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Random Matrix Theory

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Machine LearningProbabilityStatistics·Captain: mikedeng1

High-Dimensional Probability VI: The Hanson-Wright InequalityTextbook

Motivation

Sums of independent random variables are well understood: Bernstein's inequality and its relatives give sharp, non-asymptotic tail bounds for ∑iaiXi\sum_i a_i X_i∑i​ai​Xi​ whenever the XiX_iXi​ are independent and light-tailed. Many quantities that arise in high-dimensional statistics and random matrix theory, however, are not linear but quadratic in an independent sample — the squared norm of a random vector after a linear transformation, a quadratic-form test statistic, the diagonal of a sample covariance matrix, or the number of edges cut by a random partition in a random graph. A quadratic form X⊤AX=∑i,jAijXiXjX^\top A X = \sum_{i,j} A_{ij} X_i X_jX⊤AX=∑i,j​Aij​Xi​Xj​ is a sum with dependent terms: XiXjX_iX_jXi​Xj​ and XiXkX_iX_kXi​Xk​ share the factor XiX_iXi​, so classical sum-of-independent-variables tools do not apply directly.

The Hanson-Wright inequality, first obtained by Hanson and Wright (1971) for sub-gaussian variables and later sharpened and popularized in this form by Rudelson and Vershynin (2013, "Hanson-Wright inequality and sub-gaussian concentration," Electronic Communications in Probability), closes this gap: it gives a concentration inequality for X⊤AXX^\top A XX⊤AX around its mean with the same two-regime (sub-gaussian near the center, sub-exponential in the tail) shape as Bernstein's inequality for linear sums. It is now a standard tool wherever quadratic statistics of independent data are analyzed: covariance estimation, compressed sensing, randomized numerical linear algebra, and the analysis of random matrices more broadly draw on it routinely.

Setting

Fix a probability space and let X=(X1,…,Xn)X = (X_1, \dots, X_n)X=(X1​,…,Xn​) be a random vector whose coordinates X1,…,XnX_1, \dots, X_nX1​,…,Xn​ are independent, mean zero, and sub-gaussian: each XiX_iXi​ has a finite sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm ∥Xi∥ψ2\|X_i\|_{\psi_2}∥Xi​∥ψ2​​, the smallest t>0t > 0t>0 with Eexp⁡(Xi2/t2)≤2\mathbb E \exp(X_i^2/t^2) \le 2Eexp(Xi2​/t2)≤2. Write K=max⁡i∥Xi∥ψ2K = \max_i \|X_i\|_{\psi_2}K=maxi​∥Xi​∥ψ2​​.

Let A=(Aij)i,j=1nA = (A_{ij})_{i,j=1}^nA=(Aij​)i,j=1n​ be an n×nn \times nn×n real matrix, with no constraint on its diagonal, and form the quadratic form

X⊤AX=∑i,j=1nAijXiXj.X^\top A X = \sum_{i,j=1}^n A_{ij} X_i X_j.X⊤AX=i,j=1∑n​Aij​Xi​Xj​.

Two matrix norms measure the size of AAA: the Frobenius norm ∥A∥F=(∑i,jAij2)1/2\|A\|_F = \bigl(\sum_{i,j} A_{ij}^2\bigr)^{1/2}∥A∥F​=(∑i,j​Aij2​)1/2 (the Euclidean norm of AAA's entries) and the operator (spectral) norm ∥A∥=sup⁡∥x∥2=1∥Ax∥2\|A\| = \sup_{\|x\|_2=1} \|Ax\|_2∥A∥=sup∥x∥2​=1​∥Ax∥2​ (the largest singular value of AAA). Always ∥A∥≤∥A∥F≤n ∥A∥\|A\| \le \|A\|_F \le \sqrt{n}\,\|A\|∥A∥≤∥A∥F​≤n​∥A∥, so the two norms can differ by a factor as large as n\sqrt nn​ — the gap between them is exactly what produces the inequality's two regimes below.

Formalization targets

Goal — Theorem 6.2.1 (Hanson-Wright inequality)

P{ ∣X⊤AX−E X⊤AX∣≥t }  ≤  2exp⁡ ⁣[−cmin⁡ ⁣(t2K4∥A∥F2, tK2∥A∥)]for every t≥0,P\bigl\{\, |X^\top A X - \mathbb E\, X^\top A X| \ge t \,\bigr\} \;\le\; 2 \exp\!\left[-c \min\!\left(\frac{t^2}{K^4 \|A\|_F^2},\ \frac{t}{K^2 \|A\|}\right)\right] \qquad \text{for every } t \ge 0,P{∣X⊤AX−EX⊤AX∣≥t}≤2exp[−cmin(K4∥A∥F2​t2​, K2∥A∥t​)]for every t≥0,

where c>0c > 0c>0 is an absolute constant, not depending on nnn, XXX, AAA, or ttt. Stating the constant only as "some absolute ccc" (rather than pinning it to a numeral) is deliberate: the book's own proof does not track a sharp value, and a goal that only asserts the shape of the bound survives any later improvement to ccc.

Significance

The result itself. Hanson-Wright turns a two-dimensional (in i,ji,ji,j) dependency structure into a one-dimensional concentration statement controlled by two scalar quantities, ∥A∥F\|A\|_F∥A∥F​ and ∥A∥\|A\|∥A∥. This is what makes it usable: a practitioner bounding a quadratic statistic need only compute these two norms, not analyze the joint dependency structure of {XiXj}\{X_iX_j\}{Xi​Xj​} directly. It specializes to Bernstein's inequality (Chapter 2 of this book) when AAA is diagonal, and it underlies non-asymptotic guarantees for covariance estimation, the Johnson-Lindenstrauss lemma via a different route, and the concentration of Lipschitz functions of sub-gaussian vectors.

Formalizing it. The published proof of Hanson-Wright is not a single argument but a chain of four steps: a decoupling reduction (Section 6.1), a direct computation for Gaussian chaos (Lemma 6.2.2), a comparison lemma extending the Gaussian bound to general sub-gaussian vectors via a replacement trick (Lemma 6.2.3), and a final assembly that separates the diagonal part (handled by Bernstein's inequality) from the off-diagonal part (handled by decoupling and comparison). This mission formalizes the goal theorem's statement and the first, most reusable link in that chain — the decoupling machinery of Section 6.1, which reduces the analysis of the dependent chaos X⊤AXX^\top A XX⊤AX to the independent-once-conditioned bilinear form X⊤AX′X^\top A X'X⊤AX′ — together with the chapter's separate contraction principle (Section 6.7), a general comparison tool for Rademacher-weighted sums used repeatedly in the book's later chaining chapters. The Gaussian MGF computation and the replacement-trick comparison lemma (Lemmas 6.2.2–6.2.3) are left as future milestones on top of this mission: they require Gaussian rotation invariance and the singular value decomposition of AAA, substantially more machinery than the milestones included here.

Difficulty

The obvious first idea — treat X⊤AX=∑i,jAijXiXjX^\top A X = \sum_{i,j} A_{ij}X_iX_jX⊤AX=∑i,j​Aij​Xi​Xj​ as if it were a sum of independent terms and apply Bernstein's inequality termwise — fails immediately: the terms AijXiXjA_{ij}X_iX_jAij​Xi​Xj​ for fixed iii are not independent across jjj, since they all share the factor XiX_iXi​. Decoupling (Theorem 6.1.1) is the non-obvious fix: it replaces the off-diagonal chaos by a bilinear form X⊤AX′X^\top A X'X⊤AX′ in an independent copy X′X'X′, which genuinely does become a sum of independent terms once one of the two vectors is conditioned on. The price is a universal constant factor of 444 and the restriction to diagonal-free matrices, which is exactly why the full Hanson-Wright proof must separate the diagonal contribution to E X⊤AX\mathbb E\,X^\top A XEX⊤AX (handled directly by Bernstein's inequality, Chapter 2) before decoupling can be applied to what remains.

Formalization scope

Random variables and vectors are real-valued on an explicit probability space (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P). The sub-gaussian norm is HighDimProb.Concentration.subgaussianNorm, the Orlicz-ψ2\psi_2ψ2​-norm definition already published for this series (01-concentration), reused here as a reference item rather than redefined. K=max⁡i∥Xi∥ψ2K = \max_i \|X_i\|_{\psi_2}K=maxi​∥Xi​∥ψ2​​ is written as a finite supremum over the coordinate index, ⨆ i, subgaussianNorm P (X i); because the index type is always a Fintype (Fin n), this supremum is well-defined and, at the degenerate index n=0n=0n=0, reduces to a true (if content-free) instance of the inequality rather than a vacuous or false one. The Frobenius and operator norms of AAA are this mission's own frobeniusNorm and opNorm, stated directly from their defining formulas rather than through Mathlib's scoped matrix-norm typeclass instances, which are deliberately not global defaults (to avoid a diamond between the two norms) and so are unsuitable for a statement that needs both simultaneously. Every place the goal or a milestone integrates a quantity, that quantity is required Integrable, guarding against Mathlib's convention of returning 0 for the Bochner integral of a non-integrable function — without these hypotheses, a mean-zero or expectation hypothesis could hold vacuously, or a conclusion could hold trivially, for reasons having nothing to do with the book's mathematics.

The formalization deliberately does not restrict AAA's diagonal in the goal theorem: doing so would collapse Hanson-Wright to a restatement of Bernstein's inequality for the special case of a diagonal matrix, discarding the chapter's actual content, which is handling the off-diagonal, genuinely quadratic dependence between coordinates. The diagonal-free restriction does appear, correctly, in the Decoupling theorem (6.1.1), whose proof needs it.

Reusable beyond this mission: frobeniusNorm and opNorm are needed by any future chapter using matrix norms (Chapter 4's random matrix norms, Chapter 9's matrix deviation inequality); the decoupling theorem and convex decoupling lemma are the standard entry point for any later formalization of chaos concentration; the contraction principle is reused throughout the book's chaining chapters (7 and 8). Welcome contributions include the Gaussian MGF and comparison lemmas (6.2.2–6.2.3) needed to complete a full proof of the goal theorem, and the two-sided version of Bernstein's inequality needed for the diagonal part of that proof.

Selected references

  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018. DOI: 10.1017/9781108231596.
  • D. L. Hanson, F. T. Wright, "A bound on tail probabilities for quadratic forms in independent random variables," Annals of Mathematical Statistics 42 (1971), 1079–1083.
  • M. Rudelson, R. Vershynin, "Hanson-Wright inequality and sub-gaussian concentration," Electronic Communications in Probability 18 (2013), no. 82, 1–9. https://arxiv.org/abs/1306.2872
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Linear algebraNumerical AnalysisProbability·Captain: mikedeng1

Randomized Algorithms for Estimating the Trace of an Implicit Symmetric Positive Semi-Definite Matrix IV: Sample Bound for Hutchinson's Trace EstimatorResearch Paper

Motivation

Many computations need the trace of a matrix AAA that is never formed explicitly and can only be applied to vectors: the trace of a matrix function such as trace(A−1)\mathrm{trace}(A^{-1})trace(A−1) or log⁡det⁡A=trace(log⁡A)\log\det A = \mathrm{trace}(\log A)logdetA=trace(logA) in statistics and lattice QCD, the Frobenius norm ∥B∥F2=trace(BTB)\|B\|_F^2 = \mathrm{trace}(B^TB)∥B∥F2​=trace(BTB) of an operator, or the number of triangles of a graph. The standard tool is Monte-Carlo estimation, introduced by M. F. Hutchinson (Hutchinson 1989): average MMM quadratic forms ziTAziz_i^TAz_iziT​Azi​ over random sign vectors ziz_izi​. Each sample costs one matrix–vector product, uses one random bit per entry, and needs only additions and subtractions.

Before Avron and Toledo (2011), only the variance of such estimators had been analysed. A small variance does not say how many samples guarantee a given relative error with a given probability. Avron and Toledo gave the first bounds of this kind for several estimators. This mission covers the bound for Hutchinson's estimator, their Theorem 7.1.

Setting

A Rademacher random variable takes the values +1+1+1 and −1-1−1, each with probability 1/21/21/2. Let A∈Rn×nA \in \mathbb{R}^{n\times n}A∈Rn×n be symmetric positive semi-definite. Draw M≥1M \ge 1M≥1 independent random vectors z1,…,zM∈Rnz_1, \ldots, z_M \in \mathbb{R}^nz1​,…,zM​∈Rn whose MnMnMn entries are independent Rademacher variables. Hutchinson's trace estimator is

HM=1M∑i=1MziTAzi.H_M = \frac{1}{M}\sum_{i=1}^{M} z_i^TAz_i .HM​=M1​i=1∑M​ziT​Azi​.

A single sample zTAzz^TAzzTAz is an unbiased estimator of trace(A)\mathrm{trace}(A)trace(A) (Lemma 2.1 of the paper, due to Hutchinson). For symmetric AAA its variance is 2(∥A∥F2−∑iAii2)2\bigl(\|A\|_F^2 - \sum_i A_{ii}^2\bigr)2(∥A∥F2​−∑i​Aii2​), twice the squared Frobenius mass of AAA off the diagonal.

Given ϵ>0\epsilon > 0ϵ>0 and δ∈(0,1)\delta \in (0,1)δ∈(0,1), a random estimator TTT is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A) if

Pr⁡(∣T−trace(A)∣≤ϵ trace(A))≥1−δ.\Pr\bigl(|T - \mathrm{trace}(A)| \le \epsilon\,\mathrm{trace}(A)\bigr) \ge 1 - \delta .Pr(∣T−trace(A)∣≤ϵtrace(A))≥1−δ.

The rank rank(A)\mathrm{rank}(A)rank(A) is the number of nonzero eigenvalues λj\lambda_jλj​ of AAA, counted with multiplicity.

Formalization targets

Goal: Theorem 7.1, sample bound for HMH_MHM​

For every symmetric positive semi-definite AAA, every 0<ϵ≤1/20 < \epsilon \le 1/20<ϵ≤1/2 and every 0<δ<10 < \delta < 10<δ<1,

M≥6ϵ−2ln⁡ ⁣(2 rank(A)δ)⟹HM is an (ϵ,δ)-approximator of trace(A).M \ge 6\epsilon^{-2}\ln\!\left(\frac{2\,\mathrm{rank}(A)}{\delta}\right) \quad\Longrightarrow\quad H_M \text{ is an } (\epsilon,\delta)\text{-approximator of } \mathrm{trace}(A).M≥6ϵ−2ln(δ2rank(A)​)⟹HM​ is an (ϵ,δ)-approximator of trace(A).

The bound depends on AAA only through its rank. It does not depend on the dimension nnn, on the condition number, or on how the trace is spread over the diagonal.

Milestones

  1. Lemma 7.2 (Achlioptas 2001, Lemma 5). For a unit vector α∈Rn\alpha \in \mathbb{R}^nα∈Rn and S=1M∑i=1M(αTzi)2S = \frac1M\sum_{i=1}^M(\alpha^Tz_i)^2S=M1​∑i=1M​(αTzi​)2, for every ϵ>0\epsilon > 0ϵ>0,
Pr⁡(∣S−1∣≥ϵ)≤2exp⁡ ⁣(−M2(ϵ22−ϵ33)).\Pr(|S - 1| \ge \epsilon) \le 2\exp\!\left(-\frac{M}{2}\left(\frac{\epsilon^2}{2} - \frac{\epsilon^3}{3}\right)\right).Pr(∣S−1∣≥ϵ)≤2exp(−2M​(2ϵ2​−3ϵ3​)).
  1. Per-direction bound (proof of Theorem 7.1, p. 8:11). Let r≥1r \ge 1r≥1 and 0<ϵ≤1/20 < \epsilon \le 1/20<ϵ≤1/2. If M≥6ϵ−2ln⁡(2r/δ)M \ge 6\epsilon^{-2}\ln(2r/\delta)M≥6ϵ−2ln(2r/δ), then Pr⁡(∣S−1∣≥ϵ)≤δ/r\Pr(|S - 1| \ge \epsilon) \le \delta/rPr(∣S−1∣≥ϵ)≤δ/r.
  2. From directions to the trace (proof of Theorem 7.1, p. 8:11). Write A=UΛUTA = U\Lambda U^TA=UΛUT and yi=UTziy_i = U^Tz_iyi​=UTzi​. If ∣1M∑iyij2−1∣≤ϵ|\frac1M\sum_i y_{ij}^2 - 1| \le \epsilon∣M1​∑i​yij2​−1∣≤ϵ for every jjj with λj≠0\lambda_j \ne 0λj​=0, then ∣HM−trace(A)∣≤ϵ trace(A)|H_M - \mathrm{trace}(A)| \le \epsilon\,\mathrm{trace}(A)∣HM​−trace(A)∣≤ϵtrace(A). This step is deterministic.
  3. Lemma 2.1 (Hutchinson). E(zTAz)=trace(A)\mathrm{E}(z^TAz) = \mathrm{trace}(A)E(zTAz)=trace(A), and for symmetric AAA, Var(zTAz)=2(∥A∥F2−∑iAii2)\mathrm{Var}(z^TAz) = 2(\|A\|_F^2 - \sum_i A_{ii}^2)Var(zTAz)=2(∥A∥F2​−∑i​Aii2​).

Significance

Theorem 7.1 gives a practitioner an explicit number of matrix–vector products after which Hutchinson's method is guaranteed to reach relative accuracy ϵ\epsilonϵ with confidence 1−δ1-\delta1−δ. No bound was available before, although the method had been in wide use for two decades. The bound exceeds the one the same paper proves for Gaussian test vectors (20ϵ−2ln⁡(2/δ)20\epsilon^{-2}\ln(2/\delta)20ϵ−2ln(2/δ)) by a ln⁡(rank(A))\ln(\mathrm{rank}(A))ln(rank(A)) factor. The authors conjecture that this factor is not needed. Later work removed it: Roosta-Khorasani and Ascher (2015) proved a rank-free bound for the Rademacher case, and Cortinovis and Kressner (2022) extended sample bounds to indefinite matrices. Sample bounds of this type underlie variance-reduced estimators such as Hutch++ (Meyer et al. 2021).

The theorem is proved in the literature. To the platform's knowledge it has no machine-checked proof. Formalizing it produces a checked Rademacher concentration inequality for averages of squared linear forms (Achlioptas' lemma, which is also a core lemma of database-friendly Johnson–Lindenstrauss projections), and a checked spectral reduction from a quadratic-form estimator to its eigen-directions. Neither is currently in Mathlib.

Difficulty

The estimator is not an average of independent copies of a bounded variable with a small range: a single sample zTAzz^TAzzTAz can deviate from trace(A)\mathrm{trace}(A)trace(A) by an amount comparable to ∥A∥Fn\|A\|_F\sqrt n∥A∥F​n​. Chebyshev's inequality with the variance of Lemma 2.1 only gives a polynomial dependence on 1/δ1/\delta1/δ. Hoeffding's inequality applied to zTAzz^TAzzTAz directly gives a dependence on nnn and on the size of the entries of AAA. Unlike the Gaussian case, the estimator cannot be written as a weighted sum of independent chi-squared variables, because rotating a Rademacher vector does not give another Rademacher vector. The central difficulty is Lemma 7.2: a tail bound for (αTz)2(\alpha^Tz)^2(αTz)2 that holds uniformly over every unit direction α\alphaα, including directions in which αTz\alpha^TzαTz is far from Gaussian (for α=e1\alpha = e_1α=e1​ it is a constant).

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℝ, and positive semi-definiteness is Matrix.PosSemidef. The Rademacher law is 12(δ1+δ−1)\tfrac12(\delta_1 + \delta_{-1})21​(δ1​+δ−1​) on ℝ. The sample space is Fin M → Fin n → ℝ with the product of MnMnMn copies of this law (hutchinsonSampleMeasure), so the law of the estimator is constructed, not assumed. HM(ω)=(M:R)−1∑iωi⋅(Aωi)H_M(\omega) = (M:\mathbb{R})^{-1}\sum_i \omega_i\cdot(A\omega_i)HM​(ω)=(M:R)−1∑i​ωi​⋅(Aωi​). Probabilities are Measure.real, and the (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator is Definition 4.1 verbatim. rank(A)\mathrm{rank}(A)rank(A) is Matrix.rank. In Lemma 7.2 the i.i.d. copies QiQ_iQi​ are the functions (α⋅zi)2(\alpha\cdot z_i)^2(α⋅zi​)2 on this product space.

Corrections of printed statements, each recorded in the item's Formalization Note:

  • Theorem 7.1 is printed without a range on ϵ\epsilonϵ. Its proof needs M2(ϵ22−ϵ33)≥Mϵ26\frac{M}{2}(\frac{\epsilon^2}{2} - \frac{\epsilon^3}{3}) \ge \frac{M\epsilon^2}{6}2M​(2ϵ2​−3ϵ3​)≥6Mϵ2​, which holds exactly when ϵ≤1/2\epsilon \le 1/2ϵ≤1/2. Without a range the printed statement is false: take A=1n11TA = \frac1n\mathbf 1\mathbf 1^TA=n1​11T, n=104n = 10^4n=104, ϵ=10\epsilon = 10ϵ=10 and δ=10−4\delta = 10^{-4}δ=10−4. The condition admits M=1M = 1M=1, while Pr⁡(H1>11)≈9⋅10−4>δ\Pr(H_1 > 11) \approx 9\cdot10^{-4} > \deltaPr(H1​>11)≈9⋅10−4>δ. The goal and milestone 2 are therefore stated for 0<ϵ≤1/20 < \epsilon \le 1/20<ϵ≤1/2.
  • Lemma 2.1 is printed for an arbitrary n×nn\times nn×n matrix. The variance formula fails for non-symmetric AAA: for A=(0100)A = \begin{pmatrix}0&1\\0&0\end{pmatrix}A=(00​10​) the variance is 111, not 222. Symmetry is assumed for the variance part only.
  • Proof of Theorem 7.1. The proof writes Λ=UAUT\Lambda = UAU^TΛ=UAUT together with yi=UTziy_i = U^Tz_iyi​=UTzi​. These fit together only for A=UΛUTA = U\Lambda U^TA=UΛUT, which is the convention of milestone 3.

