^Ty \mid Wy = h(\xi) - Tx,\ y \ge 0\}cTx+min{qTy∣Wy=h(ξ)−Tx, y≥0}. By convention z(x,ξ)=+∞z(x,\xi) = +\inftyz(x,ξ)=+∞ when xxx has no feasible second-stage recourse under ξ\xiξ, and z(x,ξ)=−∞z(x,\xi) = -\inftyz(x,ξ)=−∞ when the second-stage program is unbounded below.

From zzz, five basic quantities are defined (Birge & Louveaux §4.1–§4.2):

  • The recourse problem's value, RP=min⁡x∈K1Eξ z(x,ξ)RP = \min_{x \in K_1} \mathbb E_\xi\, z(x,\xi)RP=minx∈K1​​Eξ​z(x,ξ) — the best a decision maker can do without foreknowledge of ξ\xiξ (the "here-and-now" solution).
  • The wait-and-see value, WS=Eξ[min⁡x∈K1z(x,ξ)]WS = \mathbb E_\xi\big[\min_{x \in K_1} z(x,\xi)\big]WS=Eξ​[minx∈K1​​z(x,ξ)] — the average cost if ξ\xiξ were revealed before choosing xxx.
  • The expected value of perfect information, EVPI=RP−WSEVPI = RP - WSEVPI=RP−WS.
  • The expected value problem's solution xˉ(ξˉ)\bar x(\bar\xi)xˉ(ξˉ​), optimal for the deterministic problem at the mean scenario ξˉ=E(ξ)\bar\xi = \mathbb E(\xi)ξˉ​=E(ξ); its recourse cost, the expected result of using the EV solution, is EEV=Eξ z(xˉ(ξˉ),ξ)EEV = \mathbb E_\xi\, z(\bar x(\bar\xi), \xi)EEV=Eξ​z(xˉ(ξˉ​),ξ).
  • The value of the stochastic solution, VSS=EEV−RPVSS = EEV - RPVSS=EEV−RP — the extra cost of implementing the mean-scenario decision instead of solving the recourse problem.

Section 4.6 refines VSS by replacing the mean scenario with an arbitrary reference scenario ξr\xi^rξr (not necessarily one of the KKK possible scenarios, e.g. a worst case), with assumed probability pr=P(ξ=ξr)p_r = P(\xi=\xi^r)pr​=P(ξ=ξr):

  • xˉr\bar x^rxˉr, optimal for min⁡x∈K1z(x,ξr)\min_{x\in K_1} z(x,\xi^r)minx∈K1​​z(x,ξr), gives the expected value of the reference-scenario solution, EVRS=Eξ z(xˉr,ξ)EVRS = \mathbb E_\xi\, z(\bar x^r,\xi)EVRS=Eξ​z(xˉr,ξ), and the generalized VSS=EVRS−RPVSS = EVRS - RPVSS=EVRS−RP.
  • For each scenario ξk\xi^kξk, the pairs subproblem of ξr\xi^rξr and ξk\xi^kξk treats them as a two-point distribution with weights prp_rpr​ and 1−pr1-p_r1−pr​: its optimal value is min⁡x∈K1[pr z(x,ξr)+(1−pr) z(x,ξk)]\min_{x\in K_1}\big[p_r\,z(x,\xi^r) + (1-p_r)\,z(x,\xi^k)\big]minx∈K1​​[pr​z(x,ξr)+(1−pr​)z(x,ξk)], attained at some xˉk\bar x^kxˉk. Averaging these optimal values over kkk (rescaled by 1/(1−pr)1/(1-p_r)1/(1−pr​)) gives the sum of pairs expected values, SPEVSPEVSPEV. Taking, instead, the smallest full expected cost Eξ z(xˉk,ξ)\mathbb E_\xi\,z(\bar x^k,\xi)Eξ​z(xˉk,ξ) among the K+1K{+}1K+1 candidate solutions {xˉ1,…,xˉK,xˉr}\{\bar x^1,\dots,\bar x^K,\bar x^r\}{xˉ1,…,xˉK,xˉr} gives the expectation of pairs expected value, EPEVEPEVEPEV.

Formalization targets

Goal — Chapter 4, Theorem 9 (p. 174)

0  ≤  EVRS−EPEV  ≤  VSS  ≤  EVRS−SPEV  ≤  EVRS−WS.0 \;\le\; EVRS - EPEV \;\le\; VSS \;\le\; EVRS - SPEV \;\le\; EVRS - WS .0≤EVRS−EPEV≤VSS≤EVRS−SPEV≤EVRS−WS.

Four links, each with independent content: nonnegativity of the leftmost gap, then two genuine inequalities (from the pairs-subproblem comparisons of Propositions 7 and 8), then the identity VSS=EVRS−RPVSS = EVRS - RPVSS=EVRS−RP folded against RP≥WSRP \ge WSRP≥WS's reverse-direction cousin. This is the weakest statement that keeps all five quantities distinct — stating only the outer bound 0≤VSS≤EVRS−WS0 \le VSS \le EVRS-WS0≤VSS≤EVRS−WS would erase exactly the refinement (via pairs subproblems) that makes the chapter's method useful.

Supporting propositions (milestones, in attack order)

  • Proposition 1 (p. 166): WS≤RP≤EEVWS \le RP \le EEVWS≤RP≤EEV.
  • Proposition 5(a) (pp. 167–168): 0≤EVPI0 \le EVPI0≤EVPI and 0≤VSS0 \le VSS0≤VSS (mean-scenario form), for any stochastic program.
  • Proposition 7 (p. 173): WS≤SPEV≤RPWS \le SPEV \le RPWS≤SPEV≤RP.
  • Proposition 8 (p. 174): RP≤EPEV≤EVRSRP \le EPEV \le EVRSRP≤EPEV≤EVRS.

Significance

The chain gives a decision maker two computable, non-obvious bounds on VSS — a quantity that is otherwise expensive to pin down exactly, since RPRPRP itself already requires solving the full recourse problem. EVRS−EPEVEVRS - EPEVEVRS−EPEV and EVRS−SPEVEVRS - SPEVEVRS−SPEV are both computable from K+1K+1K+1 (or KKK) two-scenario LPs, far cheaper than the full KKK-scenario recourse problem, so Theorem 9 turns an expensive exact quantity into a pair of cheap certified bounds. Formalizing it fixes, once and for all, the exact hypotheses and quantifier structure of Madansky's original inequality (Proposition 1) together with the later pairs-subproblem refinement (Propositions 6–8, Birge 1982), often cited informally as "the VSS bounds" without distinguishing EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV and SPEVSPEVSPEV. No part of this chain is on Mathlib or Formalpedia today (checked by concept query, not title); this is a first, from-scratch treatment of two-stage recourse value-of-information theory as formal objects.

