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High-Dimensional Probability and Statistics

Vershynin's High-Dimensional Probability and Wainwright's High-Dimensional Statistics: concentration, random matrices, and sparse recovery.

25 missions

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Machine LearningProbabilityStatistics·Captain: mikedeng1

High-Dimensional Statistics XII: An Oracle Inequality for Nonparametric Least SquaresTextbook

Motivation

Regression is usually taught with a fixed parametric model: linear regression fits a ddd-dimensional coefficient vector, and the estimation error is controlled by d/nd/nd/n. Many regression problems in practice have no such finite-dimensional description — the regressor is only known to be, say, convex, monotone, or smooth, and the estimator is a least-squares fit over the (infinite-dimensional) set of functions with that shape. This is nonparametric regression, and the basic question is the same as in the parametric case: how close is the fitted function to the truth, as a function of the sample size nnn? Answering it requires replacing "dimension" with a genuinely functional notion of complexity, since an infinite- dimensional function class can still be small enough to estimate well (a Sobolev ball) or too large to estimate at all. The theory in this mission, due to van de Geer and developed in Chapter 13 of Wainwright (High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019), gives a single non-asymptotic template — the localized Gaussian complexity — that answers this question for an arbitrary star-shaped function class, and recovers the familiar parametric and Sobolev/RKHS rates as special cases.

Setting

Fix nnn design points x1,…,xnx_1,\dots,x_nx1​,…,xn​ in an arbitrary covariate space X\mathcal XX (fixed, not random — this is the fixed-design setting) and observe

yi=f∗(xi)+σwi,i=1,…,n,y_i = f^*(x_i) + \sigma w_i, \qquad i = 1,\dots,n,yi​=f∗(xi​)+σwi​,i=1,…,n,

where f∗f^*f∗ is the unknown regression function, σ>0\sigma > 0σ>0 is a known noise level, and w1,…,wnw_1,\dots,w_nw1​,…,wn​ are i.i.d. standard Gaussian. Given a class FFF of candidate functions, the nonparametric least-squares estimate is any minimizer

f^n∈arg⁡min⁡f∈F 1n∑i=1n(yi−f(xi))2.\hat f_n \in \arg\min_{f\in F}\ \frac1n\sum_{i=1}^n \big(y_i - f(x_i)\big)^2.f^​n​∈argf∈Fmin​ n1​i=1∑n​(yi​−f(xi​))2.

Error is measured in the empirical (design-dependent) seminorm ∥g∥n2:=1n∑i=1ng(xi)2\|g\|_n^2 := \frac1n\sum_{i=1}^n g(x_i)^2∥g∥n2​:=n1​∑i=1n​g(xi​)2. A class HHH of functions is star-shaped if h∈Hh\in Hh∈H and α∈[0,1]\alpha\in[0,1]α∈[0,1] together imply αh∈H\alpha h \in Hαh∈H — every convex class containing the origin has this property, and it is the minimal structural assumption under which the theory below applies. For a star-shaped class HHH and radius δ>0\delta>0δ>0, the local Gaussian complexity

Gn(δ;H):=Ew[ sup⁡h∈H, ∥h∥n≤δ ∣1n∑i=1nwih(xi)∣ ]G_n(\delta; H) := \mathbb E_w\Big[\ \sup_{h\in H,\ \|h\|_n\le\delta}\ \Big|\tfrac1n \sum_{i=1}^n w_i h(x_i)\Big|\ \Big]Gn​(δ;H):=Ew​[ h∈H, ∥h∥n​≤δsup​ ​n1​i=1∑n​wi​h(xi​)​ ]

measures how much a mean-zero Gaussian process can be made to look like a member of HHH restricted to the ball of radius δ\deltaδ. A critical radius δn\delta_nδn​ is any positive solution of Gn(δ;H)/δ≤δ/(2σ)G_n(\delta;H)/\delta \le \delta/(2\sigma)Gn​(δ;H)/δ≤δ/(2σ); by Lemma 13.6, δ↦Gn(δ;H)/δ\delta\mapsto G_n(\delta;H)/\deltaδ↦Gn​(δ;H)/δ is non-increasing on HHH star-shaped, so this inequality always has a smallest positive solution.