For A=0A = 0A=0 the threshold involves ln⁡0\ln 0ln0. Lean's Real.log 0 = 0 turns the condition into M≥0M \ge 0M≥0, which agrees with the paper's reading ln⁡0=−∞\ln 0 = -\inftyln0=−∞. The conclusion then holds because HM=trace(A)=0H_M = \mathrm{trace}(A) = 0HM​=trace(A)=0, so no extra hypothesis is added. A formalization that took the law of the samples as a hypothesis could make that hypothesis unsatisfiable and the theorem vacuous; the constructed product space rules this out.

A complete development needs:

  • the product Rademacher measure and moment generating functions of Rademacher sums;
  • a Chernoff bound for averages of i.i.d. bounded variables on a product space;
  • the spectral theorem for real symmetric matrices, with rank equal to the number of nonzero eigenvalues;
  • a finite union bound.

The Rademacher concentration results are reusable beyond this mission. Proofs of any milestone are welcome, as are alternative proofs of Lemma 7.2.

Selected references

  • H. Avron and S. Toledo, Randomized algorithms for estimating the trace of an implicit symmetric positive semi-definite matrix, Journal of the ACM 58(2), Article 8, 2011. https://doi.org/10.1145/1944345.1944349
  • M. F. Hutchinson, A stochastic estimator of the trace of the influence matrix for Laplacian smoothing splines, Communications in Statistics – Simulation and Computation 18(3), 1059–1076, 1989. https://doi.org/10.1080/03610918908812806
  • D. Achlioptas, Database-friendly random projections, Proceedings of PODS 2001, 274–281. https://doi.org/10.1145/375551.375608
  • F. Roosta-Khorasani and U. Ascher, Improved bounds on sample size for implicit matrix trace estimators, Foundations of Computational Mathematics 15, 1187–1212, 2015. https://doi.org/10.1007/s10208-014-9220-1
  • A. Cortinovis and D. Kressner, On randomized trace estimates for indefinite matrices with an application to determinants, Foundations of Computational Mathematics 22, 875–903, 2022. https://doi.org/10.1007/s10208-021-09525-9
  • R. A. Meyer, C. Musco, C. Musco and D. P. Woodruff, Hutch++: Optimal stochastic trace estimation, SOSA 2021, 142–155. https://doi.org/10.1137/1.9781611976496.16
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Linear algebraNumerical AnalysisProbability·Captain: mikedeng1

Randomized Algorithms for Estimating the Trace of an Implicit Symmetric Positive Semi-Definite Matrix II: Exact Rank of a Projection Matrix from the Gaussian Trace EstimatorResearch Paper

Motivation

Many matrices in scientific computing are available only implicitly: one can multiply a vector by AAA, for instance by solving a linear system or applying a matrix function, but the entries of AAA are never formed. Quantities such as the trace must then be estimated from a small number of matrix–vector products. Randomized trace estimators do exactly this: draw random vectors zzz, compute the quadratic forms zTAzz^TAzzTAz, and average.

Avron and Toledo (J. ACM 58(2), 2011) gave the first sample bounds of the form "MMM samples suffice for relative error ϵ\epsilonϵ with probability 1−δ1-\delta1−δ" for the standard estimators. Among their results is a case in which the estimate is not merely approximate but exact: when AAA is a projection matrix, its trace equals its rank, an integer, and rounding a Gaussian trace estimate recovers that integer with high probability. Computing the rank of a projection arises, for example, when charge densities are computed in electronic structure calculations without diagonalization (Bekas, Kokiopoulou and Saad 2007).

Setting

Let n≥1n \ge 1n≥1 and A∈Rn×nA \in \mathbb{R}^{n\times n}A∈Rn×n. A projection matrix here is an orthogonal projection: AAA is symmetric and A2=AA^2 = AA2=A. Equivalently, AAA is symmetric and every eigenvalue of AAA is 000 or 111; its rank rank(A)\mathrm{rank}(A)rank(A) is the number of eigenvalues equal to 111.

Fix a number of samples M≥1M \ge 1M≥1. Let z1,…,zM∈Rnz_1,\ldots,z_M \in \mathbb{R}^nz1​,…,zM​∈Rn be random vectors whose MnMnMn entries are independent standard normal random variables. The Gaussian trace estimator (Definition 3.1 of the paper) is

GM=1M∑i=1MziTAzi.G_M = \frac{1}{M}\sum_{i=1}^{M} z_i^T A z_i .GM​=M1​i=1∑M​ziT​Azi​.

Its expectation is trace(A)\mathrm{trace}(A)trace(A). For x∈Rx \in \mathbb{R}x∈R, round(x)\mathrm{round}(x)round(x) denotes the nearest integer to xxx. For k≥1k \ge 1k≥1, a random variable XXX has the χ2\chi^2χ2 distribution with kkk degrees of freedom, X∼χ2(k)X \sim \chi^2(k)X∼χ2(k), if it has the law of g12+⋯+gk2g_1^2 + \cdots + g_k^2g12​+⋯+gk2​ for independent standard normal g1,…,gkg_1, \ldots, g_kg1​,…,gk​.

Formalization targets

Goal: Lemma 5.3 (p. 8:9)

For a projection matrix AAA, a failure probability δ>0\delta > 0δ>0, and every integer M≥1M \ge 1M≥1 with M≥24 rank(A)ln⁡(2/δ)M \ge 24\,\mathrm{rank}(A)\ln(2/\delta)M≥24rank(A)ln(2/δ),

Pr⁡(round(GM)≠rank(A))≤δ.\Pr\bigl(\mathrm{round}(G_M) \ne \mathrm{rank}(A)\bigr) \le \delta .Pr(round(GM​)=rank(A))≤δ.

The number of samples depends on the rank and on δ\deltaδ only; there is no accuracy parameter, and none on nnn.

Milestones, in the order the proof uses them

  1. Law of MGMMG_MMGM​. MGM∼χ2(M rank(A))MG_M \sim \chi^2(M\,\mathrm{rank}(A))MGM​∼χ2(Mrank(A)).
  2. χ2\chi^2χ2 tail bound (cited by the paper from Li, Hastie and Church 2007). For X∼χ2(k)X \sim \chi^2(k)X∼χ2(k), k≥1k\ge1k≥1 and 0<ϵ≤120 < \epsilon \le \tfrac120<ϵ≤21​,
Pr⁡(∣X−k∣≥ϵk)≤2exp⁡(−kϵ2/6).\Pr(|X - k| \ge \epsilon k) \le 2\exp(-k\epsilon^2/6).Pr(∣X−k∣≥ϵk)≤2exp(−kϵ2/6).
  1. Tail of GMG_MGM​. For rank(A)≥1\mathrm{rank}(A) \ge 1rank(A)≥1 and 0<ϵ≤120 < \epsilon \le \tfrac120<ϵ≤21​,
Pr⁡(∣GM−rank(A)∣≥rank(A)ϵ)≤2exp⁡(−M rank(A)ϵ2/6).\Pr(|G_M - \mathrm{rank}(A)| \ge \mathrm{rank}(A)\epsilon) \le 2\exp(-M\,\mathrm{rank}(A)\epsilon^2/6).Pr(∣GM​−rank(A)∣≥rank(A)ϵ)≤2exp(−Mrank(A)ϵ2/6).
  1. Eq. (2). If moreover M≥6 rank(A)−1ϵ−2ln⁡(2/δ)M \ge 6\,\mathrm{rank}(A)^{-1}\epsilon^{-2}\ln(2/\delta)M≥6rank(A)−1ϵ−2ln(2/δ), then Pr⁡(∣GM−rank(A)∣≥rank(A)ϵ)≤δ\Pr(|G_M - \mathrm{rank}(A)| \ge \mathrm{rank}(A)\epsilon) \le \deltaPr(∣GM​−rank(A)∣≥rank(A)ϵ)≤δ.
  2. Trace of a projection. trace(A)=rank(A)\mathrm{trace}(A) = \mathrm{rank}(A)trace(A)=rank(A).

Significance

The lemma turns a randomized estimator into an exact algorithm with a controlled failure probability: the rank of an implicitly given projection is obtained from O(rank(A)log⁡(1/δ))O(\mathrm{rank}(A)\log(1/\delta))O(rank(A)log(1/δ)) matrix–vector products, independently of the dimension nnn. It is also an instance where the paper's general relative-error bound for the Gaussian estimator (Theorem 5.2, whose sample count grows like ϵ−2\epsilon^{-2}ϵ−2) is improved by exploiting the spectrum of AAA: an absolute error below 12\tfrac1221​ is a relative error ϵ=1/(2 rank(A))\epsilon = 1/(2\,\mathrm{rank}(A))ϵ=1/(2rank(A)), for which the general bound would require a number of samples quadratic in the rank, whereas Lemma 5.3 needs only a linear number.

The result is proved in the paper. The mission produces a machine-checked version of it, together with two pieces of reusable substrate: the exact χ2\chi^2χ2 law of a Gaussian quadratic form in an orthogonal projection, and a two-sided χ2\chi^2χ2 tail bound with explicit constant 1/61/61/6 on the range 0<ϵ≤1/20<\epsilon\le 1/20<ϵ≤1/2. To the best of available knowledge, none of these statements is formalized in Mathlib; a platform mission on the Johnson–Lindenstrauss lemma states a χ2\chi^2χ2 concentration bound with a different exponent, (ϵ2−ϵ3)/4(\epsilon^2-\epsilon^3)/4(ϵ2−ϵ3)/4, on the open range 0<ϵ<1/20<\epsilon<1/20<ϵ<1/2, which does not cover the value ϵ=1/2\epsilon = 1/2ϵ=1/2 needed here when rank(A)=1\mathrm{rank}(A)=1rank(A)=1.

Difficulty

The deterministic part is short; the probabilistic part is not. The step "y=Uzy = Uzy=Uz has independent standard normal entries because UUU is orthogonal" is the rotation invariance of the standard Gaussian measure on Rn\mathbb{R}^nRn, and it must be combined with the independence of the MMM samples to identify the law of a sum of M rank(A)M\,\mathrm{rank}(A)Mrank(A) squares; this is a statement about product measures and pushforwards, not about moments. The χ2\chi^2χ2 tail bound is quoted by the paper without proof. Its constant 1/61/61/6 is not the constant of the usual textbook χ2\chi^2χ2 estimates, and the bound is false outside a restricted range of ϵ\epsilonϵ (see below), so a generic sub-exponential concentration inequality with unspecified constants does not deliver it. Finally, the rounding step requires matching Mathlib's round with the event ∣GM−rank(A)∣<12|G_M - \mathrm{rank}(A)| < \tfrac12∣GM​−rank(A)∣<21​.

Formalization scope

All declarations live in the namespace TraceEstimation.ProjectionRank. Matrices are Matrix (Fin n) (Fin n) ℝ. The sample space of GMG_MGM​ is Fin M → Fin n → ℝ with the product measure Measure.pi (fun _ => Measure.pi (fun _ => gaussianReal 0 1)), so the law of the estimator is constructed, not assumed. Probabilities are Measure.real of events. "Projection matrix" is A.IsHermitian ∧ A * A = A (orthogonal projection); a non-symmetric idempotent also has eigenvalues 000 and 111, but the paper's proof diagonalizes AAA by a unitary matrix, which requires symmetry. round is Mathlib's round : ℝ → ℤ; the rank is Matrix.rank. The χ2\chi^2χ2 distribution is not defined: its role is played by the pushforward of a product of standard normals under g↦∑lgl2g \mapsto \sum_l g_l^2g↦∑l​gl2​.

Corrections of the printed text, both in the χ2\chi^2χ2 tail bound (milestone 2):

  • The paper prints Pr⁡(∣X−k∣≤ϵk)≤2exp⁡(−kϵ2/6)\Pr(|X - k| \le \epsilon k) \le 2\exp(-k\epsilon^2/6)Pr(∣X−k∣≤ϵk)≤2exp(−kϵ2/6). The inner ≤\le≤ is a misprint for ≥\ge≥; the next display applies the bound with ≥\ge≥.
  • The paper gives no range for ϵ\epsilonϵ. The bound fails for ϵ=1\epsilon = 1ϵ=1 and large kkk, since Pr⁡(X≥2k)\Pr(X \ge 2k)Pr(X≥2k) decays like e−k(1−ln⁡2)/2e^{-k(1-\ln 2)/2}e−k(1−ln2)/2, slower than e−k/6e^{-k/6}e−k/6. The mission states it for 0<ϵ≤1/20<\epsilon\le 1/20<ϵ≤1/2, and milestones 3 and 4 inherit that range; the proof uses only ϵ=1/(2 rank(A))≤1/2\epsilon = 1/(2\,\mathrm{rank}(A)) \le 1/2ϵ=1/(2rank(A))≤1/2.

The goal keeps the paper's hypotheses: δ>0\delta > 0δ>0 with no upper bound, and rank(A)=0\mathrm{rank}(A) = 0rank(A)=0 allowed (both are true cases). A statement about the event ∣GM−rank(A)∣<12|G_M - \mathrm{rank}(A)| < \tfrac12∣GM​−rank(A)∣<21​, or Eq. (2) alone, is not the goal; the goal is about round(GM)\mathrm{round}(G_M)round(GM​). The sample measure is a probability measure, so the bound ≤δ\le \delta≤δ is not vacuous.

Contributions welcome beyond the milestones: rotation invariance of the standard Gaussian vector under orthogonal matrices, the moment generating function of χ2(k)\chi^2(k)χ2(k), and the spectral fact trace(A)=rank(A)\mathrm{trace}(A) = \mathrm{rank}(A)trace(A)=rank(A) for idempotents, each reusable well outside this mission.

Selected references

  • H. Avron and S. Toledo, Randomized algorithms for estimating the trace of an implicit symmetric positive semi-definite matrix, Journal of the ACM 58(2), Article 8, 2011. https://doi.org/10.1145/1944345.1944349
  • P. Li, T. Hastie and K. Church, Nonlinear estimators and tail bounds for dimension reduction in l1l_1l1​ using Cauchy random projections, in Learning Theory (COLT 2007), Lecture Notes in Computer Science 4539, Springer, 514–529, 2007 (the version the paper cites); journal version in Journal of Machine Learning Research 8, 2497–2532, 2007, https://jmlr.org/papers/v8/li07b.html
  • C. Bekas, E. Kokiopoulou and Y. Saad, An estimator for the diagonal of a matrix, Applied Numerical Mathematics 57(11–12), 1214–1229, 2007. https://doi.org/10.1016/j.apnum.2007.01.003
  • M. F. Hutchinson, A stochastic estimator of the trace of the influence matrix for Laplacian smoothing splines, Communications in Statistics – Simulation and Computation 19(2), 433–450, 1990. https://doi.org/10.1080/03610919008812866
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Randomized Algorithms for Estimating the Trace of an Implicit Symmetric Positive Semi-Definite Matrix I: Sample Bound for the Gaussian Trace EstimatorResearch Paper

Motivation

Many computations in scientific computing, statistics and machine learning need the trace of a matrix AAA that is never formed explicitly: AAA may be f(B)f(B)f(B) for a large sparse BBB, an inverse B−1B^{-1}B−1, or a product of operators, and the only access to it is the ability to compute products AzAzAz for chosen vectors zzz. Examples are log-determinant estimation in Gaussian process regression, counting triangles in graphs through trace(B3)\mathrm{trace}(B^3)trace(B3), computing charge densities in electronic structure calculations, and generalized cross-validation in regularized regression. For such matrices the nnn diagonal entries are not available, and computing them one at a time costs nnn matrix–vector products.

Randomized trace estimators replace this by a small number MMM of products: draw random vectors z1,…,zMz_1,\ldots,z_Mz1​,…,zM​ from a fixed distribution with E(ziTAzi)=trace(A)\mathrm{E}(z_i^T A z_i) = \mathrm{trace}(A)E(ziT​Azi​)=trace(A) and average the quadratic forms. Hutchinson (1989) introduced the estimator with Rademacher vectors and computed its variance; Silver and Röder (1997) used Gaussian vectors. Before Avron and Toledo (2011), the analyses of these estimators were variance computations, which do not say how many samples guarantee a given relative accuracy with a given probability. Avron and Toledo gave the first such sample bounds for several estimators, stated in terms of an (ϵ,δ)(\epsilon,\delta)(ϵ,δ) guarantee; this mission formalizes their bound for the Gaussian estimator. Later work (Roosta-Khorasani and Ascher 2015; Cortinovis and Kressner 2022) sharpened these bounds and extended them to indefinite matrices.

Setting

Let A∈Rn×nA \in \mathbb{R}^{n\times n}A∈Rn×n be symmetric positive semi-definite, and write τ=trace(A)\tau = \mathrm{trace}(A)τ=trace(A). Fix a number of samples M≥1M \ge 1M≥1. Let z1,…,zM∈Rnz_1, \ldots, z_M \in \mathbb{R}^nz1​,…,zM​∈Rn be random vectors whose MnMnMn entries are independent standard normal random variables. The Gaussian trace estimator (Definition 3.1) is

GM=1M∑i=1MziTAzi.G_M = \frac{1}{M}\sum_{i=1}^{M} z_i^T A z_i .GM​=M1​i=1∑M​ziT​Azi​.

Each term ziTAziz_i^TAz_iziT​Azi​ has expectation trace(A)\mathrm{trace}(A)trace(A), so GMG_MGM​ is unbiased. A randomized trace estimator TTT is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A) (Definition 4.1) if

Pr⁡(∣T−trace(A)∣≤ϵ trace(A))≥1−δ,\Pr\bigl(|T - \mathrm{trace}(A)| \le \epsilon\,\mathrm{trace}(A)\bigr) \ge 1-\delta ,Pr(∣T−trace(A)∣≤ϵtrace(A))≥1−δ,

that is, if its relative error is at most ϵ\epsilonϵ except on an event of probability at most δ\deltaδ.

The analysis uses the eigenvalues λ1,…,λn≥0\lambda_1,\ldots,\lambda_n \ge 0λ1​,…,λn​≥0 of AAA, listed with multiplicity, and the polynomial h(t)=∑s=2n(−2)sts∑∣S∣=s∏i∈Sλih(t) = \sum_{s=2}^{n}(-2)^s t^s \sum_{|S| = s}\prod_{i\in S}\lambda_ih(t)=∑s=2n​(−2)sts∑∣S∣=s​∏i∈S​λi​, where SSS ranges over subsets of {1,…,n}\{1,\ldots,n\}{1,…,n}; it satisfies ∏i(1−2λit)=1−2τt+h(t)\prod_i(1-2\lambda_i t) = 1 - 2\tau t + h(t)∏i​(1−2λi​t)=1−2τt+h(t).

Formalization targets

Goal: Theorem 5.2 (corrected)

For every symmetric positive semi-definite AAA, every 0<ϵ≤1/100 < \epsilon \le 1/100<ϵ≤1/10, every 0<δ<10<\delta<10<δ<1 and every natural number MMM with

M≥20 ϵ−2ln⁡(2/δ),M \ge 20\,\epsilon^{-2}\ln(2/\delta),M≥20ϵ−2ln(2/δ),

the estimator GMG_MGM​ is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A). The sample count depends on neither nnn nor AAA.

Milestones

  1. Lemma 5.1. For symmetric AAA, E(G1)=trace(A)\mathrm{E}(G_1) = \mathrm{trace}(A)E(G1​)=trace(A) and Var(G1)=2∥A∥F2\mathrm{Var}(G_1) = 2\|A\|_F^2Var(G1​)=2∥A∥F2​.
  2. Eq. (1). For symmetric AAA and every ttt with 2λit<12\lambda_i t < 12λi​t<1 for all iii, the moment generating function of Z=MGMZ = MG_MZ=MGM​ is
mZ(t)=∏i=1n(1−2λit)−M/2=(1−2τt+h(t))−M/2.m_Z(t) = \prod_{i=1}^{n}(1-2\lambda_i t)^{-M/2} = (1 - 2\tau t + h(t))^{-M/2}.mZ​(t)=i=1∏n​(1−2λi​t)−M/2=(1−2τt+h(t))−M/2.
  1. Elementary symmetric sums (p. 8:8). For non-negative x1,…,xnx_1,\ldots,x_nx1​,…,xn​ and 1≤i≤n1\le i\le n1≤i≤n, ∑∣S∣=i∏j∈Sxj≤(∑jxj)i\sum_{|S|=i}\prod_{j\in S}x_j \le (\sum_j x_j)^i∑∣S∣=i​∏j∈S​xj​≤(∑j​xj​)i; hence ∣h(t)∣≤∑j=2n(2τt)j|h(t)| \le \sum_{j=2}^{n}(2\tau t)^j∣h(t)∣≤∑j=2n​(2τt)j for t≥0t\ge0t≥0 when all λi≥0\lambda_i\ge0λi​≥0.
  2. Upper tail (pp. 8:8–8:9). If τ>0\tau > 0τ>0, M≥1M\ge1M≥1 and 0<ϵ≤0.10<\epsilon\le 0.10<ϵ≤0.1, then
Pr⁡(GM≥τ(1+ϵ))≤exp⁡(−Mϵ2/20).\Pr\bigl(G_M \ge \tau(1+\epsilon)\bigr) \le \exp(-M\epsilon^2/20).Pr(GM​≥τ(1+ϵ))≤exp(−Mϵ2/20).
  1. Both tails (p. 8:9). If τ>0\tau>0τ>0, 0<ϵ≤0.10<\epsilon\le0.10<ϵ≤0.1 and M≥20ϵ−2ln⁡(2/δ)M \ge 20\epsilon^{-2}\ln(2/\delta)M≥20ϵ−2ln(2/δ), then Pr⁡(GM≥τ(1+ϵ))≤δ/2\Pr(G_M \ge \tau(1+\epsilon)) \le \delta/2Pr(GM​≥τ(1+ϵ))≤δ/2 and Pr⁡(GM≤τ(1−ϵ))≤δ/2\Pr(G_M \le \tau(1-\epsilon)) \le \delta/2Pr(GM​≤τ(1−ϵ))≤δ/2.

Significance

The theorem gives a number of matrix–vector products, O(ϵ−2ln⁡(1/δ))O(\epsilon^{-2}\ln(1/\delta))O(ϵ−2ln(1/δ)), that suffices for a relative-error guarantee on the trace of any positive semi-definite matrix, independent of its dimension and spectrum. It is the reference row of the paper's Table I, against which the Hutchinson, normalized Rayleigh-quotient and unit-vector estimators are compared, and it is the form in which trace estimation enters the analysis of randomized algorithms for log-determinants, spectral densities and matrix functions.