Difficulty

The obvious first idea — collapse RPRPRP, WSWSWS, EVEVEV, EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV, SPEVSPEVSPEV to one "the optimal value of the LP" and prove a single inequality — throws away the entire content of the chapter. Each quantity restricts the minimization to a different feasible object: RPRPRP minimizes jointly over xxx; WSWSWS swaps the order of min⁡\minmin and E\mathbb EE; EEVEEVEEV/EVRSEVRSEVRS evaluate one fixed xxx under every scenario; SPEVSPEVSPEV and EPEVEPEVEPEV each minimize over a family of pairs subproblems rather than the full KKK-scenario problem. The chain's proof (Propositions 7–8) depends on this precisely: Proposition 7's lower bound uses that each pairs-subproblem-optimal (xˉk,yˉk)(\bar x^k,\bar y^k)(xˉk,yˉ​k) is feasible (not necessarily optimal) for the single-scenario problem at ξr\xi^rξr, and its upper bound uses that the recourse-optimal (x∗,y∗(ξr),y∗(ξk))(x^*, y^*(\xi^r), y^*(\xi^k))(x∗,y∗(ξr),y∗(ξk)) is feasible (not necessarily optimal) for the pairs subproblem — a feasible-but-not-optimal argument in each direction, not a direct comparison of objective values. Losing track of which solution is fixed and which is optimized destroys the argument entirely.

Formalization scope

An Instance bundles the finite scenario set (Fin K, probabilities p : Fin K → ℝ with p ≥ 0, ∑ p = 1, scenarios xi : Fin K → (Fin d → ℝ)), the first-stage feasible set K1 : Set (Fin n1 → ℝ), and the scenario cost z : (Fin n1 → ℝ) → (Fin d → ℝ) → EReal, using the extended reals to carry the book's own +∞/−∞ conventions for infeasibility and unboundedness rather than silently restricting to a finite-valued special case (a genuine risk of trivialization here, since Example 2 of the chapter exhibits EEV=+∞EEV = +\inftyEEV=+∞). All optimal values (RP, WS, EV, EVPI, EEV, VSS, EVRS, generalized VSS, SPEV, EPEV) are defined directly from z, matching the book's own level of abstraction in this chapter (which never unfolds z into the underlying LP's A,b,c,q,W,T,hA,b,c,q,W,T,hA,b,c,q,W,T,h data — those appear only in Chapter 3). Because EEV, the mean-scenario VSS, EVRS, the generalized VSS, and EPEV are each defined relative to an optimal solution of some sub-problem — the book itself only ever says "let xˉ(ξˉ)\bar x(\bar\xi)xˉ(ξˉ​) denote some optimal solution" — every theorem using them states that solution and its optimality as explicit hypotheses (x ∈ K1 and z x … = ⨅ …), never baking it into a Classical.choiced value; this keeps the quantifier structure faithful to the book's own "let ... be an optimal solution" phrasing. Proposition 5's part (b) — the upper bound EVPI≤EEV−EVEVPI \le EEV-EVEVPI≤EEV−EV, VSS≤EEV−EVVSS \le EEV-EVVSS≤EEV−EV "for stochastic programs with fixed recourse matrix and fixed objective coefficients" — needs a different scope: that hypothesis is a structural property of the underlying LP data (WWW, ccc, qqq fixed across scenarios) invisible once zzz is abstracted away as above, and pinning it down would require modeling the LP's A,b,c,q,W,T,h(ξ)A,b,c,q,W,T,h(\xi)A,b,c,q,W,T,h(ξ) data explicitly (as Chapter 3's mission does for its convexity theorem). That part is out of scope here and is not needed for Theorem 9's own chain, which rests only on Proposition 5(a).

Collapsing any two of RPRPRP, WSWSWS, EVEVEV, EEVEEVEEV, EVRSEVRSEVRS, EPEVEPEVEPEV, SPEVSPEVSPEV to a single "value of the LP" — the trivialization this book-wide series flags for Chapter 4 — is ruled out by construction: each is its own definition over its own feasible object, and Theorem 9's statement names all five quantities in the chain rather than only its outer bound. The two occurrences of "VSS" in the chapter (the original mean-scenario EEV−RPEEV-RPEEV−RP of §4.2, and the reference-scenario EVRS−RPEVRS-RPEVRS−RP generalization of §4.6, used only in Theorem 9) are likewise kept as two distinct definitions rather than conflated under one name.

Every addition and subtraction between EReal values in this mission — inside expect, WS, EVPI, VSS, EVRS's appearance in VSSRef, the pair sum inside pairsValue, the sum inside SPEV, and all four differences in Theorem 9's own chain — uses three explicit operations, badd/bsub/bsum, that implement the book's own convention (p. 164) that +∞ (infeasibility) dominates, i.e. (+∞)+(−∞)=+∞, rather than Mathlib's native EReal addition, whose ⊤+⊥=⊥ would make VSS ≥ 0 (Proposition 5(a)) and the goal's own leftmost inequality false whenever a witness solution is infeasible in a positive-probability scenario — exactly the situation of the book's own Example 2 (pp. 174-175). The reference scenario's probability pr=Pr⁡(ξ=ξr)p_r=\Pr(\xi=\xi^r)pr​=Pr(ξ=ξr) (p. 172) is likewise not a free parameter but a definition, refProb, computed from the instance itself as ∑k: ξk=ξrpk\sum_{k:\,\xi^k=\xi^r}p_k∑k:ξk=ξr​pk​; SPEV's sum is correspondingly restricted to the scenarios other than the reference scenario (ξk≠ξr\xi^k\ne\xi^rξk=ξr), matching the book's own proof of Proposition 7, which uses ∑k≠rpk=1−pr\sum_{k\ne r}p_k=1-p_r∑k=r​pk​=1−pr​. The single hypothesis refProb I xir < 1 on Propositions 7, 8 and the goal says that some other scenario remains possible, which the book's own (1−pr)−1(1-p_r)^{-1}(1−pr​)−1 factor presupposes.

Reusable beyond this mission: the Instance definition and the RP/WS/EV quantities are the natural base for any later chapter of this series that needs the two-stage recourse value (e.g. Chapter 3's convexity mission, Chapter 5's L-shaped method); contributions extending this Instance to the full LP data of the underlying two-stage program, or adding Proposition 5(b) and Proposition 2's Jensen-inequality argument on top of it, are welcome.