Formalization targets

Lemma 13.6. For any star-shaped HHH, δ↦Gn(δ;H)/δ\delta \mapsto G_n(\delta;H)/\deltaδ↦Gn​(δ;H)/δ is non-increasing on (0,∞)(0,\infty)(0,∞), and consequently Gn(δ;H)/δ≤cδG_n(\delta;H)/\delta \le c\deltaGn​(δ;H)/δ≤cδ has a smallest positive solution for every c>0c>0c>0.

Theorem 13.5 (special case, f∗∈Ff^*\in Ff∗∈F).

P[∥f^n−f∗∥n2≥16 tδn]≤e−ntδn/(2σ2)for all t≥δn.\mathbb P\big[\|\hat f_n - f^*\|_n^2 \ge 16\,t\delta_n\big] \le e^{-nt\delta_n/(2\sigma^2)} \qquad \text{for all } t \ge \delta_n.P[∥f^​n​−f∗∥n2​≥16tδn​]≤e−ntδn​/(2σ2)for all t≥δn​.

Theorem 13.13 (goal — general oracle inequality, f∗f^*f∗ not assumed in FFF). With δn\delta_nδn​ solving the critical inequality for ∂F:=F−F\partial F := F - F∂F:=F−F, there are universal constants (c0,c1,c2)(c_0,c_1,c_2)(c0​,c1​,c2​) such that for all t≥δnt\ge\delta_nt≥δn​,

∥f^n−f∗∥n2≤inf⁡γ∈(0,1)[1+γ1−γ∥f−f∗∥n2+c0γ(1−γ)tδn]for all f∈F,\|\hat f_n-f^*\|_n^2 \le \inf_{\gamma\in(0,1)}\left[\frac{1+\gamma}{1-\gamma}\|f-f^*\|_n^2 +\frac{c_0}{\gamma(1-\gamma)}t\delta_n\right]\quad\text{for all }f\in F,∥f^​n​−f∗∥n2​≤γ∈(0,1)inf​[1−γ1+γ​∥f−f∗∥n2​+γ(1−γ)c0​​tδn​]for all f∈F,

with probability at least 1−c1e−c2ntδn/σ21-c_1e^{-c_2nt\delta_n/\sigma^2}1−c1​e−c2​ntδn​/σ2. The goal is deliberately the statement with unresolved universal constants and an infimum over γ\gammaγ, rather than any single instantiated bound, so the target survives sharper constant tracking.

Significance

Theorem 13.13 is the "master" result behind essentially every concrete rate in the chapter: orthogonal series regression, convex/monotone regression, and (via the KRR specialization of Section 13.4) kernel ridge regression rates for Sobolev and Gaussian-kernel classes are all obtained by bounding GnG_nGn​ for a particular FFF and reading off δn\delta_nδn​. Its value is that it isolates exactly the one place where the geometry of FFF enters — the local Gaussian complexity — while the probabilistic argument (a peeling/chaining argument controlling a localized empirical process) is generic. Formalizing it produces, for the first time on the platform, the statement-level infrastructure (star-shaped classes, local Gaussian complexity, critical radius) that any future mission on a concrete nonparametric-regression rate — kernel ridge regression, convex regression, isotonic regression — can specialize, without re-deriving the oracle inequality from scratch. The proof itself (concentration of Gaussian complexity via Borell-TIS/Gaussian comparison plus a peeling argument over dyadic scales) is not attempted here; only the statement is formalized, as a draft goal for future proof contributions.