The result is proved in the paper; to our knowledge it has not been formalized in any proof assistant. The mission produces a machine-checked version with the constant 202020 and the range of ϵ\epsilonϵ made explicit, and with the misprints of the printed argument resolved (see Formalization scope). It also produces reusable pieces: the moment generating function of a Gaussian quadratic form, and the bound on elementary symmetric sums by powers of the power sum. Sharper constants, the removal of the restriction ϵ≤0.1\epsilon\le 0.1ϵ≤0.1, or a direct formalization of the lower tail through a χ2\chi^2χ2 tail bound are welcome as further theorems.

Difficulty

Unbiasedness and the variance formula do not give the result: Chebyshev's inequality with Var(GM)=2∥A∥F2/M≤2τ2/M\mathrm{Var}(G_M) = 2\|A\|_F^2/M \le 2\tau^2/MVar(GM​)=2∥A∥F2​/M≤2τ2/M yields M≥2ϵ−2δ−1M \ge 2\epsilon^{-2}\delta^{-1}M≥2ϵ−2δ−1, with a polynomial rather than logarithmic dependence on 1/δ1/\delta1/δ. A logarithmic bound needs exponential moments of GMG_MGM​, and the exponential moment of zTAzz^TAzzTAz is finite only for ttt below 1/(2λmax⁡)1/(2\lambda_{\max})1/(2λmax​); the argument has to choose ttt inside that range uniformly in the spectrum, using only λmax⁡≤τ\lambda_{\max}\le\tauλmax​≤τ. The second obstacle is distributional: zTAzz^TAzzTAz is not a sum of independent terms in the coordinates of zzz, and reducing it to a weighted sum of independent χ2\chi^2χ2 variables requires the rotation invariance of the standard Gaussian vector. The paper proves only the upper tail with an explicit constant and states that the lower tail follows "using the same technique"; that step has to be supplied.

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℝ; "symmetric positive semi-definite" is A.PosSemidef, "symmetric" is A.IsHermitian, and eigenvalues are Matrix.IsHermitian.eigenvalues. The sample space is Fin M → Fin n → ℝ with the product measure of MnMnMn copies of gaussianReal 0 1, so the law of the samples is constructed, not assumed; GM(ω)=(M:R)−1∑iωi⋅(Aωi)G_M(\omega) = (M:\mathbb{R})^{-1}\sum_i \omega_i\cdot(A\omega_i)GM​(ω)=(M:R)−1∑i​ωi​⋅(Aωi​). Probabilities are Measure.real; the moment generating function is Mathlib's mgf; the variance is Mathlib's variance, and Lemma 5.1 asserts square integrability so that neither the integral nor the variance takes its default value. The sample count is a natural number M≥1M\ge1M≥1; ϵ\epsilonϵ and δ\deltaδ are real.

Corrections of the printed text, each recorded in the item's Formalization Note:

  • Theorem 5.2 is printed without a range for ϵ\epsilonϵ and is false without one (for rank-one AAA, ϵ=100\epsilon=100ϵ=100, δ=e−400\delta=e^{-400}δ=e−400 the threshold allows M=1M=1M=1, while Pr⁡(χ12>101)≈e−50>δ\Pr(\chi^2_1>101)\approx e^{-50}>\deltaPr(χ12​>101)≈e−50>δ). The proof gives its key bound "for ϵ≤0.1\epsilon\le0.1ϵ≤0.1"; the goal is stated for 0<ϵ≤1/100<\epsilon\le 1/100<ϵ≤1/10.
  • Eq. (1) is printed for ∣λit∣≤12|\lambda_i t|\le\frac12∣λi​t∣≤21​, which admits 1−2λit=01-2\lambda_it = 01−2λi​t=0, where the moment generating function is infinite. It is stated for 2λit<12\lambda_i t<12λi​t<1. The page's sum over subsets of "the set Λ\LambdaΛ of eigenvalues" is taken over index sets, so repeated eigenvalues count with multiplicity.
  • The last paragraph of the proof prints Pr⁡(GM≤τ(1+ϵ))≤δ/2\Pr(G_M\le\tau(1+\epsilon))\le\delta/2Pr(GM​≤τ(1+ϵ))≤δ/2 for the upper tail and Pr⁡(∣GM−τ∣≤τ(1+ϵ))≤δ\Pr(|G_M-\tau|\le\tau(1+\epsilon))\le\deltaPr(∣GM​−τ∣≤τ(1+ϵ))≤δ for the conclusion; the intended statements are Pr⁡(GM≥τ(1+ϵ))≤δ/2\Pr(G_M\ge\tau(1+\epsilon))\le\delta/2Pr(GM​≥τ(1+ϵ))≤δ/2 and Pr⁡(∣GM−τ∣>ϵτ)≤δ\Pr(|G_M-\tau|>\epsilon\tau)\le\deltaPr(∣GM​−τ∣>ϵτ)≤δ. Milestone 5 states the upper and lower tail bounds.
  • Lemma 5.1 is followed by the remark that it "also applies when AAA is non-symmetric"; this is false for the variance and is not formalized. Definition 3.1 says "positive-definite"; the estimator is defined for every matrix and each theorem carries its own hypothesis.
  • The one-sided tail milestones assume trace(A)>0\mathrm{trace}(A)>0trace(A)>0; for A=0A=0A=0 their events are certain, while the goal holds trivially.

A formalization that makes the goal trivial is ruled out: the estimator's law is the explicit product Gaussian measure rather than a hypothesis, MMM ranges over all natural numbers above the threshold, and the approximator predicate is evaluated on the genuine event ∣GM−trace(A)∣≤ϵ trace(A)|G_M - \mathrm{trace}(A)|\le\epsilon\,\mathrm{trace}(A)∣GM​−trace(A)∣≤ϵtrace(A).

A complete development needs rotation invariance of the standard Gaussian on Rn\mathbb{R}^nRn (Mathlib's stdGaussian_map), the moment generating function of a squared standard normal, independence of products of Gaussian vectors, and a Chernoff bound from the moment generating function. The Gaussian quadratic-form results (milestones 1 and 2) are reusable for the other Gaussian estimators of the paper, such as the rank estimator of Lemma 5.3. Proofs of any milestone, alternative proofs of the lower tail, and helper lemmas on χ2\chi^2χ2 moment generating functions are welcome.

Selected references

  • H. Avron and S. Toledo, Randomized algorithms for estimating the trace of an implicit symmetric positive semi-definite matrix, Journal of the ACM 58(2), Article 8, 2011. https://doi.org/10.1145/1944345.1944349
  • M. F. Hutchinson, A stochastic estimator of the trace of the influence matrix for Laplacian smoothing splines, Communications in Statistics – Simulation and Computation 18(3), 1059–1076, 1989. https://doi.org/10.1080/03610918908812806
  • R. N. Silver and H. Röder, Calculation of densities of states and spectral functions by Chebyshev recursion and maximum entropy, Physical Review E 56(4), 4822–4829, 1997. https://doi.org/10.1103/PhysRevE.56.4822
  • F. Roosta-Khorasani and U. Ascher, Improved bounds on sample size for implicit matrix trace estimators, Foundations of Computational Mathematics 15, 1187–1212, 2015. https://doi.org/10.1007/s10208-014-9220-1
  • A. Cortinovis and D. Kressner, On randomized trace estimates for indefinite matrices with an application to determinants, Foundations of Computational Mathematics 22, 875–903, 2022. https://doi.org/10.1007/s10208-021-09525-9
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High-Dimensional Probability IX: The Matrix Deviation InequalityTextbook

Motivation

Random matrices with independent rows are the workhorse of high-dimensional statistics and compressed sensing: sample covariance matrices, sub-sampled measurement operators, and randomized sketches are all of this form. A basic question about such a matrix AAA is how close ∥Ax∥2\|Ax\|_2∥Ax∥2​ stays to its typical size E∥Ax∥2≈m∥x∥2\mathbb E\|Ax\|_2\approx\sqrt m\|x\|_2E∥Ax∥2​≈m​∥x∥2​ — not just for one fixed xxx, but simultaneously for every xxx in some set TTT of interest (a sphere, a cone, the difference set of a data cloud). A bound that holds only pointwise in xxx is of limited use, since most applications need to reason about the worst case over an entire geometric set at once.

This chapter proves such a uniform bound — the matrix deviation inequality — for matrices with independent, isotropic, sub-gaussian rows, controlling the deviation by a single geometric parameter of TTT, its Gaussian complexity. The result is a direct descendant of the chaining machinery of Chapter 8 (via Talagrand's comparison inequality, Chapter 8.6) and, in this book's own account, subsumes several results proved earlier by other methods — two-sided bounds on random matrices, the Johnson-Lindenstrauss lemma for infinite sets — while also yielding two new consequences central to high-dimensional convex geometry: the M∗M^*M∗ bound and the Escape theorem, both controlling how a random subspace intersects a fixed geometric set.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P). A random vector XXX in Rn\mathbb R^nRn is isotropic if its covariance matrix is the identity, Σ(X)=E[XX⊤]=In\Sigma(X)=\mathbb E[XX^\top]=I_nΣ(X)=E[XX⊤]=In​ — equivalently (the book's own Lemma 3.2.3), E⟨X,x⟩2=∥x∥22\mathbb E\langle X,x\rangle^2=\|x\|_2^2E⟨X,x⟩2=∥x∥22​ for every x∈Rnx\in\mathbb R^nx∈Rn. The sub-gaussian norm of a random vector XXX is ∥X∥ψ2:=sup⁡x∈Sn−1∥⟨X,x⟩∥ψ2\|X\|_{\psi_2}:=\sup_{x\in S^{n-1}}\|\langle X,x\rangle\|_{\psi_2}∥X∥ψ2​​:=supx∈Sn−1​∥⟨X,x⟩∥ψ2​​, the supremum over the unit sphere of the scalar sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm of its one-dimensional marginals; XXX is sub-gaussian when this is finite.

Fix a standard Gaussian random vector g∼N(0,In)g\sim N(0,I_n)g∼N(0,In​) in Rn\mathbb R^nRn (a vector whose coordinates in any orthonormal basis are independent standard normal). For a subset T⊆RnT\subseteq\mathbb R^nT⊆Rn, the Gaussian width and Gaussian complexity of TTT are

w(T):=Esup⁡x∈T⟨g,x⟩,γ(T):=Esup⁡x∈T∣⟨g,x⟩∣,w(T) := \mathbb E\sup_{x\in T}\langle g,x\rangle, \qquad \gamma(T) := \mathbb E\sup_{x\in T}|\langle g,x\rangle|,w(T):=Ex∈Tsup​⟨g,x⟩,γ(T):=Ex∈Tsup​∣⟨g,x⟩∣,

two closely related measures of the geometric size of TTT — "cousins" that agree up to a factor of 222 whenever TTT contains the origin, and agree exactly when TTT is origin-symmetric.

Formalization targets

Goal (Theorem 9.1.1, Matrix deviation inequality)

∃ C>0:Esup⁡x∈T∣ ∥Ax∥2−m∥x∥2 ∣  ≤  CK2γ(T)\exists\,C>0:\quad \mathbb E\sup_{x\in T}\bigl|\,\|Ax\|_2-\sqrt m\|x\|_2\,\bigr| \;\le\; CK^2\gamma(T)∃C>0:Ex∈Tsup​​∥Ax∥2​−m​∥x∥2​​≤CK2γ(T)

for every m×nm\times nm×n matrix AAA whose rows A1,…,AmA_1,\dots,A_mA1​,…,Am​ are independent, isotropic, sub-gaussian random vectors with K:=max⁡i∥Ai∥ψ2K:=\max_i\|A_i\|_{\psi_2}K:=maxi​∥Ai​∥ψ2​​, and every T⊆RnT\subseteq\mathbb R^nT⊆Rn (whenever γ(T)\gamma(T)γ(T) is finite). CCC is the book's own unnamed absolute constant, hard-coded to no numeral — the weakest stable form of the claim.

Milestone (Theorem 9.4.2, the M∗M^*M∗ bound)

E diam(T∩ker⁡A)  ≤  CK2w(T)m\mathbb E\,\mathrm{diam}(T\cap\ker A) \;\le\; \frac{CK^2w(T)}{\sqrt m}Ediam(T∩kerA)≤m​CK2w(T)​

for the same class of matrices AAA and any bounded T⊆RnT\subseteq\mathbb R^nT⊆Rn, where ker⁡A\ker AkerA is the (random) kernel of AAA, a subspace of codimension at most mmm. A direct one-paragraph consequence of the goal theorem (apply it to T−TT-TT−T, then restrict to ker⁡A\ker AkerA, where ∥Ax−Ay∥2\|Ax-Ay\|_2∥Ax−Ay∥2​ vanishes).

Significance

The matrix deviation inequality converts a purely algebraic quantity — how close ∥Ax∥2\|Ax\|_2∥Ax∥2​ stays to m∥x∥2\sqrt m\|x\|_2m​∥x∥2​ — into a single geometric parameter of the index set TTT, letting it subsume, via specializations of TTT, results that were previously proved by separate ad hoc arguments: two-sided singular value bounds on random matrices (TTT a sphere), Johnson-Lindenstrauss-type embeddings for possibly infinite point sets (TTT a difference set), and covariance estimation. The M∗M^*M∗ bound is one of the two classical consequences the book develops fresh from the inequality (the other, the Escape theorem, is outside this mission's scope): it answers, quantitatively, how large a random affine section of a fixed convex body typically is, a question at the heart of the local theory of Banach spaces and of compressed sensing's recovery guarantees (Chapter 10 builds directly on this chapter's machinery). Both results have long-standing, well-understood classical proofs; this mission formalizes their statements, not open research.

Difficulty

The natural first idea — bound ∥Ax∥2−m∥x∥2\|Ax\|_2-\sqrt m\|x\|_2∥Ax∥2​−m​∥x∥2​ pointwise for a fixed xxx using concentration of the norm of a sub-gaussian random vector, then take a union bound over TTT — only works when TTT is finite, and gives a bound that scales with log⁡∣T∣\log|T|log∣T∣ rather than with the actual geometric size of TTT. The book's actual route treats Xx:=∥Ax∥2−m∥x∥2X_x:=\|Ax\|_2-\sqrt m\|x\|_2Xx​:=∥Ax∥2​−m​∥x∥2​, indexed by x∈Rnx\in\mathbb R^nx∈Rn, as a genuine random process and shows it has sub-gaussian increments (∥Xx−Xy∥ψ2≤CK2∥x−y∥2\|X_x-X_y\|_{\psi_2}\le CK^2\|x-y\|_2∥Xx​−Xy​∥ψ2​​≤CK2∥x−y∥2​) — itself a nontrivial fact proved in stages (first for a single unit vector via concentration of the norm, Theorem 3.1.1; then for a pair of unit vectors via a squared-process argument; only then in full generality) — and then invokes Talagrand's comparison inequality (a consequence of the chaining machinery of Chapter 8) to pass from sub-gaussian increments directly to a bound in terms of Gaussian complexity, without ever performing a union bound over TTT itself.

Formalization scope

A is represented by its rows, A : Fin m → Ω → EuclideanSpace ℝ (Fin n), with ‖Ax‖₂ recovered as Real.sqrt (∑ i, ⟨Aᵢ,x⟩²) rather than constructing A as a Matrix/LinearMap — this matches the book's own row-by-row hypotheses exactly and is what both theorems' own proofs use directly. IsIsotropic is formalized via the book's basis-free Lemma 3.2.3 characterization (E⟨X,x⟩² = ‖x‖² for every x) rather than the matrix equation Σ(X)=Iₙ, avoiding a fixed-basis covariance-matrix construction the rest of this chunk's definitions do not otherwise need. SubgaussianVectorNorm reuses the published scalar subgaussianNorm. GaussianWidth and GaussianComplexity realize the standard Gaussian vector g ∼ N(0,Iₙ) as the identity map on Mathlib's own standard Gaussian measure on a finite-dimensional inner product space (ProbabilityTheory.stdGaussian), and both, together with the goal's own left-hand side, use a locally-defined finite-marginal expected-supremum convention (ExpSup, EReal-valued) matching the book's own footnote-3 convention (Section 7.2), reused throughout the series. Both theorems' right-hand sides presuppose their respective geometric parameter (γ(T)\gamma(T)γ(T) or w(T)w(T)w(T)) is a finite real number; since both are EReal-valued in general, each theorem takes an explicit real witness together with a proof that it equals the true value — the same finiteness-disclosure pattern 07-chaining's Dudley inequality uses for its own right-hand integral, needed here for exactly the same reason (the book's own display does not spell out why the quantity is finite, true whenever TTT is bounded, as in every application). CCC (and, in the milestone, the same CCC again — the two are not asserted equal, matching that the book states them as two separate "absolute constants") is existentially quantified before every type, instance and hypothesis it is uniform over. The M∗M^*M∗ bound milestone (m_star_bound) additionally carries the hypothesis m>0m > 0m>0: its conclusion divides by m\sqrt mm​, and without this hypothesis Lean's real-division convention (x/0=0x/0=0x/0=0) makes the right-hand side 000 at m=0m=0m=0 regardless of C,K,w(T)C, K, w(T)C,K,w(T) — false whenever TTT has positive diameter, not merely a weaker or vacuous claim. The book's own proof ("Dividing by m\sqrt mm​ yields …", p. 241) already implicitly assumes m≥1m \ge 1m≥1, matching every other use of mmm in the chapter as a positive count of measurement rows.

A trivializing formalization would fix TTT to be a finite set, collapsing the goal to the elementary union-bound case the book explicitly contrasts its own more general statement against (Section 9.1's opening paragraph: "we may choose an arbitrary subset T⊆RnT\subseteq\mathbb R^nT⊆Rn"); this mission's goal quantifies over an arbitrary Set (EuclideanSpace ℝ (Fin n)) to rule that out.

This mission covers Theorem 9.1.1 and Theorem 9.4.2 only; Theorem 9.4.7 (the Escape theorem) and Theorem 9.2.4 (covariance estimation for lower-dimensional distributions), both named as candidate milestones, are left out for lack of session time given the substantial shared infrastructure this chapter needed from scratch. ExpSup, IsIsotropic, SubgaussianVectorNorm, GaussianWidth and GaussianComplexity are reusable by any later chapter needing an isotropic or sub-gaussian random vector, or a Gaussian-width-type quantity (Chapters 4, 10, 11 of this same book series all use one or more of these notions). Solvers' contributions are welcome on: Theorem 9.1.3 (the sub-gaussian increments of the deviation process, the technical heart of the goal's proof), Talagrand's comparison inequality itself (outside this mission, in 07-chaining's companion chapter), and the one-paragraph reduction from the goal to the M∗M^*M∗ bound.

Selected references

  • S. Mendelson, A. Pajor, N. Tomczak-Jaegermann, Reconstruction and subgaussian operators in asymptotic geometric analysis, Geometric and Functional Analysis 17 (2007), 1248–1282. https://doi.org/10.1007/s00039-007-0618-7
  • V. D. Milman, A new proof of A. Dvoretzky's theorem on cross-sections of convex bodies, Funkcional. Anal. i Priložen. 5 (1971), 28–37.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 9. https://doi.org/10.1017/9781108231596
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High-Dimensional Probability VIII: Dudley's Integral InequalityTextbook

Motivation

Many questions in high-dimensional probability reduce to bounding the expected supremum of a random process (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ — the maximum, over an entire indexed family of random variables, of how large any one of them can get. When TTT is finite this is routine (a union bound over ∣T∣|T|∣T∣ terms suffices), but the interesting cases have TTT infinite, even uncountable: a supremum over a continuum of test functions, a norm expressed as a supremum over a sphere, or an empirical process indexed by a whole class of functions. A naive union bound is unusable here, since ∣T∣|T|∣T∣ is infinite.

R. M. Dudley's 1967 entropy bound (R. M. Dudley, The sizes of compact subsets of Hilbert space and continuity of Gaussian processes, Journal of Functional Analysis 1 (1967), 290–330) resolved this for Gaussian processes, controlling the expected supremum purely in terms of the metric entropy of TTT — how many balls of radius ε\varepsilonε are needed to cover TTT, at every scale ε\varepsilonε. The technique behind the proof, chaining, builds a sequence of increasingly fine finite approximations to TTT and telescopes the resulting bounds; it is one of the central tools of the field, reused throughout empirical process theory, statistical learning theory (via Vapnik-Chervonenkis theory), and non-asymptotic random matrix theory. This mission formalizes the chapter's generalization of Dudley's bound beyond Gaussian processes, to any process with sub-gaussian increments, together with the purely combinatorial Sauer-Shelah lemma that the chapter's applications to statistical learning theory build on.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P). A random process is a family (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ of real random variables on (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) indexed by an arbitrary set TTT, with no independence or measurability-of-the-supremum assumed between different ttt's. Since sup⁡t∈TXt(ω)\sup_{t\in T}X_t(\omega)supt∈T​Xt​(ω) need not be measurable in ω\omegaω for a general index set TTT, its expectation is understood — following the book's own convention, set once in Chapter 7 and reused throughout — through the process's finite-dimensional marginals:

Esup⁡t∈TXt  :=  sup⁡T0⊆T finite, nonempty Emax⁡t∈T0Xt.\mathbb E\sup_{t\in T}X_t \;:=\; \sup_{T_0\subseteq T\text{ finite, nonempty}}\ \mathbb E\max_{t\in T_0}X_t.Et∈Tsup​Xt​:=T0​⊆T finite, nonemptysup​ Et∈T0​max​Xt​.

Now fix a metric ddd on TTT, making (T,d)(T,d)(T,d) a metric space. The covering number N(T,d,ε)N(T,d,\varepsilon)N(T,d,ε), for ε>0\varepsilon>0ε>0, is the smallest cardinality of a finite ε\varepsilonε-net of TTT: a finite set N⊆TN\subseteq TN⊆T such that every point of TTT lies within distance ε\varepsilonε of some point of NNN (or N(T,d,ε):=∞N(T,d,\varepsilon):=\inftyN(T,d,ε):=∞ if no finite ε\varepsilonε-net exists). The quantity log⁡N(T,d,ε)\log N(T,d,\varepsilon)logN(T,d,ε) is the metric entropy of TTT at scale ε\varepsilonε: it measures how large TTT looks when resolved only down to scale ε\varepsilonε.