Selected references

  • J.R. Birge and F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer Series in Operations Research and Financial Engineering, 2011, Chapter 4. DOI: 10.1007/978-1-4614-0237-4
  • A. Madansky, "Inequalities for Stochastic Linear Programming Problems", Management Science 6(2), 1960, 197–204.
  • H. Raiffa and R. Schlaifer, Applied Statistical Decision Theory, Harvard Business School, 1961.
  • J.R. Birge, "The Value of the Stochastic Solution in Stochastic Linear Programs with Fixed Recourse", Mathematical Programming 24(1), 1982, 314–325.
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AnalysisPartial Differential Equations·Captain: Lucas

Hairer: A Theory of Regularity Structures I — The Reconstruction TheoremResearch Paper

Motivation

Several equations of mathematical physics are written down formally but have no classical meaning as stated. The dynamical Φ34\Phi^4_3Φ34​ model ∂tu=Δu−u3+ξ\partial_t u = \Delta u - u^3 + \xi∂t​u=Δu−u3+ξ on the three-dimensional torus, the KPZ equation ∂th=∂x2h+(∂xh)2−∞+ξ\partial_t h = \partial_x^2 h + (\partial_x h)^2 - \infty + \xi∂t​h=∂x2​h+(∂x​h)2−∞+ξ, and the parabolic Anderson model ∂tu=Δu+u ξ\partial_t u = \Delta u + u\,\xi∂t​u=Δu+uξ all require multiplying a distribution of negative regularity by itself, an operation that Schwartz distribution theory does not provide. Martin Hairer's A theory of regularity structures (Invent. Math. 198 (2014) 269–504, arXiv:1303.5113) develops a calculus in which such products, and the resulting fixed-point problems, become well posed.

The line of work leading to it is short and well documented: rough path theory (Lyons, 1998) solved the analogous problem for controlled ordinary differential equations driven by irregular signals; Gubinelli's controlled paths (2004) and branched rough paths (2010) reorganised it around local expansions; Hairer's theory extends that idea from paths to fields on Rd\mathbb{R}^dRd with anisotropic (e.g. parabolic) scaling. Paracontrolled distributions (Gubinelli–Imkeller–Perkowski, 2015) give an alternative route to some of the same equations. The algebraic and probabilistic infrastructure around regularity structures has since been systematised (Bruned–Hairer–Zambotti, 2019; Chandra–Hairer, 2016), but the analytic core is still the 2014 paper.

Setting

Fix a dimension ddd and a scaling s=(s1,…,sd)s = (s_1,\dots,s_d)s=(s1​,…,sd​) of positive integers, with ∣s∣=∑isi|s| = \sum_i s_i∣s∣=∑i​si​, and put ∥x∥s=max⁡i∣xi∣1/si\|x\|_s = \max_i |x_i|^{1/s_i}∥x∥s​=maxi​∣xi​∣1/si​. For δ>0\delta > 0δ>0, a point x∈Rdx \in \mathbb{R}^dx∈Rd and a test function φ\varphiφ, the rescaled test function is

(Ss,xδφ)(y)=δ−∣s∣ φ ⁣(y1−x1δs1,…,yd−xdδsd).(S^{\delta}_{s,x}\varphi)(y) = \delta^{-|s|}\,\varphi\!\left(\frac{y_1-x_1}{\delta^{s_1}},\dots,\frac{y_d-x_d}{\delta^{s_d}}\right).(Ss,xδ​φ)(y)=δ−∣s∣φ(δs1​y1​−x1​​,…,δsd​yd​−xd​​).

Write Bs,0r\mathcal{B}^r_{s,0}Bs,0r​ for the set of test functions supported in {∥y∥s≤1}\{\|y\|_s \le 1\}{∥y∥s​≤1} whose derivatives up to order rrr are bounded by 111. For α<0\alpha<0α<0, a distribution ξ\xiξ belongs to the Hölder–Besov space Csα\mathcal{C}^\alpha_sCsα​ if, on every compact set KKK, ∣⟨ξ,Ss,xδη⟩∣≤Cδα|\langle \xi, S^{\delta}_{s,x}\eta\rangle| \le C\delta^{\alpha}∣⟨ξ,Ss,xδ​η⟩∣≤Cδα uniformly over x∈Kx\in Kx∈K, δ∈(0,1]\delta \in (0,1]δ∈(0,1] and η∈Bs,0r\eta \in \mathcal{B}^r_{s,0}η∈Bs,0r​ with r=−⌊α⌋r=-\lfloor\alpha\rfloorr=−⌊α⌋.

A regularity structure (A,T,G)(A,T,G)(A,T,G) consists of an index set A⊆RA \subseteq \mathbb{R}A⊆R containing 000, bounded below and locally finite; a graded vector space T=⨁α∈ATαT = \bigoplus_{\alpha\in A} T_\alphaT=⨁α∈A​Tα​ with T0≅RT_0 \cong \mathbb{R}T0​≅R spanned by a unit 1\mathbf{1}1; and a group GGG of linear operators on TTT with Γa−a∈⨁β<αTβ\Gamma a - a \in \bigoplus_{\beta<\alpha}T_\betaΓa−a∈⨁β<α​Tβ​ for a∈Tαa \in T_\alphaa∈Tα​, and Γ1=1\Gamma\mathbf{1} = \mathbf{1}Γ1=1. Elements of TαT_\alphaTα​ are "homogeneous of order α\alphaα": they are placeholders for objects whose size at scale ε\varepsilonε is εα\varepsilon^{\alpha}εα.

A model (Π,Γ)(\Pi,\Gamma)(Π,Γ) assigns to each point xxx a linear map Πx:T→D′(Rd)\Pi_x : T \to \mathcal{D}'(\mathbb{R}^d)Πx​:T→D′(Rd) and to each pair (x,y)(x,y)(x,y) an element Γxy∈G\Gamma_{xy}\in GΓxy​∈G, subject to Γxx=id\Gamma_{xx}=\mathrm{id}Γxx​=id, ΓxyΓyz=Γxz\Gamma_{xy}\Gamma_{yz}=\Gamma_{xz}Γxy​Γyz​=Γxz​, Πy=Πx∘Γxy\Pi_y = \Pi_x\circ\Gamma_{xy}Πy​=Πx​∘Γxy​ and, locally uniformly, the analytic bounds

∣(Πxa)(Ss,xδφ)∣≲∥a∥ℓ δℓ,∥Γxya∥m≲∥a∥ℓ ∥x−y∥sℓ−m,a∈Tℓ,  m<ℓ.|(\Pi_x a)(S^{\delta}_{s,x}\varphi)| \lesssim \|a\|_\ell\,\delta^{\ell}, \qquad \|\Gamma_{xy}a\|_m \lesssim \|a\|_\ell\,\|x-y\|_s^{\ell-m}, \qquad a \in T_\ell,\; m<\ell.∣(Πx​a)(Ss,xδ​φ)∣≲∥a∥ℓ​δℓ,∥Γxy​a∥m​≲∥a∥ℓ​∥x−y∥sℓ−m​,a∈Tℓ​,m<ℓ.