Difficulty

The naive route to Theorem 13.13 is to bound ∥f^n−f∗∥n\|\hat f_n - f^*\|_n∥f^​n​−f∗∥n​ pointwise via the basic inequality 12∥f^n−f∗∥n2≤σn∑iwi(f^n(xi)−f∗(xi))\tfrac12\|\hat f_n-f^*\|_n^2 \le \tfrac{\sigma}{n}\sum_i w_i(\hat f_n(x_i)-f^*(x_i))21​∥f^​n​−f∗∥n2​≤nσ​∑i​wi​(f^​n​(xi​)−f∗(xi​)) and then bound the right side by σ Gn(δ;∂F)\sigma\,G_n(\delta;\partial F)σGn​(δ;∂F) for δ=∥f^n−f∗∥n\delta = \|\hat f_n-f^*\|_nδ=∥f^​n​−f∗∥n​ — but δ\deltaδ is itself random (it depends on the estimate), so this is circular: the bound on the right depends on the very quantity being bounded. The chapter's actual argument resolves this with a peeling device: partition the event space by which dyadic annulus ∥f^n−f∗∥n\|\hat f_n-f^*\|_n∥f^​n​−f∗∥n​ falls into, and apply a uniform (non-circular) bound on each annulus separately via Gaussian concentration, summing a geometric series of tail probabilities. This is the step every first attempt misses, and it is why the local Gaussian complexity — rather than the simpler global complexity of Chapter 4/5 — is the right object: localizing to radius δ\deltaδ is what makes the per-annulus bound tight enough for the final sum to converge.

Formalization scope

Design points are an arbitrary type X (no topology or metric structure is needed for the statements themselves); the least-squares estimate is represented as a Prop (IsLeastSquaresEstimate) picking out any function achieving the empirical minimum, matching the book's "any minimizer" phrasing rather than assuming uniqueness. The local Gaussian complexity is defined as an expectation over an explicit i.i.d.-standard-Gaussian noise vector on an abstract probability space, with the inner supremum taken over the subtype of the radius-restricted slice of the class — this is well-defined (not the junk value 0 of an unbounded Set ℝ supremum) whenever the slice is nonempty, which holds automatically for any nonempty star-shaped class (taking α=0\alpha=0α=0 exhibits 000 in the class). Since neither X nor H carries a topology, separability or countability constraint, SatisfiesCriticalInequality adds an explicit Integrable hypothesis on that same supremum (added in revision), guarding against Mathlib's Bochner integral silently returning the junk value 0 for a non-measurable integrand — a value that would otherwise trivially satisfy the critical inequality for every positive δ, regardless of the function class's actual local complexity. The trivializing formalization to rule out here is stating Theorem 13.13's universal constants after the quantification over the function class and sample size, which would let (c0,c1,c2)(c_0,c_1,c_2)(c0​,c1​,c2​) secretly depend on the instance and make the "universal" claim vacuous; this mission places the constant quantifiers first, before the class, design and noise data they must not depend on. A complete downstream development would add: the concentration-of-Gaussian-complexity step (Borell–TIS or a comparable tail bound), the peeling argument, and the metric-entropy / Dudley-integral machinery of Section 13.2.1 for bounding GnG_nGn​ explicitly on concrete classes (Sobolev balls, RKHS balls) — none of which is attempted here.

Selected references

  • M. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019, Chapter 13. https://doi.org/10.1017/9781108627771
  • S. van de Geer, Empirical Processes in M-Estimation, Cambridge University Press, 2000.
  • S. van de Geer, "Estimating a regression function," Annals of Statistics, 18(2):907-924, 1990. https://doi.org/10.1214/aos/1176347627
5 thms3 active usersReviewed
Machine LearningProbabilityStatistics·Captain: mikedeng1

High-Dimensional Statistics XIII: A Localized Uniform LawTextbook

Motivation

Every consistency guarantee for an empirical-risk-minimization procedure — the Lasso, kernel ridge regression, maximum likelihood — ultimately rests on relating an empirical average to its population expectation, uniformly over the class of candidate functions or parameters being searched. Chapter 4 established the classical form of this connection: a uniform law of large numbers, bounding sup⁡f∈F∣∥f∥n2−∥f∥22∣\sup_{f\in F}|\|f\|_n^2-\|f\|_2^2|supf∈F​∣∥f∥n2​−∥f∥22​∣ by an absolute quantity governed by the (unlocalized) complexity of FFF. Such a bound is often wasteful: it treats a function with small population norm the same as one with large population norm, when intuitively the empirical and population norms of a small function should already agree closely. This mission formalizes the sharper, localized form of this uniform law — the same localization principle Chapter 13 used for nonparametric least squares, now applied directly to the empirical-versus-population norm comparison itself, giving relative rather than absolute control and recovering optimal convergence rates that the unlocalized theory misses.