A process (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ has sub-gaussian increments with parameter K≥0K\ge0K≥0 if

∥Xt−Xs∥ψ2  ≤  K d(t,s)for all t,s∈T,\|X_t-X_s\|_{\psi_2}\;\le\;K\,d(t,s)\qquad\text{for all }t,s\in T,∥Xt​−Xs​∥ψ2​​≤Kd(t,s)for all t,s∈T,

where ∥⋅∥ψ2\|\cdot\|_{\psi_2}∥⋅∥ψ2​​ is the sub-gaussian (Orlicz) norm of Chapter 2: the smallest u>0u>0u>0 with Eexp⁡((Xt−Xs)2/u2)≤2\mathbb E\exp((X_t-X_s)^2/u^2)\le2Eexp((Xt​−Xs​)2/u2)≤2. This says the increments of the process are controlled by the metric ddd the way a Gaussian process's increments are controlled by its own canonical metric d(t,s):=∥Xt−Xs∥L2d(t,s):=\|X_t-X_s\|_{L^2}d(t,s):=∥Xt​−Xs​∥L2​ — but without assuming (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ is Gaussian.

A class of Boolean functions FFF on a set Ω\OmegaΩ shatters a subset Λ⊆Ω\Lambda\subseteq\OmegaΛ⊆Ω if every function g:Λ→{0,1}g:\Lambda\to\{0,1\}g:Λ→{0,1} arises as the restriction to Λ\LambdaΛ of some f∈Ff\in Ff∈F. The VC (Vapnik-Chervonenkis) dimension vc(F)\mathrm{vc}(F)vc(F) is the largest cardinality of a subset of Ω\OmegaΩ shattered by FFF (or ∞\infty∞ if arbitrarily large finite subsets, or an infinite one, are shattered) — a purely combinatorial measure of how rich the class FFF is.

Formalization targets

Goal (Theorem 8.1.3, Dudley's integral inequality)

∃ C>0:Esup⁡t∈TXt  ≤  CK∫0∞log⁡N(T,d,ε)  dε\exists\,C>0:\quad\mathbb E\sup_{t\in T}X_t\;\le\;CK\int_0^\infty\sqrt{\log N(T,d,\varepsilon)}\;d\varepsilon∃C>0:Et∈Tsup​Xt​≤CK∫0∞​logN(T,d,ε)​dε

for every mean-zero random process (Xt)t∈T(X_t)_{t\in T}(Xt​)t∈T​ on a metric space (T,d)(T,d)(T,d) with sub-gaussian increments parameter K≥0K\ge0K≥0, whenever the integral is finite. CCC is the book's own unnamed absolute constant, never depending on TTT, KKK, or the process. This is the weakest stable form of the claim: no numeral is hard-coded for CCC, and the statement asks only for the shape of the bound, matching what the book actually proves.

Milestone (Theorem 8.3.16, Sauer-Shelah lemma)

∣F∣  ≤  ∑k=0d(nk)  ≤  (end)d,d:=vc(F),|F|\;\le\;\sum_{k=0}^{d}\binom nk\;\le\;\left(\frac{en}{d}\right)^{d},\qquad d:=\mathrm{vc}(F),∣F∣≤k=0∑d​(kn​)≤(den​)d,d:=vc(F),

for every class FFF of Boolean functions on a finite nnn-point set Ω\OmegaΩ. This is a purely combinatorial fact, with no probability involved, but it is the bridge (via the covering-number bound Theorem 8.3.18, outside this mission's scope) between the chapter's Dudley-inequality engine and its statistical-learning applications — a bound on how large a finite class of Boolean functions can be, in terms of a single combinatorial complexity parameter.

Significance

Dudley's inequality is, in the book's own words, "the main result" of the chaining chapter: it converts a purely geometric quantity — the metric entropy of an index set, computable in many cases from covering-number estimates already available for balls, ellipsoids, and other convex bodies — into a probabilistic control on the size of a random process indexed by that set. This is what lets later chapters (uniform laws of large numbers over function classes, the matrix deviation inequality, the Dvoretzky-Milman theorem on almost-spherical sections of convex bodies) bound suprema over infinite, even uncountable, index sets without ever performing a union bound. The bound is also known to be tight only up to a logarithmic factor in general — Sudakov's minoration inequality (Chapter 7) gives a matching lower bound for Gaussian processes, and the book's own Exercise 8.1.12 exhibits a set where the two bounds genuinely diverge — so the constant CCC here cannot in general be sharpened away.

The Sauer-Shelah lemma is one of the two founding results of VC theory (together with the Glivenko-Cantelli-type uniform convergence it feeds into), independently discovered by Vapnik and Chervonenkis, Sauer, and Shelah in the early 1970s; it underlies the sample-complexity bounds of statistical learning theory (a hypothesis class with finite VC dimension is PAC-learnable) and, through Theorem 8.3.18, gives one of the two standard routes (the other being direct combinatorial counting) to bounding covering numbers of infinite function classes.

Both results are decades old and have long-established, standard proofs; no open mathematical question is being formalized. What this mission contributes is the machine-checked statement infrastructure — the goal and the Sauer-Shelah milestone, together with the definitions (CoveringNumber, ProcessESup, Shatters, VcDim) a faithful Lean rendering of either result needs — for a solver to close with a proof. No formalization of Dudley's inequality or the Sauer-Shelah lemma is known to exist on the platform prior to this mission.

Difficulty

The natural first idea for bounding Esup⁡t∈TXt\mathbb E\sup_{t\in T}X_tEsupt∈T​Xt​ is a single-scale ε\varepsilonε-net argument: replace TTT by a finite ε\varepsilonε-net, bound the maximum over the (finite) net by a union bound using the sub-gaussian tail, and separately bound the error of replacing TTT by the net using the Lipschitz-in-probability control the sub-gaussian-increments hypothesis gives. This works, but it only ever sees TTT at one fixed resolution ε\varepsilonε, and optimizing over ε\varepsilonε afterward gives a bound with an extra log⁡(1/ε)\sqrt{\log(1/\varepsilon)}log(1/ε)​-type loss that does not match Dudley's inequality. The actual difficulty is genuinely multi-scale: chaining builds a whole sequence of nets at dyadic scales ε=2−k\varepsilon=2^{-k}ε=2−k simultaneously, connects each point of TTT to its nearest net point at every scale to form a "chain" of successive approximations back to a single fixed basepoint, and telescopes the resulting sum of increments — turning XtX_tXt​ itself into a sum of differences between successive links of the chain, each individually well controlled by the sub-gaussian hypothesis at its own scale. Passing from the resulting discrete sum over dyadic scales (Theorem 8.1.4) to the continuous integral of the goal is a further, separate technical step.

For the Sauer-Shelah lemma, the natural first idea — bound ∣F∣|F|∣F∣ directly by counting — has no obvious purchase on an arbitrary class of Boolean functions. The actual argument goes through Pajor's lemma, which reduces bounding ∣F∣|F|∣F∣ to counting the shattered subsets of Ω\OmegaΩ instead of the functions in FFF themselves; only then does the cardinality bound d=vc(F)d=\mathrm{vc}(F)d=vc(F) on shattered sets become directly usable, via a binomial-sum estimate.

Formalization scope

CoveringNumber T ε is ℕ∞-valued (ℕ∞ = WithTop ℕ), defined as the infimum, over the subtype of finite ε\varepsilonε-nets of the whole type T (an instance of MetricSpace T), of their cardinality; the infimum of the empty family in this complete lattice is ⊤, reproducing "N:=∞N:= \inftyN:=∞ if no finite net exists" with no case split. ProcessESup is EReal-valued, defined as the supremum over finite nonempty T0⊆TT_0\subseteq TT0​⊆T of the Bochner integral of the finite max — EReal, not ℝ, because a real-valued supremum would silently return the junk value 000 if the family of marginal expectations were unbounded above. Shatters and VcDim are direct transcriptions of Definition 8.3.1, with VcDim valued in ℕ∞ via a supremum of Set.encard over the (always-nonempty, since ∅\varnothing∅ is trivially shattered) subtype of shattered subsets. The goal's mean-zero hypothesis is stated as Integrable (X t) P ∧ ∫ X t = 0 rather than the bare equation, since a non-integrable variable's Bochner integral is 0 in Mathlib by convention regardless of its true mean — a bare-equation hypothesis would let a non-mean-zero, non-integrable process satisfy the theorem vacuously. Two further hypotheses make explicit what the book's own displayed statement treats as understood without spelling out: that N(T,d,ε)N(T,d,\varepsilon)N(T,d,ε) is finite for every ε>0\varepsilon>0ε>0 (total boundedness of TTT), and that the resulting integrand is integrable on (0,∞)(0,\infty)(0,∞) — both hold whenever TTT is totally bounded, since the integrand vanishes once ε≥diam(T)\varepsilon\ge\mathrm{diam}(T)ε≥diam(T), so neither hypothesis excludes any case the book's own proof does not also need. [Nonempty T] excludes the degenerate empty index set. The absolute constant CCC is existentially quantified ahead of every type, instance, and hypothesis it is uniform over, and pinned to no numeral, matching "CCC is an absolute constant" — a formalization hard-coding a specific numeral for CCC would be invalidated by the next sharper constant in the literature and would not match what the book proves.

A trivializing formalization of the Sauer-Shelah lemma would fix vc(F)\mathrm{vc}(F)vc(F) at a hard-coded small value, or drop the second (exponential) inequality in favor of the weaker first one; this mission's statement keeps both inequalities, with ddd genuinely computed from VcDim, and handles the d=0d=0d=0 boundary (where the exponential bound's base involves a division by zero under Lean's x/0=0 convention) explicitly rather than excluding it, since x^0=1 still recovers the book's correct bound ∣F∣≤1|F|\le1∣F∣≤1 there.

This mission covers Theorem 8.1.3 and Theorem 8.3.16 only; Theorem 8.3.18 (covering numbers via VC dimension) and Theorem 8.2.3 (the uniform law of large numbers, the chapter's direct application of Dudley's inequality) are left out, not approximated, for lack of the additional empirical- process measurability machinery — the class of Lipschitz functions of Eq. (8.22), measurability of the resulting empirical process — that a faithful statement of either would need beyond what this mission's items already provide. CoveringNumber and ProcessESup are reusable by any later chapter needing a metric space's covering numbers or a general random process's expected supremum (this book's own Chapters 7, 9, and 11 all use one or both); Shatters and VcDim are reusable by any later development of VC theory or statistical learning theory. Solvers' contributions are welcome on: the chaining argument itself (the mission's hardest open leaf, via the discrete dyadic form of Theorem 8.1.4), Pajor's lemma underlying Sauer-Shelah, and the binomial-sum estimate closing its second inequality.

Selected references

  • R. M. Dudley, The sizes of compact subsets of Hilbert space and continuity of Gaussian processes, Journal of Functional Analysis 1 (1967), 290–330. https://doi.org/10.1016/0022-1236(67)90017-1
  • N. Sauer, On the density of families of sets, Journal of Combinatorial Theory, Series A 13 (1972), 145–147. https://doi.org/10.1016/0097-3165(72)90019-2
  • V. N. Vapnik, A. Ya. Chervonenkis, On the uniform convergence of relative frequencies of events to their probabilities, Theory of Probability & Its Applications 16 (1971), 264–280. https://doi.org/10.1137/1116025
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 8. https://doi.org/10.1017/9781108231596
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High-Dimensional Probability IV: Norms of Random Matrices with Sub-gaussian EntriesTextbook

Motivation

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

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

Setting

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

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

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

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

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

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

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

Formalization targets

Goal (Theorem 4.4.5)

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

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

Selected references

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

Motivation

Many hard combinatorial optimization problems — finding the maximum cut of a graph, deciding the ground state of an Ising spin system, bounding the correlation of a physical system — can be written as maximizing a bilinear form over sign vectors xi∈{−1,1}x_i \in \{-1, 1\}xi​∈{−1,1}. Exhaustive search over 2n2^n2n sign patterns is intractable, so practitioners relax the problem: replace each sign xix_ixi​ by a unit vector XiX_iXi​ in a higher-dimensional space and optimize the resulting inner products instead. This relaxation, a semidefinite program, is convex and solvable in polynomial time. The question is how much is lost in the relaxation — whether its optimal value can be far from the true, combinatorial optimum.

Grothendieck's inequality, proved by Alexander Grothendieck in 1953 in the context of Banach space theory (Résumé de la théorie métrique des produits tensoriels topologiques, Bol. Soc. Mat. São Paulo 8 (1953), 1–79), answers this for a broad class of such relaxations: replacing signs by unit vectors in an arbitrary Hilbert space changes the optimal value by at most an absolute, dimension-free constant factor. The inequality has since become a standard tool across combinatorial optimization, Banach space geometry, and (via the Goemans-Williamson algorithm for maximum cut, Section 3.6 of the source) approximation algorithms; see U. Haagerup, The Grothendieck inequality for bilinear forms on C∗C^*C∗-algebras, Adv. Math. 56 (1985) for the tightest known constant, and Alon–Naor, Approximating the cut-norm via Grothendieck's inequality, SIAM J. Comput. 35 (2006), for the algorithmic connection this mission's Theorem 3.5.6 sets up.

Setting

Fix positive integers m,nm, nm,n. Consider a real m×nm \times nm×n matrix A=(aij)A = (a_{ij})A=(aij​). Say AAA is normalized if for every choice of numbers x1,…,xm,y1,…,yn∈{−1,1}x_1, \dots, x_m, y_1, \dots, y_n \in \{-1, 1\}x1​,…,xm​,y1​,…,yn​∈{−1,1},

∣∑i=1m∑j=1naij xiyj∣  ≤  1.\Bigl| \sum_{i=1}^m \sum_{j=1}^n a_{ij}\, x_i y_j \Bigr| \;\le\; 1.​i=1∑m​j=1∑n​aij​xi​yj​​≤1.

This says AAA, viewed as a bilinear form on {−1,1}m×{−1,1}n\{-1,1\}^m \times \{-1,1\}^n{−1,1}m×{−1,1}n, has sup-norm at most 111. Now let HHH be any real Hilbert space — a real vector space equipped with an inner product ⟨⋅,⋅⟩\langle \cdot, \cdot \rangle⟨⋅,⋅⟩ complete in the induced norm — and consider vectors u1,…,um∈Hu_1, \dots, u_m \in Hu1​,…,um​∈H and v1,…,vn∈Hv_1, \dots, v_n \in Hv1​,…,vn​∈H, each of unit norm ∥ui∥=∥vj∥=1\|u_i\| = \|v_j\| = 1∥ui​∥=∥vj​∥=1. Replacing the scalar product xiyjx_i y_jxi​yj​ by the inner product ⟨ui,vj⟩\langle u_i, v_j \rangle⟨ui​,vj​⟩ in the same bilinear form gives ∑i,jaij⟨ui,vj⟩\sum_{i,j} a_{ij} \langle u_i, v_j \rangle∑i,j​aij​⟨ui​,vj​⟩, a real number depending on the choice of HHH and of the unit vectors. The question is how large this can be, uniformly over every such choice.

Formalization targets

Grothendieck's inequality (Theorem 3.5.1)

A normalized  ⟹  ∣∑i,jaij ⟨ui,vj⟩∣  ≤  KA \text{ normalized} \;\Longrightarrow\; \Bigl| \sum_{i,j} a_{ij}\, \langle u_i, v_j\rangle \Bigr| \;\le\; KA normalized⟹​i,j∑​aij​⟨ui​,vj​⟩​≤K

for every real Hilbert space HHH and unit vectors ui,vj∈Hu_i, v_j \in Hui​,vj​∈H, where KKK is a constant depending on neither AAA, its dimensions, nor HHH. This mission's goal formalizes the book's own first-pass bound K≤288K \le 288K≤288 (Section 3.5), proved by a Gaussian truncation argument; it does not fix a numeral for KKK, only that some absolute constant works, matching the shape of the true statement rather than a specific numeral that a sharper argument (the book's own Section 3.7 gives K≤1.783K \le 1.783K≤1.783) would immediately obsolete. See Formalization scope below for why this is the goal, not the sharper bound.

Significance

The result itself. Grothendieck's inequality is the single fact that makes semidefinite relaxation a provably good algorithmic strategy rather than a heuristic: whatever the true, hard-to-compute combinatorial optimum of a {−1,1}\{-1,1\}{−1,1}-valued bilinear optimization is, the tractable Hilbert-space relaxation cannot overshoot it by more than the constant KKK. Milestone Theorem 3.5.6 makes this concrete for positive-semidefinite matrices, showing the semidefinite relaxation SDP(A)(A)(A) of the integer program INT(A)(A)(A) satisfies INT(A)≤(A) \le(A)≤ SDP(A)≤2K⋅(A) \le 2K \cdot(A)≤2K⋅ INT(A)(A)(A) — the guarantee underlying the Goemans-Williamson 0.878-approximation algorithm for maximum cut (Theorem 3.6.5 of the source, out of scope for this mission; see Formalization scope).

Formalizing it. The inequality and its two chapter milestones are proved but not previously formalized on this platform (checked by concept search for "Grothendieck", "semidefinite", "positive-semidefinite", and "max-cut" — no hits beyond the unrelated Grothendieck-Teichmüller group). What remains after this mission is the sharper K≤1.783K \le 1.783K≤1.783 argument of Section 3.7 (the "kernel trick"), a separate, heavier development building on positive-definite kernels, and full proofs of every milestone below (currently open sorry goals).

Difficulty

The statement of Grothendieck's inequality contains no randomness, yet every known elementary proof is probabilistic; this is itself a striking feature of the result. The obvious approach — bound ∑i,jaij⟨ui,vj⟩\sum_{i,j} a_{ij}\langle u_i,v_j\rangle∑i,j​aij​⟨ui​,vj​⟩ directly by exploiting the normalization hypothesis on AAA — fails because the normalization hypothesis only controls AAA against sign vectors, and there is no way to project an arbitrary unit vector in a Hilbert space onto {−1,1}\{-1,1\}{−1,1} without losing information. The book's proof instead represents each unit vector ui,vju_i, v_jui​,vj​ via a scalar Gaussian random variable ⟨g,ui⟩\langle g, u_i\rangle⟨g,ui​⟩ for a single Gaussian vector ggg, recovering the inner products in expectation (Exercise 3.3.5); but these Gaussian variables are unbounded, so the normalization hypothesis (which bounds AAA against bounded ±1\pm 1±1 inputs) cannot be applied to them directly. The core technical step is a truncation argument: splitting each Gaussian variable into a bounded part and a small-L2L^2L2-norm unbounded remainder, applying the hypothesis to the bounded parts, and bounding the remainder terms by treating them as elements of the Hilbert space L2L^2L2 and invoking the very inequality being proved (Theorem 3.5.1 itself, applied with H=L2H = L^2H=L2) as a self-referential bootstrap — this is why the proof fixes KKK as the smallest valid constant before starting, rather than building it up from scratch.

Formalization scope

The goal and both milestones work with the real matrix and real inner product space directly; H is required to be a complete real inner product space (NormedAddCommGroup, InnerProductSpace ℝ, CompleteSpace), matching the book's "any Hilbert space." No dimension bound on HHH is imposed — the inequality's content is exactly that KKK does not grow with dim⁡H\dim HdimH.

This mission does not formalize the sharper K≤1.783K \le 1.783K≤1.783 bound of Section 3.7, nor Theorem 3.6.5 (the 0.878-approximation guarantee for maximum cut via randomized rounding): the latter's statement quantifies over "the result of a randomized rounding of the solution of the semidefinite program," which would drag a specific algorithm into the audited statement rather than keeping it a self-contained mathematical claim (the statement/proof-separation trap this series' triage rubric flags). Grothendieck's identity (Lemma 3.6.6), the key fact behind that rounding step, is included on its own as a milestone, stated with an explicit, named random sign variable rather than an opaque "rounding procedure."

A trivializing formalization would state the goal with KKK allowed to depend on AAA, mmm, nnn, or HHH — every such bound is easy (e.g. K=∑ij∣aij∣K = \sum_{ij} |a_{ij}|K=∑ij​∣aij​∣) and carries none of the theorem's content; the Lean statement rules this out by quantifying KKK before every other object. INT(A)\mathrm{INT}(A)INT(A) and SDP(A)\mathrm{SDP}(A)SDP(A) (Theorem 3.5.6) are defined from scratch in this chunk's namespace, using Matrix.PosSemidef from Mathlib for the positive-semidefiniteness hypothesis (which bundles the real-symmetric condition); Mathlib has no ready-made SDP-value construction to reuse. The sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm used by Theorem 3.1.1 is reused, unchanged, from the 01-concentration mission in this series (HighDimProb.Concentration.SubgaussianNorm) rather than redefined.

Selected references

  • A. Grothendieck, Résumé de la théorie métrique des produits tensoriels topologiques, Bol. Soc. Mat. São Paulo 8 (1953), 1–79.
  • U. Haagerup, The Grothendieck inequality for bilinear forms on C∗C^*C∗-algebras, Adv. Math. 56 (1985), 93–116.
  • N. Alon, A. Naor, Approximating the cut-norm via Grothendieck's inequality, SIAM J. Comput. 35 (2006), 787–803.
  • M. X. Goemans, D. P. Williamson, Improved approximation algorithms for maximum cut and satisfiability problems using semidefinite programming, J. ACM 42 (1995), 1115–1145.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 3, DOI 10.1017/9781108231596.
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High-Dimensional Probability V: The Johnson-Lindenstrauss LemmaTextbook

Motivation

Any dataset of NNN points can be described exactly by embedding it in Rn\mathbb R^nRn for nnn large enough — but a large nnn is expensive: nearest-neighbor search, clustering, and streaming algorithms all scale with the ambient dimension, not with NNN. The question that opens this mission is whether the dimension can be cut down while leaving the data's geometry — the pairwise distances between points — essentially untouched.

Johnson and Lindenstrauss answered this in 1984, while studying extensions of Lipschitz maps into Hilbert space (W. Johnson, J. Lindenstrauss, Extensions of Lipschitz mappings into a Hilbert space, Contemp. Math. 26 (1984), 189–206): NNN points in any Euclidean space, of any dimension nnn, can be mapped by a single linear map into a space of dimension only O(ε−2log⁡N)O(\varepsilon^{-2}\log N)O(ε−2logN), distorting every pairwise distance by at most a factor of 1±ε1\pm\varepsilon1±ε. The map does not depend on the data beyond its cardinality — a single random object works simultaneously for the whole point set with high probability. This is now one of the standard tools of randomized dimension reduction, cited across nearest-neighbor search, streaming linear algebra, compressed sensing, and machine learning pipelines that need to shrink feature dimension before a downstream algorithm runs.