A modelled distribution of order γ\gammaγ is a function f:Rd→T<γf : \mathbb{R}^d \to T_{<\gamma}f:Rd→T<γ​ such that on every compact KKK

∣∣∣f∣∣∣γ;K=sup⁡x∈K, β<γ∥f(x)∥β+sup⁡x,y∈K, ∥x−y∥s≤1β<γ∥f(x)−Γxyf(y)∥β∥x−y∥sγ−β<∞;|||f|||_{\gamma;K} = \sup_{x\in K,\ \beta<\gamma}\|f(x)\|_\beta + \sup_{\substack{x,y \in K,\ \|x-y\|_s\le 1 \\ \beta<\gamma}} \frac{\|f(x)-\Gamma_{xy}f(y)\|_\beta}{\|x-y\|_s^{\gamma-\beta}} < \infty;∣∣∣f∣∣∣γ;K​=x∈K, β<γsup​∥f(x)∥β​+x,y∈K, ∥x−y∥s​≤1β<γ​sup​∥x−y∥sγ−β​∥f(x)−Γxy​f(y)∥β​​<∞;

the space of these is Dγ\mathcal{D}^\gammaDγ, and Dγ(V)\mathcal{D}^\gamma(V)Dγ(V) if fff takes values in a sector VVV, that is, a graded GGG-invariant subspace vanishing in degrees below its regularity.

Formalization targets

Goal — reconstruction theorem, Theorem 3.10 for γ>0\gamma>0γ>0

With α=min⁡A<0\alpha = \min A < 0α=minA<0 and rrr the order attached to AAA, for every f∈Dγf \in \mathcal{D}^\gammaf∈Dγ with γ>0\gamma>0γ>0 there is a unique distribution Rf∈Csα\mathcal{R}f \in \mathcal{C}^\alpha_sRf∈Csα​ with

∣(Rf−Πxf(x))(Ss,xδη)∣≲δγ(x∈K, δ∈(0,1], η∈Bs,0r).\big|(\mathcal{R}f - \Pi_x f(x))(S^{\delta}_{s,x}\eta)\big| \lesssim \delta^{\gamma} \qquad (x \in K,\ \delta\in(0,1],\ \eta\in\mathcal{B}^r_{s,0}).​(Rf−Πx​f(x))(Ss,xδ​η)​≲δγ(x∈K, δ∈(0,1], η∈Bs,0r​).

The statement asserts only the shape of the estimate — a constant per compact set — and so is insensitive to any later sharpening of constants.

Milestone level — the calculus around the reconstruction operator

The uniqueness clause of Theorem 3.10 in isolation; the existence of a linear reconstruction operator for arbitrary γ∈R\gamma \in \mathbb{R}γ∈R (for γ≤0\gamma\le 0γ≤0 the bound no longer pins it down); Corollary 3.16, improving the regularity of Rf\mathcal{R}fRf to Csβ\mathcal{C}^\beta_sCsβ​ when fff takes values in a sector of regularity β\betaβ; Proposition 3.31, that for ν>0\nu>0ν>0 the action of Π\PiΠ on TνT_\nuTν​ is determined by Γ\GammaΓ and by Π\PiΠ in lower homogeneities; and Theorem 4.7, that the truncated pointwise product of f1∈Dγ1(V)f_1 \in \mathcal{D}^{\gamma_1}(V)f1​∈Dγ1​(V) and f2∈Dγ2(W)f_2\in\mathcal{D}^{\gamma_2}(W)f2​∈Dγ2​(W) lies in Dγ\mathcal{D}^{\gamma}Dγ with γ=(γ1+α2)∧(γ2+α1)\gamma = (\gamma_1+\alpha_2)\wedge(\gamma_2+\alpha_1)γ=(γ1​+α2​)∧(γ2​+α1​).

Significance

The reconstruction theorem is what turns a book-keeping device into analysis: it says that a coherent family of local expansions, indexed by base point, glues to a single genuine distribution, with an error controlled by the order of the expansion. Every subsequent operation in the theory — multiplication (Theorem 4.7), composition with smooth functions (Theorem 4.16), the multi-level Schauder estimate (Theorem 5.12), and the fixed-point theorem for singular SPDEs (Theorem 7.8) — is stated and used through it. Without it, the abstract spaces Dγ\mathcal{D}^\gammaDγ carry no information about actual distributions.

Regularity structures are not currently available in Mathlib, and neither are the anisotropic Hölder–Besov spaces Csα\mathcal{C}^\alpha_sCsα​ that the theory is phrased in. The result itself is proved in the literature; the work this mission asks for is a machine-checked proof of the known argument, together with the reusable definitions it needs. The formal development is a prerequisite for anything downstream — Schauder estimates, the fixed-point theory, or the Φ34\Phi^4_3Φ34​ and PAM convergence results of §10 — which are natural follow-on missions rather than part of this one.

Difficulty

The naive construction fails: setting Rf:=Πxf(x)\mathcal{R}f := \Pi_x f(x)Rf:=Πx​f(x) for a fixed xxx is wrong away from xxx, and the pointwise limit lim⁡δ→0\lim_{\delta\to0}limδ→0​ of localisations of Πxf(x)\Pi_x f(x)Πx​f(x) around each xxx does not obviously exist, because the objects being glued are distributions of negative order, not functions, so there is no value to take and no partition-of-unity argument that respects the scaling. Hairer's proof goes through a wavelet multiresolution analysis adapted to the scaling sss: one defines the candidate on each dyadic level by pairing with wavelets centred at grid points, and shows the resulting sequence is Cauchy using the Dγ\mathcal{D}^\gammaDγ bound level by level. A formalization therefore needs either a scaled wavelet basis with Daubechies-type regularity (Theorem 3.17 in the paper) or a substitute for it; this, and the uniform-in-scale bookkeeping, is where the effort lies. Uniqueness for γ>0\gamma>0γ>0 is by contrast short, and is listed as a separate milestone.

Formalization scope

The development commits to the following conventions, fixed in the mission's definition files. Points of Rd\mathbb{R}^dRd are Fin d → ℝ. Test functions are smooth and compactly supported, forming a submodule of all real-valued functions, and a distribution is a linear functional on that submodule; the pairing is extended by 000 to non-test functions, and a lemma in the definition file certifies that rescaling maps test functions to test functions, so no statement is vacuous for that reason. Hairer's Bs,0r\mathcal{B}^r_{s,0}Bs,0r​ consists of CrC^rCr functions; here it consists of smooth ones, which defines the same spaces Csα\mathcal{C}^\alpha_sCsα​. The model space is the algebraic direct sum ⨁a∈ATa\bigoplus_{a\in A} T_a⨁a∈A​Ta​ over the index set, each TaT_aTa​ a real normed space, with QaQ_aQa​ the corresponding projection; the structure group is a subgroup of the linear automorphisms of that direct sum. Sectors are families of subspaces Va⊆TaV_a \subseteq T_aVa​⊆Ta​; Hairer's requirement that each VaV_aVa​ admit a complement is automatic in this algebraic setting. The integer rrr appearing in the model bounds is the smallest one with ℓ>−r\ell > -rℓ>−r for all ℓ∈A\ell \in Aℓ∈A, which is part of the definition of a model rather than a free parameter. All statements quantify over an arbitrary regularity structure, an arbitrary model, and an arbitrary compact set, so they are not satisfiable by a degenerate choice; the goal in particular claims existence, membership in Csα\mathcal{C}^\alpha_sCsα​, and uniqueness simultaneously.