Setting

Fix a probability distribution PPP over a covariate space XXX and nnn i.i.d. samples x1,…,xn∼Px_1,\dots,x_n\sim Px1​,…,xn​∼P. For f:X→Rf:X\to\mathbb Rf:X→R, the population norm is ∥f∥22:=∫Xf(x)2 P(dx)\|f\|_2^2:=\int_Xf(x)^2\,P(dx)∥f∥22​:=∫X​f(x)2P(dx) and the empirical norm is ∥f∥n2:=1n∑i=1nf(xi)2\|f\|_n^2:=\frac1n\sum_{i=1}^nf(x_i)^2∥f∥n2​:=n1​∑i=1n​f(xi​)2; by linearity of expectation, E[∥f∥n2]=∥f∥22\mathbb E[\|f\|_n^2]=\|f\|_2^2E[∥f∥n2​]=∥f∥22​, so the question is how tightly ∥f∥n2\|f\|_n^2∥f∥n2​ concentrates around ∥f∥22\|f\|_2^2∥f∥22​, uniformly over a function class FFF. A class FFF is star-shaped around the origin if f∈F,α∈[0,1]  ⟹  αf∈Ff\in F,\alpha\in[0,1]\implies\alpha f\in Ff∈F,α∈[0,1]⟹αf∈F, and bbb-uniformly bounded if ∥f∥∞≤b\|f\|_\infty\le b∥f∥∞​≤b for every f∈Ff\in Ff∈F. The relevant complexity measure is the population localized Rademacher complexity

Rn(δ;F):=Eε,x[ sup⁡f∈F, ∥f∥2≤δ ∣1n∑i=1nεif(xi)∣ ],R_n(\delta;F) := \mathbb E_{\varepsilon,x}\Big[\ \sup_{f\in F,\ \|f\|_2\le\delta}\ \Big| \tfrac1n\sum_{i=1}^n\varepsilon_if(x_i)\Big|\ \Big],Rn​(δ;F):=Eε,x​[ f∈F, ∥f∥2​≤δsup​ ​n1​i=1∑n​εi​f(xi​)​ ],

where ε1,…,εn\varepsilon_1,\dots,\varepsilon_nε1​,…,εn​ are i.i.d. Rademacher signs independent of the samples — note that, unlike Chapter 13's Gaussian complexity for fixed design points, this expectation integrates out the randomness of the samples themselves, since this chapter treats {xi}\{x_i\}{xi​} as genuinely random throughout. A critical radius δn\delta_nδn​ is any positive solution of Rn(δ;F)≤δ2/bR_n(\delta;F)\le\delta^2/bRn​(δ;F)≤δ2/b.

Formalization targets

Theorem 14.1 (goal). Given FFF star-shaped and bbb-uniformly bounded, and δn\delta_nδn​ solving the critical inequality, for any t≥δnt\ge\delta_nt≥δn​,

∣∥f∥n2−∥f∥22∣≤12∥f∥22+t22for all f∈F,\Big|\|f\|_n^2-\|f\|_2^2\Big|\le\frac12\|f\|_2^2+\frac{t^2}2 \qquad\text{for all }f\in F,​∥f∥n2​−∥f∥22​​≤21​∥f∥22​+2t2​for all f∈F,

with probability at least 1−c1e−c2nt2/b21-c_1e^{-c_2nt^2/b^2}1−c1​e−c2​nt2/b2; and if additionally nδn2≥2c2log⁡(4log⁡(1/δn))n\delta_n^2\ge\frac2{c_2}\log(4\log(1/\delta_n))nδn2​≥c2​2​log(4log(1/δn​)),

∣∥f∥n−∥f∥2∣≤c0δnfor all f∈F,\big|\|f\|_n-\|f\|_2\big|\le c_0\delta_n \qquad\text{for all }f\in F,​∥f∥n​−∥f∥2​​≤c0​δn​for all f∈F,

with probability at least 1−c1′e−c2′nδn2/b21-c_1'e^{-c_2'n\delta_n^2/b^2}1−c1′​e−c2′​nδn2​/b2.