Setting

Fix a probability space (Ω,F,Prob)(\Omega,\mathcal F,\mathrm{Prob})(Ω,F,Prob). A random orthogonal projection of rank mmm in Rn\mathbb R^nRn is a map P:Ω→(Rn→Rn)P:\Omega\to(\mathbb R^n\to\mathbb R^n)P:Ω→(Rn→Rn), continuous and linear for each ω\omegaω, such that almost surely PωP_\omegaPω​ is idempotent (Pω∘Pω=PωP_\omega\circ P_\omega = P_\omegaPω​∘Pω​=Pω​), self-adjoint, and has range of dimension mmm — i.e. PωP_\omegaPω​ is the orthogonal projection onto some mmm-dimensional subspace Eω⊂RnE_\omega\subset\mathbb R^nEω​⊂Rn. It is uniformly distributed in the Grassmannian Gn,mG_{n,m}Gn,m​ (written E∼Unif(Gn,m)E\sim\mathrm{Unif}(G_{n,m})E∼Unif(Gn,m​)) when its law is rotation invariant: for every orthogonal transformation UUU of Rn\mathbb R^nRn, the conjugated map ω↦U∘Pω∘U−1\omega\mapsto U\circ P_\omega\circ U^{-1}ω↦U∘Pω​∘U−1 has the same law as PPP. Conjugating a projection by UUU is exactly the projection onto the image of its range under UUU, so this says the law of the random subspace E=range(P)E=\mathrm{range}(P)E=range(P) is invariant under the full orthogonal group — the operational definition Vershynin himself uses for a "uniformly distributed" random subspace, since no coordinate-free formula for such a subspace's law is given directly.

A companion notion drives the proof: a random vector XXX is uniform on the Euclidean sphere of radius rrr, X∼Unif(r Sn−1)X\sim\mathrm{Unif}(r\,S^{n-1})X∼Unif(rSn−1), when it lies on that sphere almost surely and its law is likewise rotation invariant. And a real random variable YYY is sub-gaussian with sub-gaussian (ψ2\psi_2ψ2​) norm ∥Y∥ψ2:=inf⁡{t>0:Eexp⁡(Y2/t2)≤2}\|Y\|_{\psi_2} := \inf\{t>0:\mathbb E\exp(Y^2/t^2)\le 2\}∥Y∥ψ2​​:=inf{t>0:Eexp(Y2/t2)≤2}, the standard non-asymptotic measure of how light-tailed YYY's distribution is (a bounded or Gaussian random variable has finite ψ2\psi_2ψ2​ norm; the tail probability P{∣Y∣≥s}\mathbb P\{|Y|\ge s\}P{∣Y∣≥s} then decays at least as fast as 2exp⁡(−cs2/∥Y∥ψ22)2\exp(-cs^2/\|Y\|_{\psi_2}^2)2exp(−cs2/∥Y∥ψ2​2​)).

Formalization targets

Goal (Theorem 5.3.1, Johnson-Lindenstrauss Lemma)

∃ C,c>0:m≥Cε2log⁡∣X∣  ⟹  Prob{∀x,y∈X: (1−ε)∥x−y∥2≤∥nm Pω(x−y)∥2≤(1+ε)∥x−y∥2}  ≥  1−2exp⁡(−cε2m)\exists\,C,c>0:\quad m\ge\frac{C}{\varepsilon^2}\log|X| \;\Longrightarrow\; \mathrm{Prob}\Bigl\{\forall x,y\in X:\ (1-\varepsilon)\|x-y\|_2\le \bigl\|\sqrt{\tfrac nm}\,P_\omega(x-y)\bigr\|_2\le(1+\varepsilon)\|x-y\|_2\Bigr\} \;\ge\;1-2\exp(-c\varepsilon^2 m)∃C,c>0:m≥ε2C​log∣X∣⟹Prob{∀x,y∈X: (1−ε)∥x−y∥2​≤​mn​​Pω​(x−y)​2​≤(1+ε)∥x−y∥2​}≥1−2exp(−cε2m)

for every finite X⊂RnX\subset\mathbb R^nX⊂Rn, every ε>0\varepsilon>0ε>0, and every random orthogonal projection PPP of rank mmm uniformly distributed in Gn,mG_{n,m}Gn,m​. The universal quantifier over pairs x,y∈Xx,y\in Xx,y∈X sits inside the single probability event — this is the union-bound content that makes the statement a genuine simultaneous guarantee for the whole point set, not a restatement of the single-vector lemma below for one fixed pair. Both constants are the book's own unnamed absolute constants, never depending on nnn, mmm, N=∣X∣N=|X|N=∣X∣, or ε\varepsilonε; this is the weakest stable form of the claim (no numeral is hard-coded for CCC or ccc), matching the book's own statement exactly.

Significance

The lemma gives a universal, data-oblivious dimension-reduction guarantee: the target dimension m=O(ε−2log⁡N)m=O(\varepsilon^{-2}\log N)m=O(ε−2logN) depends only on the number of points and the desired distortion, never on the ambient dimension nnn or on the geometry of the specific point set. This is what makes it usable as a black-box preprocessing step ahead of an algorithm whose cost scales with nnn — the projection is drawn once, without looking at the data, and works with high probability for every pairwise distance simultaneously. The bound is also known to be essentially optimal in NNN: Alon (Problems and results in extremal combinatorics, Discrete Math. 273 (2003)) showed a lower bound of Ω(ε−2log⁡N/log⁡(1/ε))\Omega(\varepsilon^{-2}\log N/\log(1/\varepsilon))Ω(ε−2logN/log(1/ε)) on the target dimension, so the log⁡N\log NlogN dependence cannot be removed.

The theorem itself has been proved for decades and admits several proof strategies (this book's route through Lipschitz concentration on the sphere; the original volume/measure-concentration argument; later "sparse" or structured variants of the projection for faster computation). This mission formalizes the classical dense-Gaussian-projection proof route as Vershynin presents it, building the sphere-concentration engine (Theorem 5.1.4) and the single-vector projection lemma (Lemma 5.3.2) that the union-bound argument for the goal rests on. No machine-checked formal proof of this chain is known to exist on the platform prior to this mission (see Formalization scope below); what is contributed is the statement infrastructure — the goal and its two direct supporting lemmas, stated with explicit, unpinned absolute constants — for solvers to close.

Difficulty

The natural first idea — bound the distortion of a single fixed vector under a random projection, then take a union bound over the (N2)\binom N2(2N​) pairwise differences — is exactly the strategy Lemma 5.3.2 and the goal use, but it does not by itself explain why the single-vector concentration bound (Lemma 5.3.2(b)) holds with the stated sub-gaussian-type tail. That bound is not elementary: it reduces to a uniform concentration statement for an arbitrary Lipschitz function of a uniformly random point on a high-dimensional sphere (Theorem 5.1.4), since ∥Pz∥2\|Pz\|_2∥Pz∥2​, viewed as a function of a rotated copy of zzz, is a 111-Lipschitz function on the sphere. Proving that every Lipschitz function concentrates — not just linear ones, for which sub-gaussianity was already established in Chapter 3 — needs a genuinely different tool: comparing the sub-level sets of an arbitrary Lipschitz function to spherical caps via an isoperimetric inequality on the sphere. This geometric input is what makes the concentration phenomenon behind Johnson-Lindenstrauss a dimension-free fact rather than a special property of coordinate projections.

Formalization scope

XXX is a Finset of points in EuclideanSpace ℝ (Fin n), matching "a set of NNN points"; NNN is read off as X.card. The random subspace E∈Gn,mE\in G_{n,m}E∈Gn,m​ is represented throughout by the orthogonal projection PPP onto it (IsUniformProjection), following the book's own statements, which are phrased in terms of PPP rather than EEE; the scaled map Q=n/m PQ=\sqrt{n/m}\,PQ=n/m​P of the goal is written Real.sqrt (n/m) • P ω applied to x - y, using linearity of PωP_\omegaPω​ to realize Qx−Qy=Q(x−y)Qx-Qy = Q(x-y)Qx−Qy=Q(x−y). Both "uniform on the sphere" and "uniform in the Grassmannian" are defined operationally by rotation invariance of the underlying law, since Mathlib has no ready-made normalized surface measure on a general-radius Euclidean sphere or Haar-measure construction on the Grassmannian/orthogonal group to build a canonical uniform object from; rotation invariance uniquely determines the corresponding measure among those supported on the relevant set, so the operational and constructive definitions coincide extensionally. Every "absolute constant" in the book (CCC in Theorem 5.3.1's sample-complexity hypothesis, ccc in every failure-probability bound, and the sub-gaussian constant CCC of Theorem 5.1.4) is existentially quantified ahead of the dimension, sample size, and every other object, and pinned to no numeral — a formalization that hard-coded a specific numeral for any of these would be invalidated by the next sharper constant in the literature and would not match what the book actually proves.

A trivializing formalization is one that states the conclusion for a single fixed pair x,yx,yx,y rather than universally over all pairs inside one event; that would collapse the union-bound content that makes this a dimension-reduction statement for a whole point set (with NNN points), rather than a restatement of the single-vector Lemma 5.3.2(b). This mission's goal statement is built to rule that out explicitly (see Formalization targets above).

Reusable infrastructure: subgaussianNorm (the Orlicz ψ2\psi_2ψ2​ norm, restated per Vershynin Definition 2.5.6) and the rotation-invariance idiom for "uniformly distributed" random geometric objects are of independent interest to any later chapter needing sub-gaussian random vectors or random subspaces/projections (e.g. Chapters 4, 6, 7, 9, 11 of this same book series). Solvers' contributions are welcome on: the isoperimetric inequality on the sphere and its use to prove Theorem 5.1.4 (the mission's hardest open leaf); the coordinate-projection computation underlying Lemma 5.3.2(a); and the concentration-plus-union-bound argument closing the goal from the three supporting lemmas.

Selected references

  • W. Johnson, J. Lindenstrauss, Extensions of Lipschitz mappings into a Hilbert space, Contemporary Mathematics 26 (1984), 189–206.
  • N. Alon, Problems and results in extremal combinatorics, I, Discrete Mathematics 273 (2003), 31–53. https://doi.org/10.1016/S0012-365X(03)00227-9
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 5. https://doi.org/10.1017/9781108231596
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Linear OptimizationOperations ResearchOptimization·Captain: mikedeng1

Understanding and Using Linear Programming IX: Basis Pursuit Recovers Sparse Solutions Exactly iff the Kernel Misses the CrosspolytopeTextbook

Motivation

A deep-space probe sends a vector w∈Rkw\in\mathbb{R}^kw∈Rk encoded as z=Qw∈Rnz=Qw\in\mathbb{R}^nz=Qw∈Rn, and up to about 8% of the transmitted numbers may be corrupted arbitrarily. Section 8.5 of Matoušek and Gärtner's Understanding and Using Linear Programming (Springer 2007, DOI 10.1007/978-3-540-30717-4) shows that decoding reduces to finding a sparse solution of an underdetermined linear system Ax=bAx=bAx=b, and that under suitable conditions this sparse solution is found exactly by a single linear program. The same problem arises in signal processing (sparse representations in redundant wavelet dictionaries) and in computer tomography, and it is the core of what became known as compressed sensing.

Timeline, as recorded in the book's references:

  • 1999: Chen, Donoho and Saunders introduce basis pursuit, minimizing the ℓ1\ell_1ℓ1​-norm subject to Ax=bAx=bAx=b (SIAM J. Sci. Comput. 20).
  • 2005: Candès, Rudelson, Tao and Vershynin prove that for every α∈(0,1)\alpha\in(0,1)α∈(0,1) there is β(α)>0\beta(\alpha)>0β(α)>0 such that a random ⌊αn⌋×n\lfloor\alpha n\rfloor\times n⌊αn⌋×n matrix is exact for ⌊βn⌋\lfloor\beta n\rfloor⌊βn⌋-sparse vectors with probability exponentially close to 1 (FOCS 2005).
  • 2006: Donoho, via neighborliness of centrally symmetric polytopes, obtains the constants α=0.75\alpha=0.75α=0.75, β=0.08\beta=0.08β=0.08 used in the book, and shows that no ⌊0.75n⌋×n\lfloor 0.75n\rfloor\times n⌊0.75n⌋×n matrix is exact for r>0.25nr>0.25nr>0.25n when nnn is large (Discrete Comput. Geom. 35).
  • 2006: Linial and Novik prove further upper bounds showing that these existence results are asymptotically optimal (Discrete Comput. Geom. 36).

Setting

Let AAA be a real m×nm\times nm×n matrix with m<nm<nm<n and b∈Rmb\in\mathbb{R}^mb∈Rm. The support of x∈Rnx\in\mathbb{R}^nx∈Rn is supp⁡(x)={i:xi≠0}\operatorname{supp}(x)=\{i: x_i\ne 0\}supp(x)={i:xi​=0}. For an integer r≥0r\ge 0r≥0, a sparse solution of Ax=bAx=bAx=b is an xxx with Ax=bAx=bAx=b and ∣supp⁡(x)∣≤r|\operatorname{supp}(x)|\le r∣supp(x)∣≤r. The ℓ1\ell_1ℓ1​-norm is ∥x∥1=∣x1∣+⋯+∣xn∣\|x\|_1=|x_1|+\dots+|x_n|∥x∥1​=∣x1​∣+⋯+∣xn​∣.

Basis pursuit is the optimization problem

(BP)minimize ∥x∥1  subject to x∈Rn, Ax=b,\text{(BP)}\qquad\text{minimize } \|x\|_1\ \text{ subject to } x\in\mathbb{R}^n,\ Ax=b,(BP)minimize ∥x∥1​  subject to x∈Rn, Ax=b,

which is equivalent to the linear program

(BP′)minimize u1+⋯+un  subject to Ax=b, −u≤x≤u, u≥0.\text{(BP}'\text{)}\qquad\text{minimize } u_1+\dots+u_n\ \text{ subject to } Ax=b,\ -u\le x\le u,\ u\ge 0 .(BP′)minimize u1​+⋯+un​  subject to Ax=b, −u≤x≤u, u≥0.

The matrix AAA is BP-exact for rrr if for every b∈Rmb\in\mathbb{R}^mb∈Rm: whenever Ax=bAx=bAx=b has a solution x~\tilde xx~ with at most rrr nonzero components, x~\tilde xx~ is the unique optimal solution of (BP). The crosspolytope is B1n={x:∥x∥1≤1}B^n_1=\{x:\|x\|_1\le 1\}B1n​={x:∥x∥1​≤1}, the kernel of AAA is L={x:Ax=0}L=\{x: Ax=0\}L={x:Ax=0}, and L+z={ℓ+z:ℓ∈L}L+z=\{\ell+z:\ell\in L\}L+z={ℓ+z:ℓ∈L}. For zzz with ∥z∥1=1\|z\|_1=1∥z∥1​=1, the cone at zzz is Cz={t(x−z):t≥0, x∈B1n}C_z=\{t(x-z): t\ge 0,\ x\in B^n_1\}Cz​={t(x−z):t≥0, x∈B1n​}, and LLL is good for zzz if (L+z)∩B1n={z}(L+z)\cap B^n_1=\{z\}(L+z)∩B1n​={z}.

Formalization targets

Goal: Lemma 8.5.4 (reformulation of BP-exactness)

For m<nm<nm<n and r≤mr\le mr≤m:

A is BP-exact for r  ⟺  ∀z∈Rn with ∥z∥1=1, ∣supp⁡(z)∣≤r:(L+z)∩B1n={z}.A \text{ is BP-exact for } r\iff \forall z\in\mathbb{R}^n\ \text{with}\ \|z\|_1=1,\ |\operatorname{supp}(z)|\le r:\quad (L+z)\cap B^n_1=\{z\}.A is BP-exact for r⟺∀z∈Rn with ∥z∥1​=1, ∣supp(z)∣≤r:(L+z)∩B1n​={z}.

This is the book's geometric characterization of exact recovery, and the statement on which the known probabilistic proofs are built.

Milestones

  1. Observation 8.5.1: Ax=bAx=bAx=b has at most one sparse solution for every bbb if and only if every 2r2r2r or fewer columns of AAA are linearly independent.
  2. The remark after it (p. 169): under m<nm<nm<n, that column condition forces m≥2rm\ge 2rm≥2r.
  3. Equivalence of (BP) and (BP′) (p. 170): in every optimal solution of (BP′), ui=∣xi∣u_i=|x_i|ui​=∣xi​∣; and xxx is optimal for (BP) iff (x,∣x∣)(x,|x|)(x,∣x∣) is optimal for (BP′).
  4. From the proof of Lemma 8.5.4 (p. 173): if Az=bAz=bAz=b, the solution set of Ax=bAx=bAx=b is exactly L+zL+zL+z.
  5. From "Intuition for BP-exactness" (p. 174): for ∥z∥1=1\|z\|_1=1∥z∥1​=1 and ∣supp⁡(z)∣≤r|\operatorname{supp}(z)|\le r∣supp(z)∣≤r, LLL is good for zzz iff L∩Cz={0}L\cap C_z=\{0\}L∩Cz​={0}.

Further draft item: Theorem 8.5.2

With m=⌊0.75n⌋m=\lfloor 0.75n\rfloorm=⌊0.75n⌋, r=⌊0.08n⌋r=\lfloor 0.08n\rfloorr=⌊0.08n⌋ and AAA an m×nm\times nm×n matrix of independent N(0,1)N(0,1)N(0,1) entries, there is a constant c>0c>0c>0 such that for every nnn

Pr⁡[A is BP-exact for r] ≥ 1−e−cm.\Pr[A \text{ is BP-exact for } r]\ \ge\ 1-e^{-cm}.Pr[A is BP-exact for r] ≥ 1−e−cm.

The book states this without proof. It is included as a separate theorem, not a milestone of the goal.

Significance

Lemma 8.5.4 converts an algorithmic property, that an ℓ1\ell_1ℓ1​ linear program returns a prescribed sparse vector for every right-hand side, into a purely geometric property of the kernel of AAA relative to the low-dimensional faces of the crosspolytope. With milestone 5 it becomes the statement that LLL avoids a finite family of cones, which is where union bounds over faces and estimates for random subspaces enter. Observation 8.5.1 separates what is information-theoretically possible (uniqueness of sparse solutions) from what is computationally achievable by linear programming; finding a sparse solution directly is NP-hard in general. Theorem 8.5.2 is the quantitative payoff: a fixed fraction of arbitrary gross errors can be corrected by solving one linear program.

All of these results are proved in the literature; Lemma 8.5.4, Observation 8.5.1 and the milestones are elementary, and Theorem 8.5.2 rests on Donoho's polytope-neighborliness analysis. The platform has a related formalization of Wainwright's restricted nullspace property (Theorem 7.8 of High-Dimensional Statistics, namespace HighDimStat.SparseLinear), which fixes a support set SSS rather than characterizing exactness for all rrr-sparse vectors through the crosspolytope. A machine-checked proof of Theorem 8.5.2 with the constants 0.750.750.75 and 0.080.080.08 is, to our knowledge, not available anywhere; it would require substantial Gaussian and high-dimensional geometry infrastructure.

Difficulty

For the goal and milestones the difficulty is bookkeeping, not ideas: the scaling between a sparse solution x~\tilde xx~ and the boundary point x~/∥x~∥1\tilde x/\|\tilde x\|_1x~/∥x~∥1​, the case x~=0\tilde x=0x~=0, and the fact that BP-exactness quantifies over all right-hand sides bbb while the geometric side quantifies over boundary points of the crosspolytope.

Theorem 8.5.2 is of a different order. A union bound over the (nr)2r\binom{n}{r}2^r(rn​)2r faces of dimension r−1r-1r−1 reduces it to bounding the probability that a random (n−m)(n-m)(n−m)-dimensional subspace meets one cone CFC_FCF​ nontrivially, and getting that probability small enough to beat the combinatorial factor with the stated numerical constants is the hard part. Rough asymptotic estimates do not give 0.080.080.08 at α=0.75\alpha=0.75α=0.75.

Formalization scope

Vectors are functions Fin n → ℝ (the book's indices 1,…,n1,\dots,n1,…,n become 0,…,n−10,\dots,n-10,…,n−1) and matrices are Matrix (Fin m) (Fin n) ℝ. The ℓ1\ell_1ℓ1​-norm is written out as ∑i∣xi∣\sum_i|x_i|∑i​∣xi​∣, since Mathlib's norm on Fin n → ℝ is the sup norm. The support is a Finset of indices. Optimality in (BP) and (BP′) is stated against every feasible point; no infimum is taken, so an empty or unbounded feasible set cannot create a spurious optimum. "Every 2r2r2r or fewer columns" ranges over finsets of distinct column indices, column jjj being Aᵀ j. The hypotheses m<nm<nm<n and r≤mr\le mr≤m of Lemma 8.5.4 are kept as on the page, although the equivalence does not use them; m<nm<nm<n is also the standing assumption of §8.5 needed for m≥2rm\ge 2rm≥2r.

In Theorem 8.5.2 the random matrix has the product law of independent gaussianReal 0 1 entries, the constant c>0c>0c>0 is quantified before nnn, and measurability of the BP-exact event is part of the conclusion, so the bound concerns a genuine probability rather than an outer measure.

A trivializing formalization is ruled out: BP-exactness requires uniqueness among all minimizers for every right-hand side, not just optimality of x~\tilde xx~, and the crosspolytope condition is an equality of sets, not an inclusion that zzz alone would satisfy.

All definitions live in one module (MatousekLP.SparseRecovery.BasisPursuit); the ℓ1\ell_1ℓ1​ and support vocabulary is reusable for later sparse-recovery missions. Contributions are welcome on every milestone, on the goal, and on the infrastructure towards Theorem 8.5.2 (Gaussian measures on matrix spaces, measurability of the BP-exact event, the face structure of the crosspolytope).