Infrastructure that a complete proof will need, and which is reusable beyond this mission: scaled wavelet bases on Rd\mathbb{R}^dRd, the elementary theory of Csα\mathcal{C}^\alpha_sCsα​ (including the positive-regularity case), and basic operations on compactly supported test functions under anisotropic rescaling. Contributions of any of these as separate lemmas are welcome, as are reductions that decompose the goal into wavelet-level estimates.

Selected references

  • M. Hairer, A theory of regularity structures, Inventiones Mathematicae 198 (2014) 269–504. arXiv:1303.5113, DOI:10.1007/s00222-014-0505-4
  • T. Lyons, Differential equations driven by rough signals, Revista Matemática Iberoamericana 14 (1998) 215–310. DOI:10.4171/RMI/240
  • M. Gubinelli, Controlling rough paths, Journal of Functional Analysis 216 (2004) 86–140. arXiv:math/0306433
  • M. Gubinelli, P. Imkeller, N. Perkowski, Paracontrolled distributions and singular PDEs, Forum of Mathematics Pi 3 (2015) e6. arXiv:1210.2684
  • Y. Bruned, M. Hairer, L. Zambotti, Algebraic renormalisation of regularity structures, Inventiones Mathematicae 215 (2019) 1039–1156. arXiv:1610.08468
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🏆Completed
CombinatoricsGraph Theory·Captain: burkh4rt

The Bunkbed Conjecture is FalseResearch Paper

Motivation

Let G=(V,E)G=(V,E)G=(V,E) be a finite connected graph. In Bernoulli bond percolation each edge is independently retained with probability PPP and deleted otherwise, and one writes PP[u↔v]\mathbb{P}_P[u \leftrightarrow v]PP​[u↔v] for the probability that vertices uuu and vvv lie in the same component of the resulting random subgraph. Comparing such connection probabilities is a basic and genuinely hard problem: computing them exactly is #P\#\mathsf{P}#P-hard.

The bunkbed graph is built from two copies of GGG, joined by vertical edges called posts above a chosen set T⊆VT \subseteq VT⊆V of transversal vertices. Percolation is performed on the two copies while every post is retained. Writing vvv for a vertex in the lower copy and v′v'v′ for its counterpart upstairs, Kasteleyn conjectured in 1985 that being connected within a level is always at least as likely as crossing between levels.

The conjecture is intuitively compelling — crossing levels appears to require "using up" a post — and it resisted proof for forty years. A short timeline:

  • 1985 — Kasteleyn formulates the conjecture; it is recorded as Remark 5 of van den Berg–Kahn (2001), which is how the source cites it.
  • Positive results accumulate for special cases: wheels, complete graphs, complete bipartite graphs, graphs symmetric with respect to an automorphism exchanging uuu and vvv, one or two transversal vertices, and in the P↑1P \uparrow 1P↑1 limit.
  • 2024 — Hollom refutes the 333-uniform hypergraph analogue. This alone does not settle the graph case: it is impossible to simulate a single 333-hyperedge by bond percolation on a gadget graph.
  • 2025 — Gladkov, Pak and Zimin disprove the conjecture outright, with an explicit counterexample and without computer assistance.

Section 7 of the source is a candid account of a large-scale machine-learning-guided search that failed to find a counterexample, and of why the problem is unusually ill-suited to experimental testing.

Setting

Fix a finite graph with vertex set VVV and edge set EEE, and a retention function w:E→[0,1]w : E \to [0,1]w:E→[0,1] (the uniform case is w≡Pw \equiv Pw≡P). A configuration is a subset S⊆ES \subseteq ES⊆E of open edges, occurring with probability

P(S)  =  ∏e∈Sw(e)∏e∈E∖S(1−w(e)),\mathbb{P}(S) \;=\; \prod_{e \in S} w(e) \prod_{e \in E \setminus S} \bigl(1 - w(e)\bigr),P(S)=e∈S∏​w(e)e∈E∖S∏​(1−w(e)),

and P[u↔v]\mathbb{P}[u \leftrightarrow v]P[u↔v] is the total probability of those SSS for which uuu and vvv are connected in (V,S)(V, S)(V,S).

Given T⊆VT \subseteq VT⊆V, the bunkbed graph has vertex set V×{0,1}V \times \{0,1\}V×{0,1}. Its edges are a copy of EEE in each level together with a post {(t,0),(t,1)}\{(t,0),(t,1)\}{(t,0),(t,1)} for every t∈Tt \in Tt∈T. In bunkbed percolation the two level-copies are percolated independently while all posts are retained; Pbb\mathbb{P}^{\mathrm{bb}}Pbb denotes the resulting connection probabilities.

Formalization targets

Goal — the bunkbed conjecture is false

¬  (∀ G connected, ∀ T⊆V, ∀ 0<P<1, ∀ u,v∈V:PPbb[u↔v]  ≥  PPbb[u↔v′])\neg\;\Bigl(\forall\,G \text{ connected},\ \forall\,T \subseteq V,\ \forall\,0<P<1,\ \forall\,u,v \in V:\quad \mathbb{P}^{\mathrm{bb}}_P[u \leftrightarrow v] \;\ge\; \mathbb{P}^{\mathrm{bb}}_P[u \leftrightarrow v'] \Bigr)¬(∀G connected, ∀T⊆V, ∀0<P<1, ∀u,v∈V:PPbb​[u↔v]≥PPbb​[u↔v′])

Supporting target — the explicit counterexample (Theorem 1.2)

∃ G, ∣V∣=7,222, ∣E∣=14,442, ∣T∣=3, ∃ u,v:P1/2bb[u↔v]  <  P1/2bb[u↔v′]\exists\, G,\ |V| = 7{,}222,\ |E| = 14{,}442,\ |T| = 3,\ \exists\, u,v:\qquad \mathbb{P}^{\mathrm{bb}}_{1/2}[u \leftrightarrow v] \;<\; \mathbb{P}^{\mathrm{bb}}_{1/2}[u \leftrightarrow v']∃G, ∣V∣=7,222, ∣E∣=14,442, ∣T∣=3, ∃u,v:P1/2bb​[u↔v]<P1/2bb​[u↔v′]

Supporting target — hyperedge simulation (Lemma 4.1)

For the gadget GnG_nGn​ on n+1n+1n+1 vertices,

Pabc Pa∣b∣c  −  Pab∣c Pac∣b  >  (n1−P1+P−1)Pa∣bc.P_{abc}\,P_{a|b|c} \;-\; P_{ab|c}\,P_{ac|b} \;>\; \Bigl(n\tfrac{1-P}{1+P} - 1\Bigr) P_{a|bc}.Pabc​Pa∣b∣c​−Pab∣c​Pac∣b​>(n1+P1−P​−1)Pa∣bc​.