Significance

Theorem 14.1 is the technical engine behind two of the book's other sharp results: Example 14.2's derivation of the optimal n−1/2n^{-1/2}n−1/2 rate for bounded quadratic function classes (where the unlocalized analogue of this theorem only achieves the slower n−1/4n^{-1/4}n−1/4 rate), and, more broadly, every later argument in the book that needs to translate an empirical-norm guarantee (as produced directly by an M-estimator's optimality, e.g. Chapter 13's nonparametric least-squares bounds) into a population-norm guarantee, or vice versa. The gap between the "absolute" uniform law of Chapter 4 and the "relative" one here is exactly the difference between a bound that is only informative for functions of order-one population norm, and one that remains sharp arbitrarily close to the origin — which is precisely where a consistent estimator's error eventually lives. Formalizing the statement produces, for the first time on the platform, the localized-Rademacher-complexity vocabulary at the population level (as opposed to Chapter 13's fixed-design Gaussian-complexity version), reusable by any future mission needing to pass between empirical and population norms.

Difficulty

The naive approach — apply Hoeffding's inequality to ∣∥f∥n2−∥f∥22∣|\|f\|_n^2-\|f\|_2^2|∣∥f∥n2​−∥f∥22​∣ for a fixed fff, then union-bound (or apply the unlocalized Rademacher-complexity uniform law of Chapter 4) over FFF — gives a bound whose complexity term does not shrink as ∥f∥2→0\|f\|_2\to0∥f∥2​→0, since it uses the complexity of all of FFF regardless of a given function's own size. This is exactly the sub-optimality Example 14.2 exhibits concretely: the naive bound gives rate n−1/4n^{-1/4}n−1/4 where the truth is n−1/2n^{-1/2}n−1/2. The fix is not merely technical bookkeeping — it requires a genuine peeling argument over dyadic norm-scales (exactly as in Chapter 13's proof of Theorem 13.13), applying the localized complexity Rn(δ;F)R_n(\delta;F)Rn​(δ;F) at the scale δ=∥f∥2\delta=\|f\|_2δ=∥f∥2​ appropriate to each individual fff, and controlling the resulting geometric sum of tail probabilities across scales. A reader's first instinct — bound ∥f∥2\|f\|_2∥f∥2​ in terms of ∥f∥n\|f\|_n∥f∥n​ and substitute — is circular, since ∥f∥n\|f\|_n∥f∥n​ is itself the random quantity being controlled.

Formalization scope

The covariate space X carries an arbitrary MeasurableSpace structure (no topology needed for the statement); the sample sequence and the Rademacher signs are both represented as families of measurable functions on a shared probability space Ω, with their joint independence stated as a single IndepFun between the two vector-valued sequences (rather than building a combined-index iIndepFun), since it is the two sequences — not each pair of individual variables — whose independence the book invokes. The two conclusions of Theorem 14.1 are stated as a conjunction with the second gated behind its own extra hypothesis, never collapsed into a single implication, since the book's own statement keeps them syntactically and logically distinct (the second requires a strictly stronger and additional condition on top of the first's). The universal constants (c1,c2,c0,c1',c2') are quantified before every instance object, so they cannot secretly depend on the function class, sample size, or radius. Every f ∈ F is required measurable (hF_meas, added in revision): the book's own framing implicitly restricts to measurable, square-integrable f throughout (p. 454), and without this hypothesis the population norm popNormSq, which appears directly in the goal's conclusion, could silently take Mathlib's Bochner-integral junk value 0 for a non-measurable, pointwise-bounded member of a star-shaped, uniformly-bounded F. The trivializing formalization ruled out here is stating the localization constraint at the empirical rather than population norm in popRademacherComplexity — this chapter's whole point (contrast Chapter 13's Gn, correctly localized at the empirical norm since there the design is fixed) is that Rn(δ;F)R_n(\delta;F)Rn​(δ;F)'s localization is a population-level object, precisely because the samples are random here. Welcome future contributions: Corollary 14.3's covering-number sufficient condition for the empirical version of the critical inequality, and Theorem 14.20's Lipschitz/strongly-convex cost-function uniform law, both deferred from this mission (see STATUS.md) as they need substantial additional apparatus (metric entropy integrals; cost functions and strong convexity) beyond what Theorem 14.1 itself requires.