Selected references

  • J. Matoušek and B. Gärtner, Understanding and Using Linear Programming, Springer Universitext, 2007, §8.5. https://doi.org/10.1007/978-3-540-30717-4
  • S. S. Chen, D. L. Donoho and M. A. Saunders, Atomic decomposition by basis pursuit, SIAM J. Sci. Comput. 20(1), 1999, 33–61. https://doi.org/10.1137/S1064827596304010
  • E. J. Candès, M. Rudelson, T. Tao and R. Vershynin, Error correction via linear programming, Proc. 46th IEEE FOCS, 2005, 295–308. https://doi.org/10.1109/SFCS.2005.5464411
  • D. L. Donoho, High-dimensional centrally symmetric polytopes with neighborliness proportional to dimension, Discrete Comput. Geom. 35, 2006, 617–652. https://doi.org/10.1007/s00454-005-1220-0
  • N. Linial and I. Novik, How neighborly can a centrally symmetric polytope be?, Discrete Comput. Geom. 36, 2006, 273–281. https://doi.org/10.1007/s00454-006-1235-1
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Convex OptimizationMachine LearningProbability+1·Captain: mikedeng1

The Power of Convex Relaxation: Near-Optimal Matrix Completion II: Exact Nuclear-Norm Recovery from Nearly Minimally Many EntriesResearch Paper

Motivation

Many data sets are large matrices of which only a small fraction of the entries is observed, and of which the underlying object is believed to have low rank: user–item rating tables in collaborative filtering, distance matrices in sensor-network localization, and measurement matrices in structure-from-motion. Matrix completion asks when the missing entries can be recovered exactly. Rank minimization subject to the observed entries is intractable in general. Its convex relaxation, nuclear-norm minimization, is a semidefinite program, and the question is how many randomly placed entries it needs.

Timeline:

  • 2008–2009. Candès and Recht (arXiv:0805.4471) proved that nuclear-norm minimization recovers an incoherent n×nn\times nn×n matrix of rank rrr from about μ0n6/5rlog⁡n\mu_0 n^{6/5} r\log nμ0​n6/5rlogn uniformly sampled entries, and from n5/4n^{5/4}n5/4 in the low-rank regime. They also showed that about μ0nrlog⁡n\mu_0 nr\log nμ0​nrlogn entries are necessary for any method.
  • 2010. Candès and Tao (doi:10.1109/TIT.2010.2044061), the source of this mission, closed most of the gap. Under a strong incoherence assumption, Cμ2nrlog⁡6nC\mu^2 nr\log^6 nCμ2nrlog6n entries suffice (Theorem 1.2), within a polylogarithmic factor of the information-theoretic limit, which the same paper sharpens (Theorem 1.7).
  • 2009–2011. Keshavan, Montanari and Oh (arXiv:0901.3150) obtained comparable bounds for a non-convex method. Gross (arXiv:0910.1879) and Recht (arXiv:0910.0651) later gave much shorter proofs of an O(μ0nrlog⁡2n)O(\mu_0 nr\log^2 n)O(μ0​nrlog2n) bound under a different incoherence condition, using matrix Bernstein inequalities and a "golfing" construction of the dual certificate.

Setting

Fix M∈Rn×nM \in \mathbb{R}^{n\times n}M∈Rn×n of rank rrr with singular value decomposition M=∑k=1rσkukvk∗M = \sum_{k=1}^r\sigma_k u_kv_k^*M=∑k=1r​σk​uk​vk∗​, where σk>0\sigma_k>0σk​>0 and {uk}\{u_k\}{uk​}, {vk}\{v_k\}{vk​} are orthonormal. Let PU=∑kukuk∗P_U = \sum_k u_ku_k^*PU​=∑k​uk​uk∗​, PV=∑kvkvk∗P_V = \sum_k v_kv_k^*PV​=∑k​vk​vk∗​, and let E=∑kukvk∗E = \sum_k u_kv_k^*E=∑k​uk​vk∗​ be the sign matrix. The tangent space TTT at MMM is the image of the projection

PT(X)=PUX+XPV−PUXPV,\mathcal{P}_T(X) = P_UX + XP_V - P_UXP_V,PT​(X)=PU​X+XPV​−PU​XPV​,

and PT⊥=I−PT\mathcal{P}_{T^\perp} = \mathcal{I} - \mathcal{P}_TPT⊥​=I−PT​.

MMM obeys the strong incoherence property with parameter μ\muμ if every entry of PUP_UPU​ and PVP_VPV​ is within μr/n\mu\sqrt r/nμr​/n of the corresponding entry of (r/n)I(r/n)I(r/n)I, and every entry of EEE is at most μr/n\mu\sqrt r/nμr​/n in absolute value.

An observation set Ω⊆[n]×[n]\Omega \subseteq [n]\times[n]Ω⊆[n]×[n] is either a uniformly random mmm-subset (the uniform model) or contains each entry independently with probability p=m/n2p = m/n^2p=m/n2 (the Bernoulli model). PΩ\mathcal{P}_\OmegaPΩ​ keeps the entries in Ω\OmegaΩ and zeroes the rest. The program is

minimize ∥X∥∗ subject to PΩ(X)=PΩ(M),(I.3)\text{minimize } \|X\|_* \text{ subject to } \mathcal{P}_\Omega(X) = \mathcal{P}_\Omega(M), \qquad \text{(I.3)}minimize ∥X∥∗​ subject to PΩ​(X)=PΩ​(M),(I.3)

where ∥X∥∗\|X\|_*∥X∥∗​ is the sum of the singular values.

The analysis uses the centered operators QΩ=p−1PΩ−I\mathcal{Q}_\Omega = p^{-1}\mathcal{P}_\Omega - \mathcal{I}QΩ​=p−1PΩ​−I and QT=PT−ρ′I\mathcal{Q}_T = \mathcal{P}_T - \rho'\mathcal{I}QT​=PT​−ρ′I, where ρ=r/n\rho = r/nρ=r/n and ρ′=2ρ−ρ2\rho' = 2\rho-\rho^2ρ′=2ρ−ρ2. It also uses the random matrices (QΩQT)kQΩ(E)(\mathcal{Q}_\Omega\mathcal{Q}_T)^k\mathcal{Q}_\Omega(E)(QΩ​QT​)kQΩ​(E), where the operator is applied to EEE from the right. ∥⋅∥\|\cdot\|∥⋅∥ denotes the spectral norm.

Formalization targets

Goal: Theorem 1.2 (Matrix Completion II)

There is an absolute constant C>0C>0C>0 such that, for every fixed MMM as above and m≤n2m \le n^2m≤n2 uniformly sampled entries,

m≥Cμ2nrlog⁡6n  ⟹  Pr⁡[M is the unique solution of (I.3)]≥1−n−3.m \ge C\mu^2 nr\log^6 n \implies \Pr\bigl[M \text{ is the unique solution of (I.3)}\bigr] \ge 1 - n^{-3}.m≥Cμ2nrlog6n⟹Pr[M is the unique solution of (I.3)]≥1−n−3.

The constant CCC is not fixed; the goal asserts only its existence.

Milestones (in attack order)

  1. Lemma 3.1. A dual certificate YYY with PΩ(Y)=Y\mathcal{P}_\Omega(Y)=YPΩ​(Y)=Y, PT(Y)=E\mathcal{P}_T(Y)=EPT​(Y)=E, ∥PT⊥(Y)∥<1\|\mathcal{P}_{T^\perp}(Y)\|<1∥PT⊥​(Y)∥<1, together with injectivity of PΩ\mathcal{P}_\OmegaPΩ​ on TTT, implies unique recovery. This is already proved on the platform.
  2. Theorem 3.2 (Rudelson selection estimate). With probability at least 1−3n−β1-3n^{-\beta}1−3n−β,
p−1∥PTPΩPT−pPT∥≤CRμ0nrβlog⁡n/m,p^{-1}\|\mathcal{P}_T\mathcal{P}_\Omega\mathcal{P}_T - p\mathcal{P}_T\| \le C_R\sqrt{\mu_0nr\beta\log n/m},p−1∥PT​PΩ​PT​−pPT​∥≤CR​μ0​nrβlogn/m​,

provided the right-hand side is below 111. 3. Lemma 8.1. An exact expansion of (QΩPT)kQΩ(\mathcal{Q}_\Omega\mathcal{P}_T)^k\mathcal{Q}_\Omega(QΩ​PT​)kQΩ​ in powers of QΩQT\mathcal{Q}_\Omega\mathcal{Q}_TQΩ​QT​ with explicit recursive coefficients. 4. Lemma 8.2. The coefficients are at most λ⌈(k−j)/2⌉4k\lambda^{\lceil (k-j)/2\rceil}4^kλ⌈(k−j)/2⌉4k, with λ=ρ′/p\lambda = \rho'/pλ=ρ′/p. 5. Lemma 3.3. On the event ∥(QΩQT)kQΩ(E)∥≤σ(k+1)/2\|(\mathcal{Q}_\Omega\mathcal{Q}_T)^k\mathcal{Q}_\Omega(E)\| \le \sigma^{(k+1)/2}∥(QΩ​QT​)kQΩ​(E)∥≤σ(k+1)/2, the same terms with PT\mathcal{P}_TPT​ obey the bound with an extra factor 1+4k+11+4^{k+1}1+4k+1. 6. Theorem 3.6 (Moment bound II). Let A=(QΩQT)kQΩ(E)A = (\mathcal{Q}_\Omega\mathcal{Q}_T)^k\mathcal{Q}_\Omega(E)A=(QΩ​QT​)kQΩ​(E) and rμ=μ2rr_\mu = \mu^2 rrμ​=μ2r. Then

Etrace⁡((A∗A)j)≤n(C(j(k+1))6nrμ/m)j(k+1).\mathbb{E}\operatorname{trace}\bigl((A^*A)^j\bigr) \le n\bigl(C(j(k+1))^6nr_\mu/m\bigr)^{j(k+1)}.Etrace((A∗A)j)≤n(C(j(k+1))6nrμ​/m)j(k+1).
  1. Corollary 3.7. Under (I.12), with probability at least 1−n−31-n^{-3}1−n−3 the certificate (III.10) exists and has ∥PT⊥(Y)∥≤1/2\|\mathcal{P}_{T^\perp}(Y)\|\le 1/2∥PT⊥​(Y)∥≤1/2.

Significance

Theorem 1.2 shows that a polynomial-time convex program recovers an incoherent low-rank matrix from a number of entries that is linear in nrnrnr and within a polylogarithmic factor of what any method requires. It turned nuclear-norm minimization from a heuristic into a method with near-optimal guarantees, and much of the later work on low-rank recovery, robust PCA and phase retrieval uses its framework of dual certificates, tangent spaces and incoherence.

The theorem is proved; formalizing it is the remaining work here. None of these results has a machine-checked proof. The platform already has the Candès–Recht definitions (nuclear norm, SVD data, Bernoulli model, tangent projection), the deterministic Lemma 3.1, and the Bernoulli-to-uniform transfer. This mission adds:

  • the trace-moment bound, which is the combinatorial core of the paper;
  • the deterministic operator algebra of Appendix A;
  • the assembly into the main theorem.

Shorter later proofs (Gross, Recht) use a different incoherence condition. A formal proof of the goal along either route is welcome, provided it proves the statement as given.

Difficulty

The obvious approach bounds each term ∥(QΩPT)kQΩ(E)∥\|(\mathcal{Q}_\Omega\mathcal{P}_T)^k\mathcal{Q}_\Omega(E)\|∥(QΩ​PT​)kQΩ​(E)∥ of the Neumann series for the certificate separately, using noncommutative Khintchine inequalities and decoupling. This is what Candès and Recht did, and it fails beyond small kkk: the entries of these matrices are coupled through the same random indicators, and the bounds degrade with kkk. That is where their n6/5n^{6/5}n6/5 comes from.

The moment method avoids this but has its own obstruction. Taking absolute values inside the expansion of Etrace⁡(A∗A)j\mathbb{E}\operatorname{trace}(A^*A)^jEtrace(A∗A)j loses a factor of rrr, which gives the quadratic dependence of Theorem 1.1. The linear bound needs sign cancellations among the coefficients of QT\mathcal{Q}_TQT​ to be tracked through a nested induction over "generalized spider" configurations (Section VI). Replacing PT\mathcal{P}_TPT​ by QT\mathcal{Q}_TQT​ (Lemma 3.3) is necessary for those cancellations. Without it the diagonal coefficients are of size r/nr/nr/n instead of r/n\sqrt r/nr​/n.

Formalization scope

  • Objects. Matrices are Matrix (Fin n) (Fin n) ℝ (MatrixCompletion.RealMatrix). The SVD is the platform structure SVD M r. Logarithms are natural. Probabilities are the platform's finite sums: successProb (uniform mmm-subsets), bernoulliEventProb and bernoulliExpectation. The spectral norm is spectralNorm. The definitions of matrix_completion_{basic,svd,bernoulli,tangent} are reused, not restated.
  • Square case. Theorem 1.2 is printed "under the same hypotheses as in Theorem 1.1", for n1×n2n_1\times n_2n1​×n2​ matrices. The paper proves only n1=n2=nn_1=n_2=nn1​=n2​=n (Section I-H), and the goal and milestones 3–7 are square. Theorem 3.2 is quoted from Candès–Recht and is stated rectangular, as printed.
  • Rank. "The same hypotheses" is read as the matrix hypotheses (fixed MMM, strong incoherence, uniform sampling), not as r=O(1)r = O(1)r=O(1): (I.12) carries rrr, the paper calls the result general and nonasymptotic, and Section VI never uses bounded rank. The goal holds for every rrr.
  • Constants. Every "numerical constant" (CCC, CRC_RCR​, c0c_0c0​) and every O(⋅)O(\cdot)O(⋅) is an existential absolute constant quantified before all other variables. The goal's CCC absorbs the standing assumptions n≥C′n \ge C'n≥C′ and m≥2nrm\ge 2nrm≥2nr. Where a milestone needs (I.22), 2nr≤m2nr\le m2nr≤m is an explicit hypothesis, and m≤n2m\le n^2m≤n2 is explicit wherever a probability or p≤1p\le 1p≤1 appears.
  • Correction of Theorem 3.6. The printed bound (III.27) omits the factor nnn and the O(1)j(k+1)O(1)^{j(k+1)}O(1)j(k+1) constant of the paper's own final display (p. 2070), and as printed it is false: for k=0k=0k=0, j=1j=1j=1 and a flat rank-one matrix, the left side exceeds the right by the factor n(1−p)n(1-p)n(1−p). The formal statement is the bound the paper derives, n (C(j(k+1))6nrμ/m)j(k+1)n\,(C(j(k+1))^6nr_\mu/m)^{j(k+1)}n(C(j(k+1))6nrμ​/m)j(k+1), under nrμ≤mnr_\mu\le mnrμ​≤m, which that derivation uses and which (I.12) implies. The milestone text is kept verbatim.
  • Deterministic lemmas. Lemmas 3.3, 8.1 and 8.2 hold for every fixed Ω\OmegaΩ. The event (III.18) is a hypothesis, not a probability.
  • Certificate. YYY of (III.10) exists only when PΩ\mathcal{P}_\OmegaPΩ​ is injective on TTT, so Corollary 3.7's event includes injectivity. YYY is characterized as the minimum-Frobenius-norm solution of PΩ(Y)=Y\mathcal{P}_\Omega(Y)=YPΩ​(Y)=Y, PT(Y)=E\mathcal{P}_T(Y)=EPT​(Y)=E (p. 2061).
  • Ruling out trivialization. The hypothesis m≤n2m\le n^2m≤n2 is there only because successProb is 000 for m>n2m>n^2m>n2; it does not exclude any case the paper covers. The failure probability stays n−3n^{-3}n−3 and is not traded for a constant. The constant CCC may not depend on nnn, rrr, μ\muμ or MMM, so it cannot be chosen to make (I.12) unsatisfiable. For fixed CCC, (I.12) is satisfiable with m≤n2m \le n^2m≤n2 for every large nnn and every r≤n/(Cμ2log⁡6n)r \le n/(C\mu^2\log^6 n)r≤n/(Cμ2log6n).
  • Not covered. Proposition 6.1 (the summand bound on generalized spiders) is the heart of Theorem 3.6. It needs the admissible-quadruplet combinatorics of Sections IV–VI as definitions, and is left to solvers as a lemma of their own. Contributions formalizing Sections IV–VI (the moment expansion (IV.10), admissible pairs, the cancellation identities (VI.1)–(VI.4)) are welcome and reusable for mission I of this series.

Selected references

  • E. J. Candès and T. Tao, The Power of Convex Relaxation: Near-Optimal Matrix Completion, IEEE Trans. Inf. Theory 56(5):2053–2080, 2010. https://doi.org/10.1109/TIT.2010.2044061
  • E. J. Candès and B. Recht, Exact Matrix Completion via Convex Optimization, Found. Comput. Math. 9:717–772, 2009. https://arxiv.org/abs/0805.4471
  • R. H. Keshavan, A. Montanari and S. Oh, Matrix Completion from a Few Entries, IEEE Trans. Inf. Theory 56(6):2980–2998, 2010. https://arxiv.org/abs/0901.3150
  • D. Gross, Recovering Low-Rank Matrices from Few Coefficients in Any Basis, IEEE Trans. Inf. Theory 57(3):1548–1566, 2011. https://arxiv.org/abs/0910.1879
  • B. Recht, A Simpler Approach to Matrix Completion, J. Mach. Learn. Res. 12:3413–3430, 2011. https://arxiv.org/abs/0910.0651
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Linear algebraNumerical AnalysisProbability·Captain: mikedeng1

Randomized Algorithms for Estimating the Trace of an Implicit Symmetric Positive Semi-Definite Matrix V: Sample Bound for the Mixed Unit Vector Trace EstimatorResearch Paper

Motivation

Many computations in numerical linear algebra, statistics and computational physics need the trace of a matrix AAA that is never formed explicitly: AAA may be an inverse, a matrix function f(B)f(B)f(B), or a product of large operators, and the only affordable access is a routine that returns AvAvAv or vTAvv^TAvvTAv for a given vector vvv. Monte Carlo trace estimators handle this setting: draw random vectors zzz and average the quadratic forms zTAzz^TAzzTAz, each of which costs one matrix–vector product.

Avron and Toledo (J. ACM 2011) compare such estimators by the number of samples MMM that guarantee relative error ϵ\epsilonϵ with probability 1−δ1-\delta1−δ, and by the number of random bits each sample consumes. Hutchinson's estimator (Hutchinson 1990) and the Gaussian estimator need Ω(n)\Omega(n)Ω(n) random bits per sample. Section 8 of the paper studies two estimators that sample only from the nnn standard basis vectors and so need about log⁡2n\log_2 nlog2​n bits per sample, which allows the samples to be generated in advance. The plain version has a sample bound that depends on how uneven the diagonal of AAA is; the mixed version first multiplies AAA on both sides by a random orthogonal mixing matrix of the kind introduced by Ailon and Chazelle (2006) for the fast Johnson–Lindenstrauss transform and used by Avron, Maymounkov and Toledo (2010) in least-squares solvers. This mission formalizes the resulting sample bound, Theorem 8.4.

Setting

Let n≥1n \ge 1n≥1, let A∈Rn×nA \in \mathbb{R}^{n\times n}A∈Rn×n be symmetric positive semi-definite, and let e1,…,ene_1,\ldots,e_ne1​,…,en​ be the standard basis of Rn\mathbb{R}^nRn.

A random variable TTT is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A) if

Pr⁡(∣T−trace(A)∣≤ϵ trace(A))≥1−δ\Pr\bigl(|T-\mathrm{trace}(A)| \le \epsilon\,\mathrm{trace}(A)\bigr) \ge 1-\deltaPr(∣T−trace(A)∣≤ϵtrace(A))≥1−δ

(Definition 4.1).

The unit vector estimator with MMM samples is

UM=nM∑i=1MziTAzi,U_M = \frac{n}{M}\sum_{i=1}^M z_i^TAz_i,UM​=Mn​i=1∑M​ziT​Azi​,

where z1,…,zMz_1,\ldots,z_Mz1​,…,zM​ are independent uniform random samples from {e1,…,en}\{e_1,\ldots,e_n\}{e1​,…,en​} (Definition 3.4). Each term ziTAziz_i^TAz_iziT​Azi​ is a diagonal entry of AAA chosen uniformly at random. Its behaviour is governed by

rD(A)=n⋅max⁡iAiitrace(A),r_D(A) = \frac{n\cdot\max_i A_{ii}}{\mathrm{trace}(A)},rD​(A)=trace(A)n⋅maxi​Aii​​,

which lies between 111 and nnn.

A random mixing matrix is F=FD\mathcal F = FDF=FD, where the seed FFF is a fixed orthogonal n×nn\times nn×n matrix and DDD is diagonal with i.i.d. Rademacher entries, Pr⁡(Dii=±1)=1/2\Pr(D_{ii}=\pm1) = 1/2Pr(Dii​=±1)=1/2 (Definition 3.5). The seed enters through

η=max⁡i,j∣Fij∣2,\eta = \max_{i,j}|F_{ij}|^2,η=i,jmax​∣Fij​∣2,

which satisfies 1/n≤η≤11/n \le \eta \le 11/n≤η≤1; normalized DFT and Hadamard matrices attain η=1/n\eta = 1/nη=1/n, DCT and DHT matrices have η=2/n\eta = 2/nη=2/n (p. 8:5).

The mixed unit vector estimator is

TM=nM∑i=1MziTFAFTzi,T_M = \frac{n}{M}\sum_{i=1}^M z_i^T\mathcal F A\mathcal F^T z_i,TM​=Mn​i=1∑M​ziT​FAFTzi​,

with z1,…,zMz_1,\ldots,z_Mz1​,…,zM​ as above, independent of DDD (Definition 3.6). It is the unit vector estimator applied to FAFT\mathcal FA\mathcal F^TFAFT, whose trace equals trace(A)\mathrm{trace}(A)trace(A).

Formalization targets

Goal: Theorem 8.4

For every orthogonal seed FFF, every symmetric positive semi-definite AAA, every ϵ>0\epsilon > 0ϵ>0, δ∈(0,1)\delta \in (0,1)δ∈(0,1) and every M≥1M \ge 1M≥1,

M ≥ 2n2η2ϵ−2ln⁡(4/δ)ln⁡2(4n2/δ)⟹TM is an (ϵ,δ)-approximator of trace(A).M \ \ge\ 2n^2\eta^2\epsilon^{-2}\ln(4/\delta)\ln^2(4n^2/\delta) \quad\Longrightarrow\quad T_M \text{ is an } (\epsilon,\delta)\text{-approximator of } \mathrm{trace}(A).M ≥ 2n2η2ϵ−2ln(4/δ)ln2(4n2/δ)⟹TM​ is an (ϵ,δ)-approximator of trace(A).