Significance

The result itself. A forty-year-old conjecture in percolation theory is false, and prior positive results are thereby sharpened rather than superseded: it becomes interesting to delimit exactly which families of graphs do satisfy the inequality. The refutation also settles the Counting, Weighted, Alternative and Computational variants listed in §8.1, and shows the random-cluster analogue cannot be pushed from q=2q=2q=2 down to q=1q=1q=1.

Formalizing it. Nothing here is open; the mission produces machine-checked versions of published results, and as a by-product the first percolation theory in Lean. Mathlib currently contains no percolation of any kind — no connection probabilities, no bunkbed graph, no hypergraph percolation. That infrastructure is reusable far beyond this mission. The source itself notes (§8.2) that its central combinatorial lemma was independently verified by computer; a formal proof would replace that check with a certificate.

Difficulty

The obvious approach — exhibit a small graph and compute both probabilities — is hopeless, and the source explains why at length. A graph with mmm edges has 2m2^m2m configurations; for the counterexample here the probability gap is on the order of 10−433110^{-4331}10−4331, so no sampling argument can detect it, and exact enumeration is out of reach. Section 7 records a substantial computational search that found nothing and, in hindsight, could not have.

The proof is instead structural, and its difficulty is concentrated in one place. Hollom's refutation of the hypergraph version cannot be transferred directly, because a single 333-hyperedge cannot be simulated by bond percolation on any gadget graph. The source's answer is to prove a robust version of Hollom's lemma (Lemma 3.3) which survives the inexact simulation that gadget graphs do provide, and this robustness is what Lemma 4.1's inequality quantifies. Lemma 3.3 is proved by constructing a weight-preserving involution on a refined configuration space — the technical heart, and the milestone a solver should expect to spend the most effort on.

Formalization scope

The development commits to the following conventions.

  • Everything is finite and rational-valued, hence computable: connection probabilities are ℚ and evaluate by #eval, and small instances close by decide.
  • A graph is given by an explicit edge Finset and realised through SimpleGraph.fromEdgeSet; connectivity is Mathlib's SimpleGraph.Reachable.
  • Percolation is a sum over the powerset of the edge set, weighted as displayed above, of a reachability indicator. Edge weights are per-edge (Sym2 V → ℚ), since the gadget GnG_nGn​ genuinely needs two different weights: its spokes are retained with probability 1−P1-P1−P and its path edges with probability PPP.
  • In the bunkbed, level 0 is the lower copy; posts over T are unconditionally present and are not percolated. The two levels are percolated independently.
  • ⚠️ Planarity is omitted from the goal. Theorem 1.2 asserts the counterexample is planar, and Mathlib has no notion of a planar graph — no IsPlanar, no Euler formula, no Kuratowski. Building one is a larger project than this mission. The formalized statement of Theorem 1.2 is therefore strictly weaker than the published one, and the goal is instead the negation of the conjecture, which is exactly the source's own "In particular, the BBC is false." Contributions adding planarity are welcome and would strengthen the milestone.
  • Ruling out a trivializing reading: the conjecture must be negated as stated, over all connected graphs, transversal sets and 0<P<10<P<10<P<1. Weakening it to a fixed graph, or to P∈{0,1}P \in \{0,1\}P∈{0,1}, or dropping connectivity, would make the refutation vacuous.

Infrastructure. Mathlib supplies SimpleGraph, boxProd, Reachable with a DecidableRel instance, fromEdgeSet, edgeFinset and Finset.powerset. It supplies no percolation, so this mission ships two definition files: Bernoulli bond percolation with the bunkbed construction and the five triple-partition probabilities, and hypergraph percolation with Hollom's hypergraph and the Wierman–Ziff five-state model. One known gap: Mathlib's Reachable decision procedure enumerates walks and is far too slow to evaluate the 646464-configuration check of Lemma 3.1 by decide. A solver will want a linear-time reachability procedure together with a proof that it agrees with Reachable; that is itself a worthwhile reusable contribution.

Selected references

  • J. van den Berg and J. Kahn, A correlation inequality for connection events in percolation, Ann. Probab. 29 (2001), 123–126 — Kasteleyn's conjecture appears as Remark 5.
  • T. Hollom, A new proof of the bunkbed conjecture in the p↑1p \uparrow 1p↑1 limit, Discrete Math. 347 (2024), 113711.
  • T. Hollom, The bunkbed conjecture is not robust to generalisation, arXiv:2406.01790 (2024).
  • T. Hutchcroft, P. Nizić-Nikolac, A. Kent, The bunkbed conjecture holds in the p↑1p \uparrow 1p↑1 limit, Comb. Probab. Comput. 32 (2023), 363–369.
  • N. Gladkov, I. Pak, A. Zimin, The bunkbed conjecture is false, Proc. Natl. Acad. Sci. USA 122 (2025), no. 24, e2420725122. doi:10.1073/pnas.2420725122; preprint arXiv:2410.02545.
  • J. C. Wierman and R. M. Ziff, Self-dual planar hypergraphs and exact bond percolation thresholds, Electron. J. Combin. 18 (2011).
  • G. R. Grimmett, Percolation, 2nd ed., Springer, 1999.
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Machine Learning·Captain: naimengye

Speculative Actions: Cost-Latency Analysis for Agentic SpeculationResearch Paper

Motivation

An LLM agent acting in an environment spends most of its wall-clock time waiting. Each step — a model call, a tool or MCP request, a browser action, sometimes a human reply — must complete before the next can be issued, and the round trips dominate end-to-end latency: a chess game between two reasoning agents runs for hours, and an operating-system tuning task for tens of minutes. When a training or prompt-optimization loop repeats such a run thousands of times, the waiting is the cost.

Speculative actions (Ye, Ahuja, Liargkovas, Lu, Kaffes, Peng, ICLR 2026) transplants a classical systems idea — speculative execution in microprocessors, and speculative decoding for LLM inference — to the agent's environment loop. A cheap, fast speculator guesses the action a slow, authoritative actor is about to produce, the guess is used to launch the next environment call early, and the work is committed only when the actor's real action confirms the guess. The interface stays sequential and lossless; the internals run in parallel.

What makes this a formalization target rather than an engineering report is the paper's §5 cost–latency analysis. Speculating more branches buys hit probability but costs tokens, and the paper derives closed-form expressions for both sides of that trade — a self-contained piece of applied probability sitting underneath a systems paper. This mission asks for those expressions, machine-checked.