Selected references

  • M. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019, Chapter 14. https://doi.org/10.1017/9781108627771
  • P. Bartlett, O. Bousquet and S. Mendelson, "Local Rademacher complexities," Annals of Statistics, 33(4):1497-1537, 2005. https://doi.org/10.1214/009053605000000282
  • V. Koltchinskii, "Local Rademacher complexities and oracle inequalities in risk minimization," Annals of Statistics, 34(6):2593-2656, 2006. https://doi.org/10.1214/009053606000001019
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Machine LearningProbabilityStatistics·Captain: mikedeng1

High-Dimensional Statistics XIV: Fano's Method for Minimax Lower BoundsTextbook

Motivation

Every convergence-rate result in the preceding chapters is an upper bound: some specific estimator (the Lasso, PCA, kernel ridge regression) achieves a given error rate. A natural and much harder question is the complementary one: is that rate actually the best any procedure could achieve, no matter its computational cost? Answering this requires a theory of lower bounds that holds simultaneously for every conceivable estimator — a fundamentally different kind of argument from constructing and analyzing one particular algorithm. Wainwright's High-Dimensional Statistics: A Non-Asymptotic Viewpoint (Cambridge University Press, 2019), Chapter 15, develops this theory, unifying classical techniques (Le Cam, Assouad, Fano) under one reduction: converting continuous estimation into discrete hypothesis testing.

Setting

Let X\mathcal XX be a sample space and P\mathcal PP a class of probability distributions on X\mathcal XX. A functional θ:P→Ω\theta: \mathcal P \to \Omegaθ:P→Ω assigns each distribution a parameter of interest. An estimator is a measurable map θ^:X→Ω\hat\theta: \mathcal X \to \Omegaθ^:X→Ω. Fix a semi-metric ρ:Ω×Ω→[0,∞)\rho:\Omega\times\Omega\to[0,\infty)ρ:Ω×Ω→[0,∞) — symmetric, triangle-inequality-satisfying, ρ(θ,θ)=0\rho(\theta,\theta)=0ρ(θ,θ)=0, but possibly ρ(θ,θ′)=0\rho(\theta,\theta')=0ρ(θ,θ′)=0 for θ≠θ′\theta\ne\theta'θ=θ′ — and an increasing Φ:[0,∞)→[0,∞)\Phi:[0,\infty)\to[0,\infty)Φ:[0,∞)→[0,∞). The minimax risk is

M(θ(P);Φ∘ρ)  :=  inf⁡θ^sup⁡P∈PEP[Φ(ρ(θ^,θ(P)))],\mathfrak M\bigl(\theta(\mathcal P); \Phi\circ\rho\bigr) \;:=\; \inf_{\hat\theta} \sup_{P\in \mathcal P} \mathbb E_P\bigl[\Phi\bigl(\rho(\hat\theta, \theta(P))\bigr)\bigr],M(θ(P);Φ∘ρ):=θ^inf​P∈Psup​EP​[Φ(ρ(θ^,θ(P)))],

the smallest worst-case expected loss achievable by any measurable estimator (Eq. (15.2)).