Milestones

  1. Lemma 8.1. For symmetric AAA, E(U1)=trace(A)\mathrm{E}(U_1) = \mathrm{trace}(A)E(U1​)=trace(A) and Var(U1)=n∑iAii2−trace2(A)\mathrm{Var}(U_1) = n\sum_{i}A_{ii}^2 - \mathrm{trace}^2(A)Var(U1​)=n∑i​Aii2​−trace2(A).
  2. Theorem 8.2. UMU_MUM​ is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A) whenever
M≥12ϵ−2ln⁡(2/δ) rD2(A).M \ge \tfrac12\epsilon^{-2}\ln(2/\delta)\,r_D^2(A).M≥21​ϵ−2ln(2/δ)rD2​(A).
  1. Lemma 8.3. For U∈Rn×mU \in \mathbb{R}^{n\times m}U∈Rn×m with orthonormal columns and δ>0\delta > 0δ>0, with probability at least 1−δ1-\delta1−δ,
∣(FU)ij∣≤2ηln⁡(2mn/δ)for all i,j.|(\mathcal FU)_{ij}| \le \sqrt{2\eta\ln(2mn/\delta)} \quad\text{for all } i,j.∣(FU)ij​∣≤2ηln(2mn/δ)​for all i,j.
  1. Proof of Theorem 8.4, p. 8:13. With probability at least 1−δ/21-\delta/21−δ/2 over DDD, 0≤(FAFT)jj≤2ηln⁡(4n2/δ) trace(A)0 \le (\mathcal FA\mathcal F^T)_{jj} \le 2\eta\ln(4n^2/\delta)\,\mathrm{trace}(A)0≤(FAFT)jj​≤2ηln(4n2/δ)trace(A) for all jjj, and hence
rD(FAFT)≤2nηln⁡(4n2/δ).r_D(\mathcal FA\mathcal F^T) \le 2n\eta\ln(4n^2/\delta).rD​(FAFT)≤2nηln(4n2/δ).

Significance

Theorem 8.2 alone shows that the unit vector estimator can need order n2n^2n2 samples: when the trace is concentrated on one diagonal entry, rD(A)=nr_D(A) = nrD​(A)=n. Theorem 8.4 removes the dependence on AAA entirely. For a Fourier-type seed with η=Θ(1/n)\eta = \Theta(1/n)η=Θ(1/n) the bound becomes O(ϵ−2ln⁡(1/δ)ln⁡2(n/δ))O(\epsilon^{-2}\ln(1/\delta)\ln^2(n/\delta))O(ϵ−2ln(1/δ)ln2(n/δ)) samples for every positive semi-definite AAA, while each sample still costs about log⁡2n\log_2 nlog2​n random bits, and the nnn bits of DDD are drawn once. Among the estimators of the paper this is the only one with both an AAA-independent sample bound and logarithmic randomness per sample (Table I, p. 8:5). Lemma 8.3 is a standalone statement about randomized orthogonal transforms that is used well beyond trace estimation, in the analysis of subsampled randomized Hadamard transforms, sketching-based least squares, and fast Johnson–Lindenstrauss embeddings.

All results of the mission are proved in the literature: Lemma 8.3 in the cited works, the rest in the paper. As far as the platform's catalogue shows, none has a machine-checked proof. The mission produces checked statements of the paper's Section 8 with their exact constants, a probability model for random sign matrices and uniform basis-vector sampling that other randomized linear-algebra missions can reuse, and, once proved, a checked instance of Hoeffding's inequality applied to a concrete estimator.

Difficulty

The obvious argument for Theorem 8.4 applies Theorem 8.2 to FAFT\mathcal FA\mathcal F^TFAFT. That matrix is random, so Theorem 8.2, which is a statement about a fixed matrix, cannot be applied directly: the proof must condition on DDD, use that the samples ziz_izi​ are independent of DDD, and combine a failure event over DDD with a conditional failure event over the ziz_izi​, each with probability at most δ/2\delta/2δ/2. The second difficulty is Lemma 8.3: each entry (FU)ij=∑kFikDkkUkj(\mathcal FU)_{ij} = \sum_k F_{ik}D_{kk}U_{kj}(FU)ij​=∑k​Fik​Dkk​Ukj​ is a Rademacher sum whose coefficient vector has squared norm at most η\etaη, and the bound needs a sub-Gaussian tail for such sums together with a union bound over all mnmnmn entries. Bounding the diagonal of FAFT\mathcal FA\mathcal F^TFAFT through the diagonal of AAA alone does not work: each mixed diagonal entry depends on all entries of AAA, including the off-diagonal ones.

Formalization scope

Everything is over R\mathbb{R}R. The paper allows complex unitary seeds; since the estimator uses the transpose FT\mathcal F^TFT, the mission takes FFF real orthogonal (FTF=IF^TF = IFTF=I). Matrices are Matrix (Fin n) (Fin n) ℝ, "symmetric positive semi-definite" is Matrix.PosSemidef, and n≥1n \ge 1n≥1 is assumed throughout. The sample spaces are explicit product measures: indices k1,…,kMk_1,\ldots,k_Mk1​,…,kM​ uniform on Fin n with zi=ekiz_i = e_{k_i}zi​=eki​​, the diagonal of DDD with the nnn-fold Rademacher product law, and, for TMT_MTM​, the product of the two, which makes DDD and the ziz_izi​ independent as the paper assumes implicitly. Probabilities are Measure.real. η\etaη and max⁡iAii\max_i A_{ii}maxi​Aii​ are maxima over finite nonempty index sets; rDr_DrD​ uses real division, whose value at trace(A)=0\mathrm{trace}(A) = 0trace(A)=0 is irrelevant because a positive semi-definite matrix with zero trace is 000. The sample-count thresholds are exactly the paper's constants.

Deviations from the page, all recorded in the items' Formalization Notes: Definition 3.4 and Theorem 8.2 are stated for positive semi-definite rather than positive definite AAA (the proof uses only Aii≥0A_{ii} \ge 0Aii​≥0); Table I's entry 8ϵ−2ln⁡(4n2/δ)ln⁡(4/δ)8\epsilon^{-2}\ln(4n^2/\delta)\ln(4/\delta)8ϵ−2ln(4n2/δ)ln(4/δ) for the mixed estimator, which disagrees with Theorem 8.4, is not used; the proof of Theorem 8.4 prints the conditional failure probability as "≤1−δ/2\le 1-\delta/2≤1−δ/2" where δ/2\delta/2δ/2 is meant, and no statement copies it; Remark 8.5 ("for some small CCC") has no pinned constant and is not stated.

A formalization in which DDD is an arbitrary orthogonal diagonal matrix, the ziz_izi​ are correlated with DDD, or the law of the estimator is assumed rather than constructed would make the goal either false or a restatement of its hypotheses; the product-measure model rules this out.

Needed infrastructure: Hoeffding's inequality for bounded i.i.d. sums (in Mathlib as sub-Gaussian moment generating function bounds), a sub-Gaussian tail for Rademacher linear combinations, conditioning on one factor of a product measure, and the spectral theorem for real symmetric matrices. The Rademacher sign model and the random-mixing-matrix entry bound are reusable beyond this mission. Proofs of any milestone, and alternative arguments for Lemma 8.3, are welcome.

Selected references

  • H. Avron and S. Toledo, Randomized algorithms for estimating the trace of an implicit symmetric positive semi-definite matrix, J. ACM 58(2), Article 8, 2011. https://doi.org/10.1145/1944345.1944349
  • N. Ailon and B. Chazelle, Approximate nearest neighbors and the fast Johnson–Lindenstrauss transform, STOC 2006. https://doi.org/10.1145/1132516.1132597
  • H. Avron, P. Maymounkov and S. Toledo, Blendenpik: Supercharging LAPACK's least-squares solver, SIAM J. Sci. Comput. 32(3), 2010. https://doi.org/10.1137/090767911
  • M. F. Hutchinson, A stochastic estimator of the trace of the influence matrix for Laplacian smoothing splines, Comm. Statist. Simulation Comput. 19(2), 1990. https://doi.org/10.1080/03610919008812866
  • W. Hoeffding, Probability inequalities for sums of bounded random variables, J. Amer. Statist. Assoc. 58, 1963. https://doi.org/10.1080/01621459.1963.10500830
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Linear algebraNumerical AnalysisProbability·Captain: mikedeng1

Randomized Algorithms for Estimating the Trace of an Implicit Symmetric Positive Semi-Definite Matrix III: Sample Bound for Normalized Rayleigh-Quotient Trace EstimatorsResearch Paper

Motivation

Many computations in numerical linear algebra, statistics and computational physics need the trace of a matrix AAA that is never formed explicitly: AAA may be an inverse, a matrix function f(B)f(B)f(B), or a product of large operators, and the only affordable access is a routine that returns AvAvAv for a given vector vvv. Examples include log-determinants and the generalized cross-validation criterion in statistics, counting eigenvalues in an interval, and charge densities in electronic-structure computations. Monte Carlo trace estimators handle this setting: draw random vectors zzz, and average the quadratic forms zTAzz^TAzzTAz, each of which costs one matrix–vector product.

Hutchinson (1990) introduced the estimator with Rademacher vectors and computed its variance. Avron and Toledo (J. ACM 2011) replaced variance statements with sample bounds: how many samples MMM guarantee relative error ϵ\epsilonϵ with probability 1−δ1-\delta1−δ. Section 6 of their paper proves one such bound for an entire class of estimators at once, the normalized Rayleigh-quotient trace estimators, which contains Hutchinson's estimator and the unit vector estimator. This mission formalizes that bound (Theorem 6.1).

Setting

Let A∈Rn×nA \in \mathbb{R}^{n\times n}A∈Rn×n be symmetric positive semi-definite, with eigenvalues 0≤λ1≤⋯≤λn0 \le \lambda_1 \le \cdots \le \lambda_n0≤λ1​≤⋯≤λn​ and rank rank(A)\mathrm{rank}(A)rank(A). Write λn\lambda_nλn​ for the largest eigenvalue and

κf(A)=largest nonzero eigenvalue of Asmallest nonzero eigenvalue of A,\kappa_f(A) = \frac{\text{largest nonzero eigenvalue of }A}{\text{smallest nonzero eigenvalue of }A},κf​(A)=smallest nonzero eigenvalue of Alargest nonzero eigenvalue of A​,

defined for A≠0A \ne 0A=0; it is the condition number of AAA on its range.

A normalized Rayleigh-quotient trace estimator of AAA with MMM samples is

RM=1M∑i=1MziTAzi,R_M = \frac1M\sum_{i=1}^M z_i^TAz_i,RM​=M1​i=1∑M​ziT​Azi​,

where z1,…,zMz_1,\ldots,z_Mz1​,…,zM​ are independent random vectors in Rn\mathbb{R}^nRn with ziTzi=nz_i^Tz_i = nziT​zi​=n and E(ziTAzi)=trace(A)\mathrm{E}(z_i^TAz_i) = \mathrm{trace}(A)E(ziT​Azi​)=trace(A) for each iii (Definition 3.2). The vectors need not be identically distributed. Hutchinson's vectors (±1\pm1±1 entries, i.i.d. uniform) and the vectors n ek\sqrt n\,e_kn​ek​ with kkk uniform are instances.

A random variable TTT is an (ϵ,δ)(\epsilon,\delta)(ϵ,δ)-approximator of trace(A)\mathrm{trace}(A)trace(A) if

Pr⁡(∣T−trace(A)∣≤ϵ trace(A))≥1−δ\Pr\bigl(|T-\mathrm{trace}(A)| \le \epsilon\,\mathrm{trace}(A)\bigr) \ge 1-\deltaPr(∣T−trace(A)∣≤ϵtrace(A))≥1−δ

(Definition 4.1).

Formalization targets

Goal: Theorem 6.1, in the form its proof establishes

For every nonzero symmetric positive semi-definite AAA, every ϵ>0\epsilon>0ϵ>0, δ∈(0,1)\delta\in(0,1)δ∈(0,1), and every normalized Rayleigh-quotient estimator RMR_MRM​ of AAA,

M ≥ ln⁡(2/δ)⋅n2 κf2(A)2 rank2(A) ϵ2⟹RM is an (ϵ,δ)-approximator of trace(A).M \ \ge\ \frac{\ln(2/\delta)\cdot n^2\,\kappa_f^2(A)}{2\,\mathrm{rank}^2(A)\,\epsilon^2} \quad\Longrightarrow\quad R_M \text{ is an } (\epsilon,\delta)\text{-approximator of } \mathrm{trace}(A).M ≥ 2rank2(A)ϵ2ln(2/δ)⋅n2κf2​(A)​⟹RM​ is an (ϵ,δ)-approximator of trace(A).

Milestones (the displayed steps of the proof, p. 8:10)

  1. trace(A) κf(A)≥rank(A) λn\mathrm{trace}(A)\,\kappa_f(A) \ge \mathrm{rank}(A)\,\lambda_ntrace(A)κf​(A)≥rank(A)λn​.
  2. For every zzz with zTz=nz^Tz = nzTz=n:  0≤zTAz≤λnzTz=nλn≤nrank(A)trace(A) κf(A)\ 0 \le z^TAz \le \lambda_n z^Tz = n\lambda_n \le \frac{n}{\mathrm{rank}(A)}\mathrm{trace}(A)\,\kappa_f(A) 0≤zTAz≤λn​zTz=nλn​≤rank(A)n​trace(A)κf​(A).
  3. For every t>0t>0t>0:
Pr⁡(∣RM−trace(A)∣≥t)≤2exp⁡(−2M2rank2(A)t2Mn2trace2(A)κf2(A)).\Pr(|R_M-\mathrm{trace}(A)| \ge t) \le 2\exp\left(-\frac{2M^2\mathrm{rank}^2(A)t^2}{M n^2\mathrm{trace}^2(A)\kappa_f^2(A)}\right).Pr(∣RM​−trace(A)∣≥t)≤2exp(−Mn2trace2(A)κf2​(A)2M2rank2(A)t2​).
  1. For every ϵ>0\epsilon>0ϵ>0:
Pr⁡(∣RM−trace(A)∣≥ϵ trace(A))≤2exp⁡(−2Mrank2(A)ϵ2n2κf2(A)).\Pr(|R_M-\mathrm{trace}(A)| \ge \epsilon\,\mathrm{trace}(A)) \le 2\exp\left(-\frac{2M\mathrm{rank}^2(A)\epsilon^2}{n^2\kappa_f^2(A)}\right).Pr(∣RM​−trace(A)∣≥ϵtrace(A))≤2exp(−n2κf2​(A)2Mrank2(A)ϵ2​).

Significance

The result is distribution-free within the class: it needs only normalization and unbiasedness, so it covers Hutchinson's estimator, the unit vector estimator and any future normalized scheme with one argument. For well-conditioned matrices of full or nearly full rank the required number of samples is O(ϵ−2ln⁡(1/δ))O(\epsilon^{-2}\ln(1/\delta))O(ϵ−2ln(1/δ)), independent of nnn. For ill-conditioned matrices the bound degrades with κf2(A)\kappa_f^2(A)κf2​(A), which is the reason the paper proves sharper estimator-specific bounds in Sections 7 and 8; Theorem 6.1 is the baseline those results are compared against (Table I, p. 8:5).

The theorem is proved in the paper. No machine-checked version of it, or of any sample bound for trace estimators, is known to exist. The formalization adds a precise statement of the class of estimators on a general probability space, a corrected threshold (see below), and a Lean development that connects Mathlib's spectral theorem for symmetric matrices with its Hoeffding inequality for independent bounded variables.

Difficulty

Each step is short on paper; the work is in the interfaces. The eigenvalue inequality of milestone 1 requires relating the number of nonzero eigenvalues (with multiplicity) to rank(A)\mathrm{rank}(A)rank(A) and handling the maximum and minimum over the nonzero spectrum. Milestone 2 is the Rayleigh-quotient bound zTAz≤λnzTzz^TAz \le \lambda_n z^TzzTAz≤λn​zTz, which is a consequence of the spectral decomposition rather than a one-line identity. Milestone 3 applies Hoeffding's inequality to summands that are bounded only almost surely, are not identically distributed, and whose mean is fixed by hypothesis rather than computed; the two-sided bound must be assembled from two one-sided tails, and the event ∣RM−trace(A)∣≥t|R_M - \mathrm{trace}(A)| \ge t∣RM​−trace(A)∣≥t must be rescaled to a statement about the sum ∑iziTAzi\sum_i z_i^TAz_i∑i​ziT​Azi​. A naive attempt that fixes a particular distribution for the ziz_izi​ (Rademacher, say) proves a different, narrower theorem and does not settle the goal.

Formalization scope

  • Matrices and spectrum. AAA is Matrix (Fin n) (Fin n) ℝ with A.PosSemidef and A ≠ 0; eigenvalues are Mathlib's IsHermitian.eigenvalues. λn\lambda_nλn​ is lambdaMax (the maximum eigenvalue) and κf(A)\kappa_f(A)κf​(A) is kappaF (maximum over minimum of the finite set of nonzero eigenvalues); both are Finset.max'/min'/sup' of nonempty finite sets. κf(0)\kappa_f(0)κf​(0) is a placeholder, and every statement assumes A≠0A \ne 0A=0.
  • Probability model. A general probability space (Ω,P)(\Omega, P)(Ω,P) and random vectors z : Fin M → Ω → Fin n → ℝ satisfying IsNormalizedRayleighSample P A z: each ziz_izi​ measurable, the family mutually independent (iIndepFun), ziTzi=nz_i^Tz_i = nziT​zi​=n almost surely, and ∫ziTAzi dP=trace(A)\int z_i^TAz_i\,dP = \mathrm{trace}(A)∫ziT​Azi​dP=trace(A). The estimator is universally quantified over this class. Unbiasedness is required for the given AAA only, as on the page. Probabilities are P.real of events; M≥1M \ge 1M≥1 is a natural number and 1/M1/M1/M is (M : ℝ)⁻¹.
  • Correction of the printed statement. Theorem 6.1 and Table I print the threshold 12ϵ−2n−2rank2(A)ln⁡(2/δ)κf2(A)\tfrac12\epsilon^{-2}n^{-2}\mathrm{rank}^2(A)\ln(2/\delta)\kappa_f^2(A)21​ϵ−2n−2rank2(A)ln(2/δ)κf2​(A). The last display of the proof gives ln⁡(2/δ) n2κf2(A)/(2 rank2(A)ϵ2)\ln(2/\delta)\,n^2\kappa_f^2(A)/(2\,\mathrm{rank}^2(A)\epsilon^2)ln(2/δ)n2κf2​(A)/(2rank2(A)ϵ2), with the exponents of nnn and rank(A)\mathrm{rank}(A)rank(A) swapped. The printed version is false: for n=2n=2n=2, A=e1e1TA=e_1e_1^TA=e1​e1T​, z=2 ekz=\sqrt2\,e_kz=2​ek​ with kkk uniform and ϵ=δ=1/2\epsilon=\delta=1/2ϵ=δ=1/2 it admits M=1M=1M=1, while R1∈{0,2}R_1\in\{0,2\}R1​∈{0,2}. The goal states the proof's threshold.
  • Indexing slip. The proof writes 0=λ1=⋯=λk0=\lambda_1=\cdots=\lambda_k0=λ1​=⋯=λk​ with k=n−rank(A)+1k=n-\mathrm{rank}(A)+1k=n−rank(A)+1 and κf(A)=λn/λk\kappa_f(A)=\lambda_n/\lambda_kκf​(A)=λn​/λk​, which would make λk=0\lambda_k=0λk​=0; milestone 1 states the inequality with κf\kappa_fκf​ as defined, not the indexing.
  • Non-trivialization. The hypotheses of the class are satisfiable (by the unit vector and Hutchinson estimators), A≠0A\ne0A=0 excludes the degenerate κf(0)\kappa_f(0)κf​(0), and all divisions in the statements have positive denominators, so no statement holds vacuously or through a junk value.
  • Reusable parts. A proof of milestone 2 is a general Rayleigh-quotient bound for symmetric matrices; milestone 3 is a two-sided Hoeffding bound for independent, almost surely bounded, non-identically distributed summands, useful well beyond this mission. Contributions welcome: proofs of any milestone, and a sorry-free instance showing a concrete estimator (e.g. n ek\sqrt n\,e_kn​ek​) satisfies IsNormalizedRayleighSample.

Selected references

  • H. Avron and S. Toledo, Randomized algorithms for estimating the trace of an implicit symmetric positive semi-definite matrix, Journal of the ACM 58(2), Article 8, 2011. https://doi.org/10.1145/1944345.1944349
  • M. F. Hutchinson, A stochastic estimator of the trace of the influence matrix for Laplacian smoothing splines, Communications in Statistics – Simulation and Computation 19(2), 433–450, 1990. https://doi.org/10.1080/03610919008812866
  • W. Hoeffding, Probability inequalities for sums of bounded random variables, Journal of the American Statistical Association 58(301), 13–30, 1963. https://doi.org/10.1080/01621459.1963.10500830
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Convex OptimizationMachine LearningProbability+1·Captain: mikedeng1

The Power of Convex Relaxation: Near-Optimal Matrix Completion I: Exact Nuclear-Norm Recovery with Quadratic Dependence on the RankResearch Paper

Motivation

Matrix completion asks to recover a low-rank matrix from a small random subset of its entries. It models collaborative filtering (a ratings matrix with most entries missing), sensor-network localization from partial distance matrices, and system identification. The natural estimator, the matrix of least rank that agrees with the observations, is NP-hard to compute in general. Candès and Recht (Found. Comput. Math. 2009) proposed to replace the rank by the nuclear norm (the sum of the singular values), its convex envelope, and proved that this convex program recovers the matrix exactly from O(n6/5rlog⁡n)O(n^{6/5} r \log n)O(n6/5rlogn) random entries under incoherence assumptions.

Candès and Tao (IEEE Trans. Inf. Theory 2010) sharpened the sample size to within logarithmic factors of the information-theoretic minimum nrlog⁡nn r\log nnrlogn. This mission formalizes their first result, Theorem 1.1, whose proof is a direct moment computation, together with the lemmas on which that proof rests.