Setting

Fix a horizon TTT and index steps t=0,1,…,T−1t = 0, 1, \dots, T-1t=0,1,…,T−1. At each step a policy maps the state to an API call; the actor executes it with latency Exp(β)\mathrm{Exp}(\beta)Exp(β), while the speculator proposes candidate actions with latency Exp(α)\mathrm{Exp}(\alpha)Exp(α), where β<α\beta < \alphaβ<α (the speculator is faster in expectation). A speculative branch hits when the action it guesses implies the same next call the actor's true action would have implied; branches hit independently across steps with probability ppp.

Two knobs define the two regimes analyzed. Breadth kkk: at each step, launch kkk independent one-step speculations in parallel, each immediately followed by a real call. At least one of the kkk succeeds with probability

p(k)  =  1−(1−p)k.p(k) \;=\; 1 - (1-p)^k .p(k)=1−(1−p)k.

Depth: follow a single branch, extending it whenever a speculative or real call returns and pruning subtrees the actor contradicts.

The quantity driving both results is SnS_nSn​, the expected number of hits by round nnn. A hit consumes the following step's speculation window — after a correct guess the next call is already cached, so no new speculation is launched there — which yields the two-term recursion

S0=0,S1=p,Sn=p (1+Sn−2)+(1−p) Sn−1.S_0 = 0, \qquad S_1 = p, \qquad S_n = p\,(1 + S_{n-2}) + (1-p)\,S_{n-1}.S0​=0,S1​=p,Sn​=p(1+Sn−2​)+(1−p)Sn−1​.

Write Tseq,MseqT_{\mathrm{seq}}, M_{\mathrm{seq}}Tseq​,Mseq​ for the latency and token cost of strictly sequential execution, and Tspec,MspecT_{\mathrm{spec}}, M_{\mathrm{spec}}Tspec​,Mspec​ for their speculative counterparts. In the depth regime latencies are taken deterministic: aaa for a real call, b<ab < ab<a for a speculative one.

Target

The goal theorem is the finite-horizon latency ratio for breadth-focused speculation (Proposition 1), with p(k)p(k)p(k) abbreviated pkp_kpk​:

E[Tspec]E[Tseq]=1−1T αα+β[(T−1)pk1+pk+pk2(1+pk)2−pk2(1+pk)2(−pk)T−1].\frac{\mathbb{E}[T_{\mathrm{spec}}]}{\mathbb{E}[T_{\mathrm{seq}}]} = 1 - \frac{1}{T}\,\frac{\alpha}{\alpha+\beta} \left[\frac{(T-1)p_k}{1+p_k} + \frac{p_k^2}{(1+p_k)^2} - \frac{p_k^2}{(1+p_k)^2}(-p_k)^{T-1}\right].E[Tseq​]E[Tspec​]​=1−T1​α+βα​[1+pk​(T−1)pk​​+(1+pk​)2pk2​​−(1+pk​)2pk2​​(−pk​)T−1].

The supporting targets, ordered as the analysis builds them:

  1. the closed form Sn=p1+pn+p2(1+p)2(1−(−p)n)S_n = \frac{p}{1+p}n + \frac{p^2}{(1+p)^2}\bigl(1 - (-p)^n\bigr)Sn​=1+pp​n+(1+p)2p2​(1−(−p)n) solving the recursion;
  2. the per-hit saving E[(B−A)+]=αβ(α+β)\mathbb{E}[(B-A)^+] = \frac{\alpha}{\beta(\alpha+\beta)}E[(B−A)+]=β(α+β)α​ for independent A∼Exp(α)A \sim \mathrm{Exp}(\alpha)A∼Exp(α), B∼Exp(β)B \sim \mathrm{Exp}(\beta)B∼Exp(β);
  3. the T→∞T \to \inftyT→∞ limit 1−pk1+pk⋅αα+β1 - \frac{p_k}{1+p_k}\cdot\frac{\alpha}{\alpha+\beta}1−1+pk​pk​​⋅α+βα​, and the resulting 50% ceiling: the latency reduction is strictly below 12\tfrac1221​ for every pk≤1p_k \le 1pk​≤1;
  4. the cost counterpart (Theorem 4), finite-horizon and in the limit, with k~\tilde kk~ the number of distinct actions across the kkk branches;
  5. the depth-focused time and cost identities (Theorem 6), whose latency coefficient is ppp rather than p1+p\frac{p}{1+p}1+pp​ — raising the speedup ceiling from 12\tfrac1221​ to 111;
  6. the structure of confidence-aware selective speculation (Theorem 3 and Corollary 5): with sorted per-branch confidences, the marginal hit-probability gain is non-increasing, so the optimal breadth is the greedy threshold rule "add a branch while Δ⋆δq(m)≥c\Delta^\star \delta q(m) \ge cΔ⋆δq(m)≥c".

Significance

The analysis is what turns speculation from a trick into a tunable system. Proposition 1 and Theorem 4 are governed by the same quantity pkp_kpk​, so a practitioner who can estimate hit probability can choose kkk offline against a latency/cost budget rather than by trial. The 50% ceiling is a genuine negative result — it says breadth alone cannot do better, and motivates the depth regime, where the ceiling becomes 1. Theorem 3 explains why confidence-based branch selection is cheap in practice: the whole dynamic program collapses to one scalar continuation value, so a runtime system sorts confidences and adds branches greedily in O(k)O(k)O(k) per step.

The paper's proofs are pen-and-paper and, as far as we are aware, none of these results has a machine-checked proof. Three parts reward formalization specifically. The recursion's closed form is derived by a characteristic-equation argument with a particular solution that collides with the homogeneous part — routine but error-prone. The per-hit saving is an honest two-dimensional integral over independent exponentials. And Theorem 6's cost expression is stated in the paper with a floor function and then immediately replaced by an approximation, so formalizing it forces a decision about which claim is actually being asserted (see Formalization scope).

Difficulty

The obvious first move on the recursion — guess a constant particular solution — fails, because r=1r = 1r=1 is a root of the characteristic polynomial r2−(1−p)r−pr^2 - (1-p)r - pr2−(1−p)r−p and a constant trial collides with the homogeneous family; the particular solution is linear in nnn, and the p2(1+p)2\frac{p^2}{(1+p)^2}(1+p)2p2​ coefficient comes out of matching both initial conditions, not one.

The interesting hypothesis is the one the recursion's shape encodes and the prose states only in passing: a hit at round ttt removes the speculation window at round t+1t+1t+1. Drop it and the recursion becomes one-term and the answer changes.

For the per-hit saving, the difficulty is analytic rather than algebraic: the inner antiderivative of (b−a)αe−αa(b-a)\alpha e^{-\alpha a}(b−a)αe−αa must be handled, and the outer integral runs over an unbounded interval, so integrability has to be established rather than assumed.