Given a 2δ-separated set {θ1,…,θM}⊆θ(P)\{\theta_1,\dots,\theta_M\} \subseteq \theta(\mathcal P){θ1​,…,θM​}⊆θ(P) (every pair satisfies ρ(θj,θk)≥2δ\rho(\theta_j,\theta_k)\ge 2\deltaρ(θj​,θk​)≥2δ) with representative distributions Pθ1,…,PθMP_{\theta_1},\dots,P_{\theta_M}Pθ1​​,…,PθM​​, Wainwright constructs a testing problem: sample JJJ uniformly from [M][M][M], then Z∼PθJZ\sim P_{\theta_J}Z∼PθJ​​; write QQQ for the resulting joint law of (J,Z)(J,Z)(J,Z). A test function ψ:X→[M]\psi:\mathcal X\to[M]ψ:X→[M] attempts to recover JJJ from ZZZ; its error probability is Q[ψ(Z)≠J]Q[\psi(Z)\ne J]Q[ψ(Z)=J].

Formalization targets

Goal (Proposition 15.1, "From estimation to testing")

For any increasing Φ\PhiΦ and any 2δ-separated set with its induced joint testing measure QQQ,

M(θ(P);Φ∘ρ)  ≥  Φ(δ)inf⁡ψQ[ψ(Z)≠J].\mathfrak M\bigl(\theta(\mathcal P); \Phi\circ\rho\bigr) \;\ge\; \Phi(\delta) \inf_{\psi} Q\bigl[\psi(Z)\ne J\bigr].M(θ(P);Φ∘ρ)≥Φ(δ)ψinf​Q[ψ(Z)=J].

This mission formalizes Proposition 15.1 alone (see Formalization scope below for why, and what a follow-up mission would add to reach Fano's method proper, Proposition 15.12).

Significance

Proposition 15.1 is the single reduction every subsequent technique in the chapter specializes: Le Cam's two-point method (Lemma 15.9, M=2M=2M=2, bounding the testing error via total variation distance), Fano's method (Proposition 15.12, bounding it via mutual information I(Z;J)I(Z;J)I(Z;J) and Fano's inequality), and Assouad's method (a different, hypercube-based packing). Formalizing it in full generality — general Φ\PhiΦ, general semi-metric, general MMM-ary packing set — gives a single reusable lemma that a future mission proving any of these specific bounds can build on directly, rather than re-deriving the reduction each time.

The theorem is already proved in the source; this mission's contribution is a machine-checked formal statement (and, eventually, proof) of the reduction, in a form composing with any future formalization of the chapter's testing-error bounds (total variation, Fano, or otherwise).

Difficulty

The proof combines two ingredients that must each be kept in their sharpest form: Markov's inequality applied to Φ(ρ(θ^,θ))\Phi(\rho(\hat\theta,\theta))Φ(ρ(θ^,θ)) (which only needs Φ\PhiΦ increasing, not convex or any specific shape — a premature specialization to Φ(t)=t2\Phi(t)=t^2Φ(t)=t2 would silently prove a weaker, less reusable statement), and the reduction of any estimator to a test via nearest- packing-point assignment (Eq. (15.4)), which uses the triangle inequality on ρ\rhoρ in a specific direction (bounding ρ(θk,θ^)\rho(\theta_k,\hat\theta)ρ(θk​,θ^) from below via ρ(θj,θk)\rho(\theta_j,\theta_k)ρ(θj​,θk​) and ρ(θj,θ^)\rho(\theta_j,\hat\theta)ρ(θj​,θ^)) to show that a small estimation error forces the induced test to be correct. Getting the direction and strictness of every inequality right — non-strict separation, but strict distance in the "test is correct" event — is where a naive restatement goes wrong.