Timeline:

  • 2009, Candès–Recht: exact recovery from m≳μ0n6/5rlog⁡nm \gtrsim \mu_0 n^{6/5} r \log nm≳μ0​n6/5rlogn entries.
  • 2010, Candès–Tao (this paper): m≳μ4nr2(log⁡n)2m \gtrsim \mu^4 n r^2 (\log n)^2m≳μ4nr2(logn)2 (Theorem 1.1, general-rank form) and m≳μ2nrlog⁡6nm \gtrsim \mu^2 n r \log^6 nm≳μ2nrlog6n (Theorem 1.2), plus a lower bound of order nrlog⁡nn r \log nnrlogn for every method (Theorem 1.7).
  • 2011, Gross (IEEE Trans. Inf. Theory) and Recht (JMLR): m≳μ0nrlog⁡2nm \gtrsim \mu_0 n r \log^2 nm≳μ0​nrlog2n by the "golfing scheme", with a different proof.

Setting

Let M∈Rn×nM \in \mathbb R^{n\times n}M∈Rn×n have rank rrr and singular value decomposition M=∑k=1rσkukvk∗M = \sum_{k=1}^r \sigma_k u_k v_k^*M=∑k=1r​σk​uk​vk∗​ with σk>0\sigma_k > 0σk​>0 and orthonormal uku_kuk​, vkv_kvk​. Write PU=∑kukuk∗P_U = \sum_k u_k u_k^*PU​=∑k​uk​uk∗​, PV=∑kvkvk∗P_V = \sum_k v_k v_k^*PV​=∑k​vk​vk∗​ and E=∑kukvk∗E = \sum_k u_k v_k^*E=∑k​uk​vk∗​. The matrix obeys the strong incoherence property with parameter μ>0\mu > 0μ>0 if, for all indices a,a′,b,b′a, a', b, b'a,a′,b,b′,

∣⟨ea,PUea′⟩−rn1a=a′∣≤μrn,∣⟨eb,PVeb′⟩−rn1b=b′∣≤μrn,∣Eab∣≤μrn.\Bigl|\langle e_a, P_U e_{a'}\rangle - \tfrac{r}{n}1_{a=a'}\Bigr| \le \mu\tfrac{\sqrt r}{n},\qquad \Bigl|\langle e_b, P_V e_{b'}\rangle - \tfrac{r}{n}1_{b=b'}\Bigr| \le \mu\tfrac{\sqrt r}{n},\qquad |E_{ab}| \le \mu\tfrac{\sqrt r}{n}.​⟨ea​,PU​ea′​⟩−nr​1a=a′​​≤μnr​​,​⟨eb​,PV​eb′​⟩−nr​1b=b′​​≤μnr​​,∣Eab​∣≤μnr​​.

For a set Ω⊂[n]×[n]\Omega \subset [n]\times[n]Ω⊂[n]×[n] of observed positions, the nuclear-norm program is

minimize ∥X∥∗subject to Xab=Mab  ((a,b)∈Ω).(I.3)\text{minimize } \|X\|_* \quad \text{subject to } X_{ab} = M_{ab}\ \ ((a,b)\in\Omega). \qquad \text{(I.3)}minimize ∥X∥∗​subject to Xab​=Mab​  ((a,b)∈Ω).(I.3)

In the uniform model Ω\OmegaΩ is a uniformly random mmm-subset of [n]×[n][n]\times[n][n]×[n]; in the Bernoulli model each entry is included independently with probability p=m/n2p = m/n^2p=m/n2.

The proof works with the tangent space TTT at MMM and its projection PT(X)=PUX+XPV−PUXPV\mathcal P_T(X) = P_UX + XP_V - P_UXP_VPT​(X)=PU​X+XPV​−PU​XPV​, the sampling projection PΩ\mathcal P_\OmegaPΩ​, and the centered operators QΩ=p−1PΩ−I\mathcal Q_\Omega = p^{-1}\mathcal P_\Omega - \mathcal IQΩ​=p−1PΩ​−I and QT=PT−ρ′I\mathcal Q_T = \mathcal P_T - \rho'\mathcal IQT​=PT​−ρ′I, where ρ=r/n\rho = r/nρ=r/n and ρ′=2ρ−ρ2\rho' = 2\rho - \rho^2ρ′=2ρ−ρ2. The candidate certificate YYY of (III.10) is the matrix of least Frobenius norm with PΩ(Y)=Y\mathcal P_\Omega(Y) = YPΩ​(Y)=Y and PT(Y)=E\mathcal P_T(Y) = EPT​(Y)=E.

Formalization targets

Goal: Theorem 1.1, general-rank form (I.11)

There is an absolute constant CCC such that, for every strongly incoherent MMM of rank rrr and every m≤n2m \le n^2m≤n2,

m≥Cμ4nr2(log⁡n)2  ⟹  Pr⁡uniform[M is the unique solution of (I.3)]≥1−n−3.m \ge C\mu^4 n r^2(\log n)^2 \implies \Pr_{\text{uniform}}\bigl[M \text{ is the unique solution of (I.3)}\bigr] \ge 1 - n^{-3}.m≥Cμ4nr2(logn)2⟹uniformPr​[M is the unique solution of (I.3)]≥1−n−3.

Milestones

  1. Lemma 3.1: a matrix YYY supported on Ω\OmegaΩ with PT(Y)=E\mathcal P_T(Y) = EPT​(Y)=E and ∥PT⊥(Y)∥<1\|\mathcal P_{T^\perp}(Y)\| < 1∥PT⊥​(Y)∥<1, together with injectivity of PΩ\mathcal P_\OmegaPΩ​ on TTT, certifies that MMM is the unique solution (already proved on the platform).
  2. Lemma 5.1 (exponent bound): ∣J∣+∣K∣−∣Q∣−∣Ω∣≤−∣Q′∣+1|J|+|K|-|Q|-|\Omega| \le -|Q'|+1∣J∣+∣K∣−∣Q∣−∣Ω∣≤−∣Q′∣+1 for every admissible pair.
  3. Lemma 5.2 (pair counting): at most (Cj(k+1))2j(k+1)+q(Cj(k+1))^{2j(k+1)+q}(Cj(k+1))2j(k+1)+q strongly admissible pairs have ∣Q′∣=q|Q'| = q∣Q′∣=q.
  4. Theorem 3.4 (moment bound I): with A=(QΩQT)kQΩ(E)A = (\mathcal Q_\Omega\mathcal Q_T)^k\mathcal Q_\Omega(E)A=(QΩ​QT​)kQΩ​(E) and rμ=μ2rr_\mu = \mu^2 rrμ​=μ2r,
Etrace⁡(A∗A)j≤(Cj(k+1))2j(k+1) n (nrμ2/m)j(k+1).\mathbb E\operatorname{trace}(A^*A)^j \le (Cj(k+1))^{2j(k+1)}\, n\,(n r_\mu^2/m)^{j(k+1)}.Etrace(A∗A)j≤(Cj(k+1))2j(k+1)n(nrμ2​/m)j(k+1).
  1. Corollary 3.5: under the goal's sampling condition and the Bernoulli model, with probability at least 1−n−31-n^{-3}1−n−3, PΩ\mathcal P_\OmegaPΩ​ is injective on TTT and ∥PT⊥(Y)∥≤1/2\|\mathcal P_{T^\perp}(Y)\| \le 1/2∥PT⊥​(Y)∥≤1/2.

The Bernoulli-to-uniform transfer (at most doubling the failure probability) is already on the platform and is included as a supporting item.

Significance

Theorem 1.1 shows that a tractable convex program recovers every strongly incoherent matrix of bounded rank from O(n(log⁡n)2)O(n(\log n)^2)O(n(logn)2) random entries, while Theorem 1.7 of the same paper shows that no method can succeed with fewer than order nlog⁡nn\log nnlogn. The gap is a single logarithmic factor. The result also requires nothing of the singular values, only of the singular vectors.

The theorem is proved in the literature, and later work improved the rank dependence (Theorem 1.2 of the same paper, and the golfing-scheme results of Gross and Recht). As far as is known, none of these results has a machine-checked proof. The mission produces a formal version of the full moment-method argument. Its combinatorial core, the admissible-pair calculus of Sections IV–V, is a self-contained counting problem for closed paths in a grid and is reusable for other trace-moment bounds of random operators. The Candès–Recht mission on the platform already supplies the deterministic duality step (Lemma 3.1) and the model transfer.

Difficulty

The obvious route bounds the Neumann series ∑k∥(QΩPT)kQΩ(E)∥\sum_k \|(\mathcal Q_\Omega\mathcal P_T)^k\mathcal Q_\Omega(E)\|∑k​∥(QΩ​PT​)kQΩ​(E)∥ term by term with noncommutative Khintchine inequalities and decoupling. That is how the earlier n6/5n^{6/5}n6/5 bound was obtained, and it degrades as kkk grows because the indicator variables in the higher terms are strongly coupled. The moment method replaces these tools by an exact expansion of Etrace⁡(A∗A)j\mathbb E\operatorname{trace}(A^*A)^jEtrace(A∗A)j as a sum over "spider" configurations of paths in [n]×[n][n]\times[n][n]×[n]. The difficulty moves into combinatorics. Configurations have to be grouped by admissible pairs, the exponent of nnn has to be matched against the powers of 1/p1/p1/p (Lemma 5.1), and the configurations have to be counted with enough precision that the sum over qqq converges (Lemma 5.2). A naive count of pairs gives (2j(k+1))4j(k+1)(2j(k+1))^{4j(k+1)}(2j(k+1))4j(k+1), which is too large by a square.

Formalization scope

  • Square case. Theorem 1.1 is printed for n1×n2n_1\times n_2n1​×n2​ matrices, but the paper proves only the square case (Section I-H: "we shall work exclusively with square matrices"). Every statement is for Matrix (Fin n) (Fin n) ℝ.
  • General rank. The goal and Corollary 3.5 are stated in the general-rank form (I.11), m≥Cμ4nr2(log⁡n)2m \ge C\mu^4 n r^2(\log n)^2m≥Cμ4nr2(logn)2. The paper states this form explicitly on p. 2055, and the proof of Corollary 3.5 derives it as (III.26). For r=O(1)r = O(1)r=O(1) it is the printed Theorem 1.1 and the printed Corollary 3.5.
  • Constants. Every constant ("numerical constant CCC", c0c_0c0​, and O(M)M:=(CM)MO(M)^M := (CM)^MO(M)M:=(CM)M) is an existential absolute constant quantified before nnn, rrr, mmm, MMM, μ\muμ, jjj, kkk and qqq. A constant allowed to depend on nnn or MMM would make (I.11) unsatisfiable for large CCC and the goal vacuous; that formalization is ruled out.
  • Standing assumptions. The paper assumes n≥C′n \ge C'n≥C′ and m≥2nrm \ge 2nrm≥2nr (I.22) throughout. In the goal and in Corollary 3.5 they are absorbed by CCC, since strong incoherence forces μ≥1\mu \ge 1μ≥1. Theorem 3.4 carries 2nr≤m2nr \le m2nr≤m explicitly. Theorem 3.4 omits r=O(1)r = O(1)r=O(1) and (I.10), since Section V uses only its own proviso m≥nrμ2m \ge n r_\mu^2m≥nrμ2​. Every statement also carries m≤n2m \le n^2m≤n2, without which the uniform model is empty.
  • Probability. The uniform model is the platform's successProb (a ratio of finite counts). The Bernoulli model uses bernoulliEventProb and bernoulliExpectation with p=m/n2p = m/n^2p=m/n2. The logarithm is natural, and the failure probability is written 1 / n^3.
  • Recovery. "Unique solution of (I.3)" is IsUniqueMinimizer: every other matrix that agrees with MMM on Ω\OmegaΩ has strictly larger nuclear norm. Stating recovery conditionally on the existence of a certificate would reduce the goal to Lemma 3.1; the goal instead bounds the probability of recovery itself.
  • Admissible pairs. The index i∈[j]i \in [j]i∈[j] is 0-based, the cyclic successor is finRotate, and the lexicographic order is compared through positions. Pair values are counted in Fin (2j(k+1)+1), which contains every admissible value, so the count is exact and finite.
  • New definitions. centeredTangentProjection (QT\mathcal Q_TQT​), momentMatrix (AAA), and the admissible-pair calculus. Strong incoherence (A1–A2) is the shared definition CandesTao.Shared.StrongIncoherence, used by this mission and by the companion mission II. The QT\mathcal Q_TQT​ definition is drafted independently in mission II.

Contributions are welcome on any milestone. Lemmas 5.1 and 5.2 are finite combinatorics and need no analysis. Theorem 3.4 additionally needs the expansion (IV.4) of the trace moment and the moment bounds for centered Bernoulli variables of Section IV-C. Corollary 3.5 also uses Theorem 3.2 (Rudelson selection estimate) and Lemma 3.3 (replacing PT\mathcal P_TPT​ by QT\mathcal Q_TQT​), which are milestones of the companion mission The Power of Convex Relaxation: Near-Optimal Matrix Completion II.

Selected references

  • E. J. Candès and T. Tao, The Power of Convex Relaxation: Near-Optimal Matrix Completion, IEEE Trans. Inf. Theory 56(5):2053–2080, 2010. https://doi.org/10.1109/TIT.2010.2044061
  • E. J. Candès and B. Recht, Exact Matrix Completion via Convex Optimization, Found. Comput. Math. 9(6):717–772, 2009. https://doi.org/10.1007/s10208-009-9045-5
  • D. Gross, Recovering Low-Rank Matrices From Few Coefficients in Any Basis, IEEE Trans. Inf. Theory 57(3):1548–1566, 2011. https://doi.org/10.1109/TIT.2011.2104999
  • B. Recht, A Simpler Approach to Matrix Completion, J. Mach. Learn. Res. 12:3413–3430, 2011. https://jmlr.org/papers/v12/recht11a.html
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Machine LearningProbabilityStatistics·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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Machine LearningOptimizationProbability+1·Captain: mikedeng1

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 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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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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High-Dimensional Probability XI: Dvoretzky-Milman's TheoremTextbook

Motivation

A striking fact discovered by Dvoretzky in the 1960s (conjectured by Grothendieck, and sharpened into its modern quantitative form by Milman in 1971) is that every high-dimensional convex body, however irregular, contains a round slice: a random low-dimensional section (or projection) of any bounded convex set in Rn\mathbb R^nRn is, with high probability, close to a Euclidean ball — provided the dimension of the slice is small enough relative to a single geometric parameter of the body. This is remarkable because it holds for every bounded set, arbitrarily irregular; no special structure is assumed beyond boundedness. This chapter proves the theorem in its Gaussian form, as a culmination of every geometric and probabilistic tool the book develops: chaining and Dudley's inequality (Chapter 8), the matrix deviation inequality (Chapter 9), and Gaussian width and the stable dimension (Chapter 7) all combine into a single closing argument.

Setting

Fix a subset T⊆RnT\subseteq\mathbb R^nT⊆Rn. For a standard Gaussian vector g∼N(0,In)g\sim N(0,I_n)g∼N(0,In​), the Gaussian width of TTT is w(T):=Esup⁡x∈T⟨g,x⟩w(T) := \mathbb E\sup_{x\in T}\langle g,x\ranglew(T):=Esupx∈T​⟨g,x⟩ (Chapter 7), and the stable dimension of a bounded TTT is d(T):=w(T)2/diam(T)2d(T) := w(T)^2/\mathrm{diam}(T)^2d(T):=w(T)2/diam(T)2 up to an absolute constant factor (Definition 7.6.2) — a robust substitute for the ordinary linear-algebraic dimension of TTT, which can jump discontinuously under a small perturbation of TTT, unlike d(T)d(T)d(T).

An m×nm\times nm×n Gaussian random matrix with i.i.d. N(0,1)N(0,1)N(0,1) entries is a random matrix AAA each of whose mnmnmn entries is an independent standard normal random variable.

Formalization targets

Goal (Theorem 11.3.3, Dvoretzky-Milman's theorem, Gaussian form)

∃ c>0:m≤cε2d(T)  ⟹  P[(1−ε)B⊆conv(AT)⊆(1+ε)B]≥0.99\exists\,c>0:\quad m\le c\varepsilon^2 d(T) \;\Longrightarrow\; \mathbb P\bigl[(1-\varepsilon)B \subseteq \mathrm{conv}(AT) \subseteq (1+\varepsilon)B\bigr] \ge 0.99∃c>0:m≤cε2d(T)⟹P[(1−ε)B⊆conv(AT)⊆(1+ε)B]≥0.99

for every m×nm\times nm×n Gaussian random matrix AAA with i.i.d. N(0,1)N(0,1)N(0,1) entries, every bounded T⊆RnT\subseteq\mathbb R^nT⊆Rn containing the origin, and every ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1), where BBB is the Euclidean ball of radius w(T)w(T)w(T) centered at the origin. The probability 0.990.990.99 is the book's own literal numeral, not a free parameter — this is the theorem the book actually states, not a family of theorems indexed by a confidence level.

Significance

Dvoretzky-Milman's theorem is one of the foundational results of the local theory of Banach spaces (asymptotic geometric analysis): it says every nnn-dimensional normed space contains an almost-Euclidean subspace of dimension proportional to (a geometric invariant closely related to) log⁡n\log nlogn in the worst case, and much larger for spaces whose unit ball is already well-behaved (the stable dimension of the cube [−1,1]n[-1,1]^n[−1,1]n, for instance, is proportional to nnn itself — Example 11.3.6). This underlies results throughout convex geometry, compressed sensing, and high-dimensional statistics wherever a random low-dimensional projection needs to be shown to preserve geometric structure. The book's own framing makes clear why this chapter is placed last: the theorem's proof is a genuine capstone, invoking Chevet's inequality (itself built from the matrix deviation inequality of Chapter 9, which is built from chaining, Chapter 8) as its main technical tool.

The theorem and its proof are classical (Milman 1971; this book's specific route via Chevet's inequality is a standard modern exposition). This mission formalizes the goal theorem's statement — including its two supporting geometric quantities, Gaussian width and stable dimension, and the notion of a Gaussian random matrix — as a complete, faithful target for a solver, in the book's own sub-namespace built for this chapter (no dependency here is reusable from an earlier chunk, since none of this book series' Chapter 7 or Chapter 9 definitions has yet been published).

Difficulty

The natural first idea — bound conv(AT)\mathrm{conv}(AT)conv(AT) directly using concentration of ∥Ax∥2\|Ax\|_2∥Ax∥2​ for each fixed x∈Tx\in Tx∈T — runs into exactly the uniform-supremum obstacle the whole book has been building tools to overcome: a bound that holds for one xxx at a time, even with a union bound over a net of TTT, does not obviously extend to the full convex hull without first controlling sup⁡x∈T∣⟨Ax,y⟩−w(T)∥y∥2∣\sup_{x\in T}|\langle Ax,y\rangle - w(T)\|y\|_2|supx∈T​∣⟨Ax,y⟩−w(T)∥y∥2​∣ uniformly over both x∈Tx\in Tx∈T and yyy on the unit sphere of the target space — a two-parameter supremum. The book's actual route goes through Chevet's inequality, itself proved using the matrix deviation inequality's own chaining-based argument, to control this two-sided supremum, and then converts the resulting inequality into the containment (1−ε)B⊆conv(AT)⊆(1+ε)B(1-\varepsilon)B\subseteq\mathrm{conv}(AT)\subseteq(1+\varepsilon)B(1−ε)B⊆conv(AT)⊆(1+ε)B via a support- function duality argument (a convex body is pinned down by its support function, so bounding sup⁡x∈T⟨Ax,y⟩\sup_{x\in T}\langle Ax,y\ranglesupx∈T​⟨Ax,y⟩ uniformly over yyy on the sphere is exactly what is needed).

Formalization scope

A is Ω → Matrix (Fin m) (Fin n) ℝ with an explicit IsGaussianMatrix hypothesis (entries i.i.d. N(0,1)N(0,1)N(0,1), formalized entrywise with joint independence). conv(AT) is convexHull ℝ of the image of T under A's mulVec, round-tripped through EuclideanSpace's continuous linear equivalence with the underlying function type. w(T) reuses this mission series' ExpSup/GaussianWidth convention (redefined locally, per the drafts-cannot-import-drafts rule, following the same ProbabilityTheory.stdGaussian-based realization of a standard Gaussian vector as 08-matrix-deviation). The stable dimension d(T)d(T)d(T) is formalized directly as w(T)2/diam(T)2w(T)^2/ \mathrm{diam}(T)^2w(T)2/diam(T)2 rather than via the book's literal (but only asymptotically equivalent, per Exercise 7.6.1) definition through a squared Gaussian width h(T−T)2h(T-T)^2h(T−T)2 — the goal theorem's own proof uses only the inequality direction of that equivalence, and the goal's hypothesis already carries an unpinned absolute constant that absorbs the equivalence constant, so this substitution preserves the theorem's exact truth content (see StableDimension's own doc-comment and MODERATION_NOTES.md for the full argument) rather than approximating it.

Ball-center deviation, disclosed. The book's printed theorem statement carries no hypothesis that TTT contains the origin; its proof opens by translating TTT so that it does ("Translating TTT if necessary, we can assume that TTT contains the origin"), and Remark 11.3.4 then confirms the ball is centered at the origin in that case. This mission states the WLOG-reduced case directly — adding 0∈T0\in T0∈T as an explicit hypothesis — rather than also formalizing the translation argument that recovers the fully general (untranslated) statement. This is disclosed as a genuine narrowing of the literal printed statement, though not of what the book's own proof actually establishes.

This mission covers Theorem 11.3.3 only, with no milestones: BRIEF.md explicitly instructs that if the chapter's full proof chain (general matrix deviation inequality, Chevet's inequality, random projections of sets — Theorems 11.1.5, 11.2.4, 11.3.1) proves too heavy for the session, milestones should be cut rather than the goal substituted. All three are left out, not approximated, given this chapter's five from-scratch definitions already needed for the goal's own statement. ExpSup, GaussianWidth, StableDimension and IsGaussianMatrix are reusable by any later development needing Gaussian width, the stable dimension, or a Gaussian random matrix. Solvers' contributions are welcome on the goal theorem itself and, beyond this mission's current scope, on the three named milestones.

Selected references

  • A. Dvoretzky, Some results on convex bodies and Banach spaces, Proc. Internat. Sympos. Linear Spaces (Jerusalem, 1960), 123–160.
  • V. D. Milman, A new proof of A. Dvoretzky's theorem on cross-sections of convex bodies, Funkcional. Anal. i Priložen. 5 (1971), 28–37.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 11. https://doi.org/10.1017/9781108231596
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