The asymptotic statements need the oscillating term (−pk)T−1(-p_k)^{T-1}(−pk​)T−1 controlled uniformly — it is bounded, not vanishing termwise in an obvious way — before the 1T\tfrac1TT1​ prefactor can be taken to zero.

Formalization scope

Everything is over R\mathbb{R}R. The model lives in one definition bundle, Def_SpecActions_model, in namespace SpecActions; the mission's Lean names match the prose symbols (SnS_nSn​ is hits, p(k)p(k)p(k) is phit, k~\tilde kk~ is kt).

The model is formalized at the level the paper's own proofs use: E[T]\mathbb{E}[T]E[T] and E[M]\mathbb{E}[M]E[M] are defined by the expressions Appendix A derives for them (specTime, specCost, and their depth analogues), and the theorems assert the algebraic and asymptotic identities relating those quantities. Deriving those expressions from a measure-theoretic model of the execution trace is deliberately not in scope — with one exception: milestone 2 states the per-hit saving as a genuine iterated integral against the exponential densities, so the one probabilistic step the paper actually computes is formalized as an integral rather than assumed.

Conventions a solver should know before starting:

  • Statements are quantified over α,β>0\alpha, \beta > 0α,β>0 and 0≤pk≤10 \le p_k \le 10≤pk​≤1; the standing assumption β<α\beta < \alphaβ<α is not imposed, since none of the identities need it.
  • Finite-horizon statements carry 1≤T1 \le T1≤T, and T−1T-1T−1 is natural-number subtraction — the T=0T = 0T=0 case is excluded rather than silently truncated.
  • hits takes pkp_kpk​ (the per-step hit probability p(k)p(k)p(k)), not the per-branch ppp; phit relates the two, and Thm_SpecActions_phit_bounds supplies the 0≤p(k)≤10 \le p(k) \le 10≤p(k)≤1 range facts the other statements assume.
  • Theorem 6's cost is stated as the exact identity, not the paper's approximation. The paper gives an exact expression involving ⌊a/b⌋\lfloor a/b \rfloor⌊a/b⌋ and then an ≈\approx≈ form with a2b−12\frac{a}{2b} - \frac122ba​−21​; these coincide only when a/ba/ba/b is an integer. The milestone asserts the exact floor version, which is what the proof establishes.
  • The 50% ceiling is stated as the strict bound pk1+pk⋅αα+β<12\frac{p_k}{1+p_k}\cdot\frac{\alpha}{\alpha+\beta} < \frac121+pk​pk​​⋅α+βα​<21​, which holds for all admissible parameters; the paper's "upper bound of 50%, occurring when p=1p=1p=1 and α=∞\alpha = \inftyα=∞" describes an unattained supremum.
  • Theorem 3's dynamic program is formalized as the two facts that carry its content — diminishing marginal returns, and optimality of the greedy threshold breadth — rather than as a Bellman recursion over a mode process, which would require a full MDP development.

Reusable beyond this mission: the two-term linear recursion solved in milestone 1, and the E[(B−A)+]\mathbb{E}[(B-A)^+]E[(B−A)+] computation for independent exponentials, which is a standard fact absent from Mathlib. Contributions extending the model toward an actual measure on execution traces — deriving specTime rather than defining it — are welcome as follow-on work.

Selected references

  • Naimeng Ye, Arnav Ahuja, Georgios Liargkovas, Yunan Lu, Kostis Kaffes, Tianyi Peng. Speculative Actions: A Lossless Framework for Faster Agentic Systems. ICLR 2026. arXiv:2510.04371 — Proposition 1 (p. 4), Appendix A (pp. 13–14), Theorem 3 (p. 10), Theorem 4 (p. 19), Corollary 5 (p. 22), Theorem 6 (p. 23).
  • Yaniv Leviathan, Matan Kalman, Yossi Matias. Fast Inference from Transformers via Speculative Decoding. ICML 2023. arXiv:2211.17192 — the speculate-verify pattern at token level.
  • Wenyue Hua, Mengting Wan, Shashank Vadrevu, Ryan Nadel, Yongfeng Zhang, Chi Wang. Interactive Speculative Planning. 2024. arXiv:2410.00079 — depth-oriented speculation on a single planning branch.
  • Yilin Guan et al. Dynamic Speculative Agent Planning. 2025. arXiv:2509.01920 — online RL for choosing speculation depth under a cost-latency trade-off.
  • Robert M. Tomasulo. An Efficient Algorithm for Exploiting Multiple Arithmetic Units. IBM Journal of Research and Development, 1967. DOI:10.1147/rd.111.0025 — speculative execution in hardware.
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Optimization·Captain: viratkota

Kelly's Criterion: the optimal fraction for an even-money betResearch Paper

Motivation

In 1956 Kelly answered a question that looks like gambling and is really about information: if a channel gives you a noisy advance signal about a sequence of bets, how much is that signal worth? His answer was that the maximum exponential rate of growth of a gambler's capital equals the rate of transmission over the channel -- so information rate and capital growth rate are the same quantity in different units. The betting fraction that achieves it is now called the Kelly criterion, and it is the basis of a large practical literature on position sizing.

The result is short, entirely explicit, and has no analytic subtleties -- which makes it a good formalization target and a surprising gap: the platform currently has fifteen missions on bandit algorithms and none on optimal growth.

Setting

This mission formalizes the simplest case of Kelly's Section 4: an even-money bet with no track take, won independently with probability p and lost with probability q = 1 - p. A gambler stakes a fixed fraction l of current wealth on each bet, so wealth is multiplied by 1 + l on a win and 1 - l on a loss. The exponential rate of growth is

G(l)=plog⁡(1+l)+qlog⁡(1−l).G(l) = p \log(1+l) + q \log(1-l).G(l)=plog(1+l)+qlog(1−l).

Kelly shows this is maximised at l = p - q, with maximum value 1 + p log p + q log q in bits. We state G in nats (natural logarithm), so the maximum carries an additive log 2; dividing by log 2 recovers Kelly's bit-valued form, which is exactly 1 - H(p) for the binary entropy H. The maximiser is unaffected by the choice of base.

What is being asked

The goal theorem is that l = 2p - 1 maximises G over the admissible range (-1, 1) when the bet is favourable (p > 1/2). Milestones supply the maximum value (Kelly's information-rate identity), the admissibility of the maximiser, and the concavity that makes the first-order condition sufficient.

Source

J. L. Kelly Jr., A New Interpretation of Information Rate, Bell System Technical Journal 35 (1956) 917-926, Section 4 ("the simplest case"). The growth-rate expression and the maximiser l = p - q are stated there; the maximum value in bits is Kelly's eq. for G_max.

The identity and maximiser were checked numerically before drafting: for p = 0.55, 0.6, 0.7, 0.9 the claimed maximum matches log 2 + p log p + q log q to six decimals, and a grid search over (-1, 1) at 1e-5 resolution returns 2p - 1 in every case.

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