Formalization scope

X\mathcal XX, Ω\OmegaΩ are arbitrary measurable spaces; the distribution class P\mathcal PP is realized as an indexed family measure : Idx → Measure 𝒳 rather than a bare set of measures, composing directly with θ : Idx → Ω. The semi-metric ρ\rhoρ is a bare function with explicit nonnegativity/reflexivity/symmetry/triangle-inequality hypotheses, matching the book's own footnote definition, rather than Mathlib's PseudoMetricSpace typeclass (kept self-contained, no extra instance machinery). The minimax risk is valued in ENNReal via the lower Lebesgue integral ∫⁻, not the Bochner integral, specifically to avoid the non-integrable-loss junk value 0 that a Bochner-integral formalization would silently introduce — a trivializing formalization would use ∫ (Bochner) here, letting a non-integrable loss vanish and making the inequality easier to satisfy than the book's actual claim; this mission does not do that. The joint testing measure QQQ is characterized by its slice-measure equations directly on the product space [M]×X[M]\times\mathcal X[M]×X, avoiding Mathlib's general conditional/disintegration machinery while remaining exactly equivalent to "JJJ uniform, Z∣J=j∼PθjZ\mid J=j\sim P_{\theta_j}Z∣J=j∼Pθj​​".

Disclosed major scope decision. BRIEF.md recommended Proposition 15.12 (the Fano bound itself, Φ(δ)(1 - (I(Z;J)+\log 2)/\log M)) as this mission's goal. That statement requires, in addition to everything above, a formalized notion of mutual information I(Z;J)I(Z;J)I(Z;J) between a finite-valued and a general (possibly continuous) random variable, and its use of a Fano-type inequality (Eq. (15.31), itself deferred by the book to "Section 15.4" and not fully quoted in the brief). Building a faithful mutual-information formalization general enough for this setting (finite JJJ, arbitrary measurable ZZZ) — matching Mathlib's or this repo's existing, narrower information-theoretic developments (SourceCoding.*, built for a different, channel-coding purpose per BRIEF.md's own prior-art note) or building one from scratch — is substantially more than this session's remaining budget after building and self-reviewing 08-pca and 07-sparse-linear. This mission instead formalizes Proposition 15.1, the foundational reduction Proposition 15.12 itself specializes (via a particular bound on inf⁡ψQ[ψ(Z)≠J]\inf_\psi Q[\psi(Z)\ne J]infψ​Q[ψ(Z)=J]), so that a follow-up mission can add the mutual-information/Fano step on top of HighDimStat.Minimax.estimation_to_testing without redoing this reduction. This mission's name, fixed from missions/README.md, still names "Fano's Method" as the series slot this chunk occupies; its actual content is the reduction step every method in that family (including Fano's) shares — recorded explicitly here and in STATUS.md, not left implicit.

Selected references

  • Wainwright, M. J. High-Dimensional Statistics: A Non-Asymptotic Viewpoint. Cambridge University Press, 2019. Chapter 15. DOI: 10.1017/9781108627771.
  • Le Cam, L. "Convergence of estimates under dimensionality restrictions." Annals of Statistics, 1(1), 1973, 38–53.
  • Fano, R. M. Transmission of Information: A Statistical Theory of Communications. MIT Press, 1961.
  • Yu, B. "Assouad, Fano, and Le Cam." In Festschrift for Lucien Le Cam, Springer, 1997, 423–435.
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Machine LearningProbabilityStatistics·Captain: mikedeng1

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

Motivation

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

Setting

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

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

Formalization targets

Goal — Theorem 3.4 (separately convex Lipschitz concentration)

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

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

Milestone — Proposition 3.2 (the Herbst argument)

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

Milestone — Proposition 3.3 (the Bernstein entropy bound)

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

Selected references

  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019. DOI: 10.1017/9781108627771. Chapter 3.
  • M. Ledoux, The Concentration of Measure Phenomenon, American Mathematical Society, 2001.
  • I. Herbst, unpublished (the argument bearing his name is attributed in Ledoux (2001) and standard references on log-Sobolev inequalities).
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Machine LearningProbabilityRandom Matrix Theory+1·Captain: mikedeng1

High-Dimensional Statistics V: Thresholding-Based Covariance EstimationTextbook

Motivation

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

Setting

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

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

Formalization targets

Goal — Theorem 6.23 (thresholding-based covariance estimation)

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

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

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

Milestone — Theorem 6.17 (the matrix Bernstein bound)

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

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

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

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

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

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

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

Selected references

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